A) \[\frac{2}{\sqrt{3}}v\]
B) \[\frac{v}{\sqrt{3}}\]
C) v
D) \[\sqrt{3}\,v\]
Correct Answer: A
Solution :
Let mass A moves with velocity v and collides in elastically with mass B, which is at rest. According to problem mass A moves in a perpendicular direction and let the mass B moves at angle q with the horizontal with velocity v. Initial horizontal momentum of system (before collision) = mv ....(i) Final horizontal momentum of system (after collision) \[~~=mVcos\theta \] ....(ii) From the conservation of horizontal linear momentum mv = mV cosq Þ v = V cosq ...(iii) Initial vertical momentum of system (before collision) is zero. Final vertical momentum of system \[\frac{mv}{\sqrt{3}}-mV\sin \theta \] From the conservation of vertical linear momentum \[\frac{mv}{\sqrt{3}}-mV\sin \theta =0\]Þ\[\frac{v}{\sqrt{3}}=V\sin \theta \] ...(iv) By solving (iii) and (iv) \[{{v}^{2}}+\frac{{{v}^{2}}}{3}={{V}^{2}}({{\sin }^{2}}\theta +{{\cos }^{2}}\theta )\] Þ \[\frac{4{{v}^{2}}}{3}={{V}^{2}}\] Þ \[V=\frac{2}{\sqrt{3}}v\].You need to login to perform this action.
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