(b) By using $r_{n} = r_{0}\frac{n^{2}}{Z}$; where $r_{0} =$ Radius of the Bohr orbit in the ground state atom. So for $He^{+}$ third excited state $n = 4,Z = 2,r_{0} = 0.5\mathring{\mathrm{A}} \Rightarrow r_{4} = 0.5 \times \frac{4^{2}}{2} = 4\mathring{\mathrm{A}}$