Unit 3 · Spec 3.1.8

Thermodynamics & Born-Haber Cycles

Born-Haber cycles, lattice enthalpy of formation and dissociation, hydration and solution enthalpies, entropy, Gibbs free energy feasibility, and feasibility temperature calculations for OxfordAQA A-Level Chemistry.

1. Standard Enthalpy Definitions

Thermodynamics examines the energy changes and driving forces that dictate whether chemical reactions occur spontaneously. To construct energy cycles for ionic lattices, several standard enthalpy terms are required:

Standard Enthalpy of Formation (ΔfH) The enthalpy change when one mole of a compound is formed from its elements, with all substances in their standard states under standard conditions.
Example: Na(s) + ½Cl₂(g) → NaCl(s) [ΔH = −411 kJ mol⁻¹]
First Ionisation Energy (IE₁) The enthalpy change when one mole of electrons is removed from one mole of gaseous atoms to form one mole of gaseous 1+ ions. It is always endothermic.
Example: Na(g) → Na⁺(g) + e⁻ [ΔH = +496 kJ mol⁻¹]
The second ionisation energy removes an electron from each 1+ ion: Mg⁺(g) → Mg²⁺(g) + e⁻ [ΔH = +1451 kJ mol⁻¹]
Bond Dissociation Enthalpy The enthalpy change when one mole of a covalent bond is broken, with the molecule and the fragments all in the gaseous state.
Example: Cl₂(g) → 2Cl(g) [ΔH = +244 kJ mol⁻¹]
For chlorine, the bond enthalpy (+244) is twice the enthalpy of atomisation (+122), because atomisation makes only one mole of Cl atoms.
Lattice Enthalpy of Formation (ΔHlatt) The enthalpy change when one mole of a solid ionic compound is formed from its constituent gaseous ions under standard conditions (298 K, 100 kPa). This process is strongly exothermic (negative value).
Example: Na⁺(g) + Cl⁻(g) → NaCl(s) [ΔH = −788 kJ mol⁻¹]
Lattice Enthalpy of Dissociation The enthalpy change when one mole of a solid ionic lattice is completely broken into its constituent gaseous ions under standard conditions. This process is strongly endothermic (positive value, exactly equal in magnitude but opposite in sign to the lattice enthalpy of formation).
Example: NaCl(s) → Na⁺(g) + Cl⁻(g) [ΔH = +788 kJ mol⁻¹]
Standard Enthalpy of Atomisation (ΔHat) The enthalpy change when one mole of gaseous atoms is formed from an element in its standard state. This process is always endothermic.
Example: Na(s) → Na(g) [ΔH = +107 kJ mol⁻¹]
Example: ½Cl₂(g) → Cl(g) [ΔH = +122 kJ mol⁻¹]
First Electron Affinity (ΔHEA1) The enthalpy change when one mole of gaseous 1- ions is formed from one mole of gaseous atoms by gaining one electron per atom.
Example: Cl(g) + e⁻ → Cl⁻(g) [ΔH = −348 kJ mol⁻¹] (exothermic)

The enthalpy of hydration is defined in Section 4. Data books differ slightly, so the same quantity can have a slightly different value in different questions (for example, EA(Cl) is given as −348 or −349 kJ mol⁻¹). Always use the values in the question.

First vs Second Electron Affinity

The first electron affinity is exothermic because the incoming electron is attracted to the positive nuclear charge of the neutral atom. However, the second electron affinity (e.g. O⁻(g) + e⁻ → O²⁻(g) [ΔH = +798 kJ mol⁻¹]) is always endothermic because energy must be supplied to overcome the strong electrostatic repulsion between the negative ion and the incoming electron.

2. Born-Haber Energy Cycles

Lattice enthalpies cannot be measured directly through experimental calorimetry because it is practically impossible to assemble a solid crystal directly from isolated gaseous ions. Instead, we apply Hess's Law using a thermodynamic cycle known as a Born-Haber cycle.

A Born-Haber cycle connects the standard enthalpy of formation of an ionic solid with the series of steps required to vaporise, atomise, and ionise the constituent elements into gaseous ions:

ΔHf = ΔHat(metal) + IE₁(metal) + ΔHat(non-metal) + ΔHEA1(non-metal) + ΔHlatt(formation)

Rearranging for the standard lattice enthalpy of formation gives:

ΔHlatt(formation) = ΔHf − [ΔHat(metal) + IE₁(metal) + ΔHat(non-metal) + ΔHEA1(non-metal)]

3. Born-Haber Cycle Diagram

The diagram below displays the complete energy level progression for sodium chloride. Endothermic stages are represented by upward arrows (+ values) and exothermic stages by downward arrows (- values):

Born-Haber Cycle for Sodium Chloride (NaCl) Enthalpy, H / kJ mol⁻¹ Na⁺(g) + e⁻ + Cl(g) (+725) Na⁺(g) + Cl⁻(g) (+377) Na(g) + Cl(g) (+229) Na(g) + ½Cl₂(g) (+107) Na(s) + ½Cl₂(g) (0) NaCl(s) (−411) ΔfH = −411 ΔatH(Na) = +107 ΔatH(Cl) = +122 IE₁(Na) = +496 EA₁(Cl) = −348 Lattice formation = −788

Born-Haber Cycle for MgCl₂

For a compound such as MgCl₂, the cycle has more steps:

  • Mg forms Mg²⁺, so you need the first and second ionisation energies.
  • There are two chloride ions, so you need 2 × the enthalpy of atomisation of chlorine and 2 × the electron affinity of chlorine.
Born-Haber Cycle for Magnesium Chloride (MgCl₂) Enthalpy, H / kJ mol⁻¹ Mg(s) + Cl₂(g) (0) Mg(g) + Cl₂(g) (+148) Mg⁺(g) + e⁻ + Cl₂(g) (+886) Mg²⁺(g) + 2e⁻ + Cl₂(g) (+2337) Mg²⁺(g) + 2e⁻ + 2Cl(g) (+2581) Mg²⁺(g) + 2Cl⁻(g) (+1883) MgCl₂(s) (−642) ΔfH = −642 ΔatH(Mg) = +148 1st IE(Mg) = +738 2nd IE(Mg) = +1451 2 × ΔatH(Cl) = +244 2 × EA(Cl) = −698 Lattice formation = −2525
Worked Example: Lattice Enthalpy of Formation of MgCl₂
Use the data (kJ mol⁻¹) to calculate the lattice enthalpy of formation of MgCl₂.
ΔfH(MgCl₂) = −642
ΔatH(Mg) = +148
First IE(Mg) = +738; second IE(Mg) = +1451
ΔatH(Cl) = +122 (½Cl₂(g) → Cl(g))
EA(Cl) = −349

Step 1: Add up the steps from the elements to the gaseous ions:

148 + 738 + 1451 + (2 × 122) + (2 × −349)

= 148 + 738 + 1451 + 244 − 698 = +1883 kJ mol⁻¹

Step 2: Use Hess's law:

Lattice formation = ΔfH − (sum of the other steps)

= −642 − 1883 = −2525 kJ mol⁻¹

The most common mistake is to forget the ×2 for chlorine. Each mole of MgCl₂ contains two moles of Cl⁻ ions.

4. Enthalpies of Solution and Hydration

When an ionic solid dissolves in water, the crystal lattice breaks apart and the separated ions become surrounded by polar water molecules. The overall energy change is known as the standard enthalpy of solution.

Enthalpy of Solution (ΔHsol) The enthalpy change when one mole of an ionic solid dissolves in an amount of water large enough so that dissolved ions do not interact with each other under standard conditions.
Example: NaCl(s) + aq → Na⁺(aq) + Cl⁻(aq)
Enthalpy of Hydration (ΔHhyd) The enthalpy change when one mole of gaseous ions is converted into one mole of aqueous ions under standard conditions. This is always exothermic because new ion-dipole electrostatic bonds are formed between ions and polar water molecules.
Example: Na⁺(g) + aq → Na⁺(aq) [ΔHhyd = −406 kJ mol⁻¹]
Example: Cl⁻(g) + aq → Cl⁻(aq) [ΔHhyd = −364 kJ mol⁻¹]

The relationship between these terms is given by the Hess cycle:

ΔHsol = ΔHlatt(dissociation) + Σ[ΔHhyd(ions)]

Or equivalently: ΔHsol = −ΔHlatt(formation) + ΔHhyd(cations) + ΔHhyd(anions)

Example (NaCl): ΔHsol = +788 + (−406) + (−364) = +18 kJ mol⁻¹.

The measured value is +3.9 kJ mol⁻¹; the cycle value differs because the data come from different sources and are rounded.

Worked Example: Enthalpy of Solution of KCl
Use the data (kJ mol⁻¹) to calculate the enthalpy of solution of potassium chloride.
Lattice dissociation enthalpy of KCl = +711
Enthalpy of hydration of K⁺ = −322
Enthalpy of hydration of Cl⁻ = −364

Step 1: Write the cycle: KCl(s) → K⁺(g) + Cl⁻(g) → K⁺(aq) + Cl⁻(aq)

Step 2: Add the steps:

ΔsolH = +711 + (−322) + (−364) = +25 kJ mol⁻¹

The positive value means KCl dissolves endothermically, so the solution cools. The measured value is about +17 kJ mol⁻¹. Values vary slightly between data sources, so a cycle value does not always match the measured value exactly.

5. The Ionic Model & Polarisation

Theoretical lattice enthalpies can be calculated using electrostatics and Coulomb's law. This calculation assumes the purely ionic model:

  • Ions are modelled as perfect, unpolarisable spheres.
  • Electrostatic charges are treated as point charges located at ion centres.
  • The only bonding forces acting between ions are purely electrostatic attractions and repulsions (zero covalent character).
Compound Theoretical Lattice Enthalpy / kJ mol⁻¹ Experimental Born-Haber Value / kJ mol⁻¹ Discrepancy & Nature of Bonding
NaCl -770 -788 Close agreement (2.3% difference): almost perfectly ionic.
MgCl₂ -2326 -2525 Moderate difference: small, highly charged Mg²⁺ ion polarises Cl⁻ electron clouds.
AgCl -833 -905 Large difference (8.6%): Ag⁺ polarises the Cl⁻ ion, so the bonding has some covalent character.
AgI -736 -858 Large discrepancy (16.6% difference): large iodide ion is easily polarised by silver cation, introducing substantial covalent bonding.
Comparing the Born-Haber Value with the Perfect Ionic Model
  • If the two values are close, the compound is almost purely ionic (NaCl).
  • If the Born-Haber value is larger (more exothermic) than the perfect ionic model value, the bonding has some covalent character.
  • Example: AgCl. Perfect ionic model −833 kJ mol⁻¹; Born-Haber −905 kJ mol⁻¹. The Ag⁺ ion distorts (polarises) the electron cloud of Cl⁻. Some electron density is shared, so the lattice is stronger than the ionic model predicts.

6. Entropy (ΔS)

Entropy (S) is a quantitative measure of the disorder or randomness of a chemical system, measured in units of J K⁻¹ mol⁻¹. A system with higher randomness and more available energy distributions possesses higher entropy.

Factors Controlling Entropy

  • Physical State: Solids have the lowest entropy (ordered crystal lattice); liquids have moderate entropy; gases have the highest entropy (rapid, random molecular movement): S(solid) < S(liquid) << S(gas).
  • Number of Particles: Reactions that produce an increase in the number of moles of gas exhibit a large positive entropy change (ΔS > 0).
  • Temperature: Increasing temperature increases molecular kinetic energy and rotational/vibrational microstates, increasing entropy.

The standard entropy change of a chemical reaction is calculated as:

ΔS = Σ[S(products)] − Σ[S(reactants)]

Predicting the Sign of ΔS

  • Melting and boiling increase entropy (ΔS positive). Particles become more disordered: solid → liquid → gas.
  • Dissolving a solid usually increases entropy. The ions or molecules spread out through the solution.
  • A reaction that makes more moles of gas has a positive ΔS. A reaction that makes fewer moles of gas has a negative ΔS.
Worked Example: ΔS and Feasibility for the Haber Process
N₂(g) + 3H₂(g) → 2NH₃(g)   ΔH = −92 kJ mol⁻¹
Standard entropies (J K⁻¹ mol⁻¹): N₂ = 192, H₂ = 131, NH₃ = 193
(a) Calculate ΔS. (b) Find the temperature at which ΔG = 0.

(a) Step 1: Products minus reactants:

ΔS = 2(193) − [192 + 3(131)] = 386 − 585 = −199 J K⁻¹ mol⁻¹

ΔS is negative because 4 moles of gas become 2 moles of gas.

(b) Step 2: Convert units. ΔS is in J K⁻¹ mol⁻¹ but ΔH is in kJ mol⁻¹. Either divide ΔS by 1000 (−0.199 kJ K⁻¹ mol⁻¹) or multiply ΔH by 1000 (−92 000 J mol⁻¹).

Step 3: Set ΔG = 0, so T = ΔH / ΔS:

T = −92 000 / −199 = 462 K

ΔH and ΔS are both negative, so the reaction is feasible below 462 K. Above this temperature, the positive −TΔS term is bigger in size than the negative ΔH, so ΔG is positive.

7. Gibbs Free Energy (ΔG) & Feasibility

Whether a chemical reaction is thermodynamically feasible depends on both the enthalpy change (ΔH) and the entropy change (ΔS), linked through temperature (T in Kelvin) via the Gibbs free energy equation:

ΔG = ΔH − TΔS

Criterion for Reaction Feasibility A chemical reaction is thermodynamically feasible at a given temperature if and only if ΔG ≤ 0.
Unit Reconciliation Warning (kJ vs J)

ΔH is usually given in kJ mol⁻¹, while ΔS is given in J K⁻¹ mol⁻¹. To use the Gibbs equation correctly, you MUST convert ΔS into kJ K⁻¹ mol⁻¹ by dividing by 1000 before evaluating ΔG!

Enthalpy Change (ΔH) Entropy Change (ΔS) Gibbs Equation Term (−TΔS) Feasibility Outcome
Exothermic (ΔH < 0) Positive (ΔS > 0) Always negative Feasible at all temperatures (ΔG < 0 always).
Endothermic (ΔH > 0) Negative (ΔS < 0) Always positive Never feasible at any temperature (ΔG > 0 always).
Endothermic (ΔH > 0) Positive (ΔS > 0) Negative at high T Feasible only above threshold temperature: T ≥ ΔH / ΔS.
Exothermic (ΔH < 0) Negative (ΔS < 0) Positive at high T Feasible only below threshold temperature: T ≤ ΔH / ΔS.

Calculating the Threshold Feasibility Temperature

At the exact boundary where a reaction transitions from non-feasible to feasible, ΔG = 0:

0 = ΔH − TΔS ⇒ T = ΔH / ΔS

Linear Graphical Analysis (ΔG vs T)

Plotting ΔG on the y-axis against absolute temperature T on the x-axis gives a straight line following y = mx + c:

  • y-intercept: ΔH
  • Gradient: −ΔS (negative of entropy change)
  • x-intercept: Feasibility transition temperature (T = ΔH / ΔS)

8. Worked Calculations

Worked Example 1: Born-Haber Calculation for NaCl
Calculate the standard lattice enthalpy of formation for sodium chloride using the following experimental thermodynamic data:
ΔHf[NaCl(s)] = −411 kJ mol⁻¹
ΔHat[Na(s)] = +107 kJ mol⁻¹
First ionisation energy of Na = +496 kJ mol⁻¹
ΔatH (½Cl₂(g) → Cl(g)) = +122 kJ mol⁻¹
First electron affinity of Cl = −348 kJ mol⁻¹

Step 1: Write out the Hess's Law relationship:

ΔHf = ΔHat(Na) + IE₁(Na) + ΔHat(Cl) + ΔHEA1(Cl) + ΔHlatt

Step 2: Substitute the known values:

−411 = (+107) + (+496) + (+122) + (−348) + ΔHlatt

−411 = +377 + ΔHlatt

Step 3: Solve for ΔHlatt:

ΔHlatt = −411 − 377 = −788 kJ mol⁻¹

The standard lattice enthalpy of formation of sodium chloride is −788 kJ mol⁻¹ (or lattice dissociation enthalpy = +788 kJ mol⁻¹).

Worked Example 2: Feasibility Temperature for CaCO₃ Decomposition
For the thermal decomposition of calcium carbonate:
CaCO₃(s) → CaO(s) + CO₂(g)
ΔH = +178 kJ mol⁻¹ and ΔS = +161 J K⁻¹ mol⁻¹.
Calculate the minimum temperature in Kelvin at which this decomposition becomes thermodynamically feasible.

Step 1: Reconcile units between enthalpy and entropy:

ΔH = +178 kJ mol⁻¹

ΔS = +161 / 1000 = +0.161 kJ K⁻¹ mol⁻¹

Step 2: Set ΔG = 0 for the feasibility threshold:

ΔG = ΔH − TΔS = 0

T = ΔH / ΔS

Step 3: Calculate the threshold temperature:

T = 178 / 0.161 = 1105.6 K (or 832.6 °C)

At temperatures above 1106 K, TΔS exceeds ΔH, causing ΔG to become negative and making decomposition feasible.

Worked Example 3: Using a Born-Haber Cycle to Find the Electron Affinity
A Born-Haber cycle can find any one missing term, not only the lattice enthalpy. Use the data (kJ mol⁻¹) to find the first electron affinity of chlorine.
Lattice enthalpy of formation of NaCl = −788
ΔfH(NaCl) = −411
ΔatH(Na) = +107; ΔatH(Cl) = +122
First IE(Na) = +496

Step 1: Write the Hess's law relationship:

ΔfH = ΔatH(Na) + ΔatH(Cl) + IE₁(Na) + EA(Cl) + lattice formation

Step 2: Substitute:

−411 = 107 + 122 + 496 + EA − 788

−411 = −63 + EA

Step 3: Rearrange:

EA = −411 + 63 = −348 kJ mol⁻¹

The value is negative, as expected for a first electron affinity.

Go deeper

These UK AQA pages cover the same ideas in more detail. They may include content that is not in 9620.

Exam-Style Practice Questions

Test your understanding of these core syllabus concepts with targeted questions and detailed explanations.

Question 1: Why is the second electron affinity of oxygen endothermic (+798 kJ mol⁻¹)?

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Correct Answer: B

The O⁻ ion already carries a net negative charge. Adding a second electron requires energy to overcome the repulsive force between like negative charges.

Question 2: The theoretical lattice enthalpy of silver iodide is −736 kJ mol⁻¹, whereas the experimental Born-Haber value is −858 kJ mol⁻¹. What accounts for this discrepancy?

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Correct Answer: B

Large iodide ions are easily distorted (polarised) by silver cations. This electron cloud sharing introduces partial covalent bonding, making the crystal lattice stronger than predicted by the pure ionic model.

Question 3: A reaction has ΔH = −85 kJ mol⁻¹ and ΔS = −120 J K⁻¹ mol⁻¹. Under what temperature conditions is this reaction thermodynamically feasible?

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Correct Answer: B

When ΔH < 0 and ΔS < 0, the −TΔS term is positive. For ΔG to remain negative, the temperature must be low enough so that −TΔS does not outweigh the exothermic ΔH.

Question 4: On a graph of ΔG versus absolute temperature T, what chemical quantities are represented by the gradient and y-intercept?

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Correct Answer: B

Comparing ΔG = −ΔS × T + ΔH to y = mx + c shows that the gradient m = −ΔS and the y-intercept c = ΔH.

Question 5 (3 marks): Use the data (kJ mol⁻¹) to calculate the lattice enthalpy of formation of magnesium oxide, MgO. ΔfH(MgO) = −602; ΔatH(Mg) = +148; first IE(Mg) = +738; second IE(Mg) = +1451; ΔatH(O) = +249; first EA(O) = −141; second EA(O) = +798.

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Answer

Sum of steps from the elements to the gaseous ions = 148 + 738 + 1451 + 249 − 141 + 798 = +3243 kJ mol⁻¹.
Lattice formation = −602 − 3243 = −3845 kJ mol⁻¹.

Mark points

  • Both ionisation energies and both electron affinities included (second EA positive)
  • Sum of steps = +3243
  • Lattice enthalpy of formation = −3845 kJ mol⁻¹ (sign needed)

Question 6 (2 marks): Calculate the enthalpy of solution of potassium bromide, KBr. Lattice dissociation enthalpy of KBr = +679 kJ mol⁻¹; enthalpy of hydration of K⁺ = −322 kJ mol⁻¹; enthalpy of hydration of Br⁻ = −335 kJ mol⁻¹. State whether the solution warms or cools as KBr dissolves.

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Answer

ΔsolH = +679 + (−322) + (−335) = +22 kJ mol⁻¹. The value is positive (endothermic), so the solution cools.

Mark points

  • ΔsolH = lattice dissociation + sum of hydration enthalpies = +22 kJ mol⁻¹
  • Endothermic, so the temperature of the solution falls

Question 7 (4 marks): 2SO₂(g) + O₂(g) → 2SO₃(g), ΔH = −197 kJ mol⁻¹. Standard entropies (J K⁻¹ mol⁻¹): SO₂ = 248, O₂ = 205, SO₃ = 257. Calculate ΔS and the temperature above which the reaction is no longer feasible.

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Answer

ΔS = 2(257) − [2(248) + 205] = 514 − 701 = −187 J K⁻¹ mol⁻¹.
At ΔG = 0, T = ΔH / ΔS = −197 000 / −187 = 1053 K (1050 K to 3 s.f.).
Both ΔH and ΔS are negative, so the reaction is feasible below 1053 K and not feasible above it.

Mark points

  • ΔS = −187 J K⁻¹ mol⁻¹
  • Units converted (ΔH in J mol⁻¹, or ΔS in kJ K⁻¹ mol⁻¹)
  • T = ΔH / ΔS = 1053 K
  • Not feasible above this temperature, because the positive −TΔS term outweighs the negative ΔH, so ΔG > 0

Question 8 (2 marks): Predict the sign of ΔS for each change and give a reason: (a) H₂O(l) → H₂O(g); (b) CaCO₃(s) → CaO(s) + CO₂(g).

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Answer

(a) Positive: a liquid becomes a gas, so the particles are more disordered.
(b) Positive: a solid makes a gas, so the number of moles of gas increases from 0 to 1.

Mark points

  • (a) Positive, liquid to gas (more disorder)
  • (b) Positive, moles of gas increase