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Chemistry · Ch 5 — Electrochemistry

Gibbs energy of cell reactions and cell potential

5.8.1

Gibbs energy of cell reactions and cell potential

The electrical work done in a galvanic cell is the electricity (charge) passed multiplied by the cell potential:

Electrical work=amount of charge passed×cell potential\text{Electrical work} = \text{amount of charge passed} \times \text{cell potential}

The charge of one mole of electrons is FF coulombs. For a cell reaction involving nn moles of electrons, the charge passed is nFnF coulombs, and hence

electrical work=nFEcell\text{electrical work} = nFE_{cell}

W. Gibbs, in 1878, concluded that the electrical work done in a galvanic cell is equal to the decrease in Gibbs energy, −ΔG-\Delta G, of the cell reaction. It then follows that

Electrical work=−ΔG,and thus−ΔG=nFEcell\text{Electrical work} = -\Delta G, \quad\text{and thus}\quad -\Delta G = nFE_{cell}

orΔG=−nFEcell...(5.27)\text{or}\quad \Delta G = -nFE_{cell} \qquad \text{...(5.27)}

Under standard state conditions we write

ΔG0=−nFEcell0...(5.28)\Delta G^0 = -nFE^0_{cell} \qquad \text{...(5.28)}

Eq. (5.28) explains why Ecell0E^0_{cell} is an intensive property. We know that ΔG0\Delta G^0 is an extensive property, since its value depends on the amount of substance. If the stoichiometric equation of the redox reaction is multiplied by 2 — that is, the amounts of substances oxidised and reduced are doubled — ΔG0\Delta G^0 doubles, and the moles of electrons transferred also double. The ratio

Ecell0=−ΔG0nFthen becomesEcell0=−2 ΔG02 nF=−ΔG0nFE^0_{cell} = -\frac{\Delta G^0}{nF} \quad\text{then becomes}\quad E^0_{cell} = -\frac{2\,\Delta G^0}{2\,nF} = -\frac{\Delta G^0}{nF} …