scholarly journals Stability of Talagrand’s Gaussian transport-entropy inequality via the Föllmer process

Author(s):  
Dan Mikulincer
Keyword(s):  
2015 ◽  
Vol 115 (3) ◽  
Author(s):  
Robie A. Hennigar ◽  
Robert B. Mann ◽  
David Kubizňák

2016 ◽  
Vol 85 (302) ◽  
pp. 2815-2837 ◽  
Author(s):  
Emmanuel Audusse ◽  
François Bouchut ◽  
Marie-Odile Bristeau ◽  
Jacques Sainte-Marie

2018 ◽  
Vol 187 (1) ◽  
pp. 95-107
Author(s):  
Qingzhong Huang ◽  
Ai-Jun Li
Keyword(s):  

Author(s):  
Christos Varsakelis ◽  
Miltiadis V. Papalexandris

AbstractA conundrum in non-equilibrium thermodynamics of heterogeneous mixtures with microstructure concerns the selection of thermodynamic currents and forces in the entropy production rate from the multitude of available options. The objective of this article is to demonstrate that the low-Mach-number approximation can narrow down this ambiguity. More specifically, by postulating that the post-constitutive equations are well behaved with respect to this perturbation analysis we assert that thermal non-equilibrium should be chosen as an independent force even if this requires the explicit manipulation of the entropy inequality. According to our analysis, alternative choices result in post-constitutive equations; the incompressible limit of which gives rise to questionable predictions.


1973 ◽  
Vol 74 (1) ◽  
pp. 185-197
Author(s):  
K. A. Lindsay

AbstractIn this paper we study a mixture of a viscous fluid and an elastic solid using a global Clausius–Duhem entropy inequality. Results are similar in character to those obtained by previous writers using a more restricted type of entropy inequality. Special attention is given to the case of a mixture of a Newtonian fluid and an elastic solid.


2010 ◽  
Vol 140 (6) ◽  
pp. 1161-1186 ◽  
Author(s):  
Wolfgang Dreyer ◽  
Christiane Kraus

We study the thermodynamic consistency of phase-field models, which include gradient terms of the density ρ in the free-energy functional such as the van der Waals–Cahn–Hilliard model. It is well known that the entropy inequality admits gradient and higher-order gradient terms of ρ in the free energy only if either the energy flux or the entropy flux is represented by a non-classical form. We identify a non-classical entropy flux, which is not restricted to isothermal processes, so that gradient contributions are possible.We then investigate equilibrium conditions for the van der Waals–Cahn–Hilliard phase-field model in the sharp interface limit. For a single substance thermodynamics provides two jump conditions at the sharp interface, namely the continuity of the Gibbs free energies of the adjacent phases and the discontinuity of the corresponding pressures, which is balanced by the mean curvature. We show that these conditions can be also extracted from the van der Waals–Cahn–Hilliard phase-field model in the sharp interface limit. To this end we prove an asymptotic expansion of the density up to the first order. The results are based on local energy estimates and uniform convergence results for the density.


2013 ◽  
Vol 11 (8) ◽  
Author(s):  
Mehmet Ersoy ◽  
Frédéric Golay ◽  
Lyudmyla Yushchenko

AbstractWe propose a 1D adaptive numerical scheme for hyperbolic conservation laws based on the numerical density of entropy production (the amount of violation of the theoretical entropy inequality). This density is used as an a posteriori error which provides information if the mesh should be refined in the regions where discontinuities occur or coarsened in the regions where the solution remains smooth. As due to the Courant-Friedrich-Levy stability condition the time step is restricted and leads to time consuming simulations, we propose a local time stepping algorithm. We also use high order time extensions applying the Adams-Bashforth time integration technique as well as the second order linear reconstruction in space. We numerically investigate the efficiency of the scheme through several test cases: Sod’s shock tube problem, Lax’s shock tube problem and the Shu-Osher test problem.


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