Static, Isotropic Metric: Dependence on x & dx

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SUMMARY

The discussion centers on the properties of a Static, Isotropic metric as described in Weinberg's book, specifically its dependence on variables ##x## and ##dx## through rotational invariants such as ##dx^2, x \cdot dx, x^2##, and functions of ##r \equiv (x \cdot x)^{1/2}##. It is established that while ##dx^2## appears to depend on angles ##\theta## and ##\varphi##, it remains invariant under rotations due to the nature of distances being invariant. The invariance is attributed to the coordinated transformation of angles during rotation, which preserves the value of ##dx^2##.

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davidge
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In Weinberg's book it is said that a Static, Isotropic metric should depend on ##x## and ##dx## only through the "rotational invariants" ##dx^2, x \cdot dx, x^2## and functions of ##r \equiv (x \cdot x)^{1/2}##. It's clear from the definition of ##r## that ##x \cdot dx## and ##x^2## don't depend on the angular displacement. What I don't understand is why ##dx^2## is invariant under rotations, since it's the "pure" metric when written in spherical coordinates, and so it depends on the usual angles ##\theta## and ##\varphi##.
 
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davidge said:
What I don't understand is why ##dx^2## is invariant under rotations

Because it's a distance (an infinitesimal one, but still a distance), and distances are invariant under rotations.

davidge said:
it depends on the usual angles ##\theta## and ##\varphi##.

Formally, yes, but if you do a rotation of the coordinates, you will find that ##\theta## and ##\varphi## change in concert in such a way as to leave ##dx^2## invariant.
 
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