4.7 Article

Gap resonance from linear to quartic wave excitation and the structure of nonlinear transfer functions

期刊

JOURNAL OF FLUID MECHANICS
卷 926, 期 -, 页码 -

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2021.659

关键词

wave-structure interactions

资金

  1. University ofWestern Australia
  2. Woodside Energy
  3. Shell
  4. Lloyd's Register [IH140100012]
  5. Australian Research Council [DE190101296]
  6. Australian Research Council
  7. Bureau Veritas

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The study investigates the resonant response of water waves in a narrow gap between two fixed rectangular boxes, showing that these resonances can be driven through both linear wave excitation and nonlinear processes. It is found that the time histories of gap resonances excited through different nonlinear interactions are remarkably similar. The research suggests that the nonlinear sum-frequency transfer functions for gap resonances depend strongly on the output frequency sum of the interacting linear components, but only weakly on the frequency difference.
Resonant response of water waves in a narrow gap, with the interaction of multiple highly resonant modes, is an interesting hydrodynamic phenomenon with practical applications. Gap resonances between two identical fixed rectangular boxes are experimentally investigated for unidirectional waves with broadside incidence. We show that gap resonances can be driven through both linear wave excitation and nonlinear processes, i.e. frequency doubling, tripling and quadrupling - apparently new observations. It is striking that the time histories of the gap resonances excited through different nonlinear interactions are remarkably similar to each other. It seems likely that the nonlinear sum-frequency transfer functions for gap resonances depend strongly on the output frequency sum of the interacting linear components, but only weakly on the frequency difference. In terms of their structure in multiple frequency space (at second order the bi-frequency plane for two components), these transfer functions must then have a near-flat form in the direction(s) perpendicular to the leading diagonal. This is supported by our potential flow calculations of the quadratic transfer functions (QTFs). It is therefore convenient to approximate the QTF matrix as 'flat' in the direction perpendicular to the leading diagonal. This approximation is justified through experimental data that includes viscous damping. It is too complex, if not impossible, to calculate the full cubic or quartic transfer functions as direct evidence. However, the experimental analysis does provide some support for the near-flat structure being applicable to transfer functions above second order. The flat form approximation greatly reduces lengthy calculations of the high-order transfer functions.

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