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Stefanos Georgiadis

Publications and source records attributed to Stefanos Georgiadis.

11 recordsLinked to original sources

Global existence of weak solutions for the Maxwell--Stefan system in the whole space

We prove the global-in-time existence of weak solutions to the isothermal Maxwell--Stefan system on the whole space $\mathbb R^3$. The main difficulty is that, unlike in bounded domains, the concentrations generally have infinite mass and the standard mixing entropy is not finite. We therefore work with the relative entropy with respect to a strictly positive constant equilibrium state. The proof proceeds by solving the problem on balls $B_R$ with no-flux boundary conditions, using the bounded-domain entropy theory, and deriving estimates independent of $R$. These estimates yield uniform control of the relative entropy, the gradients $\nabla\sqrt{c_i}$, and the fluxes $J_i$. Passing to the limit $R\to\infty$ is achieved by local compactness and a diagonal argument. The resulting weak solution satisfies the Maxwell--Stefan system in the sense of distributions and obeys a global relative entropy inequality.

math.AP↗

Analysis of a nonisothermal Maxwell--Stefan system with degenerate thermal conductivity

We prove the global-in-time existence of weak solutions for the Maxwell--Stefan--Fourier system with physically motivated degenerate thermal conductivity $κ(θ)=θ^α$, for $0<α\leq2$. In contrast to existing nonisothermal compressible theories based on nondegenerate conductivities, the entropy inequality no longer gives control of the quantities $\nablaθ$ and $\nabla \logθ$. The main new ingredient is a renormalized energy estimate, which yields compactness of the temperature and allows the identification of the degenerate heat flux.

math.AP↗

On the existence of non-negative weak solutions for $1D$ fourth order equations of gradient flow type

In this paper, we consider a family of one-dimensional fourth order evolution equations arising as gradient flows of the Korteweg energy, i.e. the $L^2$-norm of the first derivative of some power of the density. This family of equations generalizes the Quantum-Drift-Diffusion equation and the Thin-Film equation. We prove the global-in-time existence of {\em non-negative} weak solutions without requiring any upper bound on the exponent of the power of the density in the energy.

math.AP↗

Renormalized solutions for the Maxwell--Stefan system with an application to uniqueness of weak solutions

We give conditions that guarantee uniqueness of renormalized solutions for the Maxwell-Stefan system. The proof is based on an identity for the evolution of the symmetrized relative entropy. Using the method of doubling the variables we derive the identity for two renormalized solutions and use information on the spectrum of the Maxwell-Stefan matrix to estimate the symmetrized relative entropy and show uniqueness. We then show that weak solutions for the Maxwell-Stefan system have sufficient regularity to produce renormalized solutions. Combining the two results yields a uniqueness result for weak solutions of the Maxwell-Stefan system with bounded fluxes.

math.AP↗

Alignment via friction for nonisothermal multicomponent fluid systems

The derivation of an approximate Class-I model for nonisothermal multicomponent systems of fluids, as the high-friction limit of a Class-II model is justified, by validating the Chapman-Enskog expansion performed from the Class-II model towards the Class-I model. The analysis proceeds by comparing two thermomechanical theories via relative entropy.

math.AP↗

Three results on the Energy conservation for the 3D Euler equations

We consider the 3D Euler equations for incompressible homogeneous fluids and we study the problem of energy conservation for weak solutions in the space-periodic case. First, we prove the energy conservation for a full scale of Besov spaces, by extending some classical results to a wider range of exponents. Next, we consider the energy conservation in the case of conditions on the gradient, recovering some results which were known, up to now, only for the Navier-Stokes equations and for weak solutions of the Leray-Hopf type. Finally, we make some remarks on the Onsager singularity problem, identifying conditions which allow to pass to the limit from solutions of the Navier-Stokes equations to solution of the Euler ones, producing weak solutions which are energy conserving.

math.AP↗

Global existence of weak solutions and weak-strong uniqueness for nonisothermal Maxwell-Stefan systems

The dynamics of multicomponent gas mixtures with vanishing barycentric velocity is described by Maxwell-Stefan equations with mass diffusion and heat conduction. The equations consist of the mass and energy balances, coupled to an algebraic system that relates the partial velocities and driving forces. The global existence of weak solutions to this system in a bounded domain with no-flux boundary conditions is proved by using the boundedness-by-entropy method. A priori estimates are obtained from the entropy inequality which originates from the consistent thermodynamic modeling. Furthermore, the weak-strong uniqueness property is shown by using the relative entropy method.

math.AP↗

Non-isothermal multicomponent flows with mass diffusion and heat conduction

A type-I model of non-isothermal multicomponent systems of gases describing mass diffusive and heat conductive phenomena is presented. The derivation of the model and a convergence result among thermomechanical theories in the smooth regime are discussed. Furthermore, the global-in-time existence of weak solutions and the weak-strong uniqueness property are established for the corresponding system with zero barycentric velocity.

math.AP↗

Asymptotic derivation of multicomponent compressible flows with heat conduction and mass diffusion

A Type-I model of a multicomponent system of fluids with non-constant temperature is derived as the high-friction limit of a Type-II model via a Chapman-Enskog expansion. The asymptotic model is shown to fit into the general theory of hyperbolic-parabolic systems, by exploiting the entropy structure inherited through the asymptotic procedure. Finally, by deriving the relative entropy identity for the Type-I model, two convergence results for smooth solutions are presented, from the system with mass-diffusion and heat conduction to the corresponding system without mass-diffusion but including heat conduction and to its hyperbolic counterpart.

math.AP↗