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

Debye–Huckel–Onsager Conductance Equation01:28

Debye–Huckel–Onsager Conductance Equation

The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...
Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion03:48

Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion

Although gaseous molecules travel at tremendous speeds (hundreds of meters per second), they collide with other gaseous molecules and travel in many different directions before reaching the desired target. At room temperature, a gaseous molecule will experience billions of collisions per second. The mean free path is the average distance a molecule travels between collisions. The mean free path increases with decreasing pressure; in general, the mean free path for a gaseous molecule will be...
Carrier Transport01:21

Carrier Transport

The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Distance Problem01:29

Distance Problem

When an object's velocity changes over time, the total distance traveled can be determined by summing small displacement intervals over short increments. This approach approximates the true distance through numerical summation and the use of integral calculus. An estimate of the total displacement can be obtained by measuring velocity at regular intervals and multiplying each value by the corresponding time step.If a runner accelerates over the first three seconds of a race, speed measurements...
Protein Diffusion in the Membrane01:24

Protein Diffusion in the Membrane

Proteins show rotational as well as lateral diffusion across the membrane. The lateral diffusion of proteins was confirmed through the cell fusion experiment where mouse and human cells were fused, resulting in hybrid cells. When the human and mouse cells fused, the specific membrane proteins on human and mouse cells were marked with the red and green-fluorescent markers, respectively. Initially, the red and green fluorescence was located on the respective hemisphere of the cell. As time...

You might also read

Related Articles

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

Sort by
Same author

Nonconvergence of the Wang-Landau algorithms with multiple random walkers.

Physical review. E·2016
Same author

Effect of particle-hole symmetry on the behavior of tracer and jump diffusion coefficients.

Physical review. E, Statistical, nonlinear, and soft matter physics·2013
Same author

Single-file diffusion in a box: effect of the initial configuration.

Physical review. E, Statistical, nonlinear, and soft matter physics·2012
Same author

Hard versus soft dynamics for adsorption-desorption kinetics: Exact results in one-dimension.

Physical review. E, Statistical, nonlinear, and soft matter physics·2010
Same author

One-dimensional diffusion: validity of various expressions for jump rates.

Physical review. E, Statistical, nonlinear, and soft matter physics·2010
Same author

Additional constraints in adsorption-desorption kinetics.

Physical review. E, Statistical, nonlinear, and soft matter physics·2009

Related Experiment Video

Updated: May 26, 2026

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
06:55

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

Published on: September 26, 2016

One-dimensional diffusion: discrepancy between exact results and Monte Carlo calculations.

J J Torrez Herrera1, G A Ranzuglia, S J Manzi

  • 1Departamento de Física, Instituto de Física Aplicada (INFAP)-Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Universidad Nacional de San Luis, San Luis, Argentina.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|December 21, 2011
PubMed
Summary

The study compares exact diffusion coefficient expressions with Monte Carlo simulations. Anomalies arise in interaction kinetics, revealing necessary constraints for particle diffusion beyond detailed balance, impacting physical soundness.

More Related Videos

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging
06:34

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging

Published on: September 2, 2016

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package
06:37

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package

Published on: September 17, 2021

Related Experiment Videos

Last Updated: May 26, 2026

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
06:55

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

Published on: September 26, 2016

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging
06:34

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging

Published on: September 2, 2016

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package
06:37

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package

Published on: September 17, 2021

Area of Science:

  • Condensed matter physics
  • Statistical mechanics

Background:

  • The collective diffusion coefficient is crucial for understanding particle transport.
  • Previous work by Payne and Kreuzer provided an exact expression for this coefficient in 1D.

Purpose of the Study:

  • To compare the exact expression for the collective diffusion coefficient with Monte Carlo simulations.
  • To investigate the behavior of different hopping kinetics, particularly interaction kinetics.

Main Methods:

  • Comparison of an analytical expression with results from Monte Carlo simulations.
  • Analysis of various hopping kinetics, including initial-state, final-state, and interaction kinetics.

Main Results:

  • No anomalies were observed for initial- and final-state interaction kinetics.
  • Interaction kinetics, even with detailed balance, require additional constraints for particle diffusion.
  • A phase diagram emerged, highlighting regions where the exact solution appears physically unsound.

Conclusions:

  • Additional constraints beyond detailed balance are essential for particle diffusion under interaction kinetics.
  • Monte Carlo simulations reveal discrepancies with the exact solution in specific regions, suggesting limitations of the analytical model.
  • A potential explanation for these discrepancies is proposed.