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

Wald-Wolfowitz Runs Test I01:17

Wald-Wolfowitz Runs Test I

The Wald-Wolfowitz test, also known as the runs test, is a nonparametric statistical test used to assess the randomness of a sequence of two different types of elements (e.g., positive/negative values, successes/failures). It examines whether the order of the elements in a sequence is random or if there is a pattern or trend present. This nonparametric test applies to any ordered data despite the population and sample data distribution, even if a higher sample size is available.
The test works...
Wald-Wolfowitz Runs Test II01:17

Wald-Wolfowitz Runs Test II

The Wald-Wolfowitz runs test, commonly referred to as the runs test, is a nonparametric test used to assess the randomness of ordered data. The test evaluates the number of runs, which are consecutive sequences of similar elements within the data. If the number of runs is significantly higher or lower than expected, the data is considered non-random, indicating a detectable pattern or structure.
For binary data, runs are identified using symbols such as + and −, or equivalently, 1s and 0s. In...
Random Variables01:09

Random Variables

A random variable is a single numerical value that indicates the outcome of a procedure. The concept of random variables is fundamental to the probability theory and was introduced by a Russian mathematician, Pafnuty Chebyshev, in the mid-nineteenth century.
Uppercase letters such as X or Y denote a random variable. Lowercase letters like x or y denote the value of a random variable. If X is a random variable, then X is written in words, and x is given as a number.
For example, let X = the...
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

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 we...
Basic Discrete Time Signals01:16

Basic Discrete Time Signals

The unit step sequence is defined as 1 for zero and positive values of the integer n. This sequence can be graphically displayed using a set of eight sample points, showing a step function starting from n=0 and remaining constant thereafter.
The unit impulse or sample sequence is mathematically expressed as zero for all n values except at n=0, where it is one. The unit impulse sequence, denoted by δ(n), is the first difference of the unit step sequence, while the unit step sequence u(n) is the...
The de Broglie Wavelength02:32

The de Broglie Wavelength

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...

You might also read

Related Articles

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

Sort by
Same author

Helium spin-echo as a surface-sensitive probe of vibrational energy dissipation.

Faraday discussions·2026
Same author

Single-molecular diffusivity and long jumps of large organic molecules: CoPc on Ag(100).

Frontiers in chemistry·2024
Same author

Attenuation of Photoelectron Emission by a Single Organic Layer.

ACS applied materials & interfaces·2022
Same author

Standard deviation of microscopy images used as indicator for growth stages.

Ultramicroscopy·2022
Same author

Coexistence of nanowire-like hex and (1 × 1) phases in the topmost layer of Au(100) surface.

Nanotechnology·2018
Same author

Phthalocyanine arrangements on Ag(100): From pure overlayers of CoPc and F<sub>16</sub>CuPc to bimolecular heterostructure.

The Journal of chemical physics·2018

Related Experiment Video

Updated: Jun 27, 2026

Asymmetric Walkway: A Novel Behavioral Assay for Studying Asymmetric Locomotion
08:19

Asymmetric Walkway: A Novel Behavioral Assay for Studying Asymmetric Locomotion

Published on: January 15, 2016

Asymmetric one-dimensional random walks.

Grazyna Antczak1, Gert Ehrlich

  • 1Department of Materials Science and Engineering, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA. antczak@mrl.uiuc.edu

The Journal of Chemical Physics
|December 3, 2008
PubMed
Summary

Particle movement on surfaces involves biased random walks. Analyzing displacement moments, especially the third moment, reveals the directionality and asymmetry of these diffusion processes.

Area of Science:

  • Physics
  • Physical Chemistry
  • Materials Science

Background:

  • Surface diffusion is crucial for processes like catalysis and thin-film growth.
  • Particle movement under external fields often exhibits directional bias.
  • Understanding random walk dynamics is fundamental in statistical mechanics.

Purpose of the Study:

  • To analyze one-dimensional surface diffusion with asymmetric jump rates.
  • To investigate how displacement distribution moments reveal diffusion asymmetry.
  • To determine the utility of the third moment in characterizing biased random walks.

Main Methods:

  • Modeling particle movement as a one-dimensional random walk with unequal forward and backward jump rates.
  • Calculating moments of the displacement distribution for nearest-neighbor and next-nearest-neighbor jumps.

More Related Videos

Studying Cell Rolling Trajectories on Asymmetric Receptor Patterns
04:24

Studying Cell Rolling Trajectories on Asymmetric Receptor Patterns

Published on: February 13, 2011

Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis
06:44

Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis

Published on: September 23, 2025

Related Experiment Videos

Last Updated: Jun 27, 2026

Asymmetric Walkway: A Novel Behavioral Assay for Studying Asymmetric Locomotion
08:19

Asymmetric Walkway: A Novel Behavioral Assay for Studying Asymmetric Locomotion

Published on: January 15, 2016

Studying Cell Rolling Trajectories on Asymmetric Receptor Patterns
04:24

Studying Cell Rolling Trajectories on Asymmetric Receptor Patterns

Published on: February 13, 2011

Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis
06:44

Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis

Published on: September 23, 2025

  • Examining the displacement distribution and its evolution with changing jump rate asymmetry.
  • Main Results:

    • Developed a framework to analyze one-dimensional biased random walks.
    • Showed that moments of the displacement distribution provide insights into jump processes.
    • Demonstrated that the third moment clearly indicates the asymmetry of the random walk.

    Conclusions:

    • The third moment of displacement is a robust indicator of asymmetry in biased diffusion.
    • This analysis offers a method to quantify directional bias in surface diffusion.
    • Understanding these asymmetric random walks is key to controlling surface phenomena.