The maximum theoretical efficiency of a fuel cell is governed by the ratio of the change in Gibbs free energy (\(\Delta G\)) to the change in enthalpy (\(\Delta H\)) of the electrochemical reaction. This is expressed as \(\eta_{thermo} = \frac{\Delta G}{\Delta H}\). Crucially, fuel cells are not heat engines and are therefore not constrained by the Carnot efficiency limit, allowing for significantly higher theoretical conversion efficiencies.

















