Abstract:The gradient-drift instabilities of partially magnetized plasmas in plasma devices with crossed electric and magnetic fields are investigated in the framework of the two-fluid model with finite electron temperature in an inhomogeneous magnetic field. The finite electron Larmor radius (FLR) effects are also included via the gyroviscosity tensor taking into account the magnetic field gradient. This model correctly describes the electron dynamics for k ? q e > 1 in the sense of Pad e approximants (here, k ? and q… Show more
“…A very complete overview of the theory of instabilities in partially magnetized plasmas of E B discharges that includes the effects of density gradients, magnetic field gradients, electron gyroviscosity and collisions has been recently given by A. Smolyakov and his colleagues 9,10,20,24,48 .…”
Section: Dispersion Relation In the Near-anode Regionmentioning
confidence: 99%
“…(19) of Ref. 10 ) to properly describe the ion acoustic wave, and the wavelength of the instability at the maximum growth rate should depend on the Debye length for lower values of the plasma density.…”
Section: Dispersion Relation In the Near-anode Regionmentioning
confidence: 99%
“…The results presented here give a useful estimate of the average magnetic field (more precisely root mean square magnetic field) in the near-anode region below which electron transport can be considered as classical and above which azimuthal instabilities leading to anomalous transport are likely to develop. The effect of the magnetic field gradient present in the near-anode region of Hall thrusters will be explored in a future work and the results from PIC simulations will be compared with the predictions from the theory 9,10,20,48 .…”
Section: A Assumptions and Relevance To The Near-anode Region Of Magmentioning
confidence: 99%
“…The design of Hall thrusters or magnetrons is such that the E B and P B electron drift currents are in the azimuthal direction of a cylindrical geometry (these plasma devices are sometimes called "closed drift" devices 6 ). Since ions are essentially not magnetized, the azimuthal velocity of electrons is much larger than that of ions, and this difference in velocity can generate charge separation and trigger numerous types of instabilities [7][8][9][10] .…”
Section: Introductionmentioning
confidence: 99%
“…In this first approach we consider the simplifying assumption of a constant magnetic field in the near-anode region. Magnetic field gradients can modify the development of these instabilities 10,20,[46][47][48][49] and we leave the study of their effect for future work.…”
Electron and ion transport in the near-anode region of a partially magnetized plasma under conditions typical of Hall thrusters or magnetron discharges is studied with fully kinetic, Particle-In-Cell Monte Carlo Collision (PIC-MCC) simulations assuming a uniform magnetic field and no ionization. We derive a simple relation that defines the magnetic field at the transition point between negative and positive sheath. For magnetic fields around or above this transition point, PIC-MCC simulations show the development of short wavelength azimuthal instabilities that cascade to longer wavelengths ("rotating spokes") as the magnetic field is increased. Both short-wavelength and large-wavelength fluctuations can coexist under some conditions. A detailed study of the fluid dispersion relation is used to analyze the PIC-MCC results. Small coherent structures can be associated with the destabilization of ion sound waves by density gradient and collisions. Longer wavelengths or rotating spokes are characteristic of the collisionless Simon-Hoh instability. The small structures are dominant for larger plasma density gradients while the larger structures correspond to smaller density gradients and larger magnetic fields. Anomalous transport associated with these instabilities can be significant, with effective collision frequencies larger than 2 × 10 7 s −1 in xenon for magnetic fields above the transition point.
“…A very complete overview of the theory of instabilities in partially magnetized plasmas of E B discharges that includes the effects of density gradients, magnetic field gradients, electron gyroviscosity and collisions has been recently given by A. Smolyakov and his colleagues 9,10,20,24,48 .…”
Section: Dispersion Relation In the Near-anode Regionmentioning
confidence: 99%
“…(19) of Ref. 10 ) to properly describe the ion acoustic wave, and the wavelength of the instability at the maximum growth rate should depend on the Debye length for lower values of the plasma density.…”
Section: Dispersion Relation In the Near-anode Regionmentioning
confidence: 99%
“…The results presented here give a useful estimate of the average magnetic field (more precisely root mean square magnetic field) in the near-anode region below which electron transport can be considered as classical and above which azimuthal instabilities leading to anomalous transport are likely to develop. The effect of the magnetic field gradient present in the near-anode region of Hall thrusters will be explored in a future work and the results from PIC simulations will be compared with the predictions from the theory 9,10,20,48 .…”
Section: A Assumptions and Relevance To The Near-anode Region Of Magmentioning
confidence: 99%
“…The design of Hall thrusters or magnetrons is such that the E B and P B electron drift currents are in the azimuthal direction of a cylindrical geometry (these plasma devices are sometimes called "closed drift" devices 6 ). Since ions are essentially not magnetized, the azimuthal velocity of electrons is much larger than that of ions, and this difference in velocity can generate charge separation and trigger numerous types of instabilities [7][8][9][10] .…”
Section: Introductionmentioning
confidence: 99%
“…In this first approach we consider the simplifying assumption of a constant magnetic field in the near-anode region. Magnetic field gradients can modify the development of these instabilities 10,20,[46][47][48][49] and we leave the study of their effect for future work.…”
Electron and ion transport in the near-anode region of a partially magnetized plasma under conditions typical of Hall thrusters or magnetron discharges is studied with fully kinetic, Particle-In-Cell Monte Carlo Collision (PIC-MCC) simulations assuming a uniform magnetic field and no ionization. We derive a simple relation that defines the magnetic field at the transition point between negative and positive sheath. For magnetic fields around or above this transition point, PIC-MCC simulations show the development of short wavelength azimuthal instabilities that cascade to longer wavelengths ("rotating spokes") as the magnetic field is increased. Both short-wavelength and large-wavelength fluctuations can coexist under some conditions. A detailed study of the fluid dispersion relation is used to analyze the PIC-MCC results. Small coherent structures can be associated with the destabilization of ion sound waves by density gradient and collisions. Longer wavelengths or rotating spokes are characteristic of the collisionless Simon-Hoh instability. The small structures are dominant for larger plasma density gradients while the larger structures correspond to smaller density gradients and larger magnetic fields. Anomalous transport associated with these instabilities can be significant, with effective collision frequencies larger than 2 × 10 7 s −1 in xenon for magnetic fields above the transition point.
The detailed analysis of stability of azimuthal oscillations in partially magnetized plasmas with crossed electric and magnetic fields is presented. The instabilities are driven by the transverse electron current which, in general, is due to a combination of E Â B and electron diamagnetic drifts. Marginal stability boundary is determined for a wide range of the equilibrium plasma parameters. It is shown that in some regimes near the instability threshold, only the low-frequency long-wavelength oscillations are unstable, while the short-wavelength high-frequency modes are stabilized by the finite Larmor radius effects. Without such stabilization, the high-frequency modes have much larger growth rates and dominate. A new regime of the instability driven exclusively by the magnetic field gradient is identified. Such instability takes place in the region of the weak electric field and for relatively large gradients of plasma density (q s =l n > 1, where q s is the ion-sound Larmor radius and l n is the scale length of plasma density inhomogeneity).
It is shown that the transport in low temperature, collisional, bounded plasma is enhanced by instabilities at high magnetic field. While the magnetic field confines the electrons in a stable plasma, the instability completely destroys the confinement such that the transport becomes independent of the magnetic field in the highly magnetized limit. An analytical expression of the instability-enhanced collision frequency is proposed, based on a magnetic field independent edge-to-center density ratio.
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