Acceleration due to gravity at depth $d$ from the surface of earth $g^{\prime}=g\left(1-\frac{d}{\mathrm{R}}\right)=g\left(\frac{\mathrm{R}-d}{\mathrm{R}}\right)$
Let $\mathrm{R}-d=y$,
$g^{\prime}=\frac{g y}{R}$
Force on a body of mass $m$ at point $P$,
$\mathrm{F}=-m g^{\prime}$ (force is considered negative
$\mathrm{F}=-\frac{m g}{\mathrm{R}} \cdot y \quad \ldots$ (1) toward the centre)
$\therefore \mathrm{F} \propto-y$
$(A)$ Restoring torque in case $A =$ Restoring torque in case $B$
$(B)$ Restoring torque in case $A < $ Restoring torque in case $B$
$(C)$ Angular frequency for case $A > $ Angular frequency for case $B$.
$(D)$ Angular frequency for case $A < $ Angular frequency for case $B$.
$(A)$ the speed of the particle when it returns to its equilibrium position is $u_0$.
$(B)$ the time at which the particle passes through the equilibrium position for the first time is $t=\pi \sqrt{\frac{ m }{ k }}$.
$(C)$ the time at which the maximum compression of the spring occurs is $t =\frac{4 \pi}{3} \sqrt{\frac{ m }{ k }}$.
$(D)$ the time at which the particle passes througout the equilibrium position for the second time is $t=\frac{5 \pi}{3} \sqrt{\frac{ m }{ k }}$.