18,720 research outputs found

    On the chain length dependence of local correlations in polymer melts and a perturbation theory of symmetric polymer blends

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    The self-consistent field (SCF) theory of dense polymer liquids assumes that short-range correlations are almost independent of how monomers are connected into polymers. Some limits of this idea are explored in the context of a perturbation theory for mixtures of structurally identical polymer species, A and B, in which the AB pair interaction differs slightly from the AA and BB interaction, and the difference is controlled by a parameter alpha Expanding the free energy to O(\alpha) yields an excess free energy of the form alpha z(N)ϕAϕBz(N)\phi_{A}\phi_{B}, in both lattice and continuum models, where z(N) is a measure of the number of inter-molecular near neighbors of each monomer in a one-component liquid. This quantity decreases slightly with increasing N because the self-concentration of monomers from the same chain is slightly higher for longer chains, creating a deeper correlation hole for longer chains. We analyze the resulting NN-dependence, and predict that z(N)=z∞[1+βNˉ−1/2]z(N) = z^{\infty}[1 + \beta \bar{N}^{-1/2}], where Nˉ\bar{N} is an invariant degree of polymerization, and β=(6/π)3/2\beta=(6/\pi)^{3/2}. This and other predictions are confirmed by comparison to simulations. We also propose a way to estimate the effective interaction parameter appropriate for comparisons of simulation data to SCF theory and to coarse-grained theories of corrections to SCF theory, which is based on an extrapolation of coefficients in this perturbation theory to the limit N→∞N \to \infty. We show that a renormalized one-loop theory contains a quantitatively correct description of the NN-dependence of local structure studied here.Comment: submitted to J. Chem. Phy

    Universality of subleading corrections for self-avoiding walks in presence of one dimensional defects

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    We study three-dimensional self-avoiding walks in presence of a one-dimensional excluded region. We show the appearance of a universal sub-leading exponent which is independent of the particular shape and symmetries of the excluded region. A classical argument provides the estimate: Δ=2ν−1≈0.175(1)\Delta = 2 \nu - 1 \approx 0.175(1). The numerical simulation gives Δ=0.18(2)\Delta = 0.18(2).Comment: 29 pages, latex2
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