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The glass transition in polymer melts
Author(s) -
Baschnagel Jörg,
Lobe Bernhard
Publication year - 1994
Publication title -
macromolecular symposia
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.257
H-Index - 76
eISSN - 1521-3900
pISSN - 1022-1360
DOI - 10.1002/masy.19940810108
Subject(s) - glass transition , amorphous solid , thermodynamics , materials science , polymer , logarithm , inverse , monte carlo method , crystallization , exponential function , lattice (music) , statistical physics , condensed matter physics , physics , chemistry , crystallography , mathematics , composite material , mathematical analysis , geometry , statistics , acoustics
This paper presents some results of a Monte Carlo simulation for the glass transition in two‐ and three‐dimensional polymer melts. The melt was simulated by the bond‐fluctuation model on a d ‐dimensional cubic lattice which was combined with a two‐level hamiltonian favouring long bonds in order to generate a competition between the energetic and topological constraints in the system. This competition prevents crystallization and makes the melt freeze in an amorphous structure as soon as the internal relaxation times match the observation time of the simulation set by the cooling rate. The freezing point of the melt, i.e the glass transition temperature T g , thus depends upon the cooling rate and additionally upon the chain length of the polymers. The dependence of the glass transition temperature on the cooling rate was closely analysed in three and that on the chain length in both two and three dimensions, resulting in a non‐linear relationship between T g and the logarithm of the cooling rate and a linear relationship between T g and the inverse chain length, respectively. In addition to this behaviour of the melt during the cooling process an example for the relaxational properties of the three‐dimensional model is provided by a quantitative analysis of the incoherent intermediate scattering function in the framework of the idealized mode coupling theory.