(a) As angular momentum is conserved in the absence of a torque, therefore
$I_{0}\omega_{0} = I\omega$
$\left( \frac{2}{3}MR^{2} \right)\left( \frac{2\pi}{T_{0}} \right) = \left\lbrack \frac{2}{5}MR^{2} + \frac{2}{5}\frac{MR^{2}}{5 \times 10^{19}}\ \right\rbrack\frac{2\pi}{T}$
$\frac{T}{T_{0}} = 1 + \frac{1}{5 \times 10^{19}}$
$\frac{T}{T_{0}} - 1 = \frac{1}{5 \times 10^{19}} = 2 \times 10^{- 20}$
$\frac{T - T_{0}}{T_{0}} = 2 \times 10^{- 20}\ or\ \frac{\mathrm{\Delta}T}{T_{0}} = 2 \times 10^{- 20}$