Received:16October2015
Revised:10November2015
Accepted:12November2015
PublishedonlineinWileyOnlineLibrary
RapidCommun.MassSpectrom.2016,30,415–422(wileyonlinelibrary.com)DOI:10.1002/rcm.7459
Measurementofextremely2H-enrichedwatersamplesbylaserspectrometry:applicationtobatchelectrolyticconcentrationofenvironmentaltritiumsamples
L.I.Wassenaar*,B.Kumar,C.Douence,D.L.BelachewandP.K.Aggarwal
InternationalAtomicEnergyAgency,ViennaInternationalCenter,A-1400,Vienna,Austria
RATIONALE:Naturalwatersamplesartificiallyorexperimentallyenrichedindeuterium(2H)atconcentrationsupto
10,000ppmarerequiredforvariousmedical,environmentalandhydrologicaltracerapplications,butaredifficulttomeasureusingconventionalstableisotoperatiomassspectrometry.
METHODS:2Herewedemonstratethatoff-axisintegratedcavityoutput(OA-ICOS)laserspectrometry,alongwithH-enrichedlaboratorycalibrationstandardsandappropriateanalysistemplates,allowsforlow-cost,fast,andaccuratedeterminationsofwatersampleshavingδ2HVSMOW-SLAPvaluesuptoatleast57,000‰(~9000ppm)ataprocessingrateof60samplesperday.
RESULTS:Asonepracticalapplication,extremely2H-enrichedsamplesweremeasuredbylaserspectrometryandcomparedtothetraditional3HSpike-Proxymethodinordertodeterminetritiumenrichmentfactorsinthebatchelectrolysisofenvironmentalwaters.Highly2H-enrichedsamplesweretakenfromdifferentsetsofelectrolyticallyconcentratedstandardsandlow-level3(<10TU)IAEAinter-comparisontritiumsamples,andallcasesreturnedaccurateandpreciseinitiallow-levelHresults.
CONCLUSIONS:Theabilitytoquicklyandaccuratelymeasureextremely2H-enrichedwatersbylaserspectrometrywillfacilitatetheuseofdeuteriumasatracerinnumerousenvironmentalandotherapplications.Forlow-leveltritiumoperations,thisnewanalyticalabilityfacilitateda10–20%increaseinsampleproductivitythroughtheeliminationofspikestandardsandgravimetrics,andprovidesimmediatefeedbackonelectrolyticenrichmentcellperformance.Copyright©2016JohnWiley&Sons,Ltd.
Naturalwaters(1H2HO)artificiallyenrichedindeuterium(2H)intopureH2gas.[8–11]However,mostIRMSlaboratoriesarewellabovenaturalabundancemassfractionsareusedasreluctanttomeasurewatersextremelyenrichedin2HonIRMSpowerfultracersinmedical,environmental,2andhydrologicalinstruments(minorcollectornotoptimized),oronsampleapplications.AwidespreadapplicationofH-enrichedwaterpreparationapparatusroutinelyusedfornaturalabundanceisindoublylabelledwater(DLW)[1,2]usedforenergyexpenditurewaters(contamination).SomeIRMSsamplepreparationtestingofhumansandanimals.Otherapplicationsincludedevicessufferfromconsiderablebetween-samplecarryover,experimentsoftissueturnover,[3,4]usingdeuteriumasanespeciallywhenmeasuring2H-enrichedwatersamplesthatartificialtracerinfield[5,6]andlaboratoryhydrogeologicaloraffectdozensofsubsequentsampleswithouttheapplicationdiffusionexperiments,andforbatchelectrolyticenrichmentofcarryovercorrectionmodels.[12]IRMSmaysufferfromlargeoftritiuminenvironmentalwatersamples.[7,8]Thehighδscaleexpansionatenriched2Hconcentrationswhenusingconcentrationsof2HcomparedtonaturalwatersrangefromH2gas.Moreover,moststableisotopelaboratoriesdonotslightlyabovenaturalabundancemassfractions(~150ppm)haveappropriatestandardswithδ2HVSMOW-SLAPvaluesoftoextremevaluespotentiallysurpassing10,000ppmdeuterium1000‰ormore.[11]Asaresult,moststableisotopelaboratories(e.g.δ2HVSMOW-SLAPupto60,000‰).
areHydrogenisotope(δ2H)assaysofliquidwatersamplesare2unwillingtoaccept,orcannotmeasure,extremelyH-enrichedwatersamplesforanyoftheaforementionedtraditionallycarriedoutusingdual-inletorcontinuous-flowapplications.
isotope-ratiomassspectrometry(IRMS)usingeitherH2O(water)/H2(gas)equilibration,orZn/Cr/Chigh-temperature2In2001,thefirstlaser-basedmeasurementsofhighlyH-enrichedwatershadaδ2HVSMOW-SLAPlimitofaboutchemicalreactor(HTC)reductionmethods,viaconversion
15,000‰,withdemonstrablyimprovedreductioninbetween-samplememorycomparedtocontemporaryIRMSmethods,withsamplemeasurementtimesontheorderof*Correspondence40min.[13]Since2009,low-cost,commercialwaterisotopeEnergyAgency,to:ViennaL.I.Wassenaar,InternationalInternationalCenter,AtomicA-1400laserspectrometershaveovertakenVienna,18IRMSastheprimarymeanstomeasureδ2H(andδO)innaturalwaters.RequiringE-mail:l.wassenaar@iaea.org
Austria.
littlewater(<1000nL)andfewconsumables,andwith
RapidCommun.MassSpectrom.2016,30,415–422Copyright©2016JohnWiley&Sons,Ltd.
415L.I.Wassenaaretal.
minimaltraining,laser-basedwaterisotopemeasurementsareatastageofwidespreadadoptionandaffordability.[14,15]Thefirsttestsof2H-enrichedDLWwaterbycommercialcavityringdown(CRDS)laserspectrometryshowedsuccesswithsampleshavingδ2HVSMOW-SLAPvaluesupto~750‰,butrequiredmorethan20sampleinjectionstoovercomesignificantbetween-samplememory;hence,only15samplesperdaycouldbemeasured.[16]However,withrecentdevelopmentsinlaserspectrometry,thepotentialformodernliquidwaterisotopelaserinstrumentationhasnotbeenadequatelyexploredforextremely2H-enrichedwatersamples,whichmaybeusefulfortheaforementionedapplications,orintracerorexperimentalstudies.
Theobjectiveofthispaperistwofold:(i)todemonstratethatcommercialoff-axisintegratedcavityoutputlaserspectrometry(OA-ICOS)canbeusedtorapidlyobtainaccurateandpreciseδ2HVSMOW-SLAPvaluesforbothnaturalabundanceandwatersamplesextremelyenrichedindeuteriumupto57,000‰,and(ii)subsequentlytodemonstratetheefficacyofusingthisanalyticalcapabilityforlaser-based2H-enrichmentmethodstoimprovetheproductivityofenvironmentaltritiumlaboratoriesengagedinbatchmodeelectrolyticenrichmentof3H.
(e.g.gramsH2O)ofthespikesamplebeforeandafterelectrolysis.InitialtritiumconcentrationsofunknownsamplesprocessedthroughtheTEUaredeterminedbyrearrangement:
Ti¼Tf=ððVi=VfÞÁRÞ
(2)
Thetritiumrecoveryfactor(R),unfortunately,canonlybedeterminedonspikecells.HencespikerecoveriesandderivedenrichmentparametersareaveragedandappliedequallytoallTEUcellscontainingunknownsamples.QuantitativewaterrecoveriesandaccurateweighingarecriticalintheSpike-Proxymethod.Disadvantagesareasignificantreductioninsamplethroughputbecauseofthespikerequirement.
AnalternativetotheSpike-Proxymethodisthe2H-enrichmentmethod,[8]whichleveragesthefactthat2H(HDO)iscorrespondinglyconcentratedinaTEUelectrolysisprocess,albeittoalesserextentthantritium(HTO)duetodifferentnetisotopefractionationfactorsandvaporlosses.Nevertheless,tritium(ifpresent)anddeuteriumareverystronglycorrelatedduringelectrolyticenrichment.[8,9]Becausetheelectrolyticallyenriched2Hsamplecanbemeasuredasanindependentvariable,itprovidesameansfordeterminingthe3H-enrichmentfactorsforeachcell.Thisledtotheconceptofacellconstant(k)thatcorrelatesthe3H-and2H-enrichmentfactorstoeachother:[19]k¼lnðTf=TiÞ=lnðDf=DiÞ
(3)
HMETHODFORDETERMINING
ELECTROLYTICTRITIUMENRICHMENT
Tritiumisapopularradiotracerofshort-termhydrologicandgroundwaterresidencetimes,[17]butexceedinglylowconcentrationsinenvironmentalwatersnowadaysaretoolowfordirectdecaycounting.Thuswatersamplestypicallyrequirepre-concentrationof3Hbyelectrolyticenrichment.[7,18]Methodsforpre-concentratingtritiumusing250–1000mLwatersamplesemploysetsofmild-steelalkalineelectrolysiscells,orpolymerelectrolyticmembraneunits.[9,19,20]Alltritiumenrichmentunits(TEUs)havethreecommonalities:(i)pre-distillationofsamplestoremovedissolvedions,(ii)electrolytic3Henrichmentofthedistilledsamplesto8–60mLfinalvolume,and(iii)decaycountingbyliquidscintillation(LSC)orgasproportionalcounting(GPC)instruments.Dependingonthe3Hconcentration,startingandfinalsamplevolumes,electrolyticcell-type,andoperationalconditions,watersamplesmaybeenrichedin3Hbyfactorsof10–90timesormore[7]asneededforLSCorGPC.Notably,2Hiscorrespondinglyconcentratedduringelectrolysis.
AcriticalrequirementforanyTEUisaccuratedeterminationofthetritiumenrichmentfactorforeachcellinordertocorrecteachsamplebacktoitsoriginal3Hconcentrationintheenvironment(withappropriatedecaycorrection).MostlaboratoriesusetheSpike-Proxymethod,whereby10–20%ofsamplesprocessedthroughtheTEUarehigh-concentrationtritiumstandards(spikes).Thetritiumrecovery(R)isdeterminedfrompre-andpost-electrolysisgravimetricH2Orecoveries(Vfinal/Vinitial)andmeasurementofspike3Hconcentrationsbeforeandafterelectrolyticenrichment:
R¼ðTfÁVfÞ=ðTiÁViÞ
(1)
2whereDisthefinal(f)andinitial(i)sample2Hconcentrationinppm,andTisasabove.Rearrangementallowsdeterminationoftheinitialunknowntritiumconcentration(Ti)ofasamplebyknowingk(foreach,orbyaveragingidenticalcells),measuring3Hintheelectrolyticallyenrichedsample(Tf),andmeasuringtheinitialandenriched2Hconcentrations:
Ti¼Tf=ðDf=DiÞk
(4)
Akeyrequirementofthe2Hmethodfordeterminingtritiumenrichmentfactorsisaccuratedeterminationofthecellconstant(k)forallTEUcells,bytheabilitytomeasureextremely2H-enrichedliquidwatersamples.Thecellconstantisdeterminedempiricallybycoupled2Hand3Hspiketesting,alongwithcarefulgravimetricrecoveries.Thecellconstantcanbedeterminedforindividualcells,oraveragedifidenticalbehaviorcanbedemonstratedforeachTEUset.[19]Anaddedbenefitofthe2Happroachiseliminationoflaboriousgravimetricweighingsteps(seeEqn.(4)).Whileeliminationofgravimetricweighingseemsattractive,bymaintainingitthedeuteriumrecoveryfactor(Rd)foreachcellcanalsobedetermined:
Rd¼ðDfÁVfÞ=ðDiÁViÞ
(5)
whereTisthetritiumconcentrationofthespike(netcountsperminute(CPM)afterbackgroundsubtraction)before(i)andafter(f)electrolysis,andVisthewatervolume
The2Hrecoveryfactorfacilitatesimmediatedetectionofelectrolyticcellperformancedegradation,bynothavingtowaitforweeksforspikeLSCcountingcompletion.Todate,the2Hmethodisemployedbyfewlaboratories,andinallcaseshighly2H-enrichedsamplesareusuallydilutedbyafactorof1000ormoretothenaturalabundancerange[7]andmeasuredbytraditionalIRMSatconsiderableextracost.Therequisitelargedilutionsandisotopemassbalancebudgetingcontributesignificanterrortotheoverallprocess.
416wileyonlinelibrary.com/journal/rcmCopyright©2016JohnWiley&Sons,Ltd.RapidCommun.MassSpectrom.2016,30,415–422
Measurementofextremely2H-enrichedwatersbylaserspectrometry
EXPERIMENTAL
resultsofelectrolyticallyenrichedsamplesandspikesas2measuredbylaserspectrometry.EachlaboratorystandardH-enrichedcalibrationstandards
wasmeasuredseveralhundredtimesagainstIAEA605andInordertomeasureextremely2H-enrichedwatersamples,IAEA606.Notably,IHLW-68waspredictedtofallappropriateenrichedcalibrationstandardsareneededthatconsiderablyoutsidethecalibrationrangeoftheIAEA605spantheδrangeofthesamples.[11,12]Untilrecently,noandIAEA606referencematerials.
primaryreferencewatershighlyenrichedindeuteriumwereavailable.In2015,theInternationalAtomicEnergyAgencyTritiumenrichmentunittestwatersamples
(IAEA,Vienna,Austria)announcednew2H-(and18O-)Allthe3Hwatersamplesfor2H-enrichmenttestingwereenrichedprimaryHDOstandards.[21]Forthepurposesofspikestandardstritiumenrichment,twoofthesestandards(IAEA605,3thatweremeasuredforvolumetricmassbalancesandHand2Hconcentrations,using250mLandIAEA606)wereusefulforthedevelopmentof2H-enriched500mLpre-andpost-electrolyticTEUsystems.Asecondsetlaboratorycalibrationstandards.Theδ2HVSMOW-SLAPvaluesoftestsamplesconsistedof500mLlow-level3HsamplesoftheIAEAprimaryreferencewatersaresummarizedinfromthe2012IAEATRICinter-comparison.[23]TheTRICTable1.Owingtothesmallamountofreferencematerialssamplesallowedustodeterminehowwelllaser-based2Hprovided(20mL),weprepared20Lofthree2H-enrichedmethodsresultedintritiumenrichmentfactorsthatreturnedlaboratorystandardwatersforuseindailynormalization;accurateandpreciseoriginallow-level3Hresults.
theselaboratorystandardswerecalibratedusingassignedBatchelectrolyticenrichmentswereconductedusingmildvaluesforIAEA605andIAEA606.
steel24-cellTEUsystems(250mL,500mL)attheIAEAThreenewlaboratorystandardswerepreparedgravimet-IsotopeHydrologyLaboratory(IHL)whichhavebeeninrically[22]usingdistilledtapwater(δ2HVSMOW-SLAP=–77‰),useforover20years.ThealkalineTEUsystemanditsandbyadding32–200gof99.9993%deuteriumoxideoperationarefullydescribedintheIAEAtritiumstandard(Sigma-Aldrich,St.Louis,MO,USA)inordertospantheoperatingprocedure(SOP)availablefromtheIsotopeδ2Hrangefor250–2000mLelectrolyticallyenrichedsamplesHydrologyLaboratory.[24]Briefly,theIHLusestheSpike-obtainedintypicaltritiumoperations(estimatedtobeintheProxymethodwhere3ofthe24(13%)samplesineach6000–60,000‰rangeforδ2HVSMOW-SLAP).ThelaboratoryTEUprocessingbatcharespikes.Thesespiketripletsarestandardswerehomogenizedfor1weekpriortoisotopicadvancedbyonepositionineachnewelectrolyticrun.Thus,analysisandstoredat0.5barargongaspressureinsteelspikesarecycledthroughtheTEUevery8runs,andareusedsiphon-dispensingcontainers.Allδ2HVSMOW-SLAPcalibrationstodetermineenrichmentparametersforalltheremainingwereconductedbyoff-axisintegratedcavityoutputlasercells.Forthistest,0.5mLpre-andenrichedspikesamplesspectrometry,asdescribedbelow.
weresampledopportunisticallyfor2HfromroutineIHLInordertoobtainassignedδ2HVSMOW-SLAPvaluesforthesampleprocessingoperations.Onediscrete500mL,laboratorystandards,weconductedtwo-pointdata24-sample,TEUanalysissetcontainedtriplicatesamplesofnormalizationusingIAEA605andIAEA606ascalibrationlow-levelTRICtestwatersamples.Deuteriumsamplingstandards,withthelaboratory2standardsmeasuredasconsistedoftakinga0.5mLsub-sampleofthepre-electrolysisunknowns.Aftercalibration,δHVSMOW-SLAPvalueswerespike(naturalabundance,afterpre-distillation)anda0.5mLassignedtoallthree2H-enrichedlaboratorystandards(IHLsub-samplefromthe10–12mLfinalelectrolyticallyenrichedW-62,IHLW-63andIHLW-68)andusedtonormalizethe
post-distilledsample(extremely2H-enriched).Allthe
Table1.2HVSMOW‐SLAPvaluesofprimaryisotopicallyenrichedreferencewaters,gravimetricestimatesandlaserspectrometricassayofthreehighly2H‐enrichedIHLlaboratorywaterstandardsusedinroutinetritiumprocessingIAEAPrimaryStandardsδ2HVSMOW‐SLAP(‰)
2H(ppm)
VSMOW20142.8SLAP2IAEA6055,997.9–427.51088.8.2IAEA606
15,993.62639.9EnrichedLaboratoryStandardsδ22(‰H,VSMOWgravimetric)‐SLAPδ2(‰HVSMOW,measured)‐SLAPNH(ppm)
IHLW‐629249–909173.7±34901582.1IHLIHLWW‐‐6368
17,91958,211––18,28257,057
18,0.2±656,842.8±10
320116
2960.629.1
aGravimetricestimateswerebasedon20L(kg)ofdistilledtapwater(δ2HVSMOW‐SLAP=–77‰)andadding32.00,.00and200.00gof99.9993deuteriumoxide,assuming1%weighingerror.Gravimetricestimatesweremadebymixingandisotopelaboratory.
N=numbermassofbalancemeasurementsequations.[22]bmadebylaserspectroscopy.Boldfaceismean±SEM,withassignedδvaluesusedintheIHLRapidCommun.MassSpectrom.2016,30,415–422Copyright©2016JohnWiley&Sons,Ltd.wileyonlinelibrary.com/journal/rcm
417L.I.Wassenaaretal.
distilledpre-andpost-electrolysissamplesfor2Hanalysiswerestoredintightlysealed1.5mLTeflonseptumcappedlaserspectrometryvialsuntilanalysis.Laseranalyseswereconductedwithin1dayto1weekaftercollection.Tritiummeasurements
Unenrichedandenrichedspikesamplescorrespondingtothesame2Hsub-samplesweremeasuredbyliquidscintillationcounting(LSC)onaQuantulus1220™(PerkinElmer,Akron,OH,USA).Thetritium-countingprocedureisfullydescribedintheIAEASOP.[24]Briefly,8mLofpre-andpost-enrichedspikesweremixedwith12mLofUltimaGolduLLT™(PerkinElmer)scintillationcocktailandallowedtostabilizeinthedark.TheLSCtemplateconsistedof24unknownenrichedsamplesincluding3enrichedspikes,aswellas2unenrichedspikes,2calibrationstandards,and4backgroundsamples.Thetotalcountingtimewas500min/sampleconductedover10countingcycles(approx.12days).OptimaloperationoftheQuantulusLSChasbeendescribedpreviously.[25]Allspectralregionsofinterestwereoptimizedforlow-level3Hbetacountinginwatertoobtainthehighestfigureofmerit(FOM).NetCPMvaluesforpre-andpost-enrichedspikeswereobtainedbysubtractionofthemeanbackgroundCPM(~0.5to0.8CPM)onaperrunbasis.Forthisstudy,weextractednetCPMdataofpre-andpost-spikedataobtainedfrommultipleQuantulusLSCrunscoveringtheperiodfromOctober2014toJuly2015,andwheredeuteriummeasurementswereconducted.AlldataprocessingwasdoneusinganExcel-basedTritiumInformationManagementSystem(TRIMS)developedattheIHL.ErrorpropagationwasdeterminedforalltheprocessingstepsasoutlinedintheIAEASOP,andthiswasincludedinthefinaluncertaintyreportingofthe3Hresults.Laserspectrometryfor2H-enrichedsamples
Severaloff-axisintegratedcavityoutputwaterisotopelaserinstrumentsfromLosGatosResearch(MountainView,CAUSA)weretestedfordirectlymeasuringhighly2H-enrichedwaters.Wetested1st-3rdgenerationLosGatosResearchlaserinstrumentsandfoundtheydidnotcorrectlyreportδ2Hvaluesabove~12,000–15,000‰,despiteapparentlygoodisotopologueopticalspectrometry,dueinternalsoftwarelimitationsintheseolderinstruments(DougBaer,LosGatosResearch,personalcommunication).InthisstudywethereforeusedthenewestLosGatosResearchliquidwaterisotopeanalyzermodel912-0032(4thgeneration).
Forlaser-basedHDOmeasurements,allthepre-andenrichedpost-electrolysissamplesandlaboratorycalibrationstandardswereseparatedintothreegroups.Thefirstcomprisedpre-enrichmentsampleshavingnaturalabundance2Hlevels.Theseweremeasuredbyroutinelaserspectrometryusingnaturalabundancewaterstandards,controls,anddata-processingproceduresusingLIMSforLasers2015,asfullydescribedelsewhere.[15,26]Abatchof24TEUpre-enrichedwatersamplesandstandardsemployedananalysisprotocolof8injections,ignoringthefirst4,atarateof11min/sample.
Forextremely2H-enrichedwatersamplesbeyondtheVSMOW-SLAPcalibrationscale,thesameprocedurewasusedbutwithsomemodifications.First,watersampleswereseparatedbyTEUsizeandtheexpecteddegreeof2Henrichment.Forexample,250mLcelland500mLcell
deuteriumsamplesweregroupedseparately.Forthe250mLTEUsystem,wepredictedδvaluesaround12,000‰andthereforeusedatwo-pointcalibrationusinglaboratorystandardsIHLW-62(lowstandard)andIHLW-63(highstandard);inthecaseofthe500mLTEUor1000mLandhigherexperimentalenrichmentssamples,weusedIHLW-62(lowstandard)andIHLW-68(highstandard),andIHLW-63wasusedasacontrol(Table1).
Theonlyotherminormodificationforlaserspectrometrycomparedwiththenaturalabundanceprocedureswasthenumberofinjectionspervial.Owingtothehighlyenriched2Hlevels,weempiricallydeterminedthat12injections,ignoringthefirst4,wassufficienttoobtainaccurateresultsandminimizebetween-samplememorycorrectionsasquantifiedbyLIMSforLasers2015.Thisresultedinananalysisrateof16min/sampleforeachenrichedsample.FortheroutineTEUsetsof24samples,thistranslatedtoonly504injectionspersetonthelaserinstrument,wellwithinhigh-performanceseptaspecifications(SupelcoThermogreenLB-2,6mmdisks;Supelco,Bellefonte,PA,USA).Includinglaboratorystandardsandcontrols,theprocessingratewas60unknownsamplesperday.Ifthelaserinstrumentusedforhighly2H-enrichedsampleswassubsequentlyneededfornaturalabundancewatersamples(pre-enrichedsamples,allothersamples),approximately50sequentialinjections(approximately1h)oftapwaterwassufficienttoflushawaytheresidualmemoryofthe2H-enrichedwatersamples.Inshort,completesetsofpre-andpost-electrolysiswatersamplescouldbeanalyzedbylaserspectrometryinlessthan48h,therebyprovidingnearimmediatefeedbackonthebatchTEUelectrolyticenrichmentperformance.
Alllaser-baseddeuteriumresults(δ2HVSMOW-SLAP)wereprocessedandreportedinthe‰notationrelativetotheVSMOWstandard,andprocessedusingLIMSforLasers2015.Theδvaluesdataweretransformedintomassfractionsdeuterium(ppm)using:
ÀÁ
Dppm¼δ2HVSMOW-SLAPþ1000=ðδ2HVSMOW-SLAPþ1000
(6)þ1000=0:00015576ÞÁ1000000
RESULTSANDDISCUSSION
2H-enrichedlaboratorystandards
Gravimetricallydeterminedandlaser-measuredδ2HVSMOW-SLAPvaluesforthreeIHLlaboratorystandardsmeasured
relativetoIAEA605andIAEA606aresummarizedinTable1.InthecaseofIHLW-62andIHLW-63,thelaserspectrometry-measuredδ2Hresultsfellwithintheδrangepredictedbygravimetricdeterminations.ForsampleIHLW-68,themeasuredδ2Hvaluewasonlyslightlylowerthanpredictedbygravimetriccalculations,probablybecausethesamplewasfaroutsidetheIAEA605andIAEA606referencecalibrationrange,andduetopossibleeffectsofveryslightisotopicδ-scalecompressiononthelaserinstrument.Asafurthercheck,wemeasuredIHLW-63asanunknownsampleusingassignedvaluesofIHLW-62andIHLW-68ascalibrationstandards.Inthiscase,IHLW-63returnedaδ2HVSMOW-SLAPvalueof+18,232±33‰(n=38),closetothatreportedinTable1,andwithintherangepredictedby
418wileyonlinelibrary.com/journal/rcmCopyright©2016JohnWiley&Sons,Ltd.RapidCommun.MassSpectrom.2016,30,415–422
Measurementofextremely2H-enrichedwatersbylaserspectrometrygravimetricestimates.Withoutprimarystandardscoveringeachtripletwasthemeanoftwomeasurements,summarizedthishigherδrange,theIHLW-68valueremainstentative,inTable2.Theindividualcellconstantswereremarkablybutforsucha2highenrichmentwasremarkablyclosetosimilarwithinandacrossbothmild-steelTEUsystems.ForthepredictedδHvalue.Forourpurposes,weacceptedthe250mLTEUsystem,themeancellconstantkwasthelaser-measuredδ2HvaluesinTable1ascorrect,and1.0542±0.0044,withanoverallrangefortheindividualcellstheseδvaluesandtheiruncertaintieswereassignedforallbetween1.0460and1.0620.Forthe500mLTEUsystemthesubsequentroutine3Helectrolysisanddata-processingmeancellconstantwas1.0592±0.0101,withtheoverallrangeoperations.Sampleδvalueconversionsintomassfractionsforindividualcellsrangingfrom1.0509to1.0670.AStudent’s(ppm)arelistedinTable1.FortheprimaryRMsandt-testrevealedthattherewasnosignificantdifferencelaboratorystandards,themassfractionsofdeuteriumbetweenthemeancellconstantsofthe250mLand500mLrangedfrom.2ppm(VSLAP2)to2639.9ppm(IAEA606),TEUsystems(p=0.058).ThemeancellconstantforthewhereastheenrichedIHLlabstandardsrangedfromcombined250and500mLTEUsystemswastherefore1582.1ppm(IHLW-62)to29.1ppm(IHLW-68).These1.0555±0.0048.Forallsubsequentcalculations,andduetofindingsshowthatcommerciallaserspectrometrycanbetheabsenceoflongtrackrecordsforindividualcellconstants,usedtoquicklyandaccuratelymeasurewatersamplesweusedthemeancellconstantanditsuncertaintyasextremelyenrichedin2H,andhavingδ2Hvaluesuptoatapplicabletothe250mLand500mLIHLTEUsystems.
least57,000‰,andpossiblyevenhigher.
TodemonstratehowwellusingacellconstantkrecoveredTheenrichedlaboratorystandardIHLW-68waspreparedintheinitialmeasuredCPMforbothIHLelectrolysissystems,anticipationofelectrolyticenrichmentoflarge1–2Lsamples,Eqn.(4)wasusedtodeterminetheinitialsample3HCPMwhichwillbeincreasinglyrequiredasenvironmental3Hlevelsvalues.InTable2,acomparisonof3Hinit(e.g.un-enricheddeclinetobackgroundlevels.Indeed,therecentTRICtestspike)withtheelectrolyticallyenrichedspiketriplicatesrevealedthatonlylaboratoriesthatenrichedwatersamplesCPM,andapplicationoftheuniformcellconstant,revealed50×orhigherwereabletoachieveaccurateandpreciseexcellentperformanceindeterminingtheinitial3Hcontentresultsforlow-level(<5TU)tritiumtestsamples.[23](lastcolumn),despitethefactTEUsampleenrichmentsCurrently,fewlaboratoriesenrichsamplesgreaterthanwereconductedovera10-monthperiodwithtwodifferent500mL(e.g.δ2HVSMOW-SLAPof~25,000‰)duetoextracostTEUsystemsandusingthreedifferentLSCcounters.Notably,orthelack2ofasuitableTEUapparatus.Theabilitytodirectlynogravimetricdatawasrequiredwiththe2HmethodmeasureHatextremeconcentrationsbylaserspectrometrytodetermineprovidesanewwaytoquicklydeterminecellperformance3thetritiumenrichmentfactorsortheinitialsampleHcontent.
and3H-enrichmentfactorsbeforehand,withouthavingtoPoorlyperformingcell#4showedamarkedlydifferentwaitweeksforLSCspike-countingresults.kconstant(1.1219)fromthegoodcells.Importantly,applicationofthemeasuredcellconstantyieldedanResultsoftritiumspikestandards
inaccurate3Hrecovery(10.91CPMvsactual8.82CPM),indicatingthatthe2H-derivedcellconstantscannotbeusedTheresultsof3Hand2Hassaysonspikesprocessedonblindlytoremedybadlyperformingcells.Poorlyperforming250mLand500mLTEUsystemsbetweenOctober32014andcellsshouldberemovedfromtheTEUandreconditioned.July2015aretabulatedinTable2.The2HandHrecoveriesMonitoringdeuteriumrecoveryfactorsisthereforeanforeachelectrolyticcellweredeterminedusingEqns.(1)importantcontrolinevaluatingTEUcellperformance.Ourand(5).Theaveragedeuteriumrecoveryforthe250mLdataTEUwas74.4±1.6%,withanoverallrangeforindividual2suggestthat3HresultsobtainedfromcellswithpoorHrecoveries(e.g.<70%onIHLTEUsystems)shouldnotcellsofbetween71and77%.Theaveragedeuteriumbeaccepted.These2Hcontrolcriteriawillneedtoberecoveryonthe500mLTEUwas77.0±1.0%,witharangedevelopedforeachuniquelaboratoryTEUsystem.Ideally,forindividualcellsofbetween75and79%.Notably,cell#4overtimeitmaybepossibletoobtainrobustindividualmean(excludedfromsummaries)wasknowntobeperformingcellkconstantcriteriabymaintainingregularoroccasionalbadly,andwasintheprocessofbeingreconditionedafterspiketesting.Whiletheuseofindividualcellconstantsseemschemicaltreatment.ThisTEUcell2stillindicatedpoor2Hintuitivelysuperior,itremainstobeseenwhetherindividualrecoveryofonly54.8%.Thus,Hcanalsobeusedasancellconstants,versusindicatorformonitoringcell-enrichmentperformanceprior3averagedcellconstants,providesdemonstrablybetterHresultsafterallsourcesofuncertaintytostartingLSCcounting.Inourcase,athresholdof70%arefactoredin.
fordeuteriumrecoveryappearedtobeareasonablelowerboundtorevealcelldegradation,uponwhichcellreconditioningmaybewarranted,andsamplesfromdegradedcellsshouldEvaluatingthe2Hmethodforaccuracyandprecisionnotbeused.Similarly,themean3Hrecoveryonthe250mLThefinaltestconsistedofapplyingthe2H-3H-determinedTEUsystemwas86.3±2.2%,withanoverallrangeformeancellconstantktoaroutinesetof24samplesprocessedindividualcellsof81–%.Themean3Hrecoveryforbyenrichmentonthe500mLTEUsystem(includingpoorlythe500mLTEUsystemwas92.4±2.1%,withanoverallperformingcell#4),andthencomparingthefinaltritiumrangeforindividualcellsoffrom90to97%.Poorlyperforming(TU±SD)outcomeswiththoseobtainedusingthecell#4hadalow33Hrecoveryofonly81.0%.
conventionalSpike-Proxymethod.ThistestsetincludedThecell2H-Hconstant(k)valuesforthe250mLandtriplicatesoftheIAEAtritiuminter-comparisonsamples,500mLTEUs2weredeterminedusingEqn.(3)andthewhichconsistedoffivelow-levelsamples<8TUhavingmeasuredδHand3Hvaluesfromeachtriplicatedspikewell-established3Hvalues,[23]threespikestandards(knownandcell.TheinitialCPMoftheunenrichedspikesamplefor
TU),twounknownsamples(oneDIwaterplacedincell#4)
RapidCommun.MassSpectrom.2016,30,415–422Copyright©2016JohnWiley&Sons,Ltd.wileyonlinelibrary.com/journal/rcm
419L.I.Wassenaaretal.
Table2.Resultsof250mLand500mLTEUspikesamplesfordeterminationofindividualandaverage2H-3Hcellconstants(k)Electrolysis
ID250mL
140514051405140614061406140714071407140814081408140914091409141014101410141114111411500mL
241924192419242024202420242124212421242224222422242424242424242524252425CellConstant
MeanSD
aCounterIDQ3Q3Q3Q3Q3Q3Q2Q2Q2Q1Q1Q1Q1Q1Q1Q1Q1Q1Q1Q1Q1Q2Q2Q2Q1Q1Q1Q1Q1Q1Q3Q3Q3Q3Q3Q3Q2Q2Q2
Cell#1011121617181920212223241234567192021222324123456101112131415
VoVfgrams
2Hinit2Hfinal2H
3Hinit3Hfinal3HCell
3H
ppm143.5143.4143.5143.6143.7143.7143.5143.6143.6143.7143.7143.7143.6143.6143.6143.7143.7143.6143.5143.6143.7143.6143.4143.4143.5143.5143.4143.4143.5143.6143.6143.6143.5143.4143.5143.7143.5143.4143.4
2365.32398.62363.82303.92323.32300.92178.92208.22329.72204.32247.92102.32172.52207.42076.921.12176.22186.22299.02177.32219.73754.33385.83251.03373.23676.43530.03578.43347.63639.13548.03526.03530.63454.73486.63634.13331.13292.43533.0
Recovery%
75.475.072.775.373.373.971.275.371.673.175.373.876.476.474.675.877.074.275.874.172.478.476.175.677.276.676.176.576.478.154.877.776.477.377.477.178.179.175.5
9.138.918.739.219.109.019.24
cpm173.48177.31174.46165.53167.76167.28150.80153.73162.83167.28168.82158.12160.33163.61154.80158.21158.25160.29168.18161.22163.20271.96242.11233.05270.34294.93282.27282.85265.97288.30322.03261.80261.41252.06252.266.23229.95226.48244.42
Recovery%constantInitial
87.087.184.487.185.386.781.186.282.486.688.286.688.9.387.788.4.386.786.185.282.4.290.1.792.792.091.190.190.592.381.093.992.191.991.692.296.497.393.4
1.05081.05331.05311.05271.05461.05721.04751.04951.05001.06201.05771.05971.05601.05721.06071.05681.05451.05731.04601.05161.04901.05601.05351.05481.05791.05661.05631.05091.05381.05161.12191.05931.05831.05471.05281.05561.06711.06611.06
9.009.069.068.848.8.958.548.588.599.379.269.319.119.149.239.048.9.058.999.149.078.688.618.9.659.619.609.4.579.5010.918.928.908.778.728.808.328.298.31
249.4249.2249.2249.5249.3249.1249.3249.3249.1249.6249.4249.8249.6249.6250.0249.4249.5249.5249.4249.8249.98.4498.98.98.5499.0498.7498.5498.9498.98.7498.4498.0498.7499.0498.9499.5499.3499.5
11.411.211.011.711.311.511.712.211.011.912.012.612.612.412.912.512.712.211.812.211.715.016.116.616.414.915.415.316.315.411.115.815.516.015.915.216.817.215.3
8.669.5.638.828.808.02
250mL500mLAll1.05421.06081.05550.00440.00500.0048
Themeancellconstantkwasusedtodetermine3Hinitialinthefinalcolumn.Definitionsandequationsforrecoveryandthecellconstantaregiveninthetext.Q=QuantulusID.bResultsaresortedbyincreasingdateofanalysis(October2014toJuly2015)asspikeswererotatedthrougheachTEUsystem.cNoteunderperformingCell#4inthe500mLsystemisevidentbypoor2Hand3Hrecoveries.
andoneenrichedbackgroundsample.Theuseoftheseinter-comparisonsamplesallowedindependentverificationoftheaccuracyofperformanceofthe2HandSpike-ProxymethodstoobtainenrichmentfactorsandproduceaccuratefinalTUresults.
Theelectrolysis,2HandLSCcountingtestresultsareshowninTable3,andgivecomparativeoutcomesusingthelaser2H-enrichmentandSpike-Proxymethods.WiththetraditionalSpike-Proxymethod,threemeasuredspikesshowninTable3wereusedtodeterminethemeantritium
420wileyonlinelibrary.com/journal/rcmCopyright©2016JohnWiley&Sons,Ltd.RapidCommun.MassSpectrom.2016,30,415–422
Measurementofextremely2H-enrichedwatersbylaserspectrometry
Tablesamples,3.Resultsofa500mL,24-sample,TEUrunwithspikes,TRICandunknownsamples,2comparingthetritiumenrichmentfactors,2HrecoveryandthefinalTUplusuncertainties,andanenrichedcomparingbackgroundtheH-enrichmentandSpike-Proxymethods
Cell#SamplenameLabNo.Sampling
dateEnrichment
TUUncertaintyRecoveryEnrichment
TUUncertainty
Spikemethod
2H-Enrichmentmethod
1
Spike24227/30/201429.7537.865.3876.529.8535.343.3423SpikeSpike
239724217/30/20147/30/201427.829.5539.16550.905.165.6176.478.127.830.3540.42536.513.573.4945AlmendrasTRICJuly24547/15/20112.106TRICT252011T242455244912/1/201239.812/1/201228.328.47.560.12.12.4.360.120.1977.534.076.928.728.67.450.134.330.100.1878TRIC2.8TRICT23245112/1/201229.0TRICT22T212509251412/1/201212/1/201227.930.21.100.1076.52.880.450.120.1176.929.177.928.131.01.100.090.440.120.111011TRICTRICT20T252510251512/1/201212/1/201230.829.60.007.380.070.2675.976.630.829.80.007.340.070.251213TRIC29.414TRICT242511TRICT23T22251912/1/2012252012/1/201212/1/201228.84.600.1529.827.62.881.280.1077.20.1178.079.029.54.5428.52.820.151.240.100.111516TRICTRICT20T202521251612/1/201212/1/201231.629.3-0.120.30-0.090.0974.976.531.229.4-0.120.31-0.090.091718TRIC29.219TRICT212512TRICT21T22251712/1/2012251312/1/201212/1/201230.30.650.1128.930.40.661.180.1375.50.0976.479.730.40.650.1131.90.651.120.130.092021TRICTRICT23T24251835012/1/201212/1/201229.028.82.724.570.130.1477.275.729.328.62.694.610.120.142223TRIC28.024
SampleT25250EnrichedTK-11
Deadwater
250250
10/12/201412/1/20121/26/2009
30.27.790.2928.329.8
1.530.42
0.0677.30.16
76.776.1
30.57.710.2829.8
1.520.42
0.060.16
Table4.Comparisonofknown-valueIAEATRICinter-recoveryfactorswereabove75%,indicatingthattheTEUcomparisoncellswereperformingaswellasexpected.Therewasalsolaser2H-enrichmentsamples,andenrichedSpike-Proxyandprocessedmethods
usingtheexcellentagreementamongthe3H-enrichmentfactorsdeterminedbythe2H-enrichmentandSpike-Proxymethods,2withnosignificantdifferenceinthemeantritiumenrichmentEnrichmentH-factorsobtainedusingthesemethods(Student3’st-test,sampleTRICKnownvaluemethodSpikemethodN
p=0.388).AsummaryoftheinternationalHinter-comparisontestsampleresultsMean
SDMeanSD2isgiveninTable4.FortheTRICtestsamples,theH-enrichmentandSpike-ProxyTRICT257.517.580.217.500.193methodsbothyieldedaccurateandpreciseoutcomesTRIC4.49comparedwiththeirwell-establishedvalues.Inshort,theTRICT24T234.372.744.512.830.130.092.800.150.1033TRICtestsampleresultsconfirmedthatthelaser-based2H-TRIC1.15enrichmentmethodprovidedafasterandreliablewaytoTRICT221.120.090.580.08obtainaccurate3H-enrichmentfactorsforalltypesofTRICT21T200.431.1900.590.06
0.1230.22
0.06
0.120.22
33
electrolyticenrichmentcellsystems.
CONCLUSIONS
enrichmentparameter,whichwasapplieduniformlytoallthesamplecells,versusthe2HmethodwhereweusedtheTheuseofoff-axisintegratedcavityoutputlaserspectrometryaveragecellconstantasdeterminedabovefortheTEUtoaccuratelyanddirectlymeasureextremely2H-enrichedsystem.ThereportedfinalTUvaluesandtheirpropagatedwatersupto57,000‰(~9000ppmdeuterium)uncertaintieswereobtainedbydataprocessingwiththe2atarateof60samples/daywillfacilitatetheuseofHasatracerinIHLTRIMSsoftware.Encouragingly,itwasobviousfromenvironmentalandhydrologicalapplications.TheincorporationtheresultsinTable3thattheSpike-Proxyandlaser2H-ofthelaser-based,2H-enrichmentmethodintolow-levelenrichmentmethodsbothreturnednearlyidenticalandtritiumoperationscanfacilitatea10–20%increaseinsampleaccurateresultsforthelaboratoryspike(542.1CPM)withinthroughputbyeliminationofreplicatedspikestandards,andtheexpectedmeasurementuncertainty(10%).Forallcellslaboriousgravimetrics,andbyprovidingimmediatefeedbackinthe500mLTEUsystem(except#4),thedeuterium
onthequalityofelectrolyticcellperformance.Additional
RapidCommun.MassSpectrom.2016,30,415–422Copyright©2016JohnWiley&Sons,Ltd.wileyonlinelibrary.com/journal/rcm
421L.I.Wassenaaretal.
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Acknowledgements
ThisresearchwasfundedbytheInternationalAtomicEnergyAgency.WethankD.BrummerandC.Sambandamforassistancewithsampleprocessing.Wethankthereviewersfortheirconstructivecomments.
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