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Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

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7<br />

Shallow-water problems<br />

7.1 Introduction<br />

<strong>The</strong> ¯ow of water in shallow layers such as occur in coastal estuaries, oceans, rivers,<br />

etc., is of obvious practical importance. <strong>The</strong> prediction of tidal currents and elevations<br />

is vital for navigation and for the determination of pollutant dispersal which,<br />

unfortunately, is still frequently deposited there. <strong>The</strong> transport of sediments<br />

associated wth such ¯ows is yet another ®eld of interest.<br />

In free surface ¯ow in relatively thin layers the horizontal velocities are of primary<br />

importance and the problem can be reasonably approximated in two dimensions.<br />

Here we ®nd that the resulting equations, which include in addition to the horizontal<br />

velocities the free surface elevation, can once again be written in the same conservation<br />

form as the Euler equations studied in previous chapters:<br />

@<br />

@t ‡ @Fi ‡<br />

@xi @Gi ‡ Q ˆ 0 for i ˆ 1; 2 …7:1†<br />

@xi Indeed, the detailed form of these equations bears a striking similarity to those of<br />

compressible gas ¯ow ± despite the fact that now a purely incompressible ¯uid (water)<br />

is considered. It follows therefore that:<br />

1. <strong>The</strong> methods developed in the previous chapters are in general applicable.<br />

2. <strong>The</strong> type of phenomena (e.g. shocks, etc.) which we have encountered in compressible<br />

gas ¯ows will occur again.<br />

It will of course be found that practical interest focuses on di€erent aspects. <strong>The</strong><br />

objective of this chapter is therefore to introduce the basis of the derivation of the<br />

equation and to illustrate the numerical approximation techniques by a series of<br />

examples.<br />

<strong>The</strong> approximations made in the formulation of the ¯ow in shallow-water bodies<br />

are similar in essence to those describing the ¯ow of air in the earth's environment<br />

and hence are widely used in meteorology. Here the vital subject of weather prediction<br />

involves their daily solution and a very large amount of computation. <strong>The</strong> interested<br />

reader will ®nd much of the background in standard texts dealing with the subject,<br />

e.g. references 1 and 2.

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