Would Newton's shell theorem prevent binary planet systems?

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SUMMARY

The shell theorem, which states that a spherically symmetric mass exerts no net gravitational force on objects inside it, does not support the formation of binary planet systems with two equal masses. The discussion highlights that while the shell theorem applies to spherically symmetric distributions, binary planets do not meet this criterion due to their external gravitational interactions. The example of Pluto and Charon is noted as a binary system, but it is emphasized that the gravitational dynamics differ significantly from the conditions required by the shell theorem.

PREREQUISITES
  • Understanding of Newton's shell theorem
  • Knowledge of gravitational forces and mass distribution
  • Familiarity with binary systems in astrophysics
  • Concept of spherically symmetric distributions
NEXT STEPS
  • Research the implications of Newton's shell theorem in astrophysics
  • Explore the dynamics of binary planet systems and their formation
  • Study gravitational interactions in non-spherically symmetric systems
  • Investigate the characteristics of Pluto and Charon as a binary system
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Astronomers, astrophysicists, and students studying gravitational dynamics and binary systems will benefit from this discussion.

DarkStar42
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Would the shell theorem prevent a binary planet system, with two ideally equal masses, structure etc?
 
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The shell theorem is true, and there are probably binary planets around (and Pluto/Charon are similar to a binary planet). Clearly not.

Why would you expect that?
 
mfb said:
The shell theorem is true, and there are probably binary planets around (and Pluto/Charon are similar to a binary planet). Clearly not.

Why would you expect that?
I meant two planets of the same mass and make up(ideally).

7UMDB63.jpg


take these two binary planets, of equal construction(green+red). In the shell theorem, the green part of the planet, would have no gravitational pull on the red part of the planet, so there is nothing to hold the red part on...and so on.
 

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The shell theorem holds for a spherically symmetric distribution. Your setup is not spherically symmetric.
 
Orodruin said:
The shell theorem holds for a spherically symmetric distribution. Your setup is not spherically symmetric.
yes, I think you're correct...I've jumped the gun again...:cry:
 
Orodruin said:
The shell theorem holds for a spherically symmetric distribution. Your setup is not spherically symmetric.
or maybe I'm right(probably not...)...surely if the shell theorem holds for a whole sphere, it would also hold for a symmetrical two body system...?
 
yes,if I'm right; in the process of the formation of a binary planet system, from dust, one of the planets, would have to be smaller than the other, by some factor, I would guess.
 
You are confusing the term "symmetric" (by which you mean a mirror symmetry) with "spherically symmetric" (which requires dependence on nothing but distance from a center point, no angular dependence). The latter is much more restrictive, and is the only time the shell theorem applies.
 
Ken G said:
You are confusing the term "symmetric" (by which you mean a mirror symmetry) with "spherically symmetric" (which requires dependence on nothing but distance from a center point, no angular dependence). The latter is much more restrictive, and is the only time the shell theorem applies.
ok so I may well have jumped the gun, but is there still something to the idea?

So maybe the shell theorem wouldn't apply exactly, but just enough to cause a binary system, to need to have two different sized planets?
 
  • #10
ok, there's probably next to nothing in the idea...
 
  • #11
It doesn't apply at all to the whole system, not even approximately. You can use it for the planets separately. For a test mass on the surface of a planet, you can calculate the gravitational force from that planet and the force from the other planet with it. The former will win by a large margin.
 
  • #12
DarkStar42 said:
or maybe I'm right(probably not...)...surely if the shell theorem holds for a whole sphere, it would also hold for a symmetrical two body system...?
Your saying that because the second planet is outside the first planet, according to the shell theorem, the second planet exerts no gravitational force on the first planet, right? But in the shell theorem, the mass outside the shell is counter-balanced by the mass of the shell on the opposite side - it's spherically symmetric. In the two planet example, there's no mass on the other side of the first planet to counter-balance the gravitational attraction of the second planet.
 

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