FAD1018 Thermochemistry — Formula Sheet & Intuition
1. Calorimetry — "How much heat?"
$$q = mc\Delta T$$
| Symbol | Meaning | Unit |
|---|---|---|
| $q$ | Heat absorbed/released | J or kJ |
| $m$ | Mass of substance | g |
| $c$ | Specific heat capacity | J/g·K |
| $\Delta T$ | Temperature change ($T_f - T_i$) | °C or K |
[!tip] $q$ is positive when heat is absorbed (system gets hotter), negative when released.
Bomb vs Coffee-Cup — Intuition
| Coffee-cup (constant pressure) | Bomb (constant volume) | |
|---|---|---|
| Container | Open to atmosphere | Sealed, rigid |
| Measures | $\Delta H$ directly | $\Delta U$ (internal energy) |
| Formula | $q_p = \Delta H$ | $q_v = C_v \Delta T$ |
| Can expand? | Yes | No |
Why bomb measures $\Delta U$ not $\Delta H$: Enthalpy is $H = U + PV$. At constant pressure, $\Delta H = \Delta U + P\Delta V = q_p$. But in a sealed bomb, $\Delta V = 0$ and pressure changes instead — so $q_v = \Delta U$.
Why $\Delta H \approx \Delta U$ for burning graphite: $\text{C}(s) + \text{O}_2(g) \rightarrow \text{CO}_2(g)$. One mole gas in, one mole gas out → $\Delta n_g = 0$ → $\Delta H = \Delta U + \Delta n_g RT = \Delta U$.
The flow:
- Temp rises → calorimeter absorbed heat → $q_{cal} = C\Delta T$
- That heat came from the reaction → $q_{rxn} = -q_{cal}$ (conservation)
- Volume is fixed → $q_{rxn} = \Delta U_{rxn}$
- Divide by moles to get per mole
2. First Law — Conservation of Energy
$$\Delta U = q + w$$
- $\Delta U$ = change in internal energy
- $q$ = heat absorbed by system
- $w$ = work done on system
3. Enthalpy Types — Exact Exam Definitions
| Symbol | Name | Exact definition |
|---|---|---|
| $\Delta H^\circ_f$ | Standard enthalpy of formation | Enthalpy change when 1 mole of compound is formed from its elements in their standard states |
| $\Delta H^\circ_c$ | Standard enthalpy of combustion | Enthalpy change when 1 mole of substance is burned completely in oxygen |
| $\Delta H^\circ_{neut}$ | Enthalpy of neutralisation | Enthalpy change when acid and base neutralise to form 1 mole of water |
| $\Delta H^\circ_{sol}$ | Enthalpy of solution | Enthalpy change when 1 mole of solute dissolves in a solvent |
| $\Delta H^\circ_{vap}$ | Enthalpy of vaporisation | Enthalpy change when 1 mole of liquid changes to gas |
| $\Delta H^\circ_{fus}$ | Enthalpy of fusion | Enthalpy change when 1 mole of solid changes to liquid |
| $\Delta H^\circ_{sub}$ | Enthalpy of sublimation | Enthalpy change when 1 mole of solid changes directly to gas |
| $\Delta H^\circ_{at}$ | Enthalpy of atomisation | Enthalpy change when 1 mole of substance is converted to gaseous atoms |
| Lattice energy | — | Enthalpy change when gaseous ions form 1 mole of ionic solid |
[!warning] Key phrasing traps
- Every definition starts with "Enthalpy change when..."
- $\Delta H_f^\circ$: must say "elements" and "standard states"
- $\Delta H_c^\circ$: must say "1 mole" and "completely in oxygen"
- $\Delta H_{neut}^\circ$: must say "1 mole of water"
- Lattice energy: "gaseous ions" → "ionic solid" (opposite direction)
4. Hess's Law — "Path doesn't matter"
$\Delta H$ for a reaction is the same regardless of pathway.
From Formation Enthalpies (most common exam problem)
$$\Delta H^\circ_{rxn} = \sum \Delta H^\circ_f(\text{products}) - \sum \Delta H^\circ_f(\text{reactants})$$
Procedure:
- Multiply each $\Delta H^\circ_f$ by its stoichiometric coefficient
- Sum products, subtract sum of reactants
[!warning] Watch the signs $\Delta H^\circ_f$ for elements in standard state = zero (e.g. O₂(g), C(graphite), H₂(g))
From Bond Enthalpies
$$\Delta H^\circ_{rxn} = \sum(\text{bonds broken}) - \sum(\text{bonds formed})$$
| Sign | |
|---|---|
| Breaking bonds | Endothermic (+) |
| Forming bonds | Exothermic (-) |
[!tip] Draw the Lewis structures to count bonds. The formula already handles the sign — broken − formed.
Enthalpy of Solution
$$\Delta H^\circ_{sol} = \Delta H^\circ_{lattice} + \Delta H^\circ_{hyd}$$
| If | Then dissolution is |
|---|---|
| $ | \Delta H_{hyd} |
| $ | \Delta H_{hyd} |
5. Gibbs Free Energy — "Will it happen?"
$$\Delta G = \Delta H - T\Delta S$$
| $\Delta G$ | Meaning |
|---|---|
| $< 0$ | Spontaneous (favourable) |
| $= 0$ | Equilibrium |
| $> 0$ | Non-spontaneous |
Spontaneity Cheat Sheet
| $\Delta H$ | $\Delta S$ | Spontaneous? |
|---|---|---|
| $-$(exo) | $+$ (more disorder) | Always |
| $-$(exo) | $-$ (less disorder) | At low T only |
| $+$(endo) | $+$ (more disorder) | At high T only |
| $+$(endo) | $-$ (less disorder) | Never |
[!tip] Mnemonic Exothermic + disorder = always go. Endothermic - disorder = never go. Mixed ones depend on T.
Related: Connection to Other Topics
| Formula | Links To |
|---|---|
| $\Delta G^\circ = -RT \ln K$ | Chemical Equilibrium |
| $\Delta G^\circ = -nFE^\circ_{cell}$ | Electrochemistry |
6. Lattice Energy
Energy required to separate 1 mol ionic solid into gaseous ions.
Factors:
| Factor | Higher charge | Smaller ion |
|---|---|---|
| Effect on LE | ↑ Higher LE | ↑ Higher LE |
Born-Haber Cycle (Hess's Law applied to ionic compounds): $$\Delta H^\circ_f = \Delta H_{at} + IE + \Delta H_{at} + EA + LE$$
7. Problem-Type Mapping
| Question pattern | Formula / method |
|---|---|
| "Calculate heat released when X g burns..." | $q = mc\Delta T$ or $q_v = C_v \Delta T$ |
| "Calculate $\Delta H$ using formation data..." | $\Delta H^\circ_{rxn} = \sum \Delta H^\circ_f(\text{prod}) - \sum \Delta H^\circ_f(\text{react})$ |
| "Calculate $\Delta H$ using bond enthalpies..." | $\sum(\text{bonds broken}) - \sum(\text{bonds formed})$ |
| "Determine if reaction is spontaneous at T..." | $\Delta G = \Delta H - T\Delta S$, check sign |
| "At what T does reaction become spontaneous?" | Set $\Delta G = 0$, solve $T = \Delta H / \Delta S$ |
| "Calculate lattice energy / construct Born-Haber" | Hess's Law cycle |
| "Define $\Delta H_f^\circ$ / $\Delta H_c^\circ$ / $\Delta H_{neut}^\circ$ / lattice energy" | Exact definitions from section 3 |
Related
- Thermochemistry — concept page
- FAD1018 W15 — Thermochemistry — lecture source
- FAD1018 Phase Equilibria & Thermochemistry — Drill Guide — step-by-step for Q25-36
- FAD1018 - Basic Chemistry II