Abstract
The generalization of the Hamilton’s and Onsager’s variational principles for dissipative hydrodynamical systems is represented in terms of the mechanical and the heat displacement fields. A system of equations for these fields is derived from the extreme condition for action with a Lagrangian in the form of the difference between the kinetic and the free energies minus the time integral of the dissipation function. The generalized hydrodynamic equation system is then evaluated on the basis of the generalized variational principle. At low frequencies, this system corresponds to the traditional Navier–Stokes equation system, and in the high frequency limit it describes propagation of acoustical and heat modes with the finite propagation velocities.
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Maximov, G.A. (2010). Generalized Variational Principle for Dissipative Continuum Mechanics. In: Maugin, G., Metrikine, A. (eds) Mechanics of Generalized Continua. Advances in Mechanics and Mathematics, vol 21. Springer, New York, NY. https://doi.org/10.1007/978-1-4419-5695-8_31
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DOI: https://doi.org/10.1007/978-1-4419-5695-8_31
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