Step 1: The charge on a discharging capacitor decays exponentially with the RC time constant:
\[ Q(t) = Q_0\, e^{-t/RC}. \]
Step 2: The activity of a radioactive sample decays exponentially with its mean life \(\tau\) (where the decay constant is \(\lambda = 1/\tau\)):
\[ A(t) = A_0\, e^{-t/\tau}. \]
Step 3: The ratio is
\[ \frac{Q(t)}{A(t)} = \frac{Q_0}{A_0}\, e^{-t\left(\frac{1}{RC} - \frac{1}{\tau}\right)}. \]
For this ratio to be constant in time, the exponent must vanish, i.e. \(\frac{1}{RC} = \frac{1}{\tau}\), so \(RC = \tau\).
Step 4: Solve for \(R\):
\[ R = \frac{\tau}{C} = \frac{20\times 10^{-3}\ \text{s}}{100\times 10^{-6}\ \text{F}} = 200\ \Omega. \]
\[ \boxed{R = 200\ \Omega} \]