Regular Optimal Control Problems with Quadratic Final Penalties
Hamilton’s canonical equations (HCEs) have played a central role in Mechanicsafter (i) their equivalence with the principle of least action, and (ii) the variationalcalculus leading to the Euler-Lagrange equation, were established and applied (see[1]). Also, since the foundational work of Pontryagin...
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| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2008 |
| País: | Argentina |
| Institución: | Consejo Nacional de Investigaciones Científicas y Técnicas |
| Repositorio: | CONICET Digital (CONICET) |
| Idioma: | inglés |
| OAI Identifier: | oai:ri.conicet.gov.ar:11336/18581 |
| Acceso en línea: | http://hdl.handle.net/11336/18581 |
| Access Level: | acceso abierto |
| Palabra clave: | Optimal Control Nonlinear Systems Boundary Problems https://purl.org/becyt/ford/2.4 https://purl.org/becyt/ford/2 |
| Sumario: | Hamilton’s canonical equations (HCEs) have played a central role in Mechanicsafter (i) their equivalence with the principle of least action, and (ii) the variationalcalculus leading to the Euler-Lagrange equation, were established and applied (see[1]). Also, since the foundational work of Pontryagin [22], HCEs have been atthe core of modern optimal control theory. When the problem concerning ann-dimensional control system and an additive cost objective is regular [19], i.e.when the Hamiltonian H(t, x, lambda, u) of the problem is smooth enough and can beuniquely optimized with respect to u at a control value u0(t, x, lambda) (depending onthe remaining variables), then HCEs appear as a set of 2n ordinary differentialequations whose solutions are optimal state-costate time trajectories. |
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