Deriving The Schwarzschild Solution - Simplifying The Components

Simplifying The Components

On each hypersurface of constant, constant and constant (i.e., on each radial line), should only depend on (by spherical symmetry). Hence is a function of a single variable:

A similar argument applied to shows that:

On the hypersurfaces of constant and constant, it is required that the metric be that of a 2-sphere:

Choosing one of these hypersurfaces (the one with radius, say), the metric components restricted to this hypersurface (which we denote by and ) should be unchanged under rotations through and (again, by spherical symmetry). Comparing the forms of the metric on this hypersurface gives:

which immediately yields:

and

But this is required to hold on each hypersurface; hence,

and

Thus, the metric can be put in the form:

with and as yet undetermined functions of . Note that if or is equal to zero at some point, the metric would be singular at that point.

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