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.
prof. RNDr. Eduard Feireisl, DrSc.
Šárka Nečasová, Milan Pokorný
chairmen