• CN:11-2187/TH
  • ISSN:0577-6686

›› 1979, Vol. 15 ›› Issue (1): 86-99.

• 论文 • 上一篇    下一篇

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叶轮机械三元流动流函数方程组——S1和S2流面的统一数学方程组

吴文权   

  1. 中国科学院
  • 发布日期:1979-01-01

Stream Function Equations of Three-Dimensional Flow in Turbomachine——Unified Equations Governing Fluid Flow on S1 and S2 Relative Stream Surfaces

Wu Wenquan   

  1. Academia Sinica
  • Published:1979-01-01

摘要: 随着计算机和计算技术的发展,直接求解叶轮机械三元流动成为新发展的一个问题。本文提出了直接求解叶轮机械三元流动的一个方法。在本文中引入了三元流动流函数。对吴仲华叶轮机械三元流动通用理论中的S1和S2相对流面理论作了统一的数学表达,进一步阐明了流面的意义,对流面理论中连续方程所引入的流片厚度τ作了一个严格的数学推导。所得的结果同流面理论中的结果,和其物理意义都是一致的。这样所得的流动图案是最一般的情况。而我们以往常常使用的任意回转面流动、圆柱面流动、轴对称流动等都是其中某些简化的特例。由所引入的三元流动流函数,从叶轮机械基本方程组,推导得出了包括S1和S2两族流面上流动的统一流函数方程组。由此可以明确看到S1和S2两族流面相互迭代计算的意义和途径。进一步讨论了方程组正问题求解的边界条件和求解方法,从而提出了直接求解三元流动的一种新的方法。在这方法是同时直接求解三元空间内计算节点上ψ1和ψ2两个流函数值。这两个ψ1和ψ2是通过两个联立的流函数方程组迭代求解而得的。解得两个流函数值后,从而再解出所有气动参数。这方法不同于其它直接解速度分量形式的三元流动方程。后者是求解三元空间内计算节点上三个或三个以上未知数。因此看来这个新方法有可能比其他直接解法更容易在计算机上求得完整的三元流动解。

Abstract: The direct solution of three-dimensional flow in turbomachine are developed recently with the aid of computer and computational mathematics. In this papers, a new method is presented. The three-dimensional flow stream functions were introduced. The unified mathematical expressions for S1 and S2 relative stream surfaces model of Wu’s general flow theory for turbomachine were obtained. Further, the significance of stream surfaces was elucidated with these stream functions. Thickness of the stream surface appeared in the continuity equation of the stream surface model was derived in different way. These results coincided with those obtained from the stream surfaces model, and the physical significances of thickness of the stream surface were the same. Thus, the general flow pictures were obtained. And usually, the flow cases, such as arbitrary revolution surface, cylindrical surface, and axisymmetrical surface etc..met the special cases. The unified stream function equations governing the fluid flow on S1 and S2 relative stream surfaces were derived with the aid of the three-dimensional stream functions according to Wu’s basic aero-thermodynamic equations of flow in turbomachine. The significance and the approach of the iterative calculation of S1 and S2 stream surfaces can be easily understood. Further, the boundary conditions and the method of solution of the equations were discussed. So a new method of direct solution for three-dimensional flow in turbomachine is presened here. In this way, the both stream functions Ψ1 andΨ2, are calculated on computational nodes in three-dimensional space. The values of Ψ1 andΨ2 are obtained by iterative solution of two simultaneous stream function equations. All the aero-thermodynamic parameters can be obtained, by the general formulae. This method is different from the solution of three-dimensional flow equations expressed with respect to velocity components. In the latter case, three or more unknown functions must be calculated. This new method is probably more easy than the conventional methods in order to get the integral three-dimensional flow in turbomachine with the aid of computers.