2012
DOI: 10.1063/1.4737114
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Global model of a gridded-ion thruster powered by a radiofrequency inductive coil

Abstract: International audienceA global (volume-averaged) model of a gridded-ion thruster is proposed. The neutral propellant (xenon gas) is injected into the thruster chamber at a fixed rate and a plasma is generated by circulating a radiofrequency current in an inductive coil. The ions generated in this plasma are accelerated out of the thruster by a pair of DC biased grids. The neutralization downstream is not treated. Xenon atoms also flow out of the thruster across the grids. The model, based on particle and energ… Show more

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Cited by 67 publications
(62 citation statements)
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“…27,28 The model we present explains recent thruster performance levels and offers a theoretical guide to achieving improved performance to make these systems competitive with the more well-established gridded ion engines and Hall-effect thrusters.…”
Section: Introductionmentioning
confidence: 98%
“…27,28 The model we present explains recent thruster performance levels and offers a theoretical guide to achieving improved performance to make these systems competitive with the more well-established gridded ion engines and Hall-effect thrusters.…”
Section: Introductionmentioning
confidence: 98%
“…Such a coupling is representative of real-life conditions observed while testing RF thrusters. The developed model is in contrast to the other RF thruster models (developed for example by Volkmar [13,30], Chabert [12] or Gartner [14]) that only looked at a specific aspect of the RF thruster operation, concentrating on either predicting the thruster's performance or the temperature distribution but not both in a coupled fashion. It was observed that if the coupling between the thruster's temperatures and performance is not consistent, an error of up to about 10% in the RFG input power can be incurred at high mass utilization efficiencies.…”
Section: Resultsmentioning
confidence: 99%
“…Nevertheless, he did not look at the electromagnetic aspect of RF thruster operation, which prevented him from calculating the total thruster input power and efficiency. Chabert et al [12] extended Goebel's model and included the electromagnetic part by introducing the aforementioned transformer assumptions. Volkmar et al developed a 3D Biot-Savart solver to calculate the coil impedance and used the magnetic diffusion equation to determine the electromagnetic field distribution inside the plasma represented by the uniform 0D model [13].…”
Section: Introductionmentioning
confidence: 99%
“…This is regarded as crucial since most numerical models of RF ion thrusters use 2D rotational symmetric methods-or even 1D and 0D methods-which cannot predict the axially induced field components caused by the pitch of the coil. [13][14][15][16] ..The discrete form of the Laplacian operator in Cartesian coordinates can be derived by a Taylor expansion and subsequent dropping of the discretization error, as shown in 17):…”
Section: )mentioning
confidence: 99%