Using the Arrhenius equation, the activation energy "E_a" can be calculated from the plot of "\\text{ln}(k)" in function of "1\/T" :
"\\text{ln}(k) = \\text{ln}(A) - \\frac{E_a}{RT}" ,
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:
"E_a = 13862\\cdot8.314 = 115.25" kJ/mol.
Now we can get the standard enthalpy of activation "\\Delta H^\u2021" at 100°C, using the following relation:
"\\Delta H^\u2021 = E_a-RT"
"\\Delta H^\u2021 = 115249-8.314\\cdot(273.15+100) = 112.15" kJ/mol.
However, in order to get the standard entropy of activation, we must use Eyring equation:
"\\text{ln}(\\frac{k}{T}) = \\text{ln}(\\frac{k_B}{h}) +\\frac{\\Delta S^\u2021}{R} - \\frac{\\Delta H^\u2021}{RT}" .
Using its linearization, the slope will be "-\\Delta H^\u2021\/R" , while the intercept will be a fuction of the entropy: "\\Delta S^\u2021\/R + \\text{ln}(\\frac{k_B}{h})" , where "k_B" 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 "\\Delta H^\u2021 = 13511\\cdot8.314 = 112.33" kJ/mol and the entropy of activation "\\Delta S^\u2021 = (24.317-23.76)\\cdot8.314 = 4.60" (J/(mol K)). Note that the enthalpies obtained are very close: 112.33 and 112.15 kJ/mol.
Answer: "E_a = 115.25" kJ/mol, "\\Delta H^\u2021 =112.33" (112.15) kJ/mol and "\\Delta S^\u2021 = 4.60" J/(mol K).
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