Orbital and friction heating on a planet or moon oceans, or interior
Tidal heating (also known as tidal working or tidal flexing) occurs through the
.
Moons of Gas Giants
Tidal heating is responsible for the geologic activity of the most volcanically active body in the
Enceladus is similarly thought to have a liquid water ocean beneath its icy crust, due to tidal heating related to its resonance with
Dione. The
water vapor geysers which eject material from Enceladus are thought to be powered by friction generated within its interior.
[2]
Earth
Munk & Wunsch (1998) estimated that Earth experiences 3.7 TW (0.0073 W/m2) of tidal heating, of which 95% (3.5 TW or 0.0069 W/m2) is associated with ocean tides and 5% (0.2 TW or 0.0004 W/m2) is associated with
Earth tides, with 3.2 TW being due to tidal interactions with the Moon and 0.5 TW being due to tidal interactions with the Sun.
[3] Egbert & Ray (2001) confirmed that overall estimate, writing "The total amount of tidal energy dissipated in the Earth-Moon-Sun system is now well-determined. The methods of space geodesy—altimetry, satellite laser ranging, lunar laser ranging—have converged to 3.7 TW
..."
[4]
Heller et al. (2021) estimated that shortly after the Moon was formed, when the Moon orbited 10-15 times closer to Earth than it does now, tidal heating might have contributed ~10 W/m2 of heating over perhaps 100 million years, and that this could have accounted for a temperature increase of up to 5°C on the early Earth.[5][6]
Moon
Harada et al. (2014) proposed that tidal heating may have created a molten layer at the core-mantle boundary within Earth's Moon.[7]
Io
Jupiter's closest moon Io experiences considerable tidal heating.
Formula
The tidal heating rate, , in a satellite that is
(
), and has an
eccentric orbit is given by:
where
,
,
, and
are respectively the satellite's mean radius,
mean orbital motion,
orbital distance, and eccentricity.
[8] is the host (or central) body's mass and
represents the imaginary portion of the second-order
Love number which measures the efficiency at which the satellite dissipates tidal energy into frictional heat. This imaginary portion is defined by interplay of the body's rheology and self-gravitation. It, therefore, is a function of the body's radius, density, and rheological parameters (the
shear modulus,
viscosity, and others – dependent upon the rheological model).
[9][10] The rheological parameters' values, in turn, depend upon the temperature and the concentration of partial melt in the body's interior.
[11]
The tidally dissipated power in a nonsynchronised rotator is given by a more complex expression.[12]
See also
References