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Enceladus tiger stripes tidal heating
Enceladus tiger stripes tidal heating








enceladus tiger stripes tidal heating

Stability and exchange of subsurface ice on Mars. The stability of ground ice in the equatorial region of Mars. Temperature evolution and vapour pressure build-up in porous ices.

enceladus tiger stripes tidal heating

Viscoelastic models of tidal heating on Enceladus. Tectonic processes on Europa: tidal stresses, mechanical response and visible features. Patterns of fracture and tidal stresses on Europa. Strike-slip faults on Europa: global shear patterns driven by tidal stress. Subsurface oceans on Europa and Callisto: constraints from Galileo magnetometer observations. Distribution of strike-slip faults on Europa. Eruptions arising from tidally controlled periodic openings of rifts on Enceladus. A shear heating origin for ridges on Triton. Thermal consequences of strike-slip motion on Europa. Monte Carlo simulations of the water vapor plumes on Enceladus. Cassini ion and neutral mass spectrometer: Enceladus plume composition and structure. A clathrate reservoir hypothesis for Enceladus’ south polar plume. Cassini dust measurements at Enceladus and implications for the origin of the E ring. Cassini encounters Enceladus: background and the discovery of a south polar hot spot. Cassini observes the active south pole of Enceladus.

enceladus tiger stripes tidal heating

We predict that the tiger-stripe regions with highest relative temperatures will be the lower-latitude branch of Damascus, Cairo around 60° W longitude and Alexandria around 150° W longitude. The tidal displacements required imply a Love number of h 2 > 0.01, suggesting that the ice shell is decoupled from the silicate interior by a subsurface ocean. The ice shell thickness needed to produce the observed heat flux is at least 5 km.

enceladus tiger stripes tidal heating

Vapour produced by this heating may escape as plumes through cracks reopened by the tidal stresses 10. Here we show that the most likely explanation for the heat 2 and vapour production 6, 7 is shear heating by tidally driven lateral (strike-slip) fault motion 1, 8, 9 with displacement of ∼0.5 m over a tidal period. Neither model addresses how delivery of internal heat to the near-surface is sustained. The plume characteristics 1 and local high heat flux 2 have been ascribed either to the presence of liquid water within a few tens of metres of the surface 1, or the decomposition of clathrates 5. We predict that the tiger-stripe regions with highest relative temperatures will be the lower-latitude branch of Damascus, Cairo around 60 degrees W longitude and Alexandria around 150 degrees W longitude.Enceladus, a small icy satellite of Saturn, has active plumes jetting from localized fractures (‘tiger stripes’) within an area of high heat flux near the south pole 1, 2, 3, 4. The tidal displacements required imply a Love number of h2 > 0.01, suggesting that the ice shell is decoupled from the silicate interior by a subsurface ocean. The ice shell thickness needed to produce the observed heat flux is at least 5 km. Vapour produced by this heating may escape as plumes through cracks reopened by the tidal stresses. Here we show that the most likely explanation for the heat and vapour production is shear heating by tidally driven lateral (strike-slip) fault motion with displacement of approximately 0.5 m over a tidal period. The plume characteristics and local high heat flux have been ascribed either to the presence of liquid water within a few tens of metres of the surface, or the decomposition of clathrates. Enceladus, a small icy satellite of Saturn, has active plumes jetting from localized fractures ('tiger stripes') within an area of high heat flux near the south pole.










Enceladus tiger stripes tidal heating