2013
DOI: 10.1063/1.4817743
|View full text |Cite
|
Sign up to set email alerts
|

Hall thruster plasma fluctuations identified as the E×B electron drift instability: Modeling and fitting on experimental data

Abstract: Microturbulence has been implicated in anomalous transport at the exit of the Hall thruster, and recent simulations have shown the presence of an azimuthal wave which is believed to contribute to the electron axial mobility. In this paper, the 3D dispersion relation of this E Â B electron drift instability is numerically solved. The mode is found to resemble an ion acoustic mode for low values of the magnetic field, as long as a non-vanishing component of the wave vector along the magnetic field is considered,… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

4
101
0

Year Published

2014
2014
2023
2023

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 110 publications
(105 citation statements)
references
References 19 publications
4
101
0
Order By: Relevance
“…Since one of the purposes of this paper is to illustrate how PIC MCC simulation can help identify and understand instabilities in E × B devices, we focus below on a particular micro-turbulence in the mm scale that has been predicted by PIC MCC simulations [40][41][42]73], observed by collective scattering experiments [28,42,[82][83][84] and leads to an increase of electron conductivity consistent with the measurements. This instability is termed as "electron-cyclotron drift instability" and results from the resonant coupling between Bernstein electron modes and ion acoustic waves.…”
Section: Wwwfrontiersinorgmentioning
confidence: 93%
“…Since one of the purposes of this paper is to illustrate how PIC MCC simulation can help identify and understand instabilities in E × B devices, we focus below on a particular micro-turbulence in the mm scale that has been predicted by PIC MCC simulations [40][41][42]73], observed by collective scattering experiments [28,42,[82][83][84] and leads to an increase of electron conductivity consistent with the measurements. This instability is termed as "electron-cyclotron drift instability" and results from the resonant coupling between Bernstein electron modes and ion acoustic waves.…”
Section: Wwwfrontiersinorgmentioning
confidence: 93%
“…The general behavior of the growth rate of the instability is shown for several values of the k z parameter in We solve the dispersion relation numerically in Python 27 using the technique described in Ref. 20, where the solution is obtained through fixed point iteration using the relative error as a stopping condition. We use the convergence condition that |1 − ω i+1 /ω i | < 10 −6 for i ≥ 15.…”
Section: Linear Features Of the Electron Cyclotron Drift-instabilitymentioning
confidence: 99%
“…2D axial-azimuthal simulations [14][15][16] , and 2D radialazimuthal simulations [17][18][19] . Many of these works focused on the possibility that ECDI simply becomes the ion sound instability analogous to the case of unmagnetized plasma 13,20 . We have shown in our previous nonlinear simulations that the transition to ion sound (which for the 1D case is only possible due to nonlinear diffusion in the short wavelength regime) does not occur 21 and the instability is driven by the dominant m = 1 cyclotron resonance.…”
Section: Introductionmentioning
confidence: 99%
“…Based on the parameters typical for experiments described in this Letter (electric field magnitude « 1 04 V /m , magnetic field magnitude of 8.8 mT at the measurement position), excited modes in the magnetron plasma are expected at wave number values which correspond to length scales on the order of a millimeter and below. However, the expected cyclotron resonances can be smoothed, result ing in an observed mode dispersion relation which is nondiscrete [9], To rapidly illustrate this, linear kinetic theory results for typical magnetron parameters (given in the figure caption) for an argon plasma are shown in propagation) smoothes the resonances. The resulting dispersion relation is linear and the corresponding mode group velocity is 2.5 km/s.…”
mentioning
confidence: 93%