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Related Concept Videos

Motion Of A Charged Particle In A Magnetic Field01:22

Motion Of A Charged Particle In A Magnetic Field

A charged particle experiences a force when moving through a magnetic field. Consider the field to be uniform and the charged particle to move perpendicular to it. If the field is in a vacuum, the magnetic field is the dominant factor determining the motion. Since the magnetic force is perpendicular to the direction of motion, a charged particle follows a curved path. The particle continues to follow this curved path until it forms a complete circle. Another way to look at this is that the...
Magnetic Damping01:17

Magnetic Damping

Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
Torque On A Current Loop In A Magnetic Field01:13

Torque On A Current Loop In A Magnetic Field

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...
Magnetic Field due to Moving Charges01:25

Magnetic Field due to Moving Charges

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...
Potential Due to a Magnetized Object01:24

Potential Due to a Magnetized Object

Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
Magnetic Vector Potential01:15

Magnetic Vector Potential

In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...

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Scanning SQUID Study of Vortex Manipulation by Local Contact
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Dynamics of a pinned magnetic vortex.

R L Compton1, P A Crowell

  • 1School of Physics and Astronomy, University of Minnesota, 116 Church Street SE, Minneapolis, Minnesota 55455, USA.

Physical Review Letters
|October 10, 2006
PubMed
Summary

We studied magnetic vortex dynamics in ferromagnetic films. The vortex core

Area of Science:

  • Condensed matter physics
  • Magnetism and magnetic materials

Background:

  • Magnetic vortices are fundamental spin structures in ferromagnetic materials.
  • Defects in magnetic films can pin magnetic vortices, influencing their dynamics.

Purpose of the Study:

  • To investigate the amplitude-dependent dynamics of a single magnetic vortex pinned by a defect.
  • To understand the transition between low- and high-excitation regimes and the role of depinning.

Main Methods:

  • Experimental observation of magnetic vortex core gyration in a ferromagnetic film.
  • Varying excitation amplitudes to probe different dynamic regimes.
  • Applying static in-plane magnetic fields to map pinning site distributions.

Main Results:

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Scanning SQUID Study of Vortex Manipulation by Local Contact
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  • At low amplitudes, vortex gyration frequency is determined by a single pinning site.
  • At high amplitudes, frequency depends on the magnetostatic energy of the confined vortex.
  • A sharp transition occurs due to vortex depinning from the defect.

Conclusions:

  • The study reveals distinct dynamic behaviors of a pinned magnetic vortex based on excitation amplitude.
  • Depinning from defects is a critical mechanism governing vortex dynamics.
  • The method allows for characterization of pinning site distributions.