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时间:2019-03-14
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1、IVHighViscosityFlashingTwo-PhaseFlowAlbertR.MullerChairman,DIERSHighViscosityVentFlowProjectsCommitteeHarryS.ForrestChairman,DIERSPhaseHILarge-ScaleIntegralTestCommitteeHaroldG.FisherChairman,DIERSTechnicalCommitteeI.INTRODUCTION1-1.GeneralDiscussionofHighViscosityFlowinReliefSystems
2、ChapterII,"PressureReliefSystemFlow,"coversmostaspectsofflashingtwo-phaseflowinwhichbothliquidandvaporand/orgasarepresentatthesametimeinareliefsystem.Mostofthesimplifiedmodelsdevelopedforthedesignofemergencyreliefsystemsarespecificforturbulentflowwherethefrictionlossisasmallfractiono
3、fthetotalpressuredrop.Simplifiedmodelsbasedonlaminarflowhavealsobeendeveloped(seeAppendixIV-A).Experimentswithviscousfluids(e.g.,rubbercementat20%solidsandpolystyrene-ethylbenzenesolutionsat60%polymer)illustratedtheeffectofhighviscosityinincreasingthefrictionlossinareliefline.Inturbu
4、lentflashingflowsystems,arelieflineof1000pipediametersinlengthisrequiredtoreducetheflowto50%ofthatinafrictionlessnozzleofthesamediameter.However,inlaminarflashingflowwithaliquidphaseviscosityofover100centipoise,thefrictionallossofasmalldiameterrelieflinewitha200LIDreducedtheflowtoabo
5、utonetenththatofafrictionlessnozzle.ForagivenviscosityandrelieflineLID,thefrictionlossincreasesasthepipediameterdecreases.Ifthepipediameterissmallenough,theflowratemaybeseveralordersofmagnitudelessthanthatforfrictionlessnozzleflow.Afewexperimentsindicatedthattheeffectofliquidviscosit
6、yonfrictionlosscouldbeminimizedforpipingconfigurationswithanareaflowreductionlessthan7pipediametersfromthevesselfollowedbyalargerdiametertailpipe.Thisresultappearstobeduetoachangefromaliquidtoavaporcontinuousflowregime.However,theparametersthatcontroltherelieflineflowregimearenotfull
7、yunderstoodandtherecommendedmethodtodesignreliefsystemsforviscousflowisdirectscalingusingthemethodsdescribedinthissection.1-2.WhyHighViscositySystemsRequireSpecialConsiderationMostoftheexperimentalworkearlyintheDIERSprojectwaswithlow-viscositysystems(i.e.,systemsthathadviscositiesles
8、sthan50centi
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