Radio-frequency ion thruster with magnetic shielding of the discharge chamber walls

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We presented the results of a computational study on optimizing the shape of the main elements of a radio-frequency ion thruster – the discharge chamber and the ion-extraction system grids. The possibility of improving the integral characteristics of thrusters and ion sources due to the use of an additional magnetostatic field in the RF discharge region was considered. The performed series of calculations made it possible to determine the optimal geometry of the discharge chamber and of the RIT ion-extraction system grids, as well as the configuration of the additional magnetic field, at which the best values of the integral characteristics were achieved.

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Sobre autores

V. Abgaryan

Moscow Aviation Institute (National Research University)

Email: melnikov.andrey.sp@yandex.ru

Research Institute of Applied Mechanics and Electrodynamics

Rússia, Moscow, 125080

D. Demchenko

Moscow Aviation Institute (National Research University)

Email: melnikov.andrey.sp@yandex.ru

Research Institute of Applied Mechanics and Electrodynamics

Rússia, Moscow, 125080

A. Melnikov

Moscow Aviation Institute (National Research University)

Autor responsável pela correspondência
Email: melnikov.andrey.sp@yandex.ru

Научно-исследовательский институт прикладной механики и электродинамики

Rússia, Moscow, 125080

O. Peisakhovich

Moscow Aviation Institute (National Research University)

Email: melnikov.andrey.sp@yandex.ru

Research Institute of Applied Mechanics and Electrodynamics

Rússia, Moscow, 125080

Bibliografia

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2. Fig. 1. Simplified design diagram of the initial configuration of the high-frequency ion engine

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3. Fig. 2. Dependences of the working fluid utilization coefficient (a), ionization price (b) and the increase in “effective thrust” (c) on the relative height of the discharge chamber

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4. Fig. 3. Dependences of the working fluid utilization coefficient (a), ionization price (b) and the increase in “effective thrust” (c) on the relative deflection of the electrodes

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5. Fig. 4. Two-dimensional distributions of the concentration of charged particles

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6. Fig. 5. Distribution of induction of additional constant magnetic field with the winding of the first configuration (current in the winding 5.5 A)

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7. Fig. 6. Dependence of the increase in “effective thrust” on the average induction of the additional constant magnetic field

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8. Fig. 7. Two-dimensional distributions of the concentration of charged particles

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