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Momentum and angular momentum in relativistic classical particle mechanics

dc.contributor.authorJordan, T.F.
dc.contributor.authorShukre, C.S.
dc.date.accessioned2012-08-06T09:14:54Z
dc.date.available2012-08-06T09:14:54Z
dc.date.issued1972
dc.descriptionRestricted Access.en
dc.description.abstractFor a classical-mechanical system of any fixed number of particles it is observed that space-translation invariance and conservation of angular momentum imply conservation of momentum. For three particles it is shown, as previously for two, that Poincaré invariance implies that the total kinematic momentum cannot be a constant of motion unless the accelerations are zero. The equations involved make it appear most likely that this is true for any number of particles.en
dc.identifier.citationPhysical Review D, 1972, Vol.5, p799-801en
dc.identifier.issn1550-7998
dc.identifier.issn1550-2368(Online)
dc.identifier.urihttp://hdl.handle.net/2289/5194
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.relation.urihttp://adsabs.harvard.edu/abs/1972PhRvD...5..799Jen
dc.relation.urihttp://dx.doi.org/10.1103/PhysRevD.5.799en
dc.rights1972 American Physical Societyen
dc.titleMomentum and angular momentum in relativistic classical particle mechanicsen
dc.typeArticleen

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