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Hermann Minkowski (1864–1909) found that the theory of special relativity could be best understood as a four-dimensional space, since known as the Minkowski spacetime.. In physics, Minkowski space (or Minkowski spacetime) (/ m ɪ ŋ ˈ k ɔː f s k i,-ˈ k ɒ f-/ [1]) is the main mathematical description of spacetime in the absence of gravitation.
By 1908 Minkowski realized that the special theory of relativity, introduced by his former student Albert Einstein in 1905 and based on the previous work of Lorentz and Poincaré, could best be understood in a four-dimensional space, since known as the "Minkowski spacetime", in which time and space are not separated entities but intermingled in ...
The very first sentence of Minkowski space says "In physics, Minkowski space (or Minkowski spacetime) is the main mathematical description of spacetime in the absence of gravitation", and later in the lead "Minkowski space is closely associated with Einstein's theories of special relativity and general relativity and is the most common ...
1907-8 – Hermann Minkowski introduces the Minkowski spacetime and the notion of tensors to relativity. His paper was published posthumously. [45] [46] [47] 1909 – Max Born proposes his notion of rigidity. [48] [49] 1909 – Paul Ehrenfest states the Ehrenfest paradox. [50] [51]
Minkowski space is named for the German mathematician Hermann Minkowski, who around 1907 realized that the theory of special relativity (previously developed by Poincaré and Einstein) could be elegantly described using a four-dimensional spacetime, which combines the dimension of time with the three dimensions of space.
Hermann Minkowski. Poincaré's attempt of a four-dimensional reformulation of the new mechanics was not continued by himself, [54] so it was Hermann Minkowski (1907), who worked out the consequences of that notion (other contributions were made by Roberto Marcolongo (1906) and Richard Hargreaves (1908) [88]).
At the same time, he accepts that both the old model of Abraham (1902) and the later model of Bucherer & Langevin (1904) are consistent with the data. 1907 – Max Von Laue describes how the relativistic velocity-addition formula recreates the Fresnel drag coefficients. 1908 – Hermann Minkowski publishes his spacetime formalism of special ...
Thus, the separation into "true" and "local" times of Lorentz and Poincaré vanishes – all times are equally valid and therefore the relativity of length and time is a natural consequence. [9] [10] [11] In 1908, Hermann Minkowski introduced the concept of a world line of a particle [12] in his model of the cosmos called Minkowski space.