NASA-TN-D-6391-1971 Wind-tunnel investigation of an external-flow jet-flap transport configuration having full-span triple-slotted flaps《带有全翼展三开缝襟翼的外流喷气襟翼运输结构的风洞研究》.pdf
《NASA-TN-D-6391-1971 Wind-tunnel investigation of an external-flow jet-flap transport configuration having full-span triple-slotted flaps《带有全翼展三开缝襟翼的外流喷气襟翼运输结构的风洞研究》.pdf》由会员分享,可在线阅读,更多相关《NASA-TN-D-6391-1971 Wind-tunnel investigation of an external-flow jet-flap transport configuration having full-span triple-slotted flaps《带有全翼展三开缝襟翼的外流喷气襟翼运输结构的风洞研究》.pdf(269页珍藏版)》请在麦多课文档分享上搜索。
1、NASA TECHNICAL NOTE WIND-TUNNEL INVESTIGATION OF AN EXTERNAL-FLOW JET-FLAP TRANSPORT CONFIGURATION HAVING FULL-SPAN TRIPLE-SLOTTED FLAPS Lnrzgley Research Center and C. Robert Carter NATIONAL AERONAUTICS AND SPACE ADMINISTRATION WASHINGTON, D. C. AUGUST 1971 Provided by IHSNot for ResaleNo reproduct
2、ion or networking permitted without license from IHS-,-,-TECH Ll8RARY KAFB, NM 1. Report No. I 2. Government Accession No. I 3. Recipients Catalog No. NASA TN D-6391 4. Title and Subtitle I 5. Report Date WIND-TUNNEL INVESTIGATION OF AN EXTERNAL-FLOW JET-FLAP TRANSPORT CONFIGURATION HAVING FULL- SPA
3、N TRIPLE-SLOTTED FLAPS 7. Authorb) Lysle P. Parlett, H. Douglas Greer, and Robert L. Henderson (Langley Research Center), and C. Robert Carter (Langley Directorate, U.S. Army Air Mobility R similar data from references 1 and 2 are shown for comparison. This plot shows that the partial-span flap arra
4、ngement of reference 1 had a more forward flap center-of- pressure and aerodynamic-center location than the full-span flap arrangements of refer- ence 2 and of the present study. In all cases the center of pressure moved rearward with increases in thrust and the aerodynamic center moved forward with
5、 increases in thrust through the low-thrust range and then began to move rearward with further increases in thrust. The longitudinal stability and trim characteristics of the model with tail on are plotted in figures 20 to 28 for the clustered-engine arrangement and in figures 29 to 31 for the sprea
6、d-engine arrangement. These data show, in general, that the model with flap down was longitudinally stable up to the stall and could be trimmed in pitch up to the 10 Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-highest thrust settings by the appli
7、cation of blowing to the horizontal tail used in the tests. The utilization of blowing on the tail was not meant to imply that blowing would be needed in full-scale operation but was intended to give lift on the model tail which would be representative of a full-scale tail with a slotted elevator (a
8、 maximum CL of 2.5 would be expected). The longitudinal instability indicated in figures 22 and 23 is a result of tail stall caused by improper tail geometry for the particular tests involved. For example, for the data in figure 23 the chord of the tail leading-edge flap was reduced to one-half its
9、original length and this change caused the tail to be ineffective at the high thrust settings. The original tail leading-edge flap was used for all the remaining tests. Figures 24, 25, and 26 show the effect of changing the rear flap element to higher and lower settings for possible use in glide-pat
10、h control. Similar data are presented in figure 27 in which the flap element was deflected symmetrically for only the outer flap span. The data of figure 28 show the effect of symmetric spoiler deflection for possible use in glide-path control. In the tests of figure 28(e) the projecting slot lip wa
11、s removed to enlarge the slot of the inboard and center flap segments. A comparison of the data of figure 28 with data of figure 20(a) shows that a symmetric spoiler deflection of 30 pro- duced decremental lift coefficients of about 1.0 at the higher thrust settings. A comparison of the spread-engin
12、e data of figures 29 to 31 with the clustered- engine data of figures 20 to 28 shows no major differences in longitudinal stability and trim characteristics for the two engine arrangements. A summary of the pitching- moment characteristics from these data and the data from references 1 and 2 (see fi
13、g. 32) shows that !he static stability and trim characteristics for the model of the pres- ent investigation were generally similar to those for the models of references 1 and 2, but the trim requirements were greater. The results of flow surveys to measure the downwash characteristics in the vicini
14、ty of the horizontal tail are presented in figures 33 and 34 for the clustered-engine arrange- ment and in figures 35 and 36 for the spread-engine arrangement. These data are sum- marized in figure 37 in terms of the downwash factor 1 - plotted against thrust coefficient Cp for tests with and withou
15、t leading-edge blowing. Figure 37 shows that the horizontal-tail effectiveness generally decreased with increasing engine thrust. The use of leading-edge blowing resulted in an increase in horizontal-tail effectiveness for the spread-engine arrangement but generally produced adverse effects for the
16、clustered- engine arrangement. ( - :) Lateral Stability A few tests were made to determine the variation of the lateral aerodynamic coef- ficients with angle of sideslip. These tests were made with power off and power on and 11 Provided by IHSNot for ResaleNo reproduction or networking permitted wit
17、hout license from IHS-,-,-for both symmetric and asymmetric power conditions. The data, which are presented in figure 38, show that the aerodynamic coefficients varied fairly linearly with sideslip; hence, the remainder of the lateral stability studies were made in terms of sideslip derivatives dete
18、rmined from tests at k5O sideslip. Plots of the static lateral stability derivatives against angle of attack are presented in figures 39 to 46 for various model configurations and thrust levels, with and without leading-edge blowing. These plots show that in all tail-on configurations (figs. 40, 42,
19、 and 44 to 46) the model has directional stability +Cn and positive effective dihedral ( P ( -%) through most of the angle-of-attack range up to the stall. The directional stability is virtually unaffected by change in angle of attack; effective dihedral, however, increases with increasing angle of
20、attack up to the stall. In all tail-on configurations, the applica- tion of thrust produced notable increases in directional stability throughout the angle-of- attack range. At angles of attack near the power-off stall angle, thrust also produced large increments in effective dihedral. Leading-edge
21、blowing, which like thrust is effec- tive in delaying stall, markedly increases the effective dihedral near the power-off stall angle of attack. The spanwise distribution of the thrust appears to have very little effect on direc- tional stability or effective dihedral. Engine-out static stability da
22、ta, presented in fig- ures 41 (tail off) and 42 (tail on), are very similar to those for the corresponding all- engine cases presented in figures 39(b) and 40(b), respectively. Likewise, leading-edge- blowing data for the clustered-engine arrangement (fig. 40(b), for instance) are similar to those f
23、or the spread-engine arrangement (fig. 45(a). Spanwise discontinuity in flap deflection has no noticeable effect on the stability derivatives, as is shown by a compar- ison of figure 45(b) with figure 46. Basic Asymmetric Moments (Engine Inoperative) Lateral characteristics obtained for the model wi
24、th one engine inoperative are pre- sented in figures 47 to 50 for the clustered-engine arrangement and in figures 51 to 53 for the spread-engine arrangement. Because in a powered-lift system a loss of an engine results in loss of lift, plots of the lateral characteristics with one engine out are acc
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