(b)
For first excited state ($i.e$., second energy level)
$\ \ \ \ \ \ \ \ \ \ \ \ \ n = 2$
$\ \ \ \ \ \ \ \ \ \ \ r_{n} = \frac{a_{0}.n^{2}}{Z}$
$\ \ \ \ \left( where,\ a_{0} = Bohr\ radius = 0.53\ \mathring{\mathrm{A}} \right)$
$\ \ \ \ \ \ \ \ \ \ \ r_{2} = \frac{a_{0}(2)^{2}}{1}\ \ \ \ \ \ \ \ \ \ \ \ \ \ (for\ H,Z = 1)$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = 4a_{0}$