\`x^2+y_1+z_12^34\`
Advanced Search
Article Contents
Article Contents

Global weak solutions in a three-dimensional Keller-Segel-Navier-Stokes system modeling coral fertilization

  • * Corresponding author

    * Corresponding author 
Abstract / Introduction Full Text(HTML) Related Papers Cited by
  • We consider an initial-boundary value problem for the incompressible four-component Keller-Segel-Navier-Stokes system with rotational flux

    $ \begin{align} \left\{ \begin{array}{l} n_t+u\cdot\nabla n = \Delta n-\nabla\cdot(nS(x,n,c)\nabla c)-nm,\quad x\in \Omega, t>0,\\ c_t+u\cdot\nabla c = \Delta c-c+m,\quad x\in \Omega, t>0,\\ m_t+u\cdot\nabla m = \Delta m-nm,\quad x\in \Omega, t>0, \qquad \qquad \qquad \qquad \qquad \qquad (*)\\ u_t+\kappa(u \cdot \nabla)u+\nabla P = \Delta u+(n+m)\nabla \phi,\quad x\in \Omega, t>0,\\ \nabla\cdot u = 0,\quad x\in \Omega, t>0\\ \end{array}\right. \end{align} $

    in a bounded domain $ \Omega\subset \mathbb{R}^3 $ with smooth boundary, where $ \kappa\in \mathbb{R} $ is given constant, $ S $ is a matrix-valued sensitivity satisfying $ |S(x,n,c)|\leq C_S(1+n)^{-\alpha} $ with some $ C_S> 0 $ and $ \alpha\geq 0 $. As the case $ \kappa = 0 $ (with $ \alpha\geq\frac{1}{3} $ or the initial data satisfy a certain smallness condition) has been considered in [18], based on new gradient-like functional inequality, it is shown in the present paper that the corresponding initial-boundary problem with $ \kappa \neq 0 $ admits at least one global weak solution if $ \alpha>0 $. To the best of our knowledge, this is the first analytical work for the full three-dimensional four-component chemotaxis-Navier-Stokes system.

    Mathematics Subject Classification: 35K55, 35Q92, 35Q35, 92C17.

    Citation:

    \begin{equation} \\ \end{equation}
  • 加载中
  • [1] N. BellomoA. BelloquidY. Tao and M. Winkler, Toward a mathematical theory of Keller–Segel models of pattern formation in biological tissues, Math. Models Methods Appl. Sci., 25 (2015), 1663-1763.  doi: 10.1142/S021820251550044X.
    [2] X. Cao, Boundedness in a quasilinear parabolic–parabolic Keller–Segel system with logistic source, J. Math. Anal. Appl., 412 (2014), 181-188.  doi: 10.1016/j.jmaa.2013.10.061.
    [3] M. ChaeK. Kang and J. Lee, Global existence and temporal decay in Keller–Segel models coupled to fluid equations, Comm. Partial Differential Equations, 39 (2014), 1205-1235.  doi: 10.1080/03605302.2013.852224.
    [4] R. DuanA. Lorz and P. A. Markowich, Global solutions to the coupled chemotaxis-fluid equations, Comm. Partial Differential Equations, 35 (2010), 1635-1673.  doi: 10.1080/03605302.2010.497199.
    [5] E. E. Espejo and T. Suzuki, Reaction terms avoiding aggregation in slow fluids, Nonlinear Anal. Real World Appl., 21 (2015), 110-126.  doi: 10.1016/j.nonrwa.2014.07.001.
    [6] E. E. Espejo and M. Winkler, Global classical solvability and stabilization in a two-dimensional chemotaxis-Navier-Stokes system modeling coral fertilization, Nonlinearity, 31 (2018), 1227-1259.  doi: 10.1088/1361-6544/aa9d5f.
    [7] Y. Giga, Solutions for semilinear parabolic equations in $L^p$ and regularity of weak solutions of the Navier–Stokes system, J. Differential Equations, 61 (1986), 186-212.  doi: 10.1016/0022-0396(86)90096-3.
    [8] J. Gu and F. Meng, Some new nonlinear Volterra-Fredholm type dynamic integral inequalities on time scales, Appl. Math. Comput., 245 (2014), 235-242.  doi: 10.1016/j.amc.2014.07.056.
    [9] P. HeY. Wang and L. Zhao, A further study on a 3D chemotaxis-Stokes system with tensor-valued sensitivity, Appl. Math. Lett., 90 (2019), 23-29.  doi: 10.1016/j.aml.2018.09.019.
    [10] T. Hillen and K. Painter, A user's guide to PDE models for chemotaxis,, J. Math. Biol., 58 (2009), 183-217.  doi: 10.1007/s00285-008-0201-3.
    [11] D. Horstmann, From 1970 until present: the Keller–Segel model in chemotaxis and its consequences. I, Jahresber. Deutsch. Math.-Verein., 105 (2003), 103-165. 
    [12] S. Ishida, Global existence and boundedness for chemotaxis–Navier–Stokes system with position-dependent sensitivity in 2D bounded domains, Discrete Contin. Dyn. Syst., 32 (2015), 3463-3482.  doi: 10.3934/dcds.2015.35.3463.
    [13] S. IshidaK. Seki and T Yokota, Boundedness in quasilinear Keller–Segel systems of parabolic–parabolic type on non-convex bounded domains, J. Differential Equations, 256 (2014), 2993-3010.  doi: 10.1016/j.jde.2014.01.028.
    [14] Y. Ke and J. Zheng, An optimal result for global existence in a three-dimensional Keller–Segel–Navier–Stokes system involving tensor-valued sensitivity with saturation, Calc. Var. Partial Differential Equations, 58 (2019), 27pp. doi: 10.1007/s00526-019-1568-2.
    [15] E. Keller and L. Segel, Model for chemotaxis, J. Theor. Biol., 30 (1971), 225-234.  doi: 10.1016/0022-5193(71)90050-6.
    [16] A. Kiselev and L. Ryzhik, Biomixing by chemotaxis and enhancement of biological reactions, Comm. Partial Differential Equations, 37 (2012), 298-318.  doi: 10.1080/03605302.2011.589879.
    [17] A. Kiselev and L. Ryzhik, Biomixing by chemotaxis and efficiency of biological reactions: The critical reaction case, J. Math. Phys., 53 (2012), 9pp. doi: 10.1063/1.4742858.
    [18] J. LiP. Pang and Y. Wang, Global boundedness and decay property of a three-dimensional Keller–Segel–Stokes system modeling coral fertilization, Nonlinearity, 32 (2019), 2815-2847.  doi: 10.1088/1361-6544/ab159b.
    [19] Y. Li and Y. Li, Finite-time blow-up in higher dimensional fully-parabolic chemotaxis system for two species, Nonlinear Anal., 109 (2014), 72-84.  doi: 10.1016/j.na.2014.05.021.
    [20] X. LiY. Wang and Z. Xiang, Global existence and boundedness in a 2D Keller-Segel-Stokes system with nonlinear diffusion and rotational flux, Commun. Math. Sci., 14 (2016), 1889-1910.  doi: 10.4310/CMS.2016.v14.n7.a5.
    [21] J.-G. Liu and A. Lorz, A coupled chemotaxis–fluid model: Global existence, Ann. Inst. H. Poincaré Anal. Non Linéaire, 28 (2011), 643-652.  doi: 10.1016/j.anihpc.2011.04.005.
    [22] J. Liu and Y. Wang, Global weak solutions in a three-dimensional Keller-Segel-Navier-Stokes system involving a tensor-valued sensitivity with saturation, J. Differential Equations, 262 (2017), 5271-5305.  doi: 10.1016/j.jde.2017.01.024.
    [23] A. Lorz, Coupled chemotaxis fluid equations, Math. Models Methods Appl. Sci., 20 (2010), 987-1004.  doi: 10.1142/S0218202510004507.
    [24] K. Painter and T. Hillen, Volume-filling and quorum-sensing in models for chemosensitive movement, Can. Appl. Math. Q., 10 (2002), 501-543. 
    [25] Y. Peng and Z. Xiang, Global existence and boundedness in a 3D Keller–Segel–Stokes system with nonlinear diffusion and rotational flux, Z. Angew. Math. Phys., 68 (2017), 26pp. doi: 10.1007/s00033-017-0816-6.
    [26] B. Perthame, Transport Equations in Biology, Frontiers in Mathematics, Birkhäuser Verlag, Basel, 2007. doi: 10.1007/978-3-7643-7842-4.
    [27] J. Simon, Compact sets in the space $L^{p}(0, T; B)$, Ann. Mat. Pura Appl., 146 (1986), 65-96.  doi: 10.1007/BF01762360.
    [28] H. Sohr, The Navier–Stokes Equations. An Elementary Functional Analytic Approach, Birkhäuser Advanced Texts: Basel Textbooks, Birkhäuser Verlag, Basel, 2001. doi: 10.1007/978-3-0348-8255-2.
    [29] Y. Tao and M. Winkler, Boundedness in a quasilinear parabolic–parabolic Keller–Segel system with subcritical sensitivity, J. Differential Equations, 252 (2012), 692-715.  doi: 10.1016/j.jde.2011.08.019.
    [30] Y. Tao and M. Winkler, Locally bounded global solutions in a three-dimensional chemotaxis–Stokes system with nonlinear diffusion, Ann. Inst. H. Poincaré Anal. Non Linéaire, 30 (2013), 157-178.  doi: 10.1016/j.anihpc.2012.07.002.
    [31] Y. Tao and M. Winkler, Boundedness and decay enforced by quadratic degradation in a three-dimensional chemotaxis–fluid system, Z. Angew. Math. Phys., 66 (2015), 2555-2573.  doi: 10.1007/s00033-015-0541-y.
    [32] J. I. Tello and M. Winkler, A chemotaxis system with logistic source, Comm. Partial Differential Equations, 32 (2007), 849-877.  doi: 10.1080/03605300701319003.
    [33] I. Tuval, L. Cisneros and C. Dombrowski, et al., Bacterial swimming and oxygen transport near contact lines, Proc. Natl. Acad. Sci. USA, 102 (2005), 2277–2282. doi: 10.1073/pnas.0406724102.
    [34] Y. Wang and X. Cao, Global classical solutions of a 3D chemotaxis–Stokes system with rotation, Discrete Contin. Dyn. Syst. Ser. B, 20 (2015), 3235-3254.  doi: 10.3934/dcdsb.2015.20.3235.
    [35] Y. WangL. LiuX. Zhang and Y. Wu, Positive solutions of an abstract fractional semipositone differential system model for bioprocesses of HIV infection, Applied Math. Comput., 258 (2015), 312-324.  doi: 10.1016/j.amc.2015.01.080.
    [36] Y. Wang and Z. Xiang, Global existence and boundedness in a Keller–Segel–Stokes system involving a tensor-valued sensitivity with saturation, J. Differential Equations, 259 (2015), 7578-7609.  doi: 10.1016/j.jde.2015.08.027.
    [37] Y. Wang and Z. Xiang, Global existence and boundedness in a Keller-Segel-Stokes system involving a tensor-valued sensitivity with saturation: The 3D case, J. Differential Equations, 261 (2016), 4944-4973.  doi: 10.1016/j.jde.2016.07.010.
    [38] Y. WangM. Winkler and Z. Xiang, Global classical solutions in a two-dimensional chemotaxis–Navier–Stokes system with subcritical sensitivity, Ann. Sc. Norm. Super. Pisa Cl. Sci., 18 (2018), 421-466. 
    [39] M. Winkler, Boundedness in the higher-dimensional parabolic–parabolic chemotaxis system with logistic source, Comm. Partial Differential Equations, 35 (2010), 1516-1537.  doi: 10.1080/03605300903473426.
    [40] M. Winkler, Global large-data solutions in a chemotaxis–(Navier–)Stokes system modeling cellular swimming in fluid drops, Comm. Partial Differential Equations, 37 (2012), 319-351.  doi: 10.1080/03605302.2011.591865.
    [41] M. Winkler, Stabilization in a two-dimensional chemotaxis–Navier–Stokes system, Arch. Ration. Mech. Anal., 211 (2014), 455-487.  doi: 10.1007/s00205-013-0678-9.
    [42] M. Winkler, Boundedness and large time behavior in a three-dimensional chemotaxis–Stokes system with nonlinear diffusion and general sensitivity, Calc. Var. Partial Differential Equations, 54 (2015), 3789-3828.  doi: 10.1007/s00526-015-0922-2.
    [43] M. Winkler, Global weak solutions in a three-dimensional chemotaxis–Navier–Stokes system, Ann. Inst. H. Poincaré Anal. Non Linéaire, 33 (2016), 1329–-1352. doi: 10.1016/j.anihpc.2015.05.002.
    [44] M. Winkler, Does fluid interaction affect regularity in the three-dimensional Keller-Segel System with saturated sensitivity?, J. Math. Fluid Mech., 20 (2018), 1889-1909.  doi: 10.1007/s00021-018-0395-0.
    [45] M. Winkler and K. C. Djie, Boundedness and finite-time collapse in a chemotaxis system with volume-filling effect, Nonlinear Anal., 72 (2010), 1044-1064.  doi: 10.1016/j.na.2009.07.045.
    [46] F. Xu and L. Liu, On the well-posedness of the incompressible flow in porous media, J. Nonlinear Sci. Appl., 9 (2016), 6371-6381.  doi: 10.22436/jnsa.009.12.37.
    [47] C. Xue and H. G. Othmer, Multiscale models of taxis-driven patterning in bacterial populations, SIAM J. Appl. Math., 70 (2009), 133-167.  doi: 10.1137/070711505.
    [48] Q. Zhang and X. Zheng, Global well-posedness for the two-dimensional incompressible chemotaxis–Navier–Stokes equations, SIAM J. Math. Anal., 46 (2014), 3078-3105.  doi: 10.1137/130936920.
    [49] J. Zheng, Boundedness of solutions to a quasilinear parabolic–elliptic Keller–Segel system with logistic source, J. Differential Equations, 259 (2015), 120-140.  doi: 10.1016/j.jde.2015.02.003.
    [50] J. Zheng, Boundedness of solutions to a quasilinear parabolic–parabolic Keller–Segel system with a logistic source, J. Math. Anal. Appl., 431 (2015), 867-888.  doi: 10.1016/j.jmaa.2015.05.071.
    [51] J. Zheng, A note on boundedness of solutions to a higher-dimensional quasi-linear chemotaxis system with logistic source, ZAMM Z. Angew. Math. Mech., 97 (2017), 414-421.  doi: 10.1002/zamm.201600166.
    [52] J. Zheng, Global weak solutions in a three-dimensional Keller-Segel-Navier-Stokes system with nonlinear diffusion, J. Differential Equations, 263 (2017), 2606-2629.  doi: 10.1016/j.jde.2017.04.005.
    [53] J. Zheng, Boundedness in a two-species quasi-linear chemotaxis system with two chemicals, Topol. Methods Nonlinear Anal., 49 (2017), 463-480.  doi: 10.12775/TMNA.2016.082.
    [54] J. Zheng, An optimal result for global existence and boundedness in a three-dimensional Keller-Segel-Stokes system with nonlinear diffusion, J. Differential Equations, 267 (2019), 2385-2415.  doi: 10.1016/j.jde.2019.03.013.
    [55] J. Zheng, A new result for the global boundedness and decay property of a three-dimensional Keller-Segel-Stokes system modeling coral fertilization, preprint.
    [56] J. Zheng, et. al., A new result for global existence and boundedness of solutions to a parabolic–parabolic Keller–Segel system with logistic source, J. Math. Anal. Appl., 462 (2018), 1–25. doi: 10.1016/j.jmaa.2018.01.064.
    [57] J. Zheng and Y. Wang, A note on global existence to a higher-dimensional quasilinear chemotaxis system with consumption of chemoattractant, Discrete Contin. Dyn. Syst. Ser. B, 22 (2017), 669-686.  doi: 10.3934/dcdsb.2017032.
  • 加载中
SHARE

Article Metrics

HTML views(2695) PDF downloads(291) Cited by(0)

Access History

Other Articles By Authors

Catalog

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return