(a) From Einstein’s theorem
Relativistic momentum $= \frac{m_{0}v}{\sqrt{1 - v^{2}/c^{2}}}$
Putting $v = 2v$
We get $p = \ \frac{m_{0}(2v)}{\sqrt{1 - {(2v}^{2})/c^{2}}} = 2\left( \frac{m_{0}v}{\sqrt{1 - {4v}^{2}/c^{2}}} \right)$
So, the momentum becomes more than the double.