What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?

Self-diffusivity of a large tracer ring polymer, D r , immersed in a matrix of linear polymers with N l monomers each shows unusual length dependence. D r initially increases, and then decreases with increasing N l . To understand the relationship between the nonmonoton...

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Main Authors: Benjamin Crysup, Sachin Shanbhag
Format: Article
Language:English
Published: MDPI AG 2016-11-01
Series:Polymers
Subjects:
Online Access:http://www.mdpi.com/2073-4360/8/12/409
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spelling doaj-56a44862465442149eb5eb8f00cad1502020-11-25T00:36:35ZengMDPI AGPolymers2073-43602016-11-0181240910.3390/polym8120409polym8120409What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?Benjamin Crysup0Sachin Shanbhag1Department of Scientific Computing, Florida State University, Tallahassee, FL 32306, USADepartment of Scientific Computing, Florida State University, Tallahassee, FL 32306, USASelf-diffusivity of a large tracer ring polymer, D r , immersed in a matrix of linear polymers with N l monomers each shows unusual length dependence. D r initially increases, and then decreases with increasing N l . To understand the relationship between the nonmonotonic variation in D r and threading by matrix chains, we perform equilibrium Monte Carlo simulations of ring-linear blends in which the uncrossability of ring and linear polymer contours is switched on (non-crossing), or artificially turned off (crossing). The D r ≈ 6 . 2 × 10 − 7 N l 2 / 3 obtained from the crossing simulations, provides an upper bound for the D r obtained for the regular, non-crossing simulations. The center-of-mass mean-squared displacement ( g 3 ( t ) ) curves for the crossing simulations are consistent with the Rouse model; we find g 3 ( t ) = 6 D r t . Analysis of the polymer structure indicates that the smaller matrix chains are able to infiltrate the space occupied by the ring probe more effectively, which is dynamically manifested as a larger frictional drag per ring monomer.http://www.mdpi.com/2073-4360/8/12/409ring polymercyclic polymerdiffusionprobe diffusionpolymer blendMonte Carlo simulation
collection DOAJ
language English
format Article
sources DOAJ
author Benjamin Crysup
Sachin Shanbhag
spellingShingle Benjamin Crysup
Sachin Shanbhag
What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
Polymers
ring polymer
cyclic polymer
diffusion
probe diffusion
polymer blend
Monte Carlo simulation
author_facet Benjamin Crysup
Sachin Shanbhag
author_sort Benjamin Crysup
title What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
title_short What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
title_full What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
title_fullStr What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
title_full_unstemmed What Happens When Threading is Suppressed in Blends of Ring and Linear Polymers?
title_sort what happens when threading is suppressed in blends of ring and linear polymers?
publisher MDPI AG
series Polymers
issn 2073-4360
publishDate 2016-11-01
description Self-diffusivity of a large tracer ring polymer, D r , immersed in a matrix of linear polymers with N l monomers each shows unusual length dependence. D r initially increases, and then decreases with increasing N l . To understand the relationship between the nonmonotonic variation in D r and threading by matrix chains, we perform equilibrium Monte Carlo simulations of ring-linear blends in which the uncrossability of ring and linear polymer contours is switched on (non-crossing), or artificially turned off (crossing). The D r ≈ 6 . 2 × 10 − 7 N l 2 / 3 obtained from the crossing simulations, provides an upper bound for the D r obtained for the regular, non-crossing simulations. The center-of-mass mean-squared displacement ( g 3 ( t ) ) curves for the crossing simulations are consistent with the Rouse model; we find g 3 ( t ) = 6 D r t . Analysis of the polymer structure indicates that the smaller matrix chains are able to infiltrate the space occupied by the ring probe more effectively, which is dynamically manifested as a larger frictional drag per ring monomer.
topic ring polymer
cyclic polymer
diffusion
probe diffusion
polymer blend
Monte Carlo simulation
url http://www.mdpi.com/2073-4360/8/12/409
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