Part 1 · Chapter 10

Electrochemistry

Turning chemistry into electricity and back — cells, electrode potentials, the Nernst equation, conductance, and the laws of electrolysis

Fundamentals of Chemistry Prof. Mithun Mondal Reading time ≈ 52 min
i What you'll learn
  • The difference between a galvanic cell (chemistry → electricity) and an electrolytic cell (electricity → chemistry).
  • Electrode potential, the standard hydrogen electrode, and the electrochemical series.
  • The EMF of a cell and the Nernst equation for non-standard conditions.
  • The links \(\Delta G^\circ=-nFE^\circ\) and \(E^\circ=\tfrac{0.0591}{n}\log K\).
  • Conductivity, molar conductivity, and Kohlrausch's law.
  • Faraday's laws of electrolysis, and how batteries, fuel cells and corrosion work.
Section 10-1

Two Kinds of Electrochemical Cell

Electrochemistry studies the two-way conversion between chemical and electrical energy. A galvanic (voltaic) cell uses a spontaneous redox reaction to produce electricity; an electrolytic cell uses an external current to drive a non-spontaneous reaction. In both, oxidation occurs at the anode and reduction at the cathode — only the sign of the electrodes flips between the two.

FeatureGalvanic cellElectrolytic cell
Energy changechemical → electricalelectrical → chemical
Reactionspontaneous \((\Delta G<0)\)non-spontaneous \((\Delta G>0)\)
Anodenegative \((-)\), oxidationpositive \((+)\), oxidation
Cathodepositive \((+)\), reductionnegative \((-)\), reduction
One rule never changes: oxidation is always at the anode and reduction always at the cathode. What flips between cell types is which electrode is positive — so reason from the half-reaction, not the sign.
Section 10-2

The Galvanic Cell & Cell Notation

The classic galvanic cell is the Daniell cell: a zinc electrode in \(\ce{ZnSO4}\) and a copper electrode in \(\ce{CuSO4}\), joined by a salt bridge that completes the circuit while keeping the solutions from mixing. Zinc dissolves (oxidation); copper deposits (reduction); electrons travel through the external wire from zinc to copper.

V e⁻ → salt bridge Zn anode (−) Cu cathode (+) ZnSO₄ CuSO₄
The Daniell cell: zinc gives up electrons that reduce copper ions
Cell reaction and notation
\[ \ce{Zn + Cu^2+ -> Zn^2+ + Cu} \]
\[ \ce{Zn(s) | Zn^2+(1\,M) || Cu^2+(1\,M) | Cu(s)} \]
Anode on the left, cathode on the right; a single bar \(|\) is a phase boundary and the double bar \(||\) is the salt bridge.
Section 10-3

Electrode Potential & the SHE

Each electrode has a tendency to gain or lose electrons, measured as its electrode potential. Only differences are observable, so we fix a reference: the standard hydrogen electrode (SHE) is assigned \(E^\circ=0\ \text{V}\). Potentials measured against it, under standard conditions (1 M, 1 bar, 298 K), are standard electrode potentials and are tabulated as reduction potentials.

EMF of a cell
\(E^\circ_{\text{cell}}=E^\circ_{\text{cathode}}-E^\circ_{\text{anode}}\)

Both values are reduction potentials. A positive \(E^\circ_{\text{cell}}\) means the cell reaction is spontaneous as written. For the Daniell cell, \(E^\circ_{\text{cell}}=0.34-(-0.76)=1.10\ \text{V}\).

Section 10-4

The Electrochemical Series

Arranging electrodes by standard reduction potential gives the electrochemical series. A more positive \(E^\circ\) marks a stronger oxidising agent (more readily reduced); a more negative \(E^\circ\) marks a stronger reducing agent. The series predicts displacement, cell EMF, and reactivity at a glance.

Reduction half-reaction\(E^\circ\) (V)
\(\ce{F2 + 2e^- -> 2F^-}\)\(+2.87\)
\(\ce{Cu^2+ + 2e^- -> Cu}\)\(+0.34\)
\(\ce{2H+ + 2e^- -> H2}\)\(0.00\) (SHE)
\(\ce{Zn^2+ + 2e^- -> Zn}\)\(-0.76\)
\(\ce{Li+ + e^- -> Li}\)\(-3.04\)
A metal displaces ions below it. Zinc (\(-0.76\)) lies below copper (\(+0.34\)) in reactivity-by-potential, so \(\ce{Zn}\) reduces \(\ce{Cu^2+}\) — but not the reverse. The same logic tells you which metals liberate \(\ce{H2}\) from acids (those with negative \(E^\circ\)).
Section 10-5

EMF & the Nernst Equation

Standard potentials assume 1 M concentrations. The Nernst equation corrects the EMF for any concentration, showing how a cell's voltage falls as it discharges toward equilibrium.

Nernst equation
\[ E_{\text{cell}}=E^\circ_{\text{cell}}-\frac{RT}{nF}\ln Q=E^\circ_{\text{cell}}-\frac{0.0591}{n}\log Q\quad(298\ \text{K}) \]
\(Q\) is the reaction quotient, \(n\) the electrons transferred, \(F=96500\ \text{C mol}^{-1}\). At equilibrium \(E_{\text{cell}}=0\) and \(Q=K\).
Section 10-6

EMF, Gibbs Energy & the Equilibrium Constant

The EMF is electrical work per unit charge, so it ties directly to the free-energy change of the reaction — the bridge between this chapter and thermodynamics. Setting \(E_{\text{cell}}=0\) at equilibrium links \(E^\circ\) to the equilibrium constant.

🔗
Three quantities, one reaction
\(\Delta G^\circ=-nFE^\circ_{\text{cell}},\qquad E^\circ_{\text{cell}}=\frac{0.0591}{n}\log K\)

A positive \(E^\circ\) ⇒ negative \(\Delta G^\circ\) ⇒ \(K>1\): all three say "spontaneous." The Nernst, thermodynamic, and equilibrium pictures are one statement seen three ways.

Section 10-7

Conductance of Electrolytes

Electrolytic solutions conduct by ion movement. The resistance of a column of solution gives its conductivity \(\kappa\) (conductance of a unit cube), and dividing by concentration gives the molar conductivity \(\Lambda_m\) — the conductance of all the ions from one mole of electrolyte.

From resistance to molar conductivity
\[ \kappa=\frac{1}{R}\cdot\frac{l}{A},\qquad \Lambda_m=\frac{\kappa\times1000}{c} \]
\(l/A\) is the cell constant; \(c\) is in mol L\(^{-1}\), giving \(\Lambda_m\) in S cm\(^2\) mol\(^{-1}\).
strong electrolyte weak electrolyte Λ°ₘ Λₘ √c
Strong electrolytes extrapolate to Λ°ₘ; weak ones rise steeply near infinite dilution
Section 10-8

Kohlrausch's Law

At infinite dilution every ion moves independently, so the limiting molar conductivity \(\Lambda^\circ_m\) is just the sum of the ionic contributions. This is Kohlrausch's law of independent migration, and it lets us find \(\Lambda^\circ_m\) for weak electrolytes — which can never be reached directly by dilution.

Independent ionic migration
\[ \Lambda^\circ_m=\nu_+\lambda^\circ_+ + \nu_-\lambda^\circ_-,\qquad \alpha=\frac{\Lambda_m}{\Lambda^\circ_m} \]
The degree of dissociation \(\alpha\) of a weak electrolyte is the ratio of its molar conductivity to its limiting value; combine with Ostwald's law for \(K_a\).
Section 10-9

Electrolysis & Faraday's Laws

In electrolysis, a current forces a non-spontaneous redox reaction — depositing metals, refining copper, producing chlorine and aluminium. Faraday's two laws quantify how much is transformed.

+ anode (+) cathode (−) electrolyte
An electrolytic cell: the battery drives a non-spontaneous reaction
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Faraday's laws of electrolysis
\(w=\dfrac{M\,I\,t}{nF}=\dfrac{E\,I\,t}{F},\qquad Q=It\)

First law: mass deposited is proportional to the charge \(Q=It\). Second law: for the same charge, masses of different substances are proportional to their equivalent weights \(E=M/n\). One mole of electrons is one faraday, \(F=96500\ \text{C}\).

Section 10-10

Batteries, Fuel Cells & Corrosion

Practical cells apply these ideas. Primary batteries (the dry Leclanché cell) are used once; secondary batteries (the lead storage battery, nickel–cadmium) are rechargeable; fuel cells (the \(\ce{H2}\!-\!\ce{O2}\) cell) convert fuel directly to electricity with high efficiency. Corrosion is an unwanted galvanic process — iron rusts where it acts as an anode.

DeviceTypeNote
Dry (Leclanché) cellprimary\(\ce{Zn}\) anode, \(\ce{MnO2}\)/C cathode, ≈ 1.5 V
Lead storage batterysecondary\(\ce{Pb}\)/\(\ce{PbO2}\) in \(\ce{H2SO4}\); rechargeable
\(\ce{H2}\!-\!\ce{O2}\) fuel cellfuel cellcontinuous fuel feed; water is the only product
Corrosion is a cell you didn't build. Stopping rust means breaking the circuit — coating the metal, galvanising with zinc, or attaching a more active "sacrificial" anode (cathodic protection) that corrodes in the iron's place.
Worked Examples

Putting It to Work

1 Standard cell EMF

Problem. Find \(E^\circ_{\text{cell}}\) for the Daniell cell. \(E^\circ_{\ce{Cu^2+/Cu}}=+0.34,\ E^\circ_{\ce{Zn^2+/Zn}}=-0.76\ \text{V}\).

Solution. Copper is reduced (cathode), zinc oxidised (anode):

Working
\[ E^\circ_{\text{cell}}=0.34-(-0.76)=1.10\ \text{V}\ (>0,\ \text{spontaneous}) \]
2 Nernst equation

Problem. For the Daniell cell with \([\ce{Zn^2+}]=0.1\) and \([\ce{Cu^2+}]=0.01\ \text{M}\), find \(E_{\text{cell}}\).

Solution. Here \(n=2\) and \(Q=[\ce{Zn^2+}]/[\ce{Cu^2+}]\):

Working
\[ E=1.10-\frac{0.0591}{2}\log\frac{0.1}{0.01}=1.10-0.0295=1.07\ \text{V} \]
3 Gibbs energy from EMF

Problem. Find \(\Delta G^\circ\) for the Daniell cell \((E^\circ=1.10\ \text{V},\ n=2)\).

Solution. Apply \(\Delta G^\circ=-nFE^\circ\):

Working
\[ \Delta G^\circ=-2\times96500\times1.10=-2.12\times10^{5}\ \text{J}=-212\ \text{kJ} \]
4 Equilibrium constant from EMF

Problem. Find \(K\) for the Daniell cell reaction \((E^\circ=1.10\ \text{V},\ n=2)\).

Solution. Use \(E^\circ=\frac{0.0591}{n}\log K\):

Working
\[ \log K=\frac{2\times1.10}{0.0591}=37.2\ \Rightarrow\ K\approx1.6\times10^{37} \]
5 Faraday's law

Problem. A current of \(2.0\ \text{A}\) flows for \(30\ \text{min}\) through \(\ce{CuSO4}\). Find the mass of copper deposited \((M=63.5,\ n=2)\).

Solution. Charge \(Q=It=2.0\times1800=3600\ \text{C}\):

Working
\[ w=\frac{M\,Q}{nF}=\frac{63.5\times3600}{2\times96500}=1.18\ \text{g} \]
6 Degree of dissociation

Problem. Acetic acid has \(\Lambda^\circ_m=390.5\) and, at \(0.1\ \text{M}\), \(\Lambda_m=5.2\ \text{S cm}^2\text{mol}^{-1}\). Find \(\alpha\) and \(K_a\).

Solution. \(\alpha=\Lambda_m/\Lambda^\circ_m\), then Ostwald's law:

Working
\[ \alpha=\frac{5.2}{390.5}=0.0133;\quad K_a=\frac{c\alpha^2}{1-\alpha}\approx1.8\times10^{-5} \]
Review

Chapter Summary

Cells

Galvanic = spontaneous (chemical→electrical); electrolytic = driven. Anode oxidises, cathode reduces.

EMF

\(E^\circ_{\text{cell}}=E^\circ_{\text{cathode}}-E^\circ_{\text{anode}}\); positive means spontaneous.

Nernst

\(E=E^\circ-\tfrac{0.0591}{n}\log Q\); voltage falls as the cell discharges.

Links

\(\Delta G^\circ=-nFE^\circ\) and \(E^\circ=\tfrac{0.0591}{n}\log K\) — one reaction, three views.

Conductance

\(\Lambda_m=\tfrac{\kappa\times1000}{c}\); Kohlrausch gives \(\Lambda^\circ_m\) and \(\alpha=\Lambda_m/\Lambda^\circ_m\).

Electrolysis

Faraday: \(w=\tfrac{MIt}{nF}\); \(F=96500\ \text{C}\) per mole of electrons.

Practice

Problems

Identify the cathode and anode half-reactions first, then choose between EMF, Nernst, and Faraday relations. Take \(F=96500\ \text{C mol}^{-1}\) and \(\tfrac{0.0591}{n}\) at \(298\ \text{K}\). Difficulty rises down the list.

  1. Write the cell notation and \(E^\circ_{\text{cell}}\) for a cell made from \(\ce{Mg^2+/Mg}\,(-2.37)\) and \(\ce{Ag+/Ag}\,(+0.80)\).
  2. State which is the anode and which the cathode in a galvanic cell and in an electrolytic cell, with the sign of each.
  3. Predict whether \(\ce{Fe}\) can displace \(\ce{Cu^2+}\) from solution, using \(E^\circ_{\ce{Fe^2+/Fe}}=-0.44\) and \(E^\circ_{\ce{Cu^2+/Cu}}=+0.34\).
  4. A cell has \(E^\circ=0.46\ \text{V}\) and \(n=2\). Find \(\Delta G^\circ\).
  5. For the cell in Problem 4, find the equilibrium constant \(K\).
  6. Find \(E_{\text{cell}}\) for \(\ce{Zn|Zn^2+(0.01\,M)||Cu^2+(0.1\,M)|Cu}\) given \(E^\circ=1.10\ \text{V}\).
  7. The conductivity of \(0.02\ \text{M}\ \ce{KCl}\) is \(2.77\times10^{-3}\ \text{S cm}^{-1}\). Find its molar conductivity.
  8. Given \(\lambda^\circ_{\ce{Na+}}=50.1\) and \(\lambda^\circ_{\ce{Cl-}}=76.3\), find \(\Lambda^\circ_m\) of \(\ce{NaCl}\).
  9. How long must \(5\ \text{A}\) flow to deposit \(9.6\ \text{g}\) of copper \((M=63.5,\ n=2)\)?
  10. The same charge is passed through \(\ce{AgNO3}\) and \(\ce{CuSO4}\) in series. If \(1.08\ \text{g}\) of \(\ce{Ag}\) is deposited \((M=108)\), find the mass of \(\ce{Cu}\) \((M=63.5)\).
  11. Explain, using \(E^\circ\) values, why a magnesium block protects a buried iron pipeline from corrosion.
  12. A weak acid at \(0.05\ \text{M}\) has \(\Lambda_m=7.8\) and \(\Lambda^\circ_m=390\ \text{S cm}^2\text{mol}^{-1}\). Find \(\alpha\) and \(K_a\).
Tip: EMF is the hinge of the chapter. From \(E^\circ\) you reach spontaneity \((\Delta G^\circ=-nFE^\circ)\), equilibrium \((E^\circ=\tfrac{0.0591}{n}\log K)\), and any non-standard voltage (Nernst). Conductance and Faraday's laws are the bookkeeping of the ions doing the work.