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Global existence and regularity in a three-dimensional Keller-Segel-Navier-Stokes system with indirect signal production

  • *Corresponding author: Jianing Xie

    *Corresponding author: Jianing Xie

The first author is supported by [Shandong Provincial Natural Science Foundation (No. ZR2022JQ06) and the National Natural Science Foundation of China (No. 11601215)]. The Corresponding author is supported by [the Program Funded by Liaoning Province Education Administration (No. LJ212410173063) and the National Natural Science Foundation of China (No. 12401248)].

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  • We consider a degenerate quasilinear Keller-Segel-Navier-Stokes system with indirect signal production

    $\begin{align} \left\{ \begin{array}{l} n_t+u\cdot\nabla n = \Delta n^m-\nabla\cdot( nS(x,n,v)\nabla v),\quad x\in \Omega, t>0,\\ { }{ v_{ t}+u\cdot\nabla v = \Delta v-v+w},\quad x\in \Omega, t>0,\\ { }{w_{t}+u\cdot\nabla w = \Delta w-w+n},\quad x\in \Omega, t>0,\\ u_t+\kappa(u \cdot \nabla)u+\nabla P = \Delta u+n\nabla \phi,\quad x\in \Omega, t>0,\\ \nabla\cdot u = 0,\quad x\in \Omega, t>0\\ \end{array}\right. \end{align} \quad\quad\quad (KSNF)$

    in a bounded domain $ \Omega\subseteq \mathbb{R}^3 $ with a smooth boundary, where $ m>0,\kappa\in \mathbb{R} $ is a given constant, $ \phi\in W^{2,\infty}(\Omega) $. Here, $ S(x,n, v) $ is a given parameter matrix on $ \Omega\times[0,\infty)^2 $ whose Frobenius norm satisfies $ |S(x,n,v)|\leq C_S(1+n)^{-\alpha} $ with $ C_S>0 $ and $ \alpha\geq0 $. It is shown that whenever $ m +\alpha> \frac{5}{4} $, for any nonnegative initial data which is sufficiently smooth, the corresponding Neumann-Neumann-Neumann-Dirichlet initial-boundary problem possesses at least one globally weak solution, and that this solution is uniformly bounded with respect to the norm in $ L^1(\Omega)\times L^2(\Omega)\times L^2(\Omega)\times L^2(\Omega; \mathbb{R}^3) $. This work improves previous results of several other authors (see Remark 1.1).

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

    Citation:

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  • [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] T. Black, Global very weak solutions to a chemotaxis-fluid system with nonlinear diffusion, SIAM J. Math. Anal., 50 (2018), 4087-4116.  doi: 10.1137/17M1159488.
    [3] T. Black, Global solvability of chemotaxis-fluid systems with nonlinear diffusion and matrix-valued sensitivities in three dimensions, Nonlinear Anal., 180 (2019), 129-153.  doi: 10.1016/j.na.2018.10.003.
    [4] X. Cao, Fluid interaction does not affect the critical exponent in a three-dimensional Keller-Segel-Stokes model, Z. Angew. Math. Phys., 71 (2020), 61.  doi: 10.1007/s00033-020-1285-x.
    [5] X. Cao and X. Gao, Critical mass in a quasilinear parabolic-elliptic Keller-Segel model, J. Diff. Eqns., 361 (2023), 449-471.  doi: 10.1016/j.jde.2023.03.005.
    [6] T. Cieślak and C. Stinner, Finite-time blowup and global-in-time unbounded solutions to a parabolic-parabolic quasilinearKeller-Segel system in higher dimensions, J. Diff. Eqns., 252 (2012), 5832-5851.  doi: 10.1016/j.jde.2012.01.045.
    [7] T. Cieślak and C. Stinner, New critical exponents in a fully parabolic quasilinear Keller-Segel system and applicationsto volume filling models, J. Diff. Eqns., 258 (2015), 2080-2113.  doi: 10.1016/j.jde.2014.12.004.
    [8] F. Dai, How far do indirect signal production mechanisms regularize the three-dimensional Keller-Segel-Stokes system?, Calculus Var. Partial Diff. Eqns., 62 (2023), 119.  doi: 10.1007/s00526-023-02461-2.
    [9] F. Dai and B. Liu, Global solvability and asymptotic stabilizationin a three-dimensional Keller-Segel-Navier-Stokessystem with indirect signal production, Math. Models Methods Appl. Sci., 31 (2021), 2091-2163.  doi: 10.1142/S0218202521500469.
    [10] F. Dai and B. Liu, Boundedness and asymptotic behavior in a Keller-Segel(-Navier)-Stokes system with indirect signal production, J. Diff. Eqns., 314 (2022), 201-250.  doi: 10.1016/j.jde.2022.01.015.
    [11] F. Dai and B. Liu, Global weak solutions in a three-dimensionalKeller-Segel-Navier-Stokes system with indirect signalproduction, J. Diff. Eqns., 333 (2022), 436-488.  doi: 10.1016/j.jde.2022.06.015.
    [12] M. Di FrancescoA. Lorz and P. Markowich, Chemotaxis-fluid coupled model for swimmingbacteria with nonlinear diffusion: Global existence and asymptotic behavior, Discrete Cont. Dyn. Syst., 28 (2010), 1437-1453. 
    [13] M. Ding and J. Lankeit, Generalized solutions to a chemotaxis-Navier-Stokes system with arbitrary superlinear degradation, SIAM J. Math. Anal., 54 (2022), 1022-1052.  doi: 10.1137/21M140907X.
    [14] M. Ding and W. Wang, Global boundedness in a quasilinear fully parabolic chemotaxis system with indirect signalproduction, Discrete Contin. Dyn. Syst., Ser. B., 24 (2019), 4665-4684.  doi: 10.3934/dcdsb.2018328.
    [15] J. FuhrmannJ. Lankeit and M. Winkler, A double critical mass phenomenon in a no-flux-Dirichlet Keller-Segel system, J. Math. PuresAppl., 162 (2022), 124-151.  doi: 10.1016/j.matpur.2022.04.004.
    [16] K. Fujie and T. Senba, Application of an Adams type inequality to a two-chemical substances chemotaxis system, J.Diff. Eqns., 263 (2017), 88-148.  doi: 10.1016/j.jde.2017.02.031.
    [17] K. Fujie and T. Senba, Blowup of solutions to a two-chemical substances chemotaxis system in the critical dimension, J. Diff. Eqns., 266 (2019), 942-976.  doi: 10.1016/j.jde.2018.07.068.
    [18] D. Horstmann and M. Winkler, Boundedness vs. blow-up in a chemotaxis system, J. Diff. Eqns., 215 (2005), 52-107.  doi: 10.1016/j.jde.2004.10.022.
    [19] B. Hu and Y. Tao, To the exclusion of blow-up in a three-dimensional chemotaxis growth model with indirect attractant production, Math. Models Methods Appl. Sci., 26 (2016), 2111-2128.  doi: 10.1142/S0218202516400091.
    [20] S. IshidaK. Seki and T. Yokota, Boundedness in quasilinear Keller-Segel systems of parabolic-parabolic type onnon-convex bounded domains, J. Diff. Eqns., 256 (2014), 2993-3010.  doi: 10.1016/j.jde.2014.01.028.
    [21] W. Jäger and S. Luckhaus, On explosions of solutions to a system of partial differential equations modellingchemotaxis, Trans. Am. Math. Soc., 329 (1992), 819-824.  doi: 10.1090/S0002-9947-1992-1046835-6.
    [22] C. Jin, Global solvability and boundedness to a coupled chemotaxis-fluidmodel with arbitrary porous medium diffusion, J. Diff. Eqns., 265 (2018), 332-353.  doi: 10.1016/j.jde.2018.02.031.
    [23] C. Jin, Global classical solution and stability to a coupled chemotaxis-fluid model with logistic source, Discrete Cont. Dyn. Syst., 38 (2018), 3547-3566.  doi: 10.3934/dcds.2018150.
    [24] C. Jin, Global classical solution to the chemotaxis-Navier-Stokes system with some realistic boundary conditions, Proc. Roya. Soci. Edin. Sect. A: Math., 154 (2024), 445-482.  doi: 10.1017/prm.2023.19.
    [25] E. Keller and L. Segel, Model for chemotaxis, J. Theor. Biol., 30 (1971), 225-234.  doi: 10.1016/0022-5193(71)90050-6.
    [26] J. Lankeit, Long-term behaviour in a chemotaxis-fluidsystem with logistic source, Math. Models Methods Appl. Sci., 26 (2016), 2071-2109.  doi: 10.1142/S021820251640008X.
    [27] F. Li and Y. Li, Global existence of weak solution in a chemotaxis-fluid system with nonlinear diffusion and rotational flux, Discrete Contin. Dyn. Syst., 24 (2019), 5409-5436.  doi: 10.3934/dcdsb.2019064.
    [28] D. LiC. Mu and P. Zheng, Boundedness and large time behavior in a quasilinear chemotaxis model for tumor invasion, Math. Models Methods Appl. Sci., 28 (2018), 1413-1451.  doi: 10.1142/S0218202518500380.
    [29] G. LiY. Tao and M. Winkler, Large time behavior in a predator-prey system with indirect pursuit-evasion interaction, Disc. Cont. Dyna. Syst. B., 25 (2020), 4383-4396.  doi: 10.3934/dcdsb.2020102.
    [30] M. Li and Z. Xiang, Convergence analysis from the indirect signal productionto the direct one, J. Diff. Eqns., 367 (2023), 834-889.  doi: 10.1016/j.jde.2023.05.033.
    [31] K. Osaki and A. Yagi, Finite dimensional attractors for one-dimensional Keller-Segel equations, Funkcial. Ekvac., 44 (2001), 441-469. 
    [32] J. Simon, Compact sets in the space $L^{p}(O, T; B)$, Annali di Matematica Pura ed Applicata, 146 (1987), 65-96.  doi: 10.1007/BF01762360.
    [33] Y. Tao and M. Winkler, Boundedness in a quasilinear parabolic-parabolic Keller-Segel system with subcritical sensitivity, J. Diff. Eqns., 252 (2012), 692-715.  doi: 10.1016/j.jde.2011.08.019.
    [34] J. I. Tello and D. Wrzosek, Predator-prey model with diffusion and indirect prey-taxis, Math. Models Methods Appl. Sci., 26 (2016), 2129-2162.  doi: 10.1142/S0218202516400108.
    [35] I. Tuval, L. Cisneros, 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.
    [36] Y. Wang, Global weak solutions in a three-dimensionalKeller-Segel-Navier-Stokes systemwith subcritical sensitivity, Math. Models Methods Appl. Sci., 27 (2017), 2745-2780.  doi: 10.1142/S0218202517500579.
    [37] Y. Wang and Z. Xiang, Global existence and boundedness in a Keller-Segel-Stokes system involving atensor-valued sensitivity with saturation, J. Diff. Eqns., 259 (2015), 7578-7609.  doi: 10.1016/j.jde.2015.08.027.
    [38] Y. Wang and Z. Xiang, Global existence and boundedness in a Keller-Segel-Stokes system involving a tensor-valuedsensitivity with saturation: The 3D case, J. Diff. Eqns., 261 (2016), 4944-4973.  doi: 10.1016/j.jde.2016.07.010.
    [39] Y. Wang and L. Yang, Boundedness in a chemotaxis-fluid system involvinga saturated sensitivity and indirect signalproduction mechanism, J. Diff. Eqns., 287 (2021), 460-490.  doi: 10.1016/j.jde.2021.04.001.
    [40] M. Winkler, Does a volume-filling effect always prevent chemotactic collapse?, Math. Methods Appl. Sci., 33 (2010), 12-24.  doi: 10.1002/mma.1146.
    [41] M. Winkler, Global large-data solutions in a chemotaxis–(Navier-)Stokes system modeling cellular swimming influid drops, Comm. Partial Diff. Eqns., 37 (2012), 319-351.  doi: 10.1080/03605302.2011.591865.
    [42] M. Winkler, Finite-time blow-up in the higher-dimensional parabolic-parabolic Keller-Segel system, J. Math. Pures Appl., 100 (2013), 748-767.  doi: 10.1016/j.matpur.2013.01.020.
    [43] M. Winkler, Boundedness and large time behavior in a three-dimensional chemotaxis–Stokes systemwith nonlinear diffusion and general sensitivity, Calculus Var. Partial Diff. Eqns., 54 (2015), 3789-3828.  doi: 10.1007/s00526-015-0922-2.
    [44] M. Winkler, Global weak solutions in a three-dimensional chemotaxis–Navier-Stokes system, Ann. Inst.H. Poincaré Anal. Non Linéaire, 33 (2016), 1329-1352. 
    [45] M. Winkler, Does fluid interaction affect regularity in the three-dimensional Keller-Segel System with saturated sensitivity?, J. Math. Fluid Mechanics, 20 (2018), 1889-1909.  doi: 10.1007/s00021-018-0395-0.
    [46] M. Winkler, A three-dimensional Keller-Segel-Navier-Stokes system with logistic source: global weak solutions and asymptotic stabilization, J. Func. Anal., 276 (2019), 1339-1401.  doi: 10.1016/j.jfa.2018.12.009.
    [47] M. Winkler, Boundedness in a three-dimensional Keller-Segel-Stokes system with subcritical sensitivity, Appl. Math. Lett., 112 (2021), 106785.  doi: 10.1016/j.aml.2020.106785.
    [48] M. Winkler, A family of mass-critical Keller-Segel systems, Proc. Lond. Math. Soc., 124 (2022), 133-181.  doi: 10.1112/plms.12425.
    [49] M. Winkler and K. C. Djie, Boundedness and finite-timecollapse in a chemotaxis system with volume-filling effect, Nonlinear Anal. TMA., 72 (2010), 1044-1064.  doi: 10.1016/j.na.2009.07.045.
    [50] Z. Xiang and L. Yang, Critical mass for the Cauchy problem of a chemotaxismodel with indirect signal production mechanism, J. Evol. Eqns., 25 (2025), 26.  doi: 10.1007/s00028-024-01053-7.
    [51] C. Xue and H. G. Othmer, Multiscale models of taxis-driven patterning in bacterial populations, SIAMJ. Appl. Math., 70 (2009), 133-167.  doi: 10.1137/070711505.
    [52] H. Ye and C. Jin, Global classical solutions for chemotaxis-fluids system with mixed boundary conditions, Z. Angew. Math. Phys., 74 (2023), 30.  doi: 10.1007/s00033-022-01924-4.
    [53] P. Yu, Blow-up prevention by saturated chemotactic sensitivity in a 2D Keller-Segel-Stokes system, Acta Appl. Math., 169 (2020), 475-497.  doi: 10.1007/s10440-019-00307-8.
    [54] W. ZhangP. Niu and S. Liu, Large time behavior in a chemotaxis model with logistic growth and indirect signalproduction, Nonlinear Anal., RWA., 50 (2019), 484-497.  doi: 10.1016/j.nonrwa.2019.05.002.
    [55] J. Zheng, Boundedness of solutions to a quasilinear parabolic-elliptic Keller-Segel system with logistic source, J. Diff. Eqns., 259 (2015), 120-140.  doi: 10.1016/j.jde.2015.02.003.
    [56] J. Zheng, Global weak solutions in a three-dimensional Keller-Segel-Navier-Stokes system with nonlinear diffusion, J. Diff. Eqns., 263 (2017), 2606-2629.  doi: 10.1016/j.jde.2017.04.005.
    [57] J. Zheng, An optimal result for global existence and boundedness in a three-dimensional Keller-Segel-Stokes system with nonlinear diffusion, J. Diff. Eqns., 267 (2019), 2385-2415.  doi: 10.1016/j.jde.2019.03.013.
    [58] J. Zheng, Eventual smoothness and stabilization in a three-dimensional Keller-Segel-Navier-Stokes system with rotational flux, Calculus Var. Partial Diff. Eqns., 61 (2022), 52.  doi: 10.1007/s00526-021-02164-6.
    [59] J. Zheng and Y. Ke, Global bounded weak solutions for a chemotaxis-Stokessystem with nonlinear diffusion and rotation, J. Diff. Eqns., 289 (2021), 182-235.  doi: 10.1016/j.jde.2021.04.020.
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