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dc.contributor.authorMatvejev, Vadim
dc.contributor.authorMatvejev, Oleg
dc.contributor.authorGrøn, Øyvind
dc.date.accessioned2016-12-15T07:45:47Z
dc.date.accessioned2017-04-03T11:14:57Z
dc.date.available2016-12-15T07:45:47Z
dc.date.available2017-04-03T11:14:57Z
dc.date.issued2016-02
dc.identifier.citationAmerican Journal of Physics 2016, 84(6):419-425language
dc.identifier.issn0002-9505
dc.identifier.urihttps://hdl.handle.net/10642/4641
dc.description.abstractWe present an apparent paradox within the special theory of relativity, involving a trolley with relativistic velocity and its rolling wheels. Two solutions are given, both making clear the physical reality of the Lorentz contraction, and that the distance on the rails between each time a specific point on the rim touches the rail is not equal to 2 p R ,where R is the radius of the wheel, but 2 p R = ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi 1 R 2 X 2 = c 2 q ,where X is the angular velocity of the wheels. In one solution, the wheel radius is constant as the velocity of the trolley increases, and in the other the wheels contract in the radial direction. We also explain two surprising facts. First that the shape of a rolling wheel is elliptical in spite of the fact that the upper part of the wheel moves faster than the lower part, and thus is more Lorentz contracted, and second that a Lorentz contracted wheel with relativistic velocity rolls out a larger distance between two successive touches of a point of the wheel on the rails than the length of a circle with the same radius as the wheels.language
dc.language.isoenlanguage
dc.publisherAmerican Association of Physics Teacherslanguage
dc.titleA relativistic trolley paradoxlanguage
dc.typeJournal article
dc.typePeer reviewedlanguage
dc.typeJournal article
dc.date.updated2016-12-15T07:45:47Z
dc.description.versionpublishedVersionlanguage
dc.identifier.doihttp://doi.org/10.1119/1.4942168
dc.identifier.cristin1356670


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