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Fundamentals of Electric Propulsion: Ion and Hall Thrusters

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Fundamentals of Electric Propulsion: Ion and Hall Thrusters ( fundamentals-electric-propulsion-ion-and-hall-thrusters )

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Ion Thruster Plasma Generators 93 RF and microwave ion thrusters utilize ion accelerator and electron-neutralizer implementations nearly identical to that of the DC-discharge ion thruster. However, these thrusters do not employ a discharge hollow cathode or anode power supply. These components are replaced by rf or microwave antenna structures, sources of microwave radiation and compatible discharge chambers to ionize the propellant gas and deliver the ions to the accelerator structure. These thrusters also utilize either applied or self-generated magnetic fields to improve the ionization efficiency of the system. The three thruster plasma generators to be discussed here, DC electron discharge, rf, and microwave discharge, have been successfully developed and flown in space. The principles of these different classes of plasma generators are described in the following sections after a discussion of the plasma generator efficiency that can be expected in an idealized case. 4.2 Idealized Ion Thruster Plasma Generator It is worthwhile to examine an ion thruster in the simplest terms to provide an understanding of the dominant processes in the particle flows and energy transport required to produce the plasma. The idealized thruster model has power injected by arbitrary means into a volume filled with neutral gas to produce ionization and neutral gas excitation, with all the ions going to the accelerator grids and an equal number of plasma electrons going to the wall to conserve charge. This is illustrated schematically in Fig. 4-3. For this model, the thruster discharge chamber has a volume V that fully encloses the plasma that is produced by ionization of neutral gas by the plasma electrons. The ions from the plasma flow only to the accelerator grid structure (perfect confinement elsewhere in the discharge chamber) with a current given by the Bohm current: Xeo Fig. 4-3. Idealized ion thruster with the ions assumed going to the grids and electrons going to the chamber wall. Chamber Wall e− Xe+ Accelerator Grids

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