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首页> 外文期刊>Numerical Heat Transfer, Part B. Fundamentals: An International Journal of Computation and Methodology >Co-located variables approach using implicit Runge-Kutta methods for unsteady incompressible flow simulation
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Co-located variables approach using implicit Runge-Kutta methods for unsteady incompressible flow simulation

机译:使用隐式Runge-Kutta方法的共处变量方法,用于非稳态不可压缩流模拟

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A numerical method for transient incompressible viscous flow simulation is presented with a nonstaggered grid (co-located variables) approach. A special class of implicit Runge-Kutta (RK) methods is used for time discretization in conjunction with finite-volume-based semi-implicit pressure linked equations (SIMPLE) algorithm. Owing to the use of implicit RK methods, the proposed method can be used to achieve an arbitrarily high order of accuracy in time-discretization which is otherwise limited to second order in the majority of the currently available simulation techniques. The nonstaggered grid method was tested by solving for velocity field in a lid-driven square cavity. In the test case calculations, the Power Law scheme of Patankar [9] was used in spatial discretization, and time discretization was performed using a second-order implicit Runge-Kutta method. The results from the current method were compared with the results obtained from the staggered grid method of Ijaz and Anand [10-12]. The current method produced results that were nearly equivalent to the ones obtained by using the staggered grid approach. Moreover, the current method was found to have better convergence characteristics compared to the staggered grid method when applied to the lid-driven square cavity problem.
机译:提出了一种非交错网格(同位变量)方法的瞬态不可压缩粘性流模拟数值方法。一类特殊的隐式Runge-Kutta(RK)方法与基于有限体积的半隐式压力链接方程(SIMPLE)算法一起用于时间离散。由于使用了隐式RK方法,因此可以将所提出的方法用于在时间离散化方面获得任意高的精度,而在大多数当前可用的仿真技术中,该精度仅限于二阶。通过求解盖驱动方腔中的速度场,测试了非交错网格方法。在测试用例计算中,将Patankar [9]的幂定律方案用于空间离散化,并使用二阶隐式Runge-Kutta方法执行时间离散化。将当前方法的结果与Ijaz和Anand [10-12]的交错网格方法获得的结果进行比较。当前方法产生的结果几乎与使用交错网格方法获得的结果相同。此外,当将当前方法应用于盖驱动方腔问题时,与交错网格方法相比,它具有更好的收敛特性。

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