Evaluation of ion current density distribution on an extraction electrode of a radio frequency ion thruster

2016 ◽  
Vol 26 (1) ◽  
pp. 015004 ◽  
Author(s):  
P Masherov ◽  
V Riaby ◽  
V Abgaryan
2017 ◽  
Vol 927 ◽  
pp. 012014 ◽  
Author(s):  
V V Denisov ◽  
S S Kovalsky ◽  
N N Koval ◽  
I V Lopatin ◽  
E V Ostroverkhov ◽  
...  

1974 ◽  
Vol 52 (12) ◽  
pp. 1057-1062 ◽  
Author(s):  
C. S. MacLatchy ◽  
P. C. Budgel ◽  
J. R. Miner

The positive ion current density on the surface of a spherical probe immersed in a flowing flame plasma has been measured under thin sheath conditions. The hydrodynamic Reynolds number ranged from 96 to 720. No pronounced real fluid effects have been observed in the current density although the probe is observed by Schlieren photography to exhibit boundary layer separation and wake formation. In spite of the real fluid behavior of the plasma fluid, the thin sheath theory describes the current density distribution on the probe surface very effectively. This is attributed to the formation and entrainment of a shielding layer of fluid, voided of charge during its passage through the sheath.


2021 ◽  
Vol 2021 ◽  
pp. 1-7
Author(s):  
Huong T. T. Nguyen ◽  
Hoai-Duc Vu ◽  
Jichul Shin

Phenomenological behavior of ion beam acceleration through the grid system in 50 W class RF ion thruster has been investigated using PIC simulation and evaluated by experimental test using Faraday probe. Beam trajectory for various grid voltages reveals that the metal engine cover of the ion thruster which is needed to seal RF coil around the discharge chamber affects the beam divergence angle. Simulation result shows that the divergence angle increases by 10.52% mainly because of the larger radial electric field in the presence of the metal engine cover. The divergence angle increases as the accelerator grid voltage increases. The current density distribution measured by the Faraday probe shows a bigger divergence angle with the engine cover installed. For the test cases with mass flow rates from 3 sccm to 4 sccm at the RF power of about 50 W, the current density distribution exhibits the 2nd peak at the radial position about 4 cm from the centerline.


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