The electric potential and ion distributions within a cylinder and a sphere
at various salt concentration have been obtained analytically by solving t
he Poisson-Boltzmann equation in terms of series solutions. At a fixed rati
o of co-ion to counterion concentrations at the center of the aqueous core
(alpha < 1) or a given amount of added salt, the existence of the upper lim
it of the counterion concentration at the center has been observed regardle
ss of the surface charge density. It is a consequence of counterion condens
ation on the charged surface. The upper limit depends on the value of a and
increases rapidly when alpha --> 1. At high surface charge density, the co
unterions are strongly attracted to the surrounding of the surface. A bound
ary layer with the thickness inversely proportional to the surface charge d
ensity is formed. Both the effects of curvature and salt addition hence bec
ome unimportant, and the surface potential is primarily determined by the s
urface charge density.