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Induced Electric Fields01:23

Induced Electric Fields

3.7K
The fact that emfs are induced in circuits implies that work is being done on the conduction electrons in the wires. What can possibly be the source of this work? We know that it’s neither a battery nor a magnetic field, as a battery does not have to be present in a circuit where current is induced, and magnetic fields never do any work on moving charges. The source of the work is in fact an electric field that is induced in the wires. For example, if a stationary conductor is placed in a...
3.7K
Magnetic Field of a Solenoid01:18

Magnetic Field of a Solenoid

3.9K
A solenoid is a conducting wire coated with an insulating material, wound tightly in the form of a helical coil. The magnetic field due to a solenoid is the vector sum of the magnetic fields due to its individual turns. Therefore, for an ideal solenoid, the magnetic field within the solenoid is directly proportional to the number of turns per unit length and the current. Conversely, the magnetic field outside the solenoid is zero.
Consider a solenoid with 100 turns wrapped around a cylinder of...
3.9K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

8.6K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
8.6K
Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

4.7K
Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
4.7K
Electric Field Inside a Conductor01:20

Electric Field Inside a Conductor

6.0K
When a conductor is placed in an external electric field, the free charges in the conductor redistribute and very quickly reach electrostatic equilibrium. The resulting charge distribution and its electric field have many interesting properties, which can be investigated with the help of Gauss's law.
Suppose a piece of metal is placed near a positive charge. The free electrons in the metal are attracted to the external positive charge and migrate freely toward that region. This region then...
6.0K
Induced Electric Fields: Applications01:27

Induced Electric Fields: Applications

1.6K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.6K

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Related Experiment Video

Updated: Jun 27, 2025

Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
07:03

Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals

Published on: August 15, 2018

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Electric-field-induced multiferroic topological solitons.

Arthur Chaudron1, Zixin Li2, Aurore Finco3

  • 1Laboratoire Albert Fert, CNRS, Thales, Université Paris-Saclay, Palaiseau, France.

Nature Materials
|May 6, 2024
PubMed
Summary
This summary is machine-generated.

Researchers stabilized unique antiferromagnetic spin textures in multiferroic BiFeO3 thin films using electric fields. This breakthrough enables electrical control over these topological states, paving the way for advanced antiferromagnetic spintronic devices.

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Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
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Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
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Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
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Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Spintronics

Background:

  • Antiferromagnetic skyrmions offer advantages over ferromagnets for solitonic information technologies, including immunity to dipolar fields and ultrafast dynamics.
  • Controlling topological objects in antiferromagnets remains a significant challenge, hindering their technological application.

Purpose of the Study:

  • To investigate the electrical control and stabilization of topological antiferromagnetic states in multiferroic materials.
  • To explore the potential of magnetoelectric multiferroics for writing, detecting, and erasing topological antiferromagnetic entities.

Main Methods:

  • Stabilization of ferroelectric center states using a radial electric field in multiferroic BiFeO3 thin films.
  • Analysis of antiferromagnetic spin cycloid flux closures and distinct core entities under varying electric field polarities.
  • Tuning epitaxial strain to electrically design canted antiferromagnetic domains.

Main Results:

  • Ferroelectric center states were successfully stabilized in BiFeO3 thin films via radial electric fields.
  • Polar textures containing flux closures of antiferromagnetic spin cycloids were observed, with core structures dependent on electric field polarity.
  • Electrically designable canted antiferromagnetic domains were achieved by tuning epitaxial strain.

Conclusions:

  • The study demonstrates the ability to electrically write and manipulate topological antiferromagnetic states in multiferroic BiFeO3.
  • These findings open new avenues for creating reconfigurable topological states in magnetoelectric antiferromagnets for future spintronic applications.