Mass & Stress-Energy Tensor: Why Not Explicitly?

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SUMMARY

The stress-energy tensor describes the flow of energy and momentum through space-time, but mass does not appear explicitly within it. Instead, "relativistic mass" is a component of the tensor, illustrating the relationship between energy and momentum. In special relativity, invariant mass is defined as the Lorentz invariant length of the energy-momentum 4-vector for isolated systems. In non-flat space-time, alternative concepts such as ADM mass, Bondi mass, or Komar mass are necessary to describe mass accurately.

PREREQUISITES
  • Understanding of stress-energy tensor in general relativity
  • Familiarity with energy-momentum 4-vector
  • Knowledge of invariant mass in special relativity
  • Concepts of ADM, Bondi, and Komar mass
NEXT STEPS
  • Study the derivation and applications of the stress-energy tensor in general relativity
  • Learn about the energy-momentum 4-vector and its implications in physics
  • Research the definitions and uses of ADM, Bondi, and Komar mass in curved space-time
  • Examine Taylor & Wheeler's "Space-time Physics" for insights on invariant mass
USEFUL FOR

Physicists, students of general relativity, and anyone interested in the intricacies of mass and energy in the context of space-time dynamics.

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Why doesn't mass show up in the stress-energy tensor explicitly?
 
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The stress energy tensor describes the flow of energy and momentum through space-time. Multiplying the stress-energy tensor by the velocity (4-velocity) of an observer gives the energy and momentum contained within a unit volume according to that observer.

"Relativistic mass" is another name for energy, and is one component of the stress-energy tensor, so in that sense "mass" could be considered to be one part of the stress-energy tensor. But it's not the whole tensor - since momentum and energy are intertwined in a similar manner to space and time. Energy is thus not a tensor, it's one component of a tensor. Mass in special relativity, in the sense of invariant mass, is defined as the Lorentz invariant length of the energy-momentum 4-vector - of an isolates system or particle. The "isolation" aspect is sometimes not stressed, but if you read the fine print in say, Taylor & Wheeler's "Space-time Physics", you'll see that it is assumed that one has an isolated system or an isolated particle when one talks about the invariant mass of the system or particle. If the system is isolated, and in flat space-time, one can find the invariant mass of the system from the stress-energy tensor by integrating the stress-energy tensor to find the total energy, the total momentum, and using the relationship E^2 - p^2 = m^2 (throw in factors of c as needed, if one is not using units where c=1).If one does not have flat space-time, one needs a different concept of mass. The details start to get technical here, I'll just mention that one might use the ADM mass, the Bondi mass, or the Komar mass, if one of them happens to apply. For some situations none of them apply.
 
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