Abstract:We identify two likely normal faults on Europa, of lengths z30 and 11 km. A simple flexural model of fault-related topography gives effective elastic thicknesses of 1.2 and 0.15 km, respectively, and the resulting inferred fault strength is of order 1 MPa. The maximum fault displacement: length ratio for each fault is z0.02, comparable with values on silicate planets. We combine this observation with a modified linear elastic fracture mechanics model to conclude that the shear modulus of the Europan surface mu… Show more
“…Possible seismic sources on Europa include the opening of tensile cracks due to the Jovian tides, as tide-induced cracks might lead to quakes ranging from 2 to 4 in moment magnitude. Nimmo and Schenk (2006) have also identified regions of normal faults on Europa by analyzing Galileo data, indicating potential quakes up to M w ¼ 5.3 magnitude. The frequency of such proposed events remains unknown.…”
“…Possible seismic sources on Europa include the opening of tensile cracks due to the Jovian tides, as tide-induced cracks might lead to quakes ranging from 2 to 4 in moment magnitude. Nimmo and Schenk (2006) have also identified regions of normal faults on Europa by analyzing Galileo data, indicating potential quakes up to M w ¼ 5.3 magnitude. The frequency of such proposed events remains unknown.…”
“…Unlike Mars or Earth, digital elevation models are only available for small areas on the icy satellites, with topographic information being obtained primarily through point photoclinometric and stereographic techniques on these bodies. Nimmo and Schenk (2006) used this technique on Europa to identify a normal fault scarp that was too subtle to easily identify in surface imagery. Digital elevation models created from stereo images have recently been used to investigate graben geometries and to infer properties of lithospheric thicknesses of icy satellites (Giese et al, 2006.…”
“…Young's modulus of ice is estimated to be a few GPa (Nimmo & Schenk 2006;see Collins et al 2010 for a review) and this is about 10 times lower than the Young's modulus for rocky materials. To explore the affect of softer icy ends on the semi-major axis drift rate, we ran a simulation of a body that is not homogeneous.…”
We use numerical simulations to measure the sensitivity of the tidal spin down rate of a homogeneous triaxial ellipsoid to its axis ratios by comparing the drift rate in orbital semi-major axis to that of a spherical body with the same mass, volume and simulated rheology. We use a mass-spring model approximating a viscoelastic body spinning around its shortest body axis, with spin aligned with orbital spin axis, and in circular orbit about a point mass. The torque or drift rate can be estimated from that predicted for a sphere with equivalent volume if multiplied by 0.5where b/a and c/a are the body axis ratios and index α c ≈ 1.05 is consistent with the random lattice mass spring model simulations but α c = 4/3 suggested by scaling estimates. A homogeneous body with axis ratios 0.5 and and 0.8, like Haumea, has orbital semi-major axis drift rate about twice as fast as a spherical body with the same mass, volume and material properties. A simulation approximating a mostly rocky body but with 20% of its mass as ice concentrated at its ends has a drift rate 10 times faster than the equivalent homogeneous rocky sphere. However, this increase in drift rate is not enough to allow Haumea's satellite, Hi'iaka, to have tidally drifted away from Haumea to its current orbital semi-major axis.
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