REG NACA-TR-920-1948 The development and application of high-critical-speed inlets.pdf
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1、!ru.s. DEPARTMENTOF COMMERCENationalTechnicalInformationServiceNACA-TR-920THE I)EVELOPMENT AND APPLICATION OF HIGH-CRITICAL-SPEED INLETSD.D. Baals, et alNational Advisory Committee for AeronauticsWashington, D.C.Provided by IHSNot for ResaleNo reproduction or networking permitted without license fro
2、m IHS-,-,-TI_i|iProvided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-REPORT No. 920THE DEVELOPMENT AND APPLICATION OF HIGH-CRITICAL-SPEED NOSE INLETSBy DONALD D. BAALS, NORMAN F. SMITH, and JOHN B. WRIGHTSUMMARYAn analysis of the nose-inlet shapes develop
3、ed in previousinvestigations to represent the optimum from the standpoint ofcritical speed has shown that marked similarity exists betweenthe nondimensional profiles of inlets which have widely differ-ent proportions and critical speeds. With the nondimensionalsimilarity of such profiles established
4、, the large differencesin the critical speeds of these nose inlets must be a function oftheir proportions.An investigation was undertaken in the Langley 8-foothigh-speed tunnel to establish the effects of nose-inlet propor-tions on critical 3lach number and to develop a rational methodfor the design
5、 of high-critical-speed nose inlets to meet desiredrequirements. The nondimensional ordinates of the B noseinlet, which were developed in a previous investigation to beoptimum .from the standpoint of critical speed, were extendedand modified slightly to improve the fairing. These ordinates,now desig
6、nated the NACA 1-series, were then applied to agroup of nose inlets involving a systematic variation of pro-portions. Wind-tunnel tests of these nose inlets were madethrough wide ranges of inlet-velocity ratio and angle of attackat .tiach numbers of 0.3 and 0.4. Tests of representativenose inlets we
7、re carried to high speed (a maximum .tlachnumber qf 0.7). Pressure distributions and critical .tIachnumber characteristics are presented for each of the nose inletstested. The results of these tests show that the length ratio(ratio of length to maximum diameter) of the nose inlet is theprimary facto
8、r governing the maximum critical speed. Theeffect of inlet-diameter ratio (ratio of inlet diameter to maxi-mum diameter) on critical speed is, in general, secondary;but this ratio has an important function in governing the extentof the inlet-velocity-ratio range for maximum critical speed.The highes
9、t critical Mach number attained for any of the noseinlets tested was 0.89.The data have been arranged in the form of design charts.from which NACA l-series nose-inlet proportions can beselected for given values of critical ,VIach number and airflowquantity. Examples of nose-inlet selections are pres
10、ented fora typical je_-propulsion installation (critical ,t/lach number of0.83) and for two conventional radial-engine installations(critical ,_Iach number of 0.76).The selection charts and NACA 1-series ordinates areshown to be applicable to the design of cowlings with spinnersand to the design of
11、high-critical-speed fuselage scoops. Thepossibility of application of the NACA 1-series ordinates tothe experimental development of wing inlets is also indicated.INTRODUCTIONMarked increases in airplane speeds have created a demandfor design data on high-critical-speed air inlets suitable foruse wit
12、h jet-propulsion units, gas-turbine propeller units,and conventional engine installations. Previous develop-ment programs on air inlets have produced the NACA Ccowling having a critical Mach number of 0.63 (reference 1)and the B nose inlet having a critical Mach number of 0.84(reference 2). These in
13、lets have widely different propor-tions; the first is short with a large-diameter air inlet; thesecond is of considerably greater length with a small-diameterair inlet. Each nose inlet was developed to represent theoptimum design from the standpoint of critical speed forthe particular proportions in
14、volved.Little information has been available on air inlets havingproportions in the range between these two specific shapes.The research program reported herein was undertaken atthe Langley 8-foot high-speed tunnel to establish the effectsof variations of nose-inlet proportions on the critical Machn
15、umber and to develop a rational method for the design ofnose inlets intermediate to the NACA C cowling and B noseinlets, both in proportions and in design critical Machnumbers. Such data have direct application to the designof high-critical-speed nose inlets and to the development ofscoop-type air i
16、nlets.SYMBOLSa speed of sound, feet per secondV velocity, feet per secondM Mach number (V/a)V1/Vo inlet-velocity ratioa model angle of attack, measured from model centerline, degreesdensity, slugs per cubic footratio of specific heats (for air, 1.40)static pressure, pounds per square footpressure co
17、efficient (_0P)critical pressure coefficient, corresponding to localMach number of 1.0mass flow, slugs per second (pAir)area, square feet ,mass-flow coefficient “_: .dynamic pressure, pounds per square foot (2 pV“)“- “_535pPP*p,mAmqProvided by IHSNot for ResaleNo reproduction or networking permitted
18、 without license from IHS-,-,-536aH0Ddd/DXX/DFYYrKREPORT NO. 920_NATIONAL ADVISORY cOMMITTEE FOR AERONAUTICStotal-pressure loss between free stream and measure-ment station, pounds per square foottotal conical-diffuser angle, degreesmaximum diameter of nose inletinlet diameterinlet-diameter ratiodis
19、tance from entrance, measured along nose-inletcenter linenose-inlet length, measured from inlet to maximum-diameter stationlength ratiomaximum frontal area of nose inlet, corresponding toD, square feetordinate measured perpendicular to reference linemaximum ordinate, measured perpendicular to ref-er
20、ence line at maximum-diameter station (Seetable I.)nose-inlet lip radiusarbitrary factor (See section entitled “Effects ofvariations in basic profile“ and fig. 7.)Subscripts:rain minimumcr critical0 free stream1 nose-inlet entranceDESIGN ANALYSISDRRIVATIONOF BASICNOSl OI_DINATE3The A, B, and C nose
21、inlets presented in reference 2 werederived experimentally in a systematic series of wind-tunneltests to approach the optimum from the standpoint of criticalspeed. A comparison from reference 2 of the nondimensionalprofiles for these nose inlets having different proportions(fig. 1) indicates a simil
22、arity of profile for all three inlets.Marked similarity of profile is noted for the B and C noseinlets; the A nose inlet, however, varies somewhat from thebasic profile of the B and C nose inlets. This variation isbelieved to be due to the limitations encountered in the testsof reference 2, which in
23、volved the fairing of this nose inletof large diameter into the basic streamline body at a given80.66V7 Y.30,vos. _., U_c“ _ -_NAC,4 Ill bo_ill,= _,i fIx.40f/-X _ -.25L 1t1,/0 .20 ,.30 .50 .60 ,70 .80 90=TXFio_az l.-Comp_rfaon d uondmenston_ p_flie$ _d pm_rtio_ of the $r_ high-c_ft_l.speed nose nle_
24、 developed in _s_ _ rderen_ 2,/.O0Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-THE DEVELOPMENT AND APPLICATION OF HIGH-CRITICAL-SPEED NOSE INLETS 537point and with a given slope. These limitations were notserious for the B and C nose inlets, which
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