Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency

Abstract Development of a magnetic nozzle radiofrequency (rf) plasma thruster has been one of challenging topics in space electric propulsion technologies. The thruster typically consists of an rf plasma source and a magnetic nozzle, where the plasma produced inside the source is transported along t...

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Main Author: Kazunori Takahashi
Format: Article
Language:English
Published: Nature Publishing Group 2021-02-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-021-82471-2
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spelling doaj-c2d6cc35c9ca4dec88f26f36097f93bb2021-02-07T12:32:59ZengNature Publishing GroupScientific Reports2045-23222021-02-0111111210.1038/s41598-021-82471-2Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiencyKazunori Takahashi0Department of Electrical Engineering, Tohoku UniversityAbstract Development of a magnetic nozzle radiofrequency (rf) plasma thruster has been one of challenging topics in space electric propulsion technologies. The thruster typically consists of an rf plasma source and a magnetic nozzle, where the plasma produced inside the source is transported along the magnetic field and expands in the magnetic nozzle. An imparted thrust is significantly affected by the rf power coupling for the plasma production, the plasma transport, the plasma loss to the wall, and the plasma acceleration process in the magnetic nozzle. The rf power transfer efficiency and the imparted thrust are assessed for two types of rf antennas exciting azimuthal mode number of $$m=+1$$ m = + 1 and $$m=0$$ m = 0 , where propellant argon gas is introduced from the upstream of the thruster source tube. The rf power transfer efficiency and the density measured at the radial center for the $$m=+1$$ m = + 1 mode antenna are higher than those for the $$m=0$$ m = 0 mode antenna, while a larger thrust is obtained for the $$m=0$$ m = 0 mode antenna. Two-dimensional plume characterization suggests that the lowered performance for the $$m=+1$$ m = + 1 mode case is due to the plasma production at the radial center, where contribution on a thrust exerted to the magnetic nozzle is weak due to the absence of the radial magnetic field. Subsequently, the configuration is modified so as to introduce the propellant gas near the thruster exit for the $$m=0$$ m = 0 mode configuration and the thruster efficiency approaching twenty percent is successfully obtained, being highest to date in the kW-class magnetic nozzle rf plasma thrusters.https://doi.org/10.1038/s41598-021-82471-2
collection DOAJ
language English
format Article
sources DOAJ
author Kazunori Takahashi
spellingShingle Kazunori Takahashi
Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
Scientific Reports
author_facet Kazunori Takahashi
author_sort Kazunori Takahashi
title Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
title_short Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
title_full Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
title_fullStr Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
title_full_unstemmed Magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
title_sort magnetic nozzle radiofrequency plasma thruster approaching twenty percent thruster efficiency
publisher Nature Publishing Group
series Scientific Reports
issn 2045-2322
publishDate 2021-02-01
description Abstract Development of a magnetic nozzle radiofrequency (rf) plasma thruster has been one of challenging topics in space electric propulsion technologies. The thruster typically consists of an rf plasma source and a magnetic nozzle, where the plasma produced inside the source is transported along the magnetic field and expands in the magnetic nozzle. An imparted thrust is significantly affected by the rf power coupling for the plasma production, the plasma transport, the plasma loss to the wall, and the plasma acceleration process in the magnetic nozzle. The rf power transfer efficiency and the imparted thrust are assessed for two types of rf antennas exciting azimuthal mode number of $$m=+1$$ m = + 1 and $$m=0$$ m = 0 , where propellant argon gas is introduced from the upstream of the thruster source tube. The rf power transfer efficiency and the density measured at the radial center for the $$m=+1$$ m = + 1 mode antenna are higher than those for the $$m=0$$ m = 0 mode antenna, while a larger thrust is obtained for the $$m=0$$ m = 0 mode antenna. Two-dimensional plume characterization suggests that the lowered performance for the $$m=+1$$ m = + 1 mode case is due to the plasma production at the radial center, where contribution on a thrust exerted to the magnetic nozzle is weak due to the absence of the radial magnetic field. Subsequently, the configuration is modified so as to introduce the propellant gas near the thruster exit for the $$m=0$$ m = 0 mode configuration and the thruster efficiency approaching twenty percent is successfully obtained, being highest to date in the kW-class magnetic nozzle rf plasma thrusters.
url https://doi.org/10.1038/s41598-021-82471-2
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