Activation energy \((E_a)\) are rate constant (\(k_1\) and \(k_2\)) of a chemical reaction at two different temperatures (\(T_1\) and \(T_2\)) are related by: |
\(ln\frac{k_2}{k_1} = \frac{E_a}{2.303 R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) \(ln \frac{k_2}{k_1} = -\frac{E_a}{R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) \(ln \frac{k_2}{k_1} = \frac{E_a}{R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) \(ln\frac{k_2}{k_1} = -\frac{E_a}{2.303 R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) |
\(ln \frac{k_2}{k_1} = \frac{E_a}{R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) |
The correct answer is option 3. \(ln \frac{k_2}{k_1} = \frac{E_a}{R}\left[\frac{1}{T_1} - \frac{1}{T_2}\right]\). Most of the chemical reactions are accelerated by increase in temperature. It has been found that for a chemical reaction with rise in temperature by 10°, the rate constant is nearly doubled. The effect of temperature on the rate of a reaction and hence on the rate constant k, was proposed by Arrhenius (1889). The equation is called Arrhenius equation, is usually written in the form
\(k Ae^{-E_a/RT}\) ---------(i) where, the pre-exponential factor, \(A\) is a constant and is called frequency factor (because it gives the frequency of binary collisions and the reacting molecules per second per litre), \(E_a\) is the energy of activation, \(R\) is gas constant \(T\) is the absolute temperature The two quantities ‘\(E_a\)’ and ‘\(A\)’ are together called Arrhenius parameters. The energy of activation \((E_a)\) is an important quantity as it is characteristic of the reaction. Using the above equation its value can be calculated. Taking logarithm on both sides of equation (i), we get \(ln k = ln\left(Ae^{-E_a/RT}\right)\) \(⇒ ln k = ln A + ln (e^{-E_a/RT})\) \(⇒ ln k = ln A + \left(\frac{-E_a}{RT}\right)\) \(∴ ln k = ln A - \frac{E_a}{RT}\) --------(ii) If the value of the rate constant at temperature T1 and T2 are k1 and k2 respectively, then we have \(⇒ ln k_1 = ln A - \frac{E_a}{RT_1}\) ---------(iii) and \(⇒ ln k_2 = ln A - \frac{E_a}{RT_2}\) -----------(iv) Subtracting equation (iii) from equation (iv), we get \(ln k_2 - ln k_1 = -\frac{E_a}{RT_2} - \left(-\frac{E_a}{RT_1}\right)\) \(⇒ ln k_2 - ln k_1 = \frac{E_a}{RT_1} - \left(-\frac{E_a}{RT_2}\right)\) \(⇒ ln \frac{k_2}{k_1} = \frac{E_a}{RT_1} - \left(-\frac{E_a}{RT_2}\right)\) \(⇒ ln \frac{k_2}{k_1} = \frac{E_a}{R} \left[\frac{1}{T_1} - \frac{1}{T_2}\right]\) |