ImageVerifierCode 换一换
格式:PDF , 页数:48 ,大小:1.38MB ,
资源ID:836372      下载积分:10000 积分
快捷下载
登录下载
邮箱/手机:
温馨提示:
如需开发票,请勿充值!快捷下载时,用户名和密码都是您填写的邮箱或者手机号,方便查询和重复下载(系统自动生成)。
如填写123,账号就是123,密码也是123。
特别说明:
请自助下载,系统不会自动发送文件的哦; 如果您已付费,想二次下载,请登录后访问:我的下载记录
支付方式: 支付宝扫码支付 微信扫码支付   
注意:如需开发票,请勿充值!
验证码:   换一换

加入VIP,免费下载
 

温馨提示:由于个人手机设置不同,如果发现不能下载,请复制以下地址【http://www.mydoc123.com/d-836372.html】到电脑端继续下载(重复下载不扣费)。

已注册用户请登录:
账号:
密码:
验证码:   换一换
  忘记密码?
三方登录: 微信登录  

下载须知

1: 本站所有资源如无特殊说明,都需要本地电脑安装OFFICE2007和PDF阅读器。
2: 试题试卷类文档,如果标题没有明确说明有答案则都视为没有答案,请知晓。
3: 文件的所有权益归上传用户所有。
4. 未经权益所有人同意不得将文件中的内容挪作商业或盈利用途。
5. 本站仅提供交流平台,并不能对任何下载内容负责。
6. 下载文件中如有侵权或不适当内容,请与我们联系,我们立即纠正。
7. 本站不保证下载资源的准确性、安全性和完整性, 同时也不承担用户因使用这些下载资源对自己和他人造成任何形式的伤害或损失。

版权提示 | 免责声明

本文(NASA NACA-TN-4185-1958 Wind-tunnel investigation of effect of sweep on rolling derivatives at angles of attack up to 13 degrees and at high subsonic Mach numbers including a semiemvati.pdf)为本站会员(progressking105)主动上传,麦多课文库仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对上载内容本身不做任何修改或编辑。 若此文所含内容侵犯了您的版权或隐私,请立即通知麦多课文库(发送邮件至master@mydoc123.com或直接QQ联系客服),我们立即给予删除!

NASA NACA-TN-4185-1958 Wind-tunnel investigation of effect of sweep on rolling derivatives at angles of attack up to 13 degrees and at high subsonic Mach numbers including a semiemvati.pdf

1、NATIONALADVISORYCOMMITTEEFORAERONAUTICSTECHNICAL NOTE 4185WIND-TUNNELINVESTIGATIONOF EFFECT OF SWEEPONROLLINGDERIVATIVESAT ANGLESOF ATTACK UP TO 13 ANDAT GHSUBSONICMACHNUMBERS, INCLUDINGA SEM3,EMPIRZCALMETHODOF ESTIMATINGTHE ROLLINGDERIVATIVESBy JamesW. WigginsLangleyAeronauticalLaboratoryLangleyFie

2、ld, Va.WashingtonJanuary1958s3.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-TECHLIBRARYKAFB,NMT.,-.P.,NATIONALADVISORYCOMMITIEETECHNICALNoTEI!llllllllllllill;ll!FORAERONAUTICSUClwhereasa stableconditionisindicatedonlyattheextremeratesofroll.Theres

3、ultspresentedinfigureU showthat,ofthewingsinvestigated,tl.d.splanformshowedunfavorabledamping-in-rollcharacteristics(indicatedby C overthelargest. testrangesofMachnumberandangleofattack.thatis,zeroorslightlynegativevaluesareobtainedattheloweranglesofattackandpositivevalues. areobtainedatthehighertes

4、tanglesofattack.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-8“Infigure13, thevariationsented.Negativevaluesof pof CyP withangle(lateralforcedueindicatedatthehighertestanglesofattackandatNACATN4185ofattackispre-torolling)aremostMachnumbersforallco

5、nfigurationstested.A discussionandpossibleexplanationofthebehaviorof Cnp and Cy throughthetestangle-of-attackandMachPnumberremgeandamethodforestimatingthesederivativesarepresentedinthefollowingsection.EstimationsofRollingDerivativesRollinRmomentduetorolling.-A comparisonoftheexperimentalhowever,thee

6、xperi-mentalandpredictedvaluesshowsimilartrends.Yawinamomentduetorollinz.-Inreferences14and15,methmlserepresented”orthepredictionof Cnp throughanusingcorrespondingexperimentaldragdata.Thehasbeenshowntopredictp throughthetestangle-of-attackrangemethodinreference14angle-of-attackrange .Provided by IHS

7、Not for ResaleNo reproduction or networking permitted without license from IHS-,-,-2T NACA.with.*enceTN4185 9considerablybetterresultsthanthemethoddescribedinrefer-1. Thisresultisprobabwduetothefactthatthemethodofref-erence15predicts%p yetirapolatingfromthepotential-flowtheorybyuseofexperimentaldrag

8、dataandanempiricallydete?hinedfactorthatisproportionaltoadrsg-centermomentarm;whereastheprocedureofreference14predictsCn byusingtheexperimentaldragdatatoPproportion%p relativetotwolmownconditions.Briefly,themethodofreference14consistsofproportioningp relativetotheconditionofpotentialflowwheretheresu

9、ltantforceisnormaltotherelativewindandtotheconditionforwhichtheresultantforceisnormaltothewingchord.Anequationispresentedtheretiforevaluat Cnp fortriangdsrwings.However,forotherwingplanforms,thisequationmustbenmdifiedasfollows:thepotential-flowvalueof p fortriangularplanforms(ref.16) mustbereplacedb

10、ythevalueforwingsoftaperratiosotherthanO,andanadditionalterm,showninreference15forlow-aspect-ratiowhgs tobearesultofwing-tipsuction,mustbecon-sidered.Withtheseconsiderationsapplied,thefollowingeqmtioncanbewritten:a71(C%=-CZptsna-K-CZp tanm- )()b% + Cnp (1)CL tip suctionwherethepotential-flowvaluesof

11、 p/ canbedeterminedfromref-erence17aneitherexperimentalorchowever,thisresultisnotsurprisinginasmuchastheexperimentalvaluesof Cyp fortheunsweptwing(which=e dueprimarilytotipsuction)presentedinfigure17indicatethat,withinthetestrangesofMachnumberandangleofattack,thetip-suctioncontributioncanbeneglected

12、.ThedataforaMachnumberof0.15(fig.17)wereobtainedfromreference18.Theleading-edgecontributionto Cnp wouldbeexpectedtovary.considerablywithleading-edgeradii;consequently,infigure21low-speedProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-N(4CAm 4185 IL.r

13、esultssrepresentedfor12.percent-thickwings(ref.19)whoseleading-.-1 edgeradiivsryfroma verysharpone to a very bluntone. Thewingsreportedinreference19hadanaspectratioof2.61, a taperratioof1.0,and450sweepback.A comparisonofexperimentalp withcal-culatedvaluesevaluatedbyuseofequation(1)ispresentedtifigur

14、e22forthewingsofthepresentinvestigationatvariousMachnmberswherebothexperimentalandcalculatedvalusof Ctp wereused;thetip-suctioncontributionto C9 wasassumedtobeO. Theagreementiscon-sideredgoodforallwingstestedwhereeitherexperimentalorcalcu-latedClp areusedinequation(1),andtherestitspresentedinfig-ure

15、s21and22indicatethatthepresentmethodofestimatingCnp(eq.(1),withouttip-suctioneffects)isapplicableoverlsrgersngesofleading-edgeradii,wingthickness,andsubsonicMachnumbers.Lateralforceduetorolling.-Anexpressionfordeterminhg Cypforthepotential-flowcasecanbeobtainedfromreference17andwrittenas.4and,forthe

16、nonpotentialthewingchordplane,Cyp= CL A+cosA t=AA+kcosAcase,whentheresultantforceisnormaltowouldbeeqwl toO. Byconsideringthetip-suctioncontributionandbyapplyingthefactorK,theequationcanbewrittencYp (=K )+cOsA tanA +A+4COSAwherethetipcontributionto Cyp canbe() (2)p tipsuctionexpressedas()CYP %=tipsuc

17、tion AInfigure23,valuesof Cyp evaluatedbyequation(2)andvaluesdeterminedbythepotential-flowmethodofreference15arecomparedwithlow-speeddataofreference19. Intheapplicationofequa-tion(2),thecontributionofthetipwasassumedtobezero;however,. theorderofmagnitudeofthetip-suctioncontributionisindicated.Provid

18、ed by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-I-2 NACATN4185inthecomparisonofthevaluesdeterminedbytheproceduresdescribedinreferences15and17.Betteragreementisindicatedwhenequation(2)ofthepresentpaperisused;however,thisagreementisnotsurprisinginasmuchasthe

19、methodsofreferences15and17donotaccountforanynonpotential-floweffectsontheleading-edgecontribution.Theresultsofthepresentinvestigationarecomparedwithvaluesevaluatedbyuseofeqyatidn(2),withouttip-suctioneffects,infigure24. Theagree-mentshownisreasonablygood,particularthenegativetrendindicatedatthehighe

20、rtestanglesofattack.CONCLUSIONSAninvestigationconductedtodeterminetheeffectsofsweepangleontherollingderivativesathighsubsonicMachnumbersandhighsnglesofattackfora seriesofsweptwingswithaspectratioof4,taperratioof0.6,andNACA6zo06airfoilsectionsindicatesthefollowingconclusions:1.Theresults showlargered

21、uctionsinthedamping-in-rollderiva-tive Czp atthehighertestanglesofattackforallwingstested.Ofthewingsinvestigated,theresultsforthe32.6osweptbackwingshowedunfavorabledsmping-in-rollclw?acteristics(indicatedby Up) overthelargestrangesofangleofattackandMachnumber.2. Wingfencesonthe45sweptbackwingatthe65

22、-percent-semispanstationareshowntoimprovethedamping-b-rollderivativeCzp atthehighertestanglesofattackrelativetotheclean-wingconfiguration.3. h general,thevariationofthedamping-in-rollderivative%patzeroangleofattackwithsweepanglewasonlyinfairagreementwiththepredictedvariationwithsweepangle,inasmuchas

23、the32.6sweptbackwingshowedmoredampinginrollintheMachnumberrangefrom0.85to0.93thananyoftheotherplsmforms.4.Thepredictedvariationof Czp atzeroangleofattackwithMachnumberwasingoodagreementwiththeexperimentaltrenduptothecriticalMachnumber.5. Contrsrytopredictionsbasedonpotential-flowtheory,theyawingmome

24、ntduetoroll- Cnp waspositivemd thelateralforceduetorollingCyp wasnegativeatthehighertestanglesofattackforall.#y-.4wingstested.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-NACATN4185 136. Theresultsindicatea lossinwing-tipsuctionwithinthetest-i ran

25、gesofMachnumbersndangleofattackinvestigated.7. PresentedhereinisamethodofestimatingCnp (yawingmcmentduetorolling)and Cyp (lateralforceduetorolling)throughthetestangle-of-attackrange.Thismethodisshowntobeapplicableoverlsrgerangesofleading-edgeradii,wingthickness,andsubsonicMachnumbers.LangleyAeronaut

26、icalLaboratory,NationalAdvisoryCommitteeforAeronautics,LangleyField,Vs.,MarchU, 1954.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-14 NACATN4185REFERENCES1.Wiggins,JsmesW.,ad Kuhn,RichardE.: Wind-TunnelInvestigationoftheAerodynamicCharacteristicsin

27、PitchofWing-l?uselsgeCom-binationsatHigh-S.g79.2785.37 4:3491.46 3.81lfx).oo 3.35Leading-edgeradius=0.0006z.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-:T.%NACATN4185 17L1-fti iReknivewind RollingmomentandrollingvelocityzFigurel.-Systemofaxesused

28、showingpositivedirectionofforces,moments,es, =d elotiesa71.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-.Fuss81Length 49Ehl.Atarn.dish. 5 in./+tion of max. dknn 30 in.T 30” % -.,S?6”-=-+_. %3B-4-O.6-CW6Figure2.-I13,?.6-4- 0.6-006Sketch of fourWhg:

29、Arua P.W Sr/ftSpan 3.oftcm? 675in.Root ii25 in.Msan aarvoamk W 765ftASPSCtrut.% 4.0Taper ratio 6?6imidsnce oRimi oAiWi smtbn/waii8i to fueei NACA 63A08 $ 04 .08 .12 -,0804 0 . .08pbmPbm 27(b) 32.6-4-.6-006 ting.Figure8.-continued.IProvided by IHSNot for ResaleNo reproduction or networking permitted

30、without license from IHS-,-,-Unflacjtjedsymbok, cktm wingFkgged symbols, fence onQ=/08 a= /2.9.04M Ao .03 0,8500 .02 0.7UU0 .0/ o.509q o 0-.01-.02-.03-.04-./2 -Q8 -,04 (_(_ .(% .(% ./2 -./2 -.08 JJ# $ .04 .08 ./2m 2P(c) 45-4-.6-006 Wing.Figure8.- Concluded.1. . 11 IEt=Provided by IHSNot for ResaleNo

31、 reproduction or networking permitted without license from IHS-,-,-NACATN4185.27M.8500moo .0/5oocn oMB500.500 c o-.0/From b-#o+gpia pb- From+nto-w= /3u-./2 -.08 04 Opb2VFigure9.- Variationofyawingmomentwithinhightestangle-of-attackrange.04 .(28 ./2wing-tiphelixanglepb/2V “-3.6-4-.6-006wing.-Provided

32、 by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-M93 h.91 A.550.70 n500Czpo0000.I-2-.3-.4.,024A ngfeaFigure10.-.6 8 /0 12 Mof C?t)ack,a, day3.6-4- .6-ci)6 wing.Vaxiatioof ClPnotcarectedru0302468 #j2j4Angle of utfmk, Q,d.(b) 32.6-A-.(5-006 W*.with angle of att

33、ackforwingstested.Datafor aeroelasticdistortion.IIProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-. a71 IIll(Unfged symbols) cleon whg.93ho -(Flagged symkk+j fence onMUnce&inties Indicated on fure8. I.9/ A.850.70a75.500“O 2 4 6 8 /0 IZA ngfe of attack, a, deg(C) 45-4-.6-006 wing.Fre 10,-000000/4(d)02468Angle of atfack,a,cg60-46-006Concluded.wing .!2Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-

copyright@ 2008-2019 麦多课文库(www.mydoc123.com)网站版权所有
备案/许可证编号:苏ICP备17064731号-1