Abstract

As a special case of the general principle of minimal entropy production discussed in earlier parts of this series, we relate here the hydrodynamic Navier–Stokes equation including its non-linear term, to the minimisation of ∫∑ i( ∇v i) 2 dV , for fixed boundaries. The connection is made explicit for incompressible stationary flow; we shortly consider generalisations to the general pressure tensor, the non-stationary process, compressibility, and the principle of minimal entropy production.

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