Could Expansion Explain Gravity Mathematically?

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The discussion explores the idea of whether gravity could be mathematically explained by the expansion of the universe, with participants noting that for this to hold, the Earth would need to expand rapidly while the Moon expands at a different rate. One perspective highlights that gravity can be viewed through General Relativity, where the acceleration of the Earth's surface creates an effect similar to gravity without relative motion. The conversation also touches on using accelerometers and theoretical definitions of proper acceleration to understand this relationship. A participant mentions a derivation linking gravity to Hubble's law, suggesting that the acceleration of gravity can be equated to the universe's expansion rate. Overall, the thread delves into the complex interplay between expansion and gravitational effects, seeking mathematical clarity.
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Could somebody show me mathematically why/why not gravity could/couldn't directly be caused by expansion -everything pulling/moving away from each other? When you are in a car, and you are accelerating, your body wants to stay where it was a moment before... Thus your head gets thrown back into the seat until you stop accelerating... Is this why we have gravity? Say a planets particles are moving away from each other, and that this is happening at an ever increasing rate... Is that why we have "gravity"? I wouldn't mind seeing it mathematically.

PS this time i am NOT posing a theory... I am just asking to see this mathematically. ;)
 
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Hi amaruq! :smile:

Well, yes it could, but the Earth would have to be expanding really fast for that to work, while the Moon would have to be expanding less fast …

so we'd notice that the Moon was getting smaller! :wink:
 
Thank you for going easy on me lol
 
Ok, the Earth obviously isn't exploding. But it's in fact the GR viewpoint that the surface of the Earth is accelerating, and that gravity is the effect of that acceleration. This is realized by curving space and time appropriately, so that there is acceleration without relative motion.
 
Ich said:
… there is acceleration without relative motion.

That doesn't make any sense …

how can we define acceleration without motion? :confused:
 
how can we define acceleration without motion?
Operationally, by using an accelerometer (e.g. force or displacement of a test mass). Theoretically, by defining a suitable "proper acceleration", i.e. the covariant derivative of the world line (not sure about the wording).
 
You can derive the inertial reaction of local matter to the acceleration of the universe (best estimates based upon a c velocity recession at the putative Hubble sphere of radius R and a flat universe, yields the isotropic acceleration is (c^2)/R (Smolin). With a little manipulation, G turns out to be (Hc/4(pi))(meters^2)/kgm

There have been several derivations on these boards - One chap did it using the acceleration from Hubbles law - i.e., equate the acceleration of gravity to the acceleration from the derivative of v= HR, and therefore dv/dt = H(dr/dt) = (H^2)R
I think he got it published in an electronics magazine. I have it around here somewhere. His derivation gave the result in perms of the density which is the same as what you get if you solve for G in the equation for critical density that comes out of the Einstein - de Sitter universe That is G =(3H^2)/8(pi)rho

Cheers
 
beautiful!
 
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