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We develop a general formalism for including nonelectrostatic interactions, such as excluded volume interactions, in the Poisson−Boltzmann (PB) equation. The resulting theory can be applied to any boundary condition and is as easy to numerically implement as the original PB equation. As a specific example, we combine the PB equation with the Boublik−Mansoori−Carnahan−Starling equation of state to model charged hard-sphere systems. This theory is applied to a charged sphere immersed in a salt solution, and the electric field and ion distribution about the sphere are computed.
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Lue et al. (1999) studied this question.
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