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Related Concept Videos

Torque On A Current Loop In A Magnetic Field01:13

Torque On A Current Loop In A Magnetic Field

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The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
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Magnetic Field due to Moving Charges01:23

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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...
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Force On A Current Loop In A Magnetic Field01:17

Force On A Current Loop In A Magnetic Field

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Magnetic forces on wires carrying current are most frequently applied in motors. A DC motor is a device that converts electrical energy into mechanical work. In motors, wire loops are enclosed in a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate. The direction of the current is reversed once the loop's surface area is lined up with the magnetic field, causing a constant torque on the loop. During the process, commutators...
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Magnetic Force Between Two Parallel Currents01:13

Magnetic Force Between Two Parallel Currents

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Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
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Magnetic Force On A Current-Carrying Conductor01:25

Magnetic Force On A Current-Carrying Conductor

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Moving charges experience a force in a magnetic field. Since the magnetic fields produced by moving charges are proportional to the current, a conductor carrying a current creates a magnetic field around it.
Consider a compass placed near a current-carrying wire. The wire experiences a force that aligns the needle of the compass tangentially around the wire. Thus, the current-carrying wire produces concentric circular loops of magnetic field. The magnetic field generated by a wire can be...
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Magnetic Field Of A Current Loop01:16

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Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
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Related Experiment Video

Updated: Nov 16, 2025

Radio Frequency Magnetron Sputtering of GdBa2Cu3O7âˆ'ÃŽ ´/ La0.67Sr0.33MnO3 Quasi-bilayer Films on SrTiO3 STO Single-crystal Substrates
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Radio Frequency Magnetron Sputtering of GdBa2Cu3O7âˆ'ÃŽ ´/ La0.67Sr0.33MnO3 Quasi-bilayer Films on SrTiO3 STO Single-crystal Substrates

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Current-Induced Spin Torques on Single GdFeCo Magnetic Layers.

David Céspedes-Berrocal1,2, Heloïse Damas1, Sébastien Petit-Watelot1

  • 1Institute Jean Lamour, Université de Lorraine, CNRS, Nancy, F-54000, France.

Advanced Materials (Deerfield Beach, Fla.)
|February 19, 2021
PubMed
Summary

Researchers developed new spintronic materials without heavy metals, utilizing gadolinium iron cobalt (GdFeCo) for strong self-torques and efficient spin current generation. This advances high-performance spintronics.

Keywords:
amorphous ferrimagnetic GdFeCospin-orbit torquespin-orbitronicsspintronics

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Spintronics

Background:

  • Spintronics utilizes spin-orbit coupling (SOC) for spin currents and torques, often relying on 3d metals with small SOC.
  • Conventional spintronics employs 5d heavy metals (e.g., Pt) for enhanced SOC, but this study introduces an alternative.
  • Inversion symmetry breaking is crucial for Rashba and Dzyaloshinskii-Moriya interactions in spintronic devices.

Purpose of the Study:

  • To introduce novel material architectures for high-performance spintronics that exclude nonmagnetic 5d heavy metals.
  • To demonstrate strong current-induced torques ('self-torques') in single ferrimagnetic GdFeCo layers.
  • To investigate the spin current emission properties of GdFeCo layers.

Main Methods:

  • Fabrication of material architectures excluding nonmagnetic 5d heavy metals.
  • Experimental demonstration of current-induced torques on single ferrimagnetic GdFeCo layers.
  • Characterization of spin current generation and spin-orbit coupling effects.
  • Measurements of spin anomalous Hall effect and spin Hall effect symmetries.

Main Results:

  • Demonstrated very strong current-induced 'self-torques' on single GdFeCo layers, attributed to Gd 5d SOC and interface-engineered inversion symmetry breaking.
  • Observed enhancement of these self-torques around the magnetization compensation temperature.
  • Determined very large spin current emission from GdFeCo, with 80% (20%) spin anomalous Hall effect (spin Hall effect) symmetry.

Conclusions:

  • A new material platform for spintronics is presented, enabling 'self-torques' on single magnetic layers without heavy metals.
  • This platform facilitates efficient spin current generation directly from magnetic layers.
  • The findings open new avenues for advanced spintronic device designs and functionalities.