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R2.2 How fast? The rate of chemical changeIB Chemistry SL: Revision notes

Section 1

Measuring rate

The rate of reaction is the change in concentration of a reactant or product per unit time, in mol dm⁻³ s⁻¹. In practice we follow any property that changes with concentration: volume of gas (gas syringe), mass loss as gas escapes, colour (colorimeter), conductivity, or the time for a fixed amount of precipitate to form.

The mean rate over an interval is Δ(quantity) ÷ Δt. When a fixed amount of product is formed each time, rate ∝ 1/time. Rate is highest at the start and falls as reactants are used up.

Key termsrate of reactionmean rate
Exam tip

Always check the time unit: a rate in cm³ s⁻¹ is 60 times bigger as a number when written in cm³ min⁻¹.

Section 2

Collision theory

Particles react only when they collide with energy at least equal to the activation energy and with the correct orientation (collision geometry): the reacting parts of the particles must meet. Most collisions are unsuccessful.

The average kinetic energy of particles is proportional to the temperature in kelvin. A rise from 293 K to 303 K increases average kinetic energy by only about 3%, so collision frequency hardly changes.

Key termsactivation energycollision geometrykinetic energy

Section 3

Factors affecting rate

  • Concentration (solutions) and pressure (gases): more particles per unit volume → more frequent collisions.
  • Surface area of a solid: powder exposes more particles → more frequent collisions.
  • Temperature: particles move faster (more collisions) and, far more importantly, a much larger proportion of collisions have E ≥ Ea.
  • Catalyst: lowers Ea so a larger proportion of collisions succeed.

Increasing the volume of a solution at the same concentration does not change the rate.

Key termsconcentrationsurface areapressure
Common mistake

Saying higher temperature works mainly because of 'more collisions'. The key reason is the larger proportion of collisions with E ≥ Ea.

Section 4

Maxwell–Boltzmann distributions

A Maxwell–Boltzmann distribution plots the number of particles against their kinetic energy. It starts at the origin, rises to a peak (the most probable energy), then falls with a long tail that never touches the energy axis. The area under the curve is the total number of particles.

Higher temperature: the peak is lower and moves to higher energy; the area is unchanged; much more area lies beyond Ea.

Lower Ea (catalyst): the curve is unchanged; the Ea line moves left, so more area lies beyond it.

Key termsMaxwell–Boltzmann distributionmost probable energy

Section 5

Catalysts and energy profiles

A catalyst increases the rate by providing an alternative reaction pathway with a lower Ea; it is not used up. On an energy profile, reactants and products are at the same levels with or without a catalyst, so ΔH is unchanged; only the maximum is lower.

Exothermic: products below reactants. Endothermic: products above reactants. For an exothermic reaction, Ea(reverse) = Ea(forward) + |ΔH|; for an endothermic reaction, Ea(reverse) = Ea(forward) − ΔH. A catalyst lowers the forward and reverse Ea by the same amount.

Key termscatalystenergy profilealternative pathway

Must know

  • Rate = change in concentration per unit time (mol dm⁻³ s⁻¹).
  • Successful collision: E ≥ Ea and correct orientation.
  • Average kinetic energy ∝ temperature in kelvin.
  • Temperature raises the proportion with E ≥ Ea; a catalyst lowers Ea.
  • Catalysts do not change ΔH and lower both forward and reverse Ea.

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