NASA NACA-RM-A52F18-1952 The longitudinal characteristics at Mach numbers up to 0 92 of a cambered and twisted wing having 40 degrees of sweepback and an aspect ratio of 10《在马赫数达到0.pdf
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1、RESEARCH MEMORANDUM THE LONGITUDINAL CHARACTERISTICS AT MACH NUMBERS UP TO 0.92 OF A CAMBERED AND TWISTED WING HAVING 40 OF - SWEEPBACK AND AN ASPECT FLAT10 OF 10 By George G. Edwards, Bruce E. Tinling, and Arthur C. Ackerman . Ames Aeronautical Laboratory CLASSlFRlYWlN CA%t!li-d am l NATIONAL ADVIS
2、ORY COMMITTEE FOR AERONAUTICS WASHINGTON September 15, 1952 Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-LX , 1 NATIoRALADvIsORY COMMZMEE FCRAERONAUTICS RESEARCH MEM-UM . THELCNGITUDINBL CHARACTWISTICSAT MACHNUMBREM UP TO 0.92 SWEEPBACK AM) AN ASI
3、?ECT RATIO OF 10 By George G. Edwards, Bruce E. TinUng, and Arthur C. Ackerman SUMMARY A swept-back Wang, in combination with a fuselage, of a type con- sidered suitable for long-range, high-speed airplaneghas been investi- gated in the Ames Xational methods but must be estimated on the basis of pa;
4、 2; .856 .875 -894 0912 1.001 1.001 1.002 1.002 1.003 1.004 1.005 1.006 1.007 l.OOB - - - 0.250 .598 .697 -794 .823 -850 .8-* NACA RM 5218 To establish the magnitude of possible aeroelastic effects, a static load test of the model ting was made to determine the twist due to bending. A lOCO-pound loa
5、d was dfstributed along the span according to the theoretical distribution calculated for incompressible flow for a lift coefficient of 1.0 by the method of reference 10. The results are presented in figure 5. For convenience, the loads on the wing per unit lift coefficient for various test conditio
6、ns sre also presented in this figure. Calculations from these data indicate that the twist due to bending, ACP, at the test condition where the aerodynamk load is greatest (?i - 0.25, R = ,COO,OOO) is about -2.20 (at the tip) per unit lift coefficient. The aerodynantlc data have not been corrected f
7、or the effects of this aeroelastic distortion. RESULTS . Results of tests of the wing alone are presented in figures 6 and 7. Figure 6 shows lift, drag, and pitching-moment data obtained at Reynolds nu all Reynolds numbers and occurred at a lift coefficfent of about 0.4 as shown by figure 22. An inc
8、rease of Reynolds number increased the lift-drag ratfo markedly at lift coefficients greater than 0.8. High speed.- As may be noted from the data of figure 7, the angle of attack for zero lift varied only slightly from its design value of -lo throughout the range of Mach numbers from 0.25 to 0.92. T
9、he pitching- moment coefficfent at zero lift, however, became slightly negative with increasing Mach number, attatiing a value of -0.015 at a mch number of 0.92. The reduction in longitudinal stability and abrupt increase in drag occurred at lower lift coeffFcients as the Mach number was increased.
10、!l?he flow changes accompanying these stabflity and drag changes can be observed in the tuft photographs in figures 18(c) and 18(d). At a B in fact, they msde the wing-fuselage combination longitudinally stable at the stall. The three small fences (A, B, and C) did not substantially improve the pitc
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