Two sensitizers, [Ru(bpy)₂(dcb)]²⁺ (RuC) and [Ru(bpy)₂(dpb)]²⁺ (RuP), where bpy is 2,2′-bipyridine, dcb is 4,4′-dicarboxylic acid-2,2′-bipyridine and dpb is 4,4′-diphosphonic acid-2,2′-bipyridine, were anchored to mesoporous TiO₂ thin films and utilized to sensitize the reaction of TiO₂ electrons with oxidized triphenylamines, TiO₂(e⁻) + TPA⁺ → TiO₂ + TPA, to visible light in CH₃CN electrolytes. A family of four symmetrically substituted triphenylamines (TPAs) with formal E^o(TPA^+/0) reduction potentials that spanned a 0.5 eV range was investigated. Surprisingly, the reaction followed first-order kinetics for two TPAs that provided the largest thermodynamic driving force. Such first-order reactivity indicates a strong Coulombic interaction between TPA⁺ and TiO₂ that enables the injected electron to tunnel back in one concerted step. The kinetics for the other TPA derivatives were non-exponential and were modelled with the Kohlrausch–William–Watts (KWW) function. A Perrin-like reaction sphere model is proposed to rationalize the kinetic data. The activation energies were the same for all of the TPAs, within experimental error. The average rate constants were found to increase with the thermodynamic driving force, consistent with electron transfer in the Marcus normal region.