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Magnetic field deformation due to electron drift in a Hall thruster
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The strength and shape of the magnetic field are the core factors in the design of the Hall thruster. However, Hall current can affect the distribution of static magnetic field. In this paper, the Particle-In-Cell (PIC) method is used to obtain the distribution of Hall current in the discharge channel. The Hall current is separated into a direct and an alternating part to calculate the induced magnetic field using Finite Element Method Magnetics (FEMM). The results show that the direct Hall current decreases the magnetic field strength in the acceleration region and also changes the shape of the magnetic field. The maximum reduction in radial magnetic field strength in the exit plane is 10.8 G for an anode flow rate of 15 mg/s and the maximum angle change of the magnetic field line is close to 3° in the acceleration region. The alternating Hall current induces an oscillating magnetic field in the whole discharge channel. The actual magnetic deformation is shown to contain these two parts.
Title: Magnetic field deformation due to electron drift in a Hall thruster
Description:
The strength and shape of the magnetic field are the core factors in the design of the Hall thruster.
However, Hall current can affect the distribution of static magnetic field.
In this paper, the Particle-In-Cell (PIC) method is used to obtain the distribution of Hall current in the discharge channel.
The Hall current is separated into a direct and an alternating part to calculate the induced magnetic field using Finite Element Method Magnetics (FEMM).
The results show that the direct Hall current decreases the magnetic field strength in the acceleration region and also changes the shape of the magnetic field.
The maximum reduction in radial magnetic field strength in the exit plane is 10.
8 G for an anode flow rate of 15 mg/s and the maximum angle change of the magnetic field line is close to 3° in the acceleration region.
The alternating Hall current induces an oscillating magnetic field in the whole discharge channel.
The actual magnetic deformation is shown to contain these two parts.
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