neighbor analysis (CNA)(28). The gray atoms have the hcp structure, and the black atoms have structures other than
hcp and fcc. The figures show only z < Lz/2 of the crystal
particle. Figure 5 (i) and (ii) respectively presents results
for the low crystal volume fraction case, F(L43R12f10), and the high crystal volume fraction case, D(L29R12f34).
The particle size is the same in both cases. While the crys- tal orientation that we chose easily causes deformationno inside-particle structure changes are confirmed for the lower crystal volume fraction case (Fig. 5 (i)). When the crystal volume fraction is high (Fig. 5 (ii)), the particle de- formation begins from the sides of particle for the stress concentration that was described in the previous section. The partial-dislocation-based deformation mechanism is dominant because the particle size is very small. Many stacking faults are introduced into the particle, and they
neighbor analysis (CNA)(28). The gray atoms have the hcp structure, and the black atoms have structures other than hcp and fcc. The figures show only z < Lz/2 of the crystal particle. Figure 5 (i) and (ii) respectively presents results for the low crystal volume fraction case, F(L43R12f10), and the high crystal volume fraction case, D(L29R12f34). The particle size is the same in both cases. While the crys- tal orientation that we chose easily causes deformationno inside-particle structure changes are confirmed for the lower crystal volume fraction case (Fig. 5 (i)). When the crystal volume fraction is high (Fig. 5 (ii)), the particle de- formation begins from the sides of particle for the stress concentration that was described in the previous section. The partial-dislocation-based deformation mechanism is dominant because the particle size is very small. Many stacking faults are introduced into the particle, and they
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