2020
DOI: 10.1109/tps.2020.2982541
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Numerical Model of a Helicon Plasma Thruster

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Cited by 27 publications
(26 citation statements)
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“…The main characteristics of a cathode-less plasma thruster are: (i) a very simple architecture, which helps keeping at bay the cost of these systems; (ii) no electrodes in contact with the plasma neither for generation nor acceleration; (iii) possibility of operating the thruster with different propellants without a drastic redesign; (iv) absence of a neutralizer provided that the ejected plasma is currentfree and quasi-neutral. The main components of a cathodeless plasma thruster are: (i) a dielectric tube inside which the neutral gas propellant is ionized; (ii) a Radio Frequency (RF) antenna working in the MHz range that provides the power to produce and to heat up the plasma [26], (iii) permanent magnets that generate the magneto-static field required to enhance the plasma confinement [27,28] and to improve the thrust via the magnetic nozzle effect [29][30][31].…”
Section: Magnetically Enhanced Plasma Thrustermentioning
confidence: 99%
See 1 more Smart Citation
“…The main characteristics of a cathode-less plasma thruster are: (i) a very simple architecture, which helps keeping at bay the cost of these systems; (ii) no electrodes in contact with the plasma neither for generation nor acceleration; (iii) possibility of operating the thruster with different propellants without a drastic redesign; (iv) absence of a neutralizer provided that the ejected plasma is currentfree and quasi-neutral. The main components of a cathodeless plasma thruster are: (i) a dielectric tube inside which the neutral gas propellant is ionized; (ii) a Radio Frequency (RF) antenna working in the MHz range that provides the power to produce and to heat up the plasma [26], (iii) permanent magnets that generate the magneto-static field required to enhance the plasma confinement [27,28] and to improve the thrust via the magnetic nozzle effect [29][30][31].…”
Section: Magnetically Enhanced Plasma Thrustermentioning
confidence: 99%
“…9. The following properties are assumed [30] • Ion temperature T i = 0.3 eV, electron temperature T e = 3 eV • Ions and electrons injection flux Γ = 5 × 10 20 m −2 s −1 • Ions speed V 0 = 1370 m/s…”
Section: Plume Analysismentioning
confidence: 99%
“…
Figure 1.Schematic of a MEPT that highlights the separation between production stage and acceleration stage (Magarotto et al. 2020 a ). Note that only the acceleration stage is simulated in this study.
…”
Section: Introductionmentioning
confidence: 99%
“…The y-component of the drift, instead, is zeroed at each cycle due to the linear polarization of the EM fields produced by the birdcage antenna. In the exhaust region, the applied magnetic field B 0 is diverging, therefore partial thrust will also be provided by an EM nozzle effect, this can be investigated by numerical methods such as [49][50][51], however this is out of scope within this paper.…”
Section: Theoretical Description Of the Birdcage Antennamentioning
confidence: 99%