# Refolding dynamics of stretched biopolymers upon force quench

Source: [Refolding dynamics of stretched biopolymers upon force quench](<https://www.sota2.com/research/paper/68fa2f241e209131ce869a9d>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-28T13:53:36.585Z

Authors: Changbong Hyeon, Greg Morrison, David L. Pincus, D. Thirumalai

Published: 2009-11-18T13:14:17.000Z

## Abstract

Single molecule force spectroscopy methods can be used to generate folding trajectories of biopolymers from arbitrary regions of the folding landscape. We illustrate the complexity of the folding kinetics and generic aspects of the collapse of RNA and proteins upon force quench, using simulations of an RNA hairpin and theory based on the de Gennes model for homopolymer collapse. The folding time, $\\tau\_F$, depends asymmetrically on $\\delta f\_S = f\_S - f\_m$ and $\\delta f\_Q = f\_m - f\_Q$ where $f\_S$ ($f\_Q$) is the stretch (quench) force, and $f\_m$ is the transition mid-force of the RNA hairpin. In accord with experiments, the relaxation kinetics of the molecular extension, $R(t)$, occurs in three stages: a rapid initial decrease in the extension is followed by a plateau, and finally an abrupt reduction in $R(t)$ that occurs as the native state is approached.   The duration of the plateau increases as $\\lambda =\\tau\_Q/\\tau\_F$ decreases (where $\\tau\_Q$ is the time in which the force is reduced from $f\_S$ to $f\_Q$). Variations in the mechanisms of force quench relaxation as $\\lambda$ is altered are reflected in the experimentally measurable time-dependent entropy, which is computed directly from the folding trajectories. An analytical solution of the de Gennes model under tension reproduces the multistage stage kinetics in $R(t)$. The prediction that the initial stages of collapse should also be a generic feature of polymers is validated by simulation of the kinetics of toroid (globule) formation in semiflexible (flexible) homopolymers in poor solvents upon quenching the force from a fully stretched state. Our findings give a unified explanation for multiple disparate experimental observations of protein folding.

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## Original sources and implementation

[Original paper](<https://arxiv.org/abs/0911.3530>)

[PDF](<https://arxiv.org/pdf/0911.3530.pdf>)