<p>A nonconforming <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> finite element is constructed by enriching the conforming <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> finite element space with nine <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> nonconforming bubbles, on each tetrahedron. Here, the divergence of the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> bubble is not a <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> polynomial, but a <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> polynomial. This nonconforming <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> finite element, combined with the discontinuous <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> finite element, is inf-sup stable for solving the Stokes equations on general tetrahedral grids. Consequently, such a mixed finite element method produces quasi-optimal solutions for solving the stationary Stokes equations. With these special <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10444_2025_10244_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> bubbles, the discrete velocity remains locally pointwise divergence-free. Numerical tests confirm the theory.</p>

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A nonconforming P3+B4 and discontinuous P2 mixed finite element on tetrahedral grids

  • Xuejun Xu,
  • Shangyou Zhang

摘要

A nonconforming \(P_3\) P 3 finite element is constructed by enriching the conforming \(P_3\) P 3 finite element space with nine \(P_4\) P 4 nonconforming bubbles, on each tetrahedron. Here, the divergence of the \(P_4\) P 4 bubble is not a \(P_3\) P 3 polynomial, but a \(P_2\) P 2 polynomial. This nonconforming \(P_3\) P 3 finite element, combined with the discontinuous \(P_2\) P 2 finite element, is inf-sup stable for solving the Stokes equations on general tetrahedral grids. Consequently, such a mixed finite element method produces quasi-optimal solutions for solving the stationary Stokes equations. With these special \(P_4\) P 4 bubbles, the discrete velocity remains locally pointwise divergence-free. Numerical tests confirm the theory.