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Almost-dispersionless pulse transport in long quasiuniform spring-mass chains: A different kind of Newton's cradle

Ruggero Vaia*

  • Istituto dei Sistemi Complessi, Consiglio Nazionale delle Ricerche, I-50019 Sesto Fiorentino, Italy and Istituto Nazionale di Fisica Nucleare, Sezione di Firenze, I-50019 Sesto Fiorentino, Italy

  • *ruggero.vaia@isc.cnr.it

Phys. Rev. E 97, 043001 – Published 23 April, 2018

DOI: https://doi.org/10.1103/PhysRevE.97.043001

Abstract

Almost-dispersionless pulse transfer between the extremal masses of a uniform harmonic spring-mass chain of arbitrary length can be induced by suitably modifying two masses and their spring's elastic constant at both extrema of the chain. It is shown that a deviation (or a pulse) imposed to the first mass gives rise to a wave packet that, after a time of the order of the chain length, almost perfectly reproduces the same deviation (pulse) at the opposite end, with an amplitude loss that is as small as 1.3% in the infinite-length limit; such a dynamics can continue back and forth again for several times before dispersion cleared the effect. The underlying coherence mechanism is that the initial condition excites a bunch of normal modes with almost equal frequency spacing. This constitutes a possible mechanism for efficient energy transfer, e.g., in nanofabricated structures.

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References (19)

  1. F. Hermann and M. Seitz, Am. J. Phys. 50, 977 (1982).
  2. S. Hutzler, G. Delaney, D. Weaire, and F. MacLeod, Am. J. Phys. 72, 1508 (2004).
  3. P. Glendinning, Phys. Rev. E 84, 067201 (2011).
  4. A. Rosas and K. Lindenberg, Phys. Rev. E 69, 016615 (2004).
  5. S. Flach and C. R. Willis, Phys. Rep. 295, 181 (1998).
  6. A. Sarmiento, R. Reigada, A. H. Romero, and K. Lindenberg, Phys. Rev. E 60, 5317 (1999).
  7. M. Ramm, T. Pruttivarasin, and H. Häffner, New J. Phys. 16, 063062 (2014).
  8. T. J. G. Apollaro, L. Banchi, A. Cuccoli, R. Vaia, and P. Verrucchi, Phys. Rev. A 85, 052319 (2012).
  9. L. Banchi and R. Vaia, J. Math. Phys. 54, 043501 (2013).
  10. A. Cantoni and P. Butler, Linear Algebra Appl. 13, 275 (1976).
  11. The frequencies (13) are in increasing order.
  12. F. Hermann and P. Schmälzle, Am. J. Phys. 49, 761 (1981).
  13. P0 has to be halved, but for simplicity of notation this is understood in the text: see the last paragraph of Appendix pp3.
  14. H. B. Dwight, Tables of Integrals and Other Mathematical Data, 4th ed. (MacMillan, New York, 1961).
  15. L. Banchi, T. J. G. Apollaro, A. Cuccoli, R. Vaia, and P. Verrucchi, New J. Phys. 13, 123006 (2011).
  16. D. G. Cahill, W. K. Ford, K. E. Goodson, G. D. Mahan, A. Majumdar, H. J. Maris, R. Merlin, and S. R. Phillpot, J. Appl. Phys. 93, 793 (2003).
  17. P. M. Norris, N. Q. Le, and C. H. Baker, J. Heat Transfer 135, 061604 (2013).
  18. B. N. Parlett, The Symmetric Eigenvalue Problem (SIAM, Philadelphia, 1998).
  19. This expression of ψk is useful for numerical calculations, e.g., using the function atan2(y,x) whose range is in [π,π].

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