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Face-centered cubic periodic boundary conditions

Figure 3 shows the time-dependence of various temperatures for an example simulation of an elastic-plastic shock in the [110] direction in an approximately cubic perfect 25688 atom face centered cubic Lennard-Jones crystal. This computational cell size is large enough to prevent artificial influence of the periodic boundary conditions on the deformation mechanisms inside the computational cell. [13] In terms of the standard Lennard-Jones... [Pg.307]

Fig. 4. Snapshot from a simulation at room temperature of 259 water molecules, one 1 ion and 4 non-mobile layers of a face-centered cubic mercury crystal with (111) surface structure. Only the basic cell is shown periodic boundary conditions are applied in the x and y directions only. Fig. 4. Snapshot from a simulation at room temperature of 259 water molecules, one 1 ion and 4 non-mobile layers of a face-centered cubic mercury crystal with (111) surface structure. Only the basic cell is shown periodic boundary conditions are applied in the x and y directions only.

See other pages where Face-centered cubic periodic boundary conditions is mentioned: [Pg.490]    [Pg.507]    [Pg.65]    [Pg.191]    [Pg.708]    [Pg.263]    [Pg.22]    [Pg.245]    [Pg.902]    [Pg.332]    [Pg.191]   
See also in sourсe #XX -- [ Pg.332 ]




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Condition periodicity

Conditioning period

Face centered

Face cubic

Face-centered cubic

Face-centered cubic periodic boundary

Periodic boundary

Periodic boundary conditions

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