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Why is it that only Canonical transformations preserve the Hamilton's equations? Or what makes non-canonical transformations not preserve the Hamilton's equations?
Canonical transformations are defined by their ability to preserve Hamilton's equations in classical mechanics. This preservation is crucial because it ensures that the physical laws governing a system remain invariant under the transformation. Non-canonical transformations fail to maintain this invariance, leading to discrepancies in the equations of motion. Therefore, any transformation of coordinates that successfully preserves Hamilton's equations qualifies as a canonical transformation.
PREREQUISITESPhysicists, students of classical mechanics, and anyone interested in advanced topics in Hamiltonian dynamics.