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We identify the existence of two different shear bands during the early stages of crack formation. In our simulations, such bands are evident in the free-surface conditions and when the applied solicit is large enough (see Figs. 7 and 8). These bands correspond to the two shear-transition fronts that we observe experimentally; the steady-state crack velocity in two dimensions thus follows equation (8), which is derived from the rate-of-shear theory of fatigue crack growth in metals. The scatter of observed velocities in Fig. 2 is significantly larger than the predicted scatter in Figs. 3 and 4, suggesting that the model provides a reasonable description of the early stages of crack growth during oscillatory loading.
This experiment reveals a mechanism for the shape of the crack tip during the propagation from initiation to steady state. To begin with, we consider a shape-memory polymer (SMPS) confined between two opposite crack fronts. The SMPS material has a relatively high modulus when it is pulled in the normal direction but a much lower modulus when it wants to twist around the crack. Whenever the polymer twists around the crack, it experiences a stress increase. At sufficiently high stress, the polymer and the crack then get locked together and continue to twist around each other.
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