<p>In this article, we investigate the nonlinear stability of the Couette flow under the Boussinesq equations with only vertical dissipation in <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="21_2025_978_Article_IEq1.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {T}}\times {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">T</mi> <mo>×</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>. Inspired by the work of Wei and Zhang [Tunis. J. Math. 5(3):573-592 (2023)] and taking into account perturbations with different sizes, we can address the influence of buoyancy term within the coupled system. We obtain a stability result under the initial perturbations condition: <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="21_2025_978_Article_IEq2.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="356" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert \omega ^{(0)}\Vert _{H^b}+\nu ^{-1/2}\Vert \theta ^{(0)}\Vert _{H^b}+\nu ^{-1/6}\Vert \partial _x\theta ^{(0)}\Vert _{H^b}\lesssim \nu ^{1/3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>ω</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </msup> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>H</mi> <mi>b</mi> </msup> </msub> <mo>+</mo> <msup> <mi>ν</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>θ</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </msup> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>H</mi> <mi>b</mi> </msup> </msub> <mo>+</mo> <msup> <mi>ν</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>6</mn> </mrow> </msup> <msub> <mrow> <mo stretchy="false">‖</mo> <msub> <mi>∂</mi> <mi>x</mi> </msub> <msup> <mi>θ</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </msup> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>H</mi> <mi>b</mi> </msup> </msub> <mo>≲</mo> <msup> <mi>ν</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>3</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="21_2025_978_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(b\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Stability of the Couette Flow for 2D Boussinesq Equations with Only Vertical Dissipation

  • Qian Li,
  • Wen Luo,
  • Zekai Luo

摘要

In this article, we investigate the nonlinear stability of the Couette flow under the Boussinesq equations with only vertical dissipation in \({\mathbb {T}}\times {\mathbb {R}}\) T × R . Inspired by the work of Wei and Zhang [Tunis. J. Math. 5(3):573-592 (2023)] and taking into account perturbations with different sizes, we can address the influence of buoyancy term within the coupled system. We obtain a stability result under the initial perturbations condition: \(\Vert \omega ^{(0)}\Vert _{H^b}+\nu ^{-1/2}\Vert \theta ^{(0)}\Vert _{H^b}+\nu ^{-1/6}\Vert \partial _x\theta ^{(0)}\Vert _{H^b}\lesssim \nu ^{1/3}\) ω ( 0 ) H b + ν - 1 / 2 θ ( 0 ) H b + ν - 1 / 6 x θ ( 0 ) H b ν 1 / 3 , where \(b\ge 2\) b 2 .