Resource Library · SP 250
Leak Calibration Service
Inside this document
Every page is full-text indexed — open a page directly in the PDF viewer.
Page 1
NISTMeasurementServices: . . T . ^^^^^^^^^^^^^^^^^^^^^^^^^^ ResearchInformationCenter NationalInstituteofStandards andTechnology Gaitbersburg,Maryland203*) NISTLeakCalibration Service CharlesD.EhrlichandStuartA.Tison U.S...
Open at page →
Page 3
NiSTMEASUREMENTSERVICES: NISTLeakCalibrationService CharlesD.EhrlichandStuartA.Tison Thermophysics Division ChemicalScienceandTechnologyLaboratory NationalInstituteofStandardsandTechnology Gaithersburg,MD20899 January199...
Open at page →
Page 4
NationalInstituteofStandardsandTechnologySpecialPublication250-38 Natl.Inst.Stand.Technol.Spec.Publ.250-38,89pages(Jan.1992) CODEN:NSPUE2 U.S.GOVERNMENTPRINTINGOFFICE WASHINGTON: 1992 ForsalebytheSuperintendent ofDocumen...
Open at page →
Page 5
PREFACE Calibrations andrelatedmeasurement services oftheNational InstituteofStandardsandTechnologyprovidethemeansformakers andusersofmeasuringtoolstoachievelevelsofmeasurement accuracythatarenecessarytoattainquality,pro...
Open at page →
Page 6
ServicesUsersGuide1989,pages49to51.Inquiriesconcerning thecontentsofthesedocumentsmaybedirectedtotheauthor(s)or tooneofthetechnicalcontactpersonsidentifiedintheUsers Guide. Suggestionsforimprovingtheeffectiveness andusef...
Open at page →
Page 7
TABLEOFCONTENTS Page Preface iii 1.Introduction 1 2.DescriptionoftheNISTLeakCalibrationService 2 3.DesignPhilosophyandTheory 3 DesignPhilosophy: Introduction 3 DesignPhilosophy:NISTPrimaryLeakStandard 3 FlowintoUpperCham...
Open at page →
Page 8
TABLEOFCONTENTS(CONTINUED) Page 6.QualityControl 30 ControlCharts 30 Closed-Reservoir HeliumPermeationLeaks 30 Upper-to-Lower ChamberFlowRatio 31 ComparisonofPrimaryStandards 31 FlowmeterIntercomparisons 31 DomesticInter...
Open at page →
Page 9
LISTOFTABLES Page 1 1. ConversionofUnitsforUniversalbasLionscant\&) 4 2. BellowsFlowmeterUncertainties 21 3. SummaryofUncertainties forFlowintotheUpperChamber 25 4. SummaryofUncertainties forFlowintotheLowerChamber 27 A-...
Open at page →
Page 10
LISTOFFIGURES Page 1. SimpleSchematicoftheNISTPrimaryLeakStandard 40 2. SchematicoftheNISTPrimaryLeakStandard 41 3. ValvingSequenceforLeakCalibrationThroughUpperChamber 42 4. ValvingSequenceforLeakCalibrationThroughLower...
Open at page →
Page 11
1 .INTRODUCTION Theindustrialneedfordemonstratedaccuracyoflow-rangegasflowrateor leakratemeasurements usedtocalibrate leakdetectorsandgasanalyzers, traceabletoarecognizedstandardsauthority,promptedtheNationalInstitute of...
Open at page →
Page 12
2.DESCRIPTIONOFTHENISTLEAKCALIBRATIONSERVICE TheThermophysics Division oftheNational Institute ofStandards and Technology provides aCalibration Service* forheliumpermeation leak artifactsintherange 10" 8 to 10"11 mol/s(2...
Open at page →
Page 13
3.DESIGNPHILOSOPHYANDTHEORY DESIGNPHILOSOPHY: INTRODUCTION ThePrimaryLeakStandard thathasbeendeveloped atNIST isshown schematically infigure 1.Thistypeofapparatuswaschosenoverseveral alternatives becauseitbenefitsfromcon...
Open at page →
Page 14
FlowintoUpperChamber AfterStep 2ofthecalibration process thesystem isallowedtimeto equilibrate, atwhichpointthevalvingintheflowmeterisconfiguredandthe flowmeterelectronicsareactivatedsothattheflowrateofthegasemanating fr...
Open at page →
Page 15
(]?U1 -P L1 ) .C ol Ni=N oi = (2) R •T o1 whereP L1 isthepressureinthelowerchamber.Butthismustalsoequalthe flowrateofgasthroughthepump,whichfromeq(B12)is N sl = *L1 ' S l R•T o1 (3) EquatingNjwithN s x thengives Pui=P L...
Open at page →
Page 16
Whencomparingeq(8)andthecorresponding parameters ineq(1),notethat P r 3 replacesP w3 andthatAV/AtreplacesdV/dt. Thisisduetothefactthat intheflowmeter, itisthereference volumepressure (P r )andnotthe workingvolumepressure...
Open at page →
Page 17
equalto 1fortheslightvariations inroomtemperature, itisroutinely retainedinthedataanalysisroutine. Adifferenceof1°Cinthechamber temperature resultsinacorrection factorof1.002ineq(10). Further discussionconcerningsourceso...
Open at page →
Page 18
FromStep1,conservation offlowrate(N x )attheflowmeter, orificeand pumpgives : Pli 'S i N x = (11) and Si Pui=Pli ' ( 1+ ) • (12) Col InStep2,underequilibriumconditions, therecanbenonetflowacrossthe orifice,sothat P U2=P...
Open at page →
Page 19
P r2 .(AV/At) 2 •T rl <Rl/u>» = <16 > P rl •(AV/At), •T r2 wherethesubscript"m"referstothemeasuredquantity. Substituting eq(16) intoeq(15)andsolvingfor(R L/u)t (referencedtoS x andT Qx )gives: P r2 •(AV/At) 2 •T rl P ux...
Open at page →
Page 20
FlowintoLowerChamber Withtheupper-to-lowerchamberflowrationowdetermined, itispossibleto usethetechniqueshowninfigure4tomeasureflowratesbelow10"12 mol/s withtheflowmeter,ortomeasurehigherflowrateswithsmalleruncertainties...
Open at page →
Page 21
. . P U3 * S 3 *T ol S l N 3 /N L = • (1+ ). (25) P U1 *S l 'T o3 C ol Fromthediscussion intheprevioussection,thelastfactorontherightin eq(25), 1 4-S 1 /C ol ,isthetheoretical flowrateratio(R L/U)t forpump speed S x ando...
Open at page →
Page 22
leakorstandardleak,orbothleaks,canbevalvedintotheleakdetector. Whengasfromaleakisnotroutedtotheleakdetector,thenitisroutedto theturbopump,sothatbothleaksarecontinuously pumped. Theunknownleak isencased inatemperature-con...
Open at page →
Page 23
andeq(30)intheform a [L(T)/LJ -1 (T -T Q) (31) B= T •T, (T-T D) Jin L(T) •T (32) Notethatinbotheqs(31)and(32)theratio(L(T)/L Q)appears,andnotL Q alone,sothatitisnotnecessarytoknowtheabsolutemagnitudeoftheleak rate,butonl...
Open at page →
Page 24
4.DESCRIPTIONOFSYSTEMANDOPERATIONALPROCEDURES PRIMARYLEAKSTANDARDSYSTEMDESCRIPTION TheNISTPrimaryLeakStandard(PLS)iscomposedofthreemaincomponents; themainvacuumchamber, theleakmanifold,andaflowmeter. ThePLSmaybe usedwith...
Open at page →
Page 25
pressuresrangingfrom 1x 10" 4 to 1x10" 8 Pa. Thisrequiresthatthe turbomolecular pumphavethecapacityandstabilityoverthecorresponding flowratestoachievepumpingspeedstabilities oflessthan0.1%perhour. Itisalsonecessarythatth...
Open at page →
Page 26
closingvalveL30andopeningvalveL24iftheunknownleakisinstalledon portPi.ThegasthenflowsthroughvalvesL21andL36andenterstheupper chamberofthemainvacuumsystem,andisultimatelyevacuatedthroughthe orificeintoaturbomolecular pump...
Open at page →
Page 27
Theflowfromtheflowmeterismeasuredinthefollowingmanner. The 1Torr differential CDG(D5)iszeroedandthevariableandreservoirvolumesare isolatedbyclosingvalvesBlandB2 .Thepistonisthensetinmotionby pushingtheenablebuttonontheco...
Open at page →
Page 28
TheLCScontrolsystemusesanIBM-compatible computertocontrolthedata acquisition andanalysis ofthedata. Itsmainfunctions include the following:controlofthetemperaturebathtowithin0.02°Cofthesetpoint temperature, controlofthev...
Open at page →
Page 29
zerodrifts. Thisprocessisrepeatedforthedatapointsateachtemperature inthedatacollectionsequence. Attheconclusionofthedataacquisition theprogramperformsaleastsquarefittothedatausingthefunctionalform ofeq(33)insection 3.The...
Open at page →
Page 30
5.ASSESSMENTOFUNCERTAINTIES PRIMARYLEAKSTANDARD Flowmeters Thefundamentalequationsrelatingthemeasuredleakagerateofaleak(ata giventemperature) tothemeasuredparameters ofthePrimaryLeakStandard werederivedinsection 3(eqs(10...
Open at page →
Page 31
LO CO LU 1 — CO LU LJ 21 ZD C CD CO CD QQ <3 < O -4— > 1 II CD 1 1 --r-1m O0 1 1X1 --r-| 0 inO 1 COLOrn OOOO0O cnO en -«— 1 -r-l 1 1 0 •f— 1 1 j 1 --r-1m 1— 1 CVJ -r-lOO0 -i-t00 **sT CVJOOJ -= «-— 1 inOO0O cnO 0 --r-l -r...
Open at page →
Page 32
Table 2givesestimateduncertainties oftheindividual termsforthe "bellows"flowmeterforflowrateswhicharelower(10" 12 mol/s)thanthose presented inAppendix Dforthe"piston" flowmeter. Thisinformation is presentedgraphicallyinf...
Open at page →
Page 33
courseofaworkday,particularly intheafternoon,werenotuncommon, sothat corrections certainlyneededtobetakenintoaccount. Theassumption thatthepumpingspeed isdirectlyproportional tothe rotational frequency isdifficult toveri...
Open at page →
Page 34
foundtodependstronglyontheparticularoperatingrangeofthequadrupole instruments, andatthelowestpressures (10~ 7 Paandbelow),correctingfor thedifferential hydrogenoutgassing rendered thetotalpressure gageof marginaluse. Itw...
Open at page →
Page 35
discussanoveralluncertaintyassociatedwithanindividualmeasurement of flowratebyflowintotheupperchamber. Theequationwhichdescribesthis flowrateisreproducedhereforconvenience: P r3 (AV/At) Pul To 3 Si C o3 +S 3 R •T r3 _ P...
Open at page →
Page 36
flowratioiseq(17).Aslightlymodifiedform(thereciprocalvalue)is: P rl •(AV/At) 1 •T r2 P U2 •S 2 •T 0l (R u/L)t(Si,Tol )= — • . (17a) P r2 •(AV/At) 2 •Tr x P 01 •S x •T o2 Thefirstsetoffactorsinvolvingtheflowmeter isagaina...
Open at page →
Page 37
whichcontainselementssimilartothoseinbothofthesectionsabove. The uncertainties associatedwiththeparticularfactorsareagainafunctionof theflowrateoftheflowmeterandaresummarizedintable4. TABLE4.SummaryofUncertainties forFlo...
Open at page →
Page 38
reportispresentedinAppendixE. LEAKCOMPARATORSYSTEM Asdiscussed earlier, theexponential temperature coefficient ofhelium permeationleaksisdeterminedusingtheLeakComparatorSystem(LCS) .This isdonebyfittingtherelativeleakrat...
Open at page →
Page 39
Thisuncertainty inBmustthenbetranslated intoanuncertainty inleak rate,whichisexpressed asanadditionaluncertainty per°Cawayfromthe 23°Creferencetemperatureatwhichtheleakwasmeasuredontheprimaryleak standard. Rewritingeq(30...
Open at page →
Page 40
6.QUALITYCONTROL Oncetheoperatingcharacteristics anduncertainties ofaprimarystandard havebeenestablished, subsequent useoftheprimarystandardatthesame levelofuncertaintyrequiresperiodicverification toensurethatnoneofthe u...
Open at page →
Page 41
Asanexample,foraleakrateof 10" 9 mol/s,afillpressureof145psi(1 MPa) ,andareservoirvolumeof200cm 3 ,thetimeconstant risapproximately 3yr(1yr=3.1536xl0 7 sec). In1yr,theleakratewillhavedecayedby(1- e" 1/3 ),or28%. Mostleak...
Open at page →
Page 42
frombothflowmeterscombined. TheNISTserialnumberfortheleakusedata givenflowrateisindicatedalongthetopaxisofthefigure. Themeasured randomuncertainties areseentoslightlyincreasewithdecreasingflowrate. Figure18presentsthedif...
Open at page →
Page 43
International Intercomparisons Whiletherehavenotbeenanyinternational roundrobinsforNISTto participate insincetheleakprogrambeganin1984,aroundrobinsponsored bytheCommissionoftheEuropeanCommunities, CommunityBureauofRefere...
Open at page →
Page 44
7.FUTURE Thereareseveralareasinwhichtoconcentrate futureresearchactivities associated withtheNISTLeakCalibration Service. First, there is considerable industryinterest inhavingNISTextendthelowerendofthe serviceatleastano...
Open at page →
Page 45
servicecanbeperformedonthenewLCS. Thiswillmaketheprocessmore efficientinseveralways,reducingthecostpercalibration ofanindividual leak. 8.ACKNOWLEDGMENTS Theauthorswouldliketoacknowledge themajorcontributions ofDrs .K.E....
Open at page →
Page 47
9.REFERENCES [1] S.Dittmann, "HighVacuumStandardandItsUse,"U.S.Government PrintingOffice,NISTSpecialPublication250-34 .31(1989) [2]R.W.Hyland,CD.Ehrlich, C.R.TilfordandS.Thornberg, "Transfer LeakStudiesandComparisons ofP...
Open at page →
Page 48
[15]J.H.DymondandE.B.Smith,"TheVirialCoefficients ofGases,"Oxford UniversityPress,copyright1969 [16]J.F.O'Hanlon, "AUser'sGuidetoVacuumTechnology," J.Wiley&Sons, copyright1980 38
Open at page →
Page 49
10.BIBLIOGRAPHY Inadditiontothereferencescitedabove,theinterestedreadermaywishto consultthefollowing. Units : "Standardization andTemperatureCorrectionofCalibratedLeaks,"CM. Soloman,J.Vac.Sci.Technol.A4,327(1986) Leaks :...
Open at page →
Page 50
Flowmeter Nfm Vacuum Chamber Upper Chamber P,T Lower Chamber Turbo Pump LeakManifold Leak ,Partial Lj—UrrPressureGage Orifice Figure 1. SchematicdrawingoftheNISTPrimaryLeakStandard,showingthe majorcomponents. Thepressure...
Open at page →
Page 51
41
Open at page →
Page 52
LEAKCALIBRATIONTHROUGHUPPERCHAMBER Z5£ 35 Step3 Tch3 38= O Pu3 Turbo S3 Unknown Leak Figure3.Valvingsequenceformeasuringleakrateofunknownleakbyflowing gasfromflowmeterintotheupperchamberofthemainvacuumchamber. 42
Open at page →
Page 53
LEAKCALIBRATIONTHROUGHLOWERCHAMBER 331 Figure4.Valvingsequenceformeasuringleakrateofunknownleakbyflowing gasfromflowmeterintothelowerchamberofthemainvacuumchamber. 43
Open at page →
Page 54
Figure5.Valvingsequenceformeasuringflowrateratio. 44
Open at page →
Page 55
LeakComparator Ballasto Gas Cylinder I.G. S^Jv9 SV8 rv s = L* a I I r SV6 Computer Control System ~jTemperature Control System I L_ S.V. 6-9 1 Electrometer l: LeakDetector Figure6.SchematicdiagramoftheLeakComparatorSyste...
Open at page →
Page 56
o 0 Q 0 —9 co 0 Q. E _^ CO 0 O 6 a; w 00 5g * ?o <u e C og*t a) ^ a) $ uo 4J*d •HC 64-1 <u o ex ^ rn 2! •X3 ,0 Q)O o^a. Q 2s c I-.o 4-> 4J l-i P <uw 9}Bfc|>|B9-|p9ZI|BLUJ0N 363 bO 5-1-) 46
Open at page →
Page 57
H CC < LU DC O I- o LU LU Q < LU c<J<U o B O CD u-o m co o 0) CD 4-)t3 nj a cd cd •p o cd <u 4J (0 w }-l > B 0) •u ca !S C/5 >-l O 4-> ctl U cd C- a)B 4Jo cOu 5-1 ^ cd cd a) cuJ CD Jj S-l « CD B 0) w id 4-1 o oo _i«h a)...
Open at page →
Page 58
48
Open at page →
Page 59
CC Lil h- LU o o 111 CO o •u c l o 03 4J 4J 03 bO C •i-i o w S-i 0) 4) fa 5 ow <uo 4J C «w * °T3 eto o3 -O Hc bO cfl 034J •HW bO o3 > 03 > o3 E •-I O * *" 'H on 0)M 5-1S d b00) fa4J 49
Open at page →
Page 60
m is </) JSC <u c "<5 0) "3 §i co i- E z <a <o .2oc «s c CO~ 0>>« hWDC 1 I i ccc ooo *« </) </>jo EEd ! i I i I oo I I o T- I CM O o d q T— I q cvi I (A o £, CD (0 DC O LL o 5 o O H 0) 4-> 0) o —i fa o 05 CO 4-> c P-i 0)...
Open at page →
Page 61
(0 c (0 4> (0 0) >* £ Q. H CO ca) <5 "5 rE a>> go 3LL k. (/) 23 0)o is E_ 3 | 1 E (02 0>>« hwoc 1 I I (/)(/></) 533 ooo "5> "a>"a> 00OQ00 OOO I I o I ao I I o £ <D OC 3 o LL O o CM q I e MO a)"d i u O4J r 13 CD CP <d ,c...
Open at page →
Page 62
<£ _CD 1_ f— CD 2o CMin <£ _1CCZ) CC_l CM <N -JP CD w or cc XCMg o„ is I LU I- o o LJJ CC LU LL LU CC SJm m — eg« - St _ <o 9 a am <D cm CM - <o - • _ m <x• 1 1 1 1 CM CM C\J CNJ C\J CM T— LU LU LU LU LU LJJ LO CO CD C\J...
Open at page →
Page 63
o u to o 4-1 4-> O (4-1 CD cO ,c o 5-1 CD a, a- o o o 4-1 •U u cO o 0 y u eg Cc O cO u^ w .CO ^3 OjieyeiBymoijjeddno;j9mct| Q)U U CO de U)T-l •r-l J-l 53
Open at page →
Page 64
%AjUB9UnWOJJ.SUOI^IAeQP9ZI|BLUJ0N 54
Open at page →
Page 65
CO a> c o To £ <5 a. I- (0 ./ c a> E © HI ca o -j (0 (0 o I!s© ©</> Xa> w= 4-> • CD E cfl a> o CD 1$ <u Q)o iH* (4-1 CD j3 CD 4 ° cfl4J nintn wS cfl (DO CD p—I•— I t— I (3HM H cfl 4-> a) toCM 4->CD <U.H W>B 4-> cO tO—1 C...
Open at page →
Page 66
I CO c 05 03 O (0 £ a! 0) ^c <o.2 <D I5 0)c oo cO ll (TJ 3 oO £'= CO> CtJi_ CDO co _1 CO CD CM _J CO OQ z CO 03 « c/> 0) O) CO O < <D Q) E 5 (0o TO LL Q 5 CD <Z CO O — CD 0) E 5 o 2 O O co c° O• >z c o CD 3 z coom t-cm_i...
Open at page →
Page 67
en CO DC o CO c 2 J* CO 0) (0 E mtmm a. \- CDC = ° S£ c/> a)co >3 <])O CD CO S> SI ^o o CO 0)CM O)«•* CO,C0 c CD O u_ CD CL i GAS< 35 DCz a: <LZ LIE iZ T32 a ooo O (A >>9 CD (A >< o™ u< o3(3 <DCZDC LLLILu 5 CD CD CD zZzz...
Open at page →
Page 68
I .co I C (0 »- (/) z^ c2 0)(0 * -9 £3 O CO a E o o I CO ffi o CM — i CO m CO CO ffi CO CM *C0 ffi CM o CM o o o I o CM I CO CO DC o o COtH J-l 11I-]It £-a -> .o (1)t~) •HW S-ig>> OS3 O cfl 5-i T3O 0) 5-1 co 3-I CO CO 5-...
Open at page →
Page 69
t c o •MM 0= 0) o ]C Q. E o CM CM CO •cw eo 0) •P 0)-H 111t) 1(1 WWT3 C 2.2 jjH 4-1 4-)CU X. 1 l •H CO ux c o o 4-1 CO c o CO P. <D wd WCO 0)w P cu ap a. P c3 ccjo Pi— I 0) c o •H cO cO P 4-iC cO bOe C to C •H CO 4-> C •...
Open at page →
Page 70
t C o (0 o o JL c o V) Q_ CM CM a. \\\\\\\\\\\ Eo 0) 4JW co a) co.h (0 Cfl4J S-io X> IP Io CO CO 0) CO CO o 4-> P o o CD co 0) M Pu P C cfl P CO P O O •H CO™ o o P 29 CD cfl s cu x: CJ CO CM ctj a CO p o v . CO dj •H 0 P...
Open at page →
Page 71
11.APPENDICES APPENDIX A USEANDCONVERSIONOFUNITSOFFLOWRATEANDTHROUGHPUT Todiscussthedifferencesbetweenflowrateandthroughputunits,consider thesimpleexperimental apparatusinfigure20,whereacylindricalvolumeis dividedbyaplat...
Open at page →
Page 72
Q=P(dV/dt)=(1atm)(1cm 3 s" 1 )=1atmcm 3 s" 1 , (A4) independentofthetemperatureofthegas. Ifthegastemperature is273.15K (0°C),themolarflowrateofgascanbecomputedusingeq(A3)as Qm =Q/(RT) =(1atmcm 3 s" 1 )/[(82 .057atmcm 3 m...
Open at page →
Page 73
thisflowis1atmcm 3 s" 1 (323°C. ItisimportanttonotethatPVunitsor throughputunitsarenotreallyunitsatall,inthesensethatontheirown theydonothavecleardimensions: theyaremerelyexpressions ofconvenience thatare,infact,definedb...
Open at page →
Page 74
quadrant,astheTableAlcaptionindicates isintended, thethroughputunits canthenberegardedasflowrateunits,andconversionofflowrateunits acrosstheheavyblacklineisthenallowed. Substituting eq(All)intoeq (AlO)thengives A 3 {Pam...
Open at page →
Page 75
1x10" 7 atmcm 3 s"1@0°C=A 3 Torr1s" 1 @23°C. (A19) Then,ineq(A16) ,A A =1x10" 7 ,QA =atmcm 3 s" 1 ,andT A =0°C=273.15K,Q3 =Torr1s" 1 ,andT 3 =23°C=296.15K.FromTableAl ,theconversionfactor ineq(A17)is1atmcm 3 s" 1 =(0.760...
Open at page →
Page 76
A-6
Open at page →
Page 77
APPENDIXB GENERALTHEORYOFGASFLOWINVACUUMSYSTEMS Theflowofhighlyrarefiedgasesthroughvariouscomponents ofavacuum apparatushasbeenatopicofseriousinterestsincetheearly1900's.The worksofKnudsen[11],Smoluchowski [12],Dushman [...
Open at page →
Page 78
mol" 1 ),andthecoefficients B t arethe"virialcoefficients", whichare availableintheliteratureformanygases(e.g.,[15]). Asanexample,for heliumatroomtemperature andatmospheric pressure, thecorrection term corresponding toth...
Open at page →
Page 79
3)A/D~1 certaingeometries otherthananaperture it ispossible toderiveexplicitexpressions, suchasPoiseuilleflowthrougha'long'pipe. transitionflowThenetflowrateisingeneralafunctionof severalparameters, andadequatetheoriesar...
Open at page →
Page 80
Therateatwhichgasleavesvolume 1(orentersvolume2)isthen: dNj dN 2 N^t-0)C -e' t/T . (BIO) dt dt V x Theseresultsdemonstrate thatevenforsuchaverysimplegasflowsystemthe flowrateofthegasthroughtheorificeisconstantlychanging,...
Open at page →
Page 81
APPENDIX C Anoteonflowrateandleakrateunits CharlesD.Ehrlich CenterforBasicStandards.NationalBureauofStandards.Gaithersburg.Maryland20899 (Received31October1985;accepted28April1986) Theconfusionintheliteratureandinthelabo...
Open at page →
Page 82
CharlesD.Ehrllch:Anoteonflowrateandleakrateunits ityforconfusion isgreatlyreduced. Anothercommonpracticewithleakrateunitsistoex- presstheleakrateintermsof"standard"conditions,suchas "standardcmVs"or"cmVsSTP."Unfortunatel...
Open at page →
Page 83
APPENDIX I) Low-rangeflowmetersforusewithvacuumandleakstandards K.E.McCulloh,C.R.Tilford,C.D.Ehrlich,andF.G.Long NationalBureauofStandards.CenterforBasicStandards.Gaithersburji.Maryland20X99 (Received20October1986;accept...
Open at page →
Page 84
377 McCullohelat.:Low-rangeflowmeters(orusewithvacuumandleakstandards 377 Fro.1.Schematicoftheconstantpressure pistonflowmeter.Twodifferentsizepis- tonsareincludedtoextendtherange.The turbomolccularpumpprovidesalowref- e...
Open at page →
Page 85
378 McCullohetal. :Low-rangeflowmeters(orusewithvacuumandleakstandards 378 ballasttank,andreferencevolume.Theflowmetershave beenoperatedwithhydrogen,helium,neon,nitrogen,and argon.Thesystempressure isbroughtuptothevaluer...
Open at page →
Page 86
379 slightlyaboveatmosphericwillberequiredtocompressthe bellows.Thiswillminimizeleaks,inparticular,leakageof airintotheoil,whichwouldcausesignificanterrors,and maintainpositivecontactbetweenthepistonandthedrive mechanism...
Open at page →
Page 87
380 McCullohelal.:Low-rangeflowmeterslorusewithvacuumandleakstandards 380 D.Timeinterval:6(A/)/Af Theelapsedtimeisrecordedforeach Iurnasihemicro- meterscrewadvances.Timeintervalsarecalculatedfrom thedifferencesofsuccessi...
Open at page →
Page 88
381 A.Randomerrors Themeasuredrandomerrorsduringgaugeandleakcali- brationsdifferwithflowrateandtypeofdevicecalibrated. Thepooledstandarddeviationaboutthemeanforsixmolec- ulardraggaugesrepeatedlycalibratedoveratwo-monthpe...
Open at page →
Page 89
UNITEDSTATESDEPARTMENTOFCOMMERCE NationalBureauofStandards Gaithersburg.Maryland2QB99 SAMPLECALIBRATIONREPORT ReportDate:February 1,1988 LEAKARTIFACT Submittedby NameofCompany,Inc. Anywhere,USA TestperformedJanuary1988 N...
Open at page →
Page 90
REPORTOFTEST(continued) Page2 PROCEDURES Thisleakartifactwascalibratednear23°Cbycomparisonwith Flowmeter#2oftheNBSPrimaryLeakStandard,usingtheuppertolower chamberflowdivisiontechnique. Thetemperaturedependencewasdetermin...
Open at page →
Page 91
REPORTOFTEST(continued) Page3 "REPORTOFTEST" NBSTest#L12/240840 ReportDate :February 1,1988 + LEAKRATEvs.TEMPERATURE LeakRate LeakRate erap.(°C) mol/s stdcc/s Temp.(°C) mol/s L * stdcc/s 0 2.16E-12 4.84E-08 1 2.25E-12 5....
Open at page →
Page 93
NIST-114A U.S.DEPARTMENTOFCOMMERCE 1.PUBLICATIONORREPORTNUMBER (REV.3-90) NATIONALINSTITUTEOFSTANDARDSANDTECHNOLOGY NIST/SP-250/38 2.PERFORMINGORGANIZATIONREPORTNUMBER BIBLIOGRAPHICDATASHEET 3.PUBUCATIONDATE January1992...
Open at page →
Page 95
THESP250SERIESONNISTMEASUREMENTSERVICES* SP250-1 SpectralRadianceCalibrations PB87179883 SP250-2 FarUltravioletDetectorStandards PB87227609 SP250-3 RadiometricStandards intheVacuum Ultraviolet PB87227625 SP250-4 FrickeDo...
Open at page →
Page 96
>> D) O O c sz o <D E - Oc£ CO05 OC0§ ^h-CM tu w« § a>-=wn10u LJ C<D •0£ "Tim 3ZO 3 COCD cg wQ- cqo To oCO OQ-
Open at page →