Representation of a nonspherical ice particle by a collection of independent spheres for scattering and absorption of radiation: 2. Hexagonal columns and plates

[1] A cloud of nonspherical ice particles may be represented in radiation models by a collection of spheres, in which the model cloud contains the same total volume of ice and the same total surface area as the real cloud but not the same number of particles. The spheres then have the same volume-to-area (V/A) ratio as the nonspherical particle. In previous work this approach was shown to work well to represent randomly oriented infinitely long circular cylinders for computation of hemispherical reflectance, transmittance, and absorptance. In this paper the results have been extended to hexagonal columns and plates using a geometric optics technique for large particles and finite-difference-time-domain theory (FDTD) for small particles. The extinction efficiency and single-scattering coalbedo for these prisms are closely approximated by the values for equal-V/A spheres across the ultraviolet, visible, and infrared from 0.2 to 25 μm wavelength. Errors in the asymmetry factor can be significant where ice absorptance is weak, at visible wavelengths for example. These errors are greatest for prisms with aspect ratios close to 1. Errors in hemispheric reflectance, absorptance, and transmittance are calculated for horizontally homogeneous clouds with ice water paths from 0.4 to 200,000 g m−2 and crystal thicknesses of 1 to 400 μm, to cover the range of crystal sizes and optical depths from polar stratospheric clouds (PSCs) through cirrus clouds to surface snow. The errors are less than 0.05 over most of these ranges at all wavelengths but can be larger at visible wavelengths because of the ideal shapes of the prisms. The method was not tested for, and is not expected to be accurate for, angle-dependent radiances.

[1]  W. Wiscombe Improved Mie scattering algorithms. , 1980, Applied optics.

[2]  S. Warren,et al.  Atmospheric Ice Crystals over the Antarctic Plateau in Winter , 2003 .

[3]  J. Hansen,et al.  Light scattering in planetary atmospheres , 1974 .

[4]  A. Macke,et al.  Single Scattering Properties of Atmospheric Ice Crystals , 1996 .

[5]  Q. Fu An Accurate Parameterization of the Infrared Radiative Properties of Cirrus Clouds for Climate Models , 1996 .

[6]  Qiang Fu,et al.  Modeling of Scattering and Absorption by Nonspherical Cirrus Ice Particles at Thermal Infrared Wavelengths. , 1999 .

[7]  Andrew J. Heymsfield,et al.  A parameterization of the particle size spectrum of ice clouds in terms of the ambient temperature and the ice water content , 1984 .

[8]  Ping Yang,et al.  Light scattering by hexagonal ice crystals: solutions by a ray-by-ray integration algorithm , 1997 .

[9]  Van de Hulst,et al.  Multiple Light Scattering: Tables, Formulas, and Applications , 1980 .

[10]  Stephan Havemann,et al.  Extension of T-matrix to scattering of electromagnetic plane waves by non-axisymmetric dielectric particles: application to hexagonal ice cylinders , 2001 .

[11]  K. Liou Transfer of solar irradiance through cirrus cloud layers , 1973 .

[12]  Andrew A. Lacis,et al.  Scattering, Absorption, and Emission of Light by Small Particles , 2002 .

[13]  Tara L. Jensen,et al.  Shapes, sizes and light scattering properties of ice crystals in cirrus and a persistent contrail during SUCCESS , 1998 .

[14]  Andrew A. Lacis,et al.  Sensitivity of cirrus cloud albedo, bidirectional reflectance and optical thickness retrieval accuracy to ice particle shape , 1996 .

[15]  Petr Chylek,et al.  The Two-Stream Approximation in Radiative Transfer: Including the Angle of the Incident Radiation , 1975 .

[16]  K. Liou,et al.  Geometric-optics-integral-equation method for light scattering by nonspherical ice crystals. , 1996, Applied optics.

[17]  Ping Yang,et al.  Extinction efficiency and single‐scattering albedo for laboratory and natural cirrus clouds , 1997 .

[18]  W. Wiscombe,et al.  Mie Scattering Calculations: Advances in Technique and Fast, Vector-speed Computer Codes , 1979 .

[19]  K. Liou,et al.  Solar Radiative Transfer in Cirrus Clouds. Part I: Single-Scattering and Optical Properties of Hexagonal Ice Crystals , 1989 .

[20]  P. Wendling,et al.  Scattering of solar radiation by hexagonal ice crystals. , 1979, Applied optics.

[21]  K. Liou,et al.  Light scattering by nonspherical particles: remote sensing and climatic implications , 1994 .

[22]  A. Heymsfield Cirrus Uncinus Generating Cells and the Evolution of Cirriform Clouds. Part I: Aircraft Observations of the Growth of the Ice Phase , 1975 .

[23]  Thomas C. Grenfell,et al.  A radiative transfer model for sea ice with vertical structure variations , 1991 .

[24]  C. Bohren,et al.  An introduction to atmospheric radiation , 1981 .

[25]  K. Liou,et al.  Light scattering by hexagonal ice crystals: comparison of finite-difference time domain and geometric optics models , 1995 .

[26]  H. Gerber,et al.  Nephelometer Measurements of the Asymmetry Parameter, Volume Extinction Coefficient, and Backscatter Ratio in Arctic Clouds , 2000 .

[27]  Q. Fu,et al.  Finite-difference time-domain solution of light scattering by dielectric particles with a perfectly matched layer absorbing boundary condition. , 1999, Applied optics.

[28]  V. Vouk Projected Area of Convex Bodies , 1948, Nature.

[29]  Thomas C. Grenfell,et al.  Representation of a nonspherical ice particle by a collection of independent spheres for scattering , 1999 .

[30]  C. Mätzler Relation Between Grain Size and Correlation Length of Snow , 2002 .

[31]  K. Liou,et al.  Finite-difference time domain method for light scattering by small ice crystals in three-dimensional space , 1996 .

[32]  A. Ono,et al.  The Shape and Riming Properties of Ice Crystals in Natural Clouds , 1969 .