REG NACA-WR-L-378-1942 Wind-tunnel investigation of control-surface characteristics VIII - a large aerodynamic balance of two nose shapes used with a 30-percent-chord flap on an NA.pdf
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1、.I,“1+ “+J.F , A% July 1942Tl!mw!w! “ -g-.:.;.-._.L-7_. ,L1 !NATIONAL ADVISORY COMMITTEE FOR AERONJWFICS0RlG4NALLY ISSUEDJuly 1942 asAdvance RestrictedReprtKIND-TUNNEL INVESTIGATIONOF CONTROL-SURI?ACXcHARAc!TERIsmcsVIII - A IARG3 AERODYNAMICWCE OF TWO NOSE SHAPES7EED KITE A 30-PmC,.,L.-4k:J: -4U1,:J
2、.-T.,:. .-,-i, :-. . . r- -q(. -NACA J“mmJF?.:.,. , , : ;. . .?,.: -. . ,. ,. -_h,. . -,. ,. , , . . 1 ;. . , . . . .Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-9 . . tho overbalance and the range through which it extendedwas greater for the blun
3、t-noso flap. Unsealing the gap atthe noso of the flap caused an increase positively of,bothcf; and ChfGf a result that is in agreenont with theresults for the thin airfoil (reference 3).3ecuso the flap with 0.50cf overhang was overlalancodthroughout sor,e rnnge of deflection, it cannot ba usedwithou
4、t notifications. A trailing-edge tab deflected intho sano direction as the flap nay be used in conjunctionvith this flap nrrangencnt to ovorcone the overhalnc ofthe flap (roferonce 3). Such an unbalancing tab will in-crease the lift effectiveness of the flap, with the resultthat the deflection requi
5、red to obtain a given incrementof lift will not he so great as that for a conventional.fla of the same chord. Bec,ause chf is positive, theaflap will float against the relative wind, a factshould cause the static stability of the airplanecontrols free to exceed that with controls fixed.Rudders with
6、a large positive value of chathatwi”thand con-a71siderahle fr.iction”al damping have lean reported to causeundesirable flying qualities on a num%er of airplanes hav-ing small directional stability. These airplanes showed atendency to oscillate in yaw but the undesirable characteristic has been corre
7、cted by making ha and Morec%fnegative. Ylight tests of one airplane at Langley I!emorialAeronautical Laboratory in which the rudder had a positivevalue of ,c and the airplane had a large amount of di-arectional stalility indicated that the behavior of the air-plane was satisfactory.” A theoretical a
8、nalysis currentlybeing made at the Laboratory shows that a positive valueof ch is desirable provided that other factors are prop-aorly controlled.Pitching IlomentsCm() qThe values of the parameters ma and ()act Sflisted in ta%le III indicate the position” of the aerodynam-ic center of the airfoil. W
9、hen the lift is varied bychanging the angle of attack, at a flap deflection of 0Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-“1othe aerodynamic center of the airfoil is at the 0.235c ;,point for both flap-nose shapes with the gap sealed and atthe
10、0.225c point for bcth flap-nose shapes with the 0.005cgap. When the lift is var ed by changing flap deflection,iat an angle of attnck of O , the aerodynamic center is atthe 0,41c point foz both nose shapes with gaP sealed andat the 0.42c point fGr oth nose shapes with the 0,005cgay , Tho positions o
11、f the aerodynamic center for the pres-ent tests are in good agreement with those for the airfoilwith plain flap (reference 7). The position of the aero-dynamic contor for the flap deflected is a function ofaspect ratio (refarence 1) and will move toward the trail-ing edge as the aspect ratio is decr
12、eased. DzagThe measured vnlues” of dr.g cannot be considered abso-lute because of a relatively large unknown tunnel correc-tion. The increments of profile-drag coefficient causedby flap deflection (fig. 4), however, should be independentof tuynel effect. The medium-nose flap gave i=.nincrease inmini
13、.um profile-drag coefficient of shout 0.0022 over thatof the plain flap on the same airfoil (reference 7). Viththe l)lunt-nose flap the increase was within the experi- .marital accuracy of the tests. .Tab CharacteristicsIn general, the tal characteristics for the balancedflap are similar to those fo
14、r a tab on th plain flaP(reference 7). At a flap deflection of O , the effective-ness of the tab in changing the flap hinge-moment coeffi-cients was greatest when the tab was defleoted in conjunc-tion with the angle of .attaak. This result is oppositeto that for a tab of tho same size on an NACA 000
15、9 airfoil,for which the effectiveness of the tah was greatest whenthe tab deflection and the angle of attck wero in opposi-tion. AS previously discussed, the overbalance of theflap that occurred when the large overhang was used on theflap may be overcome by the use of a differentially oper-“ atod un
16、balancing tab deflected in the same direction asthe flap.BaI.ancing Effectiveness of Various Overhangs .The values of the hinge-moment parameters for blunt- . .-.= . , .,. ,., :- y-y - .,”. ,- ”, -.-, - -:- :.7,:. ., .,.- .* : .“: . . :.,.,:. -“.”, ; .-.,-:, ,-. ” :, .-.,:,- ., : . . .J .Provided by
17、 IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-11nose flaps on the NACA 0009 and NACA 0015 airfoils are pro-sentod as a function of aerod:?nanic balance in figure 7.Tl:e data are summarized from the investigations reportedin roforonces 2 to 8, with the exclusi
18、on of reference 6,.”3 vhich does not deal with overhanging lalances . The unsealedPPa gap was 0.005c in all cases except that it was 0.0015c forA the largest overhang on the NACA 0009-airfoil. Tho plainunbalanced flap, because it is hinged at the center of itsncso radius, has an overhang, This overh
19、ang, however, cancontribute no lalancing affect because all forces normalto the surface of the ovorhang act through the hinge axis. .Figure 7 shows that, for both airfoils, the hinge nO-nents of a balanced flap were reduced by unsealing the gap.Tho rate of change of hinge-moment parameters with incr
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