{"title":"三临界点是 I_s$ 型和 II_s$ 型分岔的交叉点","authors":"Prabakaran Rajamanickam, Joel Daou","doi":"arxiv-2407.00109","DOIUrl":null,"url":null,"abstract":"A tricritical point as a crossover between (stationary finite-wavelength)\ntype-I$_s$ and (stationary longwave) type-II$_s$ bifurcations is identified in\nthe study of diffusive-thermal (Turing) instability of flames propagating in a\nHele-Shaw channel in a direction transverse to a shear flow. Three regimes\nexhibiting different scaling laws are identified in the neighbourhood of the\ntricritical point. For these three regimes, sixth-order partial differential\nequations are obtained governing the weakly nonlinear evolution of unstable\nsolutions near the onset of instability. These sixth-order PDES may be regarded\nas the substitute for the classical fourth-order Kuramoto--Sivashinsky equation\nwhich is not applicable near the tricritical point.","PeriodicalId":501370,"journal":{"name":"arXiv - PHYS - Pattern Formation and Solitons","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-06-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Tricritical point as a crossover between type-I$_s$ and type-II$_s$ bifurcations\",\"authors\":\"Prabakaran Rajamanickam, Joel Daou\",\"doi\":\"arxiv-2407.00109\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A tricritical point as a crossover between (stationary finite-wavelength)\\ntype-I$_s$ and (stationary longwave) type-II$_s$ bifurcations is identified in\\nthe study of diffusive-thermal (Turing) instability of flames propagating in a\\nHele-Shaw channel in a direction transverse to a shear flow. Three regimes\\nexhibiting different scaling laws are identified in the neighbourhood of the\\ntricritical point. For these three regimes, sixth-order partial differential\\nequations are obtained governing the weakly nonlinear evolution of unstable\\nsolutions near the onset of instability. These sixth-order PDES may be regarded\\nas the substitute for the classical fourth-order Kuramoto--Sivashinsky equation\\nwhich is not applicable near the tricritical point.\",\"PeriodicalId\":501370,\"journal\":{\"name\":\"arXiv - PHYS - Pattern Formation and Solitons\",\"volume\":\"5 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-06-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Pattern Formation and Solitons\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2407.00109\",\"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 - Pattern Formation and Solitons","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.00109","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Tricritical point as a crossover between type-I$_s$ and type-II$_s$ bifurcations
A tricritical point as a crossover between (stationary finite-wavelength)
type-I$_s$ and (stationary longwave) type-II$_s$ bifurcations is identified in
the study of diffusive-thermal (Turing) instability of flames propagating in a
Hele-Shaw channel in a direction transverse to a shear flow. Three regimes
exhibiting different scaling laws are identified in the neighbourhood of the
tricritical point. For these three regimes, sixth-order partial differential
equations are obtained governing the weakly nonlinear evolution of unstable
solutions near the onset of instability. These sixth-order PDES may be regarded
as the substitute for the classical fourth-order Kuramoto--Sivashinsky equation
which is not applicable near the tricritical point.