Abstract:The equation of radiative transfer in non-conservative case for diffuse reflection in a plane-parallel semi-infinite atmosphere with axial symmetry has been solved by Laplace transform and Wiener-Hopf technique. We have determined the emergent intensity in terms of Chandrasekhar's H-function and the intensity at any optical depth by inversion.
“…Ghosh, Mukherjee and Karanjai (2004) studied some approximate form of H-function already studied by Karanjai (1968) and Karanjai and Sen (1971) to the case of anisotropically scattering atmosphere with Pomraning Phase function. Islam, Mukherjee, and Karanjai (2004) solved the equation of radiative transfer with Pomraning Phase function and a non-linear source in a plane semi-infinite atmosphere with axial symmetry by Laplace Transform and Wiener-Hopf technique. They determined the emergent intensity in terms of Chandrasekhar's H-function and the intensity at any optical depth by inversion.…”
The emergent intensity I (0, µ) from the equation of transfer in anisotropically scattering medium with Pomraning phase function is derived in n th approximation by using Chandrasekhar's discrete ordinate method.
“…Ghosh, Mukherjee and Karanjai (2004) studied some approximate form of H-function already studied by Karanjai (1968) and Karanjai and Sen (1971) to the case of anisotropically scattering atmosphere with Pomraning Phase function. Islam, Mukherjee, and Karanjai (2004) solved the equation of radiative transfer with Pomraning Phase function and a non-linear source in a plane semi-infinite atmosphere with axial symmetry by Laplace Transform and Wiener-Hopf technique. They determined the emergent intensity in terms of Chandrasekhar's H-function and the intensity at any optical depth by inversion.…”
The emergent intensity I (0, µ) from the equation of transfer in anisotropically scattering medium with Pomraning phase function is derived in n th approximation by using Chandrasekhar's discrete ordinate method.
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