2015
DOI: 10.1016/j.matpur.2015.05.003
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Two-velocity hydrodynamics in fluid mechanics: Part I Well posedness for zero Mach number systems

Abstract: In this paper we prove global in time existence of weak solutions to zero Mach number systems arising in fluid mechanics with periodic boundary conditions. Relaxing a certain algebraic constraint between the viscosity and the conductivity introduced in [D. Bresch, E.H. Essoufi, and M. Sy, J. Math. Fluid Mech. 2007] gives a more complete answer to an open question formulated in [P.-L. Lions, Oxford 1998]. We introduce a new mathematical entropy which clearly shows existence of two-velocity hydrodynamics with a … Show more

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Cited by 29 publications
(48 citation statements)
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“…Each of the velocity vector fields u and 2∇ϕ( ) is associated with different density (1 − κ) and κ , respectively. The main objective is not to prove global existence of solutions rigorously but to show that the two-velocity hydrodynamics is consistent with the study performed in the first part of the present series [11] for the zero Mach number system. Our formulation uses the generalized κ-temperature which is not a priori the usual temperature.…”
Section: Introductionmentioning
confidence: 89%
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“…Each of the velocity vector fields u and 2∇ϕ( ) is associated with different density (1 − κ) and κ , respectively. The main objective is not to prove global existence of solutions rigorously but to show that the two-velocity hydrodynamics is consistent with the study performed in the first part of the present series [11] for the zero Mach number system. Our formulation uses the generalized κ-temperature which is not a priori the usual temperature.…”
Section: Introductionmentioning
confidence: 89%
“…Here we construct the weak solution to the system similar to the considered in [39] modulo capillarity terms. It was however shown in [11] that this construction is compatible with the quantum capillary term of the form κ ∇(∆ √ / √ ) appearing in the ghost system [28], see also [21] for the study on quantum viscous Navier-Stokes system and [4] for a full range of compatible capillary terms. Concerning construction of approximate solutions with singular pressure, drag terms or capillarity terms, the authors gave some hints in [8] for the general setting λ( ) = 2(µ ( ) − µ( )).…”
Section: Introductionmentioning
confidence: 98%
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“…[19], Cai, Cao, Sun [10]. Recently, the interest in "two velocity models" has been revived in Bresch et al [7], [8].…”
Section: Vanishing Dissipation Limit Of Brenner's Modelmentioning
confidence: 99%
“…Remark A. 10. The rotation term in [13] was dealt with in a slightly different way, exploiting the special law of the classical component of the pressure.…”
Section: Proofmentioning
confidence: 99%