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

Equipotential Surfaces and Conductors01:16

Equipotential Surfaces and Conductors

3.6K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
3.6K
Van de Graaff Generator01:15

Van de Graaff Generator

1.8K
Van de Graaff generators (or Van de Graaffs) are devices used to demonstrate high voltage due to static electricity that can also be used for research. Robert Van de Graaff first built one in 1931 (based on original suggestions by Lord Kelvin) for use in nuclear physics research.
Van de Graaff uses both smooth and pointed surfaces, conductors, and insulators to generate large static charges and, hence, large voltages. A substantial excess charge can be deposited on the sphere because it moves...
1.8K
Charging Conductors By Induction01:15

Charging Conductors By Induction

8.2K
The Earth is a good conductor of electricity, and it is so big that it can be considered an infinite source or sink of charges. It can easily exchange charges with any matter.
Generally, conductors like metals do not allow any excess charge to be present on them. Any excess charge added to metals easily flows away, for example, when a metal is placed on the Earth. This process is called earthing.
However, conductors can be charged by a process called induction. For example, consider charging a...
8.2K
Charge on a Conductor01:26

Charge on a Conductor

4.7K
An interesting property of a conductor in static equilibrium is that extra charges on the conductor end up on its outer surface, regardless of where they originate. Consider a hollow metallic conductor with a uniform surface charge density. Since the conductor itself is in electrostatic equilibrium, there should not be any electric field inside the conductor. Now, assume a Gaussian surface enclosing the hollow portion. Applying Gauss's law, the inner surface of the hollow conductor will not...
4.7K
Coulomb's Law01:30

Coulomb's Law

10.0K
Experiments with electric charges have shown that if two objects each have an electric charge, they exert an electric force on each other. The magnitude of the force is linearly proportional to the net charge on each object and inversely proportional to the square of the distance between them. The direction of the force vector is along the imaginary line joining the two objects and is dictated by the signs of the charges involved.
Newton's third law applies to the Coulomb force — the...
10.0K
Electric Field of a Charged Disk01:23

Electric Field of a Charged Disk

2.4K
The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
2.4K

You might also read

Related Articles

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

Sort by
Same author

Hypoxia-induced inhibition of cell proliferation mediated by TFRC in mouse spermatogonial stem cells.

Reproduction, fertility, and development·2026
Same author

Artificial intelligence for carbon emissions management: advances, challenges, and future directions across monitoring, prediction, and reduction.

Carbon balance and management·2026
Same author

Extraction and characterization of microcrystalline cellulose from kelp (Laminaria japonica) waste.

PloS one·2026
Same author

A thin robot made of flexible electronics for in-situ machining and inspection of large structures.

Nature communications·2026
Same author

Structural superlubricity triboelectric nanogenerator with negligible wear and high triboelectrification efficiency.

Nature communications·2026
Same author

Reagent-Free Molecular Pendulum Biosensor with Antibody-Aptamer Dual Recognition for Protein Analysis.

ACS sensors·2026

Related Experiment Video

Updated: Sep 11, 2025

AC Electrokinetic Phenomena Generated by Microelectrode Structures
20:38

AC Electrokinetic Phenomena Generated by Microelectrode Structures

Published on: July 28, 2008

11.6K

Microscale Contact Electrification with Unprecedented High Intrinsic Charge Density.

Chaojie Chen1, Jinhui Nie2, Jie An3

  • 1Department of Mechanical and Automation Engineering, The Chinese University of Hong Kong Shatin, N.T. Hong Kong, China.

Small (Weinheim an Der Bergstrasse, Germany)
|August 18, 2025
PubMed
Summary

Contact electrification (CE) generates charge between materials. Using atomically flat surfaces of polytetrafluoroethylene (PTFE) and graphite achieved high charge density, overcoming limitations of rough surfaces.

Keywords:
contact efficiencycontact electrificationtriboelectric charge density

More Related Videos

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

8.3K
Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

3.5K

Related Experiment Videos

Last Updated: Sep 11, 2025

AC Electrokinetic Phenomena Generated by Microelectrode Structures
20:38

AC Electrokinetic Phenomena Generated by Microelectrode Structures

Published on: July 28, 2008

11.6K
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

8.3K
Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

3.5K

Area of Science:

  • Materials Science
  • Surface Physics
  • Triboelectricity

Background:

  • Contact electrification (CE) is crucial for applications like electrophotography and energy harvesting.
  • Surface roughness in CE limits effective contact area and charge density.

Purpose of the Study:

  • To enhance contact efficiency and achieve higher intrinsic charge density in CE.
  • To investigate the charging mechanism at the graphite/polytetrafluoroethylene (PTFE) interface.

Main Methods:

  • Utilized atomically flat polytetrafluoroethylene (PTFE) and graphite microflakes.
  • Analyzed charge generation and distribution at the material interface.

Main Results:

  • Achieved an unprecedented intrinsic CE charge density of 2.6 mC m-2.
  • Observed unipolar negative charging at the graphite/PTFE interface, eliminating charge cancellation.
  • Demonstrated amplified net charge density, deviating from the typical charge mosaic pattern.

Conclusions:

  • Atomically flat surfaces significantly improve CE efficiency and charge density.
  • Unipolar charging at interfaces offers a pathway to controllable and amplified triboelectric charge.
  • Findings provide fundamental insights for developing advanced materials and interfaces for CE applications.