MOVEMENT OF A RELATIVISTIC ELECTRON IN CROSSED ELECTRIC AND MAGNETIC FIELDS

Doklady BGUIR ◽

10.35596/1729-7648-2019-124-6-26-30 ◽

2019 ◽

pp. 26-30

Author(s):

A. A. Kurayev ◽

V. V. Matveyenka

Keyword(s):

Magnetic Fields ◽

Coordinate System ◽

Relativistic Electron ◽

Rotation Frequency ◽

Modern Literature ◽

Relativistic Velocity ◽

Electron Motion ◽

Relativistic Case ◽

Electric And Magnetic Fields

It is shown that the ideas about the electron motion into electric and magnetic crossed fields existing in the modern literature are incorrected. For relativistic velocity case the electron motion can't be imagined by the superposition of the drift with velocity u = E0/B0 and the rotation with frequency  = eB0/m (e, m is charge and mass of relativistic electron). In the relativistic case these motions are not separated, moreover the instantaneous rotation frequency  of relativistic electron is unstable for fixed coordinate system (E0, B0):  depends on m, which varies considerably during rotation.

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Relativistic electron motion in a resonant cavity with time varying and inhomogeneous magnetic fields

Journal of Electromagnetic Waves and Applications ◽

10.1163/156939394x00849 ◽

1994 ◽

Vol 8 (1) ◽

pp. 129-143 ◽

Cited By ~ 3

Author(s):

L.M. Zurk ◽

P.E. Serafim

Keyword(s):

Magnetic Fields ◽

Relativistic Electron ◽

Resonant Cavity ◽

Time Varying ◽

Electron Motion

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Width dependent collisionless electron dynamics in the static fields of the shock ramp, 1, Single particle behavior and implications for downstream distribution

Nonlinear Processes in Geophysics ◽

10.5194/npg-4-167-1997 ◽

1997 ◽

Vol 4 (3) ◽

pp. 167-172 ◽

Cited By ~ 2

Author(s):

M. Gedalin ◽

M. A. Balikhin

Keyword(s):

Magnetic Fields ◽

Electron Temperature ◽

Single Particle ◽

Electron Distribution ◽

Trajectory Analysis ◽

Electron Motion ◽

Electron Dynamics ◽

Electron Trajectories ◽

Electric And Magnetic Fields ◽

Downstream Distribution

Abstract. We study the collisionless dynamics of electrons in the shock ramp using the numerical trajectory analysis in the model electric and magnetic fields of the shock. Even with very modest assumptions about the cross-shock potential the electron trajectories are very sensitive to the width of the ramp. The character of electron motion changes from the fully adiabatic (with conservation of v2<perp> /B) when the ramp is wide, to the nonadiabatic one, when the ramp becomes sufficiently narrow. The downstream electron distribution also changes drastically, although this change depends on the initial electron temperature.

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Simulation of electron motion in electric and magnetic fields by java programming

2014 International Conference on Computer Technologies in Physical and Engineering Applications (ICCTPEA) ◽

10.1109/icctpea.2014.6893330 ◽

2014 ◽

Author(s):

Suhua Qian ◽

Hongji Du ◽

Masami Morooka

Keyword(s):

Magnetic Fields ◽

Electron Motion ◽

Java Programming ◽

Electric And Magnetic Fields

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Velocity Distribution Functions and Transport Coefficients of Electron Swarms in Gases in the Presence of Crossed Electric and Magnetic Fields

Australian Journal of Physics ◽

10.1071/ph950557 ◽

1995 ◽

Vol 48 (3) ◽

pp. 557 ◽

Cited By ~ 12

Author(s):

KF Ness

Keyword(s):

Distribution Function ◽

Magnetic Fields ◽

Velocity Distribution ◽

Transport Coefficients ◽

Velocity Distribution Function ◽

Distribution Functions ◽

Electron Motion ◽

Electric And Magnetic Fields ◽

Velocity Distribution Functions ◽

Spatially Homogeneous

A multi-term solution of the Boltzmann equation is used to calculate the spatially homogeneous velocity distribution function of a dilute swarm of electrons moving through a background of denser neutral molecules in the presence of crossed electric and magnetic fields. As an example, electron motion in methane is considered.

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