In 1837, Gustav Jacobi introduced Canonical Transformation in generalized coordinates and generalized momenta to simplify the Hamiltonian and make it easier to find solutions to Hamilton's equations. He described the relationships between variables as partial differential equations, which are generating functions that appear due to the Gauge Invariance of the Lagrangian.
Hamilton–Jacobi equation
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Seonglae ChoCreated
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2024 Jul 23 6:53Editor
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Seonglae ChoEdited
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2024 Jul 23 6:54Refs
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Three-body problem