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A fuel-efficient cruise performance model for general aviation piston engine airplanes

19830025620 · NASA · 1983

Public domain · NASATechnical Reports

Overview

A fuel-efficient cruise performance model which facilitates maximizing the specific range of General Aviation airplanes powered by spark-ignition piston engines and propellers is presented. Airplanes of fixed design only are considered. The uses and limitations of typical Pilot Operating Handbook…

Publisher
NASA
Document
19830025620
Year
1983
Pages
399
Chapters
19

Key points

  • The study defines a fuel-efficient cruise performance model for general aviation airplanes powered by spark-ignition piston engines.
  • Specific Range (R*) is the ground distance flown per unit mass of fuel consumed during cruising flight.
  • The model aims to minimize fuel consumption and improve safety in general aviation operations.
  • The study focuses on optimizing R* during cruise, as most fuel is consumed in this phase of flight.
  • The implementation of the cruise performance model can help pilots compute fuel requirements and adjust flight plans to ensure adequate fuel reserves.
Frequently asked questions
What is the purpose of the fuel-efficient cruise performance model?

The purpose is to define a model that facilitates maximizing Specific Range (R*) for general aviation airplanes.

What does Specific Range (R*) represent?

Specific Range (R*) represents the ground distance the airplane flies per unit mass of fuel consumed in cruising flight.

How does the study aim to improve safety in general aviation?

The study aims to improve safety by reducing fuel exhaustion and mismanagement, which are major causes of accidents.

What is the significance of optimizing R*?

Optimizing R* is significant because it can lead to a substantial reduction in fuel consumption during cruise, which is where most fuel is used.

What kind of airplanes does the study focus on?

The study focuses on general aviation airplanes powered by spark-ignition piston engines and considers only fixed design airplanes.

Chapter 5 discusses tHe perfermance ef naturally aspiTated

Chapter 5 discusses tHe perfermance ef naturally aspiTated r 51 pisten engines, and develops the NEA subsystem input-eutput medel.

Chapter 6 integrates the APA ami. NEA subsystem input-output medels to. form the new cruise perfermance model ef the airplane- atmesphere sys tem. The implementatien, use, and engine centrel requirements ef this new medel aTe discussed. Thepercentage increases in R* offered by the implementatien ef this new model in any GA airplane, relative to. R* achieved when eperating that airplane in accerdance with current GA practice. are estimated.

Finally. this new medel is compared with the POll cruise perfermance medel develeped in Chapter 2.

Chapter 7 presents cenclusio.ns and recemmendatiens as a result ef this study.

Appendix A discusses the fundamentals ef the Peint Economy Functien R*. The reader is urged t.e read tliis appendix prier to commencing a detailed reading of Chapters 3 through €> .• Appendix B describes the standard and' non-standard atmosphere models used threughout this study.

Appendix C develeps the airframe perfo~ance model used in Chapters 3 and 4.

Appendix D develops the propeller perfoTmance mo'deI us'ed in Chapter 4.

Appendix E develops the naturally aspirated sr piston engine

performance model used in Chapter 5'.

1-16 ---------------------------------- --Kpp-end-i-:iC-F-pre-senn--a--ori-ef--d-t-s-c-us-s-i(Yn-o-f---alTt-oi-gn-id-o-n-;-- -------- ------------------------------ \ detonation and knock in spark-ignition piston engines.

Following Appendix F, there is a tabulation of the nomenclature -I used throughout the chapters of this study (other symbols used in the appendices are defined locally). For historical reasons, and in consideration of other peoples' work, a conventional notation has been maintained throughout; this has sometimes resulted in the same symbol being used for different quantities. For the same reasons, English rather than Metric units have been used throughout.

Finally, the list of References is presented. Reference numbers in this list are cited in parentheses throughout the text.

Interesting Results Without unduly anticipating the logical conclusions, presented in their separate place, it may be appropriate here to consider briefly some of the difficulties overcome in, and interesting results of, the research. Given that the problem of maximizing specific range, R*, is significant, one finds that it is not amenable to theoretical solution. On the other hand, one finds that costly experimental or test data which have been accumulated are inadequate for the purpose at hand. The thesis is the propo- sition, in detail, of a prescription for experiments to be made.

I first review classical airplane cruise performance. In

principle this is very well understood. A new iTterpretation, 1-17 however, ·of that performance is given inasmuch as 1. The effects of wind and auxiliary equipment power on R* are presented in terms of new Equivalent Quantities.

2. The effects of center of gravity (c. g.) position on R* are specifically formulated in terms of a) R* appropriate to a reference c.g. position, and b) A correction factor for variations in c .g. position.

Next, classical propeller performance is reconsidered. A compact representation of the combined performance of the airframe and the propeller in terms of novel Corrected Quantities is made.

In particular, 1. Propeller performance is presented in terms of a novel non-dimensional quantity, the Speed-Thrust Coefficient, CR' This, in conjunction with the well known propeller advance ratio, facilitates computations of the effects of equivalent airspeed, gross weight, c.g. position, propeller shaft speed and atmospheric density ratio on propulsive efficiency.

2. The effects of compressibility on propeller performance are represented by a correction factor, f . Such a comp correction factor is not new, but has passed out of use since the advent of modern computational fluid mechanics.

This study identifies the importance of f for compact comp computations of General Aviation eGA) airplane c.ruise per- "1 formance; and recommends further effort in quantifying f for GA propellers.

comp 1-18 ~ ,

I

:------ -------- _~'_:::::::::::t::i::~::::::::~:::~::;::~:::~--------

I subsystem cruise performance for all values of gross weight and altitude.

Further then, I synthesize a fuel-efficient steady state per- formance model of naturally aspirated Spark-Ignition (SI) piston aero engines from a widely scattered literature. Using this model, novel Corrected Quantities are identified. The cruise performance of the Naturally aspirated MBT ignition timing Engine-Atmosphere (NEA) subsystem is then represented in terms of these Corrected Quantities.

The subsystem integration is summarized in a single block diagram illustration (Figure 6.1). This figure is an original, logical abstraction of the developments and models which are presented in the body of the work. It shows the connection between the important inputs and "controls" and the overall system per- formance which is of interest.

All this appears to have significant implications for efficient and safe GA airplane operation. Finally, 1 present calculations of the fuel savings which might be obtained by improved computer- aided operating practices. Increased specific range, R*, is conservatively estimated to be 20% to 26%.

1-19 TABLE 1.1 PARAMETERS CONTRIBUTING TO R* Variable Contributing Parameters V Equivalent airspeed E P Atmospheric ambient air absolute pressure atmos T Atmospheric ambient air temperature atmos V Geocentric wind speed and direction w Airplane heading Airframe power-off drag coefficient where W gross wei gh t airplane = he longitudinal center of gravity = position - c mearr aerodynamic chord of the wing = V Airplane true airspeed T P atmos T atmos P Auxiliary equipment power AUX

-

Propulsive efficiency = np[V , W, h, N, 0, r'1yJ np E

where N = propeller shaft rotational speed

o = atmospheric air density ratio

Mr = propeller helical tip Mach number

c The following apply to naturally aspirated and turbo- charged SI piston engines: Fuel mass flow rate per engine 1-20 ~ i ~

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1- ~ ---- -------- - -------------. -..(;~~~)-------------.----------

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Engine geometry and grade of fuel

1 I

These define Fuel-dry air mass ratio the I gni tion timing Indicated Engine shaft rotational speed Horsepower (IHP) Inlet manifold absolute pressure Inlet manifold temperature Exhaust absolute back-pressure Cylinder head temperature Detonation .....

Engine geometry These define the Lost p Horsepower m (LHP) p e IHP Indicated horsepower The following apply to Turbocharged SI piston engines: Turbocharger characteristics Aftercooler characteristics Throttling absolute pressure losses 1-21

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CHAPTER 2

-------------------------------- -------------- ------------------------------------------ ------------------------------------ - ------- ---------- ----------------- -------- CHAPTER 2 USES AND LIHITATIONS OF POH CRUISE PERFORMANCE DATA FOR MA~(IMIZINC; R* Table of Contents Page I NTRODUCTI ON. . . . . . . . . . . . . . . . . . . . • . . • . • • • • • • . • • . . . . . • . • . • . . .• 2 -1 PILOT OPERATING HANDBOOK DATA •••••••.•••••••••••••.•.•••••.• 2-1 CONSTRUCTION OF A CRUISE PERFORMANCE MODEL FROM POH DATA •.•• 2-3 Fuel F low Diagrams. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. 2-4 Power Diagrams ......................................... 2-6 Tne POHCPM... . . . • . • • • • • . • . • • . • . . • • • • • • • • • . • • • • • • • • . • • •. 2-7 APPLICATIONS OF POH CRUISE PERFORMANCE HODELS •••••...••••••• 2..:9 The Computation of R* ......•.•.•..••••.•.....••.••••... 2-11 Flight at Maximum Groundspeed .......................... 2-12 Flight at ~1aximum Possible R* .............. , ........... 2-14 Flight at a Prescribed TAS ............................. 2-17 Flight at a Prescribed Groundspeed ..................... 2-18 LIMITATIONS OF POll DATA FOR MAXIMIZING R* ••••••••.•••••••.•• 2-20 SUMMARY AND CONCLUSIONS .••.•.••••••..••••••••••••••••.•••• " 2-21 Summary. . . . . . . . . . . . . . . • . . . . . . . . . • . . . . . . . . • . . . . . . . . . . . .. 2-21 Concl usions .....................•.................... " 2-21 TABLES 2.1 - 2.3 ................•........•......•.•.....•... 2-23 FI ClJRES 2. 1 - 2. 11 • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •• 2 - 26

CHAPTER 2

CHAPTER 2 USES AND LIMITATIONS OF POH CRUISE PERFORMANCE DATA FOR MAXIMIZING R*

I NTRODU cn ON

The manufacturers of GA airplanes provide detailed cruise per- formance data for each airplane sold. These data are available in the airplane Pilot Operating Handbook (POH) and in the Federal Aviation Administration approved Flight Manual for each airplane.

This chapter describes the construction of cruise performance models frOT;) POB data, and examines the usefulness and limitations of such models for maximizing R*.

The pilot operating handbooks of a number of typical GA air- planes are first examined. The construction of cruise performance models incorporating the common cruise performance variables in this POll sample is described, and this is illustrated for two GA airplanes.

The use of a POH cruise performance model for maximizing R* is dis- cussed, and illustrated for one GA airplane. Finally, the limitations of POH cruise performance models for maximizing R* are discussed.

PILOT OPERATING HANDBOOK DATA A sample of Pilot Operating Handbooks was examined in order to determine what variables are commonly included in the cruise performance data of such handbooks.

Ten airplane types and four manufacturers were represented in the sample. These are listed in Table 2.1, along with the operating 2-1 point variables included in the POlf cruise performance data: and the operating conditions pertaining to' those data. Single' and twin engined airplanes are included in' the' list" some with naturally aspirat'ed '(', engines and others with turb-acharged engines.

The five variables common to each airplane listed' in Table 2.1 are: 1. Pressure altitude 2. Engine rotational speed 3. Engine inlet Manifold Absolute Pressure (MAP) 4. Fuel flow rate 5. True airspeed (TAS) This constitutes the majority of the listed variables.

Some of the sampled POH's specify a leaning criterion to establish the given fuel flow rates, such as an Exhaust Gas Temperature (EGT) relative to peak EGT, or a Turbine Inlet Temperature (TIT) relative to peak TIT. However, it is not clear in every case what 1 eaning procedure results in the given POH fuel flow rates. In those cases.

where the leaning criterion appropriate to the cruise performance data is clearly established in the POH: the POB informs the pilot of the TAS and fuel flow rate which will result when the airplane is flown at various pressure al titudes, wi th various combinations of ,.

MAP and RPM, under certain operat.ing conditions Cone of- which is the leaning criterion). In those c'ases where the leaning criterion appropriate to the cruise performance' data: is not c1ea·rly established in the F')H: the PUR informs the" pi.rot of the' TAS which· win result 2-2 I I

I

,

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~-~~----------~~~~-f~~~~ar~p~~~~~tu~~~-V~i~---~---------

~,

j

I combinations of MAP. RPM and fuel flow rate. under certain operating

conditions (excluding a leaning criterion).

' Sufficient information is given in each POH for the computation

of R* (Equation A.7) throughout the operating range documented.

given a knowledge track. However.

of the prevailing winds peed along I I in no case listed in Table 2.1 does the form of data presentation

I

facilitate maximizing R* in current operations.

CONSTRUCTION OF A CRUISE PERFORMANCE MODEL FROM POH DATA This section shows how the POH cruise data for an airplane may I I be used to construct a cruise performance model which facilitates the computation of operating points which maximize R* in the cruise operation of that airplane: a cruise performance model constructed i from POH cruise data is referred to as a POHCPM. The cruise data for the 1974 Cessna Centurion and the 1974 Cessna Turbo Centurion t are used for this purpose the former airplane employs a naturally aspirated engine, and the latter a turbocharged engine.

The cruise operating point variables. presented in the POH data for each of these two airplanes. are the first six variables listed in Table 2.1. The POB data format for these two airplanes is that shown in Table 2.2. The POHCPM of each of these airplanes. con- structed here from their POH data. is comprised of the following plots: t The data for these airplanes were taken from the airplane Owner's Manual in each case. The information contained in these manuals is issued for more modern airplanes in the POH. These two Owner's Manuals are here referred to as Pilot Operating Handbooks in keeping with this practice.

2-3

1. Fuel flow rate m (lbm/hr) versus true airspeed'V (statute

f T t mph), for constant values of pressure altitude eft). Such plots are referred to as Fuel Flow Dia'gt:arns.

2. MAP (inches Hg) veTS,US "V . (s:ta.tute mph) , for :constant T values of pres'surealtitude fft) ,and 'engine RPM. S:uch plots are referred to ,as Power Diagrams.

The source POH data for each of these models ,and hence th'emode1s themselves, ,apply only to the 'following operating conditions: 1. Extended range mixture (fuel~air mass ratio) : established by leaning to a specified EGT increment rich of peak EGT 2. Standard atmosphere 3. Specified gross weight 4. Fixed (but unspecified)longi'tudinal centero'f gravity (c.g.) position 5. Undercarriageretrac'ted 6. Flaps up 7. Cowl flaps: position 'not determined by author. How'ever, cowl flap position was commensurate Mithrequired Cylinder Head Temperature rCHT) in each case 8. Some specific configuration of avionics aerials and other external equipments.

;i: Fuel Flow Diagrams The POH fuel flow data for the 1974 Cessna Centurion 'and Turbo Centurion are plotted against TAS for fixed values of pressure 2-4 2 3 + + a (2.1)

V = a a a V

roof Vr + T 1 2 3 T 0 -t is fitted through the fuel altitude in flow data at each pressure these two figures. T'ne data points pressure altitude fall for .each very close to the fitted curve, the standard deviation being less than 0.5 lbm/hr in every case, except for the Turbo Centurion at 20,000 ft where the standard deviation is 0.73 Ibm/hr. Each data point corresponds to a reconunended combination of MAP and RPt>1. For this Cessna data, it is apparent that every combination of MAP and RPM, given in the POH and yielding a given TAS, corresponds to a fuel flow rate ro lying very close to the relevant altitude curve. The f t curves of Figures 2.1 and 2.2 are therefore taken to apply to all t combinations of MAP and RPM within the limits of the POH data.

The hatched boundaries of Figures 2.1 and 2.2 represent the reconunended upper cruise power limits for the respective airplanes (see also Reference 4, p. 414). Such boundaries correspond either to the maximum percentage of maximum continuous power (brake horse- power) which the manufacturer recommends for continuous normal cruise operation; or to the maximum available cruise brake horsepower when this is altitude limited; whichever is the smaller power level.

Occasionally, as in the case of the 1974 Centurion, some of the tabu- lated data points lie outside this boundary and are presented in the t This close proximity of ro to a single curve, for various combinations f of MAP and RPM at one altitSde, should not be taken as an indication that MAP and RPM have no effect on R* (see Chapter 5).

2-5 POH merely for interpolation purposes. The boundary should be drawn (as in Figure 2.1) on the basis Qf the manufacturer's recommendation and not as the upper power limit of the data tabulated for each pressure altitude. The recornrnend.ed power boundaries of Figures 2.1 and 2.2 both represent 75% maximum continuous brake hQrsepower, or less when altitude limited.

Power Diagrams The engine MAP and RPM corresponding to the (m ' VT) data points f t

of Figure 2.1, at sea level and ro,ooo ft, are plotted in Figure 2.3

for the Centurion. Similar plots corresponding to the (m ' VT) data f t points of Figure 2.2, at sea level and 20,000 ft, are shown in Figure 2.4 for the Turbo Centurion. It is apparent from Figures 2.3 and 2.4 that a great deal of redundant engine s.etting data are availabl e to the pilot for the cruise operation of these airplanes: at each TAS and pressure altitude, an infinite number of (MAP, RPM) combina- tions may be selected. At each TAS, one recorranended combination of MAP and RPM would suffice. In Figures 2.3 and 2.4, a straight line has been drawn through the set of data points appropriate to each pressure altitude. Each straight line represents an arbitrary tra- jectory of (MAP, RPM) over the TAS range at each pressure al ti tude: l l points (a, a ), (b, b ) etc. on these straight lines correspond to (2200), (2300) RPM etc. respectively. When all of the (MAP, RPM) data for one airplane are plotted against TAS, and a straight line inscribed for each pressure altitude, a unique combination of (MAP, RPM) 2-6 i I

I

I I

I

j-- :~----------may-bepres crIbe.ffor flight at any- T AS-aIid-pressuie-afiTtude-by1n~------------ I terpolating between the inscribed straight lines.

Figures 2.5 and 2.6 show the results of the above construction I ' .for the Centurion and Turbo Centurion respectively. The s traigh t lines of constant pressure altitude correspond to the inscribed

I

straight lines in that construction.

Points a, a etc. in Figure ' 2.5 (2.6) correspond to points a, a' etc. respectively in Figure

I

2.3 (2.4). Lines of constant RPM are shown dotted in Figures 2.5 and 2.6.

Plots such as Figures 2.5 and 2.6 are referred to as Power Diagrams. The fuel flow rate shown in the Fuel Flow Diagram drawn for a specific set of operating conditions, corresponds to the MAP and RPM in the Power Diagram drawn for the same set of operating conditions, at the same TAS and pressure altitude. Consequently, variations in m with MAP and RPM, at any TAS and pressure altitude, f t are accounted for in these Diagrams.

The POHCPM Figures 2.1 and 2.5 constitute a POHCPM of the 1974 Cessna Centurion, for the operating conditions stated in Figure 2.1. Figures 2.2 and 2.6 constitute a POHCPM of the 1974 Cessna Turbo Centurion, for the operating conditions stated in Figure 2.2.

The cruise performance of any GA airplane, flying in specified atmospheric conditions with a specified gross weight and c.g. position, may be completely described by one Fuel Flow Diagram and one corre- 2-7 sponding Power Diagram. (The units used in these Diagrams would be Nautical mph or Statute .mph,andlb/hror gallons/hr, .in accordance with the POH data.) Di.ffer.entFuelFlowand Power Diagrams are required to describe the airphan-e perfo.rmance for different values of: 1. Atmosl'herictempera'tureatfixed pressuT~ealti tude, 2. Gros's 'weight, 3. C.G. position.

Each pair of Diagrams would b.e;appropriate to: 1. A mixture (fuel-air 'm'3'5:sratio)esta'blished by.a specified . .. t l eanlng cTlterl0n, Undercarriage retraC'ted, 2.

3. Flaps up, 4. Cowl flaps ei therclos,ed,or .openedthe·amountnecessary to achieve a specified.CHT, ~., 5. A specified configurat:ion ;.of.avionics aerials ,and other external equipments.

The cruise performance of ,%any GA airplane in all operating con- di tions should be well repres'ented by linear interpolation between pairs of Fuel 'Flow and Power DIagrams for the ,c.onditions l-l2listed in Table 2.3. Such a set of Dia.grams, for a'given'airplane, would constitute a PGHCPM applicable to ,aU operating condi tionsof .that airplane. In the event that ·the Diagrams are found to be influenced little by c.g. position, pairs of Diagrams 'for conditions 1-6 only , i ':

i

tDiscussions with the GA manufa:cturers indicate that,&oodT~peatability of fuel flow rate, in given-atmospheric conditions and'ata given MAP and RPM, is achieved using a leaning criterion based 'onEGT or TIT, although no repeatability 'statisticswere made available to the author.

f :02-8

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I i L--.-----------------------wLu--suf£ic.e-t.o--descrihe-_the __ p_er.formanc_e .• ____ Th_e_)la~-u-e_QL-R~-.i-nc-~~~-~~------------------l ' ~~

l . continuously as the c.g. is moved from the forward limit to the aft I

I 1

I limit (see Chapter 3) so that the choice of conditions 1-6 only would !

~ I

be a conservative one. If the range of gross weights were great, it may be desirable to include an intermediate gross weight in the POHCPM.

Three values of anyone parameter in Table 2.3 affords the use of parabolic rather than linear interpolation for that parameter.

While the use of Fuel Flow and Power Diagrams reduces POH cruise data to a simple form for fixed conditions, the prospect of manually interpolating between 6 or more pairs of such Diagrams is a daunting one. However, this task is a simple one for a computer, and may be performed enroute by a microprocessor installed in the airplane.

The POHCPM may be stored in a microprocessor as sets of coefficients of cubic polynomials (describing the Fuel Flow Diagrams: see Equation 2.1) and straight lines (describing the Power Diagrams).

The following section describes some of the uses of a POHCPM.

APPLICATIONS OF POH CRUISE PERFORMANCE MODELS One obvious function of a POHCPM of a given airplane is to inform the pilot of the engine power (MAP, RPM) settings required to fly that airplane in any given operating conditions. The model is entered with values for: 1. TAS 2. Pressure altitude 3. Atmospheric temperature relative to standard 4. Gross weight 2-9 5. Center of gr.avity position and values of MAP and RPM aroe returned. The corresponding fuel flow rate, also obtainable from the POHCPM, ·would h.e established by the pilot using the le.aning c:rit,eri.on appropriate to the POHCPM Cor established directly using £n'el flow instrumentation) ..

However, a PQHCPM has wme more important uses than the compu- tation of MAP and RPM (and fuel flow rate) for specified flight COR- di tions. In this section 'weexamine the use ofcruis·e performance models for various optimizations. Inpa.rticular ,we examine the ,compu- tation of the operating point., for a particular .airplane, which sa tisfies the following alternative requirements; 1. Achieve maximum ground'speed, with an R*constraint 2 . Achi eve max imum poss ibl e R* . Maximize 3. R* while flying at a prescribed TAS whil:e at groundspeed.

4. Maximize R* fly:Ln:g a pres.cribed The use of cruise performance ::models for the ,computation of R* is first described, with the aid of the 'POHCPM of the 1974 Cessna Centurion: Figures 2.1 and 2.5. The above .four optimizations are then discussed in turn, using -the POHCPMof th:e 1974 Cessna Turbo Centurion: Figures 2.2 and 2.6. Throughout t-hesediscuss:ions~ the operating conditions areassum.ed to ,conform to thec.ondl tionsper- taining to Figures 2.1 and 2.2. Zero and non-zero wind conditions are considered: computations involving the latter employ the wind -profile shown in Figure 2.7.

2-10 the Fuel Flow Diagram, which is a graphical representation of Equation A.7:

v + V

T w t ground miles/lb (2.2) ID f t where

VG = groundspeed, mph

TAS, mph V

=

T V true windspeed component along track (see Appendix A), mph

=

w Headwind: V < 0 w Tailwind: V > 0 w

ID = Total fuel mass flow rate to all engines, lbm/hr

f t (ga11ons/hr) .

Con?ider the Fuel Flow Diagram of the 1974 Cessna Centurion: Figure 2.1.

In zero wind conditions, operation at any TAS and pressure al- titude is represented by a point on Figure 2.1: the horizontal coord- inate of the point gives the TAS (=V ), the vertical coordinate gives G the fuel flow rate, while the inverse slope of the radial line from the origin to the point gives the value of R*. For example, flight at 2,500 ft pressure altitude and 169 mph TAS (Point A in Figure 2.1)

results in a fuel flow rate ID = 87 lb/hr from which R* = 169/87 =

f t 1.94 ground miles/lb.

t(Nauticalor Statute) miles/(lb or gallon) in accordance with POH data. The present examples use statute miles/lb.

2-11 In non-zero wind cond'itions, R* is again re'adily obtained from '.

Figure 2.1. The windspeed may be represented, by plotting V alorig w the abscissa; headwinds plotted t.o the right of the origin and tail- winds to the left. Then for any operating point (TAS, Pressure Altitude: Point A say) and wind condition (Point B say),- the ground- speed is the base BC of the triangle ABC, and the value of R* is given by the inverse slope of the hypotenus'e BA.

The MAP and RPM required for flight at any given TAS and pressure a1 ti tude are obtained from the corresponding Power Diagram (Figure 2.5), and are independent of w-indspeed. The MAP and RPM, corresponding to point A in Figure 2.1 are; MAP = 24 in. Hg, RPM:: 2425.

We now address the four optimization problems previously men- tioned, using the POHCPM of the 1974 Cessna Turbo Centurio.n shown in Figures 2.2 and 2.6.

Flight at Maximum Groundspeed We here demonstrate the usee, of the POHCPM for computation of the operating point yielding maximum groundspeed with an R* constraint.

i I n zero wind conditions, maximum groundspeed is achieved by flying at the altitude where the maximlDD TAS is achieved. This al- titude and the corresponding maximumTAS is represented for the Turbo Centurion by point A on the power boundary of Figure 2.2.

I t may be impossible to fly at point A because of insufficient fuel capacity; that is, R* at point A may be unacceptably small. Let us assume that a fuel constraint exists which requires R* to be greater than or equal to some' minimum value R*. Plotting a 1 ina with c 2-12 ; I

I

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j~~ ~--- ~~- ~-~~---~~-~---l>1ope-l,lRt*lb-per--hr-JmphJ-onJig~re-2.2-m"l'-resuLLin-line-1lR.-~i" -------- -- -- ---~- ---

I , ::::d:::: t::i::t::~:i:::t:: :::U::: ::::::: ::l~:::Ven by

the point on the power boundary furthest to the right and on or below

I

the line OS: point B in the case drawn. Clearly if line OB intersects the power boundary above A, then maximum groundspeed may be achieved

l

without violating the fuel constraint by flying at A.

I~

However, only a few specific altitudes are available to the pilot, many being precluded by topography, weather, cabin environment requirements, air traffic control or perhapsNOT~1S.t As a result, it may not be possible to fly at A or B in Figure 2.2. The operating point for maximum groundspeed is then determined as the point at an

I

available altitude on or within the power boundary, on or below line OS and furthest to the right. For example, if all altitudes above 20,000 ft were unavailable, the operating point for maximum groundspeed would be point C.

In nono-zero wind conditions with no fuel constraint, maximum groundspeed is obtained in all cases by flying at point A on the power boundary of Figure 2.2. When the fuel consumption constraint R* > R* is imposed, the procedure for determining the altitude and - c TAS for maximum groundspeed is similar to that used in the zero wind case. In fact the analysis varies from the zero wind case only inas- much as the line OB with slope l/R* is drawn for each altitude separately, c the origin 0 being shifted along the abscissa to the wind component prevailing at each altitude.

I t NOTAM : Notice to airmen.

2-13 For each cruising altitude the procedure is as follows. Consider cruise at 10,000 ft pressure altitude when the minimum tolerable value of R* is R* = 2.35 miles/lb, and the winds aloft V are given by c w Figure 2.7:

1. V = 15 mph tailwind

w 2. Plot point D on Figure 2.2 corresponding to this windspeed V w

3. Plot line DE 'with slope l/R~ = 1/2.35 (lb perhr./mph). It

is possible to fly at any operating point on the 10~OOO ft line, on or below line DE.

4. To achieve the maximum allowable TAS and hence maximum groundspeed, assume flight .at point E. The groundspeed is given by VG = 177 + 15 = 192 mph.

Flight at other pressure altitudes i.s tre:at.ed in .similar fashion. The resul ts of these computations for all pr.essureal titudes from sea level to 25,000 ft are shown in Figure 2.8. There the computations are tabulated and the maximum groundspeed achievable at each pressure altitude is plotted against pressure altitude. The maximum possible groundspeed is achieved at 25,000 ft even though the largest headwind exists there. The value of R* is the same at each pressure altitude.

The engine fuel flow rate, MAP and RPM required fOT a chosen pressure altitude and TAS are obtained from Figures 2.2 and 2.6.

Fli'ght at Maximum Possible R* We here demonstrate the use of the POHCPMfor computation of the S' operating point yielding the maximum possible value of R* .

2-14 j I

I

I

" -----------------------------------------hr --zero-willd--colldi-ti-ons-;--t-he-max-imum-va-lue--o-f--R-*--aeh-ievab-l-e----at -~ .

t

I a particular altitude is obtained by flying at the point of tangency

of a radial line from the origin to the appropriate altitude curve of Figure 2.2. At sea level this flight condition is at point F in

I'

Figure 2.2; at 25,000 ft it is at point G. The pressure altitude and TAS offering the maximum possible R* correspond to the point in Figure 2.2 at which the slope of the tangent line from the origin is least (Equation 2.2).

In non-zero wind conditions the tangent line is drawn from the appropriate wind reference rather than from the origin. For example, when flying at 25,000 ft with a 40 mph headwind, maximum R* is achieved at H in Figure 2.2 rather than at G. The pressure altitude and TAS offering the maximum possible R* correspond to the point at which the slope of the tangent line drawn from the appropriate wind reference is least.

It is of interest to determine the altitude variation of the maximum value of R* achievable at each altitude (R* ) for the Turbo max Centurion. For zero wind conditions, inspection of Figure 2.2 reveals that the value of R* increases continuously from sea level to max 25,000 ft as follows:

Sea level (point F): R* = 130/57 = 2.28 miles/lb

max 25,000 ft (point G): R* = 175/70 = 2.50 miles/lb.

max This represents a variation of 9.65% of the lower value. For non-zero wind conditions, the variation depends upon the wind profile. Using the wind profile of Figure 2.7 the value of R* from sea level to max 2-15 25,000 ft has been computed and plotted inFig~re 2.9. The compu- tations, tabulated in Figure 2.9, were performed as follows at each pressure altitude: 1. V was taken from Figure 2.7 and inscribed on the abscissa w of Figure 2.2 as the wind reference 2. VT and the fuel flow rate ID were determined from Figure f t 2.2, at the point of tangency of the straight. line drawn the wind from reference to the appropriate alt:itude curve 3. V = V + Vw G T 4. R* = V G/IDf max t The computed values of R* plotted in Figure 2.9 show a maximum vari- max ation of (2.67 - 2.39)/2.39 or 11.7% of the lower value. In-this example the wind profile has increased the percentage variation of R* with altitude from that obtained in the zero wind case.

max At any pressure a1 ti tud e on the curve 0·£ Figure 2.9, the T AS may be oltained from a linear interpolation of' the TAS values tabu- 1ated in that figure. For these values of pressure aTtitude and TAS, the engine fuel flow rate, MAP and RPM are determined from Figures 2.2 and 2.6.

When a fuel constraint dictates a minimum value of R*, some al ti tudes in Figure 2.9 may be excluded from candidacy for a particular operation. Other constraints JIlay also preclude operation at· certain altitudes in Figure 2.9. In such cas:es, Figure 2.9 clearly shows the available pressure a1titude'yielding the maximum possible value of R*.

2-16 Flight ~.:t a Y;rescribed TAS To achieve an approximate trip duration, a pilot may choose to fly at a particular TAS. We here demonstrate the use of the POHCPM to compute the operating point which maximizes R* at a specified TAS.

The method of computation is independent of the choice of TAS: it is here illustrated for a TAS of 185 mph, for which all operating points lie along the line JK in Figure 2.2.

In zero wind conditions, the value of R* is determined at each

altitude as R* = VT/m at the intersection of line JK and the appro-

f t priate al ti tude curve. In this case the value of R* increases con- tinuQusly from 5,000 ft to 25,000 ft as follows:

5,000 ft: R* = 185/98 = 1.89 miles/lb

25,000 ft: R* = 185/74 = 2.50 miles/lb.

This represents a variation of 32.3% of the lower value. Note that flight below 5,000 ft is not possible at this TAS due to the presence of the power boundary.

In non-zero wind conditions, the altitude variation of R* is determined as follows. At each pressure altitude: 1. The fuel flow rate ro is obtained from the intersection of f t the line JK and the appropriate altitude curve 2. The wind component V is obtained from Figure 2.7 w V + V 3.

=

VG T w 4. R* VG/ro

=

f t

Figure 2.10 tabulates these computations for V = 185 mph and shows

T R* plotted against pressure altitude. For the wind profile used, the 2-17 value of R* varies little above 15,000 ft, reaching a maximum at x' 25,000 ft even though the maximum headwind exists there. The maximum variation of R* in Figure 2.10 is (2.42 - 2.02)/2.02 or 19.8% of the lower value. In this example the wind profile har> Significantly de-, creased the percentage variation ofR* wi thaI titu&e, from that ob- tained in the zero wind case.

At any pressure altitude the engine fuel flow rate, MAP and RPN required for flight at a TAS of 185 mph are obtained from Figures 2.2 and 2.6.

A fuel constraint which dictates a minimum value of R*, or some other constraint, may preclu&e operation at certain altitudes. In this event, Figure 2.10 clearly shows the available pressure altitude yielding the maximum value of R* at the prescribed TAS.

Flight at a Prescribed Groundspeed This mode of operation may be selected to satisfy a particular trip duration. We here demons'trate the use of the POHCPM to compute the operating point which maximizes R* at a specified groundspeed. 'The method of computation is independent of the choice of groundspeed: it is here illustrated for a groundspeed of 200 mph.

In zero wind conditions, the method is identical to that shown above for a prescribed TAS. In this case the value of R* increases I .. I continuously from 13,500 ft on the power boundary to 25,000 ft as follows:

13,500 ft: R* = 200/98 = 2.04 miles/1b

2-18 ---- ------------------ ----- ------ --2-5,000-f-t+-R-*---=----200/-81-.5--=---2-.-4-5--mi-l-es-/-l-b-.----------------------------------------- This represents a variation of 20.1% of the lower value.

In non-zero wind conditions, the altitude variation of R* is determined as follows. At each pressure altitude: 1. The wind component V is obtained from Figure 2.7 w I 2. The TAS is computed as V~ = V - V I- 1 G w 3. The fuel flow rate ro is obtained at the intersection of f t this V line and the appropriate pressure altitude curve in T Figure 2.2 4. R* = VG/inf t Figure 2.11 tabulates these computations for VG = 200 mph and shows R* plotted against pressure altitude. For the wind profile used, the value of R* reaches a maximum at 25,000 ft where the maximum headwind occurs. The maximum variation of R* in Figure 2.11 is (2.38 - 2.22)/ 2.22 or 7.21% of the lower value. The wind profile employed in this example has significantly reduced the percentage variation of R* with altitude, from that obtained in the zero wind case.

At any pressure altitude on the curve of Figure 2.11, the T AS may be obtained from a linear interpolation of the TAS values tabu- lated in that figure. For these values of pressure altitude and TAS, the engine fuel flow rate, MAP and RPM are determined from Figures 2.2 and 2.6.

As for the previous analyses, a fuel constraint which dictates a minimum value of R*, or some other constraint, may preclude operation at certain altitudes. In this event, Figure 2.11 shows the available 2-19 pressure altitude yielding the maximum value of R* at the prescribed groundspeed.

LIMITATIONS OF POH DATA FOR MAXIMIZING R* A POHCPM can only maximize R* subject to the constraints imposed by the source POH data. Two sets of such constraints are listed be- low: these constraints constitute typical significant limitations of POB data for maximizing R*.

1. POH cruise data pertain to specific values of (see Figure 1.1) : a) Gross weight W: data for more than one value of gross weight are often unavailable b) e.G. position h: data taken for more than one c.g. position has not been observed by the author for any GA airplane c) Pressure altitude and atmospheric conditions: data for specific pressure altitudes and standard atmospheric conditions are usually provided, and in many cases data for certain non-standard atmospheric conditions at these pressure altitudes are also provided.

Interpolation for performance in all cruise flight conditions is only possible when multiple data sets are provided.

2. POH data give the performance which can be expected when the airplane is operated in accordance with the manufacturer's recommendations. Those recomm'endatiorrs constrain the fol- lowing engine variables (see Figure 1.1) : P a) Inlet MAP m 2--20

I--~: ------ --- --~- ~-- -- ~ ~-1»--£ngine-=t~Hona±-.peed----~-~---- -~-NE- ------

I

c) Fuel-air mass ratio F d) Engine ignition timing The effect of each of these variables on R* is discussed in detail in Chapters 4 and 5. Current GA airplane manufac- turers' recommendations for setting these variables are not appropriate to maximum R*.

As a result of the foregoing limitations, it is concluded that a POHCPM, constructed from currently available POH cruise data, is an inadequate tool for maximizing R*.

SUMMARY AND CONCLUSIONS Sununary The POH cruise performance data for ten airplanes have been considered. The construction of cruise performance models based on POll data, the use of such models for the solution of various opti- mization problems, and the limitations of such models for maximizing R* have been discussed.

Conclusions 1. On the basis of computations performed herein, it is con- eluded that variations in R* over the cruise envelopes of GA airplanes are sufficiently large to warrant the development of airborne micro- processor cruise performance models capable of performing fuel-use optimization computations.

2-21 2. It is concluded that a POHCPM, constructed from currently available POH cruise data, is an inadequate tool for maximizing R*.

2~2 TABLE 2.1 SAMPLE PILOT OPERATING HANDBOOKS EXAMINED CRUISE OPERATING POINT VARIABLES PRESENTED AIRPLANE TYPE MANUFACTURER t 1974 Centurion t Cessna Pres~ure altitude 1974 Turbo Centurion RPM 1980 Centurion 2l0N MAP 1980 Turbo Centurion T2l0N Fuel lb/hr and/or gal/hr TAS and CAS (1) % BHP (2) Baron B55 Beech Miles/gallon (3) Baron S8P . C d·· tt peratlng on Itlons O Arrow IV PA-28RT-201 Piper Mixture - see Chapter 2.

Seneca II PA-34-200T ISA Temperature ±~ OAT (4) 1 or 2 gross weights (5) No wind M20J-201 Mooney Fixed c.g. position M20K-231 Undercarriag~ retracted Flaps up Cowl Flaps closed (6,7) CAS given for Beechcraft only.

(1) Except Beechcraft.

(2) (3) Mooney M20K-231 only. I Non-standard OAT for some airplanes only. I (4) 2 gross weights Hooney only. I (5) All airplanes listed have cowl flaps except Piper (6) Arrow IV. I Ascertained for all but the two 1974 Cessn+ airplanes.

(7) !

i tOwner's Manual tt cruise data for each airplane apply to some The specific airframe geometry, including avionics aerials and other optional external equipments.

These details were not examined.

TI1BLE Z.!

EXTENDED RANGE MIXTURE EXTENOED RANGE MIXTURE Standard Condition. ~ Z.ro Wind ~ Grou' Weigh •• 3800 Pound~ S.andard Conditions~. Zero Wind ~ Gross Weight- 3800 Pounds 7500 FEET 10,000 FEET 384 liS. (NO IUnRVE) 534 lllS. (NO RESERVE) 384 lllS. (NO RUEItVE) 534 LIlS. (NO RUERVE) IANGI ENDIt. lANGE " TAS llS.1 ENDII. RANGE ENDR. IANOE ~ TAS llS.1 ENDI.

MILES MP IH' MPH HaUl HOURS MillS HOURS HOURS MILES .PM MILES MP IHP MPH ~OUR HOURS ItPM 5.7 1065 94 4.1 '165 825 8.1 U4S 2550 23 '5 10' 81 4.4 69 187 2550 21 '190 41.0 1095 22 'J1 183 89 4.3 845 6.5 1175 82 4.'1 20 65 1111 84 810 8.4 1130 4.8 810 8.11 lU~ :1 8' 1'JI 114 77 5.0 19 61 135 8.11 1160 7,4 1235 20 83 1'12 4.9 890 166 12 5.3

'9 18 56

1080 8.3 1180 91 4.2 780 5.8 1135 2! 13 185 21 411 184 115 4.5 Ill5 855 8.1 1190 21 89 1&0 86 4.4 800 8 •. 2 171 80 4.8 20 63 820 6.5 1145 860 7.2 l220 21 65 115 82 4.1 171 5 .•• 19 59 1115 1245

5.0 845 1.0 "" 895 7.7

20 61 168 '11 55 163 10 5.5 , 41.3 1120 11\15 85 4.5 805 4.9 860 2400 23 ea 1'J9 21 63 177 19 8.'

825 8.8 7.2 1220 22 &4 114 81 5.1 890 4.' 20 59 171 74 U15 141 5.0 845 7.0 PIS 7.11 1245 21 80 168 Ui3 70 5.5 19 55 1200 1250 5.3 865 7.4 5.8 900 8.1 20 57 182 111 51 66 15"

'2

J3 84 .,:1 830 8.8 880 1225

80 4.8 59 170 74 5.2 '.2 2300 2300 21 1115 1245 5.0 845 1.0 5.5 895 22 80 188 '18 20 55 163 10 '.8 7.4 1200 900 8.1 1250 21 51 182 12 5.3 865 155 68 5.8 19 51 5.7 815 1.9 8.2 895 1245 20 53155 88 48 144 62 '.8 ,., 1185 .895 1245 5.1 855 54 162 10 5.5

2200 23 51' 188 '.2 2200 21

'4

810 1205 5.8 900 5.4 51 154 86

22 ' 58 180 '.5 20 '.1

'I 7.11 1220 895 8.6 880 144 112 41.2 21 52 154 6'J 19 48

5.'

•• 4 1225- 885 9.2 6.1 880 134 58 6.8 20 4' 148 84 18 44 9.0 1220 6.4 815 111 46 138 59 I

MANLJI1L EXTRACT

OWNERS

(974 C.fMTURION

CEssNA

TABLE 2.3 FLIGHT CONDITIONS REQUIRED FOR PO:-I CRUISE PERFORMANCE MODEL Standard Atmosphere Standard Atmosphere Standard Atmosphere II o o _30 C +30 C [

/ I I I

I Minimum Maximum r·linimum rlaxim~m r'faximu~

I Minimum

Gross Gross Gross Gross Gross Gross i Weight Weight Weight Weight Weight Weight I I N I N V1 i Position C.G. Position C.G. Position C.G. Position C.G. tion C.G. Position C.G.

posf " linlit Fwd limit 4. Fwd limit S. Fwd limit 6. Fwd limit 1. Fwd limit 2. Fwd 3.

i Aft limit Aft limit 10. Aft limit 11. Aft limit 12. Aft mit 7. Aft limit B. 9.

lt I 10 X 10 TO THE CENTI METER 46 1513 KU ,n f:L t\: F.c;o;:,l: R CO _HI:! I~ U', A N N 0\ 1)1" ••.. , '1 In l( 10 Tn 1I1[ (I-NTI"FTrn f( I ~ I, , I I H I ,,' I P f f' ..... "/" ,. 46 1513 N I N .......

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l

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I THE AIRFRAME AND THE ATMOSPHERE

i Table of Contents INTRODUCTION .•••••••••••••••••••••••• - •••••••••••••••••••••• 3-1 TIlE AIRF~ MATHE~~TICAL MODEL .••.•••••••••••••••••••••••• 3-2 DEPENDENCE OF R* ON AIRFRAME OPERATION AND A H10S PHERI C COND I TI ONS . • . • • • • • • • • . • • • • • • • • • • • • • • • • • • • • . • • • • 3 - 5 Airspeed, Altitude and Gross Weight................... 3-5 \~ind.................................................. 3-8 Auxiliary Equipment Power............................. 3-10 Center of Gravity Position ............................ 3-12 Conclusions ......................... , . . . . . . . . .. . . . . . . . 3-18 A CONVENIENT R* MODEL ......•...•..•.••••..•.••••.•..•..•.• · 3-19 SU~RY •• • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • . • • • • • • • • •• • • • • 3-19 TABLES 3.1 - 3.2 ••••••••••••••••••••••••••• - •••••••••••••.•• 3-21 - FIGURES 3.1 - 3.13 •.•••••••••••••••••••••••••••••••••••• ••• 3-23 ~ I

I

I

--------------------------- ------------------ ~--------- -- ---- --- ----- -------------------- ------- -------------------------- ------------------------------------------------------- -- -- -------------------------- ---------------------- '(

I CHAPTER 3

I THE AIRFRAME AND THE ATMOSPHERE INTRODUCTION In this chapter we commence the development of an airplane- atmosphere system performance model suitable for maximizing R*. De- tailed consideration is given to the airframe and the atmosphere only, while the propeller and engine contributions to R* are repre- sented by the variables n (the propulsive efficiency) and c (the p engine brake specific fuel consumption).

The model developed incorporates the following airframe and atmosphere variables: 1. Equivalent airspeed (EAS) V , knots E 2. Altitude, represented by the atmospheric air density ratio 0 3. Airplane gross weight W, lbf 4. Windspe~d along track V , knots w 5. Auxiliary equipment power P ' horsepower' AUX 6. Airplane longitudinal center of gravity (e.g.) position hc-.

The airframe model of Appendix C is first discussed. The effect of each of the above variables on R* is then examined, and each of those effects is illustrated for the LASA 60 airplane under the assump- tion that np and c are constants. An expression for R* (different from equivalent expressions for R* in Appendix A) is derived which, after expansion in later chapters, will prove most useful to the task of airborne computations.

3-1 THE AIRFRAME MATHEMATICAL MODEL The general airframe mathematical model presented in Appendix C constitutes expressions for: 1. The airframe drag and power required, power-off and power-on (Equations C.l - C.8) 2. The airframe drag coefficient, power-off and power-on (Equations C.9, C.lO, C.29 - C.3l).

The approximate geometric and aerodynamic characteristics of the Lockheed LASA 60 airplane are presented in Table 3.1. For this air- plane, the longitudinal range of movement of the c.g. is assumed to be limited to 0.15 < h < 0.30 by considerations of stability and control power.

Experimental power-off drag data for the LASA 60 with an unspecified c.g. position is presented in Reference 19, and reproduced here in Figure 3.1. The power-off drag polar for the LASA 60 was computed, using Equation C.29 and Table 3.1, for h = 0.15 and h = 0.30. Plots of these computations are superimposed on Figure 3.1. The computed curves fit the experimental data over the range 0.09 ~ C ~ 1.2. Deviation from L 2 2 the dat; when C > 1.2 is considered unimportant: such C values L L correspond to flight at speeds well below the minimum drag speed for which c : 0.8.

L The power-off drag coefficient of the LASA 60, with the c.g. at the aft limit (h = 0.3), is represented in this work by:

CD = 0.0402 + 0.052 C (3.1)

L 3-2

i

I ' ____ . _________________ . _______ Eg tl.E.-.1i 0..D-_ ~_~_L rep_~_e s e!!!_~ __ ~!l ___ ~Epr_~~_~!Il.Cl_!~ __ ~!E.Cl_~~h £_!~~~ ___ ~~~ __ !~r~~~ __ ~~_: _________________________ __ 'j

j

experimental data of Figure 3.1, plus an increment to the lift-independent

I

term to account for modifications made to the LASA 60 owned by Princeton University since those experimental data were collected.

I

The relationship between the drag coefficient power-off Co and the drag coefficient power-on CD is discussed in Appendix C. The difference

I

_ ON between CD and CD arises because, in powered flight, the following ON parameters have values different from those pertaining to power-off flight: 2. C m o 3. a with corresponding values of oW' LW and e o t w 5. i w -In Appendix D it is shown that variations in lift-independent drag with power result in (3.2) where the slipstream interference factor fD is a constant. Equation 3.2 reflects changes in CD and n (the term ~t2 KtStnt/S in KQ only) t pm 3-3 in Equation C.29, due to power. Substitution of Equations C.I and C.S in Equation 3.2 yields: >!'

(3.3) Changes in i te.ms 2,3 and S aho:ve. and additional effec,ts of changing nt' alter thiS' rela'tioTIshiV between C and CD for fixed values DON of C and h. The effects af such changes on CD were s,tudied for the' L LASA 60 using Equation C. 29. The data set of Table 3. I was used as a base, and items 2-5 above were separately varied. CD and the term pm t.:t 2KtStn/s in KO were constants in these computations. The: range of variation of items 2-5, and the corresponding maximum percentage variations in ICL/cDI from the value pertaining to the basic data set at the same C and h, are shown in Table. 3".2. The actual percentage L variations in CL/C , which varied with C and h, are the ~egative per- D L centage contributions to fD resulting from the variations in items 2-5. Table 3.2 applies to the range of lift· coefficient 0.3 ~ C ~ 1.2 L and to the range of c .g. position' 0.15 2. h 2. 0.3.

For most GA airplanes it is considered that the incremental changes in items 2- 5 above, due to power, will lie well w.ithin the incremental changes shown in Table 3.2. The corresponding maximum percentage variations in ICL/cDI shown in Table 3.2 are taken to indicate that the effects of power on drag, in addition to those considered in the formulation of Equation 3.3, are' small for GA airplanes., fO is taken to be a constant in this work, except in the discussion of center of gravity position. in this chapter.

3-4 ~ I

I

f ! .

DEPENDENCE OF R* ON AIRFRAME OPERATION AND ATMOSPHERIC CONDITIONS --- -- - -- ----- - -- - --- - --- -~ - -- -- - - - ---- - ---- -- ------------ - ------- - -------- --- - --- -- -------- --------------- ----- -- ----- -- -- - - -_. __ ._-_._--- ------- -; In this section, an expression for R* is derived which is equivalent

f

I ::et::r:::::u:n:X::::::::::O:o::r::u:::::d:: :~ i:h:e:::l:X:::::i::p::::::g

the propeller and engine contributions to R* in terms of the variables np and c.

The airframe and atmosphere contributions to R* are illustrated

I

for the LASA 60 under the assumption that n

and c are constants.

p

I

It is assumed initially that all of the variables contributing to the value of R* are constrained to have specific constant values, with the exception of equivalent airspeed, altitude and gross weight. A simple expression for R*, which accounts for these three variables is presented. That expression is then expanded as V ' P and hare w AUX consecutively introduced into it as explicit variables.

Airspeed, Altitude and Gross Weight In this discussion, the following assumptions are made:

np = constant = 0.75 in all Figures

c = constant = 0.45 lb/BHP.hr in all Figures

h = constant = 0.3 in all Figures.

With these assumptions, the most convenient form for R* is (3.4)

R* =

3-5 which is obtained from Equation A.12. Consideration of Appendix C (Equations C.4, C.9, C.l1 and C .. 29) reveals that PRIO is a function only of V , Wand h for a given airplane. Therefore with the above E

assumptions, P ra and R* in Equation 3.4 are functions of V and W

R E only. Figure 3.2 shows R* computed for the LASA 60, plotted against V for a range of gross weights . The family of curves in Figure 3.2 E applies to all altitudes.

Line A in Figure 3.2 represents the variation of R* with gross max weight (R* is the maximum achievable value of R* for a given gross max weight). Since R~ax corresponds to flight at maximum L/DOFF under the stated assumptions, line A also depicts the variation of minimum drag EAS with gross weight. The variation of R* and the minimum max drag EAS along line A are shown in Figure 3.3, the former being presented as a proportion of its value at W = 3,000 lb.

Equations C.Il and A.IS show that for flight at minimum drag (md) EAS with zero wind,

EAS is proportional to IW

md R* is proportional to l/W max These are the forms of the curves of Figure 3.3.

Consider the following two flight conditions: 1. Flight at constant EAS as the gross weight varies 2. Flight at constant power as the gross weight varies.

Lines Band C in Figure 3.2 represent flight at constant EAS with varying gross weight, the EAS corresponding to minimum drag for 3-6

W = 3,000 lb and W = 3,400 lb respectively. R* varies from R* along

max - ------- -- ----------------- ------ ----- ~ - - ---------- -------------------------------- ----------- -- --------- --- - -- -- -- --- -- -- - - ----

line B (C) at every gross weight except W = 3,000 (3,400) lb. This

variation is expressed as an R* penalty, defined by

R

* - R;ax]

R* PENALTY

r 100 %

= R~ x

L max

Lines Band C in Figure 3.4 correspond with lines Band C in Figure 3.2 and depict this R* penalty.

Similarly lines D and E in Figure 3.2 represent flight at constant power with varying gross weight, the power level corresponding to that required at minimum drag EAS for a gross weight of 3,000 lb and 3,400 lb respectively. These lines D and E are straight with a slope given by differentiating Equation 3.4 with P constant: R (3.5)

=

The slopes of lines D, E in Figure 3.2 are therefore different and invariant with flight density altitude. Curves D, E in Figure 3.4 correspond with lines D, E in Figure 3.2 and depict the R* penalty (also independent of density altitude) for flight at constant power as the gross weight varies.

It is clear from Figure 3.2. that both V and W have a significant E effect on R*. The curves of Figures 3.2 and 3.4 indicate that as airplane gross weight decreases during a trip due to fuel burn, it is more fuel-efficient to fly at constant EAS than to fly at constant 3-7 power, whenever the EAS exceeds the minimum drag speed. At constant V and W, R* is independent of altitude.

E Wind this discussion the following are made: In assumptions = constant = 0.75 in all Figures np c = constant = 0.45 lb/BHP.hr in all Figures = 0 PAUX constant = 0.3 in all h = Figures.

The effect of wind on R* is clearly seen from Equation A.12. With the above assumptions this is written (3.6) R* = The effect of wind is to multiply the right hand side of Equation 3.4

by the factor (1 + Vw lO/v ). For any given gross weight, P ra is

E R a function of V only. Therefore, for a given gross weight and EAS, E the effect of a given equivalent windspeed on R* is identical at all altitudes. The altitude yielding the maximum value of R*, at any gross weight and EAS, is that at which. the equivalent windspeed

V ra is a maximum. If a constant tailwind (headwind) V exists at

w w all altitudes, maximum R* is achieved by flying at sea level (the highest altitude possible).

A plot of P 10 versus V facilitates the computations in Equation E R 3.6. In particular, the EAS yielding maximum R* in any equivalent wind 3-8 I

I

I

condition is readily obtained from such a plot, as illustrated for - - -------- - ---- - -- ---- - ---- ------ -------- -- --------- ------------- ---------------_._._ ... _ .. _------------------ - ~.

the LASA 60 in Figure 3.5. The equivalent windspeed is ~nscribed on the abscissa, tailwinds to the left and headwinds to the right

t

of the origin. The straight line drawn from this V IcJpoint yields w

I

the EAS for maximum R* at the point of tangency to the appropriate gross weight curve. This construction is shown in Figure 3.5: points

t

"

t

A, Band C represent the operating points yielding maximum R* corre- sponding to equivalent windspeeds V /<J = -20, 0, + 20 knots respectively, . w for W = 2,600 lb and any altitude.

Computed performance for the LASA 60 is shown' in Figures 3.6- 3.8.

Figure 3.6 shows the EAS required to achieve maximum R*, plotted against V , for three values of the gross weight Wand two density al- w titudes. When the abscissa of Figure 3.6 is relabelled Equivalent Windspeed V IcJ without a scale change, the sea level curve for each gross weight ' w .'

f will apply to all altitudes and the 10,000 ft density altitude curves will cease to be meaningful.

Figure 3.7 shows the ratio of the maximum value of R* obtainable with wind to the maximum value of R* obtainable with zero wind, plotted against V 1cJ, for three values of gross weight. These curves apply w to all altitudes.

If an airplane is flown at the minimum drag speed in non-zero wind conditions, the maximum possible R* is not achieved. The 3-9 variation from the maximum is expressed as anR* 1>enalty, defined by

R* PENALTY- [ R*mdR~:;ax . ] x 100%

where R~d = R* atminimum.,dragllAS

R* = :maximum ·achievable'R*

max both computed for the appropriate gross . weight and ,the prevailing V w and o. Figure 3.8 shows thisR*penalty plotted against'V,;o,for three values of gross weight. These cUJ::vesapply .toallaltitudes. T·he R* penalty is in general more severe for headwinds·than'for.tailwinds.

The effect of equivalent ,windspeedonR*and upon theEASfor maximum R* is clearly significant.

Auxiliary Equipment Power In this discussion,the f61l0wingassumptionsare made: np = constant - 0 .75in:all -Figures c = constant -O.4:51b/BHP.hrin:all -'PiguT,es h = constant = 0.3 in.all Figures.

The auxiliary equipment.power deliv'eredper engine is 'defined by Equations A.4 and A.Sa. Whenc isdefine.d equalto.c' ,then P AUX is defined to be zero.

Equation A.l2 shows the,depend-ence ofR*on PAUX:

~ I

-~

(3.7) c ... i I 3-10 ,

~:------- - --~~:~~~~~:~::-=i~~~~::::::!~~:S;~~~L1°::-:-;::;::;O:~;i;;; - - -- ---

I

I to the curves of Figure 3.5. The effect of P is to shift the plot AUX

1-' of P R Iii versus VE verti call y by the cons tantamount E '1> P AUX ro-

Consequently, as P increases (decreases) from zero: AUX 1. The value of R* decreases (increases) in every flight condition, 2. The EAS yielding maximum R* increases (decreases) for any given equivalent windspeed.

Figure 3.9 shows the effects of P > 0 on R;ax (the maximum AUX achievable value of R* at a given gross weight) and on the EAS required for R* ,computed for the LASA 60. The curves are drawn for three max values of the gross weight, two density altitudes and zero wind conditions.

When the abscissas of Figure 3.9 are read as P 10, the sea level curves AUX for each gross weight apply to all altitudes, and 10,000 ft density the altitude curves cease to be meaningful.

When the Equivalent Quantities V ' vwlO and P lcr, and the gross E AUX weight are constants in Equation 3.7, R* is independent of altitude.

Equation 3.7 is now rewritten as: (3.8) 1 + The form of Equation 3.8 is convenient for the following discussion of the effects of center of gravity position on R*.

3-11 Center of Gravity Position The airframe model of Appendix C assumes that the airplane is laterally symmetric about its lengitudinal center line, with respect to' geemetry and mass distribut.ion. The airplane center of gravity (c. g.) is assumed to' lie on the longitudinal cent.er line, at a

distance he aft ef the leading edge of the mean aerodynamic chord

of the wing.

We now consider the effect on R*ef varying h. Considering the right hand side of Equation 3.8, the quantities which are functiens of hare 1. PRIcJ - see Equations C.4 and C.29 2. - Equation IL48 shews that np depends upon f , D which has been shown abeve to' demonstrate small variations with h.

P IcJ and np always appear tegether in Equation 3.8 as the ratio R n/PRIcJ. Instead ef introducing h as an independent variable into PR ra and n ' it is mere co.nvenient to: p 1. Compute np/PRIO fOT a reference c.g~ pestien hrefc, a-nd 2. Adjust that cemputed value fOT variations in h from h f' re by means of a correction factor which is somefunctien

ef dh = h - h f·'

re

This precedure is equivalent to' expanding n /P ra into a Tayler

R p .

'" I Series in dh.

3-12 I I I

I

i

j _. _.___ . _______ ~CCOrd~ng~ ,:~fi~e_ __ ______ _ __ . _____________ .

I [p n:O = p n:o at h = h C

ref I R R ref > h

J

= R* at h = h

R* ref h ref pquation 3.8 is now written: 1 + E Now from Equation A.13, Therefore

325.65 n

p and invoking Equations D.47 and 3.2,

~ = 325.65 na

L (3.10) C" V f W J P E VO R

325.65 n

L (3.11) = -=_=---~a V f W DON E J 3-13 where na = propeller efficiency in the presence of the body, f = constant.

J Equation 3.10 shows that, if fD were truly a constant, variations

in np/P ra with h could be evaluated in terms of the variation in

R L/DOFF with h, assuming na is independent of h. However, fO varies slightly with power. condition, h and C , as previously discuss:ed.

t

The variation of Tlp/PRIO with h is. therefore more accurately computed from the variation of L/DON with h, as shown by Equation 3.11.

We here evaluate the variation of L/DOFF with h for· the LASA 60 airplane, and propose a general model for such variations for GA air- planes. A general model for the variation of.L/DON with h is then proposed, and used to describe variations of R* with.h for GA airplanes (n is assumed to be independent of h.in this discussion - the validity a .

of this assumption is addressed. in Chapter 4).

Using Equation C.29 and Table 3.1, the percentage variation in L/DOFF from that pertaining to the nominal forward c.g. limit was computed for the LASA 60, as hand C were varied. The full line's L A, Band C of Figures 3.10 and 3.11 show the results of these compu-

tations for C = 0.4, C ;.. 0.8 and h = 0.3 respectively. These per-

L L centage variations in L/O with hand C may be visualized as the OFF L height of a surface, as shown schematically ih Figure 3.12. Lines A, Band C in Figure 3.12 correspond to lines A, Band C respectively in Figures 3.10 and 3.11.

The form of Figure 3.12 is considered to be typical of GA airplanes.

The height of that surface for any particular airplane is a function. of 3-14

The height of the surface behind the aft c.g. limit (nominally h = 0.3

for the LASA 60) is not of interest for current GA airplanes, since the aft c.g. limits of such airplanes are prescribed by stability -+- considerations I • From this discussion of L/DOFF for the LASA 60, the following model is proposed for variations in L/DOFF with h for GA airplanes: (3.12) where position he ~. J = L/D OFF corresponding to the c. g.

OFFJh

[

= L/DOFF corresponding to the c.g. position

;OFJ h

h e

[

ref

J ref

dh = h - h > 0 for he aft of h f e ref re

~ = positive constant

t that the maximum increases inL/D along lines A and B Note however, OFF in Figure 3.10 occur for h > 0.3, and correspond to positive tail loads.

Laitone (20) has shown that induced drag is minimized with a positive tail load (upload) for all values of C > O.

L 3-15 and both he and h e 1 ie anywher;e within the allowable c .. g. range.

ref This linearization app.ears· j:ustified on the basis of Figures 3.10 and 3.11. For t'he LASA 60 airplane.' defined by· Table 3.1, lines A, Band C of Figures 3.10 and. 3.11" (corresponding t'o' h:ref=' 0.15) give z::; '" 0.375.

The sensi ti vi ty of z::; to all the geometric and aerodYnamic characteristics appearing in Eq\1ation- C.29 for CD was'- not studied.

However, as an indication of this sensitivity, the foll.ow.ing studie:s were performed: 1. The dotted curves of Figures 3.10 and. 3 .. 11 give: the effects on z::; of a single variation in CD . , while alI pm other variables retain their values in Table 3. L For those dotted curves" h = 0.15' and z::; ",0:.467.

ref A low lift-independ.ent d,rag coefficient· therefore contributes t,o a high drag'-sensitivity to c.g.

position at any G • L 2. Figure 3.13 gives the effe.cts on z::; of varying C m o at C = 0.8, while alL other variables retain their L values in Table 3.1. Eor those' curves, h f = 0;15 re and: z::; '" 0.217 (a) for C =, 0, m o

(b) for C = -0.25, z::; '" 0.479

mo 3. Indi vidual variations in the parameters. g.iVen in Table 3.2 (with the exception of C ), within the m o limits given therein, were performed while an other variables retained their values in Table 3. L 3:...16 j I

I

I

---~ ____ --------------------- ___ ]'h_~_!:_~~~!_!..~!!K __ ~_~~~a t!.~_!l~_~_~ ___ ~~~ __ ~'!!f_~~ e _ ~~ __ ~_~_~1:'e ~~~------- -- -- --_______ _ __ __ __ _ from the surface corresponding to the basic data set of

I

I

Table 3.1 were not large in the region (0.3 < C < 1.2, - L 0.15 < h < 0.30). The corresponding variations in ~

I

(with h f = 0.15) from the basic value of 0.375 were

_ re not computed, but are expected to be small.

The effect of c.g. position on L/DON may be determined from the foregoing discussion. Running propellers effect changes in CD and pm in the parameters listed in Table 3.2, as previously discussed. It has just been shown that variations of these quantities do not change the form of Equation 3. 12, but merely the value of~. For powered flight we therefore replace ~ in Equation 3.12 by ~ and write (3.13) where ~ is a positive constant. The values of CD and the parameters pm in Table 3.2, used to compute ~ for a given airplane, should be average values pertaining to the powered flight of that airplane. The above sensitivity study of the effects on ~ of variations in CD and in pm the parameters in Table 3.2 indicates that ~ will probably differ little from ~ for most GA airplanes.

From Equation 3.11 we see that the percentage variation of np/PR I<J is identical to the percentage variation of L/DON with h.

3-17 Therefore, (3.14) h ref Using Equations 3.9 and 3~14, we now write R* for the c.g.

posi tion hc: V w (J 1

~J'

[ R* = 1 + -v;- . 1 + EP ;at~].

(1 + ~CL dh) AUX ;; p . R . , . n f re

where both hc :0 (h f + dh) c and h f e lie anywhere within the

re re allowable c.g. range. When he is aft of h .£ e, dh > O. Equation.

re.L 3.15 is applicable to standard and non-standard atmospheric conditions.

This analysis has conveniently accounted for variations of fn with h. Henceforth fn is considered to be a constant when h = h f.

re Conclusions The following conclusions may be drawn from Equation 3.15, when n (at h = h f) and c are assumed to be constants: p re 1. When all Equivalent Quantities, gross weight and c.g.

position he are constants, R* is independent of altitude and when, in addition, PAUX = 0: 2. R* increases as the c.g. is moved aft within the allowable c. g. range. The maximum value of R* is achieved, in all flight conditions, with the c.g. at the aft limit.

... I 3-18 I

I 3. The percentage increase in R*. for a given aft shift

j- -;----------------- ------- -i~posi1:±on,-±nereases-wrth-increas-i"g_~d-henGe- - - ---- ---- -- ---

I (a) Increases with increasing \II

I (b) Increases with decreasing EAS 4. The percentage increase in L/D ' shown by the full OFF lines of Figures 3.10 and 3.11. are taken to be indicative of the effect of c.g. position on R* for the LASA 60.

The influence of c.g. position on the second term of Equation 3.15 is negligible when P is small. for all values of np' AUX It is apparent that c.g. position can have a significant effect on R*. The magnitude of this effect for any particular GA airplane.

characterized by ~. depends upon the geometric and aerodynamic characteristics of that airplane.

A CONVENIENT R* MODEL Equation 3.15 is equivalent to the numerous expressions for R* in Appendix A.

In Equation 3.15. PR/O at h = h is a function of V and W

ref E only. and all other airframe and atmosphere variables are explicitly represented. The reason for expressing R* in this form will become apparent in the following chapter. where the variable nature of n p is discussed.

SUMMARY Airframe and atmosphere contributions to R* have been examined.

Equation 3.15 has been derived and will be further developed. in the 3-19 next chapter, into a model for R* which is convenient for airborne computations.

Assuming that the propulsive efficiency and the engine brake specific fuel consumption are cons.ta.nts, it has beE;ln shown that; equivalent airspeed, gross weight a.nd equivalent windspeed have significant effects on R*; longitudinal c .. g .. llosition ca.fl have a significant effect on R*, depending upon the airplane design and operation; auxiliary equipment power in general has a small effect on R*; and when all Equivalent Quantities, gross weight and c.g.

position are constants, R* is independent of altitude.

3-20 TABLE 3.1 ________________________________________________ LO_GKHEED LASA <?9 CJ-LA.RACTERI ST I CS in Appendix C.

are defined The symbols used ft S = 55.43 ft = St

-

5.46 ft c

=

ft i 16.2

=

l...

:: 0.2 "0 3.98

=

A 7.13 At

=

w = 14.854 ft b ft b 38.687 = t \\ K = 0.011 K 0.011

=

t w = 0 0.4

= ~t

~w 0.028 = 2.0 ft

=

°t go power-off flight: In degrees i 5.80

=

-0.15

C =

w m -1 = 1.575 e 5.73 radian a

=

t w = 1.0

n

0.063

=

t ° w 0.0393 = 0.2 1" CD

=

w pm Values for ow' 1"w' Kw' E:: ' a ' e , 0t' Kt' E:: and iw were determined with t t w ow the assumptions that: 1. The wing is untwisted, has a rectangular p1anfo~ and has a uniform NACA 4412 section.

2. The tai1p1ane is untwisted, has a rectangular p1anform, and has a uniform NACA 0012 section.

3-21 TABLE 3.2 LOCKHEED USA 60 EFFECTS OF PARAMETER VARIATION ON AIRFRAME LIFT TO DRNG RATIO PARAMETER PARANETER ABSOLUTE % VARIATION CL/C AT D RANGE OF VARIATION FIXED C AND. h.

L 0.3 < C < 1.2 L - - 0.15 < h. < 0.30

- -

0.1 to 0.2 < C - 2 .. 5%

-

m 5.73 + 25% per radian < a 1.5% - w [wi th corresponding changes in <5 T and w' w C]t e see Appendix - t 0.8 to 1.6 < 0.5% n t ~ <.

i 2.80 to 8.80 degrees 0.5% w , tThese variations together yield· variations of +19% and -21% in the three dimensional lift curve slope of the wing.

3"-22 i i

I

I I

"

,

I

I

I

[2

. LASA 60:

CJ) VEI(SUS

FIGURE 3.1 LocKW££.D

L fT<OM TE.STS.

DATA FEATHE.R£D PROPELLER

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~:~~~~r~.:;:~~:..:- -"-70 3-34

CHAPTER 4

CHAPTER 4 THE AIRFRAME-PROPELLER-ATMOSPHERE SUBSYSTEM Table of Contents INTRODUCTION. • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •• • • • • . • • • .• 4-1 THE PROPELLER PERFORMANCE MODEL.................... • • • • • • • • • • • 4-2 AIRFRAME-PROPELLER-ATMOSPHERE SUBSYSTEM PERFORMANCE ••••••••••• 4-3 The Kernel Functions S*, Q* andf3* ••••••••••••••••••••••• 4-4 S*, Q* and f3* at Sea Level with Specified Gross Weight and C.G. Position •••••••••••••• : •••••••••••••• 4-9 Corrected Qtlanti ties. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. 4-10 IJefini tions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. 4-10 si gni fi cance. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4 -10 Corrected Performance Plots.............................. 4-14 Contour Plots of S*, Z 4-14 and 6 *' ••••••••••••••••••••••• c X,Y,Z Plots and X,Y,f3* 4-16 Pi ots ....................... .

Propulsive Efficiency n* .•.••••••.•.••••.•••..•••••• 4-16 p Corrected Performance Model of R*c, ~ and f3............. 4-17 FormulationooooOootttt"' •••••••••.•••••••••••••••• o •••• 4-17 Center of Gravity Effects .•••••••••••••••••••••••••• 4-19 Compressibility Effects •••••••••••••••• ~ •••••••••••• 4-20 Wind Effects........................................ 4 - 21 Engine Rotational Speed and Brake Torque •••••••••••.••••• 4-22 Input-Output Model....................................... 4- 23 Implementation. • . • • • • • • • • • • • • • . • • • • • • • • • • • • . •• • • . . • • 4- 23 S~Y •••••••••••••••••••••••••••••••• • '...................... 4-24 TABLE 4.1 •••..••••••.•••.••••••.•••...•••••.••••••• ·••.••••.••• 4-25 FI GURES 4. 1 - 4. 8. • • • . • • • • • • • • • • • • . • • • • • • • • . • • • • • • • • • • • • • • • • • • 4 - 26

CHAPTER 4

CHAPTER 4 THE AIRFRAME-PROPELLER-ATMOSPHERE SUBSYSTEM INTRODUCTION

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This chapter develops an input-output model for the cruise

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performance of the airframe-propeller-atmosphere subsystem. The inputs to this model are airplane operational variables; the

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outputs are the quantities R*c (knots/brake horsepower) and the

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engine brake torque Q (lb ft).

E This subsystem model is developed by considering the perform- ance of the McCauley C33/90M-4 constant speed propeller, in con- junction with the airframe-atmosphere model of the Lockheed LASA 60 airplane discussed in Chapter 3. The McCauley C33/90M-4 con- stant speed propeller is installed on the LASA 60 airplane owned by Princeton University.

It is shown that, by presenting the performance of the air- frame-propeller-atmosphere subsystem in terms of Corrected Quantities; a compact input-output model of this subsystem, suitable for microprocessor applications, is obtained. The input-output model of this subsystem developed here for the LASA 60 airplane is assumed to typify such models for propeller-driven GA airplanes.

The propeller performance model is discussed first. The remainder of the chapter is a discussion of the airframe-prope11er- -, atmosphere subsystem performance, in which the input-output model of that subsystem is developed.

4-1 THE PROPELLER PERFORMANCE MODEL Thepropel~er:peT;f.ormanc.e model used .'inthis .workis :p.re- sented in AppendixD. The performance items .of interest here are: 1. The propulsiive e£ficiencY11 : required £or 'the compu- p tationofR":.c 2. Th:ep.r:o.p.eTler .shaft speed N (RPH) and ·torqueqa JIb ~ft) 3. The p.rope.llerbJade angle S degre.es (measured betw.eenthe plane of propeller rotation and ·the £latfaceofthe blade at a radius of O.75R,where Risthe ·p.T.o.pel1er tip radius) : requiredt:ocompute 'the contribution of compressibility ton :and'Q :pa' For straight and level s.t.eadyflight it is shown (Equations D.5-6, D.S8 and D.S9) that: (4.1) (4.2) (4.3)

s = S [VE,W, h, N, oJ

Appendix D describes the:eom p utationof ' Q and sin .t.e.rms p a of: 1. Theperformanc.e ofth.efreepropeller in the .abs.ence.of compressibilityeffec.:ts.1'heabsence· of compressibi'lity effects is denoted by the .superscript i (incompressible) 2. The propeller-body interference factors fn and f J 3. The compressibility correction factor f .comp 4..;2 i j I

I

I

!

It is shown (Equations 0.49, 0.48 and 0.40) that i (4.4)

. np = np fcomp

I (4.5) '1 (4.6)

= Qi/f

Q a a comp 0.55 and 0.57) where (Equations i i (4.7)

W, h, N, oJ

= n

EVE' na a Qi (4.8) = Qi h, N,

W, oJ

EVE' a a fD and f are constants whose magnitudes are dependent upon J the airplane geometry.

The method used to compute n , Q and 8 for the McCauley p a C33/9m1-4 constant speed propeller operating on the Lockheed LASA 60 airplane is summarized on page 0-29.

AIRFRAME-PROPELLER-ATMOSPHERE SUBSYSTEM PERFORMANCE We here develop the Airframe-Propeller-Atmosphere (APA) subsystem input-output model. This model consists of: 1. A model of the collective contribution of the airframe, propeller and atmosphere to R*: this contribution is the quantity R*c knots/brake horsepower 2. A model of the engine brake torqueQE lb ft in all straight and level steady flight conditions. The airplane operational variables are the inputs to this model; R*c and Q E are its outputs.

4-3 The model of R*-c is developed by int.roducing a model for the propulsi veefficiency np into Equation 3 . .15. nl'emod:el~f Q E is developed from a mo'delof the propeller shaft torque .~ (lb it) which is developed below.

A model of the-propeller blade angle 8 is also developed below, this being required for the computation of f which comp °nfluences both R*c and Q a· The development of the airframe-propeller-atmosphere s-ub- system input-output model proceeds in the following manner: 1. R*c, Q and 8 are expressed in terms of a a) The kernel functions S*, Q* and 8* respectively b) A number of simple correctionfact.ors, and an incremental correction in the case of8.

2. Utilizing Corrected Quantities, the kernel functions S*, Q* and 8* are represented in compact form.

A corrected p:erfbrrnancelllodeloi R*c ,Qand 8 is 3.

a defined and discussed.

4. Q is defined in terms of ~.

E 5. The input-output model is defined from -the results of $teps 3 and 4. The suitability of this input-output model to microprocessor applications, and the allocation of numerical values .to this model for GA airplanes, are then briefly discussed.

The Kernel Functions S*, Q* and 8* Consider Equation 3.15 fOr R*;and specifically the quantity 4-4 VE [np/PRIa] h therein. Invoking Equation 4.4, this quantity ref is written (4.9) E

VE [p:~lh = V [p:~lh fcomp

ref . ref We now define S* to be: (4.10) knots/BHP

(BHP = brake horsepower). It was shown in Chapter 3 that PRIO is a

function of {VE' W, h} only. This fact, together with Equations 4.5 and 4.7, gives the functional relation (4.11)

S* = S* [VE' W, h, N, oJ h

ref Substituting Equations 4.9 and 4.10 into Equation 3.15 yields:

V 10] (1 + ~CLdh)f S*

(4.12)

R*c = 1 + _w__ comp knots/BHP

V A [ E where the auxiliary equipment power loading factor A is A 1 + E ~CL dh)

=

pAux.o[ ~] (1 +

PRIO h ref ~CL dh) f ., 1 + E

=

PAU/O[~] (1+ comp

PRIO h ref (4.13)

= 1 + E PAUX.o [~:] (1 + I;;CLdh)fcomp

4-5 S* constitutes t:he' kenleJ of R*c; this kemel heing cor- rected for the effects of wind, auxiliary equipment powe.r, center of gravity position 'and compressibility by means of Equa,tion 4.12.

Consider now., the propelter' shaft torque Q. From Equation a D.29,

where E' = number of engines, e.ach driving, one propeller

p(i) = propeller shaft power, ft 1b/sec

a

= 2'TTIQ (i)

a n = N/6Q = propeller shaft speed, reVOlutions/second.

Thus (i) 5252.1 (4.14)

Q = -~=..::....~=

a ENIO ['n~i)].

p 10 " R IJ , , ,

Wi th the center of gravity toca,ted at h = h'ref"

5252.1 (4·.15) = ---=--,---=-.

Qil

a h ref

EN¥'; [n~", ].,'

IO PR , h ref Wi th the center of gravity lQcacted at h = h f' + dh., re' 5252.1 ); I I ~ I 4-6 Invoking Equations 3.14. 4.4 and 4.15.

Qil

a h ref (4.16 )

Q = -;'(-:;-l-+--::-~C-=-L:"'::;d;;:'h-::-) f-::----

a comp We now define Q* to be (4.17) lb ft

Q* =

From this and Equation 4.8 we have the functional relation (4.18)

Q* = Q* EVE' W. h. N. 0] h

ref Invoking Equation 4.17. Equation 4.16 becomes

= Q* (4.19)

lb ft Q (1 + ~CLdh)f a comp Q* constitutes the kernel of the propeller shaft torque Q ; a this kernel being corrected for the effects of center of gravity position and compressibility by means of Equation 4.19.

S* and Q* are related (Equations 4.10, 4.15 and 4.17) by 5252.1 V E (4.20)

S* =

ENIO Q* Finally, consider the propeller blade angle B, expressed functionally by Equation 4.3: B is required only for the compu- When the center of gravity is located at tation of f comp Hence (Equation h = h , B is denoted by the kernel functipn B*.

ref 4.3) , (4.21)

B* = BI = B* [V • W, h, N, 0] h degrees

h E ref ref

With the center of gravity located at h = h f + dh, this kernel

re function is corrected by the increment 6B: 4-7 S = S* + t..(3.

degrees (4.22) The Speed-Thrust Coefficient. plO:t (C~:J2) facilita,tes' the: compu- tation of t.S. Figure 4.1 shows that, when the 1±:ne:-s Q.f. constant 8 in the c~ :J2 plo.t- for the McCauley C3.3/90H-4 fr·ee· propeller are approximated by. straight lines. radiating frQIII the, origin at an equal spacing of e degrees, (4.23) where Ij; - angle from the: abscissa to the straight radial line which approximates. the 8* line on the C~:J2 pl;ot, degrees K = increment. oI 13-* bet~en lines of constant· (3* on the c~ :J2 plot, d:egre:es.

Equation 4.23 is assumed. to ty,pify the t.B. performance of propeller- 4- driven GA airplanes. FO.r t'heMcC.auley C33/9.0M-4 free propeller, , t.8 = -32. 74cos(L 758*-2) sin{l .. 7:5£*-2- 3i~~~) [Cl + ~CL dh}~-l] degreeS ..

Figure 4.1 shows that th,e straight radial line:. approximation of the constant S* lines, in the C~:J! plot for the McCauley C33/90H-4 a .

propeller, is a good approximation in the region; [1.8 ~c~ ~J.~, a 10 ~ 8* degrees 2. 23}. This is: the n01'lItal reg'ion of op,eration for the LASA 60 airplane. tt The ke.rnel functions S*,. Q-'!r' and (3* are func.tions of the: s·.arne set of variables {VE' W, h, N~o} with h = h ..

ref t Note that t.s is a functiono:f t8*,_ C and. db} only.

L tt Departures of' 8* from this range during fuel-.economical ope,ratil')ns-

may necessitate modificatloR of the expression 1/1 = 1.758*-2 d.egrees

(Figure 4.1) to accommodat:e all operational values o.f /3* in the linear approximation of Figure 4.1.

4-8 S*, Q* and S* at Sea Level with Specified Gross weight and C.G.

position: We now examine the functional dependence of 5*, Q* and S* on {V , N}; when the variables W, hand 0 are constrained to be E

[W = W , h = h ,0 = 1], this flight condition being denoted by

o ref

the subscript O. Note that VEo = V .

T

Consider SO' QQ and So for the LASA 60 airplane when

f

1. W = Wo = 3400 lb

I

2. h = h f = 0.3.

re

Figure 4.2 shows contours of SO' Q and So plotted for'variations

O

The So contours define a three-dimensional surface

in V and NO· E o with a single peak: for any given V ' the NO yielding maximum E , 0

So falls on the inscribed line passing through the peak. The QQ

contours define a second three-dimensional surface: the height

of the So surface at any point (V ' NO) may be computed from the

E

o

height of the QQ surface at the same point (V • NO) using E o Equation 4.20. Two lines of constant propeller blade angle S*

o

are also shown in Figure 4.2, constituting contours of a third

three-dimensional surface. Radial lines from the origin (V ' NO) =

E o (0, 0) in Figure 4.2 represent lines of constant propeller advance ratio J a O

Figure 4.2 is assumed to typify the SO' QQ and So performance

of propeller-driven GA airplanes.

We now examine how the functions 5*, Q* and S* vary from the

functions SO' Q and SO' as Wand 0 vary from the fixed values

O

[W = W ' 0 = 1]. This is done most efficiently by introducing a

O number of Corrected Quantities.

4-9 Corrected Quantities Definitions: The following Correcte,d QUanti't'ies are. defined::

D - D [.' woJ' Corrected airframe drag:, lb:· (4.24)

OFFc - OFFW' Corrected auxiliary equipment· (4.25) P AUX = P AUX 1 w~: ..

c power, horsepower' Correct:e.d airframe power req~ired (4.26)

= P

I w~: R (po.w er -off), horsep.o:wer: Cbrree.ted S*', knots/BHP (4.27) (4.28)

v V CorTee.te:d g~oc,entr:ic windspeed along

=

w w

JY

c trac.k, knots.

/:0 .

X V (4.29) .Gorrec:ted airspeed" knots

=

E y (4.30) N C:orrec .. ted propeller sha.ft~ speed~, RPM

=

/Y

[Wo]

z CO.-rrect:e,d' Q*, Ih ft (4.31)

= Q* w

These co-rrected quantities apply' to standard and non-standa-rd' atmosphe-ric conditions.

Significance: Consider an airplane in' straight and ley,el steady flight, in the following flight conditi'on. (denoted by subscripct 0') : 1.

Sea level, standard a,tmosphere: Density· PO' slugs/ft3 2.

Gross weight W , 1b O' 3.

Center of gravity position h = h ref 4.

True airspeed V 0" ft/sec 4,-10 (4.32)

True airspeed V = 0.5921 V , knots

T o 0 5. Prope1.1er shaft speed NO' RPH In this flight condition, the following equations apply: (4.33) 1b

La = Wo = [CLJoYzPoV6S

(4.34 ) lb

DOFFO = [CDJc:POV~S

(4.35) horsepower (4.36) (4.37) lb ft

Q* =

o 5252.1 V T (4.38) o knots/BHP

So = EN Q*

o 0

Now consider the same airplane in straight and level steady flight, in the following flight condition (no subscript): 1. Above sea level, standar~ or non-standard atmosphere: density p, slugs/ft 2. Gross weight W, 1b

3. Center of gravity position h = h f

re 4. True airspeed V, ft/sec

True airspeed V = 0.5921 V., knots

T

Equivalent airspeed Ve = Vip/PO = V~, ft/sec

(4.39) 0.5921 V , knots

Equivalent airspeed V =

e E 5. Propeller shaft speed N, RPM.

4-11 In this flight cond:±tioll the fo11iowing eql:la:tcions apply:: Ib (4.40)

L = W = C !zPO.' V ' S>

L e' 2' 11) (4.41)

DOFF = CD ~PO,Ve S

horsepower' (4.42.)

S,52,l (4.44) Q* =

ENIO[ ~ 1

. p ICY ..

R ; . .

5252.1 V: E S* kno:ts/BHP (4.45)

=

EW;- Q*" We now prescribe that,. for tires-eo two flight conditions: ( 4.46)

J = J (4.4 7)

aU' a Consequently: (4~ .48) (4.49) Hence constant; C1: corresponds. to. constant· X.

2. Since [CLJo = C'L' [CD]~ = Co (AppendIx C).

Therefore, from Equation:s 4;.34:,4.4'1, 4·.48 and 4.24, (4.50) 4-12 3. From Equations 4.35, 4.42, 4.48, 4.50 and 4.26, (4.51) 4. From Equations 4.36, 4.43, 4.47, 4.48, and 4.30, (4.52)

NO = N r~cr = y

5. Since [cDJo = CD: the Speed-Thrust Coefficient C~a

(Equation D.53) is the same in both flight conditions.

This in conjunction with Equation 4.47 yields (Figure D.6) (4.53)

S* = S*

o

(4.54 ) and thus from Equation 4.5, (4.55)

[n~ ] 0 = n~

Then from Equations 4.37, 4.44, 4.51, 4.52, 4.55 and 4.31,

rwo 1

(4.56)

Q = Q* Lw-J = Z

o

6. From Equations 4.38, 4.45, 4.49, 4.52, 4.56 and 4.27, (4.57)

S* = S* [~J = S*

o Wo c These results may be summarized as follows: Straight and level steady flight of a propeller-driven airplane under the conditions , ••• -<

h f = constant

1. = h

re 2. C constant

=

L 3. J constant

=

a 4-13 t with variations in Wand 0, results in invariance of the quantities The significance of these results in th.e present work is apparent from the converse statement: Straight and level steady flight of a propeller-driven airplane under the conditions

1. h = h = constant

ref 2. X = constant

3. Y = constant

t with variations in Wand 0, results in invariance of the quantities These results are an extension of the ideas presented by Pye(12) pp. 37, 38.

The Corrected Quantities P and Vware addressed in the AUX c c discussion of the Corrected Performance Model below.

Corrected Performance Plots Contour Plots of S*, Z andf3*: c The flight condition of Figure 4.2 corresponds to the flight condition denoted by the subscript 0 in the foregoing discussion of Corrected Quantities. Invoking the results of the latter discussion, Figure 4.2 does not change when the various quanti ties in Figure 4.2 are relabelled as follows: t In standard or non-standard atmospheric conditions.

4-14

x V (Equation 4.49)

=

T :~- ~-~--~-'-~/~.

, .. .--- y I (Equation 4.52)

=

NO />--:'.

I I Z Q* (Equation 4.56)

=

./ I

I

S* S* (Equation 4.57)

=

c 0 ..

I /f ; ..

13* 6* (Equation 4.53)

= ~~

I 0

-----~-- ).-//

. - -;--------- ../

I

t Figure 4.2 is duplicated as Figure 4 .3 in which this re1abe1lin( has been performed: Figure 4.3 shows contours of S*, Z and 6* c plotted for variations in X and Y for the LASA 60 airplane operating with h = h f = 0.3.

re From Equations 4.20, 4.27 and 4.29-4.31 we have 5252.1 X S* = knots/BHP (4.58) YZ c E Wo 5252.1 X S* = knots/BHP (4.59) YZ W- E Also, from the definition of Z (Equation 4.31), (4.60) '.'

lb ft ---.-~- ~~~:-.'-.-' The contour plots of Figure 4.3 constitute a comp1e.te-def'i~n.ttion of the functions S*, Q* and 6* (Equations 4.11, 4.18 and 4.21) for

the LASA 60 airplane operating with h f = 0.3. Note that in

re Chapter 3 where both nand c were assumed to be constants, the p maximum value of R* (=R* ) occurred at the airframe minimum .... ~-~ max . .' _.~ .. _." ---_. /./' /' drag EAS: Figure 3.3 shows this EAS to be 73.7 kts for the LAS' .. \ 60 when W = 3400 lb. Introduction of the ni model in this chapt~~ I p " has increased the EAS for maximum S* to 77.5 kts for that airc-ra.ft· with the same gross weight.

__ ---. -~-'7-

Note t that Figure 4.3 applies to standard and non-standard at~ospheric conditions.

4-15 Figure 4.3 is assumed to' typify the variatiens of {S*, Z, S*} c with {X, Y}, and hence the variations of {S*, Q*, S*} w,ith {V , W, N, cd, for propeller-driven GA airplanes. Note that each E such plet is constructed fer a specific value of Wo and a specific value ef h ; and that for the representation ef {S*, Q*, S*} ref variations with {V , W, N, o}, the values of Wo and h used in the E ref construction of such a plot may be selected arbitrarily.

X,Y,Z Plots and X,y,S* Plot;s: Figure 4.4 shows vertical sectiens through the X,Y,Z surface of Figure 4.3, for several censtant values ef Y. Plots such as Figure 4.4 will henceferthbe referred to as X,Y,Z plets. Fer a given airplane: an X,Y,Z plot and Equatiens 4.59 and 4.60 together yield S* and Q* for any set {W, X, Y}.

Figure 4.5 shows vertical sections through the X,Y,S* sur- face of Figure 4.3 for several censtant values of Y. Plots such as Figure 4 . .5 will henceforth be referred to asX~Y,S* plots.

Propulsive Efficiency n*: p It is of interest to' observe the functional nature of the

propulsive efficiency [n~Jh ' denoted n;. From Equations 4.5

ref and 4.7, (4.61 )

n* = [niJ = n* EVE' W, h, N, a J

h p p h p ref ref A plet shewing n* centeurs for variatiens in X and Y would completely p 4-16 i j !

I

I

I

I I define the function in Equation 4.61 as a three-dimensional sur-

I

face, for a given airplane and a chosen h f.

re

I

Vertical sections through the X,Y,n* surface, for several

I

p constant values of X, are shown in Figure 4.6 for the LASA 60 air-

plane with h = 0.3. As X increases, the maximum value of n*

ref p achievable also increases. Variations of n* with Y at constant p

I

X are solely responsible for variations of S* with Y at constant c

I

X in Figure 4.3.

Figure 4.6 is assumed to typify the n* performance of pro- p peller-driven GA airplanes. It is clear from this figure that n* varies greatly with the airplane operating condition.

p Corrected Performance Model of R*c, Q and S a Formulation: We now formulate a model for R*c, Q and S based on the cor- a rected quantities and corrected performance piots of the foregoing dis cus si on.

The following definitions (Equations 4.25, 4.28-4.30) are collected here for convenience: horsepower (4.62) V knots (4.63) w ,c knots (4.64 ) 4-17

{W;f

(4.65) RPM Y=N~W--W- these definitions we have: With l. From Equation 4.12, (l +~CLdh)f $* . comE (4.66)

R*c = [1 + V:cJ knots/BHP

II 2. From Equation 4.59, Wo 5252.1 X (4.67)

S* = knots/BHP

E YZ W From Equations 4.13 and 4.67, 3.

C

rAUX J

(4.68)

II = 1 + 5252.1 (1 +

~CLdh)fcomp YZ 4.19 and 4.31, 4. From Equations WZ (4.69) lb ft

Q = W

(1 + ~CLdh)f a 0 comp 5. From Equations 4.22 and 4.23, (4.70) 8 = 8* + lI8 degrees (4.71)

lI8 = -K COS1j; sin(1j;- i:@-r [(1 + ~CL dh) ~-lJ degrees

61T /180 The computation of f is performed using f plots comp comp (see page D-11) .

For given values of X and Y: Z is obtained from an X,Y,Z plot appropriate to {W ' h }; and 8* is obtained from an O ref X,Y,8* plot appropriate to {W ' h }.

ref O An X,Y,Z plot, an X,Y,8*plot, a set of f plots, .and comp Equations 4.62-4.71 together constitute the Corrected Performance 4-18 i i I

I

I

!

Model for R*c, Q and S for a given airplane.

a

I

Note that: • R*cW/W is constant for constant {V ' X, Y, dh, f , PAUX } O w c . comp c • QaW/W is constant for constant {X, Y, dh, f } 0' comp • S is constant for constant {X, Y, dh}.

Following are some remarks on this modelling method. First: the influence of center of gravity movement on propulsive efficiency is examined. Second: some typical values of f for GA air- comp planes are ,given. Third: the effect of corrected windspeed on peak R*W /W 0 and on the operating condition f~r peak R*W/W is examined.

O Center of Gravity Effects: Throughout this chapter computations of R*c and Q , for c.g.

a positions displaced a distance dhc from the reference c.g. position h f C, have been performed by multiplying S* and dividing Q* by re the factor (1 + ~CLdh).

The factor (1 + ~CL dh) was derived in Chapter 3 under the assumption that n was independent of h. This is not precisely correct. Con- a sider movement of the c.g. while maintaining constant X and con- stant Y. This results in: 1. Constant C , but varying Co (Equation C.29) L 2. Varying C~ (Equation 0.53) a 3. Constant J a . i 4. V ary~ng n and S (Figure D.6).

a 4-19 On th~ basis of Figure 3.10, it is assumed that a typical maximum variation in C with c.g. movement is 4:%. This results DON i in a 2% variation in C (Equation D.53). From Figure D.6, a 2% R a i variation in C at constant J results in a maximum variation in' R a i a n of approximately 1.5%.

a Therefore the factor (1 + E;C dh) is expected to introduce a L maximum error of 1.5% in R*c and Q ; and a maximum errol' of 1.5% a in the increment of A due to PAUX (Equation 4.68). The latter c error is expected to give a negligibly small error in A.

Compressibility Effects: Computations of f were performed for the LASA 60 airplane, comp using the Hamil ton Standard Method (21): the results of these computations are given in Table 4.1.

A detailed study of propeller compressibility effects, using the approach involving f , has not b~en performed by this comp author; such a study is desira.ble (see Appendix D). The following should be considered in an investigation of this matter (22):.

1. Computation of propeller performance in inc'ompressib1e flow may be performed using- Goldstein-Lock analysis (8) which employs 2-Dimensional (2-D) airfoil data. This is accepted practice in the propeller i.ndustry.

2. It is accepted practice in the propeller' industry to compute propeller p~rformance. in compressible flow.

using Goldstein-Lock analysis and 2-D airfoil data which 4-20 incorporate variations in airfoil lift and drag coef- ., ficients with Mach number. However, this computational method ignores two phenomena which may be important to .the actual performance: a) Three-dimensional flow near the blade tip: Radial flow near the blade tip (due to the tip vortices in the wake, and the proximity of the tip itself) reduces the effect of compressibility in the tip region.

Consequently, a 2-D analysis will tend to overestimate the compressibility effect.

b) ~he effect of compressible flow on the wake-induced velocity: Compressibility effects should be accounted for in application of the Biot-Savart law to the compu- tation of the velocity induced at each blade element by the wake.

The effects of these two phenomena on the performance should be assessed, and included in the analysis of pro- peller compressibility effects if necessary.

Full scale propeller tests will be required to give confidence in the use of any developed method for computing propeller com- pressibility effects.

Wind Effects: Equation 4.66 expresses the effect of wind on R* in terms of the Corrected Windspeed V .

w c Figure 4.7 shows variations in X,Y and R*W/W at the operating O condition for maximum R*W/W ' as corrected windspeed varies; for O 4-21 the LASA 60 airplane [h = h f = 0.3, f = 1, PAUX = 0, re comp c

c = 0.45 lb/BHP.hr]. Similar curves exist for the constraints

[h = constant f:. h f' f = constant f:. 1, PAUX = constant f:. 0, re comp c c = constant f:. 0.45 lb/BHP.hr].

The wind has no effect on ~ or B when X is fixed.

Engine Rotational Speed and Brake Torque The engine rotational speed NE (RPM) and brake torque Q (lb ft) E are required in Chapter 5 for the computation of engine brake specific fuel consumption c (lb/BHP.hr). It is convenient to compute these quantities here, in terms of the propeller shaft speed N (RPM) and torque ~ (lb ft). Figure A.2 shows the no- tation used in this derivation.

NE is simply determined by the transmission gear ratio G: (4.72)

NE = GN revolutions/minute

The engine brake torque Q is determined as follows: E horsepower AUX + P ] P =

s [1 P

s

= Q [ + 5252.1 P AUX ] a

. lb ft

Q G 1 N~ E Substitution for ~ (Equation 4.69), N (Equation 4.65), and PAUX (Equation 4.62) yields Q \ .

Q = ~ 1 + 5252.1 ... i

E G 4-22 Invoking Equation 4.68, Q becomes E lb ft (4.73) Input-Output Hodel The input-output model of the Airframe-Propeller-Atmosphere (APA) subsystem consists of the set of relationships which determine R*c and Q£ (the outputs of the model) in terms of the airplane operational variables (the inputs to the model). These relation- ships have all been formulated in the foregoing discussion. Figure 4.8 depicts this model, with its inputs and outputs, in block dia- gram form.

Implementation: .

The APA subsystem input-output model is well suited to imp1e- mentation in an airborne microprocessor, for the following reasons: 1. TIle X,Y,Z plot; the X,Y,6* plot; and presumably the f plots; comp may be stored as sets of coefficients of cubic polynomials.

The memory space required for this storage is very small.

2. All of the required equations are algebraic equations, in which the most complex functions are trigonometric func- tions.

Allocation of numerical values to the non-operational variables in the model, for a particular airplane, is readily accomplished by the airframe manufacturer. In particular: 1. The X,Y,Z plot is constructed from propeller shaft torquemeter readings of Q , in conjunction with Equation 4~69.

a 4-23 2. The X, Y, S* plot is computed from the propeller manu- facturer's data. The parameters K. 1/1 and e required by Equation 4.71 for t.S are obtained from a C~:J2 plot o.f the same propeller data.

3. The f plots could be computed for the airframe manu- comp facturer by the propeller manufacturer.

4. The value of ~ may be estimated by the airframe manu- facturer from propeller shaft torquemeter readings of Q • in conjunction wi th Equation 4 .. 69.

a SU~1ARY A propeller performance model has been discussed. The APA subsystem input-output model has been developed. This model has been presented in block diagram form in Figure 4.8, and appears suited to microprocessor applications due to its simplicity and minimal storage requirements.

4-24 I i

I

!

i TABLE 4.1 COMPRESSIBILITY CORRECTION FACTOR f comp

Flight Condition: Lockheed LASA 60, W = 3400 LB

I'

I

CD = 0.0402 + 0.052 cl (power-off)

I -j

h = h = 0.3 f = 0.98

ref J

P = 0 fD = 1.08

AUX Standard Atmosphere

I i

& _ ~ I ....

Entries in this Table are .J.. - 'I I 'I comp p p

I

DENSITY PROPELLER RPM ALTITUDE EAS ft knots 2000 2300 2600 Sea Level 80 1.0 1.0 1.0 100 1.0 1.0 1.0 10,000 80 1.0 1.0 0.994

I

1.0 1.0 0.976 Values of f were computed using the Hamilton Standard Note: comp Method of Propeller Performance Calculation, 1941 (21).

4-25

8 = 3.5 ..Iejrec$

K.,= 2 Jl!:!Jreu

"-- __ ---L-_--'- ___ C (.

o c. ~

R. a -~ - /(., Cos 1/1 Sill (?/l :!: 8) .:

C:. e 0/1'0

.L

(/ + 5 C Jh )4 RoM EIJUAlI_ ~ 53

Now L

AN)> + dh - +.aC~ }

- clh -+ -;4~"

. &.

.'. llf3· = -fC, C4a 1f 51;"("'11 - 8 I~') C: [< 1+ S C Jh)t - ,]

L

C:. B7rjlBo

= - K, CoS V' sin (1/1- ~) [( I + ! C Jh i-I] ....

L 8 rr/180 .'. SJ)IlSftl'II'(u.r, FD~ 11) ., Ad K,; Af3· = -32.74 CDS(/.75,6·-2)~(1.1S~*-Z-3.5~)[(' ... !CLJ,f-IJ FIGURE 4.1 EFFECT OF C.G. POSITION ON PROPELLER ELADE AN6LE.

11-?f; ._-------_. __ ... _ .. __ ._<_ . .-.-=, \ .

. ~ ....

lit. ",,11 ,n" HI H~ TilE CF.Nl'~'Ftrn

KI , IF I r t. A. ,':.' T I~ (" .. ~. '.' I' • "r, 1 rc,13

-

'Jf

Q* AN]) (3* CoNTOUR.S AT SEA LEVEL WITH

S, '5252.1 ~ o J(Nors / HoRSEPOWER " PROPE.LLER

RPM

i. , ., .. , .. , , I" KNOT.5 = AIRSPEED, EQUIVALENT TRUE AfRSPEf:D Vr Vc: i 0 0 I , ,

' , , ;" ,"I ' ' I'

' I . , ~ , l' "I " I;t'''''·, " ' .. ",: I 'I

:: f:":" t' '.:'! ": 'I 1" I "I' i' I' ,. • ", I '.1 .'~ I" X 't> '1) 1111 ,U~IIt.lt III' 46 1513 hi I If I I.l. ti. 1','.1 H CO . ~ .. , , I~" ..

I .• , '1' I' : .

., ... ..., .... ~ '1' ~ . I' "I'! I' 1 . . I , I ' I . I ., ~. r .• ,.... 1 _. I ." l' I

· I "'-""'r'

Sc· , Z AND f3* CONTOURS

. I I: .---~~~~~~~~~~'

*= (7* 'vJ = 5252.1 X

CoK.RECTED 'FkoPELLE12.

S HORSEPoWEIl

c J w;, 'E Y2

51-1f1F=r ToRcWE ····,····I·· .. \'··J·II' .... ,' .. , ........ "1'\'" · ': . . ;':: ill: ., ... ':: '.,: : .

LL ;1: :::1_ __ z ~ if '0 i' •.. " . ". '.

;-'''-- ....... -.- -:" I·· .. · :::: '~T; .': . . , , , I ~r-~, ~~~~~~~

./ . . .!. ..... J.. ~--+--r-"'i-~~

'

Y=

.1 " !

. , ~ • N · CoRRECT£D ; PRoPELLfR SHAFT SPEED

RPM

"T. ii" "I:' ," 8 : I' i 'I I:; I ' ,.' i' " .' ';':' :,. ".

, 'I' I' I '., . 0 :1, . ', .. :. . .90 i'.. ,.: :'.1. i· ':;'3

! 'ff I j'I',:j

. I . .: ... : . j" x = \ I 'Wo CoRRECT£D AfR5PffD ... !:; :~0 .. : 1 ,I Vr . I ,I .

E .. :.. . i. L .. 1 ... __ ._ .. _"!. ______________ ~ __ !5.'!~'!._~,_~_~~,~_ ......... [ .. ..l L .Jl.~;.

.., '-.....,..-'--------_._-----_._---._----,_._._.

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4-33

CHAPTER 5

CHAPTER 5 THE ENGINE-ATMOSPHERE SUBSYSTEM Table of Contents Page INTRODUCTIO!'-l ........................................... _ .................. .. <: :: = = 5-1 THE NATURALLY ASPIRATED ENGINE PERFORMANCE MODEL ••••••••••••• 5-3 Parameters Included in the NMBTE Performance ModeL ••••• 5-3 Desi gn Parameters.. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. 5-3 Opera tional Parameters.............................. 5-4 Parameters and Phenomena Excluded from the NMBTE Performance Model. • • . • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •• 5-5 NATURALLY ASPIRATED ENGINE PERFORMANCE: FIXED IGNITION TIMI NG. . . • . . • . • . • • . • . • . . . • • . • • . • • • • • • • • • • • . • • • • • • • • • • • • • • • . •. 5 -10 Brake Horsepower ••.•.••••••••••••••••••••••••••••••••••• 5-10 Leanout Performance •.••••••.•••.••••••••.••••••••••••••• 5-11 Fuel Metering Requirements .••.••.••••••••••••.•••••••••• 5-15 NAnJRALLY ASPIRATED ENGINE-ATMOSPHERE SUBSYSTEM PERFORMANCE: MBT IGNITI ON TIMING •••.•••••••••••••.•••••••••• 5-16 Brake Hors epower ....................... ~ . . . . . . . . . . . . . . .. 5-17 Leanout Performance ••••••••••••••••••••••••••••••••••••• 5-18 Constant P and Constant BHP Leanouts ••••••••••••••• . 5-18 m F for Minimum BSFC During Constant BHP Leanouts ••••• 5-22 F for Maximum BHP During Constant P Leanouts ••••••• 5-24 m Cons tant P and Constant BHP Leanouts from F • • • •• 5-26 m max Performance with Specified Fuel Metering Schedule ••••••• 5-28 BSFC Performance Maps at Sea Level •••••••••••••••••• 5-28 BSFC Performance Maps at Altitude ••••••••••••••••••• 5-30 A1 ti tude Variations of BSFC with Constraints ••••••••••••• 5-30 Corrected Quantities .................................... 5-32 Corrected Brake Torque.............................. 5-33 Corrected Air Mass Flow Rate •••••••••••••••••••••••• 5-35 Table of Contents (concluded) Page Corrected Part-Throttle Performance Model of p mand IDa' 5-36 Input-Output Model ••••.••.•••••.•••••••••.•••.•••••.••• 5-37 ..

5-37 Formulation for the Standard Atmosphere •••••••••••• Computational Scheme (Standard Atrrr>sphere) ••••••••• 5-42 Formulation and Comp.utations (Non-Standard Atrrospilere) • ..••••••.•.•.••..•••.••.••. a, ••••..•.••••. e-. 5-44 5-47 Implementation • •••••••••••••••••••••••••••••••••••• 5-48 Summary ................. ~ ............... e· •• ., ................ .

5-48 TURBOCHARGED ENGINES •..••••.••••.••..••••••.•••••••..•••.••.

Performance Comparison: Naturally Aspirated and Turbocharged Engines ...•..•..•••••••••..••••••..•.•..•••• 5-51 Brak.e Torque .•...•.......•• _ ...................... e_ •• 5-51 5-52 Brake Specific Fuel Consumption •••••••••••••••••••• Recommendations: TEA Subsystem Input-Output Mode1. •••. 5-54 SUMMARY. . . . . . . . . . • . . . . • • . . • • • . . . . •.• • • . • • • • . • • • . •. • •.• . • • • • •• 5-55 TABLES 5.1 - 5.4 ........•....•........................•..... '.' 5-57 FI GURES 5. 1 - 5.31.......................................... 5 -62 !

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OiAPTER 5 THE ENGINE-ATMOSPHERE SUBSYSTEM

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INTRODUCTION This chapter develops an input-output model for the cruise performance of the engine-atmosphere subsystem. The engine-

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atmosphere subsystem considered here consists of a naturally aspirated,

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spark-ignition, inlet port fuel injection, four-stroke piston aero engine; operating in the standard atmosphere or in a non-standard atmosphere.

In this development, the engine is assumed to be of fixed design. We consider only steady state operation of the engine: no attempt is made to develop a dynamic engine model. In addition, no account is taken of engine exhaust emission controls.

The tasks of the engine-atmosphere subsystem input-output model are: 1. To compute the engine control inputs required to minimize the engine Brake Specific Fuel Consumption (BSFC) at any engine operating point demanded by the APA subsystem (Chapter 4).

2. To compute the engine BSFC,c (lbm/BHP.hr). The airplane R* may then be computed from c and the value of R*c (knots/BHP) provided by the APA subsystem input-output model.

The input-output model developed here reflects current General Aviation piston engine technology in all respects but one: that of 5-1 ignition timing. All commercially available General Avia1:ionpiston engines employ fixed ignition timing. According to Chirivella (16): The magnetos are wired to ignite the mixture ata certain fixed advanced timing. Thi s feature is different from the variable timing that automobile engines areprovide.d with. The reasanfor this resides mostly in simplicity and the fact that "the engine regimes in an airplane are not subj ect to drastic changes during .flight. The optimum timing is selected for inhibiting detonation during take- off power situations. No attempt is made lateran to vary the timing for cruise power . . . The normal timing varies somewhat from engine to engine, but is on the order of 20° BTDC [before top dead center].

In the pursuit of good fuel economy,the ignition timing incorporated in the input-output model developed here is optimized for maximum brake torque in every engine operating condition. This optimum igni tion timing is called Minimum ignition advance for Best Torque (MBT), and is discussed in detail in AppendixE.

The engine-atmosphere subsystem input-output modeldevelope~ here is referred to as theNEA (Naturall yaspi ra tedMBT ignition timing Engine-Atmosphere) subsystem input-output model. This model is developed from computationsperforrned by the Naturally aspirated MBT ignition timing Engine (NMBTE) performanc.e model presented in Appendix E.

The content of the NMBTE performance model is first examined.

The performance of current technology, naturally aspirated (fixed ignition timing) General Aviation piston engines is then discussed.

We then discuss in detail the performance predictions of the NMBTE performance model, and develop the NEA subsystem input-output model.

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, Finally, turbocharged spark-ignition piston engines are discussed briefly, and some recommendations offered for the development of a Turbocharged MBT ignition timing Engine-Atmosphere (TEA) subsystem input-output model: this model is not developed in this work.

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TIlE NATURALLY ASPIRATED ENGINE PERFORMANCE MODEL The naturally aspirated engine performance model used in this

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work is presented in Appendix E. That model will here be referred to as the Naturally aspirated MBT ignition timing Engine (NMBTE) performance model.

The NMBTE performance model is an analytical-experimental hybrid which computes naturally aspirated piston engine performance in terms of Brake Horsepower (BHP) and Brake Specific Fuel Con- sumption (BSFC) Ibm/BHP.hr. The parameters included in this model are discussed brieflY below. Parameters and phenomena which affect engine performance but which have been excluded from this model are also discussed below.

Parameters Included in the NMBTE Performance Model I !

I , The parameters included in the NMBTE performance model fall into two groups: design parameters and operational parameters.

Design Parameters: Design parameters are those fixed by engine design. Since we consider engines of fixed design, these parameters are modelled 5-3 as constants. The design parameters included in theNMBTE perfonnance model, and the values given them in the present work, are presented in Table 5.1.

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Operational Parameters: Operational parameters are those under the control of the pilot. Those included in the NMBTE performance model are listed below as inputs to and outputs from the computations of that model: Inputs: F Fuel-dry air mass ratio P Inlet manifold absolute pressure, inches Hg m T Inlet manifold temperature, degrees Kelvin m P Exhaust absolute back-pressure, inches Hg e Engine shaft speed, R-PM NE Outputs: Air mass m flow rate, lbm/hr a

m Fuel mass flow rate, lbm/hr

f BHP Brake hors epower, horsepower Ibm/BHP. hr c Brake specific fuel consumption, Brake torque, Ib ft.

Q E The quanti ties F, P , T , P are common to all cylinders. The m m e quantities lit and m are equally divided between all cylinders.

. a f The NMBTE performance model assumes that: 1. Inlet manifold temperature T is equal to the atmos'pheric m ambient air temperature Ts computed from the standard atmosphere model of Apperidix B.

2. Exhaust absolute back-pressure P is equal to the e 5-4 ------------------------------------------------------------------------------------------------------ I i ,

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atmospheric ambient air absolute pressure P t computed

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amos

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from the standard atmosphere model of Appendix B (with

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appropriate units conversion).

3. The ignition timing is the Minimum ignition advance for

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Best Torque (MBT) at all times. This ensures the maximum

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r possible brake torque and the minimum possible BSFC for

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all operating points defined by the above set of inputs.

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For computations performed by the NMBTE performance model in this work: 1. The computational scheme is given on pages E-39 through E-43.

2. The fuel metering schedules used are discussed on pages E-38 and E-39, and illustrated in Figure E.18.

3. The Reference Operating Point and the Fuel Schedule l Datum Conditions are listed in Table 5.2.

4. The engine delivers maximum continuous BHP at the Reference Operating Point.

Parameters and Phenomena Excluded from the NMBTE Performance Model The parameters and phenomena excluded from the NMBTE performance model are listed below.

1. Ignition timing T: The assumption of MET ignition timing obviates the need to include ignition timing T explicitly in the NMBTE performance model: the ~~T ignition timing T at any operating point is unknown in this model.

o 5-5 Taylor (13) presents some automobile data, here repro- duced as Figure 5.1, which shows the effect on Brake Mean Effecti ve Pressure (BMEP) of variations in ignition timing L from L. Acco.rding to Taylor (13), o variations in spark timing, from that for maximum power • have the same percentage effect on brakemep at all loads and speeds. This correlation makes it pos- sible to predict the effect .ofa given departure from best-power spark advance on both output and fuel economy.

In the light of Figure E.3, however, these data would appear inapplicable to all usable equivalence ratios.

I t is unclear from Taylor (13) if the data of Figure 5.1 apply to all values of {¢, T , P , CHT ,h} .

m e With a knowledge of l and the effect on BMEPof variations o in l from L , thep.erformance of fixed ignition timing o engines might be easily modelled. Such performance has not been modelled here.

2. Cylinder Head Temperature (CHT): CHT Masnotrequi red for any performance computations. Monts (23) shows that for fixed ignition timing engines, leanouts at .constant inlet manifold pressure and constant RPM result in a maximum CHT at ¢ = 1 (see Figure 5.4) . It is assumed that the same behavior is demonstrated by engines employing MBT ignition timing. CurtiSS-Wright (IS) state that for their TC18 engine, in which the spark was advanced from 25 BTDC to 5-6 30° BTDC for cruise power settings (resulting in improved fuel economy): There is one disadvantage to using spark advance; if the mixture is ignited sooner, then the duration of the combustion period is longer; the burning takes place over a longer period of time inside the combustion chamber; the result is more heat generated inside the cylinder and higher cylinder head temperature. So spark advance requires the use of a little more cowl flap to main- tain a given cylinder head temperature.

In the NMBTE performance model, it is assumed that CHT remains within operational limits at all times.

3. Exhaust Gas Temperature (EGT): EGT was not required for any performance computations.

With regard to operating limits on EGT, Monts (2~ shows that for fixed ignition timing engines, leanouts at con- stant inlet manifold pressure and constant RPM result in a peak EGT slightly lean of ~ = I (see Figure 5.4).

When leaning at constant BHP and constant RPM with approximately MBT ignition timing, Chirivella (l~ found that ,for the Lycoming TIO=S41-E engine: . the engine temperatures do not necessarily become higher than those obtained at the best power point if one is able to lean sufficiently to the left of the TIT [Turbine Inlet Temperature] peak.

Curtiss-Wright (15) state that for the TC18 engine, when the spark was advan~ed from 25° BTDC to 30° BTDC: 5-7 since the burning takes place fora longer period of time, inside the cylinder, the resulting exhaust gas temperatures are lower. This is the main reason for using spark advance. Ex.haust gas temperatures are reduced, with resulting benefits to turbine and parts in the exhaust system.

From these observations it is concluded that MBT ignition timing will probably yield acceptably low values of EGT in all ultralean operating conditions. For simplicity in the NMBTE performance model, it is assumed that EGT never exceeds engine operational limits in any operating condition.

4. Detonation: No attempt is made in the NMBTE performance model t.o either predict the .occurrence .of detonati.on or to model its effects on engine performance. The interested reader is referred to Appendix F where these matters are briefly discussed.

S. N.on-Uniform Distributi.on of Air and Fuel to Each Cylinder: Unif.orm distribution of inducti.on air and fuel flow to all cylinders is assumed in the NMBTE perf.ormance model.

6. Atm.ospheric humidity: The NMBTE performance model assumes that the inducted air is dry.

7. Ram Effects: Inlet manifold temperature changes due to ram are neglected. Similarly, at wide open throttle (WOT), inlet manif.old absolute pressure changes due to ram are ., neglected (clearly at a given inlet manif.old absolute pressure at part throttle, ram air pressure need not be considered) .

.4 5-8 In all WOT operations, the NMBTE performance model con- siders inlet manifold absolute pressure P to be a function m of engine shaft speed NE and atmospheric ambient air abso- lute pressure P t (Appendix B) as follows: amos N , RPM at WOT (Pm/Patmos) E

I: 2,000 0.969

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2,200 0.963

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2,400 0.956 2,600 0.950 At WOT, increasing engine shaft speed results in: in- creasing absolute pressure losses in the inlet manifold, due to friction; and hence decreasing P IP t (see Ref.

m amos 24, p. 19).

8. Inlet Manifold Heat Exchanger Effects: Variations in the temperature of the cooling air surrounding the inlet mani- fold, from the atmospheric ambient temperature, may sig- nificantly affect the inlet manifold air temperature.

The relatively long length and large diameter of the modern air cooled aircraft engine's intake air manifolding make an excellent heat exchanger. In fact, we find that the inlet port temperature may be more influenced by the temperature of the air surrounding the inlet manifold than it is by the temperature of the ~onsumed air (25).

The complexity involved in modelling this installation effect has been avoided. The inlet manifold temperature T is assumed (for simplicity) equal to the atmospheric m ambient air temperature T (Appendix B) at all times in s the NMBTE performance model.

5-9 9. Inlet Manifold and Exhaust Manifold Pressure Acoustic Effects: In the NMBTE performancemodel,P (P )is taken me t.o be the mean value of the inlet (exhaust) mani fold absolute pressure .atthe inlet (exhaust) valve: variations in {Pm' P e} in time and from cylinder to cylinder, due to inlet and exhaust manifold dynamics, are ignored. The interested reader is referred to Reference 26 for a study of these phenomena.

·10. Exhaust Absolute Back-Pressure Variations from Atmospheric Ambient Air Absolute Pressure: The NMBTE performance model sets the exhaust absolute back-pressure P equal to the e atmospheric ambient air absolute pressure P t of Appendix amos B (with appropriate units conversion): variations in this condi tiondue to exhaust manifold acoustic effects, flight speed, the installation of an exhaust augmentor(24) etc.

are ignored.

NATURALLY ASPIRATED ENGINE .PERFORMANCE:FIXED IGNITION TIMING All commercially .available General Aviation piston engines employ fixed ignition timing. Before .discussing the performance predictions of the Nf..1BTE performance mode1,i t is instructive to consider the performance of these fixed igni tion timing engines.

Brake Horsepower Atypical plot ofBHP versus inlet Manifold Absolute Pre~sure 5-10 (MAP) for various constant values of engine RPM, is shown in Figure 5.2 (24). This figure was "developed from the performance of Continental 0-470-K and -L engines" (24) at standard sea level con- di tions.

Figure 5.3 (24) shows a typical sea level and altitude per- formance plot of BHP vs. inlet MAP and RPM. This Figure is (24): . used to determine the power output of a Continental 0-470-M engine at altitude. The chart at the left shows engine output at sea- level standard conditions with no ram air pres- sure applied to the carburetor intake. The chart at the right shows the effect of altitude and. is used in conjunction with the first chart.

The po:.nts corresponding to engine rpm and mani- fold pressure are located on both charts. The horsepower indicated on the sea-level chart is transferred to an equivalent point C on the altitude chart. Then a straight line is drawn from the point A to the point C to establish the altitude correction. The intersection of this line with the density altitude line (0 in the example) establishes the power output of the engine. The horsepower should be corrected by adding I percent for each 6°C . .. temperature

decrease below T [T = standard atmospheric

s s ambient temperature] and subtracting I percent for each 6°C temperature increase above T .

s The fuel-air mass ratio appropriate to each point on the power charts of Figures 5.2 and 5.3 are not given by Bent and McKinley (24).

Leanout Performance The General Aviation piston engine manufacturers usually pre- sent variations in engine power and specific fuel consumption with fuel-air mass ratio, for conditions of fixed throttle position (constant inlet MAP) and constant RPM.

5-11 Figure 5.4 (23) shows generaliz.ed mixture strength (fuel-air mass ratio) characteristics for General Aviation piston engines t with fixed ignition timing. According to Monts (23), Figure 5.4 : is a classic fixed-throttle [and fixed RPM) mixture control curve, and it depicts the relation of power (BHP or IHP), specific fuel consumption ... , cylinder head temperature (CHT), and ex- haust gas temperature (EGT) as a function of fuel/ air ratio (F/A). Although the data presented here was developed at Teledyne Continental Motors, this same rather precise relationship is valid for all aircraft piston engines regardless of manufacturer.

The F/ A at which power peaks is called "best power" and the F /A at which specific fuel consump- tion minimizes is known as "maximum economy". It is obvious from an examination of this mixture control curve that maximum fuel economy occurs at approximately .060 F/A.· Therefore, for most efficient operation and maximum energy conservation, all operation should be carried out at this mix- ture strength, unless limited by other factors.

Figure 5.5 (27) shows generalized data similar to that of Figure 5.4. With regard to Figure 5.5, Ref. 27 states: While the absolute values of [BSFC, BHP, CHT, EGT) . . . change with engine power, the re- lationship shown here is approximately true for operation over the normal flight regime of the engine from 40-100% power. Best power occurs at about 0.076 fuel-air ratio, peak cylinder head temperature at 0.067 which is the stoichiometric (chemically correct) fuel-air ratio, peak exhaust o gas temperature at 0.062, and best economy at 25F lean of peak EGT at a fuel-air ratio in the vicini ty of 0.059 . .. . While the "lean misfire limit" has been variously defined •.• , it will , t The original figure of Ref. 23 does not include the BHP curve shown in Figure 5.4; but treats the IHP curve of Figure 5.4 as both IHP and BHP, and treats the indicated specific fuel consumption curve of Figure 5.4 as both ISFC and BSFC. The modifications to the original figure of Ref. 23, presented here in Figure 5.4, were performed by Mr. F. Monts (28).

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i be defined here as a point at which the engine operator detects audible roughness in engine operation. This point is characterized by a

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sudden decrease in EGT and usually occurs between fuel-air ratios of .052 and .042 depending on the engine, ignition timing and fuel system.

A comparison of Figures 5.4 and 5.5 confirms that the relationships

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therein are not precise in general.

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Current practice in General Aviation is to lean at constant inlet MAP and constant RPM (when a constant speed propeller is installed) in cruise. As shown above, the minimum BSFC is obtained at a fuel-air mass ratio of about 0.060 using this leaning tech- nique. However, it is not always practical to lean to this fue1- air mass ratio because of engine temperature limits, detonation limits or other limits (see Ref. 27 and the discussion of Fuel Metering Requirements below). The General Aviation airframe manu- facturers recommend leaning procedures which enable the pilot to establish a safe minimum fuel-air mass ratio between "best power" and "maximum economy" (as defined above) : 1. In the absence of a fuel flow gauge, fuel pressure gauge or EGT gauge, the mixture is usually leaned until rough running is encountered, and then enrichened to re- establish smooth running.

2. An EGT gauge, fuel flow gauge or fuel pressure gauge permits the fuel-air mass ratio to be established more accurately than in (1) above. The fuel-air mass ratio may be established most precisely using an EGT gauge, by varying the fuel flow rate until the exhaust gas temperature 5-13 is a specified increment below peak EGT on the rich or lean side of peak EGT (see Figure 5.4).

The loss in BHPwhich occurs during leaning at constant inlet MAP and constant RPM is often undesirable. Constant BHP can be maintained during leaning by continuously opening the throttle and thereby increasing inlet MAP. According to Monts (23): During the late 1940 I sand 1950 I s when the air- lines operated piston engine powered aircraft, they were naturally interested in economy of operation and extended service life. To promote both of them, Wright and Pratt & Whi tney each published methods for economical cruise operation. Both were based on the use of torque meters (or BMEP gauge) and the mixture strength/power relation-

ship ... Pratt & Whitney called it the torque

drop method of setting cruise mixture . . . Simply stated, the approximate desired power was set and the mixture leaned to peak the torque reading.

The torque value was then reduced approximately 9 percent by leaning, thus establishing cruise economy mixture setting. The throttle was then opened to regain the 9 percent torque loss. The Wright method [(15)] ... was the same except a 10 percent torque drop was used . . . It should be noted that there is no loss in performance from this operation and increased service life resulted.

Although general aviation piston engines are not equipped with torque meters, approximately the same resul ts can be obtained using an EGT gauge . . . [It) is possible to identifyniixture strength from relative EGT 's. Aft.er leaning to the desired mixture strength, the throttle may be opened to regain the power lost in the fixed throttle leaning. [The only measure of power recovery for the GA pilot is Indicated Airspeed.} There seems to be no hesitation about correcting throttle settings to compensate for ambient temperatures, but there seems to be reluctance to mov~ the throttle (increase manifold pressure) td compensate for mixture strength. Obviously, if the operation is at an altitude requiring full throttle for the desired power setting, it will be necessary to suffer the airspeed loss.

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Note that such power recovery by opening the throttle is only.

feasible if:

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1. The fuel metering system maintains constant fuel-air I mass ratio as the throttle is opened; 2. The absolute value of EGT does not exceed engine limits I as the throttle is opened.

With regard to the constancy of fuel-air mass ratio in the TC18

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engine as the throttle is opened or closed, Curtiss-Wright (15) states: . if you set 10% BMEP drop mixture, leave the mixture control where it is and then move the throttle (up and down), the BMEP will change, as will the fuel flow, but the fuel-air ratio will remain about the same. It should be noted that present day carburetors are not quite capable of holding the same fuel-air ratio if the changes in airflow are substantial.

According to Curtiss-Wright (15), the 10% B~ffiP drop mixture used for cruise power settings with the TC18 engine corresponds to a fuel- air mass ratio of about 0.053, which fuel-air mass ratio was used for cruise in conjunction with a spark advanced 5° from the normal spark timing of 25° BTDC. The leaning procedure used for the TC18 engine in c·ruise wa.s equivalent to leaning at constant RPH and con- stant BHP to a fuel-air mass ratio of about 0.053.

Power recovery by opening the throttle during or after leaning in cruise is not common practice at present in General Aviation.

Fuel Metering Requirements Figure 5.6 (23) shows generalized fuel-air mass ratio requirements 5-15 of General Aviation piston engines with fixed ignition timing.

At power levels appropriate to idle, taxi and approach: arich fuel-air mass ratio is required for starting, idling (29) and smooth transient response. In the cruise power range: operationnear the "maximum economy" fuel~air -mass ratio is possible. At the higher power levels: the fuel-air mass ratio must be increased to permit the development of high power, to cool the engine and to prevent detonation.

It is emphasized that the curve of Figure 5.6 varies from engine to engine. Figure E .16 (23) shows the fuel-airmass ratio metered to the Continental IO-540-Nengine by the Beech Single Lever Power Control (23,30): the Desirable Schedule in Figure E.17 is the generalized curve of Figure 5.6.

NATURALLY ASPIRATED ENGINE-ATMOSPHERE SUBSYSTEM PERFOru.1A.~CE :MBT IGNITION TIMING We here develop the Naturally aspirated MBT igni tion timing Engine-Atmosphere (NEA) subsystem input-output model. Thismode1 is developed using the Naturally aspirated MBT ignition timing Engine (NMBTE) perfol;1Jlance model described on pages 5-3 through 5-10.

The discussion in this section proceeds as follows: 1. For the NMBTEperformance model a) A typical p1otofBHP vs. inlet MAP and RPM is pre- sented ,and compared with corresponding 'd'ata fOT fixed ignition timing engines.

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An indication of the reliability of the NMBTE performance model is obtained by the above comparisons of its per-

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formance predictions with the performance of fixed ignition

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timing engines.

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c) For various fuel metering schedules: variations in BSFC, Pm and ro with brake torque, RPM and altitude f are presented.

d) Altitude variations of BSFC with various constraints are examined.

e) Corrected quantities are identified.

f) Corrected part-throttle performance plots are developed and presented.

2. The input-output model of the NEA subsystem is presented.

Figures 5.7 - 5.26 were drawn from computations performed using the NMBTE performance model. In these figures, engine operation at wide open throttle is denoted W.O.T.

Brake Horsepower Figure 5.7 shows the variation of BHP with inlet MAP and RPM at sea level, with fuel metering schedule A, as predicted by the NMBTE performance model. Figure 5.7 is similar to the fixed ignition timing, s~a level data of Figures 5.2 and 5.3. Each of these three figures applies to a naturally aspirated engine with a displacement 5-17 of 470 cubic inches. Comparing these three (sea level) figures: 1. The rate of change ofBHP with inlet MAP at constant RPM is approximately the same.

1., 2. The smaller rat'e of -Change of BHP with RPM at constant inlet MAP in Figure '5.7 is attributed toth'e MET ignition timing in the latter figure .

Leanout Performance Constant P and Constant BHP Leanouts: m Leanout performance of the NMBTE performance model is here examined under the following conditions: 1. At constant inlet MAP and constant RPM, at 'sea level 2. At constant BHPandconstantRPM, at sea level.

Figure 5.8 shows typical leanout performance under each of these conditions. In Figure 5.'8: curves bhelled A pertain to

leanout at constant inlet MAP = 23 in. Hgand 230'0 RPM; and curves

labelled B pertain to leanout at constant BHP = 132.S5BHPand 230'0 RPM. DUTing the constant inlet 'MAP leanout A, the minimum BSFC occurred at a fue1-'airmass ratio of 0.'058 (point 1 on the right

hand side of Figure 5.8): at this ptiint the BHP = 13'2.55 which value

was used to perfonn the constant £HP 1eanout B.

Consider first the left hand side of Fi,gure 5.8, which shows the variation of BHPduring leanout A, and the variation of inlet MAP during 1 eanout B. Peak BHP on curve 'A, and minimum P on curve m B ,both occur at a f'le1-airJila~;-s'ratioF= 0.08'0. Each experimental 5-18 i i I

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BHP data point added to Figure 5.8 (denoted 0) was obtained from the generalized BHP curve of Figure 5.4 in the following manner:

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1. In Figure 5.4, let the best power fuel-air ratio be

FB = 0.078

2. In Figure 5.4, determine y% = percent best BHP at a fuel-

air ratio = x% x FB

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3. In Figure 5.8, let the peak BHP fuel-air ratio be

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Fp = 0.08, and the peak BHP be BHP = 157.97 p 4. Compute F

,BHP = y% x BHP

p and mark the point (F, BHP) as 0 in Figure 5.8.

For F ~ 0.08, the BHP curve A and the experimental data points show close agreement. [For the fixed ignition timing data, BHP tends to decrease more rapidly with decreasing F (at ultralean values of F) than the MBT ignition timing model predicts: this is an expected trend.] For F > 0.08, the model does not show close agreement with the experimental data: this discrepancy is attributed to the fact that a cubic polynominal in equivalence ratio ¢ was used to repre- sent the indicated thermal efficiency n! in the'model (see Equation 1 ' E.4l and Figure E.7). Such representation of n! may not be suf- ficiently accurate over the whole of the usable range of ¢: a table lookup of n! may prove to be more accurate.

Curve B on the left hand side of Figure 5.8 shows the extent to which the throttle must be opened, as the fuel-air mass ratio is decreased below F = 0.08, during the constant BHP leanout.

5-19 Consider now the right hand side. of Figure 5.8. First: comparing curve A with the gener.ali zed (fixed ignition timing) curve of Figure 5.5; we se.e that on the former curve the fuel-air mass ratio yielding mininrumBSFC (point 1) is 0.058, while on the latter curve it is 0.059. On curve A, the minimum BSFC = 0.4631

is 86.4% of the BSFC = 0.5360 obtained at the peak BHP fuel-air

mass ratio of 0.08; while in Figure 5.5, the minimum BSFC is approxi- mately 85% of the best power BSFC. Thus for this case of leanout at constant inlet MAP and constant RPM, the variations in both BHP and BSFC predi cted by the NMBTE performance model are quite close to those given by the generali z.ed (constant inlet MAP, constant RPH) leanout data for fixed ignition timing engines.

Second: consider the BSFC variation along the constant BHP leanout curve B in Figure 5.8. While the general shape of this

curve is s imil ar to that of curve A, the minimum BSFC = 0.4556

(point 2) is lower than the minimum BSFC = 0.4631 on curve A (point

1), and occurs at a lower fuel-air. mass ratio = 0.0495 than does

point 1. The BSFC decreases by 1. 62% along curve B front point 1 to point 2. Consequently, if the mixture is leaned at constant inlet MAP and constant RPH to the nominal "maximum economy" point 1, a further decrease in BSFC of 1.62% is possible with no loss in BHP by leaning along curve B to the true minimum BSFC point 2. In leaning at constant BHP from point 1 to point 2, the inlet MAP must be increased from 23 inches Hg to 26.17 inches Hg. Note that

the minimum BSFC point 2 at F = 0.0495 is slightly lean of the peak

5-20 , of the n! curve at F = 0.0514 (<I> = 0.7667: see Figure E. 7).

i 1

Consider now a series of leanout pairs similar to the pair I on the right hand side of Figure 5.8. At sea level and 2300 RPM, a number of constant inlet MAP leanouts were performed [P = 28, m 25, 23,20,16, 13, 10 inches Hg). From the point of minimum BSFC

I'

(point 1: F , BSFC , BHP ) each of these leanouts was continued at

I

l 1 1 cons tant BHP = BHP 1 until the point of minimum BSFC (point 2:

I

F , BSFC , BHP ) was reached. Figure 5.9 shows for each leanout 2 2 l sequence: 1. Fl and F2

2. t.BSFC % = 100 [BSFC - BSFCl)/BSFC

min 2 l plotted against percent maximum continuous (me) BHP = 100 [BHP /230).

l The increase in inlet MAP from point 1 to point 2 may also be ob- served in Figure 5.9. As the inlet MAP of point 1 decreases, the value of FI increases, reaching the stoichiometric fuel-air mass

ratio at Pm = 10"Hg. In comparison, the value of F 2 is virtually

The value of t.BSFC . % decreases as the constant at F2 = 0.0494.

ml.n percent mc BHP decreases.

As discussed previously, the current practice in General Aviation is to lean at constant inlet MAP and constant RPM. Once the "maximum economy" point is reached by this leaning technique, a further decrease in BSFC is possible with no further loss in BHP: Figure 5.9 indicates that for the engine represented therein (at sea level, 2300 RPM) this BSFC decrease is less than 2% for BHP values (at the "maximum economy" point) greater than 50% mc BHP [this is the BHP range in which General Aviation airplanes generally 5-21 operate in cruise].

For BHP values (at the "maxim1..Ull economy" point) less than 50% mc BHP, the dec.rease in BSFC from point 1 to point 2 is substantial.

This BHP range is appropriate to automobiles in constant speed dri ving conditions. From Figure 5.9, an automobile cruising at say 25% mc BHP would achieve a 4.5% decrease in BSFC if its fuel metering schedule was established on the basis of 1eanouts at {constant BHP, constant RPM} rather than at {constant inlet MAP, constant RPM}.

F for Minimum BSFC During Const.ant BHP Leanouts: Woods (31) discusses the procedures for establishing optimum fuel metering schedules. He shows that fuel-air mass ratio schedules for minimum BSFC must be obtained by leaning at constan.t BHP (rather than at constant inlet MAP) and constant RPM. This has been confirmed by the NMBTE performance model in the foregoing . t su sectlon. Woods (31) concl:udes that approximately a 4% decrease b in BSFC is achieved, wi th the Jee:p engine at constant RPM, by leaning from point 1 to point 2 in the manner described in the foregoing

subsection; and that the true minimum BSFC = BSFC occ.urs at a fuel-

. t' F = 0.9 Fltt.

(rn Figure 5.9, a dec.rease in BSFt alr mass ra 10 2 of 4% corresponds to F 2 ::: 0.78 F 1 and to BHP ::: 27.5% mc BHP) .

t Woods also shows that an equivalent correct metho.d for obtaining optimum fuel metering schedules is to: "Maximize torq:ue for a con- stant fuel consumption [fuel mass flow rate] and constant speed" (31).

ttw d (31) d h . ... ... d' 00 s oes not s.tate t e 19U1 tlOO tlDUng corre.spon .1 .. ng to· these results, but from the context of his discussion t:hat timing is assumed to be MBT.

5-22 In the present work, we are interested in determining the fuel-air mass ratio schedule yielding the minimum possible BSFC over the operational envelope {BHP, RPM, altitude} of the engine. To determine this schedule, a series of leanouts at {constant BHP, constant RPM, constant altitude} was performed using the NMBTE performance model. The results of these leanouts are shown in Table 5.3.

On the basis of these results it is proposed that, for General Aviation naturally aspirated piston engines employing MBT ignition timing:

A single value of F = F. will yield minimum BSFC in all

mln steady state operating conditions {BHP, N , H} (when F is E not constrained by other considerations). In the present

work, F. = 0.05 is used.+ The choice of a single value

mln of F. is expected to yield negligable variation in BSFC wn from the true mininrum BSFC at any operating point {BHP, N , E H} due to the flatness of the (F, BSFC) curve at such an operating point.

It is assumed in the present work that in all steady state operating conditions {BHP, N , H} of General Aviation naturally E aspirated piston engines employing MBT ignition timing, BSFC in-

creases continuously as F increases from F. = 0.05 through

mln F = 0.08 (F is defined in the next subsection).

max max t cf . CurtiSS-Wright TC18 leanout discussed on pp. 5-14 through 5-15.

5-23 In the (NMBTE perfo,nnancem0(i'e1) constantSHP Ie-anont'S de- f scribed above, inlet M;t\P P was found to reach itsmi:nimum at F = m

F = 0.08 and t:o inc:reasec:ontinuouslyas F decreasc:edfrom F =

max . max O.ost through F;. '=. 0 .•. 0.5:. In th.e 'pe,r.es:ent' work·., 'tni.:s·· s'ame b'ehavior nun of P isa:ssumed to be true of" GelYeral AViation naturally aspirated m pis ton engines employing MBT ignition timing.

Note that the value of F. = 0.05 determined above is about

mIn 16.7% leaner than the valueF = O .. Oi6.currentl.y recogniz.ed (23) as offering maximum economy for fi-xed i.gnitiontimtrrg engines. TIre

value F. = 0.05 predicted by the NMB'fE perfo:rmancemodel may .not

mln be the value found to pertain to real engines using MBT ignition timing, since it res-ul'tS from the part,tcular design parameter values used in the Nr-UnE modeL The true importance of these constant BHP lean- out resul ts is tha·t the mini1lf.um valu'e ·o.f BSFC, throughout the engine operational envel:o,pe, occursatessenti,allY'a constant v,a:lue of F. On the other hand, the value f. :; O.DS is sunn'ort'ed by the fact that: for lIun rr the leanouts at {cons'tant inl.ett-1A'P, constant RPM, se:a level} in Fi gure 5.9, the NMBTE perrormancre mod'el predicts l1Iinimum BSFC to occur in the range 0.05'65 <F < 0.059 rOT P in the rang~ 28 >P - -- m . - m inches Hg ~ 20;. This" F.rarrg;e. is s'l.ightly lean of the. l"inaximum economy" val ueF=0.06 (2.3) and F=O. 0 59 (27) for fixed ignition timing engines.

F for Maximum BHP During consta:rl't P Leanouts-: m The NMBTE perfomance l1l0del was used t!odetemi~-e the variation in fuel-air mass rati'o yielding maximum BUP, duriing leanouts at two h· 0 1 t ln .01 inches Hg.

5-24' {constant inlet MAP, constant RPM, constant altitude}, over the operational envelope of the engine. The results of these leanouts

I

are shown in Table 5.4.

On the basis of these results it is proposed that, for General Aviation naturally aspirated piston engines employing MBT ignition timing:

I

A single value of F = F will yield maximum BHP in all

max

I

steady state operating conditions {Pm' N , H} (when F is E not constrained by other considerations). In the present

work, F = 0.08 is used. The choice of a single value of

max .

F is expected to yield negligible variation in BHP from max the true maximum BHP at any operating point {Pm' N , H} due E to the flatness of the (F, BHP) curve at such an operating point.

It is assumed in the present work that, in all steady state operating conditions {Pm' N , H} of General Aviation naturally E aspirated piston engines employing }oiBT ignition timing, BHP de-

cre.ases continuously as F decreases from F = 0.08 through

max F. = 0.05.

m1n

The value of F = 0.08 predicted by the NMBTE performance

max model may not be the value found to pertain to real engines using MBT ignition timing, since it results from the particular design parameter values used in the NMBTE model. The importance of these constant P leanout results is that the maximum value of BHP, m throughout the engine operational envelope, occurs at essentially

a constant value of F. The value F = 0.08 is slightly rich of

max 5-25 J the "best power" value F = 0.078 (23) 'and F =0.076 (27) for fixed , ignition timing engines.

Cons tantPand Constant BH? L.e;anouts from F m ~x Chirivel1a (16) identifies th,e "best pow-er poi.nt" .a5 .a fuel- air mass ratio cOllDllonly sele'cted by General Aviation pilots in cruise operations: . . the "best power point" is an enginecondi tion well known to pilots and easy to reach. Further- more, and in spite ·of the power set'tings offered by the manufacturer for airpl anes provided with TIT and fuel flow gauges ,most pilots do like to operate the engine at such a point because of the safe margin in TIT and/ol' the absence of engine roughness (16).

We shall thereforee.xamine some typical cases of leanout from the fuel-air mass ratio F = 0.08, using the NMBTE performance max model. These leanouts will provide, for naturally aspirated MBT igni tion timing engines, an indication of the BSFC improvements possible relative to the BSFC values obtained using a fuel-'air mass ratio typical in current Gene.ral Aviation practice.

Figure 5.10 shows four leanouts from F = 0.08: the left

max half of this figure shows sea level performance at 2450 RPM; and the right half of this figure shows perlormanc-e at 6000 ftand 2450 RPM.

Consider the left half of Figure 5.10. At the ope.ratin'g

point 1 [F = F = 0.08, P = 17.72 inches H,g, BHP = 115= 50% mc

max m BHP] the BSFC is BSFC . Two leanouts are show,n ori:ginating from I point 1.

5-26

1. Leaning at cconstant Pm = 17.72 in. Hg, from point 1

to the minimum BSFC = BSFC at point 2, yields a decrease

in BSFC of 12.15% BSFC and a drop in BHP of 16 BHP.

I "

2. Leaning at constant BHP = 115, from point 1 to the minimum

BSFC = BSFC at point 3, yields a decrease in BSFC of

17.84% BSFC , and requires the inlet MAP to be increased l to 22.93 in. Hg.

3. Operation at point 3 rather than at point 2 yields a decrease in BSFC of 6.48% BSFC and an increase in BHP of 16 BHP.

The right half of Figure 5.10 is similar to the left half of the same figure. At point 6, the inlet MAP has been increased to 21.51 inches Hg which is almost the wide open throttle value P ~ 22.9 inches Hg.

DWOT Figure 5.10 clearly shows that significant decreases in BSFC may be achieved by leaning from the "best power" fuel-air mass ratio. The constant BHP leanouts from the "best power" point in Figure 5.10 show a maximum possible decrease in BSFC of about 17.8% of tIle "best power" BSFC. This result compares well with the ex- perimental results reported by Chirivella (16) for similar leanouts of a turbocharged Lycoming TIO-54l-E engine in flight. Chirivella's tabulated resul ts of leaning at constant BHP from the "best power" fuel-airmass ratio, with the ignition timing advanced from the standard setting of 20° BTDC to 30° BTDC, show that BSFC decreases (16) : 5-27 · .. from 11.8 up to 20.8% if s'evere roughness is allowed. The numbers become limited to 17.4% if only incipient roughness is tolerated. I f on the other hand the engine is not allowed to operate with any trace of roughness,. the best fuel economy [BSFC] improvement is identified as 14.4% at 15,000 ft altitude and 75% rated power.

When leaning from the "best power" fuel-air mass ratio, the advantages of leaning, at constant BHP rather than at constant inlet MAP are tha t : 1. No loss in BHP is suffered - 2. A substantially lower minimum BSFC is achieved: about 6% lower in the cases shown in Figure 5.10.

Of course, if WOT is encountered during a constant BHP leanout,. the full BSFC advantage of this leaning technique cannot be realized.

I I I I Performance with Specified Fuel Metering Schedule We here examine the manner in which BSFC, inlet MAP and fuel mass flow rate vary with brake torque" RPM and altitude; when fuel is metered to the engine according to the fuel metering schedules A, Band C shown in Figure E .18.

BSFC Performance Maps at SeC1. Level: Figures 5.11 - 5.13 show BSFC versus engine brake torque, for constant values of P and RPM at sea level; as computed by the m NMBTE performance model. Lines of constant percent maximum con- tinuous BHP are superimposed on these figures. Figures 5.11, 5.12, L' I I 5.13 correspond to fuel metering schedules A. B. C res'pectively.

5-28 In each of p'igures 5.11 - 5.13: • 19.:s. inl et MAP, inches Hg < 29 • 2000 < RPM < 2600 The following may be observed in Figures 5.11 - 5.13: .~ 1. At constant fuel-air mass ratio a) Brake torque increases with increasing P , at constant RPM m b) Brake torque decreases with increasing RPH, at constant P m c) BSFC decreases with increasing P , at constant RPt-1 m d) BSFC increases with increasing RPH, at constant P .

m 2. The diagrams generally move to lower BSFC and lower brake torque ranges, as the fuel metering schedule varies from A to B to C. This is to be expected from the foregoing discussion of leanout performance.

In Figures 5.11 and 5.12, the rising values of BSFC with in- creasing brake torque (at constant RPM and high BHP) are due to the rising value of F with increasing air mass fraction at high values of the latter.

With fuel metering schedule A (Figure 5.11) at any fixed RPM, minimum BSFC occurs at about 85% maximum continuous BHP. With fuel metering scheduleB (Figure 5.12) at any fixed RPM, minimum BSFC occurs at about 64% maximum continuous BHP. With fuel metering schedule C (Figure 5.13) at any fixed RPM, minimum BSFC occurs at WOT: note that fuel metering schedule C meters the fuel-air mass .J ratio F. to the engine at all times.

m~n Figures 5.14 and 5.15 correspond to Figure 5.11: • Figure 5.14 shows inl et tolAP vs. brake torque for various constant values of RPM; for fuel metering schedule A.

5-29 • Figure 5.15 shows fuel mass flow ratevs. brake torque for various constant values of RPM; for fuel metering schedule A.

• All of the information in Figure 5.11 is contained in Figures 5.14 and 5.15. In particular, fOT any brake torque and RPM in Figure 5.15, the BSFC is computed ftom Equations E.3 and E.8.

Likewise, Figures 5.16 and 5.17 correspond to Figure 5.12; and Figures 5.18 and 5.19 correspon'd to Figure 5.13.

BSFC Performance Maps at Altitude: Figure 5.20 shows BSFC versus engine brake torque, for constant values of P and· RPM at 6,000 ft al ti tude; as computed by the M>1BTE m performance model using fuel metering schedule B. Lines of constant percent maximum continuous BHP are superimposed on this figure.

Figure 5.20 may be compared to its sea level counterpart Figure 5.12. Note that in Figure 5.20: at any fixed RPM, minimum BSFC occurs at about 65% maximum continuous BHP.

Figures 5.21 and 5.22 correspond to Figure 5.20, and may be compared respectively to their sea level counterparts Figures 5.16 and 5.17.

Al ti tude Variations of BSFC with Constraints We now examine al ti tude variations in BSFC when various con- straints are imposed uppn the engine operation.

5-30 Beginning at the operating point • Sea level • P = 21.56 inches Hg m • RPM = 2100

• BHP = 55% maximum continuous (mc) BHP

• F = 0.067

five constrained altitude variations in BSFC were computed using the NMBTE performance model. The constraints imposed and the results of the computations are shown in Figure 5.23.

The constraints BHP~ = constant and RPM;a- = constant were

selected for the computations of Figure 5.23 because: Straight and level steady flight of a fixed-pitch propeller airplane with • Fixed gross weight • Fixed center of gravity position • No propeller compressi bi Ii ty effects at constant equivalent airspeed (EAS) and at various altitudes requires tha t BHP~ = constant and RPMIcr = constant (see Chapter 4) .

In Figure 5.23: 1. Compare curves A and C: the greater values of P required m for curve C result in greater decreases in BSFC with alti- tude for curve C than occur for curve A.

2. Compare curves C and B: the greater values of RPM for curve B result in sma11e~ decreases in BSFC with altitude 5-31 for curve B than occur for curveC (or curve A). Note "(: that curve B, which corresponds to the fixed-pitch pro- peller airplane at constant EAS described above, reaches a minimum BSFC at an altitude of about 8,000 ft.

3. Curves C and D are not identical, but are almost indis- tinguishabl e and are shown as a single curve. The al ti tude variations in BSFC for curve D are attributed solely to the al ti tude variations in inlet manifold temperature and exhaust absolute back-pressure.

4. Compare curves D and E: the increas ed values of RPM for curve E result in smaller decreases in BSFC with altitude for curve E than occur for curve D.

Figure 5.23 clearly shows the extent to which al ti tude. variations in BSFC depend upon the engine operational constraints. The co- location of curves C and D in Figure 5.23 is further discussed in the next subsection.

Corrected Quantities , In order to formulate a compact engine-atmosphere subsystem input-output model, we do well to make use of corrected quantities; as we did in Chapter 4 in the formulation of the APA subsystem input- output model. We here develop such corrected quanti ties using the NMBTE performance model.

5-32 Corrected Brake Torque: The co-location of curves C and D in Figure 5.23 stimulated the search for an expression for corrected brake torque in part-throttle operating conditions.

Examination of the computer computations which produced curve D (Figure 5.23) revealed that: At constant Pm = 21.56 inches Hg, constant NE = 2100 RPM,

and constant F = 0.067; BHP;';- varied from the sea level

value BHP by no more than 0.5% of BHP ' for altitude O O variations from sea level through 10,000 ft (standard atmosphere) .

To check the reality of these computations, the cruise per- formance charts in the Information Manual for the Cessna 1980 Centurion were examined, and it was found that:

For the Cessna 1980 Centurion at constant P = 22 inches

m Hg, constant NE = 2300 RPM and recommended lean mixture; the value of BHP~ at 2000 ft, 4000 ft, 6000 ft and 8000 ft (standard atmosphere) varied from the mean value BHP~ by no more than 1% BHP~. The value of the fuel-air mass ratio F for the "recommended lean mixture" is unknown to the author.

These data agree with the NMBTE performance model computations for v curve D (Figure 5.23).

Extensive computations using the NMBTE performance model were then performed to determine an expression for Corrected Brake Torque in part-throttle operating conditions. These computations revealed that: 5-33 Operation of the naturally aspirated MBT ignition timing engine here modelled, in the standard atmosphere, with con- stant values of • Inlet MAP P 1 inches Hg m • Engine speed N , RPN E • Fuel-air mass ratio F yields a brake torque Q 1b ft which is a function of altitude E H (ft) only. At sea level, Q takes the value QE' The Cor- E a rected Brake Torque Q given by E c n

Q = Q CJ 1b ft (5.1)

E E c varies from Q by less than :::..1% of Q ' for altitudes in the E E

o a

range 0 .::. H (ft) < 10,000; for constant values of {Pm' N , F} E in the ranges • 19 < P (inches Hg) < [p at WOT] - m - m • 2000.::. NE (RPN) .::. 2600 • 0.05 < F < 0.08

where CJ = atmospheric ai r density ratio at al ti tude H Cft)

(Appendix B) n = Density Index = n(F). The Density Index n is a function of the fuel-air mass ratio F only: this functional relationship is shown in Figure 5.24.

Equation 5.1 is illustrated in Figure 5.25.

It is emphasized that constancy of the corrected brake torque Q with variations in altitude applies only to engine operation E c at constant inlet MAP. Q is not constant with variations in E c altitude when the engine is run at wide open throttle at each 5-34 altitude, since inlet MAP varies with altitude in this case.

Corrected Air Mass Flow Rate: Equation E.42 shows the relationship between the air mass flow rates at any two operating points 1 and 2. Consider two operating points. one represented by the subscript 0 and the other by the absence of any subscript: for these two operating points, Equation.

E.42 becomes (5.2) lbm/hr The following assumptions are now made: 1. The operating point represented by subscript 0 is at sea level in the standard atmosphere (Appendix B), where

P = Po = ambient atmospheric absolute pressure =

atmos O 29 .92 inches Hg , .

T = TO = ambient atmospheric temperature =

atmos O 288.15 degrees Kelvin.

2. The operating point represented by the absence of'a sub- script is at any altitude in the standard atmosphere, or in a non-standard atmosphere, where

P = ambient atmospheric absolute pressure, inches Hg

atmos

Tatmos = ambient atmospheric temperature, degrees Kelvin

P P 3.

=

m mO (5.3) = NE NE 5-35 4. T T m atmos -- =< T 288.15 -i~ mO (5.4) P P e atmos -- =< P 29.92 eO With these asstmlptions, Equation 5.2 becomes T ] (1 - e: ) t p P atmos ] e:

m = m atmos

lbm/hr (5.5) [ [ a a 288.15 29.92 O

We now define the Corrected Air Mass Flow Rate m

to be a c

m :: m lbm/hr (5.6)

a a O c Substituting this definition in Equation 5.5 yields t • . . [T atmos ] (1 - E: ) [P atmos ] E:p m -m -m lbm/hr (5.7) a - a - a 288.15 29.92 c O When m is known for any conditions {P ,N }'· the value of E a mO 0 O

rn in any other operating condition {P = P ,N = N P

E E' atmos' a m ~

o

T t } may be computed using Equation 5.7. Note that Equation 5.7 amos is independent of the fuel-air mass ratio F metered to the engine.

Corrected Part-Throttle Performance Model of P and rn

m a The foregoing discussion of corrected quanti ties permi ts the fonnulation of a corrected part-throttle perfonnance model of P and m

rn. Figure 5.26 shows such a model, computed uSing the NMBTE

a performance model.

Consider the left half of Figure 5.26, which shows P versus m

this has been drawn for F = F. = 0.05 and standard

mIn 5-36 atmosphere conditions, for which the density index n = 0.57 (Figure 5.24); and is applicable to all altitudes in the standard atm0sphere.

The sea level wide open throttle line is shown. At altitudes above sea level, the WOT line moves to lower values of P than indi- m cated by this sea level WOT line. The left half of Figure 5.26 was drawn by plotting P versus Q and NE ' and relabelling the E mn n

U v o

resulting diagram in accordance with Equations 5.1 and 5.3. Dia- grams similar to the left half of Figure 5.26 may be drawn for fuel-air mass ratios F = constant ~ 0.05.

Consider the right half of Figure 5.26, which shows P versus m m and N : this diagram applies to all fuel-air mass ratios F; E a c and to all altitudes in either the standard atmosphere or any non- standard atmosphere. The sea level wide open throttle line is shown. At pressure altitudes other than sea level, the position of the WOT line varies from the position of this sea level WOT line.

The right half of Figure 5.26 was drawn by plotting P versus m a mO O and NE ' and relabelling the resulting diagram in accordance with

o

Equations 5.3 and 5.7.

Input-Output Model We now formulate the input-output model of the Naturally aspirated MBT ignition timing Engine-Atmosphere (NEA) subsystem.

Formulation for the Standard Atmosphere": The NEA subsystem input-output model is required: 5-37 1. To be co.mpatible wi th the input-output model o.f the APA subsystem (Chapter 4). This requires that {N , QE' E Ta tmos' P a tmos} be inputs to. the mode 1 (see Figure, 4. 8) .

I t will be shown that H is also separately required as an input to the NEA subsystem input-o.utput model. t 2. To output the values of fp ,F} required to. minimize BSFC, m at the operating point {N , QE' H}. The values of P E m and F are required as control inputs to the engine.

3. To output values of BHP and m in order that BSFC may be f computed. R* may then be co.mputed from this BSFC and the value o,f R*c provided by the APA subsystem input-output model.

4. To be suitable for airborne microprocessor implementation.

The required inputs and outputs of the NEA subsystem input- output model are: Brake torque, lb ft Inputs: Q E Engine shaft speed, RPM NE H Altitude, ft T Atmospheric ambient air temperature, atmos Kelvin' degrees P Atmospheric ambient air absolute pres- atmos inches Hg sure, MAP, inches Hg Outputs: P Inlet m ,,' tIn the standard atmosphere, Tatmos :Ts and P atmos are uniquely determined by H in the manner described by Appendix B.

5-38 F Fuel-air mass ratio Fuel mass flow lbm/hr m rate, f c Brake specific fuel consumption, ';- lbm/BHP.hr.

Previous discussion in this chapter (pp. 5-22 through 5-26) has shown that, for naturally aspirated MBT ignition timing engines operating in the standard atmosphere: 1. In all steady state operating conditions {QE' N , H} E requiring part-throttle or WOT: a) BSFC is minimized by operating the engine at a fuel-air

mass ratio F = F. = 0.05 (when F is not constrained

m~n by other considerations)

b) BSFC increases continuously as F increases from F =

F = 0.05 through F = F 0.08.

=

min max c) P decreases continuously as F is increased from F = m

. F. = 0.05 through F

= F = 0.08.

m~n max 2. In all steady state operating conditions {P , N , H}: E m a) Q increases continuously as F increases from F = F = E min 0.05 through F = F = 0.08.

max b) Q reaches its maximum value at F = F = 0.08.

max E [These same results lea) through 2(b) are assumed to be true for naturally aspirated MBT ignition timing engines in all operating conditions {Hp' Tatmos' Patmos} in any non-standard atmosphere.)

The cruise operating condition {QE' N , H} of the engine is E 5-39 prescribed by the APA subsystem, which subsystem also establishes the value of R*c. In order to maximize R* in every such cruise operating condition of the engine, we would like to operate the en-

g ine at the fuel-air mass ratio F = F. at all times in cruise

. m~n (see 1 (a) above). However, it may be impossible for the engine to

deliver the required value of QE' even at WOT, when F = F .. In

mln the latter case, the only way to obtain the required value of Q E is to increase F above F . :. the minimum possible BSFC will then m~n be obtained with a value of F which yields the required value of Q E at WaT (see 1 (b, c) and 2(a) above). In the operating condition {NE' H}, the engine delivers maximtml brake torque Q when operating E at WaT and F = F (see 2(b) above, and Equations E .43, E. 57}.

max In the light of these considerations, we proceed as follows in the formulation of the NEA subsystem input-output model:

1. Fuel-air mass ratios in the range (F. = 0.05) < F <

m~n (F = 0.08) only are considered.

max 2. The engine part-throttle performance is modelled at a constant fuel-air mass ratio F = F. = 0.05.

m~n

3. At fuel-air mass ratios F > (F. = 0.05) ,the engine

m~n waT perfonnance only is modelled.

The NEA subsystem input-output model consists of: 1. A corrected part-throttle performance plot such as that ~ I shown in Figure 5.26.

2. A set of five Wide Open Throttle performance plots such as those shown in Figures 5.27 and 5.28.

5-40 3 .. Equations andS.7.

S.l 5.10, following; 4. Equations 5.8 - Fuel mass flow rate Ih : f (5.8)

Ih = F m lbm/hr

f a Brake horsepower BHP: (5.9)

BHP = [33 ~~oo ] Q NE

E Brake Specific Fuel Consumption c: Ih f lbm/BHP .hr (5.10)

c = BHP

Figure 5.26 shows the part-throttle performance in terms of the corrected quantities Q The left half of Figure 5.26 E c applies to F = F. = 0.05 and to the standard atmosphere. The right m1n half of Figure 5.26 applies to all values of F, to the standard atmosphere and to all non-standard atmospheres.

Figure 5.27 shows schematic WOT performance at four values of F in the range F. < F < F [The WOT performance is presented m1n - - max at four values of F in order to permit cubic interpolation in Figure 5.29.] Each of the four Figures 5.27 (a-d) shows Q as a E function of NE and H at WOT,in the standard atmosphere, for a fixed value of F.

Figure 5.28 is a schematic WOT performance plot of P as a m function of NE and H. This figure applies to the standard atmosphere, to all non-standard atmospheres (in non-standard atmospheres, H is read as pressure altitude H ) and to all values of F.

p Note that Figures 5.27 and 5.28 are schematic: they have not 5-41 been computed using 'an accurate waT performance model. The minimtun and maximum values ef NE shown in -Figures 5.27 and 5.28 represent WaT the RPM limi ts for continuous .eperatien of the engine .

Schmidt (32) gives a numbe-r of formulae for computing the waT altitude performance (BHP , BSFC) of naturally aspirated aerO' engines frem the WaT perfermance (BHP, BSFC) ef these engines at sea level. WOT perfermance has not been fermulated in terms ef Cerrected Quanti ties in the present work and the data storage penal ty for this omission is small.

Computational Scheme (Standard Atmosphere): The use of the NEA subsystem input-output model for computing the set {Pm' F, Ih } which yields minimum BSFC for any set of inputs f {Q N H T P } is now described. The standard atmos- E' E" atmos' atmos .

phere is ass tuned. so that T :Ts (Appendix B) .

atmos

1. Enter Figure 5.27(a) with {N = N H. = H} and

EWOT E' -:waT determine Q EWOT a) If Q ~ Q it is possible to' eperate the engine with E E WOT

F = F. = 0.05, at ei'ther part-threttle or WOT. GO' to

m1n Step 2.

b) If Q < Q it is not possible to operate the engine E E WOT with F = F. = 0.05. Go to Step 3.

m1n 2. F = F . : m1n a) Cempute Q (Squation 5.1).

E c 5-42 b) Enter Figure 5.26 with {QE ' N } and determine {Pm' ma }.

E c c (Equation 5.7)

c) Compute m

a d) Compute m = F. m, Ibm/hr.

f m1n a e) The required quantities {Pm' F, m } have now been f evaluated.

fj Compute BSFC (Equations 5.9 and 5.10). Stop.

3. F > F. and WOT: m1n a) Enter each of Figures 5.27 (a, b, c, d) in turn with {QE = QE' N = N } and determine the value of the E EWOT WOT corresponding wide open throttle altitude HwOT' In Figure 5.27 (a, b, c, d) the value of HwOT is HI' H , H , H4 respectively. Store the four co-ordinate pairs [(H., F.), i = I, 2, 3, 4] so obtained.

1 1 This step is illustrated in Figure 5.27 by the points A, B, C, D each of which corresponds to the S~T.e b) Interpolate between the four co-ordinate pairs [(H., F.), i =1, 2, 3, 4] to determine the value of 1 1 F corresponding to the required altitude ii. This step is illustrated in Figure 5.29. This value of F yields the required value of Q at {N , H} and WOT. Note that E E if H exceeds the value of ~OT obtained from Figure 5.27(d) (in which F = F ) then the engine is incapable . max of developing the required value of Q at {N , H}.

E E 5-43 c) Enter Figul"e 5 .• 28 with {oN = N_, BWOT ~= B}and EWOT ~r: detenninethe requi red iril.et'f.1AP p=p m1DwOT .d) Enter the right half of rigure5.26 with {Pm' N } E .anddetennine m a c e) Compute m (£quati on 5.7).

a f) Computem (Equation 5.8).

f g) The required quantities {Pm' F, mf}have now been evaluated. P is not required for output since the m throttle is wide open.

h) Compute BSFC (Equations 5.9 and 5.10). Stop.

In the above computations, interpolations (linear, parabolic, cubic) may be performed using L.agrange's Interpolation fonnula (33).

Formulation and Computations (Non-Standard Atmosphere): In non-standard atmospheric conditions, the operating con- di tion of the engine (as demand~edby the APA sUbsystem) is defined by the set {Q N H TP } ·E' E' p' ·atmos· atm05 where H- pressure al titude, ft p

Tatmos = atmospheric ambient air temperature at H '

p degrees Kelvin P - atmospheric a11lbient air absolute pressure at atmos ",. i B , inches Hg.

P The only change in the above Formulation for the Standard Atmosphere required to account for non-standard temperature T atmos a t pressure alti tude H is: p 5-44 Altitude H must be read as pressure altitude H in the p text and in Figures 5.27 - 5.29.

The computational scheme listed in the foregoing subsection for the standard atmosphere is retained for non-standard atmos- pheres, with the following adjustments.

1. H is read as pressure altitudeH in the text and in Figures p 5.27 - 5.29.

2. It is necessary to adjust the value of Q required by the E APA subsystem, to account for non-standard temperature at H , prior to entry into the computational scheme.

p Let:

~Tatmos = [atmospheric ambient temperature (degrees

Kelvin) in the non-standard atmosphere at pres- sure altitude H ] - [atmospheric ambient . p temperature (degrees Kelvin) in the standard

atmosphere at H = H ] = T - T

P atmos s

= [rate of change of Q with

E T t when {H , Pm' N , F} are invariant: L E amos p 0 denotes that MBT ignition timing is maintained during perturbations in Tatmos]' lb ft/degree Kelvin.

brake torque (lb ft) required by the APA sub- system in the non-standard atmosphere, and 5-45 developed by the engine in the operating con- dition {H , T , P , N , F, l } in the same E p atmos m 0 non-standard atmosphere ~ brake torque (lb ft) developed by the engine in <' the standard atmosphere, in the operating con- di ti on {H = H , P , N , F, l } E P m 0 where l denotes MBT ignition timing.

o Then, liT aT atmos atmos H , P , N , F, l E P m 0 + (higher order terms in ~T t ) (5.11) amos We retain only the first 'two terms on the right hand side of Equation 5.11. The functional dependence of the derivative aQE/aTatmOS! on the variables {Hp' Pm' N , F} E H • P , N , F, l E P m 0 at l has not been determined in this work. I t may be found o that sufficient accuracy in the computations is obtained l?y allocating a constant value to this derivative: if this is not the case, some iteration may have to be incorporated into the computational scheme.

The brake torque Q = [QE]NEA is used in the computational

E scheme when computing Q and when entering Figure 5.27.

E c ,.

However, when computing BHP (Equation 5.9) and BSFC (Equation 5.10), the brake torque value used must be Q = [QEl .

E JAPA 5-46 n In computing Q =Q a for entry into Figure 5.26, the 3.

E E c density ratio a used must be the standard atmosphere value of a at the altitude H =·H ft.

P 4. The non-standard atmosphere values of T t and P tare a mos amos used to compute m (Equation 5.7).

a The NEA subsystem input-output model, appropriate to standard and non-standard atmospheric conditions, is presented in block dia- gram form in Figure 5.30.

Implementation: The principal hardware items required for implementation of the NEA subsystem input-output model are: 1. An ignition timing regulator providing MBT ignition timi ng and retarding this i gni tion timing as necessary to control detonation.

2. A fuel-air mass ratio controller providing F as commanded by the NEA subsystem input-output model. It is desirable that this controller provides a value of F within 1% of any command value of F.

3. Microprocessor.

Items 1 and 2 should be automatic control systems.

The NEA subsystem input-output model is well suited to imple- mentation in an airborne microprocessor for the following reasons: 1. Figures 5.26 - S.28 require very little memory space for data storage.

5-47 2 . The requiredcomput-ations are few and simple.

Figures 5.26 - S.28nrust be compiled from flight test data in order that installation effects may be properly accounted for.

The data requirements of thes-e "figures are self-evident, perhaps with the following exceptions: The 'flight test datanrust establish 1. The values of F to be used for the compilation of ,Figures 5'.26 and 5.27 .

2. The value of the Density Index nfor Figure 5.26.

3. The values of e:tand e:pfor Figure 5.26.

Flight test data are also required to establish the functional aT and to quantify this function

nature of aQE/ t I

amos H , P, NE,F, T pm 0 for use in the input-output model.

Summary The performance predictions of the NMBTE perforrnancemodel have been discussed. The NEAsubsys:tem input-output model has been formulated, and the use of this model 'for performance compu- tations has been discussed. This input-output model is compatible with the APA subsystem input-output model developed in Chapter 4.

The NEA subsystem input-output model issumrnarized in block diagram form in Figure 5.30.

TURBOCHARGED ENGINES The turbocharger is a mechanical device, consisting of a rotating turbine and a rotating c-ompressor, which is used in 5-48 conjunction with a piston engine. The turbine extracts power from the exhaust gas of the engine, and with this power drives the com- pressor by means of a rotating shaft. The compressor uses this power to increase the pressure (and temperature) of the engine induction air. A piston engine and turbocharger are shown schemat- ica1ly in Figure 5.31.

The shaft power output of the turbine is often controlled by means of a Waste-Gate, which is used to direct a portion of the engine exhaust gas through the turbine and to discharge the remainder of this exhaust gas directly to the atmosphere. The waste-gate is located in the Exhaust Manifold (the region of the exhaust system between the exhaust valves and the Turbine Inlet). When the waste- gate is closed, all of the engine exhaust gas passes through the turbine; and when the waste-gate is wide open, most of the engine exhaust gas is discharged directly to the atmosphere without passing through the turbine.

A throttle is placed in the engine induction system downstream of the compressor outlet. The portion of the engine induction ·system between the compressor outlet and the throttle is called the Deck; and the portion of the engine induction system downstream of the throttle is called the Inlet Manifold.

The relationships between the absolute pressures and tempera- tures of the atmosphere, deck and exhaust manifold are determined by the performance characteristics of the compressor and turbine.

In general, however, when {H , T t ' N , F, waste-gate position} E p a mos 5-49 are constants and T = constant or MBT, opening the throttle increases: 1. Inlet MAP 2. Exhaust manifold absolute pressure (this is the exhaust ".

back-pressure on the engine) 3. Turbocharger shaft rotational speed 4. Deck absolute pressure 5. Deck temperature 6. Inlet manifold temperature.

In general, these same six quanti ties are increased by closing the waste-gate, when {H , T t ' N , F~ throttle position} are con- E p a mos stants and T = constant or MBT.

Therefore both the throttle and the waste-gate may be used to control the BHP and Q of the engine, since both influence the inlet E ~~. However, an increase in inlet MAP is achieved at the expense of: an increase in inlet manifold temperature (which increases engine temperatures generally, decreases the engine indicated horsepower which decrease contributes to increasing the engine B5FC, and increases the likelihood of detonation); and an increase in engine back-pressure (which decreases volumetric efficiency and increases the engine pumping losses, both of which effects con- tribute to an increase in engine B5FC).

The performance of turbocharged spark-ignition (51) piston engines employing MBT ignition timing may be modelled by incorporating a performance model of the turbocharger compressor and turbine in the model of the naturally aspirated engine given in Appendix E.

5-50 Such modelling is a necessary prerequisite to the construction of a fuel-efficient input-output performance model of the Turbocharged MBT ignition timing Engine-Atmosphere (TEA) subsystem. The author was able to obtain the compressor performance data for a turbo- charger used in General Aviation, but was unable to obtain the corresponding turbine performance data. Consequently, turbocharged SI piston engine performance is not modelled in this work.

The author was also unable to obtain experimental performance data for naturally aspirated and turbocharged SI piston aero engines usingMBT ignition timing. In the absence of such data, and in the absence of a turbocharger performance model, no rigorous comparison of naturally aspirated and turbocharged engine performance is presented in this work.

The following remarks concerning turbocharged engine performance and the construction of a TEA subsystem input-output model are offered on the basis of the foregoing sections in this chapter.

Performance Comparison: Naturally Aspirated and Turbocharged Engines Brake Torque: The maximum brake torque Q of a naturally aspirated engine E at any operating point {H , T N , F} is limited by the maximum E p atmos' available inlet MAP P. As altitude increases, the fall in atmos- . m pheric ambient air pressure and the resultant fall in maximum {Pm' QE} for any {N , F}, seriously diminishes the performance E [decreased maximum: cruise equivalent airspeed (EAS), rate of 5-51 climb (RC), angle of climb (AC) lof an airplane powered bya naturally aspirated engine.

A turbocharger enables the P of a given engine at any {H , m p T , N , F} to be significantly increased (boosted) above the E atmos maximum P available to that engine with natural aspiration at m the same {n , T t ~ N , F}. Associated with such increases in E p amos Pm are significant increases in QE' The airplane performance improvements [increased maximum EAS, RC, AC at any {Hp' Tatmos' oNE' F}] resulting from this increase in QE' especially at altitude, has been the historical motivation for turbocharging airplane piston engines.

Brake Specific Fuel Consumption: On the basis of the discussions of naturally aspirated engines earlier in this chapter, it is assumed here that: in all steady state operating conditions {H , T t ' BHP, N } of General Aviation E p amos turbocharged piston engines employing MBT ignition timing A single value of F = F. will yield minimum BSFC (when 1.

m1n F is not constrained by other considerations) 2. BSFC increases continuously as F increases above F = F . • ID1n The ability of the turbocharger to boost P , above the maximum m P that would be available to the engine with natural aspiration, m has important consequences for the BSFC of turbocharged engines.

Consider an airplane powered by a naturally aspirated engine, and assume that the APA subsystem demands that the engine operates in the condition {H , T t ' QE' N }. It is desirable to operate E p amos 5-52

I the engine at F = F. in order to minimize BSFC. If the engine

mJ.n

cannot develop the required Q at WOT when F = F . , the only way

E mJ.n

I

I the engine can increase the brake torque to the desired value Q E I, is to increase F above F . . The maximum brake torque will be ffiJ.n developed at F = F and WOT. Increasing brake torque by mixture max

I

enrichment is accompanied by an increase in BSFC. For the naturally aspirated engine, this BSFC increase is an unavoidable penalty for operation at high brake torque: it has been demonstrated (Figure

I

5.10) that BSFC increases of about 21% may be sustained [at constant {H, QE' N } and MBT ignition timing] by mixture enrichment from E F = F. = 0.05 to F = F = 0.08.

mJ.n max Now consider an airplane powered by a turbocharged engine, and assume that the APA subsystem demands that the engine operates in the condition {H , T t ,QE' N }. I t is desirable to operate E p amos

the engine at F = F. in order to minimize BSFC. The ability of

mJ.n the turbocharged engine to boost inlet MAP to high values means that high brake torque can be developed at F = F . . Consequently, mJ.n the turbocharged engine can operate at F = F over a greater range min of flight conditions than can the naturally aspirated engine, with attendant increases in R*. The feasibility of operating turbo- charged engines ul tralean up to 75% rated BHP at high inlet MAP has been demonstrated by flight tests (16) of a Lycoming TIO-54l-E engine.

5-53 Recommendations: TEA Subsystem Input-Output Model As stated above, the performance of turbocharged SI piston engines employing MBT ignition timing may be modelled by incorporating a performance model of the turbocharger compressor and turbine in the model of the naturally aspirated engine given in Appendix E.

Such modelling is a necessary prerequisite to the construction of a fuel-efficient input-output model of the TEA subsystem.

In constructing the TEA subsystem input-output model, attention should be paid to the following: 1. Leanout performance should be examined to determine the fuel-air mass ratio F. yielding minimum BSFC during mln constant BHP 1eanouts.

2. The engine should be operated at WOT at all times, and the inlet MAP controlled by a) Waste-gate position and/or b) Variable geometry turbine nozzle ring (34).

In this manner, a given inlet MAP can be achieved with a minimum engine back-pressure and a minimum inlet manifold temperature, which conditions contribute to minimizing engi ne BS FC .

3. The option of installing an aftercoo1er downstream of the turbocharger compressor should be examined. This device cools the induction air, thereby reducing engine temperatures, increasing indicated horsepower (and hence decreasing BSFC) and decreasing the likelihood of detonation.

5-54 SUMMARY The content of this chapter is summarized briefly below.

1. A performance model of naturally aspirated, spark-ignition, inlet port fuel injection, four-stroke piston aero engines employing MBT ignition timing (the NMBTE performance model) has been presented.

2. The performance of current technology General Aviation piston engines has been discussed.

3. The performance predictions of the NMBTE performance model have been presented and discussed.

a) The 1eanout perfonnance predictions of this model indicate that: (i) The fuel-air mass ratio yielding maximum BHP in all engine operating conditions { Pm' N , H} in E the standard atmosphere is approximately constant at F = F ~ 0.080.

max

(ii) When leaning from F = F . = 0.080 at constant

max {N , H}, a substantially lower minimum BSFC is E obtained when leaning at constant BHP than when leaning at constant inlet MAP. A 6% difference in minimum BSFC for these two leaning techniques has been demonstrated.

(iii) A decrease in BSFC of approximately 17% is possible

when leaning, at constant {BHP, N , H}, from F =

E

F = 0.080 to the fuel-air mass ratio yielding

max

minimum BSFC. F = F = 0.080 is a typical

max 5-55 operating fuel-air mass ratio for General Aviation pilots.

(iv) The fuel-air mass ratio yielding minimum BSFC in all engine operating conditions {QE' NE,H} in the standard atmosphere is appro:ximat'ely con- stant atF = 'P. == 0.050.

ml.n b) BSFC performance maps have been examined.

c) The altitude variation of BSFC has been shown to be strongly dependent upon engine oper,ating .constraints.

d) Corrected quantities for engine performance have been determined. Part-throttle performance has been presented in terms of these corrected quantities.

4. TheNEA subsystem input-output model has been presented, and its use for computing performance in the standard atmosphere and in a non-standard a-tmosphere described. Implementation of the NEA subsystem input-output model has been discussed: this input-output model is well suited t.O airborne micro- processor implementation due t.O its simpliei ty and minimal st,orage requirements.

5. Turbocharged engines and their 'performance have been briefly Recommendations for the construction of a TEA reviewed.

subsystem input-output model have been offered; but this input-output model has not been developed in this work.

5-56 TABLE 5.1 ENGINE DESIGN PARAMETERS INCLUDED IN TIlE NMBTE PERFORMANCE t.lODEL Engine displacement D 470 cubic inches

=

Indicated thermal efficiency e -0.0046322

=

n! cubic (Eq. E.4l) e 1. 063657

=

1. 1

(compression ratio = 7:1) e -0.9421708

=

e 0.2200205

=

TI Kelvin Reference temperature 305.556 degrees

=

m Data for correcting indicated thermal efficiency for inlet manifold

temperature (compression ratio = 7:1)

-1 degree Kelvin

~I aT

m SI -L 10- 0.6 -1.44 x x 10- 0.8 -1.44 10- 1.0 -2.16 x x 10- 1.2 -1.08

x io-

1.4 -0.54 R o -~- 0.6 0.7 0.8 0.73 0.9 0.81 1.0 0.83 1.2 0.83 1.5 0.81 aR l -1 -0.0004 degree Kelvin

=

aT

m S I J '0 5-57 TABLE 5.1 (concluded) Lost horsepower data: Motoring coefficients 30.99 a

=

o 10- (2000 ~ RPH ~ 2600) taken a -2.705 x

=

10- from Figure E. 15. a = 1.125 x Lost horsepower coefficients k = 1.667 x x 10- 2.112 = = 0.007 10- k = 5.111 x yn Volumetric efficiency correction indices E: 0.2 = t E: 0.1

=

P 5-58 TABLE 5.2 REFERENCE OPERATING POINT AND FUEL SCHEDULE DATUM CONDITIONS USED IN THE NMBTE PERFORMANCE MODEL Reference Operating Point Inlet manifold absolute pressure P 28.42 inches Hg

=

m, ...

T Inlet manifold temperature 288.15 degrees Kelvin

=

m l P inches Hg Exhaust absolute back-pressure 29.92

=

e l Fuel-dry air mass ratio 0.084

=

Fl Brake hors epower BHP 230 hors epower

=

I Engine shaft speed 2600 RPM

=

NE Fuel Schedule Datum P Inlet manifold absolute pressure 28.42 inches Hg

=

m fsd T Inlet manifold temperature 288.15 degrees Kelvin

=

m fsd p 29.92 inches Hg Exhaust absolute back-pressure

=

e fsd Engine shaft speed N 2600 RPM

=

E fsd 5-59 TABLE 5.3 NMBTE PERFORMM~CE MODEL: CONSTANT BHP LEANOUTS During leanouts at {constant BHP, constant RPM, constant altitude}: 1. Minimum BSFC occurred at a fuel-air mass ratio F.in the range 0.0485 < F < 0.0500 2. BSFC increased continuously as F increased from the value of F which yielded minimum BSFC through the value F = 0.0935 throughout the operational envelope:

• [45% mc BHP] < BHP < [BHP at WOT and F = 0.08]

• 2000 ~ N , RPM .:. 2600 E • 0.:. H, ft < 10,000 (standard atmosphere) 5-60 TABLE 5.4 NMBTE PERFORMANCE HODEL: CONSTANT INLET MAP LEANOUTS During 1eanouts at {constant inlet MAP, constant RPM, constant alti tude}: 1. Maximum BHP occurred at a fuel-air mass ratio F in the range 0.0795 < F < 0.0805 2. BHP decreased continuously as F decreased from the value of F which yielded maximum BHP through the value

F = 0.0470

throughout the operational envelope: • 10 < Pinches Hg < [P inches Hg at WOT) - m - m

-

• 2000 ~ N , RPM < 2600 E • 0 ~ H, ft < 10,000 (standard atmosphere) 5-61 ce'

s! s!~

t--~---+---rl---+------1~---+-<><~--+---.r.~ ---t-----1----;

-E :e

t~ ~~ ~~ A~ -10 o -20 -10 -20 +10 o +10 Retard Advance Retard Advance Effect of spark timing on bmep for a number of L"S passenger-car engines (Barber, ref 12.41)

[FROM IAYLoR (13)]

1.10

J

1.00 0.98

I

........ 1-7·-

/ 0.95

/~11.5'-

c. 0.90 '" .§

VL-16.5'-

E ::s E I.

20.3' .~ 0.80 --- -- .-- I.

'0 24' .~ ~

~ 0.70 If

.", -f: ..

~ :IE VI 0.60 0.50 -30 -20 -10 o +10 +20 Retard Advance Degrees from maximum power Correlation for all apeed.a and loads.

FIC;UR£ 5./

EFFE.CTS OF IGNITION T/MJI .. /{, ON BRAKE MEAN EFFECnV£ PR£5SLJR£ .. " ...

230 [171.SS1

y

220 [IM.121 /i 1\ 210 11SS.661 /" ~~ 1\ 200 [149.21 / ~ ,

JA~

/

\

.~~ , 10 [134.281

\ / ~ /

70 [126.821 I V / q.~ / L I., [119.361 II: ...

/V V

~ /

150 [111.901 ~ V

VI .I~,,~/

140 [104.441 ~ / ,/ II: / I~ V 130 [M"} ~ 1/ V ...

/ /' 120 [89.521 ~ L/ ,/ I .. ~Y 110 [82.061 ~ , V

~

100 [74.61 '/ /' 90 [87.141 /' 80 (59.881 ./ 70 (52.221 ., [44.761 17 19 21 23 25 27 29 [57.581 [M.351 [71.131 (77.91 [84.881 [91.451 [98.221 MANIFOLD PRESSURE-lnHg (kP.I Bhp vs. intake manifold pressure vs. revolutions per minute.

(REF. 2.l})

FIGURE 5.2

lEA-LEVEL PERFORMANCE ALTITUOE PERFORMANCE fIA.I.-THROTTL.E HP '\ '\.

AT ZERO 'l"M ....... t-....

/ :) V1 ~ o Z2 V 'I V V o

.'"

V V V /

i " 'I" ~.'!

&"!L~/ C ~ 1\o..1I'S~~ " ~ '"

~~V/ 18 ,t'- ~~

o ; t\.

~ ~ 1"", &>fb-9. ~ :I..!

~.;~~~/ 17

o ", / ~~~q:;&.

N~ ~ ~ ~OO-li ~NN ."

V.

'"' o V Iii ~ O,,~ t'- .......

//'l!'1.~~ v: c: o r- _28~) r-. .......

~ V V / ,/ry.;f.~ V "j.J o 14 26 ~ ......

'" V v: ..

'-".)

" IS o i . .1' ...... ~ ./.V ./ -" 2S I 20 !'..

~ 'r-- '/ C/ ./ l/ / ~ o \I 21 p 2:-" MANIFOLD PRESSURE. INHG V ~ V V V / V .--

v: ~+Ig 18

-" o I

'/ / "

i-25 o

,/ I o 7 ~-$O 17 II II 20 21 Z2 2) 24 25 ZI 27 ZI Zt lIO MANifOLD PREIIURE-INHG O!NSIT'I' ALTITUDf-p!n Finding actual horsepower from sea-level and altitude charts.

(~£F. 24)

t="1c,uRE ·5.3

5-63

(REF. 23, FIGURE J )

IT I~ l1~tUME.ll 111111 J'HESE GflfEt.IlLrZO m/xro(E S1't.ENGTH

CHAI.IlC:reI<15 'nes APr! Y 10 11IE. FIVE. CoN)) I TlOHS

L. l!oTEl> IN FIGullE 5.5 .

5-64

(1?~F_ 27)

Ii o~· A.

'eakExhaUst ~GIS t:E ·50 i 0, Temperature ~~u.

~!..: ·100 cjC1 - w -150

If

-200

JI

~~

\

'- 'eak Cylinder Head -40

.- ~~

Tomperature 3'- ~- c!% -80

_=u

-120

Ii

·160 ~

JI

\. Best 'ower _ 0

f!

0% ...

l-f

lID c ~~~ ________________________ ~ .g Q.

I ~ 260

A. g 220

ell 180 I

'O~ _.

n :? I~-Y\~-

I

~ 60 t II ---=::: I ====

ID .04 .05 .06 .07 .08 .09 Fuel - Air Ratio Effect of fuel-air ratio on power, brake specific fuel consumption, cylinder head temperature and exhaust gas temperature at constant engine speed, manifold press- .

ure and spark timing.

THESE GEN£RALIZED MIXTURE RATIO C.Uf!VE.5 f!PPLY (35) TO: I. NlrrLl~RLLY A5P/~fl'rE:b ANb luRBOCJIIU(GE:D .$1 Plf.TON ENGJNES.

Z. ALL CDNsrllNT SE.H {Pm) NE. ' H To.t,..,os ) /'umid.;1j} Wt1"HtN p , THE NO~IlL OPE.!e.R77N~ ENVELOPE. OF THE E.NtaINE..

3. FIXED IGNJ1'/ON TiMING 'to 4-. BJ.lP IN THE 1&fNt;,E +D1- 100Z OF mAXIMUM CONTINLlOUS BHP.

5 SfAN])R~b ANI> NON- 57'"ANMRD AIMoSPHERIC c.ofll1)/TJONS.

F/(;UR.E. 5. 5' GE/tIEKRLlZED /r1IX-rU~E. RR110 Cu~vE.s.

5-65 i

I

~.'.' =- .... l. l. .l. .• I ... ' .. 1 ... t .•• 1. L. .. 1.. ._L. _L =- 1--.------;.-.

I .. 1 :.: _: ... !

I

I r1 BHP VARIATION WITH INLET MAP AND 'RPM :r::'::::::-: .- ..

!

~:'~:~::::~-:~:;:J:~~}i~:8~~~q~f~~~!~F~~;~'~~----~'"

I

I

!. ;"1

. f----- ---:-':".' ., i i.C".'

-. t '- • ... ,

-- --.------ .: ~i:: _~~~ :~ir ;.~~ ~: ~~ ~r~: ~.:: ~ ~. t

.. - .............. .

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CHAPTER 6

CHAPTER 6 THE AIRPLANE-ATMOSPHERE SYSTEM Table of Contents Page INTRODUCTION. . . . . . . . . . . . . . . . .. • . . . . . . • . . • . . . ... . . . . • . • . . . • • • . • • . .. 6-1 THE INTEGRATED SUBSYSTEM CRUISE PERFORMANCE MODEL •.•••••••••••.• 6-1 Fomulation. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. 6-1 Implementation ............................................. 6-2 The ISCPM.............................................. 6- 2 I· The peripheral Compu~ational Package ••...•...•.•.•••.•• 6-2 Computations Using the ISCPM .........••..........••.••••... 6-3 Engine Control .......... 0 • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •• 6-4 Increases in R* Relative to Current Practice ••..•.•.......•. 6-5 COMPARISON OF THE ISCPM WITH THE POH CRUISE PERFORMANCE MODEL ...•.......•••.•...•••••••••.•..•.•••••.••.•..•..•.•.•.•.•. 6-9 FIGURE 6.1 .•.................................. ·.................. 6 -11

CHAPTER 6

CHAPTER 6 TIlE AIRPLANE-ATMOSPHERE SYSTEM INTRODUCTION This chapter integrates the APA and NEA subsystem input- output models (developed in Chapters 3 through 5) to form a cruise performance model of the airplane-atmosphere system. The latter model is referred to as the Integrated Subsystem Cruise Performance Model (ISCPM).

First: the ISCPM is formulated. Second: the implementation of the ISCPM, and the use of the ISCPM for performance computations and optimizations is discussed. Third: engine control requirements of the ISCPM are discuss ed.. Fourth: the potential increases in R* offered by the ISCPM, relative to current General Aviation practice, are examined. Finally: the ISCPM is compared with the Pilot Operating Handbook Cruise Performance Hodel developed in Chapter 2.

THE INTEGRATED SUBSYSTEM CRUISE PERFOru.fANCE MODEL Fonnu1ation The APA subsystem input-output mode~ has been summarized in the block diagram of Figure 4.8. Likewise, the NEA subsystem input-output model has been summarized in the block diagram of Figure 5.30. These two block diagrams are combined in Figure 6.1.

The ISCPM is the set of relationships which detennines the outputs 6-1

S = { R*. Pm' F, lil }

out f of Fi gure 6.1 in terms of the inputs

Sin = {V ' V , W, h, P ' N , Tatmos' Hp}

w E AUX E of Figure 6.1. The ISCPM yields the point performance of the complete airplane in cruise, in the standard atmosphere or in any non-standard atmosphere; when the engine is operating at the mininrum possible BSFC commensurate with S ..

1n Implementation It is proposed that the ISCPM forms the core of an airborne microprocessor computational package. Computational software contained in this package, but extra to the ISCPM core, is referred to here as the Peripheral Computational Package (PCP).

The ISCPM: For a discussion of implementation of the ISCPM: the reader is referred to pages 4-22 and 5-47 for a discussion of the implemen- tation of the APA and NEA subsystem input-output models.

The Peripheral Computational Package: The function of the PCP is to perform computations other than those which may be performed directly by the ISCPM. The ISCPH The PCP might be can only perform point performance computations.

designed to perform tasks such as: 6-2 i I I r 1. Use the ISCPM to compute the airplane operating point

i

which maximizes R* with or without contraints 2. Use the ISCPM and an APA subsystem climb-descent input- output model, together with navigation data, to compute

I

trajectories which minimize trip time' or M with or f without constraints.

In performing these tasks, the PCP must provide the inputs {V , w

I

v W h P NTH } to the ISCPM.These inputs are

E' , , AUX' E' a tmos ' p

I

obtained by the PCP either from sensors, from direct pilot input, or as computational outputs of the PCP itself (see following sub- section). The outputs of the PCP may be used in the aircraft: to drive displays (including appropriate fuel management displays); or as command inputs to automatic control systems.

The "architecture" of the PCP is task-dependent and is not addressed here.

Computations Using the ISCPM The point performance computation which may be performed directly by the ISCPM is:

I. Computation of the set Sout = {R*, Pm' F, fuf} for any

given set Sin = {V ' V , W, h, P ' N , Tatmos' Hp}'

W AUX E E A PCP may be designed to facilitate other computations. Fol- lowing is a list of the computations which may be performed by the PCPjISCPM to maximize R* with or without constraints: II. Computation of the set {Pm' F, ro , N } yielding maximum f E R* and computation of this R*, for any given set {V , V ' W, h, P ' T t ,H}. This requires that E AUX w a mos p 6-3 computation I be performed for a number of values of N : E the value of NE yielding maximum R* is determined by interpolation; and computation I is then performed using this value of N • E III. Computation of the set {Pm' F, m , V ' N } yielding f E E maximum R* and computation of this R*, for any given set {V W h P T H} This requires that w' , , AUX' atmos' p' computation I be performed for a number of sets {V ' N }: E E the values of {V , N } yielding maximum R* are determined E E by interpolation; and computation I is then performed using these values of {V ' N }.

E E

IV. Computation of the set {Pm' F, m , V ' N , Hp} yielding

f E E maximum R* and computation of this R*, for any given set {W, h, P AUX' vertical profi Ie of atmosphericcondi tions (H , T , V)}. This requires that computation I be p atmos w performed for a number of sets {V ' N , Hp}: the values E E of {V ' N , Hp} yielding maximum R* are determined by E E interpolation; and computation I is then performed using these values of {V ' N , Hp}' E E For a given airplane and atmosphere, computation IV constitutes an unconstrained optimization of R*.

Engine Control Formulation of the airplane-atmosphere system cruise performance model in the manner shown in Figure 6.1 facilitates optimizing 6-4 tmaxirnizing) R* under various constraints. From the above discussion and Chapters 4 and 5, it is clear that such optimizations require that: 1. The pilot or the airborne microprocessor system be able to allocate values to {N , Pm' F} independently.

E 2. The engine ignition timing T be maintained at the MBT value T , the spark being retarded as necessary to control o detonation. MBT ignition timing T has been functionally o " described by Equation E.33.

These requirements preclude controlling the engine with a "single power lever" in which {N , Pm' F, T} are prescheduled. Such a E "single power lever" has been advocated by Chiri vella (16). The ISCPM requires that the engine be controlled with independent: 1. Throttle 2. Engine speed controller (propeller governor) 3. Ignition timing regulator (see p. 5-47) 4. Fuel-air mass ratio controller (see p. 5-47).

Items 3 and 4 probably should be feedback control systems.

Increases in R* Relative to Current Practice Implementation of the ISCPM in any General Aviation airplane offers significant increases in R* relative to R* achieved when operating that airplane in accordance with current GA practice.

The following discussion is based on Chapters 3 through 5.

1. Choice of {V , N} for actual" gross weight and altitude: E 6-5 Consider the LASA 60 performance in Figure 4.3: S* might c reasonably be expected to increase from 0.71 to 0.75 in typical fuel-conscious operations, and from 0.71 to 0.81 in extreme cases. Hence the ISCPM is estimated to offer S* increases of c Typical S* increase 6%

=

c Maximum S* increase 14%.

=

c An accurate knowledge of the gross weight then permits an estimate of the corresponding R* increases. We assume that the ISCPM has an accurate value of the gross weight; that the gross weight varies from the take-off gross weight

by an average of -100 lb in 3,000 lb = -3%; and that the

pilot currently uses the take-off gross weight for per- formance computations. The ISCPM therefore offers R* increases of

Typical R* increase = 9%

Maximum R* increase = 17%.

2. Choice of al ti tude to maximize effect of wind: In currently choosing cruise. altitude, the pilot is assumed to fail to take advantage of an extra five knots tailwind component available at some other altitude. The ISCPM is assumed to have the correct altitude profile of wind V. Assuming a typical true airspeed of 110 knots, w and a minimum true airspeed of 90 knots, the ISCPM offers ~ i R* increases of 6-6

Typical R* increase = 4.5%

Maximum R* increase = 5.5%.

3. Center of gravity position, auxiliary equipment power and propeller compressibility: It is assumed (conservatively) that the ISCPM offers no R* advantage due to an accurate knowledge of the airplane center of gravity position he, auxiliary equipment power PAUX' or propeller compressibility effects reflected in variations in the value of f from unity.

comp 4. Engine brake sped fic fuel consumption: From Figure 5.10, the maximum possible BSFC improvement when leaning from best power mixture with MBT ignition timing is about 17%. On the basis of Figures E.3-E.5 it is assumed that operation with given {BHP, N , H, T t } p amos E at best power mixture and with MBT ignition timing yields· about the same BSFC as achieved by operating at the same {BHP, N , Hp' T } at best power mixture with a fixed E atmos ignition timing L typical of the values of T used in current GA practice. GA pilots typically operate their engines at the best power mixture. Hence, the maximum possible BSFC improvement offered by the ISCPM over cur- rent1y achieved BSFC is about 17%. However, due to the fact that BHP decreases significantly during 1eanout at wide open throttle with the result that the engine cannot always be leaned to the fuel-fir mass ratio yielding 6-7 minimum BSFC. the maximum BSFC improvement offered. by the ISCPM is taken to be 10%. This yields a maximum. increase in R* of 11%.

It has not.been possible to compare the minimum BSFC achieved with the ISCPM with the minimum BSFC achieved when current fixed ignition timing engines are leaned in accordance with the manufacturer's recommendations.

It is assumed here that this comparison results in a typical decrease in BSFC of 5% when using the ISCPM: this yields a 5% increase in R*.

Hence the ISCPM is as.sumed to offer R* increases of

Minimum R* increase = 5%

f-Iaximum R* increase = 11%.

The total percentage increase in R* offered by the ISCPM relative to R* achieved in current practice is 6R*% which is obtained from the above as follows: Typical 6R *% = [( 1. 09 x 1. 045 x 1. OS) - IJ x 100% to [(1.09 x 1.045 x 1.11) - IJ x 100%

= 20% to 26%

Maximum llR*% = [(1.17 x 1. 055 x 1.11) - 1J x 100%

= 37%.

These figures are taken to apply to all GA airplanes powered by naturally aspirated SI piston engines. The savings are per- ceived as significant. Implementation of a cruis~ performance model similar to the ISCPM. in GA airplanes powered by 6-8 turbocharged 51 piston engines, is expected to result in values of ~R*% which substantially exceed these figures. (The turbo-

I

charged engine can operate at the fuel-air mass ratio offering minimum B5FC over a greater range of flight conditions than can the naturally aspirated engine.)

I

CO~WARI50N OF THE I5CPM WITH THE POH CRUISE PERFORMANCE MODEL

I

The Pilot Operating Handbook Cruise Performance Model (POHCPH) has been developed in Chapter 2. The advantages of the ISCPM over the POHCPM are: 1. The ISCPM permits cruise performance to be computed for all values of {W, h, H , atmospheric conditions}. TIle POHCPt.1 p must interpolate between cruise performance specified for certain values of {W, h, II , atmospheric conditions}: in some p cases, cruise performance data appropriate to only one value of one or more of {W, h, atmospheric conditions} are available in the POH.

2. The ISCPM permits true optimization of R*, with the engine operating at the minimum possible B5FC at all times. The POHCPM permits optimization of R* subject to the opera- tional recommendations {Pm' RPM, m } .. of the manufacturer, f and with fixed ignition timing.

} 3. The ISCPM commands F which is established automatically by the fuel-air mass ratio controller. This precludes the fuel-inefficient operation which resul ts from poorl" executed manual leaning. The POHCPM requires manual leaning.

6-9 Consequently, the ISCPM is considered superior to the POHCPM as a tool for maximizing R*.

The ISCPM and the POHCPM have one problem in cOllllllon: both utilize calibrated cruise performance data appropriate to the airplane. However, the performance of new airplanes of the same type and model is not precisely the same; and the performance of a given airplane varies throughout its life, reflecting variations in the condition of the airframe, propeller and engine. Therefore, the cruise performance predictions of the ISCPM and the POHCPM must be expected always to vary from the actual airplane per- formance. The author has not addressed this issue, but it is one which will require study if calibrated cruise performance models are to be introduced into General Aviation.

6-10 ~-~~~~---:----~------ __ o ...... -:-.- ..... ------.-;----~-

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CHAPTER 7

CHAPTER 7 CONCLUSIONS AND RECOMMENDATIONS Table of Contents

I

I

CONCLUSIONS ••••••••••••••••••••••••••••••••••••••••••• " ••••• 7-1 RECOMMENDATIONS •••••••••••••••••••••••••••••••••••••••••••• 7-4

CHAPTER 7

CHAPTER 7 CONCLUSIONS AND RECOMMENDATIONS CONCLUSIONS 1. Variations in Specific Range over the cruise envelopes of General Aviation eGA) airplanes are sufficiently large to warrant the development of a methodology for performing cruise fue1'-useoptimization computations.

2. Currently available Pilot Operating Handbook (POH) cruise performance data are not suitable for developing such a methodology because, in general, these data are appropriate to constrained airplane operation. POH cruise data typically apply to constrained values of a) Gross weight b) Center of gravity position c) Pressure altitude and atmospheric conditions d) Engine inlet manifold pressure e) Engine rotational speed f) Engine fuel-air mass ratio g) Engine ignition timing.

A methodology for cruise fuel-use optimization requires performance data which cover the operating range of these items (a-f), and which correspond to optimized engine ignition t:iming.

3. The abovementioned deficiencies of POH data are overcome by the new cruise performance model developed in Chapters 7-1 3 through 6. The POH data deficiencies are overcome by r this model as follows: a) Cruise performance data are presented in terms of novel Corrected .Quantities which incorporate variations in gross weight, atmospheric density ratio, and atmospheric ambient temperature and pressure in such a way as to generalize a specific airplane's performance for all values of gross weight, pressure altitude, atmospheric conditions, engine inlet manifold pressure and engine rotational speed.

b) The model incorporates a simple formulation of the effects of airplane longitudinal center of gravity position on cruise performance.

c) The model incorporates data for the useful range of engine fuel-air mass ratio.

d) The model assumes optimized engine ignition timing.

4. The new cruise performance model yi eldsthe outputs {specific range, inlet manifold pressure, fuel-air mass ratio, and fuel mass flow rate} corresponding to any given values of the inputs {geocentric true windspeed along track, equiv- alent airspeed, gross weight, longitudinal center of gravity position, auxiliary equipment power, engine rotational speed, pressure altitude, and atmospheric ambient temperature}, when the engine is operating at the minimum possible brake specific fuel consumption commensurate with the inputs.

7-2 This cruise performance· model appears sui table for air- borne microprocessor implementation.

5. The new model may be used to compute the airplane operating point which maximizes specific range, with or without con- straints. A methodology for performing these computations

I

has been presented. In combination with a climb/descent

I

model for the airframe-propeller-atmosphere subsystem, the new model might be used to compute trajectories which minimize trip time or trip total fuel consumption, with or without constraints. Implementation of the new model shall contribute to achieving the efficiency and safety objectives discussed in Chapter 1.

6. It is concluded that, for GA airplanes powered by naturally aspirated spark-ignition piston engines: implementation of the new cruise performance model developed herein will yield a) Typical increases in specific range of 20% to 26% b) Maximum increases in specific range of 37% above the values of specific range currently achieved by such airplanes. Implementation of a cruise performance model similar to this model, in GA airplanes powered by turbocharged spark-ignition piston engines, is expected to yield specific range increases (above the specific range values currently achieved by such airplanes) which sub- stantially exceed these figures.

7-3 RECOMMENDA TI ON5 1. The new cruise performance model developed in this work, for GA airplanes powered by naturally aspirated piston engines employing optimized ignition timing, should be f subjected to experimental verification.

2. In order to implement the new cruise performance model in GA airplanes, development of the following hardware items may usefully be pursued: a) A microprocessor system capable of performing specific range optimization computations based on the methodology presented in this work b) An ignition timing regulator c) A fuel-air mass ratio controller.

These hardware items may be incorporated into an airplane cruise computation/control system. This system should be evaluated in an engine test cell and in flight.

3. The cruise performance model developed hereil1 should be extended to GA airplanes powered by turbocharged 51 piston engines. Then, for this extended model, recommendation 2 should be pursued.

4. The question of the accuracy of the cruise performance model over the life of the airplane should be studied.

Such a study should consider the sensitivity of the airplane performance to degradation of its subsystems (airframe, propeller, engine); and the feasibility of collecting 7-4 flight data, using standardGA airplane instrumentation, I to recalibrate the model (if necessary) periodically throughout the life of the airplane.

5. The cruise performance models for naturally aspirated and turbocharged piston engine GA airplanes should be extended to include climb/descent. The resulting models should be used .to study the minimization of trip total fuel con- sumption.

7-5

APPENDIX A

APPENDIX A FUNDAMENTALS OF THE POINT ECONOHY FUNCTI ON Table of Contents Page INTRODUCTION •••.••••••••.•••••••••••••••••••••.••••••••••.•• ' A-I Groundspeed ........••.......••..•••................•... A-I Fuel Mass Flow Rate and Brake Horsepower ............... A-2 Auxil iary Equipment Power .............................. A-3 EQUIVALENT Q'JANTITIES ................................. ~ • • • •• A-4 EXPRESSIONS FOR THE POINT ECONOMY FUNCTION ••••• ; •••••••••••• A-S FIGURES A.I - A.2 •••••••••••••.•.•••••••••••••••••.••• · •••••• A-7

APPENDIX A

APPENDIX A FUNDAMENTALS OF THE POINT ECONOMY FUNCTION INTRODUCTION The airplane Point Economy Function, denoted by R*, is a scalar quantity with the units: ground distance travelled per unit mass of fuel burned. The units of R* used in this work are ground nautical t miles per Ibm.' R* is the integrand in the Breguet range formula (3).

In this study, only straight and level steady flight is con- sidered.

The fundamental expression for R* is: Groundspeed

R* =

Fuel mass flow rate ground nautical miles/Ibm = (A. 1) where

VG = Groundspeed, knots

fi = Total fuel mass flow rate to all engines,. lbm/hr

f t Groundspeed The navigation wind triangle is shown in Figure A.l. The achieved groundspeed is:

·r The exception is Chapter 2, where statute miles are used as the distance

uni 4 when that unit is used in POH data.

A-I where V Airplane true airspeed, knots

=

T V Geocentric true windspeed along track, knots

=

w > 0 V for tailwinds w V < 0 for headwinds w 6 Angle of drift, degrees.

=

In General Aviation, 6 is typically 10 degrees or less, in .which case the cosine of 6 is approximately unity. This study adopts the simpli- fication (A.2) Fuel ~-1ass Flow Rate and Brake HorseEower The total fuel mass flow rate to all engines, m is: f t m

= Em = E P c lbm/hr (A.3)

f f E t where E Number of engines, each driving one propeller

=

ro Fuel mass fl owra t e per engine, lbm/hr

=

f P Brake horsepower (BHP) per engine

=

E c Engine Brake Specific Fuel Consumption

=

(BSFC), lbm/BHP.hr.

When an engine is tested by the manufacturer, the published brake horsepower and the associated BSFC apply wi th the following typical Primary Equipment operating: A. Primary Equipment: • Magnetos A-2 • Mechanical fuel pump • Oil pump • Starter drive train (portion) • Tachometer.

When the engine is installed in an airplane, some Secondary Equipment is also driven by the engine shaft. This typically includes: B. Secondary Equipment: • Generator or alternator • Propeller governor pump • Vacuum pump • Hydraulic system pump • Air conditioning system (if any).

The motive power delivered by the hydraulic system to drive the under- carriage and perhaps flaps, is an intermittant power which is ignored here. The other items of secondary equipment draw power continuously.

The primary and secondary equipment are collectively referred to as Standard Equipment.

In this work, P (Equation A.3) is the brake horsepower that each E engine delivers after power to drive the Standard Equipment has been drawn from the engine shaft. 'Th'is is illustrated in Figure A.2. The torque Q (lb ft) associated with P is referred to as Brake Torque: E E Q is given by Equation E.3.

E Auxiliary Equipment Power It is sometimes desirable to determine the effect on R* of adding some extra item of mechanical, hydraulic or electrical equipment to the aircraft, which draws motive power from the engine.

A-3 Such items are referred to as Auxiliary Equipment, and the Auxiliary Equipment Power consumed per engine is denoted P horsepower. From t AUX Figure A. 2, (A.4) where P = shaft horsepower CSHP) delivered to the propeller.

s The shaft specific fuel consumption c' lbm/SHP.hr is defined by (A.S)

m = E P c'

f s

t Substitution-of this result in Equation A.3 yields CA. Sa) P and c' may be determined experimentally with the aid of a torque- s meter mounted between the engine shaft flange and the propeller hub.

lfuen c' is determined in this manner, and c defined equal to c', then PAUX is defined to be zero.

EQUIVALENT QUANTITIES The most common example of an Equivalent Quantity in airplane work is the Equivalent Airspeed (EAS) defined by (A.6)

~ I

A-4 !

j

I

I

where

V = Airplane equivalent airspeed, knots

E

I

V = Airplane true airspeed, knots

T

cr = Atmospheric air density ratio (Appendix B: standard or non-

I

standard atmosphere) .

-.

By analogy with the EAS, four other Equivalent Quantities are These are: this Nork.

used in Equivalent windspeed, knots

ra

V w Airframe equivalent power required, horsepower

P ra

R Equivalent auxiliary equipment power, horsepower

PAUX ro

Equivalent propeller shaft speed, RPH

N ro

where

P = Airframe power required (power-off), horsepower (Appendix C)

R N = Propeller shaft speed, RPM.

EXPRESSIONS FOR lliE POINT ECONOMY FUNCTION

f

Combining Equations A.I - A.4 yields V + Vw T CA.7) R*

=

m f t V + V (A.S) T' w

=

E P c E V + V (A.9) T w

=

c E(P + P AUX) S In straight and level steady flight, P is expressed (Appendix D) as

s

(D.29) A-S where n = propulsive efficiency.

p .

Equation A.9 may the-refore be written _ V + Vw T . R* (A.lO)

-[~: + E p~xJ c

In terms of the various Equivalent Quantities, the following expressions apply: V + V 10 E w R* = (A.ll)

= [1 + VwlOJ ___ V..;:.E ____ _

(A .12) VE (P R 10 + E T1p P AUX 10 ) The airframe power required (Appendix C) is P = 6080.2 DOFF V /(550 x 3600) horsepower T R horsepower (A.13) where DOFF = airframe drag force (power-off), lbf (Appendix C).

For those cases where PAUX is zero, we therefore have: L 1 ~ (A.I4 ) DOFF W c

= 325.65 [1 + V w ro J _L_ l ~ . (A. 15)

V DOFF W c E where W = airplane gross weight, lbf L = airplane lift force = W, lbf.

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j ::: -;11:- :;:: 11:1 .:j t I. 11'1 I':.; :t:: ~;:·I·:·;:;:::.r iiU. ~ .:. ;::: ;'1-:; rl' i: I( :-!:; ~:. t~~~'4i'l :;11y:i :i:i iii: ;::I~i;; ::~ :::~ ::::1::1'1 ~:II !!i: 11'li lill !II'I li!I:: I I i: rl" :~:: : .; :-:t :::1' :ill ;::: :':: ::p It'j II, \' . 1;1 ';::. :': .,'.' I:~~~ :,:: ,'Ii ':;: :'t I: I. ': :;~I .:: -6' .ll~""i;: ~w. lill 1, : : I: .;:: ~::;I::~: ;:~: :: i J I 'I:: I,ll 'I; l' i II11 i: : III: I,:: ::'; : ,: :!;: ~li ql: 11 1 l : ;::: :iq ::.: HI'I ·I I t Iii' l d::III: '::'1':: p- :'1' :;:, ;1:: jill 1111: 1IIIUlllI: ~'\j : .... \ ... ill" ;m' I::: ::1: In: :1:: :::. ill:.:;::: .'::1.: '. : il:: *,'d: ,hi Ill' H 1:: :1 : In: ::., :::~ :'::::]1: :.:: F 1 ;:: :J!, ;::: IIII 'I 1:1 I '::: ';:. ::, :.' :. ::;; :i:: 1,1: qli ,::l~t >' I· ,.:;. i'v 1 '; ;!i I:i'!l j !,': :. : :;:: :!:;I::-' ;::: ::;: '111 ;,!: 1111:1'1 'I! I;!' ;:1 ! :; ~,d :,,: ; :: ;.;: :!:! :li' I t.:...: "L!",:"I ., ,. II 1,,; .t-. .... \... . ...... ,' Iij"H-+HIEi.!. .... , .. I .. " ,,,,I!ll!.I!i!: .,1. ............ , .... >11 LL!J "11'1. , I. ,w.lj .. , , .. '~'I:" ...... , .•• r;:-- ::-::r~~~: ::Ji !I·:lll.: 'll! ':1: ~:: ~ ,. ~.".".' .'~"'!".' :.~r: ~rr~~~ 11;' ~'·:·l:·t: .. :'" .... ii' ; 7!!:w: :'Hrrr ~n: i~:' :~;:I!"'" :';'I!";-:' O:i:I,' . : ;, II', I::: :::: "'~:-T!:" ~:~:~.~: ....... ~:;-:- .:;i :;:~ .: ::, :::i j:" l:.:!!:i 1,.1 ';: :1': ,.' , !:t;:~....,.-:-;".: 11\ ',. • '. ,,';. ;!! Ii:: ": ·i.· 1;'1: I' .. : I ., :: :.:: :1:: I::: ,;. :::: '1' ,;: '::. :.: :;: :::: ••• ,." ........ , .... 'I~' .f" ".' .. ,. " •. I I . I:~ ,., .. 01 •••• II, " " I ... ,,,,. I"~ ••• , •• , •• , II.,. ,.,. , '\" "~, "" ~'" ••••• ill , •••••• ". ,I •• · ...... f'" .... "1' ! .' .:;. '.':::: i! : iii: !Iii :;ji ::. :'; ~'.' : iii:: ;::.!" '.: I" :;!' .!:! 1::; ::::1::: ·:::1: . Ii': \:.': :;:: :::: .:: :::: : ':i:;: . I .::; ::l: '" ........ _H 1l-~:8 •. J ........... ,. .. .. I ........ , ............. ,. .. . .!.I ...... l-4~. ··-t'_· .. _ ...... ,... , .............. , ~ ................... , ....... --_ ....... -'-:-:1:: ..

. :. : < i::. Hi: :;:; ;::: ! 'j':::' . I I!:: :': ::: ;. I;: ! i:. !:ii:: :i:.:~:I> I :::1' I: i i : .. :i ·::, L:. :::. ','1:':' .: .: i·::· l :.:.' .11.'.: .... :: :'::::: I::::!!:: : .. . .. 1.. I I : I... .' :: .:!.; ! I·;!:: I.:::-! : ' ::' . i:' ::::!::::-.:::. : .,:, . ! ::!

.--:~; ...... ~~ ...... - :....... . I. ................... ;... "'j,' ~j;i4'E .. ··I·A· ......... 1_ .. .-.. ...... "'" .... \. .................. I: .. · .... :.. .... . ... ,- .. .

.

II: ... ": 1> ;t::: I!: .:::;::: :L1/t' M· .. ~ I: i ! 1 . ·1···:·' : : :1; "1'"

.......... ,.,., . i I I., ..... ,I ... '1' rlu, ... ., I ...... ·; .. 1 .... , .• , ',"" . . ~.. :. ! . ! ' ' ~ . ; , : .' .:! , : . ; . ," i : ' :. . _.:.

.l I(l x to TO tHI: CENTIMETHl

-

46 1513 K'~frl't A,rr';'.lJ?(O U~I'I''''''''' > I I l I ,.

, .i . I

I

I . i

APPENDIX B

I i !

!

APPENDIX B THE STANDARD AND NON-STANDARD ATMOSPHERE MODELS I

I ~

Table of Contents

I

I

Page TIlE STANDARD ATMOSPHERE MODEL .............................. B-1 Nomenclature .......•...•.....•••••..••.•.......•...... B-1 Sea Level Conditions .•.......•..••••... , .....•........• B-1 Altitude Condit'ions ..........•.........•..•.......••.. B-2 TIlE NON-STANDARD ATMOSPHERE MODEL ....•.•..•..............•. B-3 Nomenc'l a ture. . . . . . . . • . • . . . . . . . . . . . • . • . . . . . • . . . . . . . . • .. B-3 Density and Density Ratio ......••.•.•..••...•.......•. B-4 i i

I

I i APPENDIX B THE STANDARD AND NON-STANDARD ATMOSPHERE MODELS

I '

THE STANDARD ATMOSPHERE MODEL The standard atmosphere model used in this work yields the charac- teristics of the U.S. Standard Atmosphere. 1962 in the troposphere

I'

(18). Zero humidity is assumed throughout the Standard Atmosphere in the present work.

I

Nomenclature The notation used for this atmospheric model is as follows: absolute pressure lbf/ft Sea level ambient Po Kelvin level ambient temperature degrees Sea TO Sea level density slugs/ft Po ft/sec Sea level gravitational acceleration go ft.lbf/lbm.

Gas constant for dry air R a degree Kelvin sea level II Geometric altitude above (= density altitude) ft at altitude H lbf/ft P Ambient absolute pressure atmos degrees Kelvin T =T Ambient temperature at altitude H atmos s shigs/f't P Density at altitude H Pressure ratio P /P at O altitude H atmos e Temperature ratio Ts/TO at altitude H a Density ratio p/PO at altitude H Sea Level Conditions lbf/ft

Po = 2116.22

degrees Kelvin

TO = 288.lS

B-1 0.076474/g = slugs/ft

Po

T = 32.1741 ft/sec . go The perfect gas law states (B .1) Patmos = pgoRaTs Application of this law to the conditions at sea level yields (B.2) Ra =96.03474 ft.lbf/lbm.degree Kelvin Altitude Conditions The temperature lapse rate is virtually linear with geometric altitude, such that e = 1 - L H (B .3)

The value of L yielding the correct value of 9 (18) at H = 10,000

ft is L = 6.87239 x 10- (B.4) The value of L in Equation B.4 is used here, in· conjunction with Equation B.3, to compute 9 at altitude H.

The pressure ratio 0 is given (7) by l/LToRa (B.5)

o = 9

Substituting Equations B.2 and B.4 in Equation B.5 yields o = 95.2583 However, using the value of 9 (computed by Equations B.3 and B.4) at H = 10 ,000 ft, in conjunction with the value of 0 (18) at H= 10,000 ft, yields:

o = 95.25581

(B.6) B-2 Equation B.6 is used here, in conjunction with Equations B.3 B.4, to compute ° at altitude H.

and H,

6 and ° at altitude

Having computed (B.7) T T 6

=

0 s (B.8) P

= Poo

atmos The density P at altitude H is then computed using Equation B.1.

The density ratio a at altitude H is computed from (B.9) mE NON -ST A.\lDARD ATMOS PHERE MODEL Zero humidity is assumed throughout every non-standard atmosphere in this work.

I Nomenclature ft Pressure altitude H P Ambient absolute pressure at P atmos lbf/ft pressure altitude H p Ambient temperature at pressure T atmos degrees Kelvin al titude H p Slugs/ft Density at pressure altitude H P p Density ratio p/PO at pressure altitude Hp' where Po is the sea level density (slugs/ft ) in the Standard Atmosphere.

B-3 The pressure al ti tude H (ft) at any point {P t· , T t }, in any p a mos amos non-standard atmosphere, is defined to be equal to the altitude H (ft) which corresponds to P in the Standard Atmosphere. An atmos atmosphere is Non-Standard when T at H is not equal to the atmos p ambient temperature T in the Standard Atmosphere at H = H .

s P Density and Density Ratio The density P at {H ' Patmos' Tatmos} is computed using p the perfect gas law: P atmos 3

p = ---::,"'-'-::::-:...-- s lugs/ft (B.lO)

R T g o a atmos The density ratio a at {Hp' Patmos' Tatmos} is then p (B.11)

o =

where Po is the sea level density (slugs/ft ) in the Standard

Atmosphere.

B-4

APPENDIX C

APPENDIX C THE AIRFRAME PERFORMANCE MODEL I ) Table of Contents I NTRODUCTI ON. . • . • . • • • • • • • • • • • • • • • • . • . • • • • . • • . • . • • • . . • • . • • •• C-l AIRFRAME D~G AND POWER REqUIRED ..•.••••••.••.•.••..••••.•• C-l THE AIRFRAME DRAG POLAR ••.••.••.••.•••••••••••..••••••••••• C-3 Power-Off Flight .••••••••..••••••••••••••••••••••••••• C-4 Power-On Flight •.••.•••.••.•••••••••...•••••.•••••••• '. C-lS FI GURES C. 1 - C. 3. . . • • . . • • • • • . . . • • • • . • • • • • • • • . • • • • • • • • • • . .• C-17 i j

I

I i APPENDIX C THE AIRFRAME PERFORMANCE MODEL INTRODUCTION

I

I The airframe contributes to the value of the Point Economy Function, R* in that it determines the quantity of thrust work required to propel

I '

the airplane per unit of ground distance travelled. Only straight and level steady flight is here considered. The items of modelling interest are the airframe aerodynamic drag and the airframe power required.

I

In this appendix, the well known equations for airframe drag and power required are presented. In addition, an expression for the airframe drag coefficient, in both power-off and power-on flight, is developed. The latter expression quantifies the influence of airframe geometry, aerodynamic characteristics, center of gravity position and power-effects on the airframe drag coefficient.

AIRFRAME.DRAG AND POWER REQUIRED The power-off airframe drag is given by 1 2 (C .1) .

DOFF = CD 2 P V S

1 2 (C.2)

= CD 2 Po Ve S

where

= power-off airframe drag, 1bf

= power-off drag coefficient

= atmospheric air density, Slugs/ft

C-1

Po = standard sea level value of p, slugs/ft (Appendix B)

V = true airspeed, ft/sec

V = equivalent airspeed = V~, ft/sec e 0 atmospheric density ratio = = p/PO ., ft- airframe reference area S = = wing area, The airframe power required (power-off) P is given by R P = DOFF V/5S0 R (C.3) horsepower

= DOFF V /550 .fO

The airframe equivalent power required, as defined in Appendix A, is therefore

P 10

= DOFF V /550

R (C.4 ) horsepower 1 3

=

CD 200 Ve 5/550 Equations C.l - C.4 describe the power-off flight condition. The equations for power-on drag DON' power required PR and equivalent ON

power required P 10 are identical to Equations C.l - C.4 except

R ON that the power-on drag coefficient C replaces CD' That is, DON 1 2 (C.5)

= CD 2 P V S

DON ON V S (C.6) C = "2 Po e DON P = DON V/550 RON horsepower (C.7) =

DON V /550 10

I

C-2 !

i

I

(C .8) horsepower

I

~ The drag coefficients CD and CD may, in general, be expressed ON as cubic polynomials in terms of the lift coefficient C : L (C.9) C D (C.lO) + k ' C + k' C + k' C L 2 L 3 L l The lift coefficient C is defined by, L I 2

L = W = C "2 P V S

L (C.11 ) I 2 = C "2 Po Ve S L where

L = airplane lift force, Ibf

W = airplane gross weight, lbf.

The quantities CD ' CD ' k., k! (i = 1,2,3) are discussed below.

o 0 Plots of CD versus C and CD versus C , as described by Equations L L ON C.9 and C.IO, are referred to as the airframe power-off drag polar and the airframe power-on drag polar respectively.

" THE AIRFRAME DRAG POLAR The following discussion develops an expression for the airframe C-3 power-off drag polar in terms of the airframe geometry, aerodynamic characteristics and center of gravity (c.g.) position. By suitable adjustment of the values of certain parameters in that expression, the ~.

airframe power-on drag polar is obtained.

A specified airframe geometry is assumed, with the exception of the tailplane ·geometry. In particular, this discussion pertains to a specified geometry of the undercarriage, high lift devices, cowl flaps and other variable geometry devices. The airplane is assumed to be trimmed by varying the tailplane geometry.

TIle airplane is assumed to be laterally symmetric about its longitudinal centerline, with respect to geometry and mass distribution.

Therefore only longitudinal variations in c. g. posi tion are considered.

The airplane geometry is shown in Figure C.l.

Power-Off Flight The following definitions apply (36): ft b wing span,

=

w tailplane span < b, ft b

=

t - w chord, ft c local wing

=

c = mean aerodynamic chord of the wing, ft. c is defined by

b /2 _ 2 w c dy feet

c = -

j

S 0 complete C lift coefficient of airplane

=

L C lift coefficient of airplane less tailplane

=

L w C lift coefficient of tailplane

=

L t G-4

C = pitching moment coefficient of complete

m airplane. about the airplane c.g.

= pitching moment coefficient of the airplane less tailplane, about the aerodynamic center C of the airplane less tailplane

he = distance of the airplane center of gravity aft

of the leading edge of the mean aerodyTlamic chord of the wing, ft

h c = distance of the aerodynamic center C of the

o airplane less tailplane aft of the leading edge of the mean aerodynamic chord of the wing, ft

-t = tail arm = distance of the tailplane aerodynamic

center aft of the aerodynamic center C of the airplane less tailplane, ft L = lift of complete airplane = gross weight W, lbf

L = lift of airplane less tailplane, lbf_

w

L = lift of tailplane, lbf

t

M = pitching moment of complete airplane about the

airplane c.g., ft lbf

M = pitching moment of aerodynamic forces for the

c airplane less tailplane about the aerodynamic center C of the airplane less tailplane, ft lbf · f 2

S = wlng area, t

--~

St = tailplane area, ft

V = tail volume ratio = St-t/Se

C-s

n = tailplane efficiency = q/q = t P V~/tP V = (dynamic

t pressure at tailplane)/(freestream dynamic pressure).

We have (36, 37):

L = C t P V S

L C !.P V S L

=

L w 2 w 1 2 L C PV

=

St I n t t L t

H C }p V S c

=

m

Mc = C }p V S c

m 0- (C.12)

C = C + C (h-h ) - C :t If - (h-h ] n

m J t

o mo Lw Lt Also, L + L L

=

w t St C C (C.13)

= + C S n

L L L t w t Therefore from Equations C.12 and C.13, (C .14)

C = C + C (h-h ) - C V n

L m mo 0 L t t

In trimmed straight and level steady flight C = 0, so that from

m Equation C .14, (C.lS) Also from Equation C.13, C-6 I

I

i

!

i (C .16)

I

The following definitions Consider the power-off airplane drag.

I '

apply: of wing A aspect ratio

=

w ratio of tailplane aspect

=

At airplane power-off drag coefficient

=

CD drag coefficient of airplane power-off parasite

=

CD pw less tailplane lift-independent part of CD

=

CD pw pmw coefficient of tailplane power-off parasite drag C

=

D pt lift-independent part of CD

=

CD pt pmt CD. = airplane power-off induced drag cOefficient ].

DOFF = airplane power-off drag, lbf

= power-off parasite drag of airplane less tailplane, lbf D pw power-off parasite drag of tailplane, including fuselage/

Dpt =

tailplane interference drag, lbf D. = airplane power-off induced drag, lbf.

].

We have, 1 2

= CD 2"P V S

C-7 .!.. P V S = Co 2 .

pw pw 1 V2 -p = St n Co Opt t 2 pt .!.. p V S D.

=

CO.

).

+ 0 + O.

= 0

DOFF pw pt St + C (C.17) + = Co Co S n CO.

t Opt PW The parasite drag coefficients Co may be written (9, 3S): and Co pt PW ~ )2 + K (C (C.lS)

=

Co CD L w w pw pmw w ~ )2 + (C .19) K C

=

e Co Co t L t pmt pt t where are constants. The quantities ~w and ~t are included to account for non-symmetric wing and tailplane sections respectively. In order to trim the airplane in level flight, the lift of the tailplane is established at the required valu~(Equation C.15) by deflecting the elevator and/or trim tab, or by changing the incidence of the (all- moving) tailplane. For the small tailplane geometry changes so involved, the quantities Co and K are assumed to retain constant t pmt values.

C-S i i

i

I

I Laitone (20) demonstrates the use of the equation

I

for the induced drag of a biplane, as it applies to computations of the induced drag of a monoplane wing and tailplane. In the case of a monoplane with an ellipticallY loaded wing and tailplane in potential flow, the biplane induced drag equation (9, 20) yields (C.20) where 0wt = a coefficient dependent upon the span ratio b/b w and the gap g (the vertical distance between the two wings), but independent of the stagger distance (the horizontal distance between the two wings) with potential flow.

By invoking ~funk's equivalence theorem for stagger (9), Laitone (20) shows that the mutual interference between the lying and tailplane (the middle term of Equation C.20) can be computed with the tailplane at infinity downstream of the wing (~ ~ 00), with a gap g.

equal-to that of the actual airplane: In addition, Laitone gives the following expression for a wt (C.2l) t This procedure is adopted here. The mutual interference is computed for the tailplane placed at infinity downstream of its actual position on the airplane. with the wing wake assumed to be a flat vortex sheet extending to infinity downstream of the aerodynamic center C of the airplane less tailplane. The mutual interference is then adjusted for rollup of the flat vortex sheet into a horseshoe vortex (9).

C-9 This equation yields the value of 0wt appropriate to a tailplane operating in conjunction with an elliptically loaded wing. The wing wake is assumed to extend back to infinity, from the elliptically loaded wing, as a flat vortex sheet. Laitone (20) states that the value of 0wt given by Equation C.2l is accurate within 7% for btlb ::: 0.6, within 2% for bt/bw = 0.3, and within 1% for b Ib < 0.25 .

. w t w- Referring to Figuie C.2, we may write

g = 1 [g + £, tan (a -i ) ] cos (a -i )! (C.22)

o w w w w Ci = angle of attack of the zero-lift line of the airplane where w less tail plane to the freestream velocity vector, radians go = vertical distance of tailplane below wing when Ci = i , w w ft.

Note that g is always positive; go is positive (negative) when the tailplane lies below (above) the wing. The angle of attack a of the zero-lift line of an untwisted wing to the freestream velocity vector is given by (9): radians (C.23) C-10 i !

n

I

I

!

where . -1

a = wing section lift curve slope, radian

o w 1 = correction factor for wing spanwise loading.

w

I '

Figure C.3 (9) shows typical values of Tw = T

for untwisted wings of 'rectangular planform.

I

The angle a in Equation C.22 is here computed from Equation C.23 w with Cl = a.

w The biplane Equation C.20 applies to two wings operating in an ~ 1 2

airstream with a dynamic pressure q = 2"P V When the wing operates

in an airstream with dynamic pressure q, and the tailplane operates in one with dynamic pressure Equation C.20 becomes ntq, then L L 1 Lw 20 w t wt

L2 1

D. = (C.24)

r 2

1 2 2 + + 1.

2"P V iT b bwb lilt

b~nt

w t ~ ....

In coefficient form, Equation C.24 is, 2 2

C 0 b 2C C In C n

St St t wt w L L L t L t w w t -- + + -- (C.25)

=

CD.

iTA iTA b S iTAt S t 1 w W When the wing and tailplane are not elliptically loaded, and al)owing the wing wake to roll up into a horseshoe vortex (9), Equation C.2S becomes: ,(' + (C.26) C-ll where

Ow' 0t = induced drag correction factors for

spanwise loading of the wing and tailplane respectively. Figure C.3 (9) shows typical

values of Ow = ° or 0t = ° for untwisted wings

of rectangular planform.

Also

e = E'/E = 2/(E/E ) (C.27)

t 0 where E = wing wake downwash angle at downstream infinity (measured on the wing longitudinal centerline), due to a wing with lift coefficient CLand any load w distribution, and having a horseshoe vortex wake, radians E' = 2E = wing wake downwash angle at downstream infinity o (measured on the wing longitudinal centerline), due to an elliptically loaded wing with lift coefficient C and a flat vortex-sheet wake, radians L w

E = C /nA = downwash angle at the center of pressure

L o w w of an elliptically loaded wing with lift coefficient C ' radians.

L w Values of E/E , for an elliptically loaded wing and for a rectangular o wing with various aspect ratios, are given by Glauert (9, pg. 168).

The quantity 0wt in Equations C.21 and C.26 is assumed here to be invariant with the lift distribution of the wing,' ar.d to be the same for a horseshoe vortex wake as it is for a flat vortex sheet wake.

C-12 -----.------------------------------------------------------------------- In the foregoing discussion, the wing downwash has received very simple treatment. However the calculation of wing downwash is, in general, very complex; this matter is discussed in detail by Spreiter and Sacks (39).

Substitution of Equations C.18, C.19 and C.26 into Equation C.17 yields: (C.28)

rn

t S where Substituting Equations C.lS and C.16 into Equation C.28 then yields: 1+0 ] S t _t.:;..,..._

(£ C )2 [K + l+OwJ+

C [K

m t 9., m w nA + nAt Sv n o o w t 2 St n t + ~ K -- - t t S (this equation is continued on the next page) C-13 \.

- - 2 [1 - ~ (h-h )J ~ K NOW W 1+0 ] S + (h-h ) 2 K + nA t _~ o t [ t sv n t (C.29) Equation C.29 may be expressed as (Co 30) The coefficients KO' .Kl and K2 are dependent upon C inasmuch as L + O'wtb/bt is dependent on C (see Equations C.21, Co22,C.23 and C.16)'.

L t Also, CD and CD (Equations C.18 and C.19) might be w,ritten more pw pt accurately as cubic polynomial s in C and C respectively.

L L ·w t C-14 Consequently the curve given by EquationC.30 maybe represented by a least squares cubic fit of the form

I

I

CD = CD + klC + k2C~ + k3C~ (C.9)

L \; o as previously written. Equation C.9 describes the airframe power-off drag polar.

I

Power-On Flight In powered flight, the following parameters may have values + different from those pertaining to power-off flight at the same C : L 2. C m o 3. a with corresponding values of oW' TW and e o t w 4.

i 5.

w Substitution of these power-on values in Equation C.29 gives the power- on drag polar, C (C.3l) DON A least squares cubic fit of Equation C.3l then yields the coefficients of Equation C.lO. The relationship between CD and C may be deter- DON mined from a comparison of Equations C.30 and C.3l or Equations C.9 and C.lO.

tWe assume that the thrust vector passes horizontally through the air- plane c.g. so that the foregoing lift and pitching moment equations are unaffected by the application of power. (This is not always the case.)

C-15 Of particular interest in the present study is the influence of c.g. position on the power-on drag polar. As shown by the foregoing analysis, variations in longitudinal c.g. position necessitate changes in the tailplane and wing lift forces (Equations C.lS and C.16) so as to trim the airplane. These lift variations result in vari- ations in both lift-dependent parasite drag and induced drag (Equations C.18, C.19 and C.26). These drag variations in turn cause

changes in the coefficients KO' 'Ki and Ki in Equation C.3l. Such

changes in drag, due to longitudinal movement of the c.g., are re- ferred to as "trim drag." Associated changes in the airplane power- on drag polar result in changes in the airplane power-on lift/drag ratio,' which affects the value of R*.

C-16 .

7AIL?LA/'I£ he

w

I

(REFC~E.NCE 36, p. 50)

AIRPLANE. GE.OMeTRY

C.I

F/~UR£ 'f'AiH ~ •. N2~D_- I·

-E~= ..... ::..'1AILPI.A/'I£

F/{;UR£ C.2

C-17 Recl:&ngu.I.,. Ael"'Ofoil$ O·S~----·----~~~-----r----~ f 0·1 ~----~------~-----+----~ 1·0 0'5 1'5 2·0 Aja.

o Fig. 85.

-,

A OF

ASPECT "RATIO 'WING

a =

WING S.E.CTlON LIFT CUfVf SLOPE.

D ( 2. -!)IMfN~JONRL FLDW) , "'fETe. ~/r.DIAN.

't = (O~ECTION Fltc101C FoR 'WIN~ SrANWIS£ LoA1>JtJG EFFEC.-rS, ON

WING fitNt:.U OF AT/ACt:..

b - CoT<f?.ECTION FAeroe. FoE:. WIlliG SPAll/WIsE LOAblNG £FFECTS. ON WINtJ, IN1::JLJC£1> J:J/?AG. COEFFICIEN'I.

(REF£R£Nc£ 9) p. 14-7 )

AE'i.DDYNIfM/C ~HAf!AC1'EJ:.lsr/(;~ of UN1'W/~'E1J

FIGURE C.3

'WINGS 'Wt,H REC.TANGULA£, "PLIINFoleM.

C-1S !

!

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i

I APPENDIX D THE PROPELLER PERFORMANCE MODEL

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Table of Contents

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INTRODUCTION. . . . . . . • . . . . • . . . • . . . . . . . . • . • . • . . . . . . • . . . . . . • . . . . . .. D-l mE FREE PROPELLER ....•.........••.•.••.••••.•••...•••.•.•..•.. D-2 Perfonnance Characteristics............................... D-2

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Perfonnance Characteristics: Incompressible Aerodynamics. . . . . . . . . • • . • . . . • . . • • • .• . • . • . . . . . • • • . • . . • .. D-6

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Performance Characteristics: Compressible Aerodynamics. . • . • . • • . . • . • • • • • • • • • . . • • • . • . . . . . . . • . • • . . .• D- 7 mE INSTALLED PROPELLER........................................ D-l2 Computation of Installed Propeller Performance from Free Propeller Perfonnance ...•...••••..••••..•.•....•.• D-14 Influence of the Slipstream on the Body •..... · .......••.•.• D-19 Propulsive Efficiency ................••.•...........•.••.• D-23 The Speed-Thrust Coefficient .••..•••.••••.••...•••••• D-25 Propeller Shaft Torque ..••..........•.....••.......••..•.• D-28 Propeller Blade Angle ...••.•..•...•.•••...•............••• D-28 PERFORMANCE MODEL ............•.......•.•• ~ • . • . • . . . • . • . • . . . • . . •• D- 29 CHARACTERISTICS OF 'mE ~1cCAULEY C33/90M-4 CONSTA.~T SPEED FREE PROPELLER.............................................. D- 30 Geometry. . . . . • . • • . • . . • . • • • . • . . • • • . • • . . • . . • . . . . • . • • • . . • .. . .• D- 30 Perfonnance: Incompressible Aerodynamics ...••.....•....•• D-30 TABLES D.l-D. 2.· •.........•••.••.•••••.•.•.•• , ..•••••.••..•••... D-33 FIGURES D.l-D.9 ........................•.....•.•••.........•... D-37

APPENDIX D

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I APPENDIX D

I

THE PROPELLER PERFORMANCE MODEL INTRODUCTION

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I This Appendix presents a method for modelling the per- f J formance of a propeller operating in the presence of an airframe (installed propeller), and the propulsive efficiency of the

I

propeller-airframe combination; in terms of the performance of

I

the propeller operating in isolation from any body (free pro- peller).. Compressible flow effects on performance are modelled as a correction factor ~lich adjusts efficiency and torque computed under the assumption of incompressible flow.

Specification of the performance of a propeller-body com- bination in terms of the free propeller performance facilitates computation of the former performance when only free propeller per- formance data are available.

The discussion is appropriate to fixed pitch propellers (those made in one piece, and ground-adjustable propellers) and to variable pitch propellers (controllable pitch and constant speed propellers). These various propeller types are described by Bent and McKinley (24).

The geometry and performance of the McCauley C33j9Q}.1-4 con- stant speed free propeller are presented and discussed at the conclusion of this Appendix.

D-1 THE FREE PROPELLER Performance Characteristics Dimensional analysis shows that the thrust developed by any free propeller, having a specific blade shape and number of blades, may be expressed by the functional relation 2 4 '

T = (pn d ) f [ J, B, ~, H] (0.1)

T Similarly, the shaft torque required to turn the propeller may be expressed by the functional relation (0.2)

where T = Thrust of the free propeller, lb

Q = Shaft torque of the free propeller, lb ft

p = Density of the air, slugs/ft n = Propeller rotation rate, revolutions/second

d = Propeller diameter, ft

J = Advance ratio = V/nd

B = Representative blade angle, degrees

~ = Reynolds number = vN£N/v

M = Representative Mach number

v = Free stream airspeed parallel to propeller shaft

axis, ft/sec v = Kinematic viscosity of air, ft /sec.

The performance of all geometrically similar propellers is charac- terized by the same function fT and the same function fQ' In this work unless otherwise stated, the blade angle B is the c.ngle between the plane of rotation of the propeller and the D-2 ------ -------------------------------------------------------------------------- i !

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!

i

flat face of the blade, at a radius of O.7SR (where R = d/2 is

the propeller tip radius, ft).

I The definition of the Reynolds number requires the use of a

I~

representative speed v (ft/sec) and length £N (ft). Since the N airflow over the elements of a propeller blade varies greatly

I

from the hub to the tip, a number of choices for these quantities

I

is available. Glauert (1) defines

v = nnd, ft/sec

N £N = d/2, ft as useful quantities for evaluating ~.

A useful representative Mach number is the helical tip Mach number MT given by (D.3)

where V = Helical tip speed. ft/sec

T1P a = Speed of sound in air, ft/sec.

The dimensional quanti ties on both sides of Equations D.l and D.2 are combined to give the non-dimensional thrust and torque coefficients: T (D.4) C = T pn d g (D .5) C = Q 2 5 pn d D-3 Using Equations D.4and D.S and substituting M.r for H, the functional relations D.l and D.2 become (0.6)

C = fT[J, e, ~, MTI

T (0.7)

C = fQ[J, e, ~, MTI

Q General aviation airplane propellers operate at values of the Reynolds number ~ (as defined above) of approximately 10 .

For values ·of ~ < 10 , the thrust and torque coefficients can show a strong dependence on~. However, according to Glauert (1), for ~ > 10 , ·"important changes of the propeller character- istics . . . are improbable. . Consequently, full scale propeller " characteristics, such as those used in the present work, are treated as being independent of Reynolds number.

As a result of their performance-invariance with Reynolds number, we have, for full-scale airplane propellers: (0.8)

C = fT[J, e, ~~1

T (0.9)

C = fQ[J, e, M.r1

Q The power P eft lb/sec) needed to drive the propeller is the product of the torque and the shaft speed; and a non-dimensional power coefficient C is defined by p (0.10)

C =

p The efficiency of the propeller is defined by 1V CTJ (0.11) 11 = P = C p 0-4

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For some purposes it is convenient to use propeller character- istics other than C , C ' C and n. It is sometimes convenient p T Q to use the forward speed V instead of nd in defining non-dimensional

I

I coefficients. By multiplying both C and C by 1/J2 we obtain T Q C T T = -= (0.12) T c 2 2 J2 pV d r-

g

~= (0.13) and Q = c 2 3 J2 pV d In the design of propellers, use is often made of the non- dimensional Speed-Power coefficient C defined by s

C = -L = V [..k.-j5 (0.14)

s 1/5 2 C Pn p Since C does not contain the propeller diameter as a factor, it s is useful for detennining the optimum diameter propeller of any family of geometrically similar propellers, for specific operating conditions of the airplane and the engine (4, 7, 8, 10).

Polar diagrams, consisting of plots of C /J2 versus C /J2 p T are used in various forms for airplane performance analysis (4), including range computation. Kerber (2) makes use of a plot of T versus J for estimating propeller performance by the Lesley- c Reid Method. A scaled plot of T versus J2 is presented by Von c Mises (4) who discusses its usefulness in determining the optimum diameter propeller of any family, given values of the thrust, altitude, airspeed and engine revolutions.

In this work, use is made of the Speed-Thrust coefficient C defined by R 0-5 J 1 = -- = (D .15) C R If

IS c

piotted against J .

Performance Characteristics: Incompressible Aerodynamics The functional dependence of C and C on the helical tip T Q Mach number ~~ (Equations D. 8 and D. 9) is important only when the value of ~ exceeds some critical value. For subcritical helical tip Mach numbers, the propeller flow field is essentially incompres- sible; then this dependence on ~·Lr may be ignored; and we may write: Ti (D.16) (D.17) (D.18) i (D.19) n (D.20) = (D.2l)

=

(D.22) D-6 f

I

i

!

J (D.23) = ~

T /p o

T where the superscript i denotes incompressible aerodynamics.

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I At the end of this Appendix, the ~1cCauley C33/90H-4 constant speed propeller is described; its free performance as computed by

I '

McCauley (using incompressible aerodynamics) tabulated (Table D.l); ~ , U.l.

and the assumptions underlying those computations listed. Figure depicts the geometry of this propeller; Figures D.2-D.4 are plots of the data in Table D.l showing C~, C~ and ni plotted against J for fixed values of (3; and Figures D.5-D.7 show plots of C~ and i C computed from Table D.l. The McCauley C33/90H-4 constant speed R propeller is installed on the Lockheed LASA 60 airplane owned by Princeton University.

Performance Characteristics: Compressible Aerodynamics As the helical tip Mach number increases toward unity, the propeller blade airfoil characteristics are affected by the onset of compressibility. When this occurs, the functional dependence of CT_and C on ~Lr (Equations D.8 and 0.9) must be considered.

Q For fixed values of J and (3: C is observed to increase slightly T

above C~ and then to decrease, while C rises above c; at fir,st

p slowly and then more rapidly; as the helical tip ~mch number in- creases toward unity (40). Glauert (1), considering the effects of compressibility on the blade airfoil characteristics, states: At comparatively low speeds the lift and drag coefficients both increase, and in consequence the torque coefficient of the propeller also increases, while the thrust D-7 coefficient remains sensibly constant since the increases of the lift and drag coefficients produce opposite effects on the thrust of the propeller. This conclusion has been confirmed by flight tests [British A.R.C. R. and ft1. 1173, 1928J which showed no change of the thrust coefficient and an increase of the torque coefficient. At higher speeds the thrust coefficient would decrease owing to the decrease of the lift coefficient The helical tipspeed (~~ch number) at which C begins to fall T and C to rapidly rise is called the Critical Helical Tipspeed p (~ch Number). Helical tip Mach numbers less (greater) than the critical value are referred to as subcritical (supercritical).

When the helical tip Mach number is supercritical, propeller performance may be characterized, at a constant value of ~, by variations of C and C with J and S (plots of such performance T Q have the same form as those appropriate to incompressible aero- dynamics). When these performance characteristics are available for a number of values of r.Lr,the' performance in any operating condi tion may be obtained by interpolation. This method of performance estimation requires a large quantity of data.

In the present work, propeller performance in all operating condi tions is computed from the performance appropriate to incompressible aerodynamics, the effects of compressibility on the efficiency and thrust coefficient being accounted for by the use of Compressibility Correction Factors f and f' as comp comp follo.ws: i

= n ( J. S) f .. ( J, S, r.L)

n (J, S, ~) comp "T ~.

D-8 I j

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General Aviation airplane propellers are assumed to operate with helical tip Mach numbers not greatly in excess of the critical

I'

value. Noting the quote from Glauert above (pp. D-7 and D.B) we therefore set fl = 1. Consequently, comp (D.24) (D.25) (D.26) Before computer technology significantly impacted the propeller industry, a common method for computing f was included in the comp "Hamil ton Standard r.1ethod of Propeller Performance Calculation, II 1941 (21). That method is based upon the correction curves of Fred Weick (10).

The Hamilton Standard Method uses an effective helical tip- speed V defined as T1P E D-9

= speed of sound at sea level, a

where f SL c speed of sound at altitude, a

fh = correction factor for blade thickness ratio at 0.75 tip radius

f = correction factor for blade angle of attack

ex For a given propeller, fh is a constant, so that V is a function TIp E only of ~Lr and blade angle of attack distribution. 111e value of f is computed from the ratio J/J , where J is the actual advance ex m ratio, and J is the advance ratio yielding maximum efficiency at m the operating value of C ' The value of f is determined by comp s entering a plot of f versus V with the values of V comp TIP TIP E E here in Figure 0.8).

and J (this plot is reproduced m This method of computing f is not accurate for four comp reasons: 1. The correction curves used (Figure 0.8), taken directly from Weick (10), were computed from propeller experimental performance data by an only approximate method (10).

2. These correction curves are entered with a value for J , which is not a measure of a singl e performance item m at the operating condition of the propeller.

3. The value of f is computed in an indirect manner.

ex 4. The thickness ratio correction fh is approximate. In <: discussing this correction, Hamil ton Standard (21) state: "Since this correction factor is really a function of some thickness factor integrated along the blade, one 0-10 would expect a correction based on the three-quarter station to be only approximate."

A more accurate method for computing f for a particular comp propeller is required. Such a method has not been determined here.

In the present work, it is assumed that: ,

.... for a given free propeller, may be re-

presented by a number of plots here referred to as f comp Plots.

2. The free propeller f plots are assumed to be applicable comp to the same propeller installed on an airframe, with the provision that: J and ~ are computed using the reduced· forward speed f JV (see the following discussion of the Installed Propeller).

A number of items that should be considered in a detailed study of f are briefly discussed in Chapter 4 (pp. 4-20 and 4-21) .

comp Values of f. for some typical flight conditions of the comp Lockheed LASA 60 airplane, computed using the Hamilton Standard Method (21), are given in Chapter 4.

J 0-11 THE INSTALLED PROPELLER Free propeller performance characteristics do not directly specify the performance of the same propeller installed on an airframe. The installed propeller operates in the presence of the airframe body (fuselage, lifting surfaces, un,dercarriage) and " ..• 311 ilJlportant mutual interference [arises]: tl)(' fJO\\' around the body modifies the conditions under which the propeller operates, and the flow generated by the propeller augments the drag of the body. This mutual interference may be compl icated also by the proximity of the wings of the airplane, whose lift is modified by the slipstream of the propeller" (Glauert, 1).

The following definitions are adopted:

DOFF = power-off airframe drag (Appendix C), lb

DON = power-on airframe drag (Appendix C), lb

D = DOFFIE, lb

Da = DONIE = "apparent drag" (Glauert, 1), lb

E = number of engines, each driving one propeller

T = free propeller thrust (tension in the propeller shaft), lb

T = installed propeller thrust (tension in the propeller

a shaft) called "apparent thrust" (Glauert, 1), Ib

T = propulsive thrust: the apparent thrust less the increase

p in drag of the body due to the action of the propeller, lb.

D-12

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I T = T - (0 - 0) (0;27) p a a T is that thrust available to overcome the power-off p

I

drag of the airplane. and to enable the airplane to

I

climb or maneuver.

Q = free propeller shaft torque, lb ft

I '

Q = installed propeller shaft torque, called "apparent torque"

a (Glauert, 1), lb ft

p = free propeller shaft power, ft lb/sec = 2TInQ

I

P = installed propeller shaft power, ft lb/sec = 2TInQ .

a a The superscript i is added to propeller performance quantities to denote incompressible aerodynamics, while the absence of a super- script denotes compressible aerodynamics.

TIle performance of a particular propeller-body combination is expressed by equations identical to Equations 0.1-0.26 defining free propeller performance, with the following alterations (10, 40, . T(i) T(i) 1. replaces p Q(i) Q(i) replaces 2.

a p(i) p(i) 3. replaces a (i) replaces n(i) 4. (propulsive efficiency) Tlp f(i) f(i) replaces 5.

T T P fCi) fCi) replaces 6.

Q Q a (ft/sec).

and V is the airplane true airspeed 0-13 efficiency n (i) The propulsive is given by p (i)V T(i)V T p

n (i) = -,P,:-:-:-_

(D.28)

=

p p(i) a

In straight and level steady flight, T(i) = D so that the pro-

p pulsive efficiency is Ci) DV rtp = pCi) a = _~P:-!:R,,---_ (0.29) EP(i) /550 a

where P = airframe power required (power-off), horsepower

R = 00FFV/550 horsepower (Appendix C)

P = engine shaft horsepower

s = p(i)/550 horsepower (Appendix A).

a The performance of the propeller-body combination is not always available. The next two subsections address the computation of such performance from the performance characteristics of the free propeller.

Computation of Installed Propeller Performance from Free Propeller Performance Tractor propellers (those mounted in front of the body) and pusher propellers (those mounted behind the body) operate in a flow which is different from the free stream. "The body does not have the effect of a change of velocity which is uniform throughout 0-14 I i

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I i the entire plane of the propeller disc. With bodies of ordinary shape, having their longitudinal center lines in the neighborhood of the propeller shaft axis, the velocity of the air with respect

I

I to the body is reduced very greatly at the center but practically

I ~

none out as far as the propeller tips" (10) . The drag of the fuselage, wings and undercarriage influence this flow field

I

while in genera! the tail surfaces have a negligible effect on it.

Glauert (1) discusses the evaluation of apparent propeller thrust and torque for a propeller operating in such a non-uniform flow field. For a freestream velocity V and a body present, Glauert represents the axial velocity in the plane of the propeller (propeller absent) as Vel - h) where h is a function of radial position on the blade. The thrust and torque of each annular element of the propeller are calculated "as if it [the annular.

element] were operating in a stream of velocity Vel - h).

Integration along the blades then gives the apparent thrust T a and the apparent torque Q " (Glauert, 1). More generally, h is a a function of both the radial position on the blade and the blade azimuth. The body also causes each blade element to experience a tangential and a radial velocity component. Glauert ignores the small perturbations in tangential and radial velocity caused by the body. In relation to the axial velocity he states: J "AI though in detailed calculations it is necessary to use values of the parameter h which vary along the blade of the propeller, for many purposes it is sufficiently accurate to use a suitable average effective value of h for the whole propeller. The t With tractor propeller(s).

D-1S estimation of the behavior of the propeller as modified by the interference of the body then follows quite simply from the characteristics of the undisturbed propeller . . . The apparent thrust and torque of the propeller in the presence of the body and at the advance-diameter ratio J are determined as the free I thrust and torque of the propeller at the lower advance-diameter ratio (1 - h)J and at the same rate of rotation" (1).

For the installed propeller, the advance ratio J is defined as for Equation D.1, V

J =

where V = airplane true airspeed, ft/sec.

In addition, we define f , the propeller J-factor, to be J

f = 1 - h, h constant (D .30)

J and the apparent advance ratio (the advance ratio seen by the installed propeller) J as a The installed propeller characteristics are then written: T(i) (J) T(i) (J )

= T(i)(f J) =

(D.32) a a J (D.33) The installed performance coefficients are T(i) a C(i) (D.34) '"

=

Ta 2 4 pn d Q(i) a C(i) (D.35) ~ ..

=

Q a pn d D-16 ------------------------------------------------------------------------- pei) 2nnQ(i) a a e(i) (0.36) 2ne~i) =

= =

p 3 5 3 pn d pn d a -a -' propeller efficiency is and the installed e(i)J T(i) T a (fJV) -(i) a a (0.37)

y = =

na e(i) 2nnQ (i) a Pa The use of free propeller characteristics (incompressible) for the computation of installed characteristics (incompressible) is summarized in Table 0.2.

Installed performance at any {J, S, ~} may be computed by: 1. Assuming a value for f J and using the free propeller chQracteristics (incompressible) in the manner described in Table 0.2.

Computing the compressibility correction factor f 2.

comp (see the above discussion of cOTilpressibil i ty effects on free propeller performance).

3. Computing the thrust, installed efficiency and propeller shaft torque from: i C = C If Q comp Q a a Ti (0.38) T

=

a a i (D.39) f n n

=

comp a a (0.40)

Q =

Q!/f a comp 0-17 The operation of a propeller on an airplane results in the propeller axis being skewed to the airstream at all values but one of the wing angle of attack, and consequently at all values but one of the equivalent airspeed, for a given airplane weight and center of gravity position. Wind tunnel tests "have sho\rn that the effect of this inclination of the axis is to increase the thrust and torque of the propeller" (Glauert, 1). In the same Reference Glauert also concludes however "that the thrust and torque of a propeller are not altered by a small velocity of sideslip or angle of yaw." He quotes experimental results indicating notice- able increases in the torque coefficient at sideslip angles of 10 degrees, and rapid increases of the torque coefficient with fUrther increases in sideslip angle. Weick (10) states that "in actual flight the propeller axis assumes angles as high as 10 or l2deg. with respect to the flight path. Full-scale tests in the 20-ft. Propeller Research Tunnel of the N.A.C.A. have shown, however, that the propeller characteristics are practically unaffected within that range" (see also Reference 21). Consequently in this work, installed propeller characteristics are considered invariant with airplane angle of attack.

The influence of the wing circulation on the thrust and torque coefficients, in effectively skewing the propeller shaft to the flow, is neglected in the same manner that the effects of airplane attitude are neglected. Any perturbation in propeller axial velocity caused by wing circulation is included in the value of f .

J D-18 ~-------~-- Dommasch (8) states that the presence of the wing may improve the propulsive efficiency of a single rotation propeller "by removing some of the rotation of the wake." Removing the wake rotation effects a change in the induced velocity field of the propeller; and such changes from free-propeller operation are grossly accounted for here in the value of fJo For a specific airframe-propeller combination, the value of f is here considered to be invariant with flight condition.

J The magnitude of f is dependent upon the airplane geometry.

J Influence of the Slipstream on the Body In general, the presence of the slipstream in trimmed powered flight causes changes in the values of the following variables from the values they take in trimmed power-off flight at the same value of the lift coefficient C (see Appendix C): L 1. CD pm 3. with corresponding values of 0 , T and e t w w 4.

i 5.

w The drag coefficient of the body in trimmed powered flight therefore D-19 differs from that pertaining to trimmed power-off flight at the same C .

L In determining the effect of the slipstream on drag, we first consider the lift-independent drag alone. The variations in lift-independent drag due to power here considered correspond to changes in C and n (the term ~~KtStn/S in K 0 only) in t Dpm Equation C.29. These variations are (Glauert, 1): "(1) The increase of body drag due to the increased velocity in the slipstream.

(2) The mutual reaction between the body and propeller due to the pressure gradient in the slipstream.

(3) The shielding of the nose of the body or the inclusion of the boss of the propeller inside the body."

The drag of the body with propeller absent may be written: (D .41)

where D = DOpp/E, Ib

DO = (the entire lift-dependent drag, plus the lift- independent drag of those parts of the airplane outside the region to be influenced by the slip- stream when the propellers are running)/E. lb

D. = (the lift-independent drag of those parts of the

l.

airplane inside the region to be influenced by the slipstream when the propellers are running)/E. lb.

When the propellers are running, the lift-independent drag of those parts of the body wi thin each slipstream is altered to D.

l.a and we may write D-20 (0.42) o = DO + D.

a l.a G1auert (1), in considering those parts of the body totally immersed in the slipstream, shows that the apparent drag o. may l.a be written: . (0.43) where A : 1, and B is a constant dependent upon the airplane geometry. Glauert (1) shows that the value of A is, in general·, approximately unity, especially in those cases where the free pro- peller thrust has been evaluated from blade forces alone (has not included the drag of the boss) which is true in the present work.

In addition, he indicates that the value of B may vary with the propeller advance ratio, but he neither includes such an effect in his analysis nor discusses the magnitude of the variation.

Consequently any such variation of B will be ignored here (see also Reference 21). From Equation D.27, the propulsive thrust is

T = T (0 - 0)

a P a From Equations 0.41 and 0.42, (0.44)

Tp = Ta - (Oia - 0i)

Substituting Equation 0.43 in Equation 0.44 yields and since D. is a lift-independent drag, it may be expressed as l.

a constant multiple of the dynamic pressure pV /2. Consequently,

T = T (1 - e:)

p a 0-21 where E is a small constant. Defining the slipstream inte.rference as factor fD constant = = fo 1 - E we then have

T = f T (0.45a)

a 0 p It is assumed that the above argument applies equally to compres- sible and incompressible propeller aerodynamics, and that fo retains the same value in both cases. Then

Ti = f Ti (0.45b)

a 0 p and In straight level steady flight the propulsive thrust Ti = T = 0 and hence p p T(i)

= =

foO a a and hence (0.46) Equation 0.46, in which fo is constant, was derived from a consideration of power effects on lift-independent drag alone.

It is shown in Chapter 3 that the effects of power on the drag, in addition to those effects considered in the formulation of Equation 0.46, are small for the LASA 60 airplane. The additional effects, arising from variations in items 2- 5 (p. D-19) due to power, . are taken to be small for GA airplanes in general.. In this work, all power effects on drag are subsumed into f . While D fO is not strictly constant with variations in power, it is assumed 0-22 to be constant in Equation D.46.

Equations D.30-D.46 are applicable to both tra~tor and pusher propeller installations. The magnitudes of f and fD are dependent J upon the airplane geometry.

Propulsive Efficiency From Equations D.37, D.4S and D.28, T(i)Cf V) Ci) a J = na 2 nQ(i) 1T a (f T(i))(f V) D E J = 2 (i) 'IT1lQ a f f n (i) (D.47) = D J P i na i .

(D.48) = np fDfJ Substituting Equation D.39 in Equation D.47 yields i

= na fcomE

np fDfJ (D.49)

= n~ fcomp

The foregoing discussion has established the fact, expressed by Equations D.48 and D.49, that the propulsive efficiency for any set {J, 13, ~} may be expressed in' terms of: 1. The installed propeller efficiency ni computed using a incompressible aerodynamics for the set {J , f3}: the a computation of ni has been discussed.

a 2. The propeller-body interference factors fD and f .

J D-23 3. The compressibility correction factor f comp The operation of the installed propeller in straight steady flight is subject to the following constraints: I. The propeller and airframe move with the same forward speed.

II. The propeller shaft torque is a constant multiple (the transmission gear ratio G) of the engine shaft t torque.

III. The propeller shaft speed is a constant multiple (the inverse of the transmission gear ratio G) of the engine shaft speed.

In straight steady level flight, the following force constraint must also be satisfied: IV. The sum of the thrusts ET(i) from all propellers is a equal to the power-on airframe drag foOOFF (Equation 0.46).

The above four constraints apply to the operation of propellers with fixed or variable pitch. All fixed pitch propellers operate with the additional and final constraint: V. The blade angle B is invariant.

We now seek an understanding of the functional nature of i na subject to the constraints I and IV. This is achieved through i a study of the Speed-Thrust Coefficient CR. Presentation of . i propeller performance in terms of C is an extension of th~ method R " of analysis presented by Pye (12) and Kerber [The Lesley-Reid Method] (2) for the performance analysis of fixed pitch propellers.

tAf . 1 .. P h b d f h .

ter aUX1 1ary equ1pment power AUX as een remove rom t e eng1ne shaft: see Figure A.2.

0-24 The Speed-Thrust Coefficient: Consider the problem of determining the propeller speed n revolutions/second and blade angle 8 which maximize the efficiency of a given free propeller, under the constraints of a prescribed forward speed, air density and thrust. Assume that compressi- bility effects are absent.

This computation is facilitated by plotting a propeller parameter that incorporates all of the known quantities i (V, p, T , d) versus a second propeller parameter containing the unknown n, for fixed values of blade angle 8 and efficiency ni.

Two such parameters are respectively Ti and J. The computation c i proceeds by calculating the value of T from the given quantities, c i and picking off the T :J plot that value of J which corresponds c i to maximum efficiency at the fixed value of T. The blade angle c required is readily determined at the resulting {T~, J} point.

The required value of n is then calculated from the value of J.

The task of interpolation on such a plot is made easier by plotting I Ci = _J_ = (D. 50) R~

q-

T c Vd (D. 51)

=

.( i

'T /p

i i versus J for fixed values of Band n. The quantity C is here R defined as the propeller Speed-Thrust Coefficient. The plot of C~:J2 for the McCauley C33/90M-4 constant speed free propeller is presented in Figure D.6. Plotted in this manner, the lines of D-25 constant blade angle S are almost straight and equally spaced.

The dotted contour lines of constant efficiency clearly define a three-dimensional surface, an efficiency ridge. The line of maximum efficiency running up this ridge indicates the maximum efficiency achievable for any value of C~; and the corresponding value of J2 provides the propeller speed n necessary to achieve that efficiency when V and d are known. In Figure D.7 C~ is plotted against l/J which is essentially a scale of n revolutions/ second for any fixed values of V and d: the efficiency ridge is again clear. For any fixed value of the blade angle S, the efficiency ni is seen to remain almost constant at the higher i values of CR.

Now consider an airplane in straight and level steady flight, with E propellers each providing identical thrust. Then, for each propeller, J fJVd i a C CD.52)

= =

R a

{l /Ti/

a P T a where V is the airplane true airspeed, ft/sec (constraint I).

Invoking Equation D.46 for Ti (constraint IV) and Equation C.I a for DOFF' CD. 53)

=

For a given airplane, the only variable on the right hand side of Equation D.53 is the airframe power-off drag coefficient CD' whici1 is a function only of V ' Wand h (Appendix C) where E D-26

V = equivalent airspeed,knots

E

W = gross weight, lb

h = center of gravity position.

For any value of CD' the "right hand side of Equation D.53 may be i computed (values of C so computed for the LASA 60 airplane are R a plotted in Figure ·D.9).

Entering the i i with this computed value of C gives the variation of ina' S} R a i with J~, and the values of {J , S} yielding maximum na are obtained.

a Now (D. 54)

where N = 60n = propeller revolutions/minute

t o = atmospheric density ratio (Appendix B).

For a given airframe and propeller in straight and level steady flight, the C~ :J~ plot (such as Figure D.6) therefore represents a i a three-dimensional surface, whose height na is i i[ (D. 55)

n = n V , W, h, N, oJ

E a a and upon which lines of constant S are inscribed.

For a given airframe and propeller in straight and level steady flight, the C ' :J 2 plot, the f nlots and Equations D.48 R a a comp .

and D.49 together define: (D. 56) "j This is a complete definition of n .

p tStandard and non-standard atmospheric conditions.

D-27 Propeller Shaft Torque Since the airframe power required P is a function only of R {V , W, h, o} (Appendix C and Chapter 3), we have from Equations D.29, E D.48 and 0.55: i

pi =

W, h, N, 27TnQ

p![V , =

oJ E a a Qi .

Hence the propeller shaft torque ~s: a

Qi =

w, h, N, (D. 57) Q;[V , oJ a E For a given airframe and propeller in straight and level steady flight, the c~ :J~ plot, the c~ :J plot and Equation D.36 a a a together define the function in Equation 0.57. This is a complete definition of Qi.

. a Similarly, from Equations D.29 and D.56:

P = 27TnQ = Pa[V , W, h, N, 0, MTJ

a a E Hence the propeller shaft torque Q is: a

Q = Qa[V ' W, h, N, 0, ~~] (D. 58)

a E For a given airframe and propeller in straight and level steady flight, the c~ :J~ plot, the c~ :J plot, the f a a a comp plots, and Equations D.36 and 0.40 together define the function in Equation 0.58. This is a complete definition of Q .

a Q and N are used in the computation of the engine shaft a torque and rotational speed respectiv.ely (constraints II and III).

Propeller Blade Angle "".

For a given airframe and propeller in straight and level 0-28 I !

I

I

I

!

steady flight, the lines of constant B in the c~ :J; plot define

a the functional relation (D. 59)

S = SeVE' W, h, N, oJ

I ~

Equation D.59 displays no MT dependence by virtue of Equations

D.38 and D.52.

PERFORMANCE MODEL For a given set {V , W, h, N, 0, M } the propulsive T E efficiency n , the propeller shaft torque Q and the propeller p a blade angle B are computed in this work as follows: 1. Assume values for f and fD J i 2. Compute C - Equation D.53 R a 3. compute J - Equation D.31 a i 4. Compute C - Equation D.52 T a 5. Compute B - Figure D.6 i 6.

Compute c - Figure D.3 P a i 7.

Compute na Equation D.37 i 8. - Equation D.48 Compute np 9. Compute pi - Equation D.36 a i i 10. ompute

C Q = P 121rn

a a Finally, the effects of compressibility are included: 11. Compute f - See page D-11 comp 12.

Compute np - .Equation D.49 13. Compute Q - Equation D.40 a D-29 The computation of 8 (Step 5) could be performed using Figure 0.2

with the available values of ci and J . The advantages of using

a a the Speed-Thrust Coefficient Figure 0.6 are: 1. It affords physical insight into the variation of {: i I i na in {V , W, h, N, cr} space, E i 2. It identifies the trajectory of maximum na in {V , W, h, N, o} space.

E CHARACTERISTICS OF THE McCAULEY C33/90M-4 CONSTANT SPEED FREE PROPELLER Geometry The geometric data of Figure 0.1 were provided by the McCauley Accessory Division of the Cessna Aircraft Company (Drawing Number 90M). The modified RAF.6 section used is described by Weick (10).

Performance: Incompressible Aerodynamics The performance characteristics of the McCauley C33/90M-4 constant speed free propeller (provided by McCauley) are presented in Table 0.1. The power coefficient C~, efficiency ni, and thrust coefficientC~ are given for a range of advance ratios J from zero through 0.9, for various values of the blade angle 8 degrees.

The data were computed using a Goldstein-Lock analysis (1, 8). McCauley was not able to provide any supporting test data.

The following should be noted with regard to the computations: 1. The propeller was assumed to operate in a free stream of uniform velocity. No account was taken of the presence 0-30 of a body in determining the inflow velocity or the wake structure. The free stream velocity was parallel to the propeller shaft axis.

2. Radial integration was performed between 20% and 100% of the propeller tip radius R. In this manner the presence of the spinner was recognized, although no account was taken of its effect on the inflow velocity field.

3. Zero drag is attributed to the radial stations inboard of 0.2R.

4. The analysis used experimental two-dimensional lift and drag coefficient data from early NACA tests of modified RAF.6 airfoil sections with various thickness to chord ratios (similar data are given by Weick, 10). These data were taken for a Reynolds number of 1.0 x 10 , based on airfoil chord as the length measure.

5. The thickness and chord distributions of the C33/90M-4 propeller blade were properly represented in the analysis.

6. For those inboard stations where the blade sections deviate from the modified RAF.6 (0.2R-0.35R). the section was assumed to be a modified RAF.6 section with the correct thickness and chord.

7. No account was taken of compressihility effects.

8. The blade angle 8 is measured between the plane of rotation and the flat face of the blade, at a radius of O.75R. Although the computations assume rigid propeller D-31 blades, the performance figures may be used for a flexible propeller when S is considered to be the blade angle in operation (5, 10).

The performance characteristics in Table D.l are plotted in Figures D.2-D.4.

D-32 TABLE D.l PERFORMANCE CHARACTERISTICS OF C33/90M-4 TYPE PROPELLER i.

"li-

Ci..

CT ~ J --'::::P.- .0807 .0245 .0928 .0308 I .1009 'Y 14 .0373 .1062 .0441 .1058 .0525 .1033

I

.0629 .1009 .0719 .0998 .0771 .0995 .0785

I 26

.0995 .0787 .0721 .0244 .2953 .1 .0849 .2748 .0309 .1 .0974 .2551 .0382 .1 .1049 .2310 .0454 .1 .1076 .2045 .0526 .1 .1054 .1695 .0622 2() .1 .1022 .1402 .0729 .1 .1000 .1241 .0806 .1 .1187 .0994 .0837 .1 .1184 .0993 .0839 .1 .0607 .5164 .0235 .2 .0739 .4875 .0303 .2 .0868 .4579 .0379 .2 .0998 .4300 .0464 .2 .1093 .4004 .0546 .2 .1093 .3527 .0620 .2 .1051 .2890 .0727 .2 .1013 .2439 .0831 .2 .0995 .2223 .0895 .2 .0991 .2173 .0912 .2 .0473 .6696 .0212 .3 .0607 .6453 .O?8~ 1~ .3 .0740 .6132 .0362 .3 .0875 .5808 .0452 .3 .1005 .5501 .0548 .3 .1109 .5188 .0641 .3 .1128 .4667 .0725 .3 ~ i .1052 .3790 .0833 .3 .1011 .3259 .0931 .3 .0993 .3021 .0986 .3 D-33 TABLE D.1 (continued) PERFOID1ANCE OIARACTERISTICS OF C33/90M-4 TYPE PROPELLER I..

'?,i.

ci.

~ eT J -p- 'C' .0170 .7519 .0320 .4 10 .0460 12 .0244 .7542 .4 .0598 14 .0328 .7293 .4 .0422 .0736 16 .6973 (:, .4 .0871 .0524 .6648 .4 18 .1002 .6334 .4 20 .0633 .1107 .0741 .5976 .4 22 .1147 24 .0836 .5487 .4 .1067 .

. 4548 .4 26 .0938 .1017 28 .1031 .3944 .4 .6911 .0155 10 .0112 .5 .8053 .0298 12 .0185 .5 .0441 .8102 14 .0272 .5 .7864 .0585 16 .0372 .5 .0725 .0480 .7551 .5 .0860 .7227 20 .0595 .5 .6866 .0993 22 .0723 .5 .6517 .1099 24 .0843 .5 .6096 .1151 26 .0944 .5 .5221 .1095 28 .1049 .5 .0277 .0198 .8396 .6 14 .0424 .0300 .8490 .6 16 .8261 .0570 18 .0414 .6 .0710 20 .0536 .7949 .6 .0845 22 .0670 .7568 .6 .0979 24 .0814 .7219 .6 .6933 .1091 26 .0944 .6 .1150 .1048 .6584 .6 28 .1110 .1160 .5741 .6 30 .1047 .1241 .5061 .6 32 .0408 .0326 .8751 .7 .0554 .0455 .8529 .7 .814h .0693 22 .0596 .7 .0829 24 .0746 .7777 .7 .0968 .7501 26 .0903 .7 .1084 .1042 .7281 .7 .1148 .1156 .6954 .7 .1118 .1274 .6145 .7 .1066 .5499 34 .1357 .7 .1015 .1414 .5027 .7 }., D-34 I i I.

I TABLE D.1

I

(concluded)

I

l PERFORMAl~CE CHARACTERISTICS OF C33j90M-4 TYPE PROPELLER

I

, i t.

'fli- '($ J ~ ~- .8 22 .0500 .8596 .0537 I .8 , .0659 .8240 .0679 .8 26 .0821 .7961 .0817 .8 .0990 .0960 .7755 .8 30 .1l43 .1079 .7553 f .8 32 .1269 .7233 .1l47 ..

.8 .1393 .6459 .1125 • " .0 36 .1479 .1080 .5843 I .8 38 .1541 .5394 .1039 I:; ~8 40 .1540 .5264 .1013 .9 .0549 .8579 .0523 .9 26 .0721 .8343 .0668 :, 28 .9 .0896 .8154 .0812 .9 :0 .1080 .7959 .0955 .9 32 .1250 .7763 .1078 .9 34 .1388 .1148 .7441 .9 36 .1517 .6701 .1129 .9 38 .1607 .6113 .1092 .9 .1670 .5691 .1056 .9 .1672 .5538 .1029 : ~ D-35 TABLE 0.2 DETERMINATION OF INSTALLED PROPELLER CHARACTERISTICS FROM FREE PROPELLER CHARACTERISTICS IN THE ABSENCE OF COMPRESSIBILITY EFFECTS

Each free propeller chart with coordinates ex, y, S) may be used

directly to determine the characteristics of any geometrically similar propeller installed on an airplane (when scale effects due to Reynolds number variation are negligible), by reading the coordinates ex, y, 8) as ex , y , 8) defined below.

a a Free Propeller Installed Propeller Characteristics Characteristics x y x Ya a fJV i i i i

= V 4 2 4

T /pn d T /pn d J C J C

= =

= nd

nd T a T a a i i 2d 5 Qi/pn2d5 Qi /pn J C J C

= =

a a Q Q a i i i i 3 5 3 p /pn d p /pn d C J C J

=

=

P a P a a i i i i i CiJ/C .J J C J /C n

n =

=

T P a a TaP a a i Ti 2 2 Ti

= Ti / pf2V2d 2

J J T /PV d

=

c a a J c a

-

2 2 Qi Qi Qi/ 2d Qi /Pf V d 3 J PV J

=

=

c a c a J a . 1/5 . 1/5 i i 1 V[p/p n ] C C J J fJv[p/P~n2]

=

=

S a S a i i i J C J C Vd/IT /p

= = fJVd/!T;/P

R a R a 0-36

------,---, ---------

---_ .. _'*'----_.--,_ .. _--"

.. ,-~

lA v. ;::w, (,,1 -

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APPENDIX E

i I

I

APPENDIX E

I

THE NATURALLY ASPIRATED ENGINE PERFORMANCE MODEL Table of Contents Page 1 NTRODUCTI ON. . • . • . . . . . • • . • • . • . • • • . . • • • . • • • • • • • . • • . . . • . . . . • • •. E-l Basic Definitions ....•...•.•.•.•..••.....•.•...•.••••.•• E-2 Design Parameters and Operational Parameters ..•..••.•••• E-4 INDICATED HORSEPOWER......................................... E-6 Air Mass Flow Rate ...••.•....•....••.••..•.•...••.••••.. E-6 Inlet Air Density .......••••.•.•.. ~ •..•••....•.••••••••• E-7 Volumetric Efficiency ..•..•.••.••••..••......•..•••••••• E-9 Fuel-Air Ratio ....••••.... '" ..•..••••••..••..••.••••••• E-13 Indicated Thermal Efficiency ••.••.•••.•...••••.•..•••••• E-14 Equivalence Ratio and Ignition Timing ••.••••.• .•••• E-19 Engine Shaft Speed .•. .••.••••••••••••..••..•••••••• E-23 Inlet Manifold Pressure and Exhaust Back-Pressure •• E-24 Cylinder Head Temperature ••••••••.•••.•••.••••••••• E-26 Humidi ty . ..•••••••••••.••••••••••••••••.••••..••••• E-27 Inlet Manifold Temperature •••••••••••••.••••••••••• E-27 Summary of Effects on Indicated Thermal Efficiency. E-30 Summary of Indicated Horsepower Variations .•.•.. ; ...•.•• E-31 LOST HORSEPOWER ......•...•..•..•••.••.••••.....•........••... E-32 Pumping Losses .•.•.•••.•••••.•.•••••.•.•.•••..••••.••••• E-32 Mechanical Friction .•.•••.•••••••••••••.•.••.••••..••••• E-35 Total Lost Mean Effective Pressure and Lost Horsepower •• E-35 Lost Horsepower Based on the Motoring Test •••••.•.•.•••• E-36 -;' .

FUEL METERING SCHEDULE ....................................... E-38 COMPUTATION OF NATURALLY ASPIRATED ENGINE PERFOR}~CE ....••.• E-39 Required Engine Characteristics ••••••••.••••.•.••••••••• E-39 Reference Operating Point •••••••.••••.•...••...••.•.•••• E-40 Table of Contents (concluded) Page Fuel Schedule Datum .•••..•.....••••.....•• " .••••••..•..•• E-4l General Operating Point .....•..••.•.••...••......•..••.. E-42 TABLE E.l .•.•....•.••••.•.•.........••••..••..•...•..•.... " .•• E-44 FIGURES E.l - E.lS .....•.•..•..•...•..••.•.•.. 0 •••••••••••••• E-4S

APPENDIX E

APPENDIX E THE NATURALLY ASPIRATED ENGINE PERFORMANCE MODEL INTRODUCTION This Appendix presents a method for the computation of the per- formance of naturally aspirated, spark-ignition, fuel injection, 4-stroke reciprocating internal combustion engines, measured in terms of Brake Horsepower and Brake Specific Fuel Consumption. The method involves: 1. Computation of Indicated Horsepower at the required operating point, from a) The indicated horsepower developed at a reference operating point.

b) Scaling functions of the operational parameters.

2. Computation of the Lost Horsepower at the required oper- ating point.

Uniform distribution of induction air and fuel flow to all cylinders is assumed, a condition closely approached by an engine with a well designed induction system and a fuel injection system. This discussion pertains to well designed engines utilizing inlet port fuel injection systems. The difficulties of modelling the ~ffects of non-uniform induction air distribution due to bad inlet manifold design, or non-uniform fuel distribution associated with E-l carbureted engines, are avoided.

The engine is assumed to operate with all cylinder heads at a common uniform temperature. Similarly, a uniform inlet manifold· tempera- ~ ..

ture is assumed betwe.en the throttle butterfly and the inlet valves.

All computations pertain to a dry atmosphere. For details on the effects of humidity on engine performance, refer to Taylor (13).

Basic Definitions The macroscopic gas processes which determine the work output of any spark-ignition, 4-stroke reciprocating internal combustion engine may be characterized by a pressure~volume (pV) cycle diagram.

Such a diagram, typical of a naturally aspirated aircraft engine, is shown in Figure E.l, which represents the processes in one cylinder.

Following Obert (29) the Indicated work of each cycle is de- fined as area (A+C) of Figure E.l, while the Pumping Work is defined as area (B+C). The indicated work is the energy delivered to the piston by the gases in the cylinder during each cycle; while the pump- ing work is the work done per cycle by the piston in expelling burnt gases from the cylinder and drawing in a fresh charge.

The Indicated Horsepower (IHP) of the engine is the rate at which indicated work is done on all the pistons of the engine.

The Pumping Horsepower (PHP) is the rate at which pumPing work is done by all the engine pistons.

Associated with the gas processes of Figure E.l, but not· shown therein, is the work done by the entire engine in overcoming mechanical friction. The horsepower required for this is denoted by MHP (Mechanical E-2 I !

I

I

!

j friction Horsepower).

The horsepower consumed by pumping and mechanical friction is

I

not available as useful power at the engine shaft, and therefore is i referred to herein as Lost Horsepower (LHP): [, lliP = PHP + MHP tE.l) The horsepower available for useful work at the engine shaft is Brake Horsepower (BHP):

I

P = BHP IHP - lliP (E.2)

=

E 21T .

(E.3) Q

=

NE (33-000) E , brake where engine torque (lb ft)

Q[ =

N = engine shaft speed (revolutions/ninute) E Mean effective pressure (MEP) is work done per unit time, divided by engine power-stroke displacement per unit time (13). Hence, brake mean effective pressure is (29): "(E.4) B~ffiP = 458.33 (BHP)/DN E where D = total engine displacement (cubic ft). Similarly, indicated mean effective pressure is: IMEP = 458.33 (IHP)/DN (E.5) E and the lost mean effective pressure is:

LMEP = IMEP - BMEP

= 458.33 (LHP)/DN (E.6) E The fuel economy of a reciprocating internal combustion engine is usually measured by its Indicated Specific Fuel Consumption (ISFC) or its Brake Specific Fuel Consumption (BSFC). If the fuel mass flow rate into the engine is ~f lbm/hr then: E-3 m f ISFC Ibm/IHpohr (E.7) = -- IHP .( m f lbm/BHpohr BSFC (E.8) = BHP Consequently, 1 1 LHP --= (E.9) ISFC - BSFC m f Design Parameters and Operational Parameters Many parameters, both design and operational, determine the quan- tities IHP, LHP and hence BHP, ISFC and BSFC. Full treatment of these parameters may be found in References 11-14, 29.

Design parameters are those fixed by engine design such as: engine geometry, co~pression ratio, valve timing, gasoline octane rating, fuel metering system, air induction system, exhaust system, bearing design and so on. In the present study the design parameters are con- sidered quantities not under our control.

Operational parameters characterize the environment and mode of operat~on of the engine. These are: 1. Fuel-dry air mass ratio 2. Ignition timing 1 3. Inlet manifold absolute pressure P m 4. Inlet manifold temperature 5. Cylinder head temperature 6. Exhaust back-pressure P e 7. Exhaust gas temperature T e 8. Engine shaft speed i i

I

I

I

i

9. Engine brake torque Q _ E 10. Atmospheric mass ratio water vapour/dry air h These apply to both naturally aspirated and turbocharged engine types.

I

I .

Each operational parameter is here considered to be measurable during

I f

the operation of the engine; and with the exception of atmospheric humidity, each is considered to be controllable (its steady state

I

value may be set within a finite range). However, the operational , parameters are not independently controllable, so that only a limited number of them may be prescribed at anyone time. The means availa- ble for controlling the operational parameters are: a) Fuel flow lever b) Variable spark-advance system c) Throttle d) Induction air heater (and after-cooler in the case of turbocharged engines) e) Engine cowl flaps f) Turbine waste-gate and nozzle geometry, in the case of turbo- ·charged engines g) Propeller governor h) Flight altitude The operational parameters primarily influenced by each of these con- troIs are indicated in Table E.l.

The discussion following addresses the computation of engine per- forrnance, and it$ variation with changes in the operational parameters 1-10, with the exception of atmospheric humidity.

E-S INDICATED HORSEPOKErr The well known expression for indicated horsepower is \vri tten (13): .

(E.10) IHP = KJ m Q n· f c 1.

:: KJ m::? F Q" n. CEo 1 ~) _ c 1.

J = mechanical equivalent of heat = 777.98 ft.lb/Btu

m = fuel mass flo .... · rate, lbr.l/hr

f • m = -dry air mass flow rate, Ibm/hr a

F = fuel-dry air mass ratio = ;f/;a

Q = heat of combustion per unit mass fuel, Btu/Ibm c

n. = indicated thermal efficiency

1.

Aviation gasoline is here taken to have the properties (13): Chemical composition C H17 = 113 Molecular weight t<1 f 0.067 Stoichiometric fuel-dry air mass ratio

=

Fc Q 19,020 Lower heat of combustion, Btu/Ibm

=

c Using Equation E.ll we may write, for a change in operating condi- tions from point 1 to point 2: (E.12) Air Mass Flow Rate The total induction mass flow rate (denoted m. lbm/hr) through 1.

the engine consists of a mixture of dry air, fuel and water vapour.

E-6 This induction mixture flo~ rate is conveniently expressed in terms of the volumetric efficiency of the engine (13):

m. = 60 n NED p./2 lbm/hr (E. 13)

1 v 1

where nv = volumetric efficiency based on inlet manifold density

NE = engine shaft speed, revolutions/minute

D = total displacement volume of the engine, cu ft

p. = density of mixture at the inlet port, lbm/cu ft

Defined in this way, lithe volumetric efficiency measures the pumping performance of the cylinder and valves alone" (13). This definition is the most convenient measure of pumping performance in turbocharged engines, and is retained for use ~ith natu~ally aspirated engines.

Letting p be the mass of dry air per unit volume of fresh mix- Tn

ture at the inlet port, (and since ~ /p = ~./p.)we have the dry air

a m 1 1 mass flow rate mas: a lbm/hr (E .14) Hence the variation in dry air mass flo~ rate from operating con- dition 1 to 2 is: m a -.-= (E.lS) .

Inlet Air Density The inlet manifold density of dry air is expressed (13) as: p 1 m P = lbm/ft (E.l6)· RT m ~l a m

+ F (,.t) +

rl

h(~) ]

If

l

E-7 In this work, where engines using inlet port fuel injection are stud- ied, we may take (13) : p inlet manifold absolute = pressure, lb/ft m T inlet manifold absolute temperature, degrees Kelvin

=

m R = gas constant for dry air a

= 96.03474 ft lb/lbm.degree Kelvin

Ma = molecular weight of dry air

= 28.96408

Mw = molecular weight of water

= 18.016 (Ref. 42) h = mass ratio of water vapour to dry air where P and Tare m m measured.

The values of Rand!-! have been computed from the sea level values a a of pressure, temperature and density in the standard atmosphere (see Appendix B).

The contribution of F in Equation E.16 is here ignored since fuel evaporation is by no means complete during the induction process with inlet port fuel injection. In addition, humidity is not considered as a variable in this study: a11 computations pertain to a dry atmos- phere. Consequently, Equation E.16 is here usee in the form: (E.17) and the variation in inlet manifold dry air density from operating con- dition 1 to 2 is: (E.18) E-8 Volumetric Efficiency The volumetric efficiency (based on inlet manifold conditions .f as defined by Equation E.14) may be expressed by the functional rela- tionship: (E. 19) where engine shaft speed

=

NE CHT cylinder head temperature

=

manifold temperature inlet absolute

=

Tm p inlet manifold absolute pressure

=

m p exhaust absolute back-pressure

=

e equivalence ratio, defined as:

<P =

fuel-air mass ratio of fresh mixture ¢

=

stoichiometric fuel-air mass ratio (E. 20) All engine design ratios have been omitted from Equation E.19 since they are not variables. We seek an expression for the variation of

ny when the operational parameters in Equation E.IS are varied from

condition 1 to condition 2.

Taylor (13) writes the functional relation for volumetric effi- ciency in the form of non-dimensional groups. He has (with some re- arrangement) : (E.2l) I I .

I d where

Z = inlet valve Bach Index, defined in terms of piston

speed and speed of sound in the inlet manifold

~ = Reynolds Index based on the speed of sound in the

E-9 inlet manifold

C = specific heat of fresh mixture at constant pressure

p Tc = coolant temperature (for 1iquid~coo1ed engines), here taken to be cylinder head temperature Rl, ... R = engine design ratios.

n Taylor (13) shows that:·

a) n., is a unique function of Hach Index Z for a given engine

(Z is defined by Equat ion E. 44) . For the reasonab 1y sma 11 variations in piston speed and inlet manifold temperature encountered herein, with variation of operating condition for a given engine, the functional dependence of nv on Z is ignored.

b) nv is a non-linear function of P/P , dependent on the value m of Z. Variations of nv with back-pressure are reflected in variations of Brake and Indicated horsepower.

Lycoming (25) states: HMany tests have been made, includ- ing some at Lycoming, which show that the weight air consumed, and therefore the IHP developed at constant mixture strength, is inversely proportional to the exhaust back pressure raised to the one tenth power." Pye (12) states: "The effect of a change of the exhaust back pressure upon theBHP of an engine win depend a good deal upon the speed and the valve timing; and the magnitude of the effect will be different according to whether the back pressure is above or below that in the inlet manifold."

In the present work, the functional dependence of vo.1u-

metric efficiency on engine ·pressure ratio P IP is taken to be

m e E-10

I'

(E.22a) I .

I'

and E = 0.1 is used as a typical value.

p c) The effect of Reynolds Index ~ on volumetric efficiency is

I

I

negligible.

d) Volumetric efficiency varies almost in direct proportion to S.

TO.

m Lycoming (25) have found that, for Lycoming naturally aspirated aircraft engines employing inlet port fuel injection, the indicated horsepower and the air mass flow rate are both pro- S portional to l/TO. , ~t sea level (and at altitudes above sea level - Reference 43) where T is the fuel injection sys- tern airbox inlet absolute temperature (the airbox houses the air throttle butterfly).

In the present work involving naturally aspirated inlet port fuel injection engines, we modify this Lycoming result and write m a where T is the inlet manifold absolute temperature. Cornpar- m ing this expression with Equation E.14 yields E-11 £:

n a: T t

v m so that This variation accounts for i) The effect of fuel evaporation on the mixture tempera- ture at inlet valve closing ii) Heat transfer to the mixture from the engine: from the inlet port, inlet valve and cylinder walls while the inlet valve is open.

In accordance with the findings of Lycoming, £:t = 0.2 is used

in this work as a typical value; and this value is here taken to be invariant \\i th flight al ti tude.

e) Coolant temperature change (in liqui~cooled engines) has a small effect on volumetric efficiency over a range of 610±SOOR. The variation is expressed as + 2000 + 2000 T ...

~2 (coolant temperatures T and T in degrees Rankine) about c c I o

a nominal operating point T = 6l0 R. The corresponding

c l nominal operating point cylinder head temperature (CHT) o would be greater than 6l0 R, and a lOR variation in coolant temperature would correspond to a larger variation in CHT.

With air-cooled engines, the temperature of the cooling air affects the CHT which in turn affects volumetric efficiency E-12 i i , i

I

I

I I (as here defined) by heat transfer from the inlet port,.

inlet valve and cylinder walls. This effect is accounted

I

I

for with normal levels of CHT and changing T by the factor m in Equation E.22b. Variations in CHT itself are here con- sidered to have no effect on that factor, nor to vary

I'

volumetric efficiency when T is fixed. It is recognized m that large departures in CHT from normal values will almost

I

certainly violate these two assumptions.

f) Fuel-air ratio affects the temperature drop of the inducted mixture due to fuel evaporation. The effect of fuel evapora- tion on volumetric efficiency, included in (d) above, is here considered to be invariant with fuel-air ratio.

Considering items (a)-(f) above together, the change in volumetric efficiency (for engines employing inlet port fuel injection) from op- erating point 1 to 2 is expressed: (E.23) Fuel-Air Ratio Equation E.l2 shows that the variation in IHP from condition 1 to 2 is in direct proportion to the variation in fuel-air ratio, for con- stant dry air mass flow rate and constant indicated thermal efficiency.

Note that (E.24) E-13 where ¢ = equivalence ratio.

In General Aviation piston engines, fuel is metered to the engine for three purposes: 1. To provide a combustible mixture for the development of power.

2. To aid in cooling the engine, especially at high power levels.

3. To ensure detonation-free operation.

The fuel-air ratio appropriate to the various regions of engine opera- tion is discussed under the heading Fuel Metering Schedule below.

Indicated Thermal Efficiency The indicated thermal efficiency measures the efficiency of con- version to indicated work of the total heat energy available in the fuel burned. The total available heat energy per unit mass of fuel is Q , the lower heat of combustion (13).

c Comparison of Equations E.7 and E.lO shows the relationship between indicated thermal efficiency and indicated specific fuel consumption, (E.25)

n = KJQ (ISFC)

i c The indicated thermal efficiency of a spark ignition reciprocating internal combustion engine can never exceed the ideal efficiency of the 'constant-volume air cycle' for which (E. 26)

where r = the compression ratio of the cycle

y = the ratio of specific heats for air, considered as a perfect

gas.

Whi Ie useful in establishing an upper bound for efficiency, the constant E-14 volume air cycle does not consider the phenomenon of combustion. The idealized cycle which does _consider combustion is the 'constant volume fuel-air cycle'whose indicated efficiency is somewhat lower than that of Equation E.26 because (13) of: Variations in specific heats of the gases Progressive and incomplete oxidation of the fuel to CO~ and 2.

£.

Real four-stroke spark ignition,engines demonstrate indicated thermal efficiencies below those computed for their equivalent constant volume fuel-air cycles which "represent the limit which can be approach- ed by spark-ignition engines" (13). Departures from this limit, accord- ing to Taylor (13) may be attributed to: 1. Leakage - blow-by, usually insignificant 2. Incomplete combustion - failure to reach theoretical chemical - equilibrium before the exhaust valve opens.

3. Progressive burning - finite flame speed.

4. Time losses - the loss of work done on the pistons due to piston motion during combustion.

5. Heat losses - losses of heat energy to the piston, cylinder head and cYlinder walls during the compression and expansion strokes.

6. Exhaust losses due to opening the exhaust valve before bot- tom dead center. This loss is seen as a romdoff in the pV cycle diagram during the blowdown process.

As a consequence of these considerations, the following functional relation may be written for the indicated thermal efficiency of a given E-15 engine burning a particular t)~e of fuel: (E.27)

where l = ignition timing: the number of crank angle degrees before

top dea~ center (BTDC) at which the spark (ignition event) occurs.

In Equation E.27 the compression ratio and engine geometry (including valve timing and number of ignition pOints per cylinder) have been omit- ted since they are here considered to be constants, as are mixture homo- geneity and the condition of the spark. In addition, the residual ex- haust gas fraction is accounted for by cp, P, P and T .

. m e m , Since indicated work is obtained directly from the pV cycle diagram, the indicated thermal efficiency may be obtained from the pV cycle diagram and a knowledge of the fuel mass burned during the cycle. The contribution

to n of each of the arguments of f2 in Equation E.27 might well be described

i in terms of its effect on the pV diagram. It is more convenient however, to consider an equivalent plot of cylinder pressure versus crank angle for this purpose.

Figure E.2 shows a typical trace of cylinder pressure versus crank.

angle for the compression and power strokes. The magnitude of the indicated work is determined by: The magnitude of 0, the location of the pressure peak in crank (a) angle degrees after top dead center (ATDC) I "

(b) The magnitude Pc of the peak cylinder pressure

curve (c) The shape of the pressure versus crank angle of (A+C) E.1.

Figure E.2, which together determine the area of Figure E-16 i j {

I

I We are concerned with maximizing indicated thermal efficiency , and therefore with maximizing the sum contribution of (a)-(c) to indicated work for a given mass of fuel burned. Maximizing indicated thermal efficiency contributes to minimizing BSFC (Equations E.25 and E.9).

It is well known that for wide variations in the operating

I conditions of any spark-ignition internal combustion engine, maximum

torque is obtained when the pressure peak Po falls within a very small

I

neighborhood of 0=0 (a constant) crank angle degrees ATDC. Pye (11) o determines a single angle 0=0 = 12 ATDC for the engines in his discussion; o Curtiss Wright (15) claim 0 ~ 15 ATDC for their Turbo Compound TCl8 o

engine; and Powell (44) found 0 = 15.7 ATDC a good mean value for his

o t work with a CFR engine . Since variation of the location of Po cannot significantly affect the Lost Horsepower, it is apparent that indicated work and hence indicated thermal efficiency are both maximized by so positioning the pressure peak, Consider the operational parameters which determine the location 0 of the pressure peak Po' Following the ignition event, there is a delay interval during which no appreciabfe rise in cylinder pressure occurs due to combustion. The delay interval is characterized by a time period Td and a change in crank angle ed' Following the delay interval is the pressure rise interval, during which the cylinder pressure rises to its peak value. The pressure rise interval is characterized by a time period T and a change in crank p angle e ' The following functional relations may be written from Pye(ll) p and Taylor (13): This t fact stimulated tne successful attempt by Powell (44) to use cylinder pressure peak position feedback in the closed-loop control of ignition timing for minimum brake specific fuel consumption.

E-17

Td = f (<I» (E.28)

6 = f (N ,<I» (E.29)

d 4 E (E.30)

6 = f (<I>, TT' P , f, h)

p 5 T where TT is the mixture temperature at the ignition event.

p is the mixture pressure at the ignition event.

T f is the residual exhaust gas fraction.

PyeCll) shows that Td is not sensitive to changes in T and P ; also Td t t was found to be virtually independent of engine speed N , but dependent on ¢.

E Consequently 8 varies approximately in direct proportion to N , and d E varies with ¢.

The pressure rise time T decreases with increasing flame p speed, which in turn increases with turbulence level and hence with engine speed. As a result, 8 is virtually independent of NE for fixed values p of ¢, T , P , f and h. The flame speed is strongly dependent on ¢ t t and T (29); it is also dependent on f(l1) and h( 13,44).

t Consequently the crank angle interval between the ignition event and the peak of the cylinder pressure is, from Figure E.2 and Equations E.29, and E.30: (E. 31) where, for a given engine: T and P have been assumed to be determined t t by Pm' T , CHT and h; and the residual gas fraction f of the charge by m ¢, Pm' P and Tm' e Rearranging, (E.32) For maximum n. we have 6~6 a constant, for variations in the engine 1 0 operating conditions: in particular for variations in the arguments of the function f6 of Equation E.32. Constancy of 6 under these conditions can only be achieved through variation of ignition timing t. The value of t=-r which establishes maximum torque and hence maximum n. in any o 1 E-18 operating condition is ca.1led Minimum ignition advance for Best Torque (MBT). Considering any variation in 0 about 0 at MBT to be itself dependent only on the arguments of f6' we may express the MBT ignition timing T as o (E.33) "Generally, the purpose of using a spark timing other than that for best power is either to control detonation or to make it unnecessary to re-adjust the spark as a function of engine operating conditions" (Taylor 13). Detonation is discussed in Appendix F.

The use of fixed ignition timing is the current practice in General Aviation piston engines.

Variation of n with each of the arguments of f2 in Equation

i E.27 is now considered.

EquivaZence Ratio and Ignition Timing: These two arguments are considered together because of their power- ful interaction in determining n.. Figure E. 3 (45) depicts the performance of a naturally aspirated Vo1kswagon automobile engine tested under the conditions: 1. Constant RPM .

2. Constant fuel flow rate m f 3. Air-fuel ratio and hence torque varied by throttling.

Hence Pm is not constant.

No indication is given by Reference 45 of the variation of P , T , CHT and h in Figure E.3. The parameter A is the inverse of e m E-19 equivalence ratio ¢ (A < 1 is a mixture richer than stoichiometric, A > 1 is a mixture leaner than stoichiometric). Variation of BMIP ( (which is proportional to engine shaft torque) and BSFC are shown along lines of constant ignition timing 'T. For mixtures richer than stoichiometric, BSFC and torque show a very weak dependence on igni tion timing; for mixtures leaner than stoichiometric they sho\\' a marked dependence on ignition timing. MBT timing establishes the upper boundary of the BMEP curves, and the lower boundary of the BSFC curves. With MBT timing, BSFC falls continuously as the mixture

is leaned, reaching a minimum around A = 1.3 (¢ = 0.77). No indication

of the onset of rough running is given on the curves of Figure E.3.

Figure E. 4 (16) depicts similar data taken with a Lycoming TIO- 541-E (turbocharged) aircraft engine, in flight at constant BHP and con- stant RPt-l; rough running regions are indicated. For these data, P m and CHT vary as shown; while variations in P ,T and h are not e m presented in Ref. 16. These data show a decrease in BSFC of about 18% from ¢ = 1 to ¢ = 0.75, along the lower envelope of the curves.

Since 35 spark advance was not established to be MBT (16), a further decrease in BSFC may indeed have been possible with ignition timing advanced beyond 35 BTDC.

Figure E.5 (16) depicts similar data taken with a Lycoming TIO- 541-E (turbocharged) aircraft engine, in flight at constant inlet manifold pressure and constant RPM; rough running regions are indicated.

For these data, BHP and CHT vary as shown; while variations in P , e Tm and h are not presented in Ref. 16.

E-20 I i I

I

!

i

Figures E.3-E.5 show similar trends in BSFC with variations in ¢ and ignition timing. These data suggest that, for a fixed set {N , (m or BHP or Pm)' P , T , CHT, h}: E f e m

I'

I 1. Lowest BSFC is obtained with ¢ < 1 and MBT ignition timing

I ~

2. For constant ¢ > 1: BSFC is not sensitive to ignition timing so that a wide range of ignition timings is essentially

I

"IBT.

I

3. For constant ¢ < 1: departure from MBT can result in large increases in BSFC.

The BSFC curves of FiguresE.3-E.5 show brake performance and therefore reflect variations in pumping losses and mechanical friction.

If the pumping and mechanical friction losses were removed from these data, and the brake performance thereby reduced to indicated performance, one would expect curves for ISFC similar in form to these BSFC curves.

Since n is inversely proportional to ISFC (Equation E.25), we expect

i (fOT a given engine) a variation of n. with ¢ and ignition timing similar to that shown in Figure E.6, for constant values of {NE,(m or BHP or Pm)' P , T , CHT, h}. The envelope of these curves f e m corresponds to MBT ignition timing. MBT ignition timing becomes progressively more advanced as ¢ decreases.

Throughout.the following discussion, and in keeping with Equation E.27, indicated thermal efficiency will be considered to be a function of Pm rather than ro or BHP. The following notation is f defined: E-2l

n! = indicated thermal efficiency for an equivalence

ratio ~, a set S'

= {Nt pI P' T' CHT' h'} and

E' m'. e' m' , , MBT ignition timing 'r~. A curve such as that shown in Figure E.7 (suitably adjusted for compression ratio and engine geometry) is appropriate to every General Aviation piston engine. Note that n! is a simple function of equivalance ratio ~.

n' = equivalent constant volume fuel-air cycle indicated

o efficiency corresponding to ~ and S'.

n- = indicated thermal efficiency corresponding to

equivalence ratio ~, a set S = {N , Pm' P ' Tm'

E e CHT, h}, and ignition timing 'r. S ~ S'.

= equivalent constant volume fuel-air cycle indicated efficiency corresponding to ~ and S.

Variation of the operating conditions from the set S' to the set S, and in the ignition timing, results in:

an" an-\

an-, 1 dN + 1 dP 1 dP +

n = n!

i 1 ~NE S!¢> E ~p m S' ,¢> m + ~ S' ,¢> e n an- , an-, a -, + __ 1 dT +

a (~HT) d (CHT) + ~ dh

aTm S',¢> m S',¢> S',¢>

n

+ _1_ dT a -\

(E.34) + (higher order terms) aT S',~ E-22

where dN = NE-N etc., and the partial derivatives are evaluated

E E

for the conditions (S' ,¢).

When MBT ignition timing is employed, the constraint Equation E.33 applies. Considering this constraint in conjunction with Equation E.34 (and neglecting terms higher than first order therein) we may write:

an. I

+ ani I dP + anil dT

+ + apl dP

n· = n!

m 1 1

W- e w- m

m S' t+- L ,'¥, 0 e S' t+- L m S' t+- L • '¥. 0 • '¥. 0 (E.35)

+ ani I d (CHT) + anil dh

a(CHT) s' ¢

Clh S' t+- ,'¥.L • • L 0 o where the subscript 1" is used to indicate that MBT ignition o timing is maintained during each perturbation.

Following is a discussion of each of the perturbation terms on the right of Equation E.35.

Engine Shaft Speed: Figure E.8 shows some data from References 11 and 13 on

the effects of engine speed on n.. In both cases fuel-air ratio

t was constant and MBT timing was used. According to Pye (11): "an increase or decrease of speed as much as 20 per cent. above or below the normal speed of an engine will have a very small The variation in n. which does occur effect on efficiency".

with change of speed is the result of the collective contributions of: t The use of MBT ignition timing is implied rather than explicitly stated by Pye(ll).

E-23 (a) Decreased heat loss to piston, cylinder walls and cylinder head during combustion and expansion, due to decreasing time for heat transfer as speed increases, (b) Increased rate of heat transfer to piston, cylinder walls and cylinder head, due to increased scouring action of the gases (turbulence) over the metal surfaces as speed increases, (c) Varying effect of the fixed valve timing with speed changes.

The speed variations encountered in General Aviation piston engines in cruise are typically NE ~ 300 RPM, with NE in the range 2200-260n 'RPM, The percentage speed variations are therefore within 15% of the midrange value N , E In this study therefore, variations of indicated thermal efficiency n. wi th changes in engine speed are ignored when t-1BT timing is employed: Cln. \ 1 = 0 is assumed.

Cl~E S',¢,T o InZet ManifoZd Pressure and Exhaust Back-Pressure: Figure E.9(a) shows data from Reference 13 on the effect of inlet pressure PI ~ Pm On indicated thermal efficiency of fuel- air cycles, for various valuesof equivalence ratio FR = ¢. (fuel l-octene) and inlet temperature TI ~ T , Over the range 0.5 < m PI < 2.0 atmospheres, there is negligible variation in indicated thermal efficiency. These figures are supported for a real £-24 I i

j

I

I cycle by Taylor (13, page 131) wherein varying Pm from 28 to 20 '.l.

inches Hg absolute, with MBT, altered n. from 0.292 to 0.304: As an engine is throttled, there is a progressive rise in the proportion of residual exhaust gas which mixes with the

I 'I

fresh charge during each cycle. This dilution decreases the flame speed and with fixed ignition advance, resul ts in a dramatic fall

I

in indicated thermal efficiency: see curve 'a' of Figure E.9(b)

I

taken from Pye (I 1) "'!"! According to Pye (11): " ... the only way of

avoiding the fall of efficiency when a homogeneous mixture is throttled is the provision of adequate ignition advance". With t-fBT ignition timing, curve 'b' (wherein ignition timing is progressively advanced as the throttle is closed) of Figure E.9(b) first rises slightly (as does the quoted data for the real cycle of Tayler (13)) and then drops back to its full load value.

However, the variation from a constant value of n. with

throttling at t.1BT is slight.

The quantity of residual exhaust gas in the cylinder is influenced not only by Pm' but also by the exhaust back-pressure MBT ignition advance nullifies the influence of P on e n , as was the case with P (13).

i m Consequently in this study, variations of indicated thermal efficiency n. with changes of inlet manifold pressure and exhaust ...

'These figures were obtained on a CFR engine , 3 1/4 x 4 1/2 inch:

compression ratio 6:1, P =

30 in. Hga, Tm = lSOOF, NE = 1200 rpm,

$ = 1.13. e

ratio is constant in Figure E.9(b), ttlt is" assumed that equivalence a fact not stated by Pye(ll).

E-2S back-pressure are assumed negligible. when MBT ignition timing is employed: an.

i \

an

~ = 0 is assumed.

=

ar-

m S' .</l.l e S' .</l.L o o CyZinder Head Temperature: Discussing a typical heat balance for an engine of compres- sion ratio 5:1. Pye(n) states: "The important thing to grasp about the relationship between I.H.P. and heat loss to the cylinder walls is ... that even if it were possible to run an engine under truly adia batic conditions in which this loss to the cylinder walls was entirely suppressed, that would only mean an increase in the heat to I.H.P. of some 4 per cent. of the total." The majority of heat lost to the cylinder walls cannot be converted to indicated work even in this ideal case.

~e therefore consider that variations in Cylinder Head Temperature resulting from changes in heat flow raW from the burned gases are not indicative of significant variations in indicated thermal efficiency.

As a result of these considerations, this study assumes that indicated thermal efficiency shows no direct dependence on cylinder head temperature:

an· an. I

1 1 -- - ~ - 0 is assumed.

a(CHT) - o(CHT) SI .</l,L - o • !

In some installations, cylinder head temperature influences inlet manifold temperature T and thereby indirectly influences indicated m thermal efficiency. The effect of inlet manifold temperature T on m indicated thermal efficiency is discussed below.

E-26 I -,

I

Humidity:

I' The effect of humidity on indicated thermal efficiency is

I

I discussed by Taylor (13). In this study, humidity is not considered

I

to be a variable: all computations pertain to a dry atmosphere.

I

I: Hence h' = dh = O.

InZet ManifoZd Temperature: As a result of the above discussion, Equation E.35 is contracted to (E.36) The author ~as unable to obtain data showing the explicit variation

of n with Tm' as required by the derivative in Equation E.36. The

i following means was therefore adopted for computing variations ~f n. with T .

1 m Let R

=

no/n~ R n!/n'

=

(E.37) 0 1 0

=

Rl ni/n o E-27 Figure E.IO(a) taken from Taylor (13) shows the variation of R = (constant volume fuel-air cycle indicated efficiency)/

(constant volume fuel-air cycle indicated efficiency forTI =

O

T~ = 700 R ) with inlet temperature TI = Tm' The curves are

drawn for various values of FR = 4> (fuel l-octene) and inlet

pressures PI = Pm (atmospheres). Indicated efficiency is

apparently most sensitive to inlet temperature Tm with fuel- air ratios near stoichiometric, and with low manifold pressures. It is assumed in this work that Figure E.IO(a) is typical of General Aviation piston engines, and that it is typical for all temperatures T'. That is, m aR(4),P ,T )\ m m (E. 38) R = R(4),P ,T ) = I + aT dT m rn m 5' m where

aR(4),p ,T )1

m m a

!L

=

aT

aT n 4> =

FR 700 ] l T

[ =

m 5' atmos.

P'

=

PI = I

m O 700 R

Tl =

dT = T -T' m m m FIGURE E.lO(a) The small influence of PIon R is ignored.

Figures E.lO(b-e), also from Taylor (13), show typical variations of (indicated thermal efficiency)/(indicated efficiency of the equivalent constant volume fuel-air cycle) with compression ratio r, exhaust pressure p /inlet pressure p., equivalence ratio e 1 FIF ' and inlet temperature Ti(MBT ignition timing is assumed throughout).

c Comparing the present notation with that shown in these figures: E-28 I i I

I

!

P Present Notation: Figures E.IO(b-e)

e = Pe

P p.

=

m = F/F <P c T T.

=

m 1

I'

n· = n

I

For a given compression ratio engine. it is apparent that the effects of P /P mare negligible. and that the effects of <P and Tm are independent. Hence: aRI(<p,T) (E.39)

= R (<P.T )1 +

aT m 1 dT m o m $' ;r m $''[ o . , 0

where R = R (<P,T )1 is given by Figure E.IO(d)

o 0 m S' '[ • 0 I m)

aR (¢,T I is the slope of Figure E.lO(e)

aT m S' '[ , 0 dT = T - T' m m m

T' = 550 Rankine in Figure E.IO(d)

m It is assumed in this work that Figures E.IO(b-e) are typical of General Aviation piston engines.

Now n n' o 0 fiT n1 o 1 RI R

= -R-

o E-29 Therefore (E. 40) Equation E.40 is used in this work in the computation of n. for MBT ignition timing. For these computations: 1. n! is represented by a cubic equation (E.41) where the coefficients eo' e , e , e l 2 3 are constants (see Figure E.7) 0 0

2. T' = 550 Rankine = 305.556 Kelvin

m

3. dT = Tm - T~

m 4. Figures E.lO (a,d,e) and Equations E.38 and E.39 supply the bracketed quantities on the right hand side of Equation E.40.

Figure E.ll shows a typical variation of the quantity RIR/R (Equation E.40)with T , computed from the data of Figure o m E.IO.

SU17'U71ary of Effeatson Indicated Thermal Efficienay: Indicated thermal efficiency n· has been sho~~ to be a function of {¢,L,NE,Pm,Pe,Tm,CHT,h}.

r.

MBT ignition timing maximizes n. for all sets {¢,NE,P ,P ,T ,CHT,h}.

1 m e m Maximizing n. contributes to minimizing BSFC. In this study MBT E-30 j i

I

!

ignition timing is assumed for all modes of engine operation.

This assumption reducesn. to a function of <p and T··, given by 1 m Equations E.40 and E.41.

The contributions of <p,l andP to n. (Equation E.34) are I m 1 /i shown schematically in Figure E.12. The variations of n. with <p in the vertical plane A correspond to Figure E.6; while the variations

I

of n. in the plane B (constant ¢) are postulated on the basis of Figure E.9. It is postulated that similar figures will be

I

obtained when llP is replaced by either llN , llP , llT , llCHT m E e m or llh in Figure E.12, noting that an./aT I , O.

1 m SI If, l ,'t', 0 Summary of Indicated Horsepower Variations Combining Equations E.15, E.18 and E.23, the variation of air mass flow rate from operating point 1 to operating point 2 is: (E.42) Then, from EquationsE.12, E.24 and E.42, the variation of indicated horsepo\\er from operating point 1 to operating point 2 is: (l-E ) (l+E:p) t E P T P p n· NE m m e <P2 l 2 l IHP IHP

=

p- p

2 r-

I n.

N m m

~ e

El 2 l 2 (E.43) .)

E-31 Jhere n .. and '1 •. are separately computed from Equation E.40.

1l.2 . 1

LOST H6RSEPOW~~

The lost ,lhean effective pressure and hence the lost horsepower ~¥e detetmiri~a. by the energy required for pumping, plus that t~q'llited tdov~rcome mechanical friction.

"'-': ..

Losses of mean effective pressure due to pumping occur at .... ;. / : inlet and exhaust valves. Taylor 03) has for the inlet valve: (E. 44)

:: ]

fbr a giVen engine, where ~rep. is the mean inlet pressure during the inlet ~tt6ke, arid Z is the inlet valve Mach Index defined as: (non-dimensional) Z = [!?d] s,

c:-a

t(b/d) 2 30 C. IgyR 1 m = (E.4S) ."

:: cylinder bore, ft where b d inlet valve diameter, ft

=

t piston stroke, ft

-

S = mean piston speed = 2tN /60, ft/sec

E

C ~ fueari inlet flow coefficient

i-

a :!!:speed of sound at the inlet valve, ft/sec

E-32

g = gravitational acceleration. ft/sec

y = ratio of specific heats for the inducted

fuel-air mixture R = inducted mixture gas constant. ft. Ib/lbm. oK m

Z Ra = gas constant for dry air (Equation E.16)

C - constant

z

Figure E.13(a) from Taylor (13) shows a typical relationship represented by Equation E.44. The effect of P /P is negligible e m (Pm = Pi' P - Pe)' Linearizing this curve gives the expression: e (E.46) We expect an expression similar to Equation E.44 for the exhaust valve. Taylor (13), instead of defining an exhaust valve Mach Index Ze' expresses the exhaust MEP in terms of the inlet valve Mach Index: (E.47) for a given engine. The temperature and pressure at exhaust valve opening, which are "chiefly dependent on the volumetric efficiency, the fuel-air ratio, and the compression ratio" (13) have been characterized by Z, P /P ,F (and compression ratio, which is here e m not included for an engine of fixed design). "In spark-ignition engines, variations in fuel-air ratio are generally within the range in which . .J E-33 the effect on pumping losses is small" (13). The effect of varying F on the exhaust gas temperature, and hence on the speed of sound at the exhaust valve, is thus taken to be small. In the previous discussion of volumetric efficiency, it was determined that the effect of P /P on n was small for the engines . m e v here discussed. Hence it is expected that the effect of Pe/P m in Equation E.47 would also be small for these engines. Consequently we may write MEP (E.48)

Pee = fe [2]

where the exhaust valve flow characteristics are expressed approximately by the inlet valve characteristics.

Figure E.13(b) from Taylor (13) shows a typical relationship represented by Equation E.48 for an engine in which the effect of P /P is not negligible: these curves have P < P. Taking the e m e - m form of these curves to be general, we may linearize Equation E.48 to: k > 0 (E.49) e for application to General Aviation piston engines.

Combining EquationsE.46 and E.49, the total lost mean effective pressure due to pumping is: PMEP = MEP MEP.

e (E.50) E-34 From Equation E.50 it is clear that: (a) Increasing inlet manifold pressure P m decreases pumping losses, (b) Increasing exhaust back-pressure P e increases pumping losses, (c) Increasing engine speed increases both inlet and exhaust pumping losses.

Mechanical Friction The discussion by Taylor (13) permits the approximate representation of lost mean effective pressure due to mechanical friction: (E. 51) Total Lost Mean Effective Pressure and Lost Horsepower Combining Equations E.SO and E.Sl, the total lost mean effective pressure is LHEP = PMEP + MMEP (E.S2)

I

(E. 53) The lost horsepower is then:

LHP = (LMEP) DN /45S.33 (E.54)

E 2 3 for LMEP (lb/in ), D(ft ), NE(RP}'O.

E-35 Lost Horsepower Based on the Motoring Test Taylor (13) states: "The mechanical friction mep of an engine can be measured by measuring indicated and pumping mep with an indicator and the bmep by means of a dynamometer ... Friction measurements by means of indicator diagrams are rare, and in most cases the basic data must corne from the results of motoring tests ..• It has been shown that motoring-test results are a reasonably accurate measure of mechanical-pIus-pumping friction when imep is in the range of 100 psi and, in the case of four-stroke engines, when Pe/Pi is nearly 1.0.

Thus in estimating friction for supercharged or throttled engines, in which these conditions do not hold, suitable correction factors must be applied to motoring-test data."

In the absence of data taken with the engine firing, it is not possible to evaluate the constants in Equation E.53. An equivalent expression for the lost horsepower, based upon motoring-test data, is obtained as follows.

Taylor (13) shows that a reasonable estimate of LMEP for a firing engine is:

~ffiP = LMEP + x (P -P ) + y (IMEP-lOO) (E .55)

oem where LMEP is the result of a motoring test (with P and P oem near one atmosphere). All pressures in Equation E.55 have units of lb/in .

Values for x and yare given in Figure E.14(13), from which it is apparent that: E-36 I i

j

I

I

x = 1 - k Z

x (E.56) where k constant > 0 = x = constant > 0 Yo

I '

k = 2 k 'i./60 = constant > 0 yn ys The lost horsepower of the firing engine is then:

I

LHP = (LMEP) DN /458.33

E

= LHP + DN [x(P -P) + y (IMEP-lOO)]/458.33

o E e m (E.57) (IMEP-lOO)]/458.33 where LHP = the lost horsepower obtained during the motoring test, o with P ~ P ~ 1 atmosphere.

e m

= (U1EP 0) DN / 458.33 horsepower

E LMEP, P ,P and IMEP have the units Ib/in .

e m The motoring horsepower LHP may be represented by a quadratic o algebraic equation in engine speed NE(RPM): (E.58) where the coefficients a ' aI' a are constants. Representative o motoring horsepower data for General Aviation aircraft piston engines -, are shown in Figure E. 15 (28) .

Equations E.57 and E.58 are used in this work to determine the Lost Horsepower in all operating conditions.

E-37

l

FUEL METERING SCHEDULE Fuel metering requirements for spark ignit~on reciprocating internal combustion engines are discussed by Obert (29) . Figure E .16 taken from Reference 15 shows the fuel-air ratio used by the Curtiss-Wright TC18 Turbo Compound Engine.

A rich fuel-air ratio (¢>l) is required during idling, decreasing to a lean fuel-air ratio (¢<l) requirement for medium-power operation. The fuel-air ratio must be enrichened again at high power levels.

Figure E.17 (from Reference 23) shows the mixture schedule used by the Beech Single Lever Power Control system. While the previous Figure E.16 carries air mass flow rate along the abscissa, Figure E.17 shows an abscissa of percent rated power. Since air mass flow rate is related to IHP by Equation E.ll, these two representations are essentially equivalent.

While a constant lean fuel-air ratio is appropriate during cruise below about 75% rated power, richer mixtures are necessary at higher powers for three reasons: -1. Full power can only be developed with a rich mixture.

"Best Power Mixture" at wide open throttle (indeed, at any constant air mass flow rate) is a fuel-air

ratio of approximately 0.08, ¢ = 1.2 (11, 23), with

MBT timing.

2. Excess fuel is required to provide cooling for the engine.

3. A rich mixture is required to avoid detonation (see Appendix F).

E-38 For studies of engine performance in this work, the fuel- air schedules shown in Figure E.18 are used. The abscissa sca.1e is the mass fraction of dry air consumed at some specified Fuel Schedule Datum condition (see below). Schedule A represents cruise operation near best power mixture, enrichening to a fuel-

air ratio of 0.084 (¢ = 1.25) at maximum air mass fraction

(cf. Figure E.17). Schedule B differs from Schedule A at low values of the air mass fraction, representing the Desirable Schedule of Figure E.17; while Schedule C gives a constant lean fuel-air ratio in all operating conditions.

Humidity will affect metered fuel-air ratio in a manner determined by the installation. Humidity is not considered in this study.

COMPUTATIOr-< OF NATURALLY ASPIRATED ENGINE PERFORMANCE The procedure used here to compute the performance of a naturally aspirated engine at a prescribed operating point requires the specification of certain engine characteristics; a Reference Operating Point Condition; and a Fuel Schedule Datum Condition.

Required Engine Characteristics The following characteristics must be specified for the computation of engine performance: 1. Engine displacement,cu ft D -' E-39 2. Fuel metering schedule F (x)

F = fuel/dry air mass ratio

x = (dry air mass flow rate)

(dry air mass flow rate at the Fuel Schedule Datum) 3. Coefficients of the cubic Equation E.4l 4. Manifold temperature pertaining to Equation E.4l T' m

s. aR I versus ¢ (Equation E.38)

aT m 5' .

6. R versus ¢ (Equation E.39) o 7. cR (Equation E.39) l

ar-

m 8. Motoring coefficients (Equation E.58) 9. LOst horsepower coefficients (Equation E. 57) k ,C..,.

x '"' 10. Volumetric efficiency correction indices (Equation E. 23) Reference Operating Point The performance of the engine at the Reference Operating Point (den?ted by subscript 1) is completely defined by the above char- acteristics and the following set of mutually consistent operating parameters: 1. Inlet manifold absolute pressure P inches Hg m l 2. Inlet manifold temperature T deg. K m l 3. Exhaust absolute back-pressure P inches Hg e 4. Fuel/dry air mass ratio Fl 5. Brake horsepower BHP horsepower 6. Engine shaft speed RPM N El E-40 When values for these parameters have been specified, the remainder of tneengine performance at the Reference Operating Poi~t may be computed as follows: 1. LHP Equations E.S7, E.S81 Iteration on I IMEP 2. lMEP Equations E.2, E.S IHP l' l 3. Equations E.40, E.4l n.

.

4. ID Equation "E.IO f .

5. m m

=

IFl a fl l 6. Equation E.17 Pm 7. Equation E.14 nv Fuel Schedule Datum The Fuel Schedule Datum condition (denoted by subscript fsd) is nominally Wide Open Throttle at maximum continuous RPM at sea level; but it can be any other desired condition.

The dry air mass flow rate corresponding to this condition may be computed from a knowledge of the engine performance at the Reference Operating Point, and the following set of parameters: P inches Hg· 1. Inlet manifold absolute pressure mfsd deg. K 2. Inlet manifold temperature T mfsd P inches Hg 3. Exhaust absolute back-pressure efsd Engine shaft speed N RPM 4.

E fsd E-4l When values for these parameters have been specified, the corresponding dry air mass flow rate may be computed as follows: -(" !

1. Fuel Metering Schedule F(x) at x = 1

F fsd 2.

Equation E.17 P - mfsd 3. Equation E.23 (using the Reference Operating n - vfsd Point value n ) vI .

4. m Equation E.14 afsd General Operating Point Utilizing the computed performance at the Reference Operating Point and the Fuel Schedule Datum, the performance of the engine.

at any other operating point (denoted by subscript 2) may be computed by specifying the set: Inlet manifold absolute pressure P inches Hg l.

m 2. Inlet manifold temperature T deg. K.

m 3. Exhaust absolute back-pressure P inches Hg e 4. Engine shaft speed RPM NE follows: The computation of the performance proceeds as Equation E.17 1.

Pm 2. Equation E.23 (using the Reference nv ) Operating Point value nv .

3. Equation E.14 m a -(

4. m 1m

x =

a a 2 fsd Fuel Metering Schedule F(x) 5.

F2 E-42 Equation E.20 6.

¢2 .

7. m

=

Fil

f a 2 2 E.40, E.41

I Equations

8.

n· I :1 E.10 Equation IHP 9.

I

I

Equation E.5 10. lMEP

I Equations E.57, E.S8

I!. LHP

I

Equation E.2 BHP 12.

E.8 Equation 13. BSFC Equation E.3 14. Torque Q E * * * * * * * * * * * * * * * * E-43 TABLE E.1 PRIMARY INFLUENCE OF CONTROLS ON ENGINE OPERATIONAL PARAMETERS Propeller Flight Pue1 Variable Spark- Throttle Induction Air Cowl Flaps Turbine Waste- Engine Governor Altitude Plow Advance System Heater and/or Gate & Nozzle Oper'!

Geometry Control Lever After-Cooler Paramo F X T X .

P X X " m X X T X IJ:I X X X X X CIIT P X X e X T X X X e X NE X X X X Q[ h X

INDICATED WORK

~r<EA(A~C)

I

PUMPING WORK I

AREA (.8 +c)

I

L....--_..l-- _______ -.... _.-.... ___ V

F,GURE E.I TYPICAL PI.ES5Vf.E - VOLlJME. CYC-U :bJIlG£.AIl1 fo~ A

NAfvt.{fUY AS,f/fAT£1) AIR.t..t.Aff ENGINE..

TDC

P.

~I

CRANK ANGLE

,

//

-' £I5E 1NT£R.VflL

'DE.LAY INre,.wtL

fLRr~£b eRRH/( AN6L.£ ~ ELAPsE}) CRANK. IINGI..£ f)t> fLAf!£b Tt,.,E ~ £LAPso liME. r,.

IYPlc.RL -r"ACE ()J: CYLIN1::>£R. ~E.S.s OR/:. VERSUs

F'GtJ{(E E .2

cfll NK liNGLE..

E-45 b. [g/PSh]

BSFC

B~1EP 350r---~-~-""""---""""'-----

(p/CM . 7 t--~4--~

6 .

. n = 2500 U min

Q= 33 [mm /Asp·Zl tTl I ~ Q'\ ,r-----~------~--~~--~~ n ~ 2500 U/mtn ZZP.20°I<Wv.O.T.

Q:I 33 [mm /Asp·Zl

.. I

. . ., 3 __ ~~~ __ ~ __ ~ ____ ~ __ ~~ 150~~~~~~--~--~~~-----J 0,0 0,9 ',0 1,1 1,2 1,3 1,4 1,5 0,8 . 0,9 1,0 1,1 1,2 1,3 1,' 1,5' . ----).

X

A = AIR FUEL RATIO

STOICH. AIR FUEL RATIO

NOTE: FUEL QUANTITY KEPT CONSTANT I' AIR QUANTITY VARIED BY THROTTLING.' SINGLE SPARK ',IGNITION, r , c- "EF. .

FI£;URE E.3· TYPIcAL EFFccrS OF FUEL-AIR. Rltrio AN)) IGNI-r,ON T:lfY1ING 0# °'ERF()~AW"E. (" 45) .--------.---.--~--.---.-.1 ~ 1~r-------------~--'--------------' • E t:.

r:-:====-=-+ oX ~ 1600

~

~ 0- S 1!!OO ~ T\ II.

-

~ • ~ 0- 1400 0.6

X 10"} FLY 251

+31)- o 2S-} FLY 2S1 'il 3S-

rn

.

~ ~ 35 .5 25~_---,,""=- __ ~-----:-L:----...,.L,,--~.

0.6 1.1

Leanout Curves for 2400 rpm, at 15,000 ft, Constant Power = 55J, and Several

Ignition Timings (---Unstable Operation, Roughness) A- X ...

.

~ !

E

c w '" ~ ~ ...

w VI ~ ...

:n

0 t x: (j"\ ~ w ...

:w: c:.

....

w ~

... 100 1500

~ '" ~ w Z

rn iii

tTl .

"" ;;) , ...

~ 0.6 1400

\1\

X 20" ~ FLT 251 + 30· -\!

A- o 25° FLT 251 l: I V 35· ~

Y Z'

§

::J at '" Z l: 0.5 u .!: , -' w ~ ...

'" ::> V1 !:l '" W ...

...

A.

V w a ...

....

'" 0 t!

~

~ ~ 0.4 1.1 0.6 <I> Leanout Curves for 2400 rpm, at 15,000 ft, Constant Manifold Pressure = 27 in. "g., and Several Ignition Timings (---Unstable Operation, Roughness) I i I

I

SCHEMATIC.

I

I TYPICAL VliRIAlioN.5 of IN:I>icAr£J) THERMAL EFFie/ENe. Y

WrrH E!JvIVALENCE fAlIO Mob 1G,·"r/ON "filING

I

I

I

IND't:.AT£-l> iHfJ?MAL.

EfF IC,ENe. Y E,NE..LOPe. C,,;t.."E

/'

MBT IGNITION "lffINC, I CDHST'IIHT :

I

N f m; Dr 13HP tIf' 1;

I

~

Tm

CHT

h

(

1.6 0·6 1.0 1.2 1.4 EQUIVALENCE. RAffo ~ IGrtrnoN n",''''6 7: .b£~~' BibC.

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t

Ii: ill '\:! :ld ::\1 ljl Illi 11111lililli ili:d i· ;jJlJi ~~l lllUliIU., J lilJllilitlli jll! \.:j Jl :~·Il:::i::i: :;)' ;Jj il!1 J Ii);: iJ11IL!III:!lilllllililill tlilitl Iii Ii :[11 'II dHlllli uill

~

'f',1\ IiL .'111'1 OJ LJ j~.~J \I t J .LH 1J>f £[ S r 9v , Vi)~')..~1 t13J.JWL1N3:J 3HJ. 01 01 X 01 :l"H ~....,,; ~.

,../ '-

-

I:::· ...... , ..... .

r-~--:-~rii t: L ......•. _ ........ ___ .. _.

i r:' . i'3!

·~~~~~.~.:-~,~::._:~.~~~~.t·,~·~~-:·~·:::~·:~_·.:t:.·~_::J·}·.~~;]:·1:;::t-~j:I::t.·~.11·r:~j·=-~:t~~:~I:.~~I~~~~--:-_:::l:.·:·~-~:·.:.:~.:t.ll··j'~:.·~:.~.·~·::I:.'~::~l.±.::::~~!:::::Ir=~::~··~~~~·~·~·~·=-·~::~·t:~·:~:~:~: :~·:~-~·:~::·~·~·:··::·t::·::~·~·=:·: .. ~~ :. . ~~. :.: . . : : .: .. : ·:::::::=1::::::·::~:f·:=:::::::~-·-·-·-·~-·-·--·-· -.~ z· r--·· .

'.

t.

L ...

f······-· g':: .. :: E-Sl '32 C::=====t""--r---r-b~-"""-"""=:::::::I'32 ....

~ '30 ~ >- -+---i---i---::::.IrIC-..;...--t----i·30 1.051---+-";- 'r2~ c::a~ 1~~ 1.00 .~- '28 < It-+--~~--t_---I!---__f----i·28 \.,)14.1

~

0.to'--~1.0-~I.o:---::St-::.0--f:4.0:---=5"".0 --i..

a F---+---t---+----+---+-----I·Z6 ~, Jtr""Q!P>aE~ PERCENTAGE OF FULL LOAD VARIED BY iHROTTLE

(a)

c

REF. 13)

40 SO. 60 70 80 90 100 ( 'P~ 82

( b) ThBrmal efficiency under throttled conditiooa. Speed. 1,500 r.p.m. Com·

~ ratio I): 1. (0) Ignition fixed .. for maximum power at full throttle, IIlId (b)' ignition adjusted for maximum power at each throttle eetting.

FIGU~E E.9

1.0r--""T"""--,----,.--.

1.0 -.j

1 J

0.8~-:~~~~~~ 0.8

J i I r J I

!-- ~0.6 'IF, - O.gl. 1.0.1.175. 1.43- 0.61---t- 'I'. - 1.175 .,.

0.4 r- 6 0.4

"i - 55O"R

Ti • 550" R. 6!iO" R ",,- - 1.10 0.2

I 'I I

o 1.05 3 4 5 6 7 8 9 10 11 r

(6)

1Jl.oorrt~~

1.0 1.0 0-"1--"'-+--1 ,·-4 'II;,

.... .~

-"" , 1.175 0.8 ~~ 0.8 ::2 r== '.-= ~ " \0,91 ~ o.~ 100 0.6 J> 0.6 r_6 ~ Ti _I5O"R 0.4 0.4 !--

I- "''''1- 1.10

P. 'I' - 1.10

0.2 0.2 t--

· i

o

REF. 13)

0.7 0.8 0.9 1.0 1.1 1.2 13 1.4 1.5 ( (J) FIFe ~( B2.

Fie 5-21. Comparieon of efficiencis of actual cyclee with efficiencieB of equivalent fuel-&ir cyclEll!-1p&rk-ignition encines: '10- efficiency of equivalent CODBtant 'fOlume fue1-&ir cycle with octane;" - indicated efficiency of eFR, 3~ x 4~ in engine, 1200 ,,_ rpm; fuel, gueoU8 butane, CaB.. (Van Duen and Bartas, ref 5.21) (~EF. 13 ) po.~ 134) .;).

FI GURE. E. 10

E-S2 --------- ---------------------------~--------- II ~ II~ 'I( 10 TClTHrrftlTII'.HTfq ,1 '-, p·,11 t 1 ,. " ~ I ." • I I ,~ ref' I I .• ". ' 'I' • I

"'

U1 ~ StHEMArlC

PoS1'tJLAfE.~ iYPICAL VA'RIA1'iONS OF IH1HCltTEb mEJeMAL EFFICIENCY r'ji

WITH ¢) r AND ~

,It

ENVELoPE ctJ~vE.

ENVELoPE UJWE£ )Y}.

'YJI

filS, ibNlilON ,/MING £: ~pl. = 0

\ I'rI ,

\,,, s¢r

~ £,1 J)O

~--rl.'l

VERtiCAL PLANE A

::

N'

N

CONSTANT : E E

pI

::

e m

,<;.

nft1ING :: ,eN 1-r,D"" 't .l>EG~EES BTl>c.

r..'

r: e

4! 4! 'Z"'. < < 't, L, t"3 ?:s

::. T'

...,

~

.v,

I

CHT = CHT

hi

':

h

FIGURE £.12

E-S4 I !

, I

I

I

!

1.0 ., , :--""'0

I 6'

~.

I fl- 0.8

Jea.

.5 I

~

I I ,

~

0.6 "\ 0.2 0.4 0.6 z Fig 9-19. Ratio of inlet-stroke mep to inlet pressure: CFR engine 3U x H-g in; r - 4.9; T, - 580°F; P./Pi - 1.0,0.5, and 0.25; 'Y ~ 1.2. (From indicator diagrams taken by Livengood and Eppes in connection with ref 6.44.)

(Q.)

(~EF. 13 , r~e. 342)

I Pc/Pi '-- - J 0.25 V- I I / O.SO

L 101

/

L

/ V 1.0 / .J1-" ~, ....... !""'"'"""'" ~

-

0 0 0.2 0.4 0.6 0.8 1.0 1.2 Z Fis 9-18. Ratio of exhausWtroke mep to exhaust Pl"Ellll!lU'e: CFR engine, 3~ x 4~ in, r - 4.9; T. - 580°F; p.l,. - 1.0,0.5, and 0.25; ., ~ 1.2. (From indicator diagnuns taken by Uw:ogood and Eppes in connection with ref 6.-44)

(b)

F'6URE E ./3

E-55 1.0 r-.

I':

r-

0.9 -r-.

r--

"-

0.8 ~Si5~.0 (a.)

-

r--;r-,

---

0.7

'"

.-

\0 ~

"

i 0.6 a.

l'..

~ i" 0.5 ~ .5 0.4 >t

~

0.3 o GrisdIIt ODd FIIoc*. '" uo .p', o CfR enciM. ~. rei 6.44 0.2 r--

-.....;,~ 1. - •. PIyInoutIt 1941 til;. tIInIIIIIII. rei 9.714

l> li-cyfinder MrIft ..... IIri*I _ 0.1 .. "i...

o 0.1 0.2 0.3 0.4 0.5 0.6 Z 0.101-+--+--+--+--+-+-+--1

(6) :e 0.081-+--+--+--+--+-

I

i 0.06 1--+--+--+--+=",""",,-+--+---1-

.5 0.04·1--~,.;oo::::-+--+- ~"'-~-+-----~--+---1 >.

Motoring test correction factors: fmep - fmepo + z(P. - Pi) + y(imep - 1(0). y taken from Fig 9-10; :z: from motoring testB. (See Fi, 6;24 for "y.)

F,GURE E.14

) £-56

=f- ·i\ . .-.- OBTAINED FROM: t= = ...... '='. V.:.E .~~, .=

= = .. V.::.o:: APPROX/lt1ATUY WIDE. OPEJJ THROTTLE. = ~~_ - ~

II/lffORING TESTS AT APPROXIMATELY SEA LEVEL.

= 7!":t: = ---r' .x/- ~_1: ...

--

--l=: ~f'\- .- :r-< .

_. ...

--;.

f -~ ....

-:-:::= ~-- ' .. ~:-:: ·t~ f~ .. ~_.--:.l' - ::::: =:: -- .- .

:;::::- .. :.~I=- -=1'_:1::~

... -

:~-·-i " ~- ----+-----

_.- =1':_-'·_-=

- -- - .. -~ .". -- ..- .-

--+-- --"' __ L~ • • .... __ 1=:._.: ~- :f- y=

-C. ( REF. 28 )

FIGURE E.15

E-S7 TAKE'()ff,\ POWER ENRICHMENT

VAlVE OPENS \Q.lMB 1

AUTO-RICH POSSIBLE

LIGHT ---'iii

DETONATION ::§1 AUTO·LEAN

o 2 4 6 . a 10 12 14 16 18 20 22

AlRFLOW- THOUSANDS OF lBS./HIt

(eEl:, 15) fDje 17)

FIGURE, E.16

E-58 '<' tTl I V1 \0 .- --0--- ---~ .--' :.--+-

~.::' .. ~' ::~ji~~~:j~;~~~; ;::~~ ~ ~::3~'§:~ ~~~~;~~~~: ~:~~~~iti:~i~~~l~if:;~;?h: ~

[::;L_~:.· .::~;:F~:::~~r:~.:.:::...· ~=:;:=r.=::.. ::=~-=-:§~_-=i~ :"':;': --: ... _=t~=~:.::: <=::::::.:.j..:.:, · .. ·:=I~=.:::f-*:.~~:;?L~·;~~;::!::: t~

L~:~:I:::::::~J:~=:~: ~E,--:.=~:=:c - _=+=== f=-'-:"-:: ---t= __ E:f:~~X:~::~Y: :S··

~::~:=:c:::~::::=~T=·:~::·~.E - .:_. I-:-.~ -:t::c::=" . ...:.:.~ +i~

~::;u:u:I~:~~~~~~=~;;~~C==::~ ~~~ =:i~~;~l

.. _.- . ... -.

. . ~A 1-:-- ..... ..c. •. -.- .. --<--:.::::t---===f-'--- .... _.= __ -+- ___ .• ..c.:3-=:t .. :=±=- ____ ._._~c .•.. _ ..... ~ C) ,.. ~" ':is:''' .... - .... --- - ---. .. --.. =' - .=:::~ ... =~-. . . ..... .

f:~~ .~;~:J[~=;:~~:~;j ,~u ===~:c~ ;

::t ... --.·-.· .. u~.~.~..u+~~~~~;~l=~~~~;;.~ ~.: =::±;~.:-~;:~ .~

--::1.:;:~:~1===f~:~: ====-~~ ·fCr-::= ::~~i=.:·:~~~~=::--~~ :::.=:-- ~=~~~~: t-=~::::i:~~· r-"-e .. ~ : ... ;: :~:::::t~:::~=~~c-=-::~:§:-~::::~~= ::::~::-1.:~==f~:::~-.-:~~~ - :==--::=i=:== =~.::::~:~::::: • ::::~~~::. E~ :.

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APPENDIX F

APPENDIX F AUTOIGNITION, DETONATION AND KNOCK IN SPARK-IGNITION PISTON ENGINES Table of Contents DEFINITIONS ...........................•.................... F-l FACTORS INFLUENCING THE OCCURRENCE OF KNOCK ................ F-2 ENGINE PERFORMANCE MODELLING.. . . . . . . . • . . . . . . . • . . . . .. . . . . . .. F-3 c

APPENDIX F

APPENDIX F AUTOIGNITION, DETONATION AND KNOCK } IN SPARK-IGNITION PISTON ENGINES DEFINITIONS The phenomena of autoignition, detonation and knock are dis- cussed at length by Obert (29) .

Autoignition is a spontaneous chemical reaction (oxidation) in the unburned mixture, ahead of the flame front in the combustion chamber. This reaction may be either explosive (usual) or non- explosive.

Knock is the noise accompanying autoignition. According to Obert (29): In general, knock is the term used to signify any unusual sound that arises because of autoignition in the combustion process. In automotive work, borderline knock is defined as audible knock apparent in a quiet test room. In aviation work, such borderline knock would be quite inaudible . . • Here vibration pickups are attached to the engine and, quite arbitrarily, a certain level of indication is specified to be objection- able knock.

. . • A detonating wave has been proposed as the mechanism for explosive autoignition ••. It woul d be well to . . • explain that the terms detonation and knock are used synonymously by most engineers although, to the physical chemist, de- tonation is a unique propagation of combustion by a shock wave at superacoustic velocity.

A complete understanding of autoignition phenomena has not yet been reached. It is well recognized, however, that severe autoignition is destructive in an engine. This is especially true in aircraft engines where light structures are used.

F-l FACTORS INFLUENCING THE OCCURRENCE OF KNOCK Amongst those factors which influence the occurrence of knock in Spark Ignition (SI) engines, Obert (29) lists temperature, density, time and composition factors here quoted.

\ A. TEMPERATURE FACTORS. Increasing the temperatur·eof the unburned mixtu.re by any of the following factors will increase the possibility of knock in the SI engine: 1. Raising the compression ratio ..

(a) Supercharging 2. Raising the inlet air temperature 3. Raising the coolant temperature 4. Raising the temperatures of the cylinder and combustion-chamber walls (a) Opening the throttle (increasing the load) 5. Advancing the spark timing . . .

B. DENSITY FACTORS. Increasing the densi tyof the unburned mixture by any of the following .wi 11 in- crease the possi bi! ityof knock in the SIengine: 1. Opening the thrott1e (increasing the load) 2. Supercharging the engine (a) Raising the compression ratio 3. Advancing the spark timing C. TIME FACTORS. Increasing the time of exposure of the unburned mixture to autoigniting conditions by any of the following factors will increase the pos- sibi1ityof knock in the SI engine: 1. Increasing the distance the flame has to travel in order to traverse thecomhustion chamber 2. Decreasing the ·turbulence of the mixture and thus decreasing the speed of the flame .

3. Decreasing the speed of the engine, thus (a) decreasing the turbulence of the mixture .

(b) increasing the time available for preflame reactions D. COMPOSITION. The properties of the fuel and the fuel- air ratio are the primary means for controlling knock, once the compression ratio and engine dimen- sions are selected. The probability of knock is decreas ed by L Increasing the octane rating of the fuel • . .

.2. Either rich or lean mixtures . . • 3. Stratifying the mixture so that the end gas is less reactive I ./-- 4. Increasing the humidity of the entering air F-2 ENGINE PERFORMANCE MODELLING No attempt is made in this study to either predict the occurrence of detonation or to model its effects on engine per- formance. It is assumed that detonation-free operation prevails at all times.

In justification of this assumption, the flight test experience of Reference 16 is invoked. In those experiments, fuel-air ratios, ignition timings and manifold pressures were employed which were beyond the domains of current General Aviation engine practice.

The latter two resulted in the simultaneous occurrence of: 1. Advanced spark 2. High inlet manifold pressure 3. High inlet manifold temperature 4. Moderately high cylinder head temperature.

Each of these conditions is conducive to detonation. Nevertheless Chirivella (16) states that detonation was not observed: During the initial flights and at high power settings, detonation equipment was used to monitor the engine operation • . . It was soon realized that the techniques used to gather the experimental data were not detonation-limited.

The detonation equipment was then removed from the ai rcraft.

The engine used in these experiments was a Lycoming TIO-54l-E.

The absence of detonation in the flight tests of Reference 16 is probably largely attributable to the use of low fuel-air ratios in conjunction with items 1-4 above. Figure E.16. taken from Reference 15, shows how lean (as well as rich) fuel-air ratios in F-3 the Curtiss-Wright TCl8 Compound_ engine penni tted higher air mass flow rates than would have been possible with a stoichiometric mixture, due to the shape of the detonation boundary. In general, detonation is most probable with fuel-air ratios in the vicinity' of stoichiometric.

However, while- spark advances from 20° BTDe (standard for the Lycoming TIO-54l-E) to 35° BTDC were used in the flight tests of Reference 16, the spark advance for maximum torque (MBT timing) was not identified. Obert (29) states that "maximum power [torque] is obtained wi th the usual 51 engine (and fuel) when the spark is adjusted to the point of audible knock." The use of MBT ignition timing thus commonly corresponds to the. presence of some level of detonation. Some detonation may therefore have been encountered in the flight tests of Reference 16 had the spark been further advanced to MBT.

The assumption of MBT ignition timing in this work, with its attendant fuel economy advantages" is made in- the knowledge that such an operational mode may approach an autoigni tion condition.

F-4 NOMENCLATURE APA Airframe-Propeller-Atmosphere -- ( b Tailplane span, ft t b Wing span, ft w BHP Brake Horsepower Bt-1EP Brake Mean Effective Pressure BSFC Brake Specific Fuel Consumption c Brake specific fuel consumption, lbm/BHP. hr c Mean aerodynamic chord of the wing, ft c' Shaft specific fuel consumption, lbm/SHP.hr Airframe power-off drag coefficient CD C Airframe power-on drag coefficient DON C Airframe lift coefficient T ...

C Power coefficient p C Torque coefficient Q C Speed-Thrust coefficient R C Speed-Power coefficient

s

C Thrust coefficient T CAS Calibrated Airspeed OIT Cylinder Head Temperature d Propeller diameter, ft dh Increment in center of gravity position h Airframe drag (power-off). lbf DOFF N-l Corrected airframe drag, lbf Airframe drag (pow.er-on), lbf Number of engi'nes ,each driving 'one propeller EGT Exhaust Gas Temperature Compressibility correction factor Slipstream interference factor Propeller J-factor Fuel-dry air mass ratio of fresh mixture entering the engine F Stoichiometric fuel-dry air mass ratio c Sea level gravit'ationalacceleration, ft/sec Transmission gea'r ratio GA GeneralAvi a tion h Distance of the airplane center of gravity aft of the leading edge of the mean aerodynamic chord of the wing, fraction of c.The quantity hrefisa reference value of h.

h Atmospheric mass~ratio of water vapour/dry air (Chapter 5 andAppendixE only) Geometric al ti:tud·eabove sealeveJin the standard H atmosphere (=dens.i-tyaltitude), ft Pressure al ti tude, ft H P IHP Indicated Horsepower ISA International Standard Atmosphere ISCPM Integrated Subsystem Cruise: Performance Hodel ISFC Indicated Specific Fuel Consumption J Propeller advance ,ratio J Propeller apparent advance ratio a N-2 L Airframe lift, lbf LHP Lost Horsepower

m Air mass flow rate into each engine, lbm/hr

a Corrected air mass flow rate into each engine, lbm/hr

m

a c Fuel mass flow rate into each engine, lbm/hr ID f ID Total fuel mass flow rate to all engines, lbmihr f t M Total fuel mass burned during a trip, Ibm f Propeller helical tip Mach number MT f.1AP Inlet Manifold Absolute (static) Pressure MBT Minimum ignition advance for Best Torque Propeller shaft speed, revolutions/second n n Density Index N Propeller shaft speed, RPM N Commanded propeller shaft speed, RPM c Engine shaft speed, RPM NE NACA National Advisory Committee for Aeronautics NASA National Aeronautics and Space Administration NEA Naturally aspirated MBT ignition timing Engine-Atmosphere NMBTE Naturally aspirated MBT ignition timing Engine OAT Outside Air Temperature (=atmospheric ambient air temperature) - \ P Installed propeller shaft power, ft lb/sec a P Atmospheric ambient air absolute pressure, Ibf/ft atmos Auxiliary equipment power consumed per engine, horsepower PAUX P Corrected auxiliary equipment power, horsepower AUX c N-3 P Exhaust abselute static back-pressure, inches Hg e Brake horsepower (BHP) per engine Inlet manifold absolute static pressure, inches Hg Airframe power 'required (power-off), horsepower Corrected airframe power required (power-off), horsepower Airframe power required (power-on), horsepower Propeller shaft power, horsepower Peripheral Computational Package POH Pilot Operating Handbook POHCPM Pilot Operating Handbook Cruise Performance Model Installed propeller shaft torque (apparent torque), lb ft Engine brake torque, lb ft Corrected brake torque, lb ft Q* Kernel of Q , lb ft a R Propeller tip radius, ft R Gas constant for dry air, ft.lbf/lbm.degree Kelvin a R* Point Economy Function (=Specific Range), ground nautical miles/Ibm RPM Revolutions Per Minute

S Airframe reference area = wing area, ft

S* The kernel of R*c, knots/BHP ) S* Corrected S*,knots/BHP c N-4 SI Spark Ignition T Atmospheric ambient air temperature at pressure atmos altitude H , degrees Kelvin.

p j T Inlet manifold temperature, degrees Kelvin m T Propulsive thrust, lbf p T Atmospheric ambient air temperature at altitude H in s the standard atmosphere, degrees Kelvin T~ True Airspeed TEA Turbocharged MBT ignition timing Engine-Atmosphere TIT Turbine Inlet Temperature V True airspeed, ft/sec Equivalent airspeed, ft/sec V e V Equivalent airspeed, knots E Groundspeed, knots ~ V True airspeed, knots T V Geocentric true windspeed along track, knots w V Corrected geocentric true windspeed along track, knots w c W Airplane gross weight, lbf WOT Wide Open Throttle X Corrected airspeed, knots Y Corrected propeller shaft speed, RPM Z Corrected Q*. lb ft Inlet valve ~~ch Index Z N-5 Angle of attack, degrees Propeller blade angle, degrees S S* Kernel of S, degrees y Airplane flight path angle to horiz'Ontal, degrees Denotes an increment E Index for correcting volumetric efficiency for effect's P of engine pressure ratio Index for correcting volumetric efficiency for effects of inlet manifold temperature Constant which describes the effect of airplane longi- tudinal center of gravity position on L/DON Free propeller efficiency n Installed propeller efficiency I ndicated thermal effic iency n· ~ PrQPulsive efficiency Kernel of n n* ,p p Tailplane efficiency Volumetric efficiency Constant which describes the effect of airplane longitudinal center of gravity position on L/DOFF Angular spacing of straight radial lines approximating e the constantS lines in the Ch:J2 plot, degrees Auxiliary equipment power loading factor p Atmospheric air density, slugs/ft Atmospheric air density at sea level in the standard atmosphere, slugs/ft

o Atmospheric air density ratio = p/PO

N-6 L_ Ignition timing, crankshaft degrees before top dead center L MBT ignition timing, crankshaft degrees before top o dead center Equivalence ratio Airplane heading, degrees True N-7 REFERENCES 1. Durand, W. F., (Editor-in-Chief), Aerodynamic Theory, Vol. 4, Julius Springer, Berlin, 1935. (H. G1auert, "Airplane Prope11ers," pp. 169-360.)

2. Durand, W. F., (Editor-in-Chief), Aerodynamic meory, Vol. 5, Julius Springer, Berlin, 1935. (L. V. Kerber, "Airplane Per- formance," pp. 223-341.)

3. Perkins, C. D. and Hage, R. E., Airplane Performance, Stability and Control, John Wiley & Sons, New York, 1949.

4. Von Mises, R., Theory of Flight, Dover, New York, 1959.

5. Diehl, W. S., Engineering Aerodynamics, The Ronald Press Company, New York, 1936.

6. Hemke, P. E., Elementary Applied Aerodynamics, Prentice Hall, New Jersey, 1956.

7. Dornmasch, D. 0., e~ al., Airplane Aerodynamics, Pitman, London, 1961.

8. Dornmasch, D.O., Elements of Propeller and Helicopter Aero- dynamics, Pitman, New York, 1953.

9. Glauert, H., The Elements of Aerofoil and Airscrew Theory, Cambridge University Press, 1947.

10. Weick, F. E., Aircraft Prope11er Design, HcGraw Hi11, New York, 1930.

11. Pye, D. R., The Internal Combustion Engine, Vol. 1, Principles, Oxford University Press, London: Humphrey ~li1ford, 1937.

12. Pye, D. R., The Internal Combustion Engine, Vol. 2, The Aero- Engine, Oxford University Press, (Clarendon), 1934.

R-l 13. Taylor, C. F., The Internal Combustion Engine in Theory and Practice, Vol. I, MIT Press,; Cambridge, Mass., 19:77.

14. Taylor, C. F., The Inte.rnal Combustion Engine in Theo'ry and Practice, Vol. 2, HIT P'ress, Cambridge,. Mass., .1977' ..

15. Curtiss-Wright Corporation (Wright Aeronautical Division), Wood-Ridge, New Jersey, "H.asic Theory of Operation-Turbo Com- pound Engine," 1962.

16. Chirivella, J. E., "Ultralean Combustion in General Aviation Piston Engines," JPL Publication 79-75, Jet Propulsion Labora- tory, Pasadena, CA, December 1979.

17. Donovan, A. F., et. al. (Editors)~. High Speed Aerod>:namics and Jet Propulsion, Vol. 8, High Speed Problems of Aircraft and Experimental t.1ethods, Princeton University Press, Princeton, 1961. (I. L. Ashkenas, "'l1ethods of Performance Calculation at High Speed," pp. 3-56.)

18. NASA, USAF, U.S. WEA1HERBUREAU,.U.S. Standa.rdAtmosphere, 19·62, U. S. Government Printing O'ffice', Washington~ D .. C., 1962.

19. Staley, C. W., "An In Flight Investigation of the Performance of a. Simple Thrust Measuring Device for Propener Driven Airplanes," Department Qf Mechanical and Aerospace Engineering, T-9G9, Princeton University, 1.970.

20. Lai tone, E. V., "Positive· Tail Loads for Hinimum Induced Drag of Subsonic Aircraft," Journal of Aircraft, Vol. 15, No. 12, 197&:., 21. Hamilton Standard Propellers- (United Aircraft Corporation) ,; J East Hartford, Connecticut, ''Hamil t.on Standard Hethod of Propeller Performance Calculation," 1941.

R-2 22. Private co~unication with Dr. J.Dav~d Kocurek, Group Engineer, Bell Helicopter, Fort Worth, Texas, October 1981.

23. Monts, Frank, "Energy Conservation in General Aviation Piston Powered Aircraft," First National Conference on Energy Conser- vation in General Aviation, Transportation Technology Department, Western Michigan University, October, 1977.

24. Bent, R. D. and McKinley, J. L., Aircraft Powerplants, Gregg Division, McGraw Hill, New York, 1978.

25. Avco Lycoming, Williamsport, Pennsylvania, '~orsepower Correction Factors and Operating Techniques for Engine Development and Calibration," Avco Lycoming Report No. 2268, Vol. 1 (Vol. 2), 1960 (1964).

26. Smith, P. H. and Morrison, J. C., The Scientific Design of Exhaust and Intake Systems, G. T. Foulis, Hen1ey-on-Thames, Oxfordshire, 1971.

27. Rezy, B. J. et. al., "Concepts for Reducing Exhaust Emissions and Fuel Consumption of the Aircraft Piston Engine," SAE 790605, 1979.

28. Private communication with Mr. Frank Monts, Mooney Aircraft Corporation, Kerrville, Texas, November 1979.

29. Obert, E. F., Internal Combustion Engines and Air Pollution, Harper and Row, New York, 1973.

30. Woodward Governor Company, Aircraft Controls Division, Rockford, Illinois, "Single Lever Power Control," no date.

R-3 31. Woods, R. L., "A Study of Optimum Engine Scheduling and Its Application to Fluidic Fuel Injection", U.S. Arrny:Materie1 Command, Harry Diamond Laborat.ories, Washington, D. C ..• 1973.

32. Schmidt, F., The Internal Combustion Engine, Chapman -and Hall, London, 1965.

33. Wylie Jr., C. R., Advanced Engineering MathematicS, -McGraw Hill, New York, Third Edition (International Student Edition) , J966 ..

34. Wallace, F. J. et. a1., "Variable Geometry Turbocharging-The Realistic Way Forwa.rd," SAE810336, 1981.

35. Private communication with Mr. BernardJ. Rezy, :Director (Advanc.ed En.:gineering) , Te1:e.dyne Continenta1 Motors, 'Mobile, Alabama, July 1981.

36. Babister, A. W., Aircraft S'tability and .Control, Pergam'on, New York, 1961.

37. Seckel, E., StabiUty and:Contro1 .of Airp1an:es 'and Helicopters, Academic Press, New York, .1972.

38. Abbott,.I. H.and Von D:oenaoff, A.E._, TheOTl:ofWins :Sections, Dover, New York, 1959.

39 .. Spreiter, J .R. and Sacks,A. H., "The Rolling Up of the Trailing Vortex Sheet and Its Effect on the DownwashB'ehindWings," Journal of the Aeronautical Sciences, January 1951.

40. Wood, D. H., "Full Scale -Tests of Metal Propellers a-t High Tip S.peeds," NACA TR 375, 1931.

41. Durand, W.F., "Int.eraction 'Between Air Propellers and Airplane Structures",NACA TR 235., '1926.

42. Walbce. J. 1-1. and Hobbs, P. V., Atmospheric Science--An Introductory Survey, Academic Press, New York, 1977.

43. Private communication with Mr. Allen Light, Vice President- Engineering, Avco Lycoming Williamsport Division, Pennsylvania, December 1980.

44. Powell, J. D., "Closed Loop Control of Spark Timing," Auto- motive Engine Control Workshop, Transportation Systems Center, DOT, Cambridge, Mass., July 1975.

45. Zeilinger, K., Beitrag zur Untersuchung der Schadstoff Emissionen eines Ottomotors unter besonderer Berilcksichtigung des instationaren Motorbetreibes, (Ph.D. Thesis) University of Munchen, Germany, 1974.

* * * * * * * * ) R-5 1. Report No. I 2. Gover-nment Accession' No .. 3. Recipient's Catalog No.

NASA CR-1-72188 5.- Report Date' 4. Title and Subtitle A Fuel-Efficient Cruise Performance AUGUst lqR~ Model for General Aviation Piston 6 .. Performing Organization Code Engine Airplanes 7. Authorlsl 8. Performing Organization Report No.

Richard C. H. ParkinS'on 1527-T 1-------------------------------+ 10: Work Unit No.

9. Performing Organization Name and Address- Princeton Uni versi ty 11. Contractor Grant No.

Department of Mechanical and Aerospace Engineer ng Princeton, NJ Ncr; 31-001-252 I- ____________________________ ~ 13. Type of Report and Period Cr'lered 12. Sponsoring Agency Name and Address C t t R" t National Aeronautics & Space Administration onracor e'por Washington, DC 20546 14. Sponsoring Agency Code 15. S!Jppleme,ntary Notes. .

Langl.ey Technlcal Monltor: Wi.lliam E. Howell Final Report Dissertation presented to Princeton University for Ph.D. degree.

16. Abstract: This report presents a fueT .... efficient cruise performance model which fac-ilitates maximizing. the specific range. of General Aviation airplanes powered by spark-ignition piston engines and propellers. Air- planes of fixed design only are considered. The uses and limitations of typical Pilot Operating Handbook cruise performance data, for construct- ing cruise performance models suit:able for maximizing specific range, are first examined. These data are found to be inadequate for constructing such models. A new model of G.eneral Aviation piston .... prop airplane cruise performance is then developed. This model consists of two subsystem models: the airframe-propeller-atmo.sp.here subsystem model; and the enginel- atmosphere subsystem. model. The new model facilitates maximizing specific range; and by virtue of its implicity and low volume data storage requirements, appears suit'able for airborne microprocessor imple- mentation.

17. Key Words (Suggested by Autbl)r(s» 18: Distribution Statement Aircraft propulsion Unclassified - Unlimited Aircraft propulsion controls Aircraft propulsion modeling Subject Category 07 19. Security Oassif. (of this report) 20. Security Classif. (of this page) 21. No. of Pages 22. Price 398 AI?

Unclassified Unclassified N-305 For sale by the National Technica</ Information Service, Springfield, Virginia 22161

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19830025620
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1983
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