UPSC Civil Services (Mains), Chemistry optional · 2018 · Paper I
Q4(d)(i). Slopes of the fusion and sublimation curves of water
Question
Explain why fusion curve of ice has negative slope whereas sublimation curve has positive slope in the phase diagram.
Answer in brief
Clapeyron: dp/dT=Δ H/TΔ V. Both Δ_(fus)H and Δ_(sub)H are positive. Ice is less dense than water, so Δ_(fus)V<0 and the fusion slope is negative (-135 bar K⁻¹); on sublimation the volume increases enormously, so Δ_(sub)V>0 and the slope is positive.
Key points
- Along any two-phase line μ_α=μ_β, which gives the Clapeyron equation (dp)/(dT)=ΔₜᵣₛHT ΔₜᵣₛV. Melting and sublimation both absorb heat, so the sign of the slope is the sign of Δ V.
- ice has an open, hydrogen-bonded structure and is less dense than water (0.917 against 1.000 g cm⁻³ at 0°C). Melting shrinks the volume: Δ_(fus)V=18.02-19.65=-1.63 cm³ mol⁻¹. 2pt] (dp)/(dT)=6008273.15×(-1.63×10⁻⁶)= -1.35×10⁷…
- higher pressure lowers the melting point (by about 0.74 K per 100 bar). Pressure favours the denser phase, water (Le Chatelier).
- ice → vapour; Δ_(sub)H>0 and the vapour occupies far more volume than the solid, Δ_(sub)V≈ Vₘ(g)=RT/p>0. The slope is positive: (dln p)/(dT)=Δ_(sub)HRT² (Clausius–Clapeyron), and the vapour pressure of ice rises steeply with T.
The full model answer
Written out in full, as it should go in the answer booklet. The solution page with its diagrams follows it.
- Along any two-phase line μ_α=μ_β, which gives the Clapeyron equation (dp)/(dT)=ΔₜᵣₛHT ΔₜᵣₛV. Melting and sublimation both absorb heat, so the sign of the slope is the sign of Δ V.
- Fusion: ice has an open, hydrogen-bonded structure and is less dense than water (0.917 against 1.000 g cm⁻³ at 0°C). Melting shrinks the volume: Δ_(fus)V=18.02-19.65=-1.63 cm³ mol⁻¹. 2pt] (dp)/(dT)=6008273.15×(-1.63×10⁻⁶)= -1.35×10⁷ Pa K⁻¹ (-135 bar K⁻¹)
- The line leans to the left: higher pressure lowers the melting point (by about 0.74 K per 100 bar). Pressure favours the denser phase, water (Le Chatelier).
- Sublimation: ice → vapour; Δ_(sub)H>0 and the vapour occupies far more volume than the solid, Δ_(sub)V≈ Vₘ(g)=RT/p>0. The slope is positive: (dln p)/(dT)=Δ_(sub)HRT² (Clausius–Clapeyron), and the vapour pressure of ice rises steeply with T.
- Water is unusual; for most substances (CO₂) the solid is denser and the fusion line leans to the right.
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All parts of Question 4
- 4(a)(i) Crystal defects; stoichiometric defects10 marks
- 4(a)(ii) Conduction in semiconductors5 marks
- 4(b)(i) Why PVᵞ is constant in an adiabatic and PV in an isothermal change5 marks
- 4(b)(ii) Cold air descending into a valley5 marks
- 4(c)(i) Effusion of H₂ and N₂ through a fine glass filter10 marks
- 4(c)(ii) Vapour and gas from the critical temperature5 marks
- 4(d)(i) Slopes of the fusion and sublimation curves of water5 marks
- 4(d)(ii) Three liquid–liquid phase diagrams5 marks