Angular speed of rod shot by bullet

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Homework Help Overview

The discussion revolves around the angular speed of a rod that is shot by a bullet, involving concepts from conservation of momentum and energy in a rotational dynamics context.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore conservation of linear momentum and angular momentum, questioning the applicability of each in the context of the problem. Some express uncertainty about the calculations and the assumptions made regarding energy conservation.

Discussion Status

There is an ongoing exploration of different conservation principles, with some participants suggesting that angular momentum is the key focus while others express concerns about the implications of energy conservation. Multiple interpretations of the problem's conditions are being discussed.

Contextual Notes

Participants note that the problem may be overspecified, with various parameters provided that could lead to different calculations of energy lost or final velocities. The conditions regarding the distance from the pivot and energy conservation are highlighted as potentially confusing.

songoku
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Homework Statement
A rod with mass ##M## and length ##L## meter is pivoted at its center and put in vertical position, then a bullet of mass ##m## with initial speed ##u## is directed at a point ##x## meter from the top of the rod (##x## < ##0.5~L##) and the bullet will penetrates through the rod with final speed ##v##. Considering no energy lost and ignoring mass of rod lost when the bullet penetrates, find the angular speed of the rod
Relevant Equations
Conservation of linear momentum

Conservation of angular momentum

Circular motion
1) Applying conservation of linear momentum:

$$m.u = M.V + m.v$$

where ##V## is final linear speed of the rod

$$V=\frac{m.u-m.v}{M}$$2) Applying formula of circular motion:
$$V=\omega . r$$
$$\omega = \frac{\left(\frac{mu-mv}{M} \right)}{\frac{1}{2}L-x}$$

Is this correct?And can this be solved by using conservation of angular momentum? This is what I tried:

Applying conservation of angular momentum:
$$m.u.(\frac{1}{2}L-x)=m.v.(\frac{1}{2}L-x)+I \omega$$
$$(\frac{1}{2}L-x)(m.u-m.v)=\frac{1}{12} ML^2 \omega$$
$$\omega = \frac{(\frac{1}{2}L-x)(m.u-m.v)}{\frac{1}{12} ML^2}$$I am really not sure about my working. Thanks
 
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Linear momentum is not conserved because the pivot exerts an external force. Angular momentum about the pivot is conserved assuming that the bullet goes through very fast.
 
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Something tells me you have to use conservation of energy because the statements says no energy lost.
 
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Angular momentum of the whole system is conserved. Only that is needed.
Condition x≤L/2 is strange; condition about the energy is strange as well
$$xmu=J\omega+xmv$$
 
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Delta2 said:
Something tells me you have to use conservation of energy because the statements says no energy lost.
I agree that that's what the problem says but the issue is that if we conserve energy, the answer is different from what one gets from angular momentum conservation. Angular momentum is conserved because the torque due to gravity about the pivot can be ignored if the bullet goes through fast enough.

The energy conservation route gives a result that is independent of the distance ##x## from the pivot where the bullet strikes. So why is that distance given? Also, unless the energy transfer from bullet to rod is mediated by conservative forces, I don't see how energy can be conserved. Bullets going through rods usually do not exert conservative forces.

I favor ignoring the energy conservation clause and proceeding with angular momentum conservation.
 
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wrobel said:
Angular momentum of the whole system is conserved. Only that is needed.
Condition x≤L/2 is strange; condition about the energy is strange as well
$$xmu=J\omega+xmv$$
Shouldn't the distance measured from the pivot, so ##\frac{1}{2}L - x## since ##x## is measured from top of rod?

Thanks
 
kuruman said:
I agree that that's what the problem says but the issue is that if we conserve energy, the answer is different from what one gets from angular momentum conservation. Angular momentum is conserved because the torque due to gravity about the pivot can be ignored if the bullet goes through fast enough.

The energy conservation route gives a result that is independent of the distance ##x## from the pivot where the bullet strikes. So why is that distance given? Also, unless the energy transfer from bullet to rod is mediated by conservative forces, I don't see how energy can be conserved. Bullets going through rods usually do not exert conservative forces.

I favor ignoring the energy conservation clause and proceeding with angular momentum conservation.
Yes, the problem is overspecified. We are given u, v, m, M, x and L. From these we can calculate the energy lost.
Conversely, we can take energy as conserved and calculate v.
 
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songoku said:
Shouldn't the distance measured from the pivot, so ##\frac{1}{2}L - x## since ##x## is measured from top of rod?

Thanks
Yes, it should.
 
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haruspex said:
Yes, the problem is overspecified. We are given u, v, m, M, x and L. From these we can calculate the energy lost.
Conversely, we can take energy as conserved and calculate v.
Will the energy lost be: ##\frac1 2 mu^2 - \frac 1 2 mv^2 - \frac 1 2 J \omega^2## where ##J## is the moment of inertia of the rod?

Thanks
 
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songoku said:
Will the energy lost be: ##\frac1 2 mu^2 - \frac 1 2 mv^2 - \frac 1 2 J \omega^2## where ##J## is the moment of inertia of the rod?

Thanks
It would be that with ##\omega## being what you get using angular momentum conservation.
 
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  • #11
I wrote the formula for the following configuration

cvbc.png
 
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  • #12
Thank very much for all the help and explanation kuruman, Delta2, wrobel, haruspex
 

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