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NP^CR L[ NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS WAllTIll ME RE PORT ORIGINALLY ISSUED November 1945 as Advance Confidential Report L5G10 EFFECTS OF COMPRESSIBILITY ON THE MAXIfIM LIFT CHARACTERISTICS AND SPAiWISE LOAD DISTRIBUTION OF A 12-FOOT-SPAN FIGBTER-TYPE WING OF NACA 2'-SERfIES AIRFOIL SECTIONS By E. 0. Pearson, Jr., A. J. Evans and. F. E. West, Jr. Langley Memorial Aeronautical Laboratory Langley Field., Va. NACA WASHINGTON NACA WARTIME REPORTS are reprints of papers originally 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 now unclassified. Some of these reports were not tech- nically edited. All have been reproduced without change in order to expedite general distribution. DOCUMENTS DEPARTMENT L 51 Digitized by the Internet Archive in 2011 with funding from University of Florida, George A. Smathers Libraries with support from LYRASIS and the Sloan Foundation http://www.archive.org/details/effectsofcompres001ang U.-AJA ACR No. L5G10 NATIONAL ADVTSORY COMMITTEE FOR AERONAUTICS AD- !3I CC: :,DET.IAL REPORT n?...,I. ,II C .CiE : e ..r 1.-" -.:T7i LIFT C'? 12-I"-CF --'I,-'- I l- CF n- J I-L Z TiTI(-IT r, E. GC. F: :"-': *T A. *J. E;;-s. L,.& 1" i ", _. ', *. Fc.rce sr. red r : r.e-di stri ution r s-c- 0 arcr, e- n c c ere made on a f'ir r e:--t :e vwi. r .:.1 of f ,-.- -t onr -l iT!ACA.C 2 C- -iet i: -- r .: in .l J.-. : 10-faot hicK: ..-,e-:i. t :.-,l t- c"t -t. ? ..V: th ee -- o, re.-- i- bil- t thee -:i. '- ;. 1l c. s .- .. e .- t c a., ,t n- :-i I.. vwise lo?.,J c'.i tr-l-;.>r.,.:*'. .. := T -, .. ..E :i n-" ,,f att ,2.: ,: irve tica- er ': .:- ft :n -1i '- to h h :ber r-n .e was from ,.C2, t. 0. t 7.-aii ainC. :-ediu ..rL e f attack and from 0.15 .'., ', C 'rr -- 1 rre r-.ries f ttac::. In the i.'.a:h nur.'zer r-rgre frm '. 15 t 0.5 ',5 theF mnaxiru.m l t c ieff' i': c nt -'r.t ino .t : ','ith rnc re :si3r.7 i.Ccnf ...-...' a" .e'r.>-,r se -ra '_I--r. ter ha-,',inr re. cea ec a ;'ta.: ''. t a ch r :. .:..f ,..-0, at .[., c: nt.:'l ;-T r : i- e" '.Ih,.- '- r :. : r 2,e i ,..2i r^- .-es ,i :n. :t i;,..]tri lift cce:-"-ci -; c r- irr ": '.. -1. z .:.-_er c .:..- c,-_ -, -- !" ,'J.-..ed. At J t": e f-1-. li :. c it i. u-iI to Ain.' P r e 'v.-_t' :. le I f .c i:c..? .;: ,1 .-'- tiE :i. n l at whl ic" r. ..r: :e, f- ,r. re a T.-. ,; -a,,-. tii-- 7.,1',: "': _, rn the .a -i:"j.. li 't c l i 'L rT r -. a.." : l'- to 1I'' c .-n t1-: r aL --l . Io i ini -,- n cl-.-,,.i ,s in t.e s<,an l :-d1 di- :tr.ib.tio:i wer. f,.,' to:' cu r ic' -he :t: all :it r:;-- -f th-: t st sfeeCs. ."-n the 'i-, sta iil .:.t i;h :-rm. c s, the-. result nL l,- ad unce. -. "'nt S ,',Jerat- .:.iut. :ar. SLt ift, wla ch resulted r i i :ease iin ot '--din;- r .: =rt 't. to about 10 p-,rrcent. NACA ACR No. L5G10 INT TRODUCTIOIT Wind-tunnel tests of a rectangular wing of NACA 0012 airfoil section (reference 1) showed that the maximum lift coefficient reached a peak value at the low Mach number of 0.19 and decreased rapidly as the L.. number M was increased from this value up to the highest .T-.:- number of the tests (Mi 0.35). Although these tests were necessarily limited in scope, they indicated the importance of a knowledge of the effect of compressibility on the maximum lift coefficient both in the estimation of the maneuvering performance and loads of high-speed aircraft and in the-interpretation of wind-tunnel maximum lift data as applied to the-prediction of airplane character- istics at low speeds. More- recent two-dime.nsional. wind-tunnel tests of a number of propeller-type -airf.oils over a relatively large is.iC number range (reference 2) showed effects for the thicker airfoils similar -to those .o.f reference 1 and in addition .showed large-increases in the maximum lift coef- ficient starting at iach -numbers of about 0.5. Flight tests of fighter airplanes reported in references 3 and 4 showed..large decrea-ses in the lift coefficient corre- sponding to the stall.up to Mach numbers of about 0.6. A high-speed wind-tunnel investigation of a number of three-dimensional wings of different airfoil sections has been undertaken to provide more detailed information on the -high-speed stalling phenomena. Measurements to determine the' effect of compressibility on the spanwise load distribution were included in the program because of the related importance of the load distribution as a determining factor of the strength requirements of wings.- The present report gives the preliminary results of force and pressure measurements in the Langley 16-foot high- speed tunnel on the first of a series of wings. The model tested was a fighter-type wing having an aspect ratio of 6, a taper ratio of 2:1, and conventional IIHAT'. 230-series airfoil sections. CO7 TDE:?I AL CONFIDE_' IAL TACA ACR :T,-.. L5C-'10 V trp."c QCrr l. fe t IC second Sc:ree, 71 cf :, il,:' in .iii.r ft r ,.rec ,_nd r,': "'A r. er ( ) p ir. r -;.=n t ', -1 r .. i-i-. ,' --- f 'ot R 1R n', .' n'.:. i'e, - p r, / p coefCxiciernt .',f '"i co-ity :.f :ii. ,'ILo- rer Lact--ecord iTn f-i'rc in-: ad- ':ol e i-t tM u .:ii tui ed st rea t-. value . C C ior.- '.:- : .-..1 -C r A c. r r t1 ..t tlir. s t, D eq i .- I Ci. .ne g P > -. tiv ti.-;n-l te -t r e:-t on, s- / /.c , S v.inf ;-re j.:u-.--e feet b vi; .i _n', feet 7 s : n ..- :! .: _e m' r 1i f r.n the ;l e d.:' .. 1. L c. aii f.il ch'r.,", t pl- n .:f -- :"me-i ..., feet r,.e t 1 ch:.,rd, fe 1 2 ) . ..I, C*i2L At : 11-IHe lc feet t 1- ii.r r'-.. r, ; % i rf.-I fl-r. i.,n CO? .-.. f..hn'.ing T : r'- '- 9.:-, O_- :.ri i e t C C' F I LIBi? ThE C D':I D 7i". AL '7.,-,- Q L._ ,_ . 4 CC'ITIDE.'IAL NACA ACR No. LSG10 L wing lift, pounds CL wing lift coefficient n section normal force (force per unit span), pounds per foot cn section normal-force coefficient n I c load coefficient cs / b I c .2 0C, wingp normal-force coefficient 2 -V 4 c -cn dy . a corrected anPle of attack of the root section. (section at the plane of syrm-etfry), degrees dALL angle-of-attack correction due to the jet bouni.nrv-induced uopwash at the lifting line, degrees (57.3 6 5 L) 8 a function of the ratio cf wing span to tunnel diameter 1 + 4 b 8 16 \D/ 64 D da3SC angle-of-att'ack correction due to the jet boundoary-_induced streamline curvature, degrees '-5 Dl JLL\ \l " APPARATU.S AND -TTHODS A diag.ra.ratic sketch of the -"ig model used in- the tests is given in figure 1. The ohrinci.-1' dimensions given in the fig-ure and other pertinent information are given in the following list: COTTPIDE-TIAL .,ACA ACR -o. L5G10 CC'I;FIDE:TIAL 5 p t . . 1 Sft . . i T .=-. c t . . . -'"c rit C :. -; or -.: n..A lic ti"; "t '. ut) *:', 7 , Tip < .r 'on .. .. .. 7.'. . ihec ...al ( i. c r: le 1i chcr'1 line) ..e . 7s':eep.:ac!: ( il:n -L. 4 ch .ra line), cec 18 The .i:ng :.- :. i ilt-.p :- 61 ,? -,-,tm:' \rtio:, sand m ." s mnE.chine.d in vuch a ;a::Lre: A.'it s. f ce eCle:..ent-t c DTL'",iecting eq, al perce.-.ra e-cl-w,,-.-, _, :., 7 r h- roct ac ,i t r .-1tia-,-s :ere st ra 1-.t lines. Thirt--tr re :e-'e r e r'ifi -e se i :tr t''.t d c 'er each of sI 'i ?.-- c -.n-, t :-.. ,:a-'' Fe L. atiot:? ..:rich are i' en i, -1 :-e .'e c ro ."' i st" .i :l i:r. .f presz,.'re ifi.:s -.' a t--'ical :ec t n i ?l.:o 'h A in fi;:ire 1. T : r: -ure t' .'Iere or .u-1. t o t of t.e "'i.In to :n ltir.lc-t ; :.,e er -- i t e t c -- .:e L :ieans of the bt, :.. .nt L.r...- i.n - iure .' th i r T te-t -.e 'tco : rr u.t *.' - removed i-d 'I-,e -.. re c l.:ce '.ith a r :ii r-. '.sich" is .shown iL: fi, ire i. The *-n. 'n.as ,.ntel. a -t the t1um:el e r.ter llne r shielded .?ru : h -.- ncr a tlic.:ness-r.:or.. ?ti. of 0.15. The te .i .r.e K-t r. rac i c c'e '. '..a? C. 4. - ure .3 i a .'-ac o r'h f '. he -u inc sc.-ntc: '..'- r-c' in Vie t'-r.el c r the for- te es.. I -.: rcf -:.> te-t r _-J : e-*e : ith ':. L-'? of a c :c. -. .,.:- t .-'t :.',', 'i e : e turL "iel S. n e 'I .- .. ied fr',' aboit 150 ailes 1 r he .i. t- t: :-._r.'.r: -e a'.. _r".ir 'abl in-, c-, -r -vin. -_ :.'_ f.' at -- :,..: t' e_?- C an 4 .Ei..- a.:,.r ..:i .t, elr- 20 11 s 3 ere 'u .- r. 'The ccrr.e- D .C r nc.... -.. .. .r -e i C _x 1. an t e c:r -= -c n.. i e:.rC .F :-. e s fr o > e- t" :-. 1 x 1 i e- e -I .:. - t .i- n 3f' '- er.e .en .-i n'.- --.:? .-;i- i- :-- :.,- c ve ; i r-'- iC s -" : f :.t c: -"1.t i.L-.--L-,0 .:; ts : .' l e1 Lu ,.el s eed -l a -:,'t -' .[* 1 A 16 iE .:i.-, :..: rre- s-'of-ds tI a [ac.h n.r,;:.er cf acut 0.i,'5. In -i e d ter- i'.:i r i -..c o .a; --i..:.u,i li-t ,c ; :..- .e ra s a .... t i nt 1 ects '.e-e ...e ,itfh th? t;n -iel r. ,e held. o ;sta',1 while the an e of attac- "'- -. -ied in rl- recio.e ne ,r r -a:u -u lft. The *7 on.e c_-le-of-att ck r.ane f' t'-= teots v i os from -i', t.: '4c C,'I ,IDEi: 'I.L YACA ACR 'D. LSC10 in the lood-distribution te-ts' the static pressures over the six wing sections, as indicated by several mul tiple-tube manoreters, vere recorded photographically. The chordwise pressure distributions determined from these photographic records 'ere integrated echanicall-' to find the e -ct i1 normal-force coefficients. Force data. The force data have been corrected for strut tares, air-stream misalinement, and tunnel-wall effects. The strut tare forces were deter -mined from tests with the wing inverted with and u-ithut image st.:' :rt struts I installed. A photograph of the inverted : win2 with tohe image struts instal ed is given in figure 5. The largest increments of lift coeffLci ent due to the support struts v-ere between 0.07 and 0.04. The effective miLsalineTrent annle of the air stream was determined front te ts of the .in, u-ri .ht and inverted with the image struts installed and was found to be constant at 0.150 throughout the speed range of the tests. In order to prevent air leaCkae through the strut shields, thin rubber diaphragms were fitted around the bases of the shields An additional correction to the lift was necessitated because of a pressure differential across the disphragms. This pressure differential was measured during the force te,-tE by means of a nicro- mancmeter, and a calibration was ~:sde with the wing removed to determine the variation of lift f force with pressure differential. This correction was very small in the region of maximum lift (less than one-half of 1 percent at all speeds). The effects of the tunnel walls were accounted for by the methods of references 5, 6, and 7 as follows: The principal part of the angle-of-attack correction given in reference 5 is -ALL = 5.36 CL d ee This equation is strictly valid only for the case of an elliptical spanwise load distribution. A check calculation CO -IDEKTIAL CONFIDENTIAL ITACA 2 No. L5G10 CCTT DI' TRIAL 7 by a more e-xact but more detailed procedure based on the e::_ erinentally determined span loading revealed that the 'l-i :. -.;. "'- i "" f- .7 :,." : ": L 1' of 1.0 thIe ":e.E: t"ia r A: .. .:'' ect -n t .-r ie of ttta c..: due r n nr: ",ced ci .t re : L .:. ; c cul:. 1 D o2 S. e e ', L . and_ .. to., /-1 T I- iThis e-.,.a ion is ba-e ,: e ,.: i i:- .. :,".r-e--- itl he- cfl T o e 1 7 ..- F e. o::a "... n. ., r' '- .. '_'. 7 _" 7 ,, rr t -. I U c i 1 'ach riL..< CLr .'. . C.r.re _ct t. h- i : : .. .a vre:sure, and :;r.ch : ;".. .:" : te... c n- it : i-i:t Cue to con'stic'-e.:r. effec ;--r ca a e r.'.e -.etI':d :'-' re.fere .e '. a-.'" '' : ct r e '. i-- i . )- 4 I- ct S '-c t .La o ama 2 :.re the :r &d.t' Ar.d fii t c1 a rectar-'m'lar ur.tnel. c: 5 CE:, is the .;;n- p rof 11-:1rse coef ici Z The t'-,' e ns of .e 1 t the en fi n tgiv? the v loci ; i -cre -e. t. d'i e, -- ec ly, :. tu"' solid'* co tfrlct:.-r an- ".':a.:e 2r s:r cr.-- i : .ne S".- .: the f e a :iitu.de of the -'_:e c::nw-,. {-ti,?n effect i a f-''ic' ti.n of the -elo -city lo. i : --'" .: "-_" r.'r" ize :' t th e- r e* ti U n i? exrre-sec ir. re."' ,- :f t::e or .,-.f. ':- c the.re. ical r' ea9 n. n 3 ']- 1e _r:.:I le.. of c,,'I triic- ti-)n :ffe r,: fi:. :, ?:-- '. e .* ,-- i- -i c r,: .,r tur -el ;:iets at the r'r I-ent t i_ ar: :.. '- -e .::_ r I- t r z- h t-_ re:.r--Cent :r.e e.-t :.'ai la l. e ..:-r... r.. r-i, AT p,:.:ified for the :a-e if' the i: rcwl .-el, .he e' i'..Ati '-- ecr,.e _r ,-'',.6 t +. __c, -( .>)20 4>: KI i2 2: OK- ID:::TI AL.. ( 00: ....IL UAC" T 7-` L -10 where -a in this case is the .. eg height of the tuel in the regio occupied b, the iming. The_ constrictior. corrections to tIe dy-namic pressure, -:ac-h nu nber (refer- ence 5), ad. v:in- lift coefficient are as o Ilows: 80 2AV --S 2-Q 1-= 1 + 0.2T C Q The corrections r: ere small f. r low anrcle of attLc over the r nire ch .n.u-:;er range. At a georetric an;le of a c. of a a n r of .7 th corrections to the lift coefficient .nc ach n r ere, respctively,. 1.0 percent and 0.6 percent. At angles of at.acc above cthe stall here te drag becere very lar'e (-n1icm.tive of a 'lare vaie)) the corr~c<-iois aOeri f7oe i o,-tance. At a eor.eKi'o an"ye of attac- of 24 arn a lach number of 0.6 the correcon:. th lift co cient a.-----. .ach number were 1. 2 percent nd .2 percent, r espectively. P.e s s ure-Ftribution data.- The res sre-cIstrib-ution data e... ,,ca crecreo for oe principal effects of trhe support str at in t"-at the free-st-ea val ue of static pressure and .-Inainic pressure upon v: ich the .r-s3ure coe:fficients .ere based v'era rete:m'insd ifr-. a survey of the flow in the test section -ith the support struts and shields installed. Some pmall lo_-l effects of the struts on the sani.-se load distribution re.ain. -.-:- se effects .will be discussed in the section entitled "Results and Discu ssion." The effect of the tunnel "alls orn the ,? .. load distribution wasa considered "nd found to be very '.rall; consequently these Cdata as presented are uncorrected for tunnel-'wa.l interference. .""- ~~_.,- I TU'_O " 4Wing lift characteristic! (force test res.lts).- The lift l..:: :.::- 'ie:: ,: ... ..:. .- 7, :. :,- :-' ---ie NACA "? 7-. L5C-10 COFT'L l. TAIT 9 cf a t -- .: c. 9. c f-.l.u. er re sl.- i.. P .-. *:i ' Fi-" i re ite- .:' in .r.:. i:e o t-" ter, of the Se t .-. t t i r i :L_ T 1 e r or ta-n-.i ,_. 'he 7.a..e J:tae .: t-P c'.e- t' E-,.oint ?.lT S 1- rP. -., 'e- 9-, the -'-:. zontal i--- :r.:nm >,',r c .-.-tar.t az tcn :- : ce a-- of a*ria'. .di ;-.,. :' fi -re 7. *he '-.-"i -'1 ri of) ].o': c f'_.'itt .t . w -ith .c.: n.-be, ir I-,*. ". r ;',-rr'v "nh: rma:-:im:.'t litt a :.3 : r :-''er -' 1' a t t :.... ,'' :. ., -.. e' rd ..-. .: .': 3 : -:f .c 'u .. ..- -t.'.+.,'* ;-: :,,% i- i' ? *.-L,.1',- C r c t . .: a n .. ..... . it c. I e E t -. ; Cnt c.e,?_~e r --,:r : t --. .:. 9 :I : .: -. i .f ..- .'. u.iu nl'.i ? eir .f "... .,. :a ? C .-: T :. :' : 0 .5 a : ." f .-* t : -." iet-;' -.:c- -; '-i.'. :- rc Tt. S- f'i& = t :. nJ:. t ,. t . -a,-a L i. .. nt- d t' f-a : - :i t .: .lu :- '. .-. --.. ,- -. :_ ...Z -" t: t t .: t D- - - h, ...... r -,.. . o .' .' '.. c. 5 -." 1 1 ..: e F e r *- 1 r- 1 a.:y .Lel7 t .. -. .-.t ..-c Tch i; le of :ac'c 1C'-' U 1:: ;-n:r 1 Yin :9.it at i 'c.0- or9 e- 1 1 -n . T'1 a i.. .. : r r. te 1 t .21 t e:.- t_. i -.. . t.. n ( ;-- .e. t .-:. t :. ' t'j t r-at t'-mvi. n'. L '. ti.c _.'t w' -: ir.i. :.. : -, e -ficient o "-' '. ... t I. l ~".-'" -, : -. r' cr, -. c prre :r-:'i to :> ns-e I!: :l;-rt -- -' rv *: -f ,r- --_e *, i ...a in .'a. i '-l t decreases in ".' r. r l. .- e .:.. .el.y -,a '-,'.'-i. Tt 'i rP. c expected o 'c re'. ,v "-. : i. ,r-,.,.: : r1 .r v.- nt rto .~,:-.l 1 *'.il. :' i :l' r r : .: .-r : i t : C the :-r'>.t t )c e fic .1 c Li. L r e. rle f: e (-- i'e -c )-. Thus, L :11 .. n c, e l i T-. a t :: lev t c..t) '1 :...-.. t .e a s.'. ] -,f rp :-,- a a inc '-ie. of at,:-c: o ,ly -a feew S01 ID 7t1L 10 ." 3'ITTAL ITTACA ."T- -o. L510 degrees above the .all, and the arl r lift coefficients -otainable .M..t be o-.nly sli, tly eater- than those r..rese-ted. by the lo'er cdashed curve of fi-.cre Tail b'-ffetf l a-lso li 7ely to occur en the flov: sept rates .frv:: te .In., co that pilotin- technique cannot be over- loo-ked &a a possible deter mi;nin factor. fly, at very hih .a! numbers it is possible that actual instability- S nountee, in which case hiih angles of attack '- h lift. iht bO obtained inadvertently ra t Eless Sgan.isoe oad tir.-b-aution.- Spanx:ise 1oadC .diztri- tbutin c r ve-s for- ri r of vale of in c nor-:a>l-force coufficient :4id ,ac; rii cr are uhonn in fi'ne 10. As I etiond previously- te pri ipal e "ect of the sm....o 1s ruts (wh ich i F to -incr ase the effective 'trear- velociz;) was acc d for cal. atin el .t the struts installe, _he 0oc efot of t-e :truts is to rede.uce tie .lit.. at a ien anlte f atta- a all amount and to vrod:cre a -.-liht cisuortiaon n the span loadin 'hi_ ..",tion .ay b-e seen a- a dip in the curve s of pfi u re 10 near the spanvise station X- = 0.65. The 4 lzd and O/.- dashed curves of fiur 10 r ...resent the Coad istrit.i ons before and after theI stall, repec -ivelT. It'he c::rve- of figure 11 s:--a.i-e the changes in span loa liP g cT.b -ore ?'-uad to occ zr ; tie hi-her- te'p t sceed- 9To s niicant chan c in the ---an loading were found to oc"ur belo-'' the stall at any of the rpead of tIhe test, ev..-:n .hen 1h aes eere 'll established over the center part of the. -ig. Change in the 3'an loadinv were observed to tl:e pla o e bve he high-speed stll, however, the center of load beino lifted outboard, f-_: e -.-.'.-i at the .. .her L. e -s were fou;li to be me..ate. The largest corresponding increase in ending o'ent at the root (for constant lift) was found to be about 10 percent at a 7ach nuLr r of 0.55 ac a w ing normal-fo'rce coefficie.t of aboht C.95. The chan-es in load i tribution due to stalling at low speeds 1 ere somewhat lar e r than those at hih s ...-: but ar not of particular si ificance because the total lift cannot be -fai ntaitnd beyond the stall. A comrpearison- of the exper--:entally determined load distribution curves at I = 0.i0 with those 1clculted. by the r-ethod of reference 8 is shown in fi.---e 12 for values of wing normal-force coefficient of 0 and 1.0. CO3it .- .-A.L ..CA ACR i"o. LEG10 C:)ITT F ITIAL 11 .-.e ,---ze *:.ent -h- 7 r, i" t 1--. '- U" at e?:i.-L-[ r i.r the u. -"t -I c' -,- t o' hie -i-t ,urve .. n L. -t u .-'. f- st.- of a t:-e._.. .; -' "' .-. -.ries -t i .-,.- L... . i t :7. r T re ._- _," -,-: ~, .e C, : _: . a 1- t .X -. 't .- t c".'; t c re- .: e a -,C- R ..I 9. .e t , tuE "R n i. t'. v "*:'- ,i.v.w v u .. '. 2,_ ,-,J -.-:..- c ,;" ; v-< _ i^'...1 !' f l-c ; ,'_ :_. .-r. ot ... :i t, z .- .-,,r-,- T ,-.,-' o t. t .e Ot '.;f-E .- : t i -" .-.t r.ir.. ..l .- t -..-': c c..i 'e.e .f, _i C t at uP- i._' .. e *'r.:'- .'! -Ift i U; -.. '" e; '. *. e' ac -.e t at,"- r*.i,;-. r t ... .- ...'.?t L._e .r'-, e. A.t " .i. '. -. e t i : L the n xi-:, : ?. t c ef 'i t ".:-- t -- .. 'J' to 12 i..-:.onci- t}e' 'rle at .-.. .e ,r I. ) ...i'i. s dll . .C.. ., c : _.:r occurred ..e l:'- t).-A1 .?.t& l.t'-- '- f 2,- : te sct,,. ,. .-er ..tc c -:,a:-. ,.:. cccarre- d ". ~":aXTle.d t "- _-. ,ec,. -Icr 1of "-y '-itI" r- t ,..* .f. ..- oc i:'.ir in '-: a.:9 i in *':* : :.':. at ''" :. 1 i c t-', -, 1'-" *,:c7FTL'ET-, 'T- L 12 CONFIDENTIAL HACA ACR No. L5G10 lift ,as about 10 percent and occurred at a T'.ach number of 0.55 aind. ot a vi:ing norrial-force cbefficient of about C.95. Lsrigley T;ieror.ial Aerornautical Laboratory National Advisory Comraittee for Aeronautics Langley Field, !:a. C C' Li7 L --AL NACA ACR No. L5GIO REFEREICES 1. ?use, Thoiss C.; S:.m Lffects of Reynoldt and iBach .iurb.e-rs .n thc Lift of an JACA C01i2 Rectangular .jinc in- e tne i.CA Ir.-Foc Pressure Tunnel. CA, C.' Uo. L529, 1?h3. 2. Cl.arH-, Harol. E.: ffeec s of Compressioillty on cA-XimUIr E i Lf't Co' ef ic e'-ts for Six Fr-.pc 1ler Airfoils. 1 JACA .S.C Co. L L21a, 19a . . Rhoide, iichari V.: 'Correl.ti'n of Fii'-t Data on Limit -Fressur CoefficiEnts ani. T'hir Rfatj.cn to High-tp.,i d PurE4bli *-d C critical fail Losad. .iC-&: j no. *L I2 1 12. .. Iisscn, Jar.:e' ;'., a.d G.leL.erg., Eurnett L.: Effect of vac:h ar- -I' ir o ldS :ui.imbar's on thre Fowc-r-COf f iiaximru.i Lift Coeicirt Obtainaole *:,n I F-.1-1 airplanee as Dttetmlined in Flit. ;AC t. A A ,o. 4LF28, 5. Goldstein, S., 'nd Yowuns, A. D.. The Linepr- Pertur- bation Theory of Compress ible Flw, with Ap'pli- cations to Wind-Trunnl Interference. i. F. io. 1909, Britich A.A.C., 1903. 6. Lotz, IrmganrJ Cor'rc tiDn of Dovmirnsh in indJ1 Tunnels of Circzlcr' and Elliptic Sections. ,AGCA Ti. -1o. ,ol, 1956. 7. Tho-;i, A.. Bloekace Cor-'ectio'ns an-d Ch:.ng. in the .A.E. Hi h S .ed T-uan, l. ep. 'c'. AEro 1C;1, British n. .e., U. ,. Anon.: *Spa nws e .ir-Load Liscrio'icion, AGC-1(1), Army-AIavy-C oirme:rce Co:..i c oin -:ircraftt FHequire- mernts. U. n. Govt. Printing O f.ce, pril 1958. CONFIDENTIAL COIFIDEI-TIAL NACA ACR No. L5GlO 000 cn car 42 "e 3 zyz (j j I I I I I 2 1 a z_1 y __ *\ V - - .7 -70 o - fe --- -^-^- ^ -- _:^ 3 0 ?\ ^ ^ ^r u NH -- ^ -- Co '* 1'^~ *U) l \-\ ^ -^ i A i ^ V^q r ^ i, i i ; r i Z \ ^^ '?{ Fig. 1 NACA ACR No. L5G10 Fig.. 2 44. 0 CE K.o oD YA~o4 Cl, ., ",a o t 4 0 CE .- 0c 0 . 'a 0i;. , -O'a .Z.:.. "Q' EO Cl Z I, ba *r4 Cv C.4 ... ., C S- t .-.; -4 -- NACA ACR No. L5G10 Fig. 3 _0 C.-' I.-I 0 EE bn. OC E 00 OJ4 .z o C.c NACA ACR No. L5G10 8x /0o 7 6" 4 -Q ) rz W 2 / 0 /f1ach number, Al F-/u.re 4.- Vacria,'iorn of average Reynolds .n'm7ber with Mach number. S= x2.0 f e -f. Fig. 4 CONFIDENTIAL NATONL DVSOY--- ____ __CMIE FOARNUI _/ __ __ __ __ __ OMTTEFBAEO/TC / CNFDENIA .3 4 .5 .6 NACA ACR No. L5G10 Fig. 5 co ) D4 -* mU2 bo o 0~ 0 0 .) C.) 0 00 I-I bD -4* C.0 NACA ACR No. L5G10 o .' .2 3 .4 .5 .6 .7 (*cr io = C ) ,21 2 -& -4 C 4 5 ,2 20 mo ^ = .21 CONFIDENTIAL F Cgure 6 Lv ;, cre .-* .*;: b- -r C a-.le c-.c- ar'e "-act' u- qier. Fig. 6 NACA ACR No. L5G1O .2 .3 .4 .5 .6 7 -.= ,I -.2 -8 -4 0 4 8 Lx 'eq 2 .'C 2.0 ( cr 'v=.2 ) Fure 7- cacrc et as a nc.c anacie r a.tack arnd Macn rJrnoDer. Fig. 7 NACA ACR No.. L5G10 1.6 1.4 1.Z CONFIDENTIAL _________ \ /Vaximu.m l'iff SF coefficient Lift czeffic t \ e-t obtained a.t 2 ,o o30 above the an/e of \ cz/fack oat which r/n//al .sebaraticrn of the flow fromr7 the wIny occurred (see f/,. 97) NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS CONFIDENTIAL Fi/oyre 6. - Var/at/on of winy mrncx/munrm /ift coefficient with /V1ac7h number. CL mTax Fig. 8 NACA ACR.No. L5G10 CONFIDENTIAL I _. SO -- /. : O , ' .65------^- 70 ..7 NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS CONFIDENTIAL -/Z2 -8 -4 o 4 d~q F/qure q- Variaton of wi lq ,f cfefficie 't witn ae of atracK for several/ Mctch rnmbers.. ,'2 .'6 Fig. 9 NACA ACR No.. L5G10 .6 -0-=- --- 0 0 0 __ __ E l I I-- -- -- -- .6 a0 .s J Fig. 10a,b Frac t/on? of semispan - (b) M -0.40. NATIONAL ADVISORY COMMITTEE FOA AERONAUTICS CONFIDENTIAL Figure /0. Spanwlvse /oad dislritfon curves for several/ values of winq .rjoria/l-force coe ff.,cient a d /lacr. w.va, cr. NACA ACR No. L5G10O /..*_ __ -- S.6 U ---- *J .82~ U o 0 ./ <,2 0 . -41 O^ OJ -- -- - Fig. 10c,d CONFIDENTIAL Fract,ion of sem/nspan, y (c) M-=0.50. .F/gur. /O0- Confql,'wed. Fraction of semispan., (d) W = 0. 55. NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS CONFIDENTIAL NACA ACR,No. L5G10 CONFIDENTIAL Fraction of semispan, -l (e)1 = 0.60. Fracti/on of semispan (f) M=o.625. CONFIDENTIAL. NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS F/u we /0. Cont/nued Fig. lOe,f NACA ACR No. L5G0~. Fract/iol of 6emispan , (9) M=0.65. Figure /O. Concluded. Froctlon of 'em/lpon - (h) = C. 7. NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS CONFIDENTIAL Fig. lOg,h NACA ACR No. L5G10 . c / ./t opt'Q7 I/ 1 > 0 z *| z ~L) O' ON^ 00 SQ$ $- '- < "r ^ ) lb^ K)0 Fig. 11 NACA ACR No. L5G10 sq u '4uapypoo poo 7 4 IT N -I N-. U -J 0 O ^| Fig. 12 UNIVERSITY OF FLORIDA 3 1262 08104 973 5 UNIVERSITY OF FL.RiDA DOCULIMETS DEPART',EN'T 120 MARSTON SC;EwCE UJsp-Y RO. BOX 117011 GAINESVILLE, FL 32611-7011 USA |