Orbital Angular Momentum as Generator for Circular Translations

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SUMMARY

The discussion focuses on the interpretation of orbital angular momentum as a generator for circular translations, specifically referencing Binney's textbook. Participants clarify that the notation ##\vec{\alpha} = \alpha \hat{n}## defines the angle of rotation and its direction, where ##\hat{n}## is the unit normal to the plane of rotation. The confusion arises from understanding the relationship between the angle of rotation, the position vector ##\vec{x}##, and the unit normal vector. The discussion emphasizes that ##\vec{\alpha}## lies along the axis of rotation, which is crucial for compactly expressing the rotation operator ##U##.

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  • Understanding of angular momentum concepts in physics
  • Familiarity with vector notation and operations
  • Knowledge of rotation matrices and their applications
  • Basic grasp of the definitions used in Binney's "Galactic Dynamics"
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  • Study the derivation of the rotation operator ##U## in quantum mechanics
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Homework Statement



Taken from Binney's Text, pg 143.

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Homework Equations





The Attempt at a Solution



From equation (7.36): we see that ##\delta a## is in the direction of the angle rotated, ##\vec{x}## is the position vector, and ##\vec{n}## is the unit normal to the plane of rotation.

51dctx.png


But at the last line of (7.37), we see that ##\vec{\alpha} = \alpha \vec{n}##. Why is the angle rotated now the same direction as the unit normal to the plane?
 
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I'm not sure if I'm understanding your question. But, I think it's just a matter of definition. The symbol ##\vec{\alpha}## is defined to be ##\alpha \hat{n}##. Note how Binney uses the definition symbol (or equivalence symbol) \equiv. This definition allows the rotation operator ##U## to be written more compactly. An angle of rotation has a certain magnitude about a certain axis. In this case ##\alpha## is the angle of rotation and ##\hat{n}## is the direction of the axis of rotation. The notation ##\vec{\alpha} = \alpha \hat{n}## is just a way to express that.
 
TSny said:
I'm not sure if I'm understanding your question. But, I think it's just a matter of definition. The symbol ##\vec{\alpha}## is defined to be ##\alpha \hat{n}##. Note how Binney uses the definition symbol (or equivalence symbol) \equiv. This definition allows the rotation operator ##U## to be written more compactly. An angle of rotation has a certain magnitude about a certain axis. In this case ##\alpha## is the angle of rotation and ##\hat{n}## is the direction of the axis of rotation. The notation ##\vec{\alpha} = \alpha \hat{n}## is just a way to express that.

If ##\alpha## is the angle of rotation and ##\hat{n}## is the direction vector of rotation, then wouldn't ##\delta a = \delta \alpha## x ##x## be into the plane, perpendicular to the plane of rotation?
 
##\hat{n}## is a unit vector perpendicular to the plane of rotation. It points along the axis of rotation. So, ##\hat{n} \times \vec{x}## lies in the plane of rotation.

Since ##\vec{\alpha} = \alpha \hat{n}##, ##\vec{\alpha}## also lies along the axis of rotation (perpendicular to the plane of rotation). For example, a rotation in the x-y plane of ##\pi## radians could be written ##\vec{\alpha} = \pi \hat{z}##
 
TSny said:
For example, a rotation in the x-y plane of ##\pi## radians could be written ##\vec{\alpha} = \pi \hat{z}##

That doesn't make sense at all..Usually ##\vec{\alpha}## is the direction vector in which the system moves - I would say it's more like ##\alpha_x \vec{i} + \alpha_y \vec{j}##
 
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