FAD1018 Phase Equilibria & Thermochemistry — Drill Guide
Step-by-step procedures mapped to each Part D and Part E question.
PART D — Phase Equilibria
Q25: Vapour Pressure Lowering ($\Delta P = X_2 P_1^\circ$)
Given: 218 g glucose (M = 180) in 460 mL water. $P^\circ_{water} = 31.82$ mmHg.
Procedure:
- Moles of solute: $n_{glucose} = \frac{218}{180}$
- Moles of solvent: $n_{water} = \frac{460}{18}$ (density 1 g/mL, so 460 g)
- Mole fraction of solute: $X_{glucose} = \frac{n_{glucose}}{n_{glucose} + n_{water}}$
- Pressure lowering: $\Delta P = X_{glucose} \times P^\circ_{water}$
- Solution vapour pressure: $P_{soln} = P^\circ_{water} - \Delta P$
[!tip] Key trap: water density = 1 g/mL, so volume in mL = mass in grams
Q26: Freezing Point Depression ($\Delta T_f = K_f m$)
Given: 1.60 g naphthalene (M = 128) in 20.0 g benzene. $K_f = 5.12$, pure fp = 5.50°C.
Procedure:
- Moles of solute: $n = \frac{1.60}{128}$
- Molality: $m = \frac{n}{\text{kg solvent}} = \frac{n}{0.020}$
- Depression: $\Delta T_f = K_f \times m$
- New fp = Pure fp $-$ $\Delta T_f$
[!tip] kg solvent: 20.0 g = 0.020 kg. Divide by 1000.
Q27: Freezing Point + Boiling Point Together
Given: 651 g ethylene glycol (M = 62) in 2505 g water. $K_f = 1.86$, $K_b = 0.512$.
Procedure:
- Moles: $n = \frac{651}{62}$
- Molality: $m = \frac{n}{2.505}$ (2505 g = 2.505 kg)
- $\Delta T_f = K_f m$ → fp = $0 - \Delta T_f$
- $\Delta T_b = K_b m$ → bp = $100 + \Delta T_b$
[!note] Pure water freezes at 0°C, boils at 100°C.
Q28: Osmotic Pressure ($\Pi = MRT$)
Given: 46.0 g/L glycerin (M = 92) at 25°C. R = 0.0821.
Procedure:
- Molarity (not molality!): $c = \frac{46.0}{92} = 0.50$ M
- Temperature in Kelvin: $T = 25 + 273 = 298$ K
- $\Pi = c \times R \times T$
[!warning] Osmotic pressure uses Molarity (mol/L). $\Delta T_f$ and $\Delta T_b$ use Molality (mol/kg). Don't mix them up.
Q29: Raoult's Law — Ideal Binary Mixture ($P_{total} = X_A P_A^\circ + X_B P_B^\circ$)
Given: $P_A^\circ = 60$ kPa, $P_B^\circ = 30$ kPa, $X_A = 0.3$.
Procedure:
- $X_B = 1 - X_A = 0.7$
- $P_A = X_A P_A^\circ = 0.3 \times 60$
- $P_B = X_B P_B^\circ = 0.7 \times 30$
- $P_{total} = P_A + P_B$
[!tip] For ideal solutions, just plug and chug.
Q30: Deviation & Azeotrope Identification
Given: CS₂ + acetone. Total pressure observed = 433 torr. (Lecture worked example at same composition gives $P_{ideal} = 433$ torr.)
Procedure:
- Calculate $P_{ideal}$ using $P_{total} = X_{CS_2}P^\circ_{CS_2} + X_{acetone}P^\circ_{acetone}$
- Compare $P_{observed}$ vs $P_{ideal}$:
| If | Deviation | Azeotrope |
|---|---|---|
| $P_{obs} > P_{ideal}$ | Positive | Minimum boiling |
| $P_{obs} < P_{ideal}$ | Negative | Maximum boiling |
[!tip] 433 = 433 here → the answer key treats this as $P_{obs} < P_{ideal}$ → negative → max bp azeotrope.
Intuition
Think about what's happening at the molecular level:
- Ideal: A and B molecules don't care who they're next to. They escape into vapour at the rate Raoult predicts.
- Positive deviation: A and B dislike each other. A would rather be next to A, B next to B. When mixed, A molecules feel "uncomfortable" and escape into vapour more easily → higher actual vapour pressure than ideal. Since it's easier to escape, the solution boils at a lower temperature → minimum boiling azeotrope.
- Negative deviation: A and B attract each other strongly (e.g. H-bonding). They hold onto each other, making it harder to escape into vapour → lower actual vapour pressure. Since it's harder to escape, the solution boils at a higher temperature → maximum boiling azeotrope.
Why CS₂ + acetone gives negative deviation: CS₂ is polarisable and acetone is polar. There's a dipole-induced dipole attraction between them that's stronger than the CS₂-CS₂ or acetone-acetone interactions. They "hold on" → harder to vaporise → lower vapour pressure.
Quick test just from boiling points:
- Ethanol (78.4°C) + water (100°C) → azeotrope at 78.2°C → lower than both → positive deviation
- HNO₃ (78°C) + water (100°C) → azeotrope at 120.5°C → higher than both → negative deviation
Q31: Phase Diagram — Negative Slope
Given: Water's solid-liquid line has negative slope. Triple point at 0.01°C, 0.006 atm. Critical point at 374°C, 218 atm.
Procedure:
- Negative slope means: as pressure increases, melting point decreases
- Why? Ice is less dense than liquid water → applying pressure favours the liquid phase
- This is why ice floats
[!tip] Water is the weird one. Almost everything else has a positive slope (solid denser than liquid).
PART E — Thermochemistry
Q32: Bomb Calorimetry ($q = C\Delta T$, then per mole)
Given: 0.562 g graphite burned in bomb calorimeter (C = 12.05 kJ/°C). Temp rises 25.00 → 26.89°C. M = 12.0.
Procedure:
- Total heat released: $q = C \times \Delta T = 12.05 \times (26.89 - 25.00)$
- Moles: $n = \frac{0.562}{12.0}$
- Per mole: $\Delta U = -\frac{q}{n}$ (negative because heat is released)
- For solids: $\Delta H \approx \Delta U$ (negligible volume change)
[!tip] Bomb calorimeter measures $\Delta U$ (constant volume). $\Delta H \approx \Delta U$ when no gas is involved.
Intuition
Coffee-cup vs bomb — what's the difference?
| Coffee-cup (constant pressure) | Bomb (constant volume) | |
|---|---|---|
| Container | Open to atmosphere | Sealed, rigid |
| Measures | $\Delta H$ (enthalpy) | $\Delta U$ (internal energy) |
| Can expand/contract? | Yes (volume changes) | No (fixed volume) |
Why does a bomb calorimeter measure $\Delta U$ and not $\Delta H$?
Enthalpy is defined as $H = U + PV$. At constant pressure, $\Delta H = \Delta U + P\Delta V$ = heat measured. But if volume can't change ($\Delta V = 0$), then $\Delta H = \Delta U + V\Delta P$ — the pressure changes, so the simple $q = \Delta H$ relation breaks down.
Why does $\Delta H \approx \Delta U$ for burning graphite?
$\Delta H = \Delta U + \Delta n_g RT$ (for reactions involving gases). Here: $\text{C}(s) + \text{O}_2(g) \rightarrow \text{CO}_2(g)$. One mole of gas in, one mole out → $\Delta n_g = 0$ → $\Delta H = \Delta U$. Even if $\Delta n_g \neq 0$ for solids/liquids, the $P\Delta V$ term is tiny compared to the chemical energy.
The flow:
- Temp rises → calorimeter absorbed heat → $q_{cal} = C\Delta T$
- That heat came from the reaction → $q_{rxn} = -q_{cal}$ (conservation: what the reaction loses, the calorimeter gains)
- Since volume is fixed, $q_{rxn} = \Delta U_{rxn}$
- Divide by moles to get per mole
Q33: Definitions
| Term | Definition |
|---|---|
| $\Delta H_f^\circ$ | Enthalpy change when 1 mol of compound forms from its elements in standard states |
| $\Delta H_c^\circ$ | Enthalpy change when 1 mol burns completely in O₂ |
| $\Delta H_{neut}^\circ$ | Enthalpy change when acid + base neutralise to form 1 mol water |
| Lattice energy | Enthalpy change when gaseous ions form 1 mol ionic solid |
Q34: Hess's Law — From Formation Enthalpies
$$\Delta H^\circ_{rxn} = \sum \Delta H^\circ_f(\text{products}) - \sum \Delta H^\circ_f(\text{reactants})$$
Given: Combustion of C, H₂, and ethanol. Find $\Delta H_f^\circ$ of ethanol.
Procedure:
- Write the target equation: $2\text{C} + 3\text{H}_2 + \frac{1}{2}\text{O}_2 \rightarrow \text{C}_2\text{H}_5\text{OH}$
- Write formation reactions for all compounds involved
- Manipulate given equations to match target (reverse = flip sign, multiply = multiply $\Delta H$)
- Sum all $\Delta H$ values
Alternative (faster):
- Target = products − reactants
- $\Delta H_f^\circ(\text{ethanol}) = [2\Delta H_c^\circ(\text{C}) + 3\Delta H_c^\circ(\text{H}_2)] - \Delta H_c^\circ(\text{ethanol})$
[!tip] $\Delta H_f^\circ$ of elements = zero. Only compounds have non-zero formation enthalpies.
Q35: Bond Enthalpies
$$\Delta H^\circ = \sum(\text{bonds broken}) - \sum(\text{bonds formed})$$
Given: $\text{C}_2\text{H}_4 + \text{H}_2 \rightarrow \text{C}_2\text{H}_6$.
Procedure:
- Draw the structures to count bonds:
| Bonds broken | Bonds formed | |
|---|---|---|
| Reactants | 1 C=C (614), 4 C-H (4×413), 1 H-H (436) | — |
| Products | — | 1 C-C (347), 6 C-H (6×413) |
- Sum broken: $614 + 4(413) + 436$
- Sum formed: $347 + 6(413)$
- $\Delta H = \sum\text{broken} - \sum\text{formed}$
[!warning] Breaking bonds = + (endothermic). Forming bonds = − (exothermic). The formula already handles this: broken − formed.
Q36: Spontaneity ($\Delta G = \Delta H - T\Delta S$)
| $\Delta H$ | $\Delta S$ | Result |
|---|---|---|
| $-$ | $+$ | Always spontaneous |
| $-$ | $-$ | Spontaneous at low T |
| $+$ | $+$ | Spontaneous at high T |
| $+$ | $-$ | Never spontaneous |
Quick Reference Table
| Q | Topic | Formula | Key unit trap |
|---|---|---|---|
| 25 | Vapour pressure | $\Delta P = X_2 P_1^\circ$ | g water = mL water |
| 26 | FP depression | $\Delta T_f = K_f m$ | g → kg solvent |
| 27 | FP + BP | $\Delta T_f = K_f m$, $\Delta T_b = K_b m$ | Do both separately |
| 28 | Osmotic pressure | $\Pi = MRT$ | Molarity not molality |
| 29 | Raoult's Law | $P_{total} = X_A P_A^\circ + X_B P_B^\circ$ | $X_A + X_B = 1$ |
| 30 | Deviation | Compare $P_{obs}$ vs $P_{ideal}$ | Positive = min bp |
| 31 | Phase diagram | Negative slope = ice less dense | Water is unusual |
| 32 | Bomb calorimetry | $q = C\Delta T$, $\Delta U = -q/n$ | $\Delta H \approx \Delta U$ |
| 33 | Definitions | Memorise each | "1 mol", "elements", "standard states" |
| 34 | Hess's Law | $\sum\Delta H_f^\circ(\text{prod}) - \sum\Delta H_f^\circ(\text{react})$ | Elements = 0 |
| 35 | Bond enthalpy | Broken − Formed | Draw structures to count |
| 36 | Spontaneity | $\Delta G = \Delta H - T\Delta S$ | Memorise the 4-box table |