For the reversible reaction \( A \rightleftharpoons B \) with forward rate constant \( k_1 \) and reverse rate constant \( k_2 \), the rate of change of the concentration of A is governed by both the forward loss and the reverse gain:
\[
-\frac{d[A]}{dt} = k_1[A] - k_2[B]
\]
Using mass balance \( [B] = [A]_0 - [A] \) (starting from pure A) gives a linear first-order differential equation in \( [A] \) whose solution decays exponentially toward the equilibrium concentration, with the exponential rate constant equal to \( (k_1 + k_2) \). Testing each option against this exponent:
- \( \frac{1}{k_1} \): This only accounts for the forward reaction and would apply only if the reverse reaction were absent, which is not the case here.
- \( \frac{1}{k_2} \): This only accounts for the reverse reaction, ignoring the forward rate constant entirely, so it cannot represent a system where both directions actively proceed.
- \( \frac{1}{(k_1 - k_2)} \): Subtracting the two rate constants does not correspond to any term that appears in the differential equation governing the approach to equilibrium, and it could even become undefined or negative if \( k_2 > k_1 \), which is not physically meaningful for a time constant.
- \( \frac{1}{(k_1 + k_2)} \): This matches exactly the combined exponential decay constant that emerges when the forward and reverse rate expressions are combined into a single differential equation for \( [A] \).
The relaxation toward equilibrium in a reversible first-order reaction is governed jointly by both rate constants, and their sum is what sets the exponential time constant.
Therefore, the correct answer is \( \dfrac{1}{(k_1+k_2)} \).