$$$$ KBBT NOTICE CHAT 11/09/12 21:16:41 7124 DATE 11/09/12 Operateur KBBT Voir aussi : NAVI KMAB -------------- KMBT DUDW EQEX SYNTAXE ( EQEX ) : Cf operateur EQEX __________________ 'OPER' 'KBBT' coef'INCO' 'UN' 'PRES' Description : _____________ The KBBT operator discretizes the terms Div U and Grad P by a finite element method, in order to keep symetric the linear system. ------------- Contents : __________ coef coefficient FLOTTANT or CHPOINT SCAL SOMMET (volumic porosity) or CHPOINT VECT SOMMET (directional porosity) or MOT beta stabilization parameter FLOTTANT UN Velocity field CHPOINT VECT SOMMET or MOT PRES Pressure field CHPOINT SCAL CENTRE or MOT CHPOINT SCAL CENTREP1 or MOT CHPOINT SCAL CENTREP0 or MOT the type has to be given with the option key word INCOD When coefficients are of type MOT, the operator looks for data in INCO table at the index corresponding to the given name. Comments ________ Considering the Stokes or Navier-Stokes equations for an incompressible viscous flow. A U + Grad P = F : momentum equation -Div U = 0 : continuity equation where U and P are respectively the velocity and the pressure, A an invertible operator (usually diffusion/advection operator). In the variational formulation the term 'Grad P' is integrated by part which leads to a symetric system the continuity equation being written : - Div U = 0 . t | A -B |(U) (F) | |( ) =( ) |-B 0 |(P) (0) t / where B is the matrix of | P Div W dv |v (W test function for the velocity) / B is the matrix of | q Div V dv |v (q test function for the pressure) The KBBT operator constructs the matrices corresponding to the operators B and Bt (only B is stored) ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: REMARK : Considering the sign of the second equation an eventual source term must be negative. ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: 1/ Associated boundary conditions : Integrating by parts and using the divergence theorem we get : / / / | W*Grad P dv = | P n ds - | P Div W dv |v |s |v The surface integral is ommited which leads to the natural induced boundary condition: / | P n ds = 0 (n outward normal) |s Additional induced boundary conditions can appear whith other operator like LAPN. See operator TOIM in order to impose a value to the surface integral. :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: 2/ If all normal velocities are prescribed (zero or not) all around the boundaries, it is NECESSARY to impose the pressure at a point. It ist the case for all incompressible flows in a closed cavity. ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: 3/ If the coefficient is of type CHPOINT SCAL SOMMET (volumic porosity H) the operator computes : / / / / | W*H*Grad P dv = | WHP n ds - | P H Div W dv - | P W Grad H dv |v |s |v |v 4/ If the coefficient is of type CHPOINT VECT SOMMET (directional Porosity Hi ) the operator computes : / / / / | W*Hi*Grad P dv = | WHi P n ds - | P Hi Div W dv - | P W Grad Hi dv |v |s |v |v Options : (EQEX) _________ OPTI INCOD CENTRE CENTREP1 CENTREP0
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