A simple pendulum exhibits simple harmonic motion (SHM) only at small angles near the equilibrium position due to the non-linear nature of the restoring force. At larger angles, the relationship between the angle and the restoring force becomes more complex, causing the period of the pendulum to increase rather than remain constant. The acceleration of the pendulum bob is proportional to sin(θ), which approximates θ only for small angles, allowing for SHM. As the angle increases, the pendulum's motion deviates from SHM, and additional vibrations can occur. Therefore, the conditions for SHM are strictly limited to small angular displacements.