Molecular Dynamics Study of Commensurate-Incommensurate Phases in Hexamethylenetetramine Suberate

2002 ◽  
Vol 731 ◽  
Author(s):  
Yuansheng Pan ◽  
David Brown ◽  
Gervais Chapuis

AbstractIncommensurate structure of Hexamethylenetetramine suberate (C6H12N4)(HOOC-(CH2)6-COOH) has been solved from single crystal x-ray diffraction data. A molecular dynamics simulation of this system was carried out from 15 K to 580K. A second-generation consistent forcefield (CFF) and a compensating pressure tensor field were used to describe the interactions between atoms and to account for deficiencies in the forcefield. Starting from the experimental 298K structure, the phase transitions were investigated over an extended temperature range. A high symmetry commensurate structure exists at temperatures between 410K and 290K. For temperatures lower than 290K, a new periodicity appears in the structure. The system reaches a low symmetry lock-in phase at about 150K. An incommensurate structure appears between the high and low symmetry phases between 290K and 150K. The new periodicity associated with the incommensurate modulation is due to the appearance of additional long range ordering of the carbon chains. The present simulation not only reproduces well the experimental x-ray diffraction results but also gives new insight into the origin of the incommensurate behavior.

2000 ◽  
Vol 56 (4) ◽  
pp. 738-743
Author(s):  
Jan Dillen ◽  
Martin W. Bredenkamp ◽  
Mare-Loe Prinsloo

The crystal structure of 5-O-tert-butyldimethylsilyl-3,4-O-carbonyl-1,2-O-cyclohexylidene-2-oxo-3-oxa-4-bornanylcarbonyl-D-myo-inositol has been studied by single-crystal X-ray diffraction at both room temperature and 173 K. At room temperature, the tert-butyldimethylsilyl group exhibits dynamical disorder. A molecular dynamics simulation was used to model the disorder and this indicates that the group librates between two stable conformations in the crystal. Approximate relative energies of the different forms and energy barriers for the transition were obtained by empirical force field methods. Calculations of the thermal motion of the atoms are in good qualitative, but fair to poor quantitative agreement with the X-ray data.


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