We determine the local charge dynamics of a z−z electrolyte embedded in a
varying-section channel. By means of an expansion based on the length scale
separation between the axial and transverse direction of the channel, we derive
closed formulas for the local excess charge for both, dielectric and conducting
walls, in 2D (planar geometry) as well as in 3D (cylindrical geometry). Our
results show that, even at equilibrium, the local charge electroneutrality is
broken whenever the section of the channel is not homogeneous for both
dielectric and conducting walls as well as for 2D and 3D channels.
Interestingly, even within our expansion, the local excess charge in the fluid
can be comparable to the net charge on the walls. We critically discuss the
onset of such local electroneutrality breakdown in particular with respect to
the correction that it induces on the effective free energy profile experienced
by tracer ions