J Baez' The meaning of Einstein's Equations

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Discussion Overview

The discussion centers around J. Baez's paper on the meaning of Einstein's equations, specifically focusing on the interpretation of the stress-energy tensor and its implications regarding momentum and pressure in spacetime. Participants are exploring the theoretical aspects of this interpretation and seeking clarification on specific statements made in the paper.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • DaTario seeks to understand how the flow of momentum relates to pressure as described by Baez, particularly in the context of the stress-energy tensor.
  • One participant suggests visualizing a box of particles moving in one direction to illustrate how momentum flows and contributes to pressure, indicating a relationship between momentum transport and pressure components.
  • A hint is provided regarding the transformation of the stress-energy tensor, suggesting that participants consider how tensors behave under boosts and transformations.
  • DaTario expresses that the information available on Baez's website is similar to that in the paper, indicating a desire for deeper understanding beyond what is provided in those sources.

Areas of Agreement / Disagreement

The discussion does not reach a consensus on the proof of the relationship between momentum flow and pressure, and participants express varying levels of understanding and need for clarification on the topic.

Contextual Notes

There are unresolved aspects regarding the mathematical transformations of the stress-energy tensor and the implications of these transformations for understanding pressure and momentum flow. The discussion reflects a need for further exploration of these concepts.

DaTario
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J Baez' "The meaning of Einstein's Equations"

Hi All,

I am trying to study the paper of Jonh Baez in the july editon of Am. J. of Phys. on the meaning of Einstein's equation.

At a given point he says:

"The components of [itex]T_{\alpha \beta}[/itex] (stress-energy tensor) say how much momentum in the [itex]\alpha[/itex] direction is flowing in the [itex]\beta[/itex] direction through a given point of space-time, where [itex]\alpha \beta[/itex] = t, x, y, z. The flow of x-momentum in the x-direction is the pressure in the x-direction denoted [itex]P_x[/itex], and similarly for y and z. It takes a while to figure out why pressure is really the flow of momentum, but its eminently worth doing."

Does anybody know how to prove this last statement.


Thank you in advance



DaTario
 
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Thank you for the answer, but in his site there is the same information as in the paper I have in hands.

Best Regards

DaTario
 
DaTario said:
Hi All,

I am trying to study the paper of Jonh Baez in the july editon of Am. J. of Phys. on the meaning of Einstein's equation.


DaTario


It's a bit hard to read your post since you haven't closed the latex tags properly. The latex support was added on to an existing system, so that [.itex] does not close with [.\itex] as one would expect, but rather with [./itex].
(Remove the dots!).

In answer to your question, imaginie a small box with a swarm of particles in it which move back in forth in only the x direction.

The particles will be transporting x momentum in both directions across the box. The stress energy tensor of this box will be represented by the energy density of the particles, plus an additional diagional component which represents the x- pressure.

If you are familar with how tensors transform, start with the stress-energy tensor of a fluid at rest, which is easy (it has only one term, the energy density T_00, or if you prefer T^00).

Then boost it so it consists of a fluid and/or swarm of particles moving in the +x direction.

hint: the transform is [tex] T^{cd} = T^{ab} L^c{}_a L^d{}_b[/tex]

where [itex]L^i{}_j[/itex] is the transformation matrix, the same one that you would transform any 4-vector with, i.e.

[tex] x^b = x^a L^b{}_a<br /> [/itex]<br /> <br /> [end hint]<br /> <br /> Boost your original tensor again in the opposite direction, so it represents a fluid and/or swarm of particles moving in the -x direction.<br /> <br /> Add the two boosted tensors together - you'll get a tensor that represents the situation I described, where particles move in both directions.[/tex]
 
DaTario said:
Thank you for the answer, but in his site there is the same information as in the paper I have in hands.

Best Regards

DaTario

I thought it might be a good idea to put it into the hands of the rest of us.
 
Am. J. of Phys. july edition (printed version) 2005. pg 644.

Thank you for the explanation. It was really enlightening.

Best Regards,

DaTario
 

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