Metric in SR: \eta^{\alpha \beta}=\eta_{\alpha \beta}?

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Discussion Overview

The discussion revolves around the relationship between the metric components \(\eta^{\alpha \beta}\) and \(\eta_{\alpha \beta}\) in different coordinate systems, specifically questioning whether this equality holds in all coordinate systems or is limited to inertial ones. The scope includes theoretical considerations of spacetime metrics in special relativity.

Discussion Character

  • Debate/contested

Main Points Raised

  • One participant questions whether \(\eta^{\alpha \beta}=\eta_{\alpha \beta}\) is valid in all coordinate systems or only in inertial coordinate systems.
  • Another participant notes that in non-inertial coordinate systems, the symbol \(g_{\alpha \beta}\) is used instead of \(\eta_{\alpha \beta}\), indicating that \(g_{\alpha \beta}\) is generally not equal to \(g^{\alpha \beta}\), which is its inverse.
  • A further contribution states that \(g^{\alpha \beta}=g_{\alpha \beta}\) implies an orthonormal coordinate basis, which is said to correspond only to inertial coordinates in flat spacetime.

Areas of Agreement / Disagreement

Participants express differing views on the conditions under which \(\eta^{\alpha \beta}=\eta_{\alpha \beta}\) holds, indicating that the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

The discussion highlights the distinction between inertial and non-inertial coordinate systems and the implications for the metric components, but does not resolve the underlying assumptions or definitions that may affect these relationships.

dEdt
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Does [tex]\eta^{\alpha \beta}=\eta_{\alpha \beta}[/tex] in all coordinate systems or just inertial coordinate systems?
 
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dEdt said:
Does [tex]\eta^{\alpha \beta}=\eta_{\alpha \beta}[/tex] in all coordinate systems or just inertial coordinate systems?

For non-inertial coordinate systems, the symbol [itex]g_{\alpha \beta}[/itex] is used instead of [itex]\eta_{\alpha \beta}[/itex]. And in general, [itex]g_{\alpha \beta}[/itex] is unequal to [itex]g^{\alpha \beta}[/itex]. [itex]g^{\alpha \beta}[/itex] is the inverse of [itex]g_{\alpha \beta}[/itex].

Here's an example: In polar coordinates [itex]t, \rho, \phi, z[/itex],

[itex]g_{tt} = 1[/itex]
[itex]g_{zz} = -1[/itex]
[itex]g_{\rho \rho} = -1[/itex]
[itex]g_{\phi \phi} = -\rho^2[/itex]

[itex]g^{tt} = 1[/itex]
[itex]g^{zz} = -1[/itex]
[itex]g^{\rho \rho} = -1[/itex]
[itex]g^{\phi \phi} = -\frac{1}{\rho^2}[/itex]
 
[itex]g^{\alpha \beta}=g_{\alpha \beta}[/itex] means that the coordinate basis is orthonormal, which only corresponds to 'inertial coordinates' (Minkowski coordinates) in flat spacetime.
 
Thanks guys.
 

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