{"title":"Structural transitions of a Semi-Flexible Polyampholyte","authors":"Rakesh Palariya, Sunil P. Singh","doi":"arxiv-2408.15921","DOIUrl":null,"url":null,"abstract":"Polyampholytes (PA) are charged polymers composed of positively and\nnegatively charged monomers along their backbone. The sequence of the charged\nmonomers and the bending of the chain significantly influence the conformation\nand dynamical behavior of the PA. Using coarse-grained molecular dynamics\nsimulations, we comprehensively study the structural and dynamical properties\nof flexible and semi-flexible polyampholytes'. The simulation results\ndemonstrate a flexible polyampholyte (PA) chain, displaying a transition from a\ncoil to a globule in the parameter space of the charge sequence. Additionally,\nthe behavior of the mean-square displacement (MSD), denoted as $<(\\Delta\nr(t))^2>$, reveals distinct dynamics, specifically for the alternating and\ncharge-segregated sequences. The MSD follows a power-law behavior, where\n$<(\\Delta r(t))^2> \\sim t^\\beta$, with $\\beta \\approx 3/5$ and $\\beta \\approx\n1/2$ for the alternating sequence and charge-segregated sequence in the absence\nof hydrodynamic interactions, respectively. However, when hydrodynamic\ninteractions are incorporated, the exponent $\\beta$ shifts to approximately 3/5\nfor the charge-segregated sequence and 2/3 for the well-mixed alternating\nsequence. For a semi-flexible PA chain, varying the bending rigidity and\nelectrostatic interaction strength ($\\Gamma_e$) leads to distinct, fascinating\nconformational states, including globule, bundle, and torus-like conformations.\nWe show that PA acquires circular and hairpin-like conformations in the\nintermediate bending regime. The transition between various conformations is\nidentified in terms of the shape factor estimated from the ratios of\neigenvalues of the gyration tensor.","PeriodicalId":501146,"journal":{"name":"arXiv - PHYS - Soft Condensed Matter","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Soft Condensed Matter","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.15921","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Polyampholytes (PA) are charged polymers composed of positively and
negatively charged monomers along their backbone. The sequence of the charged
monomers and the bending of the chain significantly influence the conformation
and dynamical behavior of the PA. Using coarse-grained molecular dynamics
simulations, we comprehensively study the structural and dynamical properties
of flexible and semi-flexible polyampholytes'. The simulation results
demonstrate a flexible polyampholyte (PA) chain, displaying a transition from a
coil to a globule in the parameter space of the charge sequence. Additionally,
the behavior of the mean-square displacement (MSD), denoted as $<(\Delta
r(t))^2>$, reveals distinct dynamics, specifically for the alternating and
charge-segregated sequences. The MSD follows a power-law behavior, where
$<(\Delta r(t))^2> \sim t^\beta$, with $\beta \approx 3/5$ and $\beta \approx
1/2$ for the alternating sequence and charge-segregated sequence in the absence
of hydrodynamic interactions, respectively. However, when hydrodynamic
interactions are incorporated, the exponent $\beta$ shifts to approximately 3/5
for the charge-segregated sequence and 2/3 for the well-mixed alternating
sequence. For a semi-flexible PA chain, varying the bending rigidity and
electrostatic interaction strength ($\Gamma_e$) leads to distinct, fascinating
conformational states, including globule, bundle, and torus-like conformations.
We show that PA acquires circular and hairpin-like conformations in the
intermediate bending regime. The transition between various conformations is
identified in terms of the shape factor estimated from the ratios of
eigenvalues of the gyration tensor.