Why the curvature of spacetime is related to momentum?

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SUMMARY

The discussion centers on the relationship between the curvature of spacetime and momentum within the framework of relativistic gravity theories. It establishes that the Einstein tensor, which describes spacetime curvature, and the stress-energy tensor, which represents mass and energy distribution, are both rank-2 tensors. The conversation emphasizes that momentum in this context refers to momentum density through a volume element in spacetime, rather than the conventional speed of particles. Additionally, it highlights the integration of energy density, energy flux, pressure, and mechanical stress as components of the energy tensor.

PREREQUISITES
  • Understanding of Einstein's General Relativity
  • Familiarity with tensor calculus
  • Knowledge of the stress-energy tensor
  • Concept of momentum density in physics
NEXT STEPS
  • Study the Einstein field equations in General Relativity
  • Learn about the properties and applications of rank-2 tensors
  • Explore the concept of energy-momentum tensors in relativistic physics
  • Investigate the implications of momentum density in curved spacetime
USEFUL FOR

Physicists, students of theoretical physics, and researchers interested in the intersection of gravity, momentum, and spacetime curvature will benefit from this discussion.

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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