Stress–energy–momentum pseudotensor: Difference between revisions

 
===Verification===
Examining the 4 requirement conditions we can see that the first 3 are relatively easy to demonstrate:
#Since the Einstein tensor, <math>G^{\mu \nu}\,</math>, is itself constructed from the metric, so therefore is <math>t_{LL}^{\mu \nu} </math>
#Since the Einstein tensor, <math>G^{\mu \nu}\,</math>, is symmetric so is <math>t_{LL}^{\mu \nu} </math> since the additional terms are symmetric by inspection.