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An Adaptive Metamodel-Based Subset Importance Sampling approach for the assessment of the functional failure probability of a thermal-hydraulic passive system

Nicola Pedroni, Enrico Zio

To cite this version:

Nicola Pedroni, Enrico Zio. An Adaptive Metamodel-Based Subset Importance Sampling approach

for the assessment of the functional failure probability of a thermal-hydraulic passive system. Applied

Mathematical Modelling, Elsevier, 2017, 48, pp.269-288. �10.1016/j.apm.2017.04.003�. �hal-01652225�

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Applied Mathematical Modelling 48 (2017) 269–288

ContentslistsavailableatScienceDirect

Applied Mathematical Modelling

journalhomepage:www.elsevier.com/locate/apm

An Adaptive Metamodel-Based Subset Importance Sampling approach for the assessment of the functional failure

probability of a thermal-hydraulic passive system

Nicola Pedroni

a,

, Enrico Zio

a,b

aChair on Systems Science and the Energetic Challenge, Fondation Electricité de France (EdF), Laboratoire Genie Industriel (LGI), Université Paris-Saclay-Ecole CentraleSupelec, Grande Voie des Vignes, 92290 Chatenay-Malabry, France

bEnergy Department , Politecnico di Milano , Via Ponzio 34/3 , 20133 Milano , Italy

a r t i c l e i n f o

Article history:

Received 9 June 2015 Revised 8 March 2017 Accepted 3 April 2017 Available online 7 April 2017 Keywords:

Nuclear passive safety system Small failure probability Efficient Monte Carlo Subset Simulation

Non-parametric importance sampling Adaptive metamodeling

a b s t r a c t

AnAdaptiveMetamodel-BasedSubsetImportanceSampling(AM-SIS)approach,previously developedbytheauthors,ishereemployedtoassessthe(small)functionalfailureprob- abilityofathermal-hydraulic(T-H)nuclearpassivesafetysystem.Theapproachrelieson aniterativeImportanceSampling(IS)schemethatefficientlycouplesthepowerfulcharac- teristicsofSubsetSimulation(SS)andfast-runningArtificialNeuralNetworks(ANNs).In particular,SSandANNsareintelligentlyemployedtobuildandprogressivelyrefineafully nonparametricestimatoroftheideal,zero-varianceImportanceSamplingDensity(ISD),in orderto:(i)increasetherobustnessofthefailureprobabilityestimatesand(ii)decrease thenumberofexpensiveT-Hsimulationsneeded(togetherwiththerelatedcomputational burden).

The performance ofthe approach is thoroughlycompared tothat of otherefficient MonteCarlo(MC)techniquesonacasestudyinvolvinganadvancednuclearreactorcooled byhelium.

© 2017 Elsevier Inc. All rights reserved.

1. Introduction

Thenuclearindustryischaracterizedbylevelsofriskthatareamongthelowestwithrespecttoanyengineeringappli- cation,asrequestedbythestrongpublicperception.Inthepastandcurrentgenerationsofreactordesigns,theselowlevels ofriskaretypically achievedby resortingmostlytoactive safetysystems.Ontheother hand,themostinnovative reactor concepts,suchasthoseofGenerationIV,aimatrelyingalmostentirelyonpassivesafetysystems,thusbecomingasmuch independentaspossible fromany kindofexternal input, especiallyenergy [1]. Moreover, thesimplicityof thedesign of thesesystemsissuchthatmechanicalfailuresbecomeveryunlikelytohappen,incontrasttoactivesystems[2–7].

Yet, uncertainties in the operation of these systems (due to not fully understood physical phenomenaand scarce, if notnull,operatingexperience[8,9])maygiverisetofunctionalfailures.Apassivesystemfailstoperformitsfunction(e.g., decayheatremovalbynaturalcirculation)duetodeviationsfromitsexpectedbehavior,whichleadtheloadimposedonthe systemtoovercomeitscapacity[10–24].Aclassicalapproachtoestimatingsuchfunctionalfailureprobabilitystemsfromthe deterministicmodelingofthe Thermo-Hydraulics(T-H)ofthepassivesystemby a(possiblylong-running)computer code

Corresponding author.

E-mail addresses: [email protected] , [email protected] (N. Pedroni), [email protected] , [email protected] (E. Zio).

http://dx.doi.org/10.1016/j.apm.2017.04.003 0307-904X/© 2017 Elsevier Inc. All rights reserved.

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andthesubsequentMonteCarlo(MC)propagationoftheuncertainties,describedbyproperlyidentifiedProbabilityDensity Functions (PDFs), tosome modeloutputs withrespecttowhichthe failureeventis defined.The propagationisbasedon repeatedcomputerruns(orsimulations)oftheT-Hcodeincorrespondenceofdifferentsetsoftheuncertaininputvalues sampledfromtheirPDFs[25–36].

Inpractice,apassivesafetysystemisobviouslydesignedsothatitsfailure isarareevent.As aconsequence,its prob- ability offailure isquite small(e.g.,about105 orless) andits estimationmayrequirea large amountof T-Hcomputer coderuns[37].Sinceeachsimulationofthedetailed,mechanisticT-Hmodelmaytakeseveralhoursinsomecases[33],the standardMCsimulation-basedproceduretypicallyrequiressignificantcomputationalefforts.Moreefficienttechniquesmust thenbesought[38,39].

Twofamiliesofmethodsaretypicallyemployed toaddresstheseissues.Onone side,fast-runningsurrogateregression models(alsocalledresponsesurfacesormetamodels)canbeproperlybuilttomimictheresponseoftheoriginalT-Hmodel code:sincethemetamodelis,ingeneral,muchfastertobeevaluated,theproblemoflongcomputingtimesiscircumvented.

Severalkindsofsurrogatemetamodelshavebeenrecentlyapplied tosafety-relatednuclear, structuralandhydrogeological problems,includingpolynomialResponseSurfaces(RSs)[40–43],polynomialchaos expansions[44–47],stochastic colloca- tions[48,49],ArtificialNeuralNetworks(ANNs)[50–53],SupportVectorMachines(SVMs)[54,55]andkriging[56–61].

Ontheotherside,advancedMonteCarloSimulationmethodscanbeadoptedtorealizerobustestimationsbymeansof alimitedamountofrandomsamples[62–64].ThisclassofmethodsincludesStratifiedSampling[65,66],SubsetSimulation (SS) [67–74],the Response Conditioning Method (RCM) [75,76]for structuralreliability analysis (also developed from SS andemployingapproximatesolutions), LineSampling(LS) [77–84]andsplittingmethods[85–89].However, theadvanced MCSmethodsthatisadoptedmorefrequentlyisperhapsImportanceSampling(IS),wheretheoriginalPDFoftheuncertain inputsis replaced by aproper Importance SamplingDensity (ISD):this favorsthe MC samplesto lie closeto the failure region, thusartificiallyincreasing the frequencyofthe (rare)failure event[90–92].Inthis respect,itis possibleto show thatthereisanoptimal(ideal)ISDthatmakesthestandarddeviationoftheMCestimatorequaltozero.Ontheotherhand, thisoptimalISDcannot be used inpractice,because itsmathematical expressioncontainsthe (aprioriunknown) failure probabilityitself.Withinthiscontext,severaltechniquesinvariousfieldsofresearchhavebeenproposedtoapproximatethe

“ideal” optimalISD:see,e.g.,theAdaptive Kernel(AK)[93,94],theCross-Entropy(CE)[95–97],theVariance Minimization (VM)[98]andtheMarkovChainMonteCarlo-ImportanceSampling(MCMC-IS)[99]methods.

Inthepresentpaper,theAdaptiveMetamodel-basedSubsetImportanceSampling(AM-SIS)method,originallydeveloped bytheauthors[100],isadopted.Intheapproach,thecharacteristicsofseveraladvancedcomputationalmethodsofliterature areefficientlycombined.Inparticular,SSandANNmetamodelsarecoupledwithinan adaptiveISschemeinthefollowing twostages[99,100]:

1. arandomsampleapproximatelydistributedastheideal,zero-varianceISDiscreatedbyresortingtotheSubsetSimulation (SS)technique.NoticethatatthisstepwesubstitutetheexpensiveT-HcodewithanANNmetamodel(adaptivelyrefined intheareasclosetothefailureregionbymeansofthesamplesiterativelyproducedbySS),withtheaimofreducingthe relatedcomputationalburden.Then,weadoptafullynonparametricPDF(proposedinRef.[99]andrelyingontheGibbs Sampler[101])to“fit” thesamplestherebygeneratedandobtainanestimatorfortheoptimalISD;

2. weemploythequasi-optimalISDestimatorbuiltatstep(1)above toperformImportanceSampling(IS)andassessthe functionalfailureprobabilityoftheT-Hpassivesystem.

Noticethattheideaof“interlacing” metamodelswithefficientMCSschemeshasbeenalreadyproposedintheliterature fordecreasingthecomputationalburdenassociatedtothequantificationofsmallprobabilities:see,e.g.,Refs.[102–113].In theseworks,themetamodelisbuiltandprogressivelyrefined(bymeansofsamplesintelligentlygeneratedbytheadvanced MCtechnique)untiladesiredlevelofaccuracyandprecisioninthefailureprobabilityestimateisobtained.

ThemaincontributionsofthepresentworkwithrespecttothereferencepaperbyRef.[99]arethefollowing:

weadoptSubsetSimulation(SS)forthegenerationofsamplesapproximatelydistributedaccordingtothezero-variance ISD;

weemployANNstodecreasethecomputationaleffortrelatedtotheapproximationofthezero-varianceISD:inpartic- ular,wetrainthesemetamodelsthroughanadaptivealgorithmthat makesasmartuseofthesamplesproducedby SS withtheobjectiveofprogressivelyamelioratingtheANNaccuracyaroundthefailureregion;

weassesstheefficiencyofAM-SISintheestimationofsmallfunctionalfailureprobabilitieswithaverysmallnumberof callstotheT-Hcode(e.g.,oftheorderoffewtensorhundreds):thisisrelevantforthosepracticalcaseswhereasingle simulationneedsseveralhourstorun;

weextensivelyandsystematicallycomparetheperformanceofAM-SIStothatofnumerousotheradvancedprobabilistic simulationmethodsofliterature.

Inaddition,thenovelcontentsofthispaperinrelationtothepreviousarticlebytheauthors[100]arethefollowing:

inRef. [100], thefocus ofthe comparisonsbetween AM-SISand other MC schemes (inparticular, standard MCS, LHS [65],IS[90–94]andLS[77–84])isexclusivelyputontheefficiencyofstage(2)ofthealgorithm,i.e.,ofrandomimpor- tancesamplingforfailureprobabilityestimation.Inthiswork,instead,comparisonsaremadealsotoothermethodsthat combineSSandmetamodelsandthatareveryclosetostage(1)ofourapproach.Inparticular,thefollowingtechniques

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N. Pedroni, E. Zio / Applied Mathematical Modelling 48 (2017) 269–288 271

are considered: (i) the 2SMART algorithm [105],which combines SSandSVMs inan original active learningscheme, wherefew trainingpointsare placedsequentiallyinthe uncertainvariablespace,inorderto builda sequenceofSVM metamodels asaccurate surrogatesoftheSSintermediate thresholds;(ii)theNeuralNetwork-basedSubset Simulation (SS-NN) method [113], inwhich informationis transferred from theMCMC algorithm to theANN trainingprocess in ordertoefficientlyconstructthemetamodelinasequenceof“movingwindows”;

also the performance of stage (1) of the AM-SIS method is assessed more thoroughly by carrying out a larger set of comparisons(e.g.,byconsideringdifferentsamplesizesforfailureprobabilityestimation);

we have modifiedandimproved the techniqueadoptedto identify, selectand“distribute” in the entireuncertain in- put space the (training) samples used to adaptivelyrefine the ANN metamodelthrough the iterations of theAM-SIS algorithm.

AlltheanalysesareperformedwithregardstothesamecasestudyconsideredinRef.[100],whichconcernsaGas-cooled FastReactor(GFR)cooledbynaturallycirculatingheliumafteraLossOfCoolantAccident(LOCA)(modifiedfromRef.[26]).

Theremainderofthepaperisorganizedasfollows.InSection2,theconceptsoffunctionalfailureanalysisforT-Hpassive systemsaresyntheticallysummarized.Section3,aquitedetaileddescriptionoftheAM-SIStechniqueproposedinthiswork isgiven.Section4presentsthecasestudyconcerningthepassivecoolingofaGFR,andthecorrespondingresultsareshown anddiscussed inSection5.Someconclusionsaredrawn inthelastSection. Finally,forthesake ofpaperself-consistency, theAppendixreportsthoroughmathematicaldetails concerningtheconstruction ofthefullynonparametricISDproposed inRef.[99]andbasedonthewell-knownGibbsSampler[101].

2. ThequalitativeandquantitativestepsoffunctionalfailureanalysisofT-Hpassivesystems

Thebasicsteps ofthe qualitative andquantitativephase ofthe functionalfailure analysisofa T-Hpassivesystem are [25]:

1.Characterizetheaccidentscenarioinwhichthepassivesystemunderconsiderationoperates;

2.Definethefunctionthatthepassivesystemisexpectedtoperform,e.g. decayheatremoval,vesselcooling anddepres- surization,etc.

3.Identify thedesignparameters values(e.g.,power level,systempressure,heatexchangerinitial walltemperature, etc.) relatedtothereferenceconfigurationofthepassivesystemandthecorrespondingnominalfunction.

4.Identifythepossiblefailuremodesofthepassivesystemfortheaccidentscenariounderconsideration.

5.Build a mechanistic, best-estimate (typicallylong-running) T-H modelto simulatethe passive systembehavior in the accidentscenarioofinterestandperformbestestimatecalculations.

6.IdentifythefactorsofuncertaintyintheresultsofthebestestimateT-Hcalculations.Inthepresentwork, weconsider onlyepistemicuncertainties(duetothelimitedknowledgeonsomephenomenaandprocesses– e.g.,models,parameters andcorrelationsusedintheT-Hanalysis– andtothepaucityoftherelatedoperationalandexperimentaldataavailable), asdonealsointhepreviousarticlebytheauthors[100].

7.Quantifytheuncertaintiesidentifiedatthepreviousstepbyproperprobabilitydistributions.

8.Propagatethe(epistemic)uncertaintiesthroughthedeterministic T-Hmodelinorderto assesstheprobabilityoffunc- tionalfailureofthepassivesystem.Formally,let:x={x1,x2,…,xj,…,xni}bethevectoroftherelevantuncertain(input) model parameters/variables;

μ

y(x) be a (possiblynonlinear) deterministic function representing thecomplex, compu- tationally expensiveT-Hcode;y={y1,y2,…,yl,…,yno}=

μ

y(x) bethe vectorofthe (uncertain)T-H modeloutputsof interest;Y(x)beasingle-valuedindicatoroftheperformanceofthepassivesystem(e.g.,thefuelpeakcladdingtemper- ature); and

α

Yalimitvaluethat representsthesystemfailure criterion.1Forillustratingpurposes,wesupposethatthe passive systemfunctionscorrectlyaslongasY(x) <

α

Y.The probability P(F) ofsystemfunctionalfailure can,then, be expressedbythemultidimensionalintegral:

P

(

F

)

= ... IF

(

x

)

q

(

x

)

dx, (1)

whereq(·) is thejoint ProbabilityDensity Function (PDF)describing the uncertaintyinthe parameters x,Fis thefailure region(where Y(x) ≥

α

Y) andIF(·) isan indicator function such that IF(x) = 1,if xF(i.e.,ifY(x) ≥

α

Y) and IF(x) = 0, otherwise(i.e.,ifY(x)<

α

Y).

TheMCSprocedure forestimating(1)entailsthat a typicallylarge numberNTofsamples ofthevalues ofthesystem parameters xbe drawn fromthe corresponding probability distributionsand usedto evaluate(y(x) and) Y(x) by running theT-Hcode.AnestimatePˆ(F)NT oftheprobabilityoffailureP(F)can,then,becomputedbydividingthenumberoftimes thatY(x) >

α

Y by thetotalnumberofsamplesNT.The costrelatedtothisprocess canbe impractical,whentherunning time foreach T-Hmodel simulation (i.e.,foreach evaluation ofY(x))takes severalhours (which is oftenthe caseforT- Hpassivesystems). Inordertotackletheseissues,we adopttheAdaptive Metamodel-basedSubsetImportance Sampling

1Note that the choice of a single-valued performance function does not reduce the generality of the approach, because any multidimensional vector of physical quantities (i.e., the vector y of the outputs of the T-H code in this case) can be conveniently re-expressed as a scalar parameter by resorting to suitable min-max transformations: see Refs. [67,68,72] for details.

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(AM-SIS)method(proposedbytheauthorsinRef.[100]),whichcombinesthecharacteristicsoftwoadvancedMCSschemes (i.e.,ImportanceSampling-ISandSubsetSimulation-SS)andametamodel(i.e.,anArtificialNeuralNetwork-ANN)(Section3).

3. TheAdaptiveMetamodel-BasedSubsetImportanceSampling(AM-SIS)method

TheAdaptiveMetamodel-basedSubsetImportanceSampling(AM-SIS)method,proposedinRef.[100]andhereemployed, basicallyrelies onan iterative Importance Sampling(IS) scheme,whereby theImportance SamplingDensity (ISD) iscon- structedandadaptivelyrefinedsoastofavortheMCsamplestobenearthefailureregion,thusincreasingthefrequencyof occurrenceofthe(rare)failureevent[90–92].Inmoredetail,itconsistsoftwomainsteps[98,99,118]:

1. Webuildan estimatorgˆ(x)oftheso-called“optimalISD”g(x)= IF(Px()Fq)(x),i.e.,theISDthat minimizesthevariance of theMCestimatorPˆ(F)NT [90–92,107](Section3.1);

2. WeperformImportanceSampling(IS),inwhichtheestimatorgˆ(x)builtatstep1aboveisemployedasanISDinorder toassessthefunctionalfailureprobabilityP(F)(1)oftheT-Hpassivesystem(Section3.2).

3.1. Adaptiveapproximationoftheideal,zero-varianceISDbymeansofSubsetSimulationandmetamodels

Manyapproacheshavebeenproposed to approximatethe optimalISDg(x) ortoatleast identifyoneproviding small standarddeviationoftheMCestimator:see,e.g.,Refs.[90,91,94–99]fordetails.Theestimatorgˆ(x)is,here,constructedin twostages:

a. weemploytheSubset Simulation(SS)method[67,68,70,73]to createapopulation

{

zmF : m=1,2,...,M

}

ofMsamples

approximatelydistributedaccordingtotheoptimalISDg(·)(4),i.e.,

{

zmF : m=1,2,...,M

}

g(·)=IF(·)q(·)/P(F).2No- ticethatherewesubstitutetheexpensiveT-Hcodey(x)=

μ

y(x)withaquick-runningANNregressionmodel(adaptively refinedbymeansofthesamplesiterativelyproducedbySS),withtheaimofreducingthecomputationalburdenrelated tothisstep(Section3.1.1);

b. we “fit” the samples

{

zmF :m=1,2,...,M

}

by means of a proper PDF, in order to obtain an estimator gˆ(x) for g(x). To this aim, we adopt the fully nonparametric PDF proposed in Ref. [99] and relying on the Gibbs Sampler [101](Section3.1.2).

3.1.1. SubsetSimulationandadaptivelytrainedANNmetamodelsforproducingsamplesdistributedaccordingtotheoptimalISD As highlighted above, in order to build an estimator gˆ(·) for g(·)=IF( · )q( · )/P(F) we need a population

{

zmF : m=1,2,...,M

}

ofM samples approximately distributedaccording to the optimal ISD, i.e.,

{

zmF : m=1,2,...,M

}

g(·).TheSubsetSimulation (SS)methodishereadoptedto thisaim.Thestrength ofSSisthatitconvertsthesimulation of a singleevent (in thiscase, the failure eventF) into a sequence ofnF simulations ofintermediate conditional events correspondingtosubsetsFi,i=1,2,…,nF,oftheuncertainparameterspace.Duringsimulation,MarkovChainMonteCarlo (MCMC)basedontheMetropolis–Hastings(MH)algorithm[67]isemployedtoproducetheconditionalsamples(belonging to theintermediate subregionsFi):in thisway,thesuccessive intermediate subsetsFiare progressivelypopulatedby the conditionalsamplesuptothetarget(failure)regionF[67,68].Itcanbeshownthatfollowingthisprocedure,thestationary densityofthe(failure)pointslyinginFisq(·|F)=IF(·)q(·)/P(F),whichisexactlytheideal,zero-varianceISDg(·)[67,73]. Ontheother hand,itis worthnotingthat asinglerun oftheSSmethodmayrequirea significant numberNc ofevalua- tionsofthelong-runningmodel,dependingonthemagnitudeofP(F) (i.e.,approximatelyNc=M·logp0[P(F)],withM≥100 forproducingreliable estimates,whichmayimplyeventhousandsofcalls to theT-Hcode).Thus, inorderto reducethe associatedcomputational burden,we substitutethe T-Hcodey(x)=

μ

y(x) bya regressionmodelf(x,w),dependingona

vectorofadjustableparameterswtobeproperlycalibratedbymeansofafinite(andpossiblyreduced)setofinput/output dataexamples (i.e.,patterns),alsocalledDesignOfExperiments(DOE)[114].In thiswork, three-layered feed-forwardAr- tificialNeuralNetworks (ANNs)trained bythe errorback-propagation algorithm areconsidered [52,53,115–117]. Theyare structuredinthreelayers(namely,theinput,hiddenandoutputlayers),whichcontainrespectivelyni,nhandnocomputing elements(named neuronsornodesandmathematicallydescribedbysigmoidalbasisfunctions).Thesecomputingunitsare linkedbyweighedconnections(calledsynapses).DetailsaboutANNregressionmodelsarenotreportedhereforbrevity:the interestedreadermayrefertothecitedreferencesandthecopiousliteratureinthefield.

The coreof the method (proposedin Ref. [100] andadopted inthe present manuscript) isthat the ANN metamodel is builtandadaptivelyrefined bymeans ofthe samplesiterativelyproduced by SSitself,accordingto thefollowing steps [105,119](Fig.1):

1. ConstructandtrainaninitialANNregressionmodelf(z,w0)bymeansofaDOED0TR=

{

(z0p,y0p),p=1,2,...,NT0R

}

consti-

tutedbyNTR°elementsselectedbyplainrandomsampling,LatinHypercubeSampling(LHS),partial/fullfactorialdesigns orother more sophisticated experimental design methods. Byso doing, we create a “first trial” surrogate ofthe T-H

2Notice that the change of name of the ‘dummy input vector’ from x to z has no ‘conceptual reason’ and is done only for notational simplicity and coherence with the description of the method reported in the following Sections.

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N. Pedroni, E. Zio / Applied Mathematical Modelling 48 (2017) 269–288 273

Fig. 1. Sketch of the procedure used for generating samples distributed as the ideal, zero-variance ISD by means of Subset Simulation and adaptively trained ANN regression models within the AM-SIS algorithm ( Section 3.1.1 ).

model coderepresentedby theunknown nonlineardeterministic function y=

μ

y(z).Notice that theANNstructure (in

practice,thenumbernh0 ofhiddenneurons)hastobechosensothatthetotalnumbern0p,ANN ofadjustableparameters w0islowerthanthesizeoftheDOE(i.e.,n0p,ANN <NTR0);

2.Run SS employing the ANN regression model f(z, w0) (instead of the original T-H code) to generate M samples

{

zmnF,0:m=1,2,...,M

}

approximatelydistributedasg(·)=q(· |F)=IF(·)q(·)/P(F).Noticethatthissimulationisalmost costlessfromthecomputationalviewpoint,sinceitrequirescallingonlythefast-runningANNmodelf(z,w0)insteadof thelong-runningT-Hcode

μ

y(z):thus,thenumberMofconditionalsamplesiterativelyproducedbytheSSalgorithmin eachintermediateconditionalregionFicanbechosentobequitelarge,inordertoincreasetheaccuracyandrobustness oftheprocedure(e.g.,M=50,000inthispaper);

3.ProduceanestimatePˆ(F)NANNT,0ofthefailureprobabilityP(F)byusingf(z,w0)(theestimateprovidedbySSattheprevious step2canbestraightforwardlyused).Asforstep2above,thisoperationisalmostcomputationallycostless;

4.Sett=0and

ε

P(F)=100%,wheretistheiterationindexand

ε

P(F)standsfortherelativevariationbetweentwoconsec- utiveANN-basedestimatesofP(F)producedduringtheadaptiveanditerativeprocedureofmetamodelrefinement;

5.while

ε

P(F) >

ε

thP(F)(i.e.,thechangebetweentheANN-basedfailureprobabilityestimatesattwoconsecutiveiterationsis largerthanaproperthreshold

ε

thP(F))andNTRt<NTRmax(i.e.,thesizeoftheDOE– inotherwords,theoverallnumberof coderuns– remainssmallerthanamaximalpredefinedvalueNTRmax),repeatthefollowingoperationsinordertorefine theANNregressionmodelinproximityofthefailureregionFandtoproduceasampleapproximatelydistributedasthe

“ideal” ISDg(·)=IF(·)q(·)/P(F):

(a) t=t+1;

(b) selectNadd points{zaddp : p= 1,2,…, Nadd}amongall those producedby SSatiteration (t – 1):a highfractionof thesepointsisselected“around” thelimitstateinordertobetterdescribetheresponseoftheT-Hpassivesystemin theareasclosetothefailureregionF;theremainingelementsare“distributed” inproximityoftheboundariesofthe otherintermediateconditionalsubsetsFiidentifiedbySS.Bysodoing,areliable“anchoring” oftheANNmetamodel is possible also in the relevant areasof the uncertain input space “visited” by the SS algorithm (in order not to interrupttheflowofthepresentation,furthertechnicaldetailsaboutthissteparegivenattheendofthisSection);

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(c)join the Nadd new elements to the current DOE after Nadd new evaluations of the system perfor- mance function by means of the original T-H model

μ

y(z): thus, DtTR=Dt−1TRDaddTR , where DaddTR =

{

(zaddp ,yaddp =

μ

y(zaddp )),p=1,2,...,Nadd

}

; also, the size NtTR of DtTR is NTtR=NtTR1+Nadd. It is important to note thatnowthecurrentDOEisobviouslyenrichedintheareasclosetothefailureregion;

(d)employtheupdatedDOEDtTR toconstructanupdated ANNregressionmodelf(x,wt).SincethesizeoftheDOEhas increased, alsothe numberofthe ANNadjustable parameters(in practice, thenumber ofhiddenneurons) can be increaseduntilntp,ANN <NTtR.Also,noticethatthenewANNmetamodelf(x,wt)isnowexpectedtobemoreaccurate indescribingthebehavioroftheoriginalT-HcodearoundtheregionFofinterest;

(e) generateMsamples

{

zm,tnF : m=1,2,...,M

}

approximatelydistributedasg(·)byrunningSSwiththeANNregression modelf(x,wt);

(f)produceanANN-basedestimatePˆ(F)NANNT,t ofP(F)andcompute

ε

P(F)as

|

Pˆ(F)NANNT,tPˆ(F)NANNT,t1

|

/Pˆ(F)NANNT,t1.NoticethatSS hastoberunateachiterationinordertoobtainboththesamples

{

zmnF,t:m=1,2,...,M

}

andthefailureprobability estimates Pˆ(F)NANNT,t used forthe convergencecheck. In order to “remove” thevariability that stems from different random numbers (in subsequent simulations), the random generator is reinitialized using the same seed at each iteration;

6. thefailureregionFdoesnotchangeexcessivelyfromoneiterationtoanother,i.e.,itisreliably“located”,andtheANNis sufficientlyaccurateinitsproximity [119].Thus,thevectors

{

zm,tnF :m=1,2,...,M

}

producedatthelast iterationtare

retainedasifthey werethe“optimalones”

{

zmF : m=1,2,...,M

}

,distributedastheideal,zero-varianceISDg(·)=IF(· )q(·)/P(F).

At the end of the procedure, the total number Nc,aux of T-H code runs carried out to refine the metamodel is Nc,aux=NTRt=NTR0+t·Nadd.

Someconsiderationsareinorderwithrespecttothealgorithmabove.Asalreadysaid,atstep4.bNaddpointsareselected (amongallthosegeneratedbySS)tobeaddedtothecurrentDOEDt−1TR .ArelevantfractionKoftheseNaddpointsischosen

“across” thelimit state,inproximity ofthefailure regionFnFF.Thisispractically implementedasfollows: (i)consider all the SSsamplesbelongingto thefailure region FnFF={z: Y(z) >

α

Y} andto theprecedingintermediate conditional regionFnF1={z:Y(z)>ynF-1}asa‘pool’ofpossiblecandidatestobeincludedintotheDOE(noticethattheseSSsamples

‘cover’ thelimitstate);(ii)identifythecandidateforwhichtheminimaldistancefromtheelementsofthecurrentDOEis thelargestwithrespecttotheother candidatesofthe‘pool’,andaddittothecurrentDOE(thisallowsfillingthe“empty”

areasoftheinputspace);(iii)removetheselectedvectorfromthe‘pool’ofcandidates;(vi)repeatsteps(ii)–(iii)untilK·Nadd newelementsareincludedintotheDOE.

Bymeansofthesameprocedure,theremaining(1–KNaddvectorsareequally“distributed” inproximityofthebound- ariesoftheotherSSintermediateconditionalregions:bywayofexample,thesetofcandidatesconsideredforrefiningthe ANNinproximityofregion Fi={z:Y(z) >yi}isobviouslyrepresentedby allthe SSsamples lyingacross thresholdyi,i.e., {z:Y(z) > yi-1Y(z) <yi+1}.Thiswayofproceedingensures an acceptablequality ofthe ANNmetamodelalsoinother

“key areas” ofthe uncertain input spacebesides the failure region F itself: actually, in order to produce a set of points

{

zmF : m=1,2,...,M

}

thataredistributedasg(·)=IF( ·)q(·)/P(F),theSSalgorithmneedstograduallyandaccuratelyvisit theentireuncertain inputspaceandits intermediateconditional regions.Differently fromRef.[100] (whereK wassetto 0.5bytrial-and-errorandtheremaining(1–K)Naddpointswererandomlydistributedacrosstheuncertaininputspace),in thispaperthe fractionK mentionedaboveiscomputedas2Nadd/nF:inotherwords,thenumberofpointsusedtorefine the metamodelaroundthe limit state{z: Y(z)=

α

Y}is twicethe numberofthose usedto improvetheANNinproximity ofthe other intermediate SSthresholds.Thischoice is motivatedasfollows:(i) higherimportance is giventothe failure regionwithrespecttootherareasoftheuncertaininputspace;(ii)thevalueofKchangesdependingonthenumbernF of intermediate regions,i.e.,accordingtothemagnitudeofthefailureprobability P(F);(iii)thisvalue isempiricallyfoundto performsatisfactorilyonthecasestudyanalysed.

Onlyforillustrationpurposes,Fig.2pictoriallyshowsthekeyconceptsunderlyingtheprocedureforenrichingtheDOE.

Therectangles representtheelementsofthe currentDOEinregions FnFFandFnF1,whereasthecircles representthe

‘pool’ofpossiblecandidatesgeneratedbySS.Wesupposethatthreeamongthesecandidateshavetobeselectedandadded tothe DOE.At eachstep,we identifythecandidatewhoseminimaldistancefromtheelementsofthecurrentDOEisthe largest withrespect to the other candidates ofthe ‘pool’ (see thearrows inFig. 2). Thiscandidate is addedto the DOE, whichisthusdynamicallyupdated.Theprocedure isrepeated(illustrative stepsa–dinFig.2) untilthedesirednumberof points(i.e.,threeinthecaseofFig.2)isincluded.

Also, noticethatsteps 2and4.fofthealgorithmabove requirethecomputationofan ANN-basedestimate Pˆ(F)NANNT of P(F).However, approximatingtheoriginal systemmodeloutputby anANNempiricalregressionmodel(trained bymeans ofafiniteset ofdata) bearstwoeffects: (i)thecorresponding estimatesmaybesubjecttoabias (whichmakes themnot accurate); (ii) the associated estimates are subject to additional uncertainty (which makes them less precise). To address issue(i), we employa Bootstrap-basedBias Correction(BBC) procedurerelying on an ensembleofB(e.g., B= 100)ANN regressionmodelsconstructedonB‘fictitious’datasetsrandomlysampledwithreplacementfromtheoriginalone:seeRefs.

[52,53,120]fordetails.Ontheotherhand,wedonottackleissue(ii).Actually,contrarytootherworksofliteratureinvolving thecombinationofmetamodelingandadvancedMCS,e.g., Refs.[103–111],inthispaperwe donotusethemetamodelto

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N. Pedroni, E. Zio / Applied Mathematical Modelling 48 (2017) 269–288 275

Fig. 2. Conceptual steps underlying the procedure for enriching the DOE in proximity of the failure region F (step 4.b of the iterative algorithm of ANN refinement). Rectangles: current DOE; circles: ‘pool’ of candidates generated by SS; arrows: candidate added to the DOE. a) identification of the first candidate to be added; b) inclusion of the first candidate into the DOE and selection of the second; c) inclusion of the second candidate into the DOE and selection of the third; and d) inclusion of the third candidate into the DOE.

providethefinalestimatePˆ(F)NT ofthefailureprobability: instead,we employitonlyasa“support tool” forconstructing thequasi-optimalISD(infacts, intheISphaseofthepresentmethodtheoriginalsystemmodelisused,seethefollowing Section3.2). Inother words,theonlyobjectiveoftheANN-based iterativealgorithmdescribedabove isthatofaccurately

“locating” the failure region F of interest without any bias: in this view,we perform only the amount of system model evaluationsthat are strictly necessaryto achieve thisobjective,whereas no furthercode runsare devotedto increase the precision(or,conversely,toreducetheuncertainty)ofthemetamodelestimates.

Inaddition,discussioniswarrantedontheconvergencecriterionadopted(step4.fabove).Actually,(i)theultimategoal ofthisfirststage ofAM-SISistodrawsamplesthatare asatisfactoryrepresentationofthequasi-optimalISDand(ii)the ANNtrainedhereisnot usedinthefollowing failureprobability estimationstep(Section3.2). Thismayleadtoconclude thatthefailure probability estimatedthrough theiterationsofSSandANN(steps3 and4.f) isnota“proper” measure of convergenceforthealgorithmofFig.1.Ontheother hand,itisimportanttonoticethattheaccuracyandunbiasednessof theANNdiscussed above(i.e.,itscapabilityofcorrectly“classifying” and“distinguishing” safeandfailure configurations)is absolutelyfundamentalforobtainingsamplesdistributedasg(·)=IF(·)q(·)/P(F)bymeansofSS.Inthisrespect,alsonote thatthe correctidentificationoffailure/safe pointscombinedwiththe mechanismofMCMC(which cangenerate random samplesdistributedaccordingto anyPDF)should beenoughto guaranteethatthesystemconfigurations producedatthe endofstep6ofthealgorithmarerepresentativeoftheoptimalISDg(·).

Obviously,theseconsiderations do not implythat theconvergence criterion selected isthe only possible(or the best overall). Forexample, one could alsolook atthe difference (say,through relative entropy) [121] betweentheestablished ISDsatsubsequentiterations.Ontheotherhand,convergenceofanentireprobabilitydistributionoverthewholeuncertain parameterspacemaybemuchmoredemanding(intermsofrequiredcoderuns)thanasimpleclassificationoffailure/safe configurations.

Finally,aconsiderationisinorderwithrespecttotheimpactofthedimensionalityoftheproblem(i.e.,ofthedimension ofx)ontheANNqualityand,thus,onthedensityapproximation.Increasingthedimensionoftheuncertainvariablespace actuallybrings ratherchallengingissues,includingtheso-calledcurseofdimensionality.In practice,weare tryingto train a metamodelon a learningdataset whose size isnot increased sufficiently withthe dimension ofthe space, giving rise totheso-calledempty spacephenomenon[105].Thisissueseems unavoidableandlimitsthe applicationofanyalgorithm belongingto themetamodelfamily toengineering problemswitha smallnumber ofinput parameters (say tens), unless some dimensionality reduction strategy is adopted: e.g., principal component analysis, feature selection orextraction and sensitivityanalysismethods[122–124].

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3.1.2. ConstructinganestimatoroftheoptimalISDbymeansofafullynonparametricProbabilityDensityFunction(PDF) TheiterativeANN-basedalgorithmpresentedabove producesapopulationofsamplesapproximatelydistributedasthe ideal,zero-variance ISD: however,these samplescannot be used directlyto define an unbiased IS estimator,because the corresponding sampling densityg(·) isnot knownexplicitly. Moreover, thesampled states

{

zmF :m=1,2,...,M

}

are not

independent.A first(naive) ideamight beto justusetheempirical distributionof

{

zmF :m=1,2,...,M

}

forIS sampling.

Butthis distributiondoesnot satisfy therequirementof havinga nonzerodensitywherever IF(x)q(x) > 0.Tosatisfy this requirement, asecond ideaistofita kerneldensityestimatetothissample, basedonakernelwhosedensityisnonzero wherever IF(x)q(x) > 0 [93,94]. However, kernel densityestimation by standard methods is difficult in highdimensions.

Finally, inRef. [99] the authors propose toadopt the one step ahead transitiondensity

κ

(x|z) ofa Markov chain,when

the chain isin state zmF,andaverage over the Mstates

{

zmF : m=1,2,...,M

}

.In thisway, the optimal ISDg(x) can be

approximatedbygˆ(x)(2):

gˆ

(

x

)

= 1 M

M

m=1

κ (

x

|

zmF

)

. (2)

FollowingthesuggestionofRef.[99],inthispaperweusethetransitiondensity

κ

(x

|

zmF)adoptedbytheGibbsSampler [101](seetheAppendixforthoroughtechnicaldetails).

The advantageoftheISD(2)is thatit isnotlimitedby parametric models(e.g.,normal,exponential,lognormal, etc.), asithappensinsteadfortheCrossEntropy (CE)[95] orVarianceMinimization(VM)[125]techniques.Ontheother hand, forISD(2)thepositivitycondition(i.e.,thatgˆ(x)>0wheneverIF(x)q(x)>0)isnotguaranteedintherare-eventsetting.

Thus,gˆ(x)isheremodifiedtoassurethatitisnonzeroovertheentiresupportofg(x).Tothisaim,weconsidera“weighed average” of ˆg(x)with the original densityq(x), i.e.:

gˆw

(

x

)

=w·q

(

x

)

+

(

1w

)

·gˆ

(

x

)

, (3)

wherewisaweightarbitrarilyselectedbetween0and1(inthiswork,w=0.01).

3.2. ImportancesamplingfromtheestimatoroftheoptimalISD

Thewell-known‘compositionmethod’isemployedtodrawNTsamplesfromgˆw(x)(3).Inextremesynthesis,fork=1,2,

…,NT,auniformrandomnumberuisgeneratedin[0,1):ifu<w,thenthevectorxkissampledfromtheoriginalPDFq(x);

otherwise,fromgˆ(x)=M1 M

m=1

κ

(x

|

zmF)(2)(forthesakeofbrevity,wedonotreportheredetailsaboutthestepsnecessary todrawsamplesfromthemixturegˆ(x)(2)oftransitiondensities:theinterestedreaderisreferredtotheAppendix).

SincethefailureprobabilityP(F)=Eq[IF(x)q(x)](1)canbeobviouslyexpressedalsoasEgˆ w[IFg(ˆx)q(x)

w(x) ],the AM-SISestimator Pˆ(F)NT of the failure probabilityP(F) is then[90–99]:

Pˆ

(

F

)

NT =N1

T NT

k=1

IF

xk

q

xk

ˆ gw

xk

= 1 NT

NT

k=1

IF

xk

q

xk

w·q

xk

+

(

1w

)

·gˆ

xk

. (4)

The sample standard deviation

σ

ˆ[Pˆ(F)NT] of (4) can be also straightforwardly computed since the realizations IF(xk)q(xk)/gˆw(xk),k=1,2,…,NT,areindependent.Withrespecttothat,itisalsoworthnotingthattheestimatorsPˆ(F)NT and

σ

ˆ[Pˆ(F)NT] are unbiased forthemeanandthe standarddeviation, even if(i)the samples

{

zmF : m=1,2,...,M

}

itera-

tively generatedby SSare byconstruction not independentandare notexactly distributedasg(x) (see Section3.1.1) and (ii)thequalityoftheISDapproximationinthefirststepofthealgorithmislow(seeSection3.1.2).Ontheotherhand,the performanceoftheAM-SISalgorithmobviouslydependsonthequalityofthisapproximation.

Noticeagainthattheoriginalsystemmodel(not theANNmetamodelemployedattheprevious step)isusedinthisIS- basedfailureprobabilityestimationphase.Actually,asexplainedinSection3.1.1,oneoftheeffectsoftheapproximationof theoriginalsystemmodeloutputbyanempiricalregressionmodel(trainedbymeansofafinitesetofdata)isthattheas- sociatedestimatesaresubjecttoadditionaluncertainty(whichmakesthemlessprecise).EmployinginsteadtheANNonlyas a“supporttool” forconstructingthequasi-optimalISD(i.e.,foraccurately“locating” thefailureregionF)allowsperforming onlytheamountofsystemmodelevaluationsthat arestrictly necessarytoachieve thisobjective: thus,noadditionalcode runsaredevotedtoincreasetheprecision(or,conversely,toreducetheuncertainty)oftheANNmetamodelestimates,with obviousbenefitsfromthepointofviewofthereducedcomputationalcost.

4. Casestudy:functionalfailureanalysisofaT-Hpassivesystemofliterature

Asinthepreviouspaperbytheauthors[100],thecasestudyinvolvesaGas-cooledFastReactor(GFR)cooledbynatural convectionaftera LossOfCoolantAccident(LOCA) [26].The reactorisa600-MWGFRcooled byheliumflowingthrough separatechannelsinasiliconcarbidematrixcore[126].

Incase ofaLOCA, long-termheatremovalis ensured bynaturalcirculation ina givennumberNloops of identicaland parallelheatremovalloops.However,inordertoachieveasufficientheatremovalratebynaturalcirculation,itisnecessary

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N. Pedroni, E. Zio / Applied Mathematical Modelling 48 (2017) 269–288 277

Fig. 3. One loop of passive decay heat removal system of the 600-MW GFR [26] .

tomaintainan elevatedpressureevenaftertheLOCA.Thisisaccomplishedby aguardcontainment,whichsurroundsthe reactorvesselandpowerconversionunit,andholdsthepressureatalevelthatisreachedafterthedepressurizationofthe system[26].

TheconfigurationofthepassivesystemfortheremovalofdecayheatisshownschematicallyinFig.3,whereonlyone loopoutofNloopsisreportedforclaritysake:theflowpathofthecoolingheliumgasissuggestedbytheblackarrows.As showninFig.3,theloophasbeendividedintoNsections =18sections;technicaldetailsaboutthegeometricalandstructural propertiesofthesesectionsarenotreportedhereforbrevity:theinterestedreadermayreferto[26].

It isworth notingthat as inRef. [26] the subjectof thepresent analysisis the quasi-steady-state naturalcirculation coolingthat takesplaceafter theLOCAtransienthasoccurred. Thus,the analyses hereafterreportedrefer tothissteady- state periodandare conditional tothe successfulinceptionof naturalcirculation.As aconsequence, theanalyses donot considerthe probability ofnot startingnaturalconvectionnor theprobability ofnot buildingup andmaintaininga high pressurelevelintheguardcontainment.

4.1. ThedeterministicT-Hmodel

Tosimulatethesteady-statebehaviorofthesystem,aone-dimensionalthermal-hydraulicMATLABcodehasbeenimple- mented.Thecodetreatsall theNloopsmultipleloopsasidenticalandeachloopisdividedinNsections =18sections(Fig.3).

Further,thesectionscorresponding tothe heater(i.e.,the reactorcore,item 4inFig.3) andthecooler (i.e.,theheatex- changer, item 12 in Fig. 3) are divided ina proper numberNnodes of axial nodes to compute the temperatureand flow gradientswithsufficientdetail(40nodesarechosen forthepresentanalysis).Boththeaverageandhotchannelsaremod- eledinthecoresothattheincrease intemperatureinthe hotchannelduetotheradial peakingfactorcanbe calculated [26].

Fromastrictly mathematicalpointofview,obtaining asteady-statesolutionamountstodropping thetimedependent termsintheenergyandmomentumconservationequations[127];inpractice,thecodebalancesthepressurelossesaround theloopssothatfrictionandformlossesarecompensatedbythebuoyancyterm, whileatthesametimemaintainingthe heatbalanceintheheater(i.e.,thereactorcore,item4inFig.3)andcooler(i.e.,theheatexchanger,item12inFig.3).

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Table 1

Equations governing the heat transfer process in each node l = 1, 2, …, N nodesof both the heater and the cooler of the 600-MW GFR passive decay heat removal system of Fig. 3 , together with a description of the physical parameters and their units of measure.

Heat transfer equations

Q ˙ l= m ˙ c p,l(T out,lT in,l), l = 1 , 2 , . . . , N nodes (5)

˙

m c p,l(T out,lT in,l)= S lh l(T wall,lT bulk,l), l = 1 , 2 , . . . , N nodes (6)

Parameter Description Unit of measure

Q ˙ l Heat flux in the l th node kW

˙

m l Mass flow rate in the l th node kg/s

c p,l Specific heat at constant pressure in the l th node kJ/kg K

T out,l Temperature measured at the outlet of the l th node K

T in,l Temperature measured at the inlet of the l th node K

T wall,l Temperature measured at the wall channel of the l th node K

T bulk,l Temperature measured at the bulk of the l th node K

S l Heat-exchanging surface in the l th node m 2 h l Heat transfer coefficient in the l th node kW/m 2K

Table 2

Equation stating the balance between buoyancy and pressure losses along the closed loop of the 600-MW GFR passive decay heat removal system of Fig. 3 , together with a description of the physical parameters and their units of measure.

Mass flow rate equation

Nsections

s=1 [ ρsg H s+ f sLs Ds

˙ m2 2ρsA2s + K s m˙2

2ρsA2s] = 0 (7)

Parameter Description Unit of measure

ρs Coolant density in the s th section of the loop kg/m 3 H s Height of the s th section of the loop m f s Friction factor in the s th section of the loop / L s Length of the s th section of the loop m D s Hydraulic diameter of the s th section of the loop m

˙

m Mass flow rate in the s th section of the loop kg/s A s Flow area of the s th section of the loop m 2 K s Form loss coefficient of the s th section of the loop

Eqs.(5)and(6)inTable1governtheheattransferprocessineachnode l=1,2,…,Nnodesofboththeheaterandthe cooler.

Eq.(5)inTable1statestheequalitybetweentheenthalpy increasebetweentheflow attheinletandtheflow atthe outletinanynode,whereas Eq.(6)inTable 1regulatestheheat exchangebetweenthechannel wallandthebulkofthe coolant.

Themassflow rateisdetermined byabalance betweenbuoyancyandpressurelossesalongtheclosedloop according toEq.(7)inTable2.

Eq.(7)inTable2statesthatthesumofbuoyancy(firstterm),frictionlosses(secondterm)andformlosses(thirdterm) shouldbeequaltozeroalongtheclosedloop[26].

Noticethattheheattransfercoefficientshl,l=1,2,…,Nnodes,in(6)inTable1arefunctionsofthefluidcharacteristics andthegeometry,andarecalculatedthroughpropercorrelationscoveringforced-,mixed-andfree-convectionregimes,in bothturbulentandlaminarflow;further,differentNusseltnumbercorrelationsare usedinthedifferentregimestoobtain valuesfortheheattransfercoefficients.Alsothefrictionfactorsfs,s=1,2,…,Nsections,in(7)inTable2arefunctionsofthe fluid characteristicsandgeometryandarecalculated usingappropriatecorrelations[26].Aniterativealgorithmisusedto findasolutionthatsatisfiessimultaneouslytheheatbalanceandpressurelossequations.

4.2. UncertaintiesinthedeterministicT-Hmodel

There is incomplete knowledge onthe properties ofthe system andthe conditions inwhich the passive phenomena develop.Thiskindofuncertainty,oftentermedepistemic,affectsthemodelrepresentationofthepassivesystembehavior [9,29,128].

Theninemodelparametersx={xj: j=1, 2, ..., 9}affectedbyepistemicuncertaintyaresummarizedinTable3[26]:the meanandstandarddeviationsofthecorrespondingGaussianPDFsarealsoreported.

Thesequentialstepsundertakentopropagatetheepistemic(i.e.,modelandparameter)uncertaintiesthroughthedeter- ministicT-HequationsdescribedinthepreviousSection4.1are:

i Drawsamplesoftheuncertaininput parametersx1 (i.e.,power),x2 (i.e.,pressure)andx3 (i.e.,coolerwalltemperature) fromtherespectiveepistemicprobabilitydistributions(Table3).

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