<p>In this paper, we study the nonlinear asymptotic stability of the 2D Boussinesq equations near the Couette flow in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb{T}\times \mathbb{R}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mo>×</mo> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> under the condition that the Richardson number satisfies <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\gamma^{2} &gt; {1\over 4}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msup> <mi>γ</mi> <mrow> <mn>2</mn> </mrow> </msup> <mo>&gt;</mo> <mrow> <mfrac> <mn>1</mn> <mn>4</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. We allow for different viscosity <i>ν</i> and thermal diffusivity <i>μ</i> and establish stability in the regime <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu^{3}\leq \nu \leq\mu^{ {1\over 3}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msup> <mi>μ</mi> <mrow> <mn>3</mn> </mrow> </msup> <mo>≤</mo> <mi>ν</mi> <mo>≤</mo> <msup> <mi>μ</mi> <mrow> <mrow> <mfrac> <mn>1</mn> <mn>3</mn> </mfrac> </mrow> </mrow> </msup> </math></EquationSource> </InlineEquation>. We show that if the initial perturbation is sufficiently small in <i>H</i><sup><i>N</i>+1</sup> × <i>H</i><sup><i>N</i>+2</sup> (with <i>N</i> ⩾ 6) in the sense that, for some sufficiently small <i>α</i> &gt; 0 (0 &lt; <i>α</i> ≪ 1), <Equation ID="Equ1"> <EquationSource Format="TEX">\(\parallel v_{\text{in}}-(y,0)\parallel_{H^{N+1}}+\parallel\rho_{\text{in}}+\gamma^{2}y-1\parallel_{H^{N+2}}\leq\varepsilon_{0}\min\{\nu,\mu\}^{{1\over 2}+{4\over 3}\alpha},\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo stretchy="false">∥</mo> <msub> <mi>v</mi> <mrow> <mtext>in</mtext> </mrow> </msub> <mo>−</mo> <mo stretchy="false">(</mo> <mi>y</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> <msub> <mo>∥</mo> <mrow> <msup> <mi>H</mi> <mrow> <mi>N</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </mrow> </msub> <mo>+</mo> <mo>∥</mo> <msub> <mi>ρ</mi> <mrow> <mtext>in</mtext> </mrow> </msub> <mo>+</mo> <msup> <mi>γ</mi> <mrow> <mn>2</mn> </mrow> </msup> <mi>y</mi> <mo>−</mo> <mn>1</mn> <msub> <mo>∥</mo> <mrow> <msup> <mi>H</mi> <mrow> <mi>N</mi> <mo>+</mo> <mn>2</mn> </mrow> </msup> </mrow> </msub> <mo>≤</mo> <msub> <mi>ε</mi> <mrow> <mn>0</mn> </mrow> </msub> <mo form="prefix" movablelimits="true">min</mo> <mo fence="false" stretchy="false">{</mo> <mi>ν</mi> <mo>,</mo> <mi>μ</mi> <msup> <mo fence="false" stretchy="false">}</mo> <mrow> <mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> <mo>+</mo> <mrow> <mfrac> <mn>4</mn> <mn>3</mn> </mfrac> </mrow> <mi>α</mi> </mrow> </msup> <mo>,</mo> </math></EquationSource> </Equation> then the Couette flow is asymptotically stable. The recent result of Zhai and Zhao (2023) represents an important contribution to this problem, and our work constitutes a substantial improvement.</p>

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Stability threshold analysis of the Boussinesq system with general viscosity near the Couette flow

  • Tao Liang,
  • Jiahong Wu,
  • Xiaoping Zhai

摘要

In this paper, we study the nonlinear asymptotic stability of the 2D Boussinesq equations near the Couette flow in \(\mathbb{T}\times \mathbb{R}\) T × R under the condition that the Richardson number satisfies \(\gamma^{2} > {1\over 4}\) γ 2 > 1 4 . We allow for different viscosity ν and thermal diffusivity μ and establish stability in the regime \(\mu^{3}\leq \nu \leq\mu^{ {1\over 3}}\) μ 3 ν μ 1 3 . We show that if the initial perturbation is sufficiently small in HN+1 × HN+2 (with N ⩾ 6) in the sense that, for some sufficiently small α > 0 (0 < α ≪ 1), \(\parallel v_{\text{in}}-(y,0)\parallel_{H^{N+1}}+\parallel\rho_{\text{in}}+\gamma^{2}y-1\parallel_{H^{N+2}}\leq\varepsilon_{0}\min\{\nu,\mu\}^{{1\over 2}+{4\over 3}\alpha},\) v in ( y , 0 ) H N + 1 + ρ in + γ 2 y 1 H N + 2 ε 0 min { ν , μ } 1 2 + 4 3 α , then the Couette flow is asymptotically stable. The recent result of Zhai and Zhao (2023) represents an important contribution to this problem, and our work constitutes a substantial improvement.