Phase transitions in single macromolecules: Loop-stretch transition versus loop adsorption transition in end-grafted polymer chains

dc.contributor.authorZhang, Shuangshuang
dc.contributor.authorQi, Shuanhu
dc.contributor.authorKlushin, Leonid I.
dc.contributor.authorSkvortsov, Aleksander M.
dc.contributor.authorYan, Dadong
dc.contributor.authorSchmid, Friederike
dc.contributor.departmentDepartment of Physics
dc.contributor.facultyFaculty of Arts and Sciences (FAS)
dc.contributor.institutionAmerican University of Beirut
dc.date.accessioned2025-01-24T11:25:10Z
dc.date.available2025-01-24T11:25:10Z
dc.date.issued2018
dc.description.abstractWe use Brownian dynamics simulations and analytical theory to compare two prominent types of single molecule transitions. One is the adsorption transition of a loop (a chain with two ends bound to an attractive substrate) driven by an attraction parameter ϵ and the other is the loop-stretch transition in a chain with one end attached to a repulsive substrate, driven by an external end-force F applied to the free end. Specifically, we compare the behavior of the respective order parameters of the transitions, i.e., the mean number of surface contacts in the case of the adsorption transition and the mean position of the chain end in the case of the loop-stretch transition. Close to the transition points, both the static behavior and the dynamic behavior of chains with different length N are very well described by a scaling ansatz with the scaling parameters (ϵ - ϵ∗)NΦ (adsorption transition) and (F - F∗)Nν (loop-stretch transition), respectively, where Φ is the crossover exponent of the adsorption transition and ν is the Flory exponent. We show that both the loop-stretch and the loop adsorption transitions provide an exceptional opportunity to construct explicit analytical expressions for the crossover functions which perfectly describe all simulation results on static properties in the finite-size scaling regime. Explicit crossover functions are based on the ansatz for the analytical form of the order parameter distributions at the respective transition points. In contrast to the close similarity in equilibrium static behavior, the dynamic relaxation at the two transitions shows qualitative differences, especially in the strongly ordered regimes. This is attributed to the fact that the surface contact dynamics in a strongly adsorbed chain is governed by local processes, whereas the end height relaxation of a strongly stretched chain involves the full spectrum of Rouse modes. © 2018 Author(s).
dc.identifier.doihttps://doi.org/10.1063/1.5013346
dc.identifier.eid2-s2.0-85041430795
dc.identifier.pmid29390835
dc.identifier.urihttp://hdl.handle.net/10938/26233
dc.language.isoen
dc.publisherAmerican Institute of Physics Inc.
dc.relation.ispartofJournal of Chemical Physics
dc.sourceScopus
dc.subjectTransition flow
dc.subjectAdsorption transitions
dc.subjectAnalytical expressions
dc.subjectBrownian dynamics simulations
dc.subjectCrossover functions
dc.subjectDynamic relaxation
dc.subjectFinite size scaling
dc.subjectQualitative differences
dc.subjectSingle macromolecules
dc.subjectAdsorption
dc.titlePhase transitions in single macromolecules: Loop-stretch transition versus loop adsorption transition in end-grafted polymer chains
dc.typeArticle

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