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I came across a question regarding linear momentum $L$ and it's conservation, however I tried and got confused. It reads: A $40kg$ girl stands on the very edge of a rotating disc of mass $50kg$ and radius $2 meters$. She then throws a rock of mass $5kg$ at a speed of $10m/s$ which causes the rock to rotate in a clockwise direction. What is the angular velocity of the disc after the rock is thrown?

My attempt was to find the angular velocity caused by the rock using $v = wr$. I am unsure of how exactly to take into consideration the inertia of the girl disc system or if this is even the right approach. Also, since the disc would be rotating in a clockwise direction after the throw, would the angular velocity be negative? Please offer assistance.

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  • $\begingroup$ If the rock was held by the girl then it already has rotation, The act of throwing did not "cause it to rotate". The act of throwing the rock did not change the angular momentum of the rock. $\endgroup$ Commented May 19, 2020 at 12:21
  • $\begingroup$ Usually, $L$ is the designation for angular momentum. Does the question needs editing? $\endgroup$ Commented Oct 5 at 2:10

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...causes the rock to rotate in a clockwise direction

I think that means the velocity vector of the rock is in a direction such as it were thrown out of a clockwise motion of the disc. In that case, the disc itself, along with the girl will rotate in an anti-clockwise direction.

The total angular momentum is $0$. The rocks angular momentum as it is thrown out of your hands is $mvr$, for mass and velocity of the stone and radius of the disc.

Divide the negative of this quantity with the moment of inertia of the girl + disc and you shall get your answer. The sign convention is pretty arbitrary. I would say you consider the anti-clockwise rotation as the one having positive angular velocity.

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I hope my interpretation is correct.

1) The girl/disc/rock system is initially at rest.

2) The girl throws the rock and it exits the girl/disc system, tangentially to the disc, at $10\frac{m}{s}$

3) The angular momentum of the rock equals $m*v*r=5*10*2$

4) The angular momentum of the whole system must be conserved at zero, so the girl/disc system must have an angular momentum that counters $5*10*2$.

The angular momentum of the girl/disc system will be:

$$H_{axis}=100=I_{disc}\omega_{disc} + I_{girl}\omega_{girl}$$

Are these enough hints?

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I came across a question regarding linear momentum $L$ and its conservation

The question is actually about conservation of angular momentum. If the rock is thrown to the right, it is considered to be rotating clockwise about the centre of rotation of the system.

Also, since the disc would be rotating in a clockwise direction after the throw, would the angular velocity be negative?

Since angular momentum is conserved, the disc would rotate in the opposite direction to the thrown rock. Since the initial angular momentum of the sytem was zero the final total angular momentum remains zero. This means the angular momentum of the girl plus the disk is equal to the negative of the rock's final angular momentum. We are free to choose which direction of rotation is considered positive but more often than not clockwise rotation is conventionally treated as negative rotation. If the final angular momentum of the rock is $-mvr$, the angular momentum of the girl and the disk combined must be equal to $mvr$. So we have:

$$I_{\text{girl}} \omega +I_{\text{disk}} \omega = m_{\text{rock}} v \ r \implies m_{\text{girl}} r^2 \omega + m_{\text{disk}} r^2 \omega = m_{\text{rock}} v \ r.$$

Now just solve the equation for $\omega$. The result for the angular velocity of the girl and the disk should be positive, and that implies anticlockwise rotation.

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