Yarman, Nuh TolgaKholmetskii, Alexander L.Missevitch, Oleg V.Yarman, TolgaEnerji Sistemleri Mühendisliği / Energy Systems Engineering2024-05-252024-05-25201430008-42041208-604510.1139/cjp-2014-01402-s2.0-84909619266https://doi.org/10.1139/cjp-2014-0140https://hdl.handle.net/20.500.14517/753Yarman, Tolga/0000-0003-3209-2264We show that in the derivation of the frequency of Thomas precession, the fact of implementation of rotation-free Lorentz transformations between a laboratory frame, K-L, and Lorentz frames K(t) co-moving with a particle with spin at any time moments, t, has principal importance. Choosing for the observation of the particle's motion any other inertial frame, K, related with K-L by the rotation-free transformation, we have to realize that the transformations between K and K(t) at any t are no longer rotation-free. This way we provide a resolution of the known paradox by Bacry (H. Bacry. Nuovo Cimento, 26, 1164 (1962)) and suggest a reinterpretation of the Thomas precession, which is further discussed.eninfo:eu-repo/semantics/closedAccess[No Keyword Available]ArticleQ4Q3921113801386WOS:000344602200014