A Monte Carlo study of the second virial coefficient of semiflexible ring polymers

A Monte Carlo (MC) study was made of the second virial coefficient A 2 of the ideal Kratky–Porod (KP) worm-like ring using a model composed of infinitely thin bonds with harmonic bending energy between successive bonds. Two kinds of statistical ensembles were generated: one composed of configuration...

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Bibliographic Details
Published in:Polymer journal Vol. 42; no. 9; pp. 735 - 744
Main Authors: Ida, Daichi, Nakatomi, Daisuke, Yoshizaki, Takenao
Format: Journal Article
Language:English
Published: London Nature Publishing Group UK 01-09-2010
Nature Publishing Group
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Summary:A Monte Carlo (MC) study was made of the second virial coefficient A 2 of the ideal Kratky–Porod (KP) worm-like ring using a model composed of infinitely thin bonds with harmonic bending energy between successive bonds. Two kinds of statistical ensembles were generated: one composed of configurations of all kinds of knots with the Boltzmann weight, called the mixed ensemble, and the other composed of only those of the trivial knot, called the trivial-knot ensemble. The effective volume V E excluded to one ring by the presence of another, resulting only from a topological interaction, and also the mean-square radius of gyration 〈 S 2 〉 were evaluated for each ensemble. The dimensionless quantity λV E / L 2 proportional to A 2 was found to be a function only of the reduced total contour length λL , as in the case of λ 〈 S 2 〉/ L , where λ −1 is the stiffness parameter of the KP ring and L is its total contour length. The quantity λV E / L 2 first increased and then decreased after passing through a maximum at λL ≃5, as λL was increased. A comparison with literature data for ring atactic polystyrene in cyclohexane at Θ shows that the present MC results may qualitatively explain the behavior of the data. The effective volume V E excluded to a Kratky–Porod (KP) worm-like ring by the presence of another, resulting only from a topological interaction, was evaluated by Monte Carlo simulations. The quantity λV E / L 2 proportional to the second virial coefficient A 2 was shown to be a function only of λL with λ −1 the stiffness parameter of the KP ring and L its total contour length.
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ISSN:0032-3896
1349-0540
DOI:10.1038/pj.2010.61