In simple harmonic motion (SHM), the displacement of a particle and its acceleration are related through the differential equation:
\(a(t) = -\omega^2 x(t)\),
where \(x(t)\) is the displacement, \(a(t)\) is the acceleration, and \(\omega\) is the angular frequency.
This equation shows that displacement and acceleration are out of phase by \(\pi\) radians because acceleration is proportional to the negative of displacement.
To understand the phase relationship, consider the expressions for displacement and acceleration in terms of phase:
Since \(a(t) = -\omega^2 x(t)\), the acceleration is inverted with respect to the displacement, indicating a phase difference of \(\pi\) radians.
This means that when the particle is at a displacement of \(x(t)\), the acceleration \(a(t)\) is maximally negative, and vice versa, completing the understanding of their phase difference.
Thus, the correct answer is \(\pi\) radians.