In simple harmonic motion (SHM), the displacement \( x \) at time \( t \) is given by:
\[
x = A \sin \omega t
\]
where \( \omega = \frac{2\pi}{T} \) is the angular frequency.
Given that the particle moves from equilibrium (i.e., \( x=0 \) at \( t=0 \)) to \( x = \frac{A}{2} \) in time \( t \):
\[
\frac{A}{2} = A \sin \omega t \implies \sin \omega t = \frac{1}{2}
\]
Therefore,
\[
\omega t = \sin^{-1} \left(\frac{1}{2}\right) = \frac{\pi}{6}
\]
Recall \(\omega = \frac{2\pi}{T}\), so:
\[
\frac{2\pi}{T} t = \frac{\pi}{6} \implies t = \frac{\pi}{6} \times \frac{T}{2\pi} = \frac{T}{12}
\]
However, this is the time taken to reach \( +\frac{A}{2} \) for the first time after starting at 0 (equilibrium).
Note: The particle moves from 0 to \( \frac{A}{2} \) within this time.
Hence, the time taken is:
\[
t = \frac{T}{12}
\]
This matches option (A).
Wait, the options given in the question are different from the final result.
The correct time from equilibrium to \( \frac{A}{2} \) is \( \frac{T}{12} \).
If your options differ, the answer is option (A) \(\frac{T}{12}\).