# Poisson Brackets And Angular Momentum Components

When Poisson Brackets are taught as part of an Analytical Mechanics courses, examples are commonly shown which anticipate analogue results in QM. One such example, which the the book I'm using ([1]) shows, is that since the components of the angular momentum vector $L$ obey the relation

$$\displaystyle [L_i,L_j] = \epsilon_{ijk}L_k \tag{1},$$

they obviously do not obey the canonical variable relations $[p_i,p_j] = 0$ and therefore no two components of $L$ can serve as canonical variables at the same time. It then goes on to show that $L^2$ commutes with $L_i$, so that this pair can be used as canonical variables. An analogue result is standard QM fare about commutation relations and observation.

I seem to have found a counter-example. If we write The hamiltonian for a free particle, by starting with the Lagrangian in spherical coordinates $(r,\theta,\phi)$, we end up with

$$\displaystyle H=\frac{{p_r}^2}{2 m}+\frac{{p_\theta}^2}{2 m r^2}+\frac{{p_\phi}^2}{2 m r^2 \sin ^2(\theta )}$$

with generalized momenta

$$\displaystyle p_r= m\dot{r},\quad p_\theta=m r^2 \dot{\theta},\quad p_\phi=m (r \sin (\theta))^2 \dot{\phi}$$

It's easy to see from the definition that $$p_\phi=L_z\quad\text{and} \quad p_\theta= L_x.$$ This looks like a counterexample. I did not arrive at this hamiltonian through a canonical transformation, but it is a "legal" hamiltonian and two of the canonical variables/momenta are two components of $L$, contradicting the claim above.

As an additional quandary, the book shows that Poisson Brackets are canonical invariants, i.e. preserved under canonical transformations, but when I calculated $[L_x,L_z]$ in Cartesian coordinates, I got the result $[L_x,L_z]-L_y$ as (1) suggests, and when I calculated $[L_x,L_z]$ in the phase space of spherical coordinates I got the result $[p_\theta,p_\phi]=0$ as I'd expect from a pair of canonical variables..

These results seem to contradict one another. What's the explanation?

[1] Hamill, Patrick. "Student's Guide to Lagrangians and Hamiltonians", p.130.

• Hint: The correct identification is $p_{\phi}=L_z$ and $p_{\theta}^2=\vec{L}^2-\frac{L_z^2}{\sin^2\theta}$. May 27, 2018 at 10:33

Thanks @Qmechanics, the hint was all it took.

The error in OP stems from miscalculating the angular momentum vector.

When motion is restricted to a plane perpendicular to one of the Cartesian coordinate axes (say $z$), the angular momentum vector has a non-zero component only in the direction perpendicular to the plane ($z$). Its magnitude is $L_z = m r^2 \dot{\theta}$.

When we move to 3d space, though, it is incorrect to calculate each component of $L$ individually, as if motion were restricted to one plane "at a time". Instead, you have to do the general calculation:

\begin{align*} \vec{r} &=(r \sin (\theta ) \cos (\varphi ),r \sin (\theta ) \sin (\varphi ),r \cos (\theta ) )\\ \dot{\vec{r}} &= ( -r \dot{\varphi } \sin (\theta ) \sin (\varphi )+\dot{\theta } r \cos (\theta ) \cos (\varphi )+\dot{r} \sin (\theta ) \cos (\varphi ), \\\quad&\dot{r} \sin (\theta ) \sin (\varphi )+r \dot{\varphi } \sin (\theta ) \cos (\varphi )+\dot{\theta } r \cos (\theta ) \sin (\varphi ), \\\quad &\dot{r} \cos (\theta )-\dot{\theta } r \sin (\theta ))\\ \vec{ L} &= r \times (m \dot{\vec{r}}) \end{align*} The result is a little hairy, but it shows that $L_x \ne m r^2 \dot{\theta}$ and therefore OP statement that $L_x = p_\theta$ is false.

Luckily, $L^2$ (a scalar) has a friendly form: $$\displaystyle L^2 =m^2 r^4 \left(\overset{.}{\varphi }^2 \sin ^2(\theta )+\overset{.}{\theta }^2\right)$$ So the identity pointed out by @Qmechanic is easy to prove:

$$(p_\theta)^2 = L^2 - \frac{L_z^2}{\sin^2(\theta)}$$

Therefore, in the Hamiltonian given in OP the two conjugate momenta are not components of $\vec{L}$ (only p_\phi is), so the commutation relations derived for components of $L$ is not violated. The two momenta $p_\theta,p_\phi$ are however canonical variables and therefore obey the canonical commutation relations: $$[p_\theta,p_\phi]=0$$ as they should.