Idea: Match the two time constants so both quantities fall off at the same rate.
Radioactive side: Activity is $A = \lambda N = \lambda N_0 e^{-\lambda t}$. The mean (average) life is $\tau = 1/\lambda = 20\ \text{ms}$, so $A \propto e^{-t/\tau}$ with $\tau = 20\times 10^{-3}\ \text{s}$.
Capacitor side: A charged capacitor released across a resistor loses charge as $Q \propto e^{-t/(RC)}$, so its characteristic time is $RC$.
Constant ratio condition: The quotient $Q/A$ carries the factor $e^{-t/(RC)}/e^{-t/\tau} = e^{-t\left(1/RC - 1/\tau\right)}$. It is time independent only when the decay rates are identical:
\[ \frac{1}{RC} = \frac{1}{\tau} \;\Rightarrow\; RC = \tau. \]
Plugging in the numbers,
\[ R = \frac{\tau}{C} = \frac{0.020}{100\times 10^{-6}} = 200\ \Omega. \]
Hence the resistance must be 200 ohm.
\[ \boxed{R = 200\ \Omega} \]