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Advanced Differential Approximation Formulation of the P_N Method for Radiative Transfer

机译:P_N方法用于辐射传递的高级微分近似公式

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The spherical harmonics (P_N) method, especially its lowest order, i.e., the P_1 or differential approximation, enjoys great popularity because of its relative simplicity and compatibility with standard models for the solution of the (overall) energy equation. Low-order P_N approximations perform poorly in the presence of strongly nonisotropic intensity distributions, especially in optically thin situations within nonisothermal enclosures (due to variation in surface radiosities across the enclosure surface, causing rapid change of irradiation over incoming directions). A previous modification of the P_N approximation, i.e., the modified differential approximation (MDA), separates wall emission from medium emission to reduce the nonisotropy of intensity. Although successful, the major drawback of this method is that the intensity at the walls is set to zero into outward directions, while incoming intensity is nonzero, resulting in a discontinuity at grazing angles. To alleviate this problem, a new approach, termed here the "advanced differential approximation (ADA)," is developed, in which the directional gradient of the intensity at the wall is minimized. This makes the intensity distribution continuous for the P_1 method and mostly continuous for higher-order P_N methods. The new method is tested for a 1D slab and concentric spheres and for a 2D medium. Results are compared with the exact analytical solutions for the ID slab as well as the Monte Carlo-based simulations for 2D media.
机译:球谐函数(P_N)方法尤其是其最低阶(即P_1或微分逼近)由于其相对简单并且与用于(整体)能量方程的标准模型兼容而受到广泛欢迎。在存在强烈的非各向同性强度分布的情况下,低阶P_N近似效果很差,尤其是在非等温外壳内的光学薄情况下(由于外壳表面的表面辐射率变化,导致入射方向上的辐射发生快速变化)。 P_N逼近的先前修改,即修改的微分逼近(MDA),将壁发射与介质发射分开以减小强度的各向异性。虽然成功,但此方法的主要缺点是在向外的方向上,壁处的强度设置为零,而入射强度为非零,导致掠射角不连续。为了减轻这个问题,开发了一种新的方法,在此称为“高级微分逼近(ADA)”,其中将墙体处的强度方向梯度最小化。这使得强度分布对于P_1方法是连续的,而对于高阶P_N方法几乎是连续的。新方法已针对一维平板和同心球以及二维介质进行了测试。将结果与ID平板的精确解析解决方案以及基于Monte Carlo的2D媒体模拟进行比较。

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