## 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
Monte Carlo simulation of tetrahedral chains, 7 the shape of linear and star-branched polymers near to theta-conditions
✍ Scribed by Gerhard Zifferer
- Publisher
- John Wiley and Sons
- Year
- 1994
- Tongue
- English
- Weight
- 997 KB
- Volume
- 3
- Category
- Article
- ISSN
- 1022-1344
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✦ Synopsis
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 to the total energy of the configuration) a variation of the thermodynamic quality of the solvent is simulated by a variation of the energy parameter ϕ near the value of ϕ~θ~ = ‐0,475, characteristic of theta‐conditions. For theta‐conditions various quantities characteristic of the instantaneous shape of polymers exhibit similar values as found for nonreversal random walks; furthermore, while linear theta‐chains are slightly less asymmetric than athermal ones, the opposite behaviour is found for star‐branched polymers. Clearly, for all thermodynamic conditions the asymmetry of configurations decreases with increasing number of arms but remains appreciable even for F = 12.
📜 SIMILAR VOLUMES
## 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.