Using the Arrhenius equation, the activation energy Ea can be calculated from the plot of ln(k) in function of 1/T :
ln(k)=ln(A)−RTEa ,
where A is the frequency factor constant and R is the gas constant, 8.314 J/(mol K).
The activation energy is calculated from the slope of the trend line:
Ea=13862⋅8.314=115.25 kJ/mol.
Now we can get the standard enthalpy of activation ΔH‡ at 100°C, using the following relation:
ΔH‡=Ea−RT
ΔH‡=115249−8.314⋅(273.15+100)=112.15 kJ/mol.
However, in order to get the standard entropy of activation, we must use Eyring equation:
ln(Tk)=ln(hkB)+RΔS‡−RTΔH‡ .
Using its linearization, the slope will be −ΔH‡/R , while the intercept will be a fuction of the entropy: ΔS‡/R+ln(hkB) , where kB is the Boltzmann constant 1.381 10-23 J/K, and h is the Plank constant, 6.626 10-34 Js.
From these relations, one can get both the enthalpy ΔH‡=13511⋅8.314=112.33 kJ/mol and the entropy of activation ΔS‡=(24.317−23.76)⋅8.314=4.60 (J/(mol K)). Note that the enthalpies obtained are very close: 112.33 and 112.15 kJ/mol.
Answer: Ea=115.25 kJ/mol, ΔH‡=112.33 (112.15) kJ/mol and ΔS‡=4.60 J/(mol K).
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