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A particle of mass \( m_{0} \), travelling at speed \( v_{0} \), strikes a stationary particle of mass \( 2 m_{0} \). As a result the
\( \mathrm{P} \) particle of mass \( m_{0} \) is deflected through \( 45^{\circ} \) and has

W. a final speed of \( \frac{v_{0}}{\sqrt{2}} \). Then the speed of the particle of mass \( 2 m_{0} \) after this collision is
(1) \( \frac{v_{0}}{2} \)
(2) \( \frac{v_{0}}{2 \sqrt{2}} \)
(3) \( \sqrt{2} v_{0} \)
(4) \( \frac{v_{0}}{\sqrt{2}} \)
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