Mapping of rotational isomeric state chains with asymmetric torsional potential energy functions on a high coordination lattice: Application to polypropylene

A high coordination lattice model was recently introduced for simulating coarse-grained rotational isomeric state (RIS) chains in which the bonds have symmetric torsional potential energy functions, E(φ)=E(−φ). This symmetry was exploited in the coarse-graining and mapping onto the high coordination lattice, thereby making the procedure unsuitable (without modification) for application to chains where one or more bonds has an asymmetric torsion potential energy function, E(φ)≠E(−φ). The necessary modification is described here, and then documented by mapping previously described RIS models for isotactic and syndiotactic polypropylene onto the high coordination lattice. Each bead on the high coordination lattice represents a monomer unit, C3H6, of polypropylene. The conditional probabilities derived from the RIS model form the basis for the acceptance of the single bead moves used in the Monte Carlo simulations on the 2nnd lattice. The simulated chains have reasonable mean-square end-to-end distances and m...

[1]  E. Helfand,et al.  Conformational state relaxation in polymers: Time-correlation functions , 1982 .

[2]  R. Glauber Time‐Dependent Statistics of the Ising Model , 1963 .

[3]  I. Bahar,et al.  Investigation of local motions in polymers by the dynamic rotational isomeric state model , 1987 .

[4]  I. Bahar,et al.  Intramolecular Contributions to Stretched-Exponential Relaxation Behavior in Polymers , 1994 .

[5]  Ulrich W. Suter,et al.  Conformational Theory of Large Molecules: The Rotational Isomeric State Model in Macromolecular Systems , 1994 .

[6]  M. Volkenstein,et al.  Statistical mechanics of chain molecules , 1969 .

[7]  W. Mattice,et al.  New high-coordination lattice model for rotational isomeric state polymer chains , 1995 .

[8]  G. Fytas,et al.  Intercomparisons of dielectric relaxation, dynamic light scattering, and viscoelastic properties of the local segmental motion in amorphous polymers , 1988 .

[9]  U. Suter,et al.  Epimerization of 2,4,6,8-tetramethylnonane and 2,4,6,8,10-pentamethylundecane, low molecular weight model compounds of polypropylene , 1975 .

[10]  Pemra Doruker,et al.  Reverse Mapping of Coarse-Grained Polyethylene Chains from the Second Nearest Neighbor Diamond Lattice to an Atomistic Model in Continuous Space , 1997 .

[11]  F. Kremer,et al.  Molecular dynamics in bulk cis-polyisoprene as studied by dielectric spectroscopy , 1990 .

[12]  G. Floudas,et al.  Dynamics of the glass‐forming liquid di‐2‐ethylhexyl phthalate (DOP) as studied by light scattering and neutron scattering , 1992 .

[13]  W. Mattice,et al.  Rotational isomeric state models for polyoxyethylene and polythiaethylene on a high coordination lattice , 1996 .

[14]  W. Mattice,et al.  Simulation of polyethylene thin films on a high coordination lattice , 1998 .

[15]  Junhan Cho,et al.  Estimation of Long-Range Interaction in Coarse-Grained Rotational Isomeric State Polyethylene Chains on a High Coordination Lattice , 1997 .

[16]  Wayne L. Mattice,et al.  Introduction of short and long range energies to simulate real chains on the 2nnd lattice , 1996 .

[17]  Robert L. Jernigan,et al.  Conformational Energies of n-Alkanes and the Random Configuration of Higher Homologs Including Polymethylene , 1966 .

[18]  R. Zwanzig,et al.  Dielectric relaxation and dynamic susceptibility of a one‐dimensional model for perpendicular‐dipole polymers , 1975 .