“…Since the generalized forces are functions of the corresponding generalized coordinates, the potential E must be the state function of independent state variables Q and A, i.e., E(Q, A). It happens in the majority of problems in electrostatics, e.g., in the case of a spherical conductive body immersed in a dielectric medium, but it does not happen in the case of a double electric layer [5,6], where the variables A and Q = qA are not independent, which does not satisfy the recipe for obtaining Maxwell relations [8], as discussed earlier [5][6][7]9,10]. Actually, in a double electric layer the potential E is a single-value function of the surface charge density q, i.e., q = kE, and q is independent of A just as it takes place in a parallel-plate capacitor [5,6].…”