NASA NACA-RM-L50A04-1950 Longitudinal characteristics of two 47 7 degrees sweptback wings with aspect ratios of 5 1 and 6 0 at Reynolds numbers up to 10 x 10(exp 6)《在雷诺数为10x10(指数6).pdf
《NASA NACA-RM-L50A04-1950 Longitudinal characteristics of two 47 7 degrees sweptback wings with aspect ratios of 5 1 and 6 0 at Reynolds numbers up to 10 x 10(exp 6)《在雷诺数为10x10(指数6).pdf》由会员分享,可在线阅读,更多相关《NASA NACA-RM-L50A04-1950 Longitudinal characteristics of two 47 7 degrees sweptback wings with aspect ratios of 5 1 and 6 0 at Reynolds numbers up to 10 x 10(exp 6)《在雷诺数为10x10(指数6).pdf(27页珍藏版)》请在麦多课文档分享上搜索。
1、RESEARCH MEMORANDUM LONGITUDINAL CBARACTERBTICS OF TWO 47. SPTBACK WINGS WITH ASPECT RATICE OF 5.1 AND 0.4AT REYNOLDS NUMEIERS UP TO 10 X 10 66 ,W By Rein0 J. Salmi and Robert J. CarroSd 2 u Langley Aeronautical Laboratory 0 Langley Air Force Base, Va. z d “9 . t .fi t ts NATIONAL ADVISORY COMMITTEE
2、 FOR AERONAUTICS WASHINGTON c March 30,1950 Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-WCA RM L5OAOk By Rein0 J. salmi asd Robed J. Carroe A low-peed Inverrtigatian of the lcngitudinal aerodynamic charac- teristics of a 47-70 sweptback wing was
3、conducted in the Langley 1Ffoot preseure tunnel in order to provide laz-cale data cm relatively high- aspec-atgo sweptback wings. The wlng featured intemhmgeable - tips whidh prcwided aspect ratios of 5.1-and 6.0 with corre6-p- taper ratios of 0.383 and 0.33. Nkc 6-0 airfoil eectians were emglaged n
4、ormal to the 0.286 chord line. The data were obtained through a range of Reynold8 nunibera varying frcm approximately 1.1 X 106 to 10.0 X lo6 asd Mach nmbers of 0.06 to 0.25. The maximum lift coefficient increased slind 6.0 in; at moderate lift coefficients. The abrupt metable moment break can be at
5、tributed to sepaz-atian nem the tips. Figure 6 Micatea the preaence af _spanwise cross fl“ prior to the initial separatian. As the angle of attack wa8 increased, the S and, a shown by the plota of y1tcMn.g moment agaimt angle of attack- (figs. 4 and 51, the slope of the momazt curve becams negahive,
6、 thus LndicatFng stability at the masimam lift;. Some of the curve8 of pitching mcansnt agabst angle of attack for the high Reynolds nw to note that the pitc-t curve obtained at a Reynolds number of about 1.10 x lo6 exhibited an increase ln sta- bility prior to the unstable %rebly inboard of the tip
7、e. Lift Characterfstics Maximum lift coefficients of 1 .lg asd 1.20 were obtained at a Reynolds ntrmber of about 8.0 x lo6 for the aspect ratio 5.1 and 6.0 we, respectively. Figure 7 shows that the lift coefficinnts increased Brightly with increasing Reynoldi lLulziber in the range of Regnalde nmibe
8、r from a%out 2 .O X IO6 to 8.0 X IO6. A decrease in “ri, occurred When the Reynolds mer. was Fncreaeed to about 10.0 X I_gnolda nuniber of 6.0 x lo6 and approx3mately 0.03 at a Reynolds rimer of 3.0 x 10 6 . The lift-curve slopes were unaffected by roughness. Flgure g(b) ahowe that the roughnees caw
9、ed a canaiderable reduc- tion in the inflection Urt caefficient at a Reynolds nmber of about 6.0 X 10 but had a negligible effect at a Reynolds number of 3.0 x 106. The effect of the rarghnesa is eimilcr to the effect of a low ReynoliFB number in that the energy of the turbulent boundmy layer is red
10、uced sild se-paratim may occur at a lower anae of attack. 6 At a Reyn0ld.e number of 6.0 x 10 , the pitc-t curves were 6 lineax up to the Mlecticm Uft coefficient for both the smooth and rough configuratiane. The aerodynamic canter shifted fmward about 2.3 percent mean aerodynamic chord, however, wf
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