Checkpoint 3 — IQ3: Entropy & Gibbs Free Energy
Covering Lessons 11–13: entropy definition & prediction, calculating ΔS°, the Third Law, Gibbs free energy, spontaneity, and the Haber process paradox.
What’s Covered
- Entropy as microstates
- Units: J K⁻¹ mol⁻¹
- Predicting ΔS sign (Δn(gas))
- Second Law of Thermodynamics
- Third Law: S = 0 at 0 K
- S°(elements) ≠ 0
- ΔS° = ΣS°(products) − ΣS°(reactants)
- J → kJ conversion for L13
- ΔG = ΔH − TΔS
- ΔG < 0 → spontaneous
- Four ΔH/ΔS combinations
- Tcross = ΔH/ΔS
Multiple Choice — 10 marks
1. Entropy is best defined as:
2. For $2\text{H}_2\text{O}_2\text{(l)} \to 2\text{H}_2\text{O(l)} + \text{O}_2\text{(g)}$, the sign of ΔS is:
3. An endothermic reaction can be spontaneous if:
4. A student writes: "S°[N₂(g)] = 0 because N₂ is an element in its standard state." This is incorrect because:
5. For $\text{N}_2\text{(g)} + 3\text{H}_2\text{(g)} \to 2\text{NH}_3\text{(g)}$:
S°[N₂(g)] = 191.6, S°[H₂(g)] = 130.7, S°[NH₃(g)] = 192.4 J K⁻¹ mol⁻¹. What is ΔS°?
6. For $\Delta G = \Delta H - T\Delta S$, which unit conversion must be performed before substituting ΔS°?
7. A reaction has ΔH° = −45 kJ mol⁻¹ and ΔS° = +120 J K⁻¹ mol⁻¹. This reaction is:
8. A reaction has ΔH° = +120 kJ mol⁻¹ and ΔS° = +200 J K⁻¹ mol⁻¹. What is the crossover temperature (T where ΔG = 0)?
9. The Haber process (N₂ + 3H₂ → 2NH₃, ΔH < 0, ΔS < 0) is run at 400–500°C. At this temperature, ΔG is:
10. Diamond is thermodynamically spontaneous to convert to graphite at 25°C (ΔG < 0). This means:
Short Answer — 20 marks
Q11 (4 marks)
For each reaction, predict the sign of ΔS and give a brief justification:
(a) $\text{CaCO}_3\text{(s)} \to \text{CaO(s)} + \text{CO}_2\text{(g)}$
(b) $2\text{H}_2\text{(g)} + \text{O}_2\text{(g)} \to 2\text{H}_2\text{O(l)}$
(c) $\text{NH}_4\text{NO}_3\text{(s)} \to \text{NH}_4^+\text{(aq)} + \text{NO}_3^-\text{(aq)}$ (dissolution)
(d) $\text{N}_2\text{O}_4\text{(g)} \to 2\text{NO}_2\text{(g)}$
(a) ΔS > 0 — Δn(gas) = 1 − 0 = +1. CO₂ gas is produced from solid reactant only → large increase in microstates.
(b) ΔS < 0 — Δn(gas) = 0 − (2+1) = −3. Three moles of gas → zero moles of gas (liquid water) → major decrease in microstates and translational freedom.
(c) ΔS > 0 — ionic solid dissolves → NH₄⁺ and NO₃⁻ ions dispersed freely in aqueous solution. No gas change, but increased freedom of ions in solution → more microstates.
(d) ΔS > 0 — Δn(gas) = 2 − 1 = +1. One mole of gas → two moles of gas → more particles, more microstates.
Q12 (5 marks)
(a) Explain why $S°[\text{O}_2\text{(g)}] = 205.2 \text{ J K}^{-1}\text{mol}^{-1}$, while $\Delta H_f°[\text{O}_2\text{(g)}] = 0$. Reference the Third Law in your answer.
(b) Calculate ΔS° for: $\text{C(graphite)} + \text{O}_2\text{(g)} \to \text{CO}_2\text{(g)}$
S°: C(graphite) = 5.7, O₂(g) = 205.2, CO₂(g) = 213.8 J K⁻¹ mol⁻¹
(a) The Third Law of Thermodynamics states that the entropy of a perfect crystal at absolute zero (0 K) is exactly zero. This provides an absolute reference point — entropy can be measured as it accumulates from 0 K to any temperature. At 25°C (298 K), O₂(g) has been "warmed up" from 0 K through every energy input (heating as a solid, melting at 54 K, vaporising at 90 K, further heating as a gas to 298 K) — it has accumulated 205.2 J K⁻¹ mol⁻¹ of real entropy. In contrast, ΔHf°[O₂(g)] = 0 is a human convention — we arbitrarily define the enthalpy of elements in their standard state as zero (a relative reference). Entropy has an absolute physical zero; enthalpy does not. These are fundamentally different conventions.
(b) ΔS° = ΣS°(products) − ΣS°(reactants)
ΔS° = 213.8 − (5.7 + 205.2) = 213.8 − 210.9 = +3.0 J K⁻¹ mol⁻¹
Qualitative check: Δn(gas) = 1 − 1 = 0 → ΔS ≈ 0. The small positive value is consistent — no net change in moles of gas, but the very low S° of graphite (ordered solid, S° = 5.7) means the products have slightly more entropy overall. ✓
Q13 (6 marks)
For the decomposition of dinitrogen tetroxide: $\text{N}_2\text{O}_4\text{(g)} \to 2\text{NO}_2\text{(g)}$
ΔH° = +57.2 kJ mol⁻¹; ΔS° = +175.6 J K⁻¹ mol⁻¹
(a) Identify the ΔH/ΔS combination category and predict whether this reaction is spontaneous at low or high temperature.
(b) Calculate ΔG° at 25°C. Is the reaction spontaneous at 25°C?
(c) Calculate ΔG° at 100°C. Is the reaction spontaneous at 100°C?
(d) Calculate Tcross and convert to °C.
(a) ΔH > 0, ΔS > 0 → Row 4 (endothermic, more disorder). Prediction: spontaneous only at high temperature — the +TΔS term must grow large enough to outweigh the positive ΔH. Not spontaneous at low T; becomes spontaneous above Tcross.
(b) Convert: T = 298 K; ΔS = +175.6 ÷ 1000 = +0.1756 kJ K⁻¹ mol⁻¹
ΔG° = 57.2 − (298 × 0.1756) = 57.2 − 52.33 = +4.87 kJ mol⁻¹ > 0 → non-spontaneous at 25°C
Consistent with prediction — just below Tcross, so ΔG is barely positive.
(c) T = 100 + 273 = 373 K
ΔG° = 57.2 − (373 × 0.1756) = 57.2 − 65.50 = −8.3 kJ mol⁻¹ < 0 → spontaneous at 100°C
Consistent with prediction — above Tcross, so ΔG is negative. ✓
(d) Tcross = ΔH°/ΔS° = 57.2 / 0.1756 = 325.7 K = 52.7°C ≈ 53°C
Above 53°C: spontaneous. Below 53°C: non-spontaneous. This explains why the brown NO₂ gas is more prevalent at higher temperatures (e.g. in a warm flask vs cold flask — familiar from Module 5 equilibrium demonstrations).
Q14 (5 marks)
A student states: "A reaction with ΔH < 0 and ΔS < 0 will never be spontaneous because the negative entropy change works against it."
Evaluate this claim. In your answer: (i) identify the ΔH/ΔS category; (ii) explain using $\Delta G = \Delta H - T\Delta S$ when this reaction is spontaneous; (iii) give a real chemical example.
Evaluation: The student's claim is incorrect.
(i) ΔH < 0, ΔS < 0 corresponds to Row 3 in the four-combination table: spontaneous at low temperature; becomes non-spontaneous above Tcross.
(ii) Using ΔG = ΔH − TΔS: when ΔH < 0 and ΔS < 0, the TΔS term is negative (since ΔS < 0), so −TΔS is positive. The equation becomes: ΔG = (−ve) − (−ve) = (−ve) + (+ve). At low temperatures, the TΔS term is small (small T × |ΔS|), so the dominant term is the negative ΔH → ΔG < 0 (spontaneous). At high temperatures, T × |ΔS| becomes large, the positive contribution eventually exceeds |ΔH|, and ΔG becomes positive (non-spontaneous). The crossover temperature Tcross = ΔH/ΔS marks this transition.
(iii) Real example: The Haber process, N₂(g) + 3H₂(g) → 2NH₃(g), has ΔH° = −92.4 kJ mol⁻¹ and ΔS° = −198.9 J K⁻¹ mol⁻¹. At 25°C (298 K), ΔG° = −33.1 kJ mol⁻¹ → spontaneous. Above Tcross = 465 K (192°C), ΔG° becomes positive → non-spontaneous. The reaction is spontaneous, just not at high temperatures — directly disproving the student's claim. The negative ΔS "works against" spontaneity at high T but does not prevent spontaneity altogether at low T.
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