2009
DOI: 10.1038/nature08108
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Strong tidal dissipation in Io and Jupiter from astrometric observations

Abstract: Io is the volcanically most active body in the Solar System and has a large surface heat flux. The geological activity is thought to be the result of tides raised by Jupiter, but it is not known whether the current tidal heat production is sufficiently high to generate the observed surface heat flow. Io's tidal heat comes from the orbital energy of the Io-Jupiter system (resulting in orbital acceleration), whereas dissipation of energy in Jupiter causes Io's orbital motion to decelerate. Here we report a deter… Show more

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Cited by 350 publications
(489 citation statements)
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“…The elastic Love numbers were measured with accuracy only for the Earth and Mars, respectively, k e ≈ 0.3 (Mathews et al 1995), and k e ≈ 0.15 (Konopliv et al 2006). For the gaseous planets only the ratio k 2 /Q is known for Jupiter and Saturn, respectively, k 2 /Q ≈ 1.1 × 10 −5 (Lainey et al 2009), and k 2 /Q ≈ 2.3 × 10 −4 (Lainey et al 2012). The relaxation times are totally unknown for both terrestrial and gaseous planets, but if one is able to estimate Q, then τ and τ e can be estimated through expressions (46) and (56).…”
Section: Application To Close-in Planetsmentioning
confidence: 99%
“…The elastic Love numbers were measured with accuracy only for the Earth and Mars, respectively, k e ≈ 0.3 (Mathews et al 1995), and k e ≈ 0.15 (Konopliv et al 2006). For the gaseous planets only the ratio k 2 /Q is known for Jupiter and Saturn, respectively, k 2 /Q ≈ 1.1 × 10 −5 (Lainey et al 2009), and k 2 /Q ≈ 2.3 × 10 −4 (Lainey et al 2012). The relaxation times are totally unknown for both terrestrial and gaseous planets, but if one is able to estimate Q, then τ and τ e can be estimated through expressions (46) and (56).…”
Section: Application To Close-in Planetsmentioning
confidence: 99%
“…In our final solution we use the theory of the motion of the Galilean satellites developed by Lainey et al (2009) Astrometric results of the observations may have the form of any corrected relative position of satellites X(t * ) = X th (t * ) + D x , Y(t * ) = Y th (t * ) + D y together with the associated time instant t * inside the time interval of the event. Although this is not mandatory, we assume that t * is the time instant when √ X 2 + Y 2 takes its minimum value, t * is the time of the closest apparent approach of the satellites.…”
Section: Extracting Astrometric Data From the Photometry Of Satellitementioning
confidence: 99%
“…However, using the currently estimated tidal dissipation parameters to extrapolate backward in time predicts that the Moon was at Earth's surface about *2 Gyr ago (MacDonald, 1964), which contradicts the standard impact model for the lunar origin [note that numerous issues remain such as the origin of Earth's and the Moon's obliquities (Touma and Wisdom, 1994) and the perturbations from other planets (Ć uk, 2007)]. The deceleration of Io's orbital velocity has also been tentatively detected and seems broadly consistent with tidal theory (Aksnes and Franklin, 2001;Lainey et al, 2009). However, these data lie in the same regime, that of nearly circular orbits.…”
Section: Tidal Heatingmentioning
confidence: 85%