{"title":"三维声湍流:弱湍流与强湍流","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":"{\"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}","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}
Three-Dimensional Acoustic Turbulence: Weak Versus Strong
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.