A summary of Lagrangian and Hamiltonian formalisms is given in tabular form.
| Lagrangian Formalism | Hamiltonian Formalism | |
| 1). Basic Variables | \( q_{k}, \dot{q}_{k}\) | \( q_{k}, p_{k}\) |
| 2). States | Rep by a point | Rep by a point |
| in configuration space | in phase space | |
| 3). EOM | Euler Lagrange | Hamilton's EOM |
| EOM | \( \dot{q}_{k} =\frac{\partial H}{\partial p_{k}}\) | |
| \( \frac{\partial L}{\partial {q}_{k}} - \frac{d}{dt} \left( \frac{\partial L}{\partial \dot{q}_{k}} \right) = 0\) | \( \dot{p}_{k} = - \frac{\partial H}{\partial q_{k}} \) | |
| 4). Action | Hamilton's and | Wiess acion |
| Principle | Wiess action | Principle in phase |
| Principle gives | space gives EOM | |
| Laws of motion | ||
| 5). System | Contained in | Described \ by |
| Specific information | Lagrangian | Hamiltonian |
| (Interactions) | ||
| 6). Full \ solution | Values of \(q_{k}, \dot{q}_{k}\) \ at | Values of \( q_{k}, p_{k}\) |
| requires | initial time | at initial time |
| 7). Conservation | Related to | Generators of |
| \ Laws | Symmetries of \(L\) | transformations have |
| in configuration | zero Poisson bracket | |
| space | with the Hamiltonian | |
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