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- Derivations_of_the_Lorentz_transformations abstract "In the fundamental branches of modern physics, namely general relativity and its widely applicable subset special relativity, as well as relativistic quantum mechanics and relativistic quantum field theory, the Lorentz transformation is the transformation rule under which all four vectors and tensors containing physical quantities transform according to in spacetime.The prime examples of such four vectors are the four position and four momentum of a particle, and for fields the electromagnetic tensor and stress–energy tensor. The fact that these objects transform according to the Lorentz transformation is what mathematically defines them as vectors and tensors, see tensor.Given the components of the four vectors or tensors in some frame, the "transformation rule" allows one to determine the altered components of the same four vectors or tensors in another frame, which could be boosted or accelerated, relative to the original frame. A "boost" should not be conflated with spatial translation, rather it's characterized by the relative velocity between frames. The transformation rule itself depends on the relative motion of the frames. In the simplest case of two inertial frames the relative velocity between enters the transformation rule. For rotating reference frames or general non-inertial reference frames, more parameters are needed, including the relative velocity (magnitude and direction), the rotation axis and angle turned through. There are many ways to derive the Lorentz transformations utilizing a variety of mathematical tools, spanning from elementary algebra and hyperbolic functions, to linear algebra and group theory.This article provides a few of the easier ones to follow in the context of special relativity, for the simplest case of a Lorentz boost in standard configuration, i.e. two inertial frames moving relative to each other at constant (uniform) relative velocity less than the speed of light, and using Cartesian coordinates so that the x and x′ axes are collinear.".
- Derivations_of_the_Lorentz_transformations thumbnail Lorentz_transforms_2.svg?width=300.
- Derivations_of_the_Lorentz_transformations wikiPageExternalLink 0107091.
- Derivations_of_the_Lorentz_transformations wikiPageID "39499535".
- Derivations_of_the_Lorentz_transformations wikiPageRevisionID "604777871".
- Derivations_of_the_Lorentz_transformations subject Category:General_relativity.
- Derivations_of_the_Lorentz_transformations subject Category:Quantum_mechanics.
- Derivations_of_the_Lorentz_transformations subject Category:Special_relativity.
- Derivations_of_the_Lorentz_transformations comment "In the fundamental branches of modern physics, namely general relativity and its widely applicable subset special relativity, as well as relativistic quantum mechanics and relativistic quantum field theory, the Lorentz transformation is the transformation rule under which all four vectors and tensors containing physical quantities transform according to in spacetime.The prime examples of such four vectors are the four position and four momentum of a particle, and for fields the electromagnetic tensor and stress–energy tensor. ".
- Derivations_of_the_Lorentz_transformations label "Derivations of the Lorentz transformations".
- Derivations_of_the_Lorentz_transformations sameAs m.0vpvk2c.
- Derivations_of_the_Lorentz_transformations sameAs Q15198210.
- Derivations_of_the_Lorentz_transformations sameAs Q15198210.
- Derivations_of_the_Lorentz_transformations wasDerivedFrom Derivations_of_the_Lorentz_transformations?oldid=604777871.
- Derivations_of_the_Lorentz_transformations depiction Lorentz_transforms_2.svg.
- Derivations_of_the_Lorentz_transformations isPrimaryTopicOf Derivations_of_the_Lorentz_transformations.
