Abstract
Recently it has become possible to make a series of simulations on a supercomputer of the molecular motion of a pentacontane (C50H102) crystal containing close to 10000 atoms. Such a crystal is big enough to serve as a model of a macroscopic crystal. It can also serve as a model for polyethylene. The large volume of detailed information on the structure and motion permits a new level of understanding. Information on crystal appearance, pseudo‐symmetric crystal structures, picosecond time‐scale formation of conformational defects and the beginning of the melting process is presented.
Original language | English |
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Pages (from-to) | 245-255 |
Number of pages | 11 |
Journal | Macromolecular Theory and Simulations |
Volume | 2 |
Issue number | 2 |
DOIs | |
State | Published - Mar 1993 |