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Special Relativity

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Part of the book series: Undergraduate Lecture Notes in Physics ((ULNP))

Abstract

Much of our presentation here will be an abbreviation of the treatment provided in the text The Classical Theory of Fields [[45], pp. 273–306]. Because of the importance that must be attached to an understanding of the basis of special relativity, which Einstein called der Schritt (the step) [[89], p. 163], we have elected not to simply summarize the results.

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Notes

  1. 1.

    The terminology Einstein used was clock. We have used timepiece because the clock with hands is becoming less common.

  2. 2.

    If this time of transit were not the same synchronization would not be possible and time would lose its meaning for points that are not in our immediate neighborhood.

  3. 3.

    From the German Gedankenexperiment. In a thought experiment it must be possible to construct the required apparatus and to perform all the measurements. A thought experiment is not fanciful.

  4. 4.

    The standard term is “observer” for the German Beobachter. The use of person seems less awkward here.

    With modern timepieces a single person can gather the data.

  5. 5.

    Hermann Minkowski was a German mathematician of Lithuanian Jewish descent. He was one of Einstein’s professors at the Eidgenössische Polytechnikum in Zürich.

  6. 6.

    The designation 4-vector is that used by Jackson. We choose it here as well.

  7. 7.

    Separate inertial frames must contain (material) measuring instruments, i.e. rods and timepieces.

  8. 8.

    The geometrical definition of a cone includes both \(x^{\text {0}}>0\) and \(x^{ \text {0}}<0\).

  9. 9.

    Here, as in our discussion of electrodynamics, we use Q rather than the traditional q to designate electrical charge. In this text q is reserved for the generalized coordinates.

  10. 10.

    The terms in (8.68) are all simply numbers and commute.

  11. 11.

    We note that CM designates center of mass in nonrelativistic (Newtonian) mechanics. The designation here as center of momentum is standard.

  12. 12.

    In Newtonian, 3 dimensional space this would mean perpendicular.

  13. 13.

    Of course this was already clear from the fact that a non-electromagnetic force must hold the nucleus together.

  14. 14.

    We can verify this result by partial differentiation.

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Correspondence to Carl S. Helrich .

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Helrich, C.S. (2017). Special Relativity. In: Analytical Mechanics. Undergraduate Lecture Notes in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-44491-8_8

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