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Related Concept Videos

π Electron Effects on Chemical Shift: Overview01:27

π Electron Effects on Chemical Shift: Overview

An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0, resulting in...
Charging Conductors By Induction01:15

Charging Conductors By Induction

The Earth is a good conductor of electricity, and it is so big that it can be considered an infinite source or sink of charges. It can easily exchange charges with any matter.
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Induced Electric Dipoles01:29

Induced Electric Dipoles

A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
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Induced Electric Fields: Applications01:27

Induced Electric Fields: Applications

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...
Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle01:19

Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle

Inductively coupled plasma (ICP) is the most widely used plasma source in atomic emission spectroscopy (AES), also known as Inductively Coupled Plasma Optical Emission Spectroscopy (ICP-OES). The ICP source, or torch, consists of three concentric quartz tubes with argon gas flowing through them. A spark from a Tesla coil initiates the ionization of argon, generating a high-temperature plasma.
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Atomic Emission Spectroscopy: Lab

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Electrochemical Etching and Characterization of Sharp Field Emission Points for Electron Impact Ionization
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Nonlocal electron kinetics in a planar inductive helium discharge

Seo1, Chung, Hong

  • 1Department of Physics, Korea Advanced Institute of Science and Technology, Taejon 305-701, South Korea.

Physical Review. E, Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics
|December 2, 2000
PubMed
Summary

Measurements in helium plasma revealed a bi-Maxwellian electron energy distribution function (EEDF) at low pressures. This indicates distinct electron groups, influenced by plasma conditions and electron interactions.

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Last Updated: Jul 25, 2026

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Area of Science:

  • Plasma Physics
  • Atomic and Molecular Physics

Background:

  • Understanding electron behavior in plasmas is crucial for various applications.
  • The electron energy distribution function (EEDF) dictates plasma properties.
  • Helium, a non-Ramsauer gas, is used in this planar inductive plasma study.

Purpose of the Study:

  • To measure the EEDF in a helium planar inductive plasma.
  • To investigate factors influencing EEDF formation, particularly at low pressures.
  • To calculate the electron energy diffusion coefficient using simulations.

Main Methods:

  • Electron energy distribution function (EEDF) measurement using the ac superposition method.
  • Helium pressure range: 10-100 mTorr.
  • Two-dimensional simulation to calculate the electron energy diffusion coefficient.

Main Results:

  • A bi-Maxwellian EEDF was observed at low helium pressures (< 20 mTorr).
  • This bi-Maxwellian distribution features a distinct low-energy electron group.
  • Factors contributing to the bi-Maxwellian EEDF include capacitive field effects, ambipolar potential, and low electron-electron collision frequency.

Conclusions:

  • The bi-Maxwellian EEDF in helium plasma is influenced by electron cooling, heating rates, and confinement.
  • Electron-electron collision frequency, estimated via total electron bounce frequency, plays a key role.
  • The findings provide insights into electron dynamics in low-pressure inductive plasmas.