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Babuska-Brezzi condition

Hughes, T. J. R., Franca, L. P. and Balestra, M., 1986. A new finite-element formulation for computational fluid dynamics. 5. Circumventing the Babuska-Brezzi condition - a stable Petrov-Galerkin formulation of the Stokes problem accommodating equal order interpolations. Cornput. Methods Appl. Meek Eng. 59, 85-99. [Pg.109]

It can be easily seen from this simple example that the problem is that the number of displacement boundary constraints (or BCs) and incompressibility constraints is equal to the number of kinematic dof, and therefore, the system cannot be solved for any deformation mode. The mathematical theory behind this phenomenon is based on the Babuska-Brezzi condition [7] that numerically is related to the solvability of Eq. (8.14). [Pg.391]

Triangular Crouzeix-Raviart elements [63] were selected, which verify the so-called Babuska-Brezzi compatibility conditions (quadratic approximation for the velocity discontinuous linear approximation for the isotropic part of the stress tensor discontinuous quadratic approximation for the stresses) (Fig. 18). [Pg.312]

If a discrete inf-sup inequality is satisfied by the velocity and pressure elements, then the discrete problem has a unique solution converging to the solution of the continuous one (see equation (27) of the chapter Mathematical Analysis of Differential models for Viscoelastic Fluids). This condition is referred to as the Brezzi-Babuska condition and can be checked element by element. Finite element methods for viscous flows are now well established and pairs of elements satisfying the Brezzi-Babuska condition are referenced (see [6]). Two strategies are used to compute the numerical solution of these equations involving velocity and pressure. [Pg.241]

An element for the stress components composed of 16 sub-elements (4x4) on which bilinear (continuous) polynomials are used, was introduced by Marchal and Crochet in [28]. This leads to a continuous C° approximation of the three variables. The velocity is approximated by biquadratic polynomials while the pressure is linear. Fortin and Pierre ([17]) made a mathematical analysis of the Stokes problem for this three-field formulation. They conclude that the polynomial approximations of the different variables should satisfy the generalized inf-sup (Brezzi-Babuska) condition introduced by Marchal and Crochet and they proved it was the case for the Marchal and Crochet element. In order to take into account the hyperbolic character of the constitutive equation, Marchal and Crochet have implemented and compared two different methods. The first is the Streamline-Upwind/Petrov-Galerkin (SUPG). Thus a so-called non-consistent Streamline-Upwind (SU) is also considered (already used in [13]). As a test problem, they selected the "stick-slip" flow. With SUPG method applied to this problem, wiggles in the stress and the velocity field were obtained. In the SU method, the modified weighting function only applies to the convective terms in the constitutive equations. [Pg.245]


See other pages where Babuska-Brezzi condition is mentioned: [Pg.72]    [Pg.129]    [Pg.177]    [Pg.511]   
See also in sourсe #XX -- [ Pg.391 ]




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