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Related Concept Videos

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...
Maxwell-Boltzmann Distribution: Problem Solving01:20

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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
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Maxwell's Equation Of Electromagnetism01:29

Maxwell's Equation Of Electromagnetism

James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to understanding the nature of Saturn's rings. He is probably best known for having combined existing knowledge on the laws of electricity and magnetism with his insights into a complete overarching electromagnetic theory, which is represented by...
Plane Electromagnetic Waves I01:30

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The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
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Related Experiment Video

Updated: May 27, 2026

Building Langmuir Probes and Emissive Probes for Plasma Potential Measurements in Low Pressure, Low Temperature Plasmas
08:10

Building Langmuir Probes and Emissive Probes for Plasma Potential Measurements in Low Pressure, Low Temperature Plasmas

Published on: May 25, 2021

Rarefaction shock in plasma with a bi-Maxwellian electron distribution function.

A Diaw1, P Mora

  • 1Centre de Physique Théorique, École Polytechnique, CNRS, FR-91128 Palaiseau, France.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|November 9, 2011
PubMed
Summary

A rarefaction shock forms in plasma expansion when hot and cold electron temperatures differ significantly. This shock influences ion acceleration, with theoretical models showing excellent agreement with numerical simulations.

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Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

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Last Updated: May 27, 2026

Building Langmuir Probes and Emissive Probes for Plasma Potential Measurements in Low Pressure, Low Temperature Plasmas
08:10

Building Langmuir Probes and Emissive Probes for Plasma Potential Measurements in Low Pressure, Low Temperature Plasmas

Published on: May 25, 2021

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

Area of Science:

  • Plasma Physics
  • Astrophysics
  • Computational Physics

Background:

  • Collisionless plasma expansion into a vacuum is fundamental to space and laboratory plasmas.
  • Bi-Maxwellian electron distributions can lead to complex plasma behaviors, including shock formation.
  • Previous studies identified conditions for shock waves but lacked a complete theoretical description of rarefaction shocks and their impact on ion acceleration.

Purpose of the Study:

  • To theoretically and numerically investigate the one-dimensional collisionless expansion of plasma with bi-Maxwellian electrons into a vacuum.
  • To develop a comprehensive model for rarefaction shocks and their effect on ion acceleration.
  • To validate the theoretical model against numerical simulations.

Main Methods:

  • Theoretical modeling of plasma expansion with a bi-Maxwellian electron distribution.
  • Derivation of analytical expressions for rarefaction shock characteristics.
  • Numerical simulations using a hybrid code to model plasma expansion.

Main Results:

  • A shock wave is predicted when the hot to cold electron temperature ratio exceeds 5+√24.
  • The theoretical model provides a complete description of the rarefaction shock and its influence on ion acceleration.
  • Excellent agreement was found between analytical predictions and hybrid code simulation results.

Conclusions:

  • The study successfully models rarefaction shocks in bi-Maxwellian plasmas.
  • The findings clarify the role of electron temperature anisotropy in plasma expansion dynamics.
  • The validated theoretical framework can be applied to understand ion acceleration in similar plasma environments.