Q3(a)(i). Signs of Δ H and Δ G when hot tea cools
At constant pressure, the temperature of a fixed amount of hot tea in a cup decreases spontaneously to room temperature. What will be the sign of (I) Δ H and (II) Δ G of this process? Give reason(s) in support of your answer.
Answer in brief
(I) Δ H<0: heat leaves the tea at constant pressure. (II) Δ G of the tea (the system) is positive: G rises as T falls, (∂ G/∂ T)ₚ=-S. The test "Δ G<0 for a spontaneous change" holds only at constant T and p; here T falls, and the spontaneity shows as Δ Sₜₒₜₐₗ>0.
Key points
- Sign of Δ H. At constant pressure, with no work other than expansion, Δ H=qₚ. The tea gives heat to the room, qₚ<0, so Δ H<0. In numbers: Δ H=∫_Tₕₒₜ^(T₀)Cₚ dT=Cₚ(T₀-Tₕₒₜ)<0.
- Sign of Δ G. G is a state function, and at constant pressure dG=-S dT. The tea has S>0 and dT<0, so Δ G=-∫_Tₕₒₜ^(T₀)S dT>0Δ G>0 The Gibbs energy of the tea rises as it cools (G=H-TS; TS falls more than H).
- No contradiction. Δ G≤0 is the test of spontaneity only for a change at constant T and p. The tea's temperature changes, so its Δ G says nothing about spontaneity.
- The real criterion is the total entropy. Tea: Δ Sₜₑₐ=Cₚln(T₀/Tₕₒₜ)<0. Room (at T₀): Δ Sᵣₒₒₘ=-Δ H/T₀=Cₚ(Tₕₒₜ-T₀)/T₀>0. Since (x-1)>ln x for x=Tₕₒₜ/T₀>1, Δ Sₜₒₜₐₗ>0: the cooling is spontaneous.
The full model answer
Written out in full, as it should go in the answer booklet. The solution page with its diagrams follows it.
- Sign of Δ H. At constant pressure, with no work other than expansion, Δ H=qₚ. The tea gives heat to the room, qₚ<0, so Δ H<0. In numbers: Δ H=∫_Tₕₒₜ^(T₀)Cₚ dT=Cₚ(T₀-Tₕₒₜ)<0.
- Sign of Δ G. G is a state function, and at constant pressure dG=-S dT. The tea has S>0 and dT<0, so Δ G=-∫_Tₕₒₜ^(T₀)S dT>0Δ G>0 The Gibbs energy of the tea rises as it cools (G=H-TS; TS falls more than H).
- No contradiction. Δ G≤0 is the test of spontaneity only for a change at constant T and p. The tea's temperature changes, so its Δ G says nothing about spontaneity.
- The real criterion is the total entropy. Tea: Δ Sₜₑₐ=Cₚln(T₀/Tₕₒₜ)<0. Room (at T₀): Δ Sᵣₒₒₘ=-Δ H/T₀=Cₚ(Tₕₒₜ-T₀)/T₀>0. Since (x-1)>ln x for x=Tₕₒₜ/T₀>1, Δ Sₜₒₜₐₗ>0: the cooling is spontaneous.
- Numbers. One mole of tea taken as water, 80°C → 25°C (Cₚ=75.3 J K⁻¹ mol⁻¹, Sₘ=69.9 J K⁻¹ mol⁻¹ at 298 K): Δ H=-4.14 kJ; Δ Sₜₑₐ=-12.7 J K⁻¹; Δ Sᵣₒₒₘ=+13.9 J K⁻¹; Δ Sₜₒₜₐₗ=+1.1 J K⁻¹; Δ Gₜₑₐ=-∫ S dT=+4.21 kJ.
- Where "Δ G<0" comes from. The quantity that is negative is Δ H-T₀Δ Sₜₑₐ, the Gibbs energy change counted at the fixed room temperature T₀: Δ H-T₀Δ Sₜₑₐ=-T₀Δ Sₜₒₜₐₗ=-0.34 kJ. Answer keys that print Δ G<0 mean this; for the tea itself Δ G>0.
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All parts of Question 3
- 3(a)(i) Signs of Δ H and Δ G when hot tea cools10 marks
- 3(a)(ii) Units of a, b, c and Δ S, Δ H from Δ G=a+bT+cT²15 marks
- 3(b) Partial molar Gibbs energy (chemical potential)10 marks
- 3(c) Polonium: cubic class and cell edge from three Bragg reflections15 marks