Angular Momentum for Man and Bullet

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SUMMARY

The discussion focuses on the conservation of angular momentum in a system involving a man standing on a massless rod and firing a bullet. The key conclusion is that since there is no external torque acting on the system, the angular momentum remains conserved. The angular momentum of the man after firing the bullet can be expressed as Mmanω(l/2)^2, while the bullet's contribution is given by mbVb sin(θ)/(Mman(l/2)). The confusion arises from the changing radial vector of the bullet, which must be accounted for in the calculations.

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Homework Statement


A man, mass M, stands on a massless rod which is free to rotate about its center in the horizontal plane. The man has a gun (massless) with one bullet, mass m. He shoots the bullet with velocity Vb, horizontally. Find the angular velocity of the man as a function of the angle θ which the bullet's velocity vector makes with the rod.

Homework Equations


Torque = r x F
L = r x mv
T = dL/dt

The Attempt at a Solution


There's no external torque acting on the system of the man and the bullet. Torque = 0 = dL/dt means that L is conserved. The system was at rest meaning Lint was 0. The angular momentum for the man is Mmanω(l/2)^2 post firing. Here's my problem, the bullet's radial vector is changing. r = < l/2 + Vbcos(θ)t, vbsin(theta)t>x<mbVbcosθ, mbVbsinθ>
The book gives the answer as mbvbsinθ/(mman(l/2))
Where did I go wrong?
 
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The angular momentum of something that has no external torques applied is conserved, so it is sufficient to consider the angular momentum of all parties concerned at a particular representative instant. The instant after the bullet is fired (t = 0+) seems like a reasonable choice...

You could, if you were so inclined, write the bullet's radius in the form of a vector function of time, r(t), and express its velocity as a vector, too. Then its angular momentum would be given by mb r(t) x v, which you'll probably find comes out as a constant value after slogging through the math.
 

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