
(d) Using conservation of linear momentum, we have
$mv_{0} = mv + 2mv$
Or $v = \frac{v_{0}}{3}$
Using conservation of energy, we have
$\frac{1}{2}mv_{0}^{2} = \frac{1}{2}kx_{0}^{2} + \frac{1}{2}(3m)v^{2}$
Where $x_{0}$=compression in the spring ,
$\therefore mv_{0}^{2} = kx_{0}^{2} + (3m)\ \frac{v_{0}^{2}}{9}$
Or $kx_{0}^{2} = \ mv_{0}^{2} - \frac{mv_{0}^{2}}{3}$
Or $kx_{0}^{2} = \frac{2mv_{0}^{2}}{3}$
$\therefore k = \frac{2mv_{0}^{2}}{3x_{0}^{2}}$