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9$ SECURITY INFORMATION --n
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RESEARCHMEMORANDUM”
INVESTIGATION OF INTERNALI
OF A 1OOO-POUND-THRUST
FILM COOLING OF EXHAUST NOZZLE
LIQUID-AMMONIA LIQUID-OXYGEN
&OCKET
By Andrew E.Abrarnson
LewisFlightPropulsionLaboratoryCleveland,Ohio
CUSSIFDID~
l%iuumerielcmtalmldmmtlonmff-tlnsti NatlmhlB-femecfGmUzdtOIWbauitib meacdncd M .ssPfOmSOwm,me m,u.s.c.,SECS.764ad 794,theImmmfsslonorramhtlonofwIdchh qnbumrtoanumutbrlzedperwnlaPrOMMtadWlaw.
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.
<
NATIONAL ADVISORY coMMITTEEjj ‘FOR AERONAUTICS “
WASHINGTON ~ ~ w
IT IU.CARM E52C26
●
IUYTIONAL.
ADVISORYCO14MXTE3FOR
RESEARCHMEMORANDUM
,.
AEROMDI’K!S
INW3STIGATIONOF INIEMKLFILMCOOIZNGOFEXHAUSTNOZZLEOFA
1OOO-POUND-THRUSTLI~-MM3NIli LJC/llD-OXYGENROCKET
ByAndrewE.Abrsmson
E, SUMM4RY.* *-”-
An investigateio~”&
-rnal filmcoolingoftheexhaustnozzleofa 1(MO-pound-@rust “._nia liquid-oxygenrocketenginewasundertaken.The@p~.&enJ$.Covereda rangeof oiidant-fuelratioswiththecombustion--e~essure varyingfrom220to 275poundspersquareinchabsolute~a~~d anhydrousliquida.uznoniawereusedascoolantstiththeco&E%tf’$pwconstitutingfromabout12to 25percentofthetotalflow. Kl!!#c&@3 wasinjecteduniformlyaboutthecir-cumferenceoftheno-e eadwzance. ,-
U’lw%’Withwateras.as ol$$?,”approxhately%6percentofthetotalpro-
pellantandcoolant~~w wasrequiredtofilm-cooltheentirenozzleandwithanhydrous~qqid snmonia,approximately19percentofthetotalflowwasrequired.~
..Themaximumspecificimpulseobtainedfromanuncooledrocket
enginewas207poun+secondsperpouredor83percentof thetheoretical .equilibriumspecificimpulse.Whentheentirenozzlewasfilm-cooledwithammonia,themaximumspecificimpulseobtainedwas162pound-secondsperpoundor only78percentofthespecificimpulseobtainedwitha correspondinguncooledengine.AlthoughtheperformmceoftheuncooledrocketenginewaElow,thisreductioninperformancewasof sufficientmagnitudetomakefilmcoolingoftheentirenoz-zleby annulartijectionof ammoniaatthenozzleentranceappesrundesirable.
INTRODUCTION
engines,inwhichhightemperaturesandaccompanyingdensitiesareencountered,oneofthemajorproblemsis
Inrockethighheat-fluxthatofprovidinga suitablecombustion&sniberandnozzle;[email protected]._t’hemethodsOf COOliWthesecomponentsoftherocketenginewhichhavereceivedthemostemphasissxetranspirationcooling(references1 to 6),regenerativecooling,andfilmcooling.
2 NACARME52C269
InternalfilmcooMngisa promisingmethodofcoolingandappearsto offersomeadvantagesoverregenerativecooling,suchas simplicity”of designandlowweightofthrustchamber.Ingeneral,ifa rocketpropellantistobe a satisfactorycoolant,itmusthavethereqtiedheat-absorbingcapacity.Forregenerativecooling,theheat-absorbingcapacityofa propellantisdeterminedby theamountofheatitcanabsorbintheliquldstate;forfilmcooling,however,theheat-absorbingcapacityincludesnotonlytheheatthatcanbe absorbedintheliquidstatebutalsothelatentheatofvaporization.Whereastheheat-transferrateto a filmcoolantishigherthanthatto a regenera-tivecoolant,thelargerheat-absorbingca~cityofa filmcoolant,ingeneral,morethancompensatesfortheincreasedheat-transferrate.HencesomepropelJszrbsnotsuitableasregenerative.coolantsmaybeusedasfilmcoolants.Fora givenapplication,h~yever,thewrits ofeachmethodof coolingsretobe consideredandin“tiomerocketengines,a combinationofbothregenerativeandfilmcoolingisused.
Investigationsrelatingtofilmcoolingunderidealizedconditionsaregiveninreferences7 to 10. A ViSUd-StudyOf:theflOWCh.=ELC-terlsticsof Iiqtidfilmsovera r-e ofgas-stresmconditionsisgiveninreference7. Thestabilityofliqtidfilni2establishedbyaslot-typeliq,,dinjectororientedat differentan@es tothewald.isreportedinreference8 forvariousgas-strewconditions.Filmcool-ofa hydrogen-oxygenflametubewithwaterisreportedinreference9anda preliminarycorrelationoffilm-coollngheat-transferresultsobtainedatairtemperaturesto 2000°F ina 4-inch-diameterductwithwaterasa coolantisgiveninreference10. Applicationof filmcoolingtorocketenginesisreported”inreferencesU.to 13. A con-siderablereductionoftheheatloadtotheregenerativecoolantby -useoffilmcoolingwithwaterinanacid-anilinerocketengineisreportedinreferenceIl..Filmcoolingtheconioustionchsmberofanmmnonia-oxygenrocketwithwater,’smmnia,andethylalcoholwas
-.
reportedinreference12. Theperformanceoftherocketwiththecom-bustionchaniberfilm-cooledwithsmnoniawasas goodastheperformanceofa similaruncooledrocketengine.Filmcoolhgthenozzleof anacid-anilinerocketby injectingwaterthroughseveralindividualtijec-torslocatedatvariousstationsalongtherocketnozzleresultedinaconsiderablereductioninthenozzlewalltemperature(reference13).
Previousinvestigationshavenotdeterminedthefeasibilityofcompletelyfilmcoolingthenozzle.Thefivestigationreportedhereti-wasconductedattheNACALewis.laboratoryinorderto determinethispossibility.A 1000-pound-thrustliqpid-smmonia13x@d-oxygenrocketemployingannularinjectionofthecoolantatthenozzleentrancewasused.Waterandliquidammoniawereusedas coolants.Thenozzlewalltemperaturewasdeterminedby skinthermocouplesspottedontheoutsidesurfaceofthenozzleatthedesiredpositions.
—---
—-
....—L
—
-.—
NACARME52C26
SYMBOLS
F
1
ThefolZowingsynibolsareusedinthisreport:
engine thrust, lbforce
specificimpulseofrocketengine, thrust(lbforce)totalL@id flowrate(lb/see)
ratioof combustion-chambervolumetonozzlethroatarea,in.
codmstion-chaiberpressure,lb/sqb. abs
fuelflow,lb/see
liquid-coolantflow,
oxidantflow,lb/see
\
lb/see
APPARATUS
Therocketengineusedforthisinvestigation(fig.1) consistedof a propellantinjectorincorporatinga gunpowdersquibigniter,anuncooledcombustionchaxiber,a coolantinjector,anda thin-wallednozzle.A gas-pressurizedpropellantandcoolantfeedsystemwasused.ThecharacteristiclengthL* oftheenginewas42 inches.
Propellantinjector.- An impinging-setpropellantinjectorasshownonfigure2 wasused. It consistedof 24pairsof jetsofone-on-oneimpingementapproximately0.375inchfromtheinjectorface.
Ignitionsystem.- Thepropellantinjectorwasdesignedto incorpo-ratea gunpowdersquibigniterat thecenteroftheinjector.Thesquibwasignitedby electricpower.
Combustionchamber.- Thecombustionchamberwasmadeofmildsteelhavinga 4-inchinsidedismeterwithwalls3./2inchthickanda lengthof6.70inches.A flangefromthecotiustiohchambermountedtherocketmotortothethruststand.
Coolantinjector.- Thecoolantinjectorwasmountedbetweenthecombustionchamberandtheexhaustnozzle.Thei?ijectorprovidedasupplyannulusforthecoolantfromwhichthecoolmtflowedthroughanannui&slotto theinsidesurfaceofthenozzle,as shownonfigure3.Theslotwas0.010inchwideandinclined30°tothecenterlineof therocketandthusdirectedthecoolamtalongth6nozzlesurface.ItWSS
.-
.
4. < ,.Midt“” 2JACARME52C26
necessarytoprovidea lipon thecoolantinjectorto coverthejointof coolantin~ectcmandnozzle,as slightmisalinementofthecoolantinjectorandnozzleencounteredduringassenjblywouldotherwiseresultinnonuniformcoolant.distribution.
Exhaustnozzle.- Theconvergent-divergentexhaustnozzle,madeofstainlesssteel,3S shownonfime 4. Thenozzlehadthefollowingdimensions:wallthickness,0.095inch;throatdiameter,1.85inches;exitdiameter,3.69inches;exit-throatarearatio,3.96;convergenthalf-angle,30°;anddivergenthalf-angle)15°. Thedesignexpansionratiowas20.4.Onthenozzlewerespotted34 chromel-alumelskinthermocouplesarrangedinfourlongitudinalrowsatthepositionsgiveninthefollowingtable:
DistancedownstreamIhmiberof Circumferentialofnozzleentrance thermocouplesspacingof
(in.) thermocouples(deg)
—0.5 1 360.9 4 901.4 4 901.9 4 90a2.35 4 902.9 4 903.3 1 3604.3 4 905.3 4 906.1 4 90
%ocationofnozzlethroat
,
.—..
—
--.
——.
. .
—
Propellantsandcoolants.- [email protected] oxygenandanhydrousliquidsmmoniawereusedaspropellants.Anhydrousliquida?mnoniaandfiltered ““ ‘
.—
waterfromthecitymainswereusedas coolants.—
Instrumentation.- me yropelht [email protected] percentby theuse ofa straingageattachedtoa counter-balancedweighingbeamwhichs~orted thepropellanttanks.Theout-putof thestraingagewasrecordedcontinuouslyas a functionoft--ona self-balancingpotentiometer.Coolantflowwasmeasuredwithanaccuracyof0.02poundpersecondby anarea-typeflowmeter.
Thethrustoftherocketenginewasmeasuredwithanaccuracyof10youndsbymeansofa straingageattachedtoa parallelogramthruststand;theoutput-ofthestraingagewasrecordedby a self-balancingpotentiometer.
—
,
.
.N-Pm.3J
NACARM E52C26.
Theoutputs
. .
of12 chromel-alumelthermocoupleswere. anaccuracyof0.125millivoltinthe10-millivoltrange
5
measuredtithby a recording
.
.
.
.
self-balancingpotentiometer.Theoutputsof 16oftheremainingther-mocoupleswererecordedbymeansofa single-channeloscillographinconjunctionwitha selectorswitchmaking10 contactsa second.Accu-racyof 0.2millivoltina 22-millivoltrangewasobtained.
Theccmibustion-chaniber5 poundspersquareinchbyrecorder.
pressurewasmeasuredwithm accuracyofmeansofa Bourdon-tubetypestrip-chart
In operatingtherocket,thesquibwasfirstignitedandthenpro-pelhntandcoolantflowswerestartedshmib%neously.If thenozzleremainedcon@etelycooled,therocketwasoperatedforapproximately15 secondssoasto obtainreliabledata.E thenozzle became over-heatedbecauseof insufficientcoolantflowor &propercoolantdis-tribution,therunwastemrlnatedwithin5 secondstopreventburnoutofthenozzle.
Reductionofperformancedata.- Allperformancedatawerecorrec-tedto a commoncombustion-chamberpressureof 250poundspersqmeinchabsoluteforpurposesof comparison.A plotof specific@ulseagainstcombustion-chsnberpressureobtainedfromreference14 showedthatthechangeintheoreticalspecificimpulsefora changeincombustion-chamberpressurefrom Pc,l to PC,2 couldbe approximatedby theeqmtion
fortherangeof
AI = 79.5
cotiustion-chsmber—encounteredinthistivestigation.
Pc 1log~PC,2
pressuresandoxidant-fuelratiosTheoxidant-fuelratiowascalcu-
latedlyneglectingthecoobt flow.~ coolantflowwasincludedinthedeterminationof thespecifichpulseandthusgavethethrustperpoundof cotiinedpropellantandcoolantflow.
Uncooledrocketperformance.- Theperformanceofanuncooledrocketengines3milartotheengineusedforthefilm-coolingrunswasdeterminedforpurposesof comparison.Thisuncooledrocketengineconsistedof thesamecombustionchambersndpropellantInjectorthatwereusedforthefilm-coolingruns.Thecoolsntin~ectorandthethin-wall.ednozzlewerereplacedwitha solid-comernozzle.Thechs2+ac-teristiclengthoftheuncooledenginewas35inchesas compredwith42 inchesforthefti-cooledengine. .
.—
6 NACARME52C26.
RESULTSANDDISCUSSION
me PerttientdataobtainedfromtherunsaretabulatedfitableI. -Theoxidant-fuelratiobyweightvariedbetween1.35and3.98.Theconibustion-chaniberpressurevsxiedbetween220and275poundspersquareinchabsoluteandthecoolantflowconstitutedfromabout12 to 25per-
#centofthetotalflow. m
CoolantResults
Nozzlewallte~erature.- Thewalltemperatureprofileof-thenozzlewhencompletelyfilm-cooledtithwaterisshownonfigure5(a).Alsoshownistheboilingpointofwatercorrespondingtothepres&revariationalongthenozzle.Thewalltemperaturerisesrapidlydown-streamofthecoolantinjectorto a value slightlybelowtheboilingpointofwaterandremainsslightlybelowtheboilingpointfortheremaininglengthofthenozzle.Thenozzlewalltemperatureprofileobtainedwithsmmoniaasa coolantisgivenonfigureS(b).Thewalltemperatureisapproximately100°F alongtheentirenozzle,whereastheboilingpointofammoniavariesfrom@ F atthenozzleentranceto -35°F attheexit.Walltemperaturesexceedingtheboilingpointofammoniawerealsoencounteredwhenammoniawasusedtofilm-cooltheconibustionchamberofa rocketengine(reference12). A possibleex@a-nationforthisphenomenonwasthata fuel-richlow-temperatureregionexistsnearthewallandthusgivesa regionhavinga lowdiffusionratewhichwouldtendtoallowsuperheatingoftheliquid.Anotherpossibleexplanationisthat,astheexhaustgasescontaina highper-centageofwatervapor,theliquidsmmmniaalongthewallcouldabsorbsomewatervaporandthuschangetowmnoniumhydroxide,whichhasahigherboilingpoint.Stillanotherpossibilityisthattheliqtidanmmniadoesnotcoverthenozzlesurfaceina continuousliqyidsheet~thatis,thefilmconsistsofa mixtureofvaporanddroplets.
Coolantflowreqtied to film-cooltheentirenozzle.- Fortherocketconfigurationusedinthisinvestigation,theminimumcoolantflowrequiredforfilmcoolingtheenttie-nozzlewithwaterwasapprox-imately16percentofthetotalflowandwithammonia,approximately19percentofthetotalflow.Forlowercoolantflows,theliqtidfilmterminatesupstreamofthenozzleexitandtheportionofthenozzlewhichisnotprotectedby a liquidfilmbecomesoverheated.
Theperformanceis shownonfigme 6oxidant-fuelratio.
PerformanceResults
obtainedforthevariouse~rimentalconditionstiwhichspecificimpulseisplottedagainstTheexperimentalspecificimpulseobtainedforthe
—.
—
—
— .—
.
.
.
——
b
—
.
NACARME52C!26 7●
Ng
N
uncooledrocketengineislow,a~proximately83percentof thetheo-reticalperformance.Thetheoreticalperformanceisforcompletecom-bustionat 250poundspersquareinchabsolutefollowedby shiftingequilibriumisentropicexpamsionto 1 atmxphereabsoluteTressure.Theexperimentalspecificimpulseobtainedwhentheentireexhaustnozzlewasfilm-cooledwasconsiderablylowerthanthatobtainedfortheuncooledengine.Theuseof ammoniaas a coolantresultedinaslightlyhigherspecificimpulsetk wasobtainedwithwaterasaCoolx!at.
Amaxhum specificiqml.seof 207pound-secondsperpoundwasobtainedfortheuncooledengine,whereasonly78percentof thisvalueor 162pound-secondsperpoundwasobtainedwhentheentireexhaustnozzlewasfti-cooledwithammonia.Althoughtheperformanceoftheuncooledrocketenginewaslow,thisreductioninperformancewasof sufficientmagnitudetomakefilmcoo13ngoftheentirenozzlebyannularinJectionof.snmmniaat thenozzleentranceappearundesirable.
COITCLUDIKG~
Inasmuchasfi3mcoolingof theenttieexhaustnozzleby injec-tionof thecoolantat thenozzle entranceresultsinan intolerablelossinperformance,othercoolingaidsormethodsforthenozzle,
. suchasregenerativecoolingor ceramicliningsor coatings,maybesought. Also,thereisa possibilityoffilmcoolinga portionoftheconvergentsectionofthenozzlewitha reactivecoolantwithout
-’ adverselyaffecthgtheperfornm.nceoftherocket.Eromconsiderationoftheresidencetimeof a particleintheexhaustnnzzle(fig.7),itisevidentthstifa giv,entimeisrequiredforthevaporizedcooLurt-to diffuseandburn,thenonlythatwhichvaporizesupstreamofa givenstationalongthenozzlewilJeffectivelyburninthenozzleandenhancetheperformanceoftherocket.Further,heatthatisreleasedatlowpressureinthenozzle doesnothaveasgreatanexpansionratioandcan-notcontributeasmuchtoperformanceaswouldbe possibleif itwerereleasedintheconibustionchsmber.Thefactthattheperformanceobtainedwhen a reactivecoolantwasused,however,exceededthatobtainedfromem inertcoolant(fig.6) tidicatesthatperformancegainwasobtainedfromsomeofthereactivecoolant.
SUMMARYW RESULTS
*
.
Internalfilmcoolingofthenozzleof a 1000-pound-thrustliquid-smmnialiquid-o~genrocketenginewitha 42-@h characteristiclengbhwasinvestigatedwithconibustion-chsniberpressuresfrom220to275pounds~ersquareinchabsoluteovera rangeof oxidant-fuel
8
ratiosfrom1.35~o3.98.coolantswiththecoolantcentofthetotalflow.
-NACARM E52C26.-.-=.-:.-‘--*#: -=,.
Waterandliqpidazmnoniawereusedasflowconstitutingfromabout12to 25per- .—
Theresultsoftheinvestigationcanbe sumnsrizedasfollows:k
1.Theentirenozzleoftherocketenginewasfilm-cooledwith*n.
waterandtithliquidanunoniaby uniformannularinjectionof theN
coolantatthenozzleentrance.Whenwaterwasusedasa coolant,16percentofthetotalflowwasrequiredto cooltheentirenozzle.Withliquidanmmniaasa coolant,19percentofthetotalflowwasrequiredto,cooltheentirenozzle.
2.Themaximumspecificimpulseobtainedwhentheentirenozzlewasfilm-cooledwithliquidammoniawas162pound-secondsperpoundor 78percentofthema.xlmumspecificimpulseobtainedfroma correspon-dinguncooledengine.Thisreductioninperformanceisof sufficient .magnitudetomakefilmcoolingoftheentirenozzleby annularinjec-
—
tionofamnoniaatthenozzleentranceappesrundesirable.
LewisFlightPropulsionLaboratoryNationalAdvisoryCommitteeforAeronautics
Cleveland,Ohio.
REFERENCES
1.Duwez,Pol,andWheeler,H.L.: PreliminaryExpertientsonthe.
Sweat-CoolingMethod.Prog.Rep.No.3-13,PowerPlantLab.pro~.No.MX527.JetPrag.Lab.,C.I.T.,JiIly18,1946. (ATSCContractNo.W-33-0380-ac-4320.)
2.Duwez,Pol,andWheeler,E.L.,Jr.: An ExperimentalStudyofSweatCoolingwithNitrogenandHydrogen.Prog.Rep.No.4-47,—.
PowerPlantLab.Prod.No.MX801,JetProp.Lab.,C.I.T.,Sept.24,1947. (AMCContractNo.W-535-ac-20260,OrdnanceDept.ContractNO.W-04-2004RD-455.)
3.Duwez,Pol,andw’heeler,H. L.,Jr.: HeatTransferMeasurementsina NitrogenSweat-CooledPorousTube.Prog.Rep.No.4-48,PowerPlantLab.Proj.No.MX301,JetProp.Lab.,C.I.T.,Nov.6, 1947.(AM!ContractNo.W-535-ac-20260,OrdnanceDept.ContractNo.W-04-200-CRD-455.)
4.Rannie,W. D.: A SimplifiedTheoryofPorousWallCooling.Prog.Rep.No.4-50,PowerPlantLab.Proj.To.MX801,JetProp.Lab.,C.I.T.,NOV.24,1947. (AMCContractNo.W-535-ac-20260,OrdnanceDept.ContractNo.W-04-2004RD-455.)
a
.
2T NACARM E52C26●
5..
xlPnQ
6.
.
.
7.
8.
9.
10.
Il.
12.
13.
14.
1
oanright,RichardB.:pirationCoolingof
9
~eliminaryExperimentsof GaseousTrans-RocketMotors.Prog.Rep.No.1-75,Power
PIantLab.Proj.No.MX.801,JetProp.Lab., C.I.’T., Nov. 24,M48.(AMCContractNo.W-535-ac-20260,OrdnanceDept.ContractNo.W-04-200-ORD-455.)
Jheeler,H. L.,Jr.: TheInfluenceofWallWterialontheSweat-CoolingProcess.Prog.Rep.No.4-90,JetMay3,1949. (OrdinanceDept.ContractNo.
Kinney,GeorgeR.,andAbramson,AndrewE.:larLiquidFlowwithCocurrentAirFlowinNACARME51C13,1951.
prO~. Lab., C.I.’I’., .W-04-200-QRD-455.)
InvestigationofAnnu-HorizontalTubes.
Zucrow,M. J.,Beighley,C. M.,andKhuth,E.: ProgressReportontheStabilAtyofLiqtidFi3nsforCoolingRocketMotors.Tech.Rep.No.23,PurdueUniv.,Nov.~, 1950. (ContractN6-ORI-1O4,TaskOrderI,NR 220-042,Phase7,Pro3ectSquid.)
Schurman,GlennA.: An InvestigationofFilmCoolingina Flameltibe.Prog.Rep.No.1-74,PowerPlantM. Proj.No.MX801,JetProp.Lab.,C.I.T.,June30,1948. (MC ContractNo.W-535-ac-20260,OrdnanceDept.ContractNo.w-04-2oo-om-455*)
Kimney,GeorgeR.,andSloop,JohnL.: InternalFiJmCoO1-ingExperimentsina 4-InchDuctwithGasTemperaturesto 2000°F.NACARME50F19,1950.
Boden,RobertH.: HeatTransferinRocketMtors andtheApplica-tionofFiImandSweatCooling.A.S.M.E.Trans.,vol.73,no.4,May1951,pp.385-390.
Morrel.1,Gerald:Investigationof ~ternalFilmCmlingof1000-Pound-ThrustLiqyid-lmmmnia- Liquid-OxygenRocket-EngineCcmibus-tionChamber.NAC!ARME5U304,1951.
Sloop,J.L.,andHnney,GeorgeR.: hternal-Fi3mCoolingofRocketNozzles.NACARME8A29a,1948.
Winternitz,P.F.: SumaryReportonTheoretical,LaboratoryandExperimentalInvestigationsofHighEnergyPropellants.Ammonia,vol.II,Rep.No.RMI-293-S7,ReactionMotors,Inc.,Oct.30,1950. (Bur.Aero.,NavyContractNOa(s)9469.)
.
Run
—
OxiaentfllmW.
(lb/see)
I
TAmEI— PlRFOFu4AwmIM!I!AFRCM RWKET-lWZ2LE FIIX-CO- EXJ?ERIMENI’S
Fuel flow coolantmlnletConibu6tlcm-clmrberkLdmlt.-Wf
Cocib?ntflowflmn pressure fuel ratio loowJ( Wo+wf+wz)
(lb/see) ‘1(;) P= neglecting (percent)
(Ib/see) (lb/sqfi. abs)coolantwJwf
ICcd.mlt, Wati
J-L1 2.58 1.872 2.60 1.923 2.65 1.554 2.51 1.675 3.00 1.716 2.90 1.89
78910U.12I-3141516171819
2.532.913.102.952.822.732.902.983.J23.533.262.813.00
8pecific
-Beincludingcoolant
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L 701.511.341.40L 511.401.291.181.06.89.93
L 931.76
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1.341.351.291.X5.70
1.251.1.11.071.101.IJ.1.171.02.8s
1.041.431.281.17.91
%rrect-edto a cmimatian-chmilx
826829810816894905
233232232230245250
L 381.331.841.501.751.53
Coolmt, anhydroueliquid enuncmia
’968875890858851855780707792736763986100L
240m.250245240248225230225220220272275
1.491.93”2.322.101.861.952.252.532.953.983.531.451.71
presmm d 250 Ib/aqin. abs.
----22.823.623.619.312.7
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lti144152155165
2Z. K..,20.0 ‘19.420.220.422.118.616.920.024.423.419.816.0
l-w160 ‘161159157161154160156m144164174
.
2462 . .
9“
Fi@re 1. - Rocket engine used for investigation of nozzle film cmlhg.
F’J
.,IJ 1
Fmlre 2. - Propellant InJector.
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..r
.,
EHUI
%’Nm
, ●
1“
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CD-2654
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b
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1-FiKW 3, - Cmpcment wrte of cdant in,jectmr.
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Hgum 4. - ThJJ-1-walleaSWlnl.cas-st.eelex.hmmt mz Zle.
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. .,.,1 Z9PZ ,,
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NAC!ARME52C26 .. . :.
r
/
\
Rocketnazzlecontour\ / ‘
Nozzleexit
HOzzlethroat
400 \ .\
\ -I?orznalboiung pointof
/ waterat existing pressure\
300 I-1 \8 0 \
.
$$
.--
* 203sA.-l Gi!
a
100
y%y
o 1 2 3 4 5 6
Figure5. - TypicalnozzleSymbolsreferto
Distancealongnozzle,in.
(a)Coolant,water.
walltemperature profile fcm entirenozzlefLlm-cooled.clifferent longitudinal rows of thermocouples.
,
7
.
. .
. .
0 1 2 3 4 5
Distance almg nc.mlo, In.
(b) Coolant, Uquid ammnia.
Et—
—
—
—
7
1 1
6
Figure 5. - ccmdudad. Tgpical nmda mu tqparature mile fm mttie noazls film-
cooled. 2@01E rafm to difr~ent lmgitudinel row of thamocovplm.
1’
I I
, .,,!
1’ ,,, ii: 29P-Z
i
.
i?
E!
.
, , t ● s
zII Uncooled rocket
o Nozzle film-cooled with mmoniaA Nozzle film-cooledwith water
– – -83 percent of theoretical —specific @mil.ae
Canbuation-chambercmidant-fuelratio, Wok
Figure 6. - COIIQZriBOll Of ptX’fOJ31WlCe of uncooled rocket engine with parfornmnce obtained when
dxmat nozzle waa film-cooled with water m liauld annnmia. E@eclflc Inumlae valuee ace
corrected to ccenbuation-chamberpressore of 250-pJUndBper squ&e inch ab;olutewith expansionto 1 atmosphere. Coolmt flow variea frau 16.9 to 24.4 percent of total flow.
-.
/
2.
—.
.6 I I
Rocket
<
mm’
.5 \ / <
Co?lta.lr IHozzleexit
Eozzleentrance
~ ‘4
\
j.,‘P
:: \
;Ix .2
.1
-~ ~
o-z -1 0 1 2 3 4 5 6 7
Dlstencealmg rocketrotor,in.
Figme 7..-Rirticl.ereddmce timefromnomle exitvith asmqtion of unifcnmone-dlmensimMIfum. (bal)wtion.chemberpreemre, 254)poudx per BquareM absolute;totaltau@rature,45600F.