(a) Extension is first case
$\mathrm{\Delta}l_{1} = 2a - a = a$
From Hooke’s law
$F = k\mathrm{\Delta}l_{1}$
$mr\omega^{2} = ka$
$m(2a)\omega^{2} = ka$
$2ma\left( \frac{2\pi}{T} \right)^{2} = ka$
In second case,
$m(3a)\left( \frac{2\pi}{T^{'}} \right)^{2} = k(3a - 2a)$
On dividing Eq. (ii) by Eq. (i)
$T^{'} = \sqrt{\frac{3}{2}}T$