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'''Tidal heating''' (also known as '''tidal working''') occurs through the [[tidal friction]] processes: orbital and rotational energy are dissipated as heat in the crust of the moons and planets involved. [[Io (moon)|Io]], a moon of [[Jupiter]], is the most volcanically active body in the [[solar system]], with no impact craters surviving on its surface. This is because the tidal force of Jupiter deforms Io;<ref>{{Citation
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| title = Melting of Io by Tidal Dissipation
| url = http://links.jstor.org/sici?sici=0036-8075%2819790302%293%3A203%3A4383%3C892%3AMOIBTD%3E2.0.CO%3B2-8
| year = 1979
| journal = Science
| pages = 892–894
| volume = 203
| issue = 4383
| last1 = Peale    | first1 =  S. J.
| last2 = Cassen    | first2 =  P.
| last3 = Reynolds    | first3 =  R. T.
| accessdate = 2010-10-12 
| doi = 10.1126/science.203.4383.892 | pmid=17771724|bibcode = 1979Sci...203..892P }}</ref> the [[orbital eccentricity|eccentricity]] of Io's orbit (a consequence of its participation in a [[Orbital resonance|Laplace resonance]]) causes the height of Io's tidal bulge to vary significantly (by up to 100 m) over the course of an orbit; the friction from this tidal flexing then heats up its interior. A similar but weaker process is theorised to have melted the lower layers of the ice surrounding the rocky mantle of Jupiter's next large moon, [[Europa (moon)|Europa]].  Saturn's moon [[Enceladus (moon)|Enceladus]] is similarly thought to have a liquid water ocean beneath its icy crust. The [[cryovolcano|water vapor geysers]] which eject material from Enceladus are thought to be powered by friction generated within this moon's shifting ice crust.<ref>Peale, S.J. Tidally induced volcanism. Celest. Mech. & Dyn. Astr. 87, 129–
155, 2003.</ref>
 
The total amount of tidal heating <math>q_{tid}</math> is given by
:<math>q_{tid} = 63 \rho n^5 r^4 e^2 / 38 \mu Q</math>
where <math>r</math> is the satellite’s radius, <math>n</math> is the mean orbital motion, <math>e</math> is the eccentricity of the orbit, <math>Q</math> is a dimensionless dissipation factor, and <math>\mu</math> is the shear modulus. The role of tidal heating is sometimes expressed by dimensionless number C equal to quotient of tidal heating and total internal heating.<ref>Czechowski, L., 2006, Parameterized model of convection driven by tidal and radiogenic heating, Adv. Space Res, 38, 4, 788-793</ref>
 
==See also==
* [[Cryovolcano]]
* [[Tidal acceleration]]
* [[Tidal locking]]
 
==References==
{{Reflist}}
 
[[Category:Planetary science]]
[[Category:Tides]]
 
 
{{Geophysics-stub}}
{{Planetary-science-stub}}

Latest revision as of 14:50, 29 September 2014

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