Concept:
According to the Rydberg formula, the wavelength of a spectral line emitted during an electronic transition in a hydrogen atom is given by
\[
\frac{1}{\lambda}
=
R
\left(
\frac{1}{n_1^2}
-
\frac{1}{n_2^2}
\right),
\]
where:
• $R$ is the Rydberg constant,
• $n_1$ is the lower energy level,
• $n_2$ is the higher energy level.
For the Balmer series,
\[
n_1 = 2.
\]
Also, according to Bohr's model of the hydrogen atom, the radius of the $n^{\text{th}}$ orbit is
\[
r_n \propto n^2.
\]
Therefore,
\[
\frac{r_{\text{higher}}}{r_{\text{lower}}}
=
\frac{n_2^2}{n_1^2}.
\]
Hence, we first determine the value of the higher orbit $n_2$.
Step 1: Substitute the given wavelength into the Rydberg formula
Given,
\[
\lambda=\frac{7.2}{R}.
\]
Therefore,
\[
\frac{1}{\lambda}
=
\frac{R}{7.2}.
\]
Using the Balmer series relation,
\[
\frac{R}{7.2}
=
R
\left(
\frac{1}{2^2}
-
\frac{1}{n_2^2}
\right).
\]
Cancelling $R$ from both sides,
\[
\frac{1}{7.2}
=
\frac{1}{4}
-
\frac{1}{n_2^2}.
\]
Since
\[
7.2=\frac{36}{5},
\]
we obtain
\[
\frac{1}{7.2}
=
\frac{5}{36}.
\]
Thus,
\[
\frac{5}{36}
=
\frac{1}{4}
-
\frac{1}{n_2^2}.
\]
Step 2: Calculate the higher energy level
Rearranging,
\[
\frac{1}{n_2^2}
=
\frac{1}{4}
-
\frac{5}{36}.
\]
Taking LCM $36$,
\[
\frac{1}{n_2^2}
=
\frac{9-5}{36}
=
\frac{4}{36}
=
\frac{1}{9}.
\]
Hence,
\[
n_2^2=9
\]
and therefore,
\[
n_2=3.
\]
So the electronic transition occurs from
\[
n_2=3
\quad \text{to} \quad
n_1=2.
\]
Step 3: Find the ratio of orbital radii
Since
\[
r_n \propto n^2,
\]
we have
\[
\frac{r_{\text{higher}}}{r_{\text{lower}}}
=
\frac{r_3}{r_2}
=
\frac{3^2}{2^2}
=
\frac{9}{4}.
\]
Therefore,
\[
r_{\text{higher}} : r_{\text{lower}}
=
9 : 4.
\]
\[
\boxed{9:4}
\]