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Comment on Clebsch’s 1857 and 1859 papers on using Hamiltonian methods in hydrodynamics

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Abstract

The present paper is a companion of two translated articles by Alfred Clebsch, titled “On a general transformation of the hydrodynamical equations” and “On the integration of the hydrodynamical equations” (https://doi.org/10.1140/epjh/s13129-021-00015-8, https://doi.org/10.1140/epjh/s13129-021-00016-7). The originals were published in the “Journal für die reine and angewandte Mathematik” (1857 and 1859). Here we provide a detailed critical reading of these articles, which analyzes methods, and results of Clebsch. In the first place, we try to elucidate the algebraic calculus used by Clebsch in several parts of the two articles that we believe to be the most significant ones. We also provide some proofs that Clebsch did not find necessary to explain, in particular concerning the variational principles stated in his two articles and the use of the method of Jacobi’s Last Multiplier. When possible, we reformulate the original expressions by Clebsch in the language of vector analysis, which should be more familiar to the reader. The connections of the results and methods by Clebsch with his scientific context, in particular with the works of Carl Jacobi, are briefly discussed. We emphasize how the representations of the velocity vector field conceived by Clebsch in his two articles, allow for a variational formulation of hydrodynamics equations in the steady and unsteady case. In particular, we stress that what is nowadays known as the “Clebsch variables”, permit to give a canonical Hamiltonian formulation of the equations of fluid mechanics. We also list a number of further developments of the theory initiated by Clebsch, which had an impact on presently active areas of research, within such fields as hydrodynamics and plasma physics.

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Change history

  • 10 August 2021

    The article has been updated as of the addition of“(PEMAT)” in the affiliation of Gérard Grimberg

Notes

  1. Hankel (1861), Beltrami (1871, 1872, 1873, 1874, 1904), Basset (1888), Hicks (1882), Lamb (1895), Duhem (1901).

  2. Bateman (1929), Herivel (1954, 1955), Calkin (1963), Lin (1963), Bretherton (1970), Seliger and Whitham (1968).

  3. Merzbach (2018): 136, Clebsch (1854): 17–18.

  4. Clebsch (1854, 1856, 1857a).

  5. Jacobi (1846, 1851).

  6. Clebsch (1856, 1857a, 1857b, 1858a, 1858b, 1858c, 1859a, 1859b, 1861, 1862, 1863). For detailed biographical information on Clebsch, see Burau (1970–1980) and Various Authors (1873a, 1873b).

  7. Kummer (1847).

  8. Jacobi (1844): 251.

  9. Jacobi (1844): 222, 266, Jacobi (1845): 262, 266.

  10. Hamilton (1834, 1835), Jacobi (1837): 128–136, Jacobi (1862, 1866). For the genesis of Hamilton–Jacobi equations see Nakane and Fraser (2002).

  11. Clebsch (1861, 1862, 1863).

  12. Hawkins (2005, 2013), Clebsch (1861, 1862, 1863).

  13. Hawkins (2005): 395–396, Cartan (1899): 240.

  14. Cauchy (1815), Hankel (1861), Frisch and Villone (2014), Frisch et al. (2017).

  15. Lagrange (1760–1761): 462, where he derives Euler equations for the case of a barotropic fluid.

  16. Cayley (1845, 1847, 1851, 1857), Hesse (1855), Grassmann (1844), Riemann (1854).

  17. Euler (1757), Truesdell (1954b): XCI–C.

  18. Truesdell (1954a): 27.

  19. Pfaff (1814).

  20. Clebsch uses the index notation of Jacobi, \(a,\,a',\,a^{(2)},\ldots a^{(n-1)}\). Here we deviate slightly from the original notation by Clebsch and prefer to let the values of the index of the variables go from 1 to n.

  21. Jacobi (1844): 203.

  22. Basset (1888): 34–38.

  23. Euler (1757): 347.

  24. Hesse (1855): 248.

  25. For the two-dimensional case, see Lamb (1895): 263. For the Casimir invariant, see Morrison (1998), Holm et al. (1985).

  26. Helmholtz (1858), Frisch–Grimberg–Villone (2017).

  27. Jacobi (1844): 255–256, Jacobi (1846): 104, Jacobi (1866): 77–78.

  28. Jacobi (1866): 77.

  29. Hicks (1882): 59, Basset (1888): 30, Truesdell and Toupin (1960): 427.

  30. Jacobi (1890): 137–138, Jacobi (1890): 393, Lanczos (1970): 238, Landau and Lifshitz (1976): 148.

  31. See, for instance, Kuznetsov and Mikhailov (1980), Morrison (1998) and Gallavotti (2010).

  32. See, e.g. Morrison (1998) and Holm et al. (1985).

  33. Lin (1963).

  34. Kuznetsov and Mikhailov (1980).

  35. Falkovich and L’vov (1995), Zakharov et al. (1985); Zakharov and Kuznetsov (1997).

  36. Sahraoui et al. (2003).

  37. Rund (1977a, 1977b).

  38. Morrison (1998).

  39. Morrison (1982), Morrison and Greene (1980), Kuznetsov and Mikhailov (1980), Morrison and Hazeltine (1984), Morrison et al. (1984), Marsden and Weinstein (1983), Marsden et al. (1984), Cendra and Marsden (1987), Holm and Kupershmidt (1983), Zakharov (1989).

  40. Yoshida (2009).

  41. Grad and Rubin (1958), Mendes et al. (2005), Jackiw et al. (2000), Jackiw and Polychronakos (2000), Ghosh (2002), Deser et al. (2001), Balkovsky (1994).

  42. Scholle et al. (2020).

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Acknowledgements

GG and ET are grateful to Uriel Frisch, without whom the realization of this article would not have been possible. GG and ET are also thankful to the two Reviewers, who provided useful and constructive comments which helped improving the paper. GG wishes to thank the Observatoire de la Côte d’Azur and the Laboratoire J.-L. Lagrange for their hospitality and financial support.

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Correspondence to Emanuele Tassi.

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Grimberg, G., Tassi, E. Comment on Clebsch’s 1857 and 1859 papers on using Hamiltonian methods in hydrodynamics. EPJ H 46, 17 (2021). https://doi.org/10.1140/epjh/s13129-021-00014-9

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