The quantum electromagnetic zero-point energy of a conducting spherical shell of radius r has been computed to be ΔE(r)0.09c2r. The physical reasoning is analogous to that used by Casimir to obtain the force between two uncharged conducting parallel plates, a force confirmed experimentally by Sparnaay and van Silfhout. However, while parallel plates are attracted together because of the zero-point energy, a conducting sphere tends to be expanded. Thus although relevant for the understanding of the quantum-mechanical zero-point energy, the result invalidates Casimir's intriguing model for a charged particle as a charged conducting shell with Poincar\'e stresses provided by the zero-point energy and a unique ratio for e²c independent of the radius.
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Timothy H. Boyer (1968) studied this question.
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