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Existence of Homogeneous Euler Flows of Degree \(-\alpha \notin [-2,0]\)

  • Ken Abe

摘要

We consider ( \(-\alpha \) - α )-homogeneous solutions to the stationary incompressible Euler equations in \({\mathbb {R}}^{3}\backslash \{0\}\) R 3 \ { 0 } for \(\alpha \geqq 0\) α 0 and in \({\mathbb {R}}^{3}\) R 3 for \(\alpha <0\) α < 0 . Shvydkoy (2018) demonstrated the nonexistence of ( \(-1\) - 1 )-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 1 ( R 3 \ { 0 } ) and ( \(-\alpha \) - α )-homogeneous solutions in the range \(0\leqq \alpha \leqq 2\) 0 α 2 for the Beltrami and axisymmetric flow; namely, that no ( \(-\alpha \) - α )-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 1 ( R 3 \ { 0 } ) for \(1\leqq \alpha \leqq 2\) 1 α 2 and \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 2 ( R 3 \ { 0 } ) for \(0\leqq \alpha < 1\) 0 α < 1 exist among these particular classes of flows other than irrotational solutions for integers \(\alpha \) α . The nonexistence result of the Beltrami ( \(-\alpha \) - α )-homogeneous solutions \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 2 ( R 3 \ { 0 } ) holds for all \(\alpha <1\) α < 1 . We show the nonexistence of axisymmetric ( \(-\alpha \) - α )-homogeneous solutions without swirls \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 2 ( R 3 \ { 0 } ) for \(-2\leqq \alpha <0\) - 2 α < 0 . The main result of this study is the existence of axisymmetric ( \(-\alpha \) - α )-homogeneous solutions in the complementary range \(\alpha \in {\mathbb {R}}\backslash [0,2]\) α R \ [ 0 , 2 ] . More specifically, we show the existence of axisymmetric Beltrami ( \(-\alpha \) - α )-homogeneous solutions \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 1 ( R 3 \ { 0 } ) for \(\alpha >2\) α > 2 and \((u,p)\in C({\mathbb {R}}^{3})\) ( u , p ) C ( R 3 ) for \(\alpha <0\) α < 0 and axisymmetric ( \(-\alpha \) - α )-homogeneous solutions with a nonconstant Bernoulli function \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 1 ( R 3 \ { 0 } ) for \(\alpha >2\) α > 2 and \((u,p)\in C({\mathbb {R}}^{3})\) ( u , p ) C ( R 3 ) for \(\alpha <-2\) α < - 2 , including axisymmetric ( \(-\alpha \) - α )-homogeneous solutions without swirls \((u,p)\in C^{2}({\mathbb {R}}^{3}\backslash \{0\})\) ( u , p ) C 2 ( R 3 \ { 0 } ) for \(\alpha >2\) α > 2 and \((u,p)\in C^{1}({\mathbb {R}}^{3}\backslash \{0\})\cap C({\mathbb {R}}^{3})\) ( u , p ) C 1 ( R 3 \ { 0 } ) C ( R 3 ) for \(\alpha <-2\) α < - 2 . This is the first existence result on ( \(-\alpha \) - α )-homogeneous solutions with no explicit forms. The level sets of the axisymmetric stream function of the irrotational ( \(-\alpha \) - α )-homogeneous solutions in the cross-section are the Jordan curves for \(\alpha =3\) α = 3 . For \(2<\alpha <3\) 2 < α < 3 , we show the existence of axisymmetric ( \(-\alpha \) - α )-homogeneous solutions whose stream function level sets are the Jordan curves. They provide new examples of the Beltrami/Euler flows in \({\mathbb {R}}^{3}\backslash \{0\}\) R 3 \ { 0 } whose level sets of the proportionality factor/Bernoulli surfaces are nested surfaces created by the rotation of the sign \(``\infty ''\) ` ` .