thermo-mechanical and atomistic assessment of first wall ...€¦ · g. gonzalez-rubio, o....
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Thermo-mechanical and Atomistic Assessment of First Wall, and Optics in
non-protective chamber in Inertial Fusion Energy
J M Perlado, A Rivera, R González-Arrabal, O. Peña, D Garoz*, M. Panizo
Ins$tutodeFusiónNuclear,ETSII,UniversidadPolitécnicadeMadrid,Spain.
*also,MechanicsofMaterialandStructures,[email protected]
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SUMMARY
THERMOMECHANICALEFFECTSFORDIFFERENTIFEREACTORASSUMPTIONS:DEFININGFWTHICKNESS
GRAINBOUNDARIESEFFECTSINHBEHAVIOUR:COMPUTATIONANDEXPERIMENTS
EFFECTSOFPLASMONICNANOPARTICLESINOPTICSBEHAVIOUR
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24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
WorkingparametersforHiPERdifferentschemesofimplementa9on
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DeposiEonofEnergyinFWfromTargetinDirectDriveDEMOHiPER
10%ofEnergyisdepositedwithindepthsupto100μmbythemostenergeEcions(>1MeV).
moredetailsinGarozetal,NuclearFusion
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24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
Reactor“start-up”Emes:
lowerthan~6sforPrototype(1Hz,50MJ)
and
~60sforDemo(10Hz,154MJ)
TwosituaEons:
“startup”
and
Steadystate
Steadystate Start-up
ODS-RAFM(925K)
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TemperatureevoluEonduringapulseoncethesteadystateregimeisreachedforHiPER
bothinProtoandDemoresults.3400K
Justajer1shot
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pulse=duringpulse
base=whenthematerialrecoverthebasetemperature
PulseheaEng
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24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
MonocrystalineinsimulaEonsNOGB.
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GBsdramaEcallyaffect thevacancyconcentraEon,beingmuchhigher forsampleswithalargeGBdensitythanforthosewithoutGBs.Thekeyreasonisthatmostofthevacanciesannihilate with SIAs in absence of GBs, whereas in NW, at this temperature in whichvacanciesareimmobile,alargerfracEonofvacanciessurvivesajertheirradiaEonduetotheefficientroleofGBsassinksforSIAs.
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DifferencesbecauseofprocedureinMWnoGBatall
NoGB=DiffusionH,at400nmvacancies
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(a)DifferencesareobservedwhencomparingresultsfortheCGWtothosefortheMWsamples.ThereasonisthatthesimulaEons(MW)donotconsiderGBsatall,whereassomeGBsexistintheCGWsample.
(b)ForNW-H,resultsclearlyindicatesHdiffusionalongthedepthdirecEon.
(c)FortheMW-Co-CH,themainHretenEonpeaklocatesat~400nm.ThisresultindicatesthatintheabsenceofGBs,HatomsdiffusealongtheirradiaEondirecEon,andintheirmigraEontothesurface,Hatomsreacharegionhighlypopulatedbyvacanciesat~400nm,wheretheygettrapped,explainingthedifferencesintheHprofilebetween150and540nm.
(d)ForNW-Co-CH,thereisgoodagreementbetweenmeasuredandsimulatedHprofile.InaddiEon,thetotalHretenEonisalmostthesameinthesimulaEonsasintheexperimentsanddiffusionisobserved.
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(f)ThemeasuredandsimulatedHprofilesagreequitewellfortheNW-Seq-CH.BothprofilesshowHretenEonpeakat~650nm.Moreover,thetotalmeasuredandsimulatedretainedfracEonsarequitesimilar.
WhenSequenEalC-H,weobservethattheenhancementfortheNWislowerthanthatfortheMWsamples.ThissupportstheideaoftheGBsacEngasdiffusionpathsforH.ThepresenceofahigherGBdensityinNWleadstoahigherprobabilityofHreleasealongGBs,beinglessaffectedbythepresenceofthehighervacancyconcentraEonsinducedbyCirradiaEon.
WhencomparingthedatafortheMW-Co-CHandfortheMW-Seq-CH,weobserveaclearinfluenceoftheirradiaEonprocedureitselfontheHretenEon,eventhoughtheconcentraEonofvacanciesissimilarinbothcases.
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Hatomsaremainlytrappedinvacancieslocatedintheinteriorofthegrains.ThenextquesEonistoesEmatethetypeandsizeofclusterswhereHatomsaretrapped.Studyisongoingexperimentally(M.Panizoetal.,tobepublished)
AccordingtooursimulaEons,sincevacanciesareimmobileatRT,morethan90%ofHatomsareretainedinmonovacancieswithdifferentHcontent.Moreover,DFTdatashowthatthatthemaximumnumberofHatomsthatcanbeaccommodatedinsidethemonovacancyis10.Fromthesedatawecanconcludethatself-healinginWwouldhappenattemperaturesinwhichthemobilityofvacanciesisacEvated.
Thisremark,togetherwiththefactthatGBsfavorsHrelease,indicatethatnanostructuredWmaybeacandidateforPFMapplicaEons,asithasahigherradiaEonresistancethanthetradiEonallyCGW
24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
TheirradiaEonofgoldnanorodcolloidswithafemtosecondlasercanbetunedtoinducecontrollednanorodreshaping,yieldingcolloidswithexcepEonallynarrowlocalizedsurfaceplasmonresonancebands.HighlyconcentratedsilvercolloidalnanoparEclesoluEonswereproducedthankstofslaserablaEonanditwasdemonstratedthatsuchembeddedplasmonicnanoparEclesmaybeviablecandidatestoreducedamagesproducedonopEcsbyswijheavyionsduetothechangeoftheirshapeunderirradiaEon
G.Gonzalez-Rubio,O.Peña-Rodriguezetal.,Femtosecondlaserreshapingyieldsgoldnanorodswithultranarrowsurfaceplasmonresonantes,Science358,640,2017
PlasmonicNanoparEclesandOpEcs
O.Peña-Rodríguez,etal.,Understandingtheion-inducedelongaEonofsilvernanoparEclesembeddedinsilica,NatureScienEficReports,7:922,2017
24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
24/10/18 IAEAFEC2018,Ahmedabad(India),J.M.Perladoetal.,InsEtutoFusiónNuclear/UPM,IFE/1-4
ACKNOWLEDGEMENT
WorkunderNa,onalResearchRADIAFUSENE-2012-39787-CO6,
MadridGovernmentTECHNOFUSION(II)-CM,S2013/MAE-2745,and
EurofusionToIFEProjectAWP15-ENR-01/CEA-02