GR in Newtonian Limit: Understanding Weak Fields & Inequalities

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Discussion Overview

The discussion revolves around the implications of weak gravitational fields in the context of General Relativity, particularly focusing on the inequalities related to the components of the metric perturbation ##\bar{h}^{\mu \nu}## and the energy-momentum tensor ##T^{\mu \nu}##. Participants are examining the reasoning behind these inequalities and the conditions under which they hold.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant references a proof from Schutz's book that establishes the relationship ##\Box \bar{h}^{\mu \nu} = -16\pi T^{\mu \nu}## for weak gravitational fields and questions the derivation of the inequalities ##|\bar{h}^{00}|>>|\bar{h}^{0i}|>>|\bar{h}^{ij}|## based on the dominance of the components of ##T^{\mu \nu}##.
  • Another participant notes that without a source term, the solution for ##\bar{h}^{0i}## would be identically zero, suggesting that this implies ##\bar{h}^{0i}## must be small.
  • A subsequent reply questions the interpretation of ##\bar{h}^{0i}## being a constant and whether this would still satisfy the equality, indicating confusion about the implications of boundary conditions.
  • Another participant clarifies that if ##\bar{h}^{0i}## is a constant, it would not satisfy homogeneous boundary conditions and could be absorbed into the zeroth order metric.

Areas of Agreement / Disagreement

The discussion reflects some disagreement regarding the implications of boundary conditions on the components of ##\bar{h}^{\mu \nu}## and the interpretation of the absence of sources. Participants are exploring different perspectives without reaching a consensus.

Contextual Notes

There are unresolved assumptions regarding the nature of the boundary conditions and the implications of setting certain components of the energy-momentum tensor to zero. The discussion does not clarify how these assumptions affect the inequalities presented.

Silviu
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Hello! I am reading A first course in General Relativity by Schutz and at a point he proves that for a weak gravitational field and assuming ##\Lambda = 0## we have ##\Box \bar{h}^{\mu \nu} = -16\pi T^{\mu \nu}##. Leaving the notations aside, he says that for a weak gravitational field (and non-relativistic speeds) we have ##|T^{00|}>>|T^{0i}|>>|T^{ij}|## and this implies ##|\bar{h}^{00}|>>|\bar{h}^{0i}|>>|\bar{h}^{ij}|##. Can someone explain to me why do we have this last inequality? This is Chapter 8.3 in the second edition. Like for example, taking ##T^{0i}=0##, we get ##\Box\bar{h}^{0i}=0##. Why does this implies in any way that ##\bar{h}^{0i}## is very small? Thank you!
 
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The right-hand side is the source term. Without a source, your solution is identically ##\bar h^{0i} = 0## (assuming homogeneous boundary conditions).
 
Orodruin said:
The right-hand side is the source term. Without a source, your solution is identically ##\bar h^{0i} = 0## (assuming homogeneous boundary conditions).
Sorry I am a bit confused, if ##\bar{h}^{0i}## is a constant, doesn't the equality still holds?
 
If it is a constant it does not satisfy homogenous boundary conditions. Also, you could just absorb it into the zeroth order metric.
 

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