Step 1: Write the Arrhenius equation in log form.
The rate constant depends on temperature as \[ \ln k = \ln A - \frac{E_a}{R}\cdot\frac{1}{T} \] This is a straight line of \(\ln k\) versus \(1/T\) with intercept \(\ln A\).
Step 2: Read the intercept from the graph.
The line cuts the \(\ln k\) axis at \(6\), so \(\ln A = 6\).
Step 3: Convert the data to consistent units.
\(E_a = 6.64\ kJ\,mol^{-1} = 6640\ J\,mol^{-1}\) and \(R = 8.3\ J\,K^{-1}mol^{-1}\). Now the joules cancel cleanly.
Step 4: Put in the target rate constant.
We want \(k = e^2\), so \(\ln k = 2\). Substitute into the equation: \[ 2 = 6 - \frac{6640}{8.3\,T} \]
Step 5: Solve for the temperature.
Rearrange: \(\dfrac{6640}{8.3\,T} = 6-2 = 4\), so \[ T = \frac{6640}{8.3\times 4} = \frac{6640}{33.2} \]
Step 6: Compute and conclude.
Since \(33.2\times 200 = 6640\), we get \(T = 200\ K\).
\[ \boxed{T = 200\ \text{K}} \]