{"title":"Existence of Homogeneous Euler Flows of Degree \\(-\\alpha \\notin [-2,0]\\)","authors":"Ken Abe","doi":"10.1007/s00205-024-01974-0","DOIUrl":null,"url":null,"abstract":"<div><p>We consider (<span>\\(-\\alpha \\)</span>)-homogeneous solutions to the stationary incompressible Euler equations in <span>\\({\\mathbb {R}}^{3}\\backslash \\{0\\}\\)</span> for <span>\\(\\alpha \\geqq 0\\)</span> and in <span>\\({\\mathbb {R}}^{3}\\)</span> for <span>\\(\\alpha <0\\)</span>. Shvydkoy (2018) demonstrated the <i>nonexistence</i> of (<span>\\(-1\\)</span>)-homogeneous solutions <span>\\((u,p)\\in C^{1}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> and (<span>\\(-\\alpha \\)</span>)-homogeneous solutions in the range <span>\\(0\\leqq \\alpha \\leqq 2\\)</span> for the Beltrami and axisymmetric flow; namely, that no (<span>\\(-\\alpha \\)</span>)-homogeneous solutions <span>\\((u,p)\\in C^{1}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(1\\leqq \\alpha \\leqq 2\\)</span> and <span>\\((u,p)\\in C^{2}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(0\\leqq \\alpha < 1\\)</span> exist among these particular classes of flows other than irrotational solutions for integers <span>\\(\\alpha \\)</span>. The nonexistence result of the Beltrami (<span>\\(-\\alpha \\)</span>)-homogeneous solutions <span>\\((u,p)\\in C^{2}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> holds for all <span>\\(\\alpha <1\\)</span>. We show the nonexistence of axisymmetric (<span>\\(-\\alpha \\)</span>)-homogeneous solutions without swirls <span>\\((u,p)\\in C^{2}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(-2\\leqq \\alpha <0\\)</span>. The main result of this study is the <i>existence</i> of axisymmetric (<span>\\(-\\alpha \\)</span>)-homogeneous solutions in the complementary range <span>\\(\\alpha \\in {\\mathbb {R}}\\backslash [0,2]\\)</span>. More specifically, we show the existence of axisymmetric Beltrami (<span>\\(-\\alpha \\)</span>)-homogeneous solutions <span>\\((u,p)\\in C^{1}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(\\alpha >2\\)</span> and <span>\\((u,p)\\in C({\\mathbb {R}}^{3})\\)</span> for <span>\\(\\alpha <0\\)</span> and axisymmetric (<span>\\(-\\alpha \\)</span>)-homogeneous solutions with a nonconstant Bernoulli function <span>\\((u,p)\\in C^{1}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(\\alpha >2\\)</span> and <span>\\((u,p)\\in C({\\mathbb {R}}^{3})\\)</span> for <span>\\(\\alpha <-2\\)</span>, including axisymmetric (<span>\\(-\\alpha \\)</span>)-homogeneous solutions without swirls <span>\\((u,p)\\in C^{2}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\)</span> for <span>\\(\\alpha >2\\)</span> and <span>\\((u,p)\\in C^{1}({\\mathbb {R}}^{3}\\backslash \\{0\\})\\cap C({\\mathbb {R}}^{3})\\)</span> for <span>\\(\\alpha <-2\\)</span>. This is the first existence result on (<span>\\(-\\alpha \\)</span>)-homogeneous solutions with no explicit forms. The level sets of the axisymmetric stream function of the irrotational (<span>\\(-\\alpha \\)</span>)-homogeneous solutions in the cross-section are the Jordan curves for <span>\\(\\alpha =3\\)</span>. For <span>\\(2<\\alpha <3\\)</span>, we show the existence of axisymmetric (<span>\\(-\\alpha \\)</span>)-homogeneous solutions whose stream function level sets are the Jordan curves. They provide new examples of the Beltrami/Euler flows in <span>\\({\\mathbb {R}}^{3}\\backslash \\{0\\}\\)</span> whose level sets of the proportionality factor/Bernoulli surfaces are nested surfaces created by the rotation of the sign <span>\\(``\\infty ''\\)</span>.</p></div>","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2024-04-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s00205-024-01974-0","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
引用次数: 0
Abstract
We consider (\(-\alpha \))-homogeneous solutions to the stationary incompressible Euler equations in \({\mathbb {R}}^{3}\backslash \{0\}\) for \(\alpha \geqq 0\) and in \({\mathbb {R}}^{3}\) for \(\alpha <0\). Shvydkoy (2018) demonstrated the nonexistence of (\(-1\))-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) and (\(-\alpha \))-homogeneous solutions in the range \(0\leqq \alpha \leqq 2\) for the Beltrami and axisymmetric flow; namely, that no (\(-\alpha \))-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) for \(1\leqq \alpha \leqq 2\) and \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) for \(0\leqq \alpha < 1\) exist among these particular classes of flows other than irrotational solutions for integers \(\alpha \). The nonexistence result of the Beltrami (\(-\alpha \))-homogeneous solutions \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) holds for all \(\alpha <1\). We show the nonexistence of axisymmetric (\(-\alpha \))-homogeneous solutions without swirls \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) for \(-2\leqq \alpha <0\). The main result of this study is the existence of axisymmetric (\(-\alpha \))-homogeneous solutions in the complementary range \(\alpha \in {\mathbb {R}}\backslash [0,2]\). More specifically, we show the existence of axisymmetric Beltrami (\(-\alpha \))-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) for \(\alpha >2\) and \((u,p)\in C({\mathbb {R}}^{3})\) for \(\alpha <0\) and axisymmetric (\(-\alpha \))-homogeneous solutions with a nonconstant Bernoulli function \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) for \(\alpha >2\) and \((u,p)\in C({\mathbb {R}}^{3})\) for \(\alpha <-2\), including axisymmetric (\(-\alpha \))-homogeneous solutions without swirls \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) for \(\alpha >2\) and \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\cap C({\mathbb {R}}^{3})\) for \(\alpha <-2\). This is the first existence result on (\(-\alpha \))-homogeneous solutions with no explicit forms. The level sets of the axisymmetric stream function of the irrotational (\(-\alpha \))-homogeneous solutions in the cross-section are the Jordan curves for \(\alpha =3\). For \(2<\alpha <3\), we show the existence of axisymmetric (\(-\alpha \))-homogeneous solutions whose stream function level sets are the Jordan curves. They provide new examples of the Beltrami/Euler flows in \({\mathbb {R}}^{3}\backslash \{0\}\) whose level sets of the proportionality factor/Bernoulli surfaces are nested surfaces created by the rotation of the sign \(``\infty ''\).