Titlebook: New Directions in Mathematical Fluid Mechanics; The Alexander V. Kaz Andrei V. Fursikov,Giovanni P. Galdi,Vladislav V. Book 2010 Birkhäuse

jet-lag

Superconducting Vortices: Chapman Full Model,agnetic field is given on the entire boundary of the domain and on the inflow part of the boundary an extra condition is required for the vorticity. This part of the boundary is unknown before resolving the problem. In fact we investigate the “free boundary problem”.

妈妈不开心

Augmented Lagrangian Method and Compressible Visco-plastic Flows: Applications to Shallow Dense Avangham type system with applications to dense avalanches. For the sake of completeness we also present a method showing that such a system may be derived for a shallow flow of a rigid-viscoplastic incompressible fluid, namely for incompressible Bingham type fluid with free surface. When the fluid is

carotid-bruit

,Finite-dimensional Control for the Navier—Stokes Equations,ven moment of time a velocity field with the null projection on the finitedimensional subspace spanned by eigenfunctions of the Stokes operator. The control is selected from this subspace too. On the basis of estimates of the solution for the subdifferential Cauchy problem for a Navier—Stokes system

厌烦

四目在模仿

acrophobia

Optimal Neumann Control for the Two-dimensional Steady-state Navier-Stokes equations,acts at a part of the boundary which is contiguous to the rigid boundary where the no-slip condition holds. Further, certain constraints are imposed on the control and the phase variable. We derive an existence theorem as well as the corresponding optimality system

amenity

On Some Boundary Value Problem for the Stokes Equations with a Parameter in an Infinite Sector,, we are concerned in this paper with the boundary value problem for the stationary Stokes equations with a parameter in an infinite sector with the slip and the stress boundary conditions. Existence of the unique solution is proved in weighted Sobolev spaces.

conceal

ostrish

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