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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

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

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around ships, to industrial processes such as ®lling of moulds. All these situations deal<br />

with a ¯uid which is incompressible and in which the viscous e€ects either can be<br />

important or on the other hand may be neglected. <strong>The</strong> only di€erence from solving<br />

the type of problem which we have discussed in the previous chapter is the fact<br />

that the position of the free surface is not known a priori and has to be determined<br />

during the computation.<br />

On the free surface we have at all times to ensure that (1) the pressure (which<br />

approximates the normal traction) and tangential tractions are zero unless speci®ed<br />

otherwise, and (2) that the material particles of the ¯uid belong to the free surface<br />

at all times.<br />

Obviously very considerable non-linearities occur and the problem will have to be<br />

solved iteratively. We shall therefore concentrate in the following presentation on a<br />

typical situation in which such iteration can be used. <strong>The</strong> problem chosen for the<br />

more detailed discussion is that of ship hydrodynamics though the reader will<br />

obviously realize that for the other problems shown somewhat similar procedures<br />

of iteration will be applicable though details may well di€er in each application.<br />

5.2.2 Free surface wave problems in ship hydrodynamics<br />

Figure 5.2 shows a typical problem of ship motion together with the boundaries<br />

limiting the domain of analysis. In the interior of the domain we can use either the<br />

x 2<br />

x 1<br />

Fig. 5.2 A typical problem of ship motion.<br />

η<br />

Datum<br />

Free surface<br />

Ω<br />

Ship<br />

Free surface ¯ows 145<br />

u 0

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