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Thermal history of the Jovian satellite Io
Institution:1. IVG, Institute for Combustion and Gas Dynamics – Reactive Fluids, Fluid Dynamics and CENIDE, Center for Nanointegration Duisburg-Essen, University of Duisburg-Essen, Carl-Benz-Str. 199, 47057 Duisburg, Germany;2. Department of Natural Sciences, The Open University of Israel, 4353701 Raanana, Israel;3. School of Chemistry, Tel Aviv University, Ramat Aviv, 69978 Tel Aviv, Israel;4. Institute of Laser Physics, University of Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany;1. Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama, Meguro-ku, Tokyo 152-8551, Japan;2. Earth-Life Science Institute, Tokyo Institute of Technology, Ookayama, Meguro-ku, Tokyo 152-8550, Japan
Abstract:The discovery of large volcanic eruptions on Io suggests that Io is one of the most geologically active planetary bodies. The energy source of this geologic activity is believed to be tidal heating induced by Jupiter. A number of thermal history calculations were done to investigate the effect of tidal heating on the thermal history of Io taking into account solid state convection and advective heat transfer. These simulations show that the total tidal heating energy in Io is almost equal to the advectively transferred heat, indicating that the observed heat flow from Io is nearly equal to the total tidal heating energy. Since total tidal heating energy is dependent on the radius of the liquid mantle and the internal dissipation factor (Q), the radius of the liquid mantle can be estimated for a given value of Q. Some reasonable thermal history models of Io were obtained using a model with Q ≈ 25–50 in which the magma source of Ionian volcanism is at a depth of 100–300 km. The models satisfy the heat flow data and the existence of a thick lithosphere. Using a model with Q = 25 and L = 300 km (thickness of the advective region) as the standard model (model II), we then studied the effect of convective heat transfer and the initial temperature distribution on the Ionian thermal history. In these calculations, the other parameters are the same as in the standard model (model II). These calculations show that although the temperature distribution in the central region reflects the difference in the efficiency of convective heat transfer and initial temperature distribution, the temperature distribution in the outer region does not changes appreciably.
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