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7DesignandAnalysis
ofHeterogeneousCatalyticReactors
Thereactorsdiscussedinthischapter:
packedbedcatalyticreactor
fluidizedbedreactor
Objectives:desiredconversion
reactionvolume(amountofcatalyst)7.1TransportPhenomenainaPackedBed7.1.1Flowoffluidinafixedbed
walleffect
transitionfromlaminartoturbulentflow
pressuredropThepressuredropthroughapackedbedis
(fromPrinciplesofChemicalEngineering)whereu0isthesuperficialvelocity,andaisthespecific(external)surfacearea.Withtheequivalentdiameterds=6/a,(7.1)Re<10,laminarflow;Re>1000,fullydevelopedturbulence.(7.1)(7.2)andwherefisthefrictionalcoefficient,Exercise:Chap.7:37.1.2AxialmassandheattransferItistheratioofconvectiontodiffusion,whereDaistheaxialdiffusioncoefficient
includingmoleculardiffusion,vortexdiffusionandsoon.=ReSc
Definethe
Pecletnumberforaxialmasstransferas
DefinePecletnumberforaxialheattransferasItistheratioofconvectiontothermaldiffusion,whereeaistheaxialeffectiveconductioncoefficientincludingconduction,convectionandradiation.=RePrPecletnumberWhenPe>>1,thebackmixingcanbeneglectedwithrespecttotheconvection,i.e.PFR.Chap.5:
rateofconvection
rateofdispersionTheparticleReynoldsnumberis
ExperimentsshowthatwhenRep>10,(Pea)m=2forgas,(Pea)m=0.31forliquid.NotetherelationPe=(Pea)m
L/dp
andL/dp>>50formostoffixedbedreactors.Pe>>100PFRNon-isothermalcondition:
homogeneousreactors:
(Pea)m
(Pea)h
fixedbedreactors:
heattransfer:influidandsolidphasesmasstransfer:influidphaseonly(Pea)h
(Pea)m/3ForL/dp>150
PFR7.1.3RadialmassandheattransferThemassandheattransferinradialdirectionalwaysexists.heatcarrier7.2MathematicalModel
forFixedBedReactorspseudo-homogeneousmodel
theeffectsofmassandheattransferarenegligible.heterogeneousmodelsimultaneousmomentum,heatandmasstransfer.Heterogeneousmodel:Simplifications:largeL/dp(negligiblebackmixing)largeG(negligibleresistanceforheatandmasstransferinboundarylayers)averageT
andcincrosssection
PFR
(forfluidoutsideparticlesandparticles)+
(effectofinternaldiffusion)or0Massbalance:Energybalance:(7.9)(perunitvolume)Forcoolingorheatingmedium:(perunitmasscatalyst)(7.13)(7.10)Momentumbalance:
Theeffectofpressuredifferenceonreactionsmaybeneglectedexceptunderhighpressureandlargepressuredifference.(7.11)Boundaryconditions:
atZ=0,XA=0,
T=T0,Tc=Tc0,
p=p0
(7.12)Calculations:
XAL(heightofthefixedbed)
XA,Loperationcondition
IfL/dpisnotsolargethattheeffectofbackmixingshouldbeconsidered.Forisothermalsinglereactionswithconstant-volume,thedispersionmodelis(7.18)Boundarycondition:(closed-closed)(7.20c)atZ=L,(7.20a)atZ=0,Dataforreactordesign:(1)dataonreactionkinetics
orderofreaction,rateconstant,…(2)dataonthermodynamics
heatofreaction,heatcapacity,equilibriumconstant,…(3)dataontransportphenomena
viscosity,diffusivity,conductivity,…
poresizedistribution,p,b,specificsurfacearea,…7.3AdiabaticFixedBedReactors7.3.1TypesofadiabaticfixedbedreactorssinglepackedbedreactorstagedpackedbedreactorsRadialheattransfer?No!gasincoolant
withintercooling
withcoldshotcoolingfeedoroneofreactants7.3.2Calculation
foradiabaticfixedbedreactorsForasingleadiabaticfixedbedreactor,thecalculationissimilartothatinChap.4.Fromtheenergybalance,wehave
T
T0=XA(7.23)whereFromthemassbalance,weobtain
thelength(orheight)ofthereactor(7.24)
or
thevolumeofcatalyst(7.25)7.3.3StagedadiabaticfixedbedreactorsHereweonlyconsiderthosewithintercooling.gasinheatcarriercA1,T1cA1,T20cA0,T0cA2,T2anadiabaticfixedbedreactorheatexchangerFigure7-4.Reversibleexothermicreaction:equilibriumoptimumtemp.XATABCDEFgasinheatingcA1,
T1cA1,T20cA0,T0cA2,T2cA2,T30cA3,T3ABDCFEGoperatinglineOptimization:
minimumcostforproduct
maximumthroughput
minimumamountofcatalyst:Forcertainnumberofstages,rateandcompositionoffeed,andfinalconversion,thevariablesforoptimizationareXAiandTi0,total2N1variables.Exercises:Chap.7:6,157.4PackedBedReactors
withHeatExchangedp<D/8toavoidchanneling,butiftheparticleistoosmall,thepressuredifferenceincreases.heatcarrierfeed
product
Shellandtubereactor:Comparisonwithadiabaticpackedbedreactors:
moreuniformtemperaturedistribution
lessbackmixing
easiertoscale-upRelationoftemperatureandconversion:adiabatic:theslopeofoperatinglineisconstant;withheatexchange:theslopechanges.
FromEqs.(7-9)and(7-10),(7.32)rateofheattransferrateofheatreleaseFigure7.6:reversibleexothermicreactionadiabatic(AK)XATequilibriumoptimumtemp.AK(7.32)rateofheatreleaserateofheattransferbetter
withheatexchange:
hotspot
mayexist.Theposition:dT/dz
=0.Figure4C:reversibleendothermicreaction
adiabatic
XATZ
withheatexchange:
coldpoint
mayexistFigure7.7:axialtemperaturedistributionTemperaturerunaway:thetemperatureatthehotspotincreasesrapidlyasthefeedtemperatureincreases.TZ7.5PackedBedReactorswithSelf-heating
Thereactionisexothermicandthefeedisheatedbytheheatofreaction.
countercurrent
cocurrent
T0LT0LThepackedbedreactorswithself-heatingisaspecialcaseofthosewithheatexchange.Bothmaybeoperatedcountercurrentlyor
cocurrently,andhavethephenomenaofhotspot,temperaturerunaway,….
7.6EffectsofParameters
Weusuallyconcernwiththeeffectsofparametersonthetemperatureathotspot,temperatureT0andconcentrationwA0
ofthefeedtemperatureofcoolantTc
operatingpressurePrateofheattransferU/d…Itneedsextensivelycomputation.Exercises:Chap.7:12,17
7.7FluidizedBedReactorsMainparts:shellgasdistributorheatexchangedeviceinternalsgas-solidseparatorparticlechargeanddischargedevice
lgulgpumffixedbedMNfluidizedbedApplications:
gas-solidliquid-solidgas-liquid-solidComparisonoffixedandfluidizedbedreactors:(1)backmixing(2)particlesizeandfluidvelocity(3)lossofcatalystandreplacement(4)controloftemperature(5)design7.8CatalyticReactorsinLaboratoryexperimentalmethodsforfindingreactionrateasafunctionoftemperature,pressure,composition,…7.8.1Basicrequirements
Todeterminetheintrinsickinetics,effectsofheatandmasstransfershouldbeeliminated.
Thegradientsofconc.andtemp.resultinginmassandheattransfer:
insideandoutsideparticle
radialandaxialdirectionofreactorIftheeightgradientsareeliminated,thereactorisamixedflowreactor
(reactorwithoutgradients).Atleast,theflowisaplugflow.Basicrequirements:
isothermalandidealflow.7.8.2Typesofexperimentaldevices(1)Integral(plugflow)reactorwithsmalldiameter,e.g.,D
1cm(PFR),mergedinanisothermalb
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