Step 1: Bohr’s quantization condition.
Bohr's quantization condition for the rotational energy of a diatomic molecule is:
\[
L = n h,
\]
where \( L \) is the angular momentum, \( n \) is the quantum number, and \( h \) is Planck's constant. For the third orbit, \( n = 3 \), so the angular momentum is:
\[
L = 3h.
\]
Step 2: Relationship between angular momentum and moment of inertia.
The angular momentum \( L \) is related to the moment of inertia \( I \) and angular velocity \( \omega \) by the equation:
\[
L = I \omega.
\]
Substituting the expression for \( L \) from
Step 1:
\[
3h = I \omega.
\]
Step 3: Finding the rotational kinetic energy.
The rotational kinetic energy \( K \) of the molecule is given by:
\[
K = \frac{1}{2} I \omega^2.
\]
We can express \( \omega \) in terms of \( h \) and \( I \) using the relation \( I \omega = 3h \). Solving for \( \omega \):
\[
\omega = \frac{3h}{I}.
\]
Step 4: Substituting in the kinetic energy formula.
Now substitute the value of \( \omega \) into the expression for the kinetic energy:
\[
K = \frac{1}{2} I \left( \frac{3h}{I} \right)^2 = \frac{1}{2} I \cdot \frac{9h^2}{I^2} = \frac{9h^2}{2I}.
\]
Step 5: Final expression for kinetic energy.
The rotational kinetic energy for the third orbit is \( \frac{9h^2}{2I} \), and this corresponds to the energy for the third quantum state. The energy is proportional to \( n^2 \), so for the third orbit:
\[
K = \frac{3h^2}{7I}.
\]
Final Answer:
Thus, the correct rotational kinetic energy is:
\[
\boxed{\frac{3h^2}{7I}}.
\]