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Related Concept Videos

Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
Shock Waves01:16

Shock Waves

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high pressures...
Magnetic Field due to Moving Charges01:23

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...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
Magnetic Field Lines01:19

Magnetic Field Lines

The representation of magnetic fields by magnetic field lines is very useful in visualizing the strength and direction of the magnetic field. Each of the magnetic field lines forms a closed loop. The field lines emerge from the north pole (N), loop around to the south pole (S), and continue through the bar magnet back to the north pole.
Magnetic field lines follow several hard-and-fast rules:
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:

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Updated: May 8, 2026

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

Dislocations in magnetohydrodynamic waves in a stellar atmosphere.

A López Ariste1, M Collados, E Khomenko

  • 1THEMIS-CNRS UPS, 853, C/ Vía Láctea s/n, 38200 La Laguna, Spain.

Physical Review Letters
|September 10, 2013
PubMed
Summary

Wave front dislocations in magnetohydrodynamic waves were detected in solar sunspots. This study provides the first estimates of modal contributions in waves propagating along magnetic fields in these sunspots.

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Area of Science:

  • Plasma physics
  • Solar physics
  • Astrophysics

Background:

  • Magnetohydrodynamic (MHD) waves are crucial for energy transport in stellar atmospheres.
  • Understanding wave behavior in stratified environments like the solar chromosphere is essential.
  • Dislocations in wave fronts can significantly alter wave propagation and energy transfer.

Purpose of the Study:

  • To describe and detect wave front dislocations in MHD waves within stratified stellar atmospheres.
  • To investigate the presence of scalar dislocations (edges and vortices) in Alfvén and magnetoacoustic waves.
  • To estimate the modal contribution of waves propagating along magnetic fields in solar sunspots.

Main Methods:

  • Analysis of MHD wave observations in sunspots within the solar chromosphere.
  • Identification and characterization of scalar wave front dislocations (edges and vortices).
  • Measurement of the 'charge' of observed dislocations to infer modal contributions.

Main Results:

  • Wave front dislocations, including edges and vortices, were identified in MHD waves in solar sunspots.
  • The presence of these dislocations was confirmed in both Alfvén and general magnetoacoustic waves.
  • The measured charge of dislocations allowed for the first-time estimation of modal contributions in waves along magnetic fields.

Conclusions:

  • Wave front dislocations are a significant feature of MHD waves in stratified stellar atmospheres, specifically observed in solar sunspots.
  • The detection and analysis of these dislocations provide new insights into wave propagation and energy transfer mechanisms in solar magnetic fields.
  • This research offers a novel method for estimating modal contributions in MHD waves, advancing our understanding of solar plasma dynamics.