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5th Year OL · Chemistry
Chemical transformations · Rate and mechanisms

Rate, collisions and activation

A bar of iron rusts over months, yet iron wool held in a Bunsen flame glows and burns in seconds. The chemical change is the same; what differs is how fast it happens. Chemical kinetics asks how fast a reaction goes and why.

Average and instantaneous rate

Drop magnesium into dilute hydrochloric acid. The bubbles fizz furiously at first and are barely visible a few minutes later. How can we define and measure a rate that changes from moment to moment?

Concentration of a reactant against time, a falling curve. A dashed secant line between two points gives the average rate; a tangent at one point gives the instantaneous rate. [A]time t₁t₂ Secant: average rate Tangent: instantaneous rate

In the laboratory you measure a rate by following a concentration (or a volume of gas, or a colour change) over time. The initial rate is found from the slope of the tangent at $t = 0$. Repeat the experiment at least three times: random errors make the replicates differ slightly, so take the mean and quote the spread (for example $\pm$ the uncertainty). A small spread means good precision; a mean close to the true value means good accuracy. Three standard investigations: (1) $\mathrm{CaCO_3} + \mathrm{HCl}$, where the $\mathrm{CO_2}$ given off is collected in a gas syringe, or the loss of mass is followed on a balance; (2) $\mathrm{Na_2S_2O_3} + \mathrm{HCl}$, where you time how long the sulfur precipitate takes to hide a cross under the conical flask; (3) the decomposition of $\mathrm{H_2O_2}$, where the volume of oxygen is measured over time (a catalyst such as manganese(IV) oxide speeds it up).

The curve of $[\mathrm{A}]$ against time is not a straight line. At the start there is plenty of reactant and the rate is high; as it is used up, the rate falls. The instantaneous rate of disappearance of A is the negative of the slope of the tangent to the curve at that time. To get the rate of reaction, divide by the coefficient of A.

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In a closed reactor of constant volume at $300\,\text{K}$, the gas-phase decomposition of dinitrogen pentoxide is monitored according to the reaction:…

In a closed reactor of constant volume at $300\,\text{K}$, the gas-phase decomposition of dinitrogen pentoxide is monitored according to the reaction:

$$2\,\mathrm{N_2O_5}\,(\mathrm{g}) \rightarrow 4\,\mathrm{NO_2}\,(\mathrm{g}) + \mathrm{O_2}\,(\mathrm{g})$$

Over an interval of $40\,\text{s}$, the concentration of $\mathrm{N_2O_5}$ decreases from $0.100\,\text{mol}\times\text{L}^{-1}$ to $0.064\,\text{mol}\times\text{L}^{-1}$.

  1. a) Calculate the mean rate of disappearance of $\mathrm{N_2O_5}$ over that time interval.
  2. b) Determine the overall mean rate of the reaction normalised by the stoichiometry, and the mean rate of formation of $\mathrm{NO_2}$.
Solve
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The decomposition of reactant $\mathrm{A}$ in aqueous solution according to $\mathrm{A}\,(\mathrm{aq}) \rightarrow \mathrm{B}\,(\mathrm{aq}) + \mathrm{C}\,(\mathrm{aq})$…

The decomposition of reactant $\mathrm{A}$ in aqueous solution according to $\mathrm{A}\,(\mathrm{aq}) \rightarrow \mathrm{B}\,(\mathrm{aq}) + \mathrm{C}\,(\mathrm{aq})$ at $25\,^\circ\text{C}$ is studied kinetically. The concentrations of $\mathrm{A}$ are measured as a function of time, giving: at $t = 0\,\text{s}$, $[\mathrm{A}] = 0.80\,\text{mol}\times\text{L}^{-1}$; at $t = 10\,\text{s}$, $[\mathrm{A}] = 0.50\,\text{mol}\times\text{L}^{-1}$; at $t = 20\,\text{s}$, $[\mathrm{A}] = 0.32\,\text{mol}\times\text{L}^{-1}$; and at $t = 30\,\text{s}$, $[\mathrm{A}] = 0.22\,\text{mol}\times\text{L}^{-1}$. The observed variation over time is illustrated below.

0 10 20 30 0.20 0.40 0.60 0.80 t (s) [A] (mol/L) (0; 0.80) (10; 0.50) (20; 0.32) (30; 0.22)
  1. a) Calculate the mean rate of disappearance of $\mathrm{A}$ over the three successive intervals: $[0, 10]\,\text{s}$, $[10, 20]\,\text{s}$ and $[20, 30]\,\text{s}$.
  2. b) Compare the three values numerically and explain, using collision theory, the cause of the variation observed as the reaction proceeds.
Solve

Collision theory: effective collisions

In a litre of gas at room temperature there is an enormous number of collisions every second, yet most reactions do not happen instantly. Why do nearly all collisions achieve nothing?

Two collisions between CO and NO₂: one with a suitable orientation that can react, and one with an unsuitable orientation that cannot. O C O N O suitable orientation (C meets an O of NO₂) O C N O O wrong orientation (C meets the N: no O transfer)

Only a tiny fraction of collisions meet both requirements. That is why, despite billions upon billions of collisions per second, most reactions are not instantaneous. A higher temperature gives more particles with energy $\ge E_a$; a higher concentration gives more collisions per second.

Factors that change the rate

Collision theory explains each factor:

  • Concentration (or pressure for gases): more particles in the same volume means more collisions per second. Limitation: it does not always change the rate, for example if the reaction is limited by a catalyst surface that is already full.

  • Surface area: crushing a solid exposes more particles, so more collisions per second.

  • Temperature: more particles have energy $\ge E_a$, and they also collide more often.

  • Catalyst: gives a route with lower $E_a$. Limitations: a catalyst can become saturated or be poisoned, and then it stops working.

Catalysed and uncatalysed profiles

A catalyst gives the reaction a different route with a lower activation energy. On an energy profile diagram the peak is lower, but the reactants and products stay at the same levels, so $\Delta H$ is unchanged. Both the forward and the reverse activation energies fall by the same amount.

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Consider the overall gas-phase reaction between carbon monoxide and nitrogen dioxide: $$\mathrm{CO}\,(\mathrm{g}) + \mathrm{NO_2}\,(\mathrm{g}) \rightarrow…

Consider the overall gas-phase reaction between carbon monoxide and nitrogen dioxide:

$$\mathrm{CO}\,(\mathrm{g}) + \mathrm{NO_2}\,(\mathrm{g}) \rightarrow \mathrm{CO_2}\,(\mathrm{g}) + \mathrm{NO}\,(\mathrm{g})$$

Use a simplified collision model with transfer of an oxygen atom between these molecules, without necessarily identifying it with the complete real mechanism:

  1. a) Explain why not all collisions between $\mathrm{CO}$ and $\mathrm{NO_2}$ molecules lead to the formation of products, stating the two essential requirements for a collision to be effective.
  2. b) Justify which of the two relative orientations favours the reaction: the carbon atom of $\mathrm{CO}$ striking an oxygen atom of $\mathrm{NO_2}$, or the oxygen atom of $\mathrm{CO}$ striking the nitrogen atom of $\mathrm{NO_2}$.
Solve
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Two reactors are designed to study two competing bimolecular pathways starting from the same gaseous reactant $\mathrm{X}$: Pathway 1:…

Two reactors are designed to study two competing bimolecular pathways starting from the same gaseous reactant $\mathrm{X}$:

Pathway 1: $2\,\mathrm{X}\,(\mathrm{g}) \rightarrow \mathrm{Y}\,(\mathrm{g})$, exothermic with $\Delta H_1^\circ = -80\,\text{kJ}\times\text{mol}^{-1}$ and $E_{a,1} = 45\,\text{kJ}\times\text{mol}^{-1}$.

Pathway 2: $2\,\mathrm{X}\,(\mathrm{g}) \rightarrow \mathrm{Z}\,(\mathrm{g})$, exothermic with $\Delta H_2^\circ = -150\,\text{kJ}\times\text{mol}^{-1}$ and $E_{a,2} = 90\,\text{kJ}\times\text{mol}^{-1}$.

The steric factor for Pathway 1 is very restrictive ($p_1 = 0.01$) owing to the requirement for precise spatial alignment, whereas for Pathway 2 it is not very restrictive ($p_2 = 0.80$). The total collision frequency $Z$ is identical for both pathways.

  1. a) Write the modified Arrhenius rate constant ($k = p\times Z\times\exp(-E_a/(R\times T))$) and determine the temperature at which both pathways would have exactly the same rate constant ($k_1 = k_2$).
  2. b) Assuming the entropies of both products are equal, compare their thermodynamic stability using the Gibbs energy. Distinguish which pathway forms product faster initially at temperatures below or above the calculated threshold, and why this kinetic preference does not determine the final composition if both pathways are reversible and reach equilibrium. Data: $R=8,314\,\mathrm{J}\times\mathrm{mol}^{-1}\times\mathrm{K}^{-1}$.
Solve

Energy profiles and activation energy

Use the catalyst button in the widget to compare the catalysed and uncatalysed profiles: the peak drops, but the reactant and product levels (and so $\Delta H$) do not move. This is true for exothermic ($\Delta H < 0$) and endothermic ($\Delta H > 0$) reactions alike.

Two energy profile diagrams: an exothermic reaction where products are lower than reactants, and an endothermic reaction where products are higher. reactants products activated complex Ea ΔH < 0 Exothermic reactants products activated complex Ea ΔH > 0 Endothermic

The next diagram compares the same exothermic reaction with and without a catalyst: the catalysed peak is lower, but the reactant and product levels are the same.

Energy profile of an exothermic reaction with and without a catalyst: the catalysed peak is lower, and the reactant and product levels are unchanged. reactants products uncatalysed catalysed Same ΔH, lower Ea with a catalyst

In the widget, raising $E_a$ makes the hill higher (a slower reaction). Changing $\Delta H$ with $E_a$ fixed moves the level of the products: the top of the hill (the forward $E_a$) stays where it is, but the reverse activation energy changes, because it is the height from the products up to the same peak.

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In the industrial synthesis of ammonia: $$\mathrm{N_2}\,(\mathrm{g}) + 3\,\mathrm{H_2}\,(\mathrm{g}) \rightleftharpoons 2\,\mathrm{NH_3}\,(\mathrm{g}) \quad \Delta…

In the industrial synthesis of ammonia:

$$\mathrm{N_2}\,(\mathrm{g}) + 3\,\mathrm{H_2}\,(\mathrm{g}) \rightleftharpoons 2\,\mathrm{NH_3}\,(\mathrm{g}) \quad \Delta H^\circ = -92.2\,\text{kJ}$$
  1. a) Distinguish conceptually between the rate of a chemical reaction and its extent or equilibrium yield.
  2. b) If the working temperature is increased from $300\,^\circ\text{C}$ to $500\,^\circ\text{C}$, justify which kinetic parameter increases and what happens to the thermodynamic equilibrium constant $K_p$, explaining why a higher rate does not imply a greater final amount of product.
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The potential energy diagram for the elementary gas-phase process: $$\mathrm{A}\,(\mathrm{g}) + \mathrm{B}\,(\mathrm{g}) \rightleftharpoons \mathrm{C}\,(\mathrm{g}) +…

The potential energy diagram for the elementary gas-phase process:

$$\mathrm{A}\,(\mathrm{g}) + \mathrm{B}\,(\mathrm{g}) \rightleftharpoons \mathrm{C}\,(\mathrm{g}) + \mathrm{D}\,(\mathrm{g})$$

shows that the enthalpy of the reactants is $H_R = 45\,\text{kJ}\times\text{mol}^{-1}$, the enthalpy of the products is $H_P = 85\,\text{kJ}\times\text{mol}^{-1}$, and the energy corresponding to the transition state (activated complex) is $H_{\neq} = 130\,\text{kJ}\times\text{mol}^{-1}$.

  1. a) Calculate the enthalpy of the forward reaction ($\Delta H^\circ$), the forward activation energy ($E_{a,\text{dir}}$) and the activation energy of the reverse process ($E_{a,\text{inv}}$).
  2. b) Explain what the activated complex represents physically and justify which of the two processes (forward or reverse) will have the greater rate constant at the same temperature, assuming identical pre-exponential factors.
Solve
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A gas-phase reaction proceeds along the uncatalysed forward energy profile with $E_{a} = 115.0\,\text{kJ}\times\text{mol}^{-1}$ and standard enthalpy change…

A gas-phase reaction proceeds along the uncatalysed forward energy profile with $E_{a} = 115.0\,\text{kJ}\times\text{mol}^{-1}$ and standard enthalpy change $\Delta H^\circ = -35.0\,\text{kJ}\times\text{mol}^{-1}$. When a solid heterogeneous catalyst is added, the forward activation energy is reduced to $68.0\,\text{kJ}\times\text{mol}^{-1}$. Take $R = 8,314\,\text{J}\times\text{mol}^{-1}\times\text{K}^{-1}$ and a temperature of $500\,\text{K}$.

  1. a) Determine the activation energy of the reverse reaction without a catalyst and with a catalyst. State whether the presence of the catalyst changes the enthalpy of reaction or the equilibrium constant.
  2. b) In a simplified estimate of the energy barrier, the Boltzmann factor $\exp(-E_a/(R\times T))$ is used. Calculate the ratio between these factors for the catalysed and uncatalysed routes in the forward direction at $500\,\text{K}$. This factor is not the complete energy distribution, nor does it by itself guarantee an effective collision.
Solve
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To quantify the rate of oxidation of the iodide ion by hydrogen peroxide in acidic medium: $$\mathrm{H_2O_2}\,(\mathrm{aq}) + 2\,\mathrm{I^-}\,(\mathrm{aq}) +…

To quantify the rate of oxidation of the iodide ion by hydrogen peroxide in acidic medium:

$$\mathrm{H_2O_2}\,(\mathrm{aq}) + 2\,\mathrm{I^-}\,(\mathrm{aq}) + 2\,\mathrm{H^+}\,(\mathrm{aq}) \rightarrow \mathrm{I_2}\,(\mathrm{aq}) + 2\,\mathrm{H_2O}\,(\mathrm{l})$$

three independent replicates are carried out in a buffered solution at $298\,\text{K}$. The measured concentrations of $\mathrm{I_2}$ formed after $120\,\text{s}$ are: Replicate 1: $(3.52 \pm 0.04)\times 10^{-3}\,\text{mol}\times\text{L}^{-1}$; Replicate 2: $(3.60 \pm 0.04)\times 10^{-3}\,\text{mol}\times\text{L}^{-1}$; Replicate 3: $(3.56 \pm 0.04)\times 10^{-3}\,\text{mol}\times\text{L}^{-1}$, starting in all cases from a zero initial concentration of $\mathrm{I_2}$. The time is measured with a stopwatch of uncertainty $\pm 1\,\text{s}$.

  1. a) Determine the mean concentration of $\mathrm{I_2}$ at $t = 120\,\text{s}$ with a conservative estimate of the uncertainty, and calculate the mean rate of formation of $\mathrm{I_2}$ over that interval with its corresponding uncertainty. Use, as the convention for this exercise, $\Delta c=(c_{\max}-c_{\min})/2+0.04\times10^{-3}\,\mathrm{mol}\times\mathrm{L}^{-1}$ and $\Delta v/v=\Delta c/\bar c+\Delta t/t$.
  2. b) Deduce the normalised mean rate of the reaction and the mean rate of consumption of the iodide ion $\mathrm{I^-}$ over that time interval, giving the correct units.
Solve

Back to the start: iron wool burns in seconds because its fine strands expose a far larger surface to the oxygen. This increases the number of collisions per second, and so the number of effective collisions with energy $\ge E_a$. A solid bar has little surface exposed, so it reacts very slowly.

Summary

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