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<rdf:Description rdf:about="https://catalogues.royalsociety.org:443/CalmView/record/catalog/PP/18/9" xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <dc:title>Paper, 'On instability of periodic motion' by William Thomson</dc:title>
  <dc:description>A printed proof of Thomson's paper. Thomson writes: 'Let ψ, φ, χ, ϑ be generalised coordinates of a system; and let A (ψ, φ, . . . . , ψ', φ', . . . . ) be the action in a path (2 above) from the configuration (ψ', φ',. . . .) to the configuration (ψ, φ, . . . .) with kinetic energy (E—V) with any given constant value for E, the total energy; V being the potential energy, of which the value is given for every possible configuration of the system.' Includes a postscript, dated 10 November 1891, in which Thomson discusses Henri Poincaré's 'Sur le problème des trois corps et les équations de la dynamique'.

Annotations in pencil and ink.

Subject: Physics / Mathematics

Received 12 November 1891. Read 26 November 1891.

A version of this paper was published in volume 50 of the Proceedings of the Royal Society as 'On instability of periodic motion'.</dc:description>
  <dc:date>1891</dc:date>
</rdf:Description>