Are Lx, Ly, Lz (the components of Angular Momentum)independent to each other?

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The discussion centers on the independence of the components of Angular Momentum (Lx, Ly, Lz) in Classical Mechanics. It references the Poisson bracket identity, suggesting that if true, the components are not independent. However, a counterargument highlights that in specific cases, such as planar motion, Lx and Ly can be zero while Lz remains variable, indicating a form of independence. The interpretation of the Poisson bracket is also debated, with examples provided to clarify its implications. Overall, the relationship between the components of Angular Momentum remains a nuanced topic in classical physics.
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In Classical Mechanics, are the three components of Angular Momentum L:

Lx, Ly, Lz

independent to each other?

It seems that there is an identity in Classical Mechanics (Sorry, I can hardly remember where I saw it):

[Li, Lj] = εijk Lk.

Note: [] is Poisson Bracket, εijk is Levi-Civita Tensor

If the identity is true, then the three components of Angular Momentum are not independent to each other.
 
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Angular momenta are independent of each other. Take the obvious case of planar motion in the xy-plane. Then Lx and Ly are zero, and Lz can be anything.
 
yicong, Of course you are misinterpreting the meaning of the Poisson bracket. Note for example in three dimensions with Cartesian coordinates xi, the Poisson bracket relationship [xi, xj] = 0 for i and j not equal.
 
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