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The Relativity Principle

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Abstract

The principle of the indistinguishability of inertial systems, or the equivalence of all of them, stands at the beginning of physics when it became an exact science.

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Notes

  1. 1.

    Einstein uses the term ‘coordinate system’ instead of the term preferred in later years, that we also use, ‘reference system’ or ‘frame’.

  2. 2.

    The former spelling used by FitzGerald, Lorentz and Einstein was ‘ether’ .

  3. 3.

    In literature, it is conventionally called ‘reciprocity principle’. Since we will formulate in Sect. 3, a reciprocity theorem, that has nothing to do with this reciprocity principle, we use here the notion ‘elementary relativity’. Also Ignatowski (1910) used this term when he writes: ‘So it must apparently hold: \(q' = -q\), ...’. Furthermore, it has to be respected that the reciprocity principle is derived as consequence from the relativity principle, cp. Berzi, Gorini (1969), while our elementary relativity principle is independently only a synchronisation recipe.

  4. 4.

    That means that the orientation of axes is conserved, i.e. for \(v\longrightarrow 0\) the space and time axes of inertial systems should have the same direction.

  5. 5.

    From an arithmetic point of view, the entirety of transformations (63) represents a mathematical group, both for classical space-time with \(k = 1\), and for the relativistic case with \(k =1/\sqrt{1 - v^2/c^2}\), s. Chap. 3, Sect. 2 and Chap. 4, Sect. 4. In this way, the equivalence of inertial systems is secured.

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Correspondence to Helmut Günther .

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Günther, H., Müller, V. (2019). The Relativity Principle. In: The Special Theory of Relativity. Springer, Singapore. https://doi.org/10.1007/978-981-13-7783-9_2

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  • DOI: https://doi.org/10.1007/978-981-13-7783-9_2

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  • Print ISBN: 978-981-13-7782-2

  • Online ISBN: 978-981-13-7783-9

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