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 three components of Angular Momentum (Lx, Ly, Lz) in Classical Mechanics. It is established that the Poisson bracket identity [Li, Lj] = εijk Lk indicates that these components are not independent of each other. The example of planar motion in the xy-plane illustrates that while Lx and Ly can be zero, Lz can vary, suggesting a dependency among the components. Misinterpretations of the Poisson bracket's implications are also addressed, emphasizing the need for clarity in understanding these relationships.

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yicong2011
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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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