Near exit plane non-resonant light induced fluorescence spectroscopy is performed in a Hall effect low-power Xenon thruster at discharge voltage of 250~V and anode flow rate of 0.7~mg/sec. Measurement of the axial and radial velocity components are performed, exciting the $6s~^2[3/2]^o_2\rightarrow6p~^2[3/2]_2$ transition at $823.16$~nm in XeI and the $5d~[4]_{7/2}\rightarrow6p~[3]^o_{5/2}$ transition at $834.724$~nm in XeII. No significant deviation from the thermal velocity is observed for XeI. Two most probable ion velocities are registered at a given position with respect to the thruster axis, which are mainly attributed to different areas of creation of ions inside the acceleration channel. The spatial resolution of the set-up is limited by the laser beam size (radius of the order of $0.5$~mm) and the fluorescence collection optics, which have a view spot diameter of $8$~mm.
Dancheva, Y., Biancalana, V., Damiano, P., Fabrizio, S. (2013). Measurement of XeI and XeII velocity in the near exit plane of a low-power Hall effect thruster by light induced fluorescence spectroscopy. REVIEW OF SCIENTIFIC INSTRUMENTS, 84(6), 065113-1-065113-6 [10.1063/1.4811664].
Measurement of XeI and XeII velocity in the near exit plane of a low-power Hall effect thruster by light induced fluorescence spectroscopy
DANCHEVA, YORDANKA;BIANCALANA, VALERIO;
2013-01-01
Abstract
Near exit plane non-resonant light induced fluorescence spectroscopy is performed in a Hall effect low-power Xenon thruster at discharge voltage of 250~V and anode flow rate of 0.7~mg/sec. Measurement of the axial and radial velocity components are performed, exciting the $6s~^2[3/2]^o_2\rightarrow6p~^2[3/2]_2$ transition at $823.16$~nm in XeI and the $5d~[4]_{7/2}\rightarrow6p~[3]^o_{5/2}$ transition at $834.724$~nm in XeII. No significant deviation from the thermal velocity is observed for XeI. Two most probable ion velocities are registered at a given position with respect to the thruster axis, which are mainly attributed to different areas of creation of ions inside the acceleration channel. The spatial resolution of the set-up is limited by the laser beam size (radius of the order of $0.5$~mm) and the fluorescence collection optics, which have a view spot diameter of $8$~mm.File | Dimensione | Formato | |
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https://hdl.handle.net/11365/44617
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