The bracket of two functions is the derivative of one along the Hamiltonian vector field of the other. The example is deliberately concrete; it is a test of the statement, not a substitute for it.
Start locally
A symplectic manifold \((M^{2n},\omega)\) has a closed nondegenerate two-form. A Hamiltonian \(H:M\to\mathbf R\) determines a vector field through contraction with \(\omega\).
The first display fixes the mathematical data. I label it \(\mathsf{data}\) mentally, while the next is the \(\mathsf{claim}\); the bridge between them is the displayed \(\Longrightarrow\), not an automatic implication.
Compute before generalising
This is the algebraic core of the note. Once this line is correct, the surrounding interpretation has something solid to refer to.
The global view
The abstraction earns its keep by explaining why the same computation reappears. The notation compresses repeated reasoning without erasing the hypothesis that licenses it.
Edge conditions
Symplectic geometry has no preferred notion of distance. Nondegeneracy of a two-form is not positive definiteness of a metric.
The result is compact enough to reuse without pretending that the caveat has disappeared. The worked line remains the quickest consistency check.