The Classical Theory of Fields¶
Landau, L. D., & Lifshitz, E. M. (1975). The Classical Theory of Fields. Pergamon Press.
Cited by¶
1 citation across 1 artifact.
Each citation links to the sentence it supports in the citing article.
Domain-specific¶
- Momentum
- Classical mechanics — linear (\(m\mathbf{v}\)) and angular (\(\mathbf{r}\times\mathbf{p}\)) momentum conserved under translational and rotational symmetry and exchanged in collisions and impulse. Special relativity — momentum as the spatial part of the four-momentum \((E/c, \mathbf{p})\), conserved in particle interactions under the larger Poincaré symmetry
This sourceLandau and Lifshitz's treatment of the four-momentum of a free particle and its conservation in interactions.
Supported in partVerified against the work's full text
“conservation of energy and [momentum], there is conservation of angular [momentum], that is, of the”
- Classical mechanics — linear (\(m\mathbf{v}\)) and angular (\(\mathbf{r}\times\mathbf{p}\)) momentum conserved under translational and rotational symmetry and exchanged in collisions and impulse. Special relativity — momentum as the spatial part of the four-momentum \((E/c, \mathbf{p})\), conserved in particle interactions under the larger Poincaré symmetry
Verification¶
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