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Supercomputer Simulation of Crystal Defects

19 mobile chains 16 of 100 CH2-groups in each chain 12 (surrounded byl8 [Pg.525]

The details of the mechanism of formation of a kink can be deduced from Fig. 5.101, where one chain that develops a kink has been drawn in a sequence of snapshots, spaced 0.1 ps apart. The perspective is as before in Figs. 1.47 and 5.97. [Pg.525]

By inspection, one can see that the kink is the result of the collision of a transverse (A), torsional (B), and longitudinal vibration (C) between 0.5 and 1.1 ps (see also Fig. 1.47). After formation, this particular kink defect had a life time of about 2 ps. [Pg.526]

The mechanism of twisting of a single chain is illustrated in Fig. 5.102. One can see a very gradual twist starts at about 1.5 ps, and is completed after 2.3 ps. After this [Pg.526]

The sequence of Figs. 5.103-105 illustrates the details of the diffusion of a chain through the crystal. The figures refer to a chain that was driven into the direction of [Pg.527]


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