NASA NACA-TN-3314-1955 A technique utilizing rocket-propelled test vehicles for the measurement of the damping in roll of sting-mounted models and some initial results for delta an.pdf
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1、NATIONALADVISORY COMMITTEEFOR AERONAUTICSTECHNICAL NOTE 3314A TECQUE UTIIJZING ROCKET-PROPELLEDTEST VEHICLES FOR THE MEASUREMENT OF THE DAMPING IN ROLLOF STING-MOUNTED MODELS ANDDELTA AND UNSWEPTBy William M. Bland, Jr.,SOME INITIAL RESULTS FORTAPERED WINGSand Carl A. SandahlLangley Aeronautical Lab
2、oratoryLangley Field, Va.WashingtonMay 1955Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-1s TECHLIBRARYKAFB,NM :IWTIOIWL ADVISORY COMMITTEE FOR AERONAUTS IllllllllullllllullllllllllI00LL032 jTECHNICAL NOTE 3314A TECHNIQUE UTILIZING ROCKET-PROPEILED
3、TEST V12W2LES FOR TEE MEA OF TEE DAMPING IN ROLLOF STING-MOUNTEDMODELS AND SOME INITIAL RESULTS FORDELTA AND UNSWEPT TKPERED lCD12S1I however, the agreementa71 improved with increasingMach nuniber. Ihcreased section thicknessdecreased the damping in roll of the delta wings throughout the Machnuaiber
4、range investigated.“INTRODUC!KIONThe Langley Pilotless Aircraft Research Division is utilizing twoexperimental techniques emplng rocket-propelled test vehicles forthe determination of the -ing-in-roll derivative at high stisonic,transonic, and supersonic speeds at relatively large Reynolds nwibers.O
5、ne technique which is used for determining the demping in roll.of wing-fuselage cozibinationsis described in reference 1. The other techniquewhich is used for determining the damping in roll of wings alone and ofwing-fuselage conitxinationsis described herein. The Reynolds numbersobtained with the u
6、se of this technique, although somewhat lower thanthose obtained with the technique of reference 1, are still fairly high(1x 106 to 3 x 106).6%upersedes re6ently declassified lUlCARML50D24, 1950,sProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-2 NACA
7、 TN 3314Also presented herein are scme initial results obtainedby thepresent technique for a series of configurationshaving wings of aspectratio 4. The configurationsinvestigated included a delta-wing-fuselage conibinationhaving a wing made frgm a flat plate wi.thbeveledleading and trailing edges, t
8、wo delta wings-having 45 of leading-edgesweep - one with a 4-percent-thick symmetricaldouble-wedge airfoil sec-tion and the other with a g-percent-thicksymmetrical dcnible-wedgeairfoil section, and an unswept tapered wing hav, 0.5 taper ratiowith a 4.6-percent-thick symmetrical double-wedge airfoil
9、section.clPC2pbzLsbPvMRczYSYMBOLSdCzdamping-in-ro derivative,nd pbELrolling-mment coefficient, qsbwing-tip helix angle,rolling moment, ft-lbradisnsdynamic pressure, lb/sq ftwing area, sq ftwing span, ftrolling velocity, radiarm/secflight-path velocity, ft/secMach numberReynolds numiberwing chord, ft
10、based on wingwing mean aerodynamic chord,lateral coordinatemean aerodynamicz b/2J730 c2dy, ftchordProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-NACA TN 33149t thickness, ftw A aspect ratio obtained by extending wing leading and trailtigedges to mod
11、el center lineA leading-edge sweep angle, degh taper ratioMETHODThe general arrangement of the test vehicle is illustrated in fig-ures 1 and 2. The wing under investigationwas attached to a torsionspring balce arranged to form a sting mount in the nose of the testvehicle. In flight the entire test v
12、ehicle was forced to rollby thestabilizing fins, each of which was set at an angle of ticidence. Arocket motor accelerated the test vehicle to the maximum Mach number,after which the test vehicle decelerated through the test Mach nuniberrange. Time histories of the rolling moment generated by the te
13、st wing,the flight-path velocity, and the rolling velocity were obtained. Thesedata, in conjunction with atmospheric data obtained by radiosonde meas-urements, permitted the evaluation of the damping-in-roll derivative%P as a function of Mach nuniber.a71A ssmple flight path illustrattig the useful.r
14、ange of a flight andsome tical conditions is shown h figure 3. Typical time histories.of some of the measured qusmtities are shown h figure 4.A photograph of a test vehicle mounted on the zero-length launcheris shown in figure 5.INSTRUMENTA!TIONThe torsion spring balsnce shown in figure 6 consisted
15、of a shsftwhich transmitted the rolling moment generated by the test wing to ahelical torsion spring which permitted angular movement relative to thetest vehicle proportional to the rolling moment. The angular movementsof the shsft were transmitted to a condenser-typepickup which was usedin conjunct
16、ion with standard NACA telemetry.The rolling velocity was obtainedby the method of reference 2.except that the telemeter and telemeter antenna performed the functionsof the spinsonde described in the reference. The telemeter antennaa71Provided by IHSNot for ResaleNo reproduction or networking permit
17、ted without license from IHS-,-,-4 NACA TN 3314consisted of two rods which were inserted in the trailing edges of two a71diametrically opposed driving fins as shown in figure 1. This antennaarrangement produced the plane polarized radim-signal required for themethod of reference 2. The ground record
18、ing equipmentwas the same as *that described in reference 2.The flight-path velocity was measured by a Doppler radar veloctieter.The altitude, which was obtainedby integratingthe velocity-time curve,was correlated with radiosonde measurements ofalong the flight path made at the time of eachTEST CONF
19、IGURATIONSatmospheric conditionstest flight.The configurationstested, all of which had an aspect ratio of 4.00,were (1) a delta-wing-fuselage combination employing an airfoil sectionhaving fla,tsides and symmetricallybeveled leading and trailing edges(f. 7), (2) a delta- having45 of leading-edge swe
20、ep witha-k-percent-thick symmetrical double-wedge airfoil section, (3) a delta wing having 45 of leading-edge sweep with a g-percent-thick symmetricaldouble-wedge airfoil section, and (4) a wing having a taper ratio of 0.5with an unswept 50-percent-chordline and a 4.6-percent-thicksymmetricaldole-we
21、dge airfoil section.The gecxnetriccharacteristicsof the con-figurations tested are summarized in table I. Photographs of the testconfigurations are shown in figure 8. The wing surfaceswere carefullyground and polished after being machined from steel plate. The distancefrom the trailing edge of the r
22、oot chord of the wings to the nose of the a71test vehicle was-held constant as showz.in figure 1:ACCURACYThe maximum possible systematic errors in the valuessented herein due to the ltiitations of the measuring andsystems are estimated to be within the following limits:.of cl p pre-recording Delta w
23、ings Unswept tapered wing I ,M Error in Cz M Error in CzP P1.7 *().008 1.7 “- +0.0151.4 *.013 1.2 *.030k.033 1.0 * .041:? *.053 .7 * .100Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-NACA !IIT3314 5a71 The variation of these possible errors is due
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