<p>In this paper, we study the stability for the 2-D plane Poiseuille flow (1 − <i>y</i><sup>2</sup>, 0) in a channel <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11425_2024_2382_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{T}\times(-1,1)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mo>×</mo> <mo stretchy="false">(</mo> <mo>−</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> with the Navier-slip boundary condition. We prove that if the initial perturbation for the velocity field <i>u</i><sub>0</sub> satisfies that <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11425_2024_2382_Article_IEq2.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="126" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert{u}_{0}\Vert_{H^{{7\over{2}}+}}\leqslant{\epsilon}_{1}\nu^{2/3}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo fence="false" stretchy="false">∥</mo> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <msub> <mo>∥</mo> <mrow> <msup> <mi>H</mi> <mrow> <mrow> <mfrac> <mn>7</mn> <mrow> <mn>2</mn> </mrow> </mfrac> </mrow> <mo>+</mo> </mrow> </msup> </mrow> </msub> <mo>⩽</mo> <msub> <mrow> <mi>ϵ</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> <msup> <mi>ν</mi> <mrow> <mn>2</mn> <mrow> <mo>/</mo> </mrow> <mn>3</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> for some suitable small 0 &lt; <i>ϵ</i><sub>1</sub> ≪ 1 independent of the viscosity coefficient <i>ν</i>, then the solution to the Navier-Stokes equations is global in time and does not transit from the plane Poiseuille flow. This result improves the result of Ding and Lin (2022).</p>

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Stability for the 2-D plane Poiseuille flow in a finite channel

  • Shijin Ding,
  • Zhilin Lin

摘要

In this paper, we study the stability for the 2-D plane Poiseuille flow (1 − y2, 0) in a channel \(\mathbb{T}\times(-1,1)\) T × ( 1 , 1 ) with the Navier-slip boundary condition. We prove that if the initial perturbation for the velocity field u0 satisfies that \(\Vert{u}_{0}\Vert_{H^{{7\over{2}}+}}\leqslant{\epsilon}_{1}\nu^{2/3}\) u 0 H 7 2 + ϵ 1 ν 2 / 3 for some suitable small 0 < ϵ1 ≪ 1 independent of the viscosity coefficient ν, then the solution to the Navier-Stokes equations is global in time and does not transit from the plane Poiseuille flow. This result improves the result of Ding and Lin (2022).