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TheEnhancementofConvec/veHeatTransferinanAluminumOxideNanoaerosol
EmpiricalStudyMaulinTrivediDec9,2015
MechanicalandManufacturingEngineering
Applica/ons
§ Deep-cooledcombinedturbojetcycle— ThrustoverwiderangeofMach
number— Intakeairhasveryhigh
temperature— Energyextractedisaddedback
tofuelstream§ Heattransferapplica/onsuse
fluidsorairasheatcarriers.— Thermalconstraints— Physicalconstraints— Cost
2
Figure1:DASSGN1EngineConceptFrom:h(ps://en.wikipedia.org/wiki/Space_Engine_Systems
Applica/ons
§ Heattransferapplica/onsusefluidsorairasheatcarriers.— Thermalconstraints— Physicalconstraints— Cost
§ Reac/onEnginesLtd.— Highsurfacearea
§ SpaceEngineSystems— Enhancedthermalproper/es
Figure2:SABREPre-coolerFrom:h(p://www.reac;onengines.co.uk/heatex_work.html
3
Background
§ Solidpar/clesinsuspensionincreasesthermalconduc/vity(Maxwell,1881).— Massorvolumefrac/onofpar/cles— Surfaceareatovolumera/o
§ Nanopar/cles— Sizes1-100nm— Veryhighsurfaceareatovolumera/o
§ Nanofluids:Nanopar/clessuspendedinliquidphasecarriers(Choi,1995).
§ Nanoaerosols:Nanopar/clessuspendedingaseousphasecarriers.
4
Background:Nanofluids
§ 40%heattransferenhancement(Herisetal.,2006).
§ 39%increaseinheattransfer(Xuanetal.,2003).
§ Dependencyonmassfrac/onandReynoldsnumber
Figure3:NusseltnumbervsPecletnumberFrom:Heris,S.Z.,Etemad,S.G.,&Esfahany,M.N.(2006).Experimentalinves/ga/onofoxidenanofluidslaminarflowconvec/veheattransfer.Interna;onalCommunica;onsinHeatandMassTransfer,33(4),529-535. 5
Background:Nanoaerosol
Figure4:Nusseltnumbervsmassloading Figure5:Nusseltnumbervspar/clesizeAdaptedfrom:Murray,D.B.(1994).Localenhancementofheattransferinapar/culatecrossflow—IIExperimentaldataandpredictedtrends.Interna;onaljournalofmul;phaseflow,20(3),505-513.
6
Background:Mechanisms
§ Increasedthermalcapacity
§ Conduc/onbetweenimpac/ngpar/cles
§ Thermalenergytransportbyreboundingpar/cles
§ Flowstructureeffects
§ Othereffects(Williams,2015)
§ Limi/ngmechanisms
7
Mo/va/on
§ Nanopar/clesvs.Micro-par/cles§ Availabilityinaerospaceindustryasanalterna/vefuel
— Largeenergycontentperunitvolumeandmass— Lowerigni/ontemperaturesandhigherburningrate— Safeandefficientstorage
§ Nanofluidsareproveneffec/veinheattransferapplica/ons§ Volumetricheatcapacityofnanoaerosolismuchhighercompared
tonanofluids— ρCpra/oismuchhigherfornanoaerosolthanfornanofluids
8
Objec/ves
§ Firstexperimentalinves/ga/on§ Lowpar/cleconcentra/on
— Massfrac/onfornanofluids,O(10-1)— Massfrac/onfornanoaerosols,O(10-4)
§ Theore/calmodeltopredictenhancement§ Par/clesizevs.heattransferenhancement
9
ExperimentalSet-up
12Figure7:ExperimentalSet-up
PressureRegulator
CompressedAir
PressureGauge
FlowMeter
Par/cleInjector
UpstreamThermistor
HotWire
DownstreamThermistor
Par/cleCollec/onTank
Air-onlyTests
§ Validateexperimentalapparatus§ PerformedoverflowReynoldsnumberrangeof1420-11,200§ Nusseltnumbercalculatedbyequa/ngconvec/veheat
transferratetothechangeinenthalpy§ Experimentalresults(withoutpar/cles)werecomparedto
Zukauskasempiricalrela/onof§ Establishbaseline
13
Air-onlyTests:Cont.
14
0
2
4
6
8
10
12
14
16
18
20
0 2000 4000 6000 8000 10000 12000
NusseltNum
ber
ReynoldsNumber[tubediameter],Re
ZukauskasRela/onExperimentalAirTests
Figure8:Valida/onofexperimentalset-up
AirTests:Cont.
15
0
2
4
6
8
10
12
14
16
18
20
0 2000 4000 6000 8000 10000 12000
NusseltNum
ber
ReynoldsNumber[wirediameter],Re
ZukauskasRela/onExperimentalAirTests
Figure8:Valida/onofexperimentalset-up
FlowCondi/onsForPar/cleTests
Nanopar/cle:Informa/on
§ Approximatelysphericalwith112nmavg.dia.
§ Agglomeratesofavg.870nm.
§ Dispersedthroughcustom-builtinjec/onsystem.
16
Figure9:SEMimageofAl2O3par/cles
Nanopar/cle:Injec/onSystem
§ Gravityassistedthroughorificeof0.75mm
§ Oscilla/onsprovidedtopreventclogging
§ 510mmoftubingallowssemlingofbiggerpar/cles
17
Figure10:Par/cleInjec/onSystem
Par/cleHousing
Off-balanceMotor
Air-flowpipe
UpstreamThermistor
Par/cleTests
§ Experimentswithpar/cleswereperformedatflowReynoldsnumbers:6000,7500and8900.
§ Par/cleflowratemeasuredanereachtestusinghighlysensi/vemassbalance.
§ Par/clemassloadingrangedfrom0.01%-0.33%.§ NusseltnumberateachReynoldsnumbercalculatedusing
samemethodologyasairtests.— Effec/veproper/es
18
ExperimentalResults:Cont.
19
Figure11:EffectofmassloadingonNuatRe=6000
y=9.5795x0.5809R²=0.70653
0%
5%
10%
15%
20%
25%
30%
35%
40%
45%
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
%NuIncrease
%Par/cleMassLoading
Raw%NuIncrease Predicted%NuIncrease 95%LowerCI 95%UpperCI
ExperimentalResults:Cont.
20
Figure12:EffectofmassloadingonNuatRe=7500
y=5.3126x0.5338R²=0.61755
0%
5%
10%
15%
20%
25%
30%
35%
40%
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
%NuIncrease
%Par/cleMassLoading
Raw%NuIncrease Predicted%NuIncrease 95%LowerCI 95%UpperCI
ExperimentalResults:Cont.
21Figure13:EffectofmassloadingonNuatRe=8900
y=0.9927x0.2821R²=0.46192
0%
5%
10%
15%
20%
25%
30%
35%
40%
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
%NuIncrease
%Par/cleMassLoading
Raw%NuIncrease Predicted%NuIncrease 95%LowerCI 95%UpperCI
ErrorAnalysis
§ Systema/cerrorscalculatedbasedoninstrumenta/onandsensorlimita/ons.
§ Randomerrorscalculatedbasedont-distribu/onforα=0.05.
§ Randomerrorissignificantlyhigherthansystema/cerrors.
§ Student’st-testbetweenbaselinetestandpar/cletestatlowestpar/cleconcentra/onshowssignificantincreaseinNusseltnumber.
22
9
10
11
12
13
14
15
16
17
550 600 650 700 750 800 850 900 950
NusseltNum
ber
Cross-flowReynoldsNumber
AirTest Par/cleTest
Figure 14: Student's t-test for 95% confidencebetweenair-onlyandlowestpar/cleloadingtests
Model:Con/nuum
§ Con/nuumregime,Kn<0.01— Murray’smodelforincreasedthermalcapacity— (𝑁𝑢↓𝑁𝐴 /𝑁𝑢↓𝑎 )↓𝐼𝑇𝐶 = [1+ 𝜂↓𝑡 𝑆↓𝐿 𝑐↓𝑝 ↓𝑟𝑎𝑡𝑖𝑜 ]↑0.37
§ 𝜂↓𝑡 = 𝜏↓𝑟𝑒𝑠 /𝜏↓𝑟𝑒𝑙 ;𝜏↓𝑟𝑒𝑙 = 𝑑↓𝑝 𝜌↓𝑝 𝑐↓𝑝 ↓𝑝 /6ℎ↓𝑝 § Othereffectsareconsiderednegligibleduetolowpar/cle
loading— Flowstructuremodifica/on— Par/clerebound— Radia/on
23
Model:Free-molecular
§ Free-molecularregime,Kn>10— ModifiedMurray’smodelusingthefree-molecularrelaxa/on/me,τrel
— ObtainedfromFilippovandRosner’senergybalance§ 𝜌↓𝑝 𝐶↓𝑝↓𝑝 𝑉↓𝑝 𝑑𝑇↓𝑝 /𝑑𝑡 =𝛼𝜋𝑎↑2 𝑛↓𝑔 𝑐 𝑘↓𝑏 (1/2 (𝑇↓𝑝 − 𝑇↓𝑔 )(𝛾+1/𝛾−1 ))
§ 𝜏↓𝑟𝑒𝑙 = 2𝜌↓𝑝 𝑐↓𝑝 𝑑↓𝑝 /9𝑛↓𝑔 𝑐 𝑘↓𝑏 ; 𝑛↓𝑔 = 𝑃𝑁↓𝑎𝑣 /𝑅𝑇 ; 𝑐 =√8𝑘↓𝑏 𝑇↓𝑔 /𝜋𝑚↓𝑔
— Subs/tuteτrelintoMurray’smodeltoobtainNusseltnumberenhancement
24
Model:Transi/on
§ Transi/onregime,0.01<Kn<10— HarmonicmeansuggestedbySherman(1963)wasusedtointerpolate𝑞↓𝑡𝑟 .
— 𝜏↓𝑟𝑒𝑙,𝑡𝑟 = 𝜌↓𝑝 𝑐↓𝑝 𝑑↓𝑝 ↑2 /𝑞↓𝑡𝑟 /𝑞↓𝑐 12𝑘↓𝑓 ; 𝑞↓𝑡𝑟 /𝑞↓𝑐 = 1/1+ 19/6 𝐾𝑛
— Thera/o 𝑞↓𝑡𝑟 /𝑞↓𝑐 canbeobtainedfromLiu(2006).— Knudsennumbereffectsareincorporatedintothe/mescale
25
Model:Comparison
26
1.00
1.10
1.20
1.30
1.40
1.50
1.60
1.70
1.80
1.90
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
NuRa
/o[N
u_su/N
u_a]
SolidMassFrac/on,%[m_solid/m_air*100]ExperimentalFit ExperimentalData Transi/onalModel
MurrayModel FreeMolecularModel 95%ConfidenceBand
Figure15:Comparisonofcon;nuummodel,free-molecularmodel,transi;onalmodelandexperimentaldataforRe=6000
27
1.00
1.10
1.20
1.30
1.40
1.50
1.60
1.70
1.80
1.90
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
NuRa
/o[N
u_su/N
u_a]
SolidMassFrac/on,%[m_solid/m_air*100]ExperimentalFit ExperimentalData Transi/onalModel
MurrayModel FreeMolecular 95%ConfindenceBand
Figure16:Comparisonofcon;nuummodel,free-molecularmodel,transi;onalmodelandexperimentaldataforRe=7500
Model:Comparison
28
1.00
1.10
1.20
1.30
1.40
1.50
1.60
1.70
1.80
1.90
0.00% 0.05% 0.10% 0.15% 0.20% 0.25% 0.30% 0.35%
NuRa
/o[N
u_su/N
u_a]
SolidMassFrac/on,%[m_solid/m_air*100]ExperimentalFit ExperimentalData Transi/onalModel
MurrayModel FreeMolecularModel 95%ExperimentalBand
Figure17:Comparisonofcon;nuummodel,free-molecularmodel,transi;onalmodelandexperimentaldataforRe=9000
Model:Comparison
Model:EffectofPar/cleSize
29
1.00
2.00
3.00
4.00
5.00
6.00
7.00
8.00
9.00
10.00
0 10 20 30 40 50 60 70 80 90 100
NusseltNum
berR
a/o
Par/cleDiameter,[nm]
SolidLoading0.25% SolidLoading0.5% SolidLoading0.75% SolidLoading1%
Figure18:Effectofpar/clesizeonNusseltnumberra/oatRe=9000usingtransi/onalmodel
Discussion:Experimental
§ Onlysmallpar/clemassloadingisrequiredtoprovidealargeincreasetoNusseltnumber.
§ Murray(1994)required~100%massloadingtoachievesimilarresults.
§ Higherenhancementamributedto:— Smallerpar/cles— LowerReynoldsnumber
30
From:Murray,D.B.(1994).Localenhancementofheattransferinapar/culatecrossflow—IIExperimentaldataandpredictedtrends.Interna;onaljournalofmul;phaseflow,20(3),505-513.
Discussion:Experimental
§ Onlysmallpar/clemassloadingisrequiredtoprovidealargeincreasetoNusseltnumber.
§ Murray(1994)required~100%massloadingtoachievesimilarresults.
§ Higherenhancementamributedto:— Smallerpar/cles— LowerReynoldsnumber
31
From:Murray,D.B.(1994).Localenhancementofheattransferinapar/culatecrossflow—IIExperimentaldataandpredictedtrends.Interna;onaljournalofmul;phaseflow,20(3),505-513.
Discussion:Model
§ EffectsofincreasedReynoldsnumberandturbulencemodifica/onareinsignificant.
§ Therelaxa/on/merepresents63%ofheattransfer,thusresul/nginhigherpredic/onofheattransferenhancement.
§ Experimentaldatabetweencon/nuumandfree-molecularpredic/on.
§ Transi/onalmodelagreeswithexperimentaldata.— For0.01<Kn<10
§ Manyothereffectsarenotincluded.
32
Conclusion
§ Heattransferenhancementusingnanoaerosolhasbeenexperimentallydemonstratedforthefirst/me.
§ Largeheattransferenhancement(~36%)wasobservedatrela/velylowpar/cleloading(~0.35%).
§ Experimentaldataisprovedtobesta/s/callysignificant.§ ObservedtrendsareconsistentwiththeoryproposedbyMurray.§ Murray’smodelismodifiedforfree-molecularandtransi/onregime.
— Transi/onmodelagreeswithexperimentaldata.— Transi/onmodelextendedtopredicteffectofpar/clesizeovermassloading
0.25%-1%.— Othereffectsneedtobeincorporated.
33
Acknowledgements
§ AlbertaInnovatesTechnologyFutures§ NaturalSciencesandEngineeringResearchCouncil§ SpaceEngineSystems§ UniversityofCalgary§ Dr.CraigJohansen
34
References
1. Maxwell,J.C.(1881).Atrea;seonelectricityandmagne;sm(Vol.1).Clarendonpress.2. Choi,S.U.S.(1995).Enhancingthermalconduc/vityoffluidswithnanopar/cles.ASME-
Publica;ons-Fed,231,99-106.3. ZeinaliHeris,S.,Etemad,S.G.,&NasrEsfahany,M.(2006).Experimentalinves/ga/on
ofoxidenanofluidslaminarflowconvec/veheattransfer.Interna;onalCommunica;onsinHeatandMassTransfer,33(4),529-535.
4. Xuan,Y.,&Li,Q.(2003).Inves/ga/ononconvec/veheattransferandflowfeaturesofnanofluids.JournalofHeattransfer,125(1),151-155
5. Murray,D.B.(1994).Localenhancementofheattransferinapar/culatecrossflow—IHeattransfermechanisms.Interna;onaljournalofmul;phaseflow,20(3),493-504.
6. Murray,D.B.(1994).Localenhancementofheattransferinapar/culatecrossflow—IIExperimentaldataandpredictedtrends.Interna;onaljournalofmul;phaseflow,20(3),505-513.
7. Bianco,V.,Manca,O.,Nardini,S.,andVafai,K.,HeatTransferEnhancementWithNanouids,April12015,CRCPress
35