JpGU-AGU Joint Meeting 2020

講演情報

[E] ポスター発表

セッション記号 P (宇宙惑星科学) » P-PS 惑星科学

[P-PS01] Outer Solar System Exploration Today, and Tomorrow

コンビーナ:木村 淳(大阪大学)、Kunio M. Sayanagi(Hampton University)、土屋 史紀(東北大学大学院理学研究科惑星プラズマ・大気研究センター)、Steven Douglas Vance(NASA Jet Propulsion Laboratory, California Institute of Technology)

[PPS01-P04] Tidally heated convection and the occurrence of melting in icy satellites: application to Europa

*Kenny Vilella1Gael Choblet2Wei-En Tsao3Frederic Deschamps3 (1.Hokkaido University、2.LPG Nantes、3.Institute of Earth Sciences, Academia Sinica)

キーワード:Europa, Icy Satellites, Thermal convection, Melting, Cryovolcanism, Tidal Heating

Observations of icy satellites have revealed widespread marks of cryovolcanism. Because aqueous cryomagmas are negatively buoyant, two processes are required to explain these observations: one mechanism to generate melt close enough to the surface, and another one to transport this melt to the surface. Here, we investigate the generation of melting in a systematic way, using a set of 85 numerical simulations where we vary the viscosity contrast, Rayleigh number, and tidal heating rate. Applied to Europa, and considering a hydrosphere composed of pure water, our simulations suggest that isolated melt pockets can be generated close to the surface (≈5 km) as long as the ice layer thickness (d*) remains modest (15<d*<35 km). However, the generation of melting becomes increasingly difficult as the amount of anti-freeze compounds in the subsurface ocean increases. Furthermore, the proportion of melting increases very sharply with increasing tidal heating rate. In particular, when the tidal heating rate exceeds a threshold, an asymptotic regime is reached where the surface heat flux remains constant, i.e., the tidal heat generated above this threshold is only used for melting the ice shell. In that regime, we found a direct relationship between the surface heat flux and d*. Finally, we provide a new assessment of Europa's thermal state. Using available constraints, we propose that the ice shell thickness should exceed 25 km. However, d*≈25-35 km implies a tidal power (>3 TW) much larger than expected. An extrapolation of the trends suggested by our results indicates that a more reasonable tidal power (<1 TW) would involve d*≈80-100 km.