Energy and Efficiency: Why are our piston aircraft engines so @#$%*! inefficient?
Cessna TTx · Service Bulletins
Overview
This document discusses the efficiency of piston aircraft engines, specifically focusing on the Continental IO-550 engine, which is commonly used in the Cessna TTx. It provides an in-depth analysis of the thermal and mechanical inefficiencies that affect engine performance, including fuel consumption rates and the impact of various operational settings. The author, Mike Busch, shares insights on how pilots can improve engine efficiency through better operational practices, such as leaning mixtures and optimizing power settings. The document is intended for pilots and aviation enthusiasts who seek to understand the complexities of engine performance and efficiency.
- The Continental IO-550 engine at maximum takeoff power consumes approximately 26.6 gallons/hour.
- At cruise power settings with a lean of peak mixture, fuel consumption can drop to about 13 gallons/hour.
- The thermal efficiency of the IO-550 engine is around 26% at maximum power and improves to about 34% at cruise with LOP settings.
- Key factors affecting engine efficiency include Otto cycle efficiency, volumetric efficiency, and mechanical losses.
- Pilots can improve efficiency by leaning mixtures aggressively and optimizing power settings.
Document
Source
Originally published by www.savvyaviation.com. Sprinkle hosts a reference copy with an added summary, specifications and searchable full text.
Document details
- Type
- Service Bulletins
- Year
- 2014
- Pages
- 3
- File size
- 191 KB
- Publisher
- www.savvyaviation.com
Most owners only have the POH. Here's the essential set for the Cessna TTx.
- Pilot's Operating Handbook / AFM
- Checklist
- Maintenance Manual
- Parts Catalog (IPC)
- Systems & Wiring
- Service Bulletins
- Type Certificate (TCDS)
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In this document
Engine Efficiency Calculations
The document provides detailed calculations on the efficiency of the Continental IO-550 engine at various power settings. For instance, at maximum takeoff power, the engine consumes approximately 26.6 gallons per hour, translating to a thermal efficiency of about 26 percent. At cruise power settings with a lean of peak (LOP) mixture, the fuel consumption drops to around 13 gallons per hour, improving efficiency to approximately 34 percent.
Factors Affecting Efficiency
Several factors contribute to the inefficiency of piston engines, including Otto cycle efficiency, volumetric efficiency, mixture losses, mechanical losses, and accessory losses. The document outlines how each of these factors impacts overall engine performance and provides insights into potential improvements.
Improving Engine Efficiency
The author discusses various strategies for improving engine efficiency, such as using higher compression ratios, electronic ignition systems, and optimized mixture settings. He emphasizes the importance of pilot education in operating engines at leaner mixtures to achieve better fuel efficiency.
Safety notes
- Operating engines rich of peak EGT can lead to increased fuel consumption and reduced efficiency.
Full document text
30 Sport Aviation October 2014 MIKE BUSCH COMMENTARY / SAVVY AVIATOR OUR PISTON AIRCRAFT engines convert chemical energy into mechanical work, but they don’t do it very efficiently. It turns out that only about one-third of the energy contained in the 100LL we burn winds up getting to the propeller and doing useful work to propel us through the air. The remaining two-thirds winds up getting lost between the fuel truck and the prop hub. At today’s stratospheric avgas prices, that’s pretty depressing. LET’S DO THE MATH Consider a Continental IO-550 engine rated at 300 hp. If the fuel system is set up properly per Continental Service Bulletin SID97-3F, fuel flow at maximum takeoff power is about 26.6 gal- lons/hour or 156 pounds/hour. How much chemical energy does that fuel provide? We can calculate that. 100LL is rated at a “minimum lower heat value” of 18,700 BTUs per pound. Let’s convert that figure into something more meaningful to pilots like you and me. (1) Divide 156 pounds per hour by 3,600 seconds per hour to get 0.0433 pounds per second. (2) Multiply by 18,700 (the thermal content of 100LL in BTUs per pound) to get 810 BTUs per second. (3) Multiply by 1.414 (the horsepower equivalent to 1 BTU per second) to get 1,146 hp. Does this mean that your IO-550 consumes 100LL with ther- mal energy equivalent to 1,146 hp, and yet produces only 300 hp of output power? Unfortunately, that’s exactly what it means— and that works out to a miserable thermal efficiency of 26 percent. Good grief! Should an IO-550 really be drinking this much fuel? Well, we can calculate that, too. (1) At takeoff power, the engine is turn- ing at 2700 rpm. Since it’s a four-stroke engine, each power cycle requires two crankshaft revolutions. Therefore, the engine is operating at 1,350 power cycles per minute. (2) The displacement of the engine is 550 cubic inches, or 0.32 cubic feet. Due to induction system losses, however, the engine’s “volumetric efficiency” is only about 85 percent, so it “inhales” only about 0.27 cubic feet of air per power cycle. (3) Multiplying 1,350 power cycles per second times 0.27 cubic feet of air per cycle, we calculate that the engine should inhale 365 cubic feet of air per minute. (4) Sea level air under standard atmo- spheric conditions weighs 0.0765 pounds per cubic foot. Therefore, the engine breathes 27.9 pounds of air per minute. (5) Best power mixture requires an air- fuel ratio of about 12.5 to 1 by weight. Dividing 27.9 by 12.5, we get a fuel burn of 2.23 pounds of fuel per minute—or multiply- ing by 60, we get 134 pounds per hour or 22.3 gallons per hour calculated fuel flow at best power mixture. The actual book fuel flow figure of 26.6 gallons/hour or 156 pounds/hour is higher than this calculated value because of the Energy and Efficiency Why are our piston aircraft engines so @#$%*! inefficient? unusually rich mixture required to provide adequate detonation margins at full take- off power. WHAT ABOUT LOP? Surely engine efficiency is much better at cruise power settings with aggressively lean mixtures, right? Let’s take a look. An IO-550 engine running at 65 percent power and operating LOP uses approxi- mately 13 gallons/hour or 78 pounds/hour. What kind of thermal efficiency does that represent? Repeating the calculations: (1) Divide 78 pounds per hour by 3,600 seconds per hour to get 0.0217 pounds per second. (2) Multiply by 18,700 (the thermal con- tent of avgas in BTUs per pound) to get 405 BTUs per second. (3) Multiply by 1.414 (the horsepower equivalent to 1 BTU per second) to get 573 hp. So even at LOP cruise, the IO-550 con- sumes 573 hp worth of go-juice in order to produce 195 hp (65 percent of 300), for an efficiency of about 34 percent. Definitely better, but certainly nothing to write home about. WHY SO WASTEFUL? Here’s one breakdown of efficiency losses (from Performance of Light Aircraft by John T. Lowry, Ph.D.): Otto cycle efficiency—the thermody- namic efficiency of a four-stroke internal combustion engine—is limited by the com- pression ratio (i.e., the ratio of cylinder volumes as the piston moves from bottom- dead-center to top-dead-center). The higher the compression ratio, the greater the efficiency. For an IO-550 with a com- pression ratio of 8.5-to-1, the Otto cycle efficiency works out to about 57.5 percent. Volumetric efficiency—As mentioned earlier, the ability of the engine to breathe in its full theoretical displacement of air during each power cycle is restricted by a variety of pressure losses at various points in the induction system: air filter, throttle body, intake manifold, and intake valves. For most of our engines, volumetric effi- ciency is around 85 percent, bringing total efficiency down to 57.5 percent times 85 per- cent, or 49 percent. Mixture losses— Optimum fuel efficiency occurs at very lean mixture set- tings (so-called “best economy mixture”) with an air-fuel ratio in the vicinity of 18-to-1 by weight. Best economy mixture occurs very LOP, how- ever, and most pilots don’t operate that lean. (Not to mention that many engines won’t run smoothly that lean.) Many pilots operate rich of peak EGT in the vicinity of best- power mixture, at an air-fuel ratio around 12.5-to-1, which provides a fuel efficiency that’s only 70 percent of optimum. Even if you operate slightly LOP (let’s say at an air-fuel ratio of 16-to-1), your efficiency is just 89 percent of optimum, and that brings total efficiency down to 49 percent times 89 percent, or 44 percent. Mechanical losses—Friction losses involving the reciprocating and rotational parts inside the engine consume a signifi- cant amount of power that could otherwise be delivered to the propeller. Mechanical efficiency varies with engine speed (lower losses at lower rpm), but is typically around 88 percent, bringing total efficiency down to 44 percent times 88 percent or 38 percent. Accessory losses—A certain amount of engine power is consumed driving acces-
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sories such as magnetos, fuel pumps, alternators, vacuum pumps, hydraulic pumps, air conditioning compressors, etc. Figure this robs 5 percent of the remain- ing power, bringing total efficiency down to 36 percent. Other losses—This includes a grab bag of other inefficiencies including blow-by past the piston rings, unburned hydrocarbons in the fuel, humidity in the air, back pressure in the exhaust system, and so forth. Figure another 5 percent loss, bringing total efficiency down to 34 percent (which agrees with our earlier figure for an IO-550-B at 65 percent LOP). THERMAL AND CHEMICAL LOSSES A quite different analysis (from Fundamentals of Power Plants for Aircraft by Joseph Liston) analyzes the various thermal and chemical losses suffered by a piston aircraft engine. We’ve already seen that an internal- combustion engine is incapable of converting all the heat of combustion into mechanical energy, limited primarily by its finite compression ratio. The rest of the heat of combustion, as well as a small amount of additional heat generated by friction, is lost through the engine’s exhaust and cooling systems. There are also some chemical losses. In theory, the combustion of pure hydrocar- bon fuel at stoichiometric mixture should produce nothing but carbon dioxide (CO 2 ) and water (H 2 O). In reality, however, there’s always some sulfur in the fuel, which is transformed by combustion to sulfur dioxide (SO 2 ) and sulfuric acid (H 2 SO 4 ). If the mixture is a bit on the rich side, the exhaust also contains carbon monoxide (CO), which results from incomplete combustion, as well as some unburned carbon particles and some methane gas (CH 4 ). www.eaa.org 31 ILLUSTRATION COURTESY OF MIKE BUSCH Figure 1: Functional breakdown of efficiency losses by John T. Lowry, Ph.D. 1) Otto Cycle, 2) Volumetric, 3) Mixture, 4) Mechanical, 5) Accessory, 6) Other, 7) Net Power Output Here’s how Liston breaks this all down: Fuel energy, 100 percent Exhaust, 51.6 percent Heat, 47.0 percent Chemical, 4.6 percent CO, 3.1 percent CH 4 , 1.5 percent Other thermal, 12.2 percent Conduction to air, 7.2 percent Conduction to oil, 1.6 percent Radiation and misc., 3.4 percent Mechanical, 36.2 percent Friction losses, 4.3 percent Brake horsepower output, 31.9 percent Again, this figure agrees pretty well with our earlier 34 percent figure for the IO-550-B at 65 percent LOP cruise. CAN WE DO BETTER? What, if anything, can we do to improve this dismal efficiency? Well, don’t expect any miraculous improvements of large magnitude. But every little bit helps, and there are certainly a few areas where the potential exists for improvement. Otto cycle efficiency—As we’ve seen, the basic thermodynamic efficiency of an inter- nal combustion engine is a function of compression ratio. Unfortunately, high- compression engines have traditionally required high-octane gasoline in order to avoid detonation, and high-octane gasoline is fast becoming unobtainable because of the campaign to eliminate tetraethyl lead (TEL) from avgas. Consequently, the trend in recent years has been toward lower com- pression ratios that are compatible with low-lead or unleaded fuel. While this may be wonderful for the environment, it sure doesn’t help the thermodynamic efficiency of our engines. One bright light on the horizon is the prospect of moving from fixed-timed mag- netos to sophisticated, computerized electronic ignition systems capable of pro- tecting engines against detonation by varying ignition timing. The incorporation of variable ignition timing and detonation sensors should permit the use of higher compression ratios even with unleaded fuel. It may take a few more years before any such systems make it through FAA certification, but the prospects for improved efficiency are significant. Even more exciting is the recent advent of certificated diesel engines for piston aircraft, which run on Jet A and have 18-to-1 compression ratios that offer much greater thermal efficiency than any spark ignition gasoline engine. Volumetric efficiency—Small improve- ments in this area are possible through the use of tuned induction systems, large intake valves, venturi-style valve seats, ram recovery air scoops, and turbocharg- ing. Auto engines have even gone to multiple intake valves per cyl- inder, but the weight and complexity might make this impractical for aircraft engines. Mixture losses— Major strides have already been made in this area, partially through pilot educa- tion to encourage the use of lean mixture settings, and partially through improve- ments to engine instrumentation and mixture distribution to facilitate operation at or near best economy mixture (i.e., consider- ably LOP). Mechanical losses—The biggest thing that can be done to reduce mechanical losses is for pilots to cruise at low rpm and high manifold pressure, rather than vice versa. Small additional gains are pos- sible through the use of high-lubricity synthetic oil to reduce friction losses, but the leading all-synthetic oil (Mobil AV 1) was pulled off the market in the 1990s due to its inability to control lead depos- its, and even semi-synthetics like AeroShell 15W-50 have lead-deposit problems, particularly in small-sump engines like the ones used in the Cessna TTX and Cirrus SR22. When the lead is ultimately removed from avgas, all-syn- thetic oils may come back in favor for piston aircraft engines. Accessory losses—The conversion to electronic ignition systems may also pro- vide some small benefits by eliminating the mechanical losses involved in driving dual magnetos, although this may be par- tially offset by the requirement for electronic-ignition engines to have dual alternators. The trend toward all-electric airplanes with no pneumatics or hydrau- lics may also help slightly. For now, the best thing you can do to improve efficiency is to lean aggressively (considerably LOP if feasible), and to cruise at low rpm and high MP rather than vice versa. In the foreseeable future, fur- ther improvements may be possible through the use of variable-timing elec- tronic ignition systems and installation of higher-compression pistons. Efficiencies in the area of 40 percent are possible, but don’t expect much more than that from spark-ignition engines, at least any time soon. Mike Busch, EAA 740170, was the 2008 National Aviation Maintenance Technician of the Year, and has been a pilot for 44 years, logging more than 7,000 hours. He’s a CFI and A&P/IA. E-mail him at mike.busch@savvyaviator. com. Mike also hosts free online presentations as part of EAA’s webinar series on the first Wednesday of each month. For a schedule visit www.EAA.org/webinars. 32 Sport Aviation October 2014 Figure 2: Thermal and chemical breakdown of efficiency losses by Joseph Liston. 1) Exhaust [Heat], 2) Exhaust [Chemical], 3) Conduction to Air, 4) Conduction to Oil, 5) Radiation and Misc., 6) Friction, 7) Net Power Output ILLUSTRATION COURTESY OF MIKE BUSCH






