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

The de Broglie Wavelength02:32

The de Broglie Wavelength

32.8K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
32.8K
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

13.9K
Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about...
13.9K
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

7.9K
Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
7.9K
Angular Momentum: Single Particle01:10

Angular Momentum: Single Particle

7.6K
Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm...
7.6K
Poisson's And Laplace's Equation01:25

Poisson's And Laplace's Equation

4.1K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
4.1K
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

58.8K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
58.8K

You might also read

Related Articles

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

Sort by
Same author

Charging capacitors using diodes at different temperatures. I. Theory.

Physical review. E·2026
Same author

Charging capacitors using diodes at different temperatures. II. Numerical studies.

Physical review. E·2026
Same author

Power laws of natural swarms as fingerprints of an extended critical region.

Physical review. E·2024
Same author

Soliton approximation in continuum models of leader-follower behavior.

Physical review. E·2023
Same author

Charging capacitors from thermal fluctuations using diodes.

Physical review. E·2023
Same author

Mean-field theory of chaotic insect swarms.

Physical review. E·2023
Same journal

Erratum: Low-dimensional model for adaptive networks of spiking neurons [Phys. Rev. E 111, 014422 (2025)].

Physical review. E·2026
Same journal

Disentangling the effects of many-body forces on depletion interactions.

Physical review. E·2026
Same journal

Charge transport and mode transition in dual-energy electron beam diodes.

Physical review. E·2026
Same journal

Optimization of multisite reactions in complex compartmentalized media.

Physical review. E·2026
Same journal

Origin of geometric cohesion in nonconvex granular materials: Interplay between interdigitation and rotational constraints enhancing frictional stability.

Physical review. E·2026
Same journal

Interaction of walkers with a standing Faraday wave.

Physical review. E·2026
See all related articles

Related Experiment Video

Updated: Jan 6, 2026

Preparation of Janus Particles and Alternating Current Electrokinetic Measurements with a Rapidly Fabricated Indium Tin Oxide Electrode Array
09:55

Preparation of Janus Particles and Alternating Current Electrokinetic Measurements with a Rapidly Fabricated Indium Tin Oxide Electrode Array

Published on: June 23, 2017

8.6K

Active Ornstein-Uhlenbeck particles.

L L Bonilla1

  • 1G. Millán Institute for Fluid Dynamics, Nanoscience & Industrial Mathematics, and Department of Materials Science & Engineering and Chemical Engineering, Universidad Carlos III de Madrid, Avenida de la Universidad 30, 28911 Leganés, Spain and Courant Institute of Mathematical Sciences, New York University, 251 Mercer St, New York, New York 10012, USA.

Physical Review. E
|October 3, 2019
PubMed
Summary
This summary is machine-generated.

Active Ornstein-Uhlenbeck particles (AOUPs) achieve equilibrium probability density invariant under time reversal only if their interaction potential has zero third derivatives. Small persistence time expansions reveal deviations from equilibrium at higher orders.

More Related Videos

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
11:51

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions

Published on: February 22, 2018

9.1K
Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas
07:54

Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas

Published on: April 3, 2018

8.6K

Related Experiment Videos

Last Updated: Jan 6, 2026

Preparation of Janus Particles and Alternating Current Electrokinetic Measurements with a Rapidly Fabricated Indium Tin Oxide Electrode Array
09:55

Preparation of Janus Particles and Alternating Current Electrokinetic Measurements with a Rapidly Fabricated Indium Tin Oxide Electrode Array

Published on: June 23, 2017

8.6K
Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
11:51

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions

Published on: February 22, 2018

9.1K
Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas
07:54

Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas

Published on: April 3, 2018

8.6K

Area of Science:

  • Statistical Mechanics
  • Non-equilibrium Thermodynamics

Background:

  • Active Ornstein-Uhlenbeck particles (AOUPs) are overdamped systems subjected to interaction potentials and external noises.
  • The equilibrium properties of AOUPs, particularly in the limit of small persistence times, are a subject of ongoing research.

Purpose of the Study:

  • To determine the conditions under which AOUPs can reach an equilibrium state.
  • To analyze the deviation from equilibrium for AOUPs as a function of persistence time.

Main Methods:

  • Utilized a theorem on the time-reversed form of Langevin-Ito equations for AOUPs.
  • Applied Chapman-Enskog expansion to the Fokker-Planck equation in the limit of small persistence time (τ).

Main Results:

  • Proved that equilibrium probability density invariant under time reversal exists if and only if the interaction potential's third derivative is zero.
  • Showed that for small τ, the probability density exhibits local equilibrium in momenta, modulated by a position-dependent reduced density.
  • Demonstrated that terms up to O(τ) in the probability current expansion lead to a diffusion equation with a zero-current stationary solution.
  • Identified that O(τ²) terms introduce higher-order spatial derivatives, resulting in a non-zero current and odd momentum terms, indicating a non-equilibrium state.

Conclusions:

  • AOUPs can achieve a specific type of equilibrium only under strict conditions on their interaction potential.
  • Deviations from equilibrium become significant at higher orders of the small persistence time expansion, characterized by complex spatial derivatives and non-zero probability currents.