Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Energy Diagrams - II01:10

Energy Diagrams - II

Energy diagrams are important to understand the dynamics of a system. The topology of an energy diagram helps illustrate the equilibrium points of the system.
The point in the energy diagram at which the system’s potential energy is the lowest is known as the local minima. The system tends to stay in this position indefinitely unless acted upon by a net force. The slope of the potential energy diagram at the local minima is zero, indicating that zero net force is acting on the system. The slope...
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
Entropy02:39

Entropy

Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
Entropy01:18

Entropy

The first law of thermodynamics is quantitatively formulated via an equation relating the internal energy of a system, the heat exchanged by it, and the work done on it. A quantitative formulation of the second law of thermodynamics leads to defining a state function, the entropy.
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
The Entropy as a State Function01:14

The Entropy as a State Function

Consider an arbitrary process that moves between two specific states (A and B) in a cyclic manner. This process is reversible and broken down into smaller parts that each follow a Carnot cycle. A Carnot cycle has two isothermal (constant temperature) processes. During these processes, the ratio of the amount of heat transferred to their respective temperature remains constant. The other two processes in the Carnot cycle are also reversible but adiabatic, which means they occur without any heat...
Energy Diagrams - I01:14

Energy Diagrams - I

The dynamics of a mechanical system can be easily understood by interpreting a potential energy diagram. Since energy is a scalar quantity, the interpretation of the dynamics of the system becomes even simpler.
Take the example of a skater on a parabolic ramp. The potential energy at different points along the ramp will be proportional to the height of the ramp, which varies quadratically with the horizontal position on the ramp. As the skater moves down the ramp from the highest position,...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

The local mechanostructural properties of protein cargoes regulate nucleocytoplasmic transport.

Nature physics·2026
Same author

Observation of Robust Macroscale Structural Superlubricity.

Physical review letters·2026
Same author

Conformation-driven mechanical duality: Viscoelastic and poroelastic switching in protein hydrogels.

Acta biomaterialia·2026
Same author

Author Correction: Switching graphitic polytypes in elastically coupled cavities.

Nature nanotechnology·2026
Same author

Switching graphitic polytypes in elastically coupled cavities.

Nature nanotechnology·2026
Same author

Force writes memory: proline isomerization as a molecular memory switch.

Biochemical Society transactions·2025

Related Experiment Video

Updated: Jun 7, 2026

Nanomanipulation of Single RNA Molecules by Optical Tweezers
06:59

Nanomanipulation of Single RNA Molecules by Optical Tweezers

Published on: August 20, 2014

Hopping around an entropic barrier created by force.

Ronen Berkovich1, Sergi Garcia-Manyes, Joseph Klafter

  • 1Department of Biological Sciences, Columbia University, New York, NY 10027, USA.

Biochemical and Biophysical Research Communications
|November 6, 2010
PubMed
Summary

A force-induced entropic energy barrier explains two-state hopping in single RNA, DNA, and protein molecules. This barrier, absent at zero force, drives molecular conformational changes and is crucial for understanding single-molecule behavior.

More Related Videos

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

High-Speed Magnetic Tweezers for Nanomechanical Measurements on Force-Sensitive Elements
08:50

High-Speed Magnetic Tweezers for Nanomechanical Measurements on Force-Sensitive Elements

Published on: May 12, 2023

Related Experiment Videos

Last Updated: Jun 7, 2026

Nanomanipulation of Single RNA Molecules by Optical Tweezers
06:59

Nanomanipulation of Single RNA Molecules by Optical Tweezers

Published on: August 20, 2014

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

High-Speed Magnetic Tweezers for Nanomechanical Measurements on Force-Sensitive Elements
08:50

High-Speed Magnetic Tweezers for Nanomechanical Measurements on Force-Sensitive Elements

Published on: May 12, 2023

Area of Science:

  • Biophysics
  • Computational Biology
  • Molecular Dynamics

Background:

  • Single RNA, DNA, and protein molecules exhibit two-state hopping phenomena under stretching force.
  • This behavior is often interpreted as two-state folding/unfolding reactions, but the underlying mechanism at the single-molecule level requires further investigation.

Purpose of the Study:

  • To investigate the role of the force-induced entropic energy barrier in single-molecule two-state hopping.
  • To understand how applied force influences molecular conformations and transitions.

Main Methods:

  • Langevin dynamics simulations were employed to model molecular behavior under stretching force.
  • Free energy considerations were used to analyze the entropic barrier formation.

Main Results:

  • A force-induced entropic energy barrier was identified, separating collapsed and extended molecular states.
  • This barrier exhibits long transition state distances (up to tens of nanometers).
  • Langevin dynamics simulations reproduced the observed hopping behavior, demonstrating force-sensitive kinetics.

Conclusions:

  • The force-induced entropic energy barrier is a key factor driving the observed two-state hopping in single molecules.
  • This barrier mechanism explains phenomena not observed in bulk experiments due to the absence of force.
  • The study highlights the distinct behavior of single molecules under force compared to bulk conditions.