Energy never disappears. Reactions only go where the entropy wins. Two laws that decide what's possible in chemistry.
The required syllabus content for Unit 5, in order. Each card is one lesson-sized checkpoint.
Brainstorm everything you already know about equilibrium (reversible reactions)
Lesson 2 of Unit 5.
Lesson 3 of Unit 5.
Lesson 4 of Unit 5.
Lesson 7 of Unit 5.
In chemical transformations, energy can neither be created nor destroyed (the first law of thermodynamics).
Lesson 9 of Unit 5.
Average bond energies can be found in the data booklet!
This law is a statement of the conservation of energy.
The products have less enthalpy than the reactants and are therefore energetically more stable.
The shorter the chain of a hydrocarbon or fuel, the higher the amount of specific energy (amount of energy released per unit mass), and the more likely that the fuel combusts completely.
Lesson 16 of Unit 5.
Lesson 17 of Unit 5.
Each lesson card below mirrors the original teacher deck — syllabus refs, content, worked examples and practice questions in order.
A reversible reaction can proceed in either direction. In a closed system it reaches a point where the forward and reverse rates are equal — dynamic equilibrium.
Isotopic labelling: introduce a radioactive isotope of one element into the reactant. Over time, the label shows up in both reactant and product. Both reactions are happening — concentrations are stable because forward and reverse cancel.
For the general reaction aA + bB ⇌ cC + dD at equilibrium:
Kc = ([C]c[D]d) / ([A]a[B]b)
Kc depends only on temperature.
Pure solids and pure liquids are excluded from the K expression. Their "concentration" is essentially constant (= their density / M), absorbed into K.
For CaCO₃(s) ⇌ CaO(s) + CO₂(g): Kc = [CO₂] only.
Le Chatelier's principle: when a system at equilibrium is disturbed, it shifts in a direction that partially counteracts the disturbance.
| Disturbance | Direction of shift | Kc |
|---|---|---|
| Add reactant | Forward (consume the added reactant) | Unchanged |
| Remove product | Forward (replace the removed product) | Unchanged |
| Increase p (gases) | Toward fewer moles of gas | Unchanged |
| Increase T | Endothermic direction | Changes |
| Decrease T | Exothermic direction | Changes |
| Add catalyst | No shift (forward and reverse rates ↑ equally) | Unchanged |
2 SO₂(g) + O₂(g) ⇌ 2 SO₃(g), ΔH = −197 kJ mol⁻¹. Compromise conditions: ~450 °C and atmospheric pressure with V₂O₅ catalyst. Low p would shift right but the small mole change (3 → 2) means high p isn't worth the engineering cost.
CO₂(g) ⇌ CO₂(aq) (with subsequent H₂CO₃ formation). Bottled under high CO₂ pressure → high [CO₂(aq)]. Opening the bottle releases CO₂(g), equilibrium shifts left, CO₂ escapes as bubbles.
CO₂ + H₂O ⇌ H₂CO₃ ⇌ HCO₃⁻ + H⁺. Hyperventilation removes CO₂ → equilibrium shifts left → [H⁺] drops → blood pH rises (respiratory alkalosis). Breathing into a bag re-inhales CO₂ to restore balance.
Enthalpy H is the internal energy + pV term. Almost all chemistry happens at constant pressure, so ΔH = q (heat exchanged with surroundings).
| Type | Sign of ΔH | Direction of heat | Surroundings |
|---|---|---|---|
| Exothermic | − | Released by reaction | Get warmer |
| Endothermic | + | Absorbed by reaction | Get cooler |
Bond breaking requires energy (endothermic). Bond making releases energy (exothermic). For a complete reaction, ΔH = (energy needed to break reactant bonds) − (energy released forming product bonds).
Calorimetry measures the heat absorbed or released by a reaction:
q = m × c × ΔT
where m is the mass of the solution (g), c is the specific heat capacity (4.18 J g⁻¹ K⁻¹ for water), ΔT is the temperature change (K or °C — same numerical magnitude).
Then ΔH = ±q / n, where n is the moles of the limiting reactant. The sign convention:
A simple coffee-cup calorimeter (polystyrene cup with lid) is good enough for ΔH measurements at the IB level.
Some heat is always lost during the reaction. To minimise the error, plot T vs t every 30 s for ~5 minutes before mixing (baseline) and ~5 minutes after. Extrapolate the post-reaction line back to the moment of mixing — this is your "true" Tmax. Subtract initial T to get a more accurate ΔT.
Bond enthalpy: the energy required to break one mole of a specific bond in the gaseous state. Values are averages across many molecules.
ΔHrxn ≈ Σ(bonds broken in reactants) − Σ(bonds formed in products)
Limitations: only approximate; only really applies to gas-phase reactions (not liquids or solids where intermolecular forces also matter).
Hess's law: the enthalpy change of a reaction depends only on the initial and final states, not on the route taken. Enthalpy is a state function.
So if reaction A→D has ΔH unknown, but you know A→B→C→D with known ΔH for each step, simply sum.
ΔHrxn = Σ ΔHf(products) − Σ ΔHf(reactants)
ΔHf = standard enthalpy of formation, per mole of compound from its elements in their standard states. ΔHf of an element in its standard state = 0 by definition.
ΔHrxn = Σ ΔHc(reactants) − Σ ΔHc(products)
Useful when formation data isn't available (combustion is easier to measure for many organic compounds).
Hydrocarbon + sufficient O₂ → CO₂ + H₂O. Highly exothermic.
Example: C₃H₈ + 5 O₂ → 3 CO₂ + 4 H₂O.
Insufficient O₂ → CO (carbon monoxide, toxic) and/or C(s) (soot).
Examples: 2 C₃H₈ + 7 O₂ → 6 CO + 8 H₂O (incomplete, all the way to CO); 2 C₃H₈ + 3 O₂ → 6 C + 8 H₂O (extreme — only water and soot).
CO binds to haemoglobin ~250× more strongly than O₂. A small amount of CO permanently displaces O₂ from the blood, suffocating from the inside.
Two metrics for comparing fuels:
| Fuel | Specific energy (MJ/kg) | Energy density (MJ/dm³) |
|---|---|---|
| H₂ (liquid) | 142 | 10 |
| Methane (LNG) | 55 | 23 |
| Petrol | 47 | 34 |
| Diesel | 45 | 38 |
| Ethanol | 30 | 24 |
| Coal | 24 | 35 |
| Wood (dry) | 16 | 10 |
HL: Gibbs free energy, equilibrium constants from ΔG°, and the relationship between Kc and ΔG.
Lesson 5 of Unit 5.
Lesson 6 of Unit 5.
Lesson 12 of Unit 5.
Lesson 13 of Unit 5.
Definition: The reaction quotient (Q) is a measure of the relative amounts of products and reactants present in a chemical reaction at any given time.
The reaction quotient Q has the same form as Kc but uses current concentrations (not necessarily at equilibrium):
Q = [products]... / [reactants]... (same powers as Kc)
| Comparison | Meaning | Direction |
|---|---|---|
| Q < K | Too few products | Forward (→) |
| Q = K | At equilibrium | No net change |
| Q > K | Too many products | Reverse (←) |
ΔG° = −RT ln K: a positive K (> 1) → negative ΔG° (spontaneous). For non-equilibrium states: ΔG = ΔG° + RT ln Q.
Standard enthalpy of formation ΔH°f: enthalpy change when 1 mol of a compound forms from its elements in their standard states under standard conditions (298 K, 100 kPa).
Standard enthalpy of combustion ΔH°c: enthalpy change when 1 mol of a substance is completely burned in O₂ under standard conditions.
Both are tabulated in the IB data booklet for hundreds of compounds.
For organic compounds, ΔHf is often calculated indirectly via Hess from ΔHc values (because direct synthesis from elements is rarely practical):
ΔHc(compound) = ΣΔHf(products) − ΔHf(compound)
Lattice enthalpy can't be measured directly. A Born-Haber cycle decomposes the formation of an ionic solid into measurable steps, then uses Hess to extract the lattice enthalpy.
Sum of all 5 steps = ΔHf(MX). Rearrange to find ΔHlattice.
So MgO (2+ and 2−, small radii) has a much larger lattice enthalpy than NaCl (1+ and 1−).
Entropy S measures the dispersal of energy in a system — often described loosely as "disorder". Higher entropy = more ways for energy to be distributed.
Calculate ΔS° = ΣS°(products) − ΣS°(reactants). Tabulated S° values are absolute (positive) — unlike ΔHf values which are relative changes.
ΔG = ΔH − TΔS
A reaction is spontaneous at temperature T if ΔG < 0. Note: spontaneous means thermodynamically favoured — says nothing about rate.
| ΔH | ΔS | Spontaneous when |
|---|---|---|
| − (exo) | + | Always (at all T) |
| + (endo) | − | Never |
| − (exo) | − | Only at low T |
| + (endo) | + | Only at high T |
ΔG° = −RT ln K
This single equation links thermodynamics (ΔG°) to equilibrium (K):
ΔG = ΔG° + RT ln Q. When Q < K, ΔG < 0 and the forward reaction is favoured; when Q > K, ΔG > 0 and the reverse is favoured.
If you can't define one of these in a sentence, that's where to revise next. Click any term for its definition.