English

Dynamical Monte Carlo Study of Equilibrium Polymers : Static Properties

Soft Condensed Matter 2009-10-31 v1 Disordered Systems and Neural Networks Materials Science

Abstract

We report results of extensive Dynamical Monte Carlo investigations on self-assembled Equilibrium Polymers (EP) without loops in good solvent. (This is thought to provide a good model of giant surfactant micelles.) Using a novel algorithm we are able to describe efficiently both static and dynamic properties of systems in which the mean chain length \Lav\Lav is effectively comparable to that of laboratory experiments (up to 5000 monomers, even at high polymer densities). We sample up to scission energies of E/kBT=15E/k_BT=15 over nearly three orders of magnitude in monomer density ϕ\phi, and present a detailed crossover study ranging from swollen EP chains in the dilute regime up to dense molten systems. Confirming recent theoretical predictions, the mean-chain length is found to scale as \Lavϕαexp(δE)\Lav \propto \phi^\alpha \exp(\delta E) where the exponents approach αd=δd=1/(1+γ)0.46\alpha_d=\delta_d=1/(1+\gamma) \approx 0.46 and αs=1/2[1+(γ1)/(νd1)]0.6,δs=1/2\alpha_s = 1/2 [1+(\gamma-1)/(\nu d -1)] \approx 0.6, \delta_s=1/2 in the dilute and semidilute limits respectively. The chain length distribution is qualitatively well described in the dilute limit by the Schulz-Zimm distribution \cN(s)sγ1exp(s)\cN(s)\approx s^{\gamma-1} \exp(-s) where the scaling variable is s=γL/\Lavs=\gamma L/\Lav. The very large size of these simulations allows also an accurate determination of the self-avoiding walk susceptibility exponent γ1.165±0.01\gamma \approx 1.165 \pm 0.01. ....... Finite-size effects are discussed in detail.

Keywords

Cite

@article{arxiv.cond-mat/9805263,
  title  = {Dynamical Monte Carlo Study of Equilibrium Polymers : Static Properties},
  author = {J. P. Wittmer and A. Milchev and M. E. Cates},
  journal= {arXiv preprint arXiv:cond-mat/9805263},
  year   = {2009}
}

Comments

15 pages, 14 figures, LATEX

R2 v1 2026-07-22T12:04:03.638Z