Topic 6: Energetics
- Syllabus
- 2017
- Topic
- —
- Level
- AS
The enthalpy change, ΔH, is the heat-energy change of a system measured at constant pressure. It is normally quoted per mole of reaction as written, in kJ mol−1.
Standard conditions use a pressure of 100 kPa and a specified temperature, usually 298 K. Every substance must be in its standard state at those conditions unless another state is stated.
Physical state matters because changing state also transfers energy. For example, combustion data for liquid pentane include a different starting enthalpy from data for gaseous pentane.
Standard conditions do not mean standard temperature and pressure from gas-volume conventions. For enthalpy, state 100 kPa and the specified temperature, usually 298 K.
| Process | Energy direction for the reacting system | Relative enthalpy of products | Sign of ΔH |
|---|---|---|---|
| exothermic | heat released to surroundings | lower than reactants | negative |
| endothermic | heat absorbed from surroundings | higher than reactants | positive |
The sign refers to the reacting system. If an insulated solution warms during a reaction, the solution gains heat but the reaction system releases it, so the reaction ΔH is negative.
A value of ΔH=−200 kJ mol−1 means 200 kJ is released per mole of reaction as written. A value of +50 kJ mol−1 means 50 kJ is absorbed.
A positive temperature change of the surroundings does not give a positive reaction enthalpy. Keep the heat gained by the measured surroundings opposite in sign to the reacting system.
| Feature | Exothermic diagram | Endothermic diagram |
|---|---|---|
| reactant level | above products | below products |
| product level | below reactants | above reactants |
| ΔH arrow | downward, labelled negative | upward, labelled positive |
Label the vertical axis enthalpy, write the correct species and states on horizontal reactant and product levels, and draw the ΔH arrow directly between those levels with its value and units.
The vertical separation represents the enthalpy change. For SO3(g)+H2O(l)→H2SO4(aq), ΔH=−200 kJ mol−1, reactants must be 200 kJ mol−1 above products.
An enthalpy-level diagram is not automatically a reaction-profile diagram. Do not add an activation-energy hump when the task only asks for reactant and product enthalpy levels.
| Quantity | Definition under standard conditions, all substances in standard states |
|---|---|
| ΔrH∘ reaction | enthalpy change when the molar quantities in the stated equation react |
| ΔfH∘ formation | enthalpy change when 1 mol of a compound forms from its elements |
| ΔcH∘ combustion | enthalpy change when 1 mol of a substance burns completely in oxygen |
| ΔneutH∘ neutralisation | enthalpy change when an acid and alkali react to form 1 mol of water |
| ΔatH∘ atomisation | enthalpy change when 1 mol of gaseous atoms forms from the element |
Definitions determine equation coefficients. For formation of one mole of water(l): H2(g)+21O2(g)→H2O(l). For atomisation of chlorine: 21Cl2(g)→Cl(g).
Before choosing data, check: correct amount (usually 1 mol of the named product or substance), complete combustion where required, elemental standard states for formation/atomisation, and every physical state.
Standard enthalpy of formation is not formation from free gaseous atoms; it starts from elements in their standard states.
For the material whose temperature is measured, q=mcΔT, where q is in J, m in g, c in J g−1 °C−1 and ΔT in °C.
| Step | Mixed-solution experiment | Combustion calorimeter |
|---|---|---|
| mass heated | total mass of mixed solution, often volume × assumed density | mass of water or other heated material |
| ΔT | final/corrected temperature − initial temperature | final/corrected temperature − initial temperature |
| heat | q=mcΔT for solution | q=mcΔT for water |
| reacting amount | moles of limiting reactant or moles of reaction as written | fuel mass lost ÷ molar mass |
| molar value | ΔH=−q/(1000n) when measured surroundings gain heat | ΔcH=−q/(1000nfuel) |
If 51.0 g of solution warms by 6.9 °C and c=4.18 J g−1 °C−1, q=51.0×4.18×6.9=1.47×103 J. If 0.0273 mol reacted, ΔH=−1.47/(0.0273)=−53.9 kJ mol−1.
Do not report q in joules as ΔH in kJ mol−1. Convert J to kJ, divide by the correct reacting amount, and apply the system/surroundings sign.
Hess's Law states that the enthalpy change for a reaction is independent of the route taken, provided the initial and final states are the same.
Write the target equation, arrange known equations so unwanted species cancel, reverse any equation that runs the wrong way and change the sign of its ΔH, multiply equations and enthalpies by the same factor, then add.
| Common data | Calculation pattern for target reaction |
|---|---|
| formation enthalpies | ΔrH∘=∑ΔfH∘(products)−∑ΔfH∘(reactants) |
| combustion enthalpies | follow the cycle to common combustion products; equivalently combine equations with signs fixed by arrow direction |
| two experimental routes to one final mixture | target plus one measured route equals the other measured route |
Apply stoichiometric coefficients to every enthalpy value and preserve physical states. Confirm that adding the manipulated chemical equations gives exactly the target before adding their numbers.
Do not choose signs from whether a tabulated value is usually negative. Reverse/multiply the chemical equation first; the enthalpy sign and magnitude must follow that manipulation.
Measure two accessible reactions that share a common final state, then use Hess's Law to obtain the enthalpy of a target reaction that is difficult to measure directly.
| Stage | Action |
|---|---|
| prepare | place a measured acid volume in an insulated cup with lid; record mass/concentration and a stable initial temperature |
| react | add a known amount of the first solid, replace lid, stir and record temperature at fixed intervals; determine corrected ΔT |
| repeat | use fresh, comparable acid and the second solid under the same controlled conditions |
| calculate | for each route use q=mcΔT, moles and sign to obtain molar ΔH |
| combine | draw a labelled Hess cycle and algebraically combine the two measured enthalpies for the target |
For CaCO3(s)→CaO(s)+CO2(g), measure ΔH1 for CaCO3+2HCl and ΔH2 for CaO+2HCl to their common CaCl2(aq)+H2O(l) destination. Then ΔHtarget=ΔH1−ΔH2.
Use the same acid concentration and comparable total solution mass, ensure the chosen reagent is fully reacted, stir consistently, and repeat measurements. Record enough temperature-time data for a cooling correction.
Subtracting readings is not Hess's Law by itself. The signed combination is justified only after the balanced equations and common initial/final states are shown.
| Issue or assumption | Likely effect on measured ∣ΔH∣ | Improvement/evaluation |
|---|---|---|
| heat exchanged with surroundings | usually too small | insulation, lid and cooling correction |
| calorimeter heat capacity ignored | too small | determine/include calorimeter constant |
| solution density and c assumed equal to water | may be systematic in either direction | use measured or justified values |
| incomplete combustion or fuel evaporation | combustion magnitude too small | shield flame, improve oxygen supply, weigh promptly |
| thermometer resolution and mass/volume readings | random/measurement uncertainty | higher-resolution apparatus, repeats and uncertainty calculation |
Record temperature at fixed times before mixing, add reactants at a known time, continue readings after the maximum, plot temperature against time, fit the post-reaction cooling line and extrapolate it back to the mixing time. Use the extrapolated temperature to obtain corrected ΔT.
State the mechanism of each error, its direction where defensible, and whether it is random or systematic. Compare repeats and calculate percentage uncertainty from apparatus uncertainties rather than calling every difference 'human error'.
An improvement must address the named source of error. More repeats improve precision and reveal scatter, but they do not remove a systematic heat-loss bias.
Bond enthalpy is the enthalpy needed to break one mole of a specified covalent bond by homolytic fission in gaseous molecules. Mean bond enthalpy is the average value for that bond taken across different gaseous compounds.
Use ΔH≈∑E(bonds broken)−∑E(bonds formed). Breaking bonds requires energy and contributes positively; forming bonds releases energy and is subtracted.
Draw complete structures, count each bond in the stoichiometric equation, multiply by its mean value, total reactant bonds broken and product bonds formed, then subtract with units kJ mol−1.
Mean values average different molecular environments and refer to gaseous species. They therefore give an estimate; state changes and the actual bond environment can make the value differ from an experimental standard enthalpy.
Do not calculate products minus reactants with bond enthalpies. The reliable memory rule is energy in to break minus energy out when bonds form.
Start with a balanced reaction and ΔH=∑Ebroken−∑Eformed. Count the unknown bond as nX, where n is the total number of those bonds formed or broken in the stoichiometric reaction.
| Unknown location | Rearrangement |
|---|---|
| unknown bond is broken | nX=ΔH+∑Eformed−∑Eother broken |
| unknown bond is formed | nX=∑Ebroken−∑Eother formed−ΔH |
If the products contain 48 S–F bonds in total, keep their contribution as 48X until all known bond totals and the reaction ΔH have been inserted, then divide by 48 to obtain the mean S–F bond enthalpy.
The result should be a positive energy per mole of bonds. Recount bonds, coefficients and whether the unknown is on the broken or formed side if the sign or size is implausible.
Divide by the number of unknown bonds in the full balanced reaction, not merely the number in one molecule.
A smaller bond enthalpy means less energy is required for homolytic bond breaking, so that bond may break more readily and may help a reaction proceed faster at room temperature. A larger value indicates a stronger bond that is harder to break.
| Evidence | Bounded inference |
|---|---|
| one candidate bond has much lower enthalpy | it is a plausible bond to break first, if the mechanism requires comparable homolysis |
| all required bonds are strong | substantial activation may be needed, so reaction may be slow at room temperature |
| overall ΔH is negative | products are lower in enthalpy, but this alone says nothing decisive about rate |
Rate depends on the complete mechanism, activation energy, collision geometry, temperature and catalysts. Bond enthalpies are averaged gas-phase data and indicate only one energetic contribution.
Do not equate an exothermic reaction with a fast reaction. Thermodynamic enthalpy describes initial-to-final energy; kinetics depends on the pathway and activation barrier.