Unit 10 · Physical Chemistry

Phase Diagrams

Phase equilibrium, homogeneous and heterogeneous equilibria, one-component and two-component phase diagrams, and their applications.

10.1

Phases and Phase Equilibrium

Phase A phase is a physically distinct, homogeneous region of a system that is separated from other regions by definite boundaries (interfaces). A phase has uniform composition and physical properties throughout. Examples: ice (solid phase), liquid water, and water vapour are three phases of H2O.

Types of Phases

  • Solid phase: fixed shape and volume; particles in fixed lattice positions.
  • Liquid phase: fixed volume, variable shape; particles mobile but in contact.
  • Gas/vapour phase: variable volume and shape; particles widely separated.
  • A system may have multiple solid phases (allotropes, polymorphs) e.g. graphite and diamond are two solid phases of carbon.
  • There is only ever one liquid phase for a single component (miscible liquids count as one phase; immiscible liquids count as two).
  • There is only ever one gas phase (all gases mix completely).
Phase Equilibrium A phase equilibrium exists when two or more phases coexist in the same system without any net change over time. At equilibrium, the rate of transition from phase A to phase B equals the rate from B to A. Example: ice and liquid water in equilibrium at 0°C and 1 atm.

Conditions for Phase Equilibrium

For two phases to be in equilibrium, they must have the same:

  • Temperature (thermal equilibrium)
  • Pressure (mechanical equilibrium)
  • Chemical potential of each component (chemical equilibrium)

The chemical potential (μ) is essentially the molar Gibbs free energy. At equilibrium: μsolid = μliquid = μvapour.

Homogeneous vs Heterogeneous Equilibria

Homogeneous Equilibrium

All species involved in the equilibrium are in the same phase. Example: N2(g) + 3H2(g) ⇌ 2NH3(g) — all gaseous.
Kc or Kp expressions include all species.

Heterogeneous Equilibrium

Species are in different phases. Example: CaCO3(s) ⇌ CaO(s) + CO2(g).
Concentrations of pure solids and liquids are constant → they are omitted from K expressions. Kp = p(CO2).

Examples of heterogeneous equilibria: CaCO3(s) <==> CaO(s) + CO2(g) Kp = p(CO2) H2O(l) <==> H2O(g) Kp = p(H2O) [vapour pressure] Fe3O4(s) + 4H2(g) <==> 3Fe(s) + 4H2O(g) Kp = [p(H2O)]^4 / [p(H2)]^4 I2(s) <==> I2(aq) Kc = [I2(aq)]
10.2

The Gibbs Phase Rule

Gibbs Phase Rule F = C − P + 2
where: F = degrees of freedom (number of intensive variables — T, P, composition — that can be independently varied without changing the number of phases); C = number of components; P = number of phases present.

Understanding the Variables

  • Components (C): minimum number of chemically independent species needed to describe all phases. For pure water: C = 1.
  • Phases (P): number of distinct phases present simultaneously.
  • Degrees of freedom (F): number of variables (T, P, concentration) you can change independently while keeping the same phases.
System (C=1, e.g. water)Phases (P)F = 1 − P + 2Meaning
Single phase region (e.g. liquid only)1F = 2Both T and P can vary — bivariant
Two-phase equilibrium (e.g. liquid + vapour)2F = 1Fix T → P fixed (or vice versa) — univariant
Triple point (solid + liquid + vapour)3F = 0T and P both fixed — invariant
Example 1

Applying the Phase Rule

Apply the Gibbs phase rule to: (a) liquid water only; (b) water at its boiling point (liquid + vapour); (c) water at its triple point.

a
C=1, P=1: F = 1 − 1 + 2 = 2. Both T and P can be varied independently while keeping water in liquid phase. Bivariant system.
b
C=1, P=2: F = 1 − 2 + 2 = 1. Fix temperature → boiling point pressure fixed (or vice versa). Univariant — vapour pressure curve.
c
C=1, P=3: F = 1 − 3 + 2 = 0. Invariant — the triple point exists at one unique T and P only (0.006 atm, 0.0098°C for water). Cannot be varied at all.
10.3

One-Component Phase Diagrams

General Features of a One-Component Phase Diagram

A one-component (single substance) phase diagram plots pressure (P) on the y-axis and temperature (T) on the x-axis. It shows which phase (solid, liquid, gas) is stable at each combination of T and P.

Key Features

  • Phase regions (areas): single-phase stable regions (F=2). Solid, liquid, or gas/vapour.
  • Phase boundary curves (lines): two-phase equilibria (F=1). Three important curves:
    • Sublimation curve (solid ⇌ gas): below triple point.
    • Vapour pressure/vaporisation curve (liquid ⇌ gas): from triple point to critical point.
    • Fusion/melting curve (solid ⇌ liquid): from triple point upward.
  • Triple point (Tt, Pt): all three phases in equilibrium (F=0). Unique T and P.
  • Critical point (Tc, Pc): above this, liquid and gas phases are indistinguishable (supercritical fluid). End of vaporisation curve.
Critical Point (Tc, Pc) Triple Point (Tt, Pt) SOLID LIQUID GAS / VAPOUR Sublimation Vaporisation Fusion Temperature (T) → Pressure (P) → 1 atm Normal MP Normal BP

General one-component phase diagram (schematic)

Reading the Phase Diagram

  • The normal melting point is the T at which the fusion curve intersects P = 1 atm.
  • The normal boiling point is the T at which the vaporisation curve intersects P = 1 atm.
  • At T and P above the critical point, the substance exists as a supercritical fluid — cannot be liquefied by increasing pressure alone.
  • Moving horizontally (constant P) across phase boundaries = heating/cooling transitions.
  • Moving vertically (constant T) across phase boundaries = pressure-induced transitions.
10.4

Phase Diagram of Water

Key Data for Water

FeatureValueNotes
Triple pointT = 0.0098°C, P = 611 Pa (0.006 atm)Solid + liquid + vapour coexist
Normal melting point0°C at 1 atmFusion curve at 1 atm
Normal boiling point100°C at 1 atmVaporisation curve at 1 atm
Critical pointT = 374°C, P = 218 atmAbove this: supercritical water

Anomalous Feature: Negative Slope of Fusion Curve

The fusion curve (ice–water boundary) has a negative slope — uniquely different from most substances. This means that increasing pressure at constant temperature melts ice (converts solid to liquid).

Reason: Ice (solid) is less dense than liquid water (density: ice = 0.917 g/cm³, water = 1.00 g/cm³). Ice has an open hexagonal lattice with H-bonds; liquid water is more compact. By Le Chatelier's principle, increasing pressure favours the denser phase (liquid) → melting occurs.

Most substances have a positive slope fusion curve (solid denser than liquid).

Triple Point 0.0098°C, 611 Pa Critical Point 374°C, 218 atm ICE LIQUID WATER WATER VAPOUR 1 atm 0°C 100°C Fusion (neg. slope) Temperature → Pressure →

Phase diagram of water (schematic — not to scale)

📌
Why Ice Skates Work One classical explanation was that the pressure from the blade melts ice, creating a lubricating liquid layer. However, modern research shows the pressure effect is too small at typical skating temperatures (−10°C requires ~100 atm to melt). The primary mechanism is now understood to be frictional heating and a quasi-liquid layer naturally present on ice surfaces.
Example 2

Interpreting the Water Phase Diagram

Using the water phase diagram: (a) What phase(s) exist at 50°C and 1 atm? (b) What happens when water at 25°C is put under very high pressure? (c) Why does water boil at <100°C on a mountaintop?

a
At 50°C, 1 atm: this point is in the liquid water region (above the triple point temperature, below boiling point of 100°C, at 1 atm).
b
Liquid water at 25°C moving to higher pressure: moves upward on the diagram. The nearest phase boundary above is the fusion curve. Since the fusion curve has a negative slope, moving up eventually crosses it → water freezes under very high pressure (at 25°C you need ~2500 atm). This is different from most substances.
c
On a mountaintop, atmospheric pressure is lower than 1 atm. On the vaporisation curve, lower pressure corresponds to lower boiling temperature. So water boils at <100°C (e.g. ~90°C at 3000 m altitude where P ≈ 0.7 atm).
10.5

Phase Diagram of CO2

Key Data for CO2

FeatureValueNotes
Triple pointT = −56.6°C, P = 5.11 atmAll three phases coexist
Sublimation at 1 atm−78.5°CCO2 sublimates directly at normal pressure
Normal melting pointDoes not exist at 1 atm (triple point P > 1 atm)Liquid CO2 cannot exist at 1 atm
Critical pointT = 31.1°C, P = 73.8 atmSupercritical CO2 above this

Key Feature: Triple Point Above 1 atm

The triple point of CO2 occurs at 5.11 atm, which is above normal atmospheric pressure (1 atm). Therefore, at 1 atm, the solid–gas boundary is crossed directly — solid CO2 (dry ice) sublimates at −78.5°C without melting. Liquid CO2 can only exist at pressures above 5.11 atm.

Positive Slope of Fusion Curve (Normal)

Unlike water, CO2 has a positive slope on its fusion curve — solid CO2 is denser than liquid CO2. Increasing pressure at constant T favours the solid phase (Le Chatelier).

Supercritical CO2

Above 31.1°C and 73.8 atm, CO2 becomes a supercritical fluid — it has properties between a gas (low viscosity, high diffusivity) and a liquid (dissolves substances). Applications: supercritical CO2 extraction of caffeine from coffee, decaffeination; dry cleaning; extraction of essential oils; in HPLC (chromatography).

PropertyWaterCO2
Triple point pressure0.006 atm (<1 atm)5.11 atm (>1 atm)
Behaviour at 1 atm on heating solidMelts (solid → liquid → gas)Sublimates (solid → gas directly)
Fusion curve slopeNegative (anomalous)Positive (normal)
Solid denser than liquid?No (ice floats)Yes (normal)
Critical point374°C, 218 atm31.1°C, 73.8 atm
10.6

Two-Component Phase Diagrams

Vapour Pressure–Composition Diagrams (Raoult's Law)

For an ideal binary mixture of two miscible liquids A and B, the vapour pressure of each component follows Raoult's Law:

Raoult's Law: p_A = x_A * P_A* p_B = x_B * P_B* where: p_A = partial vapour pressure of A in mixture x_A = mole fraction of A in liquid phase P_A* = vapour pressure of pure A Total pressure: P_total = p_A + p_B = x_A*P_A* + x_B*P_B*

On a P–x diagram, the total pressure varies linearly with composition for an ideal mixture.

Boiling Point–Composition Diagram (T–x Diagram)

At constant pressure (usually 1 atm), the boiling point–composition diagram shows:

  • Liquid curve (bubble point curve): compositions and temperatures at which the liquid begins to boil.
  • Vapour curve (dew point curve): compositions and temperatures at which vapour begins to condense.
  • The region between the two curves = two-phase region (liquid + vapour in equilibrium).
LIQUID VAPOUR L + V xL xV Tie line Mole fraction of B (x_B) → A (pure) ←———————————→ B (pure) Temperature (T) → BP(A) BP(B) Liquid curve Vapour curve

T–x diagram for an ideal binary mixture (A more volatile, lower B.P.; B less volatile, higher B.P.)

The Lever Rule

At a point in the two-phase region, the relative amounts of liquid and vapour are given by the lever rule:

Moles of vapour / Moles of liquid = (x_overall - x_liquid) / (x_vapour - x_overall) where x_liquid and x_vapour are read from the ends of the tie line, and x_overall is the overall composition.

Azeotropes (Non-Ideal Mixtures)

Real mixtures may deviate from Raoult's law, forming azeotropes — mixtures with constant boiling point at a fixed composition:

  • Minimum-boiling azeotrope (positive deviation): e.g. ethanol–water (95.6% ethanol, B.P. 78.1°C). Cannot be separated beyond azeotrope composition by simple distillation.
  • Maximum-boiling azeotrope (negative deviation): e.g. HCl–water (20.2% HCl, B.P. 108.6°C). Mixture boils above both pure components.
10.7

Applications of Phase Diagrams

ApplicationPhase Diagram UsedDetails
Fractional distillation of petroleumMulti-component T–x diagramSeparation based on boiling point differences in complex mixture
Freeze-drying (lyophilisation)Water phase diagramReduce P below triple point → ice sublimates directly to vapour without passing through liquid phase. Used for food and pharmaceutical preservation.
Supercritical CO2 extractionCO2 phase diagramOperate above critical point (31.1°C, 73.8 atm). Supercritical CO2 dissolves caffeine, essential oils etc. without toxic solvents.
Pressure cookersWater phase diagramIncrease P above 1 atm → boiling point rises above 100°C → food cooks faster.
Autoclave sterilisationWater phase diagramSteam at 121°C (2 atm) kills all microbes; used in hospitals and labs.
Alloy solidificationTwo-component solid–liquid diagramEutectic point gives minimum melting temperature mixture (e.g. tin–lead solder).
Fractional distillation (ethanol–water)T–x diagram with azeotropeMaximum ethanol concentration by distillation = 95.6% (azeotrope). Pure ethanol requires molecular sieves or chemical drying.
Example 3

Freeze-Drying Using the Water Phase Diagram

Explain, with reference to the water phase diagram, how freeze-drying preserves food.

1
The food is first frozen — T is reduced below 0°C at atmospheric pressure, converting water to ice (moving left across fusion curve on phase diagram).
2
Pressure is then reduced below 611 Pa (the triple point pressure). The system is now below the triple point on the phase diagram.
3
At this low P, the ice is in the solid–gas region. Gentle heating causes the ice to sublime directly to vapour (crosses the sublimation curve) without passing through the liquid phase.
Result: food is dried without ever becoming liquid → structure and nutrients preserved, long shelf life, easily rehydrated.

No videos added yet for this unit.

✏️

Exercises

🧠

Interactive Quiz

Unit 10 Quiz — Phase Diagrams

25 Questions
Q1

A phase is defined as:

A phase is a physically distinct, homogeneous region of a system with uniform composition and properties, separated from other regions by definite boundaries. A substance can have multiple solid phases (e.g. allotropes).
Q2

The Gibbs phase rule is F = C − P + 2. For a pure substance at its triple point, F equals:

Triple point: C=1, P=3. F = 1−3+2 = 0. The system is invariant — T and P are both fixed at unique values. You cannot change either without losing one of the three phases.
Q3

What is the triple point of water?

The triple point of water is at 0.0098°C and 611 Pa (0.006 atm) — slightly above 0°C and well below 1 atm. At this unique point, all three phases (ice, liquid water, water vapour) coexist in equilibrium.
Q4

The fusion curve of water has a negative slope because:

Ice is less dense than liquid water (Vsolid > Vliquid). By Le Chatelier, increasing pressure favours the smaller-volume (denser) phase — liquid water. So increasing P at nearly 0°C causes melting → negative slope of the fusion curve. This is anomalous — most substances have a positive slope.
Q5

Why does dry ice (solid CO2) sublime at atmospheric pressure rather than melting?

CO2's triple point (5.11 atm) is above 1 atm. At atmospheric pressure, there is no liquid phase — the 1 atm isobar crosses the sublimation curve only. Solid CO2 therefore converts directly to vapour (sublimates) at −78.5°C.
Q6

Above the critical point, a substance exists as:

Above the critical temperature and pressure, there is no distinction between liquid and gas → the substance is a supercritical fluid with properties intermediate between a gas (low viscosity) and liquid (solvating ability).
Q7

For a one-component system along the vapour pressure curve (liquid + vapour equilibrium), F equals:

C=1, P=2: F = 1−2+2 = 1. Univariant — fixing T determines P (vapour pressure), and vice versa. The system has one degree of freedom along the curve.
Q8

The normal boiling point of a liquid is defined as the temperature at which:

The normal boiling point is where the vaporisation curve intersects P = 1 atm. The vapour pressure equals 1 atm, allowing bubbles to form throughout the liquid (bulk boiling).
Q9

In a heterogeneous equilibrium such as CaCO3(s) ⇌ CaO(s) + CO2(g), the equilibrium expression Kp is:

Pure solids have constant concentration (activity = 1) → omitted from K expressions. Only gaseous CO2 appears: Kp = p(CO2). This means the decomposition pressure of CO2 is constant at given T, regardless of amounts of solid.
Q10

Raoult's Law states that the partial vapour pressure of a component equals:

Raoult's Law: pA = xA × PA* — partial pressure = mole fraction in liquid × pure component vapour pressure. This holds for ideal mixtures where A–B intermolecular forces equal A–A and B–B forces.
Q11

In the T–x diagram for a binary mixture, the area between the liquid and vapour curves represents:

The region between the bubble point (liquid) curve and dew point (vapour) curve is the two-phase region: liquid and vapour coexist in equilibrium. The compositions of each phase are given by the ends of the tie line at that temperature.
Q12

The ethanol–water azeotrope at 95.6% ethanol is an example of:

Ethanol–water is a minimum-boiling azeotrope (positive deviation from Raoult's Law). It boils at 78.1°C — lower than pure ethanol (78.4°C) or water (100°C). Beyond 95.6% ethanol, distillation cannot proceed further. Pure ethanol requires molecular sieves.
Q13

Water boils at a lower temperature on a mountain than at sea level because:

The boiling point is where vapour pressure = external pressure. At altitude, atmospheric pressure is lower → the vaporisation curve is intersected at a lower temperature → water boils below 100°C. At 3000 m, P ≈ 0.7 atm and water boils at ~90°C.
Q14

Freeze-drying works by:

Freeze-drying: food is frozen (ice formed), then pressure is reduced below 611 Pa (triple point pressure of water). At this P, the system is in the solid–gas region of the water phase diagram. Ice sublimates directly to vapour, removing water without passing through liquid → preserves food structure.
Q15

Supercritical CO2 is used in coffee decaffeination because:

Supercritical CO2 (above 31.1°C, 73.8 atm) has gas-like diffusivity and liquid-like solvating power — it dissolves caffeine efficiently. Crucially, when pressure is released, CO2 returns to gas phase leaving no toxic solvent residue in the food. Safe and selective.
Q16

At the triple point of water, F = 0. This means:

F=0 means the system is invariant: both T (0.0098°C) and P (611 Pa) are uniquely determined. You cannot change either variable without destroying one of the three coexisting phases.
Q17

For a binary mixture of two components in a single liquid phase, F equals:

C=2, P=1: F = 2−1+2 = 3. T, P, and composition (e.g. mole fraction of one component) can all be independently varied while staying in the single-phase liquid region.
Q18

In a T–x diagram, a tie line connects:

A tie line is a horizontal line at constant T drawn across the two-phase region. Its endpoints on the liquid curve and vapour curve give the compositions of the liquid and vapour phases in equilibrium at that temperature. The lever rule uses the tie line to find relative amounts.
Q19

A pressure cooker works because:

Moving up the vapour pressure curve of water (higher P), the boiling point increases. A pressure cooker at ~2 atm raises the boiling point to ~121°C. Higher temperature = faster cooking (faster chemical reactions, faster protein denaturation).
Q20

The critical temperature is the temperature above which:

Above the critical temperature, no amount of pressure can liquefy the substance — liquid and vapour become indistinguishable (supercritical fluid). The kinetic energy is too high for intermolecular forces to maintain a distinct liquid phase.
Q21

The equilibrium H2O(l) ⇌ H2O(g) is an example of:

Heterogeneous equilibrium: reactant and product are in different phases (liquid and gas). Kp = p(H2O) — the concentration/activity of the pure liquid is constant and omitted.
Q22

For the ideal binary mixture of A and B, if xA = 0.6, PA* = 80 kPa and PB* = 40 kPa, the total vapour pressure is:

pA = 0.6 × 80 = 48 kPa; pB = 0.4 × 40 = 16 kPa; Ptotal = 48 + 16 = 64 kPa.
Q23

What does it mean if a binary mixture shows positive deviation from Raoult's Law?

Positive deviation: actual total vapour pressure > Raoult's Law prediction. Occurs when A–B intermolecular forces are weaker than A–A and B–B forces → molecules escape more easily → higher vapour pressure → minimum-boiling azeotrope possible.
Q24

Along the sublimation curve of a substance, the equilibrium is between:

The sublimation curve is the solid–gas boundary. Along this curve, solid and vapour are in equilibrium (F=1, univariant). It runs from absolute zero up to the triple point.
Q25

The lever rule in a two-phase region gives the:

The lever rule gives the relative amounts of two coexisting phases. Using the tie line: moles vapour/moles liquid = (xoverall − xliquid)/(xvapour − xoverall). Essential for understanding fractional distillation efficiency.
📝

Unit Test

ℹ️
Instructions Total: 50 marks  |  Time: 55 minutes  |  Attempt all questions  |  Show all working.

Section A — Short Answer

30 marks
Q1 [4 marks]

State the Gibbs phase rule and define each variable. Apply it to: (a) ice melting at 0°C and 1 atm; (b) liquid water at 60°C and 1 atm; (c) the triple point of water.

Phase rule: F = C − P + 2
F = degrees of freedom; C = number of components; P = number of phases.

(a) Ice melting (solid + liquid): C=1, P=2 → F = 1−2+2 = 1. Univariant — fixing T (0°C) fixes P (1 atm) along the fusion curve.
(b) Liquid water only: C=1, P=1 → F = 1−1+2 = 2. Bivariant — both T and P can be changed independently.
(c) Triple point: C=1, P=3 → F = 1−3+2 = 0. Invariant — T (0.0098°C) and P (611 Pa) are fixed uniquely.
Q2 [5 marks]

Sketch a labelled phase diagram for water (P vs T). On it, mark and label: (a) the three phase regions; (b) the triple point with its T and P values; (c) the critical point; (d) the normal melting point and normal boiling point; (e) the anomalous feature of the fusion curve and explain its significance.

Diagram should show:
Three regions: ICE (solid, top-left), LIQUID WATER (top-right), WATER VAPOUR (bottom-right).
Three boundary curves: sublimation (solid-gas, below triple point), vaporisation (liquid-gas, up to critical point), fusion (solid-liquid, from triple point upward).

(a) Regions clearly labelled with phases.
(b) Triple point at T = 0.0098°C, P = 611 Pa (0.006 atm).
(c) Critical point at T = 374°C, P = 218 atm (end of vaporisation curve).
(d) Normal M.P. = 0°C at 1 atm (intersection of fusion curve with P=1 atm); Normal B.P. = 100°C at 1 atm (intersection of vaporisation curve with P=1 atm).
(e) Anomalous feature: fusion curve has a negative slope (leans slightly to the left — higher P gives lower melting T). Significance: ice is less dense than liquid water; increasing pressure favours the denser phase (liquid) → melting. Opposite to most substances.
Q3 [5 marks]

Compare the phase diagrams of water and CO2, focusing on: (i) triple point pressure; (ii) behaviour at 1 atm on heating the solid; (iii) slope of fusion curve; (iv) properties of the solid vs liquid density. Explain one practical consequence of each difference.

(i) Triple point pressure: Water = 0.006 atm (below 1 atm); CO2 = 5.11 atm (above 1 atm).
Consequence: At 1 atm, water melts normally (solid→liquid→gas); dry ice sublimates (solid→gas directly). Dry ice useful for cooling without liquid mess.

(ii) Behaviour at 1 atm: Water: melts at 0°C then boils at 100°C. CO2: sublimates at −78.5°C (no liquid phase at 1 atm).

(iii) Fusion curve slope: Water: negative (anomalous). CO2: positive (normal).
Consequence: Increasing pressure on ice at ~0°C melts it (water pipe bursts in frost); increasing pressure on solid CO2 keeps it solid (used safely in pressurised fire extinguishers).

(iv) Density: Ice less dense than water (ice floats — critical for aquatic life to survive under ice). Solid CO2 denser than liquid CO2 (normal behaviour).
Q4 [5 marks]

Write Kp expressions for the following heterogeneous equilibria and explain why pure solids and liquids are excluded:
(a) CaCO3(s) ⇌ CaO(s) + CO2(g)
(b) 3Fe(s) + 4H2O(g) ⇌ Fe3O4(s) + 4H2(g)
(c) NH4HCO3(s) ⇌ NH3(g) + H2O(g) + CO2(g)

Why solids/liquids excluded: The concentration (activity) of a pure solid or pure liquid is constant at a given T (independent of amount present). Including them would just give a constant → by convention, their activity = 1 and they are omitted from K expressions.

(a) Kp = p(CO2)
(Both CaCO3 and CaO are pure solids.)

(b) Kp = [p(H2)]4 / [p(H2O)]4
(Fe and Fe3O4 are pure solids.)

(c) Kp = p(NH3) × p(H2O) × p(CO2)
(NH4HCO3 is a pure solid.)
Q5 [5 marks]

For an ideal binary mixture of hexane (P* = 150 mmHg) and heptane (P* = 45 mmHg) at 25°C:
(a) Calculate the total vapour pressure of a mixture with mole fraction of hexane xhex = 0.70.
(b) Calculate the mole fraction of hexane in the vapour phase above this mixture.
(c) Is the vapour richer or poorer in hexane compared to the liquid? What does this mean for distillation?

(a) phex = 0.70 × 150 = 105 mmHg
phep = 0.30 × 45 = 13.5 mmHg
Ptotal = 105 + 13.5 = 118.5 mmHg

(b) yhex (mole fraction in vapour) = phex/Ptotal = 105/118.5 = 0.886

(c) The vapour (yhex = 0.886) is richer in hexane than the liquid (xhex = 0.70). This makes sense because hexane is more volatile (higher P*). In distillation, the vapour phase is enriched in the more volatile component → repeated distillation (fractionation) progressively purifies hexane from the mixture.
Q6 [6 marks]

Explain the following, using phase diagrams in your answer:
(a) Why a pressure cooker allows food to cook faster at high altitude. [2]
(b) How supercritical CO2 is used in decaffeination of coffee. [2]
(c) Why mountaineers cannot make a proper cup of tea at very high altitude. [2]

(a) At high altitude, atmospheric pressure is lower than 1 atm. On the water phase diagram, moving down the vaporisation curve, lower P corresponds to lower boiling point → water boils at <100°C. A pressure cooker seals and pressurises above 1 atm, raising the boiling point above 100°C (e.g. 121°C at 2 atm). Higher T means faster chemical reactions → faster cooking. This compensates for the reduced atmospheric pressure.

(b) CO2 is brought to T > 31.1°C and P > 73.8 atm → supercritical fluid region on the CO2 phase diagram. Supercritical CO2 has gas-like diffusivity (penetrates coffee beans easily) and liquid-like solvating ability (dissolves caffeine). When pressure is released, CO2 returns to gas phase → leaves no toxic residue in coffee. Clean, efficient, selective extraction.

(c) At very high altitude (e.g. Everest base camp ~5300 m), atmospheric pressure ≈ 0.54 atm. The vaporisation curve of water is intersected at ~83°C. Tea requires >90°C to properly brew (extract flavour compounds, kill bacteria). Since water boils at only ~83°C, tea is under-extracted and does not taste right. A pressure cooker would solve this.

Section B — Extended Response

20 marks
Q7 [10 marks]

(a) Describe the one-component phase diagram of CO2. Sketch and label it, indicating: all three phase regions, the triple point (with values), the critical point (with values), and the sublimation curve. Explain why CO2 does not have a normal melting point. [5 marks]

(b) Using the Gibbs phase rule, calculate F for three different conditions on the CO2 phase diagram and explain what each value means physically. [3 marks]

(c) Explain what a homogeneous equilibrium is and give one example with its K expression. [2 marks]

(a) CO2 phase diagram:
Three regions: solid (top-left), liquid (top-middle-right), gas (bottom-right).
Triple point: −56.6°C, 5.11 atm. Critical point: 31.1°C, 73.8 atm.
Fusion curve: positive slope (normal — solid denser than liquid).
Sublimation curve: runs from bottom-left to triple point (solid–gas equilibrium below triple point).

No normal melting point: The triple point (5.11 atm) is above 1 atm. Therefore the 1 atm isobar does not cross the solid–liquid (fusion) boundary at any temperature. At 1 atm, moving from solid to gas crosses only the sublimation curve (−78.5°C). Liquid CO2 can only exist above 5.11 atm.

(b)
1. Solid CO2 only: C=1, P=1 → F = 2. Both T and P can be varied — bivariant.
2. Solid + gas (on sublimation curve): C=1, P=2 → F = 1. Fix T → P fixed (sublimation pressure) — univariant.
3. Triple point: C=1, P=3 → F = 0. T and P both fixed at −56.6°C, 5.11 atm — invariant.

(c) A homogeneous equilibrium is one where all reactants and products are in the same phase.
Example: N2(g) + 3H2(g) ⇌ 2NH3(g)
Kp = [p(NH3)]2 / (p(N2) × [p(H2)]3)
Q8 [10 marks]

(a) Describe the T–x (boiling point–composition) diagram for an ideal binary mixture. Define and identify: the liquid curve, vapour curve, two-phase region, and a tie line. Explain what the lever rule gives and derive the formula. [5 marks]

(b) Explain what an azeotrope is, distinguishing between minimum-boiling and maximum-boiling azeotropes. Give one example of each and explain why the ethanol–water azeotrope limits the purity achievable by simple fractional distillation. [5 marks]

(a)
T–x diagram (at constant P, usually 1 atm): T on y-axis, mole fraction xB on x-axis from 0 (pure A) to 1 (pure B).
Liquid (bubble point) curve: the locus of temperatures at which a liquid of given composition begins to boil. Below this curve = single-phase liquid.
Vapour (dew point) curve: temperatures at which vapour of given composition begins to condense. Above this curve = single-phase vapour.
Two-phase region: between the two curves; liquid and vapour coexist in equilibrium. F = 2−2+1 = 1 (at constant P) — univariant.
Tie line: horizontal line at constant T within the two-phase region, connecting a point on the liquid curve (xL) to a point on the vapour curve (xV).
Lever rule: Moles(vapour) × (xV − xoverall) = Moles(liquid) × (xoverall − xL)
→ nV/nL = (xoverall − xL)/(xV − xoverall)
Gives the relative moles of vapour to liquid at any point in the two-phase region.

(b)
An azeotrope is a mixture of fixed composition at which the vapour and liquid have identical composition → distillation cannot change the composition further at that point.

Minimum-boiling azeotrope (positive deviation from Raoult's Law): vapour pressure curve has a maximum → boiling point curve has a minimum. The mixture boils at a temperature below both pure components. Example: ethanol–water (95.6% ethanol, B.P. 78.1°C; pure ethanol B.P. 78.4°C, water 100°C).

Maximum-boiling azeotrope (negative deviation): vapour pressure minimum → boiling point maximum. Mixture boils above both pure components. Example: HCl–water (20.2% HCl, B.P. 108.6°C).

Ethanol–water limitation: Starting from any dilute ethanol–water mixture and distilling, the distillate becomes progressively richer in ethanol until it reaches 95.6% ethanol (azeotrope). At this point, vapour = liquid composition → no further enrichment is possible by distillation. To get 100% ethanol, physical desiccants (molecular sieves, CaO) must be used.

💳 Pay to Download

Unit notes — instant PDF download

Price
300 RWF
One-time · Download immediately after payment
Phone Number
Rwanda — MTN MoMo or Airtel Money
Network
MTN MoMo
Airtel Money
Other
Processing Payment...
Check your phone — enter your PIN to confirm.
Payment Confirmed!
Generating your PDF...
Payment Not Completed
WhatsApp
⚙️
Payment service is being set up.
Online payment is not yet available for this unit.
Please contact your teacher to get access.