On SN-PN Equivalence

Richard Sanchez
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引用次数: 4

Abstract

We consider the artificial conversion of the discrete–ordinates (SN) equations into a system of spherical harmonic (PN) equations. This is done by adding to the SN equations an artificial source that has two components. The first component transforms the SN scattering term into PN-like scattering, while the second modifies the SN streaming operator into a lower-order PN streaming operator. Denoting by and the spaces of solutions of the SN and PN equations, respectively, we define SN-PN equivalence via a constructive Proposition based on two linear morphisms, and , such that if ψ is the solution of the SN equations with source S+π*(S), then π K ψ is solution of the PN equations with source π K S. We proceed then to prove this Proposition by constructing the two components of the artificial source. We also prove that when the morphism π* is not unique, and propose a general form for the second component of the artificial source, which is shown to comprise all artificial sources previously proposed in the literature.
关于SN-PN等价
我们考虑将离散坐标方程(SN)人工转换为球谐方程(PN)系统。这是通过在SN方程中加入一个有两个组成部分的人工源来实现的。第一个组件将SN散射项转换为类PN散射,第二个组件将SN流算子修改为低阶PN流算子。我们分别用和表示SN和PN方程的解的空间,通过一个基于两个线性态射的构造命题定义了SN-PN等价,并且,使得如果ψ是源为S+π*(S)的SN方程的解,则π K ψ是源为π K S的PN方程的解,然后通过构造人工源的两个分量来证明这个命题。我们还证明了当态射π*不唯一时,并给出了人工源第二分量的一般形式,它包含了以前文献中提出的所有人工源。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Transport Theory and Statistical Physics
Transport Theory and Statistical Physics 物理-物理:数学物理
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