Answer:
Option B
Explanation:
Let the other mass at this instant is at a distance of x from the centre O.
Applying law of conservation of angular momentum, we have
$I_{1}\omega_{1}=I_{2}\omega_{2}$
$\therefore$ $(MR^{2})(\omega)$
$= \left[MR^{2} +\frac{M}{8}\left(\frac{3}{5}R\right)^{2}+\frac{M}{8}x^{2}\right]\left(\frac{8}{9}\omega\right)$
Solving this equation , we get , $x=\frac{4}{5}R$
Note If we take identical situations with both point masses, then answer will be (c) .But in that case angular momentum is not conserved.