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Beta Particle Radiation Instrumentation and Sources
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NBSMeasurementServices: Calibrationof Beta-ParticleRadiation InstrumentationandSources JohnS.Pruitt ChristopherG.Soares MargareteEhrlich NBS Special Publication 250-21 U.S.DepartmentofCommerce NationalBureauofStandards
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NBSMEASUREMENTSERVICES: CALIBRATIONOFBETA-PARTICLE RADIATIONINSTRUMENTATION ANDSOURCES JohnS.Pruitt ChristopherG.Soares MargareteEhrlich CenterforRadiationResearcli NationalMeasurementLaboratory NationalBureauofStandards...
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LibraryofCongressCatalogCardNumber:88-600514 NationalBureauofStandardsSpecialPublication250-21 Natl.Bur.Stand.(U.S.),Spec.Publ.250-21,75pages(Apr.1988) CODEN:XNBSAV U.S.GOVERNMENTPRINTINGOFFICE WASHINGTON: 1988 Forsaleby...
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PREFACE Thecalibration andrelatedmeasurement servicesoftheNationalBureau ofStandardsareintendedtoassistthemakersandusersofprecision measuringinstruments inachievingthehighestpossiblelevelsof accuracy,quality,andproductiv...
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ABSTRACT InaprojectfundedjointlybytheNationalBureauofStandards(NBS)and theNuclearRegulatoryCommission(NRC),NBShasdeveloped acalibration facilityforbeta-particle instruments andsourcesusedinradiation- protectiondosimetry....
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TABLEOFCONTENTS Page Preface 111 Abstract 1v ListofTables v1 1 ListofFigures viii 1.HistoryandDescription ofService 1 1.1QuantityforReportingCalibrationResults 1 1.2SourcesandInstrumentsAcceptedforCalibration 1 1.3Proced...
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TABLEOFCONTENTS(Continued) Page 4.4SpectralCharacterization byMeansofPulse-Height Distributions. 24 4.5Uncertainty intheCalibration ofBeta-ParticleSourcesand TransferIonizationChambersSubmittedtoNBS 31 5.Characterization...
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LISTOFTABLES Page Table1.Characteristics ofAmersham-Buchler Beta-ParticleSources 4 Table2.TypicalExamplesforCorrectionFactorstoMeasured IonizationCurrents 11 Table3.ValuesofParameters aandBforAirDensityCorrectionFactor 1...
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LISTOFFIGURES Page Figure1.Theoretical Beta-ParticleSpectrafortheRadionuclides Employed 5 Figure2.Beta-Particle CalibrationFacility 6 Figure3.Extrapolation IonizationChamber: CrossSectionthroughthe FrontPortion;Schematic...
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1.HistoryandDescription ofService Between1982and1985,theNationalBureauofStandards(NBS),with partialsupportfromtheU.S.NuclearRegulatoryCommission,developed a facilitysuitedtoestablish aserviceforcalibratingcertainuser-own...
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905r+90Yand204y]sources isreportedas3percent,thatfor^'^^Pmsourcesas 5percent,andthatforthin-window parallei-plateionizationchambersas 3percentwhencalibratedwiththe^°Sr+^^Yand 204-|-] sourcesand5percent whencalibratedwith...
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(2)anextrapolation ionizationchambersuitedforthedetermination of absorbed-dose ratestowateratdistancesfromthebeta-particle sourcesappropriate forthestudyofradiation-protection instruments; (3)arugged(althoughthin-walled)...
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Table1.Characteristics ofAmersham-Buchler Beta-Particle Sources (a)SourceStructureandActivity Radionuclide HalfLife Structure Source NominalActivity rlDt) ^ \\Kj 1 j ,UdLc 90sr+90Y 28.5y ^"^Srcarbonate 50mg/cm^Ag 1850(50...
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Beta-Particle Energy,MeV Figure1.Theoretical Beta-Particle SpectrafortheRadionuclides Employed [2],PlottedisthenumberofbetaparticlesperMeVforonetransition fromtheoriginalstate,againstbeta-particle energyinMeV, 5
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Figure2.Beta-Particle CalibrationFacility. Thesource-support standis shownattheright,theextrapolation ionizationchamberattheleft,anda beamflatteningfiltersupportedbywiresin-between. Thepicturedflattening filterisforthe^'...
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enoughtosimulate aphantomofinfinitesize. Theplateseparation ofthe ionizationchamberisvariableandcanbeaccuratelydeterminedbymeansofa micrometermeasurement (seescrewonendofchamberatleft). Thethin entrancewindowforthebetapa...
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PMMA Brass Aluminum Graphite-Coated PTPFoi Electrodes: Collecting HighVoltage Guard Fig.3.Extrapolation IonizationChamber: CrossSectionthroughtheFront Portion;SchematicRepresentation. Thecollectingandguardelectrodes(grap...
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Figure4showstheresultsofcurrentmeasurements asafunctionofplate separationwiththethreetypesofsources,afterapplication ofcertain corrections. Thesecorrections areintroduced ineq.(1)below,andare subsequentlydiscussed indeta...
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< 20 LJ q: o IA 1 111 UJ 10 < o UJ h- O LlI (T CC 0o o PLATESEPARATION,mm Fig.4.CurrentMeasurements intheExtrapolation IonizationChamberasa FunctionofNominalElectrode-Plate Separation(MicrometerReadingof ChamberDepth). T...
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Table2,TypicalExamplesforCorrectionFactorstoMeasuredIonization Currents(fromDataBooks863and868) ValueofCorrectionFactorfor SymbolCorrectiontoReferenceConditions 2oni 90sr+90Y A.ChamberCorrectionFactors ^foil entrancefoil...
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(c) ^atten' correctionforattenuation inthechamberairgap,was determinedbymeasuringchambercurrentasafunctionofdistanceybetween sourceandchamberusingafixedairgapd=0.5mm. Itwasfoundthat,after multiplyingthecurrent Ibythesqua...
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(g)^recom' correctionforionrecombination anddiffusion intheair insidethechamber, isusuallyquitesmallforprotection-level measurements. Itonlybecomesappreciable forlargeioncurrentsand/orsmallvoltages. It wascalculatedbymea...
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correctionfactor(seecorrection (d)),andaandBareconstants. Table3 showsempiricalvaluesforaand3forallthreetypesofsources,withthe beamsattenuatedbyselectedthicknesses ofPTP.Thesecorrectionswere checkedbyactualmeasurements o...
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whereW/e—energyrequiredtoproduceanionpairinair,injoulesper coulomb ; ^air^"" "'^^^''O*averagemassstoppingpowerofwatertothatofdryair, dimensionless ; pQ —densityofdryairatreferenceambientconditions (22°Cand 101.325kPa),in...
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-> 1 in <- 14.5mm 1o 13mm t 1 1 Fig.5.DesignofPTWPara1lei-PlateTransferIonizationChamber. Witha potentialof100Vacrossthechamber,absorbed-dose ratestowaterfrom roughly0.3toover30mGy/h(0.5toover50mrad/min)canbemeasured. Du...
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2.5.2PrincipleofUse Formeasurements, thefrontsurfaceofthechamberisplacedinthe calibrationplane,afterremovaloftheextrapolation chamber. Ionization currentismeasuredwithanelectrometer. Thecalibrationfactorofthe transfercha...
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Operationofthefacility isdescribed insomedetailinthesubsequent partsofsection3.Forgeneralsafetyprecautions intheoperation of electronaccelerators seethepertinentliteraturelistedinsection11,which isonfileintheofficeoftheD...
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Figure6.Monoenergetic ElectronBeam-Handling Arrangement. 19
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rates(lessthan2/s). Whenonlyonemonitorwasused,themagnitudeofbeam wanderingandfluctuations inbeamintensitywerelargeenoughtolimit dosimetryreproducibility toabout15percentwhenthebeamwasturnedoff betweenindividualmeasuremen...
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usedwerethosedescribed indetailinsection2.4.3. Theresultsareshown intable4.Sincethesourceshadbeeninitiallycalibrated atthePTB,it waspossibletocomparetheNBScalibrations withthoseobtainedatthePTBin asimilargeometryatthesam...
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4.2.1DependenceofDoseRateonOff-AxisShiftofDetector Forthisstudy,thedetectorwasmovedhorizontallywithinthecalibra- tionplanesoastocovertheentirebeamcrosssection. Typicalresultsare showninfigure7.Alongthehorizontal linepass...
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10 -5 0 5 10 DISTANCEFROMBEAMAXIS,cm 15 Fig.7.DegreeofNon-UniformityofDoseRatealongaHorizontal Linethrough theReferencePoint,Perpendicular totheBeamAxis.Reference distance: 30cmfor^osr+soy and20kji^20cmfor^'^'^Pm, -2-101...
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4.3SpectralCharacterization byMeansofMeasurements asaFunctionofDepth inPlastic Measurements weremadeofionizationcurrentintheextrapolation ioniza- tionchancerasafunctionofthickness ofpolyethyleneterephthalate (PTP) addedt...
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Figure9.IonizationCurrentasaFunctionofDepthinPTP. 25
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0 800 1600 ^2400 DEPTHINPOLYSTYRENE,mg/cm^ Figure10.Attenuation CurveinPolystyrene forthe2-mCi^osr+soySource. 26
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ENERGY.HaV Figure11. top:SpectrumofI'+^'PmSource,UsedwithFlatteningFilter. Distance: 20cm.Detectoruncol1imated, bottom: Spectrumof 20i+j-i source.UsedwithFlatteningFilter, ShowingInfluenceofLeadCollimatorwithCircular Ape...
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1000 distance: 30cm aperture: 1.6nm ENERGY. lleV ENERGY.HcV Figure12.Spectrumof^Osp+soy Sources,ShowingInfluenceofFlattening FilterandofDetectorCollimator. Thetheoretical spectrumof isshown forcomparison, 28
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_ ;jidistance:50cm ENEKGY,HeV Figure13.Spectrumof^Osr+soySourcesUsedwithoutFlatteningFilter, ShowingInfluenceofSource-to-Detector Distance. Detectorcollimatorwith circularaperture,1.6-mmindiameter. 29
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UJ z z < X o a: UJ Q. CO 3 o o 10' z— r—r~n— r— i— i— i— -r— i — -]— i — t— \— r — r 0.98MeV 10^ 10' 1— \— r T— I— I— I— r /1.05MeV JL«J I I I I I L ' ' ' ' ' L 111 ,J L 1.0 2.0 ELECTRONENERGY,MeV Figure14.EnergyCalibrat...
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(b)Influenceofsource-to-detector distancefor^QSr+^Qy .Figure13 showsthespectraldistributions atthethreedistancesspecifiedbythe sourcemanufacturer. Theeffectofdistance isseentoberelativelysmall. Therefore, achangeindistan...
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Figure15.EffectofAddedPolystyreneAbsorbersonsosr+^oy Spectrum. Detectorcollimatorwithcircularaperture,1.6mmindiameter. 32
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Theestimatesofeachtypearecombinedinquadrature, andthenthetwo resultsarecombinedinquadraturetogiveacombineduncertainty. The confineduncertainty inturnismultipliedbytwo(orthree),togivean overalluncertainty. Table5givesabre...
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Table5.Uncertainties intheDetermination ofAbsorbed-Dose RatetoWater fromMeasurements withtheExtrapolation IonizationChamber Parameter SyrTt)ol PercentUncertainty ype A' 204T190Sr+90Y Type b'^ 90Sr+90Yi'^'Pm A.CorrectedIo...
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Table6.Uncertainty intheCalibration ofBeta-Particle Sourcesand TransferIonizationChambersSubmittedtoNBS A.SourceCalibration PercentUncertainty ^ Parameter TypeA'* Type 20'*T1 i-7pm2oni90Sr+90Y 90sr+90Y Positioningofextra...
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1 I 1 1 1 cm 1 1 1 n r> r> i 1 1 \— 1// e - \ // " o 1// o ca // «» nee '/yi. " 1/X^o «* '//O o // 1- o 1/1 5 // ^ — — c c // p o 1 o j o o f ' 1 c 1 ^ 1 _ V 1 - €> - O \ \ «< ^ o o CM I8\ 1 1 1 1 1 1 I 1 1 i\ \I'll o on...
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showninthelastcolumnofthetablecorrespondtoamonitorcountingrateof 10^persecond. Atthetimeofwriting(February1988),representative values forRandforminimumabsorbed-dose levelsarebeingobtainedforthenew monitorsystem. Noassess...
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13NNVH3U3dSlNnOO >- o a: UJ z lU z o a t- o 13NNVH3U3dSINHOO 13NNVHD«3dSlNflOD O toS a;o <U-r- c5 O4-> •f— jcX. t—<u i\ r i cc L. <U£_ <4-O +-> •r-O OOJ •-J •r--O «/>c cOJ O0) t-2 +->(-> O OJJ3 r— UJo; a >c ^+j 1iA O-i-...
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0.09mm ALUMINUM uj9000 - z z < I o lU a. 0 0.5 1.0 1.5 ELECTRONENERGY.MeV 0.09mm ELECTRONENERGY.MeV Figure18.Degradation ofNominal1.5-MeVand2.5-MeVElectrons inDifferent Thicknesses ofAluminumAddedtothe0.09-mmAluminumExit...
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gure19.Degradation inAirofNominal200-keVto2.5-MeVElectronsin DifferentThicknesses ofInterveningAirLayers. 40
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6.ExamplesofPracticalStudiesPerformedwiththeBeta-Particle Beams 6.1Compatibility ofDifferent ^OSr-t-^OySourceswithExistingStandards Sincespectralcharacteristics of^Osr+^Oybeta-particle sourcesmayvary widelywithsourcegeom...
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CO o 13 o >- o O 0) o o o CO C- «J o. E o o no CO c o O Q. 00 O) (J Q. E O o CM o O o O 00 O CO 00 CO CO o o o CTiO Or-I AV o o O V o o o o (T3 U o o o 00 A CO 00 00 O) o o 4-> O CM A I — C7) <c o c: O O •• AV o o o o O...
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Figure20.lonization-versus-Depth CurvesforThreeDifferenttypesof 90sr+90YSources. Solidline:Buchler-Amersham source;dashedline: Amershamexperimental source;dash-dotted line:specialhigh-activity source usedbytheNVLAPTestin...
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Electronenergy,mcv Figure21.ComparisonofSpectrumoftheBuchler-AmershamandtheNVLAP TestingLaboratory's ^Osr+^oySources,onSemi-Logarithmic Scale. The ordinateswereadjustedforequaltotalnumberofcounts. 44
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10^ ELECTRONENERGY,MeV Figure22.ComparisonofSpectrumoftheAmershamExperimental andtheNVLAP TestingLabortory's^osp+soySources,onSemi-LogarithmicScale. The ordinateswereadjustedforequaltotalnumberofcounts. 45
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Figure23.Comparison ofSpectrumofAmershamExperimental ^^Sr+^^YSource, BareandShielded. Adding82mg/cm^ofaluminumtotheAmershamexperi- mentalsourcemakesitsspectrumsimilartothatoftheBuchler-Amersham source(fig.21). 46
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(b)thattheDOEcriterion istooloose,sinceitdoesnotdiscriminate betweentheoperationally verydifferentNVLAPandAmershamexperimental sources,whiletheISOcriteriondoes. Thehighbackgroundnoiseshownin figure20fortheexperimental Am...
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largewith350-keVelectronsaswith^^'^Csgammaradiation. "Response"here isdefinedasscalereading(indication) oftheinstrumentdividedby absorbed-dose rate. 7.3RoleofNearlyMonoenergeticElectronSourcesintheDevelopment ofaNew Gene...
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Theradiationhazardisonlymoderateforsourceswiththeactivitylevel thatwillbecalibrated inthefacilityinquestion,sinceevenadirect exposureoftheskinforabrieftimewouldnotbeserious,withthepossible exceptionoftheeyes.Howeverdirec...
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9.References [1]Mantel,J.Thebetarayspectrumandtheaveragebetaenergyofseveral isotopesofinterest inmedicineandbiology. Int.J.Appl.Radiat, Isotopes. 23,407-413(1972). [2]Cross,W.G.;Ing,H.;Freedman, N.Ashortatlasofbeta-raysp...
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[14]AmericanNationalStandardfordosimetry—personneldosimetry performance—criteriafortesting. Am.Nat.StandardsInstituteANSI N13.11-1983. [15]Referencebetaradiations forcalibratingdosimetersanddose-ratemeters andfordetermin...
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Appendices Appendix 1.SampleofCalibrationReportForm(Seesec.1.3) DG8751/87 O.S.DEPARTMENTOFCOMMERCE Page 1of2 DB873/170 NATIONALBUREAUOFSTANDARDS TEN240032 GAITHERSBURG ,MD20899 1987Sep14 REPORTOFTEST 0.5mCi204 Beta-Parti...
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Appendix 1,continued DG8751/87 Page2of2 1987Sep14 temperatureandpressureof22°Cand101.325kPa(1standardatmosphere). Iftheairdensitydifferssignificantly fromthedensityatthereference temperatureandpressure,itmaybenecessaryto...
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Appendix 2.ReportofaTriptoaDOELaboratorybyJ .S.Pruitt ThecalibrationatthislaboratoryoftheBuchler ^Pmsourceis consideredimportantbecauseitsresultsprovideatestofthevalidityof therecentlydevelopedhigh-altitude air-densityco...
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Appendix 2,continued Page2of4 where0.05848and-0.06168areaveragedDVMreadingsforoppositechamberpotential polarities, 0.9987istheDVMcalibration factor,100.17x10"^^ isthecapacitance of the100-pFcapacitor infarads,and50isthei...
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Appendix 2 ,continued Page3of4 wheredistheair-gapsettinginmillimeters and±HVisthechamberpotential in volts. ThelistedvaluesofIwerefittedtoaleast-squares straightlineasafunctionof airgapsetting, d,andtheslopeofthislinewas...
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Appendix 2,continued Page4of4 d,mm 2.5 1.5 0.5 ±HV Q- I; 25 0.02477 -0.02601 0.9964 1,0048 1.0025 1.0125 15 0.01339 -0.01603 0.9963 1.0029 1.0038 1.0131 5 0.00524 -0.00580 0.9960 1.0010 1.0107 1.0139 I,fA 5.166 2.992 1.1...
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Appendix 3 . MeasurementAssuranceStudyby.MeansofPTWTransfer IonizationChamber,Model20A7"'' (Seesection6.2) DG8555/86 DB868/107 TFN236381 1986JUN19 Page1of2 U.S.DEPARTMENTOFCOMMERCE NATIONALBUREAUOFSTANDARDS GAITHERSBURG...
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Appendix3,continued DG8555/86 1986JUN19 Page2of2 Eachchambercalibration (inGy//iC)istheratioofatissuedoserate(in y.Gy/s)andacorrectedcurrent(inpA) .Thereportedresultsarelisted belowinGy/nC: CalibrationFactor absolute rat...
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Appendix 4.PredictingBeta-ParticleResponseofInstrumentsfromtheir ResponsetoNearlyMonoenergetic Electrons(Seesec.7.1.) KadialionHroteciiimOosimclry Vol14No2pp 1IA-I15(I'«6) NuclearTechnologyPublishing PREDICTINGBETAPARTIC...
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Appendix 4,continued ( .aSi internalalgorithmsforderivingabsorbeddosefrom themeasuredpulse-heightspectra. DISCUSSIONOFEXPERIMENTSAND RESULTS Accelerator-produced, nearly monoenergetic electronbeamswereusedtomeasuretheres...
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Appendix4,continued I'RIDHTINdlihIAI'ARIICl.HHISI'ONSi: REKERENCTS 1.Ehrlich,M.,Pruill, J.S.andSoares,C.G.StandardBeta-ParticleandMonoenergelic F.lectronSourcesforihi- Calihraiionoflieia-Radiation Protection Instrumentat...
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Appendix 5.RoleofNearlyMonoenergetic ElectronSourcesintheDevelopment ofaNewGenerationofSurveyMeters: ExcerptsfromtwoPublications NUREG/CP-0050 Proceedingsofthe InternationalBetaDosimetry Symposium HeldatWashington,D.C. F...
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Appendix 5,continued LOSALAMOSPORTABLEBETA-RAYSPECTROMETER B.H.Erkkila, R.J.Brake,andD.A.Waechter LosAlamosNationalLaboratory, LobAlamos,NM87545 *ThisworkwasperformedundertheauspicesoftheU.S.DepartmentofEnergy Abstract:...
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Appendix 5,continued NUREQ/CR-4a« EOG-244* OtotributtonCatagonr:AN FIELDTESTSOFAPORTABLETISSUEEQUIVALENT SURVEYMETERFORMONITORINGMIXED BETA/GAMMARADIATIONFIELDS D.E.Martz B.L.Rich L.O.Johnson S.H.Daniel. Ill PublishedMay...
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11.ListofPertinentTablesandReportsonFileintheOfficeoftheDosimetry Group 11.1PertainingtotheCorrectionsLeadingfromIonizationMeasurementswith TheExtrapolation IonizationChambertoAbsorbedDoseRatetoWater Berger,M,J.andSeltze...
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NBS-IMA(REV.2-ao) U.S.DEPT.OFCOMM. mmmi^DADLIIORATA BIBLIOGRAPHICDATA SHEET(Seeinstructions) 1.PUBLICATIONOR REPORTNO. NBS/SP-250/21 2.PerformingOrgan.ReportNo.3.PublicationDate April 1988 4.TITLEANDSUBTITLE NBSMeasureme...
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.1
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U.S.DepartmentofCommerce NationalBureauofStandards Gaithersburg,MD20899 OfficialBusiness PenaltyforPrivateUse$300 StimulatingAmerica'sProgress 1913-1988
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