2019
DOI: 10.1002/mma.5766
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On the convergence toward nonequilibrium stationary states in thermostatted kinetic models

Abstract: A differential equation-based framework is suitable for the modeling of nonequilibrium complex systems if its solution is able to reach, as time goes to infinity, the related nonequilibrium steady states. The thermostatted kinetic theory framework has been recently proposed for the modeling of complex systems subjected to an external force field. The present paper is devoted to the mathematical proof of the convergence of the solutions of the thermostatted kinetic framework towards the related nonequilibrium s… Show more

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Cited by 8 publications
(4 citation statements)
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“…As is known, the well-posedness in the Hadamard sense of a model ensures the development of numerical methods for the analysis of the numerical solutions and simulations. The proof of the existence and uniqueness of the nonequilibrium stationary state and the convergence results can be pursued by employing fixed-point arguments, measure theory and Fourier transform; see [76][77][78].…”
Section: A Critical Analysis and Research Perspectivesmentioning
confidence: 99%
“…As is known, the well-posedness in the Hadamard sense of a model ensures the development of numerical methods for the analysis of the numerical solutions and simulations. The proof of the existence and uniqueness of the nonequilibrium stationary state and the convergence results can be pursued by employing fixed-point arguments, measure theory and Fourier transform; see [76][77][78].…”
Section: A Critical Analysis and Research Perspectivesmentioning
confidence: 99%
“…The existence of solutions of the nonequilibrium stationary problem related to (1) is proved in [31]. A proof of the convergence of the solution of (3) to the nonequilibrium stationary solution as time goes to infinity is given in [32]. In many cases of interest, as for example in the description of the diffusion of epidemics η(u * , u * ) can be supposed to be constant, i.e., there exists η > 0 such that η(u * , u * ) = η, for all u * , u * ∈ D u .…”
Section: The Continuous Activity Frameworkmentioning
confidence: 99%
“…Proof. Bearing the (27) in mind, and by using the (32), straightforward calculations show, for i ∈ {1, 2, . .…”
Section: The Discrete Activity Frameworkmentioning
confidence: 99%
“…Bellomo and coworkers stressed in particular two concepts are of the utmost relevance in applying theory of active particles to living matter: (i) new agents that are generated can have an activity different than the one of their parent agent; (ii) non destructive interactions between two agents of the same or of different species (e.g., tumor cells and immune system effectors) can induce a change of activity level in both agents. Among the most recent developments of the Bellomo theories we cite: (i) the theory of thermostatted active particles, which allows to impose physically backgrounded constraints to the activity of individuals, developed by Bianca and Menale [21][22][23]; (ii) the stochastic evolutionary theory of tumor adaptation developed by Clairambault, Delitala, Lorenzi and coworkers [24][25][26][27][28][29]. Finally, it is worth mentioning the mathematical modeling of Darwinian species emergence by Volpert and colleagues that represent the evolution of active particles uniquely subject to a Brownian force and logistic non-local growth [30][31][32].…”
Section: Introductionmentioning
confidence: 99%