A laboratory investigation of light scattering from representative components of mineral dust aerosol at a wavelength of 550 nm

被引:72
作者
Curtis, Daniel B. [1 ,2 ]
Meland, Brian [1 ]
Aycibin, Murat [1 ]
Arnold, Nathan P. [1 ]
Grassian, Vicki H. [2 ]
Young, Mark A. [2 ]
Kleiber, Paul D. [1 ]
机构
[1] Univ Iowa, Dept Phys & Astron, Iowa City, IA 52242 USA
[2] Univ Iowa, Dept Chem, Iowa City, IA 52242 USA
关键词
D O I
10.1029/2007JD009387
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
To test the applicability of Mie theory in climate models and remote sensing data retrievals, we have studied the scattering phase function and linear polarization of representative mineral dust aerosol components at a wavelength of 550 nm. The mineral components investigated include the silicate clays, kaolinite, illite, and montmorillonite, and non-clay minerals, quartz, calcite, gypsum, and hematite, as well as Arizona road dust. In each case the aerosol size distribution was simultaneously monitored with an aerodynamic particle sizer. Particle diameters in this study fall in the accumulation mode size range characteristic of long-range transport aerosols. Our results show significant discrepancies between the experimental and Mie theory phase functions. The model shortcomings are due to particle shape effects for these non-spherical mineral dust particles. We find intriguing differences in the scattering between the silicate clay and non-clay components of mineral dust aerosol in this size range. For the non-clay minerals the most significant errors are found at large scattering angles where Mie theory substantially overestimates the backscattering signal. For the silicate clay minerals, there is more variability in the comparison to Mie theory. These findings have important consequences for the radiative forcing component of global climate models and remote sensing measurements that rely on Mie theory to characterize atmospheric dust. We also present experimentally based synthetic phase functions at 550 nm, for both silicate clay and non-clay mineral dust aerosols in the size parameter range X = 2-5, which may be useful for empirical models of the scattering due to particles in the accumulation mode size range.
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页数:15
相关论文
共 41 条
[11]  
Egan W. G., 1979, OPTICAL PROPERTIES I
[12]   LIGHT-SCATTERING BY SIZE SHAPE DISTRIBUTIONS OF SOIL PARTICLES AND SPHEROIDS [J].
HILL, SC ;
HILL, AC ;
BARBER, PW .
APPLIED OPTICS, 1984, 23 (07) :1025-1031
[13]  
Hinds W.C., 1999, Aerosol technology: Properties, behavior, and measurement of airborne particles, V2nd ed., DOI [DOI 10.1016/0021-8502(83)90049-6, 10.1016/0021-8502(83)90049-6]
[14]   SCATTERING OF POLARIZED LIGHT BY POLYDISPERSE SYSTEMS OF IRREGULAR PARTICLES [J].
HOLLAND, AC ;
GAGNE, G .
APPLIED OPTICS, 1970, 9 (05) :1113-&
[15]   Coupled infrared extinction and size distribution measurements for several clay components of mineral dust aerosol [J].
Hudson, Paula K. ;
Gibson, Elizabeth R. ;
Young, Mark A. ;
Kleiber, Paul D. ;
Grassian, Vicki H. .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2008, 113 (D1)
[16]   A newly designed and constructed instrument for coupled infrared extinction and size distribution measurements of aerosols [J].
Hudson, Paula K. ;
Gibson, Elizabeth R. ;
Young, Mark A. ;
Kleiber, Paul D. ;
Grassian, Vicki H. .
AEROSOL SCIENCE AND TECHNOLOGY, 2007, 41 (07) :701-710
[17]  
IVLEV LS, 1973, IZV AS ATMOS OCEAN P, V95, P87
[18]   LIGHT-SCATTERING FROM PARTICLES OF REGULAR AND IRREGULAR SHAPE [J].
JAGGARD, DL ;
HILL, C ;
SHORTHILL, RW ;
STUART, D ;
GLANTZ, M ;
ROSSWOG, F ;
TAGGART, B ;
HAMMOND, S .
ATMOSPHERIC ENVIRONMENT, 1981, 15 (12) :2511-2519
[19]   Application of the extended boundary condition method to particles with sharp edges: a comparison of two surface integration approaches [J].
Kahnert, FM ;
Stamnes, JJ ;
Stamnes, K .
APPLIED OPTICS, 2001, 40 (18) :3101-3109
[20]   Mie simulations as an error source in mineral aerosol radiative forcing calculations [J].
Kahnert, M. ;
Nousiainen, T. ;
Raisanen, P. .
QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2007, 133 (623) :299-307