Angular Momentum: Conditions & Answers

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SUMMARY

The discussion centers on the application of the angular momentum formula L = I ω in classical mechanics. It is established that this formula is valid about any axis, provided the correct moment of inertia (I) for that axis is used. The moment of inertia is a tensor quantity, varying based on the axis of rotation, and is influenced by the mass distribution relative to that axis. The parallel axis theorem is also highlighted, which relates the moment of inertia about different axes.

PREREQUISITES
  • Understanding of angular momentum and its formula L = I ω
  • Familiarity with moment of inertia as a tensor quantity
  • Knowledge of the parallel axis theorem in classical mechanics
  • Basic concepts of rotational motion and mass distribution
NEXT STEPS
  • Study the parallel axis theorem in detail
  • Explore the concept of moment of inertia for various shapes and axes
  • Learn about the relationship between angular momentum and rotational dynamics
  • Investigate practical applications of angular momentum in real-world scenarios
USEFUL FOR

Students of classical mechanics, physics educators, and anyone seeking to deepen their understanding of angular momentum and rotational dynamics.

enippeas
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First of all, sorry for my poor english
I am studying classical mechanics and have a problem with angular momentum. I am looking many books but i can't find an exactly answer. Under what conditions can i apply L = I ω; So far i understand that i can apply this formula around either the cm or a fixed point. Is that correct; Is there any other point; Thanks
 
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That is the definition of angular momentum for an object.

You only need to choose which is the REFERENCE AXIS for the rotations considered, because the inertia momentum I is not simply a scalar quantity, but is more complicated than that. Technically it's a tensor. It means that the value of I is different depending on which directions you are looking at it.

As a help, notice the great similarity between L=Iw (angular momentum) and p=mv (momentum). They are indeed the same thing, except that the first is for rotations and the second for traslations.

However, while m (mass) is just one simple value that works whatever the direction of the movement, I is not as simple.

Hint: think of an object with a long shape, such a wooden pole. Trying to make it spin requires an easier effort if you'r spinning it around its own axis rather than trasversally. That is represented by the fact that I' (referring to the pole's axis) is smaller than I'' (referring to an axis perpendicular to the pole and crossing the pole's middle point). If you try to rotate the pole horizontally and by holding one extremity rather than the middle point, it's even more difficult: I''' (ref to an axis perpendicular to the pole but crossing one of the extremity) is even greater.

To get the same rotational speed, you need a bigger effort L when I is greater.

Conversely, with equal effort L you speed up more an object that has a small I.

I depends on how the object's mass is distributed, relative to the rotation axis. The closer the mass is located, or "lumped" around the axis, the smaller I and hence the "easier" the rotation. Typical example of this is the ballet dancers, who first spin themselves with arms extended, then they raise their arms above their head (this way, they move part of their body mass closer to the rotational axis) and get a faster rotation.
 
Welcome to PF!

enippeas said:
Under what conditions can i apply L = I ω; So far i understand that i can apply this formula around either the cm or a fixed point. Is that correct; Is there any other point; Thanks

Hi enippeas ! Welcome to PF! :smile:

L = I ω is valid about any axis.

(but not about a point)

But of course we must use the I for that axis, which will always be larger than the I for the parallel axis through the c.o.m. :smile:

From the PF Library:
The parallel axis theorem:

The Moment of Inertia of a body about an axis is

[tex]I = (I_C\,+\,md^2)[/tex]

where m is the mass, d is the distance from that axis to the centre of mass, and [itex]I_C[/itex] is the Moment of Inertia about the parallel axis through the centre of mass.

(oh, and it's "I have looked in many books, but I couldn't find an exact answer." :smile: )
 

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