Are polymer melts "ideal"?
It is commonly accepted that in concentrated solutions or melts high-molecular weight polymers display random-walk conformational properties without long-range correlations between subsequent bonds. This absence of memory means, for instance, that the bond-bond correlation function, \(P(s)\), of two...
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Published in | arXiv.org |
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Main Authors | , , , , , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
13.10.2006
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Subjects | |
Online Access | Get full text |
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Summary: | It is commonly accepted that in concentrated solutions or melts high-molecular weight polymers display random-walk conformational properties without long-range correlations between subsequent bonds. This absence of memory means, for instance, that the bond-bond correlation function, \(P(s)\), of two bonds separated by \(s\) monomers along the chain should exponentially decay with \(s\). Presenting numerical results and theoretical arguments for both monodisperse chains and self-assembled (essentially Flory size-distributed) equilibrium polymers we demonstrate that some long-range correlations remain due to self-interactions of the chains caused by the chain connectivity and the incompressibility of the melt. Suggesting a profound analogy with the well-known long-range velocity correlations in liquids we find, for instance, \(P(s)\) to decay algebraically as \(s^{-3/2}\). Our study suggests a precise method for obtaining the statistical segment length \bstar in a computer experiment. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.0610359 |