engleski

Relativistic contraction and related effects in noninertial frames

Although there is no relative motion among different points on a rotating disk, each point belongs to a different noninertial frame. This fact, not recognized in previous approaches to the Ehrenfest paradox and related problems, is exploited to give a correct treatment of a rotating ring and a rotating disk. Tensile stresses are recovered, but, contrary to the prediction of the standard approach, it is found that an observer on the rim of the disk will see equal lengths of other differently moving objects as an inertial observer whose instantaneous position and velocity are equal to that of the observer on the rim. The rate of clocks at various positions, as seen by various observers, is also discussed. Some results are generalized for observers arbitrarily moving in hat or curved spacetime. The generally accepted formula for the space line element in a non-time-orthogonal frame is found inappropriate in some cases. The use of Fermi coordinates leads to the result that for any observer the velocity of light is isotropic and is equal to c, providing that it is measured by propagating a light beam in a small neighborhood of the observer.

Ehrenfest paradox; relativistic contraction; non-time-orthogonal frame

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