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Cyclic voltammetry

Method of analyzing electrochemical reactions

  • 12 min read
  • 5 chapters

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Through Electrochemistry, Electrode potential and Electric current

Experimental method

In cyclic voltammetry (CV), the electrode potential is ramped linearly versus time in cyclical phases. The rate of voltage change over time during each of these phases is known as the scan rate (V/s). In a standard three-electrode cell, the potential is measured between the working electrode and the reference electrode, while the current is measured between the working electrode and the counter electrode. These data are plotted as current density (j, mA/cm2) versus potential (typically corrected for Ohmic/iR drop) (E, V). During the initial forward scan from t0 to t1, an increasingly oxidative (positive) potential is applied, and the anodic (positive) current increases over this time period due to the charging of the electric double layer. The spike in anodic (positive) current observed between t0 and t1 is due to the oxidation of the analyte in the solution when the correct potential is reached. The current decreases after the initial spike as the concentration of oxidable analyte is depleted near the surface of the working electrode due to mass transport limitations.

The graph often has a characteristic "duck-like" shape. Comparing the parts of the oxidation and reduction graph portions allows determination of many electrochemical parameters. For example, if the redox couple is reversible, then during the reverse scan (from t1 to t2), the oxidized analyte will start to be re-reduced, giving rise to a cathodic current of opposite polarity. The more reversible the redox couple is, the more similar the oxidation peak will be in shape to the reduction peak. The difference in potential between when the maximum current is measured in the two directions is the redox potential.

If the electron transfer at the working electrode surface is fast and the current is limited by the diffusion of analyte species to the electrode surface, then the peak current will be proportional to the square root of the scan rate. This relationship is described by the Randles–Sevcik equation. In this situation, the CV experiment only samples a small portion of the solution, i.e., the diffusion layer at the electrode surface.

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