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{{#Wiki_filter:ATTACHMENT4TOAEP'NRC'1067PROPOSEDREVISEDTECHNICALSPECIFICATIONPAGESSSi01904078S10i4PDRADGCK050003i5PpHO DEPMEMBERSOFTHEPUBLIC1.35MEMBER(S)OFTHEPUBLICshallincludeallpersonswhoarenotoccupationallyassociatedwiththeplant.Thiscategorydoesnotincludeemployeesoftheutility,itscontractorsoritsvendors'lsoexcludedfromthiscategoryarepersonswhoenterthesitetoserviceequipmentortomakedeliveries.Thiscategorydoesincludepersonswhouseportionsofthesiteforrecreational,occupationalorotherpurposesnotassociatedwiththeplant.SITEBOUNDARY1.36TheSITEBOUNDARYshallbethatlinebeyondwhichthelandisnotowned,leasedorotherwisecontrolledbythelicensee.UNRESTRICTEDAREA1.37AnUNRESTRICTEDAREAshallbeanyareaatorbeyondtheSITEBOUNDARYtowhichaccessisnotcontrolledbythelicenseeforpurposesofprotectionofindividualsfromexposuretoradiationandradioactivematerialsoranyareawithinthesiteboundaryusedforresidentialquartersorindustrial,commercial,institutionaland/orrecreationalpurposes.ALLOWABLEPOWERLEVELAPL1.38APLmeans"allowablepowerlevel"whichisthatpowerlevel,lessthanorequalto100%RATEDTHERMALPOWER,atwhichtheplantmaybeoperatedtoensurethatpowerdistributionlimitsaresatisfied.COOKNUCLEARPLANTUNIT11-7AMENDMENTNO.
{{#Wiki_filter:ATTACHMENT 4 TO AEP'NRC'1067 PROPOSED REVISED TECHNICAL SPECIFICATION PAGES SSi0190407 8S10i4 PDR  ADGCK 050003i5 P              pHO
THISPAGEINTENTIONALLYLEFTBLANKCOOKNUCLEARPLANTUNIT11-10AMENDMENTNO.
 
670650CQWa630UNACCPTABLEOPERATION24OPSIA25QPSI2100SIA610200PSI590O570]775PSIAACCEPTABLEOPERTIONPRESSURE(PS~IA177520002100225024000.00.20.40.60.81.0FRACTIONOFRATEDTHERMALPOWERBREAKPCWTSCTIONRATEDTl+RMALPOTAVG8DEGREES(0.0,617.1),(1.16,584.5),(1.20,579.7)(0.0,633.5),(1.11,603.9),(1.20,593.1)(0.0,640.3),(1.09,611.5),(1.20,598.3)(0.0,650.0),(1.06,623.2),(1.20,606.0)(0.0,659.0),(1.02,634.8),(1.20,613.0)1.2Figure2.1-1ReactorCoreSafetyLimitsFourLoopsInOperationD.C.COOK-UNIT12-2AmendmentNo.
DEP MEMBER S  OF THE PUBLIC 1.35  MEMBER(S) OF THE PUBLIC shall include all persons who are not occupationally associated with the plant. This category does not include employees of the utility, its contractors or its vendors'lso excluded from this category are persons who enter the site to service equipment or to make deliveries. This category does include persons who use portions of the site for recreational, occupational or other purposes not associated with the plant.
TAOLE2.2-1AEACTOATAll'STEHIIISTQUHENTATlOIITAlPSETPOlIITSFUIIClIOIIALUIIlT1.HanualReactorTrip2.PowerAange,NeutronFlux3.PowerRange,tleukronFlux,IllghPasl'tiveRatePosrerRange,MeutranFlux,Illgl>ltegatlveAate5.IntermediateAange,tleutronfluxTlllpSETPD)NTHathpplIcablcLawSetpolnt-c25IlofAATEDTIIEINALPOLIERIllghSetpolntc109>>ofRATEDTIIEAIIALlOMER<5>>afRATEDTIIERHALPOMEAwith1tloeconstant>2secands<5>>ufRATEDTIIEIIHALPDLIEAwltliatloeconstant>2seconds<25>>ofRATEDTIIERNLLPOMEAhLLOMABLEVALUESNothppllcabiaLawSetpolnt-c26>>ofRATEDTIIERHALPOMEAlllghSetpalnt-c110>>otRATEDTIIEAIIALPOMERc5.5"ofRATEDTIIEIIIIALPOllERwithatlaeconstant>2secondsc5.5NofAAlEOTIIERHALPOHEAwithatlaeconstant>2secondscM>>ofRATED1IIEAIIALPOMEA6.SourceAange.IIeutronFlux1.Overtemperatureafe.Overpoweril9.Pressurle'erPressure--Low10.Pressurle'erPressure--Higll<105cauntspersecondSeeIlote1SeeNote2>1875Pslgc23II5pslgll.PressurlaerkaterLevel--tllgh<92>>ofInstroaentspan<1.3xIO5countspersecondScellote3SceIlote41865ps19c2395psigc93>>ofInstruau:ntspan12.LossofFlow<<Designflowls91,6OOgpaperloop.90$of4lcslgnIloMperloop'Sg.laofdessqnflowperloop' 00CTABLE2.2-l(Continued)NOTATIONNotel:OvertemperaturebT<hTfK-Klo12-1+vS(T-T')+K(P-P')-g(bX)33lREACTORTRIPSYSTEMINSTRUMENTATIONTRIPSETPOINTSwl>ere:AT0IndicatedbTatRATEDTHERMALPOWER0Averagetemperature,FIndicatedTatRATEDTHERMALPOWER(~567.8F)avgPressurizerpressure,psigpl1+'ClS1+TSl'IndicatedRCSnominaloperatingpressure(2235psigor2085psig)Thefunctiongeneratedbythelead-lagcontrollerforTdynamiccompensationavgTimeconstantsutilizedinthelead-lagcontrollerforT<=22secs.avg=4secs.T2Laplacetransformoperator0I I~U TABLE2.2-1CotinuedREACORTRIPSYSTEMINSTRUMENTATIONNOTATIONSContinuedOperationwith4LoopsK1=1.32K=0.0230K=0.001103andf(AI)isafunctionoftheindicateddifferencebetweentopandbottomdetectorsofthephwer-rangenuclearionchambers;withgainstobeselectedbasedonmeasuredinstrumentresponseduringplantstartuptestssuchthat:(i)Forq-qbetween-37percentand+2percent,f(aI)0(whereqandqarepercentBMEDTHERMALPOWERinthetopandbottomhalvesofShecorkrespectively,andgt+qbistotalTHERMALPOWERinpercentofmvzoTHERMALPOWER).(ii)Foreachpercentthatthemagnitudeof(q-q)exceeds-37percent,theaTtripsetpointshallheautosaticallyreuu5eahPo.sspercentofitsvalueatMTEDTHERMALPOWER.1(iii)Foreachpercentthatthemagnitudeof(q-tripsetpointshallbeautomaticallyredutfo4MTEDTHERMALPOWER.q)exceeds+2percent,thehTh)2.17percentofitsvalueatI TABLE2.2-lContinuedECTORRISYSTEMNSTRUMENTATIONOTATONContinuedNote2:Overpower~T<dT[K-Ko45S1+<ST-K6(T-T")-f2(hI)]3"'3where:hT0K4K5K6~3S1+T3SIndicatedhTatRATEDTHERMALPOWERAveragetemperature,FIndicatedTatmTEDTHERMALPOWER(>>67-8>>avg1.0830.0177/FforincreasingaveragetemperatureAnd0fordecreasingaveragetemperatureo.-oa15forT>T";K6=0forT<T"ThefunctiongeneratedbytheratelagcontrollerforTdynamiccompensationavgTimeconstantutilizedintheratelagcontrollerforT10secs.avgNote3:Note4:S~Laplacetransformoperatorf2(bI)~0Thechannel's.maximumtrippointshallnotexceeditscomputedtrippointbymorethan3.2percenthTspan.Thechannel'smaximumtrippointshallnotexceeditscomputedtrippointbymorethan2.lpercenthTspan.
SITE BOUNDARY 1.36 The SITE BOUNDARY shall be that line beyond which the land  is not owned, leased or otherwise controlled by the licensee.
POWERDISTRIBUTIONLIMITSHEATFLUXHOTCHANNELFACTOR-F(Z)LIMITINGCONDITIONFOROPERATION3.2.2F(Z)shallbelimitedbythefollowingrelationships:Q~2.15[E(Z))F(Z)<PF(Z)<[4.30)[K(Z)j.P<0.5'P~THERMALPOWERRATEDTHERMALPOWER'F(Z)isthemeasuredhotchannelfactorincludinga3%m3nufacturingtoleranceuncertaintyanda5%measurementuncertainty.'K(Z)isthefunctionobtainedfromFigure3.2-3~APPLICABILITY:MODE1ACTION:WithF(Z)exceedingitslimit:ReduceTHERMALPOWERatleast1%foreach1%F(Z)exceedsthelimitwithin15minutesandsimilarlyreducet9ePowerRangeNeutronFlux-HighTripSetpointswithinthenext4hours;POWEROPERATIONmayproceedforuptoatotalof72hours;subsequentPOWEROPERATIONmayproceedprovidedtheOverpowerdeltaTTripSetpointshavebeenreducedatleast1%foreach1%F(Z)exceedsthelimit.b.IdentifyandcorrectthecauseoftheoutoflimitconditionpriortoincreasingTHERMALPOWERabovethereducedlimitrequiredbya,above;THERMALPOWERmaythenbeincreasedprovidedF(Z)isdemonstratedthroughincoremappingtobewithinitslimit.COOKNUCLEARPLANTUNIT13/42-5AMENDMENTNO.
UNRESTRICTED AREA 1.37 An UNRESTRICTED AREA  shall be any area at or beyond the SITE BOUNDARY to which access is not controlled by the licensee for purposes of protection of individuals from exposure to radiation and radioactive materials or any area within the site boundary used for residential quarters or industrial, commercial, institutional and/or recreational purposes.
n0OTABLE2.2-1(Continued)REACTORTRIPSYSTEHINSTRUHENTATIONTRIPSETPOINTSNOTATIONCHNote1:OvertemperaturehT4hTQ-Ko121+TS31(T-T')+K(P-P')-C(~X)j11+TSwl><<re-AT0IndicatedATatRATEDTHERHALPOWER0Averagetemperature,FIndicatedTatRATEDTHERHALPOWER(<567.8F)avgPressurizerpressure,psigpo1+S1+7S1'SIndicatedRCSnominaloperatingpressure(2235psigor2085psig)Thefunctiongeneratedbythelead-lagcontrollerforTdynamiccompensationavgTimeconstantsutilizedinthelead-lagcontrollerforT<=22sees/avg=4secs.'2Laplacetransformoperator0 1~2OIUUx1.0CLClN0.80X001.0(6.0,1.0)(12.0,0.9250.6468COREHEIGHT(FT)10FIGURE3.2-3K(Z)-NormalizedFsubQ(z)asafunctionofCoreHeightD.CCOOK-NIT13/42-8 i~.1gE POWERDISTRIBUTIONLIMITSNUCLEARENTHALPYHOTCHANNELFACTOR-FAHLIMITINGCONDITIONFOROPERATION3.2.3Fshallbelimitedbythefollowingrelationship:FAH<1.49[1+0.3(1-P)]WherePisthefractionofRATEDTHERMALPOWERAPPLICABILITY'ODE1ACTION:WithFexceedingitslimit-ReduceTHERMALPOWERtolessthan50%ofRATEDTHERMALPOWERwithin2hoursandreducethePowerRangeNeutronFlux-HighTripSetpointstolessthanorequalto55%ofRATEDTHERMALPOWERwithinthenext4hours,b.Demonstratethroughin-coremappingthatFiswithinitslimitwithin24hoursafterexceedingthePimitorreduceTHERMALPOWERtolessthan5%ofRATEDTHERMALPOWERwithinthenext2hours,andIdentifyandcorrectthecauseoftheout-of-limitconditionpriortoincreasingTHERMALgOWER;subsequentPOWEROPERATIONmayproceed,providedthatF"isdemonstratedthroughin-coremappingtobewithinitslimi%atanominal50%ofRATEDTHERMALPOWERpriortoexceedingthisTHERMALPOWER,atanominal75%ofRATEDTHERMALPOWERpriortoexceedingthisTHERMALPOWERandwithin24hoursafterattaining95%orgreaterRATEDTHERMALPOWER.COOKNUCLEARPLANTUNIT13/42-9AMENDMENTNO.
ALLOWABLE POWER LEVEL  APL 1.38 APL means "allowable power level" which is that power level, less than or equal to 100% RATED THERMAL POWER, at which the plant may be operated to ensure that power distribution limits are satisfied.
TABLE3.2-1DNBPARAMETERSPARAMETERLIMITS4LoopsinOperationatRATEDTHERMALPOWERReactorCoolantSystemTavgPressurizerPressureReactorCoolantSystemTotalFlowRate<570.9F)2050psig*C366,400gpmIndicatedaverageofatleastthreeOPERABLEinstrumentloops.**LimitnotapplicableduringeitheraTHERMALPOWERrampincreaseinexcessof5percentRATEDTHERMALPOWERperminuteoraTHERMALPOWERstepincreaseinexcessof10percentRATEDTHERMALPOWER.***IndicatedvalueCOOKNUCLEARPLANTUNIT13/42-14AMENDMENTNO.
COOK NUCLEAR PLANT  UNIT 1            1-7            AMENDMENT NO.
POWERDISTRIBUTIONLIMITSALLOWABLEPOWERLEVEL-APLLIMITINGCONDITIONFOROPERATION3.2.6THERMALPOWERshallbelessthanorequaltoALLOWABLEPOWERLEVEL(APL),givenbythefollowingrelationship:<~2.1>KZx100e,or100S,whicheverisless.F(Z)xV(Z)xFP'F(Z)isthemeasuredhotchannelfactorincludinga3%manufacturingtoleranceuncertaintyanda5Smeasurementuncertainty.'V(Z)isthefunctiondefinedinthePeakingFactorLimitReport.'F1.00exceptwhensuccessivesteady-statepowerdistributionmapsindicateanincreaseinmaxoverZofFZ(2)withexposure.Theneitherofthepenalties,F,shallbetaken:PF-1.02,orPF1.00providedthatSurveillanceRequirement4.2.6.2iSsatisfiedonceper7EffectiveFullPowerDaysuntiltwosuccessivemapsindicatethatthemaxoverZofFZKZ)isnotincreasing.'Theabovelimitisnotapplicableinthefollowingcoreregions.1)Lowercoreregion0$to10%inclusive.2)Uppercoreregion90%to100$inclusive.APPLICABILITY:MODE1COOKNUCLEARPLANTUNIT13/42-15AMENDMENTNO.
 
TABLE3.3-2REACTORTRIPSYSTEMINSTRUMENTATIONRESPONSETIMESFUNCTIONALUNIT1.ManualReactorTrip2.PowerRange,NeutronFluxa.HighSetpointb.LowSetpointRESPONSETIMENOTAPPLICABLE*<0.5seconds<0.5seconds*3.PowerRange,NeutronFlux,HighPositiveRateNOTAPPLICABLEIIogWR'p3RO4.PowerRange,NeutronFlux,HighNegativeRate5.IntermediateRange,NeutronFlux6.SourceRange,NeutronFlux7.OvertemperatureDeltaT&.OverpowerDeltaT9.PressurizerPressure--Low10.PressurizerPressure--Highll.PressurizerWaterLevel--High<0.5secondsNOTAPPLICABLENOTAPPLICABLE*6.0secondsNOTAPPLICABLE<1.0seconds<1.0seconds<2.0seconds*Neutrondetectorsareexemptfromresponsetimetesting.Responsetimeoftheneutronfluxsignalportionofthechannelshallbemeasuredfromdetectoroutputorinputoffirstelectroniccomponentinchannel.
THIS PAGE INTENTIONALLY LEFT BLANK COOK NUCLEAR PLANT UNIT 1          1-10              AMENDMENT NO.
TABLE3.3-4ENGINEEREDSAFETYFEATUREACTUATIOIISYSTEIIIHSTRUtlENTATIONTRIPSETPOlfITSFIIIICTIOIIALUNlT1.SAFETYINJECTION,TURBINETRIP,FEEOIIATERISOLATION,ANDtiOTORDRIVENFEEOIIATERPNIPSa.IlanuaIInltiat1onb.Aut.ornatieActustIonLogicc.ContainmentPressure-Iiighd.PressurizerPressure--Lowe.DifferentialPressureBetv>eenSteamLines--Ilighf.SteamFlowinTwoSteamLines-HighCoincidentwithT-Lov>-LmorSteamLinePressure-"-(oeTRlPSETPOINTtlotApplicableIlotApplicable<1.1psig18l5psig<100psi<1.42x10lbs/hrPromOXloadto20Kload.Ligearfrom1.42x10lbs/hrat620Xloadto3.8Bx10lbs/hratlOOXloadT>541F>>500ysigsteaiilineppessureALLOWABLEVALUESIlotAppl1cableHotApplicable<1.2psigl805psig<112psi<1.56x10lbs/hrfrom0llloadto20"load.Linearfrom1.56x10lbs/hrat620"loadto3.93x10lbs/hrat100Kload.T>539F>a/npsigsteamlineprissure TABLE3..(Continued)ENGINEEREDSAFETYFEATUREACTUATIONSYSTEHINSTRUHENTATIONTRIPSETPOIHTSnOBFUNCTIONALUNITIg2.ContainmentRadioactivity--HighTrainA(VRS-1101,ERS-1301,ERS-1305)TRIPSETPOINTSeeTable3.3-6ALLOWABLEVALUESHotApplicable3.ContainmentRadioactivity--HighTrainB(VRS-1201,ERS-1401,ERS-1405)SeeTable3.3-6HotApplicableSTEAHLINEISOLATIONa.Hanualb.AutomaticActuationLogicc.ContainmentPressure-High-Highd.SteamFlowInTwoSteamLines-HighCoincidentwithTLow-LoworSteamLineSressureavaLow5TURBINETRIPAHDFEEDWATERISOLATIONa.SteamGeneratorWaterLevel-High-HighHotApplicableHotApplicable<<29pslg61.42xl0lbs/hrfrom0%loadto2I)aload.Linearfrom1.42x10lgs/hrat20%loadto3.88x10lbs/hrat100%load.T~54lFavg->500psigsteamlinepressure467%ofnarrow-rangeinstrumentspaneachsteamgeneratorHotApplicableNotApplicable~3psig6l.56x10lbs/hrfromOiloadto20E1ogd.Linearfrom1.56x101bs/hgat20%loadto3.93x10lbs/hrat100Lload.'l'539Favg-480psigsteamlinepressure68%ofnarrow-range4'nstrumentspaneachsteamgeneratorIk
 
~REACTORCOOLANTSYSTEMtPRESSURIZERLIMITINGCONDITIONFOROPERATION3.4.4ThepressurizershallbeOPERABLEwithawatervolumelessthanorequalto928ofspanandatleast150kWofpressurizerheaters.APPLICABILITY:MODES1,2,and3.ACTION:Withthepressurizerinoperableduetoaninoperableemergencypowersupplytothepressurizerheaterseitherrestoretheinoperableemergencypowersupplywithin72hoursorbeinatleastHOTSTANDBYwithinthenext6hoursandinHOTSHUTDOWNwithinthefollowing12hours.Withthepressurizerotherwiseinoperable,beinatleastHOTSHUTDOWNwiththereactortripbreakersopenwithin12hours.SURVEILLANCEREUIREMENTS4.4.4.1Thepressurizerwatervolumeshallbedeterminedtobewithinitslimitsatleastonceper12hours.4.4.4.2TheemergencypowersupplyforthepressurizerheatersshallbedemonstratedOPERABLEatleastonceper18monthsbytransferringpowerfromthenormaltotheemergencypowersupplyandenergizingtherequiredcapacityofheaters.COOKNUCLEARPLANTUNIT13/44-6AMENDMENTNO.
670 UNACC P TABLE OPERA TION 650 24 OPSIA CQ W                                                        2  5QPSI a 630 2100 SIA 200 PSI 610
Ll'gk'4 34.5EMERGENCYCORECOOLINGSYSTEMS(ECCSACCUMULANRSLIMITINGCONDITIONFOROPERATIC'<3.5.1EachreactorcoolantsystemaccumulatorshallbeOPERABLEwith:a.Theisolationvalveopen,b.Acontainedboratedwatervolumeofbetween~2>and971cubicfeet,c.Aboronconcentrationofbetween2400ppmand2600ppm,andd.Anitrogencove."-pressureofbetween585and658psig.APPLICABILITY:MODESt,2and3.>>ACTION:a.Withoneaccu.-..gatorinoperable,exceptasaresultofaclosedisolationvalve,restoretheinoperableaccumulatortoOP'ERABLEstatuswithinonehourorbeinHOTSHUiDOWNwithinthenext8hours.b.Withoneaccumu1atorinoperableduetotheisolationvalvebeingclosed,eitheriwnediatelyopentheisolationvalveorbeinHOTSTANDBYwithinone'hourandbeinHOTSHUTDOWNwithinthenext8hours.SURVEILLANCEREUIREMENTS4.5.1EachaccumulatorshallbedemonstratedOPERABLE:a.Atleastonceperl2hoursby:l.Verifyingthewaterlevelandnitrogencover-pressureintgetanks,and2.Verifyinghateachaccumulatorisolationvalveisopen."PressurizerPressureabove1000psig.0.C.COOK-UNIT13/45-1AmendmentNo.
                                    ]775PSIA 590 O            ACCEPTABLE OPER TION 570
EMERGENCYCORECOOLINGSYSTEMSSURVEILLANCEREQUIREMENTS(Continued)d.Atleastonceper18monthsby:*1.VerifyingautomaticisolationandinterlockactionoftheRHRsystemfromtheReactorCoolantSystemwhentheReactorCoolantSystempressureisabove600psig.2.Avisualinspectionofthecontainmentsumpandverifyingthatthesubsystemsuctioninletsarenotrestrictedbydebrisandthatthesumpcomponents(trashracks,screens,etc.)shownoevidenceofstructuraldistressorabnormalcorrosion.*e.Atleastonceper18months,duringshutdown,by:l.VerifyingthateachautomaticvalveintheflowpathactuatestoitscorrectpositiononaSafetyInjectiontestsignal.2.Verifyingthateachofthefollowingpumpsstartautomaticallyuponreceiptofasafetyinjectiontestsignal:a)Centrifugalchargingpumpb)Safetyinjectionpumpc)Residualheatremovalpumpf.ByverifyingthateachofthefollowingpumpsdevelopstheindicateddischargepressureonrecirculationflowwhentestedpursuanttoSpecification4.0.5atleastonceper31daysonaSTAGGEREDTESTBASIS.1.Centrifugalchargingpump2.SafetyInjectionpump3.Residualheatremovalpump>2405psig>1345psig>165psigg.ByverifyingthecorrectpositionofeachmechanicalstopforthefollowingEmergencyCoreCoolingSystemthrottlevalves:1.Vithin4hoursfollowingcompletionofeachvalvestrokingoperationormaintenanceonthevalvewhentheECCSsubsystemsarerequiredtobeOPERABLE.*TheprovisionsofSpecification4.0.6areapplicable.CookNuclearPlantUnit13/45-5AmendmentNo.
: 0. 0      0. 2        0. 4          0. 6        0. 8        1. 0  1. 2 FRACTION OF RATED THERMAL POWER PRESSURE                                    BREAKPCWTS (PS~IA              CTION RATED Tl+RMAL PO                  T AVG    8  DEGREES 1775                    (0. 0, 617. 1), (1. 16, 584. 5), (1. 20, 579. 7) 2000                      (0. 0, 633. 5), (1. 11, 603. 9), (1. 20, 593. 1) 2100                      (0. 0, 640. 3), (1. 09, 611. 5), (1. 20, 598. 3) 2250                      (0. 0, 650. 0), (1. 06, 623. 2), (1. 20, 606. 0) 2400                      (0. 0, 659. 0), (1. 02, 634. 8), (1. 20, 613. 0)
k~~.Pn~lRWlQ'ehr$ri~P
Figure 2. 1-1 Reactor Core Safety Limits Four Loops In Operation D. C. COOK - UNIT  1            2-2                Amendment No.
)EMGENCYCORECOOLINGSYSTEMSSURVEILLANCEREQUIREMENTS(Continued2.Atleastonceper18months.BoronInjectionThrottleValvesSafetyInjectionThrottleValvesValveNumberValveNumber1.1-SI-141Ll2.1-SI-141L23.1-SI-141L34.1-SI-141L41.1-SI-121N2.1-SI-121Sh.ByperformingaflowbalancetestduringshutdownfollowingcompletionofmodificationstotheECCSsubsystemthatalterthesubsystemflowcharacteristicsandverifyingthefollowingflowrates:BoronInjectionSystemSafetyInjectionSystemLoop1BoronInjectionFlow117.5gpmLoop2BoronInjectionFlow117.5gpmLoop3BoronInjectionFlow117.5gpmLoop4BoronInjectionFlow117.5gpmLoop1and4ColdLegFlow>300gpmLoop2and3ColdLegFlow>300gpm**CombinedLoop1,2,3and4ColdLegFlow(singlepump)lessthanorequalto640gpm.TotalSIS(singlepump)flow,includingminiflow,shallnotexceed700gpm.*TheflowrateineachBoronInjection(BI)lineshouldbeadjustedtoprovide117.5gpm(nominal)flowineachloop.Undertheseconditionsthereiszerominiflowand80gpmsimulatedRCPsealinjectionlineflow.TheactualflowineachBIlinemaydeviatefromthenominalsolongas:a)thedifferencebetweenthehighestandlowestflowis10gpmorless.b)thetotalflowtothefourbranchlinesdoesnotexceed470gpm.c)theminimumflow(totalflow)throughthethreemostconservative(lowestflow)branchlinesmustnotbelessthan345.8gpm.d)Thechargingpuypdischargeresistance(2.31xPd/Qd)mustno)belessthan4.73E-3ft/gpmandmustnotbegreaterthan5.33E-3ft/gpm.(Pdisthepumpdischargepressureatrunout;Qdisthetotalpumpflowrate.)COOKNUCLEARPLANTUNIT13/45-6AMENDMENTNO.
 
I*Ol0It~
TAOLE  2.2-1 AEACTOA  TAll'STEH      IIISTQUHENTATlOII TAlP SETPOlIITS FUIICl IOIIAL UII l T                      Tlllp  SETPD)NT                            hLLOMABLE VALUES
PLIGHT5YSTKl%AQXILZ1W~ATKRSYSTLQGTQCCON)ITICNFCROPEDICN3.7.1.2AtleastthreeirdependentsteamgeneratorauxiliaryteedwaterVmsandassoc.a=edflowpathsshallbeOPEBABLEwith!Twofeedwaterpumps,eachcapableofbeingpoweredfromseparateemergencybusses,andb.CnefeedwaterpumpcaoableofbeingpoweredfromanOPERABLEsteamsupplysystem.APPLICABIL.Y:NODES1,2.and3.ACTZCN:a.wi"honeaux'aryfeedwaterpumpinoperable,restoretherequiredauxiLiaryfeedwate"umpstoOpERABLEstatuswithin72hoursorbeinatleastHOTS-ANDBYwithinthenext6boursandinHCC'HUTDCWNwxthinthefollowing6hours.b.C~Withwoa'iliaryfeedwaterpumpsirc"ablerbeinatleastHOTS-.ANDBYwi"h'n6haurSandinHOTSHU-.".WWithinthefOllOWing6hours.Withthreeauxiliaryfeedwaterpumpsi.".:perable,iamhdiatelyinit'atecorrectireactiontorestoreatleastoneauxiliaryfeedwaterpumptoOPERABLEsta'tusassoonaspossible.SURVEILLANCEREUIRENENTS4.7.1.2Eachauxi3.maryfeedwaterpumpshallbedeaenstratedOPERABLE''a.Atleastonceper31daysby>1.verifyingthateachmotordrivenpumpdevelopsan0equivalentdischargepressureof~137$psigat60F".".recirelationflow.er.'fy'ngthat,thesteamturbinedrivenpumpdevelopsancuivalertdischargepressureof>1285psigat602'nda:alowof)700gpmwhenthesecondarysteamsupplypressureisgreaterthan310psig.TheprovisionsofSoecif'cation4.0.4arenotapplicableforentryintovCDE3D.C.COOKUNIT13/475AmendmentNo.
: 1. Hanual Reactor        Trip            Hat hppl Icablc                              Not hppl lcabia
J'k-eanya,a.'~
: 2. Power Aange, Neutron        Flux      Law Setpolnt - c 25Il      of  AATED        Law    Setpolnt -   c  26>> of  RATED TIIEINAL POLIER                              TIIERHAL POMEA Illgh Setpolnt        c 109>> of RATED      lllgh Setpalnt -      c  110>> ot  RATED TIIEAIIAL l OMER                            TIIEAIIAL POMER
2.1SAFETYLIMITSBASES4LoopOperationWestinghouseFuel(15x15OFA)(WRB-1Correlation)***TypicalCellThimbleCellCorrelationLimitDesignLimitDNBRSafetyAnalysisLimitDNBR1.171.331~451.171.321.45ThecurvesofFigure2.1-1showthelociofpointsofTHERMALPOWER,ReactorCoolantSystempressureandaveragetemperatureforwhichtheminimumDNBRisnolessthantheapplicabledesignDNBRlimit,ortheaverageenthalpyatthevesselexitisequaltotheenthalpyofsaturatedliquid.~representstypicalfuelrod*representsfuelrodsnearguidetubeCookNuclearPlantUnit1B2-1(a)AmendmentNo.
: 3. Power Range,      tleukron Flux,    <   5>> af RATED TIIERHAL POMEA with          c  5.5  "of  RATED TIIEIIIIAL POllER with Illgh Pasl'tive Rate                  1  tloe constant > 2 secands                a  tlae constant    > 2 seconds Posrer Range,      Meutran Flux,      <  5>>   uf RATED TIIEIIHAL PDLIEA wltli      c  5.5 Nof AAlEO    TIIERHAL POHEA  with Illgl> ltegatlve Aate                  a  tloe constant > 2 seconds                a  tlae constant    > 2 seconds
kk SQ'ETYLIMITS.BASESThecurvesarebasedonanenthalpyhotchannelfactor>,of1.49forWestinghousefuelandareferencecosineaxialpowershapewithapeakof1.55.Anallowanceisincludedforanincreasein'P+atreducedpower,basedontheexpression:P-1.49(1+0.3(1-P)jwherePisthefractionofRATEDTHERMALPOWERNote,donotincludea4%uncertaintyvalue,sincethismeasurementuncertaintyhasbeenincludedinthedesignDNBRlimitvalues,whicharelistedinthebasesforSection2.1.1.Theselimitingheatfluxconditionsarehigherthanthosecalculatedfortherangeofallcontrolrodsfullywithdrawntothemaximumallowablecontrolrodinsertion,assumingtheaxialpowerimbalanceiswithinthelimitsofthefl(deltaI)functionoftheOvertemperaturetrip.Whentheaxialpowerimbalanceisnotwithinthetolerance,theaxialpowerimbalanceeffectontheOvertemperaturedeltaTtripswillreducethesetpointstoprovideprotectionconsistentwiththecoresafetylimits.2.1.2REACTORCOOLANTSYSTEMPRESSURETherestrictionofthisSafetyLimi,tprotectstheintegrityoftheReactorCoolantSystemfromoverpressurizationandtherebypreventsthereleaseofradionuclidescontainedinthereactorcoolantfromreachingthecontainmentatmosphere.COOKNUCLEARPLANTUNIT1B2-2AMENDMENTNO.  
: 5. Intermediate Aange, tleutron          < 25>> of RATED TIIERNLL      POMEA          c  M>>of    RATED 1IIEAIIAL POMEA flux
~I.fk'llfl'f,'A'4k'C11~5'tI~Jv"tPq SAFETYLIMITSBASESThePowerRangeNegativeRateTripprovidesprotectionforcontrolroddropaccidents.Athighpower,aroddropaccidentcouldcauselocalfluxpeakingwhichcouldcauseanunconservativelocalDNBRtoexist.ThePowerRangeNegativeRateTripwillpreventthisfromoccurringbytrippingthereactor.NocreditistakenforoperationofthePowerRangeNegativeRateTripforthosecontrolroddropaccidentsforwhichtheDNBR'swillbegreaterthantheapplicabledesignlimitDNBRvalueforeachfueltype.IntermediateandSourceRaneNuclearFluxTheIntermediateandSourceRange,NuclearFluxtripsprovidereactorcoreprotectionduringreactorstartup.ThesetripsprovideredundantprotectiontothelowsetpointtripofthePowerRange,NeutronFluxchannels.>ThesourceRangeChannelswillinitiateareactortripatabout10countspersecond,unlessmanuallyblockedwhenP-6becomesactive.TheIntermediateRangeChannelswillinitiateareactortripatacurrentlevelproportionaltoapproximately25percentofRATEDTHERMALPOWERunlessmanuallyblockedwhenP-10becomesactive.NocreditwastakenforoperationofthetripsassociatedwitheithertheIntermediateorSourceRangeChannelsintheaccidentanalyses;however,theirfunctionalcapabilityatthespecifiedtripsettingsisrequiredbythisspecificationtoenhancetheoverallreliabilityoftheReactorProtectionSystem.OvertemeraturedeltaTTheOvertemperaturedeltaTtripprovidescoreprotectiontopreventDNBforallcombinationsofpressure,power,coolanttemperature,andaxialpowerdistribution,providedthatthetransientisslowwithrespect'topipingtransitdelaysfromthecoretothetemperaturedetectors(about4seconds),andpressureiswithintherangebetweentheHighandLowPressurereactortrips.Thissetpointincludescorrectionsforchangesindensityandheatcapacityofwaterwithtemperatureanddynamiccompensationforpipingdelaysfromthecoretothelooptemperaturedetectors.Thereferenceaveragetemperature(T')andthereferenceoperatingpressure(P')aresetequaltothefullpowerindicatedTavgandthenominalRCSoperatingpressure,respectively,toensureprotectionofthecorelimitsandtopreservetheactuationtimeoftheOvertemperaturedeltaTtripfortherangeoffullpoweraveragetemperaturesassumedinthesafetyanalyses.Withnormalaxialpowerdistribution,thisreactortriplimitisalwaysbelowthecoresafetylimitasshowninFigure2.1-1.Ifaxialpeaksaregreaterthandesign,asindicatedbythedifferencebetweentopandbottompowerrangenucleardetectors,thereactortripisautomaticallyreducedaccordingtothenotationsinTable2.2-1.COOKNUCLEARPLANTUNIT1B2-4AMENDMENTNO.
: 6. Source Aange. IIeutron Flux            < 105  caunts per second                    <   1.3 x IO5 counts per second
ptgp1Q'I1
: 1. Overtemperature      af              See  Ilote  1                                Sce  llote 3
~'I5ITING.SAFETYSYSTEMSETTINGSBASESOveowerdeltaTTheOverpowerdeltaTreactortripprovidesassuranceoffuelintegrity,e.g.,nomelting,underallpossibleoverpowerconditions,limitstherequiredrangeforOvertemperaturedeltaTprotection,andprovidesabackuptotheHighNeutronFluxtrip.Thesetpointincludescorrectionsforchangesindensityandheatcapacityofwaterwithtemperature,anddynamiccompensationforpipingdelaysfromthecoretothelooptemperaturedetectors.Thereferenceaveragetemperature(T"}issetequaltothefullpowerindicatedTavgtoensurefuelintegrityduringoverpowerconditionsfortherangeoffullpoweraveragetemperaturesassumedinthesafetyanalyis.Nocreditwastakenforoperationofthistripintheaccidentanalyses;however,itsfunctionalcapabilityatthespecifiedtripsettingisrequiredbythisspecificationtoenhancetheoverallreliabilityoftheReactorProtectionSystem.PressurizerPressureThePressurizerHighandLowPressuretripsareprovidedtolimitthepressurerangeinwhichreactoroperationispermitted.TheHighPressuretripisbackedupbythepressurizercodesafetyvalvesforRCSoverpressureprotection,andisthereforesetlowerthanthesetpressureforthesevalves(2485psig).TheHighPressuretripprovidesprotectionforaLossofExternalLoadevent.TheLowPressuretripprovidesprotectionbytrippingthereactorintheeventofalossofreactorcoolantpressure.PressurizerWaterLevelThePressurizerHighWaterLeveltripensuresprotectionagainstReactorCoolantSystemoverpressurizationbylimitingthewaterleveltoavolumesufficienttoretainasteambubbleandpreventwaterreliefthroughthepressurizersafetyvalves.ThepressurizerhighwaterleveltripprecludeswaterrelieffortheUncontrolledRCCAWithdrawalatPowerevent.COOKNUCLEARPLANTUNIT1B2-5AMENDMENTNO.
: e. Overpower      il                      See Note 2                                   Sce  Ilote 4
IIf~f 34.2IOWERDISTRIBUTIONLIMITSBASESThespecificationsofthissectionprovideassuranceoffuelintegrityduringConditionI(NormalOperation)andII(IncidentsofModerateFrequency)eventsby:(a)maintainingtheminimumDNBRinthecoregreaterthanorequaltothesafetylimitDNBRduringnormaloperationandinshorttermtransients,and(b)limitingthefissiongasrelease,fuelpellettemperatureandcladdingmechanicalpropertiestowithinassumeddesigncriteria.Inaddition,limitingthepeaklinearpowerdensityduringConditionIeventsprovidesassurancethattheinitialconditionsassumedfortheLOCAanalysesaremetandtheECCSacceptancecriterialimitof2200Fisnotexceeded.Thedefinitionsofhotchannelfactorsasusedinthesespecificationsareasfollows:F(Z)NF~HeatFluxHotChannelFactor,isdefinedasthemaximumlocalheatfluxonthesurfaceofafuelrodatcoreelevationZdividedbytheaveragefuelrodheatflux,allowingformanufacturingtolerancesonfuelpelletsandrods.NuclearEnthalpyRiseHotChannelFactor,isdefinedastheratiooftheintegraloflinearpoweralongtherodwiththehighestintegratedpowertotheaveragerodpower.34.2.1AXIALFLUXDEFFERENCEAFDTargetfluxdifferenceisdeterminedatequilibriumxenonconditions.Thefulllengthrodsmaybepositionedwithinthecoreinaccordancewiththeirrespectiveinsertionlimitsandshouldbeinsertedneartheirnormalpositionforsteadystateoperationathighpowerlevels.ThevalueofthetargetfluxdifferenceobtainedunderthesecondtionsdividedbythefractionofRATEDTHERMALPOWERisthetargetfluxdifferenceatRATEDTHERMALPOWERfortheassociatedcoreburnupconditions'argetfluxdifferencesforotherTHERMALPOWERlevelsareobtainedbymultiplyingtheRATEDTHERMALPOWERvaluebytheappropriatefractionalTHERMALPOWERlevel.Theperiodicupdatingofthetargetfluxdifferencevalueisnecessarytoreflectcoreburnupconsiderations.COOKNUCLEARPLANTUNIT1B3/42-1AMENDMENTNO.  
: 9. Pres surl e'er Pressure--Low          > 1875 Pslg                                      1865 ps 19
~glIIA CObTAINMENTSYSTEMSBASES34.6.1.4INTERNALPRESSUREThelimitationsoncontainmentinternalpressureensurethat1)thecontainmentstructureispreventedfromexceedingitsdesignnegativepressuredifferentialwithrespecttotheoutsideatmosphereof8psigand2)thecontainmentpeakpressuredoesnotexceedthedesignpressureof12psigduringLOCAconditions.ThemaximumpeakpressureresultingfromaLOCAeventiscalculatedtobe11.89psig,whichincludes0.3psigforinitialpositivecontainmentpressure.34.6.1.5AIRTEMPERATUREThelimitationsoncontainmentaverageairtemperatureensurethat1)thecontainmentairmassislimitedtoaninitialmasssufficientlylowtopreventexceedingthedesignpressureduringLOCAconditionsand2)theambientairtemperaturedoesnotexceedthattemperatureallowableforthecontinuousdutyratingspecifiedforequipmentandinstrumentationlocatedwithincontainment.ThecontainmentpressuretransientissensitivetotheinitiallycontainedairmassduringaLOCA.Thecontainedairmassincreaseswithdecreasingtemperature.Thelowertemperaturelimitof60Fwilllimitthepeakpressureto11.89psigwhichislessthanthecontainmentdesignpressureof12psig.TheuppertemperaturelimitinfluencesthepeakaccidenttemperatureslightlyduringaLOCA;however,thislimitisbasedprimarilyuponequipmentprotectionandanticipatedoperatingconditions.Boththeupperandlowertemperaturelimitsareconsistentwiththeparametersusedintheaccidentanalyses.34.6.1.6CONTAINMENTVESSELSTRUCTURALINTEGRITYThislimitationensuresthatthestructuralintegrityofthecontainmentsteelvesselwillbemaintainedcomparabletotheoriginaldesignstandardsforthelifeofthefacility.Structuralintegrityisrequiredtoensurethat(1)thesteellinerremainsleaktightand(2)theconcretesurroundingthesteellinerremainscapableofprovidingexternalmissileprotectionforthesteellinerandradiationshieldingintheeventofaLOCA.AvisualinspectioninconjunctionwithTypeAleakagetestsissufficienttodemonstratethiscapability.COOKNUCLEARPLANTUNIT1B3/46-2AMENDMENTNO.
: 10. Pressurl e'er Pressure--Higll          c  23II5  pslg                                c  2395 psig ll. Pressurlaer kater Level--tllgh        <  92>>  of Instroaent    span                c 93>>  of Instruau:nt    span
0A~,.<rK.lg(,~~'P''.1h4}}
: 12. Loss of Flow                              90$  of 4lcslgn I loM                      Sg.la of dessqn flow per loop'                                   per loop'
<<Design flow      ls 91,6OO gpa  per loop.
 
00 TABLE  2.2-l (Continued)
REACTOR TRIP SYSTEM INSTRUMENTATION TRIP SETPOINTS NOTATION C    Note l: Overtemperature bT < hT fK -K o  1  2 1+v l
S (T-T')+K (P-P')-g (bX)3 3          l wl>ere:  AT 0
Indicated  b T  at  RATED THERMAL POWER 0
Average temperature,       F Indicated  T avg at  RATED THERMAL POWER  (~ 567.8 F)
Pressurizer pressure, psig pl        Indicated  RCS    nominal operating pressure    (2235 psig or 2085 psig) 1+'ClS The  function generated by the lead-lag controller for Tavg dynamic compensation 1+T S Time constants utilized in the lead-lag controller for T               = 22 secs.
l'            = 4 secs.
avg <
T2 Laplace transform operator 0                                                                    I
 
I
~U
 
TABLE  2.2-1  Co tinued REAC OR  TRIP SYSTEM INSTRUMENTATION NOTATIONS  Continued Operation with  4  Loops K1 =  1.32 K  =  0.0230 K  =  0.00110 3
and f (AI) is a function of the indicated difference between top and bottom detectors of the phwer-range nuclear ion chambers; with gains to be selected based on measured instrument response during plant startup tests such that:
(i) For q - q between -37 percent and +2 percent, f (aI) 0 (where q and q are percent BMED THERMAL POWER in the top and bottom halves of She cork respectively, and  gt  + qb  is total  THERMAL POWER  in percent of  mvzo THERMAL POWER).
(ii) For each percent that the magnitude of (q      - q ) exceeds -37 percent, the aT trip setpoint shall  he autosatically reuu5ea    hP o.ss  percent of its value at MTED  THERMAL POWER.                                                              1 (iii) For each percent that the magnitude of      (q- q  ) exceeds +2 percent, the hT its trip setpoint shall be automatically redutfo4 h)     2.17 percent of    value at I MTED  THERMAL POWER.
 
TABLE  2.2-l      Continued E CTOR    RI    SYSTEM    NSTRUMENTATIO NOTAT ON      Continued S
3 Note 2:      Overpower ~T < dT o [K4 -K5                    T  K6  (T-T") -f2(hI) ]
                                                "'3 1+<    S where:  hT 0        Indicated        hT  at  RATED    THERMAL POWER Average temperature,           F Indicated      T      at  mTED    THERMAL POWER    (>>67-8 >>
avg K4        1. 083 K5        0.0177/ F for increasing average temperature And 0 for decreasing average temperature K6        o.-oa15    for T >  T";  K6 = 0  for  T < T"
                ~3S 1+ T3S The    function generated by the rate lag controller for Tavg dynamic compensation Time constant        utilized in the rate lag controller for        T avg 10  secs.
S      ~ Laplace transform operator f2(bI) ~  0 Note 3:  The channel's .maximum    trip  point  shall not    exceed  its  computed trip point  by more than 3.2 percent hT span.
Note 4:  The channel's maximum      trip  point  shall not    exceed  its  computed trip point  by more than 2.l percent hT span.
 
POWER  DISTRIBUTION LIMITS HEAT FLUX HOT CHANNEL FACTOR - F          (Z)
LIMITING CONDITION      FOR OPERATION 3.2.2  F  (Z) shall be  limited by the following relationships:
Q
                        ~2.15 [E(Z))
F(Z)  <    P F  (Z) < [4.30) [K(Z)j    . P  < 0.5
              'P ~ THERMAL  POWER RATED THERMAL POWER
              'F (Z) is the measured hot channel factor including a 3%
m3nufacturing tolerance uncertainty and a 5% measurement uncertainty.
              'K(Z) is the function obtained from Figure 3.2-3      ~
APPLICABILITY:      MODE 1 ACTION:
With  F  (Z) exceeding    its limit:
Reduce THERMAL  POWER  at least    1% for each 1% F (Z) exceeds  the limit within 15  minutes and      similarly reduce t9e Power Range Neutron Flux-High Trip Setpoints within the next 4 hours; POWER OPERATION may proceed for up to a total of 72 hours; subsequent POWER OPERATION may    proceed provided the Overpower delta T Trip Setpoints have been reduced at least 1% for each 1% F (Z) exceeds the limit.
: b.      Identify and correct the cause of the out of limit condition prior to increasing THERMAL POWER above the reduced limit required by a, above; THERMAL POWER may then be increased provided F (Z) is demonstrated through incore mapping to be within its limit.
COOK NUCLEAR PLANT      UNIT 1                  3/4 2-5                AMENDMENT NO.
 
0n O
TABLE  2.2-1 (Continued)
REACTOR  TRIP SYSTEH INSTRUHENTATION TRIP SETPOINTS NOTATION Note 1: Overtemperature                -K 1+T 1 S    (T-T')+K3 (P-P')-C 1 (~X)j o Q1 C                            hT 4 hT 2
H                                              1+T S wl><<re -  AT 0
Indicated  A T  at  RATED THERHAL POWER 0
Average temperature,       F Indicated  T avg at  RATED THERHAL POWER    (< 567.8 F)
Pressurizer pressure, psig po        Indicated  RCS  nominal operating pressure      (2235 psig or 2085 psig) 1+    S The  function generated by the lead-lag controller for Tavg dynamic compensation 1+7 S Time constants utilized in the lead-lag controller for T                = 22 sees/
1'                                                                        avg <
                                    = 4 secs.
                                  '2 S          Laplace transform operator 0
 
1 ~ 2 O
I U
U x        00 1.0            (6. 0, 1. 0)
: 1. 0 CL Cl                                          (12. 0, 0. 925 N
: 0. 8 0
X
: 0. 6 4          6      8      10 CORE    HEIGHT (FT)
FIGURE 3. 2-3  K(Z) - Normalized      F sub Q(z) as  a  function of Core Height D. C COOK - NIT 1        3/4 2-8
 
i~.
1g E
 
POWER  DISTRIBUTION LIMITS NUCLEAR ENTHALPY HOT CHANNEL FACTOR - FAH LIMITING CONDITION      FOR OPERATION 3.2.3    F    shall be  limited by the following relationship:
FAH  < 1.49 [1 + 0.3 (1-P)]
Where  P  is the fraction of    RATED THERMAL POWER APPLICABILITY'ODE 1 ACTION:
With  F    exceeding  its limit-Reduce THERMAL    POWER to less than  50% of  RATED THERMAL POWER within  2 hours and reduce the Power Range Neutron Flux-High Trip Setpoints to less than or equal to      55% of RATED THERMAL POWER within the next 4 hours,
: b. Demonstrate  through in-core mapping that F      is within its limit within 24    hours after exceeding the Pimit or reduce THERMAL POWER to less than 5% of RATED THERMAL POWER within the next 2 hours, and Identify and correct the cause of the out-of-limit condition prior to increasing THERMAL gOWER; subsequent POWER OPERATION may  proceed, provided that F" is demonstrated through in-core mapping to be within its limi% at a nominal 50% of RATED THERMAL POWER prior to exceeding this THERMAL POWER, at a nominal 75% of RATED THERMAL POWER prior to exceeding this THERMAL POWER and within 24 hours after attaining 95% or greater  RATED THERMAL POWER.
COOK NUCLEAR PLANT      UNIT 1            3/4 2-9                AMENDMENT NO.
 
TABLE  3.2-1 DNB PARAMETERS LIMITS 4 Loops  in Operation PARAMETER                      at  RATED THERMAL POWER Reactor Coolant System Tavg          < 570.9 F
                                    )
* Pressurizer Pressure                    2050 psig Reactor Coolant System              C 366,400 gpm Total Flow Rate Indicated average of at least three OPERABLE  instrument loops.
**Limitnot applicable during either a THERMAL POWER ramp increase in excess of 5 percent RATED THERMAL POWER per minute or a THERMAL POWER step increase in excess of 10 percent RATED THERMAL POWER.
***Indicated value COOK NUCLEAR PLANT  UNIT 1            3/4 2-14                AMENDMENT NO.
 
POWER  DISTRIBUTION LIMITS ALLOWABLE POWER LEVEL - APL LIMITING CONDITION      FOR OPERATION 3.2.6    THERMAL POWER    shall  be less than  or equal to ALLOWABLE POWER LEVEL (APL), given by the following        relationship:
                          ~2.1> K Z          x 100e, or 100S, whichever is less.
F (Z)xV(Z)xF P
        'F (Z) is the measured hot channel factor including a 3%
manufacturing tolerance uncertainty and a 5S measurement uncertainty.
        'V(Z) is the function defined in the Peaking Factor Limit Report.
        'F    1.00 except when successive steady-state power distribution maps indicate an increase in max over Z of F Z (2) with exposure. Then either of the penalties, F , shall be taken:                                               P F  -  1.02, or P
F      1.00 provided that Surveillance Requirement 4.2.6.2 iS  satisfied    once per 7 Effective Full Power Days until two successive maps indicate that the max over Z of F Z K Z) is not increasing.
      'The above  limit is    not applicable in the following core regions.
: 1)   Lower core region 0$ to 10% inclusive.
: 2)  Upper core region 90% to 100$ inclusive.
APPLICABILITY:      MODE 1 COOK NUCLEAR PLANT    UNIT 1                3/4 2-15              AMENDMENT NO.
 
TABLE 3.3-2 REACTOR  TRIP SYSTEM INSTRUMENTATION RESPONSE TIMES FUNCTIONAL UNIT                                      RESPONSE TIME
: 1. Manual Reactor    Trip                          NOT APPLICABLE
: 2. Power Range,   Neutron Flux
: a. High Setpoint                              < 0.5 seconds
: b. Low Setpoint                              < 0.5 seconds*
: 3. Power Range,   Neutron Flux, High Positive Rate                              NOT APPLICABLE
: 4. Power Range, Neutron Flux, I      High Negative Rate                              < 0.5 seconds I
o
: 5. Intermediate Range, Neutron Flux                NOT APPLICABLE
: 6. Source Range, Neutron Flux                      NOT APPLICABLE
: 7. Overtemperature    Delta  T                          6.0 seconds
    &. Overpower Delta T                                NOT APPLICABLE
: 9. Pressurizer Pressure--Low                      < 1.0 seconds g  10. Pressurizer    Pressure--High                    < 1.0 seconds W
R
'p3 R
O ll. Pressurizer    Water Level--High                  < 2.0 seconds
    *Neutron  detectors are exempt from response time testing. Response time of the neutron  flux signal portion of the    channel shall be measured from detector output or input of  first electronic  component  in channel.
 
TABLE 3.3-4 ENGINEERED SAFETY FEATURE ACTUATIOII SYSTEII IHSTRUtlENTATION TRIP SETPOlf ITS FIIIICTIOIIAL UNlT                                          TRlP SETPOINT                ALLOWABLE VALUES
: 1. SAFETY INJECTION, TURBINE TRIP, FEEOIIATER ISOLATION, AND tiOTOR DRIVEN FEEOIIATER PNIPS
: a. Ilanua I  Inl ti a t 1 on                      tlot Appl icable            Ilot Appl 1 cabl e
: b. Aut.orna tie Actus t Ion Logic                  Ilot Applicable              Hot Applicable
: c. Containment Pressure        Iiigh              <  1.1 psig                  <  1.2 psig
: d. Pressurizer Pressure--Low                          18l5 psig                    l805 psig
: e. Di f ferential Pressure                        <  100  psi                  <  112 psi Betv>een Steam      Lines--Iligh
: f. Steam Flow    in Two Steam Lines              < 1.42 x 10      lbs/hr      <  1.56 x 10    lbs/hr High  Coincident or Steam Line with T Pressure-"-(oe Lov>-Lm    Prom OX load load.
to 20K Ligear from from 0ll load load. Linear from to 20" 1.42 x 10 lbs/hr            1.56 x 10 lbs/hr at620X load to 3.8B x        at620" load to 3.93 x 10    lbs/hr at  lOOX  load  10 lbs/hr at 100K load.
T>541F                      T>539F 500  ysig steaii line      >
a/n psig steam    line ppessure                      prissure
 
TABLE 3.     . (Continued)
ENGINEERED SAFETY FEATURE ACTUATION SYSTEH INSTRUHENTATION TRIP SETPOIHTS n
OB FUNCTIONAL UNIT                                            TRIP SETPOINT                        ALLOWABLE VALUES I      2. Containment Radioactivity--                See  Table 3.3-6                              Hot Applicable High Train A (VRS-1101, g          ERS-1301, ERS-1305)
: 3. Containment  Radioactivity--             See  Table 3. 3-6                              Hot Applicable High Train  B  (VRS-1201, ERS-1401,  ERS-1405)
STEAH LINE ISOLATION
: a. Hanual                                    Hot Applicable                                  Hot  Applicable
: b. Automatic Actuation Logic                  Hot Applicable                                  Not Appl icable
: c. Containment Pressure  High-High            << 2 9  pslg                                    ~  3  psig 6                                          6
: d. Steam Flow  In Two Steam Lines            1.42 x l0 lbs/hr from 0%                l.56  x 10      lbs/hr from Oi High Coincident with Tava                  load to 2I)a load. Linear from          load  to 20  E  1ogd. Linear Low-Low or Steam Line Sressure            1.42 x 10 lgs/hr at 20% load            from 1.56 x 10 1bs/hg at Low                                        to 3.88 x 10 lbs/hr at 100%            20% load to 3.93 x 10 lbs/
load.                                   hr at 100L load.
                                                                                                      'l' T
avg-~    54l F avg 539 F
                                                      >  500  psig steam line pressure          480  psig steam line pressure                          I k
5    TURBINE TRIP AHD FEEDWATER ISOLATION
: a. Steam Generator Water    Level          4 67%  of narrow-range instrument      68% of narrow-range High-High                                    span each steam generator          4'nstrument span each        steam generator
 
~ REACTOR COOLANT SYSTEM t
PRESSURIZER LIMITING CONDITION  FOR OPERATION 3.4.4  The pressurizer shall be  OPERABLE with a water volume less than or equal to 928 of span and at least 150    kW of pressurizer heaters.
APPLICABILITY:   MODES  1,2, and 3.
ACTION:
With the pressurizer inoperable due to an inoperable emergency power supply to the pressurizer heaters either restore the inoperable emergency power supply within 72 hours or be in at least HOT STANDBY within the next 6 hours and in HOT SHUTDOWN within the following 12 hours. With the pressurizer otherwise inoperable, be in at least HOT SHUTDOWN with the reactor trip breakers open within 12 hours.
SURVEILLANCE RE UIREMENTS 4.4.4.1   The pressurizer water volume shall be determined to  be  within its limits at least  once per 12 hours.
4.4.4.2  The emergency power supply for the pressurizer heaters shall be demonstrated OPERABLE at least once per 18 months by transferring power from the normal to the emergency power supply and energizing the required capacity of heaters.
COOK NUCLEAR PLANT  UNIT 1              3/4 4-6                AMENDMENT NO.
 
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EMERGENCY CORE COOLING SYSTEMS          (ECCS 3 4.5 ACCUMULANRS LIMITING CONDITION      FOR OPERATIC'<
3.5.1    Each  reactor coolant system accumulator shall          be OPERABLE  with:
: a. The  isolation valve open,
: b. A  contained borated water volume of between ~2> and          971  cubic feet,
: c. A  boron concentration      of between 2400 ppm and 2600 ppm, and
: d. A  nitrogen cove."-pressure of between        585 and 658  psig.
APPLICABILITY:        MODES    t, 2 and  3.>>
ACTION:
: a. With one    accu.-.. gator inoperable, except as a result of a closed isolation valve, restore the inoperable accumulator to OP'ERABLE status within one hour or be in HOT SHUiDOWN within the next 8  hours.
: b. With one accumu1ator inoperable due to the isolation valve being closed, either iwnediately open the isolation valve or be  in  HOT STANDBY    within one'hour    and be  in  HOT SHUTDOWN  within the next    8  hours.
SURVEILLANCE RE UIREMENTS 4.5.1    Each accumulator        shall  be demonstrated  OPERABLE:
: a. At least once per l2 hours by:
: l.      Verifying the water level      and  nitrogen cover-pressure in tge tanks, and
: 2.     Verifying hat      each accumulator    isolation valve is  open.
" Pressurizer Pressure above 1000 psig.
: 0. C. COOK  - UNIT  1                 3/4 5-1             Amendment No.
 
EMERGENCY CORE COOLING SYSTEMS SURVEILLANCE REQUIREMENTS    (Continued)
: d. At least once per    18 months  by:*
: 1. Verifying automatic isolation      and  interlock action of the  RHR system from the Reactor Coolant System when the Reactor Coolant System pressure  is above 600    psig.
: 2. A  visual inspection of the containment sump and verifying that the subsystem suction inlets are not restricted by debris and that the sump components (trash racks, screens, etc.) show no evidence of structural distress or abnormal corrosion.
: e. At least once per    18 months, during shutdown, by:
: l. Verifying that each automatic valve in the flow path actuates to its correct position on a Safety Injection test signal.
: 2. Verifying that each of the following pumps start automatically upon receipt of a safety injection test signal:
a)   Centrifugal charging    pump b)   Safety injection  pump c)  Residual heat removal    pump
: f. By verifying that each of the following pumps develops the indicated discharge pressure on recirculation flow when tested pursuant to Specification 4.0.5 at least once per 31 days on a STAGGERED TEST BASIS.
: 1. Centrifugal charging    pump            > 2405 psig
: 2. Safety Injection  pump                  > 1345  psig
: 3. Residual heat removal    pump            > 165  psig
: g. By verifying the correct position of      each mechanical stop  for the following  Emergency Core Cooling System throttle valves:
: 1. Vithin 4 hours following completion of        each valve stroking operation or maintenance on the valve        when the ECCS subsystems are required to be OPERABLE.
*The provisions  of Specification 4.0.6 are applicable.
Cook Nuclear  Plant Unit  1             3/4 5-5                  Amendment No.
 
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EM    GENCY CORE COOLING SYSTEMS SURVEILLANCE REQUIREMENTS    (Continued
: 2. At least once per  18 months.
Boron Injection              Safety Injection Throttle Valves              Throttle Valves Valve Number                Valve Number
: 1. 1-SI-141  Ll          1. 1-SI-121  N
: 2. 1-SI-141  L2          2. 1-SI-121  S
: 3. 1-SI-141  L3
: 4. 1-SI-141  L4
: h. By performing a flow balance test during shutdown following completion of modifications to the ECCS subsystem that alter the subsystem flow characteristics and verifying the following flow rates:
Boron  Injection  System          Safety Injection System Loop 1 Boron  Injection          Loop 1 and 4 Cold Leg Flow 117.5 gpm                    Flow > 300 gpm Loop 2 Boron  Injection          Loop 2 and 3 Cold Leg Flow 117.5 gpm                    Flow > 300 gpm Loop  3 Boron Injection            **Combined Loop 1,2,3 and 4 Cold Flow 117.5 gpm                    Leg Flow (single pump) less than or equal to  640 gpm. Total SIS  (single pump) flow, including Loop 4 Boron  Injection          miniflow, shall not exceed Flow 117.5 gpm                    700 gpm.
*The flow rate in each Boron Injection (BI) line should be adjusted to provide 117.5 gpm (nominal) flow in each loop. Under these conditions there is zero miniflow and    80 gpm simulated RCP seal    injection line flow.
The  actual flow in each BI line    may deviate from the  nominal so long as:
a)    the difference between the highest and lowest flow      is 10 gpm or less.
b)    the total flow to  the four branch lines does not exceed 470 gpm.
c)    the minimum flow (total flow) through the three most conservative (lowest flow) branch lines must not be less than 345.8 gpm.
d)    The charging puyp discharge resistance (2.31xPd/Qd ) must no) be less than 4.73E-3 ft/gpm and must not be greater than 5.33E-3 ft/gpm . (Pd is the pump discharge pressure at runout; Qd is the total pump flow rate.)
COOK NUCLEAR PLANT    UNIT 1              3/4 5-6                  AMENDMENT NO.
 
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AQXILZ1W ~ATKR SYST LQGTQC CON)ITICN      FCR    OPED ICN 3.7.1.2    At least three irdependent steam generator auxiliary teedwater Vms and assoc. a=ed flow paths shall be OPEBABLE with!
Two  feedwater pumps, each capable of being powered from separate emergency busses, and
: b. Cne  feedwater pump caoable of being powered from an                      OPERABLE steam supply system.
APPLICABIL .Y:    NODES    1, 2. and 3.
ACTZCN:
: a. wi"h one aux 'ary feedwater          pump inoperable, restore the required auxiLiary feedwate "umps to          OpERABLE status within 72 hours or be in at least      HOT S-ANDBY within the next 6 bours and in wxthin the following        6  hours.                      HCC'HUTDCWN
: b. With wo    a'iliary      feedwater pumps      irc" abler be in at least HOT S-.ANDBY  wi"h'n    6 haurS and  in  HOT  SHU-.".W Within the fOllOWing 6 hours.
C ~  With three    auxiliary feedwater      pumps  i.".:perable, iamhdiately init'ate correctire action to restore at least              one  auxiliary feedwater pump to      OPERABLE  sta'tus as soon as possible.
SURVEILLANCE RE UIRENENTS 4.7.1.2    Each auxi3.mary feedwater pump          shall  be deaenstrated    OPERABLE''
: a. At least once per      31  days by>
: 1. verifying that      each motor driven      pump  develops an 0 equivalent discharge pressure of          ~ 137$  psig  at 60 F
                        ".". recir elation flow.
er.'fy'ng that, the steam turbine driven pump develops an cuivalert discharge pressure of > 1285 psig at 60 2'nd a: a low of ) 700 gpm when the secondary steam supply pressure is greater than 310 psig. The provisions of Soecif'cation 4.0.4 are not applicable for entry into vCDE  3 D. C. COOK    UNIT  1                          3/47    5                    Amendment No.
 
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2.1  SAFETY LIMITS BASES 4 Loop  Operation Westinghouse Fuel (15x15 OFA)
(WRB-1  Correlation)
Typical Cell Thimble Cell Correlation Limit          1.17                  1.17 Design  Limit DNBR        1.33                  1.32 Safety Analysis Limit DNBR                      1 45
                            ~                    1.45 The curves of Figure 2.1-1 show the loci of points of THERMAL POWER, Reactor Coolant System pressure and average temperature for which the minimum DNBR is no less than the applicable design DNBR limit, or the average enthalpy at the vessel exit is equal to the enthalpy of saturated liquid.
~represents
* typical fuel rod represents fuel rods near guide tube Cook Nuclear  Plant Unit 1              B  2-1(a)              Amendment No.
 
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SQ'ETY LIMITS.
BASES The curves are based on an enthalpy hot channel factor >, of 1.49 for Westinghouse fuel and a reference cosine axial power shape with a peak of 1.55. An allowance is included for an increase in 'P+ at reduced power, based on the expression:
P -    1.49 (1 + 0.3 (1-P)j where  P  is the fraction of RATED THERMAL POWER Note, do not include a  4% uncertainty value, since this measurement uncertainty has been included in the design DNBR limit values, which are listed in the bases for Section 2.1.1.
These  limiting heat flux conditions are higher than those calculated for the range of all control rods fully withdrawn to the maximum allowable control rod insertion, assuming the axial power imbalance is within the limits of the  fl (delta I) function of the Overtemperature trip. When the axial power imbalance is not within the tolerance, the axial power imbalance effect on the Overtemperature delta T trips will reduce the setpoints to provide protection consistent with the core safety limits.
2.1.2    REACTOR COOLANT SYSTEM PRESSURE The  restriction of this Safety Limi,t protects the integrity of the Reactor Coolant System from overpressurization and thereby prevents the release of radionuclides contained in the reactor coolant from reaching the containment atmosphere.
COOK NUCLEAR PLANT  UNIT 1          B  2-2                AMENDMENT NO.
 
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SAFETY LIMITS BASES The Power Range Negative Rate    Trip provides protection for control rod drop accidents. At high power, a rod drop accident could cause local flux peaking which could cause an unconservative local DNBR to exist.
The Power Range Negative Rate Trip will prevent this from occurring by tripping the reactor. No credit is taken for operation of the Power Range Negative Rate Trip for those control rod drop accidents for which the DNBR's will be greater than the applicable design limit DNBR value for  each fuel type.
Intermediate and Source  Ran e  Nuclear Flux The  Intermediate and Source Range, Nuclear Flux trips provide reactor core protection during reactor startup. These trips provide redundant protection to the low setpoint trip of the Power Range, Neutron Flux channels.> The source Range Channels will initiate a reactor trip at about 10    counts per second, unless manually blocked when P-6 becomes active. The Intermediate Range Channels will initiate a reactor trip at a current level proportional to approximately 25 percent of RATED THERMAL POWER unless manually blocked when P-10 becomes active. No credit was taken for operation of the trips associated with either the Intermediate or Source Range Channels in the accident analyses; however, their functional capability at the specified trip settings is required by this specification to enhance the overall reliability of the Reactor Protection System.
Overtem erature  delta T The Overtemperature  delta  T trip provides core protection to prevent  DNB for all combinations of pressure, power, coolant temperature, and axial power distribution, provided that the transient is slow with respect 'to piping transit delays from the core to the temperature detectors (about    4 seconds), and pressure is within the range between the High and Low Pressure reactor trips. This setpoint includes corrections for changes in density and heat capacity of water with temperature and dynamic compensation for piping delays from the core to the loop temperature detectors. The reference average temperature (T') and the reference operating pressure  (P') are set equal to the full power indicated Tavg and the nominal  RCS  operating pressure, respectively, to ensure protection of the core limits and to preserve the actuation time of the Overtemperature delta T trip for the range of full power average temperatures assumed in the safety analyses. With normal axial power distribution, this reactor trip limit is always below the core safety limit as shown in Figure 2.1-1. If axial peaks are greater than design, as indicated by the difference between top and bottom power range nuclear detectors, the reactor trip is automatically reduced according to the notations in Table 2.2-1.
COOK NUCLEAR PLANT  UNIT 1            B 2-4                AMENDMENT NO.
 
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  'I5ITING.SAFETY      SYSTEM SETTINGS BASES Ove  ower delta  T The Overpower delta T reactor    trip  provides assurance of fuel integrity, e.g., no melting, under  all  possible overpower conditions, limits the required range for Overtemperature delta T protection, and provides a backup to the High Neutron Flux    trip. The setpoint includes corrections for changes in density and heat capacity of water with temperature, and dynamic compensation  for piping delays from the core to the loop temperature detectors. The reference average temperature (T"} is set equal to the full power indicated Tavg to ensure fuel integrity during overpower conditions for the range of full power average temperatures assumed in the safety analy is. No credit was taken for operation of this trip in the accident analyses; however, its functional capability at the specified trip setting is required by this specification to enhance the overall  reliability of  the Reactor Protection System.
Pressurizer Pressure The  Pressurizer High and Low Pressure trips are provided to limit the pressure range in which reactor operation is permitted. The High Pressure trip is backed up by the pressurizer code safety valves for RCS overpressure protection, and is therefore set lower than the set pressure for these valves (2485 psig). The High Pressure trip provides protection for a Loss of External Load event. The Low Pressure trip provides protection by tripping the reactor in the event of a loss of reactor coolant pressure.
Pressurizer Water Level The  Pressurizer High Water Level trip ensures protection against Reactor Coolant System overpressurization by limiting the water level to a volume sufficient to retain a steam bubble and prevent water relief through the pressurizer safety valves. The pressurizer high water level trip precludes water relief for the Uncontrolled RCCA Withdrawal at Power event.
COOK NUCLEAR PLANT  UNIT 1            B 2-5                AMENDMENT NO.
 
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3  4.2  IOWER DISTRIBUTION  LIMITS BASES The    specifications of this section provide assurance of fuel integrity during Condition    I (Normal Operation) and II (Incidents of Moderate Frequency) events by: (a) maintaining the minimum DNBR in the core greater than or equal to the safety limit DNBR during normal operation and in short term transients, and (b) limiting the fission gas release, fuel pellet temperature and cladding mechanical properties to within assumed design criteria. In addition, limiting the peak linear power density during Condition I events provides assurance that the initial conditions assumed for the LOCA analyses are met and the ECCS acceptance criteria limit of 2200 F is not exceeded.
The  definitions of hot channel factors    as used in these specifications are as follows:
F  (Z)      Heat Flux Hot Channel Factor, is defined as the maximum local heat  flux on the surface of a fuel rod at core elevation Z divided by the average fuel rod heat flux, allowing for manufacturing tolerances on fuel pellets and rods.
N F~          Nuclear Enthalpy Rise Hot Channel Factor, is defined as the ratio of the integral of linear power along the rod with the highest integrated power to the average rod power.
3  4.2.1    AXIAL FLUX DEFFERENCE  AFD Target flux difference is determined at equilibrium xenon conditions.
The    full length rods may be positioned within the core in accordance with their respective insertion limits and should be inserted near their normal position for steady state operation at high power levels. The value of the target flux difference obtained under these condtions divided by the fraction of RATED THERMAL POWER is the target flux difference at RATED THERMAL POWER for the associated core burnup conditions'arget flux differences for other THERMAL POWER levels are obtained by multiplying the RATED THERMAL POWER value by the appropriate fractional THERMAL POWER level. The periodic updating of the target flux difference value is necessary to reflect core burnup considerations.
COOK NUCLEAR PLANT    UNIT 1            B 3/4 2-1            AMENDMENT NO.
 
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CObTAINMENT SYSTEMS BASES 3  4.6.1.4  INTERNAL PRESSURE The  limitations on containment internal pressure ensure that 1) the containment structure is prevented from exceeding its design negative pressure differential with respect to the outside atmosphere of 8 psig and 2) the containment peak pressure      does not exceed the design pressure of  12  psig during  LOCA  conditions.
The maximum peak    pressure resulting from a LOCA event is calculated to be 11.89 psig, which includes 0.3 psig for initial positive containment pressure.
3  4.6.1.5  AIR TEMPERATURE The  limitations on containment average air temperature ensure that 1) the containment air mass is limited to an initial mass sufficiently low to prevent exceeding the design pressure during LOCA conditions and 2) the ambient air temperature does not exceed that temperature allowable for the continuous duty rating specified for equipment and instrumentation located within containment.
The containment pressure transient is sensitive to the      initially contained air mass during a LOCA. The contained air mass increases with decreasing temperature.      The lower temperature limit of 60 F  will limit the peak pressure to 11.89 psig which is less than the containment design pressure of 12 psig. The upper temperature limit influences the peak accident temperature slightly during a LOCA; however, this limit is based primarily  upon equipment protection and anticipated operating conditions.
Both the upper and lower temperature limits are consistent with the parameters used in the accident analyses.
3  4.6.1.6  CONTAINMENT VESSEL STRUCTURAL INTEGRITY This  limitation ensures  that the structural integrity of the containment steel vessel  will be maintained comparable to the original design standards  for the life of the facility. Structural integrity is required to ensure that (1) the steel liner remains leak tight and (2) the concrete surrounding the steel liner remains capable of providing external missile protection for the steel liner and radiation shielding in the event of a LOCA. A visual inspection in conjunction with Type A leakage tests is sufficient to demonstrate this capability.
COOK NUCLEAR PLANT    UNIT 1            B  3/4 6-2            AMENDMENT NO.
 
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Latest revision as of 02:17, 4 February 2020

Proposed Tech Specs Supporting Cycle 11 Fuel Cycle,Which Will Incorporate Operation of Unit at Reduced Temps & Pressures W/Intent of Reducing Steam Generator U-tube Stress Corrosion Cracking
ML17325A963
Person / Time
Site: Cook American Electric Power icon.png
Issue date: 10/14/1988
From:
INDIANA MICHIGAN POWER CO. (FORMERLY INDIANA & MICHIG
To:
Shared Package
ML17325A960 List:
References
NUDOCS 8810190407
Download: ML17325A963 (40)


Text

ATTACHMENT 4 TO AEP'NRC'1067 PROPOSED REVISED TECHNICAL SPECIFICATION PAGES SSi0190407 8S10i4 PDR ADGCK 050003i5 P pHO

DEP MEMBER S OF THE PUBLIC 1.35 MEMBER(S) OF THE PUBLIC shall include all persons who are not occupationally associated with the plant. This category does not include employees of the utility, its contractors or its vendors'lso excluded from this category are persons who enter the site to service equipment or to make deliveries. This category does include persons who use portions of the site for recreational, occupational or other purposes not associated with the plant.

SITE BOUNDARY 1.36 The SITE BOUNDARY shall be that line beyond which the land is not owned, leased or otherwise controlled by the licensee.

UNRESTRICTED AREA 1.37 An UNRESTRICTED AREA shall be any area at or beyond the SITE BOUNDARY to which access is not controlled by the licensee for purposes of protection of individuals from exposure to radiation and radioactive materials or any area within the site boundary used for residential quarters or industrial, commercial, institutional and/or recreational purposes.

ALLOWABLE POWER LEVEL APL 1.38 APL means "allowable power level" which is that power level, less than or equal to 100% RATED THERMAL POWER, at which the plant may be operated to ensure that power distribution limits are satisfied.

COOK NUCLEAR PLANT UNIT 1 1-7 AMENDMENT NO.

THIS PAGE INTENTIONALLY LEFT BLANK COOK NUCLEAR PLANT UNIT 1 1-10 AMENDMENT NO.

670 UNACC P TABLE OPERA TION 650 24 OPSIA CQ W 2 5QPSI a 630 2100 SIA 200 PSI 610

]775PSIA 590 O ACCEPTABLE OPER TION 570

0. 0 0. 2 0. 4 0. 6 0. 8 1. 0 1. 2 FRACTION OF RATED THERMAL POWER PRESSURE BREAKPCWTS (PS~IA CTION RATED Tl+RMAL PO T AVG 8 DEGREES 1775 (0. 0, 617. 1), (1. 16, 584. 5), (1. 20, 579. 7) 2000 (0. 0, 633. 5), (1. 11, 603. 9), (1. 20, 593. 1) 2100 (0. 0, 640. 3), (1. 09, 611. 5), (1. 20, 598. 3) 2250 (0. 0, 650. 0), (1. 06, 623. 2), (1. 20, 606. 0) 2400 (0. 0, 659. 0), (1. 02, 634. 8), (1. 20, 613. 0)

Figure 2. 1-1 Reactor Core Safety Limits Four Loops In Operation D. C. COOK - UNIT 1 2-2 Amendment No.

TAOLE 2.2-1 AEACTOA TAll'STEH IIISTQUHENTATlOII TAlP SETPOlIITS FUIICl IOIIAL UII l T Tlllp SETPD)NT hLLOMABLE VALUES

1. Hanual Reactor Trip Hat hppl Icablc Not hppl lcabia
2. Power Aange, Neutron Flux Law Setpolnt - c 25Il of AATED Law Setpolnt - c 26>> of RATED TIIEINAL POLIER TIIERHAL POMEA Illgh Setpolnt c 109>> of RATED lllgh Setpalnt - c 110>> ot RATED TIIEAIIAL l OMER TIIEAIIAL POMER
3. Power Range, tleukron Flux, < 5>> af RATED TIIERHAL POMEA with c 5.5 "of RATED TIIEIIIIAL POllER with Illgh Pasl'tive Rate 1 tloe constant > 2 secands a tlae constant > 2 seconds Posrer Range, Meutran Flux, < 5>> uf RATED TIIEIIHAL PDLIEA wltli c 5.5 Nof AAlEO TIIERHAL POHEA with Illgl> ltegatlve Aate a tloe constant > 2 seconds a tlae constant > 2 seconds
5. Intermediate Aange, tleutron < 25>> of RATED TIIERNLL POMEA c M>>of RATED 1IIEAIIAL POMEA flux
6. Source Aange. IIeutron Flux < 105 caunts per second < 1.3 x IO5 counts per second
1. Overtemperature af See Ilote 1 Sce llote 3
e. Overpower il See Note 2 Sce Ilote 4
9. Pres surl e'er Pressure--Low > 1875 Pslg 1865 ps 19
10. Pressurl e'er Pressure--Higll c 23II5 pslg c 2395 psig ll. Pressurlaer kater Level--tllgh < 92>> of Instroaent span c 93>> of Instruau:nt span
12. Loss of Flow 90$ of 4lcslgn I loM Sg.la of dessqn flow per loop' per loop'

<<Design flow ls 91,6OO gpa per loop.

00 TABLE 2.2-l (Continued)

REACTOR TRIP SYSTEM INSTRUMENTATION TRIP SETPOINTS NOTATION C Note l: Overtemperature bT < hT fK -K o 1 2 1+v l

S (T-T')+K (P-P')-g (bX)3 3 l wl>ere: AT 0

Indicated b T at RATED THERMAL POWER 0

Average temperature, F Indicated T avg at RATED THERMAL POWER (~ 567.8 F)

Pressurizer pressure, psig pl Indicated RCS nominal operating pressure (2235 psig or 2085 psig) 1+'ClS The function generated by the lead-lag controller for Tavg dynamic compensation 1+T S Time constants utilized in the lead-lag controller for T = 22 secs.

l' = 4 secs.

avg <

T2 Laplace transform operator 0 I

I

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TABLE 2.2-1 Co tinued REAC OR TRIP SYSTEM INSTRUMENTATION NOTATIONS Continued Operation with 4 Loops K1 = 1.32 K = 0.0230 K = 0.00110 3

and f (AI) is a function of the indicated difference between top and bottom detectors of the phwer-range nuclear ion chambers; with gains to be selected based on measured instrument response during plant startup tests such that:

(i) For q - q between -37 percent and +2 percent, f (aI) 0 (where q and q are percent BMED THERMAL POWER in the top and bottom halves of She cork respectively, and gt + qb is total THERMAL POWER in percent of mvzo THERMAL POWER).

(ii) For each percent that the magnitude of (q - q ) exceeds -37 percent, the aT trip setpoint shall he autosatically reuu5ea hP o.ss percent of its value at MTED THERMAL POWER. 1 (iii) For each percent that the magnitude of (q- q ) exceeds +2 percent, the hT its trip setpoint shall be automatically redutfo4 h) 2.17 percent of value at I MTED THERMAL POWER.

TABLE 2.2-l Continued E CTOR RI SYSTEM NSTRUMENTATIO NOTAT ON Continued S

3 Note 2: Overpower ~T < dT o [K4 -K5 T K6 (T-T") -f2(hI) ]

"'3 1+< S where: hT 0 Indicated hT at RATED THERMAL POWER Average temperature, F Indicated T at mTED THERMAL POWER (>>67-8 >>

avg K4 1. 083 K5 0.0177/ F for increasing average temperature And 0 for decreasing average temperature K6 o.-oa15 for T > T"; K6 = 0 for T < T"

~3S 1+ T3S The function generated by the rate lag controller for Tavg dynamic compensation Time constant utilized in the rate lag controller for T avg 10 secs.

S ~ Laplace transform operator f2(bI) ~ 0 Note 3: The channel's .maximum trip point shall not exceed its computed trip point by more than 3.2 percent hT span.

Note 4: The channel's maximum trip point shall not exceed its computed trip point by more than 2.l percent hT span.

POWER DISTRIBUTION LIMITS HEAT FLUX HOT CHANNEL FACTOR - F (Z)

LIMITING CONDITION FOR OPERATION 3.2.2 F (Z) shall be limited by the following relationships:

Q

~2.15 [E(Z))

F(Z) < P F (Z) < [4.30) [K(Z)j . P < 0.5

'P ~ THERMAL POWER RATED THERMAL POWER

'F (Z) is the measured hot channel factor including a 3%

m3nufacturing tolerance uncertainty and a 5% measurement uncertainty.

'K(Z) is the function obtained from Figure 3.2-3 ~

APPLICABILITY: MODE 1 ACTION:

With F (Z) exceeding its limit:

Reduce THERMAL POWER at least 1% for each 1% F (Z) exceeds the limit within 15 minutes and similarly reduce t9e Power Range Neutron Flux-High Trip Setpoints within the next 4 hours4.62963e-5 days <br />0.00111 hours <br />6.613757e-6 weeks <br />1.522e-6 months <br />; POWER OPERATION may proceed for up to a total of 72 hours8.333333e-4 days <br />0.02 hours <br />1.190476e-4 weeks <br />2.7396e-5 months <br />; subsequent POWER OPERATION may proceed provided the Overpower delta T Trip Setpoints have been reduced at least 1% for each 1% F (Z) exceeds the limit.

b. Identify and correct the cause of the out of limit condition prior to increasing THERMAL POWER above the reduced limit required by a, above; THERMAL POWER may then be increased provided F (Z) is demonstrated through incore mapping to be within its limit.

COOK NUCLEAR PLANT UNIT 1 3/4 2-5 AMENDMENT NO.

0n O

TABLE 2.2-1 (Continued)

REACTOR TRIP SYSTEH INSTRUHENTATION TRIP SETPOINTS NOTATION Note 1: Overtemperature -K 1+T 1 S (T-T')+K3 (P-P')-C 1 (~X)j o Q1 C hT 4 hT 2

H 1+T S wl><<re - AT 0

Indicated A T at RATED THERHAL POWER 0

Average temperature, F Indicated T avg at RATED THERHAL POWER (< 567.8 F)

Pressurizer pressure, psig po Indicated RCS nominal operating pressure (2235 psig or 2085 psig) 1+ S The function generated by the lead-lag controller for Tavg dynamic compensation 1+7 S Time constants utilized in the lead-lag controller for T = 22 sees/

1' avg <

= 4 secs.

'2 S Laplace transform operator 0

1 ~ 2 O

I U

U x 00 1.0 (6. 0, 1. 0)

1. 0 CL Cl (12. 0, 0. 925 N
0. 8 0

X

0. 6 4 6 8 10 CORE HEIGHT (FT)

FIGURE 3. 2-3 K(Z) - Normalized F sub Q(z) as a function of Core Height D. C COOK - NIT 1 3/4 2-8

i~.

1g E

POWER DISTRIBUTION LIMITS NUCLEAR ENTHALPY HOT CHANNEL FACTOR - FAH LIMITING CONDITION FOR OPERATION 3.2.3 F shall be limited by the following relationship:

FAH < 1.49 [1 + 0.3 (1-P)]

Where P is the fraction of RATED THERMAL POWER APPLICABILITY'ODE 1 ACTION:

With F exceeding its limit-Reduce THERMAL POWER to less than 50% of RATED THERMAL POWER within 2 hours2.314815e-5 days <br />5.555556e-4 hours <br />3.306878e-6 weeks <br />7.61e-7 months <br /> and reduce the Power Range Neutron Flux-High Trip Setpoints to less than or equal to 55% of RATED THERMAL POWER within the next 4 hours4.62963e-5 days <br />0.00111 hours <br />6.613757e-6 weeks <br />1.522e-6 months <br />,

b. Demonstrate through in-core mapping that F is within its limit within 24 hours after exceeding the Pimit or reduce THERMAL POWER to less than 5% of RATED THERMAL POWER within the next 2 hours2.314815e-5 days <br />5.555556e-4 hours <br />3.306878e-6 weeks <br />7.61e-7 months <br />, and Identify and correct the cause of the out-of-limit condition prior to increasing THERMAL gOWER; subsequent POWER OPERATION may proceed, provided that F" is demonstrated through in-core mapping to be within its limi% at a nominal 50% of RATED THERMAL POWER prior to exceeding this THERMAL POWER, at a nominal 75% of RATED THERMAL POWER prior to exceeding this THERMAL POWER and within 24 hours2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> after attaining 95% or greater RATED THERMAL POWER.

COOK NUCLEAR PLANT UNIT 1 3/4 2-9 AMENDMENT NO.

TABLE 3.2-1 DNB PARAMETERS LIMITS 4 Loops in Operation PARAMETER at RATED THERMAL POWER Reactor Coolant System Tavg < 570.9 F

)

    • Limitnot applicable during either a THERMAL POWER ramp increase in excess of 5 percent RATED THERMAL POWER per minute or a THERMAL POWER step increase in excess of 10 percent RATED THERMAL POWER.
      • Indicated value COOK NUCLEAR PLANT UNIT 1 3/4 2-14 AMENDMENT NO.

POWER DISTRIBUTION LIMITS ALLOWABLE POWER LEVEL - APL LIMITING CONDITION FOR OPERATION 3.2.6 THERMAL POWER shall be less than or equal to ALLOWABLE POWER LEVEL (APL), given by the following relationship:

~2.1> K Z x 100e, or 100S, whichever is less.

F (Z)xV(Z)xF P

'F (Z) is the measured hot channel factor including a 3%

manufacturing tolerance uncertainty and a 5S measurement uncertainty.

'V(Z) is the function defined in the Peaking Factor Limit Report.

'F 1.00 except when successive steady-state power distribution maps indicate an increase in max over Z of F Z (2) with exposure. Then either of the penalties, F , shall be taken: P F - 1.02, or P

F 1.00 provided that Surveillance Requirement 4.2.6.2 iS satisfied once per 7 Effective Full Power Days until two successive maps indicate that the max over Z of F Z K Z) is not increasing.

'The above limit is not applicable in the following core regions.

1) Lower core region 0$ to 10% inclusive.
2) Upper core region 90% to 100$ inclusive.

APPLICABILITY: MODE 1 COOK NUCLEAR PLANT UNIT 1 3/4 2-15 AMENDMENT NO.

TABLE 3.3-2 REACTOR TRIP SYSTEM INSTRUMENTATION RESPONSE TIMES FUNCTIONAL UNIT RESPONSE TIME

1. Manual Reactor Trip NOT APPLICABLE
2. Power Range, Neutron Flux
a. High Setpoint < 0.5 seconds
b. Low Setpoint < 0.5 seconds*
3. Power Range, Neutron Flux, High Positive Rate NOT APPLICABLE
4. Power Range, Neutron Flux, I High Negative Rate < 0.5 seconds I

o

5. Intermediate Range, Neutron Flux NOT APPLICABLE
6. Source Range, Neutron Flux NOT APPLICABLE
7. Overtemperature Delta T 6.0 seconds

&. Overpower Delta T NOT APPLICABLE

9. Pressurizer Pressure--Low < 1.0 seconds g 10. Pressurizer Pressure--High < 1.0 seconds W

R

'p3 R

O ll. Pressurizer Water Level--High < 2.0 seconds

  • Neutron detectors are exempt from response time testing. Response time of the neutron flux signal portion of the channel shall be measured from detector output or input of first electronic component in channel.

TABLE 3.3-4 ENGINEERED SAFETY FEATURE ACTUATIOII SYSTEII IHSTRUtlENTATION TRIP SETPOlf ITS FIIIICTIOIIAL UNlT TRlP SETPOINT ALLOWABLE VALUES

1. SAFETY INJECTION, TURBINE TRIP, FEEOIIATER ISOLATION, AND tiOTOR DRIVEN FEEOIIATER PNIPS
a. Ilanua I Inl ti a t 1 on tlot Appl icable Ilot Appl 1 cabl e
b. Aut.orna tie Actus t Ion Logic Ilot Applicable Hot Applicable
c. Containment Pressure Iiigh < 1.1 psig < 1.2 psig
d. Pressurizer Pressure--Low 18l5 psig l805 psig
e. Di f ferential Pressure < 100 psi < 112 psi Betv>een Steam Lines--Iligh
f. Steam Flow in Two Steam Lines < 1.42 x 10 lbs/hr < 1.56 x 10 lbs/hr High Coincident or Steam Line with T Pressure-"-(oe Lov>-Lm Prom OX load load.

to 20K Ligear from from 0ll load load. Linear from to 20" 1.42 x 10 lbs/hr 1.56 x 10 lbs/hr at620X load to 3.8B x at620" load to 3.93 x 10 lbs/hr at lOOX load 10 lbs/hr at 100K load.

T>541F T>539F 500 ysig steaii line >

a/n psig steam line ppessure prissure

TABLE 3. . (Continued)

ENGINEERED SAFETY FEATURE ACTUATION SYSTEH INSTRUHENTATION TRIP SETPOIHTS n

OB FUNCTIONAL UNIT TRIP SETPOINT ALLOWABLE VALUES I 2. Containment Radioactivity-- See Table 3.3-6 Hot Applicable High Train A (VRS-1101, g ERS-1301, ERS-1305)

3. Containment Radioactivity-- See Table 3. 3-6 Hot Applicable High Train B (VRS-1201, ERS-1401, ERS-1405)

STEAH LINE ISOLATION

a. Hanual Hot Applicable Hot Applicable
b. Automatic Actuation Logic Hot Applicable Not Appl icable
c. Containment Pressure High-High << 2 9 pslg ~ 3 psig 6 6
d. Steam Flow In Two Steam Lines 1.42 x l0 lbs/hr from 0% l.56 x 10 lbs/hr from Oi High Coincident with Tava load to 2I)a load. Linear from load to 20 E 1ogd. Linear Low-Low or Steam Line Sressure 1.42 x 10 lgs/hr at 20% load from 1.56 x 10 1bs/hg at Low to 3.88 x 10 lbs/hr at 100% 20% load to 3.93 x 10 lbs/

load. hr at 100L load.

'l' T

avg-~ 54l F avg 539 F

> 500 psig steam line pressure 480 psig steam line pressure I k

5 TURBINE TRIP AHD FEEDWATER ISOLATION

a. Steam Generator Water Level 4 67% of narrow-range instrument 68% of narrow-range High-High span each steam generator 4'nstrument span each steam generator

~ REACTOR COOLANT SYSTEM t

PRESSURIZER LIMITING CONDITION FOR OPERATION 3.4.4 The pressurizer shall be OPERABLE with a water volume less than or equal to 928 of span and at least 150 kW of pressurizer heaters.

APPLICABILITY: MODES 1,2, and 3.

ACTION:

With the pressurizer inoperable due to an inoperable emergency power supply to the pressurizer heaters either restore the inoperable emergency power supply within 72 hours8.333333e-4 days <br />0.02 hours <br />1.190476e-4 weeks <br />2.7396e-5 months <br /> or be in at least HOT STANDBY within the next 6 hours6.944444e-5 days <br />0.00167 hours <br />9.920635e-6 weeks <br />2.283e-6 months <br /> and in HOT SHUTDOWN within the following 12 hours1.388889e-4 days <br />0.00333 hours <br />1.984127e-5 weeks <br />4.566e-6 months <br />. With the pressurizer otherwise inoperable, be in at least HOT SHUTDOWN with the reactor trip breakers open within 12 hours1.388889e-4 days <br />0.00333 hours <br />1.984127e-5 weeks <br />4.566e-6 months <br />.

SURVEILLANCE RE UIREMENTS 4.4.4.1 The pressurizer water volume shall be determined to be within its limits at least once per 12 hours1.388889e-4 days <br />0.00333 hours <br />1.984127e-5 weeks <br />4.566e-6 months <br />.

4.4.4.2 The emergency power supply for the pressurizer heaters shall be demonstrated OPERABLE at least once per 18 months by transferring power from the normal to the emergency power supply and energizing the required capacity of heaters.

COOK NUCLEAR PLANT UNIT 1 3/4 4-6 AMENDMENT NO.

Ll' g k

'4

EMERGENCY CORE COOLING SYSTEMS (ECCS 3 4.5 ACCUMULANRS LIMITING CONDITION FOR OPERATIC'<

3.5.1 Each reactor coolant system accumulator shall be OPERABLE with:

a. The isolation valve open,
b. A contained borated water volume of between ~2> and 971 cubic feet,
c. A boron concentration of between 2400 ppm and 2600 ppm, and
d. A nitrogen cove."-pressure of between 585 and 658 psig.

APPLICABILITY: MODES t, 2 and 3.>>

ACTION:

a. With one accu.-.. gator inoperable, except as a result of a closed isolation valve, restore the inoperable accumulator to OP'ERABLE status within one hour or be in HOT SHUiDOWN within the next 8 hours.
b. With one accumu1ator inoperable due to the isolation valve being closed, either iwnediately open the isolation valve or be in HOT STANDBY within one'hour and be in HOT SHUTDOWN within the next 8 hours.

SURVEILLANCE RE UIREMENTS 4.5.1 Each accumulator shall be demonstrated OPERABLE:

a. At least once per l2 hours by:
l. Verifying the water level and nitrogen cover-pressure in tge tanks, and
2. Verifying hat each accumulator isolation valve is open.

" Pressurizer Pressure above 1000 psig.

0. C. COOK - UNIT 1 3/4 5-1 Amendment No.

EMERGENCY CORE COOLING SYSTEMS SURVEILLANCE REQUIREMENTS (Continued)

d. At least once per 18 months by:*
1. Verifying automatic isolation and interlock action of the RHR system from the Reactor Coolant System when the Reactor Coolant System pressure is above 600 psig.
2. A visual inspection of the containment sump and verifying that the subsystem suction inlets are not restricted by debris and that the sump components (trash racks, screens, etc.) show no evidence of structural distress or abnormal corrosion.
e. At least once per 18 months, during shutdown, by:
l. Verifying that each automatic valve in the flow path actuates to its correct position on a Safety Injection test signal.
2. Verifying that each of the following pumps start automatically upon receipt of a safety injection test signal:

a) Centrifugal charging pump b) Safety injection pump c) Residual heat removal pump

f. By verifying that each of the following pumps develops the indicated discharge pressure on recirculation flow when tested pursuant to Specification 4.0.5 at least once per 31 days on a STAGGERED TEST BASIS.
1. Centrifugal charging pump > 2405 psig
2. Safety Injection pump > 1345 psig
3. Residual heat removal pump > 165 psig
g. By verifying the correct position of each mechanical stop for the following Emergency Core Cooling System throttle valves:
1. Vithin 4 hours4.62963e-5 days <br />0.00111 hours <br />6.613757e-6 weeks <br />1.522e-6 months <br /> following completion of each valve stroking operation or maintenance on the valve when the ECCS subsystems are required to be OPERABLE.
  • The provisions of Specification 4.0.6 are applicable.

Cook Nuclear Plant Unit 1 3/4 5-5 Amendment No.

k~

~ . Pn ~ lR Wl Q'e h r$

ri~P

)

EM GENCY CORE COOLING SYSTEMS SURVEILLANCE REQUIREMENTS (Continued

2. At least once per 18 months.

Boron Injection Safety Injection Throttle Valves Throttle Valves Valve Number Valve Number

1. 1-SI-141 Ll 1. 1-SI-121 N
2. 1-SI-141 L2 2. 1-SI-121 S
3. 1-SI-141 L3
4. 1-SI-141 L4
h. By performing a flow balance test during shutdown following completion of modifications to the ECCS subsystem that alter the subsystem flow characteristics and verifying the following flow rates:

Boron Injection System Safety Injection System Loop 1 Boron Injection Loop 1 and 4 Cold Leg Flow 117.5 gpm Flow > 300 gpm Loop 2 Boron Injection Loop 2 and 3 Cold Leg Flow 117.5 gpm Flow > 300 gpm Loop 3 Boron Injection **Combined Loop 1,2,3 and 4 Cold Flow 117.5 gpm Leg Flow (single pump) less than or equal to 640 gpm. Total SIS (single pump) flow, including Loop 4 Boron Injection miniflow, shall not exceed Flow 117.5 gpm 700 gpm.

  • The flow rate in each Boron Injection (BI) line should be adjusted to provide 117.5 gpm (nominal) flow in each loop. Under these conditions there is zero miniflow and 80 gpm simulated RCP seal injection line flow.

The actual flow in each BI line may deviate from the nominal so long as:

a) the difference between the highest and lowest flow is 10 gpm or less.

b) the total flow to the four branch lines does not exceed 470 gpm.

c) the minimum flow (total flow) through the three most conservative (lowest flow) branch lines must not be less than 345.8 gpm.

d) The charging puyp discharge resistance (2.31xPd/Qd ) must no) be less than 4.73E-3 ft/gpm and must not be greater than 5.33E-3 ft/gpm . (Pd is the pump discharge pressure at runout; Qd is the total pump flow rate.)

COOK NUCLEAR PLANT UNIT 1 3/4 5-6 AMENDMENT NO.

I*

0 Ol It~

PLIGHT 5YSTKl%

AQXILZ1W ~ATKR SYST LQGTQC CON)ITICN FCR OPED ICN 3.7.1.2 At least three irdependent steam generator auxiliary teedwater Vms and assoc. a=ed flow paths shall be OPEBABLE with!

Two feedwater pumps, each capable of being powered from separate emergency busses, and

b. Cne feedwater pump caoable of being powered from an OPERABLE steam supply system.

APPLICABIL .Y: NODES 1, 2. and 3.

ACTZCN:

a. wi"h one aux 'ary feedwater pump inoperable, restore the required auxiLiary feedwate "umps to OpERABLE status within 72 hours8.333333e-4 days <br />0.02 hours <br />1.190476e-4 weeks <br />2.7396e-5 months <br /> or be in at least HOT S-ANDBY within the next 6 bours and in wxthin the following 6 hours. HCC'HUTDCWN
b. With wo a'iliary feedwater pumps irc" abler be in at least HOT S-.ANDBY wi"h'n 6 haurS and in HOT SHU-.".W Within the fOllOWing 6 hours6.944444e-5 days <br />0.00167 hours <br />9.920635e-6 weeks <br />2.283e-6 months <br />.

C ~ With three auxiliary feedwater pumps i.".:perable, iamhdiately init'ate correctire action to restore at least one auxiliary feedwater pump to OPERABLE sta'tus as soon as possible.

SURVEILLANCE RE UIRENENTS 4.7.1.2 Each auxi3.mary feedwater pump shall be deaenstrated OPERABLE

a. At least once per 31 days by>
1. verifying that each motor driven pump develops an 0 equivalent discharge pressure of ~ 137$ psig at 60 F

".". recir elation flow.

er.'fy'ng that, the steam turbine driven pump develops an cuivalert discharge pressure of > 1285 psig at 60 2'nd a: a low of ) 700 gpm when the secondary steam supply pressure is greater than 310 psig. The provisions of Soecif'cation 4.0.4 are not applicable for entry into vCDE 3 D. C. COOK UNIT 1 3/47 5 Amendment No.

J 'k-e any a,

a. '

~

2.1 SAFETY LIMITS BASES 4 Loop Operation Westinghouse Fuel (15x15 OFA)

(WRB-1 Correlation)

Typical Cell Thimble Cell Correlation Limit 1.17 1.17 Design Limit DNBR 1.33 1.32 Safety Analysis Limit DNBR 1 45

~ 1.45 The curves of Figure 2.1-1 show the loci of points of THERMAL POWER, Reactor Coolant System pressure and average temperature for which the minimum DNBR is no less than the applicable design DNBR limit, or the average enthalpy at the vessel exit is equal to the enthalpy of saturated liquid.

~represents

  • typical fuel rod represents fuel rods near guide tube Cook Nuclear Plant Unit 1 B 2-1(a) Amendment No.

k k

SQ'ETY LIMITS.

BASES The curves are based on an enthalpy hot channel factor >, of 1.49 for Westinghouse fuel and a reference cosine axial power shape with a peak of 1.55. An allowance is included for an increase in 'P+ at reduced power, based on the expression:

P - 1.49 (1 + 0.3 (1-P)j where P is the fraction of RATED THERMAL POWER Note, do not include a 4% uncertainty value, since this measurement uncertainty has been included in the design DNBR limit values, which are listed in the bases for Section 2.1.1.

These limiting heat flux conditions are higher than those calculated for the range of all control rods fully withdrawn to the maximum allowable control rod insertion, assuming the axial power imbalance is within the limits of the fl (delta I) function of the Overtemperature trip. When the axial power imbalance is not within the tolerance, the axial power imbalance effect on the Overtemperature delta T trips will reduce the setpoints to provide protection consistent with the core safety limits.

2.1.2 REACTOR COOLANT SYSTEM PRESSURE The restriction of this Safety Limi,t protects the integrity of the Reactor Coolant System from overpressurization and thereby prevents the release of radionuclides contained in the reactor coolant from reaching the containment atmosphere.

COOK NUCLEAR PLANT UNIT 1 B 2-2 AMENDMENT NO.

I.f k

'A

~ ll fl'f, '4 k 'C 1 1

~5

't I

~ Jv" t

Pq

SAFETY LIMITS BASES The Power Range Negative Rate Trip provides protection for control rod drop accidents. At high power, a rod drop accident could cause local flux peaking which could cause an unconservative local DNBR to exist.

The Power Range Negative Rate Trip will prevent this from occurring by tripping the reactor. No credit is taken for operation of the Power Range Negative Rate Trip for those control rod drop accidents for which the DNBR's will be greater than the applicable design limit DNBR value for each fuel type.

Intermediate and Source Ran e Nuclear Flux The Intermediate and Source Range, Nuclear Flux trips provide reactor core protection during reactor startup. These trips provide redundant protection to the low setpoint trip of the Power Range, Neutron Flux channels.> The source Range Channels will initiate a reactor trip at about 10 counts per second, unless manually blocked when P-6 becomes active. The Intermediate Range Channels will initiate a reactor trip at a current level proportional to approximately 25 percent of RATED THERMAL POWER unless manually blocked when P-10 becomes active. No credit was taken for operation of the trips associated with either the Intermediate or Source Range Channels in the accident analyses; however, their functional capability at the specified trip settings is required by this specification to enhance the overall reliability of the Reactor Protection System.

Overtem erature delta T The Overtemperature delta T trip provides core protection to prevent DNB for all combinations of pressure, power, coolant temperature, and axial power distribution, provided that the transient is slow with respect 'to piping transit delays from the core to the temperature detectors (about 4 seconds), and pressure is within the range between the High and Low Pressure reactor trips. This setpoint includes corrections for changes in density and heat capacity of water with temperature and dynamic compensation for piping delays from the core to the loop temperature detectors. The reference average temperature (T') and the reference operating pressure (P') are set equal to the full power indicated Tavg and the nominal RCS operating pressure, respectively, to ensure protection of the core limits and to preserve the actuation time of the Overtemperature delta T trip for the range of full power average temperatures assumed in the safety analyses. With normal axial power distribution, this reactor trip limit is always below the core safety limit as shown in Figure 2.1-1. If axial peaks are greater than design, as indicated by the difference between top and bottom power range nuclear detectors, the reactor trip is automatically reduced according to the notations in Table 2.2-1.

COOK NUCLEAR PLANT UNIT 1 B 2-4 AMENDMENT NO.

p t gp 1Q

'I 1

~

'I5ITING.SAFETY SYSTEM SETTINGS BASES Ove ower delta T The Overpower delta T reactor trip provides assurance of fuel integrity, e.g., no melting, under all possible overpower conditions, limits the required range for Overtemperature delta T protection, and provides a backup to the High Neutron Flux trip. The setpoint includes corrections for changes in density and heat capacity of water with temperature, and dynamic compensation for piping delays from the core to the loop temperature detectors. The reference average temperature (T"} is set equal to the full power indicated Tavg to ensure fuel integrity during overpower conditions for the range of full power average temperatures assumed in the safety analy is. No credit was taken for operation of this trip in the accident analyses; however, its functional capability at the specified trip setting is required by this specification to enhance the overall reliability of the Reactor Protection System.

Pressurizer Pressure The Pressurizer High and Low Pressure trips are provided to limit the pressure range in which reactor operation is permitted. The High Pressure trip is backed up by the pressurizer code safety valves for RCS overpressure protection, and is therefore set lower than the set pressure for these valves (2485 psig). The High Pressure trip provides protection for a Loss of External Load event. The Low Pressure trip provides protection by tripping the reactor in the event of a loss of reactor coolant pressure.

Pressurizer Water Level The Pressurizer High Water Level trip ensures protection against Reactor Coolant System overpressurization by limiting the water level to a volume sufficient to retain a steam bubble and prevent water relief through the pressurizer safety valves. The pressurizer high water level trip precludes water relief for the Uncontrolled RCCA Withdrawal at Power event.

COOK NUCLEAR PLANT UNIT 1 B 2-5 AMENDMENT NO.

II f

~

f

3 4.2 IOWER DISTRIBUTION LIMITS BASES The specifications of this section provide assurance of fuel integrity during Condition I (Normal Operation) and II (Incidents of Moderate Frequency) events by: (a) maintaining the minimum DNBR in the core greater than or equal to the safety limit DNBR during normal operation and in short term transients, and (b) limiting the fission gas release, fuel pellet temperature and cladding mechanical properties to within assumed design criteria. In addition, limiting the peak linear power density during Condition I events provides assurance that the initial conditions assumed for the LOCA analyses are met and the ECCS acceptance criteria limit of 2200 F is not exceeded.

The definitions of hot channel factors as used in these specifications are as follows:

F (Z) Heat Flux Hot Channel Factor, is defined as the maximum local heat flux on the surface of a fuel rod at core elevation Z divided by the average fuel rod heat flux, allowing for manufacturing tolerances on fuel pellets and rods.

N F~ Nuclear Enthalpy Rise Hot Channel Factor, is defined as the ratio of the integral of linear power along the rod with the highest integrated power to the average rod power.

3 4.2.1 AXIAL FLUX DEFFERENCE AFD Target flux difference is determined at equilibrium xenon conditions.

The full length rods may be positioned within the core in accordance with their respective insertion limits and should be inserted near their normal position for steady state operation at high power levels. The value of the target flux difference obtained under these condtions divided by the fraction of RATED THERMAL POWER is the target flux difference at RATED THERMAL POWER for the associated core burnup conditions'arget flux differences for other THERMAL POWER levels are obtained by multiplying the RATED THERMAL POWER value by the appropriate fractional THERMAL POWER level. The periodic updating of the target flux difference value is necessary to reflect core burnup considerations.

COOK NUCLEAR PLANT UNIT 1 B 3/4 2-1 AMENDMENT NO.

~ gl II A

CObTAINMENT SYSTEMS BASES 3 4.6.1.4 INTERNAL PRESSURE The limitations on containment internal pressure ensure that 1) the containment structure is prevented from exceeding its design negative pressure differential with respect to the outside atmosphere of 8 psig and 2) the containment peak pressure does not exceed the design pressure of 12 psig during LOCA conditions.

The maximum peak pressure resulting from a LOCA event is calculated to be 11.89 psig, which includes 0.3 psig for initial positive containment pressure.

3 4.6.1.5 AIR TEMPERATURE The limitations on containment average air temperature ensure that 1) the containment air mass is limited to an initial mass sufficiently low to prevent exceeding the design pressure during LOCA conditions and 2) the ambient air temperature does not exceed that temperature allowable for the continuous duty rating specified for equipment and instrumentation located within containment.

The containment pressure transient is sensitive to the initially contained air mass during a LOCA. The contained air mass increases with decreasing temperature. The lower temperature limit of 60 F will limit the peak pressure to 11.89 psig which is less than the containment design pressure of 12 psig. The upper temperature limit influences the peak accident temperature slightly during a LOCA; however, this limit is based primarily upon equipment protection and anticipated operating conditions.

Both the upper and lower temperature limits are consistent with the parameters used in the accident analyses.

3 4.6.1.6 CONTAINMENT VESSEL STRUCTURAL INTEGRITY This limitation ensures that the structural integrity of the containment steel vessel will be maintained comparable to the original design standards for the life of the facility. Structural integrity is required to ensure that (1) the steel liner remains leak tight and (2) the concrete surrounding the steel liner remains capable of providing external missile protection for the steel liner and radiation shielding in the event of a LOCA. A visual inspection in conjunction with Type A leakage tests is sufficient to demonstrate this capability.

COOK NUCLEAR PLANT UNIT 1 B 3/4 6-2 AMENDMENT NO.

0 A ~, .

<r K.

lg

(,~ ~

'P .

1 h 4