(b) According to energy conservation, energy remains the same
$\Rightarrow U_{parallel} = U_{series} \Rightarrow \frac{1}{2}(nC)V^{2} = \frac{1}{2}\left( \frac{C}{n} \right)V^{'2} \Rightarrow V^{'} = nV$
[$V^{'} =$ potential difference across series combination]