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34 1.2.2 Discrétisation totale, p.35 ,
79 2.3.2 Propriétés de la reconstruction en Q ij, ., vol.87, p.88 ,
124 4.3.1.1 La méthode de Lax-Friedrichs, p.126 ,
159 5.3.2 Cas 3D -Comparaison maillage grossier contre maillage finCalcul sur maillage fin, Conclusion, p.167 ,
167 5.4.2 Vent, p.168 ,
239 7.4.3.1 Schéma de Runge-Kutta explicite d'ordre 3, p.242 ,
265 8.3.4 Vers une simulation d'une torchè a plasma, p.266 ,
ou non (` a droite) la propriété (P 1 ), p.32 ,
ou non (` a droite) la propriété (P 2 ), p.33 ,
gauche) et (1 ? µ ij )/µ ij (droite) pour un maillage 3D dans une géométrie simple (a), un maillage 2D (b) et un maillage 3D dans une géométrie complexe (c) ,
? noir) et HLLC ( rouge), test 1, maillage M 90 , méthode d'ordre un. Densité (?), p.143 ,
ROE point-tirets, solution exacte trait plein, p.144 ,
ROE point-tirets, solution exacte trait plein, p.145 ,
ROE point-tirets, solution exacte trait plein, p.146 ,
ROE point-tirets, solution exacte trait plein, p.147 ,
Comparaison entre les différents solveurs, test 1, maillage M 90 , méthode d'ordre deux, p.156 ,
Densité pour les tests 1 ` a 4. Solveur HLLC, méthode d'ordre un, 60 points par direction, p.157 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b) et multipente en Q ij (c) ` a t = 0, p.160 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b) et multipente en Q ij (c) ` a t = 1, p.161 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b) et multipente en Q ij (c) ` a t = 2, p.162 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b) et multipente en Q ij (c) ` a t = 3, p.163 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b) et multipente en Q ij (c) ` a t = 4, p.164 ,
Comparaison entre la méthode d'ordre un (a), du gradient (b), multipentes Q ij (c) et multipentes M ij (d) ` a t = 4, p.166 ,
ordre un (haut), multipente en Q ij (bas), densitédensitéà t = 0,5, p.171 ,
ordre un (haut), multipente en Q ij (bas), densitédensitéà t = 1, p.172 ,
ordre un (haut), multipente en Q ij (bas), densitédensitéà t = 2, p.172 ,
ordre un (haut), multipente en Q ij (bas), densitédensitéà t = 3, p.173 ,
ordre un (haut), multipente en Q ij (bas), densitédensitéà t = 4, p.173 ,
gauche) et (1 ? µ ij )/µ ij (droite) pour le maillage grossier (a), intermédiaire (b) et fin (c), p.187 ,
vitesse axiale, (b) et pression (c) enregistrée par le premier capteur ,
Données calculées (théorie des collisions) en trait plein et régression en loi puissance en pointillés, p.210 ,
Données calculées (théorie des collisions) en trait plein et régression en loi puissance en pointillés, p.210 ,
Image extraite de [21], p.230 ,
Nombre de points de maillage présents dans la zone de cisaillement pour la configuration N, p.254 ,
vorticité instantanée pour la simulation S14, Re ? ? 3 400, p.288 ,
pression (b) et norme de la vorticité (c) instantanées pour la simulation S16, St a = 0, Contours de température, p.291 ,