Let the current drawn by the 20 \(\Omega\) resistance be \(I_1\). The current when the resistance \(R\) is added in parallel becomes \(I_2 = 2I_1\). From Ohm's law:
\[
I_1 = \frac{V}{R_1} = \frac{400}{20} = 20 \, \text{A}
\]
Now, the equivalent resistance of the parallel combination is:
\[
R_{\text{eq}} = \frac{R_1 R}{R_1 + R} = \frac{20R}{20 + R}
\]
The current doubles, so:
\[
I_2 = \frac{400}{R_{\text{eq}}} = 2I_1 = 40 \, \text{A}
\]
Solving for \(R\), we get \(R = 20 \, \Omega\).