2013
DOI: 10.1002/grl.50309
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A large‐scale flow vortex in the Venus plasma tail and its fluid dynamic interpretation

Abstract: We report on the existence of a large‐scale ion flow vortex, a curled tailward flow of solar wind H+ (SW H+), and ionospheric O+ in the Venus plasma tail. The vortex commences at dusk (−Y), driven by a transverse (to the solar wind) aberration flow component. Dusk magnetosheath and ionospheric ions move westward across the nightside into the dawn sector, from where the tailward and lateral flow merges into a tailward‐moving vortex. A fluid analysis of the SW H+ energy and momentum (E&M) transfer to O+ at the t… Show more

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Cited by 24 publications
(22 citation statements)
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“…In the ionosphere, the plasma velocity is actually dominated by the components along the Y VSO axis (with a contribution of ≈46%) followed by Z VSO (≈39%) and X VSO (≈15%) axes. These results are consistent with Lundin et al(, , ) in which the authors attributed the persistent + Y VSO directed ion flow over the northern polar region to the solar wind aberration.…”
Section: Discussionsupporting
confidence: 93%
“…In the ionosphere, the plasma velocity is actually dominated by the components along the Y VSO axis (with a contribution of ≈46%) followed by Z VSO (≈39%) and X VSO (≈15%) axes. These results are consistent with Lundin et al(, , ) in which the authors attributed the persistent + Y VSO directed ion flow over the northern polar region to the solar wind aberration.…”
Section: Discussionsupporting
confidence: 93%
“…Solar wind protons and heavy ionospheric ions display the same vortex pattern, suggesting that energy and momentum are directly transferred from the solar wind plasma to the planetary ions. The origin of the vortex has been proposed to be the orbital motion of Venus, which causes a significant aberration of the solar wind flow around Venus (Lundin et al 2013).…”
Section: Plasma In the Magnetotailmentioning
confidence: 99%
“…The latter leads to an asymmetry in the location of the Venus ionopause [ Phillips et al ., ], and a curled flow of SWH + and energized O + moving dawnward and tailward through the polar region thermosphere [ Lundin et al ., ]. The height distribution of the SWH + and ionospheric O + momentum fluxes indicates an efficient transfer of SWH + energy and momentum to O + [ Pérez‐de‐Tejada , ] at altitudes up to 1200 km [ Lundin et al ., ]. The ion flux decrease below 1000 km marks a gradual transition of ions to Energetic Neutral Atoms (ENAs) via Charge Exchange (CE).…”
Section: Introductionmentioning
confidence: 99%
“…The average ion flow over the low-altitude polar region displays a steady flow directed tailward and laterally (+Y), the plasma tail forming a large-scale vortex [Lundin et al, 2013]. On the nightside near the planet, the flow is more tangential, moving westward in the direction of the atmospheric super-rotation.…”
Section: Introductionmentioning
confidence: 99%