The charge q on a capacitor discharging through a resistor R is given by:
$q(t) = q_0 e^{-t/RC}$, where $q_0$ is the initial charge and RC is the time constant.
The activity A of a radioactive sample is given by:
$A(t) = A_0 e^{-\lambda t}$, where $A_0$ is the initial activity and $\lambda$ is the decay constant.
We are given that the ratio $\frac{q(t)}{A(t)}$ is fixed with respect to time (i.e., it is constant).
$\frac{q(t)}{A(t)} = \frac{q_0 e^{-t/RC}}{A_0 e^{-\lambda t}} = \frac{q_0}{A_0} e^{(-\frac{t}{RC} + \lambda t)} = \frac{q_0}{A_0} e^{t(\lambda - \frac{1}{RC})}$
For this ratio to be constant for all t, the exponent of the exponential term must be zero.
$\lambda - \frac{1}{RC} = 0 \implies \lambda = \frac{1}{RC}$
This means the time constant of the RC circuit must be equal to the mean life of the radioactive sample, since the mean life $\tau_{avg} = 1/\lambda$.
So, $RC = \tau_{avg}$.
We are given:
Average life, $\tau_{avg} = 30$ ms = $30 \times 10^{-3}$ s.
Capacitance, $C = 200 \, \mu\text{F} = 200 \times 10^{-6}$ F.
Now we can solve for R:
$R = \frac{\tau_{avg}}{C} = \frac{30 \times 10^{-3} \text{ s}}{200 \times 10^{-6} \text{ F}}$
$R = \frac{30}{200} \times 10^3 = \frac{3}{20} \times 1000 = 3 \times 50 = 150 \, \Omega$.