8. Reaction kinetics
- Syllabus
- 9701–2028–2029
- Section
- 8
- Level
- AS

rate=timechange in reactant or product concentration
| Term | Meaning |
|---|---|
| rate of reaction | change in the amount or concentration of a reactant consumed or product formed per unit time |
| frequency of collisions | number of collisions between reacting particles per unit time |
| effective collision | collision with sufficient energy and a suitable orientation, so reaction occurs |
| non-effective collision | collision with insufficient energy and/or unsuitable orientation, so particles separate without reacting |
Reaction rate depends on the frequency of effective collisions, not simply the total collision frequency. Conditions can increase the number of collisions per second, the fraction that meet the energy/orientation requirements, or both.
A collision is not automatically effective, and an effective collision is not defined by high frequency alone. Rate describes change per time; it does not state the final yield or equilibrium position.
| Change at constant temperature | Particle-level effect | Rate consequence |
|---|---|---|
| increase solution concentration | more reacting particles occupy the same solution volume, so collisions occur more frequently | more effective collisions per second; rate increases |
| decrease solution concentration | fewer reacting particles occupy the same volume | fewer effective collisions per second; rate decreases |
| increase gas pressure by decreasing volume | the same gas particles occupy less space and collide more frequently | more effective collisions per second; rate increases |
| decrease gas pressure by increasing volume | particles are farther apart and collide less frequently | fewer effective collisions per second; rate decreases |
At constant temperature, the energy distribution and activation-energy threshold are not changed by concentration or pressure alone. The qualitative rate change is explained by collision frequency and therefore effective-collision frequency.
Pressure is the relevant concentration-like variable for gaseous reactants, not for an incompressible liquid or solid. Do not explain these changes by saying particles move faster: at fixed temperature their average kinetic energy is unchanged.
| Data representation | Rate calculation |
|---|---|
| two concentration–time readings | secant gradient: Δconcentration / Δtime gives average rate over the interval |
| one point on a concentration–time curve | draw a tangent and calculate its gradient for instantaneous rate |
| mass, moles or gas volume against time | calculate change/time in the measured quantity, or convert to concentration if the requested rate requires it |
Product concentration has a positive gradient; reactant concentration has a negative gradient. Unless a signed derivative is requested, report the positive magnitude of a reactant-consumption rate and state which species was followed.
A product concentration increases from 0.100 to 0.340 mol dm⁻³ between 20.0 s and 80.0 s. The average rate is (0.340 − 0.100)/(80.0 − 20.0) = 4.00 × 10⁻³ mol dm⁻³ s⁻¹.
For a tangent, choose two well-separated points on the straight tangent—not two points on the curve—and calculate vertical change divided by horizontal change. A shallower concentration–time curve means a smaller rate magnitude.
Do not divide by the final clock reading when the interval begins later, mix minutes with seconds, or label mass-loss rate with concentration-rate units. The numerical unit must follow the measured vertical quantity and time unit.
Activation energy, Eₐ, is the minimum energy required for a collision to be effective. Colliding particles with energy below Eₐ cannot follow that reaction pathway to products.
Meeting the energy threshold is necessary but does not remove the orientation requirement: particles must also collide in a suitable orientation for the required bonds to rearrange.
Eₐ is an energy barrier, not the reaction enthalpy ΔH and not the average kinetic energy of the particles. An exothermic reaction can still be slow if few collisions overcome a large Eₐ.
| Sketch feature | Required representation | Meaning |
|---|---|---|
| horizontal axis | particle energy, E | energy increases to the right |
| vertical axis | number or fraction of particles with energy E | population at each energy |
| distribution curve | begins at the origin, rises to one peak, then falls with a long tail approaching the axis | particles have a spread of energies, not one energy |
| total area under curve | fixed for a fixed number of particles | total particle population |
| vertical Eₐ line | placed to the right of the peak | minimum effective-collision energy |
| area to right of Eₐ | shade beneath the tail | fraction with energy at least Eₐ |
Only the shaded fraction has sufficient energy for an effective collision; a suitable collision orientation is still required. The area, not the height of the curve where it crosses Eₐ, represents the relevant fraction.
Do not make the curve touch the energy axis at a finite high energy, start above the origin, or label the peak as Eₐ. Eₐ is a threshold line and the high-energy tail approaches the axis asymptotically.
| On raising temperature for the same particle population | Boltzmann-distribution consequence |
|---|---|
| particles have greater average speed and kinetic energy | the curve becomes lower and broader and its peak moves to higher energy |
| total number of particles is unchanged | both curves enclose the same total area and cross |
| Eₐ for the unchanged pathway is unchanged | the area to the right of the same Eₐ line increases |
Faster particles collide slightly more frequently. More importantly, a much larger fraction of collisions now has energy at least Eₐ. Together these effects increase the frequency of effective collisions, so the reaction rate rises.
Lowering temperature reverses the comparison: collision frequency falls and the area beyond Eₐ becomes smaller, so there are fewer effective collisions per second and the rate decreases.
Temperature changes the distribution, not Eₐ. Do not shift the Eₐ line when comparing temperatures for the same mechanism, and do not claim that every collision in the high-energy area reacts because orientation can still be unsuitable.
A catalyst increases the rate of a reaction without being chemically changed overall. Catalysis occurs because the catalyst provides a different reaction mechanism with a lower activation energy, Eₐ.
| Catalyst type | Phase relationship | Typical mechanism location |
|---|---|---|
| homogeneous | catalyst and reactants are in the same phase | intermediate species form within the shared phase |
| heterogeneous | catalyst is in a different phase from the reactants | reaction occurs at active sites on the catalyst surface |
At the same temperature, the Boltzmann distribution is unchanged. Draw the catalysed Eₐ line to the left of the uncatalysed Eₐ line: the area to the right of the lower threshold is larger, so a greater fraction of collisions has sufficient energy and effective collisions occur more frequently.
| Reaction-pathway feature | Uncatalysed | Catalysed |
|---|---|---|
| reactant enthalpy level | same | same |
| product enthalpy level | same | same |
| peak / forward Eₐ | higher | lower for the alternative mechanism |
| ΔH from reactants to products | same | same |
On one enthalpy-versus-reaction-progress diagram, use common reactant and product levels and draw two labelled pathways. Measure each forward Eₐ from the reactant level to its own peak; the catalysed peak must be lower, while the product–reactant difference remains unchanged.
A catalyst does not raise particle energies, shift the Boltzmann distribution, change ΔH, or alter the equilibrium constant or equilibrium composition. It is regenerated overall even though it may form intermediates during the mechanism.