Simulations establish a universal condition under which dynamic boundary condition tests for crack velocity jumps match static test outcomes despite stress relaxation effects.
The elongation vector ∆ xmm′ are defined as ∆ xmms = xm − xms − ds with d1 = (d, 0) = −d3 and d4 = (0,d ) = −d2
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Crack propagation under static and dynamic boundary conditions
Simulations establish a universal condition under which dynamic boundary condition tests for crack velocity jumps match static test outcomes despite stress relaxation effects.