5.1.1(j)-(k) - Arrhenius equation and temperature effects

5.1.1(j)-(k) - Arrhenius equation and temperature effects

Temperature changes can make a reaction seem suddenly faster or slower, even when the concentrations have not changed. In this lesson you will connect that observation to the rate constant, kk, and then use the Arrhenius equation to turn temperature-rate data into a straight-line graph. The goal is not to memorise the data-sheet equations, but to know how to use them accurately.

Temperature and the Rate Constant

For a reaction with a rate equation, the rate constant kk is the factor that links the concentrations in the rate equation to the observed rate. At a fixed temperature, kk is constant for that reaction. When the temperature changes, kk changes too.

The particle explanation comes from collision theory and Boltzmann distributions. At a higher temperature, molecules have a higher average kinetic energy. A larger proportion of molecules have energy equal to or greater than the activation energy, EaE_a, so a larger proportion of collisions can lead to reaction.

That increases the reaction rate. Since the concentration terms in a rate equation may be unchanged, the increase in rate is described by an increase in the rate constant, kk.

Activation Energy

Activation energy, EaE_a, is the minimum energy that colliding particles must have for a reaction to occur.

Worked reasoning: why kk changes

Suppose the same reaction mixture is warmed from 298 K to 308 K without changing the concentrations. The concentration terms in the rate equation have not changed, but the rate increases. The rate equation can only reflect that increase by a larger value of kk.

So the careful OCR-style chain is:

  1. temperature increases
  2. a greater proportion of molecules have energy equal to or greater than EaE_a
  3. more collisions can lead to reaction
  4. rate increases
  5. therefore kk increases

Do not say that temperature lowers the activation energy. The activation energy for the uncatalysed pathway is unchanged; the energy distribution of the molecules has changed.

The Arrhenius Equation

The Arrhenius equation gives the mathematical relationship between the rate constant and temperature:

Arrhenius Equation

k=Ae−Ea/RTk = Ae^{-E_a/RT}

The symbols mean:

SymbolMeaning
kkrate constant
AApre-exponential factor
EaE_aactivation energy
RRgas constant, provided on the data sheet
TTtemperature in K

OCR provides the equation and the gas constant on the data sheet. You still need to choose the equation correctly, substitute carefully and handle the units.

The equation contains an exponential term, e−Ea/RTe^{-E_a/RT}. This is why kk does not increase in a simple straight-line way as temperature increases. As TT increases, RTRT increases, so Ea/RTE_a/RT becomes smaller. The exponent −Ea/RT-E_a/RT becomes less negative, the exponential term becomes larger, and kk becomes larger.

Worked example: reading the direction of change

For the same reaction, compare 300 K and 330 K. The value of AA is treated as constant for this Arrhenius analysis, and EaE_a is the same activation energy for the reaction. At 330 K, the denominator RTRT is larger, so −Ea/RT-E_a/RT is less negative. Therefore e−Ea/RTe^{-E_a/RT} is larger and kk is larger.

This matches the collision explanation: higher temperature gives more molecules enough energy to react, so the rate constant increases.

To compare two temperatures without knowing AA, divide the two expressions. For constant AA and EaE_a:

k2k1=exp⁡ ⁣[EaR(1T1−1T2)].\frac{k_2}{k_1}=\exp\!\left[\frac{E_a}{R}\left(\frac1{T_1}-\frac1{T_2}\right)\right].

For Ea=40000 J mol−1E_a=40000\ \mathrm{J\,mol^{-1}}, warming from 300 K to 320 K gives an exponent of 1.002 and a ratio of 2.72. The units of EaE_a must match RR; 40.0 kJ must first become 40000 J.

Straight-Line Form

The Arrhenius equation is most useful in OCR calculations when it is rearranged into a straight-line form:

Linear Arrhenius Equation

ln⁡k=−EaRT+ln⁡A\ln k = -\frac{E_a}{RT} + \ln A

It is clearer if you write the temperature part as 1/T1/T:

ln⁡k=−EaR(1T)+ln⁡A\ln k = -\frac{E_a}{R}\left(\frac{1}{T}\right) + \ln A

This now matches the straight-line equation:

y=mx+cy = mx + c
Straight-line termArrhenius plot term
yyln⁡k\ln k
xx1/T1/T
gradient, mm−Ea/R-E_a/R
intercept, ccln⁡A\ln A

[DIAGRAM: asset_name: Lesson 5.1.1j-k: Arrhenius equation and temperature effects - diagram 01; asset_slug: 05_01_01e_arrhenius_equation_and_temperature_effects__diagram_01; recommended_method: drawn_chem; description: A clean 16:9 two-panel graph. Left panel shows the exponential increase of rate constant k with temperature T using k = A exp(-Ea/RT). Right panel shows a linear Arrhenius plot of ln k against 1/T with negative gradient -Ea/R and a note that the intercept ln A is at 1/T = 0.]
Diagram

The graph of ln⁡k\ln k against 1/T1/T has a negative gradient because EaE_a and RR are both positive, so −Ea/R-E_a/R is negative. As 1/T1/T increases, temperature is actually decreasing, so ln⁡k\ln k decreases.

Taking natural logarithms gives ln⁡k=ln⁡A+ln⁡(e−Ea/RT)\ln k=\ln A+\ln(e^{-E_a/RT}). Since ln⁡(ez)=z\ln(e^z)=z, the second term is −Ea/RT-E_a/RT. This explains why the transformation works, rather than merely naming the graph axes.

Finding Activation Energy

Once you have the gradient of an Arrhenius plot, you can calculate the activation energy:

gradient=−EaR\text{gradient} = -\frac{E_a}{R}

Rearrange:

Ea=−gradient×RE_a = -\text{gradient} \times R

Continue this lesson.

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