Supplementary Information for Chemical Characterization of ...€¦ · Supplementary Information...
Transcript of Supplementary Information for Chemical Characterization of ...€¦ · Supplementary Information...
Supplementary Information for
Chemical Characterization of Nanoparticles and Volatiles Present in
Mainstream Hookah Smoke
Véronique Perraud,1* Michael J. Lawler,1 Kurtis T. Malecha,1 Rebecca M. Johnson,2 David
A. Herman,2 Norbert Straimer,3 Michael T. Kleinman,2 Sergey A. Nizkorodov1 and James
N. Smith1
1Department of Chemistry, University of California, Irvine, CA 92697
2School of Medicine, University of California, Irvine, CA 92697
3Department of Epidemiology, University of California, Irvine, California, USA
2
1.WaterpipeSmokingProtocol
Allsmokingsessionswereperformedusingthesamewaterpipe(AnahiSmoke,model
“Fantasy”)describedinFigureS1:
FigureS1.(a)Glasswaterpipeusedinthisstudy.(b)Close-upoftheconventionaltobaccopreparationlooselypackedinsidetheheadofthewaterpipe.
Priortoanexperiment,theglasswaterpipewasentirelycleanedusingdeionizedwater
followedbyisopropylalcoholandkeptovernightinanovenmaintainedat~100°Ctoevaporate
theresidualsolvents.ThepreparationofthetobaccomixturewasadaptedfromShihadehetal.
head(containingthetobacco)
charcoals
bowlcontaining800mLofdeionizedwater
(b)Conventionaltobaccolooselypackedinsidethehead
smokinghoseconnectedtothedilutionsystem
body
(a)waterpipe
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(2012)andShihadehetal.(2014),where10goftobaccomixture,whichwerestoredinthe
darkat~4Cuntilitsuse,wereweighedandleftonthebenchatroomtemperatureovernight
forconditioning.Atthebeginningofeachexperiment,800mLofdeionizedwaterwasaddedto
thewaterpipereservoirandthedownstemwasplaced39mmunderthewatersurface.Then,
the10gofpreparedtobaccowerepackedlooselyinsidethewaterpipeheadandwrappedwith
perforatedaluminumfoil.Threecubesofcharcoalwereheatedonahotplateforabout10
min,insuringthatallthefacesofthecubewereincandescent.Thecubeswerethenplacedon
thefoilsurfaceatopthetobaccofor5minpriortothefirstpuff.Threecharcoalcubeswere
necessarytouniformlyheatthetobacco.Asmokingpump,operatingatatotalflowrateof~10
Lmin-1,wasconnectedtoasolenoidaircontrolvalve(IngersollRand,modelP251SS-012-D)
thatwastimedbyacontrolboard(TeagueEnterprises,modelTE-2)andwasusedtoprovidea
4spuffatafrequencyof2min-1.Anadditionalflowof~3Lmin-1(sumofalltheanalytical
instrumentflowrates),yieldingatotalpuffflowrateof~13Lmin-1,wasdrawnintoadilution
systemasdescribedbelow.Allsmokingsessionswereexecutedfor30min.Attheendofthe
experiment,theremainingtobaccowasweighedtoestimatethelossoftobaccoproductfor
onesession.
2.FastFlowDilutionSystem
(a)Description.Thefastflowdilutionsystem(Figure1)beginswithatwo-valvedeliverysystem
thatselectsbetweensampling~3Lmin-1ofthetotalpuffflow,whichcorrespondstothesum
oftheinletflowstoallinstruments,orthesameflowrateofpurifiedair(FTIRpurgeair
generator,ParkerBalstonmodel75-62).Thisassuredthatacontinuousflowofsampleairwas
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providedtotheinstrumentsatalltimeregardlessofwhetherornotapuffwasbeingmade.
Theuseofbothvalveswassimplytoincreasetheairthroughputthroughthesystem.The
valvesweresynchronizedtothepuffsusingatimingsignalprovidedbythecontrolboard.
Exitingthetwo-valvedeliverysystem,thesamplewasthendilutedbyacustomtwo-stagefast
flowdilutionstainlesssteeltube(Blairetal.2015).Thepuffwasdilutedfirstbyadditionofa
drypurifiedairflowof~16Lmin-1usingamassflowcontroller(SierraInstruments,model
SmartTrak50).Afractionofthedilutedflow(~3Lmin-1)wastransferredtoaseconddilution
stagethroughanorifice,whereitwasdilutedbyadditionofanother~15Lmin-1ofdrypurified
air.Again,onlyafractionofthatflow(~3Lmin-1)wasdrawnintoastainlesssteelmixing
chamber,towhichsamplingtubesfortheindividualinstrumentswereattached.Eachdilution
branchwasequippedwithacriticalorifice(O’KeefeControlsCo.,TypeK2)andHEPAfilter(Pall
Corp.,model12144)followedbyvacuumpumpstoexhausttheexcessairataconstantrate.
Thebalanceoftheflowsthroughthefastflowdilutionsystemwasevaluatedandcontrolledat
thebeginningofeachexperimenttoassurepropertransferofthesampletotheinstruments
andalsotoconfirmthatthedilutionsystemwasoperatedunderconsistenttemperatureand
pressureconditions.TheReynoldsnumberforthedilutionsystemwasestimatedtobe
1.8×102,indicatinglaminarflowconditions(Hinds1999).
Attheendofthedilutionsystemtherewasastainlesssteelcylinderactingasamixing
chamberwithatotalvolumeof4L(50cmlong;10cmdiam.).Theaverageresidencetimeof
thesampleflowinthedilutiontubewasestimatedtobe21s,whiletheresidencetimein
chamberwasabout1.3min.Thesamplewasdeliveredatthebottomofthechamberviaa0.25
cmO.D.stainlesssteeltubingwhilealltheinstrumentswereconnectedtoseparateindividual
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outletsatthetopofthechamber.Thisensuredpropermixingofthesampleandaccomplished
some“averaging”ofthepuffstomakemoreconsistentaerosolsizedistributionmeasurements.
(b)Particletransmissionefficiencythroughthedilutionsystem.Inordertodeterminethe
transmissionefficiencyofparticlesthroughthefastflowdilutionsystem,particleswere
generatedusingaconstantoutputatomizer(TSI,model3076)containingamixtureof2:1
dimethylamine/sulfuricacidinwater(DMA,Aldrich,40%wt.inwater;H2SO4,FisherScientific,
96.2%).Apressureof~20psigofdrycleanairwasusedattheinletoftheatomizerandaflow
of~2.8Lmin-1exitedtheatomizerandpassedthroughaNAFIONTMmembranedrier(Perma
PureLLC,modelFC125-240-5MP)todrytheparticles.Afractionofthisdryaerosolflow(~0.1L
min-1)wasdilutedwith1.4Lmin-1ofdrycleanairandsampledfirstthroughthefastflow
dilutionsysteminabsenceofthetwo-valvedeliverysystemusingthescanningmobilityparticle
sizer(SMPS),describedabove.Inthiscase,onlytheSMPSwasconnectedtothemixing
chamberlocatedattheendofthefastflowdilutionsystemdrawingatotalof~1.5Lmin-1
throughout.Thetwo-stagedilutionairwasreducedto10.5Lmin-1and~6.0Lmin-1forthe
dilutionstages1and2,respectively.Inaddition,thoseexperimentswerecarriedoutwithan
ultrafinecondensationparticlecounter(TSIInc.,model3025A)insteadofamodel3760particle
counterasdescribedbelow.ThefollowingflowrateswereusedfortheSMPS:1.5Lmin-1
aerosolflow,10Lmin-1sheathflow.
Thetransmissionefficiency(TE)oftheparticlesthroughthedilutiontubeitselfwas
observedtobehigh[TE(dil.tube)~1]atalldiameters(FigureS2a)whilethemixingchamber
showedreducedTEfortheparticleswithdiametersmallerthan50nm(FigureS2b).The
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resultingtransmissionefficiencycurveforthechamberwithoutthetwo-valvedeliverysystem
wasdeterminedastheratioofthesizedistributionmeasuredwiththemixingchambertothe
sizedistributionmeasuredwithout(FigureS2c).
FigureS2.Sizedistributionsof2:1DMA:H2SO4particlesmeasuredattheatomizeroutput(nodilution;greentrace)and(a)afterthedilutiontube(nomixingchamber;purpletrace),(b)afterthedilutionchamber(redtrace).(c)Resultingtransmissionefficiencyofmixingchamber.Particlesfromamixtureof2:1DMA/H2SO4weregeneratedusingaconstantoutputatomizer.Afractionoftheoutletflowoftheatomizer(0.1Lmin-1wasatomizedwith1.4Lmin-1ofdrycleanairbeforebeensampledusingthedilutionsystem.
(a)
(b)
(c)
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Then,thetwo-valvedeliverysystemwasaddedanditsefficiencycurvedetermined
usingonlyonechannel(nopuff).Fortheseexperiments,nodilutionoftheoutputofthe
atomizerwasusedpriortosamplingusingthedilutionsystem.FigureS3showstheresulting
sizedistributionandtransmissionefficiencyofthetwo-valvedeliverysystemdeterminedasthe
ratioofthesizedistributionmeasuredwiththetwo-valvedeliverysystemtothesize
distributionmeasuredwithout.
FigureS3.Sizedistributionsof2:1DMA:H2SO4particlesmeasuredafterthedilutiontube+mixingchamber(bluetrace)andafterthetwo-valvedeliverysystem+dilutiontube+mixingchamber(greentrace).(b)Resultingtransmissionefficiencyofthetwo-valvedeliverysystem.Particlesfromamixtureof2:1DMA/H2SO4solutionweregeneratedusingaconstantoutputatomizer.Afractionoftheoutletflowoftheatomizer(1.4Lmin-1)wassampledusingthedilutionsystem(nodilutionpriorsampling).
(a)
(b)
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Theoveralltransmissionefficiency,TE(overall),wasthenobtainedas:
!" #$%&'(( = !" *+(. -./% ×!" 2ℎ'4/%& ×!"(-6# − $'($%898-%4)
TheresultingoveralltransmissionefficiencythroughtheentiresystemisshowninFigureS4
anddemonstratesexcellenttransmissionforparticleslargerthan50nm(TE(overall)>89%).
FigureS4.Overalltransmissionefficiency(TE)ofthedilutionsystemcalculatedfromequation !" #$%&'(( = !" *+(. -./% ×!" 2ℎ'4/%& ×!"(-6# − $'($%898-%4).
3.WaterpipeMainstreamSmokeSampling
Relativehumidityandtemperatureweremonitoredcontinuouslyusingtwoprobes
(VaisalaCorp.,modelHMP110)locatedattheentranceofthetwo-valvesystem(sampling
mainstreamsmokefromthewaterpipe)andatthemixingchamber(aftertwo-stagedilution
withdrypurifiedair).Acarbonmonoxide(CO)monitor(ThermoFisherScientific,model48i)
wasusedtomonitortheCOlevelsinthemainstreamemissionofthewaterpipeafterthetwo-
stagedilution(flowrate~0.45Lmin-1).Calibrationoftheinstrumentwasperformedusinga
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standardgasmixturecontaining8.99ppmCOinhelium(PraxairCorp.),andacalibrationfactor
of1.08wasdetermined.
Sizedistributionsoftheparticlesemittedinthemainstreamofthewaterpipewere
measuredusingascanningmobilityparticlesizer(SMPS)composedofanelectrostaticclassifier
(TSI,Inc.,model3080L),featuringalongdifferentialmobilityanalyzer(DMA;TSIInc.,model
3081),combinedwithacondensationparticlecounter(CPC)(TSI,Inc.,model3760).Aerosol
wassampledfromthemixingchamberataflowrateof1.5Lmin-1andthesheathairofthe
DMAwas5Lmin-1withvoltagescannedfrom5V-10kV,allowingadistributionoverthemobility
diameterrangeof4to500nmtobemeasured.Aone-directionalscantimeof60swasused.
InstrumentcontrolanddataacquisitionwereperformedusingsoftwarewrittenintheLabView
programminglanguage(NationalInstrumentsCorp.).Theinversiontotheactualparticlesize
distributionwasperformedusingamodifiedversionoftheWashingtonStateUniversitySMPS
DataInversionToolkitwrittenintheIgorProprogramminglanguage(Wavemetrics,Inc.).Even
withtheeffortstodilutethemainstreamsmoke,theCPCwasnotalwaysabletocountparticles
rapidlyenoughforthehighconcentrationsmeasured.Poissoncountingstatisticswereusedto
correctthedatawhenthissaturatedcountingconditionwasapparent.
Thechemicalcompositionofultrafineparticlesfromthedilutedmainstreamwaterpipe
smokewasmeasuredusingTDCIMS(Lawleretal.2018;Smithetal.2004).Theinstrumenthad
aninletflowrateof~1.5Lmin-1andisequippedwithatime-of-flightmassspectrometerwitha
resolvingpowerof~3500(TofwerkAG,modelHTOF).Fortheseexperimentsabipolaraerosol
neutralizerwasusedtochargethesampledaerosolbecausetheunipolarchargersused
typicallywithTDCIMSsufferedfromleakscausedbythepressuredropinducedbythedilution
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system.Thislimitedourabilitytoisolatesize-dependentcomposition,sowereport
compositiontypicalofsub-100nmparticles.Polydispersedparticleswerecollectedfor2-10
minonthetipofaPtwirebyelectrostaticprecipitation.Typicalestimatedsamplemasswas
0.2-1.4ng,basedoncharacterizationofsize-resolvedcollectionefficiencyusingatomized
aerosolandthemeasuredaerosolsizedistributionsduringtheexperiments.Thecollected
particlesweresubsequentlythermallydesorbedovera1-mintemperaturerampandsoakfrom
roomtemperatureto~600˚C.Positiveionmodewasrecordedforallexperiments,
correspondingtochemicalionizationofdesorbednanoparticleconstituentsusing(H2O)nH3O+
(n=1-3)reagentions,formingH+adductsofclosed-shellmolecules,i.e.[M+H]+.
Real-timemeasurementsoftheorganicgasesfromthedilutedmainstreamsmokewere
performedusingahighresolutionPTR-ToF-MS(IoniconAnalytik,PTR-ToF-MS8000).The
operatingprincipleofthePTR-ToF-MShasbeendescribedpreviously(Jordanetal.2009).
Briefly,volatileorganiccompoundssampledbytheinstrumentcanundergoprotontransfer
reactionwiththeH3O+reagent,formingprimarily[M+H]+ionsiftheprotonaffinityofthe
analyteishigherthanthatofwater.Theinstrumentwasoperatedwithadriftvoltage,
temperatureandpressureof600V,60°Cand2.2mbarrespectively(resultinginaratioofthe
electricfield(E)tothenumberdensityofthedrifttubebuffergasmolecules(N)ofE/N~135Td
where1Td=10-17Vcm2)andaflowrateof0.1Lmin-1through1.59mmO.D.PEEKtubinginlet
heatedat70°C.Thedatawereacquiredusinga1stimeresolution.Mass-to-chargecalibration
wasverifiedatthebeginningofeachexperimentusingfourisotopicionsincludingH318O+at
m/z21.022,16O18O+atm/z33.994,(H2O)H318O+atm/z39.033andacetoneatm/z59.049([M+
H]+)fromroomair.Inaddition,headspaceoverpure1,3-diiodobenzene(98%,Sigma-Aldrich)
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wassampledatthebeginningofsomeexperimentstomasscalibratethehigherrangeofmass-
to-chargevaluesusingitscorrespondingfragmentionatm/z203.943([C6H4I2+H–I]+)
(Stockwelletal.2015).
4.ReferenceCigaretteSmokingProtocol
Thecigaretteswereconditionedatarelativehumidityof~60%bymaintainingthem
enclosedinadesiccatorabovea~75%wt.aqueousglycerolsolutionforatleast48hpriorto
use.Theinletofthedilutionsystemwasslightlymodifiedtomakeitpossibletosmokethe
cigaretteartificiallyusingapuffflowof~1Lmin-1thatwascombinedwithdrypurifiedairto
makeatotalof~3Lmin-1asrequiredbyourinstrumentsuite.Thecigarettewaslitusingan
electroniclighterforthedurationofthefirstpuffandatotalof7puffsweresmokedforeach
cigarette(2spuff;every60s).Thetotaldilutionfactorofthecigaretteemissionsampled
throughtheentiresystemincludingthe2-stageactivedilutionandthepufftimestep(2spuff;
58spurifiedair)was~3250.
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5.RelativeHumidityandTemperatureProfilesDuringWaterpipeSmoking
FigureS5.Representativerelativehumidity(RH)timeprofile(a)andtemperatureprofile(b)obtainedduringawaterpipesmokingsessionwiththeconventionaltobacco.EachdatapointcorrespondstotheaveragevalueofRHandtemperaturemeasuredovertwo-minutetimeintervals.Theblueopeneddatapointscorrespondtomeasurementsattheexitofthewaterpipehose(beforethedilutiontube)andtheredfilleddatapointscorrespondtomeasurementsatthemixingchamber.
hookahsmokingsession
hookahsmokingsession
(a)
(b)
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6.OnlineMeasurementsofVolatileOrganicCompoundsbyPTR-ToF-MS
FigureS6.TypicalunitmassresolutionPTR-ToF-MSmassspectrafromthewaterpipemainstreamsmokeofthethreetobaccosinvestigatedincluding(a)theconventionaltobacco,(b)thenicotine-freeherbaltobaccoand(c)thedarkleafunwashedtobacco,and(d)the3R4Freferencecigarette.Allspectrawerecollectedattheendofthesmokingsession(thelast10puffsforthewaterpipesamples,andthelastpuffforthecigarettesample)andthebackgroundsignalhasbeensubtractedout.ThepeaksindicatedwithastarcorrespondtotheO2
+ionatm/z32andthehydroniumion-watercomplex(H2O)2H
+atm/z37thatdidnotsubtractoutcompletely.
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FigureS7.ExpandedviewofthePTR-ToF-MSspectrashowingtheseparationofmultiplepeaksobservedatnominalm/z42,43,47,57,69,91,93,107,129and163.Theredtracecorrespondstothesample,whilethebluetraceisthebackground.
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TableS1.Relativeiondistributionnormalizedtom/z45(acetaldehyde)forwaterpipeexperimentwithglycerolonlyandallthreeinvestigatedtobaccos.Numbersinparenthesesfortheconventionaltobacco,thenicotine-freeherbaltobaccomixtureandthedarkleafunwashedtobaccorepresentonestandarddeviationofnreplicatemeasurements.
Nominalm/z Assignment Glycerol
only(n=1)Conventional
(n=4)Herbal(n=2)
Darkleaf(n=2)
31 [CH2O+H]+ 0.53 0.23(0.007) 0.02(0.002) 0.03(0.004)33 CH4O+H]+ 0.12 0.02(0.002) 0.01(0.000) 0.01(0.000)41 [C3H4+H]+ 0.09 0.17(0.006) 0.02(0.001) 0.02(0.003)43 [C2H2O+H]+ 0.37 0.07(0.006) 0.04(0.001) 0.04(0.002)45 [C2H4O+H]+ 1 1 1 157 [C3H4O+H]+ 0.23 0.26(0.008 0.25(0.002) 0.27(0.002)59 [C3H6O+H]+ 0.16 1.09(0.110) 0.08(0.007) 0.10(0.014)61 [C2H4O2+H]+ 0.66 0.10(0.011) 0.05(0.000) 0.05(0.004)75 [C3H6O2+H]+ 0.20 0.28(0.008) 0.26(0.001) 0.27(0.001)93 [C3H8O3+H]+ 0.004 0.07(0.003) 0.07(0.000) 0.07(0.000)
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FigureS8.TypicalunitmassresolutionmassspectraobtainedusingthePTR-ToF-MSfromthewaterpipemainstreamsmokeof(a)onlycharcoal+waterconditions(notobacco),(b)theconventionaltobaccowithoutcharcoal(noheat)and(c)glycerolonly(notobacco).Allspectrawerecollectedattheendofthesmokingsession(thelast10puffsforthewaterpipesamples)andthebackgroundsignalhasbeensubtractedout.Spectra(d)resultedfromnebulizedglycerolaqueousparticlesgeneratedusingahospitalnebulizer(MicroMistnebulizer;HudsonRCI®).ThepeaksindicatedwithastarcorrespondstotheO2
+ionatm/z32andthehydroniumion-watercomplex(H2O)2H+atm/z37thatdidnotsubtractoutcompletely.
17
FigureS9.ExpandedviewofthePTR-ToF-MSspectrashowingm/z79fortheconventionaltobaccomixture(redtrace),theherbaltobacco(orangetrace),thedarkleafunwashedtobacco(greentrace)comparedtothecharcoalonly(notobacco)experiment.Forcomparison,theconventionaltobaccowithoutcharcoal(pinktrace),theglycerolonly(darkbluetrace)experimentsandthe3R4Freferencecigarette(lightbluetrace)arealsoshown.Allspectraarebackgroundsubtracted.
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FigureS10.ComparisonofaveragedunitmassresolutionPTR-ToF-MSmassspectraasafunctionofsmokingtime.Eachspectrumcorrespondstoanaverageofspectratakenover10puffs(5min).Conventionaltobaccorunperformed(a)under‘normal’condition(charcoal+water+shisha)and(b)withoutwaterinthewaterpipebowl.Allspectraarebackgroundsubtracted.Negativepeakscorrespondtom/z32(O2
+)and37(H2O)2H+incompletelyremovedbythesubtraction.
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FigureS11.ExpandedviewofthePTR-ToF-MSspectracollectedfortheconventionaltobacco(withandwithoutwaterpresentinthewaterpipebowl)showingtheevolutionofthesignalatnominalm/z33,47and163asafunctionoftime(numberofpuffs).Eachspectrumcorrespondstoanaverageover10puffsandisbackgroundsubtracted.
withH2O withoutH2O
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7.SizeDistributionMeasurements
FigureS12.Typicalsizedistributionsforindividualsmokingsessionsmeasuredforthreedifferentshishasincluding(a)theconventionaltobacco,(b)thenicotine-freeherbaltobacco,and(c)thedarkleafunwashedtobacco,aswellasa3R4Freferencecigarette(d).Concentrationsarecorrectedfordilutionandsize-dependentsamplinglossesthroughtheexperimentalsystem.Thestartofthesmokingsessioncorrespondstothesuddenincreaseontheparticlenumberconcentration.
Inabsenceofcharcoal(noheat),noparticleswereobserved.Becauseoftheirsimilarities,
particlesizedistributionresultsfrom‘charcoalonly’and‘glycerolonly’experimentsare
averagedtogetherandtheresultingaverageddistributionispresentedinFigureS13b.This
similaritysuggeststhatthemajortobaccoadditiveglycerolisnottheprimarydriverofnew
particleformationorgrowthinhookahsmokeaerosol.
10
2
46
100
2
46
15:155/26/17
15:303R4F cigarette
dN/dlogDp
100101102103104105
10
2
46
100
2
46
09:455/17/17
10:00 10:15 10:30 10:45
Herbal10
2
46
100
2
46
diam
eter
(nm
)
15:005/22/17
15:15 15:30 15:45
Conventional
10
2
46
100
2
46
diam
eter
(nm
)
09:455/18/17
10:00 10:15 10:30 10:45
Dark leafunwashed
a. b.
c. d.
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FigureS13.Sizedistributionofparticlesmeasuredfromhookahmainstreamsmokecollected(a)inabsenceofwaterinthewaterpipebowl(conventionaltobacco),and(b)duringanexperimentwherethetobaccowasreplacedwith10gofglycerol.IntensityscaleisthesameasinFigure3inthemainmanuscript.
10
2
46
100
2
46
diam
eter
(nm
)
14:455/23/17
15:00 15:15 15:30
no H2O 10
2
46
100
2
46
diam
eter
(nm
)13:45
5/25/1714:00 14:15 14:30
glycerol
a. b.
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8.TDCIMSMeasurements
FigureS14.Size-binnedsamplemasscollected(ng)fromthehookahmainstreamsmokebytheTDCIMSforatypicalhookahexperiment.
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FigureS15.TDCIMSmassspectraofultrafineparticlescollectedfromhookahmainstreamsmokefrom(a)theconventionaltobacco,(b)thenicotine-freeherbaltobacco,(c)thedarkleafunwashedtobacco,and(d)the3R4Freferencecigarette.Formulasnexttothepeaksaregivenintheirdetectedionicform(asanH+adduct),withthechargesymboldroppedtoavoidclutter.Thepresentedmassspectraareaveragesoftwotofourexperimentsperformedusingthesametobacco,witherrorbarscorrespondingtoonestandarderrorofthemean.Labeledionsare“detectable”bythecriteriathattheirbackground-subtractedabundancesareeithertwostandarderrorsgreaterthanzerofortheaverage,oriftheyweretwostandarderrorsabovezeroforeveryindividualexperiment.Onlydetectableionsabove0.7%ofthetotalsignalarelabeled.Glycerolanditsclusterswereexcludedbecauseofvariableandlargegasphasebackgrounds.Therangeofthem/zaxisischosentohighlightlikelymolecular(unfragmented)specieswithhighconfidenceofformulaidentification.
0.4
0.3
0.2
0.1
0.0
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C7H
7O2
C6H
5O3
C5H
9O4
C6H
11O
4
C5H
13O
5
C6H
11O
5C
6H13
O5
C7H
19O
4C
6H13
O6
C9H
11O
4C
10H
17O
3C
8H13
O5
C9H
11O
5
C9H
13O
5C
12H
25O
2
C9H
17O
7
C12
H17
O5
C9H
19O
8
0.16
0.12
0.08
0.04
0.00
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
11O
4
C6H
11O
5
C10
H15
N2
C9H
10N
O2
C8H
13O
4
C9H
11O
4
C9H
13O
5
C12
H25
O2
C11
H15
O5
C13
H19
O4
C12
H17
O5
C9H
19O
8
0.15
0.10
0.05
0.00
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
9O4
C6H
11O
4C
6H15
O4
C6H
11O
5
C6H
13O
5
C7H
11O
5C
6H14
NO
5C
6H13
O6
C9H
11O
4C
8H13
O5
C9H
13O
5
C9H
15O
6
C8H
17O
7
C9H
17O
7 C9H
19O
8
a.
b.
c. 0.07
0.06
0.05
0.04
0.03
0.02
0.01
0.00
Sig
nal F
ract
ion
260250240230220210200190180170160150140130120m/z
C6H
7O3
C6H
9O3
C5H
8NO
3C
5H9O
4
C6H
9O4
C6H
11O
4 C6H
11O
5
C10
H11
O2
C10
H15
N2
C7H
11O
5C
6H13
O6
C13
H14
N C10
H9O
4
C7H
13O
6
C11
H13
O3
0.15
0.10
0.05
0.00
Sig
nal F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
9O4
C6H
11O
4C
6H15
O4
C6H
11O
5
C6H
13O
5
C7H
11O
5C
6H14
NO
5C
6H13
O6
C9H
11O
4C
8H13
O5
C9H
13O
5
C9H
15O
6
C8H
17O
7
C9H
17O
7 C9H
19O
8
a.
b.
0.4
0.3
0.2
0.1
0.0
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C7H
7O2
C6H
5O3
C5H
9O4
C6H
11O
4
C5H
13O
5
C6H
11O
5C
6H13
O5
C7H
19O
4C
6H13
O6
C9H
11O
4C
10H
17O
3C
8H13
O5
C9H
11O
5
C9H
13O
5C
12H
25O
2
C9H
17O
7
C12
H17
O5
C9H
19O
8
0.16
0.12
0.08
0.04
0.00
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
11O
4
C6H
11O
5
C10
H15
N2
C9H
10N
O2
C8H
13O
4
C9H
11O
4
C9H
13O
5
C12
H25
O2
C11
H15
O5
C13
H19
O4
C12
H17
O5
C9H
19O
8
0.15
0.10
0.05
0.00
Sign
al F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
9O4
C6H
11O
4C
6H15
O4
C6H
11O
5
C6H
13O
5
C7H
11O
5C
6H14
NO
5C
6H13
O6
C9H
11O
4C
8H13
O5
C9H
13O
5
C9H
15O
6
C8H
17O
7
C9H
17O
7 C9H
19O
8
a.
b.
c.
0.4
0.3
0.2
0.1
0.0
Sig
nal F
ract
ion
260250240230220210200190180170160150140130120m/z
C7H
7O2
C6H
5O3
C5H
9O4
C6H
11O
4
C5H
13O
5
C6H
11O
5C
6H13
O5
C7H
19O
4C
6H13
O6
C9H
11O
4C
10H
17O
3C
8H13
O5
C9H
11O
5
C9H
13O
5C
12H
25O
2
C9H
17O
7
C12
H17
O5
C9H
19O
8
0.16
0.12
0.08
0.04
0.00
Sig
nal F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
11O
4
C6H
11O
5
C10
H15
N2
C9H
10N
O2
C8H
13O
4
C9H
11O
4
C9H
13O
5
C12
H25
O2
C11
H15
O5
C13
H19
O4
C12
H17
O5
C9H
19O
8
0.15
0.10
0.05
0.00
Sig
nal F
ract
ion
260250240230220210200190180170160150140130120m/z
C5H
9O4
C6H
9O4
C6H
11O
4C
6H15
O4
C6H
11O
5
C6H
13O
5
C7H
11O
5C
6H14
NO
5C
6H13
O6
C9H
11O
4C
8H13
O5
C9H
13O
5
C9H
15O
6
C8H
17O
7
C9H
17O
7 C9H
19O
8
a.
b.
c.
(a)Conventional tobacco
(b)Herbaltobacco
(c)Dark leafunwashed tobacco
(d)3R4FCigarette
24
FigureS16.Highresolutionpeakfittingofnominalm/z163fortherawaveragedmassspectrumofnon-background-correctedsignalfromacigarettesmokingexperiment.C6H11O5
+(levoglucosan)andC10H15N2
+(nicotine)arethemaincontributorstothespectrum.
163.3163.2163.1163.0
m/Q (Th) (not auto-updated after calibration)
4000
3000
2000
1000
0
Ion
coun
ts p
er b
in
C9H7
O3
C6H1
1O5
C10H
11O2
C9H1
1N2O
C7H1
5O4
C11H
15O
C10H
15N2
C8H1
9O3
C12H
19
C9H2
3O2Peak list:
List 1
Area fit = 84%
25
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