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Canonical transformation
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=== Poisson and Lagrange brackets === The Poisson brackets are changed as follows: <math display="block">\{u, v\}_\eta = (\nabla_\eta u)^T J (\nabla_\eta v) = (M^T \nabla_\varepsilon u)^T J (M^T \nabla_\varepsilon v) = (\nabla_\varepsilon u)^T M J M^T (\nabla_\varepsilon v) = \lambda (\nabla_\varepsilon u)^T J (\nabla_\varepsilon v) = \lambda \{u, v\}_\varepsilon</math> whereas, the Lagrange brackets are changed as: <math display="block">[u, v]_\varepsilon = (\partial_u \varepsilon )^T \,J\, (\partial_v \varepsilon) = (M \, \partial_u \eta )^T \,J \, ( M \,\partial_v \eta) = (\partial_u \eta )^T\, M^TJ M\, (\partial_v \eta) = \lambda (\partial_u \eta )^T\, J\,(\partial_v \eta) = \lambda [u, v]_\eta</math> Hence, the Poisson bracket scales by the inverse of <math display="inline">\lambda </math> whereas the Lagrange bracket scales by a factor of <math display="inline">\lambda </math>.<ref>{{Harvnb|Giacaglia|1972|p=16}}-17</ref>
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