The previous system of equations, Eqns. 5 and
6, apply only to the electrolyte within the pores.
For porous materials, one must be explicit whether the flux equation is
for the pore space or for the
pore space and solid structure combined (bulk).
In this study, a bulk formulation is used.
For the electro-diffusive flux in Eqn. 5, it has been
shown previously that the
diffusion coefficient Di that appears in Eqn. 5 is the
bulk microstructural diffusion coefficient (
= Di), and is
independent of the pore solution composition [7]; interactions
within the pore solution are accounted for in the
remaining terms in the equation.
For a porous material with a formation
factor F, the bulk microstructural diffusion coefficient appearing in
Eqn. 5
is proportional to the self-diffusion coefficient
Ds [7]:
The self-diffusion coefficient of an ionic species is its diffusion
coefficient in water in the limit of infinite dilution [30].
Equation 7 reflects the fact that the bulk microstructural
diffusion coefficient
depends on the species i.
It is important to realize that
is not the apparent
Fickian diffusion coefficient Dai. Rather, it simply characterizes the
diffusion of an ionic species in the absence of electrostatic
interactions.
Use of the formation factor originated in geological research and has
been defined as the ratio of the conductivity of a pore solution
p to the bulk conductivity
b of a insulating
porous material filled with
that pore solution [31]:
In principle, the formation factor is a constant, at constant porosity and tortuosity (absence of chemical reaction with solid microstructure), for a particular porous material, and is independent of ionic species [7]. Since the self-diffusion coefficient of an ionic species is also a constant (at constant temperature), the flux equation for the N species has been reduced from a system of N equations with N apparent diffusion coefficients, as shown in Eqn. 5, to a system of N equations with only a single parameter, the formation factor.
In practice, determining the formation factor must be performed with some care. In porous systems containing sufficient surface charge, the ratio of the pore solution conductivity to the bulk conductivity will depend on the pore solution concentration [32,33]. This concentration dependence is due to a surface conduction contribution to the measured conductivity [34,35]. In principle, this effect can be isolated, yielding the true microstructural formation factor that is required in the equations used here.