The nonlinear partial differential equations of atmospheric dynamics govern motion on two time scales, a fast one and a slow one. Only the slow-scale motions are relevant in predicting the evolution of large weather patterns. Implicit numerical methods are therefore attractive for weather prediction
Multidomain implicit numerical scheme
โ Scribed by A. Povitsky; M. Wolfshtein
- Publisher
- John Wiley and Sons
- Year
- 1997
- Tongue
- English
- Weight
- 270 KB
- Volume
- 25
- Category
- Article
- ISSN
- 0271-2091
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โฆ Synopsis
A multidomain method for the solution of elliptic CFD problems with an ADI scheme is described. Two methods of treatment of internal boundary conditions for ADI functions are discussed, namely an explicit and a semiimplicit method. Stability conditions for the proposed methods are derived theoretically. The semi-implicit scheme is more stable than the explicit scheme, leading to improved numerical efยฎciency for multidomain computations. Numerical computations for a linear convectionยฑdiffusion equation, for buoyancy-driven recirculating ยฏow in a square cavity and for turbulent ยฏow in a square duct conยฎrmed the theoretical results. Computer runs of the multidomain code in a distributed memory multiprocessor system were successful and efยฎcient and produced reliable results.
๐ SIMILAR VOLUMES
Previous studies of interface conditions satisfying one or more of the above criteria for various applications have concen-Multidomain treatments are studied in order to solve the steady compressible Euler equations using implicit time-dependent finite trated mainly on explicit difference schemes. C
This study formulates general guidelines to extend an explicit code with a great variety of implicit and semi-implicit time integration schemes. The discussion is based on their specific implementation in the Versatile Advection Code, which is a general purpose software package for solving systems o
Possible extensions of the present scheme to further improve efficiency are also discussed.
A fully coupled, implicit, numerical scheme has been developed for solving highly stiff systems of parabolic conservation equations. The finite-domain equations are formed by integration of the governing conservation equations, expressed in vector notation, over control volumes. The central idea is