a
$\frac{ hc }{\lambda_{ a }}=13.6\left[\frac{1}{1}-\frac{1}{4^2}\right]$ $. . . . . . .(1)$
$\frac{ hc }{\lambda_0}=13.6\left[\frac{1}{ m ^2}-\frac{1}{4^2}\right]$ $. . . . . . .(1)$
$(ii) / (i),$ we get
$\frac{\lambda_{ a }}{\lambda_0}=\frac{\left[\frac{1}{ m ^2}-\frac{1}{16}\right]}{\left[1-\frac{1}{16}\right]}=\frac{1}{5}$
$\Rightarrow \frac{1}{ m ^2}-\frac{1}{16}=\frac{15}{16} \times \frac{1}{5}$
$\Rightarrow \frac{1}{ m ^2}-\frac{1}{16}=\frac{3}{16}$
$\Rightarrow \frac{1}{ m ^2}=\frac{3}{16}+\frac{1}{16}$
$\Rightarrow m =2$
from $(ii)$
$\frac{ hc }{\lambda_0}=13.6\left[\frac{1}{2^2}-\frac{1}{4^2}\right]=13.6 \times \frac{3}{10} ev$
$\Rightarrow \lambda_0=\frac{12400 \times 16}{13.6 \times 3} \mathring A$
$\Rightarrow \lambda_0 \approx 4862 \mathring A$
we have $K E_u \propto \frac{z^2}{n^2}$
$\Rightarrow \frac{ KE _2}{ KE _1}=\frac{1}{4}$
$\Delta P _{ a }=\frac{ h }{\lambda_{ a }}$
$\Delta P _0=\frac{ h }{\lambda_0}$
$\Rightarrow \frac{\Delta P _{ a }}{\Delta P }=\frac{\lambda_0}{\lambda}$