2021
DOI: 10.1016/j.jmps.2021.104593
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Chain breaking in the statistical mechanical constitutive theory of polymer networks

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Cited by 30 publications
(31 citation statements)
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“…The freely-jointed chain (FJC) model consists of N b rigid links of length b ; the links may pass through each other or overlap, and are connected in series by penaltyfree hinges [1,2,4]. This single-chain model is generalized to the uFJC model through assigning some potential energy function u to each link and allowing the link length to fluctuate away from its rest length b [5]. Here the isotensional ensemble is considered, where a fixed force f is applied to the chain and the expected chain endto-end length ξ is calculated using the partition function [6,8,22].…”
Section: Theorymentioning
confidence: 99%
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“…The freely-jointed chain (FJC) model consists of N b rigid links of length b ; the links may pass through each other or overlap, and are connected in series by penaltyfree hinges [1,2,4]. This single-chain model is generalized to the uFJC model through assigning some potential energy function u to each link and allowing the link length to fluctuate away from its rest length b [5]. Here the isotensional ensemble is considered, where a fixed force f is applied to the chain and the expected chain endto-end length ξ is calculated using the partition function [6,8,22].…”
Section: Theorymentioning
confidence: 99%
“…is necessary to obtain the single-chain mechanical response of the uFJC model since the link degrees of freedom become decoupled in the isotensional ensemble [5,6,22]. After computing the angular integrals and nondimensionalizing the integrand, the result is…”
Section: Low-to-intermediate Force Asymptoticsmentioning
confidence: 99%
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