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Randles–Sevcik equation

${\displaystyle i_{p}=0.4463\ nFAC\left({\frac {nFvD}{RT}}\right)^{\frac {1}{2}}}$

Or if the solution is at 25 °C:^[2]

${\displaystyle i_{p}=2.69\times 10^{5}\ n^{3/2}AC{\sqrt {Dv}}}$

• i_p = current maximum in amps
• n = number of electrons transferred in the redox event (usually 1)
• A = electrode area in cm²
• F = Faraday constant in C mol⁻¹
• D = diffusion coefficient in cm²/s
• C = concentration in mol/cm³
• ν = scan rate in V/s
• R = Gas constant in J K⁻¹ mol⁻¹
• T = temperature in K
• The constant with a value of 2.69×10⁵ has units of C mol⁻¹V^−1/2

For novices in electrochemistry, the predictions of this equation appear counter-intuitive, i.e. that i_p increases at faster voltage scan rates. It is important to remember that current, i, is charge (or electrons passed) per unit time. In cyclic voltammetry, the current passing through the electrode is limited by the diffusion of species to the electrode surface. This diffusion flux is influenced by the concentration gradient near the electrode. The concentration gradient, in turn, is affected by the concentration of species at the electrode, and how fast the species can diffuse through solution. By changing the cell voltage, the concentration of the species at the electrode surface is also changed, as set by the Nernst equation. Therefore, a faster voltage sweep causes a larger concentration gradient near the electrode, resulting in a higher current.

Using the relationships defined by this equation, the diffusion coefficient of the electroactive species can be determined. Linear plots of i_p vs. ν^1/2 provide evidence for a chemically reversible redox process vs the cases where redox causes major structural change in the analyte. For species where the diffusion coefficient is known (or can be estimated), the slope of the plot of i_p vs. ν^1/2 provides information into the stoichiometry of the redox process.

A more general investigation method is the plot of the peak currents as function of the scan rate on a logarithmically scaled x-axis. Deviations become easily detectable and the more general fit formula

${\displaystyle j_{max}^{\,ox,red}=j_{0}+A\cdot {\bigg (}{\frac {scan\,rate}{mV/s}}{\bigg )}^{x}}$

can be used.

In this equation ${\displaystyle j_{0}{}}$ is the current at zero scan rate at the equilibrium potential ${\displaystyle E_{0}}$. In the electrochemical lab experiment ${\displaystyle j_{0}{}}$ may be small but can nowadays easily be monitored with a modern equipment. For example corrosion processes may lead to a not vanishing but still detectable ${\displaystyle j_{0}{}}$. When ${\displaystyle j_{0}<<A}$ and x is close to 0.5 a reaction mechanism according to Randles Sevcik can be assigned.

An example for this kind of reaction mechanism is the redox reaction of ${\displaystyle \mathrm {Fe^{3+}/Fe^{2+}} }$ species as an analyte (concentration 5mM each species) in a highly concentrated (1M) background solution ${\displaystyle \mathrm {KNO_{3}} }$ on graphite electrode.

A more detailed plot with all fit parameters can be seen here.

• Online calculator for use of Randles–Sevcik equation:http://www.calctool.org/CALC/chem/electrochem/cv1

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