## Abstract A uniform star‐branched polymer model with __f__ = 3 arms based on a simple cubic lattice was studied by means of the dynamic Monte Carlo method. The model chain is athermal with excluded‐volume interactions and it is flexible. A new type of local micromodification was introduced to mak
Dynamics of star branched polymers in a matrix of linear chains — a Monte Carlo study
✍ Scribed by Andrzej Sikorski; Andrzej Kolinski; Jeffrey Skolnick
- Publisher
- John Wiley and Sons
- Year
- 1994
- Tongue
- English
- Weight
- 781 KB
- Volume
- 3
- Category
- Article
- ISSN
- 1022-1344
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
A simple cubic lattice model of the melt of 3‐arm star‐branched polymers of various length dissolved in a matrix of long linear chains (n~1~ = 800 beads) is studied using a dynamic Monte Carlo method. The total polymer volume fraction is equal to 0,5, while the volume fraction of the star polymers is about ten times smaller. The static and dynamic properties of these systems are compared with the corresponding model systems of isolated star‐branched polymers and with the melt of linear chains. It has been found that the number of dynamic entanglements for the star polymers with arm length up to 400 segments is too small for the onset of the arm retraction mechanism of polymer relaxation. In this regime dynamics of star‐branched polymers is close to the dynamics of linear polymers at corresponding concentration and with equivalent chain length. The entanglement length for star polymers appears to be somewhat larger compared with linear chains.
📜 SIMILAR VOLUMES
## Abstract By use of the pivot algorithm, star‐branched chains with __F__ = 4, 8 and 12 arms of length __n__ and linear chains (__F__ = 2) are generated on a tetrahedral lattice (120 ⩽ __nF__ ⩽ 3 840). By taking into account non‐bonded nearest‐neighbour interactions (each contact contributes an en
## Abstract By use of the pivot algorithm, star‐branched chains with __F__ = 3–12 arms of length __n, nF__ = 480, and linear chains (__F__ = 2) are generated on a tetrahedral lattice. In order to simulate different qualities of the solvent, specific short‐range interactions are taken into account.
## Abstract The simple cubic‐lattice model of polymer chains was used to study the dynamic properties of adsorbed, branched polymers. The model star‐branched chains consisted of __f__ = 3 arms of equal lengths. The chain was modeled with excluded volume, that is, in good solvent conditions. The onl
## Abstract By use of the pivot algorithm, star‐branched chains with __F__ = 4, 8 and 12 arms of length __n__ and linear chains (__F__ = 2) are generated on a tetrahedral lattice (120 ≤ __nF__ ≤ 3 840). By taking into account nearest neighbour interactions (each contact contributes an energy ϕ __kT