Mie-scattering function
Computer program for calculating normalized Mie scattering functions
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Computer program for calculating normalized Mie scattering functions
Mie scattering calculations on laser wavelengths and atmospheric aerosols
Monte Carlo method applied to pigment particle clusters, and relevance of Mie scattering function to reflected light
Calculation of Mie scattering functions
UBV colors and polarization models for reflection nebulae based on Mie scattering functions for exponential size distribution of silicate particles
Calculations of Mie scattering functions involved individual as well as mixed scattering of particles. In particular, computations were completed for a 15A particle and for particles subjected to incident light of ultraviolet wavelengths. Calculations of contaminant atmospheres for Gemini, Apollo, and Skylab considered leakage rates for the respective vehicles and the mass column density of the atmospheres surrounding them. Atmospheres for these vehicles have been computed for a uniform particle size distribution, and for a particle size distribution in which size varied.
Remote sensing of brightness temperatures of a scattering medium composed of spherical scatterers beneath a homogeneous surface layer is studied by using Mie scattering functions. We illustrate the effects of a surface layer by plotting the brightness temperatures as functions of frequency and viewing angle for different layer thicknesses, dielectric constants, and fractional scattering volumes. It is found that the brightness temperature increases when the loss tangent of the surface layer is increased and when the fractional volume occupied by the scatterers is decreased. In the absence of a surface layer the brightness temperature is usually decreasing as a function of frequency. The presence of a homogeneous layer may cause the brightness temperature to increase with frequency. At all viewing angles the vertical polarization is brighter than the horizontal polarization.
Optical radar investigations of atmosphere, and Mie scattering intensity functions for backscatter
The size distribution and complex refractive index of Martian dust-cloud particles observed in 1971 with the Mariner 9 UV spectrometer are determined by matching the observed single-scattering albedo and phase function with Mie-scattering calculations for size distributions of spheres. Values of phase function times single-scattering albedo are presented for 12 wavelength intervals in the range from 190 to 350 nm, and best-fit values are obtained for the absorption index. It is found that the absorption index of the dust particles increases with decreasing wavelength from 350 to about 210 nm and then drops off shortward of 210 nm, with a structural shoulder occurring in the absorption spectrum between 240 and 250 nm. A search for a candidate material that can explain the strong UV absorption yields TiO2, whose anatase polymorph has an absorption spectrum matching that of the Martian dust. The TiO2 content of the dust particles is estimated to be a few percent or less.
Volume backscattering functions and optical extinction coefficients for visible and IR RADIATION and selected cloud models
Mie scattering and absorption cross section for spherical particles
Aerosol mean particle size determined by rapid approximate method based on Mie light scattering theory
Temperature dependence of Mie scattering, covering absorption and scattering of electromagnetic radiation on spherical aluminum oxide particles
Radiation absorption and scattering by small spherical solid carbon particles in wavelength range 0.2 to 40 mu calculated by classical Mie theory
Mie scattering calculation to support theory that interstellar extinction is caused by graphite particles
Monte Carlo methods, Mie theory, and random walk and screen models for predicting reflective properties of paint films
Monte Carlo method used for calculating reflected and transmitted radiance of earth atmosphere
Radiation absorption and scattering by small spherical solid carbon particles in wavelength range 0.2 to 40 mu calculated by classical Mie theory