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1 Présence de gaz dans l, p.340 ,
4.1 Méthode Afin d'´ etudier l'influence des paramètres de la loi B-STMA, plusieurs configurations sont essayées. Pour cela, les 5 paramètres indépendants de la loi sont modifiés touràtour`tourà tour par rapportàrapport`rapportà une configuration de référence. Pour chaque paramètre, 5 valeurs sont choisies, les valeurs soulignées ,
0, 5m.s ?1 ;0, 8m.s ?1 ; 1m.s ?1 ;1.2m.s ?1 ; 1.5m.s ?1 ? Y l a : 0ppm ; 5ppm ; 11ppm : 15ppm, pp.10-12 ,
1300P a ; 1800P a ; 2300P a ; 2800P a ;3300P a ? p cuve : p atm ,
1 Description des codes de calcul utilisés, p.367 ,
1 Décomposition du potentiel de vitesse en deux variables séparées, p.386 ,
nous allons apporter des précisions quantàquant`quantà la mise en place de l'algorithme IDB. Pour cela, nous allons dans un premier temps présenter la décomposition de fonction utilisée pour chaque harmonique sphérique. Dans un second temps, nous donnerons des précisions sur le passage entre l'ensemble S 2 (représentatif de l'interface) et le C-espace vectoriel dans lequel la résolution du système est effectuée, Nous terminerons cette section, en explicitant les matrices et vecteurs du système ,