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Titlebook: Computational Hydraulics; An Introduction Cornelis B. Vreugdenhil Textbook 1989 Springer-Verlag Berlin Heidelberg 1989 Software.algorithm.c

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樓主: 哪能仁慈
31#
發(fā)表于 2025-3-26 23:31:24 | 只看該作者
32#
發(fā)表于 2025-3-27 04:11:01 | 只看該作者
,Convection—Diffusion,mber of causes by which a substance (such as salt or a waste material but also temperature) is spread out in addition to being transported with the mean flow: molecular diffusion, turbulent mixing, and (very importantly) variations of flow velocity over the river cross-section. For a detailed discus
33#
發(fā)表于 2025-3-27 05:30:37 | 只看該作者
,Numerical Accuracy for Convection—Diffusion,s gets quite complicated, as an additional parameter (the Courant number) comes in. For practical purposes, it is often sufficient to consider diffusion and convection separately, and in that order. The procedure is then:
34#
發(fā)表于 2025-3-27 11:20:53 | 只看該作者
Salt Intrusion in Estuaries,influence. If there is hardly any tide, the salt water will penetrate underneath the fresh river water as a “salt wedge”. Far more common is the situation where a strong tidal action takes care of a mixing process, such that the water in a particular cross-section has an almost uniform salt concentr
35#
發(fā)表于 2025-3-27 17:06:38 | 只看該作者
Boundary Layers, bottom at sufficiently high velocity, sand will be picked up and carried with the flow, even though it tends to fall back. The process by which sediment particles are kept in suspension is turbulent diffusion. Just as in chapter 11, turbulence causes an effective transport from regions with high sa
36#
發(fā)表于 2025-3-27 18:04:02 | 只看該作者
Long Waves,cal formulation can be obtained by integrating the general hydrodynamic equations over the depth or over a river cross-section. To understand the principles, it is sufficient to use a very much simplified set of equations in this chapter and the next one. For completeness, some of the corresponding
37#
發(fā)表于 2025-3-28 01:24:36 | 只看該作者
38#
發(fā)表于 2025-3-28 03:07:08 | 只看該作者
Long Waves in Two-Dimensional Areas, flood plains and similar situations. In many such cases, the wave length is so much larger than the water depth that a two-dimensional, depth-averaged mathematical model is adequate. The formulation is essentially the same as in Chapters 15 and 16, if the dependence on two horizontal coordinates .,
39#
發(fā)表于 2025-3-28 07:29:08 | 只看該作者
Potential Flow,ise there is an additional, similar equation), together with the equation of continuity .The numerical solution of these equations is not discussed in this book. There are, however, certain situations in which they can be considerably simplified. Consider a quantity called the vorticity ., which is
40#
發(fā)表于 2025-3-28 12:22:24 | 只看該作者
Variational Calculus on Lie Groups,mediate between purely theoretical and experimental. It is concerned with simulation of the flow of water, together with its consequences, using numerical methods on computers. There is not a great deal of difference with computational hydrodynamics or computational fluid dynamics, but these terms a
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