Temperature-dependent cubic-lattice-model simulation of polymer-chain dynamics

1986 ◽  
Vol 34 (3) ◽  
pp. 1984-1986 ◽  
Author(s):  
J. Naghizadeh ◽  
J. Kovac
Keyword(s):  
Polymer Chain ◽  
Lattice Model ◽  
Model Simulation ◽  
Temperature Dependent ◽  
Chain Dynamics ◽  
Cubic Lattice

Simulation of polymer chain dynamics by lattice models with excluded volume: lattice dependence

1987 ◽  
Vol 20 (6) ◽  
pp. 1362-1368 ◽  
Author(s):  
Peter H. Verdier ◽  
David E. Kranbuehl
Keyword(s):  
Polymer Chain ◽  
Lattice Models ◽  
Excluded Volume ◽  
Chain Dynamics

Comparison of the long range polymer chain dynamics of polystyrene and cis-polyisoprene using polymers randomly labeled with pyrene

Polymer ◽  
2009 ◽  
Vol 50 (23) ◽  
pp. 5456-5466 ◽  
Author(s):  
Steven J. Teertstra ◽  
Wai Yau Lin ◽  
Mario Gauthier ◽  
Mark Ingratta ◽  
Jean Duhamel
Keyword(s):  
Long Range ◽  
Polymer Chain ◽  
Chain Dynamics

scholarly journals Effect of polymer rigidity on the phase behaviour of polymer adsorption on to planar surface

2016 ◽  
Vol 36 (6) ◽  
Author(s):  
Zhiyong Yang ◽  
Aihua Chai ◽  
Peicong Zhou ◽  
Ping Li ◽  
Yongfu Yang
Keyword(s):  
Monte Carlo ◽  
Polymer Chain ◽  
Lattice Model ◽  
Polymer Adsorption ◽  
Surface Interaction ◽  
Phase Behaviour ◽  
Planar Surface ◽  
Bending Energy ◽  
Semiflexible Polymer ◽  
Dynamic Monte Carlo

We study the process of a semiflexible polymer chain adsorption on to planar surface by the dynamic Monte Carlo (DMC) method, based on the 3D off-lattice model. Both the strength of attractive monomer–surface interaction (εa) and bending energy (b) have pronounced effect on the adsorption and shape of semiflexible polymer chain. The semiflexible polymer can just fully adsorb on to the surface at certain εa, which is defined as critical εa. The essential features of the semiflexible polymer adsorption on to surface are that (i) the critical εa increases with increase in b; (ii) the shape of the fully adsorbed semiflexible polymer chain is film-like toroid, and the toroid becomes more and more perfect with increase in b. In addition, the size of toroid and the number of turns of toroid can be controlled by the b and εa.

Polymer Chain Dynamics in Intercalated Poly(ε-caprolactone)/Nanoplatelet Blends

2013 ◽  
Vol 46 (6) ◽  
pp. 2235-2240 ◽  
Author(s):  
Kevin A. Masser ◽  
Hongyi Yuan ◽  
Alamgir Karim ◽  
Chad R. Snyder
Keyword(s):  
Polymer Chain ◽  
Chain Dynamics
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