Tidal Acceleration and planetary rotation

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Tidal acceleration refers to the gravitational influence of the Moon on Earth, affecting its rotation speed and potentially leading to tidal locking. To calculate the impact of the Moon's tidal acceleration on Earth's rotation, one must consider the energy dissipation rate due to Earth's deformation, which varies based on geological factors and water distribution. Without this information, estimating the time for Earth to become tide-locked to the Moon is challenging, as a perfectly elastic Earth would not achieve tidal locking. The discussion highlights that while first-order calculations can be made, more complex modeling is necessary for accurate predictions. Ultimately, while Earth is expected to become tide-locked to the Moon over an extended timescale, precise estimates require further mathematical analysis.
AotrsCommander
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I'm struggling to get my head around tidal acceleration. I get what is IS, I know how to calculate it, but what I'm not sure is how to apply it in a way that's meaningful to me.

So. If we took a stationary Earth (i.e. non rotating, tide-locked) and have the moon magically appear in orbit and applying the moon's ≈1.1e-06N tidal acceleraton, how would I work out what effect that has on the rotation speed (and thus period) of the Earth?

For, example, how would I calculate how long it would take for the Earth to become tide-locked to the moon (because that'd be the stable end-point, yes?) Or how long a day would be some time period (say, 4 billion years) after the moon appeared?
 
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Can you show how you derived that number for tidal acceleration?
 
##a=GM\frac{d}{R^3}##

where a = tidal acceleration, G is the gravitational constant (6.67384e-11), d is the diameter of the distorted body (in this case Earth, 2*6371000m), M is the mass of the distorting body (in this case the moon, 7.347E+22kg) and R is the distance between the two bodies (384399000m).

(It is only a first-order equation, as I understand, but sufficent to my purposes.)

I calculated the numbers via spreadsheet, which gave me 1.09996E-06N

I also found http://staff.washington.edu/aganse/europa/tides/tides.html, which gave consistent results (and in fact made me realize my spreadsheet have missed G being to the E-11...!)

(I could use the more complex equation on the linked page for greater accuracy - and may do later, but for the moment, first-order is enough for me to get a handle on the numbers.)
 
AotrsCommander said:
For, example, how would I calculate how long it would take for the Earth to become tide-locked to the moon (because that'd be the stable end-point, yes?)

That's impossible without additional information. You need the rate of energy dissipation due to the cyclic deformation of Earth. That mainly depends on offshore water and the geological structure of Earth. A rigid, perfectly elastic or superfluid Earth would never be tidal locked.
 
DrStupid said:
That's impossible without additional information. You need the rate of energy dissipation due to the cyclic deformation of Earth. That mainly depends on offshore water and the geological structure of Earth. A rigid, perfectly elastic or superfluid Earth would never be tidal locked.

Ah. Right.

I'm guessing there's no easy way to make an estimate of that without some significant mathamatical (or computer) modelling, is there?

I'd ask if we know what the rate is for Earth, but I assume it would be different for a non-rotating Earth, yes? (During my reading around astrophysics these last few weeks, I saw something on tidal locking that said Earth would eventually become tide-locked to the moon, albeit on a timescale past the end of the life of the sun, which I why I thought it might be possible to estimate.)
 
UC Berkely, December 16, 2025 https://news.berkeley.edu/2025/12/16/whats-powering-these-mysterious-bright-blue-cosmic-flashes-astronomers-find-a-clue/ AT 2024wpp, a luminous fast blue optical transient, or LFBOT, is the bright blue spot at the upper right edge of its host galaxy, which is 1.1 billion light-years from Earth in (or near) a galaxy far, far away. Such objects are very bright (obiously) and very energetic. The article indicates that AT 2024wpp had a peak luminosity of 2-4 x...

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