A block of mass m moving with a velocity v hits a light spring of stiffness K attached rigidly to a stationary sledge of mass M. Neglecting friction between all contacting surfaces, the maximum compression of the spring is
The velocity of the combinational at the time of maximum compression of the spring = v = mv0M+m obtained by conserving the momentum of the system.
The Δ K.Esystem)=−[12 m v02 - 12 (M + m) v2]
By putting v = mv0M+m, we obtain ΔK.Esystem = Mmv022(M+m)
Δ P.Esystem = 12 k x2 where x = maximum compression of the spring.
⇒ (Δ PE + ΔKE)system = 0
⇒ 12 k x2 - Mmv022(M+m) = 0
⇒ x = [ √Mn(M+m)k ] v0