On numerical evaluation of the H-functions of transport problems by kernel approximation for the albedo 0 less than omega not greater than 1

Astronomy and Astrophysics – Astrophysics

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Albedo, Hamiltonian Functions, Kernel Functions, Transport Theory, Eigenvalues, Fredholm Equations, Taylor Series

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Das Gupta represented the H-functions of transport problems for the albedo w E [0, 1] in the form H(z) = R(z) - S(z) (see Das Gupta, 1977) where R(z) is a rational function of z and S(z) is regular on - 1, O]c. In this paper we have represented S(z) through a Fredhoim integral equation of the second kind with a symmetric real kernel L(y, z) as S(z) = f(z) - ~ L(y, z)S(y) dy. The problem is then solved as an eigenvalue problem. The kernel is converted into a degenerate kernel through finite Taylor's expansion and the integral equation for S(z) takes the form: S(z) = f(z) - x ~ F1(z)F,(y)S(y) dy (which is solved by the usual procedure) where Xr'S are the discrete eigenvalues and Fr'S the corresponding eigenfunctions of the real symmetric kernel L(y, z)

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