Aerosol optical depth measurements by airborne sun photometer in SOLVE II: Comparisons to SAGE III, POAM III and airborne spectrometer measurements

被引:22
作者
Russell, P
Livingston, J
Schmid, B
Eilers, J
Kolyer, R
Redemann, J
Ramirez, S
Yee, JH
Swartz, W
Shetter, R
Trepte, C
Risley, A
Wenny, B
Zawodny, J
Chu, W
Pitts, M
Lumpe, J
Fromm, M
Randall, C
Hoppel, K
Bevilacqua, R
机构
[1] NASA, Ames Res Ctr, Moffett Field, CA 94035 USA
[2] SRI Int, Menlo Pk, CA 94025 USA
[3] Bay Area Environm Res Inst, Sonoma, CA 95476 USA
[4] Johns Hopkins Univ, Appl Phys Lab, Laurel, MD 20723 USA
[5] Natl Ctr Atmospher Res, Boulder, CO 80307 USA
[6] NASA, Langley Res Ctr, SAIC, Hampton, VA 23681 USA
[7] Computat Phys Inc, Springfield, VA 22151 USA
[8] USN, Res Lab, Washington, DC 20375 USA
[9] Univ Colorado, Atmospher & Space Phys Lab, Boulder, CO 80309 USA
关键词
D O I
10.5194/acp-5-1311-2005
中图分类号
X [环境科学、安全科学];
学科分类号
08 ; 0830 ;
摘要
The 14-channel NASA Ames Airborne Tracking Sunphotometer (AATS-14) measured solar-beam transmission on the NASA DC-8 during the second SAGE III Ozone Loss and Validation Experiment (SOLVE II). This paper presents AATS-14 results for multiwavelength aerosol optical depth (AOD), including comparisons to results from two satellite sensors and another DC-8 instrument, namely the Stratospheric Aerosol and Gas Experiment III ( SAGE III), the Polar Ozone and Aerosol Measurement III (POAM III) and the Direct-beam Irradiance Airborne Spectrometer (DIAS). AATS-14 provides aerosol results at 13 wavelengths lambda spanning the range of SAGE III and POAM III aerosol wavelengths. Because most AATS measurements were made at solar zenith angles (SZA) near 90 degrees, retrieved AODs are strongly affected by uncertainties in the relative optical airmass of the aerosols and other constituents along the line of sight (LOS) between instrument and sun. To reduce dependence of the AATS-satellite comparisons on airmass, we perform the comparisons in LOS transmission and LOS optical thickness (OT) as well as in vertical OT (i.e., optical depth, OD). We also use a new airmass algorithm that validates the algorithm we previously used to within 2% for SZA<90 degrees, and in addition provides results for SZA >= 90 degrees. For 6 DC-8 flights, 19 January-2 February 2003, AATS and DIAS results for LOS aerosol OT at lambda=400 nm agree to <= 12% of the AATS value. Mean and root-mean-square (RMS) differences, (DIAS-AATS)/AATS, are -2.3% and 7.7%, respectively. For DC-8 altitudes, AATS-satellite comparisons are possible only for lambda>440 nm, because of signal depletion for shorter lambda on the satellite full-limb LOS. For the 4 AATS-SAGE and 4 AATS-POAM near-coincidences conducted 19-31 January 2003, AATS-satellite AOD differences were <= 0.0041 for all lambda>440 nm. RMS differences were <= 0.0022 for SAGE-AATS and <= 0.0026 for POAM-AATS. RMS relative differences in AOD ([SAGE-AATS]/AATS) were <= 33% for lambda<similar to 755 nm, but grew to 59% for 1020 nm and 66% at 1545 nm. For lambda>similar to 755 nm, AATS-POAM differences were less than AATS-SAGE differences, and RMS relative differences in AOD ([AATS-POAM]/AATS) were <= 31% for all lambda between 440 and 1020 nm. Unexplained differences that remain are associated with transmission differences, rather than differences in gas subtraction or conversion from LOS to vertical quantities. The very small stratospheric AOD values that occurred during SOLVE II added to the challenge of the comparisons, but do not explain all the differences.
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收藏
页码:1311 / 1339
页数:29
相关论文
共 29 条
[1]  
Bodhaine BA, 1999, J ATMOS OCEAN TECH, V16, P1854, DOI 10.1175/1520-0426(1999)016<1854:ORODC>2.0.CO
[2]  
2
[3]   RAYLEIGH-SCATTERING CALCULATIONS FOR THE TERRESTRIAL ATMOSPHERE [J].
BUCHOLTZ, A .
APPLIED OPTICS, 1995, 34 (15) :2765-2773
[4]   A vortex-scale simulation of the growth and sedimentation of large nitric acid hydrate particles -: art. no. 8300 [J].
Carslaw, KS ;
Kettleborough, JA ;
Northway, MJ ;
Davies, S ;
Gao, RS ;
Fahey, DW ;
Baumgardner, DG ;
Chipperfield, MP ;
Kleinböhl, A .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2002, 107 (D20)
[5]   LINE-BY-LINE CALCULATION OF ATMOSPHERIC FLUXES AND COOLING RATES .2. APPLICATION TO CARBON-DIOXIDE, OZONE, METHANE, NITROUS-OXIDE AND THE HALOCARBONS [J].
CLOUGH, SA ;
IACONO, MJ .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 1995, 100 (D8) :16519-16535
[6]   Atmospheric remote sensing using a combined extinctive and refractive stellar occultation technique - 2. Inversion method for extinction measurements [J].
DeMajistre, R ;
Yee, JH .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2002, 107 (D15) :ACH6-1
[7]   The detection of large HNO3-containing particles in the winter arctic stratosphere [J].
Fahey, DW ;
Gao, RS ;
Carslaw, KS ;
Kettleborough, J ;
Popp, PJ ;
Northway, MJ ;
Holecek, JC ;
Ciciora, SC ;
McLaughlin, RJ ;
Thompson, TL ;
Winkler, RH ;
Baumgardner, DG ;
Gandrud, B ;
Wennberg, PO ;
Dhaniyala, S ;
McKinney, K ;
Peter, T ;
Salawitch, RJ ;
Bui, TP ;
Elkins, JW ;
Webster, CR ;
Atlas, EL ;
Jost, H ;
Wilson, JC ;
Herman, RL ;
Kleinböhl, A ;
von König, M .
SCIENCE, 2001, 291 (5506) :1026-1031
[8]   A unified, long-term, high-latitude stratospheric aerosol and cloud database using SAM II, SAGE II, and POAM II/III data: Algorithm description, database definition, and climatology [J].
Fromm, M ;
Alfred, J ;
Pitts, M .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2003, 108 (D12)
[9]   Temperature dependent NO2 cross sections at high spectral resolution [J].
Harder, JW ;
Brault, JW ;
Johnston, PV ;
Mount, GH .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 1997, 102 (D3) :3861-3879
[10]  
Kneizys F.X., 1996, The MODTRAN 2/3 Report and LOWTRAN 7 Model