2014
DOI: 10.1063/1.4896701
|View full text |Cite
|
Sign up to set email alerts
|

Crumpled globule formation during collapse of a long flexible and semiflexible polymer in poor solvent

Abstract: By introducing explicit solvent particles and hydrodynamic interactions we demonstrate that crumpled globules are formed after the collapse of long polymer chains (N = 10(4)) in a poor solvent. During the collapse crumples of all sizes form sequentially, but small crumples are not stable and convert to blobs with Gaussian statistics. The observed effective mean squared distance R(2)(n) ∼ n(0.38) at n > Ne and contact probability index p(n) ∼ n(-0.5) at n ≫ Ne, which is not following either the model of a fract… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

5
50
0

Year Published

2015
2015
2021
2021

Publication Types

Select...
6
1

Relationship

0
7

Authors

Journals

citations
Cited by 29 publications
(55 citation statements)
references
References 48 publications
5
50
0
Order By: Relevance
“…Recent computational studies examined the role of topological constraints in the non-equilibrium (or quasiequilibrium) polymer states that emerge upon polymer collapse [15][16][17][18][19]. This non-equilibrium state, often referred to as the fractal globule [6,15], can indeed possess some properties of the conjectured equilibrium crumpled globule.…”
Section: Introductionmentioning
confidence: 99%
“…Recent computational studies examined the role of topological constraints in the non-equilibrium (or quasiequilibrium) polymer states that emerge upon polymer collapse [15][16][17][18][19]. This non-equilibrium state, often referred to as the fractal globule [6,15], can indeed possess some properties of the conjectured equilibrium crumpled globule.…”
Section: Introductionmentioning
confidence: 99%
“…The end-to-end distance r m of segments of length m in the resulting globule is predicted to scale as r m ∼ m 1=d in d space dimensions (throughout the Letter d ¼ 3). This is in contrast to the equilibrium state reached at much later times [10], where r m ∼ m 1=2 for small m, saturating at the globule size r max ¼ N 1=d , where N is the length of the polymer [21].These predictions have been tested in several simulations of polymer compaction [2,[4][5][6]11], which generally confirm that the rapidly collapsed state is not entangled, and is indeed different from the equilibrium globule. However, they do not agree upon its fractal nature.…”
mentioning
confidence: 89%
“…These predictions have been tested in several simulations of polymer compaction [2,[4][5][6]11], which generally confirm that the rapidly collapsed state is not entangled, and is indeed different from the equilibrium globule. However, they do not agree upon its fractal nature.…”
mentioning
confidence: 96%
See 2 more Smart Citations