Angular momentum in a collision

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In the discussion about angular momentum during a collision between two masses, it is established that angular momentum is conserved in the absence of external torque. The collision between mass B and mass A raises questions about whether external torque affects angular momentum conservation, particularly when considering different reference points. The calculations suggest that if angular momentum is conserved, the speed of mass A would need to be 6 m/s, but this leads to inconsistencies with kinetic energy. The conversation emphasizes the importance of defining the system boundaries and reference points for accurate angular momentum calculations. Ultimately, it concludes that while angular momentum may appear to change based on the chosen reference, it remains conserved when considering the system as a whole.
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Suppose a point mass B (m = 2 Kg) is rotating on a massless string (r = 2m) at v = 3m/s. Then KE = 9 J, p = 6 Kg m/s and L = p * r = 12 Nm (left in the sketch)
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Suppose B collides with A (m=2) the bob of a pendulum on a massless rod r = 1m. Is L conserved? It seems that there is no external torque.

If L is conserved then the speed of A must be 12 /( 1 * 2) = 6 m/s but in this case KE is 36 J, that is 4 times greater. If E is to stay the same, as it seems obvious, v must remain 3 m/s but angular momentum will then be L = 6 * 1 = 6 Nm, that is half the original 12 Nm.

- 1) Is L conserved or there has been an external torque?
- 2) If we want to use the general formula L = I / ω , L = 12, ω = v / C = 3/ 4π → I = 12*4π/3 = 48 π/ 3 is this correct?

Thanks for your help
 
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Where is the reference point about which the angular momentum of B is reckoned?
Where is the reference point about which the angular momentum of A is reckoned?
What is the sign of the angular momentum of B before the collision?
What is the sign of the angular momentum of A after the collision?

In the absence of an external torque, angular momentum with respect to a particular reference point is conserved. But if you change reference points, you will (if total linear momentum is non-zero) change angular momentum.
 
bobie said:
Is L conserved?
Around the origin of the massless string: If the two circles touch at the interaction point so there is no momentum transfer along the 1m rod, yes.

bobie said:
If L is conserved then the speed of A must be 12 /( 1 * 2) = 6 m/s
You have to be consistent with the point where you calculate your angular momentum.
 
So L remains 12 wrt to F and becomes 6 wrt to the new axis of rotation .
Can you reply also to the second question, please
 
Yes. The angular momentum wrt the new axis of rotation was 6 immediately prior to the collision and remains so afterward.

##\omega = \frac{v}{r}## The circumference, C, does not enter in.
 
jbriggs444 said:
Yes. The angular momentum wrt the new axis of rotation was 6 immediately prior to the collision and remains so afterward.
.
But what is the angular momentum of A with reference to F when it is rotating? L will not stay 12, it will always change from 12 to 24 Nm, all the time.

Secondly, doesn't A exert an external torque on B when they collide?
 
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bobie said:
But what is the angular momentum of A with reference to F when it is rotating? L will not stay 12, it will always change from 12 to 24 Nm, all the time.
Indeed, it will not remain 12. It will vary due to the external torque corresponding to the external centripetal force applied by the pendulum's axis on the bob, A.
Secondly, doesn't A exert an external torque on B when they collide?
That depends on where you draw the boundaries of the system of interest. If you consider the system to consist of B alone then yes, it is an external torque.

If you consider the system to consist of A and B together then it is part of an internal torque pair.
 
bobie said:
- 1) Is L conserved or there has been an external torque?
I am assuming that two of your unspoken assumptions are an elastic collision and frictionless passive bearings. Can you please confirm?

As was mentioned before, you have to choose where you measure angular momentum relative to. However, anywhere you choose you will have an external torque on the system. Angular momentum is not conserved.
 
DaleSpam said:
I am assuming that two of your unspoken assumptions are an elastic collision and frictionless passive bearings. Can you please confirm?

As was mentioned before, you have to choose where you measure angular momentum relative to. However, anywhere you choose you will have an external torque on the system. Angular momentum is not conserved.
Yes , elastic, frictionless. If we consider the system A,B, how do you describe conservation ov L? does the centripetal force of the rod exert a torque? when a skater pulls in her arms in the normal direction there is an (internal) torque? does L (A) vary from 12 to 24 because of the rod?
 
  • #10
Taking the system of interest to be A and B together then at the moment of the collision there are three interactions. There is the collision itself. There is the pull of the string on B and there is the pull or push of the pendulum rod on A.

The pull of the string on B is in the same direction as the displacement of A from F. It can exert no torque. The pull or push of the rod on B is in the same direction as the displacement of B from F. Further, the rod is massless and is on frictionless bearings. It can exert no torque. The collision itself is an internal interaction. It cannot change the total angular momentum of the system. Conservation of angular momentum applies. The total angular momentum of {A,B} about F will be the same before and after the collision.

The angular momentum is 12 just prior to the collision. It remains 12 just after the collision.

If ball B comes to rest after the collision (as it must to conserve energy in an elastic collision), it will have zero angular momentum. We can simplify the problem by shrinking the system of interest to consider A alone.

There is one interaction while A moves in a circular arc at the end of the pendulum rod. That is the external force of the pendulum rod on A. This force will be centripetal (i.e. toward the center of A's circular arc) and non-zero. It will have a varying component perpendicular to the displacement of A from F. At all but two points in the arc, this perpendicular component will be non-zero. That means that at almost all times it exerts a varying, non-zero torque on A about F. The angular momentum of A about F will vary over time due to this external torque.

When a skater pulls in her arms the third-law partners in the force pair (the arms on the body and the body on the arms) add to a net of zero. The change in angular momentum due to the pair is zero. In the absence of any other external torques, angular momentum will be conserved. Any change in her moment of inertia must be accompanied by a change in her angular velocity.
 
  • #11
Bobie, you are starting to go off in every different direction again. There are a bunch of good answers already in this thread, and you need to understand them before you raise any new issues.

So I've closed this thread. I will reopen it after you have sent me by PM a satisfactory answer to the following questions:
1) what is the total angular momentum of the system around the point F, before the collision?
2) what is the total angular momentum of the system around the pivot of the pendulum, before the collision?
3) what is the total angular momentum of the system around the point at which the collision happens, before the collision?
 

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