“…Assuming that for a thin‐wall pipette (e.g., RG≤2, RG= r g / r , where r g is the outer radius of the glass insulator and r the inner radius, that is, the radius of the interface) the micro‐ and nano‐ITIES are essentially uniformly accessible, and the potential dependence of the rate constant follows the Butler–Volmer equation as corroborated by the excellent agreement between theory and experimental voltammograms, the standard rate constant ( k 0 ), and the charge‐transfer coefficient ( α ), which can be determined by fitting an experimental voltammogram to a theoretical equation 8. Although several groups have reported kinetic measurements of IT reactions at micro‐ITIES,1e many IT reactions are too fast to be probed with a micro‐ITIES under steady‐state conditions. The nano‐ITIES supported at nanopipettes should be advantageous because the mass‐transport rate can be enhanced according to Equation (1),5 where m 0 is the mass‐transport rate, D the ion diffusion coefficient, and r app the effective radius.…”