Concept:
The dependence of the rate constant ($k$) of a chemical reaction on the absolute temperature ($T$) is mathematically described by the logarithmic form of the
Arrhenius Equation:
\[
k = A \cdot e^{-\frac{E_a}{RT}} \quad \Rightarrow \quad \ln k = \ln A - \frac{E_a}{R}\left(\frac{1}{T}\right)
\]
Where:
• $k$ = Rate constant of the chemical reaction.
• $A$ = Arrhenius pre-exponential frequency factor.
• $E_a$ = Activation energy required for the reaction.
• $R$ = Universal Gas Constant.
• $T$ = Absolute temperature in Kelvin (K).
When plotting $\ln k$ on the vertical $y$-axis against $\frac{1}{T}$ on the horizontal $x$-axis, the equation represents a straight line matching the standard linear form $y = mx + c$, where the slope $m = -\frac{E_a}{R}$ and the $y$-intercept $c = \ln A$.
Step 1: Extracting the value of the y-intercept ($\ln A$) from the given graph.
Looking closely at the provided Arrhenius graph, the straight line intersects the vertical $\ln k$ axis exactly at the numerical value of $6$.
By definition, the $y$-intercept occurs where the horizontal coordinate $\frac{1}{T} = 0$. Therefore:
\[
\text{Intercept} = \ln A = 6
\]
Step 2: Converting given units to standard SI units.
The problem provides the following thermodynamic constants:
• Activation Energy, $E_a = 6.64 \text{ kJ mol}^{-1} = 6.64 \times 10^3 \text{ J mol}^{-1} = 6640 \text{ J mol}^{-1}$
• Universal Gas Constant, $R = 8.3 \text{ J K}^{-1}\text{ mol}^{-1}$
It is essential to convert $E_a$ from kilojoules to joules so that the units cancel out perfectly with the units of the gas constant $R$.
Step 3: Setting up the specific Arrhenius equation for the target rate constant.
We are asked to find the specific temperature $T$ where the rate constant $k$ reaches a value of $e^2 \text{ min}^{-1}$. Let us take the natural logarithm of this target rate constant:
\[
k = e^2 \quad \Rightarrow \quad \ln k = \ln(e^2) = 2
\]
Now, substitute the values $\ln k = 2$ and $\ln A = 6$ into the logarithmic Arrhenius equation:
\[
\ln k = \ln A - \frac{E_a}{RT}
\]
\[
2 = 6 - \frac{E_a}{RT}
\]
Step 4: Isolating and computing the absolute temperature $T$.
Rearranging the algebraic terms to isolate the temperature component on one side:
\[
\frac{E_a}{RT} = 6 - 2
\]
\[
\frac{E_a}{RT} = 4
\]
Cross-multiplying to solve explicitly for $T$:
\[
T = \frac{E_a}{4R}
\]
Substituting the numerical values of $E_a$ and $R$ that we prepared in Step 2:
\[
T = \frac{6640}{4 \times 8.3}
\]
Let us calculate the product in the denominator first:
\[
4 \times 8.3 = 33.2
\]
Now, divide the numerator by this product:
\[
T = \frac{6640}{33.2}
\]
To make the division cleaner, multiply both the numerator and the denominator by 10 to eliminate the decimal:
\[
T = \frac{66400}{332}
\]
Observing that $332 \times 2 = 664$:
\[
T = 200\text{ K}
\]
The calculated absolute temperature is exactly $200\text{ K}$, which perfectly corresponds to Option (4).