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首页> 外文期刊>International Journal for Numerical Methods in Fluids >DAMPED ARTIFICIAL COMPRESSIBILITY ITERATION SCHEME FOR IMPLICIT CALCULATIONS OF UNSTEADY INCOMPRESSIBLE FLOW
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DAMPED ARTIFICIAL COMPRESSIBILITY ITERATION SCHEME FOR IMPLICIT CALCULATIONS OF UNSTEADY INCOMPRESSIBLE FLOW

机译:隐式计算非定常不可压流动的阻尼人工压缩迭代方案

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Peyret (J. Fluid Meek, 78,49-63 (1976)) and others have described artificial compressibility iteration schemes for solving implicit time discretizations of the unsteady incompressible Navier-Slokes equations. Such schemes solve the implicit equations by introducing derivatives with respect to a pseudo-time variable x and marching out to a steady state in t. The pseudo-time evolution equation for the pressure of takes the form ap/at=a~2▽.u, where a is an artificial compressibility parameter and u is die fluid velocity vector. We present a new scheme of this type in which convergence is accelerated by a new procedure for setting a and by introducing an artificial bulk viscosity b into the momentum equation. This scheme is used to solve the non-Iinoar equations resulting from a fully implicit time differencing schema for unsteady incompressible flow. We find that the best values of a and b are generally quite different from those in the analogous scheme for steady flow (J. D. Rainsbaw and V. A. Mousseau, Comput; Fluids, 18, 361-367 (1990)), owing to the previously unrecognized fact that the character of the system is profoundly altered by the presence of the physical time derivative terms. In particular, a Fourier dispersion analysis shows that a no longer has the significance of a wave speed for finite values of the physical time step A. Indeed, if one sets as usual, the artificial sound waves cease to exist when A/is small and this adversely affects the iteration convergence rale. Approximate analytical expressions fi? a and b arc proposed and the benefits of their use relative to the conventional values a ~ |u| and b=0 are illustrated in simple test calculations.
机译:Peyret(J. Fluid Meek,78,49-63(1976))等人描述了人工可压缩性迭代方案,用于求解非稳态不可压缩Navier-Slokes方程的隐式时间离散化。这样的方案通过引入关于伪时间变量x的导数并在t内进入稳态来求解隐式方程。压力的伪时间演化方程采用ap / at = a〜2▽.u的形式,其中a是人工可压缩性参数,u是流体速度矢量。我们提出了这种类型的新方案,其中通过设置a的新过程以及通过将人造体积粘度b引入动量方程来加速收敛。该方案用于求解由非隐含不可压缩流的完全隐式时间差分方案产生的非伊诺尔方程。我们发现a和b的最佳值通常与稳态流的类似方案中的值大不相同(JD Rainsbaw和VA Mousseau,Comput; Fluids,18,361-367(1990)),这是由于先前无法识别的事实物理时间导数项的存在极大地改变了系统的特性。特别是,傅立叶色散分析表明,对于物理时间步长A的有限值,波速不再具有波速的意义。实际上,如果像往常那样设置,则当A /很小时,人造声波就不复存在了。这会对迭代收敛规则产生不利影响。近似解析表达式提出了a和b及其相对于常规值a〜| u |的使用好处。在简单的测试计算中说明了b = 0。

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