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The electrical double layer forms at the electrode-electrolyte interface where solvated ions accumulate. Early models depicted it as two sheets of opposite charge. Advanced models like the Helmholtz layer describe a rigid layer of solvated ions near the electrode, while the Gouy–Chapman model adds a diffuse layer extending into the solution. The Stern model combines both structures.

The Stern model combines the rigid inner plane of ions from the Helmholtz layer with the diffuse outer layer from the Gouy–Chapman model. This hybrid approach better represents the actual electrode interface by showing how solvated ions organize in two distinct regions: a compact layer directly at the electrode surface and a dispersed layer extending into the bulk solution.

Overpotential, η, represents the deviation between the applied potential and the electrode potential. When overpotential is zero, no net current flows. As overpotential increases, current density increases according to the Butler–Volmer equation, which relates the rate of electron transfer to the driving force. This relationship determines whether oxidation or reduction dominates.

Current density measures the electron transfer rate per unit area at the electrode. When anodic current density exceeds cathodic current density, net current is anodic and oxidation occurs. Conversely, when cathodic current density surpasses anodic current density, net current is cathodic and reduction occurs. The net current density equals their difference.

The transfer coefficient, α, ranges from 0 to 1 and describes the activated complex structure during electron transfer. A value of 0 indicates the activated complex resembles reactants, while 1 indicates it resembles products. Empirical observations typically find α near 0.5. This parameter, combined with the Faraday constant and temperature, determines how current responds to overpotential changes.

The Galvani potential difference, Δϕ, represents the potential between bulk metal and solution. At equilibrium with no current drawn, this potential equals the electrode potential, E. When an external potential is applied and Δϕ deviates from E, net current flows. This deviation, called overpotential, drives oxidation and reduction reactions at the interface.

As ions attach to or leave the electrode surface, local ion concentrations change and create an electrical potential that opposes further reaction. Thermal motion disrupts this concentration gradient. Using excess supporting electrolytes minimizes these local concentration changes by maintaining uniform ionic strength throughout the solution, allowing more stable electrode behavior.