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An investigation of the diffusion errors in diffusion vortex methods

机译:扩散涡旋方法中扩散误差的研究

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To model the viscous effect, the core area of particles in Leonard's core spreading vortex method must grow linearly in time, which however results in growing convective errors and consequently causes the failure of a correct convergence of the method to the Navier-Stokes equations. The so-called diffusion vortex method was proposed and claimed to have smaller core-area growth rates because part of the viscous effect is modeled into the movement of particles. The growth rates however are non-uniform and an additional diffusion error arises due to the nonzero divergence of the diffusion velocity. The goal of this work is to analyze the associated errors of several existing versions of the diffusion vortex method and compare them with that of Leonard's. Simulations of two axisymmetric flows are performed to measure the involved diffusion errors and consequently distinguish these diffusion vortex methods. The results show that the circulation conservation is important, besides a small core-area growth rate, in obtaining a good accuracy. Under the consideration of both efficiency and accuracy, the diffusion vortex method in which each vortex particle conserves its own circulation on its core area alone is recommended.
机译:为了模拟粘性效应,伦纳德核心扩展涡旋方法中粒子的核心面积必须随时间线性增长,但这会导致对流误差增大,从而导致该方法无法正确收敛到Navier-Stokes方程。提出了所谓的扩散涡旋方法,并声称其具有较小的核心区域增长率,因为一部分粘性效应被建模为粒子的运动。然而,增长率是不均匀的,并且由于扩散速度的非零散度会产生附加的扩散误差。这项工作的目的是分析几种现有版本的扩散涡旋方法的相关误差,并将其与伦纳德的误差进行比较。进行了两个轴对称流的模拟,以测量所涉及的扩散误差,从而区分了这些扩散涡旋方法。结果表明,除了获得较小的核心面积增长率之外,循环保存对于获得良好的精度也很重要。考虑到效率和准确性,建议采用扩散涡旋方法,其中每个涡旋粒子仅在其核心区域保留自己的循环。

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