The current density

of a species
B in a given point of the solution is obtained by multiplying the flux density of that
species at the given point by the
Faraday constant
and by the
charge number
of the species:
where

is a vector which indicates the direction in which the charges transported by the
species
B flow and which gives the number of these charges going through a plane oriented perpendicular
to the vector, divided by time and by area, and

is the flux density of a minor
constituent of the solution with respect to a fixed frame of reference.
Source:
PAC, 1981, 53, 1827
(Nomenclature for transport phenomena in electrolytic systems)
on page 1833