2019
DOI: 10.1088/1361-6463/ab197e
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Modeling on plasma energy balance and transfer in a hollow cathode

Abstract: Nomenclature D = 1.2 × 10 6 A (m 2 • K 2 ) −1 , constant defined by material e = 1.602 × 10 −19 C, elementary charge E = Electric field E e = Electron kinetic energy E i = Ion kinetic energy E wall = Electric field at the emitter surface j = Current density j e = Electron current density j i = Ion current density I d = Discharge current I e = Electron current I i = Ion current k = 1.38 × 10 -23 J K −1 , Boltzmann constant m = Particle mass

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Cited by 16 publications
(14 citation statements)
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“…Discharge completion occurs in around 10 µs. Therefore, the transient plume generated by PPTs will exhibit different plasma propagation mechanisms when compared with the plume of stationary thrusters (such as ion and Hall thrusters) [30,31].…”
Section: Vacuum System and Pulsed Plasma Thrustermentioning
confidence: 99%
“…Discharge completion occurs in around 10 µs. Therefore, the transient plume generated by PPTs will exhibit different plasma propagation mechanisms when compared with the plume of stationary thrusters (such as ion and Hall thrusters) [30,31].…”
Section: Vacuum System and Pulsed Plasma Thrustermentioning
confidence: 99%
“…Again, using the NSTAR cathode conditions, b = 0.5. Electric field work consists of two terms, namely, the ohmic heating and the electron pressure-gradient work [36]. The 0-D approach does not consider the spatial distribution of the electron's temperature, which means the electric field work actually equals the ohmic heating.…”
Section: Steady-state Modelmentioning
confidence: 99%
“…The energy brought in by ions from the orifice region, P ds , is much smaller than the other terms according to [36] and therefore can be neglected. The component power balance terms are expressed as follows:…”
Section: Steady-state Modelmentioning
confidence: 99%
“…Two-dimensional models, both fluid [2], [3], [4], [5], particle in cell (PIC) [6] and Hybrid-PIC [7], have been proven to be essential in understanding the physics of hollow cathodes, and in particular the developing and dynamics of the external plume region. By solving the unsteady fluid equations along the axial and radial directions, these models are capable of investigating the plasma instabilities established in the plume region.…”
Section: Introductionmentioning
confidence: 99%