<p>A difference finite element method based on the mixed finite element pair <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="196" /> </InlineMediaObject> <EquationSource Format="TEX">\(((P_1^b,P_1^b,P_1) \times (P_1,P_1,P_1))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mrow> <mo stretchy="false">(</mo> <msubsup> <mi>P</mi> <mn>1</mn> <mi>b</mi> </msubsup> <mo>,</mo> <msubsup> <mi>P</mi> <mn>1</mn> <mi>b</mi> </msubsup> <mo>,</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <mrow> <mo stretchy="false">(</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\((P_1 \times P_0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>×</mo> <msub> <mi>P</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is presented for the three-dimensional stationary Navier–Stokes equations with damping. Moreover, based on this proposed method, a two-level discretization is constructed, which involves solving a problem of the Navier–Stokes equations with damping on coarse mesh with mesh sizes <i>H</i> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">T</mi> </math></EquationSource> </InlineEquation>, and a general Stokes problem on fine mesh with mesh sizes <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="TEX">\(h = O(H^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>=</mo> <mi>O</mi> <mo stretchy="false">(</mo> <msup> <mi>H</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="79" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau = O(\mathcal {T}^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>τ</mi> <mo>=</mo> <mi>O</mi> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="script">T</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. This two-level difference finite element method provides an approximate solution with the same convergence rate as the difference finite element solution, which involves solving a problem of the Navier–Stokes equations with damping on fine mesh with mesh sizes <i>h</i> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10255_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>τ</mi> </math></EquationSource> </InlineEquation>. Hence, it can save a large amount of computational time. Finally, all computational results support the theoretical analysis and show the effectiveness of the two-level difference finite element method for solving the considered problem.</p>

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Two-level discretization of the 3D stationary Navier–Stokes equations with damping based on a difference finite element method

  • Qi Zhang,
  • Pengzhan Huang

摘要

A difference finite element method based on the mixed finite element pair \(((P_1^b,P_1^b,P_1) \times (P_1,P_1,P_1))\) ( ( P 1 b , P 1 b , P 1 ) × ( P 1 , P 1 , P 1 ) ) - \((P_1 \times P_0)\) ( P 1 × P 0 ) is presented for the three-dimensional stationary Navier–Stokes equations with damping. Moreover, based on this proposed method, a two-level discretization is constructed, which involves solving a problem of the Navier–Stokes equations with damping on coarse mesh with mesh sizes H and \(\mathcal {T}\) T , and a general Stokes problem on fine mesh with mesh sizes \(h = O(H^2)\) h = O ( H 2 ) and \(\tau = O(\mathcal {T}^2)\) τ = O ( T 2 ) . This two-level difference finite element method provides an approximate solution with the same convergence rate as the difference finite element solution, which involves solving a problem of the Navier–Stokes equations with damping on fine mesh with mesh sizes h and \(\tau \) τ . Hence, it can save a large amount of computational time. Finally, all computational results support the theoretical analysis and show the effectiveness of the two-level difference finite element method for solving the considered problem.