We deal with a non-stationary flow of shear-thinning fluid in a bounded domain with perfect slip boundary condition. We provide a proof of the existence of a solution which is Holder continuous. This is a joint work with Jakub Tichy.
I will present new results on stochastic Navier-Stokes equations for compressible fluids. I will introduce the concept of "finite energy weak martingale solutions". These solutions are weak in the analytical sense and in the probabilistic sense as well. In addition, they allow to control the evolution of the total energy. So, we can study the asymptotic behavior of the problem. In particular, I will identify the stochastic incompressible Navier-Stokes equations (Euler equations) as target system if the Mach number (and the viscosity) tends to zero.
The possibility of moving, spatially localized pulses of constant or time periodic form in periodic media, e.g. in photonic crystals, is interesting from the mathematical as well as the applied side. An example is optical computing where such pulses could function as bit carriers.
Pulses in the form of asymptotically small and wide wavepackets can be studied with the help of envelope approximations. Hereby the envelope satisfies an effective equation with constant coefficients. We discuss rigorous results of such approximations in one spatial dimension on long time intervals for a nonlinear wave equation and a nonlinear Schrödinger equation. We concentrate on the asymptotic scaling which leads to the, so called, coupled mode equations (CMEs) of first order. CMEs have families of solitary waves parametrized by velocity, such that in the original model propagation of localized pulses is possible for a range of velocities at one fixed frequency. The justification proof relies on the Bloch transformation, Sobolev space estimates and the Gronwall inequality. Besides the idea of the proof we present also some numerical examples.
The transport of single-phase fluid mixtures in porous media is described by cross-diffusion equations for the chemical concentrations. The equations are obtained in a thermodynamic consistent way from mass balance, Darcy's law, and the van der Waals equation of state for mixtures. Including diffusive fluxes, the global-in-time existence of weak solutions in a bounded domain with equilibrium boundary conditions is proved, using the boundedness-by-entropy method. Based on the free energy inequality, the large-time convergence of the solution to the constant equilibrium concentration is shown. For the two-species model and specific diffusion matrices, an integral inequality is proved, which reveals a maximum and minimum principle for the ratio of the concentrations. Without diffusive fluxes, the two-dimensional pressure is shown to converge exponentially fast to a constant. Numerical examples in one space dimension illustrate this convergence.
We study a model of a mixture of fluids which is modeled by an incompressible nonNewtonian
(power-law) fluid. We allow that the constituents may undergo chemical
reactions and the fluid in total can transfer heat and is generally electrically charged.
We show existence of a weak solution to the corresponding system of partial differential
equations which exists globally in time and without any restriction on the size of the
data. It is a joint work with Miroslav Bulíček (Charles University in Prague) and Nicola
Zamponi (Vienna University of Technology).
Motivation for studying fluid-structure interactions (FSI) problems comes from applications in various areas including geophysics, biomedicine and aeroelasticity. The FSI problems are typically nonlinear systems of the partial differential equations of parabolic-hyperbolic type with the moving boundary. In this talk we will present an operator splitting numerical scheme, so-called the kinematically coupled scheme, for the FSI problems and show how ideas from the numerical scheme can be be used in the constructive proof of the existence of a weak solution for various FSI problems. We will also discuss the rate of convergence of the numerical scheme and its extensions.
The presented results are part of joined work with S. Canic, University of Houston and M. Bukac, University of Notre Dame.
The evolutionary model for magnetoelasticity that we consider is phrased in Eulerian coordinates. It is a system of partial differential equations that contains (1) a Navier-Stokes equation with magnetic and elastic terms in the stress tensor obtained by a variational approach, (2) a regularized transport equation for the deformation gradient and (3) the Landau-Lifshitz-Gilbert equation for the dynamics of the magnetization. The proof of existence of weak solutions is based on a Galerkin method and a fixed-point argument combined with ideas from the analysis of models for the flow of liquid crystals (F.-H. Lin and C. Liu) and of the Landau-Lifshitz equation (G. Carbou and P. Fabrie).
We consider stochastic reaction-diffusion equations with a multiplicative noise term and analyse the influence of the Brownian Motion on the solution. Therefore, we use a variational approach to show the existence of solutions for a competition model for two species. Moreover, numerical simulations will be presented for the stochastic model and compared to the deterministic case.
Ion transport can be modelled using the Poisson-Nernst-Planck (PNP) equations. In order to account for size exclusion effects in narrow ion channels, the PNP model can be modified leading to a cross-diffusion system. In this talk, the modified PNP model and some analytic and numerical results will be presented. It will be discussed how an entropy method can be applied to prove the global-in-time existence of weak solutions to the model. Furthermore, a finite volume discretization of the equations and some simulation results for a calcium- selective channel will be shown.
The stationary nonhomogeneous Navier-Stokes problem is studied in a two dimensional symmetric domain with a semi-infinite outlet to infinity (for instance, paraboloid type or channel-like). Under the symmetry assumptions on the domain, boundary values and external force the existence of at least one weak symmetric solution is proved without any restriction on the size of the fluxes, i.e. the fluxes of the boundary value over the inner and the outer boundaries may be arbitrarily large. The Dirichlet integral of the solution can be finite or infinite dependent on the geometry of the domain.
We develop a large-scale regularity theory of higher order for divergence-form elliptic equations with heterogeneous coefficient fields $a$ in the context of stochastic homogenization. Under the assumptions of stationarity and slightly quantified ergodicity of the ensemble, we derive a $C^{2,alpha}$-``excess decay'' estimate on large scales and a $C^{2,alpha}$-Liouville principle: For a given $a$-harmonic function $u$ on a ball $B_R$, we show that its energy distance to the space of $a$-harmonic ``corrected quadratic polynomials'' on some ball $B_r$ has the natural decay in the radius $r$ above some minimal (random) radius $r_0$. Our Liouville principle states that the space of $a$-harmonic functions growing at most quadratically has (almost surely) the same dimension as in the constant-coefficient case. The existence of $a$-harmonic ``corrected quadratic polynomials'' -- and therefore our regularity theory -- relies on the existence of second-order correctors for the homogenization problem. By an iterative construction, we are able to establish existence of subquadratically growing second-order correctors. This is a joint work with Felix Otto.
We study linear eigenvalue problems with singular (unbounded close to the boundary) coefficients arising in the linearization to positive solutions to some degenerate and singular problems. This improves previous work by Bertsch and Rostamian and Hernandez, Mancebo and Vega. This is related with solutions to the linear Schrödinger equation and compact solutions for some associated nonlinear problems.
Joint work with J.I.Diaz.
This talk is concerned with asymptotic profiles for solutions to the Cauchy-Dirichlet problem
for the Fast Diffusion equation (FD) in smooth bounded domains under the so-called Sobolev
subcritical condition. It is well-known that every solution of (FD) vanishes in finite time
with a power rate; more precisely, it asymptotically approaches to a separable solution
(Berryman and Holland '80). Then the asymptotic profile for each vanishing solution can be
characterized as a non-trivial solution of the Emden-Fowler equation (EF). The stability of
asymptotic profiles has been discussed for the case that (EF) has a unique positive solution;
on the other hand, the case that (EF) may have multiple (positive) solutions had not been
studied for many years.
In this talk, we shall first see how to formulate notions of stability and instability of asymptotic
profiles, and then, we shall discuss criteria to distinguish the stability of each asymptotic profile.
Moreover, we shall focus on how to treat non-isolated asymptotic profiles; indeed, (EF) may admit a
one-parameter family of positive solutions, e.g., for sufficiently thin annular domains. In particular,
for thin annular domain cases, each non-radial asymptotic profile belonging to a one-parameter family
turns out to be stable and the radial positive profile turns out to be unstable. The method of analysis
relies on variational method, uniform extinction estimates for solutions to (FD), the Lojasiewicz-Simon
inequality and energy techniques developed for doubly nonlinear evolution equations.
Nature is dominated by systems composed of many individuals with a collective
behavior. Examples include wildlife populations, biological cell dynamics, and
tumor growth. There is a fast growing interest in multi-species systems both in
theoretical biology and applied mathematics, but because of their enormous complexity,
the scientific understanding is still very poor. On a macroscopic level, such systems
may be modeled by systems of partial differential equations with cross diffusion,
which reveals surprising effects such as uphill diffusion and diffusion-induced
instabilities, seemingly contradicting our intuition on diffusion.
Major difficulties of the mathematical analysis of the cross-diffusion equations
are their highly nonlinear structure and the lack of positive definiteness of the
diffusion matrix. In this talk, a method inspired from non-equilibrium thermodynamics
is proposed, which allows for a mathematical theory of a large class of such systems.
The idea is to exploit the hidden formal gradient-flow structure by introducing
so-called entropy variables. The analysis in these variables leads to global
existence results, L^infty bounds, and large-time asymptotics results.
We apply the technique to some systems modeling populations and tumor growth.
Since the pioneer work of Leray and Hopf, Stokes and Navier-Stokes problems
have been often studied with Dirichlet boundary condition. Nevertheless, in the
opinion of engineers and physicists such a condition is not always realistic in industrial
and applied problems of origin. Thus arises naturally the need to carry out a
mathematical analysis of these systems with different boundary conditions, which
best represent the underlying fluid dynamic phenomenology. Based on the theory
of semi-groups we carry out a systematic treatment of Stokes and Navier-Stokes
equations with Navier or Navier-type boundary conditions and boundary conditions
involving the pressure in L^p-spaces. These boundary conditions are usually
called in the literature, non-standard boundary conditions on the boundary of the
fluid domain.
We study the existence of strong solutions to the stationary version of the Navier-Stokes system for compressible fluids with a density dependent viscosity under the additional assumption that the fluid is sufficiently dense. The investigation is connected to the corresponding singular limit as Mach number goes to zero.
We consider the semilinear Fisher-Kolmogorov-Petrovski-Piscounov equation for the advance
of an advantageous gene in biology. Its nonsmooth reaction function f(u) allows for the introduction of
travelling waves with a new profile. We study existence, uniqueness, and long-time asymptotic behavior
of the solutions of the initial value problem to a travelling wave.
In this talk we discuss basic properties of diffusion and reaction-diffusion equations on lattices. Formulating the problem as an abstract diff. equation in sequence spaces we show existence, uniqueness and continuous dependence on the initial condition as well as the convergence of the discretized reaction-diffusion equation. We conclude with maximum principles and a priori estimates. (joint work with Antonín Slavík and Jonáš Volek)
We aim at investigating the physically relevant situation of polytropic flows. More precisely, we consider a model arising in radiation hydrodynamics which is based on the full Navier-Stokes-Fourier system describing the macroscopic fluid motion, and a P 1-approximation of the transport equation modeling the propagation of radiative intensity. In the strongly under-relativistic situation, we establish the global-in-time existence and uniqueness of solutions with critical regularity for the associated Cauchy problem with initial data close to a stable radiative equilibrium. We also justify the non-relativistic limit in that context. For smoother (possibly) large data bounded away from the vacuum and more general physical coefficients that may depend on both the density and the temperature, the local existence of strong solutions is shown.
Compressible Navier-Stokes system with Entropy Transport serves as a simplified model for the compressible heat conducting fluid. A former result on stability of solutions to the mentioned system is extended on an existence result by giving a suitable approximative scheme. There are two formally equivalent formulations of the equation for the entropy, namely pure transport equation for the entropy $s$ and continuity equation for the entropy density $varrho s$ (where $varrho$ is the density). A crucial role in the existence part plays the possibility to switch between these formulations even in the case of weak solutions.
We present a homogenization result for a family of integral energies, where the field under consideration are subjected to periodically oscillating differential constraints in divergence form. The work is based on the theory of A-quasiconvexity with variable coefficients and on two-scale techniques.
In a very interesting paper, Szekelyhidi and Wiedemann (2012) proved that every measure valued solution to the incompressible Euler equations can be approximated by a sequence of weak solutions, implying that there is no significant difference between weak and measure valued solutions to the incompressible Euler system. In this talk we prove that such a property does not hold for the compressible case and we show the construction of a measure valued solution which can not be generated by weak solutions. Moreover we show an abstract neccesary condition for measure valued solutions to be generated by sequences of weak solutions. The proof is based on a generalization of a rigidity result by Ball and James, the necessary condition is obtained as a consequence of the works of Fonseca and Muller. We present also some connections between the compressible Euler system and problems of gradient Young measures arising in nonlinear elasticity.
This is a joint work with Elisabetta Chiodaroli, Eduard Feireisl and Emil Wiedemann.
We introduce a new concept of a dissipative measure valued solution to the compressible Navier-Stokes/Euler system based on the quantity called dissipation defect. We identify a large class of problems including certain numerical schemes generating dissipative measure valued solutions. Finally, we show uniqueness of strong solutions in the class of measure valued solutions (weak-strong uniqueness) and characterize bounded-density measure valued solutions to the Navier-Stokes system. Applications to convergence problems will be given. This is a joint work with P.Gwiazda, A.Swierczewska-Gwiazda, and Emil Wiedemann.
prof. RNDr. Eduard Feireisl, DrSc.
Šárka Nečasová, Milan Pokorný
chairmen