(c)
We know that,
$\mathrm{\Delta}E = hc.R\left\lbrack \frac{1}{n_{1}^{2}} - \frac{1}{n_{2}^{2}} \right\rbrack$
For lowest energy, of the spectral line in Lyman series, $n_{1} = 1,\ n_{2} = 2$
Hence,
$\mathrm{\Delta}E = hc.R\left\lbrack \frac{1}{1^{2}} - \frac{1}{2^{2}} \right\rbrack$
$\mathrm{\Delta}E = \frac{3hcR}{4}$