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Hall Thrusters 377 ni = nino ive nivi , t L and the neutral particle conservation equation as no= nino ive +novo, (7.4-29) (7.4-30) t L where vo is the neutral velocity and L is the axial length of the ionization zone. The perturbed behavior of the ion and neutral densities with time is linearized such that n=n + n i i,o i n =n + n , o o,o o (7.4-31) where the first term on the right-hand side denotes the unperturbed state. Combining Eqs. (7.4-29), (7.4-30), and (7.4-31) gives 2n 2 i=n n n v . (7.4-32) i,o o,o i i e This equation represents an undamped harmonic oscillator with a frequency t2 f=1 nn v2 vivo. (7.4-33) given by The low-frequency oscillatory behavior of Hall thrusters is related to the velocities of the ions and neutrals relative to the scale length of the ionization zone. This indicates that periodic depletion of the neutral gas in the ionization region causes the ion density to oscillate, which impacts the electron conductivity through the transverse magnetic field and thereby the discharge current. The ionization region location can then oscillate axially in the channel on the time scale of neutral replenishment time. The models show [53] that the oscillation depends strongly on the magnetic field strength near the channel exit, and that optimum operation of the thruster generally corresponds to high mass utilization regimes where this instability occurs. These types of oscillations, which are typically observed in the discharge current when the thrusters are operated in a voltage-regulated mode, have been called “breathing modes” [53] and “predator–prey modes” [30], and an example is shown in Fig. 7-18 for the SPT-100 Hall thruster [55]. The frequency in this experimentally observed example is about 17 kHz. However, the frequency depends on the thruster operating conditions and can range from 10 to 30 kHz for different flow rates, voltages, and magnetic fields. The 1-D numerical code i 2 i,o o,o i e 2 LPDF Image | Fundamentals of Electric Propulsion: Ion and Hall Thrusters
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