ArticlePDF Available

In Situ Monitoring of Trace Gases in a Non-Urban Environment

Authors:

Abstract and Figures

A set of commercial instruments measuring carbon monoxide (CO), ozone (O3), sulfur dioxide (SO2), and nitrogen oxides [nitric oxide (NO), nitrogen dioxide (NO2), and odd nitrogens (NOX)] was integrated and deployed in a nonurban environment. The deployment occurred between July 2, 2007 and August 7, 2007 in Richland, WA. The mixing ratios of all species were lower than in most ruralsuburban environments, and strong diurnal patterns were observed. NO2 was depleted by photochemically formed ozone during the day and replenished at night as ozone was destroyed. The highest ozone concentration during these episodes was 45 ppb. The overall average was 15 ppb with readings approaching near zero at times. This observation is low compared to average daytime summer readings of 6080 ppb in highly populated and industrialized urban areas in the Pacific Northwest region. Backtrajectory analysis and prevailing weather conditions both indicated that much of the ozone was transported locally or was produced insitu. Analysis of SO2 as a tracer for O3 advection further indicated lack of longrange regional transport of pollutants to Richland. We also present results of analysis of high ozone episodes and comparisons relative to other areas in the Pacific Northwest region. These results provide a useful sample data set to study the historical record of air quality in rural Eastern Washington.
Content may be subject to copyright.
AtmosphericPollutionResearch2(2011)8998
Atmospheric Pollution Research
www.atmospolres.com
Insitu
monitoringoftracegasesinanon–urbanenvironment
JohnMioduszewski1,2,XiaoYingYu1,VictorMorris1,CarlBerkowitz1,JuliaFlaherty1
1PacificNorthwestNationalLaboratory,AtmosphericSciences andGlobalChangeDivision,Richland,WA99354,USA
2NowatRutgersUniversity,DepartmentofGeography,Piscataway,NJ08854,USA
ABSTRACT
Asetofcommercialinstrumentsmeasuringcarbonmonoxide(CO),ozone(O3),sulfurdioxide(SO2),andnitrogen
oxides[nitricoxide(NO),nitrogendioxide(NO2),andoddnitrogens(NOX)]wasintegratedanddeployedinanon–
urbanenvironment.ThedeploymentoccurredbetweenJuly2,2007andAugust7,2007inRichland,WA.Themixing
ratiosofallspecieswerelowerthaninmostrural–suburbanenvironments,andstrongdiurnalpatternswere
observed.NO2wasdepletedbyphotochemicallyformedozoneduringthedayandreplenishedatnightasozonewas
destroyed.Thehighestozoneconcentrationduringtheseepisodeswas45ppb.Theoverallaveragewas15ppbwith
readingsapproachingnearzeroattimes.Thisobservationislowcomparedtoaveragedaytimesummerreadingsof
60–80ppbinhighlypopulatedandindustrializedurbanareasinthePacificNorthwestregion.Backtrajectoryanalysis
andprevailingweatherconditionsbothindicatedthatmuchoftheozonewastransportedlocallyorwasproducedin–
situ.AnalysisofSO2asatracerforO3advectionfurtherindicatedlackoflong–rangeregionaltransportofpollutants
toRichland.Wealsopresentresultsofanalysisofhighozoneepisodesandcomparisonsrelativetootherareasinthe
PacificNorthwestregion.Theseresultsprovideausefulsampledatasettostudythehistoricalrecordofairqualityin
ruralEasternWashington.
Keywords:
Tracegas
HYSPLIT
Nonurbanenvironment
Ozone
ArticleHistory:
Received:28May2010
Revised:20September2010
Accepted:06October2010
CorrespondingAuthor:
XiaoYingYu
Tel:+15093724524
Fax:+15093726168
Email:xiaoying.yu@pnl.gov
©Author(s)2011.ThisworkisdistributedundertheCreativeCommonsAttribution3.0License. doi:10.5094/APR.2011.011
1.Introduction
Atmospherictracegasesarechemicalcompoundsfoundin
verylowconcentrationsintheatmosphere;despitelowconcen
trations,however,theycanexertconsiderableinfluenceona
rangeofenvironmentalprocessesandhealthproblems(Seinfeld,
2004).Knowledgeoftheinteractionsamongthesegasesiscrucial
tounderstandtheiratmosphericconcentrationsandlifetimesand
theenvironmentalimpactsthatcanbeexpectedwithmodifica
tionstotheirsourcesandsinks.Ozone(O3),nitrogenoxides
(includingNO,NO2,andNOX),carbonmonoxide(CO),andsulfur
dioxide(SO2)arenotonlypollutantsthemselvesbutalsoreactwith
manyothercompoundssuchasvolatileorganiccompounds(VOCs)
leadingtochangesinatmosphericcomposition(Atkinson,2000).

Accuratein–situmeasurementsarecrucialtoprovidethe
foundationforinvestigatingcomplexphoto–oxidationprocesses.
Withpopulationgrowthbeingacommonphenomenoninmany
ruralareas,historicalrecordsarebecomingincreasinglyimportant
toidentifyairqualitytrendsassociatedwithlocalsourcesrelative
toincreasesresultingfromlongrangetransport.TheTri–Cities,
includingRichland,Pasco,andKennewickinthestateof
Washington,isoneofthestatisticallyfastestgrowingmetropolitan
areasinthecountry,definedasacoreurbanareawithatleast
50000people(USCBa,2008).Itaddedalmosttwentypercenttoits
populationinthelastsixyears(Cohen,2007),indicatingthe
importanceofdocumentingairqualitybeforetheareabecomes
farmoredeveloped.
Thestudypresentedherehastwopurposes.Froman
engineeringstandpoint,themotivationwastointegratemultiple
tracegasanalyzersintoonesystemandidentifyissuesrelatedto
thisintegrationprocess.Combiningbasictracegasanalyzersto
onesystemhasseveraladvantages.First,itsavesspace.Second,it
isconvenienttomoveortransfertheseanalyzers.Third,itprovides
integrateddataacquisitionandconsistenttimestampsforeaseof
datacollection,display,andanalysis.Inaddition,theThermo
Electron,Inc.,tracegasanalyzersusedinthisstudywerebeing
updatedfromC–Seriestoi–Series.Theneweri–Seriesinstruments
offerimprovedmeasuringcapabilities,useroptions,andstorage
space.Thisworkgivesapracticalsolutiontoissuesassociatedwith
acquiringdatafrominstrumentshavingdifferentmanufacturer
configurations.Forinstance,comparedwithstandardserial
connections,ourapproachprovidesfasttimeresolutionaseach
instrumentallows.Italsoprovidesflexibilityforuserstosettheir
owninstrumentconnectionscheme.
Thesecondpurposeofthisstudywastoprovideabasecase
ofpollutantconcentrations,andinparticular,O3concentrations,in
Richland,WA.RichlandisaruralyetgrowingareainthePacific
NorthwestregionoftheUnitedStates,whichatpresenthasozone
concentrationsfarlessthanthosefoundinurbanpartsofthe
UnitedStates.Ruralareashavehistoricallybeenunderrepresented
whenstudyingairpollutionandadatasetforRichlandpriorto
majorgrowthmayproveveryvaluableinitsfuture.Sourceregions
associatedwith“high”ozoneepisodeswerestudiedusingthe
NationalOceanicandAtmosphericAdministration’s(NOAA)
HYSPLITmodeltoidentifythebacktrajectoriesofairparcels
associatedwithelevatedpollutants.Thedeploymenttookplacein
summer,becausephotochemistryismostvigorous.Asaresult,
ozoneoftenpeaks.Thispotentiallycanprovideagoodopportunity
tostudyozoneatthisrurallocation.
90Mioduszewskietal.AtmosphericPollutionResearch2(2011)8998
2.MaterialsandMethods
2.1.Instrumentationandexperimentalsetup
Measurementsofthetracegasesweremadeusingindividual
tracegasanalyzers(ThermoElectron)forO3,CO,SO2,and
NO/NO2/NOX.Theinstrumentswereinstalledinaninstrument
rack,andtheresultingunitdeployedjustsouthofthemain
campusofthePacificNorthwestNationalLaboratory(PNNL)in
Richland,WA(lat46°21’N,long119°17’W,elevation120mMSL)
(Figure1).MapsweremadeusingtheESRIArcMapsoftware
(version9.3).Thegeographicinformationwasobtainedfromthe
WashingtonStateDepartmentofTransportation(WSDOT,2010).
Theinstrumentswerearrangedintherackaccordingtohowdata
wereloggedinsequence.Aswillbedescribedinmoredetail,the
O3analyzerwasusedtocommunicatebetweenthedatalogger
andtherestoftheinstruments.Samplecollectionwasperformed
betweenJuly2andAugust7,2007.Localstandardtime(Pacific
DaylightSavingTime,PDT)wasusedindatarecording.The
conversionbetweenuniversaltime(UTC)andPDTisUTC7hours
=PDT.
Figure1.TopisamapofthePacificNorthwestwithselectedozone
monitoringstationsidentified(NCDC,2007).Bottomisamapof
Washington’sTricitiesarea,includingtheobservationsiteatPNNLdenoted
bytheblackdot.
AlloftheinstrumentswereconnectedtoaCampbell
Scientific,Inc.,(C.S.)CR23XMicrologger.Thedatalogger
communicatedwithaDellLaptopforon–linedisplayviaaserial
cable.ThedataacquisitionprogramwaswritteninEdlog,a
programmingtoolwithinC.S.’sLoggerNet(C.S.,2002),and
downloadedtothedatalogger.Thedataloggerwasusedtostore
selectedinstrumentoutputsandcontrolinstrumentzeroandspan
checkstwiceaday.Instrumentreadingsweremeasuredas
voltagesfromtheanalogvoltageoutputsoftheinstrumentsand
transmittedtothedifferentialvoltageanaloginputsofthedata
logger(seetheSupportingMaterial,SM,FiguresS1andS2).
Ambientairwassampledthrough¼–inTeflonsamplingtubing,
whoseinletwasapproximatelyfourmetersabovethegroundand
passedthroughasamplingportinthewall.Figure2illustrateshow
airpassedthroughTeflonfilters(2µmpore,47mmZefluor,
GelmanP5PJ047)beforeenteringintotheinstruments’sample
bulkhead.Theexhaustlinesfromeachinstrumentwerecollected
intoacommonmanifoldthatreturnedtheairtotheatmosphere
afterscrubbingtheexhaustinapackfilledwithactivatedcarbon.
ADynamicGasCalibrator(ThermoElectron,Model146i)was
usedtocalibratetheinstrumentsautomaticallyonaregularbasis
usingzeroandstandardgases(ScottSpecialtyGases).Thedynamic
calibratorusestwomassflowcontrollerstoregulatetheflowof
zeroandspangas,andaTeflonmixingchambertoachieve
completemixingofthetwocomponentsatthedesired
concentrationlevel.Highpurityzeroaircontaininglessthan
0.5ppmtotalhydrocarbonswasused,whilethestandardgas
mixtureconsistedof10.1ppmNO,10.1ppmCO,and10.0ppm
SO2,balancedwithhighpurityN2.Theozoneanalyzerwas
calibratedusingaprimarystandardultraviolet(UV)photometric
ozonecalibrator(ThermoElectron,Model49C),followingtheEPA
transferstandardsforcalibrationofairmonitoringofanalyzersfor
ozone(EPA,2009).
AUVPhotometricO3Analyzer(ThermoElectron,Model49i)
wasusedtomeasureO3.AtmosphericSO2wasdeterminedwitha
TraceLevel–EnhancedPulsedFluorescenceSO2Analyzer(Thermo
Electron,Model43i).COwasdeterminedbyaTraceLevelCO
Analyzer(ThermoElectron,Model48C).Nitrogenoxides(NO,NO2,
andNOX)weremeasuredwithaTraceLevelChemiluminescence
NO–NO2–NOXanalyzer(ThermoElectron,Model42C).The
ozonatorusedtoconvertNOtoNO2requiresasupplyofdryair,
andDrierite(Cole–Parmer)wasusedtoremovewatervaporfrom
ambientairforthispurpose.Amoredetaileddescriptionofthe
principlesofoperationoftheseinstrumentsisreportedelsewhere
(Platt,1999)andtheoperationprinciplesofeachanalyzerare
brieflysummarizedinTable1.
APrecisionSpectralPyranometer(PSP)(EppleyLaboratory)
wasusedtomeasurethesolarradiationreachingEarth'ssurface.
ThePSPusesathermoelectricdevicethatproducesanelectric
currentproportionaltothebroadbandshortwavesolarradiation
reachingthedetector.Thedetectorispaintedblackandmounted
inanopticalglasssphereforprotectionfromtheelements.It
samplesatwavelengthsbetween0.3µmand3µmatoneminute
intervals.Ahumiditymeasurementprobe(Vaisala,Model
HMP45C)wasusedtomeasurethetemperature(indegrees
Celsius)andrelativehumidityofthesampledair.Windspeedand
directionweremeasuredbyapropelleranemometer(R.M.Young,
Model05103WindMonitor)locatedaboutfifteenmeterstothe
northofthetracegassamplingarea.Datawerecollectedevery
minuteandaveragedtofiveminutesforfinalreporting.
2.2.Instrumentationerror
Backgroundconcentrationchecksusingzeroairwere
conductedtocorrectinstrumentdrift.High–purityairwassentinto
theinstrumentstoobtainadailytruezero.ItiscriticalthattheCO
instrumentbecontinuouslypurgedwithalowpurgeflow(140
cc/minuterecommended)ofzeroair,otherwisesignificantdrift
mayinterferewithdataquality.Purgingisusedtoprevent
interferencefromambientlevelsofCOasairflowsthroughthe
filterwheelassembly,whichcontainsCOononesideandN2onthe
other.Allanalyzersunderwentbackgroundcorrectionsasoftenas
timepermitted,andtheCOanalyzerwascontinuouslypurgedwith
highpurityzeroairwhilesamplingwasoccurring.
Mioduszewskietal.AtmosphericPollutionResearch2(2011)899891
Figure2.AschematicdiagramoftheThermoElectronTraceGasAnalyzersuite.Thedarkestlinesindicatetubingthroughwhichambientairflows.
Table1.Basicpropertiesofthetracegasanalyzersuite(allareThermoElectroninstruments)
InstrumentPrimaryOperationPrincipleResponseTime
(seconds)
DetectionLimit
(ppb)ZeroDrift
O3(49i)O3absorptionofultravioletradiation(240nm)200.5<1ppb
NO/NO2/NOX(42C,TraceLevel)ChemiluminescencefromtheO3NOreaction600.05Negligible
CO(48C,TraceLevel)COabsorptionofinfraredradiation(4.6µm)6040<0.1ppm
SO2(43i)Pulsedultravioletfluorescence602<1ppb
3.ResultsandDiscussions
3.1.Overallobservations
Approximatelyfiveweeksofdatawerecollectedandthetime
seriesispresentedinFigure3.Theforemostobservationisthatall
concentrations,exceptforthatofCO,werequitelowrelativeto
valuesreportedelsewhere.SO2measurementswereonthelow
endofthetypicalmixingratiosof1–20ppbinrural–suburban
environments,agreeingwithpastfindings(Finlayson–Pittsand
Pitts,2000).NO,NO2,andNOXaveraged0.6,12.2,and12.7ppb,
respectively,whileCOaveraged155ppb.TypicalO3mixingratios
insimilarenvironmentspeakat80–150ppb,butthehighest
mixingratioofO3observedinRichlandwas45ppb.
Table2givesthestatisticalsummaryofthecollecteddata.The
maximummixingratioofanygivenspecieswaslowerthantypical
mixingratiosinmanyotherpartsofthecountry,withminima
sometimesapproachingthedetectionlimitoftheinstruments
(Table1).O3,aswellasNOX,hadthehigherstandarddeviations
relativetotheirrespectivemeanvaluesascomparedtoSO2and
CO.TheminimumCOvalueislowerthanliteraturevaluesin
midlatitudesinthenorthernhemisphere.Forinstance,the
minimumCOobservedbyMOPITTis50ppbinsummer,although
thiswasobtainedatmuchhigheraltitudepressureof280hPa(El
Amraouietal.,2010).Ingeneral,thepressureatourobservation
siteinsummeris990hPa.However,theaverageCOvalueissimilar
tootherlocationsbetween4060°N,i.e.,105155ppb(Wang
etal.,2003).
Therewerefourepisodesofelevatedtracegasconcen
trations:July7,2007(Julianday188),July13,2007(Julianday
194.6–194.9),July26,2007(Julianday207.4–207.6),andAugust2,
2007(Julianday214.4–214.7).Thesewereperiodswhenmostof
thespeciesexhibitedarapidincreaseinmixingratioforatleasta
fewhours.O3reacheditshighestconcentrationof44.7ppbonJuly
13,2007,SO2reachedahighof14.3onAugust2,2007,andNO,
NO2,andNOXof21.2,34.6,and54.6ppb,respectively,onAugust
2,2007.Diurnalminimummixingratioswerealsohigherthan
normalduringthesetimes,including10ppbofO3onJuly6,2007
andnear5ppbofSO2onJuly7,2007.Duetolackofwindspeed
andwinddirectiondataduringJulianday188,onlythreeoutofthe
fourepisodeswerestudiedinmoredetail.Thesearehighlightedin
thetimeseries(Figure3),i.e.EpisodesI,II,andIII.
Figure3depictsthetemporalvariationsofthetracegas
speciesandmainmeteorologicalparametersobservedduringthe
deployment.Changesinthemixingratioswerefrequently
associatedwithchangesinphotochemistry.Therelationship
betweentemperatureandO3hasbeenwellestablished,namely,
heatacceleratingthechemicalreactionsintheatmosphereresults
inhigherozoneconcentrations(ClarkandKarl,1982;Jacob,1993).
Threeepisodeswithelevatedconcentrationswerenotedin
chronologicalorderoverperiodsofapproximately1day(identified
inFigure3).Inmostepisodes,therewasaslowincreasein
concentrationofallspeciestoapeakonthedayonwhichthe
episodeisdefined,whereupontheconcentrationsdecreasedand
anothercyclestarted.ThescatterplotbetweenhourlyaverageO3
vs.GSWisillustratedinFigure4.Thesolidlineisthelinearleast–
squaresfit.
92Mioduszewskietal.AtmosphericPollutionResearch2(2011)8998
Figure3.Timeseriesofalltracegases,solarradiation(GSW),relativehumidity(RH),andtemperature(°C)overtheentiresamplingperiod(timeisinJulian
Days).Threeepisodesofelevatedtracegasconcentrationsaredenoted(I,II,andIII)intheO3plot.Superimposedaretheaveragehourly
valuesofeachtracegasspecies.Relativehumiditymeasurementswereinterruptedperiodicallyduetoinstrumentproblems.
Table2.Statisticsencompassingtheentireperiodforallspecies,allinppb.
Maximaandminimastatisticsrepresentoneminutevalues,whilethe
averageandstandarddeviationstatisticswerederivedfromvalues
averagedeveryhour
SpeciesMin.(ppb)Max.(ppb)Avg.(ppb)Std.Dev.(ppb)
O30.144.715.45.2
NO021.20.60.5
NO2036.712.24.2
NOx0.254.612.74.7
CO35.7327.915517.8
SO20.714.44.90.4
3.2.Temporalvariation
Diurnalpatternswereobservedinthetimeseriesalthough
therewerenotableexceptions.DiurnalvariationsinO3,NO,NO2,
andNOXweredistinct(Figure3),withminimumconcentrations
oftenapproachingzero.Photo–oxidationofprecursorgases,like
carbonmonoxide,isprimarilyresponsibleforthedailyriseinO3
(Nairetal.,2002).Providedthereisasufficientamountof
NO/NOX,theO3willpeakeachdayintheearlyafternoonwitha
correspondingdipinnitrogenoxides(Ghudeetal.,2006).The
diurnalvariationofO3andNOXisshowninFigure5,withNOX
reachingitspeakaround6am(PDT)andO3reachingabroader
peakbetween1pmand3pm.O3productionduringthedayis
drivenbythephotochemicalreactionbetweenhydroxylradicals,
organicperoxyradicals,andNO,whileitisremovedatnightby
depositionanddestructionbyalkenesandNO(Gerasopoulos,
2006).TheconversionofNOtoNO2byO3duringthenightisthe
primaryreactionthatincreasesNO2atnight,withthereverse
occurringduringthedaytoincreaseO3anddecreaseNO2(Mazzeo
etal.,2005).
Figure4.AscatterplotofhourlyaverageO3vs.hourlyaveragesolar
radiation(GSW).Thesolidlineisthelinearleastsquaresfit.
Althoughthedetailsofthesynopticpatternvariedfrom
episodetoepisode,thereweredistinctsimilarities.Strongridging
waspresentat500mbduringEpisodesIandIIthatgavewayto
relativelystrongcoldfronts,astheridgeaxisprogressedeastward
andlowpressureapproachedfromthenorthwest.Theupperlevel
featuresforthelattertwoepisodeswerelessamplifiedwitha
morezonalflow,butacoldfronttrailingasurfacelowpressure
systemtothenorthstillmovedthroughthearea(HPC,2007).
Winddirectionsvariedandhadminimalinfluenceonpollutant
Mioduszewskietal.AtmosphericPollutionResearch2(2011)899893
concentrations.Instead,thepresenceofastagnantairmass
appearedtocontributethemosttoepisodesofhightracegas
concentrations,agreeingwithpastobservationsthathighO3is
bestcorrelatedwithlightwindsunderhighpressure(Vukovich,
1995).
Figure5.ThehourlyaverageofNOX,CO,O3,andSO2mixingratios,andsolar
radiationduringtheentiresamplingtime.Thestandarddeviationsare
plottedaserrorbars.
3.3.Pollutanttransport
NOAA’sHYSPLITmodelisoftenusedtocomputeair
trajectoriesatdifferentlevelsoftheatmosphere.Ifairpollutants
canbeassumedtotravelwiththemeanairflow,thentheir
trajectoriescanbecalculatedusingameteorologicalmodelthat
describesairmotionatdifferentlevelsoftheatmosphere.Figure6
showsbackwardairtrajectoriesproducedbyHYSPLITduringthree
episodesofelevatedtracegasconcentrations.Thetrajectories
usedGDAS1modeldataona1degreelatitudelongitudespatial
resolution,andusedGDAS1verticalvelocitytomodelvertical
motion(DraxlerandRolph,2003).
ThesecondarywindroseofO3asafunctionofwinddirection
isshowninFigure7.PanelIdepictsEpisodeIwhenthetrace
gases,particularlyO3,registeredhigh.Windwasclearlyfromthe
southeastandsouthduringthistime,whichisalsothelocationof
themostlikelylocalpollutionsources.Thelargerandmore
industrialcitiesofPascoandKennewicklietentofifteenmilesto
theeastandsoutheast(seeFigure1),whilenearbytothesouth
aremajorroads,suchasHighway240,thataccommodate
considerabletrafficattimes.Thesearealllikelylocalsourcesfor
thisparticularepisodeofelevatedtracegases.Windwas
predominantlyfromthenorthandnorthwestduringEpisodesII
andIIIwheretherearemainlyopenlandsandlackofpollution
pointsources(Figure1).Thewindspeedwasmuchweakerduring
theseepisodesowingtotheanticyclonenearby,andmuchofthe
pollutionwaslikelyduetothestagnantairmasspresentinboth
episodes,asdiscussedpreviously(Vukovich,1995).
Therearetwotrajectoriesforeachepisode,whichare
centeredthreehoursaroundthehourofthehighestmixingratios.
Windroseswerecalculatedforthesametimetodetermineif
therewasaclearsourcefortheincreaseintheobservedtracegas
concentration(seeFigure7).Thewinddataandbacktrajectories
agreereasonablywellwitheachotherconsideringHYSPLITdoes
notmodeltherelativelyturbulentboundarylayer(Draxlerand
Hess,1998).Thedominantwinddirectionwassomewhatdifferent
ineachepisode,rangingfromsouthtonorthwestandnorth.The
southerlywindontheeveningofJuly13duringEpisodeIcould
havebroughtinpollutantsprimarilyfromtrafficfromtheTri–cities
(particularlyGeorgeWashingtonWay;seeFigure1)while
pollutantsfromthenorthandnorthwestonJuly26andAugust2
(Julianday207and214)duringEpisodesIIandIIIrespectively
couldhavebeennearbyroadssuchasHighway240andStevens
Drive,whicharetheothertwomainnorth–southroadsin
Richland.
TimeseriesofO3andSO2duringthethreeO3episodeswere
plottedinFigure8.OnlyinEpisodeIdidO3andSO2peakatthe
sametime,whichindicatedthataplumewastransportedfromthe
southandcausedelevatedO3attheobservationsite.During
EpisodesIIandIII,therisingofO3concentrationdidnotcoincide
withthatofSO2.ThisindicatedthatO3wasfromadifferentsource
andpossiblymainlycausedbylocaltraffic.
3.4.Ozoneobservationsandcomparison
ProductionofO3canbeaffectedbyNOX,VOCreactivity,and
freeradicalproduction(WalcekandYuan,1995).NOXplaysa
criticalroleinthephotochemicalformationofO3,andhasbeen
foundtobealimitingfactorintheatmosphereatruralandremote
locations(FinlaysonPittsandPitts,2000).Theprincipleformation
ofozoneisbythereactionofatomicoxygen(O)anddiatomic
oxygen(O2).Inthetroposphere,themajorsourceofatomic
oxygenisfromthephotochemicalcycleinvolvingNO,NO2,and
photolysis.ToolittleNOX,forexample,resultsin“NOXsensitive”O3
chemistry,wheretheamountofO3thatcanbeproducedislimited
bytheamountofNOXavailabletoreact(Kleinmanetal.,2005).
SinceVOCmeasurementswerenotavailableonsite,itwasnot
possibletoinvestigatethechemistrybetweenVOCsandO3/NOX.
However,theanalysisofNOXandO3wasconductedwiththe
understandingthatO3productionwasinfluencedbyNOX
concentration.
94Mioduszewskietal.AtmosphericPollutionResearch2(2011)8998

Figure6.12hourbackwardtrajectoriesofairovertheregionusingHYSPLIT,startingatIa)15:00h13July2007,Ib)21:00h14July2007,IIa)06:00h26July
2007,IIb)10:00h26July2007,IIIa)04:00h1August2007,andIIIb)10:00h1August2007(alltimesinPDT).TheGDAS1modelisusedforextrapolation,
beginningatheightsof500m,1000m,and2000mabovetheground.
Figure7.ToparewindrosesdisplayingsurfacewindspeedanddirectionforEpisodesI,II,andIII.Bottomarewindroses
displayingsurfacewinddirectionandozoneconcentrationforthesameepisodes.
Mioduszewskietal.AtmosphericPollutionResearch2(2011)899895
Figure8.TimeseriesofO3andSO2duringthethreeepisodes.Bluediamond
isSO2,reddiamondisO3.
ThescatterplotsofO3vs.NOXandOxvs.NOXareshownin
Figure9.ThetoptwopanelsdepictthehourlyaverageofO3vs.
NOXandOxvs.NOXfortheentiresamplingperiod.O3increased
withdecreasingNOXconcentration.Theoxidantconcentration
(OX),where[OX]=[O3]+[NO2],isoftenusedindeterminingthe
dominantchannelforNO2formationinaparticularenvironment
(Itanoetal.,2007).AnincreaseintheOXconcentrationswas
observedwhichimpliestheoccurrenceoftheradicalchannelfor
theformationofNO2.Itisworthmentioningthatintheenviron
mentofhighNOXemissions,positivebiascanbeintroducedonthe
OXconcentration.TheNO2toNOX(NOX=NO2+NO)ratioconverges
at0.9duringbothepisodes,whichindicates90%ambientNOXas
theprimaryNO2concentration.
Theobservedoxidantconcentrations(OX)canbeinterpreted
intermsofthesumofaNOX–independent“regional”contribution
(i.e.,theO3background)andalinearlyNOX–dependent“local”
contribution(ClappandJenkin,2001;Jenkin,2004a;Jenkin,
2004b).Thesolidlinesarelinearregressionfitsinthetoptwo
panels.TheslopeandinterceptforO3vs.NOXare–0.61±0.05and
21.45±0.82(r2=0.88),respectively.TheslopeandinterceptforOX
vs.NOXare0.39±0.05and21.45±0.82(r2=0.75),respectively.Our
regional(i.e.NOX–independent)contributiontooxidantis21.4
ppb,muchlowercomparedtothosederivedat35ppbaveraged
frommultiplesitesinJulyandAugustintheUK(ClappandJenkin,
2001).Thelocal(i.e.NOX–dependent)sourceofOXinRichlandis
muchhigherthanthoseinthesamestudybyClappandJenkin
(2001).Forexample,theoxidantslopesforJulyandAugustinthis
UKstudyare0.1,whereasourslopeis0.4.Thisindicatesthat
theregionalbackgroundofoxidantinRichlandisfairlylow.Clapp
andJenkin(2001)alsoshowedthatthelocalNOX–dependent
oxidantcontributionhasremarkablylittlevariationwithseason,
i.e.10%ofNOXlevelthroughouttheyear.Therefore,the
observationmadeinthesummercouldbequiteusefulin
estimatingthelocaloxidantamountforothertimesoftheyearin
Richland.
OneofthemostimportantlocalNOX–dependentcontri
butionsisroadtrafficexhaust.Thisisprobablythemostimportant
sourceofOXinRichland.Anothersourceoflocaloxidantcomes
fromNOreactionwithoxygentoformNO2,whichisdependenton
NOconcentration.ThismaynotbeasignificantsourceinRichland,
sincetheNOconcentrationremainedfairlylow(i.e.avgerage0.6
ppb)throughtheentiresamplingtime.Sunlight–initiatedfree
radicalcatalyzeddegradationofVOCinthepresenceofNOXleads
totheoxidationofNOtoNO2.Thisdependsonthephotolysisrates
ofradicalformationandchainlengthofNO2formation.
UnfortunatelyVOCandphotolysisrateswerenotmeasured,sono
furtherconclusioncanbedrawnfromtheothertwopotential
sourcesoflocaloxidants.
SeveralfactorsmayexplainwhyO3mixingratiosremained
lowinRichland.Rapidfreeradicalproductionislikelytoconsume
muchoftheO3duetothehighsolarfluxobservedinRichland
duringthesummer.Solarflux,measuredasshortwaveradiationin
W/m2,wasplottedwithO3mixingratios,relativehumidity,and
temperature(Figure3).Watervaporenhancestheremovalrateof
freeradicalproduction,particularlyinlow–NOXenvironments,so
thelackofwatervaporinRichlandasrepresentedbylowrelative
humiditysupportstheaforementionedfreeradicalhypothesis
(WalcekandYuan,1995).Thehourlyaveragesolarflux,O3,NOX,
CO,andSO2areplottedinFigure5.Ithasbeendemonstratedthat
O3andsolarradiationarerelated(VukovichandSherwell,2003).
Thehighozonedaysgenerallyconcurwithhighsolarradiation
measurementsonthesurface.Highradiationusuallyresultsin
highersurfacetemperatures.Itisnotsurprisingtoobserveaweak
positivecorrelationbetweensolarradiationandozone,asthe
linearleast–squaresfitproducesaslopeof0.0083±0.0006and
interceptof12.6±0.3withr2=0.18.(Figure4).Summersolar
radiationinRichlandisgreaterthaninmuchofthecountrydueto
lackofcloudcover(NCDC,2008),andthiscouldhavefacilitated
freeradicalproduction.Ontheotherhand,ozonecanbeformed
anddestroyedbyfreeradicals,suchashydroxylorperoxyradicals,
formedfromphotolysis.Pastcalculationsindicatedthatozone
reductionispossibleinmostareaswhentheUVradiationinthe
troposphereincreases,whichgiveschangesinthedissociationrate
forozoneyieldingradicalssuchas(O1D).Thisincreasein
photodissociationinducestropospherichydroxylradicals.While
thelevelsofhydroxylradicalsandhydrogenperoxideincrease,the
levelsoftroposphericozonearegenerallyreduced(Fuglestvedet
al.,1994).Sincethephotolysisrateswerenotmeasured,quantifi
cationofthiseffectisprohibited.
EPAusesthefourthhighestdaily8–houraverageO3
concentrationsmeasuredwithinanareaovereachyeartosetup
thenationalambientairqualitystandards(EPA,1998).Ozonecon
centrationsinRichland(metropolitanareapopulationof200000)
werecomparedtothoseinLosAngeles,CA(16million),Seattle
(3.5million)andSpokane,WA(400000),andMission,OR(town
populationof1000)in2007(USCBb,2008).Spokanereporteda
fourthmax8–hourO3valueof64ppb,Seattlereported46ppb,
andvalueswerecommonlyover100ppbintheLosAngelesarea
(EPA,2008).Missionisonly54milestothesouth–southeastof
RichlandandistheonlyotherEPAtracegasobservingstationin
thelowerColumbiaBasin.Thefourthmax8–hourO3valueat
Missionwas57ppb.Bycontrast,eventhehighest8–houraverage
96Mioduszewskietal.AtmosphericPollutionResearch2(2011)8998
Figure9.ScatterplotsofO3vs.NOxandOxvs.NOx.ThetwotoppanelsdepicthourlyaverageO3vs.NOxandOxvs.NOx,respectively.Thesolidlinesarelinear
leastsquaresfits.ThebottomthreepanelsareO3vs.NOxandOxvs.NOxusing10minaverageddataduringepisodesI,II,andIII,respectively.
inRichlandwaswellbelow40ppb.Theozoneconcentrationin
RichlandislowercomparedwithotherlocationsalongthePacific
region,wheretheaverageO3valueintheozonegrowingseason
(MaythroughSeptember)rangesfrom19–58ppbin1995and20–
65ppbin1996.Comparedwiththefewlocationswithozone
monitoringinthestateofWashington(WA),theaverageozonein
Richlandisabout5ppblower,i.e.,19–21ppbforotherstationsin
1995,and20–25ppbin1996inWA.Specifically,comparableto
valuesobservedinClassIairsheds,suchastheMountRainier
NationalPark(MOR),theaverageozoneconcentrationinRichland
(e.g.15ppb)issimilartothatinMOR(e.g.17.5ppb)inJulyin
2007.Otherruralareas,suchasGrandCanyonNationalPark(52
ppb),havehigheraverageozoneconcentrationinthesamemonth
thaninRichland(NPS,2010).
EventhoughRichlandandMissionareingeographically–
similarlocations,O3mixingratiosinMissionweremuchhigher
thanRichland.Althoughwecannotdefinitelyestablishan
explanationforthehighervaluesinMission,wewouldnotethatit
iseightkilometersdirectlyeastofamajoragriculturalexchange
Mioduszewskietal.AtmosphericPollutionResearch2(2011)899897
community(Pendleton,OR).Thereforeitisnotinconceivablethat
therichNOXandVOCsmixtureassociatedwithtruckstopstothe
westmaybeasourceofthehigherO3reportedatthissite.In
addition,bothPendletonandMissionlieontheUmatillaRiver,
whichcanactasanaturalcorridordownwhichpollutantsreadily
travel.Consequently,MissionlikelyreceivesmuchofitsO3by
advectionfromthewest,whereasRichland’sO3isprimarily
generatedin–situwhenthereislittleairmotion.Elevationis
similarbetweenthesetwolocations.Theaverageelevationin
Pendletonis300365mabovesealevel,andtheelevationin
Missionis370mabovesealevel.Therefore,theeffectofaltitude
onsolarfluxisinsignificantbetweenthesetwolocations(Dvorkin
andSteinberger,1999).WhilethedatafromRichlandcover5
weeks,thissamplingperiodcorrespondstoatimeoftheyear
whenO3typicallyreachesitshighestlevels.GiventhelevelsofO3
duringtheentiresamplingperiodatRichland,itisclearthat
photochemicalO3isnotthesameprobleminRichlandasinalarge
urbanarealikeLosAngeles,andthatRichlandisoneofthecleaner
sitesinthePacificNorthwestregion.
4.Conclusions
Thisworkprovidesapracticalexampleinintegrating
instrumentsandapplyingthemtoin–situmeasurements.
Operatingandmaintainingtheinstrumentsforanextended
amountoftimeinthefieldisausefultestwhichservestobolster
confidenceintheirabilitytocollectqualitydata.Moreover,the
datacollectedprovideusefulcharacteristicsoftracegasesinthe
underrepresentednon–urbanenvironment.Thisisofparticular
interesttopollutantstudiesonRichlandbecauseoftheanticipated
growthofthearea.Furthermore,theverylowmixingratiosof
manyofthetracegasspeciesmaybecomeatopicofinterestinthe
futureifpollutantscontinuetoincreaseinthisnon–urbanarea.
Acknowledgements
ThisworkwassupportedbytheOfficeofScienceand
EngineeringEducationandtheAtmosphericScienceandGlobal
ChangeDivisionatthePacificNorthwestNationalLaboratory,
DepartmentofEnergy.JohnMioduszewskiwouldliketothank
KarenWiedaofPNNL’sScienceUndergraduateLaboratory
Internshipprogramforherfinancialsupportoftheinternshipfor
JohnMioduszewski.SupportwasalsofromtheOfficeofScience
(BER),U.S.DepartmentofEnergy,undertheauspicesofthe
AtmosphericScienceProgram,underContractsDE–AC05–
76RL01830atthePacificNorthwestNationalLaboratory.
SupportingMaterialAvailable
Informationon“Gasanalyzerintegrationmethodology”,A
schematicdiagramoftheCR–23XMicrologger’sconnectionstothe
tracegasanalyzers(FigureS1),Aschematicdiagramofthewiring
connectionsbetweenthedataloggerandspecificpinsonthe
terminalblocksofeachinstrument(FigureS2).Thisinformationis
availablefreeofchargeviatheInternetathttp://www.
atmospolres.com.
References
Atkinson,R.,2000.AtmosphericchemistryofVOCsandNOX.Atmospheric
Environment34,20632101.
C.S.DataloggerSupportSoftware,2002.http://www.campbellsci.com.au/
documents/lit/b_loggernet21.pdf.
Clark,T.L.,Karl,T.R.,1982.Applicationofprognosticmeteorological
variablestoforecastsofdailymaximumonehourozone
concentrationsinthenortheasternUnitedStates.JournalofApplied
Meteorology21,16621671.
Clapp,L.J.,Jenkin,M.E.,2001.Analysisoftherelationshipbetweenambient
levelsofO3,NO2andNOasafunctionofNOXintheUK.Atmospheric
Environment35,63916405.
Cohen,A.,2007.Seattleareagrew7.2%in6years,butTriCitiespopulation
up17.8%.SeattlePostIntelligencer.http://seattlepi.nwsource.com/
local/310361_census05.html.
Dvorkin,A.Y.,Steinberger,E.H.,1999.Modelingthealtitudeeffectonsolar
uvradiation.SolarEnergy65,181187.
Draxler,R.R.,Rolph,G.D,2003.HYSPLIT(HYbridSingleParticleLagrangian
IntegratedTrajectory)ModelaccessviaNOAAARLREADYWebsite,
http://www.arl.noaa.gov/ready/hysplit4.html.NOAAAirResources
Laboratory,SilverSpring,MD.
Draxler,R.R.,Hess,G.D.,1998.AnoverviewoftheHYSPLIT_4modelling
systemfortrajectories,dispersion,anddeposition.Australian
MeteorologicalMagazine47,295308.
ElAmraoui,L.,Attie,J.L.,Semane,N.,Claeyman,M.,Peuch,V.H.,Warner,
J.,Ricaud,P.,Cammas,J.P.,Piacentini,A.,Josse,B.,Cariolle,D.,
Massart,S.,Bencherif,H.,2010.Midlatitudestratosphere
troposphereexchangeasdiagnosedbyMLSO3andMOPITTCO
assimilatedfields.AtmosphericChemistryandPhysics10,21752194.
EPA’sAirDataBase,2008.http://www.epa.gov/air/data.
EPA,2009.TransferStandardsforCalibrationofAirMonitoringAnalyzers
forOzone.Technicalassistancedocument,November2010.www.epa.
gov/ttnamti1/files/ambient.
EPA(EnvironmentalProtectionAgency),1998.Guidelineondatahandling
conventionsforthe8hourozoneNAAQS.http://www.epa.gov/
ttncaaa1/t1/meta/m25245.html.
FinlaysonPitts,B.J.,Pitts,J.N.,2000.ChemistryoftheUpperandLower
Atmosphere:Theory,Experiments,andApplications,AcademicPress.
SanDiego,pp.583585.
Fuglestved,J.S.,Jonson,J.E.,Isaksen,I.S.A.,1994.Effectsofreductionsin
stratosphericozoneontroposphericchemistrythroughchangesin
photolysisrates.TellusB46,172192.
Gerasopoulos,E.,Kouvarakis,G.,Vrekoussis,M.,Donoussis,C.,
Mihalopoulos,N.,Kanakidou,M.,2006.Photochemicalozone
productionintheeasternMediterranean.AtmosphericEnvironment
40,30573069.
Ghude,S.D.,Jain,S.L.,Arya,B.C.,Kulkarni,P.S.,Kumar,A.,Ahmed,N.,2006.
TemporalandspatialvariabilityofsurfaceozoneatDelhiand
Antarctica.InternationalJournalofClimatology26,22272242.
HPC(HydrometeorologicalPredictionCenter),2007.Dailyweathermaps.
http://www.hpc.ncep.noaa.gov/dailywxmap/.
Itano,Y.,Bandow,H.,Takenaka,N.,Saitoh,Y.,Asayama,A.,Fukuyama,J.,
2007.ImpactofNOXreductiononlongtermozonetrendsinanurban
atmosphere.ScienceoftheTotalEnvironment379,4655.
Jacob,D.J.,Logan,J.A.,Gardner,G.M.,Yevich,R.M.,Spivakovsky,C.M.,
Wofsy,S.C.,Sillman,S.,Prather,M.J.,1993.Factorsregulatingozone
overtheUnitedStatesanditsexporttotheglobalatmosphere.Journal
ofGeophysicalResearchAtmospheres98,1481714826.
Jenkin,M.E.,2004a.Analysisofsourcesandpartitioningofoxidantinthe
UKPartI:theNOXdependenceofannualmeanconcentrationsof
nitrogendioxideandozone.AtmosphericEnvironment38,51175129.
Jenkin,M.E.,2004b.Analysisofsourcesandpartitioningofoxidantinthe
UKPartII:contributionsofnitrogendioxideemissionsand
backgroundozoneatakerbsidelocationinLondon.Atmospheric
Environment38,51315138.
Kleinman,L.I.,2005.Thedependenceoftroposphericozoneproduction
rateonozoneprecursors.AtmosphericEnvironment39,575586.
Mazzeo,N.A.,Venegas,L.E.,Choren,H.,2005.AnalysisofNO,NO2,O3and
NOxconcentrationsmeasuredatagreenareaofBuenosAiresCity
duringwintertime.AtmosphericEnvironment39,30553068.
Nair,P.R.,Chand,D.,Lal,S.,Modh,K.S.,Naja,M.,Parameswaran,K.,
Ravindran,S.,Venkataramani,S.,2002.Temporalvariationsinsurface
ozoneatThumba(8.6°N,77°E)atropicalcoastalsiteinIndia.
AtmosphericEnvironment36,603610.
NCDC(NationalClimaticDataCenter),2008.ClimateMapsoftheUnited
States.http://cdo.ncdc.noaa.gov/climaps/skyc5007.pdf.
98Mioduszewskietal.AtmosphericPollutionResearch2(2011)8998
NationalParkService(NPS),2010.OzonemonitoringoverviewOzone
pollutantmonitoringinthenationalparks.http://www.nature.nps.
gov/air/monitoring/network.cfm.
Platt,U.,1999.Modernmethodsofthemeasurementofatmospherictrace
gases.PhysicalChemistryChemicalPhysics1,54095415.
Seinfeld,J.H.,2004.Airpollution:ahalfcenturyofprogress.AIChEJournal
50,10961108.
USCBa(UnitedStatesCensusBureau),2008.http://www.census.gov/
population/www/estimates/metroarea.html.
USCBb(UnitedStatesCensusBureau),2008.http://factfinder.census.gov.
Vukovich,F.M.,Sherwell,J.,2003.Anexaminationoftherelationship
betweencertainmeteorologicalparametersandsurfaceozone
variationsintheBaltimoreWashingtoncorridor.Atmospheric
Environment37,971981.
Vukovich,F.M.,1995.Regionalscaleboundarylayerozonevariationsinthe
easternUnitedStatesandtheirassociationwithmeteorological
variations.AtmosphericEnvironment29,22592273.
Walcek,C.J.,Yuan,H.H.,1995.Calculatedinfluenceoftemperaturerelated
factorsonozoneformationratesinthelowertroposphere.Journalof
AppliedMeteorology34,10561069.
Wang,Y.,Ridley,B.,Fried,A.,Cantrell,C.,Davis,D.,Chen,G.,Snow,J.,
Heikes,B.,Talbot,R.,Dibb,J.,Flocke,F.,Weinheimer,A.,Blake,N.,
Blake,D.,Shetter,R.,Lefer,B.,Atlas,E.,Coffey,M.,Walega,J.,Wert,
B.,2003.Springtimephotochemistryatnorthernmidandhigh
latitudes.JournalofGeophysicalResearchAtmospheres108,art.no.
8358.
WashingtonStateDepartmentofTransportation(WSDOT),2010.WSDOT
GeodataDistributionCatalog.http://www.wsdot.wa.gov/mapsdata/
geodatacatalog/.

Supplementary resource (1)

... However, O 3 levels have fluctuated year to year in other parts of India and worldwide ( Table 1). The concentrations of O 3 measured in this site are comparable to those reported in Richland, USA (Mioduszewski et al., 2011) and many cities in Malaysia (Awang et al., 2015). Compared to sites from China, Saudi Arabia and Indian sites Agra, Udaipur, Kanpur, Anantapur, Kannur, and Delhi, Bengaluru's concentration is low (Hassan et al., 2013;Nishanth et al., 2012;Rama Gopal et al., 2014;Tiwari et al., 2015;Tong et al., 2017;Verma et al., 2018;Xu et al., 2011;Yadav et al., 2016). ...
... The annual mean of NO X at Bengaluru is 46.64 ppbv during observation years 2015-2018, with a minimum of 7.30 ppbv to a maximum of 121.53 ppbv. The NO X concentration was comparable to that seen in a city in Ningbo, China (Tong et al., 2017), while it was higher than that observed in Kannur, Anantapur, Kanpur, Richland (USA), and Agia Marina (Cyprus) (Gaur et al., 2014;Kleanthous et al., 2014;Mioduszewski et al., 2011;Nishanth et al., 2012;Rama Gopal et al., 2014). The levels of nitrogen oxides in Bengaluru are high compared to other cities, which might be attributed to the city's rapid economic growth, industrialisation, and transportation in supporting IT and its associated industries domestically (Yang et al., 2020). ...
Article
Full-text available
Bengaluru, also considered India’s Silicon Valley, has seen steady growth in population over the years. Bengaluru’s rapid development has resulted in dwindling reservoirs, increased traffic congestion, high levels of air pollution, and, to some measure, a rise in summer temperatures. As a result of these changes in urban form over the last decade, anthropogenic heat fluxes for ozone production have increased. However, an observational study on the effects of growing urbanisation on trace gases in Bengaluru for various seasons and periods of the day is missing. Hence, in situ measurements of O3, NO, NO2, and NOX concentrations were carried out at Bengaluru, India, from January 2015 to December 2018. The data were examined for diurnal and interannual variations in trace gas mixing concentrations. The diurnal trend in O3 exhibits unimodal behaviour. Changes in photochemistry, local meteorology, and the planetary boundary layer’s distinctive features cause a rise in the value of concentrations and lead to a peak. In contrast, the diurnal trend in NO, NO2, and NOX displayed a bimodal peak due to the combined effect of vehicular emissions and the planetary boundary layer. The link involving the oxidant OX (O3 + NO2) and NOx levels were investigated to determine the NOx-independent regional and NOx-dependent local contributions to OX in the atmosphere. Daytime contributions are higher than night-time contributions, according to the present study. The observed anomalies could be the consequence of photochemical processes that produce OX.
... Use of the quadrant method for 24 h PM 2.5 data could improve the application of this method over a larger spatial extent in rural and remote areas, such as National Parks and Wilderness Pierce et al. Atmospheric Environment 196 (2019) [103][104][105][106][107][108][109][110][111][112][113][114][115][116][117] Areas where conditions influencing atmospheric pollution are not well quantified (Fine et al., 2015b;Mioduszewski et al., 2011). Use of the quadrant method to characterize concentrations of gases (e.g. ...
Article
A new statistical method, the quadrant method, was used to aid in identifying different conditions affecting the relationship between columnar aerosol optical depth (τext) and surface concentrations of particulate matter (<2.5 μg m⁻³ in aerodynamic diameter, PM2.5). The main goal of this study was to identify air pollution sources and atmospheric processes affecting gradients of atmospheric pollutants observed at two valley sites (∼1370 m) and a high elevation site (2515 m) located in and adjacent to Reno, Nevada, USA. The two valley sites were used to investigate the horizontal gradient of pollutants associated with mobile sources from high volume highways. Results indicated statistically significant differences in concentrations of criteria air pollutants between the two valley sites, located 0.03 km and >1 km from major highways. Vertical gradients were impacted by air pollution sources, including local and long-range transport, and atmospheric boundary layer stability. During periods when τext and surface PM2.5 concentrations were associated (i.e. both increase), emissions from wildfires and local pollutants in a well-mixed boundary layer dominated the relationship. During periods of no association, stable boundary layer conditions and pollution aloft created vertical heterogeneity of PM2.5 concentrations. Results showed that the quadrant method, developed for hourly data, can be used with 24 h PM2.5 and gaseous data and that it is a useful tool for identifying air pollution sources and atmospheric physics driving pollution gradients.
Article
In this study, temporal variations of surface ozone (O 3) were investigated at tropical urban site of Hyderabad during the year 2009. O 3 , oxides of nitrogen (NO x ¼ NO þ NO 2), black carbon (BC), and meteorological parameters were continuously monitored at the established air monitoring station. Results revealed the production of surface O 3 from NO 2 through photochemical oxidation. Averaged datasets illustrated the variations in ground-level concentrations of these air pollutants along different time scales. Maximum mean concentrations of O 3 (56.75 ppbv) and NO x (8.9 ppbv) were observed in summer. Diurnal-seasonal changes in surface O 3 and NO x concentrations were explicated with complex atmospheric chemistry, boundary layer dynamics, and local meteorology. In addition, nocturnal chemistry of NO x played a decisive role in the formation of O 3 during day time. Mean BC mass concentration in winter (10.92 mg m À3) was high during morning hours. Heterogeneous chemistry of BC on O 3 destruction and NO x formation was elucidated. Apart from these local observations, long-range trans-port of trace gases and BC aerosols were evidenced from air mass back trajectories. Further, statistical modeling was performed to predict O 3 using multi-linear regression method, which resulted in 91% of the overall variance.
Article
Full-text available
Continuous measurements of surface ozone (O3), NOx (NO + NO2) and meteorological parameters have been made in Kannur (11.9 °N, 75.4 °E, 5 masl), India from November 2009 to October 2010. It was observed that O3 and NOx showed distinct diurnal and seasonal variabilities at this site. The annual average diurnal profile of O3 showed a peak of (30.3±10.4) ppbv in the late afternoon and a minimum of (3.2±0.7) ppbv in the early morning. The maximum value of O3 mixing ratio was observed in winter (44±3.1) ppbv and minimum during monsoon (18.46±3.5) ppbv. The rate of production of O3 was found to be higher in December (10.1 ppbv/h) and lower in July (1.8 ppbv/h) during the time interval 0800–1000 h. A correlation coefficient of 0.52 for the relationship between O3 and [NO2]/[NO] reveals the role of NO2 photolysis that generates O3 at this site. The correlation between O3 and meteorological parameters indicate the influence of seasonal changes on O3 production. Investigations were further extended to explore the week day weekend variations in O3 mixing ratio at an urban site reveals the enhancement of O3. The variations of O3 mixing ratio with seasonal air mass flows were elucidated with the aid of backward air trajectories. This study also indicates how vapor phase organic species present in the ambient air at this location may influence the complex chemistry involving (VOCs) that enhances the production of O3 at this location
Article
Full-text available
Using an atmospheric chemical reaction mechanism applied to air parcels near the Earth`s surface, the sensitivities of ozone (O3) formation rates are quantified for changes in four meteorologically controlled parameters: temperature, sunlight intensity, water vapor mixing ratio, and isoprene concentration. Over a wide range of NO(x) and anthropogenic hydrocarbon concentrations, enhanced photolysis rates and elevated isoprene concentrations are calculated to be the most important factors contributing to increased O3 formation rates in warmer days. These results suggest that the most uncertain yet important meteorological factor controlling regional-scale O3 formation is fractional cloudiness and its impact on photolysis rates.
Article
Full-text available
This paper presents a complete characterization of a very deep stratospheric intrusion which occurred over the British Isles on 15 August 2007. The signature of this event is diagnosed using ozonesonde measurements over Lerwick, UK (60.14° N, 1.19° W) and is also well characterized using meteorological analyses from the global operational weather prediction model of Météo-France, ARPEGE. Modelled as well as assimilated fields of both ozone (O3) and carbon monoxide (CO) have been used in order to better document this event. The paper also presents a demonstration of the capability of O3 and CO assimilated fields to better describe a stratosphere-troposphere exchange (STE) event in comparison with the free run modelled O3 and CO fields. O3 and CO from Aura/MLS and Terra/MOPITT instruments, respectively, are assimilated into the three-dimensional chemical transport model MOCAGE of Météo-France using a variational 3-D-FGAT (First Guess at Appropriate Time) method within the MOCAGE-PALM assimilation system. The usefulness of assimilated MOPITT CO data in a STE study is demonstrated in this novel result. The study shows that the use of the model MOCAGE gives consistent 3-D fields capable of describing the synoptic evolution of the event. However, modelled O3 and CO vertical distributions do not provide a quantitative evaluation of the intrusion. Although the assimilation of MLS data improves the distribution of O3 above the tropopause compared to the free model run, it is not sufficient to reproduce the stratospheric intrusion event well. Conversely, assimilated MOPITT CO allows a better description of the stratospheric intrusion event. Indeed, the horizontal distribution of the CO assimilated field is consistent with meteorological analyses. Moreover, the vertical distribution of the CO assimilated field is in accordance with the potential vorticity distribution and reveals a deeper intrusion from the lower stratosphere downward to the mid-troposphere compared to the O3 assimilated field. This study clearly demonstrates the capability of the assimilation of MOPITT CO to improve the CO distribution in the upper troposphere and lower stratosphere region. In addition, the behaviour of CO assimilated field is consistent with the synoptic evolution of the meteorological conditions. Therefore, the results of this study open the perspectives for using MOPITT CO in the STE studies.
Article
Full-text available
Physical and chemical properties of the atmosphere at 0-8 km were measured during the Tropospheric Ozone Production about the Spring Equinox (TOPSE) experiments from February to May 2000 at mid (40°-60°N) and high latitudes (60°-80°N). The observations were analyzed using a diel steady state box model to examine HOx and O3 photochemistry during the spring transition period. The radical chemistry is driven primarily by photolysis of O3 and the subsequent reaction of O(1D) and H2O, the rate of which increases rapidly during spring. Unlike in other tropospheric experiments, observed H2O2 concentrations are a factor of 2-10 lower than those simulated by the model. The required scavenging timescale to reconcile the model overestimates shows a rapid seasonal decrease down to 0.5-1 day in May, which cannot be explained by known mechanisms. This loss of H2O2 implies a large loss of HOx resulting in decreases in O3 production (10-20%) and OH concentrations (20-30%). Photolysis of CH2O, either transported into the region or produced by unknown chemical pathways, appears to provide a significant HOx source at 6-8 km at high latitudes. The rapid increase of in situ O3 production in spring is fueled by concurrent increases of the primary HOx production and NO concentrations. Long-lived reactive nitrogen species continue to accumulate at mid and high latitudes in spring. There is a net loss of NOx to HNO3 and PAN throughout the spring, suggesting that these long-term NOx reservoirs do not provide a net source for NOx in the region. In situ O3 chemical loss is dominated by the reaction of O3 and HO2, and not that of O(1D) and H2O. At midlatitudes, there is net in situ chemical production of O3 from February to May. The lower free troposphere (1-4 km) is a region of significant net O3 production. The net production peaks in April coinciding with the observed peak of column O3 (0-8 km). The net in situ O3 production at midlatitudes can explain much of the observed column O3 increase, although it alone cannot explain the observed April maximum. In contrast, there is a net in situ O3 loss from February to April at high latitudes. Only in May is the in situ O3 production larger than loss. The observed continuous increase of column O3 at high latitudes throughout the spring is due to transport from other tropospheric regions or the stratosphere not in situ photochemistry.
Article
The observed reductions in stratospheric ozone since the late 1970s are likely to have affected the penetration of UV radiation into the troposphere. We have examined the sensitivity and the response of the tropospheric chemistry to such changes in UV radiation. Based on observations of ozone column densities and model calculations of changes in the ozone column densities after 1970, photodissociation rates for selected years (1970, 1980, 1990, 2000 and 2050) are calculated. These calculations give significant changes in the dissociation rates of some gases, particularly in the dissociation rate for O 3 yielding O( 1 D). This increase in photodissociation rates initiates increases in tropospheric OH. However, the model studies show that the OH changes are somewhat damped compared to the changes in short wave radiation due to strong interactions between key species in the troposphere. Ozone is reduced in most areas when the UV radiation increases, but the percentage reductions in ozone are significantly smaller than the percentage UV increases. However, during spring, O 3 increases in regions where NO x is enhanced. The calculations give increased levels of H 2 O 2 , although the magnitude of the response varies considerably with time of year and with region, and they are largest at high latitudes during spring. The relative changes in methane are found to be less than the relative changes in global average of OH since the largest relative OH changes take place outside the region of most importance for the methane oxidation (low latitudes and low altitudes). In addition, the effect is delayed in accordance with the chemical lifetime of methane (∼ 10 years). The results indicate that increased fluxes of UV due to reduced ozone columns may have contributed to the reduction in the growth rate of methane, and the magnitude of this effect is estimated to ∼ 1 3 ̅ of the reduction. It is therefore unlikely that changes in UV fluxes is the main cause of the reduction in the growth rate of methane which has been observed during the 1980s. The mechanism constitutes a negative indirect chemical effect on climate change from the ozone depleting substances, mainly the CFCs. DOI: 10.1034/j.1600-0889.1992.t01-3-00001.x-i1
Article
Fifteen years of ozone data from the United States Environmental Protection Agency's (EPA) Aerometric Information Retrieval System (AIRS) and surface and upper air meteorological data from National Weather Service (NWS) stations were used to determine the meteorological conditions in the Baltimore–Washington corridor area that are important in characterizing ozone variations. Three data sets were used in this study: the initial 15-year data set; a subset of the complete 15-year data set that was a 15-year summer data set; and another subset of the complete 15-year data set that only included those days when the daily maximum ozone concentration (DMOC) was greater than or equal to 100 ppb (DMOC⩾100 ppb). The results from this study indicated that the meteorological terms that affect ozone in the Baltimore–Washington corridor were compartmentalized; that is, the results were dependent on which data set was used in the study. When the entire 15-year data set was considered, the meteorological parameters that influenced ozone variations were temperature and dewpoint. The principal meteorological term, when only the 15-year short-term variations (i.e., variations with periods less than 30 days) of ozone were considered, was sky cover. When the 15-year summer data set was considered, the principal meteorological terms involved in the variation of ozone were temperature and sky cover; and when the data set in which the limitation DMOC⩾100 ppb was used, the principal meteorological terms were surface wind speed and sky cover. The results from this study indicated that high temperatures and large concentrations of water vapor are a necessary, but not a sufficient, condition for high ozone to be found in the Baltimore–Washington corridor. The sufficiency condition is satisfied when significant amounts of solar radiation reach and when stagnation conditions prevail in the surface layer at the same time.
Article
Surface measurements of ozone and meteorological parameters are made at a tropical coastal site, Thumba (8.6°N, 77°E, 2m) in India from April 1997 to March 1998. Ozone shows a diurnal variation with daytime higher levels and a sharp change in its values during evening time. The evening time change in ozone values with a secondary peak is found to be due to change in wind pattern from sea-breeze to land-breeze at this site. This secondary peak in ozone is weakest during monsoon period. A detailed study of the meteorological parameters shows that during nighttime, polluted air from land side moves to the nearby marine region relatively increasing the levels of ozone and precursor gases. Observations show that the onset time of daytime ozone increase and its rates are related with each other. If onset time of ozone increase is early, its increase rate is slower and vice versa. Maximum ozone levels are observed to be during March, probably due to intense photochemical production. However, this is different when compared to other Indian site like Ahmedabad, where maximum ozone levels are observed during late autumn and early winter. Monthly average ozone levels are observed to be very low (in the range of 13–22ppbv) at Thumba.
Article
Measurements of trace gas concentrations and other quantities are a crucial tool for the investigation of the processes in the atmosphere. At the same time the determination of atmospheric trace gas concentrations constitutes a technological challenge, since extreme sensitivity (some species have to be detected at mixing ratios as low as 10-13) is desired simultaneously with high specificity, i.e. the molecule of interest usually must be detected in the presence of a large excess of other species. To date no single measurement technique can, even nearly, fulfil the above and other requirements for trace gas measurements in the atmosphere. Therefore a comprehensive arsenal of techniques has been developed. Besides a large number of special techniques (like the chemiluminescence-detection of NO) universal methods gain interest, due to their relative simplicity—a single instrument can register a large number of trace species. The different types of requirements and the various techniques are discussed, special emphasis is given to spectroscopic methods, which are a successful and promising variety, that plays a large and growing role in atmospheric chemistry research. For instance only spectroscopic methods allow remote sensing of trace gas concentrations, e.g. from satellite platforms. Today many varieties of spectroscopic methods are in use (e.g. tunable diode laser spectroscopy or Fourier transform spectroscopy), the basic properties and recent applications of this technique are presented by the example of differential optical absorption spectroscopy (DOAS). Future requirements and expected developments are discussed.
Article
A simple numerical model that describes the altitude effect of solar UV flux under cloud-free conditions was developed and tested. The model computes the direct and diffuse UV irradiances for the wavelength range 290–385 nm, at any sub-polar location and time (restricted to arid areas). The input parameters include extraterrestrial solar irradiance, ozone content and vertical distribution, aerosol amounts and size distribution, SO2 and NO2 contents, surface albedo and solar zenith angle. Model results were compared with measurements made in the tropical Chilean Andes for altitudes up to 5500 m above sea level. The model and data show good agreement. For the measured direct component a linear increase with altitude was assumed, whereas model results, computed up to 15 km altitude, exhibit a non-linear behavior. However, in the lowest few kilometers a linear regression was adequate for both model and measurements. As for the diffuse component, the variation with altitude strongly depends on wavelength and solar zenith angle. At short wavelengths and large solar zenith angles, a pronounced maximum occurs at a level which depends on these parameters. The maximum cannot be observed when integrating over the UV-A range. This behavior can be understood by taking into account the sources of the diffuse flux at any given level in the atmosphere.