From Cell Potential to Thermodynamics

A galvanic cell does electrical work. The maximum electrical work a cell can do is directly linked to the Gibbs energy change of its reaction. This is one of the most beautiful connections in chemistry — it ties the electrochemistry we've built to the thermodynamics of spontaneity.

The relation is:

ΔrG=nFEcell\boxed{\Delta_r G^\circ = -nFE^\circ_{cell}}

  • ΔrG\Delta_r G^\circ = standard Gibbs energy change of the cell reaction (in J mol1^{-1}).
  • nn = moles of electrons transferred.
  • FF = Faraday constant = 96487 C mol1^{-1} (≈ 96500).
  • EcellE^\circ_{cell} = standard cell potential (V).

The minus sign captures the logic: a positive EcellE^\circ_{cell} (spontaneous cell) gives a negative ΔrG\Delta_r G^\circ (spontaneous reaction). The two ways of saying "spontaneous" agree.

Maximum work: the maximum electrical work obtainable is wmax=ΔrG=nFEcellw_{max} = -\Delta_r G^\circ = nFE^\circ_{cell}.

Linking Potential to the Equilibrium Constant

Combining ΔrG=nFEcell\Delta_r G^\circ = -nFE^\circ_{cell} with the thermodynamic relation ΔrG=RTlnKc\Delta_r G^\circ = -RT\ln K_c gives a direct bridge between the standard cell potential and the equilibrium constant:

nFEcell=RTlnKcEcell=RTnFlnKcnFE^\circ_{cell} = RT\ln K_c \quad\Rightarrow\quad E^\circ_{cell} = \frac{RT}{nF}\ln K_c

At 298 K, using the 0.059 shortcut:

Ecell=0.0591nlogKc\boxed{E^\circ_{cell} = \frac{0.0591}{n}\log K_c}

This makes intuitive sense via the Nernst equation: at equilibrium Ecell=0E_{cell}=0 and Q=KcQ=K_c, so 0=Ecell0.0591nlogKc0=E^\circ_{cell}-\dfrac{0.0591}{n}\log K_c, which rearranges to exactly this.

Link between Gibbs energy, cell emf and Kc

Reading the Signs

The three quantities EcellE^\circ_{cell}, ΔrG\Delta_r G^\circ and KcK_c are three views of the same thing — how far and which way a reaction goes:

EcellE^\circ_{cell} ΔrG\Delta_r G^\circ KcK_c Reaction
Positive Negative > 1 Spontaneous (forward)
Zero Zero = 1 At equilibrium
Negative Positive < 1 Non-spontaneous (reverse favoured)

[JEE Tip] Watch your units. With F=96487F = 96487 C mol1^{-1} and EE^\circ in volts, ΔrG\Delta_r G^\circ comes out in joules per mole. Divide by 1000 for kJ mol1^{-1}. A frequent error is mixing kJ and J when comparing with ΔG=RTlnK\Delta G = -RT\ln K.

Key Point: ΔrG=nFEcell\Delta_r G^\circ = -nFE^\circ_{cell} converts a voltmeter reading into a thermodynamic spontaneity statement. It is the most important single equation connecting the two halves of physical chemistry.

Solved Examples

Example 1: Gibbs energy from cell potential

Calculate ΔrG\Delta_r G^\circ for the Daniell cell (Ecell=1.10E^\circ_{cell}=1.10 V, n=2n=2). (F=96487F=96487 C mol1^{-1})

Solution: ΔrG=nFEcell=2×96487×1.10=212,271\Delta_r G^\circ = -nFE^\circ_{cell} = -2\times96487\times1.10 = -212{,}271 J 212.3\approx -212.3 kJ mol1^{-1}.

Answer: 212.3-212.3 kJ mol1^{-1} (negative → spontaneous).

Example 2: Equilibrium constant from E°

For a cell with Ecell=0.295E^\circ_{cell}=0.295 V and n=2n=2, find logKc\log K_c and KcK_c.

Solution: Ecell=0.0591nlogKclogKc=nEcell0.0591=2×0.2950.05919.9810E^\circ_{cell}=\dfrac{0.0591}{n}\log K_c \Rightarrow \log K_c = \dfrac{nE^\circ_{cell}}{0.0591}=\dfrac{2\times0.295}{0.0591}\approx 9.98 \approx 10. So Kc1010K_c \approx 10^{10}.

Answer: logKc10\log K_c \approx 10, Kc1×1010K_c \approx 1\times10^{10}.

Example 3: Maximum work

What is the maximum electrical work obtainable from the Daniell cell per mole of reaction? (E=1.10E^\circ=1.10 V, n=2n=2)

Solution: wmax=nFEcell=2×96487×1.10=212,271w_{max}=nFE^\circ_{cell}=2\times96487\times1.10=212{,}271 J 212.3\approx 212.3 kJ mol1^{-1}.

Answer: 212.3212.3 kJ mol1^{-1} of work per mole.

Example 4: Sign check

A cell reaction has Ecell=0.25E^\circ_{cell}=-0.25 V. Is it spontaneous, and what is the sign of ΔrG\Delta_r G^\circ?

Solution: ΔrG=nFEcell\Delta_r G^\circ=-nFE^\circ_{cell}. With EcellE^\circ_{cell} negative, ΔrG\Delta_r G^\circ is positive → the reaction is non-spontaneous as written (the reverse is favoured).

Example 5: Kc for the Daniell cell

Estimate KcK_c for the Daniell cell (Ecell=1.10E^\circ_{cell}=1.10 V, n=2n=2).

Solution: logKc=nE0.0591=2×1.100.059137.2\log K_c=\dfrac{nE^\circ}{0.0591}=\dfrac{2\times1.10}{0.0591}\approx 37.2. So Kc1037.22×1037K_c\approx 10^{37.2}\approx 2\times10^{37}.

Answer: Kc1037K_c\approx 10^{37} — enormous, confirming the reaction goes essentially to completion.

Example 6: ΔG° from electrode potentials

For Mg + 2Ag+^+ → Mg2+^{2+} + 2Ag, Ecell=3.16E^\circ_{cell}=3.16 V, n=2n=2. Find ΔrG\Delta_r G^\circ.

Solution: ΔrG=nFE=2×96487×3.16=609,880\Delta_r G^\circ=-nFE^\circ=-2\times96487\times3.16=-609{,}880 J 609.9\approx -609.9 kJ mol1^{-1}.

Answer: 609.9-609.9 kJ mol1^{-1}.

Example 7: Finding E° from ΔG°

A reaction transferring 2 electrons has ΔrG=193\Delta_r G^\circ=-193 kJ mol1^{-1}. Find EcellE^\circ_{cell}. (F=96500F=96500)

Solution: Ecell=ΔrGnF=1930002×96500=1.0E^\circ_{cell}=-\dfrac{\Delta_r G^\circ}{nF}=-\dfrac{-193000}{2\times96500}=1.0 V.

Answer: 1.01.0 V.

Example 8: Relating Kc and spontaneity

If Kc=1K_c=1 for a cell reaction, what is EcellE^\circ_{cell}?

Solution: Ecell=0.0591nlogKc=0.0591nlog1=0E^\circ_{cell}=\dfrac{0.0591}{n}\log K_c=\dfrac{0.0591}{n}\log 1=0 V. With Kc=1K_c=1 the system is balanced, so Ecell=0E^\circ_{cell}=0 and ΔrG=0\Delta_r G^\circ=0.

Example 9: Two-electron cell Kc

A cell has Ecell=0.118E^\circ_{cell}=0.118 V and n=2n=2. Find KcK_c.

Solution: logKc=2×0.1180.05913.994.0\log K_c=\dfrac{2\times0.118}{0.0591}\approx 3.99\approx 4.0. Kc104K_c\approx 10^4.

Answer: Kc1×104K_c\approx 1\times10^4.

Example 10: ΔG° in kJ from a 1-electron cell

For a cell with Ecell=0.80E^\circ_{cell}=0.80 V and n=1n=1, find ΔrG\Delta_r G^\circ in kJ. (F=96500F=96500)

Solution: ΔrG=1×96500×0.80=77,200\Delta_r G^\circ=-1\times96500\times0.80=-77{,}200 J =77.2=-77.2 kJ.

Answer: 77.2-77.2 kJ mol1^{-1}.