1. Standard Enthalpy Definitions
The heat energy transferred in a chemical reaction at constant pressure. Standard conditions (°): 100 kPa (1 bar) pressure and a stated temperature (usually 298 K / 25°C), with substances in their standard physical states.
Releases heat energy to the surroundings. ΔH is negative. The surroundings get warmer.
Examples: combustion of fuels, neutralisation.
Takes in heat energy from the surroundings. ΔH is positive. The surroundings get cooler.
Example: thermal decomposition of calcium carbonate.
The enthalpy change when one mole of a compound is formed from its constituent elements in their standard states under standard conditions.
Rule: The standard enthalpy of formation of any element in its standard physical state is zero by definition (e.g. \(\Delta_f H^\circ[\text{O}_2(g)] = 0\)).
The enthalpy change when one mole of a substance burns completely in excess oxygen under standard conditions, with all reactants and products in their standard states.
Rule: Enthalpies of combustion are always negative (exothermic).
2. Calorimetry Principles
Calorimetry measures thermal energy changes by tracking temperature changes in an aqueous solution or calorimeter:
Heat Energy Transferred Formula
\[ q = mc\Delta T \]
- \(q\) = heat energy absorbed or released in joules (J).
- \(m\) = mass of solution being heated or cooled in grams (g). We assume aqueous solutions have a density of 1.00 g cm⁻³ (so 50 cm³ = 50 g).
- \(c\) = specific heat capacity of water (4.18 J g⁻¹K⁻¹).
- ΔT = temperature change in K or °C (\(T_{\text{final}} - T_{\text{initial}}\)).
Molar Enthalpy Change Formula
\[ \Delta H = -\frac{q}{n \times 1000} \]
Where \(n\) is the amount of limiting reactant in moles (mol), dividing by 1000 converts joules to kilojoules (kJ mol⁻¹). The negative sign ensures that an exothermic temperature rise produces a negative ΔH.
3. Cooling Curve Temperature Extrapolation
In simple polystyrene cup calorimetry, heat is inevitably lost to the laboratory surroundings during the reaction. The recorded peak temperature is therefore lower than the true theoretical maximum.
Experimental Protocol (RP2 Alignment)
- Record the temperature of the initial solution every minute for 3 minutes to establish a stable baseline.
- At minute 4, add the second reactant and stir. Do not record a temperature at minute 4.
- Resume recording temperature at minute 5, taking readings every minute until minute 15.
- Plot temperature against time on graph paper.
- Draw a straight line of best fit through the cooling points, from the highest temperature onwards, and extrapolate this line back to minute 4 (the exact moment of mixing). The minute 5 reading is often still rising, so do not include it if it is below the highest temperature.
- Determine ΔT as the vertical difference between the extrapolated temperature at minute 4 and the initial baseline temperature.
- Heat is lost to the surroundings, so the measured temperature change is too small. The calculated ΔH is then smaller in size than the true value.
- Reduce heat loss with a polystyrene cup, a lid and insulation around the cup.
- Extrapolating the cooling line back to the time of mixing corrects for the heat lost while the reaction takes place.
The full method, apparatus and errors are on RP2: Measurement of an Enthalpy Change.
4. Hess's Law Cycles
The total enthalpy change for a chemical reaction is independent of the route taken, provided the initial and final states are identical.
Enthalpies of Formation Route
\[ \Delta H_r^\circ = \sum \Delta_f H^\circ(\text{products}) - \sum \Delta_f H^\circ(\text{reactants}) \]
Constituent elements in standard states form the bottom baseline. Arrows point upwards from elements to products and reactants.
Enthalpies of Combustion Route
\[ \Delta H_r^\circ = \sum \Delta_c H^\circ(\text{reactants}) - \sum \Delta_c H^\circ(\text{products}) \]
Combustion products (CO₂,H₂O) form the bottom baseline. Arrows point downwards from reactants and products to combustion products.
Formation equation: \[ 2\text{C}(s) + 3\text{H}_2(g) + \frac{1}{2}\text{O}_2(g) \rightarrow \text{C}_2\text{H}_5\text{OH}(l) \]
Applying Hess combustion formula:
\[ \Delta_f H = \sum \Delta_c H(\text{reactants}) - \sum \Delta_c H(\text{products}) \]
\[ \Delta_f H = [2(-393.5) + 3(-285.8)] - [-1367.3] \]
\[ \Delta_f H = [-787.0 - 857.4] - [-1367.3] = -1644.4 + 1367.3 = \mathbf{-277.1\text{ kJ mol}^{-1}} \]
5. Mean Bond Enthalpies
The enthalpy change required to break one mole of a specified covalent bond in gaseous molecules, averaged across a wide range of chemical compounds.
\[ \Delta H_r = \sum (\text{Bonds Broken}) - \sum (\text{Bonds Formed}) \]
Why do bond enthalpy calculations differ from experimental Hess cycles?
- Mean bond enthalpies are averages over a range of compounds. They are not the actual values for the bonds in these molecules. When both values refer to gases, the reason to give is that mean bond enthalpies are averages.
- Bond enthalpies apply only to the gaseous state. The data-book value of an enthalpy of combustion has water as a liquid, not a gas, so it differs even more.
Breaking bonds is endothermic (energy taken in). Making bonds is exothermic (energy released).
Step 1: Bonds broken (4 C-H in CH₄, 2 O=O): 4 × 413 + 2 × 498 = 2648 kJ mol⁻¹
Step 2: Bonds made (2 C=O in CO₂, 4 O-H in 2H₂O): 2 × 805 + 4 × 463 = 3462 kJ mol⁻¹
Step 3: ΔH = bonds broken - bonds made = 2648 - 3462 = -814 kJ mol⁻¹
How does this compare with Hess's law? Using enthalpies of formation with water as a gas gives -802 kJ mol⁻¹ ([-393.5 + 2(-241.8)] - [-74.8] = -802.3 kJ mol⁻¹). The 12 kJ difference is because mean bond enthalpies are averages over many compounds. The data-book ΔcH (-890 kJ mol⁻¹) differs more because there the water is a liquid.
Go deeper
These UK AQA pages cover the same ideas in more detail. They may include content that is not in 9620.
6. Practice Questions
Show Answer & Mark Scheme
Step 1: Total solution mass: \(m = 50.0 + 50.0 = 100.0\text{ g}\).
Step 2: Temperature rise: ΔT = 26.2 − 19.5 = 6.7 K.
Step 3: Heat energy released:
\[ q = mc\Delta T = 100.0 \times 4.18 \times 6.7 = 2800.6\text{ J} = 2.8006\text{ kJ} \]
Step 4: Moles of water formed: \(n = c \times V = 1.00 \times (50.0 / 1000) = 0.0500\text{ mol}\).
Step 5: Molar enthalpy change:
\[ \Delta H = -\frac{2.8006}{0.0500} = \mathbf{-56.0\text{ kJ mol}^{-1}} \]
Show Answer & Mark Scheme
Mark Scheme:
- Bonds broken: 436 + 243 = 679 kJ mol⁻¹. (1 mark)
- Bonds made: 2 × 432 = 864 kJ mol⁻¹. (1 mark)
- ΔH = 679 - 864 = -185 kJ mol⁻¹. (1 mark)
Show Answer & Mark Scheme
Mark Scheme:
- (a) ΔfH of O₂(g) is zero, because it is an element in its standard state. (1 mark)
- ΔH = Σ ΔfH(products) - Σ ΔfH(reactants) = [-393.5 + 2(-241.8)] - [-74.8]. (1 mark)
- ΔH = -877.1 + 74.8 = -802.3 kJ mol⁻¹. (1 mark)
- (b) Mean bond enthalpies are averages over a range of compounds, not the actual values in these molecules. (1 mark)
Show Answer & Mark Scheme
Mark Scheme:
- An exothermic reaction releases heat energy to the surroundings. (1 mark)
- ΔH is negative. (1 mark)
- Standard conditions: 100 kPa and a stated temperature, usually 298 K. (1 mark)