From Heisenberg's uncertainty principle:
\[
\Delta x \cdot \Delta p \geq \frac{\hbar}{2}
\]
For a particle in a box, the uncertainty in position is approximately the box length:
\[
\Delta x \approx L
\]
If the box length doubles (\( 2L \)), the uncertainty in position increases:
\[
\Delta p \propto \frac{1}{\Delta x} = \frac{1}{L}
\]
Since \( L \) becomes \( 2L \), the uncertainty in momentum reduces by half:
\[
\Delta p' = \frac{1}{2} \Delta p
\]