A novel variational derivation of the Navier-Stokes equations for incompressible flows is presented and discussed. The Lagrangian density is obtained from the exergy balance equation written for both the (Lagrangian) steady and quasi-stationary isothermal flows of an incompressible fluid. The exergy of a fluid mass (composed of a kinetic, a pressure-work, a diffusive, and a dissipative portion, the latter being the result of viscous irreversibility) is derived first, and it is then shown that a formal minimisation of the exergy variation (i.e. destruction) generates, without recurring to “local potentials”, the Navier-Stokes equations of motion under the given assumptions. The acceleration being held constant, the proposed variational method can be classified as a “restricted” principle.
The problem is also briefly discussed both in its historical perspective and in its possible formal and practical implications.
Primary Language | English |
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Journal Section | Regular Original Research Article |
Authors | |
Publication Date | September 1, 2004 |
Published in Issue | Year 2004 Volume: 7 Issue: 3 |