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This chapter describes the delta-Eddington approximation to the radiative
transport equation. In Section 4.1 the diffusion equation
is derived from the transport equation; this derivation follows that of
[30] with the exception that the Eddington phase function has
been replaced by the delta-Eddington phase function of Joseph et al.
[34]. New boundary conditions required for a number of
different physical situations are derived in Section 4.1. The results of
the previous sections are converted into dimensionless units in Section
4.2. The one-dimensional diffusion equation is solved analytically in
Section 4.3, and in Section 4.4 the calculation of flux, reflection, and
transmission is discussed. The three-dimensional cylindrically symmetric
solution to the diffusion equation is presented in Section 4.5. In Section
4.6 the solutions obtained using the diffusion approximation are compared
with exact solutions obtained with the adding-doubling method.
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