A Dirac's "GTR" Eq (27.4): how momentum ##p^\mu## varies

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Dirac's "General Theory of Relativity" outlines the derivation of Einstein's field equations from action principles, particularly in chapters 26-30, where he addresses the case of dust with a specific momentum density definition. The discussion centers on Dirac's Eq. (27.4), which describes how momentum varies under arbitrary displacements, but lacks a clear derivation. Participants express confusion over the assumptions made regarding the divergence of velocity and momentum fields, particularly in relation to the non-constancy of mass density. The conversation highlights the need for a more rigorous approach to understanding the implications of curved spacetime and the conservation laws involved. Overall, the thread seeks clarity on the derivation of Eq. (27.4) and its foundational assumptions.
  • #51
I just noticed that Dirac actually derives the Lie derivative in chapter 30, on page 60. Here he calculates the variation ##\delta g_{\mu\nu} = -\mathcal{L}_b \, g_{\mu\nu}## in order to make the reverse argument that I provided in Post #34. There, to calculate the ##\delta p^\mu## in Dirac's (27.4), I took a point transformation and considered it as a coordinate transformation. In chapter 30, Dirac has a coordinate transformation, derives the Lie derivative ##-\mathcal{L}_b \, g_{\mu\nu}##, and then considers it as a point transformation in order to find ##\delta g_{\mu\nu}##.

The odd thing is, since he does this is chapter 30, he could have done it in chapter 27 to give a solid proof of (27.4).