نتایج جستجو برای: local weak formulation

تعداد نتایج: 764529  

1995
Karsten Urban

In this paper we derive an algorithm for solving the Stokes{equations for the example of the Driven{Cavity{Problem. We treat the Stokes{equations in the divergence{free weak formulation and show the construction of divergence{free reenable functions, which will be used as trial functions in the Galerkin{method. The system will be solved by means of the preconditioned cg{method. We make use of m...

Journal: :Numerische Mathematik 2009
Norbert Heuer Francisco-Javier Sayas

This paper establishes a foundation of non-conforming boundary elements. We present a discrete weak formulation of hypersingular integral operator equations that uses Crouzeix–Raviart elements for the approximation. The cases of closed and open polyhedral surfaces are dealt with. We prove that, for shape regular elements, this non-conforming boundary element method converges and that, up to log...

1995
J. Baldwin

Classes with few models have 'homogeneous-universal' models This paper is concerned with a class K of models and an abstract notion of submodel ≤. Experience in first order model theory has shown the desirability of finding a 'monster model' to serve as a universal domain for K. In the original constructions of Jónsson and Fraissè, K was a universal class and ordinary substructure played the ro...

Journal: :SIAM Review 2014
Andrea Moiola Euan A. Spence

The usual variational (or weak) formulations of the Helmholtz equation are sign-indefinite in the sense that the bilinear forms cannot be bounded below by a positive multiple of the appropriate norm squared. This is often for a good reason, since in bounded domains under certain boundary conditions the solution of the Helmholtz equation is not unique at certain wavenumbers (those that correspon...

2003
F. Berthelin

We consider isentropic gas dynamics equations with unilateral constraint on the density and mass loss. The and pressureless pressure laws are considered. We propose an entropy weak formulation of the system that incorporates the constraint and Lagrange multiplier, for which we prove weak stability and existence of solutions. The nonzero pressure model is approximated by a kinetic BGK relaxation...

Journal: :SIAM Journal of Applied Mathematics 2003
N. Calvo Jesús Ildefonso Díaz Díaz J. Durany Emanuele Schiavi Carlos Vázquez

This paper deals with the weak formulation of a free moving boundary problem arising in theoretical glaciology Considering shallow ice sheet ow we present the mathematical analysis and the numerical resolution of the second order nonlinear degenerate parabolic equation modelling in the isothermal case the ice sheet non newtoniandynamics An obstacle problem is then deduced and analysed The exist...

2017
CHRISTOPH SCHWAB

Well-posed space-time variational formulations in fractional order Bochner–Sobolev spaces are proposed for parabolic partial differential equations, and in particular for the instationary Stokes and Navier–Stokes equations on bounded Lipschitz domains. The latter formulations include the pressure variable as a primal unknown and so account for the incompressibility constraint via a Lagrange mul...

2013
Mario Ohlberger Michael Schaefer

In this work we are considered with parameter optimization of elliptic multiscale problems with macroscopic optimization functionals and microscopic material design parameters. An efficient approximation is obtained by the reduced basis approach. A posteriori error estimates for the reduced forward problem are obtained in the periodic homogenization setting, using the so called two scale weak f...

Journal: :SIAM Journal of Applied Mathematics 2010
Josip Tambaca M. Kosor Suncica Canic D. Paniagua

We present a mathematical model for a study of the mechanical properties of endovascular stents in their expanded state. The model is based on the theory of slender curved rods. Stent struts are modeled as linearly elastic curved rods that satisfy the kinematic and dynamic contact conditions at the “vertices” where the struts meet. This defines a stent as a mesh of curved rods. A weak formulati...

2010
Sergey E. Mikhailov Norbert Heuer

∆u = ∂2u ∂x1 + ∂2u ∂x2 where x = (x1, x2) ∈ R2 are Cartesian coordinates. Even though the Poisson equation looks very special it is an important model case representing several problems from physics and engineering, e.g. electrostatics, stationary heat transfer and other diffusion problems. Variations of the techniques we will study apply to a wide class of second order so-called elliptic probl...

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