project name: high frequency physics-based earthquake...

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Project Name: High Frequency Physics-Based Earthquake System Simulations (Year 1 of 2) End of Year Summary PI NAME : Thomas H. Jordan Co-PI(s): Jacobo Bielak, Carnegie Mellon University, Po Chen, University of Wyoming, Yifeng Cui, San Diego Supercomputer Center, Philip Maechling, Southern California Earthquake Center, Kim Olsen, San Diego State University, Ricardo Taborda, University of Memphis PROGRAM : INCITE ALCF YEAR : 2015 Performance Period: January 1 - December 31, 2015 (Q1,Q2,Q3,Q4) ALCF Project Name: GMSeismicSim OLCF Project Name: GEO112 Project Usage Please comment on the use of your Mira allocation. For example, this could include periods of low utilization due to code/model development, periods of high utilization due to significant campaigns, significant use of the backfill queue or the INCITE overburn policy. If more than 50% of your allocation was used up by jobs below the capability size (less than 8-racks), please comment on the technical barriers preventing your workload or code from scaling to 8-racks and beyond. While our 2015 Mira usage produced important scientific results, our usage pattern was not optimal. One issue is that we used our 2015 ALCF allocation in the first six months of the year. Then, we continued to run jobs at a slower rate, using the back- fill queue, during the remainder of the year. We will plan for a more consistent usage of ALCF computing time during 2016 to avoid running out of allocation hours on Mira during 2016. Another issue we are working to address is the size of our routine jobs. Our best results from Mira in 2015 are from our iterative, data- intensive, full 3D tomographic improvements to 3D seismic velocity models for California. The standard calculations in this process on Mira are now 1 rack in size. However, in 2016 we expect to run tomographic inversions valid up to higher frequencies, which will require at least a factor of 8 increase in computational scale for these routine jobs. However, the data storage requirements for our inversions will also increase substantially when we move to higher frequencies. We are currently evaluating data compression techniques for use on our ALCF data that will reduce the requirements of these higher frequency inversions. We have identified data compression evaluation as priority with our ALCF Catalyst for 2016.

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Page 1: Project Name: High Frequency Physics-Based Earthquake ...hypocenter.usc.edu/research/INCITE/INCITE_2015/JORDAN_INCITE_… · Project Name: High Frequency Physics-Based Earthquake

ProjectName:HighFrequencyPhysics-BasedEarthquakeSystemSimulations(Year1of2)EndofYearSummary

PINAME:ThomasH.JordanCo-PI(s):JacoboBielak,CarnegieMellonUniversity,

PoChen,UniversityofWyoming,YifengCui,SanDiegoSupercomputerCenter,

PhilipMaechling,SouthernCaliforniaEarthquakeCenter,KimOlsen,SanDiegoStateUniversity,RicardoTaborda,UniversityofMemphis

PROGRAM:INCITEALCFYEAR:2015

PerformancePeriod:January1-December31,2015(Q1,Q2,Q3,Q4)

ALCFProjectName:GMSeismicSimOLCFProjectName:GEO112

ProjectUsagePleasecommentontheuseofyourMiraallocation.Forexample,thiscouldincludeperiodsoflowutilizationduetocode/modeldevelopment,periodsofhighutilizationduetosignificantcampaigns,significantuseofthebackfillqueueortheINCITEoverburnpolicy.Ifmorethan50%ofyourallocationwasusedupbyjobsbelowthecapabilitysize(lessthan8-racks),pleasecommentonthetechnicalbarrierspreventingyourworkloadorcodefromscalingto8-racksandbeyond.Whileour2015Mirausageproducedimportantscientificresults,ourusagepatternwasnotoptimal.Oneissueisthatweusedour2015ALCFallocationinthefirstsixmonthsoftheyear.Then,wecontinuedtorunjobsataslowerrate,usingtheback-fillqueue,duringtheremainderoftheyear.WewillplanforamoreconsistentusageofALCFcomputingtimeduring2016toavoidrunningoutofallocationhoursonMiraduring2016.Anotherissueweareworkingtoaddressisthesizeofourroutinejobs.OurbestresultsfromMirain2015arefromouriterative,data-intensive,full3Dtomographicimprovementsto3DseismicvelocitymodelsforCalifornia.ThestandardcalculationsinthisprocessonMiraarenow1rackinsize.However,in2016weexpecttoruntomographicinversionsvaliduptohigherfrequencies,whichwillrequireatleastafactorof8increaseincomputationalscalefortheseroutinejobs.However,thedatastoragerequirementsforourinversionswillalsoincreasesubstantiallywhenwemovetohigherfrequencies.WearecurrentlyevaluatingdatacompressiontechniquesforuseonourALCFdatathatwillreducetherequirementsofthesehigherfrequencyinversions.WehaveidentifieddatacompressionevaluationasprioritywithourALCFCatalystfor2016.

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ReportonProjectMilestones• Pleaseinsertacopyofthemilestonesasoutlinedintheproposal• Provideastatusoneachofthemilestones• Listanyadditionalmajoraccomplishmentsthusfarthisyear.Pleaseinclude

scientificandcomputationaldetailsofsimulationsundertaken,includingimagesifpossible

• Listanycommentstoclarifythestatusoftheprojecto Forexample,fundingchallengesslowedwork,changeofsciencescope

withanexplanation,etc DuringthisINCITEallocation,researchersfromtheSouthernCaliforniaEarthquakeCenter(SCEC)usedcomputingtimeandstoragespaceonALCFandOLCFINCITEcomputationalresourcestocarryoutresearchonhigh-frequencyphysics-basedearthquakesystemsimulations.Whilethis2015end-of-yearreportisrequestedbyALCF,wedescribetheoverallprogressinourINCITE-supportedresearchprogramusingbothOLCFandALCFresources.Wherepossible,weidentifywhichINCITEresourceswereusedtoproducespecificresults.In2015,SCECusedINCITEresourcestoinvestigateabroadrangeofscientificissues.Our2015-2016INCITEproposaldefinedthefollowingfourobjectives:

• O1:Improvetheresolutionofdynamicrupturesimulationsbyanorderofmagnitudeandinvestigatetheeffectsofrealisticfrictionlaws,geologicheterogeneity,andnear-faultstressstatesonseismicradiation.

• O2:Extenddeterministicsimulationsofstronggroundmotionsto10Hzforinvestigatingtheupperfrequencylimitofdeterministicground-motionprediction.

• O3:Computephysics-basedProbabilisticSeismicHazardAttenuation(PSHA)mapsandvalidatethoseusingseismicandpaleo-seismicdata.

• O4:Improve3Dearthstructuremodelsthroughfull3Dtomographyusingobservedseismicityandambientnoise.

Duringthefirstyearofourcurrentallocation,SCECresearchershaveprogressedtowardseachoftheseobjectives:WedefinedandimprovedanewcentralCalifornia3Dvelocitymodelusingfull3Dtomography(O4).Weproducedacomprehensive,physics-basedhazardmodelfortheLosAngelesregionvaliduptoseismicfrequenciesof1Hz(O3),weperformedhigh-frequencysimulations(upto8Hz)onTitanusingGPU-optimizedfinite-differencecodes(O2)whileincorporatingnewaspectsofearthquakephysics(O1).Here,weprovideaprogressupdateonthemilestoneswedefinedinour2015INCITEallocationrequest,followedbyasummaryofourmostsignificantaccomplishments.Theprogressmadein2015highlightsonceagainhowthispartnershipallowsustoperformthemostscientificallyadvancedearthquakegroundmotionandseismichazardcomputationsconductedworldwide.

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SummaryofMilestonesProgress:Weidentifiedthefollowingeightmilestones[M1–M8]inouroriginalINCITEallocationrequest.Abriefsummaryofprogressispresentedbelow.

Year1MilestoneDescriptions MilestoneAchievementStatusM1 Usefull3Dtomographyandcomparative

validationsusingtoimproveexistingCaliforniavelocitymodelsforuseinhighfrequencywavepropagationsimulationsat0.2Hz

Achieved.UsedMiratocalculatesixiterationsofCentralCaliforniaModel.Theimproved3DmodelisnowavailabletogroundmotionmodelersthroughSCECdistributionsoftwarecalledUCVM.

M2 Runhighfrequencyforwardsimulationsusingalternativematerialattenuation(Q)andseismicvelocitymodels(CVMs).Comparetheimpactofmaterialproperties,topography,andmodelsincludingspatialvariability(heterogeneities)andsoft-soildeposits(orgeotechnicallayers)on4Hz+simulationsbysimulatingforwardeventsusingalternativemodelsandcomparingresultsamongsyntheticsandwithdata.

Started,notcompleted.AWP-ODCandHerculescodebrancheshavetestedthesephysics.Currentlyrunningbaseline4Hzsimulationswithoutthesephysicswithgoodagreementat4Hzamong3wavepropagationcodeswithasimplevelocitystructure.

M3 Runhighfrequencyforwardsimulationsusingalternativeapproachestoincludetheeffectsofoff-faultandnear-surfaceplasticdeformation.Comparetheimpactofalternativeplasticitymodels(linear-equivalent,3D+1Dhybrid,full3Dplastic)on4Hz+simulationsbysimulatingforwardeventsandcomparingtheresultsamongsyntheticsandwithempiricalrelationshipsanddata.

Started,notcompleted.AWP-ODCandHerculescodebrancheshavetestedthesephysics.Currentlyrunningbaseline4Hzsimulationswithoutthesephysicswithgoodagreementat4Hzamong3wavepropagationcodeswithasimplevelocitystructure.

M4 Calculatea1.0HzCyberShakeHazardcurve.UseupdatedCVMs,sourcemodels,andcodestocalculateahigherfrequencyCyberShakehazardcurve

Achieved.UsedTitanandBlueWaterstocalculateaCyberShake1HzLosAngelesareaprobabilisticseismichazardmodelbasedon336site-specifichazardcurves.

Year2MilestoneDescriptions ObjectiveM5 Usefull3Dtomographyandcomparative

validationsusingtoimproveexistingCaliforniavelocitymodelsforuseinhighfrequencywavepropagationsimulationsat0.5Hz

Notstarted

M6 Runhighfrequencyforwardsimulationsusingalternativematerialattenuation(Q)andseismicvelocitymodels(CVMs).Comparetheimpactofmaterialproperties,topography,andmodels

Notstarted

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includingspatialvariability(heterogeneities)andsoft-soildeposits(orgeotechnicallayers)on8Hz+simulationsbysimulatingforwardeventsusingalternativevelocitymodelsandcomparingtheresults.

M7 Runhighfrequencyforwardsimulationsusingalternativeapproachestoincludetheeffectsofoff-faultandnear-surfaceplasticdeformation.Comparetheimpactofalternativeplasticitymodels(linear-equivalent,3D+1Dhybrid,full3Dplastic)on8Hz+simulationsbysimulatingforwardeventsandcomparingtheresultsamongsyntheticsandwithempiricalrelationshipsanddata.

Notstarted

M8 Calculatea1.5HzCyberShakeHazardcurve.UseupdatedCVMs,sourcemodels,andcodestocalculateahigherfrequencyCyberShakehazardcurve

Notstarted

MajorProjectAccomplishments:1)Wecompleteda1-HzurbanseismichazardmodelfortheLosAngelesregion(OLCFwithproductsfromALCF).SCEC'sresearchteamusedtheOLCFTitanandNCSABlueWaterssupercomputerstoperformCyberShakeStudy15.4.ThiscomputationdoubledthemaximumseismicfrequencyrepresentedintheLosAngelesurbanseismichazardmodel,from0.5Hzto1Hz(Figure1).Seismichazardcurveswerederivedfromlargeensemblesofseismogramsatfrequenciesbelowthismaximumfor336surfacesitesdistributedacrosstheLosAngelesregion.Thisnewprobabilisticmodelusesrefinedearthquakerupturedescriptionsthroughrevisionstotheconditionalhypocenterdistributionsandtheconditionalslipdistributions.ThisseismichazardcalculationusedtheCVM-S4.26.GTL3Dvelocitymodel,whichwasvalidatedandimprovedusingALCFMira,asthebestavailablesouthernCalifornia3Dvelocitymodel.TheCS15.4modelprovidesnewseismichazardinformationofinteresttobroadimpactcustomersofCyberShake,includingseismologists,utilitycompanies,andcivilengineersresponsibleforCaliforniabuildingcodes.Thenewmodel,whichsamplesthecompleteUniformCaliforniaEarthquakeRuptureForecast,willberegisteredintotheUSGSUrbanSeismicHazardMappingProject(http://earthquake.usgs.gov/hazards/products/urban/).

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TheGPU-basedanelasticwavepropagationAWP-ODCsoftwarewascoupledwiththeCPU-basedpost-processingcalculationsthatsynthesizedover300millionseismograms.InStudy15.4,SCECutilizedapproximately200pilotjobstorunCyberShaketasksonTitanresources.Over80%ofthenode-hoursburnedonTitanwerefromjobswhichranon25%ormoreofthemachine.Approximately200TBofSGTdatawastransferredfromTitantoBlueWatersautomaticallyaspartoftheworkflow.OnTitan,theacceleratedcalculationsoftheGPUStrainGreenTensor(SGT)implementationis6.3timesmoreefficientthantheCPUimplementation,comparedtheperformanceonXK7toXE6atnode-to-nodelevel,whichsavedusmorethansixtymillionofcore-hoursoverthecourseofthestudy.OurGPUdevelopmentwasrecognizedwithNVIDIA’s2015GlobalImpactAward.“Thefullthree-dimensionaltreatmentofseismic-wavepropagationhasthepotentialtoimproveseismichazardanalysismodelsconsiderably,andthatiswheretheacceleratingtechnologyisparticularlyhelpfulatthismoment,”saidThomasJordan,directorofSCEC.“WithGPUcomputingpowerwe’regaininginsightastohowthegroundwillmoveinhigh-riskareas,andhowwecanbetterplanfortheaftermathofamajorevent.”http://www.hpcwire.com/off-the-wire/sdsc-researchers-awarded-nvidia-2015-global-impact-award/2)WerefinedthecentralCalifornia3Dvelocitymodel,thatwecallCentralCaliforniaArea(CCA),andusedfull3Dtomographycomputationalmethodsto

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validateandimprovethe3Dseismicvelocitymodelusingbothobservedmoderateearthquakesandambientseismicnoiseobservations(ALCF).Wehavefurtherimprovedthecomputationalefficiencyofourfull3Dtomography(F3DT)workflowonALCFMiraandarenowapplyingittoCentralCaliforniaandstatewide.Anaccurate3Dvelocitymodelisessentialinputneededforaccuratedeterministicearthquakewavepropagationsimulations.GradualimprovementsinourvelocitymodelshaveallowedustoincorporateanincreasingvolumeofobservedseismogramsintoourF3DTworkflow,whichisallowingustoresolvefinerstructuraldetailswithhigheraccuracy.Figure2belowshowsthestudyareaandresultsfromthe6thiteration.Thestartingmodelisdefinedusinga500mgridspacingandweusetrilinearinterpolationinbetweenthegridpointswhenconstructingmeshes.Themodelcoversdepthsdownto50km.Wehavealsointegratedalossy,onlinecompressioncodezfpintothefull-3Dtomographybasedonthescattering-integralmethod(F3DT-SI)workflow.ThelastF3DTimplementation,inparticularthescattering-integralimplementation(F3DT-SI),requiredhighdiskstoragecostandtheassociatedI/Ooverheadofarchivingthe4Dspace-timewavefieldsofthereceiver-orsource-sidestraintensors.WehavesuccessfullyintegratedalossycompressionalgorithmintoourF3DT-SIworkflowtosignificantlyreducethediskspaceforstoringthesedata.

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Figure2.Shearwave(Swave)velocityat(top)2km,(middle)10km,and(bottom)20kmdepthsin(left)theinitialmodelCCA00,(middle)the6thiterationmodelCCA06,and(right)theperturbations.ThecolorbaronthelowerleftcornerofeachplotshowstherangeofthecolorscalewithredindicatingrelativelyslowSwavevelocitiesandblueindicatingrelativelyfastSwavevelocities.Blacksolidlinesshowmajorfaultsinourstudyarea.3)Weperformedhigh-frequency(upto8Hz)simulations(OLCFTitan)TheSCECresearchersranhighfrequencygroundmotionsimulationsonTitanusingGPU-enabledfinitedifferentwavepropagationsolvers,andafinite-elementwavepropagationsolver,Hercules,whichintegratesanefficientoctree-basedhexahedralmeshgeneratorwithanexplicitFEformulation.Thesecodeswereusedinaverificationandvalidationstudiesforthe2014Mw5.1LaHabraearthquakeonTitan,totesttheaccuracyofthecodes,andtoexaminehowclosethepredictedgroundmotionsaretoobservations.Wemodelgroundmotionvariabilityforlargestrike-slipandblindthrustearthquakesincludingfrequenciesupto8Hz.Theearthquakesourceisobtained

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throughdynamicrupturepropagationusingSORDalongseveralrealizationsofroughfaulttopographies.Anensembleofsourcesismodeledbyvaryingthehypocenterlocationthatresultsinsimilarmomentmagnitudes.Theslip-ratedatafromtherupturemodelingisconvertedtoakinematicsourceandinputintothewavepropagationcodeAWP-ODC,whichincorporatesfrequency-dependentattenuation(Q(f),Withersetal.,2015)aswellasDrucker-Pragerplasticity.Wealsoincludesmall-scalemediumcomplexityinbotha1D-layeredmodelanda3DmediumextractedfromSCECCVM-S4includingasurfacegeotechnicallayer.ThemediangroundmotionfollowsasimilardecayascomparedtoGMPEswhenusingaQ(f)power-lawexponentintherange0.6-0.8.Nonlineareffectsareneededtoreducenear-fieldgroundmotiontoobservablelevelsinregionsofnear-surfacelowvelocitylayers.Small-scalemediacomplexityisobservedtodecreasethepolarizationratiotothatofsimilartoobservations.Theintra-eventvariabilityforthelayeredmodelsimulationsisnearobservedvaluesofsingle-stationstandarddeviation.Small-scaleheterogeneitycansignificantlyaffecttheintra-eventvariabilityatfrequenciesgreaterthan~1Hz,becomingincreasinglyimportantatlargerdistancesfromthesource.Theintra-eventvariabilityofoursimulationsintheCVMistypicallylargerthanthatfortheobservationsatfrequencies>1Hz.However,thisdiscrepancytendstodecreasewhensmall-scaleheterogeneitiesareincluded,suggestingtheneedforahighlycomplexvelocitymodeltofitgroundmotionvariability.Plasticeffectsinthemediumalsoreducethevariability,particularlyatdistancesclosetothesource.Weuseanon-associatedDrucker-PragernonlinearrheologyfollowingthereturnmapalgorithmintheAWP-ODCcodetomodelgroundmotionsfromtheM7.8ShakeOutscenariosourcedescription(M3)includingpermanentrockdeformation.Toaccountfornonlinearityinthefaultdamagezoneandinnear-surfacesediments,weusedatwo-stepmethod.Inthefirststep,thedynamicruptureprocessincludingplasticitywassimulatedinasmallcomputationaldomainusingtheCPUversionoftheAWP-ODCfinitedifferencecode.ThesedynamicsimulationswereperformedonNCSABlueWatersorTACCStampede,whereakinematicsourcewasalsogeneratedfromthedynamicsolution.Thesourcepartitions,whichrequireupto4Tbofdiskspace,werethentransferredtoOLCFTitanusingGlobusGridFTP.ThewavepropagationresultingfromthekinematicsourcewassimulatedonTitanwithAWP-ODC,usingalargervelocitymeshthatincludesmajorurbanareasintheregion.Thesesimulationsareperformedusing700GPUsduring4hoursforamaximumfrequencyof2Hzor5,600GPUsduring7hoursforamaximumfrequencyof2Hz.ResultsconfirmthatnonlineardeformationwouldoccurinawideareaaroundthefaultandintheSanBernardinoandLosAngelesbasins,reducinglong-periodgroundmotionsintheLosAngelesbasinbyupto50%withrespecttothelinearsolution(Figure3).Theimportanceofnonlinearityincreasesassimulationsareperformedathigherfrequencies.Weexploretheeffectsoffaultzonenonlinearityonpeakgroundvelocities(PGVs)bysimulatingasuiteofsurfacerupturingearthquakesinavisco-plasticmedium.Oursimulations,covermagnitudesfrom6.5to8.0,withseveral

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realizationsofthestochasticstressdropforagivenmagnitude.Wetestthreedifferentmodelsofrockstrength,withfrictionanglesandcohesionsbasedoncriteriawhicharefrequentlyappliedtofracturedrockmassesincivilengineeringandmining.Weuseaminimumshear-wavevelocityof500m/sandamaximumfrequencyof1Hz.Inrupturescenarioswithaveragestressdrop(~3.5MPa),plasticyieldingreducesnear-faultPGVsby15to30%inpre-fractured,low-strengthrock,butlessthan1%inmassive,highqualityrock.Thesereductionsarealmostinsensitivetothescenarioearthquakemagnitude.Inthecaseofhighstressdrop(~7MPa),however,plasticityreducesnear-faultPGVsby38to45%inrocksoflowstrengthandby5to15%inrocksofhighstrength.Becauseplasticityreducesslipratesandstaticslipnearthesurface,theseeffectscanpartiallybecapturedbydefiningashallowvelocity-strengtheninglayer.Thesesimulationresultssuggestthatnonlineareffectsmayberelevantevenatlongperiods,especiallyforearthquakeswithhighstressdrop.

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ProjectProductivity• ListPapersfromworkatALCFandincludeasentenceabouthowthisisrelated

totheproject.Examplesare:o “Thisworkwasdonewithaone-monthcampaignon32racksofMira.”o “TheseresultsweredeterminedusingdatageneratedfromanALCC

project.”o “TheseresultsarefromcollaboratorswhodidnothaveALCCtimebut

usedtheresultsofourwork.”o Etc.

• ListPresentationsworkatALCFhttp://www.alcf.anl.gov/projects/high-frequency-ground-motion-simulation-seismic-hazard-analysis

• Listanyotherawards,honors,mediacoverage,etc

Papers

Lee,E.-J.,P.Chen,T.H.Jordan,P.J.Maechling,M.A.M.Denolle,andG.C.Beroza(2014),Full-3-DtomographyforcrustalstructureinSouthernCaliforniabasedonthescattering-integralandtheadjoint-wavefieldmethods,J.Geophys.Res.SolidEarth,119(8),6421–6451,doi:10.1002/2014JB011346.Thispapersummarizesthefull3DtomographyresultsfromcomputationsattheArgonneLeadershipComputingFacility.

Xu,Z.,P.Chen,andY.Chen(2013),SensitivityKernelfortheWeightedNormoftheFrequency-DependentPhaseCorrelation,PureAppl.Geophys.,170(3),353–371,doi:10.1007/s00024-012-0507-3.

Thesis

Donovan,J.(2015),ForecastingDirectivityinLargeEarthquakesinTermsoftheConditionalHypocenterDistribution,PhDThesis,UniversityofSouthernCalifornia,154pp.

Presentations

SeismologicalSocietyofAmerica,AnnualMeeting2015(SSAAM)-Lee,E.,Thomas,H.J.,Chen,P.,Maechling,J.P.,Boué,P.,Denolle,M.,Beroza,G.,&Eymold,W.K.(2015)Full-3DTomographyofCrustalStructureinCentralCalifornia.Abstractandpresentation,2015SSAAnnualMeeting.BlueWaters2015Symposium-SCECpresentedtheresultsattheannualBlueWaterssymposium,includetheCyberShakecalculation,anexampleofaSCEC,NSFBlueWaters,andINCITEresearchcollaborativeeffort.LinkstothepresentationarepostedonaSCECwikiat:

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http://scec.usc.edu/scecpedia/Blue_Waters_Symposium_2015NSFSoftwareInfrastructureforSustainedInnovation2015PIMeeting:-SCECmemberspresentedsoftwaredescriptionsandresearchresultsrelatedtoourFull3Dtomography(F3DT)andUnifiedCommunityVelocityModel(UCVM)workusingINCITEresourceataFeb2015NSFSoftwareInfrastructureforSustainedInnovation(SI2)meetingJan2015.TheNSFSI2programcurrentlyprovidesresearchfundingforsoftwareinfrastructureincludingF3DT,UCVM,AWP-ODC,andHerculesusedonourSCECINCITEresearchactivities.Moredetailsareavailableviathefollowinglinktothemeetingwebsite:https://share.renci.org/SI2PI2015/Lists/SI2PI2015Posters/View_01.aspx

NSCICoordinationMeeting(RestonVirginia)-SCECDirectoryThomasH.Jordanparticipatedinaninvitation-onlymeetinginOct2015concerningtheNationalStrategicComputingInitiative(NCSI)wherehediscussedSCECearthquakesystemscienceresearchbeingconductedusingALCF,OLCF,andNSFcomputingresources.

ExascaleComputingRFI:-SCEC’scomputationalscienceresearchgroupdevelopedadescriptionofourexascalecomputingneedsandcontributedittoaNSF/NIHHPCcommunity.SCEC’sdescriptionofourexascalecomputingneedsispostedhere:http://hypocenter.usc.edu/research/Exascale/SCEC_NCSI_Exascale.pdf

Supercomputing2015(SC15):SCECDirectoryThomasH.Jordanwasfeaturedasthe“InvitedTalkSpotlight”withhispresentationonSocietalImpactofEarthquakeSimulationsatExtremeScale.http://sc15blog.blogspot.com/2015/10/sc15-invited-talk-spotlight-societal.html

CodeDescription Pleasedescribeanymajordevelopmentorperformanceimprovementsthattookplacetoyourcode.Ifthedescriptionofthecodeissubstantiallydifferentfromearlierintheproject,pleasedescribe.SCECHPCcodeshavebeenfurtheroptimizedonINCITEresourcesin2015.Amajoreffortwastoportandintegratethenewnumericalalgorithmkernelplasticityandfrequency-dependentattenuationfeaturesintotheGPU-basedversionofAWP-ODC(OLCF).Simulationofnonlinearmaterialbehaviorrequiresanumberofadditionalvariables compared to linear computations. The added stencil kernel plasticityresultsincreasedghostcellregionfrom4to8layersinAWP-ODC,and17additionalvariablesaddedtotheoriginalcode.TheGPUcodeisrevisited,incollaborationwithDr. Peng Wang of NVIDIA. The combined new code moves advanced numericalalgorithms to a new level producing realistic seismograms at high frequencies,

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whichhasbeentestedandvalidatedfromsciencerunswiththeversioncalledAWP-ODC-PLA-QF-v2.1.0.5.ThiseffortissupportedbyNCSABlueWatersPAIDprogram.Theplasticitykernelwasabletoachieveeffectivememorythroughputof223GB/safter the tuning, or 89% of the peak, the tuned code has seen 13% overallimprovement. In addition, we have implemented and validated CUDA multi-streamingonKeplerforexecutingmultiplekernelsconcurrentlyonOLCFTitanandNCSA Blue Waters. Multistreaming was available on Fermi with 16-wayconcurrency,butCUDAstreamsmultiplexintoasinglequeue.OnKeplerthe32-wayconcurrency is allowed at full stream level, with one work queue per stream,without inter-stream dependencies. The new implementation of multi-streamingcodingisvalidatedandresults inaspeedupof17%intermsofwallclocktimeonKeplerXK7.Weplantoapplythismulti-streamingfeaturetothebaselineAWP-ODCandalsothenewplasticitycodetotakethefullperformanceadvantage.The near future plan is to complete the optimization for the velocity kernel insimilar way like performed for plasticity and stress kernel, also add parallel filewriting capability to thenewcode.Weplan to startmediumsize science runsonINCITEresources later inSpring2016,after thenewAWP-ODC implementation iscompleteandvalidated.SCECmakesextensiveuseofscientificworkflowstorunourCyberShakemodelcalculation.CyberShakeproductionrunsareourlargestheterogeneousensemblesimulationsthatdependheavilyonworkflowtechnology.ThescaleandcomplexityoftheCyberShakecalculationrequirestheautomationandreproducibilityprovidedbyworkflows.WewouldliketorunourworkflowsonbothMiraandTitan.SCEC’sexistingCyberShakeworkflowimplementationisbasedonaNSF-developedsoftwarestackthatincludesCondor,CondorDAGManager,andPegasus-WMS.Inthepast,SCEChasnotbeenabletorunourworkflowsonINCITEresourcesprimarilybecauseourworkflowsolutionrequiresremotejobsubmission.Inourcurrentworkflow-computingmodel,anexternalcomputer,atSCEC,runsaCondorDAGManagerjobqueue.Jobsaresubmittedtotheresourceprovider’sjobqueueatareasonablerate.HPCproviders,includingTACCStampede,andNCSABlueWatershavesupportedthisworkflow-computingmodelwithGlobusGRAM-basedjobsubmission.Thisyear,SCECworkedwithUSCPegasus-WMSworkflowtooldevelopers,andTitan’stechnicalgrouptodevelopasolutionthatwillenableSCECtorunourworkflowsonTitan.TitanprovidesthelargeGPUcountneededforthecomputeintensivepartofourCyberShakecalculations.Weareworkingtodeveloptechnicalsolutionthatwillenableustoliketorunthehigh-throughputpartoftheworkflowonTitan.OnceworkingonTitan,wewillworktoimplementthissolutiononMiraaswell.

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1. WhatisthecontributionmadebyLCFstaffand/orprograms(liaison/catalyst

collaboration,vendorsupport,userassistance,otherstaff,training,etc.)SCECinteractedwithALCFCatalystsandOLCFLiaison’sduring2015onstart-upcalls,onprogressreports,andintechnicaldiscussions.SCEC’sALCFCatalysthelpedusmigratelargedatasetsatALCFbetweenINCITEprojectswithoutinterruptingongoingactiveresearchusingthedata.SCEC’sOLCFliaisonshelpedcoordinatetechnicaldiscussionbetweenourworkflowdevelopmentgroupandtechnicalgroupsinsupportofourworkflowdevelopment.

NextSteps• Pleaselisttheexpectednextstepsforthiswork.Willyoubeworkingon

analysis?Ifso,where?Doyouneedadditionalallocations?Arethereupcomingpapersorpresentationsofthematerial?

• Aretherechangestocomingyearworkifyourprojectiscontinuing?Weareontracktocontinueourprogressforyear2milestones.Ourfull3DtomographyworkatALCFwillbemodifiedtorunathigherfrequencies.Thiswillrequirelargerparalleljobs.WewillworkwithALCFstaffsothatasweincreasethefrequencyofourtomographyresearch,ourroutinetomographycalculationswillscaleuptouse8racks,ormore,ofMira.

OtherCommentsPleaseanswerasapplicable:Hasthesupportreceivedfromthefollowingbeenbeneficialtoyourprojectteam?Citeexamplesifpossible• UserAssistanceCenter• CatalystsorPerformanceEngineering• VisualizationandAnalysisTeam• Operations

AnyadditionalfeedbackfromyourprojectteamfortheALCF?Pleaseincludeanyothercommentsorrequestsyouhaveaboutthefacility,allocationprogram,etc.