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Svante Arrhenius proposed in 1889 that the rate constant depends on temperature according to:
k = A e^(-Ea / RT)
where:
The equation expresses two physical ideas:
Multiplying the two gives the rate constant k: collisions per unit time x probability that they react.
Even though T appears only in the exponent, a small change in T changes -Ea/RT a lot (because Ea tends to be tens or hundreds of kJ mol^-1 while RT is only a few kJ mol^-1). A 10 K rise in temperature near room temperature roughly doubles k for a typical reaction with Ea around 50 kJ mol^-1.
Example calculation:
Ratio: 3.31/1.72 ≈ 1.92, i.e. k roughly doubles. That matches the rule of thumb.
Taking natural logarithms of both sides of k = A e^(-Ea/RT):
ln k = ln A + (-Ea/RT)
ln k = -Ea/R x (1/T) + ln A
This has the form y = m x + c, where:
So a plot of ln k (y) against 1/T (x) should be a straight line with gradient -Ea/R and intercept ln A. This is the standard OCR method for determining Ea experimentally.
A reaction is studied at five temperatures, with these k values:
| T / K | 1/T / K^-1 | k / s^-1 | ln k |
|---|---|---|---|
| 300 | 3.33 x 10^-3 | 1.0 x 10^-3 | -6.91 |
| 310 | 3.23 x 10^-3 | 2.0 x 10^-3 | -6.21 |
| 320 | 3.13 x 10^-3 | 3.9 x 10^-3 | -5.55 |
| 330 | 3.03 x 10^-3 | 7.6 x 10^-3 | -4.88 |
| 340 | 2.94 x 10^-3 | 1.4 x 10^-2 | -4.27 |
Plot ln k (y) against 1/T (x). The line is approximately straight with gradient:
Gradient = (ln k_2 - ln k_1)/(1/T_2 - 1/T_1) = (-4.27 - (-6.91))/(2.94 x 10^-3 - 3.33 x 10^-3) = 2.64 / (-3.9 x 10^-4) ≈ -6770 K
Then:
Ea = -gradient x R = -(-6770) x 8.314
= 56 300 J mol^-1
= 56.3 kJ mol^-1
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