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Atmospheric halocarbons and nitrous oxide measurements: Palmer Station monitoring, latitudinal gradients and standardization K.J. SCHILLING, D.C. DELOREY, D.R. CRONN, and W.L. BAMESBERGER Laboratory for Atmospheric Research Washington State University Pullman, Washington 99164 Latitudinal measurements. Interpretation is complete of lati- tudinal measurements of dichlorodifluoromethane (CC1 2F 2 or F-12), fluorotrichioromethane (CC1 1F or F-li), methyl chlo- roform (CH 3 CC13) 1 carbon tetrachloride (CC,), and nitrous ox- ide (N2 0) made over the remote Pacific Ocean by six C-130 USAP aircraft flights between 1976 and 1980, and one oceanographic cruise in 1983 (DeLorey, Cronn, and Farmer in press). Spatial and temporal distributions of these gases are important because of their effect on climate via stratospheric ozone depletion and their contribution to the warming of the Earth (the greenhouse effect). Since there are no known sinks for these compounds in the lower atmosphere other than the reaction of CH 3CC1 3 with the hydroxyl radical (OH), they are transported to the strat- osphere where they can be photodissociated only by ultraviolet radiation. The resulting free radicals then catalytically destroy ozone. Because stratospheric ozone absorbs ultraviolet solar radiation, its depletion could alter the radiation balance and consequently cause climatic changes (NASA 1986). These com- pounds also absorb outgoing infrared radiation and, therefore, contribute to the greenhouse effect in the same way as carbon dioxide (d0 2 ) (wMo 1986). Although latitude ranges varied for each flight, the maximum range was from 80° north to 90° south. Mean mixing ratios for the Northern and Southern Hemispheres, annual time trends, and total atmospheric burdens have been calculated for each gas. Lifetimes also were calculated for F-12, F-il, and CH1CC13 using observed annual growth rates, calculated total at- mospheric burdens, and published cumulative emissions data. Results are presented in the table. The halocarbons showed higher levels in the Northern Hemi- sphere than in the Southern Hemisphere (see the example for F-il in figure 1). This result is expected since there are larger anthropogenic emissions in the Northern Hemisphere, mainly in the mid-latitudes, than in the Southern Hemisphere. The halocarbons also showed a "Southern Hemispheric hump," where the concentrations increase from the Intertropical Con- vergence Zone (0° to 10°N) to about 10°S, then decrease from about 10°S to 30°S. This could be a result of large-scale transport between the northern and southern hemispheric air masses in the so-called Hadley cells (DeLorey et al. in press). N20 did not exhibit a noticeable latitudinal gradient. This is primarily due to its long atmospheric lifetime and geograph - ically uniform emissions from predominantly natural sources such as microbial activity in soils, freshwater, and saltwater (wMo 1986). Ratios of northern hemispheric to southern hemispheric mix- ing ratios were calculated for each study. For F-12 and F-il the ratios varied from 1.03 to 1.07 and are somewhat lower than values reported by others. Various reasons for the lower ratios could include: • free tropospheric measurements by Washington State Uni- versity vs. boundary layer measurements by others, • mid-Pacific (Washington State University) vs. continental measurements, and • large latitudinal coverage (Washington State University) vs. discrete site measurements. Northern to southern hemispheric ratios for CH 3CC1 3 also were substantially smaller than values reported by other inves- tigators (e.g., Washington State University's value for January 1978 was 1.15 ± 0.07). In addition to these reasons, the dif - ferences could be explained partly by the usual absence of Washington State University data for areas north of 33°N, where the highest concentrations occur. Northern to southern hemi- spheric ratios for both CC1 4 and N2 0 were in good agreement with measurements made by other investigators. Results for 1976-1983 latitudinal measurements 1976-1983 Total 1980 Mean Mean annual atmospheric Atmospheric Compound mixing ratioa increase burden lifetime CCl 2 F2 (F-12) 285 pptvc 6.0±0.3%/yrd 5.81 MTe 174±89 yr CCI 3 F (F-1 1) 177 pptv 6.3±0.1%/yr 3.95 MT 202±149 yr CH3CCI3 117 pptv 9.0±0.9%/yr 2.47 MT 14.5±2.2 yr CCI4 139 pptv 3.7±0.4%/yr 3.50 MT N20 301.6 ppbvt 0.3±0.04%/yr 2283 MT a Mean of northern and southern hemispheric mean mixing ratios. b Calculated for October through November, 1980. Parts per trillion by volume. Percentage per year. Megatons. Parts per billion by volume. Dashes denote 'not calculated." 268 ANTARCTIC JOURNAL

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Page 1: Atmospheric halocarbons and nitrous oxide measurements ... › ... › AJUSvXXIIn5p268.pdf · • October and November 1980; a October and November 1983; and. November and December

Atmospheric halocarbons and nitrousoxide measurements: Palmer Stationmonitoring, latitudinal gradients and

standardization

K.J. SCHILLING, D.C. DELOREY,D.R. CRONN, and W.L. BAMESBERGER

Laboratory for Atmospheric ResearchWashington State UniversityPullman, Washington 99164

Latitudinal measurements. Interpretation is complete of lati-tudinal measurements of dichlorodifluoromethane (CC1 2F2 orF-12), fluorotrichioromethane (CC1 1F or F-li), methyl chlo-roform (CH 3CC13)1 carbon tetrachloride (CC,), and nitrous ox-ide (N20) made over the remote Pacific Ocean by six C-130 USAPaircraft flights between 1976 and 1980, and one oceanographiccruise in 1983 (DeLorey, Cronn, and Farmer in press). Spatialand temporal distributions of these gases are important becauseof their effect on climate via stratospheric ozone depletion andtheir contribution to the warming of the Earth (the greenhouseeffect). Since there are no known sinks for these compounds inthe lower atmosphere other than the reaction of CH 3CC1 3 withthe hydroxyl radical (OH), they are transported to the strat-osphere where they can be photodissociated only by ultravioletradiation. The resulting free radicals then catalytically destroyozone. Because stratospheric ozone absorbs ultraviolet solarradiation, its depletion could alter the radiation balance andconsequently cause climatic changes (NASA 1986). These com-pounds also absorb outgoing infrared radiation and, therefore,contribute to the greenhouse effect in the same way as carbondioxide (d0 2) (wMo 1986).

Although latitude ranges varied for each flight, the maximumrange was from 80° north to 90° south. Mean mixing ratios forthe Northern and Southern Hemispheres, annual time trends,

and total atmospheric burdens have been calculated for eachgas. Lifetimes also were calculated for F-12, F-il, and CH1CC13using observed annual growth rates, calculated total at-mospheric burdens, and published cumulative emissions data.Results are presented in the table.

The halocarbons showed higher levels in the Northern Hemi-sphere than in the Southern Hemisphere (see the example forF-il in figure 1). This result is expected since there are largeranthropogenic emissions in the Northern Hemisphere, mainlyin the mid-latitudes, than in the Southern Hemisphere. Thehalocarbons also showed a "Southern Hemispheric hump,"where the concentrations increase from the Intertropical Con-vergence Zone (0° to 10°N) to about 10°S, then decrease fromabout 10°S to 30°S. This could be a result of large-scale transportbetween the northern and southern hemispheric air masses inthe so-called Hadley cells (DeLorey et al. in press).

N20 did not exhibit a noticeable latitudinal gradient. This isprimarily due to its long atmospheric lifetime and geograph -ically uniform emissions from predominantly natural sourcessuch as microbial activity in soils, freshwater, and saltwater(wMo 1986).

Ratios of northern hemispheric to southern hemispheric mix-ing ratios were calculated for each study. For F-12 and F-il theratios varied from 1.03 to 1.07 and are somewhat lower thanvalues reported by others. Various reasons for the lower ratioscould include:• free tropospheric measurements by Washington State Uni-

versity vs. boundary layer measurements by others,• mid-Pacific (Washington State University) vs. continental

measurements, and• large latitudinal coverage (Washington State University) vs.

discrete site measurements.Northern to southern hemispheric ratios for CH 3CC13 also

were substantially smaller than values reported by other inves-tigators (e.g., Washington State University's value for January1978 was 1.15 ± 0.07). In addition to these reasons, the dif -ferences could be explained partly by the usual absence ofWashington State University data for areas north of 33°N, wherethe highest concentrations occur. Northern to southern hemi-spheric ratios for both CC1 4 and N 20 were in good agreementwith measurements made by other investigators.

Results for 1976-1983 latitudinal measurements

1976-1983

Total1980 Mean Mean annual atmospheric Atmospheric

Compound mixing ratioa

increase burden lifetime

CCl 2 F2 (F-12) 285 pptvc 6.0±0.3%/yrd 5.81 MTe

174±89 yr

CCI3F (F-1 1)

177 pptv 6.3±0.1%/yr 3.95 MT

202±149 yr

CH3CCI3 117 pptv 9.0±0.9%/yr 2.47 MT

14.5±2.2 yr

CCI4 139 pptv 3.7±0.4%/yr 3.50 MT

N20

301.6 ppbvt

0.3±0.04%/yr 2283 MT

a Mean of northern and southern hemispheric mean mixing ratios.b Calculated for October through November, 1980.

Parts per trillion by volume.Percentage per year.Megatons.Parts per billion by volume.Dashes denote 'not calculated."

268 ANTARCTIC JOURNAL

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CDZ

>< 150

25

225

0.200

0I-ir 175

90S70S50S30SlOSION30N50N70NLATITUDE

Figure 1. CCI 3F(F-1 1)Iatitudinal distributions for the 1976 to 1980f lights and the 1983 cruise. Each data point represents a 5 degree mixing ratiomean. Key: cO June and July 1976; • January 1977; A October to November 1977; A November and December 1978; D September 1979;• October and November 1980; a October and November 1983; and. November and December 1983 (DeLorey et al. in press).

F-12 and F-il increased globally at 6 percent per year andwere consistent with emission estimates by the Chemical Man-ufacturers Association (1986). CH 3CC13 mixing ratios increasedat 9.0 ± 0.9 percent per year, faster than any of the other tracegases. CC!, increased at about 3.7 percent per year and N 20 atabout 0.3 percent per year. Although N20 increased by thesmallest percentage, it increased in magnitude faster than theother gases (about 1 part per billion by volume for N 20 vs. about17 parts per trillion by volume for F-12). Total atmosphericburdens for the halocarbons and N 20 were calculated by amethod described by Rowland et al. (1982) (see table).

Palmer Station measurements. Halocarbon and N20 time trendcalculations from 1982 to 1985 at the Clean-Air Facility at PalmerStation, Antarctica, have been completed. These calculationsare based on the finalized data set following completeion ofquality control checks (Cronn et al. 1986; Robinson et at. 1984).The mixing ratios were found to be increasing at annual rates of5.87 ± 0.10 percent for F-1 1, 5.45 ± 0.10 percent for F-12, 5.31 ±0.22 percent for CH 3CC13, 1.29 ± 0.08 percent for CCI4, and 0.24± 0.05 percent for N 20. In general, these calculations are inagreement with those made by other investigators.

A preliminary analysis of the weekly mean carbon monoxide(CO) mixing ratios at Palmer Station from 1982 to 1985 is pre-sented in figure 2. Gaps in the data are due to periods ofequipment failure or site contamination. These data, as well asmethane (CH4) and carbon dioxide (CO 2) data are currentlyundergoing final quality control checks. They will be used fortime series analyses once the data have been verified.

Calibration of secondary standards. Accurate trace gas measure-ments are dependent upon the accuracy of standards used intheir analyses. Therefore, mixing ratio values assigned to sec-ondary standards must be periodically compared to accuratelyknown primary standards. Compressed gas cylinders con-taining secondary transfer standards which had been standard-ized by static dilution techniques and stored at WashingtonState University since 1976 (Klemgard Long Term secondarystandards, KLT5) were recently compared to an NBS SRM-(National Bureau of Standards, Standard Reference Material).

These KLT5 have been used to establish gas mixing ratios in fieldstandards which in turn were used for all subsequent fieldmeasurement programs including the latitudinal gradientstudy and the project conducted at Palmer Station. The NBS SRM

was certified for N 20 with a 95 percent confidence interval ofabout 1 percent ( = 301 parts per billion). The SRM providedadvisory mixing ratios for F-12 ( 455 parts per trillion ± 15percent) and F-li ( = 323 ;arts per trillion ± 13 percent). Sincethe uncertainty in the SRM mixing ratio for all these gases wasgreater than the statistically significant difference between theold and newly calculated mixing ratios for the KLTs, applicationof correction factors will not guarantee that the values are anymore accurate. However, if one wants to compare WashingtonState University calibrations via the NBS SRM, the correctionfactors needed are 0.9975 for N 20,1.0073 for F-12, and 1.0699 forF-li.

Secondary field standards used at Palmer Station andelsewhere were also compared to the NBS SRM for CO2 and CH4.

The CO2 mixing ratio was certified with a 95 percent confidenceinterval of about 0.06 percent ( = 341.5 parts per million); theCH4 mixing ratio was advisory only ( = 1.73 parts per million± 1.7 percent). CO 2 mixing ratios calculated using the SRM

5 1300...lI0o

90--.--

70 ----;$-!Z a..--50-.X-t-

30 I I• 1

1982198319841985Figure 2. Weekly mixing ratios of carbon monoxide (CO).

1987 REVIEW 269

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agreed with the secondary standard manufacturer's suggestedvalue within 0.8 parts per million (about 0.2 percent), and werenot statistically different from them. For CH, the SRM calculatedvalue was higher than the suggested value for the secondarystandards by 1-2 percent; however, the uncertainty in the SRMCH4 mixing ratio value would not allow reassignment to be anymore accurate. Therefore, we have not changed the secondarystandard values used for generating the CH4 and CO2 PalmerStation data.

The authors wish to thank Elmer Robinson, David Harsch,Fred Menzia, Bob Stordeur, and Robert Watkins for help inacquiring the aircraft data used for the latitudinal gradientstudy. This work was supported by National Science Founda-tion grants DPP 76-00437, DPP 77-22866, DPP 79-21003, DPP81-18398, and ATM 83-12369. The Palmer Station monitoringprogram has been supported by National Science Foundationgrants [)PP 79-21003, DPP 80-05797, and DPP 85-15752.

References

Chemical Manufacturers Association. 1986. Production, sales, and cal-culated releases of CFC-11 and CFC-12 through 1985. Report of thefluorocarbon program panel, Washington, D.C.

Cronn, D.R., W.L. Bamesberger, EA. Menzia, S.F. Waylett, A.S. Way-lett, T.W. Ferrara, H.M. Howard, and E. Robinson. 1986. At-mospheric trace gas trends at Palmer Station, Antarctica: 1982-1985.Geophysical Research Letters. 13(1), 1272-1275.

DeLorey, D.C., D.R. Cronn, and J.C. Farmer. In press. Troposphericlatitudinal distributions of CCl 2F2 , CC13F, N201 CH3CCI-, and CC14 overthe remote Pacific ocean. Atmospheric Environment.

NASA. 1986. Present state of knowledge of the upper atmosphere: Anassessment report. NASA Reference Publication 1162. Washington,D.C.: U.S. Government Printing Office.

Robinson, E., W.L. Bamesberger, EA. Menzia, A.S. Waylett, and S.F.Waylett. 1984. Atmospheric trace gas measurements at Palmer Sta-tion, Antarctica: 1982-83. Journal of Atmospheric Chemistry, 2(1), 65-81.

Rowland, ES., S.C. Tyler, D.C. Montague, and Y. Makide. 1982. Theatmospheric burden of CCl2F2 . In interpretation of climate and pho-tochemical models, ozone and temperature measurements. American In-stitute of Physics Conference Proceedings Number 82.

WMO. 1986. Atmospheric ozone 1985. Assessment of our understand-ing of the processes controlling its present distribution and change.WMO global ozone research and monitoring project no. 16, WMO, Geneva,Switzerland.

Antarctic automatic weather stations,austral summer 1986-1987

CHARLES R. STEARNS and GEORGE A. WEIDNER

Department of MeteorologyUniversity of Wisconsin

Madison, Wisconsin 53706

The automatic weather stations (Aws) in Antarctica measureair temperature, wind speed and wind direction at a nominalheight of 3 meters above the surface, and air pressure at theelectronics enclosure. Some AWS units measure relative humidi-ty and/or the air temperature difference between 3 meters and0.5 meters above the surface. The AWS unit is controlled by amicrocomputer which updates the data at a nominal 10-minuteinterval and transmits three to five data points for each sensor ata nominal 200-second interval to ARGOS equipped polar orbitingsatellites.

The AWS units in Antarctica support the following studies:• Barrier wind flow along the Antarctic Peninsula and the

Transantarctic Mountains.• Katabatic flow down the Adélie Coast, Byrd Glacier,

Beardmore Glacier, and Reeves Glacier.• Mesoscale circulation on the Ross Ice Shelf.• Climatology of Byrd Station and Dome C.• Sensible and latent heat fluxes on the Ross Ice Shelf.• Oceanographic support.• Meteorological support for air operations using a local user

terminal at McMurdo Station.• Influence of Amundsen-Scott Station on the local climate.

The table gives the site name, AWS ID, location, and start datefor AWS units installed austral summer 1986-1987. Stearns andWeidner (1985, 1986) present similar tables for 1984 and 1985.Figure 1 shows the locations of the AWS units in Antarctica givenin the table. The open circles are units which were to be installedduring austral summer 1986-1987.

Didier Simone of Expeditions Polaires Francaises replacedAWS 8901 with AWS 8912 at D-10 and repaired the sensor cable. AtD-47 and D-57 the AWS electronics were replaced.

The field work for austral summer 1986-1987 included visit-ing Marilyn site to raise the tower and replace the AWS unit,Patrick and Allison sites to exchange AWS units, Martha site toinstall an AWS unit, Manuela site to replace the entire station,and Buckle Island in the Balleny Islands to install an AWS unit.

Marilyn site was visited on 10 January 1987 using an LC-130airplane. The inertial navigation system located the site, and theunit was detected on radar. The aircraft ADI detected the solar-powered beacon. The tower top was approximately 3 feet (0.9meter) above the snow. The tower was raised 3 meters, and AWS8915 and a radar reflector were installed. The AWS 8921 had notbeen received because the Synergetics antenna was brokeninternally.

On 16 January 1987 Patrick site near South Pole was visited toremove AWS 8905 and install AWS 8901 for testing. A pressuregauge was not installed. The tower was raised and the boomreoriented so that the vane zero was not in the direction of themost frequent wind.

Allison site was visited on 17 January 1987 to replace AWS 8905with AWS 8921. Two boxes of three gel-cell batteries and a reg-ulator were installed. The tower was reinstalled and the boomwas oriented so that zero was not in the most frequent winddirection. The old batteries were returned to McMurdo Stationto determine their condition after 1 year at the South Pole.

Ferrell site was visited on 23 January 1987 to replace theaerovane. The bearings had failed on the wind speed ta-

270 ANTARCTIC JOURNAL