Angular Momentum points in WHAT direction?

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Discussion Overview

The discussion centers around the direction of angular momentum, particularly in the context of a rotating disk and the application of the right-hand rule. Participants explore the conceptual and mathematical underpinnings of angular momentum, including its representation and the implications of its directionality.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants express confusion about how the angular momentum vector can point perpendicular to a rotating disk, questioning the applicability of the right-hand rule in this context.
  • One participant explains that angular momentum is derived from the cross product of the position vector and linear momentum, suggesting that the resultant vector points in the z-direction when considering motion in the x-y plane.
  • Another participant emphasizes that the right-hand rule helps describe the direction of the disk's spin, proposing that the angular momentum vector must point in a direction that maintains circular symmetry.
  • A later reply introduces the concept of angular momentum as a bivector, discussing its dual representation and how it relates to the normal vector of a surface, while also noting the accessibility of understanding angular momentum without advanced mathematical concepts.

Areas of Agreement / Disagreement

Participants generally agree that the right-hand rule is relevant for determining the direction of angular momentum, but there remains confusion and differing interpretations regarding its application and the underlying concepts. The discussion does not reach a consensus on the best way to conceptualize angular momentum in this context.

Contextual Notes

Participants highlight various assumptions about the nature of angular momentum and its representation, including the dependence on the choice of coordinate system and the mathematical framework used to describe it. Some limitations in understanding arise from the complexity of the concepts involved.

Rockazella
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Angular Momentum points in WHAT direction?!?

I just don't get this whole right hand rule thing. If you have a rotating disk, how the heck can its momentum vector product point perpendicular to the disk?! There is absolutely no motion perpendicular to the disk.

I may never understand this one, but would anyone mind atleast trying to explain?
 
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Because I'm about to fall asleep at my desk, am going to do the very quick and dirty answer. You have thusly been warned.

Angular momentum is the cross product of the position vector r and the linear momentum p. If you go do the vector algebra, you'll see that the resultant vector points in the z-direction (if you're dealing with a body moving in the x-y plane), direction dependent on just what direction you're moving in said x-y plane. So, next time you want to pull out your hair thinking about the right hand rule and how it just seems so arbitrary, take solace in that you can do nicely and neatly via the linear algebra.
 


Originally posted by Rockazella
I just don't get this whole right hand rule thing. If you have a rotating disk, how the heck can its momentum vector product point perpendicular to the disk?! There is absolutely no motion perpendicular to the disk.

I may never understand this one, but would anyone mind atleast trying to explain?

I think the right hand rule used here is to keep track of the direction the disk is spinning. It's not moving in the x and y direction so how else would you describe it's motion?
 
If we rotate the disk 180 degrees, only the vector which passes through the center and is perpendicular to the disk will point in the same direction.
This vector is expressed in Nm, which is not a force, but what we call a moment.
 
I just don't get this whole right hand rule thing. If you have a rotating disk, how the heck can its momentum vector product point perpendicular to the disk?! There is absolutely no motion perpendicular to the disk.

Why wouldn't it!

Like the others said, if a disk is spinning in the x-y plane, there's no motion in the x or y direction either. Which way would you have the vector point?

The only thing that makes sense is to have the vector point in some direction with circular symmetry. Why? Because if we rotate in the x-y plane a disk spinning in the x-y plane, the result is a disk spinning in the x-y plane, and the same vector should represent both situations. The only choice is to have a vector that points along the z axis!


A more thorough answer is that angular momentum is really a bivector. An ordinary vector is, heuristically, a line element that points in a 1 dimensional direction. A bivector is a plane element that points in a 2 dimensional direction. The angular momentum of the aforementioned disk should really be written as a real multiple of i^j where ^ means wedge product. (it "pastes" lower dimensional vectors together to form higher dimensional vectors; here it combines a vector pointing along x with a vector pointing along y to form a bivector pointing along the x-y plane)


However, any geometrical object has a dual representation. Instead of a generalized vector that points in the direction the object is going, we can write a generalized vector that points in the direction the object is not going. In particular, in 3-D geometry, any surface can be completely characterized by its normal lines, e.g. the dual to a bivector is its normal vector.

So, we use this dual vector to represent angular momentum because it's just an ordinary vector, which means we don't have to take a course in Grassman Algebra or Tensor Analysis to understand what it is.

Hurkyl
 

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