Resumen
A new conservation theorem is derived. The conserved quantity is constructed in terms of a symmetry transformation vector of the equations of motion only, without using either Lagrangian or Hamiltonian structures (which may even fail to exist for the equations at hand). One example and implications of the theorem on the structure of point symmetry transformations are presented.
Idioma original | Inglés |
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Número de artículo | 002 |
Páginas (desde-hasta) | L291-L295 |
Publicación | Journal of Physics A: General Physics |
Volumen | 25 |
N.º | 7 |
DOI | |
Estado | Publicada - 1992 |