<p>We consider (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>)-homogeneous solutions (stationary self-similar solutions of degree <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>) to the two-dimensional inviscid Boussinesq equations in a half-plane. We show their non-existence and existence with both regular and singular profile functions. More specifically, we demonstrate the following:<UnorderedList Mark="Bullet"> <ItemContent> <p>Non-existence of rotational (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>)-homogeneous solutions with regular profiles <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{1}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(0\leqq \alpha \leqq 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≦</mo> <mi>α</mi> <mo>≦</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{2}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(-1/2\leqq \alpha &lt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> <mo>≦</mo> <mi>α</mi> <mo>&lt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>;</p> </ItemContent> <ItemContent> <p>Existence of rotational (<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>)-homogeneous solutions with regular profiles <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{2}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\alpha &gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{1}(\overline{\mathbb {R}^{2}_{+}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\alpha &lt;-2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&lt;</mo> <mo>-</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>;</p> </ItemContent> <ItemContent> <p>Existence of rotational (<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>)-homogeneous solutions with <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(x_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>x</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>-symmetric singular profiles <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\((u,p,\rho ) \in C^{\infty }(\overline{\mathbb {R}^{2}_{+}}\backslash \{x_1=0\}\cup \{x_2=0\})\cap C(\overline{\mathbb {R}^{2}_{+}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>∪</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>∩</mo> <mi>C</mi> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(-1&lt;\alpha &lt; -1/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>1</mn> <mo>&lt;</mo> <mi>α</mi> <mo>&lt;</mo> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{\infty }(\overline{\mathbb {R}^{2}_{+}}\backslash \{x_1=0\}\cup \{x_2=0\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>∪</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(-1/2\leqq \alpha &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> <mo>≦</mo> <mi>α</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p> </ItemContent> </UnorderedList> The (<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(-\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation>)-homogeneous solutions with continuous profiles <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\((u,p,\rho )\in C^{\infty }(\overline{\mathbb {R}^{2}_{+}} \backslash \{x_1=0\}\cup \{x_2=0\})\cap C(\overline{\mathbb {R}^{2}_{+}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>p</mi> <mo>,</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo>∪</mo> <mrow> <mo stretchy="false">{</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>∩</mo> <mi>C</mi> <mrow> <mo stretchy="false">(</mo> <mover> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> <mo>¯</mo> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(-1&lt;\alpha &lt;-1/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>1</mn> <mo>&lt;</mo> <mi>α</mi> <mo>&lt;</mo> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> provide examples of self-similar weak solutions in <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\mathbb {R}^{2}_{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation> for the scaling exponent <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\alpha \approx -0.657\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>≈</mo> <mo>-</mo> <mn>0.657</mn> </mrow> </math></EquationSource> </InlineEquation>, at which Wang et al. (Phys Rev Lett 130(24):244002, 2023) numerically discovered the existence of backward self-similar solutions with smooth profile functions.</p>

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Stationary Self-Similar Profiles for the Two-Dimensional Inviscid Boussinesq Equations

  • Ken Abe,
  • Daniel Ginsberg,
  • In-Jee Jeong

摘要

We consider ( \(-\alpha \) - α )-homogeneous solutions (stationary self-similar solutions of degree \(-\alpha \) - α ) to the two-dimensional inviscid Boussinesq equations in a half-plane. We show their non-existence and existence with both regular and singular profile functions. More specifically, we demonstrate the following:

Non-existence of rotational ( \(-\alpha \) - α )-homogeneous solutions with regular profiles \((u,p,\rho )\in C^{1}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\) ( u , p , ρ ) C 1 ( R + 2 ¯ \ { 0 } ) for \(0\leqq \alpha \leqq 1\) 0 α 1 and \((u,p,\rho )\in C^{2}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\) ( u , p , ρ ) C 2 ( R + 2 ¯ \ { 0 } ) for \(-1/2\leqq \alpha <0\) - 1 / 2 α < 0 ;

Existence of rotational ( \(-\alpha \) - α )-homogeneous solutions with regular profiles \((u,p,\rho )\in C^{2}(\overline{\mathbb {R}^{2}_{+}}\backslash \{0\})\) ( u , p , ρ ) C 2 ( R + 2 ¯ \ { 0 } ) for \(\alpha >1\) α > 1 and \((u,p,\rho )\in C^{1}(\overline{\mathbb {R}^{2}_{+}})\) ( u , p , ρ ) C 1 ( R + 2 ¯ ) for \(\alpha <-2\) α < - 2 ;

Existence of rotational ( \(-\alpha \) - α )-homogeneous solutions with \(x_1\) x 1 -symmetric singular profiles \((u,p,\rho ) \in C^{\infty }(\overline{\mathbb {R}^{2}_{+}}\backslash \{x_1=0\}\cup \{x_2=0\})\cap C(\overline{\mathbb {R}^{2}_{+}})\) ( u , p , ρ ) C ( R + 2 ¯ \ { x 1 = 0 } { x 2 = 0 } ) C ( R + 2 ¯ ) for \(-1<\alpha < -1/2\) - 1 < α < - 1 / 2 and \((u,p,\rho )\in C^{\infty }(\overline{\mathbb {R}^{2}_{+}}\backslash \{x_1=0\}\cup \{x_2=0\})\) ( u , p , ρ ) C ( R + 2 ¯ \ { x 1 = 0 } { x 2 = 0 } ) for \(-1/2\leqq \alpha <1\) - 1 / 2 α < 1 .

The ( \(-\alpha \) - α )-homogeneous solutions with continuous profiles \((u,p,\rho )\in C^{\infty }(\overline{\mathbb {R}^{2}_{+}} \backslash \{x_1=0\}\cup \{x_2=0\})\cap C(\overline{\mathbb {R}^{2}_{+}})\) ( u , p , ρ ) C ( R + 2 ¯ \ { x 1 = 0 } { x 2 = 0 } ) C ( R + 2 ¯ ) for \(-1<\alpha <-1/2\) - 1 < α < - 1 / 2 provide examples of self-similar weak solutions in \(\mathbb {R}^{2}_{+}\) R + 2 for the scaling exponent \(\alpha \approx -0.657\) α - 0.657 , at which Wang et al. (Phys Rev Lett 130(24):244002, 2023) numerically discovered the existence of backward self-similar solutions with smooth profile functions.