Abstract
The general solution in closed form, including all the static axisymmetric solutions of Weyl, is presented in the canonical coordinates
ρ
and
z
of his line element. This general solution is constructed from an arbitrary function
f
(
z
), which coincides with his potential function along the axis of symmetry. To illustrate how the solution may be used, a particular function
f
, one resulting from a Newtonian solution, is used to find both the potential function and its associated function in the line element.
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6 articles.
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