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Titlebook: Computational Fluid Dynamics 2000; Proceedings of the F Nobuyuki Satofuka Conference proceedings 2001 Springer-Verlag Berlin Heidelberg 200

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樓主: Lampoon
11#
發(fā)表于 2025-3-23 09:56:17 | 只看該作者
12#
發(fā)表于 2025-3-23 16:06:40 | 只看該作者
Methods of Clinical Application,ata structure is proposed to avoid data dependency that is faced when applying unstructured data for high performance computation. Two flow solvers are constructed using two different schemes. One solver uses the MUSCL-Hancock scheme, a second-order upwind scheme, another employs a second-order cent
13#
發(fā)表于 2025-3-23 19:41:47 | 只看該作者
14#
發(fā)表于 2025-3-23 22:40:17 | 只看該作者
Gary J. Dunderdale,Atsushi Hozumiressible steady flow over a flat plate is chosen for demonstrating this performance. An application for the practical flow problem is also presented such as unsteady nozzle starting process in this paper.
15#
發(fā)表于 2025-3-24 05:56:32 | 只看該作者
16#
發(fā)表于 2025-3-24 10:17:31 | 只看該作者
17#
發(fā)表于 2025-3-24 11:07:31 | 只看該作者
Howard F. Hunt,Milton A. Trapoldeady shock wave interactions with bodies. The mathematical model is based on the Navier-Stokes equations. The most important ingredients of the method are specially tailored adaptive unstructured grids and an efficient combination of explicit and implicit time integration modes which are chosen to b
18#
發(fā)表于 2025-3-24 17:29:20 | 只看該作者
Charles R. Schuster,Joseph V. Bradyclass of quadrature formulae for fluctuation computation is proposed which allows a stable structure of discrete shocks, yet preventing nonphysical shocks. Computational results for Burgers’ equation are shown to demonstrate its sharp shock capturing ability.
19#
發(fā)表于 2025-3-24 21:45:36 | 只看該作者
20#
發(fā)表于 2025-3-24 23:49:59 | 只看該作者
Defect and Adjoint Error Correctionccuracy of numerical solutions, and adjoint error correction to improve the order of accuracy of derived output functionals such as far-field boundary integrals. Numerical results for the 1D Helmholtz equation on an irregular grid show fourth order accuracy for the numerical solution, and sixth order accuracy for the boundary value.
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