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Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams

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Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams. / Landa, P. S.; McClintock, P. V. E.
In: Journal of Physics A: Mathematical and Theoretical, Vol. 44, No. 47, 475501, 25.11.2011, p. -.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Landa, PS & McClintock, PVE 2011, 'Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams', Journal of Physics A: Mathematical and Theoretical, vol. 44, no. 47, 475501, pp. -. https://doi.org/10.1088/1751-8113/44/47/475501

APA

Vancouver

Landa PS, McClintock PVE. Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams. Journal of Physics A: Mathematical and Theoretical. 2011 Nov 25;44(47):-. 475501. doi: 10.1088/1751-8113/44/47/475501

Author

Landa, P. S. ; McClintock, P. V. E. / Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams. In: Journal of Physics A: Mathematical and Theoretical. 2011 ; Vol. 44, No. 47. pp. -.

Bibtex

@article{ab73a01703804876bdbe33d2eacfae88,
title = "Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams",
abstract = "We show that wave excitation and propagation in an inhomogeneous medium lead to the simultaneous appearance of a huge number of waves with different phase velocities. This phenomenon arises in any medium with inhomogeneous parameters, e. g., in fluid jets where the inhomogeneity appears as a result of the boundary layer. Because of fluctuations (however small) the waves become randomized, i.e. turbulence develops. We demonstrate that the eigenvalues depend essentially on the frequency of the perturbation and on the distance from the initial section of a jet or wave beam. We show how to find the continuous set of eigenvalues-complex wavenumbers-and corresponding eigenfunctions for any given frequency. The implication of these results is that the transition to turbulence occurs, not through the excitation of a gradually increasing number of waves, as commonly supposed, but by the simultaneous excitation of a continuous wave spectrum.",
author = "Landa, {P. S.} and McClintock, {P. V. E.}",
year = "2011",
month = nov,
day = "25",
doi = "10.1088/1751-8113/44/47/475501",
language = "English",
volume = "44",
pages = "--",
journal = "Journal of Physics A: Mathematical and Theoretical",
issn = "1751-8113",
publisher = "IOP Publishing Ltd.",
number = "47",

}

RIS

TY - JOUR

T1 - Initiation of turbulence and chaos in non-equilibrium inhomogeneous media: wave beams

AU - Landa, P. S.

AU - McClintock, P. V. E.

PY - 2011/11/25

Y1 - 2011/11/25

N2 - We show that wave excitation and propagation in an inhomogeneous medium lead to the simultaneous appearance of a huge number of waves with different phase velocities. This phenomenon arises in any medium with inhomogeneous parameters, e. g., in fluid jets where the inhomogeneity appears as a result of the boundary layer. Because of fluctuations (however small) the waves become randomized, i.e. turbulence develops. We demonstrate that the eigenvalues depend essentially on the frequency of the perturbation and on the distance from the initial section of a jet or wave beam. We show how to find the continuous set of eigenvalues-complex wavenumbers-and corresponding eigenfunctions for any given frequency. The implication of these results is that the transition to turbulence occurs, not through the excitation of a gradually increasing number of waves, as commonly supposed, but by the simultaneous excitation of a continuous wave spectrum.

AB - We show that wave excitation and propagation in an inhomogeneous medium lead to the simultaneous appearance of a huge number of waves with different phase velocities. This phenomenon arises in any medium with inhomogeneous parameters, e. g., in fluid jets where the inhomogeneity appears as a result of the boundary layer. Because of fluctuations (however small) the waves become randomized, i.e. turbulence develops. We demonstrate that the eigenvalues depend essentially on the frequency of the perturbation and on the distance from the initial section of a jet or wave beam. We show how to find the continuous set of eigenvalues-complex wavenumbers-and corresponding eigenfunctions for any given frequency. The implication of these results is that the transition to turbulence occurs, not through the excitation of a gradually increasing number of waves, as commonly supposed, but by the simultaneous excitation of a continuous wave spectrum.

U2 - 10.1088/1751-8113/44/47/475501

DO - 10.1088/1751-8113/44/47/475501

M3 - Journal article

VL - 44

SP - -

JO - Journal of Physics A: Mathematical and Theoretical

JF - Journal of Physics A: Mathematical and Theoretical

SN - 1751-8113

IS - 47

M1 - 475501

ER -