Element 3d Patcher Crack Key
Table 3 shows that the difference of the crack group occupied index is very small, the stress-softening crack model does not change the value of occupied coefficient. Young’s modulus and the tensile process of natural rubber used in the experiment are significantly different (N). The indexes of 4.2 limited mode-softening crack and Newtonian rubber are also put into the experiments, but the experimental results are consistent with the theoretical values of natural rubber. The fracture stress of the prepared rubber is 0.0125 kg/cm2, which was far below the 0.0215 kg/cm2 of 4.2 limited mode-softening crack, making it suitable for simulation.
Each singular crack body of the 3d element model of the crack group is firstly solved by the boundary conditions using a specified finite element technique as shown in Figure 5. The crack tip contact surface and the crack tip are defined as nodes, the input of the crack tip in the crack center is shown in Figure 5(a). The crack is overwritten at each step of the maximal crack displacement. The crack contact surface and the crack tip are shown in Figure 5(b). The crack propagation directions at each step are shown in Figure 5(c).
After obtaining the crack line and edge at each step, combined with the crack tip contact surface, the standard element contact surface is formed, and then the crack tip contact surface is obtained by removing the crack edge as shown in Figure 6.
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