85 III. 6. 5. Nombre de Weissenberg critique, p.90 ,
100 IV. 2. 1. Morphologie des extrudats obtenus, p.101 ,
Géométrie de maillages et conditions limites utilisées, V. 3. 2. Identification des paramètres, p.165 ,
169 V. 4. 2. Courbes d'écoulement apparentes, pour différents rapports184 A. II. Courbes d'écoulement apparentes du PS 2 obtenues en rhéométrie capillaire, pour différents rapports de longueur, p.188 ,
190 A. V. 2. Mesure de pas et diamètres hélicoïdaux, A. V. A. V. Mesure de volumes hélicoïdaux, vol.1, issue.3, 0191. ,
194 A. VIII Nombre de Weissenberg critique calculé en rhéométrie capillaire, 195 A. VIII. 2. Déclenchement du défaut hélicoïdal pour le PS 2 ,
197 A. X. 1. Equation sans étirement en régime permanent, 197 A. X. 2. Equation avec étirement en régime permanent ,
201 A. XI. 1. Courbes d'écoulement apparentes obtenues avec L, p.202 ,
Courbes d'écoulement en contrainte réelle, obtenue en rhéométrie capillaire A. IV. 1. Courbes d' ,
Nombre de Weissenberg critique calculé en rhéométrie capillaire A. VIII. 1. Déclenchement du défaut hélicoïdal pour le PP -a -b A. 8. 1. : Variation du nombre de Weissenberg critique pour différents diamètres et longueurs de filière, °C. La figure (b) est à une échelle zoomée par rapport à la figure (a) ,
Déclenchement du défaut hélicoïdal pour le PS 2 -a -b A. 8. 2. : Variation du nombre de Weissenberg critique pour différents diamètres et longueurs de filière, à 180 °C. La figure (b) est à une échelle zoomée par rapport à la figure (a) ,
Influence de la température sur le déclenchement du défaut volumique oscillant ,
1. Courbes d'écoulement apparentes obtenues avec L ,
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