Why the curvature of spacetime is related to momentum?

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Discussion Overview

The discussion revolves around the relationship between the curvature of spacetime and momentum within the context of relativistic theories of gravity. Participants explore how mass and momentum are interconnected in different reference frames and how these concepts relate to the Einstein tensor and the stress-energy tensor.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that any relativistic theory of gravity must relate to momentum, as mass in one frame corresponds to mass and momentum in another frame.
  • It is noted that the Einstein tensor, which describes spacetime curvature, is a rank-2 tensor, implying that the stress-energy tensor must also be a rank-2 tensor, with its time-space components resembling momentum in Newtonian mechanics.
  • One participant emphasizes that the momentum discussed is not about the speed of a particle through space but rather momentum density through a volume element in spacetime.
  • A later reply corrects the previous statement, clarifying that momentum density is through a volume element in space, providing a mathematical formulation for calculating total momentum and angular momentum based on energy-momentum distribution.
  • Another participant expands the discussion by mentioning that not only momentum but also energy density, energy flux, pressure, and mechanical stress are components of the energy tensor, which encapsulates the density and flux of energy and momentum.

Areas of Agreement / Disagreement

Participants express various viewpoints on the relationship between spacetime curvature and momentum, with some clarifications and corrections made, but no consensus is reached on the overall implications or interpretations of these relationships.

Contextual Notes

Limitations include potential misunderstandings regarding the definitions of momentum density and the mathematical treatment of tensors, as well as the dependence on specific reference frames and simultaneity considerations.

Brucezhou
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It must be for a relativistic theory of gravity. We know that gravity is related to mass, and mass in one frame is mass and momentum in another frame. So any relativistic theory of gravity must be related to momentum.
 
The Einstein tensor, which describes the curvature of spacetime, is a rank 2 tensor, so the stress-energy tensor that appears in the field equations (and describes the distribution of mass and energy throughout spacetime) must also be a rank-2 tensor. It just so happens that the "time-space" components of this tensor look a lot like what we normally think of as momentum in Newtonian mechanics.

It should also be noted that this momentum is not about how fast a particle travels through space (with respect to some observer), but rather, it is momentum density through a volume element in spacetime.
 
Psychosmurf said:
It should also be noted that this momentum is not about how fast a particle travels through space (with respect to some observer), but rather, it is momentum density through a volume element in spacetime.

Slight correction here but it's through a volume element in space. For example in flat space-time if we have a distribution with energy-momentum ##T^{\mu\nu}## and define a slicing of space-time relative to a family of inertial observers with global inertial frame ##(t,\vec{x})## based on their global simultaneity slices ##\Sigma_{t}## (which, as per standard simultaneity, is ##t = \text{const.}##) then ##P^{i}(t) = \int _{\Sigma_t}T^{0i}(t,\vec{x})d^{3}x## is the total momentum of the distribution. Similarly the total angular momentum of the source is ##S^{i}(t) = \sum _{j,k}\epsilon^{ijk}\int _{\Sigma_t}x^{j}T^{0k}(t,\vec{x})d^{3}x##.
 
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Not just momentum but also energy density, energy flux, pressure, and mechanical stress. In relativity all those things are different components of a single entity called "The tensor of density and flux of energy and momentum" - the "energy tensor" for short.
 

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