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All chaptersChemistry · Unit 3

Chemical Kinetics

10 articles31 formulas54 ways the board asks it
CHETemperature & Collision Theory

Arrhenius Equation & Temperature Dependence

The Arrhenius equation quantifies how rate constants rise with temperature through the activation energy EaE_a. ISC problems use either the two-temperature form to find EaE_a, or the single-equation form with AA given; mastering the logarithmic rearrangements is essential.

Arrhenius equation
k=A e−Ea/RTk = A\,e^{-E_a/RT}
AA frequency factor, EaE_a activation energy, R=8.314 J mol−1K−1R=8.314\,J\,mol^{-1}K^{-1}
Logarithmic (single-temperature) form
log⁡k=log⁡A−Ea2.303 RT\log k = \log A - \dfrac{E_a}{2.303\,RT}
slope of log⁡k\log k vs 1/T1/T is −Ea2.303R-\dfrac{E_a}{2.303R}
Two-temperature form
log⁡k2k1=Ea2.303 R(1T1−1T2)\log\dfrac{k_2}{k_1} = \dfrac{E_a}{2.303\,R}\left(\dfrac{1}{T_1} - \dfrac{1}{T_2}\right)
k1,k2k_1,k_2 are rate constants at T1<T2T_1<T_2
Fraction of effective molecules
kA=e−Ea/RT\dfrac{k}{A} = e^{-E_a/RT}
fraction of molecules with energy ≥Ea\ge E_a
  • Arrhenius equation: k=A e−Ea/RTk = A\,e^{-E_a/RT}, where AA is the frequency (pre-exponential) factor and e−Ea/RTe^{-E_a/RT} is the fraction of molecules with energy ≥Ea\ge E_a.
  • Logarithmic form: log⁡k=log⁡A−Ea2.303 RT\log k = \log A - \dfrac{E_a}{2.303\,RT}; a plot of log⁡k\log k vs 1T\dfrac{1}{T} is linear with slope −Ea2.303 R-\dfrac{E_a}{2.303\,R}.
  • Two-temperature form: log⁡k2k1=Ea2.303 R(1T1−1T2)\log\dfrac{k_2}{k_1} = \dfrac{E_a}{2.303\,R}\left(\dfrac{1}{T_1} - \dfrac{1}{T_2}\right) — the workhorse for finding EaE_a or a missing kk.
  • Rate roughly doubles for every 10 K10\,K rise near room temperature; this stems from the steep rise in molecules crossing EaE_a, not a large change in collision number.
  • Lower EaE_a means a larger rate constant; a catalyst raises kk by providing a path of lower EaE_a, not by changing TT.
  • Keep units consistent: R=8.314 J mol−1K−1R = 8.314\,J\,mol^{-1}K^{-1} gives EaE_a in joules, so convert kJ to J (or use RR in kJ) before computing.
  • The frequency factor AA depends on how often molecules collide and on the orientation needed; the temperature dependence of kk enters almost entirely through e−Ea/RTe^{-E_a/RT}.
  • From the log⁡k\log k vs 1/T1/T graph, Ea=−2.303 R×(slope)E_a = -2.303\,R\times(\text{slope}) and the intercept gives log⁡A\log A — a standard graphical-determination answer.
  • The factor (1T1−1T2)\left(\dfrac{1}{T_1}-\dfrac{1}{T_2}\right) is positive when T2>T1T_2>T_1, making log⁡(k2/k1)\log(k_2/k_1) positive — kk always increases with temperature for Ea>0E_a>0.
  • Always convert Celsius to Kelvin before substituting, e.g. 27∘C=300 K27^\circ C = 300\,K; using ∘C^\circ C directly is a fatal error.
  • When AA is given, compute kk directly from k=A e−Ea/RTk=A\,e^{-E_a/RT}; evaluate the exponent −Ea/RT-E_a/RT first, then the exponential (often supplied as a hint value).
  • Reactions with very high EaE_a are slow and strongly temperature-sensitive; near-zero EaE_a reactions are fast and almost temperature-independent.
Where the marks go
  • Mixing units of EaE_a and RR — if EaE_a is in kJ, convert to J (multiply by 10001000) before dividing by R=8.314 J mol−1K−1R=8.314\,J\,mol^{-1}K^{-1}.
  • Sign errors in (1T1−1T2)\left(\dfrac{1}{T_1}-\dfrac{1}{T_2}\right): writing it as (1T2−1T1)\left(\dfrac{1}{T_2}-\dfrac{1}{T_1}\right) flips the sign and gives a negative EaE_a.
  • Reading the slope of log⁡k\log k vs 1/T1/T as −Ea/R-E_a/R instead of −Ea/2.303R-E_a/2.303R — the 2.3032.303 comes from using log⁡10\log_{10}.
  • Forgetting to convert temperatures from ∘C^\circ C to KK before substituting into the two-temperature equation.
  • Claiming a catalyst increases AA or TT — it works by lowering EaE_a in the exponential term, leaving TT unchanged.
How the board asks it
  • Numericaltwo-temperature form solved for the activation energy
    The rate constant of a reaction is 1.5×10−3 s−11.5\times10^{-3}\,s^{-1} at 300 K300\,K and 4.5×10−3 s−14.5\times10^{-3}\,s^{-1} at 320 K320\,K. Calculate the activation energy EaE_a of the reaction (R=8.314 J mol−1 K−1)(R=8.314\,J\,mol^{-1}\,K^{-1}).
  • Numericaltwo-temperature form solved for a missing rate constant
    The activation energy of a reaction is 209.5 kJ mol−1209.5\,kJ\,mol^{-1} and its rate constant at 581 K581\,K is 1.0×10−2 s−11.0\times10^{-2}\,s^{-1}. Calculate the rate constant at 700 K700\,K (R=8.314 J mol−1 K−1)(R=8.314\,J\,mol^{-1}\,K^{-1}).
  • Numericalsingle-equation form with the frequency factor given
    For a first-order reaction, A=4×1013 s−1A=4\times10^{13}\,s^{-1} and Ea=98.6 kJ mol−1E_a=98.6\,kJ\,mol^{-1}. Calculate the rate constant kk at 400 K400\,K (R=8.314 J mol−1 K−1(R=8.314\,J\,mol^{-1}\,K^{-1}; take antilog where required)).
  • Derive / provelogarithmic form and the log⁡k\log k vs 1/T1/T plot
    Starting from k=A e−Ea/RTk=A\,e^{-E_a/RT}, derive log⁡k2k1=Ea2.303 R(1T1−1T2)\log\dfrac{k_2}{k_1}=\dfrac{E_a}{2.303\,R}\left(\dfrac{1}{T_1}-\dfrac{1}{T_2}\right) and explain how EaE_a is obtained from the slope of a graph of log⁡k\log k against 1T\dfrac{1}{T}.
  • Give reasonssteep rise of e−Ea/RTe^{-E_a/RT} with temperature
    Account for the fact that the rate of a reaction nearly doubles for a 10 K10\,K rise in temperature near room temperature, although the number of collisions increases only slightly.
  • Define / statephysical meaning of the activation energy
    Define activation energy EaE_a, and state how a reaction with a high EaE_a differs from one with a low EaE_a in the sensitivity of its rate constant to temperature.

Practise this topic

Written for Sublevo. Question text quoted anywhere in these notes is the Council’s and carries its year and paper; the board’s own diagrams are not reproduced.