, On remarqueégalement que les gradients sont bien représentés sans oscillation de contrainte au sein d'unélément. Conclusions générales En ce qui concerne la modélisation de la vitesse de propagation de fissure en fatigue biaxiale, l'effet de modification de pente observé dans les séquences où T = 1, il serait intéressant de tester l, En guise d'exemple, nous présentons après propagation le champs de contrainte pour la composante dans la direction de sollicitation, au minimum du cycle, ? 22 Figure 5.7, vol.5

I. Annexe, Mesure de la surface de fissuration par rugosimétrie SB04 : Rappelons que l'essai SB04 est exploité jusqu'à apparition d'une fissure au congé de l'éprouvette suiteà un défaut technique lors du chauffage

. Certes, Ainsi, des mesures par profilométrie ontété faites sur les des deux faces avant (Figure I.77.a) et arriére (Figure I.77.b) de l'éprouvette SB04. Ces figures illustrent l'état de flambement final de l'éprouvette suiteà l'apparition de la fissure au congé. Nous nous intéressons particuliérementà la mesure au voisinage proche de la fissure principale (zones délimitées par trait rouge pointillé). Les zones de déformation plastique sont dissymétriques de part et d'autre du trou central. Cette dissymétrie entre les deux fissures (gauche, droite) està la fois constatée du point de vu de la valeur de l'amplitude mesurée en µm, et aussi du point de vu de taille de la zone plastique. La premiére séquence de chargement de cet essai est similaireà celle appliquée sur l'éprouvette SB01 présentée précédemment. Les mesures de l'amplitude au voisinage de l'entaille (fissure correspondantà la premiére séquence), est comparableà celle mesurée sur SB01. En revanche, pour la suite de propagation, la deuxiéme séquence de l'essaiétant a déplacement LVDT imposé

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