  A nanopores's response to an electrical potential drop is characterized by
its electrical conductance, \tilde{G}. It has long been thought that at low
concentrations, the conductance is independent of the electrolyte
concentration, \tilde{c}_0, such that \tilde{G} ~ \tilde{c}_0^0. It has been
recently demonstrated that surface charge regulation changes the dependency to
be \tilde{G} ~ \tilde{c}_0^{\alpha} where the slope typically takes the values
\alpha = 1/3 or 1/2. Yet, experiments have observed slopes of 2/3 and 1
suggesting that additional mechanisms, such as convection and slip-lengths,
appear. We show that the inclusion of convection doesn't vary the slope, while
the inclusion of a slip length doubles the slope value. Here, we elucidate the
interplay between surface charge regulation, convection, and slip-lengths. We
show that when all effects are accounted for \alpha can take any value between
0 and 1. This result is of utmost importance in designing any
electro-kinetically driven nanofluidic system characterized by its conductance.
