Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory

Coherent wave groups are not only characterized by the intrinsic shape of the wave packet, but also by the underlying phase evolution during the propagation. Exact deterministic formulations of hydrodynamic or electromagnetic coherent wave groups can be obtained by solving the nonlinear Schrödinger...

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Main Authors: Yuchen He, Pierre Suret, Amin Chabchoub
Format: Article
Language:English
Published: MDPI AG 2021-08-01
Series:Fluids
Subjects:
Online Access:https://www.mdpi.com/2311-5521/6/9/308
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spelling doaj-468908c938f747388e873635753e647d2021-09-26T00:08:33ZengMDPI AGFluids2311-55212021-08-01630830810.3390/fluids6090308Phase Evolution of the Time- and Space-Like Peregrine Breather in a LaboratoryYuchen He0Pierre Suret1Amin Chabchoub2Centre for Wind, Waves and Water, School of Civil Engineering, The University of Sydney, Sydney, NSW 2006, AustraliaUniv. Lille, CNRS, UMR 8523 - PhLAM - Physique des Lasers Atomes et Molécules, F-59000 Lille, FranceCentre for Wind, Waves and Water, School of Civil Engineering, The University of Sydney, Sydney, NSW 2006, AustraliaCoherent wave groups are not only characterized by the intrinsic shape of the wave packet, but also by the underlying phase evolution during the propagation. Exact deterministic formulations of hydrodynamic or electromagnetic coherent wave groups can be obtained by solving the nonlinear Schrödinger equation (NLSE). When considering the NLSE, there are two asymptotically equivalent formulations, which can be used to describe the wave dynamics: the time- or space-like NLSE. These differences have been theoretically elaborated upon in the 2016 work of Chabchoub and Grimshaw. In this paper, we address fundamental characteristic differences beyond the shape of wave envelope, which arise in the phase evolution. We use the Peregrine breather as a referenced wave envelope model, whose dynamics is created and tracked in a wave flume using two boundary conditions, namely as defined by the time- and space-like NLSE. It is shown that whichever of the two boundary conditions is used, the corresponding local shape of wave localization is very close and almost identical during the evolution; however, the respective local phase evolution is different. The phase dynamics follows the prediction from the respective NLSE framework adopted in each case.https://www.mdpi.com/2311-5521/6/9/308nonlinear wavesPeregrine breatherrogue wavespattern formation
collection DOAJ
language English
format Article
sources DOAJ
author Yuchen He
Pierre Suret
Amin Chabchoub
spellingShingle Yuchen He
Pierre Suret
Amin Chabchoub
Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
Fluids
nonlinear waves
Peregrine breather
rogue waves
pattern formation
author_facet Yuchen He
Pierre Suret
Amin Chabchoub
author_sort Yuchen He
title Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
title_short Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
title_full Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
title_fullStr Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
title_full_unstemmed Phase Evolution of the Time- and Space-Like Peregrine Breather in a Laboratory
title_sort phase evolution of the time- and space-like peregrine breather in a laboratory
publisher MDPI AG
series Fluids
issn 2311-5521
publishDate 2021-08-01
description Coherent wave groups are not only characterized by the intrinsic shape of the wave packet, but also by the underlying phase evolution during the propagation. Exact deterministic formulations of hydrodynamic or electromagnetic coherent wave groups can be obtained by solving the nonlinear Schrödinger equation (NLSE). When considering the NLSE, there are two asymptotically equivalent formulations, which can be used to describe the wave dynamics: the time- or space-like NLSE. These differences have been theoretically elaborated upon in the 2016 work of Chabchoub and Grimshaw. In this paper, we address fundamental characteristic differences beyond the shape of wave envelope, which arise in the phase evolution. We use the Peregrine breather as a referenced wave envelope model, whose dynamics is created and tracked in a wave flume using two boundary conditions, namely as defined by the time- and space-like NLSE. It is shown that whichever of the two boundary conditions is used, the corresponding local shape of wave localization is very close and almost identical during the evolution; however, the respective local phase evolution is different. The phase dynamics follows the prediction from the respective NLSE framework adopted in each case.
topic nonlinear waves
Peregrine breather
rogue waves
pattern formation
url https://www.mdpi.com/2311-5521/6/9/308
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