Data : T = 2 s, x0 = + A (initially at positive extremity), x = \(\frac A2\)
\(\omega\) = \(\frac{2\pi}T\) = \(\frac{2\pi}2\) = \(\pi\) rad/s
Assuming the particle starts from positive extremity,
x = A cos \(\omega\)t

∴ Starting from the positive extremity, the particle takes \(\frac 13\)s to cover a distance equal to half the amplitude.