1978
DOI: 10.1038/275037a0
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Venus' rotation and atmospheric tides

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Cited by 75 publications
(70 citation statements)
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“…(156) because convection eliminates the component resulting from the fluid vertical displacement. In agreement with the early result of Ingersoll & Dobrovolskis (1978) (Eq. (4)), it is of the same form as the result given by the Maxwell model (Correia et al 2014), where we identify the Maxwell time T 0 " σ´1 0 .…”
Section: Comparison With Previous Modelssupporting
confidence: 81%
“…(156) because convection eliminates the component resulting from the fluid vertical displacement. In agreement with the early result of Ingersoll & Dobrovolskis (1978) (Eq. (4)), it is of the same form as the result given by the Maxwell model (Correia et al 2014), where we identify the Maxwell time T 0 " σ´1 0 .…”
Section: Comparison With Previous Modelssupporting
confidence: 81%
“…Additionally, thermal atmospheric tides raised on a close orbiting planet could be significant compared to gravitational tides (Gold & Soter, 1969;Ingersoll & Dobrovolskis, 1978;Leconte et al, 2015;Cunha et al, 2015). Recent work exploring the effect of thermal tides in the atmospheres of M-dwarf planets indicates that for high stellar insolation, an atmospheric torque may be generated that opposes tidally-induced spin synchronization, as is the case for Venus.…”
Section: Gravitational Effectsmentioning
confidence: 99%
“…The first possibility is that the gravitational torque on the atmosphere pushes the atmosphere away from synchronous rotation (i.e., it increases the magnitude of the atmosphere's angular momentum measured in the synchronously-rotating reference frame) as has been hypothesized for Venus (Ingersoll & Dobrovolskis 1978;Gold & Soter 1969). To balance the torque on the atmosphere, the interior must have a net angular momentum of the same sign as the atmosphere (so that both either superor subrotate).…”
Section: The Equilibrium Statementioning
confidence: 99%