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  4. Stability of internal gravity wave modes: from triad resonance to broadband instability

Stability of internal gravity wave modes: from triad resonance to broadband instability

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sword-2024-06-11T17:46:23.original.xml (130 B)
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Author(s)
Akylas, Triantaphyllos R.
โ€ข
Kakoutas, Christos
Date Issued
April 19, 2023
Journal
Journal of Fluid Mechanics
Publisher
Cambridge University Press
Citation
Akylas TR, Kakoutas C. Stability of internal gravity wave modes: from triad resonance to broadband instability. Journal of Fluid Mechanics. 2023;961:A22.
Version
Author's final manuscript
Abstract
A theoretical study is made of the stability of propagating internal gravity wave modes along a horizontal stratified fluid layer bounded by rigid walls. The analysis is based on the Floquet eigenvalue problem for infinitesimal perturbations to a wave mode of small amplitude. The appropriate instability mechanism hinges on how the perturbation spatial scale relative to the basic-state wavelength, controlled by a parameter ๐œ‡, compares to the basic-state amplitude parameter, ๐œ– โ‰ช 1. For ๐œ‡=๐‘‚(1), the onset of instability arises due to perturbations that form resonant triads with the underlying wave mode. For short-scale perturbations such that ๐œ‡ โ‰ช 1 but ๐›ผ = ๐œ‡/๐œ– โ‰ซ 1, this triad resonance instability reduces to the familiar parametric subharmonic instability (PSI), where triads comprise fine-scale perturbations with half the basic-wave frequency. However, as ๐œ‡ is further decreased holding ๐œ– fixed, higher-frequency perturbations than these two subharmonics come into play, and when ๐›ผ = ๐‘‚(1) Floquet modes feature broadband spectrum. This broadening phenomenon is a manifestation of the advection of small-scale perturbations by the basic-wave velocity field. By working with a set of โ€˜streamline coordinatesโ€™ in the frame of the basic wave, this advection can be โ€˜factored outโ€™. Importantly, when ๐›ผ = ๐‘‚(1) PSI is replaced by a novel, multi-mode resonance mechanism which has a stabilising effect that provides an inviscid short-scale cut-off to PSI. The theoretical predictions are supported by numerical results from solving the Floquet eigenvalue problem for a mode-1 basic state.
MIT Department
Massachusetts Institute of Technology. Department of Mechanical Engineering
Terms of Use
Creative Commons Attribution-Noncommercial-ShareAlike
http://creativecommons.org/licenses/by-nc-sa/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/155246
DOI of Published Version
https://doi.org/10.1017/jfm.2023.265
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