NASA NACA-CB-L4G10-1944 Wind tunnel investigation of NACA 66(215)-216 66 1-212 and 65(sub 1)-212 airfoils with 0 20-airfoil-chord split flaps《对带有0 20翼弦分裂式襟翼NACA 66(215)-216 66 1-21.pdf
《NASA NACA-CB-L4G10-1944 Wind tunnel investigation of NACA 66(215)-216 66 1-212 and 65(sub 1)-212 airfoils with 0 20-airfoil-chord split flaps《对带有0 20翼弦分裂式襟翼NACA 66(215)-216 66 1-21.pdf》由会员分享,可在线阅读,更多相关《NASA NACA-CB-L4G10-1944 Wind tunnel investigation of NACA 66(215)-216 66 1-212 and 65(sub 1)-212 airfoils with 0 20-airfoil-chord split flaps《对带有0 20翼弦分裂式襟翼NACA 66(215)-216 66 1-21.pdf(16页珍藏版)》请在麦多课文档分享上搜索。
1、l!l!lljippj-;,(,C ,.,“2T I.+.+”J.,* , .+ ,6-ww 1:.? !L- 140 1.Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-NACA C13iO . L4.G1ONAT1ONAL ADVIsoilycoMMITTEfiFOR AERoNAuTIcsC-OIWIDENTIALBULLETINWIIJ-TtThTNELINVESTIGATION OF NACA 66( 215 )-216,66,1-212
2、, A3D 651-212 AIRFOILS wImO.20-AIRFOIL-CHON3 SPLIT FLAPSBy l?ljcienF. Fullmer , Jr.SUMMARYAn.invest iatim was carried out in the NACA two-dii?lenSional low-turbulence pressure tunne1 of theNACA f16(215 )-216, 66,1-212, and 651-212 airfoil.sectionseqlippedwith split flaps having chord.s :?0percent o.
3、fthe airfoil.chord. The purpose was to determine themaxitum-l,j.ftcharacteristics of these low-drag airfoilSections withsplit flaps. All the present tests weremade at anywith chordwise laminations, and the surfaceswere paLnted and sanded “LliIti I aerOdynairlica.1y smooth.The slitflaps wee simulated
4、 by triangular blocks oflaiiinatedmahogany atta.chcd to the lower surface of themode1 One face of tb.eblock was cut to the centour ofthe flap portion of the airfoii lower surface. AI:jrpicalarrancment i.sshown in fi.ule1.Provided by IHSNot for ResaleNo reproduction or networking permitted without li
5、cense from IHS-,-,-,.I3RESULTS AND DISCUSSIONWiesection lift and pi.tching-momen.t characteristicsfor the NACA 66(215)-216, 66,1-212, and 651-21.2 airfoilsecti.on.sare presented in figures 2, 3, azmi.,respec-tivel. The lift and pi.tchi.ng-mcxnentcharacteristicsof the plain airfoil are included for c
6、omparison withtlheairfoils with flaps deflected. A comparison of theinaximumlift coefficients of the three sections testedin the present investigation is ,gtve.nin figure , withsimilar data fop the NACA 23012 airfoil from reference 2.Figu-,”e6 shows the variation of the increment of maximumsection l
7、ift coefficientAc with flap deflectionmaxfor the various airfoils.M examination of figure 5 3hows that higher maximumlfts vere obtained wih the plain NACA 651-212 airfotl.than with the plain NACA 66,1-212 airfoil. Khen thefap wpe deflated, however, the maximum lift coeffi-j.entsfor both airfoils wer
8、e approximately equal. Asimilar comparison between the two HACA 66-seriesairfoils shows that considerably hj.gherm.axim.umliftcoeif+.cientsfor all flap defleCtiOIW3were obtained ,riththe 1-percent-thick airfoil. The increments of maxirnrunlift c.oef.fici.entfor this airfoil sectjon were, on the:Pf:,
9、Z5Lper?ent hfgher than the increments obtainedwith the l!TACA6b,1-212 airfoil section. (See fig. 6.)We increased maximum lift coefficients for theriT;CA66(215)-216 air.fotlare attributed to the greaterthickness and consequent increase in leadin-edge radius.?igm”ep also shows that the maximum 1.ftcoe
10、fficientsobtained with the plain NACA 66(215)-216 air-oilat aReynolds r.umberof 6 x 106 erea;?proxirnatelythe sameas those obtained from tests of the NACA 25012 airfoilofreference 2 at an effective Reynolds numberof 3.5 x lo. For most flap deflections tested, theI values of CL and Act (figs. 5 and 6
11、) obtainedmax maxwith tb.e16-percent-thick low-drag airfoil were higherthan those obtained with the 12-percent-thick conventionalairfoil,IProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,- .-1Provided by IHSNot for ResaleNo reproduction or networking p
12、ermitted without license from IHS-,-,-3RESULTS AND DISCUSSIONm. e section liftand.pitching-moment cha.ractieristicsfoithe HACA 66(215)-216, 66,1-212, and 651-212 airfoilsectlocs are presented in figures 29 3, and , resEec-ti.vel?. T lift and pitchin-filomentcharacteristicsofthe lain airfoilare inclu
13、ded for comparison withthe a.ifilswith flaps deflected A comparison of theii.;iurlift coefficients of the three sections tested.in the present investigation is given in figure 5, withshui.lardata forthe NACA 23012 airfoil from reference 2.FiU”Lae6 snows the va-riationof the incrffientof maxisectilon
14、lift coefficient ACJ with flap deflectionmu.for the various airfoils.An examination of figure 5 shows that higher maximumlj.ftsvere obtained with the plain NACA 651-212 airfoilthan lviththe plain NMM 66,1-212 airfoil. When thefls.swere d.eflected,however, the maximum lift coeffi-cinfisfor both airfo
15、ils were approximately equal. Aj.fl.lalcoflparj.sonbetween the two NACA 66-seriesairfoils shovschatconsiderably higher m-aximmm litcoeficients for all flapdeflections were obtained withthe 16-percent-thick airfoil. The increments ofmaximumlifb coefficient for this airfoil section were, on the:vepzge
16、 34 percent higher than the increments obtainediththe JjTACA661.-212 airfoil section. (See fig. 6.)The increasd maximum lift coefficients for the?ACA 66(215)-216 airfoil are attributed to the greaterthickness and.consequent increase in leading-edge radius.pf,Tljj. ZISO shows that the maximum lift co
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