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{{#Wiki_filter:i(TELEDYNEENGINEERINGSERVICESADNISIONOFTELEDYNEBROWNENGINEERING10ForbesRoadWoburn,Massachusetts01801-2103617-932-9000FAX617-932-9970TECHNICALRESPONSETOSAFETYEVALUATIONBYTHEOFFICEOFNUCLEARREACTORREGULATIONRELATEDTOPROPOSEDDEFERMENTOFTORUSNODIFICATIONSNIAGARANOHAWKPOWERCORPORATIONNINENILEPOINTNUCLEARSTATIONUNIT1DOCKETNO.50-220NOVENBER19,1992cy211g00182921123PDRADQCK05000220PDR I
{{#Wiki_filter:i(TELEDYNEENGINEERING SERVICESADNISIONOFTELEDYNEBROWNENGINEERING 10ForbesRoadWoburn,Massachusetts 01801-2103 617-932-9000 FAX617-932-9970 TECHNICAL RESPONSETOSAFETYEVALUATION BYTHEOFFICEOFNUCLEARREACTORREGULATION RELATEDTOPROPOSEDDEFERMENT OFTORUSNODIFICATIONS NIAGARANOHAWKPOWERCORPORATION NINENILEPOINTNUCLEARSTATIONUNIT1DOCKETNO.50-220NOVENBER19,1992cy211g00182 921123PDRADQCK05000220PDR I
TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992TABLEOFCONTENSUMMARYi~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~o~~~~o~~~~~~~S1.0BACKGROUND..................................................2.0COLOADDEFINITIONCONSERVATISMS............................2.1FSTFCONSERVATISMS2.1.1FSTFENDCAPS................................2.1.2FSTFSTRUCTURALDAMPING......................2.2LDRCONSERVATISMS......................................2.2.1HARMONICCOMPONENTAMPLIFICATION.............2.2.2SUMMINGOFHARMONICCOMPONENTS...............3.0TESCOLOADREDUCTION-STRUCTURALMODEL/SHELLANALYSIS.....4.0ADDITIONALCONSERVATISMS....................................5.0APPLICABILITYOFTHECONCLUSIONSPROVIDEDINTHEREVIEWOFTHEVALIDITYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADS..........6.0NMP-1TORUSSHELLCMTR'S7.0RELEVANCETOSAFETY..8.0REFERENCE...................................................~Pae121820236TELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING PI0 TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992SUMMARYTheNRCSafetyEvaluationReport(SER)discussestwomethodsofobtainingreliefintheevaluationforcondensationoscillation(CO)loads.Thefirstmethodistocombinethe31stressharmonicsbytakingtheabsolutesumofthe4peakresponsesandaddingtothisthesquarerootofthesumofthesquares(SRSS)oftheremaining27harmonics.ThismethodhasbeenpreviouslyacceptedbytheNRC.ThesecondmethodistoincorporatetheanalyticallydeterminedCOpressurereductionfactorspresentedinNiagaraMohawkPowerCorporation'srecent,andsubjectsubmittal,reference1.TheSERadvisesthatthereviewtheyhavedonesofarsupportsthepositionthatoneortheotherofthetwoapproachesmaybeused,butnotboth.Thatis,ifcreditistakenfortherecentlydevelopedCOpressurereduction,thenall31stressharmonicsmustbecombinedbyabsolutesummation,ratherthanusingtherandomphasingrulespreviouslyapprovedfortheMarkITorusProgram.TheCOpressurereductionrepresentsnewandadditionalreliefanditsuseshouldnotprohibitusingthealreadyestablishedreliefgainedfromtherandomphasingofthestressharmonicssincethetwoanalysesareindependentofeachother.Theworkpresentedinreference1usestheContinuumDynamics,Inc.COpressurereductionresultsandcombinesthe31stressharmonicsbyabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining27harmonics.TheCOpressurereductionworkreducestheCOstressesbyapproximately17%and36%fortheeightandfourdowncomerbays,respectively.Absolutesummingthe4peakstressharmonicsandaddingtothistheSRSSoftheremaining27stressharmonicsresultsinanestimated33%lowerstressthanabsolutesummingalltheindividualharmonics.ConverselyATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING e"4d',f  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992stated,absolutesummingalltheindividualstressharmonicsoverpredictsmeasuredstressesbyabout50%.Themethodofcombiningthestressharmonicsbyabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining27stressharmonicswastheresultofextensivestructuralanalysisdonefortheoriginaltorusprogramandwasrecognizedastheappropriatewaytocorrelateFullScaleTestFacility(FSTF)measuredstresseswithFSTFanalyticallypredictedstresses.Thismethodwasavailableforallplantstouse,notjustNineMilePointUnit1(NMP-1),anditisstillvalid.TheCOpressurereductionaccountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomersandthehydrodynamicsineachbayareinphase.Thisisadifferent,andindependent,phenomenonthantheunderlyingbasistothemethodofcombiningstressharmonicsdiscussedintheprecedingparagraph.TheBrookhavenattachmenttotheSERagreesthattheendcapeffectisanFSTFconservatism.Theattachmentdoesnotquantifytheconservatism.NRC-acceptanceof-thereduced-CO.loadingaddressedhereingains-NMP-1areliefof573psiintheeightdowncomerbays,and1565psiinthefourdowncomerbays.Toseethatthisstressreductionisnominal,thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERINGC I\
TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992TABLEOFCONTENSUMMARYi~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~o~~~~o~~~~~~~S1.0BACKGROUND..................................................
TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19921.0BACKGROUNDTheMarkIProgramGeneralElectric(GE)determinedthemagnitudeoftheCondensationOscillation(CO)loadingbasedonthetestresultsfromtheFullScaleTestFacility(FSTF).TheFSTFfacilitywasonebaywithendcapstocontainthefluid,andasaresultofthecompromisesintestfacilitydesign,theseendcapscausedconservativeCOshellpressurestobemeasured.TheCOloaddefinition,basedonthesemeasuredpressures,wasconservativeontheorderof15to30percentandthiswasrecognizedatthattime.TheMarkIOwners'roupdetermineditwouldnotbecosteffectivetofundtheanalysisanddocumentationeffortnecessarytoachievefurtherreductionintheCOloaddefinitionsincemostoftheMarkIplantshadadequatemarginonCodestressallowablesfortheCOfrequencydomaineventcombinationloading.However,theNineMilePointUnit1(NHP-1)torushasathinshell(0.460in.)comparedwithmostofHarkIplants,andasaresult,thepostulatedeventcombinationwhichincludesDesignBreak/Accident(DBA)pressureandCO(eventcombination20)controlsthemarginontorusshellthickness.TeledyneEngineeringServices(TES)andNiagaraMohawkPowerCorporation(NHPC)recognizedthisproblemasbeingcriticalearlyintheHarkIprogram,andjointlytookthenecessarystepstomitigateloadsfromthiseventcombination.First,TESrefinedtheTorusAnalysisforDBApressureandCOincludingthepostprocessingofresults.Then,TESandNMPCinitiatedaseriesofthinshellmeetingsatGEforNHP-1andOysterCreek.ThesemeetingsidentifiedareasofconservatismintheloaddefinitiontobefurtherexploredbyGE.The,reductioninNHP-1DBApressureresultingfromthesemeetingswasessentialtothesuccessfulcomplianceofNMP-1totheHarkIProgramStructuralAcceptanceCriteriafortheCOeventcombination.TheDBApressure,ratherthantheCOloadingconservatisms,wereaddressedbasedoncostandtimeconsiderations.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
 
~I~P~+  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19922.0COLOADDEFINITIONCONSERVATISMSTheloadsonwhichtheTESstructuralanalysisisbasedarepresentedprimarilyinG.E.ReportNED0-21888,MarkIContainmentProgramLoadDefinitionReport(LDR),datedNovember1981(Reference3).TheseloadsweredevelopedfromtheFSTFduringtheHarkIProgramandhaveinherentconservatisms.2.1FSTFCONSERVATISHSTherearetwomajorconservatismsinherenttothegeometryoftheFSTF,theyaretheFSTFbayendcapsandthestructuraldampingassociatedwiththelowlevelofstressintheFSTFshell.2.1.1FSTFENDCAPSIn1979,ContinuumDynamics,Inc.(CDI)wasaskedbytheMarkIownersgroup,throughG.E.,toassesstheconservatismintheCondensationOscillationtorusloadsmeasuredduringtheFSTFblowdowntests.Thiseffortconfirmedgenerallyacceptedconservatisminthetestswithregardtotestinitialconditionthermodynamics,andidentifiedasignificantconservatismwhichwasnotidentifiedduringtestdesign.Thisconservatismwasintroducedbythegeometryofthetestfacility,one-sixteenthsectorwhichisequivalentlya22-1/2'egmentoftheMarkIPressureSuppressionPoolTorus.Thetestfacility,althoughfull-scaleincrosssection,attemptedtosimulateatfull-scalethecondensationphenomenoninonebayonly.Endcapswererequiredtocontainthepoolwaterandtheairspaceabovethepoolinthebay.Theanalysis,whichanalyzesthehydrodynamicconsequencesoftheseendcaps,waspresentedtotheHarkIownersin1980.Toexpeditecompletionofthisissue,theMarkIownersdecidednottopursuereducingthisconservatismatthattime.ThisworkisrevisitedforthiseffortanddevelopedspecificallyforNineMilePointUnitl.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING P0l>>  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992ThejointTESandCDIeffortpresentedinReferences1810andsummarizedhereinconsistsofananalyticalreductionintheHarkITorusProgramCondensationOscillationLoadDefinition.TheanalysisshowsthattheeightdowncomerbayshavebayaveragedCOloadswhichareconservativebyatleast19%atfrequenciesotherthan5-6Hzandforfourdowncomerbays,thebayaveragedCOloadsareconservativebyatleast38%atfrequenciesotherthan5-6Hz.Theloadconservatismsinthe5-6Hzfrequencybandare6%and28%fortheeightandfourdowncomerbays,respectively.Takingallfrequencybands(0to31Hz)intoaccountresultsinanetCOloaddefinitionconservatismof17.1%and36.1%fortheeightdowncomer(non-vent)andfourdowncomer(vent)bays,respectively.2.1.2FSTFSTRUCTURALDAMPINGDampingequalto2percentwasusedintheevaluationsperformedtodevelopthephasingrules.Theassumptionof2percentdamping,whichisappropriatefordesignresponsesfromcombinedloadsnearone-halfyieldstress,maybetoohighforthelowlevelFSTFresponse.Ifthedampingusedwereonly1.5percent,the-harmonic,responseamplitudesusedtodevelopthephasingruleswouldbesignificantlylargersuchthatthecombinedcalculatedresponseusingtheabsolutesumofthe4peakresponsesandaddingtothistheSRSSoftheremainder,wouldbeconservativecomparedtothemeasuredresponse.Inotherwords,usingtheabsolutesumoflessthanthe4peakresponses,perhapsthe3peakresponses,plustheSRSSoftheremainder,mayhaveboundedthemeasuredresponse.Inourjudgement,dampingontheorderof1.5percentwouldbemoreappropriateforFSTFresponselevelsthan2percent.Itmustbeemphasizedthatdampingof2percentismoreappropriatefordesignanalysesinwhichstresslevelsofone-halfyieldareallowable.O'TELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING J~I1  
==2.0 COLOADDEFINITION==
~i'ECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19922.2LDRCONSERVATISMSTherearetwoconservatismsassociatedwiththedevelopmentoftheLDR,G.E.ReportNEDO-21888(Reference3).Thefirstconservatismisrelatedtotheamplificationoftheindividualharmoniccomponentsbeforecombiningthecomponentsandthesecondconservatismisrelatedtothemethodusedtocombineorsumtheindividualharmonicstresscomponents.2.2.1HARMONICCOMPONENTAMPLIFICATIONForFSTFtheresponseamplificationfactorsateach0.914Hzfrequencyintervalwereusedinlieuoftheresponseamplificationfactorsatthestructuralnaturalfrequenciesineach1-Hzwindow(References4,758).Thephasingrulesweredevelopedwiththisreducedresponse.Suchanapproachdoesnotintroducetheconservatisminresponsecalculationwhichisobtainedwhenaccountingfortheresponseamplificationfactorsatthestructuralnaturalfrequenciesineach1-Hzwindow.Nocreditisgivenforthelatterapproach.2.2.2SUMMINGOFHARMONICCOMPONENTSTheLDR(Reference3)statesthatthecombinationof'individualharmonicstresscomponentsshallbesummed.Threeacceptablemethodsareavailable:1.Absolutesumofallharmoniccomponents.2.Absolutesumofthe3highestpeaksaddedtotheSRSSoftheremainingcomponentsandapplya1.15factor.3.Absolutesumofthe4highestpeaksaddedtotheSRSSoftheremainingcomponents,providedthereportedshellstressesarenotwithinafewpercentoftheallowables.iTELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
CONSERVATISMS............................
~I~1JI1g,,1I TECHNICALRESPONSETODOCKETNO.50-220NOVEHBER19,1992TheconservatismsassociatedwiththesemethodsarebasedontheboundingofthemeasuredFSTFtestshellstressresults(TestNo'sH-8,H-llBandH-12).Hethods1and2boundallthreetests,whilemethod3fallsjustshortofboundingtestH-lR.IITELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
2.1FSTFCONSERVATI SMS2.1.1FSTFENDCAPS................................
~rII  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19923.0TESCOLOADREDUCTION-STRUCTURALMODELSHELLANALYSISOscillatingloadsonthesubmergedportionofthetorusshellduringtheCOphenomenonarecausedbyperiodicoscillationssuperimposedontheprevailinglocalstaticpressures.PlantuniqueloadsarederivedfromFSTFdata.FlexiblewallloadsweremeasureddirectlyintheFSTFwhichisprototypicalofMarkIplantconfigurationswiththeexceptionoftherigidendcaps.PressuremeasurementsobtainedfromvariouslocationsonthetorusshellshowthatthelongitudinalpressureoscillationamplitudedistributionalongthetorusbottomcenterlineisessentiallyuniformfortheFSTF.Specificationofabaselinerigidwallloadisgivenaspressureoscillationamplitudeasafunctionoffrequency.ThisloadhasbeenderivedfromthemeasuredFSTFflexiblewallloadbyanalysiswithacoupledfluid-structuraldynamicmodeloftheFSTFtorus.Thederivationofthebaselinerigidwallloadisdescribedbelow:a.Afiniteelementcoupledfluid-structuraldynamicmodeloftheFSTFtoruswasexcitedatvaryingfrequencieswithaunitamplitudepressuresourceattheventexits.Thetorusshellpressureamplitudesrelativetothesourcepressure(amplificationfactors)weredeterminedasafunctionoffrequency.b.Usingtheserelativeamplitudes(amplificationfactors),theFSTFventexitsourcepressureswerederivedfromthemeasuredtorusshellpressuresatthevariousfrequencies.c.ThebaselinerigidwallloadwasderivedfromthecomputedFSTFventexitsourcepressuresbyhydrodynamicanalysis.IIITELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~I4,l TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992TheCOshellloadisspecifiedasadistributionofharmonicpressureamplitudesin1Hzbands(Reference3).Theanalysisforthisloadwasperformedbyconsideringtheeffectofunitloadsateachloadfrequency(harmonicanalysis)andthenscalingandcombiningtheindividualfrequencyeffectstodeterminetotalstressatthecriticalelement.ThethreevariationsintheCOspectrum(Reference3)wereevaluatedbyrescalingtheresultsoftheunitloadanalysis.100%ofwatermasswasusedforallCOanalysis.ThereductionfactorspresentedinTable1ofReference10wereappliedtotheindividualharmonicpressures.Thecombinationofindividualharmonicstressesintototalelementstresswasdonebyconsideringfrequencycontributionsat31Hzandbelow.TheactualcombinationwasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributorstotheSRSScombinationoftheothersforshellstress.Thiscombinationmethodanduseofthe31Hzcutoffaretheresultofextensivestructuralevaluationoffullscaletestdata,whichisreportedanddiscussedinReferences4and7.Includingthefrequencycontributionoutto50HzwouldincreasetheCOstressbyabout20psi,orlessthan1/2%.Themethodofcombiningthestressharmonicsbytheabsolutesumofthe4peaksplustheSRSSoftheremainderwastheresultofextensivestructuralanalysisdonefortheoriginaltorusprogramandwasrecognizedastheappropriatewaytocorrelateFSTFmeasuredstresseswithFSTFanalyticallypredictedstressesusingtheloaddefinition.Touseabsolutesumofallthecomponentswouldbetoignorethephasingbetweenfrequencydependentpressurecomponentsandbetweenfrequencydependentstructuralresponses,andtoassumephasingbetweentheharmoniccomponentstoproducethehighestpossiblestressresponse.Themethodofcombiningthestressharmonicsbytheabsolutesumofthe4peaksplustheSRSSoftheremainderwasavailableforallplantstouse,notjustNMP-1,andtodayremainsvalid.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING l~'I,,~)I  TECHNICALRESPONSETODOCKETNO.50-220NOVENBER19,1992Thepresentanalysis(References1510)investigatestheconservatismofthehydrodynamictorusCOloaddefinitionderivedfromdatatakenintheHarkIFSTF.ItisshownthatduringCO,thecondensationeventsatthedowncomerexitsare,asafunctionoffrequency,randominphaseformostharmoniccomponents.Asaconsequenceofthisobservation,andthegeometricalconstraintsbuiltintotheFSTF,theCOloadsdefinitionappliedtoNHP-Iisconservativefortworeasons.~AlternatedowncomerbaysinNHP-Ihavefour-eight-four-eight,etc.,downcomersperbay.TheFSTFfacility,byconstruction,assumesthatallbayshaveeightdowncomersperbay.TheFSTFmodeleda22I/2'ectorofaprototypicalHarkIsuppressionchamber.Thewaterwascontainedinthesectorbytwoveryrigidendcapswhichwouldnotexistinafullsuppressionchamber.Theseendcapshydrodynamicallyactasmirrors.Thisresultsinameasuredload,asifallbaysinafulltorushadcondensationphenomenonidenticalinphaseandamplitude,totheinstrumentedFSTFbay.TheanalysisshowsthatforNHP-I:~EightdowncomerbayshavebayaveragedCOloadswhichareconservativebyatleast19%atfrequenciesotherthan5-6Hz.~FourdowncomerbayshavebayaveragedCOloadswhichareconservativebyatleast38%atfrequenciesotherthan5-6Hz.Thepresentwork(Reference1)accountsforboththerandomphasingofthestressharmonicsandthereductioninFSTFmeasuredpressures,twoindependentphenomena.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING rll~A v,TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992InclusionofthereducedCOloadingaddressedhereingainsNHP-Iareliefof573psiintheeightdowncomerbays,and1565psiinthefourdowncomerbays.Thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.TheCOloadreductionaccountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomersandthehydrodynamicsineachbayisinphasewithadjoiningbays.IntheBrookhavenattachmenttotheSER(Reference15)itisstatedthattheendcapsintroduceanFSTFconservatism.made:Onpage3oftheBrookhavenattachment,thefollowingpointsareTheFSTFdatasupportthenotionthattheCOprocessisrandomovermostofthefrequencyspectrumconsideredintheloadmethods.Becauseofthegeometricdifferences,particularlythe4-8-4downcomerarrangement,thepressureloadsduringCOblowdownwilltendtobegreaterintheFSTFrelativetotheNHPtorusforthesamehydrodynamicflowconditions.~Theprocedureusedtoquantifytheseeffectsrepresentsastraightforwardapplicationofaconventionalhydrodynamicmethod.Theresultsarereasonableandprobablyconservativebecauseofthehighsoundspeedusedinthenumerics.Wealsoconsidertheassumptionthatacorrelationexistsbetweenbaystobeasignificantconservatism.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 0'i~  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992Theattachmentitselfdoesnotquantifytheseconservatisms.However,GeorgeBienkowski'sreviewoftheRandomPhasingRules,datedAugust25,1983(Reference14),alsoincludessomequantificationoftheseeffects.ThisisdiscussedinSection5.0herein.IIITELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING It.JI  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19924.0ADDITIONALCONSERVATISHSThefollowingisadelineationofadditionalconservatismsforwhichnocredithasbeentaken.1.UniformcorrosionoftheshellwouldcausethefrequenciestodropandtheresponsetoCOloadtodecrease.Ifthefrequenciesdrop1Hz,thenitisestimatedthatNMP-1wouldgainabout600psireliefinshellstress.2.Theanalysishasbeenperformedusing2%damping.Itisestimatedthatincreasingthedampingto4%,toaccountforwater/structuredamping,wouldgainNHP-1morethan900psirelief.Even4%dampingmaybelowforathinshelledwaterfilledstructure.3.ThehighsoundspeedusedinthedeterminationoftheCOloadreductionfactorsisconservativeasisshowninReference10.4.Curvatureeffectsofthetorus.5.TheASHECodeallowsauniform10%reductioninwallthicknessforClassMCComponents,1990Addenda,SectionXI,ParagraphIWE-3519.3.Thisisthesameasallowinga10%increaseinthematerialallowables.6.TheASMECode,SectionIII,ParagraphNf-3213.10,permitsuptoI/16inchlocalcorrosionasisexplainedinTESTechnicalReportTR-6801-2(Referencell).7.Class1allowablesforthismaterialaregreaterthanClassHCallowablesby21%,Sm=20ksiforClass1vs.Sm=16.5ksiforClassHC.HTELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
2.1.2FSTFSTRUCTURAL DAMPING......................
]tI~i4VjW  TECHNICALRESPONSETODOCKETNO.50-220NOVEHBER19$19928.CertifiedHaterialTestReports(CHTR's)fortheNHP-1shellmaterialindicatehigherallowablesthanthoseusedintheHarkIProgramAnalysis,17.6ksivs.16.5ksi(seeSection6.0).IfitbecomesnecessarytousetheCHTR's,hardnesstestscouldbeperformedonthetorusshelltoincreaseconfidenceinthematerialCHTR's.9.Thereisinherentconservatisminthefactorofsafety(FS)associatedwiththecode,FS=1/(1.lxl/4)=3.64onultimatematerialstrength.ItTELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
2.2LDRCONSERVATISMS......................................
~I4k,  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19925.0APPLICABILITYOFTHECONCLUSIONSPROVIDEDINTHEREVIEWOFTHEVALIDIYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADSGeorgeBienkowskiissuedtheresultsofhisreviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,onAugust25,1983(Reference14).Thereviewconcludedthefollowing:l.A/E'scouldeliminatethe1.15responsefactoronshellstressesiftheyuse4harmonicssummedabsolutelyaddedtotheremainingsummedSRSS(inlieuof1.15factoron3harmonicssummedabsolutelyaddedtotheremainingsummedSRSS),providedthereportedshellstressesarenotwithinafewpercentoftheallowables,otherwisetheissueshouldberevisited.Theadditionof1harmonic,tobesummedabsolutely,providesonlyabouta10%increaseintheresponsesratherthanthe15%neededtoboundtheFSTFmeasurements.2.A/E'scouldneglecttheharmoniccomponentsabove30HertzforstructureswithsimilarnaturalfrequencycontenttotheFSTForOysterCreekifspecificjustificationintheformoftorusresponsefrequencycharacteristicispresented.3.A/E'scoulduseanyvariationthatproducesatleastashigharatioofresponsetothatproduced,byabsolutesumasthehighestobservedintheFSTFandOysterCreekanalyses(63%).TherefinedshellanalysisoftheNMP-1torusshell,performedbyTES,usingthereducedCOloaddefinitionincludesthefollowing:1.TheCOloadreductionresultingfromtheFSTFendcaps,17.1%and36.1%fornon-ventandventbays,respectively.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING v.r,jl4  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19922.Thecombinationofindividualharmonicstressesintototalelementstresswasdonebyconsideringfrequencycontributionsat31Hzandbelow.TheactualcombinationwasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributorstotheSRSScombinationoftheothersforshellstress.Thiscombinationmethodanduseofthe31Hzcutoffaretheresultofextensivenumericalevaluationoffullscaletestdata.Includingthefrequencycontributionoutto50HzwouldincreasetheCOstressbyabout20psi,orlessthanI/2%.GeorgeBienkowski'sreviewoftheRandomPhasingRulesalsoaddressedthe,impactoftheendcapsonproducingconservativelymeasuredCOloads.Thisdiscussionbeginsatthebottomofpage3ofthereview.Here,thereviewreferstoanunreferencedcommunicationinReportsSMA12101.04-R002D(Reference7)andSMA12101.04-R003D(Reference8),fromDr.AlanBilanin,thatthepresenceofthebulkheadsintroducesafactorofconservatismofatleast1.33tothemeasuredCOloadingandresponsesfromwhichtheLDRamplitudes-werederived.Thisisseparatefromthephasingrulesgoverningthesummationofstressharmonics.Inaddition,an"AppendixA"ismentionedwhereinthiseffectisexamined.This"AppendixA"isassumedtobeanappendixtoGeorgeBienkowski'sreviewandithasnotbeenreviewedbyTESorCDI.ItisstatedthattheAppendixconcludesthatforfrequenciesthatarenotcorrelatedbetweenbays,theFSTFshouldproduce32%to35%higherloadsthanwouldexistinarealfacilityandthatonlythefundamentalfrequencynear6Hzshowsanycorrelationbetweendowncomers.Thereviewfurtherstatesthatifoneassumescorrelationbetweenbaysatthatfrequencyandrandomphasing(thisisnottherandomphasingofresponsestressharmonics)atallotherfrequencies,theoverallconservatismforIITELEDYNEENGlNEERlNGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~ck  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992theaveragepressure~abeaslowas17%(notethereviewsays"may"),whileattheresponseleveltheFSTFconservatismwillrangefrom18%forhoopstressto38%fortheaxialstress.TheseindependentBrookhavengeneratedresultsarenotunlikethosethatNNPCiscurrentlypresenting.RobertKennedy,inhisreportSMA12101.04-R003D(Reference8),usesthisadditional33%conservatism,advancedbyDr.AlanBilanin,toaccountfortheuncertaintyofusingonlythethreepeakresponsesfromFSTFtestsH-8,H-llBandM-12.Ontheotherhand,GeorgeBienkowskiarguesthatthisuncertaintyestimateisprobablyexcessivelyconservativeandthat7%ratherthan33%uncertaintywouldprovideahighconfidencelevelofnon-exceedance.UsingtheabovenumbersfromGeorgeBienkowski'swork,wehaveasaminimumthatthemeasuredstressesareconservativebyatleast:(1-[(1-.18)(1+.07)])100=(1-,88)100=12%Also,nomentionhasbeenmadeinGeorgeBienkowski'sreviewregardingtheeffectofthe4-8-4downcomerconfiguration.ThejointTES/CDIwork(Reference1)evaluatesthiseffectaswell.Sowearelookingfor17%reliefinthe8downcomerbaysandtheBrookhavenworkshowsatleast12%relief.Thedifferencemaybeattributedtothe4downcomerbaystoeithersideofthe8downcomerbay.Inaddition,the36%reductionthatwehaveevaluatedforthe4downcomerbaysalsoincludesthefactthatonlyhalfasmanydowncomersarepresentasareintheFSTF,aneffectnotmentionedinGeorgeBienkowski'sreview.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
2.2.1HARMONICCOMPONENT AMPLIFICATION.............
,2~gp'f  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,1992TheconservatismsrelatedtotheendcapeffectdiscussedhereinwerenotincludedinGeorgeBienkowski'sconclusionsregardingthephasingrules.Oncetheendcapeffectisincluded,thereisnoreasonwhytheresultingresponseshouldboundFSTFdata.Indeed,byitsverynature,itshouldnotboundFSTFdata.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING r1V~wg/  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,19926.0NAP-ITORUSSHELLCNTR'SCertifiedMaterialTestReortReviewforTorusShell(Reference11)TEShasreviewedtheTorusShellCertifiedHaterialTestReports(A201GrBFBX).Astatisticalanalysiswasperformedusingthis(large)sampledatatodeterminethe.99confidenceintervalestimateofthemeanyieldandultimatestrengthofthismaterial.TheCoderequiresthattheminimumyieldandminimumultimatestrengthofthematerialbeusedtodeterminetheallowablestressintensity(SgC)asfollows:SgCat70'Fisthelessorof1'15SYor1.11SUTherefore,TEShasassumedthattheminimumyieldandultimatestrengthsofthematerialareboundedbyusingtwosamplestandarddeviationsfromthestatisticallyestimatedminimummeanvalues.Basedonthecalculationsusingtheabovestatedcriteria,theCodeallowablestressintensitywouldbeestimatedat:SNC=17600at70'FUseofthisestimatedallowablestressintensitywillprovideanadditional1100psireliefascomparedtothepresentCodeallowableof16500psiwhichwasusedduringtheHarkIContainmentProgramanalysisforATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING S',fI  TECHNICALRESPONSETODOCKETNO.50-220NOVEHBER19,1992thetorusshellmaterialforthefullrangeofanticipatedeventtemperaturesfrom70to350'F.Intermsofreliefontheshellthicknessrequirements,theincreasedallowablewillprovidejustunder1/32inchesor6/.additionalmargin.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING qXmy<~),+LC  TECHNICALRESPONSETODOCKETNO.50-220NOVEHBER19,19927.0RELEVANCETOSAFETYWedonotviewthisissueasadverselyaffectingsafety.ItcanberegardedastheeffortundertakentoremoveknownconservatismsthroughrefinementofthepostulatedappliedCOloads.Inaddition,resolutionofCodeissuespertainingtotheallowablematerialstrengthandallowablenominalcorrosion,delineatedinSection4.0,"AdditionalConservatisms",ifintroduced,wouldprovideforaddedmarginforthetorusshellstresses.Also,themanyotherconservatismsdiscussedthroughoutthisresponse,ifaccountedfor,wouldfurtherreducetheshellstress.TorusCorrosionRate(>)NiagaraHohawkundertookanewcorrosionmonitoringprograminAugust,1989.Underthisprogram1'3'ridsonall40midbaybottomplateswereUTinspected.HPRAssociates,Inc.ReportHPR-1152delineatestheresultsofthisinspection.Thesemeasurementsdidnotshowanysignificantlossduetocorrosionorpittingevenatthenormalwaterlevelregion;andtherewerenowallthicknessmeasurementsthatwouldrequireapplicationofthemethodsdescribedinTeledyneReportTR-6801-2,reference11.HPRquantifiedtheshellthicknessloss,over20years,bycomparingthemeasuredshellthicknessvaluestothecalculatedoriginalplatethickness.Thirtyfourshellplates,traceabletotheoriginalmilcertifications,wereusedinthiscomparison.Originalplatethicknesseswerecalculatedusingplatedimensions,weightanddensityofthesteel.ThesethicknesseswerecomparedtotheUTthicknessobtainedinAugust,1989,onthesame34plates.Theresultsindicatedanaveragecorrosionlossof0.8milsperyear.Thisratetranslatestoatotallossof32milsoraboutI/32"overtheoriginalprojected40yearplantlife;andcomparescloselytotheratepredictedbyRadiological8ChemicalTechnology,Inc.(RCT),basedonanalysisofsludgesamplesin1979.Duetovariationsin(1)ThisinformationprovidedbyNHPC.ATELEDYNEENGlNEERlNGSERVlCESADIVISIONOFTELEDYNEBROWNENGINEERING Vrl-k  TECHNICALRESPONSETODOCKETNO.50-220NOVENBER19,1992theoriginalplatedimensionsandweights,andmeasurements,onestandarddeviationwasaddedtothe0.8milsperyear.Thisresultedinaconservativepredictionof1.26milsperyearcorrosionrate.Additionally,NiagaraMohawkPowerCorporationcommittedtoperformUTmeasurementsonasixmonthbasisandprovidetheNRCwiththeresults(Ref.November22,1989,letterC.TerrytoNRC).Sincebaselineestablishmentofthenewcorrosionprogramof1989,six(6)six-monthmeasurementshavebeenconducted,themostrecentofwhichwerejusttakeninSeptember,1992.Furtheranalysisandtrendingofthesemeasurementsindicatethataconservativecorrosionrateof1mi-l/yrincludingonestandarddeviationisamorerealisticcorrosionratethanthebaselineestimateof1.26mils/yr.Themostprobablepredictionofcorrosionrateisstill0.8mils/yr,butthelaterresultshavereducedthestandarddeviationto+0.2mils/yr.Thelatest(September,1992)UTmeasurements,onthethinnesttorusplatesindicatestheaveragethicknessoftheworstplateis0.453inches.Thisthicknessrepresentsanaverageof63individualmeasurements(calibrationadjusted)ona1'3'ridonthatworstplate.Worstcaseindividualmeasurementsonthisorotherplateshavebeenaslowas0.445inches(calibrationadjusted).Overthenextyear,theprojectedworstcaselossofthicknesswouldbeonemilor0.001".Thiswouldtheoreticallyreducetheworstgridtoa0.452"averagethicknessandtheworstindividualpointto0.444".TheaveragethicknesswouldcomplywithminimumthicknessallowedbyTeledyneReportTR-6801-2,reference2,andtheoreticallyprovideforaboutanother5yearsofoperationbeforereachingthecurrentminimumthicknessallowed.However,the0.444"individualpointwouldhavetobeanalyzedforcompliancetoTR-6801-2bythemethodsoutlinedtherein.TheanalysissubmittedunderNHPC'sMay14,1991coverletter(Reference1),totheNRCsupportsanyaveragethicknessorindividual6TELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19i1992pointdownto0.431".Inaddition,themanyotherconservatismsdiscussedherein,forwhichnocredithasbeenrequestedortakenintoaccount,wouldsupportreductionsinexcessofthis.Therefore,lossofthicknessoccurringduetoprojectedcorrosionoverthenextyearwouldbewithinlimitsofsupportinganalyses.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
2.2.2SUMMINGOFHARMONICCOMPONENTS...............
~jlV~Aall~  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,199
 
==3.0 TESCOLOADREDUCTION==
-STRUCTURAL MODEL/SHELL ANALYSIS.....
 
==4.0 ADDITIONAL==
CONSERVATISMS....................................
 
==5.0 APPLICABILITY==
OFTHECONCLUSIONS PROVIDEDINTHEREVIEWOFTHEVALIDITYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADS..........
6.0NMP-1TORUSSHELLCMTR'S7.0RELEVANCE TOSAFETY..8.0REFERENCE...................................................
~Pae121820236TELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING PI0 TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992SUMMARYTheNRCSafetyEvaluation Report(SER)discusses twomethodsofobtaining reliefintheevaluation forcondensation oscillation (CO)loads.Thefirstmethodistocombinethe31stressharmonics bytakingtheabsolutesumofthe4peakresponses andaddingtothisthesquarerootofthesumofthesquares(SRSS)oftheremaining 27harmonics.
Thismethodhasbeenpreviously acceptedbytheNRC.Thesecondmethodistoincorporate theanalytically determined COpressurereduction factorspresented inNiagaraMohawkPowerCorporation's recent,andsubjectsubmittal, reference 1.TheSERadvisesthatthereviewtheyhavedonesofarsupportsthepositionthatoneortheotherofthetwoapproaches maybeused,butnotboth.Thatis,ifcreditistakenfortherecentlydeveloped COpressurereduction, thenall31stressharmonics mustbecombinedbyabsolutesummation, ratherthanusingtherandomphasingrulespreviously approvedfortheMarkITorusProgram.TheCOpressurereduction represents newandadditional reliefanditsuseshouldnotprohibitusingthealreadyestablished reliefgainedfromtherandomphasingofthestressharmonics sincethetwoanalysesareindependent ofeachother.Theworkpresented inreference 1usestheContinuum
: Dynamics, Inc.COpressurereduction resultsandcombinesthe31stressharmonics byabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining 27harmonics.
TheCOpressurereductionworkreducestheCOstressesbyapproximately 17%and36%fortheeightandfourdowncomer bays,respectively.
Absolutesummingthe4peakstressharmonics andaddingtothistheSRSSoftheremaining 27stressharmonics resultsinanestimated 33%lowerstressthanabsolutesummingalltheindividual harmonics.
Conversely ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING e"4d',f  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992stated,absolutesummingalltheindividual stressharmonics overpredictsmeasuredstressesbyabout50%.Themethodofcombining thestressharmonics byabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining 27stressharmonics wastheresultofextensive structural analysisdonefortheoriginaltorusprogramandwasrecognized astheappropriate waytocorrelate FullScaleTestFacility(FSTF)measuredstresseswithFSTFanalytically predicted stresses.
Thismethodwasavailable forallplantstouse,notjustNineMilePointUnit1(NMP-1),anditisstillvalid.TheCOpressurereduction accountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomers andthehydrodynamics ineachbayareinphase.Thisisadifferent, andindependent, phenomenon thantheunderlying basistothemethodofcombining stressharmonics discussed inthepreceding paragraph.
TheBrookhaven attachment totheSERagreesthattheendcapeffectisanFSTFconservatism.
Theattachment doesnotquantifytheconservatism.
NRC-acceptance of-thereduced-CO.loading addressed hereingains-NMP-1areliefof573psiintheeightdowncomer bays,and1565psiinthefourdowncomer bays.Toseethatthisstressreduction isnominal,thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING C
I\
TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19921.0BACKGROUND TheMarkIProgramGeneralElectric(GE)determined themagnitude oftheCondensation Oscillation (CO)loadingbasedonthetestresultsfromtheFullScaleTestFacility(FSTF).TheFSTFfacilitywasonebaywithendcapstocontainthefluid,andasaresultofthecompromises intestfacilitydesign,theseendcapscausedconservative COshellpressures tobemeasured.
TheCOloaddefinition, basedonthesemeasuredpressures, wasconservative ontheorderof15to30percentandthiswasrecognized atthattime.TheMarkIOwners'roup determined itwouldnotbecosteffective tofundtheanalysisanddocumentation effortnecessary toachievefurtherreduction intheCOloaddefinition sincemostoftheMarkIplantshadadequatemarginonCodestressallowables fortheCOfrequency domaineventcombination loading.However,theNineMilePointUnit1(NHP-1)torushasathinshell(0.460in.)comparedwithmostofHarkIplants,andasaresult,thepostulated eventcombination whichincludesDesignBreak/Accident (DBA)pressureandCO(eventcombination 20)controlsthemarginontorusshellthickness.
TeledyneEngineering Services(TES)andNiagaraMohawkPowerCorporation (NHPC)recognized thisproblemasbeingcriticalearlyintheHarkIprogram,andjointlytookthenecessary stepstomitigateloadsfromthiseventcombination.
First,TESrefinedtheTorusAnalysisforDBApressureandCOincluding thepostprocessing ofresults.Then,TESandNMPCinitiated aseriesofthinshellmeetingsatGEforNHP-1andOysterCreek.Thesemeetingsidentified areasofconservatism intheloaddefinition tobefurtherexploredbyGE.The,reduction inNHP-1DBApressureresulting fromthesemeetingswasessential tothesuccessful compliance ofNMP-1totheHarkIProgramStructural Acceptance CriteriafortheCOeventcombination.
TheDBApressure, ratherthantheCOloadingconservatisms, wereaddressed basedoncostandtimeconsiderations.
ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~I~P~+  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.0COLOADDEFINITION CONSERVATISMS TheloadsonwhichtheTESstructural analysisisbasedarepresented primarily inG.E.ReportNED0-21888, MarkIContainment ProgramLoadDefinition Report(LDR),datedNovember1981(Reference 3).Theseloadsweredeveloped fromtheFSTFduringtheHarkIProgramandhaveinherentconservatisms.
2.1FSTFCONSERVATISHS Therearetwomajorconservatisms inherenttothegeometryoftheFSTF,theyaretheFSTFbayendcapsandthestructural dampingassociated withthelowlevelofstressintheFSTFshell.2.1.1FSTFENDCAPSIn1979,Continuum
: Dynamics, Inc.(CDI)wasaskedbytheMarkIownersgroup,throughG.E.,toassesstheconservatism intheCondensation Oscillation torusloadsmeasuredduringtheFSTFblowdowntests.Thiseffortconfirmed generally acceptedconservatism inthetestswithregardtotestinitialcondition thermodynamics, andidentified asignificant conservatism whichwasnotidentified duringtestdesign.Thisconservatism wasintroduced bythegeometryofthetestfacility, one-sixteenth sectorwhichisequivalently a22-1/2'egment oftheMarkIPressureSuppression PoolTorus.Thetestfacility, althoughfull-scale incrosssection,attempted tosimulateatfull-scale thecondensation phenomenon inonebayonly.Endcapswererequiredtocontainthepoolwaterandtheairspaceabovethepoolinthebay.Theanalysis, whichanalyzesthehydrodynamic consequences oftheseendcaps,waspresented totheHarkIownersin1980.Toexpeditecompletion ofthisissue,theMarkIownersdecidednottopursuereducingthisconservatism atthattime.Thisworkisrevisited forthiseffortanddeveloped specifically forNineMilePointUnitl.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING P0l>>  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992ThejointTESandCDIeffortpresented inReferences 1810andsummarized hereinconsistsofananalytical reduction intheHarkITorusProgramCondensation Oscillation LoadDefinition.
Theanalysisshowsthattheeightdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast19%atfrequencies otherthan5-6Hzandforfourdowncomer bays,thebayaveragedCOloadsareconservative byatleast38%atfrequencies otherthan5-6Hz.Theloadconservatisms inthe5-6Hzfrequency bandare6%and28%fortheeightandfourdowncomer bays,respectively.
Takingallfrequency bands(0to31Hz)intoaccountresultsinanetCOloaddefinition conservatism of17.1%and36.1%fortheeightdowncomer (non-vent) andfourdowncomer (vent)bays,respectively.
2.1.2FSTFSTRUCTURAL DAMPINGDampingequalto2percentwasusedintheevaluations performed todevelopthephasingrules.Theassumption of2percentdamping,whichisappropriate fordesignresponses fromcombinedloadsnearone-halfyieldstress,maybetoohighforthelowlevelFSTFresponse.
Ifthedampingusedwereonly1.5percent,the-harmonic, responseamplitudes usedtodevelopthephasingruleswouldbesignificantly largersuchthatthecombinedcalculated responseusingtheabsolutesumofthe4peakresponses andaddingtothistheSRSSoftheremainder, wouldbeconservative comparedtothemeasuredresponse.
Inotherwords,usingtheabsolutesumoflessthanthe4peakresponses, perhapsthe3peakresponses, plustheSRSSoftheremainder, mayhaveboundedthemeasuredresponse.
Inourjudgement, dampingontheorderof1.5percentwouldbemoreappropriate forFSTFresponselevelsthan2percent.Itmustbeemphasized thatdampingof2percentismoreappropriate fordesignanalysesinwhichstresslevelsofone-halfyieldareallowable.
O'TELEDYNE ENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING J~I1  
~i'ECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.2LDRCONSERVATISMS Therearetwoconservatisms associated withthedevelopment oftheLDR,G.E.ReportNEDO-21888 (Reference 3).Thefirstconservatism isrelatedtotheamplification oftheindividual harmoniccomponents beforecombining thecomponents andthesecondconservatism isrelatedtothemethodusedtocombineorsumtheindividual harmonicstresscomponents.
2.2.1HARMONICCOMPONENT AMPLIFICATION ForFSTFtheresponseamplification factorsateach0.914Hzfrequency intervalwereusedinlieuoftheresponseamplification factorsatthestructural naturalfrequencies ineach1-Hzwindow(References 4,758).Thephasingrulesweredeveloped withthisreducedresponse.
Suchanapproachdoesnotintroduce theconservatism inresponsecalculation whichisobtainedwhenaccounting fortheresponseamplification factorsatthestructural naturalfrequencies ineach1-Hzwindow.Nocreditisgivenforthelatterapproach.
2.2.2SUMMINGOFHARMONICCOMPONENTS TheLDR(Reference 3)statesthatthecombination of'individual harmonicstresscomponents shallbesummed.Threeacceptable methodsareavailable:
1.Absolutesumofallharmoniccomponents.
2.Absolutesumofthe3highestpeaksaddedtotheSRSSoftheremaining components andapplya1.15factor.3.Absolutesumofthe4highestpeaksaddedtotheSRSSoftheremaining components, providedthereportedshellstressesarenotwithinafewpercentoftheallowables.
iTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~I~1JI1g,,1I TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,1992Theconservatisms associated withthesemethodsarebasedontheboundingofthemeasuredFSTFtestshellstressresults(TestNo'sH-8,H-llBandH-12).Hethods1and2boundallthreetests,whilemethod3fallsjustshortofboundingtestH-lR.IITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~rII  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19923.0TESCOLOADREDUCTION
-STRUCTURAL MODELSHELLANALYSISOscillating loadsonthesubmerged portionofthetorusshellduringtheCOphenomenon arecausedbyperiodicoscillations superimposed ontheprevailing localstaticpressures.
PlantuniqueloadsarederivedfromFSTFdata.FlexiblewallloadsweremeasureddirectlyintheFSTFwhichisprototypical ofMarkIplantconfigurations withtheexception oftherigidendcaps.Pressuremeasurements obtainedfromvariouslocations onthetorusshellshowthatthelongitudinal pressureoscillation amplitude distribution alongthetorusbottomcenterlineisessentially uniformfortheFSTF.Specification ofabaselinerigidwallloadisgivenaspressureoscillation amplitude asafunctionoffrequency.
ThisloadhasbeenderivedfromthemeasuredFSTFflexiblewallloadbyanalysiswithacoupledfluid-structural dynamicmodeloftheFSTFtorus.Thederivation ofthebaselinerigidwallloadisdescribed below:a.Afiniteelementcoupledfluid-structural dynamicmodeloftheFSTFtoruswasexcitedatvaryingfrequencies withaunitamplitude pressuresourceattheventexits.Thetorusshellpressureamplitudes relativetothesourcepressure(amplification factors)weredetermined asafunctionoffrequency.
b.Usingtheserelativeamplitudes (amplification factors),
theFSTFventexitsourcepressures werederivedfromthemeasuredtorusshellpressures atthevariousfrequencies.
c.ThebaselinerigidwallloadwasderivedfromthecomputedFSTFventexitsourcepressures byhydrodynamic analysis.
IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~I4,l TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992TheCOshellloadisspecified asadistribution ofharmonicpressureamplitudes in1Hzbands(Reference 3).Theanalysisforthisloadwasperformed byconsidering theeffectofunitloadsateachloadfrequency (harmonic analysis) andthenscalingandcombining theindividual frequency effectstodetermine totalstressatthecriticalelement.Thethreevariations intheCOspectrum(Reference 3)wereevaluated byrescaling theresultsoftheunitloadanalysis.
100%ofwatermasswasusedforallCOanalysis.
Thereduction factorspresented inTable1ofReference 10wereappliedtotheindividual harmonicpressures.
Thecombination ofindividual harmonicstressesintototalelementstresswasdonebyconsidering frequency contributions at31Hzandbelow.Theactualcombination wasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributors totheSRSScombination oftheothersforshellstress.Thiscombination methodanduseofthe31Hzcutoffaretheresultofextensive structural evaluation offullscaletestdata,whichisreportedanddiscussed inReferences 4and7.Including thefrequency contribution outto50HzwouldincreasetheCOstressbyabout20psi,orlessthan1/2%.Themethodofcombining thestressharmonics bytheabsolutesumofthe4peaksplustheSRSSoftheremainder wastheresultofextensive structural analysisdonefortheoriginaltorusprogramandwasrecognized astheappropriate waytocorrelate FSTFmeasuredstresseswithFSTFanalytically predicted stressesusingtheloaddefinition.
Touseabsolutesumofallthecomponents wouldbetoignorethephasingbetweenfrequency dependent pressurecomponents andbetweenfrequency dependent structural responses, andtoassumephasingbetweentheharmoniccomponents toproducethehighestpossiblestressresponse.
Themethodofcombining thestressharmonics bytheabsolutesumofthe4peaksplustheSRSSoftheremainder wasavailable forallplantstouse,notjustNMP-1,andtodayremainsvalid.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING l~'I,,~)I  TECHNICAL RESPONSETODOCKETNO.50-220NOVENBER19,1992Thepresentanalysis(References 1510)investigates theconservatism ofthehydrodynamic torusCOloaddefinition derivedfromdatatakenintheHarkIFSTF.ItisshownthatduringCO,thecondensation eventsatthedowncomer exitsare,asafunctionoffrequency, randominphaseformostharmoniccomponents.
Asaconsequence ofthisobservation, andthegeometrical constraints builtintotheFSTF,theCOloadsdefinition appliedtoNHP-Iisconservative fortworeasons.~Alternate downcomer baysinNHP-Ihavefour-eight-four-eight, etc.,downcomers perbay.TheFSTFfacility, byconstruction, assumesthatallbayshaveeightdowncomers perbay.TheFSTFmodeleda22I/2'ector ofaprototypical HarkIsuppression chamber.Thewaterwascontained inthesectorbytwoveryrigidendcapswhichwouldnotexistinafullsuppression chamber.Theseendcapshydrodynamically actasmirrors.Thisresultsinameasuredload,asifallbaysinafulltorushadcondensation phenomenon identical inphaseandamplitude, totheinstrumented FSTFbay.TheanalysisshowsthatforNHP-I:~Eightdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast19%atfrequencies otherthan5-6Hz.~Fourdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast38%atfrequencies otherthan5-6Hz.Thepresentwork(Reference 1)accountsforboththerandomphasingofthestressharmonics andthereduction inFSTFmeasuredpressures, twoindependent phenomena.
ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING rll~A v,TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Inclusion ofthereducedCOloadingaddressed hereingainsNHP-Iareliefof573psiintheeightdowncomer bays,and1565psiinthefourdowncomer bays.Thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.TheCOloadreduction accountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomers andthehydrodynamics ineachbayisinphasewithadjoining bays.IntheBrookhaven attachment totheSER(Reference 15)itisstatedthattheendcapsintroduce anFSTFconservatism.
made:Onpage3oftheBrookhaven attachment, thefollowing pointsareTheFSTFdatasupportthenotionthattheCOprocessisrandomovermostofthefrequency spectrumconsidered intheloadmethods.Becauseofthegeometric differences, particularly the4-8-4downcomer arrangement, thepressureloadsduringCOblowdownwilltendtobegreaterintheFSTFrelativetotheNHPtorusforthesamehydrodynamic flowconditions.
~Theprocedure usedtoquantifytheseeffectsrepresents astraightforwardapplication ofaconventional hydrodynamic method.Theresultsarereasonable andprobablyconservative becauseofthehighsoundspeedusedinthenumerics.
Wealsoconsidertheassumption thatacorrelation existsbetweenbaystobeasignificant conservatism.
ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 0'i~  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Theattachment itselfdoesnotquantifytheseconservatisms.
However,GeorgeBienkowski's reviewoftheRandomPhasingRules,datedAugust25,1983(Reference 14),alsoincludessomequantification oftheseeffects.Thisisdiscussed inSection5.0herein.IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING It.JI  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19924.0ADDITIONAL CONSERVATISHS Thefollowing isadelineation ofadditional conservatisms forwhichnocredithasbeentaken.1.Uniformcorrosion oftheshellwouldcausethefrequencies todropandtheresponsetoCOloadtodecrease.
Ifthefrequencies drop1Hz,thenitisestimated thatNMP-1wouldgainabout600psireliefinshellstress.2.Theanalysishasbeenperformed using2%damping.Itisestimated thatincreasing thedampingto4%,toaccountforwater/structure damping,wouldgainNHP-1morethan900psirelief.Even4%dampingmaybelowforathinshelledwaterfilledstructure.
3.Thehighsoundspeedusedinthedetermination oftheCOloadreduction factorsisconservative asisshowninReference 10.4.Curvature effectsofthetorus.5.TheASHECodeallowsauniform10%reduction inwallthickness forClassMCComponents, 1990Addenda,SectionXI,Paragraph IWE-3519.3.
Thisisthesameasallowinga10%increaseinthematerialallowables.
6.TheASMECode,SectionIII,Paragraph Nf-3213.10,permitsuptoI/16inchlocalcorrosion asisexplained inTESTechnical ReportTR-6801-2 (Reference ll).7.Class1allowables forthismaterialaregreaterthanClassHCallowables by21%,Sm=20ksiforClass1vs.Sm=16.5ksiforClassHC.HTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
]tI~i4VjW  TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19$19928.Certified HaterialTestReports(CHTR's)fortheNHP-1shellmaterialindicatehigherallowables thanthoseusedintheHarkIProgramAnalysis, 17.6ksivs.16.5ksi(seeSection6.0).Ifitbecomesnecessary tousetheCHTR's,hardnesstestscouldbeperformed onthetorusshelltoincreaseconfidence inthematerialCHTR's.9.Thereisinherentconservatism inthefactorofsafety(FS)associated withthecode,FS=1/(1.lxl/4)=3.64onultimatematerialstrength.
ItTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~I4k,  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19925.0APPLICABILITY OFTHECONCLUSIONS PROVIDEDINTHEREVIEWOFTHEVALIDIYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADSGeorgeBienkowski issuedtheresultsofhisreviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,onAugust25,1983(Reference 14).Thereviewconcluded thefollowing:
l.A/E'scouldeliminate the1.15responsefactoronshellstressesiftheyuse4harmonics summedabsolutely addedtotheremaining summedSRSS(inlieuof1.15factoron3harmonics summedabsolutely addedtotheremaining summedSRSS),providedthereportedshellstressesarenotwithinafewpercentoftheallowables, otherwise theissueshouldberevisited.
Theadditionof1harmonic, tobesummedabsolutely, providesonlyabouta10%increaseintheresponses ratherthanthe15%neededtoboundtheFSTFmeasurements.
2.A/E'scouldneglecttheharmoniccomponents above30Hertzforstructures withsimilarnaturalfrequency contenttotheFSTForOysterCreekifspecificjustification intheformoftorusresponsefrequency characteristic ispresented.
3.A/E'scoulduseanyvariation thatproducesatleastashigharatioofresponsetothatproduced, byabsolutesumasthehighestobservedintheFSTFandOysterCreekanalyses(63%).TherefinedshellanalysisoftheNMP-1torusshell,performed byTES,usingthereducedCOloaddefinition includesthefollowing:
1.TheCOloadreduction resulting fromtheFSTFendcaps,17.1%and36.1%fornon-ventandventbays,respectively.
ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING v.r,jl4  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.Thecombination ofindividual harmonicstressesintototalelementstresswasdonebyconsidering frequency contributions at31Hzandbelow.Theactualcombination wasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributors totheSRSScombination oftheothersforshellstress.Thiscombination methodanduseofthe31Hzcutoffaretheresultofextensive numerical evaluation offullscaletestdata.Including thefrequency contribution outto50HzwouldincreasetheCOstressbyabout20psi,orlessthanI/2%.GeorgeBienkowski's reviewoftheRandomPhasingRulesalsoaddressed the,impactoftheendcapsonproducing conservatively measuredCOloads.Thisdiscussion beginsatthebottomofpage3ofthereview.Here,thereviewreferstoanunreferenced communication inReportsSMA12101.04-R002D (Reference 7)andSMA12101.04-R003D (Reference 8),fromDr.AlanBilanin,thatthepresenceofthebulkheads introduces afactorofconservatism ofatleast1.33tothemeasuredCOloadingandresponses fromwhichtheLDRamplitudes
-werederived.Thisisseparatefromthephasingrulesgoverning thesummation ofstressharmonics.
Inaddition, an"Appendix A"ismentioned whereinthiseffectisexamined.
This"Appendix A"isassumedtobeanappendixtoGeorgeBienkowski's reviewandithasnotbeenreviewedbyTESorCDI.ItisstatedthattheAppendixconcludes thatforfrequencies thatarenotcorrelated betweenbays,theFSTFshouldproduce32%to35%higherloadsthanwouldexistinarealfacilityandthatonlythefundamental frequency near6Hzshowsanycorrelation betweendowncomers.
Thereviewfurtherstatesthatifoneassumescorrelation betweenbaysatthatfrequency andrandomphasing(thisisnottherandomphasingofresponsestressharmonics) atallotherfrequencies, theoverallconservatism forIITELEDYNEENGlNEERlNG SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~ck  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992theaveragepressure~abeaslowas17%(notethereviewsays"may"),whileattheresponseleveltheFSTFconservatism willrangefrom18%forhoopstressto38%fortheaxialstress.Theseindependent Brookhaven generated resultsarenotunlikethosethatNNPCiscurrently presenting.
RobertKennedy,inhisreportSMA12101.04-R003D (Reference 8),usesthisadditional 33%conservatism, advancedbyDr.AlanBilanin,toaccountfortheuncertainty ofusingonlythethreepeakresponses fromFSTFtestsH-8,H-llBandM-12.Ontheotherhand,GeorgeBienkowski arguesthatthisuncertainty estimateisprobablyexcessively conservative andthat7%ratherthan33%uncertainty wouldprovideahighconfidence levelofnon-exceedance.
UsingtheabovenumbersfromGeorgeBienkowski's work,wehaveasaminimumthatthemeasuredstressesareconservative byatleast:(1-[(1-.18)(1+.07)])100
=(1-,88)100
=12%Also,nomentionhasbeenmadeinGeorgeBienkowski's reviewregarding theeffectofthe4-8-4downcomer configuration.
ThejointTES/CDIwork(Reference 1)evaluates thiseffectaswell.Sowearelookingfor17%reliefinthe8downcomer baysandtheBrookhaven workshowsatleast12%relief.Thedifference maybeattributed tothe4downcomer baystoeithersideofthe8downcomer bay.Inaddition, the36%reduction thatwehaveevaluated forthe4downcomer baysalsoincludesthefactthatonlyhalfasmanydowncomers arepresentasareintheFSTF,aneffectnotmentioned inGeorgeBienkowski's review.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
,2~gp'f  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Theconservatisms relatedtotheendcapeffectdiscussed hereinwerenotincludedinGeorgeBienkowski's conclusions regarding thephasingrules.Oncetheendcapeffectisincluded, thereisnoreasonwhytheresulting responseshouldboundFSTFdata.Indeed,byitsverynature,itshouldnotboundFSTFdata.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING r1V~wg/  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19926.0NAP-ITORUSSHELLCNTR'SCertified MaterialTestReortReviewforTorusShell(Reference 11)TEShasreviewedtheTorusShellCertified HaterialTestReports(A201GrBFBX).Astatistical analysiswasperformed usingthis(large)sampledatatodetermine the.99confidence intervalestimateofthemeanyieldandultimatestrengthofthismaterial.
TheCoderequiresthattheminimumyieldandminimumultimatestrengthofthematerialbeusedtodetermine theallowable stressintensity (SgC)asfollows:SgCat70'Fisthelessorof1'15SYor1.11SUTherefore, TEShasassumedthattheminimumyieldandultimatestrengths ofthematerialareboundedbyusingtwosamplestandarddeviations fromthestatistically estimated minimummeanvalues.Basedonthecalculations usingtheabovestatedcriteria, theCodeallowable stressintensity wouldbeestimated at:SNC=17600at70'FUseofthisestimated allowable stressintensity willprovideanadditional 1100psireliefascomparedtothepresentCodeallowable of16500psiwhichwasusedduringtheHarkIContainment ProgramanalysisforATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING S',fI  TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,1992thetorusshellmaterialforthefullrangeofanticipated eventtemperatures from70to350'F.Intermsofreliefontheshellthickness requirements, theincreased allowable willprovidejustunder1/32inchesor6/.additional margin.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING qXmy<~),+LC  TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,19927.0RELEVANCE TOSAFETYWedonotviewthisissueasadversely affecting safety.Itcanberegardedastheeffortundertaken toremoveknownconservatisms throughrefinement ofthepostulated appliedCOloads.Inaddition, resolution ofCodeissuespertaining totheallowable materialstrengthandallowable nominalcorrosion, delineated inSection4.0,"Additional Conservatisms",
ifintroduced, wouldprovideforaddedmarginforthetorusshellstresses.
Also,themanyotherconservatisms discussed throughout thisresponse, ifaccounted for,wouldfurtherreducetheshellstress.TorusCorrosion Rate(>)NiagaraHohawkundertook anewcorrosion monitoring programinAugust,1989.Underthisprogram1'3'ridsonall40midbaybottomplateswereUTinspected.
HPRAssociates, Inc.ReportHPR-1152delineates theresultsofthisinspection.
Thesemeasurements didnotshowanysignificant lossduetocorrosion orpittingevenatthenormalwaterlevelregion;andtherewerenowallthickness measurements thatwouldrequireapplication ofthemethodsdescribed inTeledyneReportTR-6801-2, reference 11.HPRquantified theshellthickness loss,over20years,bycomparing themeasuredshellthickness valuestothecalculated originalplatethickness.
Thirtyfourshellplates,traceable totheoriginalmilcertifications, wereusedinthiscomparison.
Originalplatethicknesses werecalculated usingplatedimensions, weightanddensityofthesteel.Thesethicknesses werecomparedtotheUTthickness obtainedinAugust,1989,onthesame34plates.Theresultsindicated anaveragecorrosion lossof0.8milsperyear.Thisratetranslates toatotallossof32milsoraboutI/32"overtheoriginalprojected 40yearplantlife;andcomparescloselytotheratepredicted byRadiological 8ChemicalTechnology, Inc.(RCT),basedonanalysisofsludgesamplesin1979.Duetovariations in(1)Thisinformation providedbyNHPC.ATELEDYNEENGlNEERlNG SERVlCESADIVISIONOFTELEDYNEBROWNENGINEERING Vrl-k  TECHNICAL RESPONSETODOCKETNO.50-220NOVENBER19,1992theoriginalplatedimensions andweights,andmeasurements, onestandarddeviation wasaddedtothe0.8milsperyear.Thisresultedinaconservative prediction of1.26milsperyearcorrosion rate.Additionally, NiagaraMohawkPowerCorporation committed toperformUTmeasurements onasixmonthbasisandprovidetheNRCwiththeresults(Ref.November22,1989,letterC.TerrytoNRC).Sincebaselineestablishment ofthenewcorrosion programof1989,six(6)six-month measurements havebeenconducted, themostrecentofwhichwerejusttakeninSeptember, 1992.Furtheranalysisandtrendingofthesemeasurements indicatethataconservative corrosion rateof1mi-l/yrincluding onestandarddeviation isamorerealistic corrosion ratethanthebaselineestimateof1.26mils/yr.Themostprobableprediction ofcorrosion rateisstill0.8mils/yr,butthelaterresultshavereducedthestandarddeviation to+0.2mils/yr.Thelatest(September, 1992)UTmeasurements, onthethinnesttorusplatesindicates theaveragethickness oftheworstplateis0.453inches.Thisthickness represents anaverageof63individual measurements (calibration adjusted) ona1'3'ridonthatworstplate.Worstcaseindividual measurements onthisorotherplateshavebeenaslowas0.445inches(calibration adjusted).
Overthenextyear,theprojected worstcaselossofthickness wouldbeonemilor0.001".Thiswouldtheoretically reducetheworstgridtoa0.452"averagethickness andtheworstindividual pointto0.444".Theaveragethickness wouldcomplywithminimumthickness allowedbyTeledyneReportTR-6801-2, reference 2,andtheoretically provideforaboutanother5yearsofoperation beforereachingthecurrentminimumthickness allowed.However,the0.444"individual pointwouldhavetobeanalyzedforcompliance toTR-6801-2 bythemethodsoutlinedtherein.Theanalysissubmitted underNHPC'sMay14,1991coverletter(Reference 1),totheNRCsupportsanyaveragethickness orindividual 6TELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19i1992pointdownto0.431".Inaddition, themanyotherconservatisms discussed herein,forwhichnocredithasbeenrequested ortakenintoaccount,wouldsupportreductions inexcessofthis.Therefore, lossofthickness occurring duetoprojected corrosion overthenextyearwouldbewithinlimitsofsupporting analyses.
ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~jlV~Aall~  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,199


==28.0REFERENCES==
==28.0REFERENCES==
1.TESTechnicalReportTR-7353-1,Revision2,"NineMilePointUnit1,ReductioninHarkITorusProgramCondensationOscillationLoadDefinitionandResultingEffectonMinimumShellThicknessRequirements,"datedJanuary14,1992.2.-TESReportTR-5320-1,Rev.1,"HarkIContainmentProgram,Plant-UniqueAnalysisReportoftheTorusSuppressionChamberforNineMilePointUnit1NuclearGeneratingStation,"datedSeptember21,1984.3.G.E.ReportNED0-21888,Rev.2,"MarkIContainmentProgramLoadDefinitionReport,"datedNovember1981.4.G.E.ReportNEDE-24840,"HarkIContainmentProgram-EvaluationofHarmonicPhasingforMarkITorusShellCondensationOscilla-tionLoads,"datedOctober1980.5.G.E.ReportNED0-24574,Rev.1,"HarkIContainmentProgram-Plant-Unique.LoadDefinition-NineMilePoint1NuclearGen-eratingPlant,"datedJuly1981.6.ASMEB&PVCode,SectionIII,Division1throughSummer1977.7.StructuralMechanicsAssociatesReportSHA-12101.04-R002D,"ResponseFactorsAppropriateforUsewithCOHarmonicResponseCombinationDesignRules,"datedMarch1982.8.StructuralMechanicsAssociatesReportSHA-12101.04-R003D,"AStatisticalBasisforLoadFactorsAppropriatefo}UsewithCOHarmonicResponseCombinationDesignRules,"datedMarch1982.ATELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
 
~Q~f':trl<~0  TECHNICALRESPONSETODOCKETNO.50-220NOVEMBER19,199
1.TESTechnical ReportTR-7353-1, Revision2,"NineMilePointUnit1,Reduction inHarkITorusProgramCondensation Oscillation LoadDefinition andResulting EffectonMinimumShellThickness Requirements,"
datedJanuary14,1992.2.-TESReportTR-5320-1, Rev.1,"HarkIContainment Program,Plant-Unique AnalysisReportoftheTorusSuppression ChamberforNineMilePointUnit1NuclearGenerating Station,"
datedSeptember 21,1984.3.G.E.ReportNED0-21888, Rev.2,"MarkIContainment ProgramLoadDefinition Report,"datedNovember1981.4.G.E.ReportNEDE-24840, "HarkIContainment Program-Evaluation ofHarmonicPhasingforMarkITorusShellCondensation Oscilla-tionLoads,"datedOctober1980.5.G.E.ReportNED0-24574, Rev.1,"HarkIContainment Program-Plant-Unique
.LoadDefinition
-NineMilePoint1NuclearGen-eratingPlant,"datedJuly1981.6.ASMEB&PVCode,SectionIII,Division1throughSummer1977.7.Structural Mechanics Associates ReportSHA-12101.04-R002D, "Response FactorsAppropriate forUsewithCOHarmonicResponseCombination DesignRules,"datedMarch1982.8.Structural Mechanics Associates ReportSHA-12101.04-R003D, "AStatistical BasisforLoadFactorsAppropriate fo}UsewithCOHarmonicResponseCombination DesignRules,"datedMarch1982.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING
~Q~f':trl<~0  TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,199


==28.0REFERENCES==
==28.0REFERENCES==
(Cont'd)9.G.E.SupplementarySupportEffort(SSE)ResponseNumber310,datedFebruary8,1982.10.ContinuumDynamicsTechnicalNoteNo.90-11,"ReductionofTorusShellCondensationOscillationHydrodynamicLoadsforNineMilePointUnit1,"datedNovember1990.ll.TESTechnicalReportTR-6801-2,"MarkITorusShellandVentSystemThicknessRequirements,"NineMilePointUnit1NuclearStation,January29,1988,Rev.l.12.HarkIContainmentProgram,StructuralAcceptanceCriteria,PlantUniqueAnalysisApplicationGuide,NED0-24583-1,October1979.13.TESCalculationPackage7353-1,Revision2,"NineNilePointUnit1,ReductioninHarkITorusProgramCondensationOscillationLoadDefinitionandResultingEffectonMinimumShellThicknessRequirements,"datedJanuary14,1992.14."ReviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,"byGeorgeBienkowski,datedAugust25,1983,ContainmentSystemsGroup,DepartmentofNuclearEnergy,BrookhavenNationalLaboratory.15.UnitedStatesNuclearRegulatoryCommission,"SafetyEvaluationbytheOfficeofNuclearReactorRegulationRelatedtoProposedDefermentofTorusModifications,NiagaraMohawkPowerCorporation,NineMilePointNuclearStationUnit1,DocketNo.50-220,"datedAugust25,1992.IIITELEDYNEENGINEERINGSERVICESADIVISIONOFTELEDYNEBROWNENGINEERING gg~g>.g4:}}
 
(Cont'd)9.G.E.Supplementary SupportEffort(SSE)ResponseNumber310,datedFebruary8,1982.10.Continuum DynamicsTechnical NoteNo.90-11,"Reduction ofTorusShellCondensation Oscillation Hydrodynamic LoadsforNineMilePointUnit1,"datedNovember1990.ll.TESTechnical ReportTR-6801-2, "MarkITorusShellandVentSystemThickness Requirements,"
NineMilePointUnit1NuclearStation,January29,1988,Rev.l.12.HarkIContainment Program,Structural Acceptance
: Criteria, PlantUniqueAnalysisApplication Guide,NED0-24583-1, October1979.13.TESCalculation Package7353-1,Revision2,"NineNilePointUnit1,Reduction inHarkITorusProgramCondensation Oscillation LoadDefinition andResulting EffectonMinimumShellThickness Requirements,"
datedJanuary14,1992.14."ReviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,"byGeorgeBienkowski, datedAugust25,1983,Containment SystemsGroup,Department ofNuclearEnergy,Brookhaven NationalLaboratory.
15.UnitedStatesNuclearRegulatory Commission, "SafetyEvaluation bytheOfficeofNuclearReactorRegulation RelatedtoProposedDeferment ofTorusModifications, NiagaraMohawkPowerCorporation, NineMilePointNuclearStationUnit1,DocketNo.50-220,"datedAugust25,1992.IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING gg~g>.g4:}}

Revision as of 03:32, 29 June 2018

Technical Response to SE by NRR Related to Proposed Deferment of Torus Mods, Nmp,Nmpns,Unit 1 Docket 50-220
ML18038A726
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i(TELEDYNEENGINEERING SERVICESADNISIONOFTELEDYNEBROWNENGINEERING 10ForbesRoadWoburn,Massachusetts 01801-2103 617-932-9000 FAX617-932-9970 TECHNICAL RESPONSETOSAFETYEVALUATION BYTHEOFFICEOFNUCLEARREACTORREGULATION RELATEDTOPROPOSEDDEFERMENT OFTORUSNODIFICATIONS NIAGARANOHAWKPOWERCORPORATION NINENILEPOINTNUCLEARSTATIONUNIT1DOCKETNO.50-220NOVENBER19,1992cy211g00182 921123PDRADQCK05000220PDR I

TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992TABLEOFCONTENSUMMARYi~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~o~~~~o~~~~~~~S1.0BACKGROUND..................................................

2.0 COLOADDEFINITION

CONSERVATISMS............................

2.1FSTFCONSERVATI SMS2.1.1FSTFENDCAPS................................

2.1.2FSTFSTRUCTURAL DAMPING......................

2.2LDRCONSERVATISMS......................................

2.2.1HARMONICCOMPONENT AMPLIFICATION.............

2.2.2SUMMINGOFHARMONICCOMPONENTS...............

3.0 TESCOLOADREDUCTION

-STRUCTURAL MODEL/SHELL ANALYSIS.....

4.0 ADDITIONAL

CONSERVATISMS....................................

5.0 APPLICABILITY

OFTHECONCLUSIONS PROVIDEDINTHEREVIEWOFTHEVALIDITYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADS..........

6.0NMP-1TORUSSHELLCMTR'S7.0RELEVANCE TOSAFETY..8.0REFERENCE...................................................

~Pae121820236TELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING PI0 TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992SUMMARYTheNRCSafetyEvaluation Report(SER)discusses twomethodsofobtaining reliefintheevaluation forcondensation oscillation (CO)loads.Thefirstmethodistocombinethe31stressharmonics bytakingtheabsolutesumofthe4peakresponses andaddingtothisthesquarerootofthesumofthesquares(SRSS)oftheremaining 27harmonics.

Thismethodhasbeenpreviously acceptedbytheNRC.Thesecondmethodistoincorporate theanalytically determined COpressurereduction factorspresented inNiagaraMohawkPowerCorporation's recent,andsubjectsubmittal, reference 1.TheSERadvisesthatthereviewtheyhavedonesofarsupportsthepositionthatoneortheotherofthetwoapproaches maybeused,butnotboth.Thatis,ifcreditistakenfortherecentlydeveloped COpressurereduction, thenall31stressharmonics mustbecombinedbyabsolutesummation, ratherthanusingtherandomphasingrulespreviously approvedfortheMarkITorusProgram.TheCOpressurereduction represents newandadditional reliefanditsuseshouldnotprohibitusingthealreadyestablished reliefgainedfromtherandomphasingofthestressharmonics sincethetwoanalysesareindependent ofeachother.Theworkpresented inreference 1usestheContinuum

Dynamics, Inc.COpressurereduction resultsandcombinesthe31stressharmonics byabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining 27harmonics.

TheCOpressurereductionworkreducestheCOstressesbyapproximately 17%and36%fortheeightandfourdowncomer bays,respectively.

Absolutesummingthe4peakstressharmonics andaddingtothistheSRSSoftheremaining 27stressharmonics resultsinanestimated 33%lowerstressthanabsolutesummingalltheindividual harmonics.

Conversely ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING e"4d',f TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992stated,absolutesummingalltheindividual stressharmonics overpredictsmeasuredstressesbyabout50%.Themethodofcombining thestressharmonics byabsolutesummingthe4peaksandaddingtothistheSRSSoftheremaining 27stressharmonics wastheresultofextensive structural analysisdonefortheoriginaltorusprogramandwasrecognized astheappropriate waytocorrelate FullScaleTestFacility(FSTF)measuredstresseswithFSTFanalytically predicted stresses.

Thismethodwasavailable forallplantstouse,notjustNineMilePointUnit1(NMP-1),anditisstillvalid.TheCOpressurereduction accountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomers andthehydrodynamics ineachbayareinphase.Thisisadifferent, andindependent, phenomenon thantheunderlying basistothemethodofcombining stressharmonics discussed inthepreceding paragraph.

TheBrookhaven attachment totheSERagreesthattheendcapeffectisanFSTFconservatism.

Theattachment doesnotquantifytheconservatism.

NRC-acceptance of-thereduced-CO.loading addressed hereingains-NMP-1areliefof573psiintheeightdowncomer bays,and1565psiinthefourdowncomer bays.Toseethatthisstressreduction isnominal,thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING C

I\

TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19921.0BACKGROUND TheMarkIProgramGeneralElectric(GE)determined themagnitude oftheCondensation Oscillation (CO)loadingbasedonthetestresultsfromtheFullScaleTestFacility(FSTF).TheFSTFfacilitywasonebaywithendcapstocontainthefluid,andasaresultofthecompromises intestfacilitydesign,theseendcapscausedconservative COshellpressures tobemeasured.

TheCOloaddefinition, basedonthesemeasuredpressures, wasconservative ontheorderof15to30percentandthiswasrecognized atthattime.TheMarkIOwners'roup determined itwouldnotbecosteffective tofundtheanalysisanddocumentation effortnecessary toachievefurtherreduction intheCOloaddefinition sincemostoftheMarkIplantshadadequatemarginonCodestressallowables fortheCOfrequency domaineventcombination loading.However,theNineMilePointUnit1(NHP-1)torushasathinshell(0.460in.)comparedwithmostofHarkIplants,andasaresult,thepostulated eventcombination whichincludesDesignBreak/Accident (DBA)pressureandCO(eventcombination 20)controlsthemarginontorusshellthickness.

TeledyneEngineering Services(TES)andNiagaraMohawkPowerCorporation (NHPC)recognized thisproblemasbeingcriticalearlyintheHarkIprogram,andjointlytookthenecessary stepstomitigateloadsfromthiseventcombination.

First,TESrefinedtheTorusAnalysisforDBApressureandCOincluding thepostprocessing ofresults.Then,TESandNMPCinitiated aseriesofthinshellmeetingsatGEforNHP-1andOysterCreek.Thesemeetingsidentified areasofconservatism intheloaddefinition tobefurtherexploredbyGE.The,reduction inNHP-1DBApressureresulting fromthesemeetingswasessential tothesuccessful compliance ofNMP-1totheHarkIProgramStructural Acceptance CriteriafortheCOeventcombination.

TheDBApressure, ratherthantheCOloadingconservatisms, wereaddressed basedoncostandtimeconsiderations.

ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~I~P~+ TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.0COLOADDEFINITION CONSERVATISMS TheloadsonwhichtheTESstructural analysisisbasedarepresented primarily inG.E.ReportNED0-21888, MarkIContainment ProgramLoadDefinition Report(LDR),datedNovember1981(Reference 3).Theseloadsweredeveloped fromtheFSTFduringtheHarkIProgramandhaveinherentconservatisms.

2.1FSTFCONSERVATISHS Therearetwomajorconservatisms inherenttothegeometryoftheFSTF,theyaretheFSTFbayendcapsandthestructural dampingassociated withthelowlevelofstressintheFSTFshell.2.1.1FSTFENDCAPSIn1979,Continuum

Dynamics, Inc.(CDI)wasaskedbytheMarkIownersgroup,throughG.E.,toassesstheconservatism intheCondensation Oscillation torusloadsmeasuredduringtheFSTFblowdowntests.Thiseffortconfirmed generally acceptedconservatism inthetestswithregardtotestinitialcondition thermodynamics, andidentified asignificant conservatism whichwasnotidentified duringtestdesign.Thisconservatism wasintroduced bythegeometryofthetestfacility, one-sixteenth sectorwhichisequivalently a22-1/2'egment oftheMarkIPressureSuppression PoolTorus.Thetestfacility, althoughfull-scale incrosssection,attempted tosimulateatfull-scale thecondensation phenomenon inonebayonly.Endcapswererequiredtocontainthepoolwaterandtheairspaceabovethepoolinthebay.Theanalysis, whichanalyzesthehydrodynamic consequences oftheseendcaps,waspresented totheHarkIownersin1980.Toexpeditecompletion ofthisissue,theMarkIownersdecidednottopursuereducingthisconservatism atthattime.Thisworkisrevisited forthiseffortanddeveloped specifically forNineMilePointUnitl.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING P0l>> TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992ThejointTESandCDIeffortpresented inReferences 1810andsummarized hereinconsistsofananalytical reduction intheHarkITorusProgramCondensation Oscillation LoadDefinition.

Theanalysisshowsthattheeightdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast19%atfrequencies otherthan5-6Hzandforfourdowncomer bays,thebayaveragedCOloadsareconservative byatleast38%atfrequencies otherthan5-6Hz.Theloadconservatisms inthe5-6Hzfrequency bandare6%and28%fortheeightandfourdowncomer bays,respectively.

Takingallfrequency bands(0to31Hz)intoaccountresultsinanetCOloaddefinition conservatism of17.1%and36.1%fortheeightdowncomer (non-vent) andfourdowncomer (vent)bays,respectively.

2.1.2FSTFSTRUCTURAL DAMPINGDampingequalto2percentwasusedintheevaluations performed todevelopthephasingrules.Theassumption of2percentdamping,whichisappropriate fordesignresponses fromcombinedloadsnearone-halfyieldstress,maybetoohighforthelowlevelFSTFresponse.

Ifthedampingusedwereonly1.5percent,the-harmonic, responseamplitudes usedtodevelopthephasingruleswouldbesignificantly largersuchthatthecombinedcalculated responseusingtheabsolutesumofthe4peakresponses andaddingtothistheSRSSoftheremainder, wouldbeconservative comparedtothemeasuredresponse.

Inotherwords,usingtheabsolutesumoflessthanthe4peakresponses, perhapsthe3peakresponses, plustheSRSSoftheremainder, mayhaveboundedthemeasuredresponse.

Inourjudgement, dampingontheorderof1.5percentwouldbemoreappropriate forFSTFresponselevelsthan2percent.Itmustbeemphasized thatdampingof2percentismoreappropriate fordesignanalysesinwhichstresslevelsofone-halfyieldareallowable.

O'TELEDYNE ENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING J~I1

~i'ECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.2LDRCONSERVATISMS Therearetwoconservatisms associated withthedevelopment oftheLDR,G.E.ReportNEDO-21888 (Reference 3).Thefirstconservatism isrelatedtotheamplification oftheindividual harmoniccomponents beforecombining thecomponents andthesecondconservatism isrelatedtothemethodusedtocombineorsumtheindividual harmonicstresscomponents.

2.2.1HARMONICCOMPONENT AMPLIFICATION ForFSTFtheresponseamplification factorsateach0.914Hzfrequency intervalwereusedinlieuoftheresponseamplification factorsatthestructural naturalfrequencies ineach1-Hzwindow(References 4,758).Thephasingrulesweredeveloped withthisreducedresponse.

Suchanapproachdoesnotintroduce theconservatism inresponsecalculation whichisobtainedwhenaccounting fortheresponseamplification factorsatthestructural naturalfrequencies ineach1-Hzwindow.Nocreditisgivenforthelatterapproach.

2.2.2SUMMINGOFHARMONICCOMPONENTS TheLDR(Reference 3)statesthatthecombination of'individual harmonicstresscomponents shallbesummed.Threeacceptable methodsareavailable:

1.Absolutesumofallharmoniccomponents.

2.Absolutesumofthe3highestpeaksaddedtotheSRSSoftheremaining components andapplya1.15factor.3.Absolutesumofthe4highestpeaksaddedtotheSRSSoftheremaining components, providedthereportedshellstressesarenotwithinafewpercentoftheallowables.

iTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~I~1JI1g,,1I TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,1992Theconservatisms associated withthesemethodsarebasedontheboundingofthemeasuredFSTFtestshellstressresults(TestNo'sH-8,H-llBandH-12).Hethods1and2boundallthreetests,whilemethod3fallsjustshortofboundingtestH-lR.IITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~rII TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19923.0TESCOLOADREDUCTION

-STRUCTURAL MODELSHELLANALYSISOscillating loadsonthesubmerged portionofthetorusshellduringtheCOphenomenon arecausedbyperiodicoscillations superimposed ontheprevailing localstaticpressures.

PlantuniqueloadsarederivedfromFSTFdata.FlexiblewallloadsweremeasureddirectlyintheFSTFwhichisprototypical ofMarkIplantconfigurations withtheexception oftherigidendcaps.Pressuremeasurements obtainedfromvariouslocations onthetorusshellshowthatthelongitudinal pressureoscillation amplitude distribution alongthetorusbottomcenterlineisessentially uniformfortheFSTF.Specification ofabaselinerigidwallloadisgivenaspressureoscillation amplitude asafunctionoffrequency.

ThisloadhasbeenderivedfromthemeasuredFSTFflexiblewallloadbyanalysiswithacoupledfluid-structural dynamicmodeloftheFSTFtorus.Thederivation ofthebaselinerigidwallloadisdescribed below:a.Afiniteelementcoupledfluid-structural dynamicmodeloftheFSTFtoruswasexcitedatvaryingfrequencies withaunitamplitude pressuresourceattheventexits.Thetorusshellpressureamplitudes relativetothesourcepressure(amplification factors)weredetermined asafunctionoffrequency.

b.Usingtheserelativeamplitudes (amplification factors),

theFSTFventexitsourcepressures werederivedfromthemeasuredtorusshellpressures atthevariousfrequencies.

c.ThebaselinerigidwallloadwasderivedfromthecomputedFSTFventexitsourcepressures byhydrodynamic analysis.

IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~I4,l TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992TheCOshellloadisspecified asadistribution ofharmonicpressureamplitudes in1Hzbands(Reference 3).Theanalysisforthisloadwasperformed byconsidering theeffectofunitloadsateachloadfrequency (harmonic analysis) andthenscalingandcombining theindividual frequency effectstodetermine totalstressatthecriticalelement.Thethreevariations intheCOspectrum(Reference 3)wereevaluated byrescaling theresultsoftheunitloadanalysis.

100%ofwatermasswasusedforallCOanalysis.

Thereduction factorspresented inTable1ofReference 10wereappliedtotheindividual harmonicpressures.

Thecombination ofindividual harmonicstressesintototalelementstresswasdonebyconsidering frequency contributions at31Hzandbelow.Theactualcombination wasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributors totheSRSScombination oftheothersforshellstress.Thiscombination methodanduseofthe31Hzcutoffaretheresultofextensive structural evaluation offullscaletestdata,whichisreportedanddiscussed inReferences 4and7.Including thefrequency contribution outto50HzwouldincreasetheCOstressbyabout20psi,orlessthan1/2%.Themethodofcombining thestressharmonics bytheabsolutesumofthe4peaksplustheSRSSoftheremainder wastheresultofextensive structural analysisdonefortheoriginaltorusprogramandwasrecognized astheappropriate waytocorrelate FSTFmeasuredstresseswithFSTFanalytically predicted stressesusingtheloaddefinition.

Touseabsolutesumofallthecomponents wouldbetoignorethephasingbetweenfrequency dependent pressurecomponents andbetweenfrequency dependent structural responses, andtoassumephasingbetweentheharmoniccomponents toproducethehighestpossiblestressresponse.

Themethodofcombining thestressharmonics bytheabsolutesumofthe4peaksplustheSRSSoftheremainder wasavailable forallplantstouse,notjustNMP-1,andtodayremainsvalid.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING l~'I,,~)I TECHNICAL RESPONSETODOCKETNO.50-220NOVENBER19,1992Thepresentanalysis(References 1510)investigates theconservatism ofthehydrodynamic torusCOloaddefinition derivedfromdatatakenintheHarkIFSTF.ItisshownthatduringCO,thecondensation eventsatthedowncomer exitsare,asafunctionoffrequency, randominphaseformostharmoniccomponents.

Asaconsequence ofthisobservation, andthegeometrical constraints builtintotheFSTF,theCOloadsdefinition appliedtoNHP-Iisconservative fortworeasons.~Alternate downcomer baysinNHP-Ihavefour-eight-four-eight, etc.,downcomers perbay.TheFSTFfacility, byconstruction, assumesthatallbayshaveeightdowncomers perbay.TheFSTFmodeleda22I/2'ector ofaprototypical HarkIsuppression chamber.Thewaterwascontained inthesectorbytwoveryrigidendcapswhichwouldnotexistinafullsuppression chamber.Theseendcapshydrodynamically actasmirrors.Thisresultsinameasuredload,asifallbaysinafulltorushadcondensation phenomenon identical inphaseandamplitude, totheinstrumented FSTFbay.TheanalysisshowsthatforNHP-I:~Eightdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast19%atfrequencies otherthan5-6Hz.~Fourdowncomer bayshavebayaveragedCOloadswhichareconservative byatleast38%atfrequencies otherthan5-6Hz.Thepresentwork(Reference 1)accountsforboththerandomphasingofthestressharmonics andthereduction inFSTFmeasuredpressures, twoindependent phenomena.

ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING rll~A v,TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Inclusion ofthereducedCOloadingaddressed hereingainsNHP-Iareliefof573psiintheeightdowncomer bays,and1565psiinthefourdowncomer bays.Thesevaluesaretobecomparedtoatotalcombinedstressfromallsourcesontheorderof16,025psi.TheCOloadreduction accountsfortheendcapeffectoftheFSTFinmakingitappearthatallbayshaveeightdowncomers andthehydrodynamics ineachbayisinphasewithadjoining bays.IntheBrookhaven attachment totheSER(Reference 15)itisstatedthattheendcapsintroduce anFSTFconservatism.

made:Onpage3oftheBrookhaven attachment, thefollowing pointsareTheFSTFdatasupportthenotionthattheCOprocessisrandomovermostofthefrequency spectrumconsidered intheloadmethods.Becauseofthegeometric differences, particularly the4-8-4downcomer arrangement, thepressureloadsduringCOblowdownwilltendtobegreaterintheFSTFrelativetotheNHPtorusforthesamehydrodynamic flowconditions.

~Theprocedure usedtoquantifytheseeffectsrepresents astraightforwardapplication ofaconventional hydrodynamic method.Theresultsarereasonable andprobablyconservative becauseofthehighsoundspeedusedinthenumerics.

Wealsoconsidertheassumption thatacorrelation existsbetweenbaystobeasignificant conservatism.

ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 0'i~ TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Theattachment itselfdoesnotquantifytheseconservatisms.

However,GeorgeBienkowski's reviewoftheRandomPhasingRules,datedAugust25,1983(Reference 14),alsoincludessomequantification oftheseeffects.Thisisdiscussed inSection5.0herein.IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING It.JI TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19924.0ADDITIONAL CONSERVATISHS Thefollowing isadelineation ofadditional conservatisms forwhichnocredithasbeentaken.1.Uniformcorrosion oftheshellwouldcausethefrequencies todropandtheresponsetoCOloadtodecrease.

Ifthefrequencies drop1Hz,thenitisestimated thatNMP-1wouldgainabout600psireliefinshellstress.2.Theanalysishasbeenperformed using2%damping.Itisestimated thatincreasing thedampingto4%,toaccountforwater/structure damping,wouldgainNHP-1morethan900psirelief.Even4%dampingmaybelowforathinshelledwaterfilledstructure.

3.Thehighsoundspeedusedinthedetermination oftheCOloadreduction factorsisconservative asisshowninReference 10.4.Curvature effectsofthetorus.5.TheASHECodeallowsauniform10%reduction inwallthickness forClassMCComponents, 1990Addenda,SectionXI,Paragraph IWE-3519.3.

Thisisthesameasallowinga10%increaseinthematerialallowables.

6.TheASMECode,SectionIII,Paragraph Nf-3213.10,permitsuptoI/16inchlocalcorrosion asisexplained inTESTechnical ReportTR-6801-2 (Reference ll).7.Class1allowables forthismaterialaregreaterthanClassHCallowables by21%,Sm=20ksiforClass1vs.Sm=16.5ksiforClassHC.HTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

]tI~i4VjW TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19$19928.Certified HaterialTestReports(CHTR's)fortheNHP-1shellmaterialindicatehigherallowables thanthoseusedintheHarkIProgramAnalysis, 17.6ksivs.16.5ksi(seeSection6.0).Ifitbecomesnecessary tousetheCHTR's,hardnesstestscouldbeperformed onthetorusshelltoincreaseconfidence inthematerialCHTR's.9.Thereisinherentconservatism inthefactorofsafety(FS)associated withthecode,FS=1/(1.lxl/4)=3.64onultimatematerialstrength.

ItTELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~I4k, TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19925.0APPLICABILITY OFTHECONCLUSIONS PROVIDEDINTHEREVIEWOFTHEVALIDIYOFRANDOMPHASINGRULESASAPPLIEDTOCOTORUSLOADSGeorgeBienkowski issuedtheresultsofhisreviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,onAugust25,1983(Reference 14).Thereviewconcluded thefollowing:

l.A/E'scouldeliminate the1.15responsefactoronshellstressesiftheyuse4harmonics summedabsolutely addedtotheremaining summedSRSS(inlieuof1.15factoron3harmonics summedabsolutely addedtotheremaining summedSRSS),providedthereportedshellstressesarenotwithinafewpercentoftheallowables, otherwise theissueshouldberevisited.

Theadditionof1harmonic, tobesummedabsolutely, providesonlyabouta10%increaseintheresponses ratherthanthe15%neededtoboundtheFSTFmeasurements.

2.A/E'scouldneglecttheharmoniccomponents above30Hertzforstructures withsimilarnaturalfrequency contenttotheFSTForOysterCreekifspecificjustification intheformoftorusresponsefrequency characteristic ispresented.

3.A/E'scoulduseanyvariation thatproducesatleastashigharatioofresponsetothatproduced, byabsolutesumasthehighestobservedintheFSTFandOysterCreekanalyses(63%).TherefinedshellanalysisoftheNMP-1torusshell,performed byTES,usingthereducedCOloaddefinition includesthefollowing:

1.TheCOloadreduction resulting fromtheFSTFendcaps,17.1%and36.1%fornon-ventandventbays,respectively.

ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING v.r,jl4 TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19922.Thecombination ofindividual harmonicstressesintototalelementstresswasdonebyconsidering frequency contributions at31Hzandbelow.Theactualcombination wasdonebyaddingtheabsolutevalueofthefourhighestharmoniccontributors totheSRSScombination oftheothersforshellstress.Thiscombination methodanduseofthe31Hzcutoffaretheresultofextensive numerical evaluation offullscaletestdata.Including thefrequency contribution outto50HzwouldincreasetheCOstressbyabout20psi,orlessthanI/2%.GeorgeBienkowski's reviewoftheRandomPhasingRulesalsoaddressed the,impactoftheendcapsonproducing conservatively measuredCOloads.Thisdiscussion beginsatthebottomofpage3ofthereview.Here,thereviewreferstoanunreferenced communication inReportsSMA12101.04-R002D (Reference 7)andSMA12101.04-R003D (Reference 8),fromDr.AlanBilanin,thatthepresenceofthebulkheads introduces afactorofconservatism ofatleast1.33tothemeasuredCOloadingandresponses fromwhichtheLDRamplitudes

-werederived.Thisisseparatefromthephasingrulesgoverning thesummation ofstressharmonics.

Inaddition, an"Appendix A"ismentioned whereinthiseffectisexamined.

This"Appendix A"isassumedtobeanappendixtoGeorgeBienkowski's reviewandithasnotbeenreviewedbyTESorCDI.ItisstatedthattheAppendixconcludes thatforfrequencies thatarenotcorrelated betweenbays,theFSTFshouldproduce32%to35%higherloadsthanwouldexistinarealfacilityandthatonlythefundamental frequency near6Hzshowsanycorrelation betweendowncomers.

Thereviewfurtherstatesthatifoneassumescorrelation betweenbaysatthatfrequency andrandomphasing(thisisnottherandomphasingofresponsestressharmonics) atallotherfrequencies, theoverallconservatism forIITELEDYNEENGlNEERlNG SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING 1~ck TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992theaveragepressure~abeaslowas17%(notethereviewsays"may"),whileattheresponseleveltheFSTFconservatism willrangefrom18%forhoopstressto38%fortheaxialstress.Theseindependent Brookhaven generated resultsarenotunlikethosethatNNPCiscurrently presenting.

RobertKennedy,inhisreportSMA12101.04-R003D (Reference 8),usesthisadditional 33%conservatism, advancedbyDr.AlanBilanin,toaccountfortheuncertainty ofusingonlythethreepeakresponses fromFSTFtestsH-8,H-llBandM-12.Ontheotherhand,GeorgeBienkowski arguesthatthisuncertainty estimateisprobablyexcessively conservative andthat7%ratherthan33%uncertainty wouldprovideahighconfidence levelofnon-exceedance.

UsingtheabovenumbersfromGeorgeBienkowski's work,wehaveasaminimumthatthemeasuredstressesareconservative byatleast:(1-[(1-.18)(1+.07)])100

=(1-,88)100

=12%Also,nomentionhasbeenmadeinGeorgeBienkowski's reviewregarding theeffectofthe4-8-4downcomer configuration.

ThejointTES/CDIwork(Reference 1)evaluates thiseffectaswell.Sowearelookingfor17%reliefinthe8downcomer baysandtheBrookhaven workshowsatleast12%relief.Thedifference maybeattributed tothe4downcomer baystoeithersideofthe8downcomer bay.Inaddition, the36%reduction thatwehaveevaluated forthe4downcomer baysalsoincludesthefactthatonlyhalfasmanydowncomers arepresentasareintheFSTF,aneffectnotmentioned inGeorgeBienkowski's review.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

,2~gp'f TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,1992Theconservatisms relatedtotheendcapeffectdiscussed hereinwerenotincludedinGeorgeBienkowski's conclusions regarding thephasingrules.Oncetheendcapeffectisincluded, thereisnoreasonwhytheresulting responseshouldboundFSTFdata.Indeed,byitsverynature,itshouldnotboundFSTFdata.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING r1V~wg/ TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,19926.0NAP-ITORUSSHELLCNTR'SCertified MaterialTestReortReviewforTorusShell(Reference 11)TEShasreviewedtheTorusShellCertified HaterialTestReports(A201GrBFBX).Astatistical analysiswasperformed usingthis(large)sampledatatodetermine the.99confidence intervalestimateofthemeanyieldandultimatestrengthofthismaterial.

TheCoderequiresthattheminimumyieldandminimumultimatestrengthofthematerialbeusedtodetermine theallowable stressintensity (SgC)asfollows:SgCat70'Fisthelessorof1'15SYor1.11SUTherefore, TEShasassumedthattheminimumyieldandultimatestrengths ofthematerialareboundedbyusingtwosamplestandarddeviations fromthestatistically estimated minimummeanvalues.Basedonthecalculations usingtheabovestatedcriteria, theCodeallowable stressintensity wouldbeestimated at:SNC=17600at70'FUseofthisestimated allowable stressintensity willprovideanadditional 1100psireliefascomparedtothepresentCodeallowable of16500psiwhichwasusedduringtheHarkIContainment ProgramanalysisforATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING S',fI TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,1992thetorusshellmaterialforthefullrangeofanticipated eventtemperatures from70to350'F.Intermsofreliefontheshellthickness requirements, theincreased allowable willprovidejustunder1/32inchesor6/.additional margin.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING qXmy<~),+LC TECHNICAL RESPONSETODOCKETNO.50-220NOVEHBER19,19927.0RELEVANCE TOSAFETYWedonotviewthisissueasadversely affecting safety.Itcanberegardedastheeffortundertaken toremoveknownconservatisms throughrefinement ofthepostulated appliedCOloads.Inaddition, resolution ofCodeissuespertaining totheallowable materialstrengthandallowable nominalcorrosion, delineated inSection4.0,"Additional Conservatisms",

ifintroduced, wouldprovideforaddedmarginforthetorusshellstresses.

Also,themanyotherconservatisms discussed throughout thisresponse, ifaccounted for,wouldfurtherreducetheshellstress.TorusCorrosion Rate(>)NiagaraHohawkundertook anewcorrosion monitoring programinAugust,1989.Underthisprogram1'3'ridsonall40midbaybottomplateswereUTinspected.

HPRAssociates, Inc.ReportHPR-1152delineates theresultsofthisinspection.

Thesemeasurements didnotshowanysignificant lossduetocorrosion orpittingevenatthenormalwaterlevelregion;andtherewerenowallthickness measurements thatwouldrequireapplication ofthemethodsdescribed inTeledyneReportTR-6801-2, reference 11.HPRquantified theshellthickness loss,over20years,bycomparing themeasuredshellthickness valuestothecalculated originalplatethickness.

Thirtyfourshellplates,traceable totheoriginalmilcertifications, wereusedinthiscomparison.

Originalplatethicknesses werecalculated usingplatedimensions, weightanddensityofthesteel.Thesethicknesses werecomparedtotheUTthickness obtainedinAugust,1989,onthesame34plates.Theresultsindicated anaveragecorrosion lossof0.8milsperyear.Thisratetranslates toatotallossof32milsoraboutI/32"overtheoriginalprojected 40yearplantlife;andcomparescloselytotheratepredicted byRadiological 8ChemicalTechnology, Inc.(RCT),basedonanalysisofsludgesamplesin1979.Duetovariations in(1)Thisinformation providedbyNHPC.ATELEDYNEENGlNEERlNG SERVlCESADIVISIONOFTELEDYNEBROWNENGINEERING Vrl-k TECHNICAL RESPONSETODOCKETNO.50-220NOVENBER19,1992theoriginalplatedimensions andweights,andmeasurements, onestandarddeviation wasaddedtothe0.8milsperyear.Thisresultedinaconservative prediction of1.26milsperyearcorrosion rate.Additionally, NiagaraMohawkPowerCorporation committed toperformUTmeasurements onasixmonthbasisandprovidetheNRCwiththeresults(Ref.November22,1989,letterC.TerrytoNRC).Sincebaselineestablishment ofthenewcorrosion programof1989,six(6)six-month measurements havebeenconducted, themostrecentofwhichwerejusttakeninSeptember, 1992.Furtheranalysisandtrendingofthesemeasurements indicatethataconservative corrosion rateof1mi-l/yrincluding onestandarddeviation isamorerealistic corrosion ratethanthebaselineestimateof1.26mils/yr.Themostprobableprediction ofcorrosion rateisstill0.8mils/yr,butthelaterresultshavereducedthestandarddeviation to+0.2mils/yr.Thelatest(September, 1992)UTmeasurements, onthethinnesttorusplatesindicates theaveragethickness oftheworstplateis0.453inches.Thisthickness represents anaverageof63individual measurements (calibration adjusted) ona1'3'ridonthatworstplate.Worstcaseindividual measurements onthisorotherplateshavebeenaslowas0.445inches(calibration adjusted).

Overthenextyear,theprojected worstcaselossofthickness wouldbeonemilor0.001".Thiswouldtheoretically reducetheworstgridtoa0.452"averagethickness andtheworstindividual pointto0.444".Theaveragethickness wouldcomplywithminimumthickness allowedbyTeledyneReportTR-6801-2, reference 2,andtheoretically provideforaboutanother5yearsofoperation beforereachingthecurrentminimumthickness allowed.However,the0.444"individual pointwouldhavetobeanalyzedforcompliance toTR-6801-2 bythemethodsoutlinedtherein.Theanalysissubmitted underNHPC'sMay14,1991coverletter(Reference 1),totheNRCsupportsanyaveragethickness orindividual 6TELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19i1992pointdownto0.431".Inaddition, themanyotherconservatisms discussed herein,forwhichnocredithasbeenrequested ortakenintoaccount,wouldsupportreductions inexcessofthis.Therefore, lossofthickness occurring duetoprojected corrosion overthenextyearwouldbewithinlimitsofsupporting analyses.

ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~jlV~Aall~ TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,199

28.0REFERENCES

1.TESTechnical ReportTR-7353-1, Revision2,"NineMilePointUnit1,Reduction inHarkITorusProgramCondensation Oscillation LoadDefinition andResulting EffectonMinimumShellThickness Requirements,"

datedJanuary14,1992.2.-TESReportTR-5320-1, Rev.1,"HarkIContainment Program,Plant-Unique AnalysisReportoftheTorusSuppression ChamberforNineMilePointUnit1NuclearGenerating Station,"

datedSeptember 21,1984.3.G.E.ReportNED0-21888, Rev.2,"MarkIContainment ProgramLoadDefinition Report,"datedNovember1981.4.G.E.ReportNEDE-24840, "HarkIContainment Program-Evaluation ofHarmonicPhasingforMarkITorusShellCondensation Oscilla-tionLoads,"datedOctober1980.5.G.E.ReportNED0-24574, Rev.1,"HarkIContainment Program-Plant-Unique

.LoadDefinition

-NineMilePoint1NuclearGen-eratingPlant,"datedJuly1981.6.ASMEB&PVCode,SectionIII,Division1throughSummer1977.7.Structural Mechanics Associates ReportSHA-12101.04-R002D, "Response FactorsAppropriate forUsewithCOHarmonicResponseCombination DesignRules,"datedMarch1982.8.Structural Mechanics Associates ReportSHA-12101.04-R003D, "AStatistical BasisforLoadFactorsAppropriate fo}UsewithCOHarmonicResponseCombination DesignRules,"datedMarch1982.ATELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING

~Q~f':trl<~0 TECHNICAL RESPONSETODOCKETNO.50-220NOVEMBER19,199

28.0REFERENCES

(Cont'd)9.G.E.Supplementary SupportEffort(SSE)ResponseNumber310,datedFebruary8,1982.10.Continuum DynamicsTechnical NoteNo.90-11,"Reduction ofTorusShellCondensation Oscillation Hydrodynamic LoadsforNineMilePointUnit1,"datedNovember1990.ll.TESTechnical ReportTR-6801-2, "MarkITorusShellandVentSystemThickness Requirements,"

NineMilePointUnit1NuclearStation,January29,1988,Rev.l.12.HarkIContainment Program,Structural Acceptance

Criteria, PlantUniqueAnalysisApplication Guide,NED0-24583-1, October1979.13.TESCalculation Package7353-1,Revision2,"NineNilePointUnit1,Reduction inHarkITorusProgramCondensation Oscillation LoadDefinition andResulting EffectonMinimumShellThickness Requirements,"

datedJanuary14,1992.14."ReviewoftheValidityofRandomPhasingRulesasAppliedtoCOTorusLoads,"byGeorgeBienkowski, datedAugust25,1983,Containment SystemsGroup,Department ofNuclearEnergy,Brookhaven NationalLaboratory.

15.UnitedStatesNuclearRegulatory Commission, "SafetyEvaluation bytheOfficeofNuclearReactorRegulation RelatedtoProposedDeferment ofTorusModifications, NiagaraMohawkPowerCorporation, NineMilePointNuclearStationUnit1,DocketNo.50-220,"datedAugust25,1992.IIITELEDYNEENGINEERING SERVICESADIVISIONOFTELEDYNEBROWNENGINEERING gg~g>.g4: