Step 1: Bohr’s quantization condition.
Bohr's quantization condition for rotational energy gives:
\[
E = \frac{n^2 h^2}{8 \pi^2 I}
\]
where \( n \) is the quantum number, \( h \) is Planck’s constant, and \( I \) is the moment of inertia.
Step 2: Energy in second orbit.
For the second orbit, \( n = 2 \). Substituting \( n = 2 \) into the equation gives the rotational energy in the second orbit as:
\[
E = \frac{h^2}{2I^2 \pi^2}
\]
Step 3: Conclusion.
Thus, the correct answer is (A) \( \frac{h^2}{2I^2 \pi^2} \).