A body of mass \( M \) moving at speed \( V_{0} \) collides elastically with a mass ‘\( m \)’ at rest. After the collision, the two masses move at angles \( \theta_{1} \) and \( \theta_{2} \) with respect to the initial direction of motion of the body of mass \( M \). The largest possible value of the ratio \( \dfrac{M}{m} \), for which the angles \( \theta_{1} \) and \( \theta_{2} \) will be equal, is: