2007
DOI: 10.1063/1.2799513
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Unexpected relaxation dynamics of a self-avoiding polymer in cylindrical confinement

Abstract: We report extensive simulations of the relaxation dynamics of a self-avoiding polymer confined inside a cylindrical pore. In particular, we concentrate on examining how confinement influences the scaling behavior of the global relaxation time of the chain, tau, with the chain length N and pore diameter D. An earlier scaling analysis based on the de Gennes blob picture led to tau approximately N(2)D(13). Our numerical effort that combines molecular dynamics and Monte Carlo simulations, however, consistently pro… Show more

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Cited by 48 publications
(104 citation statements)
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“…It is a dynamic variable for the polymer and is a measure of elasticity of the polymer. Our results for the effective spring constant are in good agreement with the blob model, unlike the case of the polymer inside the nanochannel [12][13][14].…”
Section: Introductionsupporting
confidence: 87%
“…It is a dynamic variable for the polymer and is a measure of elasticity of the polymer. Our results for the effective spring constant are in good agreement with the blob model, unlike the case of the polymer inside the nanochannel [12][13][14].…”
Section: Introductionsupporting
confidence: 87%
“…25 Often, bead-spring models have been used to simulate the dynamics of such polymers in confinement via Brownian Dynamics (BD) simulations, both with 7,26,27 and without hydrodynamic interactions (HI). 28 The coarse-grained nature of these models allows simulation of experimentally relevant molecular weights with a small number of beads for a sufficiently long time. 29 Because such bead-spring models do not have the necessary resolution when the confinement size is of the order of the persistence length of the polymer, finer models have been used recently for Metropolis Monte Carlo 6,22 and lattice Boltzmann-based simulations 30 of semiflexible chains in confinement.…”
Section: Introductionmentioning
confidence: 99%
“…For strong compaction, φ c has to be as large as φ c = 0.5-0.6. In this high volume fraction, (cylindrical) confinement can induce wall-layering of hard spheres (e.g., monomers and crowders) 39,54 . Accordingly, simulation details can enter into the picture of crowding, even though their consequences may not be biologically meaningful.…”
Section: Chain Compaction For the Case A C > Amentioning
confidence: 99%