Bulletin of the American Physical Society
74th Annual Gaseous Electronics Conference
Volume 66, Number 7
Monday–Friday, October 4–8, 2021;
Virtual: GEC Platform
Time Zone: Central Daylight Time, USA
Session TF13: Electric Propulsion
8:00 AM–10:00 AM,
Friday, October 8, 2021
Virtual
Room: GEC platform
Chair: Gabe Xu, University of Alabama in Huntsville
Abstract: TF13.00004 : Investigation of Hall effect thruster instabilities with axial-azimuthal PIC simulation using a collective Thomson scattering approach
9:00 AM–9:15 AM
Presenter:
Tarek Ben Slimane
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Authors:
Tarek Ben Slimane
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Cyrille Honoré
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Thomas Charoy
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Alejandro Alvarez Laguna
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Anne Bourdon
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, 91120 Palaiseau, France)
Pascal Chabert
(Ecole Polytechnique)
This work tries to benefit from the wave vector selectivity of the CTS and the resolution of the PIC results to investigate these fluctuations. This is achieved by analyzing the signal that a CTS virtual diagnostic observes from PIC. The PIC data are from a simplified benchmark by T.Charoy et al., where both the radial magnetic field and the ionization profile are fixed so that to remove the breathing mode oscillation. The collective scattering signal is calculated from the electron density maps using the expression of the scattered field.
An analysis along the channel axis highlights changes in the direction and intensity of the propagating modes between the ionization and the acceleration zones. An azimuthal dominant mode at k = 3 rad.mm-1 is enhanced throughout the channel while modes at larger k are damped. The dispersion relations are also computed as well as the fluctuation rate.
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