RESEARCH MEMORANDU~
Transcript of RESEARCH MEMORANDU~
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RESEARCH MEMORANDU~
ALTITUDE-TEST-C~ER INVESTIGATION OF PERFORMANCE
OF A 28-INCH RAM-JET ENGINE
II- EFFECTS OF GUTTER WIDTH AND BLOCKED AREA
ON’OPERATING RANGE AND COMBUSTION EFFICIENCY
By T. B. Shillito,W. L. Jones,and R. W. Kahn
Lewis FlightPropulsionLaboratoryCleveland,Ohio /“
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NATIONAL ADVISORY COMMITTEEFOR AERONAUTICS
WASHINGTONNovember 6, 19!50
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RM!IWAL ADVISORYOcMaTmE m AEEmwTIcs
RE6EARm~.
ALTITum—msT—~ mvEsTIG4TIoNa? ImRmwmE
OF A 28-R?CHRAM-JIM?-Iltll!
By T. B. SMllito, W. L: JoneEIand R*w. Kahn
h invest@atiauof the effechof flame-holderblookedaxea and@ter width an the perfcmmame of a 28-tnoh+iamter ram-$etengineat a almulated fllghtMoh numberof 2.0 and for altitudes&om40,000to 55,000feet has been oonduotedin a 10-fmt-diameteralti-tude ohmiber. The ten flameholdersinvestigatedincorporated60°annular-Vgutters,that variedin widthfrom 1.0 to 2.5 inohesendblookedfrom 40.5to 62.0peroentof the o&busticm-ohdbar area.All fhaueholderswere investigatedwith a fixed gecmetrioal arrange-
ment of the fuel-ln~eottonsystem,althoughoperationwith eitherone(auuularin:eotlon)or both (uniformQleotlon) of the two fuel-inseotionmeaifoldswas incltiedfor saneof the flameholders.
At a simulatedaltitudeof 50,000feet,lean limttsof ccmdxzs-tlon at a fuel-airratio of approSmately0.03were obtainedfcwannularInjeottonand approxlmatel.y0.04for unifomnlnjeoticm.Ths rloh limitsof owibustionwere greater than 0.065fuel-airratiofor the most stablemnflgurations. Corfibusttoneffiaienaiesfor these mnf@ratlons ringedfrom 0.7 to 1.0with uniformtijeo-tlon and from 0.4 to O.q for annularlnJeotlmh
Desirableoharaoteristiodof wide over=alloperathg fuel-air-ratiorangeand high mmbustloq +5’iqhnoy were most favorablywmbined in two flameholders. One.of theseflameholdershad2.O-lnoh-widewtters and a proseoted~ of 45.0 percentof theoanbusthn-chaiberwide guttersand achsmberarea.9
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&mea and &-other flameholderkd 2.5-lnoh-projectedarea of 60 percentof the combustion-
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2 ~ “-” HACAR4 E5C!R21 “-”~ .
..-es ti guttm widthmom 1.0 to 2.5 inohesfor oonstant
blockedarea had no appreciableeffeota combustionefftolenoy -%~overa rangeoff’uel-airratiosfra 0.04!5to 0.065ad farmmbustlon-chamberpressuressllghtlylessthan oae atmosphere.Inoreaeingthe blockedarea of the flam holdersfrom 40.0to .--.,
62.0pbroentfor constantgutterwidths‘@’1.5 and 2.0 inches.=..
resultedin an increasein oonibustionefficiencyof 5 to 10 per-cent. The blow-outlimitsof the varioussatisfactorilycorrelatedchamber-inletMaohnumberThe degree”ofcorrelattcnpreviousinvestigators.
on the basisofto gutterwidthobtainedserved
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flameholderswerethe ratioof ccmbustion- ->,raisedto the 0,45power.to vertfy the work of ‘“
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An altitude-test-chamberinvestigationof the combustion-ohamberperformanceof a 28-inoh%xn-jetenginebeingdeveloped” a
by theMsrq-t AircraftCompanyhas beeg.-~oniuctedat the NACA’Lewislaboratory.Extensivedevelopmentaltestshave been oon-duotedby the enginemanufacturerat simulatedaltitudesup to
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approximately30,000feet ami for a simulatedflightMaoh numberof 2.0. The performanceInveatlgatlwat the Lewislaboratorycoveredthe rangeof simulatsdaltitudesfrcm 40,000to55,000feet at a simulatedflightMach number”of 2.0. ..
The purposeof the pro- describedhereinw?isto determinethe effeotsof the percmta~ of octmbustian-charnberflow areablockedby the proJeotedarea of the flameholderand af flame-holdergutterwidthon the mubustian perfeoe. Resultscd?anInvestigationof severalocmfigurationsin thisprogramare repartedin reference1. A seriesof 10 V-gutterf@me holderswere eval-uated. Theseflameholdk~ were designedto povide f’smilles&varyinggutterwidthwith approximatelycanstsntblockedarea sadVSWiIJ8blo~ed areawith approxiwtelyoonstantgutterwidth. Therunsweremadewith a fixedfuel-injeoticmsystemocmsistlngof twointernalfuel-msnifoldrhgs with spring-loadedfuel-spraynozzleslooatedapproximatelyone Conibustton-chemberMsmeter upstreamofthe flameholders. Rxr e?chflameholder,altitudeoperatkmallimits,combustioneffloiemy,and pressurelossesare givenandthe effeotsof blockedareaand gutterwidthon performanceemanalyzed.
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N(ICAm! E50H21
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e The installaticmof the enginein the 10-footaltitudeohauiber% is desoribedin referenoe1. Featuresof the setuppertinentto
the presentinvestigationare repeatedherein.
Desorlptlm of elWlne. - A schematicdiagramof the engine issh&n in figure1. The enginemneisted primarilyof an outershelland an innerbody. The fowwardporticmeof the outershelland tunerbody formeden annum difYuserand the downstreampoationof the -outershellfomed the mxubustionohamberand the exitnozzle. Theflightengtiewith free-sham inletwas designedto produoea Maohnumberof 1.6 at the lip (sta.tian31) at a fllghtMach numberof 2.0.~ cwder to simulate this flow oonditiondur~ the altttude-test-ohambertivestigation,a bellmouihconvergent-divergentnozzlewasinstalledat the engineimletto acceleratethe atr frcunstagnationcomdltionein the altitudechamberto the requiredMach number. It
* was thus possibleto shulate the averageoonditloneof Maoh number,pressure,- t~ture that omur with the free-streaminletofthe fllghtocmflguratiaand to positionthe shookin the diffuser
h at the sameposlttonas in fllght. Beoauseexaotboundarylayer,Mach nuziber,and pressuregradients,and suboritioalspllloveroondt-ticmeof flightare not reproducedby this inletnozzle, the stabilityof the mibustim chamberand flightdiffuserocmibinatlcmoouldnotbe ti~stl~tedj -eOver, possibleeffectsof the inletboundaryX on velocityand pu?essuredletributionat the ocmilnzstion-ohaniberInletoouldnot be evaluated.I&au the 11P statim to the end of theinnerbody,the air-flw passagewas divergentwith the samedimen-sionsas the fllghtengine(referenoe1). The innerbody was om-neotedto the outershellby four longeroneexbendlngalmostthelengthof the innerbody.
The mnbuetbn dmiber Is 28 inohesin diameterand 46 Inoheslcmg. Attaohedto the omibustim-c@mber outletis a oonvergent-divergentetitnozzle19 incheslongwith a throatdiameterof20.75inchesand an outletdiameterof 22.44Inohes. The entireouter surfaoe of the cxxibudttonchamberand exitnozzlewas water-jaoketedto provideGooling. Fuelwas inJeotednear station197@ the flameholderswere mountedat statian239. Detaileddescriptionsof the fuel systemand the flameholdersare givensubsequently.
hetallationin altitudetest ohamber.- The Installationofthe engine& the 10-footaltitudetest ohamberis shownin fig-ure 2. 5 enginewas fittedwith a diaphragmsealat a forwardB baffleand a slldlngsealat a r- baffle. The frontbaffle
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providedan air-tightsealseparatingthe inletram-pressureatifrom the altitudeeihaust@ thuspermitteda pressuredifferenoeto be maintainedaorossthe engine. The rear bafflewall wasinstalledto keep the hot etiust gasesfrmu reolrcu.1.atlng aroundthe engine.
A suddenexpansionjetdiffuser(reference1)was Installedat the exit of the engine. This Jetdiffuserwas used to raisethe “highaltitudeoperatimallimitsiqposedby t~ laboratoryaltitude ,exhaustsystem.
Fuel-lnJeotionsystem.- The fuel system(fig.3) oonsistedoftwo manifoldseadhdividedIntofow quadrantslooatsdbetweenthelcmgeronsuppmtisand equippedwith s@ng-loaded nozzles. Adeaoriptimnof the fuelnozzlesis givenla referenoe1. The foursets, of eaahqenifold axe oonnectedoutsidethe ~lne to foatwo nmnlfoldrings. Twenty-fournozzleswere Installedin theouter (downstream)manifoldand 16 h the Inner (upstream)[email protected] flowwas.individuallyregulatedto the two ma@folds. Runs inwhiohequalfuelpressurewae 8uppliedto bothmanifoldsare deelg-nateduniform-in~eothnrunsand thosein whiohfuelwas suppliedonlyto the innermanifoldare desimated annular-in.leotionruns.
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Th- fuelusedthroughoutthe investigaticm.IWIocuune%id grade “ ._.normalheptane. ,
Flameholders.- The 10 flameholdertiusedwere of similarmnstmuoticmand weremountedin the looationshownIn fIgures1and 3 (station239). Detaileddimensionsof the flameholdersareshownin figure4. The annulargutterswere armzged in a s-redV in the longitudinalplaneand were oonneotedand suppcwtedby
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radialguttersm plates. The ~lameholdersdifferedprincipallyin gutterwidth,numberand diameterof annulargutters,and pro-~ectedarea,hereinaftere~ressed as percentageof oombustlon-ohamberarea (28-inchdiameter)or percentageblockedarea. Thefollowingtableliststhe prtioipaldeeignfeaturesof the variousflameholders:
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Fl&ueholder
123.45678910
Gutter
width(in.)
1.001.002.001.502.001.201.381.001.402.50
Blooked Lull=mulb??ofarea
(peroent)I rings
42.0 455.0 645*O 240.5 360.0 358.0 562.0 548.7 555.0 460.0 2“
Praotioaldlsposlticaof blockedarea preventeddes%gnof prectse“familiesbut the flameholdersmay be groupedin familieshavingnearlyoanstantgutterwidth or blookedarea.
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* e~le, flameholders5, 7, d 10 may be groupedto form a familyof varyinggutterwidthfrcm 1.38to 2.50 Imhes with CXC@a 2-peroentvarZEL-tion in blookedarea.
The flareoasesshownIn figure4 were IIwwUed for i&uiticKlduringflightbut were not used for s~lng duringtheseruns. Anlguitorbox similarIn prlnoipleto a m.lnlatureram Jetwas attaohedto the guttersto provideIgnitlcm.
I?uel-air-ratiometer.- The fuel-atw?atlodistributionwasmeasuredaheadof the flSmeholderby a oumneroiallyavailable.devioethat oolleoteda sampleof the mlxhzrein a l/8-lnoh4tametertubesimilarto a total-pressurethe ~ passedthe sampleover an eleo-trioallyheatedreslstanoeelament. Changesh ~t flow tlumughthe elementare msasuredwith ohangesin oompositlonof the gas.The Oument flow is proportionalto the thermalocslduotivltyof thegas,whloh Is propartlaualto the fuel-ak ratio. Canparlsonaf thesurveydatawith the fuel-alrratiomeasuredfrcm individualmetering6f fuel and air Indloatesthat the absoluteaoouraoyof the surveysis not adequatefor quantitativeoanoluskus. The trendsof thedistrlbuti~,however,are believedto be oorreotlygivenby theinstruuleult.
mst rumentatlm. - I’uelflowwas measuredwith a calibratedadjustableorifioemeter- alr flow was meaauredwtth a oanoentrio
M slm?p-edgeOrifioe. The engine-lnl.ettotal_rature and pressurewere measuredby rakBsat the bellmouthentranoe. The Ilumberend
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the looaticm of temperatureand statio-and total-presquremeasure-mentswithinthe engineare shuwnin figure1. The odbusttcm-damber-inlettotaland statlopressureswere measuredby a rakelooated”a few inchesupstreamof the flameholders. Water-oooledrakeswere usedto measuretotal‘pressurwat the ocmbustlon-chemberoutlet. St&lo pressuresIn the tist-nozzle threatwere measuredby fourwall statictubesand by eighttrailingstatiotubesmountedon streamlinedstrutsin the c?aubustionohsmiberand efiendlngdown-s-am to the nozzlet-at. The oombustian-dmmberand the exlt-nozzlecooling-waterflowand tezrpeixdmreriseweremeasuredin cinderto oaloulatethe heatremoved.
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PROCIEWHl —
The generalpmooedurefor most of the ironswas to i*fte theburnerat em Inletpressureof-approximately40 inohesof merouryabsoluteand an outletpressureof 25 Inchesof mercury,ccm-espondlngto a cabustlon-ohember-inletvelocityof approximately250 feet per
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seoond, with a fuel-alrratioof approximately0.04. When stableburningwas establi@md,the outletpressurewas slowlyreduoed .
untilohoklngomdltIonswere reachedin the exitnozzle. The englne-inletpressurewas then set to stmulatethe desiredflightconditions. . ‘
. With this pressureheld oomstant,the fuel flowwas variedh mallintervalsand dataware takenat stabilizedburningmnditlms untilrloh or lean caubustionblow-outocmrred. Ths ooastantinletpres-bureand inlettemperatureImposeduponthe ohokedInletnozzleresultedIn a mnstant alr flow throughthe enginefoirany givensimulatedaltitude. Runsweremade with t@ variousoonfiguratlmsat a simulatedflightMaoh nuniberof 2.0 and altitudesfrom 40,000to55,000feet.
The inlet-airtotalpressureat the lip statbn was mmputedfor the flightenginefor a rangeof altltudesat a fllghtMaohnumberof 2.0 from Oonioalshookrelations. The ~ssure at thebellmouthInletin the enginewas then set at the cczuputedvaluesfor eaohaltitude. This procedurenegleotsany lossin totalpres-surebetweenthe bellmouthInletand the llp.
The engine-inletair temperaturewas matntalnedat 710°A 5° Rby a oomhusticmheaterin the air supp4 Mne. ~ fuel-alrratiofor the combustionheaterwas about0.002. Ths effeotof theslightresultIng cmrbsdmtlcinof the ohargeair a the enginecombustionIs not lmounbut Is believedto be small.
NAOAIM E50H21 “
Runs Wsre IlpdeWith Unifomufuel ln$mkbl
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for all flame holdersand several flameholdere were also run with annularIn#eotim. R&flameholder2, a few runswere made In whioh unequalfuel pressureswere imposedon the fuelmqnl.foldsIn an effortto blend ~uallyfrmuannularto uniforminJeotlmo Elow-outwas deteotedby observa-tion of the flazusthrougha perlsoope,by the suddenohangeYn soundlevel,- by = automaticflmue-deteotiondevioe..Ths smols usedand methodof oaloulatlcmof oombusti- effioienoyare outllnedinthe appendix.
RESULU!SAND DISOUSSIQll
The radialdistrlbutiausof fuel-airratioand totaland staticpressuresat the ocmbustlon-ohemberInletwere measuredIn ordertooheokthe possibilityof regions of separatedflow m lrre@drvelooitycm fuel d2strlbution.The typesof fuel distributionobtainedwith unlfozmand annularInJeotionare Illustratedinfigurs5(a). As previouslymentimed, the results=e mnslderedto be qualitativeand indloattveof onlyths trends. The fuel-airratiofor mifom inJeotiondid not vary greatlyoverthe outer10 inohesof radtusbut deoreas~ slightlytowardthe oenterofthe mibustion ohambed. Annularh jeoticmproduoeda rioh regionoenteredmound the 5-inohradiuswith rapidlydeoreasimgfuel-alrrattostowardthe oenterand outerwall of the oanbustlonolianiber.The distributimsof fuel-airratio observedfor otheroperatingOarlditialsindioatedthat annularinJeotlonprovideda looallzedregionof nearly“stoiohianetriufuel-airratio,em for very le=over-allfuel-airrattos;whereas-m ~eot~~ distrlbut~ fuelmore evenlyfor all fuql-airratios.
Typioalradialdistrihutimsof totalto statiopressureratioaheadof ths flameholderare shuwnin figure5(b). The radialpressureratiogradientwas very largenear the Innerand outervans of the diffuseroutlet,but tt Is evidentthatno extendveregionsof separatedflow existedne= the walls. The ml?ibustlmlresultsgivenhereinapplyonlyto the p-iouhm mudltlons ofpressure,velooity,and fuel distrlbutiauat the ocaibustton-dmiberinletprodumd by the test engineand theirdegreeof applicabilityto otherOonditlonsof fluw is unknown.
Plots of the bastodata for eaohflame-holderoonftguratiaare shownin figures6 to 15. For eaohflameholderthe simul-taneousvariationsof e-ut-no=le vess~e =tlo p4/P5}ocmibustlau-chamberpressureratio P4@2j oawtia-omer-~etl&mh number M2’, oaibustion=ohamber-outletpressure P4, @s-flow
f=tm P$5b5$tlonsof fuel-air
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and ccmibusticmefflolencyq are givenas funo-r&tlo. Inasmuchas ctibuE&ion=ohamber-inlet”
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velocity,pre6mre, d fuel-alrrat.lovary eimultaneotif31y,theindividualeffeotsof thesevariablescm performumeaxe not separatedIn figures.6to 15. The trendsshownthereforeapplyonlyto thespeoiflocombustioncmnditlonsindioated.Superimposedon the mrvesof milxzstlon-ohamber-outl.etpressureare ltiesdenotingthe bluw-outlimitsfor both uniformand smnulsrI@eotlon. Data m?e shownforuniforminJectlonfar dl flameholdersand for.annularin~eotianfor severalflameholders. The dataare codedfor oonstantaltitude,whiohas previouslydknzssed tipliesa constantenginebellmouth-Inletpressure.
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Engineoperatlnl?Oonditians.- JhasmucK-asall runsweremadewith a ohokedexitnozzle,the ratioof nozzle-inletor mmbustlon-ohamber-outletPregsureto throatstatiopressure 24/P5 shouldinthe lde&Lane-dimensionaleasebe a funotiononlyof gas temperature “and the thermcd~ynamiopropertiesof the gas,andthereforeindepend-ent of configurationor fuel-air-ratiodIstrlbution. Departurefrcan -the Idealon6-dlmenshuilmnoepts will producediscrepanciesIn theocmbustiontemperaturesend effioienoiesoomputedby the methcdout-llnedIn the appendix. The e~erlmentalexhaust-nozzlepressure-ratiodata (part(a)of fIgs.6 to 15) showthatthe pressureratiois independentd altitudebut dependenton oonfi~atia as wellas t~e of fuel injeotion.
The cambustian-ohambertotal-pressureratio P4/P2 for eaohflsmeholderis ne=ly independentof fuel-airratioand altitude.The pressurerirbioIs mmstent beoausethe’inareasein momentumpressuredropwith increaseinfuel-airratioIS oounterbalanoedby a deoreasein fric%lon+ressuredrop. The differencesIn pres-sureratiobetweauflameholdersis a resultof differmoes infrlothn pressuredropand can..ustioneffioienoycharaoteristios.The pressureratiovariedfbcmapproximately0.90for flameholderswith high blookedarea to about0.94far low-blooked-areaflameholders.
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The mmhustl’on-chamber-inletMaoh number=S ocamputedfrcunthemeasuredtotaland statiopressurbsat instrumentstathn 2 upstreamof the flaw holderand adJustedto the oomhustlon-damberareabythe isentiropio-flowrelations. For thisreasonthe Maoh nuribers=e designatedM2t. ThisMaoh numberdoesnot actuallyexistatthe flame-holderInletbut is oonventkmallydefinedon thisbasisfor cmmenienoe of referenoe. The trendof Maohriuberwith fuel-air ratiowas similarfor eachflameholder.” TheMabh numberdeoreasedwith increasing$7x&air ratio,remhing a m?.nimumvalue between
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0.135and 0.150at the highestfuel-airrattosand a maxlmumovalue* with annularInjeotionof slightlygreaterthan 0.220at fuel-air
ratiosaround0.03. A separationin the data for ~form anda annularInjeotlonoccurredas a resultof the changein mnbustlon2 efficiencysubsequentlydlsoussed. For a few of the flameholders,
alightseparationalso ocourredwith altitudebut was so smallhmost casesthat It was obsmred by e~erimentalscatter.
Stableccunbustlonllmits.- The reductionin ccmbustim-chmtber-outletpressure PA with increasedaltitudeis shownin part (d)off@ures-6 to 15. h mmbusttan-chaniber-outletpressurefor a givenaltitudeticreasedwith fuel-ah ratio in orderto satisfyocntinui~y.For uniformlnJeotlon,burrdngwas accomplishedfrcunslightlyoverone atmosphereto approximately2/3 of sea-levelatmosphereoutlet
The burning-~essureremgewas extendedwith annular,“
pressure.injectionfor acmeflameholdersto lessthan 1/2 atmosphere.
d The burnl& blow-outlimitssu?etndlcatedon the plots afcauibustion-chsaiber-outletpressureby the dashedllnes. Althoughonlya singlellne is shownfar each limlt,the blow-outregionIs.in realltya band of fuel-airratioslocated=ound the dashedllnes. The band probablyextendsover a regtrmof about 0.005infuel-ah ratio. Thisfact [email protected] the appearaaoeof omaeionalstibleuperatingpointsoutsidethe blow-outlimttsfor sczueflameholders(forexample,flg. 9). b general,the fuel-airratioforleanblow-outInxeased as the simulatedal.tttudeincreasedforboth uniformand annularinJeotlon)whereasthe rioh lhlt fuel-airratiode6reacedwith Increasingaltitude. The operating range offuel-alr ratiosthus deoreasedwith increasingaltitudefor allflaneholders. The altitudeabovewhiohburningwas not possiblewas reachedonlyfor flameholder1. Annularinjectt~ extendedthe leanblow-outfuel-alr~tto llmltfor all flameholderstives-tlgated. The richerzoneof fuel-airratio provided by annularinjectdonapparentlyprduoed a more favcmablemixturefor ocabus-tion in the regionof the flame-holderguttersat low over-allfuel-air ra%los. The maximumoperatingrangeof fuel-alrratiosvariedfl’a a lean llmltbetween0.04and 0.05to a rtch llmltbetween0.07to 0.08for unlfonnin$eotia at the altltudesinvestigated.The leanllmltwas extendedto approximately0.03fuel-atrratiowith smnulerinJeotion.
Gas-flowparameter ● - As shownin the appemdix, the gas-flow~ameter p5A5/W5 is a functionof the ocuubusttonefficiienoyandthe ccmbuetion-chamber-outlettemperature.The &as-f’lowdata are
. presentedin this famto use as a measure of
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becausethe gas-flowPam&ster Is ccmvenhnt
mubustion perfozmuume,for estimationof
a
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enginethust, end to detezzuinethe air-fla rate throughtheengine. The gas-flowparameterincreasedwith ticreasbg fuel-airratiosup to approximatelystoiohiometricand thendecreasedslightly. Differencesbetweenflameholderswere small;far -exemple,at a fuel-airratioof 0.05 the valueof ga8-flowparemeterwas frcau61 to 64 for all flameholders. Becausecombustioneffi-cienciesfor annularinJectionare lowerthanfor unlfozminjection,the gas-flow+xmuneterourvesfor the two typesof inJection sepa-rate considerably.The gas-flow~ameter for most of the flameholderswas independentof altitude;for a few flameholders,however,a slightdecreasein the gas-flowparameteroccurredatlow fuel-airratiosas the altitudewas increased.
Combustlcmeffioienoy.- The curvesof combustionefficiencyqfollowthe sametrendsas the gas-flow-psmmetercurves. As pre-viouslymentioned,oonihstiranefficlenoyis influencedby ccunbusthn-chamber-inletpressureand velocityas wellas fuel-airratio. tigeneral,the co,nibustlonefficiencyIncreasedas the fuel-alrratioincreasedup to approximatelystoichlometrioand thendecreasedslightly.The combustionefficiencyfor a few of the flameholdersdecreasedas the altitudeincreasedbut was independentof altitudefar most configurations● The mmbustion effloiencyfor aanulerInjectionwas generallylowerthanfor uniforminJectionatcoqperablefuel-atiratios. The measuredvaluesof uniform-lnJectlanccmibustlonefffcisncdesvariedI%om 0.7 to 1.0;whereasfor annularl@ection the rangewas fha 0.4 to 0.9. Visualobservationduringannul.ar-inJectlcnoperaticmshowedthatflamewas presentonly Inthe centerof the combustionchsaiber.
Data obtainedduringrunswith blendlngof the two fuelmeni-foldsare shownIn figure7. A smoothtransttia from annularinJecthn at the lowestfuel-alrratiosto uniforminJeotionathighfuel-alrratioswas acocmplishedwithoutoperatiaualdifYhulty.The ocunbustion-effioienoycurvefollowsa ~adually Increasingtrendwith increasingfuel-airratto.
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Compartsonof over-allperfcmmmlce● - The factorsto be con- ..slderedin an over-allperformancecomparisonare pressurelosses~combuetim efficlancy,and operatingfuel-alr-ratiorange. usually,the cmlyrequirementIs to obtainthe highestpossiblecombustionefficiencyaccompaniedby thewidestattainableoperatingfuel-air- - -ratiorangeand the luuestpressureloss. For someapplications,however,an evaluationof the effectsof altitudeand fuel-al??ratioon &ese performanceparameterswith referenceto the fllghtplanand diffuseroperatingcondltiansis necesssrybeforethe mostdesirableconfiguration= be selected. Overthe range of altitUd06
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investigated,the tidestoperatingrangeand lowestleanblow-out* limitsfor both uniformand annularinjectionwere obtainedwith
flameholders3 and 10. An approximateortsm of efficiencies
kand pressurelossesoverthe rangeof steadyoperatingconditionsmay be made by ocxugm?ingmaximumcombustionefflolenoyand oombusticm-ohamber-pressweratios:
holder
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ccmbustionBfficlelmy
0.92.88.96.90
1.00.98●95.99..91.94
ccmibusthl-ohamber -
pressurerat10p4fi2
0.93.92.94.92.91.93.90.92.92●92
The data showthat oombuettoneffloiemoywas nearlyindependentofthe mubustion-chambsr-pressureratio. An efficiencyvariatianof12 peroentooourredwith a pressure-ratiovariationof only4 per-cent● l!henwu3mnuefficienciesof flameholders3, 5, 6> 7} 8~and 10 were between0.94and 1.00and may thereforebO consideredof comparableperformance;flameholder5 had the highest~efficienoy. The mibustion effioiemiesof-theotherflameholderswas from 0.88to 0.92. On the basisof the highestoonibustioneffioienoy(O.7 to 0.95) with reasonablylow pressuredrop andwidestoperatingrange obtained,flameholders3 and 10 are mn-sideredto be the best of the 10 flameholdersinvestigated.Flamehold= 3 had a slightlylowerpressureloss;whereasflameholder10 had a slightlywideroperatingrange.
Effeotsof gutterwidthand blooked=ea on ccmibustionefficiency.- The ocmbueticmeffiobnoy Is plottedas a functionofgutterwidthfor two nearlyconstantblookedareas,fuel-airratios,ad ccmibustton-ohamber-outletpv?essuresin figure16. These ourves
. are WOSS plots Of f i-es 6 tO ~ ● For thesefuel-airrattosnearstoiohlometrioand fcm thesepressuresof approximatelyone atmosphere,
.~“ - “.-’”
XL
12 ~“ NAOAM E50H21
.“
gutterwidthhad littleeffeoton the ocdbustloneffioienoyfor agivenblookedarea. Data for a fuel-airratioof 0.045 (notshown)had a similartrendat aboutthe samepressureleveh. Insuffloient
R
datawere obtained,however,to determinethe gutter-widtheffeots3
at lowerpressures.
The effeotsof blookedarea on oombustloneffibienoyare shownh figure17 for similar oonditims of pressureand fuel-airratio.A generaltrendof increasingeffioienoywith inoreasedblookedarearesultedfor gutters1.50and 2.00lnoheswide. An inoreaseof 5 to 8 perpentin ocmtmsticmeffioienoyooourredfor an inoreasein blookedarea&om about40.0to 62.0peroent. The effioienoyofflameholderswith 1.00-inohgutters,however,reaoheda maximumatan intezmwdiatevalueof blookedareaand dimreasedas the blooked -area inoreased.The ourvesfor 1.00-inohguttqm are more subJeotto errorthanthosefor widerguttersbeoausetheyare basedondata for onlythreeflameholders. A ocmsistenterrorin the datafor any cm flameholderoouldtherefareshif%the entiretrend, “Partioukmlyin view of the relativelysmallohangesin effio~enoyinvolved. “The ourvesfor the widergutters,however,are the resultof orossplotsfiotudatafor five flameholdersand are ooneidered .
more aoourate. The inoreasedeffiolenoywith izmreasedblookedm?eawas attributedto the involvementof a largerpercentageof theinocdng fuel in regionsfavorablefor ocmibustion.
Correlation of operatingr~ data.-metheol?y or buz’d.ngin the wake of bluffbodiesdevelopedin references2 and 3 andindependentlyin referenoe 4 postulatesthat ocmtinuousignithnoooursas a resultof transferof hot gasesfiaureoiroulatingeddiesor vorticesimmediatelydownstreamof the bluffbody intothebound-y regionof relativelyooldfuel-air?n.ixtures.The tempera-ture of the boundarymirhre oonseguentlyinoreasesas the flowprooeedsdownstreamuntilthe appropriate@ition temperatureis
——
reaohed. lhmm a heatbalanoebetweenthe heat-supplyrate ~uiredfor ignitionin the boundaryzoneand the rate of heatflow ficmnthe eddyregion(Seereference2 for a detailedderivation.),It canbe shownthatfor a givenfuel-air-ratiodistributicmand for aocmstantinlet-airpressureand temperature,the followlngrelationspplies:
M@= @(f)
where f is the fuel-airratio, n is the width of the bluffbodr(gutter) , euldindependentof
@ is a funotion&l notatkm. The relationis -blookedarea. The value of 0.45for the emonent a,
.
NACAm E50H21 ~ ‘“’”””9”- 13
.
detemlned emplrioallyIn referenoe2 for guttersof lomg spau,1ss used for the plotsWesentsd herein= similaroo?%elattm was
obtained,however,when an expment of 1.00was used.
Crossplotsof the faired blow-outfuel-air+rattodata of this
reportas a funoticmof the ocarelaticapemmeter ~ t/n””45 arepresentedIn figure18. Curvesam shownf= ocmstantpressuresof1400and 2000poundsper squarefoot absolute. The de@ee of cor-relationis goodfor all ourvss. The data spread1s less than halfof the gen&al trendin all oasesand iswithin the limitso% repro-ducibility.The soatterx be ~1.y causedby slightdifferencesinfuel-airdistributionfa the dmerent gutteramaqments. Althoughit is possiblethat this oorrelatlaumay be enttrelyfcmtuttous,thesimilarresultsof the referenoereportsadd considerableoredenoetothe fundsnmntalnatureof the mmzelaticm. -
-~s~ of flms 18(a)* le(b)M that deo=+s= ..pressureleveldeoreasedthe operatingfuel-a~ratlo raagebyInoreaslngthe fuel-airratiofcm leaublow-outand decreasingthe
. fuel-airratiofor rioh blow-out. As the inletMaoh nuniberwasInoreasedcm the gutterwidthwas deoreasedfor a givenpressure,a stiilarreduotionin operatingrmge ooourred. The operatingrangefor a pressureof 1400pourdsper squarefoot Is extremelysensitiveto inletMoh number. Referenoeto figure18(a)shuwsthatan inoreaseIn Maoh nuniberof 36 peroent,resultlngin aninoreasein the correlatlaparameterfk-am0.11to 0.15,produoeda demease In operatingrangeof nearly75 peroent. Compen-sationfor the fnorsasedMaoh numberby increasingthe gutterwidthto maintainocmatantoperatingraugewouldrequtreapproxi-matelydoublingthe gutterwidth. The slopeof the lean operatinglimltourveIs very largefor the lowervaluesof the oorrelathnparameter;Ocmsequemtly,furtherInoreasesIn gutterwtdth ordecaeasesin Mlet Maoh nuuiberwouldyieldvery smalldeoreasesinlesnblow-outfuel-airratio. The rloh llmttsfor the lowervaluesof the ocmrelationparameterare at fuel-airrattosgreaterthanthosefor maximumoombustion-ohauber-outlettemperatureand arethereforeconsideredsatiefaotwy. E’uturedevelopmentof ram-~etocmbustorsfor wider operatingrangewill thereforeprobablyrequirecontrolledfuel-air-ratiodistributlm ti ocmiblnatlawtth flame-holdingdevloesdesiguedto producemm?e favorabletypes of reotr-mlathg vortexflow in the flaw-holderwake or the use of speoialpllotlngdevioes.
.
,:-
—
suhMARYol’IqsuIm
An altitude-test-ohamberinvesttgatlonof the ocmbustionperfcmmanoeof 10 flameholdersin a 28-inohrsm-~etengineovera rangeof simulatedaltitudesfrcun40,000to 55,000feet and ata simulatedflightMaoh numberof 2.0 @ve the followingresults:
1. A 2-inohwide 60° gutterflame”holderwith 45-permntblockedareaand a 2.50-inohtide 60° gutterflamieholderwith60-peroentblookedarea had the most favorablemubinatlon of wideoperattngran@, high csombustIon effIolenoy,and low pressurelosses.
2. Far theseflameholders,stableopeZ%tlonat a simulatedaltitudeof 50,000feetwas obtained~with inJeotlonfimu two fuelmanifolds(uniformInjeotion)fran fuel-airrattosof approximately0.040to over0.065. bJeotion ficma singlefuelmanifold(annularInJeoticm)etiemdedthe leanblow-outfuel-airratioto approxi-mately0.030. Combustioneffioienoieswere from 0.7 to 1.0 overthe operablerangbfar uniformtiJectionand fi?om0.4 to 0.9 forannularI@eotion. Combustion-ohambempressurelosseswere 6 to8 percentof the mxubustton~ohamber-inlett~talpressure.
.
3. ~ general,annularinjeotionprovided100allyrioherandthereforemore favorablezcaesfor ocmibustlonfar the lean over-allfuel-alrratiosthanunlfcumti~eoticmand resultedIn a reduotimin leanblow-outfuel-alrratio. Cwibustioneffiolenoieswerelowerwith aanularlnJeotionthanfor unifom inJectlonat comparableover-allfuel-alrratios.
4. Ohangesin gutterwidthfhxm 1.00to 2.50 inohestitho~tant blookedarea had no appreolableeffectun mubustlomefflolenoyovera mnge of fuel-alrratiosfrom (?.045 to Q.065and for pressuresof approximately1 atimoephere.Increasingthe - -
—.—
blookedarea frcxn40.0to 62.0percentwith gutters1.50and2.00tioheswide resultedin an inoreasein mxubustlmneffIoienoyof 5 to 10 peroent. For 1.00-lnoh“widegutters,increasesinblookedareafiau 42.0to 48.0percentresultedin an Inoreasein effloienoy;furtherInoreaseto a blookedarea of 55.0percent,however,resultedin a deoreasein oombustlonefficiency.
.
NAOAW E50H21 ~-”-”””.
5. The lean and rich IMw-out fuel-air~atlodatawere o~e-+ latedby use of the rattoof mabustion-chamber-inletMach nuuiber
to the guttertidthraisedto the 0.45puwer. The degreeof ocu?-relatlonobtainedservedta verifythe work of previousinvesti-gatorsand to -nd theirwork to largersoaleoombustors.Theshapeof the ourvesobtainedindioatedthat furthergainsby
g Imreaslng gutterwidthbeycmd2.50 Inoheswouldbe very small.
m’
Lewisnight PropulsicmLaboratory,Hatimal AdtisoryCmmittee for Aeronauttos,
Clevelsnd,Ohio.
l-s
.
“
.?
16
A
a
f
6
M
n
P
P
R
T
t
w
2’
v
The following
area, sq ft
~ -
APm.mx5 - CALCWATIONS
symbols -
symbols are US9d. throu@out
empirtoal ccmstant
fuel-air ratio
aooeleratlondue to
Maohnumber
@ter width,in.
gravity,ft/0ec2
total preseure,lb/sq“ftabsolute
statlo pressure,lb/sqft absolute
@S ‘oonstant,ft-lb/(lb)(%)
totaltemperature, ‘R
statIc temperature, OR
WOlght flOW, lb/890
ratio of speoifio heats ..
combustion effiolenoy
~’ funatlonaln@atLon
Subscripts:
2 Cxxldi.tions at
2’ conditionsat
4 conditions at
5 ccmditdons at
NAM mE501121.
.
the report:
ccmbustim-ohamber inlet .(station 22P)
station2 adJuetedto combustion-chamber
combustion-chamberoutlet(station280)
exhaust-nozzle throat (station297)
—=-mm=-*
.—. .
—
---
..
-.:.?
I ... .,... . .
*
area
.
1
3 I’w2ARM E50H21
.
Oalmlatim
-
Win==—= ‘“= 17
Of Combustion~iCt9nO;
The flow at the erudneexit is assumedto be idealone-dimensional% uniform flow and the as&mption Is tie that the Maoh number at the
2 exit-nozzlethroatis 1.0 with a flow area equalto A5. Under theseconditlaasthe followingrelationmay be derived:
()’452M (y+l)T5=—w~ ZR
(1)
where y is the valuefor averagebetweentotaland statto tempera-ture at the throatend for the prevailingfuel-airrattoand R is53.5foot-poundsper poundper OR. TIM _uted temperatureT5 isthen oorreotedfor the heat reJectiaato the ombuaticm-chamberOoolingwat@ ●
dThe oaubusti~ effiolenoy Is defined as
‘T5-T2)a~ual
~ = (T5-lC2)idml(2)
ts obtainedfz@ reference5.
of p~ usedwas the numerbaltubesand fourwall statioorifices.the cxmmutedvaluesof T. end n
where the ideal temperature rise
~ oomputing T5 the valueaverageof eight~il.ing statloThe possibllttyof inaaouraoyindue to the many assuu@icms involvedis ~bvious. The magn?tudeof-the errar,however,wouldprobablynot be greatlyaffectedby oon-figuraticm,and valuesprobablysatisfactoryfor relativecowarisonwere obtained. A plot of the relations between eqyations (1)and (2)Is shownin figure19. The gas-flowparameter p5A5/W5 tsplottedas a funottonof fuel-airratiofor variousoonstantcoxtibus-ticm effiol=oiesand ocmbustion-ohaniber-outlettotaltemperaturesfor an inlettemperatureof 710°R. The plotmay be usefulforevaluatia of ccxnbustiontemperaturefrom the data presentedinthe reportor to establishthe relatlms betweenthe other ocaibus-tion -iables .
.
.
18 NACA RM E50H21
●
~.
. Rm’ERmcB
1. Jones,W. L., Shillito,T. B., and Heu–el,J. G., Jr.: Altittie-Test-ChamberInvestigationof Performanceof a 28-InohRam-Jetlhgine. I - Co.uibustionand OperationalPerformanceof RburCcmbustlon-cheuuberConflguratione.MCA RM E50~16,1950.
2. Wlllhus. GlennC.: BasloStudieson FlameStabilization. Jour.#Aero. Sci., vol. 16, no. 12, Dec. 1949, pp. 714-722.
3. Goss, W. H., and Cook, mory: The Ram Jet as a SupersonicpropulsionPlant. SAE Trans.,vol. 2, no. 4, out. 1948,PP. 642-657.
4. Reiter, Sidney, ad DeVault, R. T.: Experimental Studies ofSupersonic Raqlet Cgmbustlon. USCAL Rep. 4=9, Aero. Lab.,USCLA, June 1848. (Navy Contract NOa(s) 8257, Items 2 and
5. Mulready, Riohard C.: The Ideal Temperature Rise Due to theConstant Rmssure Cdmstlon of Hydrocarbon Fuels. Meteor
3.)
Rep. UAC-9, United Alroreft Corp.; July 1947. (Proj. Meteor,Bur. Ord. Contraot NOzxl9845 In moderation with M.I.T.)
,
.
..:.
8 .
-...
I k
.
.
E!
, ,
1
!:”..-- . ...! ,,, 1,
, s
S6srt
I combus$on ~ ‘1,
l.\timber :.,.,
.-!.. \ ,,
Longerons~ -
1!E!
1!P
.
g
. . .
. . . ..-.
.
.
I # L .
86!n.
Ii’!4
i!r
,*“”
r ,
n
u
titter
.
?lam Q3ea.
I
.
.
.
-lr
(a) A holller 4; blcdsa -, 40.5 -; m Wiw, l,SJ ~.
..,..,
1 , 86ST .,
, .,
lom
8 B481-2128
I ,1.388
t *
(e)m ho-ldm 6; monkd Llron, 60 pemunt;- Wi&hIl, i?.ooilldw.
m4m=4. -o=M.m=L ~tio alagam (ICfume ~.
.
.
mltk?r
#
..1
(f)= -e; b~ -, 58 wrmnt; gnttorwidth, 1.20 imhea.
-4. - CaItimma. achamtia d.. d fk holdmn.
,,, -
, ●
E!
,,,.
1 i.,I . em: .’.,..
,....11,,,,,,f:
, *4S1-2129
I ,
.
lxm, .
.
—
1“P
.
.
1.
,, .
. t-wvr. ‘r.?i-.
, ,.cM.la
1 ,
B!
I(1) - holds 9; b~ -, 56 -; - Viwl) 1.40-.
mm=4.-~. ~tia luagmm d f- Iddnm.
i!r
I
.
‘ Lzli?-m, . l“, 86!n
f
.’.
1“
ii
1!r
I
WA W E5CE21 33
.
.
.
.
●
9
●
●
Inner~ body ~jeothn “’
08‘ o Utiorm❑ Annular
06 u
/ Y
\
\ n
04
02
(a)Ty@oal f!uel+lr ratio distribution.1.07
1.06 ‘Inner
~ body1.06’
1.04
1.0s ‘
l.oa A
1.01
1.00.2 4 6 8 10 1S2 14
Radial dtstanoe from oenter line, in.
(b] Typical pressurematio distribution.
F18ure6. -Radial diotributlon of fuel-alr ratio and pressureratio
●
at mnlnmtion-ohamber inlet.
“~-”
IMCA RM E50H21
.’
I
Altltude(rt)
0 40,000❑ 48,000
S!*o
1.9
+ q -
1s8
1.7.(a) IMmtet-uomle pawssure ratio.
,.
●eo
-a ~ “2
.. 0- - 47 * L—
● 10●W .03 .04 ●06 .06 .W7 .08
Fue141r ratio(o) Combuethn-ohamber-inletMaohmmber.
Figure 6. - Perfomame ourves for flame holderL Gutterwidth,LOO fnoh;blooked area, 42.0 peroent;uniform lnjeothn only.
.
.
.
.
.
.
I?ACARME50H21
.
.
.
.
. rlah
Q600“
9400
2200
moo L
1800 d ——.—1600 L bl~-out
1400LAltitude
moo ‘(ft)
~ 40,000❑ 46,000
1000
600(d) Oombustlm—ohamber—ou tlet~ssure endblow-out ltits.
(e) Gas&low faotor.
“1.00” uo
+ - ~o
~. -
.60“
.60
●40.● 08 805 .04 .06 .07
Fuel-aL?rat%0●O6
(f)Ocahstiuneffislenoy.
=-e & . a~~ludedo.
Performame ourves for flame holder 1. Gutterwidth,1.00lneh~blookedarea,42.0pereent;unifomuin~ecthn only.
36 NACA RM E30H21*.....d*..,.
.
.
G“i!?
(a)mwmst-nozzle pressureratio.
.,
.30
#
.20 %
11
● 10 - - *●02 ●O5 .04 .06 ●06 .07 ,08
Fuel+lr ratio
(o)Ccmbuettoa-ohamber=-inletMaohnumber.
Fimre 7. - Performsme ourves f’orflame holder i?. Gutter width,1.00 inoh; blooked area,
—
.— ---
,..-.
.
.
55.0 peroent. .- .
.
.
.
.
m ES(H21 37
moo
2400
u:&rm 0“
Sooo— — ~blow-ou. A\
5 9 * &’
u
“
~~ ‘
\Moo
i%Iform rtohblow-out
lm d
$P o
1400 AAnuularl
/P’
blow-out~ >1200 ,L
r* ~eetion Altttude
UniformBlend5ng(ft)
1000 0 40,000> 46,000
: 50,000
600
(d) OombuetLm+ha@m=utlet messure and blcm’+utlimlts.70
a
60— — — — —
60 D>
40 D(e).Gaa-tlowfaotor.
An I I kFtel-alr ratio
(f) Ccmbuetloneffleienoy.
Ftgure 7. -Comluded. Perfomame curves for KLame holder 2. Gutterwidth, 1.00 inoh~ blookedarea, 55.0 permnt.
38 IMCA W ESlE21
,-
1
InJeotlcm AltitudeUnlfom Annular (ft)
“ot
40,0004J3,000
: w 60*000
1.9 + ~ ~b ~ ~
~ o1.8 .
1.7(a) Ea$laustmsme msmre ratio.
,.30
-1\● go
o
● 10 .● 02 .03 ●04 ●O5 .06 ●U7 ●09
Fuel+ir rat10
(o) Cmubuatton-ohamber-inlet Maoh number.. . .
.
.
.— .
●
Figure 8. - Performanceourves forflameholder3. Gutter width,%00 lnohes~blookedarea, 45.0 peroent.
.
●
✎
r
EM E5W21 39
8600“
2400
2200
2000
1600
1600~ {
1400rleh
lEOOLblow-out
+Unlfo& lean
1000 “blow-out
#kinlnllarlean h$ ediion Altltude
blow=out U!lifomllAnnuw (rt)800 0
~ Z:E: * 60,000
(d) Caibustlon-ohamber-outlet preemu?eand bl~ t I..lalltso
g 70 .
jlg60— — — — -
%$“$a ’60u
c? 40(e) Gas&low faotor.
L 00
~: .=*
d
!
i!d 7●60‘
.ij*
/ -.
h
,4C. I● 02
Figure 8. -
●03 .04 .06 .0? .08Fue14Nratlo
(f) Combustioneffloienq.
Conoluded.width, 8.00
p~rO=Oe curves rOrflameholder 30 Gutterimheo; blookedarea, 45.0 peroent.
Altltude(ft)
o 40,000❑ 48,0000 50,000
990
1.9, m ❑ &.n > ‘ .“u
. -
10e 61
107 .
.—
*
.(a)Exhaustmossle preseure ratio.
(b) Ccmbuetion+hambertotal=presmreratio.v
.02 .03 .04 ●05 .06 ●07 .OaF%el-alrratio
(o)cambuetion-hamber-inletMaohnumber.
Figure 9. - Performancemrves for flame holder 4. Gutterwidth,1.50 imhes: blooked area, 40.5 peroent~ uniform injeotion0?14.
NACA RM E5QHZ1
b
*
F
f?600L
mm
1600
1400
1000.
600.
600
(d) Combnetlon+haniber-outletpessure and blow-outlimits,
(e) Gcukflow facstor.
1.00
●8O
●60
●40.09 SOS ●04 ●O6 .06 ●07 ●08
Fue141r ratio(f) Ccunbuetimeffioienoy.
Figure 9. - Conoluded. Performanceourves~orflameholder4. Gutterwidth, 1.50 lnohes; blooked aren, 40.ESperoent; uniform lnjeotlononly.
41
42 N&2ARME50H21
.
(a) Exhauet+omle pressureratio.
(b) (haabustlon=diambertotal-pressureratio.
I I I I I I I I I I I I I
●30
1 I I 1 I I I I I
● ~vl I 1 1 1 I I I I I .,.
.02 ●O3 ●04 .03 ● 06 ●07 ● 08Fuel+ir ratio
(0) Cdilet ion+$hamber-inletMaoh manber.
Ftgure 10. - Performame cnu?veefor flame holder 6. Gutter width,2.00 inohes; blooked area, 60.0 peroent.
1
*.*.-’ --- .
.
.
.
WA RM E50H21
Ill
(d) Cambustlon-ohamberatlet pressure and blow-out limlts.
70 .
60‘ w - A
60
40—(e) Gas-iClowfaotor.
1.00
●8O .b
● 60
,40● 02 .05 ● 04 .05 ●06 .07 .08
Fuel-alr ratio(f) Ccmibustion effleienoy.
Figure 10. - Conoluded.width, $?.00
Performenoeourvesfor flame holder 5. Gutterinches; blooked area, 60.0 peroent.
44 NACA RM X50H21
o 40,0i30
1*9’
1.0
1.7(a)&haustAossle~essureratio.
(O) 0aubue610n-ohamber-inletiMaoh rnnnber.
B’lgure 11. - Performanceourveeforflameholder6. Gutterwidth,1.80 lnohee~ blooked area, 58.0 FOroent; uniform lnjeotlcm 0n4.
.
.
.
I?MA RM E501121
.
.
r
*
8600-o
. \
/ y
\ &\ ~OllU rloh\blow-out
vIMrorm leanblow-out- .
1600
1400
Altitude
o 40,000
600
600
1.00s
J“.60*
II
i . .
: .60
“% T .●40,02 ●03 ●04
Fu&z ratio●06 .07 ●O6
(r) o~tta drIOkQY.
Figure I.I..- Oonoluded. Per~omenoe ourveafor flameholder 6. titter width,1.90 lnohee; blookedarea, 66.0 QePoentj uniforminjeotion only.
46 NACARME50H21 ““
.
Uhirol.ml,@llmlaro
1.9 ‘
1.s
107(a) &@mzat+ozSle pressure ratio.
.,., ..,, ..=.=_.
:..
*—
.. s-
.-. .
8 #
IIbm1.0% -..
j~. .9 “’““,. .,
— — — — .... F + ❑
;
g~ ●8 “+ (b) (kmbtmtiau+hamber total-pressureratio.
.30
.20
●10.09 .03 .04 ●06 .06 ●07 ●08 ●09
Wel-air ratio
(e) Combuetlon-chamber-inletMaoh number. ,
..—-.
. .
-._:
. . ..
n
Figure12. - Perrozmamec)urvesforflame hol&er“7. Qutter vi~th, 1.38 “’” ““imhea; blooked area, 6$?.0pement. .
NACA RME50H21 47
(d) Ccmbustloa=ohadmr-outletpaessureand blow-out Madts.
1F
.02- 903 ●04 .08 ●O6 .07 ●0s ●O9Fuel-air ratio
(f)CcmbuetlonO.fflotenoy.
Figure 19. - conoluded. Performmoe ourvesfor flameholder‘7. Gutiterwidth,1.38 inohea;blookedarea, 6$3.0peroent.
.
NAM RM E50H21
(ft)
(a) EMmwt~zsle pressureratio.
(b) Ombustlom-ohamber totalqmessure ratio.
20.
a- ~ = a’#1 ❑ 8
G w Ou
10●05? ●03 .04 ●06
FuelGZ ratio●0? 908
(o) Cmubustlon-ohamber-inletMaoh number.
Figure 13. - Performame ourvea for flameL 00 tich; blooked area, 48.7 peroent;
holder & Gutter width,uniform injeotion only.
.
.
iG-8
--
7
.
.
.
NACA RK E50H21 49
8600
Moo
2200
blow
1600 -
.1400
lmo Altltude
1000Q 150,000
(d) Ccudmstion+hamher-tlet prensure and blow—mt limlts. .
70
.-~ 40
(e) Qas-flow f!aotor.
1.00
g; .80$a
I3~ ,60
U:● 40
.02 ●03 ●04 ●O6 ● 06 .U7 ●O6Fuel-dr ratio
(f) Combustioneffieienoy.
Figure 13. - Concluded. Performame ourvea for rlame holder 8. Gutterwidth, 1.00 inch; blooked area, 48.7 pement; uniform Injeotiononly.
.
.
MA(2ARMS$50H21
*
I
._Altitudem)
0 40,000
: ?O:Os..
.. .
n—o
❑❑
(a) Exhaust+ossle pressureratto.
..“b
—
8,. ,
.●
(b) Mabustlon-ohember total-pressureratio~
.02 .03 ●O4 .06Fuel-% ratio
●O7 .0s.
*.
(o) Canbuemxwmamber+let Mach number.
Figure 14. - Performance ourves for flame holder 9. Gutter width, ‘“ “1.40 inohesjblooked area, 55.0 peroent;uniform injeotiononly.
NACA RM E50H21 51
.WOO ~
moo ~ /
moo — — —unifc&rm 3
blow-outi+ MIIMhml\
1600‘blow-out
/
~ z’1400‘ /
1900 Altltude(ft)
o 40,0001000 ❑ 4s,000
o f50,000
(d) Combustion-ohaniber-outletpressure and blow-out 15mlts.
—(e) Gas-flow factor.
1000❑ b n %
●80 o
●60
●40.02 ●03 .04 .05 ● 06 .07 .08
Fuel-air ratio
(f) Co3nbustiaueffioienoyo
Figure 14. - Comluded. Performame Ourvea for flame holder 9. Gutterwidth, 1.40 lnohea; blocked area, 5#.O peroent; uniform ln$eotion only.
NACA RME5~1
tijeotion Altitude‘mllformAnnular (St)
o 40,000t. 46#ooo
: * 50,000u 66*000
23 109H u o
j %.8 —Eg ~> -V
1107.
ii (a’)muet+lomle pressure??atlo.
-
~r’
.-
.
.
. . *.
.
.
Figure I.& -
Fuel-air ratio(o) Codnbuetion-ohamber-inletMaoh number.
Perf%manoe owes for flame holder 10. Gutter widthi9.60 inoheet blookefl area, 60.0 peroedh
.
IOWA RM E50H21
.
53
.
.
,
1%!00,‘- l._l I Injeotion Altitude.-
t1110 b 40,000
“- Iloo
I IJugooo
-~ I 1.1 56,000/ -
,
II -n~wl-” I I800 I
600\ I p’- Anmuar lean blow-t I I I I I(d) Combustion-ohamber-outletpremmre and blow-out limlts.
(e) Gas-flowfaotor.
F1.00
●80>v
.60 ~ * *
.40..●02 .03 .04 ●06 .06 ●m
Fuel-a3r ratio
(f) Ctit%= effiolenoy.
Figure I& - ConoludecL Performanceourveo for flame holder 10. Gutterwidth, 2.50 Imhea; blooked area, 60.0 peroent.
54 d-w ~ .- IVACARM E50H21
1
1
,
Blookedarea
(peroent)
-----60 to 62—40.6 to 46
.0
..
-. .-
.8
●
7“a) Fuel-airratio, 0.05; c-stion-ohamber-outlet totalpressure P4, 1600 pouIMs per square foot absolute.
,.0‘.-
.0
,6.1.0 1.4 1.0 %.a 2.6
Clutterwldthg in.
(b) Phel-alr ratio, 0.06j oasbustlon-mer-mtlet totalpressure P4, 2000 pmnds per sqpare foot absolute.
Iilgure16. - Effeot of gutterwldti on oom@ustioneffioienoy.
r
_—.-
b
..,.-
.
.
.
.
.
.
N40A RM E50H21
Gutter width(in. )
1*O-----1.38 to 1.5—.— 2.0
●
100
—- .— -.—
.8
,6.4.
(a) Fuel-airratio, 0.05; mmbustion-ohamber-outlettotalpressure PA, 1800 pounds per squarefoot absolute.
55
*9U
— -——. .—
.0
.6 I
-“40 44 48 # 62 66 60 64Blookedarea, peroent
(b) Pueldir ratio, 0.06, mmbustion-oMmber-outlet totalpressure P4, 2000 P-S per square foot absolute.
P@ure 17. -Effech of blocked wea on mnibustloneffloieney.* . .- ;-—a. -.*.--
.
NAM RM E50H21
.
&
, Flame● i?4‘
A4
.Q~-V5
h 10
~ “m ‘Annu&ar
~blow-out
A
* ●W3
+
#Io
j’.16 ~?
!’ ‘ ‘
n
~.14
~u:;f)lnl
II v
s ● le ‘ blow-outv
*\
.10.
.06..08. ●OS - .04 .06 “.06. .07 ●06
Blow-out fuel-alr ratio(a) (Xambuatlcg&hambe&tlet tothl pressure. P4, 1400 pounds per
aquaro foot absolu,te.
Figure 180 - Oarrelatim of blow-outtits.
*
,.. =.-
8
‘Q
.
.
I’UCARM E5CIE21. 57
(b) Combuetlon+hberatlet total presml?e ?4, ~m pouuds persquare foot absolute.
Figure 18. . Conoluded. sorrel.ation of blow-outdata.
* *NACA-hWW -11-6-60- 476
NAM ml E50H21
#
60
60
40
30
,
Ocaubuetim-ohamber-outlet
*emperatuneT5(’%)
Lcc4nbustimleffioienq, q
00
— —
L/ ‘// ~ o
— — — lmo— ~ ~ . — . .
— . — — — — — — —
1
0 .02 .04 ●06 - .08. 140Fue14ir ratio
Figure 19. - Relaticms betweenwarlous oanbustlm parameters forInlet temperature d 710° R.
,.
.
. .- .=-iii&a
. .