All the stress components at a rapidly propagating crack-tipin an elastic perfectly-plastic material are the functions of θ only. Making use of this condition and the equations of steady-state motion, stress-strain relations and yield conditions, we obtain the general solutions in both the cases of anti-plane and in-plane strain. Applying these two general solutions to propagating Mode Ⅲ and Mode I cracks, respectively, the elastic perfectly-plastic and the perfectly-plastic fields at the rapidly propagating tips of Mode Ⅱ and Mode I cracks are derived.
Слепян Л.И.,Динамика трещины в упругопластическом теле,Изв.АН СССР ММТ,11,2(1976),144-153
[2]
Achenbach,J,D,and V.Dunayevsky,Fields near a rapidly propagating crack-tip in an elastic perfectly-plastic material,I.Mech.Phgs,Solids,29,4(1981),283-303.