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NACA-WR-L-373 · Wind-Tunnel Investigation of Perforated Split Flaps for Use as Dive Brakes on a Tapered NACA 23012 Airfoil

NASA (NTRS) · 1941

Open the PDFPublic domain · NASA (NTRS)Technical Reports

Overview

Aerodynamic characteristics of a tapered NACA 23012 airfoil with single and double perforated split flaps have been determined in the NACA 7- by 10-foot wind tunnel. Dynamic pressure surveys were made behind the airfoil at the approximate location of the tail in order to determine the extent and…

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Key points

  • The investigation determined the aerodynamic characteristics of a tapered NACA 23012 airfoil with single and double perforated split flaps.
  • Both single and double perforated split flaps can be effectively used as dive brakes, providing satisfactory drag control.
  • The aerodynamic effects of the perforated split flaps on the tapered airfoil were similar to those on a comparable rectangular airfoil.
  • The use of full-span perforated double split flaps can limit the indicated diving speed of an airplane to 200 miles per hour at a wing loading of 35 pounds per square foot.
  • The study provides sufficient data to predict the performance of perforated split flaps when used as dive brakes.
Frequently asked questions
What was the purpose of the wind-tunnel investigation?

The purpose was to determine the aerodynamic characteristics of a tapered NACA 23012 airfoil with perforated split flaps for use as dive brakes.

What types of split flaps were tested in the investigation?

The investigation tested both single and double perforated split flaps.

What were the findings regarding the effectiveness of the split flaps?

The findings indicated that both single and double perforated split flaps could be used to obtain satisfactory drag control.

How do the split flaps affect the diving speed of an airplane?

The use of full-span perforated double split flaps can limit the indicated diving speed to 200 miles per hour for certain wing loadings.

What is the significance of the aerodynamic characteristics found in the study?

The aerodynamic characteristics provide designers with essential information to evaluate the performance of perforated split flaps in dive control applications.

Document

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ADVISORY COMMITTE E F OR AERON A UTICS

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ORIGINALL Y ISSUED November 1941 as Advance Restricted Report WIND-TUNNEL INVESTIGATION OF PERFORA TE D SPLIT FLAPS FOR USE AS DIVE BRAKES ON A TAPERED NA CA 23012 AI RFOIL By Paul E. Purser and. Thoma s R. Turner Langley Memorial Aeronautical Lab or atory Langley Field, Va.

NAC~

WASH I NG TON NACA WARTIME REPORTS are reprints of papers o riginally issued to provide rapid distribution of advance research results to an authorized group requiring them for the war effort. They were pre - viously held under a security status but are n ow unclassified. Some of these reports were not tech- ni cally edited. All have been repr oduced without change in order to expedite general distributio n.

L - 373 FO ~ VSE _~ DI~E BR ~KE S ON A ~APERED iAGA 23012 AIRFOIL By Paul Eo P urse~ and Thomas R. Ttrner Aer o ,lyna1ui c chc .r acteristics of a ta pered. :r:: AC .i 230 12 ai rfoil with ~ ing l e an d dou b le pe r forated s p lit flaps have been detormined in t h e ~ACA 7- by l O -foot wind tun - n e1e Dyuamlc pr essu re surv eys we~0 mado behind the air - foil at the a~~roximate location of the tail in order t o deterci n e tle CXt6~t ant location ai tho \aka fo r s e vera l o f the llar a r :;: '2 .LgE'i1 ents I n D.dcl i tion , co mpu tations hav e o been mad e of ~n application o~ pe rforated doubl e s~lit fla ps for use as fighter bra es ~ T~3 r c su lts in di c~tod that sin g le or d Q able perfora t- ed s ::.;::.it f la.J?s UlD.y 'e used t o obi'l.in satisfactory d5. ;,r e cont v'L rrith , )u'C, und1:..e buffeti l!" effec ts a :1d that sin g le or 10 111 e perf orate' spiit fla p s ma~ also be sed as =i ~ ~J.'li c r 0raklO;s ~ Th e ::?e rforatGd spl i t fl~,s had approximate l y the s am e cffe~ts on the aer od ynamic and uake cha racte risti cs o i ' t'lC t-:'}JQ rc d c..i r f oil as on a. c o mpnrablc roctangula.r airfoil o The H CA hRS underta ren an extensive investigation for t h e purpose of doveloping dov ices suit ab l e for li m it- ing tl e divi ng speeds of airp l an es. As a p art of t hi s i nvestiga ~ ion Q stu ~- has been n a d e of test results ob - tained du ring t h e develop m en t of devi ce s ~ esigned primar i- ly for ot~ e r purp o sGs~ such as h i gh lift or l ateral con - trol, but ~h ich may also b e uscd fo~ d i ve control. ~ho slot -li p ai leron co mb ined wi th a full-span slotted f~ap is o ne of those d ual- purp o se d avices, and data fo_ its u se hav e be en p resented in ref e renco 10 A study was also made of a l~r g e amount of un co rrelated da t a on vario u s a i rfoi l- fl a p co nb inat i ons f ro m tests previously made f or the Bur e au of Aeronautics This study indicated t hat pe r - o fornte floublo spljt flaps would give the desired ~har ~ c t oristics ' for use as div~-control devicos . FolloTIing t his stu cc yo [.11 invo stigat ion as made of sove::.'al I1rran<;e - ments o~ Ain~lo and double split flap s on n recta~ ~ ular NACA 23012 airf oil (reference 2 ) to detorcine in 2~rc io - tail the c .crodyna::Jic an d '\'Iako cho.ractoristics of th so devicoe in orde r that dosigncrs might Doro closely eva luate their e~:ects on t~e periormance oi co ~lete nirplal es, The prcGont t~Bts TIGra uad e to dotercino tho cor Jd ynami c an~ ~ ak c c har~ctori s tica of soee of tho singlo and d ouble s plit-fl~p n ~ nngcDon ts on a tapered NACA 23012 airfoi l .

l.Iodel rh a airf ei l model used (fig. 1) was of laminated mah og - any bu i~ t t o ~he N CA 23012 profile Th e model was ta~ere d c 3 to 1 in p l ~~ fc~m wit~ a s pa n of 60 inc hG3 and an as p ect rati o c,l G~O., ~ne trailing e '_ {"B () : t:ne mo d .al TIas stre.i f- 'h t an e. tl, .Q .l'"1c.xL~' 1 u p~cr- s 'l1'fa ce Cl'd. L l 18 .te s of tll0 various sec - t:l.O ~lS ,7 01'0 iil or.o ~l2. nc ~ The per::' o_.?ted split f la ::;Js were mad9 cf sheet s te el and had a chord of 2 inches (20 pe r- ce nt o f the air~ oil m aal geou0tric cho~i). The perf or a - tio ns i n tho flap s ~oro symmetrically s p acod circular hol08 ( aoo fl~ p d ot~ i l, fig. 1) an d re m ov od 33.1 p ercent of tho originnl flnp ar OQ I n or der to fac il itat e pa rti a l - e sp an - flap tests oach fl a p was mad e in ten equal segments, eac h se g~e nt havi _g a span 0_ 20 percent of t~e airfoil se mispan~ Th e secffients on Bach semiRpan were numbered from 1 t 5 ~ r ~~r cs s ivel y fro~ the p lano of sy cm ct y out- bo ard to t h e a~ rfoil tipo S ? lit-~l~p doflections wor D mo&ouro d uith respect to tho airfoi~ surface at the hingo point anJ the gap b et we e n t h e a irfoil sur fa ce and th e flap was sealed with mO~91ing clay, ~ind Tun el ~nd Equipment The t es ts wer e cad e in the NACA 7- ~y IO-foot closed - throat ~ind tunne l io scr ibed in references 3 an d 4. The wake surve y s wore m~ dc uith a rake of eight 3/ 8 -inch diam - eter pitot tubes s~acod 2 inc hos apart . ~he r&ko was ad- just ab le so that dynamic p re osuro could bo recorded at l - inch i ntorvals ~long a vortical line 27 inches long uh ich uas l o c ated 30 inc~os (3 . 0c) behind tho qua rter - chord point 0 the a irfoil me a n aer o Qyna~ic chord and 5 inc h8s (Oe 5e) tJ tho right of tho p la n o o~ sY~illotryo This p osi- tic u ~as be li eved to be repres entativ e o~ the l o c ation of t he hinge line and m idpoi l t of the scm is pan 0 2 tho hor i- zontal ta::' l su::-facos of airplanes on which dive -e o~trol a e vicns wou ld be usad. The r3t i o of the dynam~c prossure s in t~e W~~O to tho dyna ic pr e ssuros at the sa~o points "it:l -::ho nodel romovod (support strut in p : _a ce) was ,,,,-ete r - minod fr0~ rea~ings on an inclined-tute alcoh~l manODete r.

Figu~e 2 ~s a three-q~ar t or r ea r vi ew of the ~odel mou nted in t~e uind tu~nolc ~os ts J,§~i_C~!}_ , tt _ J).9I)~. - T h8 dynaJ:'1ic Pi"CSSUre rr..aintaincd for a ll tests ~us lo.~7 pounis per sqa3r3 foot . which corre - spond.s t o n "Velocity ' of a-bout 80 miles per h ou r under stal1do . rd 8::-0.-1e'-e]. c ond.i tior..u u.nc'l_ to ar. average test Eeyno lds numbar of 609 , 000 bas~d on tho mean ge o me t ric c hord of tho illoJol (10 inQ) o '.f"j. ::' ;..§~ ~_9 ~c1~!,~o - The ~ cst e c 2n 3 i s t ed o:Z' t:1e de '>3rrli - no.ti~ '1 cf he l " it , c'i.r2g, and :pilchi:ll;-mo-:Jor.t coeffieie:1 ts and ol t:e W~kR c~ar"cteristics fo r vnr1ouo arrnn Ge~ont s of t~~ f l ~pso Double sp li t flapc wore located 20 percen t of t~o boau ~C~ atric chord from the cirfo~l tr~ilin~ e dg e a~d single sp lit flaps (lo~er surface) ~erc located o n t~e JiJe of t~e 30-pcrccnt - c~ord stations of tho atr - foil Rectionc T.ho forces aua. mO-ients i~e r e dcto:'oir..cd at o intor va: s of 2 thrc~ghout tho a~~lo-of-attack r ango iron 'oelo' ,7 zero lift to ao)\ -o Jla:~ir;:;u lift. J:'ho i'7ako Durvc~'s 1,'701'0 nnd c at interva l s of 4° throlghout tho 8a~e a~glo - of n. '~tack :'a!1g , :3 o ~o tests ~ore ~ado with th e flap perforati o ~s cove ad since the dat a in refe r ence 2 s10TIed that w~ile covering the perforations incre as ed the drag coe ~f i cient , it als o caused a very unsteady con iiti o _ of the mo del .

R~SULTS AND ~ISC~SSIO~ In the ~resentat io n of results the f ollo i'7 in g symools are use eL C ~ift coe ff icient, L C - p~tching-mo~Bllt coefficient about the qua rt o r - J . C/4 ch o rd poin+ o f the airfoil mean ~crod~namic eho d; m/qocC!

1 li~ t ill pitchin~ mo~cn t .1 P V 8 d;'{na~ic prosrn . ro at po.'nt i nako, q average dynamic pressuro for ai r stream,

i P V 0 '2

ai~foil caa~ g oo~o tr ic chord airf0il mean aerodynam~c chord , chord throu~h c centroid o f area of ~irfo il seoispan flap c~ord airfoil area b airfo i1 spa.n flap span and a anGle of attack Of upper - slrface spli~ - fl ap deflection U O ~ lo~er-surface split-flap de~le c tion -1 ~he suoRcript Lo refers t o the characteristics at zero l ift" S ince t ~ e support strut interference and tares were r elatively scall thes e corrections were applied only to the pl~in airfoil data . The standard jet-boundary corre c- tio s which vvore alJplio cl t o .... 11 t:1El f o rce-test dato. arc : where C is the jet cro ss - sectional area. A ~alue of

6 = OGl135 f or tIe closed - throat wind tunnel 1a s used in

correctin g tho results It should be noted t~at due to tho various spRn - load distri~utions of the airf oil ryith th e vario:s spl it- flap arrange l ents, these corrections are n ot strictly a l)p licable t') all tht) data. £) 0 cerrec- tion for tunnel ef ~~c t has b~ ~n applied to the wake 10ca - tion This correction i~ sma ll because of the relatively e small model uscd Q Double Split Flaps The cr0dyna m ic and wake ctaracteristics of a 60 -i nch span 3-to-l tapered ~ACA 23012 air_oil ~ith double split flaps locnted 0.20c fro~ the ai~foil trailing ed~o ara pre ~0ntei in ~igures 3, 4, and 50 The ae oiyna~ic charac - teristics are presen~ed ~s CQrves plotted against lift coefficient; and tic wa~o characteristics are shown as curves of dynawic prcssu_e ratio, q/qo' plott ed a sa inst distance D.-cove nnd belo';1 the e: :t e n cd chord. line 0_ tll0 roo 'G seccion of t' e c.irfo:' la The moth o d of presenti:r.e tile wa~e ch ar~. ctcr:'stics is illustratei in fi.;ure 4 . Th o double split f~aps Dad ?ractical l y t'le sawe ef~ects on tho aerodynamic and wa~e characte=istics of tIe tapered air- foil as they _aQ on those uf the rectangular a irfoil of reference 20 The wake surveys were made of selected rep - resentati e &_rangenents based on the restlts of ref e rence 2 and t~e dat a presented are sufficient to s~ow the ~ake charact ~risti cs of al l arrangoMents.

Si nc e the aerod~namic characteristics at and near zer o lift were consiiered of pa rticular interest to the de - signer, t~e results fr om figures 3a and 5a were plotted against flap span i~ figure 6~ ~either flap spa~ nor air- foil plan fo rm had a ~arkea e ffect on the pitch ing- ~omen t coefficients or angles ot attack at zero lift . The drag coefficients obtained with center-S Qcti o~ Qoub~c split - .------.--- ~- flaps were practically the SFl.Ille for b o th the tape_ed a ir - foil and the ecta~gu].ar airfoil of reference 2~ but t~e tip section flaps gave high e r dra~ coefficients on the tapered airfoil than on the rectangular air oil . On both airfoils the center-section flaps all o wed hibher available ma.ll.imu . lift coefficients than the tip - section _ fla-os ex - cept for one unexplained instance (60 - pcrcent-span-flaps , figo 6)v The Qifference bet~ oon the maximu~ lift coeffi - cients obt a i~able with the con tor- and tip-scction flaps was 1&8s for t~e tapdre~ airfoil than for the rectangular airfo:l of reforenco 20 Singlo Split Fla9s Th8 aerQdy~am:c and ~ake cha act eristics of a 3-to-l tap ered :~ACA 23012 airfoil wi th lowor--surface perforated split flaps locate d on a line th~o~gh the 30-percent-c : ord statioDo of the airfoil sections a_e shown in figures 7 to 9 .

The u.:'e of these flaps produceci t~e sa_ e large decrease in angle of attack for ~oro lift on the taporcd airfoil as on the r~ ~~ angula r airfoil of ref eTu,ce 2. Sinco the aerody - n am ic ' : ·~J. aracf,eris·cir.s at and noc , .~' zo:r' O lift were consid- ore d of p~rti cul a~ i~ torost tG tho designer , the results of ::iC ~' :"":'os t: , :>.no 9 wor0 roplottoc. a.gainst flap span in figu: c c 10 ..

In view 0_ t he agreement shown bet7een the tapered air f 0 i 1 t cst san d. t ~ G r () G t a. n g"C~ 1 E t r a iI - f 0 i I t G S t s 0 f ref G r- ence 2) the t ~a sets of d2 ta ~ogether should afford. su:fi - cient information ~cr t~e prediction of the performance of pe rfo ' ated split flaps when used as dive brakes o Di v ing Sl )eod T~e relatio~ship bct~ee drag coefficient , win g load - ng, and i nd ic at ed ve l ocity IO~ an airplane in a vertical i dive is s h own in fiGure 11" For otlor diving angles, t:1.C vel o city g iven on tho chart should bo multiplied by tho squaro root of tho sino of the ciiving an g le, reforrod to the horizontal. Fro~ this cha:-t, the data i n figu es 3(a) through 10c and the data i n r i g ures 3(a) through 21(0.) of reference G, i t may be shoun that the use of full-span pe~forated double s p lit flaps ~ould probably limit t o 200 miles per hou r the indicated diving speed of an air p l ane uith a 7ilg loa~in · of 35 pounds per square foot and li m- it to 250 miles per h o ur the diving speed of an airplane 7ith a ~ing loadin G of 55 pOlnds ~er squaro foot . Co r r o- spondi~ . valu e s obtained w it h the use of perforated sin- ele split flaps are : 200 ~iles per hour for a winb load- i n~ of 30 po~nds ~er square foot, and 250 miles per hour ~ for a ning loa d inG of 45 p o unds per squcre foot o r'\ ~ Figllter 3rakes In addition to the need for devices which will re duc e the diving speeds of airplanes. it appears that a need has arisen for some d e vic e which TIi ll tem~orari ly reduce the sp~ed of atta c ~ ing figh ter aircraft in order that the pilot will havo more tiwG for firing. Som e of the require - mont s which a figh t er ~rBko should ~eot arc : littl o or n o chango in tho attitudo of the air:lane 7ith f i xed controls , s ufficient "ncrcas c in lift coefficient dur in g op eration of the "0 akos to mnintain level flig"_t as t::'e speed is re - duced, and enough increas e in drag coefficient to dncele r- ate the ~irplan e TIithin a re asonable ti~e after the brakes arc ap~lied(\ n ~pplicction of fighter brakes to an airp l ane 7ith a wing !oading of 3 0 pounds per squc~c foot has beot com - pu.tod" by a: '1 a?IH' o :dmate , stop-bY-3tcp mo·c" od Tuo arrang e- o mo::).t used was the fIll syan porforated dO F. ble split flaps

located at 0.80c on the rect.a:1 g ular rAe! .. 23012 airfoil

( fig 3(a" reforence 2)0 It TIas assu~ad that both t h e a u pp er-surface and t~e lo we r-s urface flaps r cre deflectcd to 30 TIit~in 1 scco=d. and t: on the uDDer-surfaco f l a D 'I ..L. _ .J: re mained stationary uh il o the ~oTIer-surfaco flap was : e- flected to 60 in such a manner as to afford sufficient increas e in lift coefficient to maintain level fli gh t at the red i.. 1C o d speeds without a chc:.nge in angle of attack.

Althou gh rnaintuin i ng a onst~n t po~e r output of the enGin e w oul d slightly decreas e the e~fective drag increme nt and incro ase tho t~De required to slow dOTIn , this e f fect uas neglected in orQcr ~ o si~plify tho p roblem.

The results of the computations are given in Ilgure 1 2, which shows curves of speed; lift, d~ag , and pitching - moment coefficients; anole of attack; flap deflection; and acceleration plotted against time . As is shown in figure 11, the use of full -s pan perforated dou Ie split flaps should reauco the airplano speod from 300 miles per hour to 176 miles per hour i n a bout 8 seconds, with a negligible ch ang e in angle of attack and a change i n w ing pitching - Doment coefficient of only - 0 . 03 . It should be

J

ncted that at the end o f the 8 seconds the airplane stiJl has a dece 1 0rat ion of about O.6g and in ardor to continue i n level fli~Lt the lift coefficient must be increasod by an in~roaso in anslc o f attack or by a decroase in the upner - surfaco flan ~oflcction (w ~ich w oul d also docreaso t h~ d r ng cooffici~nt and deco lerat i on).

Th e effect of the ~ laps on t~e pitching - moment coeffi - cient due to th~ tail s hou l d b e determined on a complete modol of any propcsed in~tall&tion. Also a nore comploto determinatien should bo ~ado of the variation of lift and drag coe ff ic ient s with flap ~eflection, since the lift and drag data use d in computing the characteristics shown in

figure 12 w8re takon from curves ~ rawn between 8 = 30

f with no intermediate points o and I n using double sp~it flaps ns fi~hter brakes, th8 in- iti al accelcrD.tion of 1.1g could be reduced by decreasing the initia l 30 flap daflecti on or by reducing the rate of deflcct~ on and using a diffo~ential bet7een the tw o flaps , so that the sreat8r defle ction of the lower-surface flap would s upply the lift c efficient~ needed to maintain a con stant angle of ~tta c ~ o It also O- p po"l.rs p ~ s s iblo to URc lo ;rer-s lrface For: o- ratod split flaps locatod nenr thc wing loading edge 68 fighter brakes if a somewhat lower decoloration a- d so~o chango i~ t~ e attitud e of the. ir?lano is considered a.c - coptabl('le , Oper" ting FcrcoG A lar g o ~moun~ of data has boon published o~ tho hinge-~OLent c h aractoris t ics of various split-flap combi - nations , somo of Wilich arf.) presonted L1 referonces 5 to 8; an the hinge - momont character ' stics of a slot_Ii, aileron f or ~se as a dOve brake Jh c n combi~od ';7ith a full-s p an slotted flnp arc presentod i~ rcforo~cc 1. Coruparatively li ttl e is knorn , houevcr, about the ef:ects o f flap pe r - forationG or of vaiious methods o~ operation on the forces required t o deflect split flaps. Some 70rk has been dono i n England on various ~ethois of operation o f split,flaps (reforonce 9) and brief menti on is mad e of th e loads to be

8z pected o~ dive brakes in a re port 0: some Gorman re -

s earch (reference 10) . The dive brakes o f reforence 10 wera slats placed 110rm'1.l t o the airfoi l surfnce "ith a gap b et~een the airfoil and the slatso Pressure distributiorr tAs t a on these slats in d icated th a t the load on t he slat s was about 75 percent of the d~ag increase and that th9 d is trib u ti on of this load on t he slat was approximately r e c ta. n g'J.la I' 0 A ddit ion al research is recom m en ded on the e ffects of perforations and method of flap o pe ration on the hinge - mo men t c haracte ristics of perforated split flaps .

COliCLUS IO~~ S The results indicated that single or doub le perforat ed sp l :. t flapt; ma.y be used to o bt:~in sati:3factor y dive con- tr ol wi th out undue buffeting effects and that single or double psrf0rated ~p lit f la ps may also be used as fighter br akes:;> The perforated op lit flaps have approximately the sam e effect'3 (Jl the aE.l'ocl.ync..mi c and wake charac te:List ics of th e t apered airfoil as on a cemparab l o rectangular ailfoila L angley Uom orial Aeronau tic al L aboratory , National Advi90~y Oommittee for Lc ~onautics , Lan5ley .'lo ld, Va ..

REFER.ENCES 1. Rogal l o , F. M .: Aerodynami c Characteristics of a Slot - Lip Ailer on and Slotted Fla p fo r Div e Brakes . NACA ACR , Ap ri 1 1 9L. l , 2. Purser, P au E ., and Turner, Thoma s R. : Wind - Tunnel Investigation of Per forated Split Fla ? s fo r Usc as Dive Brake s on a Rec - t angular NACA 23012 Airfoil . ACA ACR , July 1 94 1.

3. Ha rr is , Thomas A .: The 7 by 10 Foot Wind Tunnel of the Nationa l

Ad vi s"ry Cornn, i ttee fo r Ae r onautics . NACA R.ep . No . 412, 193 1.

4. Wenz i nge r, C arl J. , and Hal" ris , Thomas A. : ~i'ind - TUlmel

Invest.ig ,· tion of an NACA 230 12 Airfoil with Various A rr nge - monts of Slotted Fl~ps . NACA Rep . No . 664, 1 939 .

5. Weick , }' r ed E. , and Wenz ing e r, Ca rl <T .: Wind - Tu:nnel Research ComparinG L!l.teral Co nt r ol De vi ces, Particularly at High Anlj l es o~ Attack . XI I - U Dper - Surface idle ro ns on Wings with Sulit Fh s . NA CA Rel?' No . 499, 193L. .

6. liYonzinge r , Ct:.~rl J . ~ : i nk -T unn.e l l\~easurement s o f A ir Lo~ds on Split Flaps . NL.CA TN N o. 498, 193L~ .

7. Wenzinger. Carl J. : Pr ess ure Distribution ove a Cl a rk Y- H Air "foil Section with a Suli t Fla p . lECA TN No . 627 , 1937 .

8 . Wenzinge r, Carl J . , and Rogallo , Francis M .: Resume of A 'r- L oad Dat on Slats and Flaps . NACA TN No . 690 , 1939 .

Irving~ H. B ., and Mc~"i l lan, G. A. : Some E :<pe rim en t s on the Ba1a.ncin of li ' ing B ra ke Fla~s . R . & M. No . 1864, B ritis h A.R . C ., 1939 .

10 . J acobs, Hans , and Wanne r , Ado lf: DFS Dive -C ont rol Br~kes fc Glide l"S and Airplane s; and Wanner , Adolf : Analytical Study of th e Drp~g of the DFS Dive - Control B rak e . NACA TY. No . 926 , 19 40 .

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~ (al --"- o -.4 -.2 o .2 .4 .6 ,8 1.0 /,2 Lift co efficient, C L (a' Aerodynamic characteristics.

figure 3 (a' .- Effect of 0.20e ~artial-span center-sec ti on perforated double split flaps lo cated 0.20c from the airfoil trailing edge of a SO-inch span 3:1 tapered NACA 23012 o ~irfoil. OfU,60 ; Of L,600.

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(a) o -.4 -.2 0 .e .4 .6 .8 1.0 I.e Lift coeffici ent, C L (a) Aerodynamic chaxacteristics.

figure 5 (a).- Effect of O.20c partial-.pan tip-aection perforated double split flaps located O.20c from tbe ~lr!o11 tral1ing edge of a SO-incb span 3:1 tapered NAC4 23012 airfol1. OfU,60 ; 6fL,60o.

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ci tip-se~tion A chord located ge characteristics ed • span 373 Root (b) Effect 0 ~+-~-+~-r-~ I CA 23012 o flaps - 60

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o 20 40 6 0 80 1 00 Flap span, percent airfoil span Figure 6.- Iffect of flap span on lome of the aerodynamic characteristic i of a SO-inch Ipaa 3:1 tapered HACA 23012 airfoil with 0.200 perforated dou bl e I pll t flapi o located 0 . 200 from the airfoil trailing edge. OfU,60o; OfL,60 .

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o - .4 .2 1.0 1.2 .4 -.2 .6 .8 o Lift coefficien t, Ci.

(a) Aerodynamic characteristici .

rigure 7 (a).- Effect of a 0.20c full-Ipan lower-aurface perforated aingle aplit flap located OD a line through thl 30-percent-chord atationa of the airfoil aectiona of a SO-inch span 3:1 tapered _ACA 23012 airfoil.

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o -.4 -.2 .6 /.2 a .2 .4 .8 /. 0 Lif f coe f ficien f, C L f1gure 8.- Effect of O.cOc p&rtl&l-I~an lower-surface center-Iection perforat8d 11 ngle split flapi located on a line through the 30-percent-chord stations of the airfoil sections on the aerodynamic characteriBticB of a 60-inch span 3:1 taper8d ilCl 23012 airfoil. 0fL , 60o.

HAC A Fig . 9 . /.- --r---,---.---.---.- ---.---.---.---.---.----.---.---,---.---.---.---.---~ . /~--~--+---+---4---4---~--~--_+--_+--~--~~--~--r---+---4---~--4---~

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Lift coefficient, C L Figure 9.- Effect of 0 . 20c partial-span low e r-surface tip-section perforated Bi ngle split flaps located on a line ~hrough the 30-percent-chord stat i ons of the airfoil s e ctions on the aerodynamic characteristics of a 60-inch span 3:1 tapered NAOA 23012 airfoil . OfL , 600.

Fig . l C NACA E ..

~-----------------------c ....

I I I I

J § c · o I Tip-section flaps . ~ ~ " Center-section flaps :t :t q, "

oJ u ____

1 ___ -r--...-._

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~ t}I ~-J2 o o ~ W W 00 ~ Flap span, percent airfoil span Figure 10.- Iffect of flap span on some of the aerodynamic chara ct e ristics of a S O-incb span 3 :1 tapered NACA 23012 airfoil with 0.20c lower-surface p erforated singl e split flaps located on a line through the 30-percent-chord stations of the ai rfo i l sec t ions. OfL' SOo .

Fig. 12 NACA I.e !'--'"

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0 4 /00 .1 ; o o o 6 8 2 4 o Time, t,se c Figure 12 . - Co m puted time-history characteristics during deceleration of an airplane equipped with f ighter brakes consisting of O.20c full-span perforated double split flaps located O.SOc from the wing leading edge.

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Document details

Doc number
·
NACA-WR-L-373
Publisher
·
NASA (NTRS)
Year
·
1941
Pages
·
23
File size
·
11 MB