Lorentz Transformation and time dilatation
<p>We consider two inertial frames S and and suppose that frame moves, for simplicity, in a single direction: the X -direction of frame S with a constant velocity v as measured in frame S.</p><p>Using homogeneity of space and time we derive a modified Lorentz Transformation (LT)...
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Annals of Mathematics and Physics - Peertechz Publications,
2024-01-10.
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LEADER | 00000 am a22000003u 4500 | ||
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001 | peertech__10_17352_amp_000104 | ||
042 | |a dc | ||
100 | 1 | 0 | |a Miodrag Mateljević |e author |
245 | 0 | 0 | |a Lorentz Transformation and time dilatation |
260 | |b Annals of Mathematics and Physics - Peertechz Publications, |c 2024-01-10. | ||
520 | |a <p>We consider two inertial frames S and and suppose that frame moves, for simplicity, in a single direction: the X -direction of frame S with a constant velocity v as measured in frame S.</p><p>Using homogeneity of space and time we derive a modified Lorentz Transformation (LT) between two inertial reference frames without using the second postulate of Einstein, i.e., we do not assume the invariant speed of light (in vacuum) under LT.</p><p>Roughly speaking we suppose: (H) Any clock which is at rest in its frame measures a small increment of time by some factor s=s(v). As a corollary of relativity theory (H) holds with Lorentz factor 1/γ. For s=1 we get the Galilean transformation of Newtonian physics, which assumes an absolute space and time. We also consider the relation between absolute space and Special Relativity Theory, thereafter STR.</p><p>It seems here that we need a physical explanation for (H). </p><p>We introduce Postulate 3. The two-way speed of light in and -directions are c and outline derivation of (LT) in this setting. Note that Postulate 3 is a weaker assumption than Einstein's second postulate. </p> | ||
540 | |a Copyright © Miodrag Mateljević et al. | ||
546 | |a en | ||
655 | 7 | |a Research Article |2 local | |
856 | 4 | 1 | |u https://doi.org/10.17352/amp.000104 |z Connect to this object online. |