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\(\newcommand{\PB}[1]{[#1]_\text{PB}}\) Show that the Poisson brackets of components of angular momentum \(\vec{L}\)
with the following quantities vanishes.
- \(\vec{r}\cdot\vec{p}\)
- \(\vec{r}\cdot\vec{L}\)
- \(\vec{L}\cdot\vec{p}\)
- \( \vec{L}^{\,2}\)
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4727:Diamond Point
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