{"title":"Three-Dimensional Acoustic Turbulence: Weak Versus Strong","authors":"E. A. Kochurin, E. A. Kuznetsov","doi":"arxiv-2407.08352","DOIUrl":null,"url":null,"abstract":"Direct numerical simulation of three-dimensional acoustic turbulence has been\nperformed for both weak and strong regimes. Within the weak turbulence, we\ndemonstrate the existence of the Zakharov-Sagdeev spectrum $\\propto k^{-3/2}$\nnot only for weak dispersion but in the non-dispersion (ND) case as well. Such\nspectra in the $k$-space are accompanied by jets in the form of narrow cones.\nThese distributions are realized due to small nonlinearity compared with both\ndispersion/diffraction. Increasing pumping in the ND case due to dominant\nnonlinear effects leads to the formation of shocks. As a result, the acoustic\nturbulence turns into an ensemble of random shocks with the\nKadomtsev-Petviashvili spectrum.","PeriodicalId":501167,"journal":{"name":"arXiv - PHYS - Chaotic Dynamics","volume":"102 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chaotic Dynamics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.08352","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Direct numerical simulation of three-dimensional acoustic turbulence has been
performed for both weak and strong regimes. Within the weak turbulence, we
demonstrate the existence of the Zakharov-Sagdeev spectrum $\propto k^{-3/2}$
not only for weak dispersion but in the non-dispersion (ND) case as well. Such
spectra in the $k$-space are accompanied by jets in the form of narrow cones.
These distributions are realized due to small nonlinearity compared with both
dispersion/diffraction. Increasing pumping in the ND case due to dominant
nonlinear effects leads to the formation of shocks. As a result, the acoustic
turbulence turns into an ensemble of random shocks with the
Kadomtsev-Petviashvili spectrum.