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

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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.