## 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
Monte Carlo simulation of tetrahedral chains, 6. Linear and star-branched polymers near to theta conditions
✍ Scribed by Zifferer, Gerhard
- Publisher
- Wiley (John Wiley & Sons)
- Year
- 1993
- Weight
- 986 KB
- Volume
- 2
- Category
- Article
- ISSN
- 1018-5054
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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 non‐bonded 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 in the range −0,425 to −0,525. The energy parameter ϕ~⊙~ = −0,475, characteristic of theta conditions, was evaluated by use of an intramolecular criterion (proportionality between mean‐square dimensions and total chain‐length) and confirmed by a crossover scaling analysis. Theta dimensions are found to be larger than those of nonreversal random walks, the deviation growing with increasing number of arms.
📜 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.
## 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 th