Question #73658

A small projectile of mass m moves with speed v to the right. The projectiles strikes and sticks to the end of a stationary bar of mass M, legth L, pivoted about a frictionless axle through its centre. Derive an expression for the angular velocity of the system immediately after the collision
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Expert's answer

2018-02-18T08:30:07-0500

Answer on Question #73658, Physics / Mechanics | Relativity

Question. A small projectile of mass mm moves with speed vv to the right. The projectiles strikes and sticks to the end of a stationary bar of mass MM , length LL , pivoted about a frictionless axle through its centre. Derive an expression for the angular velocity of the system immediately after the collision.

Solution.



Using the law of the conservation of angular momentum we get


mvL2=Iω,\frac {m v L}{2} = I \omega ,


where II - moment of inertia of the system after interaction.


I=mL24+ML212.I = \frac {m L ^ {2}}{4} + \frac {M L ^ {2}}{1 2}.


Hence


ω=mvL2I=mvL2(mL24+ML212)=mvmL2+ML6=6mv3mL+ML=6mv(3m+M)L\omega = \frac {m v L}{2 I} = \frac {m v L}{2 \left(\frac {m L ^ {2}}{4} + \frac {M L ^ {2}}{1 2}\right)} = \frac {m v}{\frac {m L}{2} + \frac {M L}{6}} = \frac {6 m v}{3 m L + M L} = \frac {6 m v}{(3 m + M) L}


Answer. ω=6mv(3m+M)L\omega = \frac{6mv}{(3m + M)L} .

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