A rigorous model is presented for diffusive transport of ionic surfact
ants to an adsorbing interface. The proposed model considers both the
diffusion and migration of surfactant, counterions, and background ele
ctrolyte in the electric field that develops as the charged surfactant
adsorbs at an interface. The transient electrical double-layer struct
ure arising from specific adsorption of the surfactant is calculated b
y solving the coupled Nernst-Planck and Poisson equations in the bulk
phase using a Frumkin constitutive relation for the interfacial bounda
ry condition. The resulting transient double-layer model is valid over
all time scales and for interfacial potentials and background electro
lyte concentrations of any magnitude. Therefore, the proposed model is
more general than previously derived ''quasiequilibrium'' models of i
onic surfactant transport to the interface that require instantaneous
equilibrium potentials in the double layer.(1-4) We compare results fr
om the proposed ionic surfactant transport model to results from the s
tandard Ward-Tordai model for nonionic surfactants adsorbing at a flui
d/fluid interface. For low concentrations of strongly adsorbing surfac
tant, in the absence of background electrolyte, electrostatic effects
decrease the equilibrium adsorption of surfactant by an order of magni
tude. Correspondingly, the time required for equilibration of the inte
rface is decreased. When the transient adsorption is scaled to elimina
te differences due solely to different equilibrium adsorption, we disc
over that the rate of diffusion-limited transport of an ionic surfacta
nt is decreased by an order of magnitude compared to that of an equiva
lent nonionic surfactant. Addition of nonadsorbing background electrol
yte, increasing surfactant concentration, or weaker adsorption of surf
actants decreases the electrostatic effects. A simple quasiequilibrium
model that assumes a double layer in instantaneous equilibrium with a
n electroneutral bulk solution is also developed. Comparison of this q
uasiequilibrium model to the full transient model shows that, for a ty
pical surfactant (e.g., sodium dodecyl sulfate) adsorbing at the water
/air interface, differences between the full transient model and quasi
equilibrium model occur only at times inaccessible to current dynamic
surface tension techniques.