Eimacman said:
Vanadium 50:
I believe that Io should be ignored because it is continuously heated by gravitational effects of the Jovian system, any cooling of that body would be constantly replaced by heating due to tidal flexing of Io.
That is surely a valid point. And, according to the National Geographic documentary
Naked Science -- The Moon (TV), the Moon used to be about 15x closer to Earth than it is today. It pulled up 10,000' ocean tides that dragged backwards against the then-rapid rotation of the planet (the day was about
6 hours long).
These fierce tidal forces eventually phase-locked the Moon in its orbit, and spun it out an additional ~350,000 km.
Assuming that all the
Rotational Kinetic Energy:
K = \frac{1}{2} I \omega^{2}
which the Earth has lost as it has spun down, has been converted into heat, then that
Tidal Heating Budget is:
\Delta K = \frac{1}{2} I \Delta\omega^{2}
= \frac{0.3315}{2} M R^{2} \left( \omega_{i}^{2} - \omega_{f}^{2} \right)
= \frac{0.3315}{2} M R^{2} \left( \frac{2 \pi}{T_{i}^{2}} - \frac{2 \pi}{T_{f}^{2}} \right)
= 6.544 M R^{2} \left( \frac{1}{T_{i}^{2}} - \frac{1}{T_{f}^{2}} \right)
= 3.195 \times 10^{30} J
Now, the Earth is currently venting heat at the rate of ~
4 x 1013 W*. Thus, the above
Heat Budget could power that dissipation rate for ~
2.5 billion years.
* Carroll & Ostlie. Introduction to Modern Astrophysics, pp. 818 & 797.
CONCLUSION: These fierce tidal forces have generated gargantuan quantities of heat. Perhaps that explains why Earth seems more active, even than Venus.
Alternatively, the current Tidal Heating Rate is:
\frac{\partial K}{\partial t} = -4 \pi^{2} I \frac{1}{T^{3}} \frac{\partial T}{\partial t}
\approx 2.5 \times 10^{12} W
since the current rate of spin-down is 0.0016 s century-1*. Thus, Tidal Heating currently accounts for only 6% of the Earth's rate of heat loss.
* Carroll & Ostlie. ibid., pg. ~763.
This gives a Tidal Heating Time Scale of:
\frac{\Delta K}{\frac{\partial K}{\partial t}} \approx 40 billion years
Since that is ~10x the age of the Earth, surely Tidal Heating was more important in the past. This suggests, that Tidal Heating could have once been a primary factor for the early Earth.
Widdekind:
It is also necessary to add the calculation the possibility of transuranic elements U235, U236, U237, and U238 in the core that would add heat to such a planetary body, the half life's of which can be many billions of years. The formula could give one a 'ballpark guesstimation' of the cooling of a planetary body, if you ignore any of the effects, properties here mentioned. It is theorized that the Earth's internal heat may persist for as long as 30 billion years due to nuclear heating. This is longer than the time that the Sun will be on the main sequence. Any planetary bodies of similar mass but of different composition will have different heating rates due to initial gravitational compression. Lighter element bodies will not compress and heat up like a rocky or a metallic body composed of heaver elements. Also the heaver the element composition the more likely there will be radioactive elements that will maintain heat longer than could be achieved by compression alone.
That is true. Please consider a group of planetoids of comparable composition, which of course varies by their formation zone*:
- near zone (Mercury)
- Habitable Zone (Venus, Earth, Moon, Mars, Asteroids)
- Ice Zone (Jupiter, Saturn)
- Methane-Ice Zone (Uranus, Neptune)
For all those bodies, the basic physics that tcool ~ M / R2 is probably valid. However, the constant of proportionality will change, possibly dramatically, according to bulk composition. For, Lord Kelvin calculated that the Earth's tcool ~ 80 million years (w/o nuclear fission heating). Thus, planetoids far out in the Solar System, where there may be relatively fewer heavy elements, would have less fission heating, and so cool down much more quickly. But, for 2 such similar bodies, their relative Cooling Times are probably dictated by the quantity M / R2. (Unless there are other sources of heat, like Tidal Friction.)
* Carroll & Ostlie. Introduction to Modern Astrophysics, pg. 893 ; National Geographic Naked Science -- Formation of the Solar System (TV)