Free Pearson Edexcel International A-level Chemistry · Unit 6

Activation energy and temperature-dependent rate data

What you’ll learn

  • Determine activation energy from an Arrhenius plot or two rate constants.
  • Plan temperature measurements and evaluate their effect on a rate investigation.

Understand the idea

Core practical 10 investigates how a rate constant changes with temperature. The Arrhenius relationship becomes linear when ln⁡k\ln k is plotted against 1/T1/T. Temperature must be in kelvin, and the natural logarithm is required. The line has gradient −Ea/R-E_a/R, so a negative gradient corresponds to a positive activation energy. Use a best-fit line through a range of data rather than joining successive points or choosing two adjacent noisy readings.

A relative rate such as 1/t1/t may replace kk for this purpose only if it remains proportional to kk: concentrations, clock threshold, total volume and other relevant conditions must be constant. Otherwise a temperature trend can be mixed with a concentration or endpoint trend. If both axes are calculated from measured quantities, label the transformed axes with the correct scale; a plot against 1000/T1000/T has a different numerical gradient from a plot against 1/T1/T.

The reaction mixture's temperature is the relevant measurement, not merely a bath dial setting. A supervised plan allows solutions to reach the selected temperature, checks the temperature during timing and repeats observations. Evaporation at higher temperatures can alter concentrations and is a separate source of bias. The supplied hazards determine an appropriate controlled heating method; the aim is stable measured conditions rather than simply more heating.

Key formulae

k=Ae−Ea/(RT)k=Ae^{-E_a/(RT)}

ln⁡k=ln⁡A−EaR1T\ln k=\ln A-\frac{E_a}{R}\frac1T

Ea=−R×gradientE_a=-R\times\mathrm{gradient}

ln⁡(k2k1)=EaR(1T1−1T2)\ln\left(\frac{k_2}{k_1}\right)=\frac{E_a}{R}\left(\frac1{T_1}-\frac1{T_2}\right)

Arrhenius slope reveals activation energy

Conditions. Invented Arrhenius process Eₐ = 50000 J mol⁻¹ and kref = k at 330 K. Curve ln(k/kref) = −(50000/8.314)(1/T − 1/330); temperature range about 286–400 K.

Reciprocal temperature / K⁻¹; ln(k/kref) / dimensionless.

The slope is −6013.95 K, giving Eₐ = 50.0 kJ mol⁻¹. Moving left means higher temperature and a larger rate constant; the reference crosses zero at 1/330 K⁻¹.

Open the interactive lesson to view plotted curves and coordinate tables.

Worked example

A reaction has k1=0.0020 s−1k_1=0.0020\ \mathrm{s^{-1}} at 290 K290\ \mathrm{K} and k2=0.0080 s−1k_2=0.0080\ \mathrm{s^{-1}} at 310 K310\ \mathrm{K}. Use R=8.314 J mol−1 K−1R=8.314\ \mathrm{J\,mol^{-1}\,K^{-1}} and the Arrhenius relationship to estimate EaE_a.

  1. The rate-constant ratio is k2/k1=4k_2/k_1=4, so ln⁡(k2/k1)=ln⁡4=1.3863\ln(k_2/k_1)=\ln4=1.3863.
  2. The reciprocal-temperature difference is 1/290−1/310=2.2247×10−4 K−11/290-1/310=2.2247\times10^{-4}\ \mathrm{K^{-1}}.
  3. Thus EaE_a =8.314(1.3863)/(2.2247×10−4)=8.314(1.3863)/(2.2247\times10^{-4}) =5.18×104 J mol−1=5.18\times10^4\ \mathrm{J\,mol^{-1}} =51.8 kJ mol−1=51.8\ \mathrm{kJ\,mol^{-1}}.

Answer: Approximately 51.8 kJ mol−151.8\ \mathrm{kJ\,mol^{-1}}.

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