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Canonical coordinates
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==Generalized coordinates== In [[Lagrangian mechanics]], a different set of coordinates are used, called the [[generalized coordinates]]. These are commonly denoted as <math>\left(q^i, \dot{q}^i\right)</math> with <math>q^i</math> called the '''generalized position''' and <math>\dot{q}^i</math> the '''generalized velocity'''. When a [[symplectic vector field|Hamiltonian]] is defined on the cotangent bundle, then the generalized coordinates are related to the canonical coordinates by means of the [[Hamilton–Jacobi equation]]s.
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