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Eduqas A-level Chemistry (A410QS) · PI4 — Energy changes
Mini-Lesson

PI4 · Energy changes

Eduqas PI4 asks the deepest question in chemistry: why do reactions go? You will define the enthalpy terms precisely, build Born-Haber cycles to find lattice enthalpies, compare them with the perfect ionic model, calculate enthalpies of solution, and use entropy and ΔG = ΔH − TΔS to decide feasibility.

Born-Haber entropy ΔG and feasibility enthalpy alone never tells the whole story

Work through each screen, answer every question as you go — the multiple-choice checks, the calculations and the sorting games — and collect ⭐ stars. Press Start when you are ready.

PI4 · definitions

The enthalpy definitions — say them exactly

Marks are lost here for sloppiness. Each definition needs: one mole, the state symbols, and standard conditions.

  • Enthalpy of atomisation — the enthalpy when one mole of gaseous atoms is formed from the element in its standard state. Always endothermic. Na(s) → Na(g)
  • First ionisation energy — one mole of gaseous 1+ ions from one mole of gaseous atoms. Always endothermic.
  • First electron affinity — one mole of gaseous 1− ions from one mole of gaseous atoms. Exothermic (the electron is attracted to the nucleus).
  • Second electron affinityendothermic, because you must force a second electron onto an ion that is already negative.
  • Lattice enthalpy of formation — one mole of an ionic solid from its gaseous ions. Strongly exothermic. Na⁺(g) + Cl⁻(g) → NaCl(s)
  • Enthalpy of hydration — one mole of gaseous ions dissolved in an excess of water. Exothermic.
  • Enthalpy of solution — one mole of solute dissolved to infinite dilution. Can be either sign.
Match it

Match the definitions

Tap a definition on the left, then the term it defines.

Definition
Term
PI4 · Born-Haber

The Born-Haber cycle

Lattice enthalpy cannot be measured directly, so we get it by Hess's law — via a route through gaseous atoms and ions.

ΔHf = ΔHat(metal) + IE + ΔHat(non-metal) + EA + ΔHlattrearranged: ΔH(latt) = ΔH(f) − [everything else]
Worked example — sodium chloride

ΔHf(NaCl) = −411 · ΔHat(Na) = +107 · IE₁(Na) = +496 · ΔHat(Cl) = +122 · EA₁(Cl) = −349 (all kJ mol⁻¹)

Sum of the "up and over" route: 107 + 496 + 122 + (−349) = +376

ΔHlatt = −411 − 376 = −787 kJ mol⁻¹

Two multiplication traps: for MgCl₂ you need IE₁ + IE₂ for the magnesium, and 2 × the atomisation enthalpy and 2 × the electron affinity for the chlorine. For an oxide you need the endothermic second electron affinity.

Calculate

Your turn — lattice enthalpy of NaCl

1Using ΔHf(NaCl) = −411, ΔHat(Na) = +107, IE₁(Na) = +496, ΔHat(Cl) = +122, EA₁(Cl) = −349 (kJ mol⁻¹), calculate the lattice enthalpy of formation of NaCl. Include the sign.
kJ mol⁻¹
Hint: ΔH(latt) = ΔH(f) − [107 + 496 + 122 − 349] = −411 − 376.
Calculate

Your turn — lattice enthalpy of MgCl₂

2Calculate the lattice enthalpy of formation of MgCl₂ from: ΔHf = −641, ΔHat(Mg) = +148, IE₁(Mg) = +738, IE₂(Mg) = +1451, ΔHat(Cl) = +122, EA₁(Cl) = −349 (kJ mol⁻¹). Include the sign. Remember there are two chlorines.
kJ mol⁻¹
Hint: sum = 148 + 738 + 1451 + (2 × 122) + (2 × −349) = 148 + 738 + 1451 + 244 − 698 = 1883. Then ΔH(latt) = −641 − 1883.
PI4 · ionic model

The perfect ionic model and covalent character

A theoretical lattice enthalpy can be calculated by assuming perfectly spherical ions with evenly distributed charge. Lattice enthalpy becomes more exothermic when the ions have a higher charge and a smaller radius — that is, a higher charge density.

Comparing the theoretical value with the experimental Born-Haber value is a test of the model:

  • Close agreement (e.g. NaCl) → the compound is close to purely ionic.
  • Experimental value much more exothermic than theoretical (e.g. AgI, ZnS) → there is significant covalent character. The small, highly charged cation polarises the large, easily-polarised anion, distorting its electron cloud and pulling charge into the space between the ions — extra attraction the ionic model never accounted for.

This is Fajans' reasoning: polarising power rises with small, highly charged cations; polarisability rises with large anions.

Quick check

Why the discrepancy?

?For silver iodide, the experimental (Born-Haber) lattice enthalpy is much more exothermic than the value from the perfect ionic model. What does this tell you?
PI4 · solution

Enthalpy of solution

Dissolving an ionic solid is a two-step Hess cycle: break the lattice apart into gaseous ions (endothermic — the reverse of lattice formation), then hydrate those gaseous ions (exothermic).

ΔHsol = ΣΔHhyd − ΔHlatt(formation)the minus sign is because you must REVERSE the lattice formation step

The two terms are large and nearly cancel, so ΔHsol is small — and can be either sign. That is why some salts dissolve with warming and others (ammonium nitrate in a cold pack) with cooling.

Hydration enthalpy becomes more exothermic for smaller, more highly charged ions, because the δ+ or δ− ends of the water molecules are attracted more strongly. Mg²⁺ hydrates far more exothermically than Na⁺.

Calculate

Your turn — enthalpy of solution

3For NaCl: ΔHlatt(formation) = −787, ΔHhyd(Na⁺) = −406, ΔHhyd(Cl⁻) = −363 (kJ mol⁻¹). Calculate ΔHsol. Include the sign.
kJ mol⁻¹
Hint: ΔH(sol) = [(−406) + (−363)] − (−787) = −769 + 787.
PI4 · entropy

Entropy

Entropy, S, measures the number of ways energy and particles can be arranged — loosely, the disorder. Units: J K⁻¹ mol⁻¹ (note: joules, not kilojoules).

  • Entropy rises: solid < liquid << gas. The biggest jumps come with boiling and with any reaction that increases the number of gas molecules.
  • A perfect crystal at 0 K has S = 0.
ΔS = ΣS(products) − ΣS(reactants)multiply each standard entropy by its coefficient

Quick prediction: count the moles of gas on each side. More gas out than in → ΔS is positive. That single check answers most exam questions.

Calculate

Your turn — entropy change

4Calculate ΔS for CaCO₃(s) → CaO(s) + CO₂(g), using standard entropies in J K⁻¹ mol⁻¹: CaCO₃ = 92.9, CaO = 39.7, CO₂ = 213.8. Include the sign.
J K⁻¹ mol⁻¹
Hint: ΔS = (39.7 + 213.8) − 92.9 = 253.5 − 92.9. A gas is produced, so it must be positive.
PI4 · free energy

Free energy and feasibility

ΔG = ΔH − TΔSa reaction is FEASIBLE when ΔG ≤ 0 · T in kelvin

The units trap that costs the most marks: ΔH is in kJ mol⁻¹ but ΔS is in J K⁻¹ mol⁻¹. Divide ΔS by 1000 before you subtract.

Four combinations, and only four:

  • ΔH negative, ΔS positive → ΔG negative at all temperatures. Always feasible.
  • ΔH positive, ΔS negative → ΔG positive at all temperatures. Never feasible.
  • ΔH positive, ΔS positive → feasible only at high T (TΔS must outweigh ΔH).
  • ΔH negative, ΔS negative → feasible only at low T.

At the borderline ΔG = 0, so the minimum (or maximum) feasible temperature is T = ΔH ÷ ΔS.

Calculate

Your turn — calculate ΔG

5For CaCO₃(s) → CaO(s) + CO₂(g), ΔH = +178 kJ mol⁻¹ and ΔS = +160.6 J K⁻¹ mol⁻¹. Calculate ΔG at 298 K, in kJ mol⁻¹. Include the sign.
kJ mol⁻¹
Hint: convert ΔS to kJ: 0.1606 kJ K⁻¹ mol⁻¹. ΔG = 178 − (298 × 0.1606) = 178 − 47.86.
Calculate

Your turn — the minimum temperature

6Calculate the minimum temperature, in K, at which the decomposition of CaCO₃ becomes feasible. (ΔH = +178 kJ mol⁻¹, ΔS = +160.6 J K⁻¹ mol⁻¹)
K
Hint: at the threshold ΔG = 0, so T = ΔH ÷ ΔS = 178 ÷ 0.1606.
Quick check

Feasible at every temperature

?A reaction has ΔH = −150 kJ mol⁻¹ and ΔS = +80 J K⁻¹ mol⁻¹. At which temperatures is it feasible?
Sort it

When is it feasible?

Tap a pair of ΔH and ΔS values, then the box saying when ΔG becomes negative. Remember ΔG = ΔH − TΔS.

♾️ Feasible at ALL temperatures

🔥 Feasible only at HIGH T

❄️ Feasible only at LOW T

Quick check

Never feasible

?Which combination makes a reaction thermodynamically impossible at every temperature?
PI4 · the limits of ΔG

What ΔG does and does not tell you

ΔG is a thermodynamic quantity. A negative ΔG means the reaction can happen — it says nothing at all about how fast.

Diamond → graphite has a negative ΔG at room temperature. Diamonds do not visibly turn to pencil lead, because the activation energy for rearranging the covalent lattice is enormous. The reaction is feasible but kinetically inert.

Also note: ΔG = 0 is exactly the condition for equilibrium. And ΔG relates to the cell potential by ΔG = −nFE°cell, which is why a positive E°cell means a feasible reaction — the same idea in two languages.

Recap

The big ideas to know

Definitions: one mole, correct state symbols; 2nd electron affinity is ENDOthermic

Born-Haber: ΔH(latt) = ΔH(f) − [atomisation + IEs + atomisation + EAs]

Ionic model: experimental much more exothermic than theoretical means covalent character

Solution: ΔH(sol) = ΣΔH(hyd) − ΔH(latt formation)

Entropy: S in J K⁻¹ mol⁻¹; count the moles of gas to predict the sign of ΔS

Free energy: ΔG = ΔH − TΔS — divide ΔS by 1000 first! Feasible when ΔG ≤ 0

Threshold: T = ΔH ÷ ΔS at the point where ΔG = 0

Caveat: feasible is not the same as fast (diamond → graphite)

That is the whole of PI4. Press Finish to see your score.

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