The condition at infinity gives . Matching the electric potential at gives
Consequently
This function is finite and differentiable at the origin. At the joining radius, both and match, giving and . Thus the electric field is continuous there as well as being conservative on each side. This is the potential of a uniform spherical source, with source coefficient .
Figure 1.
Continuous radial potential and inward electric field, normalized at the sphere boundary
. Details.

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