JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 103, NO. D23, PAGES 31,045-31,056, DECEMBER 20, 1998 Seasonalcourse of isoprene emissionsfrom a midlatitude deciduous forest Allen H. Goldstein Divisionof Ecosystem Sciences, Department of Environmental Science,PolicyandManagement, Universityof California,Berkeley MichaelL. Goulden, 1J. WilliamMunger,andStevenC. Wofsy Department of EarthandPlanetary Sciences, Divisionof Engineering andAppliedSciences, HarvardUniversity Cambridge,Massachusetts ChristopherD. Geron NationalRiskManagement Research Laboratory, U.S. Environmental Protection Agency,Research Triangle Park, North Carolina Abstract. Continuous measurements of wholecanopyisopreneemissions overan entire growingseasonarereportedfromHarvardForest(42ø32'N,72ø11'W). Emissionswere calculated fromtheratioof observed CO2 flux andgradient multipliedby theobserved hydrocarbon gradients.In summer1995,24-houraverageemissions of isoprene fromJune1 through October 31were32.7x 101ø molecules cm-2s-1(mgC m-2h-I = 2.8x 10• molecules cm-2s-•),andthemeanmidday mixingratiowas4.4ppbvat24 m. Isoprene emissions werezeroatnight,increased through themorning withincreasing airtemperature andlight,reached a peakin theafternoon between thepeaksin airtemperature andlight,and thendeclined withlight. Isoprene emissions wereobserved overa shorter seasonal period thanphotosynthetic carbonuptake.Isoprene emission wasnotdetected fromyoungleaves andreached a peakrate(normalized forresponse to measured lightandtemperature conditions) 4 weeksafterleafoutand2 weeksafteremissions began.The normalized emission rateremained constant forapproximately 65 days,thendecreased steadily through September andintoOctober. Totalisoprene emissions overthegrowingseason (42 kg C ha-1 yr-l)wereequalto2%oftheannual netuptake ofcarbon bytheforest.Measured isoprene emissions werehigherthantheBiogenic Emission Inventory System-IImodelby at least 40%atmiddayandshowed distinctly differentdiurnalandseasonal emission patterns. Seasonal adjustment factors(in additionto thelightandtemperature factors)shouldbe incorporated intofutureempiricalmodelsof isoprene emissions. Comparison of measured isoprene emissions withestimates of anthropogenic volatileorganic compound emissions suggests thatisoprene is moreimportant for ozoneproduction in muchof Massachusetts on hotsummerdayswhenthe highestozoneeventsoccur. modeling studieshave shown that ozone productionin the northeasternUnited States is quite sensitive to biogenic Emission of isoprene (2-methyl-l,3-butadiene)by NMHC emissions[McKeen et al., 1991; Roselieet al., 1991; terrestrialvegetationprovidesthe dominantinputof reactive Sillman et al., 1990] and that the uncertainty in those non-methane hydrocarbons (NMHC) to the atmosphere and emissionsintroduces large uncertainty into predictions of 1. Introduction influences tropospheric chemistry onbothregionalandglobal emissionsintroduceslarge uncertaintyinto predictionsof scales[Zimmerman,1979; Chameideset al., 1988; Winer et reductionsthat could be achievedthroughNMHC or NOx al., 1989; Singhand Zimmerman,1992; Fehsenfeldet al., emissioncontrolstrategies.Hirsch et al. [1996] found that 1992]. Isopreneis principallyremovedfromthe troposphere seasonalityof ozone productionefficiencyper unit NOx throughoxidationby hydroxylradicals,andin thepresence of determined fromthe HarvardForestdatawastightlycoupled oxidesof nitrogen(NOx = NO + NO2) is closelycoupledto to seasonality of isoprene emissions. Furthermore, the photochemicalproduction of ozone. Photochemical meteorological conditionsthat causethe highestisoprene INow at EarthSystemScience,Universityof California,Irvine. Copyright1998by theAmericanGeophysicalUnion. Papernumber98JD02708. 0148-0227/98/98JD-02708509.00 mixing ratios (hot, sunny,and stable)also maximize ozone production. Isopreneproductionis closely linked to photosynthetic processes[Shatkey et al., 1991], and control over its production is coupledto isoprenesynthase activity[Monson et al., 1992]. Shatkeyand Singsaas[1995] haveshownthat isoprene emission increases the thermaltoleranceof plants, 31,045 31,046 GOLDSTEIN ET AL.: SEASONAL COURSE OF ISOPRENE EMISSIONS and suggestthat protectionfrom heat may be the primary reasonplantsemit isoprene. Isopreneemissionfrom vegetationhasbeenmeasuredin natural environmentsusing branch, leaf, and whole tree enclosure[Zimmerman, 1979; Lamb et al., 1985; Lamb et al., 1986; Khalil and Rasmussen, 1992; Monson et al., 1994; Pier, 1995], tracer release[Lamb et al., 1986], mixed layer and surfacelayer micrometeorlogical techniques[Knoerr and Mowry, 1981; Lamb et al., 1985; Baldocchiet al., 1995, Guentheret al., 1996a, b, c], and in controlledlaboratory settings[Sanadze,1969; Tingey et al., 1979; Monson and Fall, 1989; Guentheret al., 1991]. Isopreneemissionrates were observedto dependon both light and temperatureand were zero at night. Studies of individual leaves showed isopreneemissionsto be linearly dependenton the flux of photosynthetically activeradiation(PAR) to a saturation point of approximately1000 gE m-2 s-l, and exponentially dependenton temperatureup to approximately35øC, where emissionsstartto level off and eventuallydeclinenear 40øC. However,Shatkeyet al. [1996] foundthat isopreneemission Boston, Massachusetts, and 100 km northeastof Hartford, Connecticut. There is a highway • 5 km to the north and a secondary road• 2 km to thewest. The siteis accessible by a dirt road, which is closed to public vehicle traffic. Measurements weremadefrom a 30 m tower,erectedin May 1989, extending7 m abovethe forest canopy. Instruments were housedin a temperaturecontrolledshacklocated15 m east of the tower. The forestis 50 to 70 yearsold with a deciduousleaf area indexof 3.5 (measured in 1994by leaf littercollectionby M. Goulden(unpublisheddata, 1994). The tree speciesin descending order of abundanceare oak (mostlyred), red maple,red pine,hemlock,birch,whitepine,andcherrywith percent basal areas (stem cross-sectionalarea at 1.37 m determined fromplot surveys(M. Gouldenunpublished data, 1994)of 36.4,21.8, 16.2,15.6,3.5, 2.9, and2.3, respectively. The terrainis moderatelyhilly (relief • 30 m), but thereis no evidenceof anomalous flow patterns thatwouldmakeeddyflux measurements at this siteunrepresentative [Mooreet al., 1996], and measurements of the local energybudgetare fromoaktreesisnotfullylightsaturated at 1000•E m-2s-1 balancedto 20% [Gouldenet al., 1996a]. underfield conditions. Isopreneemissionratesalso depend Measurements of C2-C6NMHCs weremadein air sampled on leaf age. Measurementson aspenleaves[Monsonet al., simultaneously from2 and7 m abovetheforestcanopyevery 1994] haveshownthat onsetof emissionsbeginsaftera given number of growing days above 5øC, increases for approximately3 weeks,holds steadyfor approximately8-10 weeks, and decreases thereafter. Similar results were observedusing leaf enclosures[Fuentes et al., 1995] and whole tree enclosures[Pier, 1995]. Models of troposphericchemistry and photochemical ozone production require accurate estimatesof biogenic isoprene emissions. Currently, the U.S. Environmental Protection Agency uses inventories calculated from the BiogenicEmissionInventory SystemII (BEIS2) [Geron et al., 1994]. Thesemodelscalculateemissionsusingdatabases of foresttype or speciescomposition,biomassdensity,basal emission rate (species dependent), and the responseof isopreneemissionto temperatureand PAR from Guentheret al. [1993]. Leaf temperatureand PAR are derived from ambientconditionsabovethe ecosystem, anda canopymodel is used to estimate their distribution at five vertical levels in 45 min, commencingJuly 22, 1992 [Goldsteinet al., 1995a, b, 1996]. Othertracegasmixingratiosand meteorological conditionshavebeenmeasuredcontinuously at this sitesince 1990,including CO,CO2,03,NOx,NOy(NO+ NO2+ NO3 + N205 + HNO3 + peroxyacetylnitrate + other organic nitrates+ organicaerosols),H20, rainfall,wind speed,wind direction,temperature, radiation,and eddy covariancefluxes of sensible heat,latentheat,03, NOy,andCO2[Woj•yet al., 1993, Mungeret al., 1996, 1998; Moore et al., 1996; Goulden et al., 1996a,b]. 2.2. Flux-Gradient Similarity Calculation We usea similarityapproachfor determiningisopreneflux for a whole forestecosystem, basedon other quantitiesfor which we have both mixing ratio data and direct measurements of flux [Goldsteinet al., 1996]. The tracegas flux (F) is assumedto be proportionalto the time-averaged the canopy. Two scenariosare used: (1) leaf temperatureis assumed to equalabovecanopyair temperature (BEIS2), (2) leaf temperatureis estimatedusingthe energybalancemodel of Lamb et al. [1993] (BEIS2E). The model is designedto simulatemidsummeremissionsand assumesthat, for a given ecosystem,emissionrates vary only with temperatureand PAR. The modeldoesnot includediurnalor seasonalchanges mixing ratio gradient (dC/dz) above the forest for intervals longerthanthe timescalefor the slowestsignificantturbulent events(10 min): canopyisopreneemissionsover an entiregrowingseason. [Baldocchiet al., 1995], in agreementwith our afternoon values.In this study,we computeK usingmeasurements of CO2 flux andgradientandtakethe productof thisK with the isoprenegradientto determinethe isopreneflux (Figure1). F=K dC/dz, ( 1) whereK is the exchange coefficientfor the averaginginterval. In 1993 we determinedK simultaneouslyfrom fluxes and verticalgradientsof CO2 and H20 at this site [Goldsteinet in the basal emission factors. al., 1996]. CO2 has a sourceat the groundand a sink in the In orderto quantifywhole ecosystemisopreneemissions, canopy,while H20 and isopreneare both emitted from the determinethe response to temperature,light, andphenology, canopy;thusCO2 is not strictlysimilarto theseotherscalars. assessregionalsignificance,and test the accuracyof current KCO2was 20% lower than K H20 in the afternoon(1200biogenic emission models, we built and deployed an 1800),andwas 20% higherearly in the day (0600 - 0900) automatedsystemto continuouslymeasureisoprenefluxes and late in the day (1900-2100). Theoretical calculations and relevant environmental variables which control them. In suggest thatK for isopreneandH20 shouldbe equal,butthat this paper we presenta nearly continuousrecord of whole KCO2 should be 20% lower over a deciduous forest 2. Experiment 2.1. Site We chose to use KCO2 becausewe did not have routine Harvard Forest is located in Petersham, Massachusetts measurements for H20 or temperature gradients.Our choice (42ø32'N, 72ø11'W; elevation 340 m), 100 km west of of K may introducea systematicunderestimationof the GOLDSTEIN ET AL.' SEASONAL COURSE OF ISOPRENE EMISSIONS •o 31,047 o •• 0 O• 0 o •, o ,o • • • o I o o oo o o o o oO Cb o o o o øo o ! o o o o o o i o od o 6 o o , , 182 183 , o 184 185 186 187 Day of Year 1995 Figure 1. Isoprenemixingratioat 24 m, isoprenegradient,CO2 gradient,CO2 flux, andisopreneflux (July 1 to 6, 1995). isopreneflux in the afternoonof up to 20%; additionally,we may overestimatefluxesin the morningand eveningby up to 20% thoughthe fluxes are small at thesetimes of day. The seasonalcycleof isopreneemissionsis presentedin this paper asmiddaymeanflux valuesfrom 1000 to 1500, duringwhich time the mean systematicunderestimateof the flux may be roughly 12% basedon comparisonof K from H20 and CO2 during this time of day. These systematicerrorsare smaller than the overall uncertaintyin the individual hydrocarbon flux measurementsand should not affect the long-term precision of the measurementsor modify the observed seasonalcycle, which is the primary contributionof this study.The coefficientof variation(standarddeviation/flux) for individual isopreneflux measurementsduring typical daytime summer conditionsis 28% and is mostly due to uncertainties in quantifyingthe smallgradientsof CO2 above the forest (for detailed discussionof the error analysissee Goldsteinet al., [ 1996].). 3. Measurements The analyticalsystemfor automatedin situ measurements of hydrocarbon mixing ratios and gradients has been describedin detail elsewhere[Goldsteinet al., 1995a]; thus only a brief descriptionwill be given here. Recovery of isoprenein the initial instrumentconfigurationwas low dueto losson the innersurfacesof stainlesssteeltubing.The lossof isoprenewas eliminatedin May 1995 by replacingall 1/16 inch stainless steel tubing in the sampling and preconcentration systemwith stainlesssteeltubing lined with fusedsilica(Silcosteel). Air wasdrawncontinuouslyfrom two inlets(24 and29 m). Samplesfor analysiswere extractedfrom the inlet lines and passedthrough glass cold traps at-20øC and Ascarite II (Thomas Scientific) traps to remove H20, 03, and CO2. Samples werecryogenically preconcentrated on dualtraps(40 mL min-] of air for 10 minutesonto fused silica lined 1/16 31,048 GOLDSTEIN ET AL ßSEASONAL COURSE OF ISOPRENE EMISSIONS inch OD stainlesssteeltube, Silcosteel),and injectedinto a gas chromatograph with dual flame ionizationdetectors (HewlettPackard5890 seriesII). Chromatographic separation was accomplished using30 m PLOT GS-AluminaMegabore capillary columns(J+W Scientific). Every fifth pair of sampleswas taken from the same altitude (29 m) by switchinga valve nearthe inlet of the 24 m samplingline in order to determinethe null for the observedmixing ratio gradient. The measurement system could operate continuously andunattendedfor 2 weeks,althoughdatawere normallydownloadedat 6 day intervals. Mixing ratios for most hydrocarbonswere determinedusing relative response factors[Ackman,1964, 1968; Dietz, 1967] referencedto an intemal neohexanestandard(Scott-Martin,National Institute of Standardsand Technology(NIST) traceable+ 2%) added to every samplenear the sampleinlet by dynamicdilution. Responsefactorsfor isoprenewere determinedfrom dynamic dilutionof isoprenestandards(Scott-Martin,NIST traceable+ 2%) addedto ambientair samplesnearthe sampleinlet at the top of the tower and nearthe instrumentat the bottomof the towerperiodicallyfrom May to November1995. The analyticalsystemwascheckedfor contamination daily by runningzero-airblanks. In addition,the Teflon sampling tubeswerecheckedfor contamination andmemoryeffectsby introducingzero-airat the sampleinletson top of the tower. No contaminationor memory effects were detected for isoprene,andtherewas no detectablelossof isoprenein the Teflon samplingtubes. The accuracyof the isoprenemeasurements was estimated to be +8%, based on the cumulative uncertaintyof the isoprenestandard,measurements of standardadditionflows, and the integrityof isoprenein the samplingand analysis process.Measurementprecisionwas approximately3% at 1 ppbv,5% at 0.5 ppbv, 10% at 0.2 ppbv,and20% for mixing ratios less than 0.1 ppbv, as determinedby the variance between measurements taken from the samelevel everyfifth injection.The detectionlimit wasapproximately 0.01 ppbv. 4. Effects of Isoprene Source Spatial Heterogeneity An inherent weakness in the gradient approach for quantifyingisoprenefluxesis that the lowersamplingintake has a differenteffective footprintthan the upper sampling intake. If the isoprenesource from the forest canopy is heterogeneous, this differencein footprintsfor the sample intakes could bias the measured fluxes. To determine whether isopreneemissionwas heterogeneous, we examinedwhether fluxes varied with wind direction from the tower. We calculateda normalizedemissionrate as measured/(modeled usingBEIS2E), effectivelyremovingthe influenceof light and temperature from the emission measurements,as represented by the model. Data were parsedinto four wind quadrants (0o-90ø (NE), 90ø-180 ø (SE), 180ø-270 ø (SW), and 270ø-360ø (NW)) and the mean normalized emissionrates were compared.The mean midday(1000 - 1500 EST, June 15 to August31) measuredflux was 35% higher than the model. The meannormalizedflux from the SW, NW, and NE wind quadrants agreedwithin & 6%. The SE wind quadrant was 20% lower than the mean of the other three wind quadrants(NE 1.29, SE 1.16, SW 1.39, NW 1.42). The percentageof data from eachquadrantwas 10%, 18%, 45%, and 28%, respectively.This comparisonof normalizedflux by wind quadrantsuggeststhat systematicisopreneflux errorsdueto spatialheterogeneity of isoprenesourcesat our siteareunlikelyto be higherthan20% andare probablyless than 10%. 5. Results and Discussion 5.1. IsopreneAmbient Mixing Ratios Isoprenemixing ratioshad a diurnal cycle with maximum mixingratiosin the afternoon,andminimummixingratiosat night (Figure 1). The meansummerdaytimemixing ratio at 24 m was4.4 ppbv(averagedfrom 1200 to 1600 EST, days 170-250);middaymixingratiosexceeded15 ppbvon 3 days. Mixing ratio gradients of CO2 were measured The daytimeisoprene mixingratioat 29 m wastypically25% simultaneouslywith the hydrocarbongradientsusing a lower than the 24 m mixing ratio. Summerdaytimenull differentialinfraredgas analyzer (LICOR 6251), with air gradientmeasurements showedexcellentagreementbetween from 29 m passedthroughthe referencecell and air from 24 the parallelmeasurement channelswith a meanratio of 1.007 m throughthe samplecell. Water vapor was removedfrom & 0.023 (standarddeviation). Nighttimemixingratiosvaried the air samplesusing nation dryers,and the sampleswere with atmospheric stabilityandthe previousday's emissions. assumedto be at a commontemperaturebeforeanalyzingfor On windy nightsisoprenemixing ratioswere usuallybelow CO2. The null gradientwas measuredafter everysampling the instrument detectionlimit (< 10 pptv). On stablenights period by passingair from 29 metersthroughboth cells. that followeddayswith significantemissions, mixingratios Instrumentgain was determinedby sequentialstandard weretypicallybetween0.1 and2 ppbvanddecreased slowly additionof CO2 to the sampleandthenthe referenceair. The until isopreneemissionsresumedin the morning.Therewas standarddeviationsof the zero gradientmeasurements were no observablegradientfrom 24 to 29 m duringthe stable determinedby comparingthe null gradientmeasuredevery nights(e.g. night of day 184-185), indicatingthat nighttime fifth samplingperiod(whenhydrocarbon null gradientswere isoprene losswasduemainlyto chemicalreactions (probably determined)to the zero measurement directlyfollowingthat with ozoneor nitrate)ratherthan directdeposition to the period. The standarddeviationin the zero measurements for forest. CO2 (0.18 ppm) was • 20% of the meanmiddaygradients(The seasonal coursesof isoprenemixing ratio (24 m), 0.9 ppmCO2). Flux determinations werenot attemptedwhen carbondioxideflux, percentPAR intercepted by the canopy observedgradientswere very small, i.e., within 1 standard (measured from fixed platformsat 30 and 15 m, aboveand deviation of zero. TheCO2 fluxesandgradients, andall the NMHC measurements are reportedas mole fractionsrelative to dry air at a commontemperature,avoidingthe need for densitycorrections dueto gradients in temperature or H20 [Webbet al., 1980]. belowthecanopy), andairtemperature areshownin Figure2 asmiddaymeanvalues(1000to 1500EST). Percentof PAR intercepted indicates the changein leaf densityin the forest, and increased from lessthan 40% as the leavesbeganto emerge(day 140) to 90% when the canopywas fully GOLDSTEINET AL.' SEASONALCOURSEOF ISOPRENEEMISSIONS 31,049 o o' ( o , , o 0 o e o ooo o c) c) 150 200 25O 300 Day of Year 1995 Figure 2. Isoprenemixing ratio at 24 m, CO2 flux, percentphotosynthetically active radiation(PAR) interceptedby the canopy,and air temperatureat 29 m (May to November1995, middaymeansfrom 1000 to 1500 EST). developed(approximatelyday 160). It remainedconstant decreaseas the leavesage, similar to observationsof aspen throughthe summeruntil the leavesbeganto senescearound leaves by Mortson et al. [1994]. Isoprene mixing ratios decreased rapidlyafter day 250, coincidingwith decreasedair day 240, and continuedto declineslowly asthe leavesfell off thetrees.CO2 uptakefolloweda similarpatternin thespring temperature,nighttime temperaturesfalling below 10 øC uptakeby the canopydeclining,and beginningaboutday 140 and reacheda maximum rate after regularly,photosynthetic beginning. day 160. Photosynthetic uptakedecreasedafter day 230 as leaf senescence the leavesbeganto senesce,and shut off completelyaround day 290. The first isopreneemissionsof the growingseason 5.2. Isoprene Emission Rates were detectedon day 152, when air temperatureexceeded Plate 1 showsisopreneemissionratesduring midsummer 25øC after two nights in a row with temperaturesremaining (days 165-230) as a function of both light and temperature above13øC. Isopreneemissionsdid not beginuntil the forest measuredabovethe canopyat 29 m. Isopreneemissionswere canopyhadreacheda maturestate,2 weeksafter leavesbegan not detectedduringperiodswith low light (PAR < 300 pE mto emerge and photosynthesishad begun. The seasonal 2 s-i) or air temperaturebelowapproximately13 øC.Emission changein isopreneemissionis not a functionof temperature rates increasedexponentiallywith temperatureand linearly and light alone. The processes that controlisopreneemission with PAR up to a saturationpoint of approximately1000 gE from oaks are apparentlynot active in young leaves and m-2 s-i, as has been observed in other studies. However, 31,050 GOLDSTEINET AL.' SEASONALCOURSEOF ISOPRENEEMISSIONS o o o o o 0 200 400 600 10 moleccm-2s-1 o o o - o o - 0 • 10 15 2o 25 3O Temperature(øC) Plate 1. Isopreneflux asa functionof lightandtemperature (June14 to August18, 1995). has a similar compositionto Harvard Forest maximumemissionsdid not necessarilyoccursimultaneously Massachusetts with maximumtemperatureor maximumPAR. On average, (80% is probably more accurate, based on oak tree isopreneemissions were zero at night,beganafter sunrise, distributionsin the databaseof Geron et al. [1994]), our increased throughthe morningwith increasingair temperature resultssuggestthat 105 metric tons yr-I of isopreneare and PAR, reacheda peak in the afternoonbetween the emitted from Massachusetts forests. The National Acid Program(NAPAP)[1985] estimates maxima in air temperatureand PAR, and declined with PrecipitationAssessment decreasing PAR towardthe end of the day (Figure3). The that 1.1 x 105 metric tons of volatile organiccarbon(VOC) sourcesduringthe summerin meanisopreneemissionoverthe wholegrowingseason(24 are emittedfrom anthropogenic hour mean from June to October 1995, calculated by Massachusetts.Thus, on the averageday from Junethrough integrating themean diurnal flux(Figure 3))was32.7x 10iø October,biogenicisopreneemissionsareapproximatelyequal moleculescm-2s-i, giving an annualemissionrate of 48 kg to total anthropogenicVOC emissions;however, on hot isoprene ha-I yr-1,with emissions occurring mainlyfrommid- summerafternoonswhen the highestozone episodesoccur, isopreneemissions increasedramatically.For example,mean Junethroughmid-September. aroundmidday(PAR > 1000 pE m-2 Previousabove canopyisopreneflux studiesfrom a wide isopreneemissions cm-2s-1at 20,25, variety of ecosystems in the United Statesyield estimates were89, 176,and307x 1010molecules rangingfrom 30 to 300 x 1010 moleculescm-2 s-I when and 30 + 2 øC, respectively. At 30 øC, isopreneemission standardized to air temperatures of 30øC and abovecanopy rates are approximately 9 times the 24 hour average PAR of 1000pE m-2s-I [Guenther et al., 1996a,b,c;Lambet summertimeemissionrate. In addition,isopreneis estimated al., 1985;Baldocchiet al., 1995;summarized in Geronet al, to be 2.5 times as effective for photochemicalozone 1997]. Our measurements are nearthe high end of these productionper atom of carbonas the typical mix of VOCs values (307x 1010molecules cm-2 s-1at30+ 2 øCwithPAR foundin urbanair [NationalResearchCouncil(NRC), 1991]. > 1000 gE m-2 s-i) and are in reasonable agreement with Assuming that anthropogenic VOC emissions are those at sites with similar oak abundance. substantially less temperature dependent than biogenic isopreneemissions, our measurements suggestthat isopreneis 5.3. Regional Significanceof Isoprene Emissions more importantthan anthropogenic VOCs for photochemical Redoak is the dominantisoprene-emitting plantat Harvard ozone production on hot summer days in much of Forest and in Massachusetts. If we assume that all of Massachusetts (outsideof the largesturbanareas). GOLDSTEIN ET AL.' SEASONAL COURSE OF ISOPRENEEMISSIONS Isoprene Flux 31,051 o o Temp ......PAR .//• iiII1•'•'•'••.••I• : \ / o o -- 0 -- 0 0 O0 \\ III ', -o ø - \\ _•. \ \ - o -- o 0 - o < \ \ \ O -- I / .- - •-'" 0 , / 5 10 15 20 Hour of Day Figure3. Meandiurnalcycleof isopreneflux (+ standard error)alongwith temperature at 29 m andincident photosynthetically activeradiation(PAR) (June1 to October31, 1995). Data wereparsedinto 2-hourtime windows. 6. Comparison to Net EcosystemProduction carbonby a mixtureof plantsthatdo not all releaseisoprene, and this fraction is certainly higher for plants that emit The percent of gross carbon uptake returned to the atmosphereas isopreneis strongly temperaturedependent (Figure 4, calculatedas isopreneflux divided by gross ecosystemproductionduring summermidday periods). In HarvardForest,approximately1% of the grosscarbonuptake is releasedas isopreneat 25øC, and the percentageincreases with temperature.Thesemeasurements reflectthe uptakeof isoprene. Annualisopreneemissions (42 kg C ha-1yr-1)equal2% of the net carbonuptakeat HarvardForest(2200 kg C ha-1yr-1, fiveyearmeanvalue[Goulden et al., 1996b]).Thepercentage of photosynthesized carbonthat is releasedas isoprenehas beenreportedin many studiesto be between0.1 and 3%, and occasionallyhigherfor leaf level measurements [Sharkeyet o o O- 15 20 25 Air Temperature (øC) Figure4. Percentgrosscarbonuptakereleased asisoprene asa functionof air temperature. 31,052 GOLDSTEIN ET AL.: SEASONAL COURSE OF ISOPRENE EMISSIONS to the environmentthat are not capturedby the al., 1996]. Isopreneemissions do not represent a major responses carbonlossfromthisecosystem but arepotentiallysignificant on a shortertime scaleduringhot summerdays. model. Figure5a showsan hourlymeanof the measurements and the model results for both model scenarios(BEIS2 and BEIS2E), and 5b showsthe normalizedemissionrate (using 6.1. Isoprene EmissionModel Scenarios BEIS2E) for summer 1995 (90% confidenceintervalsare The isopreneemissionmodelusedis BEIS2 as described indicated). A diurnalcourseof the normalizedemissionrate by Geronet al. [1994]. Isopreneemissionratesare assumed is apparent, increasingin the morning,maximizingaround to be 70 ggC (g-foliardry mass)-Ih-1 standardized for PAR values of 1000•tmolm-2s-•and30øCfortheoaks,and0.1 •tgC(g-foliardry mass)-•h-• for the otherspecies. Thisforest average basal emission factor (EF) was determinedby multiplyingthe fractionof oak and non-oakbasalareasby their corresponding EFs, yieldingan averageEF of 25 •tgC (g-foliardry mass)-•h-1. Sinceoakshavegreatercrownarea in proportionto basalarea comparedto other genera(e.g., birch, pine) this likely representsan underestimate of oak foliageon the orderof 5% [Geronet al., 1997]. The empiricalalgorithmsof Guentheret al. [1993] were usedto adjustemissionratesto ambientPAR andtemperature conditions.Exponential decay algorithms are applied to reducePAR and specificleaf weight at lower levelswithin forestcanopies[Geronet al., 1994]. The measured LAI of 3.5 was used in the model simulations. This model assumesthat leaf temperatures are equivalent to ambientair temperatures abovethe forestcanopy. Since leaf temperatures candiffer substantially from surrounding air temperature (especially in the upper canopy), the leaf temperatureenergybalanceof Gatesand Papian [ 1971] used by Lamb et al. [1993] and Geron et al. [1997] was also used to estimate leaf temperature in scenario BEIS2E. Vertical gradientsof humidity, wind speed, solar radiation, and air temperaturewere estimatedfrom measurements taken above the canopy by applyingthe profilesof Lambet al. [1993]. 6.2. Comparison With Models Measuredisopreneemissionswere 40% higher than the BEIS2E model and 100% higher than the BEIS2 model at midday and showeddistinctlydifferent diurnal and seasonal emissionpatterns.The currentoak basalemissionfactorof 70 •tgC g-1 h-• hasan estimateduncertaintyof + 50%. However, recentscalingstudiesat other siteshave suggestedthat rates of 100 [tgC g-1 h-1 or more may be more realistic[Guenther et al., 1996c; Lamb et al., 1996; Geron et al., 1997]. Indeed, at Harvard Forest, researchers using environmentally controlledleaf cuvettesystems(for methods,seeHarley et al. [1997] and Sharkeyet al. [1996]) measuredratesduringJuly 1995 and 1996 rangingfrom approximately70 to over 160 [tgC g-• h-• (C.D. Geron et al., manuscriptin preparation, 1998). Taken together, these results suggestthat a peak summeroak basalemissionrate of 100 [tgC g-• h-1 + 50% wouldbe moreappropriate for the model.Thesehigherbasal noon,anddecreasing in the afternoon(the normalizedratesat night, 2000 - 0500 hours, are not included in the figure because fluxes are zero for both the measurements and the model). Most likely, this apparentdiurnalcourseis due to underestimating leaf temperatureat high valuesof solarinput using the energy balancemodel [see Geron et al., 1997]. This wouldresultin the observedpatternfor diurnalchanges in the normalizedemissionrate and possiblyaccountsfor the BEIS2E model underestimates of midday fluxes. Alternatively, the isoprene emitting plants could have additional physiologicalfunctionsrelated to their diurnal cycleor incomingPAR that are not represented by the model, or the gradientflux methodcouldbe underestimating fluxes during the more stable periods in the morning and late afternoon.It is most importantfor the modelsto accurately predict isopreneemissionsduring midday, when rates are highest; thus the rest of our discussionwill focus on comparingmiddayemissionrates(1000-1500). Figures 6a and 6b show the seasonal course of the measuredand modeled isopreneemission rates, and the normalizedmidday emissionrate (1000-1500 EST, weekly mean valueswith 90% confidenceintervals). The seasonal courseof the normalizedemissionrate reachedits peak 4 weeksafterleaf out and2 weeksafteremissions began.From day 165 to 230 the normalizedrate remainedrelatively constant. The normalizedrate decreasedsteadilyafter day 230 as the leavessenesced,and essentiallywent to zero by day 300. The forestwas at its maximumisopreneemission potentialfor approximately65 days. The seasonalreduction in normalizedisopreneemissionafterday 230 coincidedwith seasonally decreasing air temperature and nighttime temperaturesfalling below 10 øC. The current model underpredictsemissionsduring most of the summer and overpredictsemissions in the spring and fall. These predictionscould lead to significanterrors in modeling photochemical03 productionand in assessing the need for legislationto regulateanthropogenicVOC emissions. The seasonal durationof strongisopreneemissionlastedonly 100 dayswith muchlower ratescontinuingfor approximately30 days,similarto theCO2 uptakepatternof theoaks[Basso•v, 1995], and shorterthan the approximately150 daysof active CO2 uptakebythewholeecosystem. Thisseasonal emission cycle needsto be includedin isopreneemissionmodelsto accuratelysimulateemissionrates. emission rates could account for the difference between the Figure 6b comparesthe seasonalchangesin normalized measuredandmodeledisoprenefluxes. midday emissionrate to an estimateof the leaf area index The diurnal and seasonalcyclesof the isopreneemission (LAI) at Harvard Forest (estimated from PAR measured rate are examinedby normalizingthe measuredisoprene abovethe canopyand at midcanopy,then scaledto summer emissionsto those calculatedwith the BEIS2 models (as maximumLAI measuredby leaf litter collection),and the describedabove). This normalizedemissionrate removesthe normalizeddifferencevegetationindex (NDVI, biweekly effectsof temperatureand PAR as representedby the model. compositeswith 1.1 km resolution,data for Harvard Forest If the normalized emission rate equals 1 then the extracted by K. MoorefromU.S. GeologicalSurveyNational measurements and model are in perfect agreement. MappingDivisionEROSdatacenter).TheNDVI composites Deviations from 1 indicate changesin the basal EF or can be usedto estimateseasonalvariationin leaf area index, GOLDSTEINET AL.' SEASONALCOURSEOF ISOPRENEEMISSIONS o o - 31,053 x x measured model(BEIS2E) model (BEIS) o x , •.. v 0 i•> - i i i 0 5 10 15 20 Hour of Day i I 10 15 20 Hour of Day Figure 5. Diurnalpatternof (a) measuredandmodeled(BEIS2 andBEIS2E; seetext for modeldescriptions) isopreneemissions, and(b) normalized(measured/modeled (BEIS2E)) isopreneemissions (June24 to August 28, 1995, hourlymeanvalueswith 90% confidenceintervals). chlorophyllcontent,and biomass[Moore et al., 1996]. The LAI and NDV! data have a seasonalpatternthat is notably consistent with the normalized midday emission rate. Isopreneis not emittedfor the first few weeksafter leafout (LAI < 1.5), then increaseswith increasingLAI and NDVI. Isopreneemissions diminishin the fall in a mannerconsistent with decreasingLAI and NDVI, but isopreneemissionsend beforethe leaveshave fallen from the trees (LAI < 1.5) and before photosynthesis has ceased. Our findings suggestthat seasonalchangesin isoprene emissionscould be modeled using NDVI data, or possibly by finer scale multispectral/temporal imagery,with minor adjustmentsfor emission initiation in the spring and cessationin the fall. Such metrics should be incorporatedinto future empirical modelsof isopreneemission. 7. Conclusions Whole canopy isoprene emissionswere measuredfrom Harvard Forest over the entire 1995 growing season. The seasonalduration of isoprene emissionswas substantially shorterthan net photosyntheticuptake. Comparisonof the measurementswith the EPA BEIS2E model gave a clear definitionof temporalchangesin the emissionrate which are not capturedby the model, and could be used to improve future models. Young leaves did not emit isoprenefor 2 weeks and did not reach their maximum rate for another 2 weeks. normalized The normalized emission emission rate remained constant for approximately 2 months, then decreasedsteadily through Septemberand October before emissionsceased. These seasonalchanges in isoprene emissionratesare importantfor two major reasons:(1) they dramaticallyaffect the regionalozone productionefficiency per NOx [seeHirsch et al., 1996] and are thus crucialfor the developmentof air quality control strategies,and (2) they provide constraints for understandingthe physiological mechanismof isopreneproduction. Current EPA models underestimateisoprene emissions at Harvard Forest in midsummerand overestimatein springand fall. The model underestimatesin midsummer are likely due to an 31,054 GOLDSTEIN ET AL.' SEASONAL COURSE OF ISOPRENE EMISSIONS o iA3 - x x o o measured o x model (BEIS2E) model (BEIS2) A ß o o • A'/ _ , AA X A A ß o ,O' A O , , O/ A o to X A o - o / A O x X - 'A O A' X i i i I 150 200 250 3OO Day of Year 1995 A • x o measured/BEIS2E A LAI + NDVI + i 150 Figure 6. i 200 Day of Year 1995 i i 250 300 Seasonalcourseof (a) measuredand modeled(BEIS2 and BEIS2E; see text for model descriptions) middayisoprene emissions (1000to 1500EST,weeklymeanvalues),and(b) normalized (measured/modeled (BEIS2E))midday isoprene emissions (with90%confidence intervals), andanindexof LAI and measurements of NDVI. underestimate in the basalemission rate.Futureempirical from anthropogenic sourcesin Massachusetts accordingto the modelsof isopreneemissionshouldincorporate seasonal NAPAP [1985] emissioninventory(1.1 x 105 metric tons). adjustmentfactors. Moreover,the importance of biogenicisopreneemissions The relativemagnitude of anthropogenic and biogenic increases dramaticallyon hot summerafternoons, coincident VOC emissions mustbe determined accurately to develop with periodsof peakphotochemical activity. In addition, usefulcleanair legislation for reducingtropospheric ozone. isoprene is approximately2.5 times as effective for In this study,isopreneemissionsfrom Massachusetts forests photochemical ozoneproduction per atomof carbonas the were estimatedto be 105 metric tons yr-1, with emissions typicalmix of VOCs foundin urbanair. Assuming that occurringmainly from mid-Junethroughmid-September.anthropogenic VOC emissionsare substantiallyless This is equivalentto the total summertimeVOC emissions temperature dependent thanbiogenicisoprene emissions, our GOLDSTEIN ET AL.: SEASONAL COURSE OF ISOPRENE EMISSIONS 31,055 Guenther, A.B., R.K. Monson, and R. Fall, Isoprene and monoterpene emission rate variability: Observations with eucalyptusandemissionrate algorithmdevelopment, d. Geophys. Res., 96, 10,799-10,808, 1991. Guenther,A.B., P.R. Zimmerman,P.C. Harley, R. Monson, and R. Acknowledgments.This work was supportedby grantsto Fall, Isopreneandmonoterpene emissionratevariability: Model HarvardUniversityfrom the U.S. Departmentof Energy's(DOE) evaluations and sensitivity analyses, d. Geophys, Res., 98, National Institute for Global Environmental Change (NIGEC) 12,609-12,617, 1993. through the NIGEC Northeast Regional Center at Harvard Guenther,A., P. Zimmerman,L. Klinger, J. Greenberg,C. Ennis, K. University(DOE CooperativeAgreementDE-FC03-90ER61010), Davis, W. Pollock, H. Westberg, E. Allwine, and C. Geron, by the NationalAeronauticsand SpaceAdministration(NAGWEstimatesof regional natural volatile organic compoundfluxes 3082), the NationalScienceFoundation(BSR-89-19300),the Long from enclosureand ambient measurements, d. Geophys,Res., results indicate that isoprene is more important than anthropogenic VOCs for photochemical ozoneproduction on hotsummerdaysin muchof Massachusetts. TermEcologicalResearch programat the HarvardForestfundedby the National ScienceFoundation(BSR-88-11764), and by Harvard University(HarvardForestandDivisionof AppliedSciences).The authorswish to thank David Fitzjarraldand KathleenMoore of the Atmospheric SciencesResearchCenterat the StateUniversityof New York at Albany for helpful discussions and for providing NDVI data. References Ackman, R. G., Fundamentalgroups in the responseof flame ionizationdetectorsto oxygenatedaliphatichydrocarbons, J. Gas Chromatog.,2, 173-179, 1964. Ackman,R. G., The flame ionizationdetector:Further commentson molecularbreakdownand fundamentalgroup responses,J. Gas Chromatog.,6, 497-501, 1968. Baldocchi,D., A. Guenther,P. Harley, L Klinger, P. Zimmerman,B. Lamb,andH. Westberg,The fluxesand air chemistryof isoprene above a deciduous hardwood forest, Philos. Trans. R. Soc. London.,Ser. ,4 350, 279-296, 1995. Bassow, S.L., Canopy photosynthesisand carbon cycling in a decidousforest:implicationsof speciescompositionand rising concentrations of CO2, Ph.D. thesis,Harvard Univ., Cambridge, Mass., 1995. Chameides,W., R. Lindsay,J. Richardsonand C. Kiang, The role of biogenichydrocarbons in urbanphotochemical smog:Atlanta as a casestudy,Science,241, 1473-1475, 1988. Dietz, W. A., Responsefactorsfor gas chromatographic analysis,J. Gas Chromatog.,1, 68-71, 1967. Fehsenfeld,F., et al., Emissionsof volatile organiccompoundsfrom vegetation and the implications for atmosphericchemistry, GlobalBiogeochem. Cycles,6, 389-430, 1992. Fuentes,J.D., D. Wang, G. Den Hartog, H.H. Neumann, T.F. Dann, and K.J. Puckett,Modelled and field measurements of biogenic hydrocarbon emissionsfrom a Canadiandeciduousforest,,4tmos. Environ., 29(21), 3003-3017, 1995. Gates, D.M., and L.E. Papian, Atlas of Energy Budgets of Plant Leaves,Academic,SanDiego, Calif., 1971. Geron, C., A. Guenther and T. Pierce, An improved model for estimatingemissionsof volatile organiccompoundsfrom forests in the easternUnited States,J. Geophys.Res.,99, 12,773-12,792, 1994. 101, 1345-1359, 1996a. Guenther,A., J. Greenberg,P. Harley, D. Helmig, L. Klinger, L. Vierling, P.Zimmerman,and C. Geron, Leaf, branch,stand,and landscapescale measurementsof volatile organic compound fluxesfrom U.S. woodlands, Tree Physiol.,16, 17-24, 1996b. Guenther,A., et al., Isoprenefluxesmeasuredby enclosure,relaxed eddy accumulation,surface-layergradient and mass balance techniques, J. Geophys,Res., 101, 18,555-18,567,1996c. Harley, P., A. Guenther,and P Zimmerman,Environmentalcontrols over isopreneemissionfrom sun and shade leaves in a mature white oak canopy,Tree Physiol.,17, 705-714, 1997. Hirsch, A.I., J.W. Munger, D.J. Jacob,L.W. Horowitz, and A.H. Goldstein,Seasonalvariationof the ozoneproductionefficiency per unit NOx at HarvardForest,Massachusetts, J. Geophys.Res., 101, 12,659-12,666, 1996. Khalil, M.A.K., and R.A. Rasmussen, Forest hydrocarbon emissions: Relationships between fluxes and ambient concentrations,d. ,4it Water Manage. ,4ssoc.,42, 810-813, 1992. Knoerr, K.R., and F.L. Mowry, Energy balance/Bowen ratio techniquesfor estimatinghydrocarbonfluxes, in ,4tmospheric BiogenicHydrocarbons,edited by J.J. Bufalini and R.R. Arnts, pp. 35-52, Butterworth,Stoneham,Mass., 1981 Lamb, B., H. Westberg,and G. Allwine, Biogenic hydrocarbon emissions from deciduous and coniferous trees in the United States,d. Geophys.Res.,90, 2380-2390, 1985. Lamb, B., H. Westberg,and G. Allwine, Isopreneemissionfluxes determinedby an atmospherictracer technique,,4tmos.Environ., 20, 1-8, 1986. Lamb, B., D. Gay, H. Westberg, and T. Pierce, A biogenic hydrocarbonemission inventory for the U.S. using a simple forestcanopymodel, ,4tmos.Environ., 27`4, 1673-1690, 1993. Lamb, B., et al., Evaluationof forestcanopymodelsfor estimating isopreneemissions,J. Geophys.Res., 101, 22,787-22,797, 1996. McKeen, S.A., E.Y. Hsie, and S.C. Liu, A studyof the dependence of rural ozone on ozone precursorsin the easternUnited States, •. Geophys.Res.,96, 15,377-15,394, 1991. Monson, R.K., and R. Fall, Isopreneemissionfrom aspenleaves: Influence of environment and relation to photosynthesisand photorespiration, Plant Physiol., 90, 267-274, 1989. Monson,R.K., C.H. Jaeger,W.W. Adams III, E.M. Driggers,G.M. Silver, and R. Fall, Relationshipsamongisopreneemissionrate, photosynthesis, and isoprenesynthaseactivity as influencedby temperature,Plant Physiol.,98, 1175-1180, 1992. Monson, R.K., P.C. Harley, M.E. Litvak, M. Wildermuth, A.B. Geron, C.D., et al., Biogenic isopreneemission: Model evaluation in a southeasternUnited States bottomland deciduous forest, J. Guenther, P.R. Zimmerman, and R. Fall, Environmental and Geophys.Res.,102, 18,889-18,901,1997. Goldstein, A.G., B.C. Daube, J.W. Munger, and S.C. Wofsy, developmentalcontrols over the seasonalpattern of isoprene Automated in-situ monitoring of atmospheric non-methane emissionfrom aspenleaves,Oecologia,99, 260-270, 1994. hydrocarbonconcentrations and gradients,J. ,4tmos.Chem.,21, Moore, K.E., D.R. Fitzjarrald, R.K. Sakai, M.L. Goulden, J.W. 43-59, 1995a. Munger, and S.C. Wofsy, Seasonalvariation in radiative and turbulent exchange at a deciduous forest in central Goldstein,A. H., C.M. Spivokovsky,and S.C. Wofsy, Seasonal Massachusetts, d. ,4ppl. Meteorol., 35, 122-134, 1996. variationsof nonmethanehydrocarbonsin rural New England: Constraints on OH concentrations in northern midlatitudes, J. Munger, J.W., S.C. Wofsy, P.S. Bakwin, S-M. Fan, M.L. Goulden, B.C. Daube, A.H. Goldstein,K.E. Moore, and D.R. Fitzjarrald, Geophys. Res.,100,21,023-21,033,1995b. Goldstein,A.H., S.M. Fan, M.L. Goulden,J.W. Munger, and S.C. Atmosphericdepositionof reactivenitrogenoxidesand ozonein a temperate deciduous forest and a subarctic woodland, 1, Wofsy, Emissionsof ethene,propene,and 1-buteneby a midlatitudeforest,J. Geophys. Res.,101, 9149-9157,1996. Measurements and mechanisms, d. Geophys.Res., 101, 12,63912,657, 1996. Goulden,M.L., J.W. Munger, S.M. Fan, B.C. Daube, and S.C. Wofsy, Measurements of carbonstorageby long-termeddy Munger, J.W., S-M. Fan, P.S. Bakwin, M.L. Goulden, A.H. correlation: Methods and a critical evaluation of accuracy, Goldstein,A.S. Colman, and S.C. Wofsy, Regionalbudgetsfor nitrogenoxidesfrom continentalsources:Variationsof rates for GlobalChangeBiol., 2, 169-182, 1996a. oxidationand depositionwith seasonand distancefrom source GouldenM.L., J.W. Munger, S.M. Fan, B.C. Daube, and S.C. regions,d. Geophys.Res., 103, 8355-8368, 1998. Wofsy, Effectsof interannualclimatevariabilityon the carbon dioxideexchangeof a temperatedeciduousforest,Science,271, National Acid PrecipitationAssessmentProgram (NAPAP), The 1576-1578, 1996b. 1985 NAPAP emissionsinventory(version2): Developmentof 31,056 GOLDSTEIN ET AL.: SEASONAL COURSE OF ISOPRENE EMISSIONS the annualdata and modelers'tapes,EPA-600/7-89-OI2a, pp. 219, U.S. Environ. Prot. Agency, Washington, D.C., 1985, (AvailablefromNatl. Tech.Inf. Serv.,Springfield,Va.). NationalResearchCouncil(NRC), Rethinkingthe OzoneProblemin Urban and Regional Air Pollution, Natl. Acad. Press., Washington,D.C., 1991. Pier, P.A., Isopreneemissionratesfrom northernred oak usinga whole-treechamber,Atmos.Environ., 29(12), 1347-1353, 1995. Roselle, S.J., T.E. Pierce, and K.L. Schere, The sensitivity of regionalozonemodelingto biogenichydrocarbons, d. Geophys. Res., 96, 7371-7394, 1991. Sanadze,G.A., Light-dependent excretionof molecularisopreneby leaves,Prog.Photosyn.Res.,II, 701-706, 1969. Sharkey,T.D., and E.L. Singsaas,Why plants emit isoprene, Nature, 374, 769, 1995. Webb, E.K., G.I. Pearman, and R. Leuning, Correctionof flux measurements for densityeffectsdue to heat and water vapour transfer,Q. d. R. Meteorol. Soc., 106, 85-100, 1980. Winer, A., J. Arey, S. Aschman,R. Atkinson,W. Long,L. Morrison, andD. Olszyk, Hydrocarbonemissionsfrom vegetationfoundin Califomia'sCentralValley, final report,Calif. Air Resour.Board contract A732-155, Statewide Air Pollut. Res. Cent., Univ. of Calif., Riverside, 1989. Wofsy, S.C., M.L. Goulden,J.W. Munger, S.M. Fan, P.S. Bakwin, B.C. Daube, S.L. Bassow,and F.A. Bazzaz, Net exchangeof CO2 in a mid-latitude forest, Science, 260,1314-1317, 1993. Zimmerman,P.R., Determinationof emissionratesof hydrocarbons from indigenous species of vegetation in the Tampa/St. Petersburg Fla. area,Final AppendixC, Rep. EPA-904/9-77-028, U.S. Environ.Prot.Agency,ResearchTrianglePark,N.C., 1979. Sharkey,T.D., F. Loreto,and C.F. Delwiche,The biochemistry of isopreneemissionfrom leavesduringphotosynthesis, in Trace Gas Emissionsby Plants,editedby T.D. Sharkey,E.A. Holland, C. D. Geron,National Risk ManagementResearchLaboratory, and H.A. Mooney, pp. 153-184, Academic,San Diego, Calif., U.S. EnvironmentalProtectionAgency,ResearchTrianglePark,NC 1991. Sharkey,T.D., E.L. Singsaas,P.J. Vanderveer,and C.D. Geron, Field measurements of isopreneemissionfrom treesin response to temperature andlight, TreePhysiol.,16, 649-654, 1996. Sillman,S., J.A. Logan,and S.C. Wofsy, The sensitivityof ozoneto nitrogenoxidesand hydrocarbons in regionalozoneepisodes,d. Geophys.Res.,95, 1837-1851, 1990. Singh,H.B., and P.B. Zimmerman,Atmosphericdistributionsand sourcesof nonmethanehydrocarbons,in GaseousPollutants: Characterizationand Cycling, edited by J.O. Nriagu, pp. 177235, JohnWiley, New York, 1992. Tingey, D.T., M. Manning., L.C. Grothaus,and W.F. Bums, The influenceof light and temperatureon isopreneemissionrates from live oak,Physiol.Plant., 47, 112-118, 1979. 27711. A. H. Goldstein,Division of EcosystemSciences,Departmentof EnvironmentalScience,Policy and Management,151 Hilgard Hall, University of California, Berkeley, CA 94720-3110. (ahg•nature.berkeley.edu). M. L. Goulden,Earth SystemScience,Universityof California, Irvine, CA 92697-3100. J. W. Munger and S.C. Wofsy Departmentof Earth and PlanetarySciences,Division of Engineeringand Applied Sciences, HarvardUniversity,Cambridge,MA 02138. (ReceivedOctober10, 1997;revisedMay 15, 1998; acceptedMay 21, 1998.)
© Copyright 2025 Paperzz