<p>This paper deals with a two-dimensional Keller-Segel-Navier-Stokes system of coral fertilization with porous medium diffusion. When the nonlinear diffusion exponents of sperms and eggs <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>m</mi> <mo>&gt;</mo> <mfrac> <mrow> <mn>1</mn> </mrow> <mn>2</mn> </mfrac> </math></EquationSource> <EquationSource Format="TEX">$m&gt;\frac{1}{2}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>l</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$l&gt;0$</EquationSource> </InlineEquation> respectively, as well as the strength of fertilization <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>μ</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$\mu &gt;0$</EquationSource> </InlineEquation>, the system possesses a global bounded weak solution. Furthermore, if <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mn>0</mn> <mo>&lt;</mo> <mi>l</mi> <mo>&lt;</mo> <mn>1</mn> </math></EquationSource> <EquationSource Format="TEX">$0&lt; l&lt;1$</EquationSource> </InlineEquation>, the corresponding global weak solution stabilizes to the spatially homogeneous equilibrium <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="109" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <msub> <mi>n</mi> <mi mathvariant="normal">∞</mi> </msub> <mo>,</mo> <msub> <mi>ρ</mi> <mi mathvariant="normal">∞</mi> </msub> <mo>,</mo> <msub> <mi>ρ</mi> <mi mathvariant="normal">∞</mi> </msub> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(n_{\infty },\rho _{\infty },\rho _{\infty },0)$</EquationSource> </InlineEquation> in an appropriate sense, where <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq6.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="182" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>n</mi> <mi mathvariant="normal">∞</mi> </msub> <mo>:</mo> <mo>=</mo> <mfrac> <mn>1</mn> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> </mrow> </mfrac> <msub> <mrow> <mo stretchy="false">(</mo> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msub> <mi>n</mi> <mn>0</mn> </msub> <mo>−</mo> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msub> <mi>ρ</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> </msub> </math></EquationSource> <EquationSource Format="TEX">$n_{\infty }:=\frac{1}{|\Omega |}(\int _{\Omega }n_{0}-\int _{\Omega } \rho _{0})_{+}$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_731_Article_IEq7.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="181" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ρ</mi> <mi mathvariant="normal">∞</mi> </msub> <mo>:</mo> <mo>=</mo> <mfrac> <mn>1</mn> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> </mrow> </mfrac> <msub> <mrow> <mo stretchy="false">(</mo> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msub> <mi>ρ</mi> <mn>0</mn> </msub> <mo>−</mo> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msub> <mi>n</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> </msub> </math></EquationSource> <EquationSource Format="TEX">$\rho _{\infty }:=\frac{1}{|\Omega |}(\int _{\Omega }\rho _{0}-\int _{ \Omega }n_{0})_{+}$</EquationSource> </InlineEquation>.</p>

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Boundedness and Large Time Behavior in a Two-Dimensional Keller-Segel-Navier-Stokes System with Nonlinear Diffusion Modeling Coral Fertilization

  • Na Huang,
  • Chunlai Mu,
  • Minghua Zhang,
  • Xu Pan

摘要

This paper deals with a two-dimensional Keller-Segel-Navier-Stokes system of coral fertilization with porous medium diffusion. When the nonlinear diffusion exponents of sperms and eggs m > 1 2 $m>\frac{1}{2}$ , l > 0 $l>0$ respectively, as well as the strength of fertilization μ > 0 $\mu >0$ , the system possesses a global bounded weak solution. Furthermore, if 0 < l < 1 $0< l<1$ , the corresponding global weak solution stabilizes to the spatially homogeneous equilibrium ( n , ρ , ρ , 0 ) $(n_{\infty },\rho _{\infty },\rho _{\infty },0)$ in an appropriate sense, where n : = 1 | Ω | ( Ω n 0 Ω ρ 0 ) + $n_{\infty }:=\frac{1}{|\Omega |}(\int _{\Omega }n_{0}-\int _{\Omega } \rho _{0})_{+}$ and ρ : = 1 | Ω | ( Ω ρ 0 Ω n 0 ) + $\rho _{\infty }:=\frac{1}{|\Omega |}(\int _{\Omega }\rho _{0}-\int _{ \Omega }n_{0})_{+}$ .