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Thermodynamics of Galvanic Cells | Chemca

Thermodynamics of Galvanic Cells | Chemca
Physical Chemistry

Thermodynamic Functions of a Galvanic Cell

By Chemca Editorial Team Last Updated: January 2026 10 min read

A galvanic cell converts chemical energy into electrical energy. The electrical work done by the cell comes at the expense of the Gibbs Free Energy ($G$) of the cell reaction. By measuring the Electromotive Force (EMF) of the cell and its variation with temperature, we can calculate fundamental thermodynamic parameters like $\Delta G$, $\Delta S$, and $\Delta H$.

1. Electrical Work and Gibbs Free Energy ($\Delta G$)

The electrical work done by a cell in one second is equal to the product of the potential difference (EMF) and the total charge passed.

If $n$ moles of electrons are transferred in the balanced cell reaction, the total charge is $nF$ (where $F$ is Faraday's constant $\approx 96500 \ C/mol$).

$$ \text{Electrical Work} = nF E_{\text{cell}} $$

According to thermodynamics, the maximum useful work done by a system (at constant T and P) is equal to the decrease in Gibbs Free Energy ($-\Delta G$).

$$ \Delta G = -nF E_{\text{cell}} $$

Conditions for Spontaneity:

  • For a spontaneous reaction, $\Delta G$ must be Negative ($\Delta G < 0$).
  • Therefore, $E_{\text{cell}}$ must be Positive ($E_{\text{cell}} > 0$).

Standard Gibbs Free Energy ($\Delta G^\circ$)

At standard conditions (1 M concentration, 1 bar pressure, 298 K):

$$ \Delta G^\circ = -nF E^\circ_{\text{cell}} $$

Relation with Equilibrium Constant ($K_{eq}$)

At equilibrium, $E_{\text{cell}} = 0$, so $\Delta G = 0$. Using the relationship $\Delta G^\circ = -RT \ln K_{eq}$:

$$ \Delta G^\circ = -2.303 RT \log K_{eq} $$ $$ E^\circ_{\text{cell}} = \frac{0.0591}{n} \log K_{eq} \quad (\text{at } 298 K) $$

2. Entropy Change ($\Delta S$)

From the fundamental thermodynamic equation $dG = VdP - SdT$, at constant pressure ($dP=0$), we have:

$$ \left(\frac{\partial G}{\partial T}\right)_P = -S \quad \implies \quad \left(\frac{\partial (\Delta G)}{\partial T}\right)_P = -\Delta S $$

Substituting $\Delta G = -nFE$:

$$ \frac{\partial}{\partial T}(-nFE) = -\Delta S $$
$$ \Delta S = nF \left(\frac{\partial E}{\partial T}\right)_P $$

Here, $\left(\frac{\partial E}{\partial T}\right)_P$ is called the Temperature Coefficient of the cell EMF.

  • If $\frac{\partial E}{\partial T} > 0$, then $\Delta S$ is positive (Disorder increases).
  • If $\frac{\partial E}{\partial T} < 0$, then $\Delta S$ is negative (Disorder decreases).

3. Enthalpy Change ($\Delta H$)

From the Gibbs-Helmholtz equation:

$$ \Delta G = \Delta H - T\Delta S $$

Rearranging for Enthalpy:

$$ \Delta H = \Delta G + T\Delta S $$

Substituting the values derived above:

$$ \Delta H = -nFE + nFT \left(\frac{\partial E}{\partial T}\right)_P $$ $$ \Delta H = nF \left[ T \left(\frac{\partial E}{\partial T}\right)_P - E \right] $$

Heat of Reaction: If the cell operates reversibly, the heat absorbed or evolved ($q_{rev}$) is given by $q = T\Delta S = nFT (\frac{\partial E}{\partial T})_P$.

4. Summary of Formulas

Parameter Formula
Gibbs Energy ($\Delta G$) $-nFE_{\text{cell}}$
Entropy ($\Delta S$) $nF (\frac{\partial E}{\partial T})_P$
Enthalpy ($\Delta H$) $-nFE + nFT (\frac{\partial E}{\partial T})_P$
Equilibrium Constant $\Delta G^\circ = -RT \ln K_{eq}$

5. Example Calculation

Problem: For a cell with $n=2$, EMF is $1.10 \ V$ at $298 \ K$, and the temperature coefficient is $-0.0005 \ V/K$. Calculate $\Delta G$ and $\Delta S$. ($F = 96500 \ C/mol$)

Solution:
1. $\Delta G = -nFE = -2 \times 96500 \times 1.10 = -212,300 \ J/mol = -212.3 \ kJ/mol$.
2. $\Delta S = nF (\frac{\partial E}{\partial T}) = 2 \times 96500 \times (-0.0005) = -96.5 \ J/K \cdot mol$.

Thermodynamics Quiz

Test your concepts on Cell Potential and Energy. 10 MCQs with explanations.

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