Opposite Side of GR: Is it Possible?

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Discussion Overview

The discussion explores the concept of an "opposite side" of General Relativity (GR), specifically considering regions in space with lower than average matter density and the implications for gravity and light behavior in such areas. Participants examine whether gravity could be perceived as repulsive in these underdense regions and how this might be described mathematically or conceptually, particularly through Newtonian approximations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that in regions of lower density, gravity could be perceived as repulsive, suggesting that light would bend away from these areas.
  • Others argue that gravity in such regions would be weaker or absent rather than repulsive, and that light would bend less inward rather than outward.
  • A participant suggests that while the original idea may hold in a Newtonian approximation, it does not imply true repulsion but rather a differential effect where masses experience stronger gravity away from the underdense region.
  • Another participant compares the situation to electric charge distribution, indicating that a hollow sphere with evenly distributed charge results in zero field inside, implying a need for an "antigravitating" entity to achieve a similar effect in gravity.
  • Some participants clarify that the analogy of a charged sphere is not appropriate, suggesting instead a model involving a diffuse fluid with positive charge and a bubble of no charge, discussing the effects on a negative test particle near this bubble.
  • There is acknowledgment that the Newtonian analog simplifies the situation due to the absence of positive and negative masses, and that the behavior of particles outside the low density bubble is crucial to understanding the dynamics involved.

Areas of Agreement / Disagreement

Participants express differing views on the nature of gravity in low density regions, with no consensus reached on whether gravity can be considered repulsive or merely weaker. The discussion remains unresolved regarding the appropriate analogies and implications of these concepts.

Contextual Notes

Participants note limitations in their analogies and assumptions, particularly regarding the behavior of gravity in relation to electric charge and the implications of Newtonian versus relativistic frameworks.

zonde
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"Opposite side" of GR

I am trying to consider kind of "opposite side" of GR.
Let's consider some area in space where density of matter is less then average density of matter across the universe and in every direction average density of matter can be viewed as being higher than at this particular place.
Then gravity in this area would be repulsive, right? Light will bend away from that area and matter will "fall out" of this place.

Is it possible to find some description of that place similar to GR description for gravitating body. Let's say we make necessary assumptions about symmetry of this situation.
Something like smoothing out of topology as you approach center contrary to bending?
 
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Then gravity in this area would be repulsive, right?
No, it would be weaker or absent.
I think you intend to express the underdensity as repulsive gravity superimposed on the attractive gravity background. You can do that in the Newtonian approximation (where superposition works), but the effect would never be light bending outwards. It will bend less inwards, that's all.
 


I think in Newtonian approximation, the OP idea can be correct, in some sense. Not that gravity is repulsive inside the low density bubble, but that the bubble acts, to some extent, as a repulsor. A mass passing near the bubble will experience stronger gravity on its side away from the bubble, so will bend away from the bubble.
 


PAllen said:
I think in Newtonian approximation, the OP idea can be correct, in some sense. Not that gravity is repulsive inside the low density bubble, but that the bubble acts, to some extent, as a repulsor. A mass passing near the bubble will experience stronger gravity on its side away from the bubble, so will bend away from the bubble.
It seems that in Newtonian approximation it should not work.
Look we can compare superposition of gravity sources with electric charge. Electric charge inside sphere where charge is evenly distributed on the surface of sphere is zero. Now as we add bigger and bigger charged surfaces of spheres (up to infinity) they would still not change field inside hollow sphere - still zero.

So with Newtonian approximation we would require some entity that possesses opposite charge of gravity i.e. antigravitating entity.
 


zonde said:
It seems that in Newtonian approximation it should not work.
Look we can compare superposition of gravity sources with electric charge. Electric charge inside sphere where charge is evenly distributed on the surface of sphere is zero. Now as we add bigger and bigger charged surfaces of spheres (up to infinity) they would still not change field inside hollow sphere - still zero.

So with Newtonian approximation we would require some entity that possesses opposite charge of gravity i.e. antigravitating entity.

You misundestood my description. A charged sphere is not the right EM analog. The right analog would be a diffuse fluid with positive charge distributed throughout, and a bubble of no charge. What happens as a negative test particle (that, for some reason, cannot be neutralized by picking up positive charges) passes near the bubble?

The key point, in my original post, is what happens to a particle passing near the low density bubble, *outside* the bubble, not inside the bubble.

However, the Newtonian analog, as described, is simpler because of the absence of positive and negative masses. It should work as described. Read the scenario more carefully.
 


PAllen said:
You misundestood my description. A charged sphere is not the right EM analog. The right analog would be a diffuse fluid with positive charge distributed throughout, and a bubble of no charge. What happens as a negative test particle (that, for some reason, cannot be neutralized by picking up positive charges) passes near the bubble?

The key point, in my original post, is what happens to a particle passing near the low density bubble, *outside* the bubble, not inside the bubble.

However, the Newtonian analog, as described, is simpler because of the absence of positive and negative masses. It should work as described. Read the scenario more carefully.
Yes you are right, charged sphere is not the right analog.
If I have not made some error then it seems that even inside the bubble is different then in charged sphere analog.
 

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