. (D.3)
La matriceA(de taille(N
1+N
2)
2) de couplage est diagonale par blocs o`ua
i(i= 1,2)
sont les matrices de convection de convection-diffusion du scalaire `a coupler de taille N
2i
dans le domaine D
iavec N
icellules. Dans les blocs extra-diagonaux nuls, on rajoute les
matrices diffusives de couplagec
1etc
2. On remarque que le syst`eme g´en´eral `a r´esoudre est
compos´e de deux produits matrice-vecteurs ind´ependants non-coupl´es. La premi`ere ´etape
consiste `a ´echanger h
eqet Y
edans les cellules `a coupler puis afin d’´eviter de changer la
structure de la matrice A, on rajoute ces flux diffusifs d’´echange apr`es le produit
matrice-vecteur i.e. :
b= b
1b
2 != (A+A
c)x= a
10
0 a
2 !x+ 0 c
1c
20
!x. (D.4)
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Dans le document
Modélisation numérique instationnaire pour la simulation du soudage TIG avec couplage plasma / bain de fusion
(Page 183-189)