
doi: 10.1007/bfb0069695
In Section 5 we introduced the notion of capacity of a body B in ℝ3 as follows: the capacity of B equals the amount of charge which, when distributed on B so as to produce equilibrium, yields a potential which is identically 1 on B. In other words, choose a measure µo on B such that Uµ o = 1 on B. Then the capacity of B = µo(B).
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