1987
DOI: 10.1038/325133a0
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Tidal heating in an internal ocean model of Europa

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Cited by 94 publications
(73 citation statements)
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“…Vertical heat flows of at least ϳ100 -200 mW m Ϫ2 are needed to put the brittleductile transition at a depth Յ2 km (McKinnon, 2000;Pappalardo et al, 1999b;Ruiz andTejero, 1999, 2000). These heat flows are clearly higher than the theoretical values of Յ50 mW m Ϫ2 calculated by classical tidal heating models (Cassen et al, 1982;Ojakangas and Stevenson, 1989;Ross and Schubert, 1987;Squyres et al, 1983) . The explanation for these high heat flows could lie in the tidal heating either of a warm ice convective layer (McKinnon and Shock, 2001;Ruiz and Tejero, 2000) or of the rock/ metal core (McKinnon and Shock, 2001).…”
Section: Introductionmentioning
confidence: 51%
See 1 more Smart Citation
“…Vertical heat flows of at least ϳ100 -200 mW m Ϫ2 are needed to put the brittleductile transition at a depth Յ2 km (McKinnon, 2000;Pappalardo et al, 1999b;Ruiz andTejero, 1999, 2000). These heat flows are clearly higher than the theoretical values of Յ50 mW m Ϫ2 calculated by classical tidal heating models (Cassen et al, 1982;Ojakangas and Stevenson, 1989;Ross and Schubert, 1987;Squyres et al, 1983) . The explanation for these high heat flows could lie in the tidal heating either of a warm ice convective layer (McKinnon and Shock, 2001;Ruiz and Tejero, 2000) or of the rock/ metal core (McKinnon and Shock, 2001).…”
Section: Introductionmentioning
confidence: 51%
“…Later on, Squyres et al (1983) calculated that an icy shell in Europa would be stable against convection if its thickness did not exceed ϳ30 km. Based on this, it was proposed that tidal heating could perhaps allow the stable existence of a conductive shell floating over an internal liquid-water ocean (Ojakangas and Stevenson, 1989;Ross and Schubert, 1987;Squyres et al, 1983).…”
Section: Shell Thickness and Heat Flow In The Onset Of Convectionmentioning
confidence: 99%
“…For a model of Europa that includes dynamic decoupling between icy shell and rocky core by an ocean, the minimum contribution to the heat flow by tidal heating in the core would be~12-16 mW m )2 (Squyres et al, 1983;Ross and Schubert, 1987). Thus, heat flow reaching to the icy shell base from the rock and metal core would be at least~20 mW m )2 (which is equivalent to a shell at most~30 km thick).…”
Section: Results and Conclusionmentioning
confidence: 99%
“…This allows us to relate the feasibility analysis for convection initiation to the thermal state of Europa. A higher effective surface temperature (caused, for example, by an insulating regolith layer (e.g., Shoemaker et al, 1982;Ross and Schubert, 1987), or by a solid-state greenhouse in the uppermost superficial ice layer (e.g., Matson and Brown, 1989)) reduces the ice shell thickness required for the onset of convection. However, the critical heat flow at the onset of convection is almost independent of the surface temperature (Ruiz and Tejero, 2003).…”
Section: Results and Conclusionmentioning
confidence: 99%
“…These effects, frequently cited by the icy Galilean satellites (e.g., Shoemaker et al, 1982;Squyres et al, 1983;Ross and Schubert, 1987), could contribute to retain internal heat, favoring the existence of an internal ocean. Similarly, the possibility of a surface layer rich in low thermal conductivity ices raising the effective surface temperature and contributing to a hotter interior on Triton has been mentioned by McKinnon et al (1995).…”
Section: Insulating Layers On the Surfacementioning
confidence: 99%