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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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5<br />

Free surfaces, buoyancy and<br />

turbulent incompressible ¯ows<br />

5.1 Introduction<br />

In the previous chapter we have introduced the reader to general methods of solving<br />

incompressible ¯ow problems and have illustrated these with many examples of<br />

newtonian and non-newtonian ¯ows. In the present chapter, we shall address three<br />

separate topics of incompressible ¯ow which were not dealt with in the previous<br />

chapters. This chapter is thus divided into three parts. In the ®rst two parts the<br />

common theme is that of the action of the body force due to gravity. We start with<br />

a section addressed to problems of free surfaces and continue with the second section<br />

which deals with buoyancy e€ects caused by temperature di€erences in various parts<br />

of the domain. <strong>The</strong> third part discusses the important topic of turbulence and we shall<br />

introduce the reader here to some general models currently used in such studies. This<br />

last section will inevitably be brief and we will simply illustrate the possibility of<br />

dealing with time averaged viscosities and Reynolds stresses. We shall have occasion<br />

later to use such concepts when dealing with compressible ¯ows in Chapter 6.<br />

However the ®rst two topics of incompressible ¯ow are of considerable importance<br />

and here we shall discuss matters in some detail.<br />

<strong>The</strong> ®rst part of this chapter, Sec. 5.2, will deal with problems in which a free<br />

surface of ¯ow occurs when gravity forces are acting throughout the domain. Typical<br />

examples here would be for instance given by the disturbance of the free surface of<br />

water and the creation of waves by moving ships or submarines. Of course other<br />

problems of similar kinds arise in practice. Indeed in Chapter 7, where we deal<br />

with shallow water ¯ows, a free surface is an essential condition but other assumptions<br />

and simpli®cations have to be introduced. Here we deal with the full problem<br />

and include either complete viscous e€ects or simply deal with an inviscid ¯uid<br />

without further physical assumptions. <strong>The</strong>re are other topics of free surfaces which<br />

occur in practice. One of these for instance is that of mould ®lling which is frequently<br />

encountered in manufacturing where a particular ¯uid or polymer is poured into a<br />

mould and solidi®es. We shall brie¯y refer to such examples. Space does not permit<br />

us to deal with this important problem in detail but we give some references to the<br />

current literature.<br />

In Sec. 5.3, we invoke problems of buoyancy and here we can deal with pure<br />

(natural) convection when the only force causing the ¯ow is that of the di€erence

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