Electrochemistry
1. Check this before you revise anything
This was Unit 3 in the previous edition. Six chapters were removed from the Class 12 Chemistry book and the survivors renumbered, so Electrochemistry moved from 3 to 2.
The renumbering was not carried through the text. Five cross-references inside this chapter still point at Unit 3, and all five are wrong as printed:
| Where | Printed as | Should be |
|---|---|---|
| Page 34, standard hydrogen electrode | Fig. 3.3 | Fig. 2.3 |
| Page 34, sum of the half-reactions | (3.5) and (3.6) | (2.5) and (2.6) |
| Page 48, the plot in Example 2.6 | Fig. 3.7 | Fig. 2.7 |
| Page 50, data for Example 2.8 | Table 3.4 | Table 2.4 |
| Page 60, Exercise 2.17 | Table 3.1 | Table 2.1 |
The last one matters most in an exam. Exercise 2.17 tells you to use "the standard electrode potentials given in Table 3.1", and Chapter 3 is Chemical Kinetics, which has no such table. The table you need is Table 2.1 on page 37 of this chapter.
This chapter has two separate question sets:
- Intext Questions, 15 of them, in boxes on pages 36, 41, 51, 54 and 58.
- Exercises, 18 of them, at the end.
Both sets are numbered 2.1, 2.2, 2.3 and so on, so an intext question and an exercise can share a label. Identify a question by its content, not its number.
The book answers almost nothing. The key on the last page covers intext 2.5, 2.6 and 2.9 only. The other twelve intext questions and all eighteen exercises have no printed answer. Every answer on this site is worked out independently, and for the three the book does give, ours agrees.
| Textbook section | Topic |
|---|---|
| 2.1 | Electrochemical cells |
| 2.2 | Galvanic cells, electrode potential, the standard hydrogen electrode |
| 2.3 | Nernst equation, equilibrium constant, Gibbs energy |
| 2.4 | Conductance of electrolytic solutions, Kohlrausch's law |
| 2.5 | Electrolytic cells, Faraday's laws, products of electrolysis |
| 2.6 to 2.8 | Batteries, fuel cells, corrosion |
2. Galvanic Cells and Electrode Potential (Textbook 2.1 to 2.2)
A galvanic cell converts the Gibbs energy of a spontaneous redox reaction into electrical work. An electrolytic cell does the reverse, using an external supply to drive a non-spontaneous reaction. The Daniell cell is the standard example of the first.
The chapter opens with a thought experiment worth remembering. Apply an opposing external voltage to a Daniell cell and raise it slowly. Below 1.1 V the cell runs normally. At exactly 1.1 V nothing flows at all. Above 1.1 V the whole thing reverses and becomes an electrolytic cell, with zinc plating out and copper dissolving.
Electrode potential is the potential difference that develops between an electrode and its electrolyte. When every species in the half-cell is at unit concentration, it is the standard electrode potential. By IUPAC convention these are always quoted as reduction potentials.
No half-cell potential can be measured on its own, since a voltmeter needs two terminals. The standard hydrogen electrode, Pt(s) | H2(g, 1 bar) | H+(aq, 1 M), is assigned exactly zero at all temperatures and everything else is measured against it.
Cell notation puts the anode on the left, a single bar for a phase boundary and a double bar for the salt bridge:
For the Daniell cell that is V.
Reading Table 2.1 is half of what this chapter asks. The species at the top left, fluorine, is the strongest oxidising agent; the species at the bottom right, lithium metal, is the strongest reducing agent. A metal displaces any metal below it in the table, and an oxidising agent attacks any reduced species below it.
3. The Nernst Equation, Gibbs Energy and K (Textbook 2.3)
Away from standard conditions the potential shifts with concentration. For the general reaction transferring electrons:
The constant V is at 298 K, so it is valid only at that temperature.
Three traps in applying it. First, solids and pure liquids never appear in . Second, a stoichiometric coefficient becomes an exponent, so two Ag+ ions contribute . Third, is the number of electrons in the balanced overall reaction, not in one half-reaction as written in the table.
At equilibrium the cell is dead. Setting gives
The link to thermodynamics closes the loop:
Note that is intensive but is extensive. Doubling every coefficient leaves the voltage unchanged and doubles both and .
Because is proportional to , small voltages hide enormous ranges of . Exercise 2.4 makes the point sharply: V with gives , while V with gives .
4. Conductance of Electrolytic Solutions (Textbook 2.4)
Two quantities, and the whole section turns on the difference between them.
Conductivity is the conductance of one unit volume of solution, held between electrodes of unit area at unit separation. Unit: S m-1 or S cm-1.
Molar conductivity is the conductance of whatever volume contains one mole of electrolyte. Unit: S m2 mol-1 or S cm2 mol-1, related by S m2 mol-1 S cm2 mol-1.
With in S cm-1 and in mol L-1 the working formula carries a factor of 1000, which converts litres to cubic centimetres:
Dropping that 1000 is the most common numerical error in the chapter.
Measurement uses a Wheatstone bridge fed by an a.c. source, since d.c. would electrolyse the solution. The cell constant is found by calibrating against a KCl solution of known conductivity: .
On dilution, always falls and always rises. Both statements follow from the definitions. Dilution puts fewer ions in each unit volume, so drops; but the volume holding one mole grows faster than falls, so climbs.
| Strong electrolyte | Weak electrolyte | |
|---|---|---|
| Dissociation | Complete at all concentrations | Partial, rising towards 1 on dilution |
| Rise of on dilution | Gradual | Small, then very steep |
| Behaviour | Not linear in | |
| Getting | Extrapolate the straight line | Kohlrausch's law only |
Kohlrausch's law of independent migration of ions states that the limiting molar conductivity is the sum of independent ionic contributions:
It gives for weak electrolytes, which cannot be reached by extrapolation, and hence the degree of dissociation and the dissociation constant .
The extrapolation is a limiting law, not an exact one. Exercise 2.10 shows this in numbers. A straight line through all five NaCl points gives an intercept near 124.7 S cm2 mol-1, but Kohlrausch's law gives 126.4. Restrict the fit to the two most dilute points and the intercept climbs to 126.1. The most concentrated point is what bends the line.
5. Electrolysis and Faraday's Laws (Textbook 2.5)
Faraday's first law: the amount of chemical change at an electrode is proportional to the quantity of electricity passed.
Faraday's second law: the same quantity of electricity liberates masses of different substances in proportion to their chemical equivalents.
In practice everything reduces to three steps: , then with C mol-1, then divide by the electrons per formula unit.
Cells in series pass identical charge, which is what makes Exercise 2.16 solvable: the silver deposited in one cell fixes the copper and zinc in the other two.
Products of electrolysis (2.5.1) are decided by competition. At the cathode the species with the highest reduction potential wins; at the anode the species that is most easily oxidised wins. In aqueous solution H+ and OH- from water are always in the competition.
Overpotential breaks the rule, and the book relies on it twice. In brine, says water ( V) should be oxidised in preference to chloride ( V), yet chlorine is what comes off. The oxygen evolution reaction is kinetically slow and needs an extra voltage, so chloride wins in practice. The same reasoning gives Cl2 rather than O2 in Exercise 2.18(iv).
A reactive anode changes everything. With silver electrodes in AgNO3 the anode simply dissolves, so nothing in solution is oxidised at all. That is electroplating, and it is why Exercise 2.18 asks parts (i) and (ii) as a matched pair.
6. Batteries, Fuel Cells and Corrosion (Textbook 2.6 to 2.8)
Primary cells cannot be recharged. The dry (Leclanche) cell has a zinc container as anode and a graphite rod in MnO2 as cathode, giving about 1.5 V. The mercury cell uses a zinc amalgam anode and HgO cathode, giving about 1.35 V that stays constant, because no dissolved species changes concentration during its life.
Secondary cells can be recharged. In the lead storage battery:
Charging reverses this exactly. Since sulphuric acid is consumed on discharge and regenerated on charging, the specific gravity of the electrolyte reads the state of charge directly, which is how a garage tests a car battery.
Fuel cells feed reactants in continuously. The H2-O2 cell used in the Apollo programme runs in concentrated NaOH over porous carbon electrodes with Pt or Pd catalysts, at about 70% efficiency against 40% for a thermal plant. Methane and methanol are the alternative fuels named in the chapter.
Corrosion is a galvanic cell set up on the metal itself. One spot oxidises, another reduces oxygen, the moisture film is the electrolyte and the metal is its own external circuit:
The Fe2+ is then oxidised further by air to hydrated ferric oxide, Fe2O3 . xH2O, which is rust. Prevention follows from the mechanism: paint or plate the surface, or attach a sacrificial block of Mg or Zn so that the iron is forced to act as cathode.
7. Where the printed chapter needs care
Example 2.3 has a printed arithmetic slip. It computes and prints the result as " J mol-1", then as " kJ mol-1". The product is J, so the joule figure has lost a digit. The kilojoule value is right.
Two exercises need data the chapter does not print. Exercise 2.4(i) requires for Cd2+/Cd and Exercise 2.6 requires for the Ag2O/Ag couple in alkali. Neither appears in Table 2.1. The standard values are V and V, and both have to be brought in from outside the book.
Table 2.1 and Exercise 2.2 disagree by 0.01 V. The table gives Mg2+/Mg as V and the exercise supplies V. Nothing turns on it, but quote whichever the question gives you.
Equation 2.29 on page 51 prints the anode reaction of copper refining as Cu(s) gives Cu2+(s) + 2e-. The copper ion goes into solution, so it is Cu2+(aq).
Section 2.5.1 labels half-cell potentials as , in each of the five competing electrode reactions used to decide the products of electrolysis. These are single-electrode values read from Table 2.1, not cell potentials. Write them as in an answer.
Table 2.4 has no entry for HCOO-, which is why intext 2.9 supplies inside the question rather than expecting you to look it up.
Summary
Electrochemistry runs in both directions: a spontaneous redox reaction can be made to deliver electrical work, and electrical work can be made to drive a non-spontaneous reaction. The Daniell cell under an increasing opposing voltage shows both, and the crossover happens at exactly 1.1 V.
Everything quantitative follows from three relations. The Nernst equation carries a standard potential to any concentration. Setting the cell potential to zero at equilibrium turns it into a route to . And ties the whole subject back to thermodynamics, so that a voltmeter reading becomes a measurement of Gibbs energy.
The conductance half of the chapter turns on one distinction: conductivity is defined per unit volume and falls on dilution, while molar conductivity is defined per mole and rises. Strong electrolytes give up by extrapolation against the square root of concentration; weak ones will not, and need Kohlrausch's law instead.
Electrolysis reduces to counting electrons, with the products decided by competing potentials and, where kinetics intervenes, by overpotential. Batteries, fuel cells and corrosion are all the same chemistry applied: two of them useful, and the third the reason bridges are painted.
