pellman
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Why must we have g_{\mu\nu}=g_{\nu\mu}? What are the physical consequences if this did not hold?
The discussion centers on the necessity of having a symmetric metric tensor, denoted as g_{\mu\nu} = g_{\nu\mu}, in the context of general relativity. It is established that a nonsymmetric metric would not yield any physical consequences and is merely a convention for mathematical consistency. The metric tensor determines the interval between events in four-dimensional spacetime, and any nonsymmetric component could be transformed into a symmetric one. Additionally, the presence of torsion is incompatible with a symmetric metric, which raises questions about observable effects in physical theories.
PREREQUISITESThis discussion is beneficial for physicists, mathematicians, and students of general relativity who seek to deepen their understanding of metric properties and their implications in theoretical physics.
pellman said:Why must we have g_{\mu\nu}=g_{\nu\mu}? What are the physical consequences if this did not hold?