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August  2019, 24(8): 3569-3590. doi: 10.3934/dcdsb.2018279

Global attractors for weak solutions of the three-dimensional Navier-Stokes equations with damping

Daniel Pardo 1, , José Valero 2,, and  Ángel Giménez 2,

1. 

Miquel Rosselló i Alemany, 51, 7 B, Palma de Mallorca, Spain
2. 

Universidad Miguel Hernández de Elche, Centro de Investigación Operativa, 03202, Elche (Alicante), Spain

* Corresponding author: jvalero@umh.es

Dedicated to Professor Peter Kloeden on his 70th birthday

Received  March 2018 Revised  June 2018 Published  October 2018

Fund Project: This work has been partially supported by Spanish Ministry of Economy and Competitiveness and FEDER, projects MTM2015-63723-P and MTM2016-74921-P, and by Junta de Andalucía (Spain), project P12-FQM-1492.

In this paper we obtain the existence of global attractors for the dynamicalsystems generated by weak solution of the three-dimensional Navier-Stokesequations with damping. We consider two cases, depending on the values of the parameter β controlling the damping term. First, we prove that for β≥4 weaksolutions are unique and establish the existence of the global attractor forthe corresponding semigroup. Second, for 3≤β<4 we define amultivalued dynamical systems and prove the existence of the global attractoras well. Finally, some numerical simulations are performed.

Keywords: Three-dimensional Navier-Stokes equations with damping, global attractors, set-valued dynamical systems, asymptotic behaviour, turbulence.
Mathematics Subject Classification: 35B40, 35B41, 35K55, 35Q30, 37B25, 58C06.
Citation: Daniel Pardo, José Valero, Ángel Giménez. Global attractors for weak solutions of the three-dimensional Navier-Stokes equations with damping. Discrete & Continuous Dynamical Systems - B, 2019, 24 (8) : 3569-3590. doi: 10.3934/dcdsb.2018279
References:
[1]

D. Bresch and B. Desjardins, Existence of global weak solutions for a 2D viscous shallow water equations and convergence to the quasi-geostrophic model, Commun. Math. Phys., 238 (2003), 211-223.  doi: 10.1007/s00220-003-0859-8.  Google Scholar

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X. Cai and Q. Jiu, Weak and strong solutions for the incompressible Navier-Stokes equations with damping, J. Math. Anal. Appl., 343 (2008), 799-809.  doi: 10.1016/j.jmaa.2008.01.041.  Google Scholar

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V. V. Chepyzhov and M. I. Vishik, Attractors for Equations of Mathematical Physics, American Mathematical Society, Providence, Rhode Island, 2002.  Google Scholar

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J. H. Ferziger and M. Peric, Computational Methods for Fluid Dynamics, Springer-Verlag, Berlin, 1999. doi: 10.1007/978-3-642-98037-4.  Google Scholar

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M. Gobbino and M. Sardella, On the connectedness of attractors for dynamical systems, J. Differential Equations, 133 (1997), 1-14.  doi: 10.1006/jdeq.1996.3166.  Google Scholar

[6]

O. V. Kapustyan, P. O. Kasyanov and J. Valero, Structure and regularity of the global attractor of a reacction-diffusion equation with non-smooth nonlinear term, Discrete Contin. Dyn. Syst. Ser. A, 34 (2014), 4155-4182.  doi: 10.3934/dcds.2014.34.4155.  Google Scholar

[7]

O. V. Kapustyan, P. O. Kasyanov, J. Valero and M. Z. Zgurovsky, Structure of uniform global attractors for general non-autonomous reaction-diffusion systems, in Continuous and Distributed Systems. Theory and Applications, M.Z.Zgurovsky and V.A. Sadovnichiy eds, 211 (2014), 163-180, Cham, Springer. doi: 10.1007/978-3-319-03146-0_12.  Google Scholar

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F. Huang and R. Pan, Convergence rate for compressible Euler equations with damping and vacuum, Arch. Rational Mech. Anal., 166 (2003), 359-376.  doi: 10.1007/s00205-002-0234-5.  Google Scholar

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Y. Kim and K. Li, Time-periodic strong solutions of the 3D Navier-Stokes equations with damping, Electron. J. Differential Equations, 2017 (2017), 1-11.   Google Scholar

[10] O. A. Ladyzhenskaya, Attractors for Semigroups and Evolution Equations, Cambridge University Press, Cambridge, New-York, 1991.  doi: 10.1017/CBO9780511569418.  Google Scholar
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J. L. Lions, Quelques Méthodes de Résolution des Problèmes Aux Limites Non Linéaires, Gauthier-Villar, Paris, 1969.  Google Scholar

[12]

A. A. Linninger, M. Xenos, D. C. Zhu, M. R. Somayaji, S. Kondapali and R. D. Penn, Cerebrospinal fluid flow in the normal and hydrocefalic human brain, IEEE Trans. Biomed. Eng., 54 (2007), 291-302.   Google Scholar

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V. S. Valero and J. Melnik AND, On attractors of multi-valued semi-flows and differential inclusions, Set-Valued Anal., 6 (1998), 83-111.  doi: 10.1023/A:1008608431399.  Google Scholar

[14] J. Robinson, Infinite-dimensional Dynamical Systems, Cambridge University Press, Cambridge, 2001.  doi: 10.1007/978-94-010-0732-0.  Google Scholar
[15]

X. Song and Y. Hou, Attractors for the three-dimensional incompressible Navier-Stokes equations with damping, Discrete Contin. Dyn. Syst. Ser. A, 31 (2011), 239-252.  doi: 10.3934/dcds.2011.31.239.  Google Scholar

[16]

X. Song and Y. Hou, Uniform attractors for the three-dimensional Navier-Stokes equations with nonlinear damping, J. Math. Anal. Appl., 422 (2015), 337-351.  doi: 10.1016/j.jmaa.2014.08.044.  Google Scholar

[17]

X. Song, F. Liang and J. Wu, Pullback D-attractors for three-dimensional Navier-Stokes equations with nonlinear damping, Bound. Value Probl., 2016 (2016), 15PP.  doi: 10.1186/s13661-016-0654-z.  Google Scholar

[18]

R. Temam, Navier-Stokes Equations, North-Holland, Amsterdam, 1979.  Google Scholar

[19]

R. Temam, Infinite-dimensional Dynamical Systems in Mechanics and Physics, SpringerVerlag, New York, 1988. doi: 10.1007/978-1-4684-0313-8.  Google Scholar

[20]

J. Valero, On locally compact attractors of dynamical systems, J. Math. Anal. Appl., 237 (1999), 43-54.  doi: 10.1006/jmaa.1999.6446.  Google Scholar

[21]

H. Versteeg and W. Malalasekra, An Introduction to Computational Fluid Dynamics: The Finite Volume Method, Prentice Hall, New York, 2007. Google Scholar

[22]

W. Wang and G. Zhou, Remarks on the regularity criterion of the Navier-Stokes equations with nonlinear damping, Math. Probl. Eng., 2015 (2015), Art. ID 310934, 5 pp. doi: 10.1155/2015/310934.  Google Scholar

[23]

Z. Zhang, X. Wu and M. Lu, On the uniqueness of strong solution to the incompressible Navier-Stokes equations with damping, J. Math. Anal. Appl., 377 (2011), 414-419.  doi: 10.1016/j.jmaa.2010.11.019.  Google Scholar

[24]

X. Zhong, Global well-posedness to the incompressible Navier-Stokes equations with damping, Electron. J. Qual. Theory Differ. Equ., 62 (2017), 1-9.   Google Scholar

[25]

Y. Zhou, Regularity and uniqueness for the 3D incompressible Navier-Stokes equations with damping, Appl. Math. Letters, 25 (2012), 1822-1825.  doi: 10.1016/j.aml.2012.02.029.  Google Scholar

show all references

References:
[1]

D. Bresch and B. Desjardins, Existence of global weak solutions for a 2D viscous shallow water equations and convergence to the quasi-geostrophic model, Commun. Math. Phys., 238 (2003), 211-223.  doi: 10.1007/s00220-003-0859-8.  Google Scholar

[2]

X. Cai and Q. Jiu, Weak and strong solutions for the incompressible Navier-Stokes equations with damping, J. Math. Anal. Appl., 343 (2008), 799-809.  doi: 10.1016/j.jmaa.2008.01.041.  Google Scholar

[3]

V. V. Chepyzhov and M. I. Vishik, Attractors for Equations of Mathematical Physics, American Mathematical Society, Providence, Rhode Island, 2002.  Google Scholar

[4]

J. H. Ferziger and M. Peric, Computational Methods for Fluid Dynamics, Springer-Verlag, Berlin, 1999. doi: 10.1007/978-3-642-98037-4.  Google Scholar

[5]

M. Gobbino and M. Sardella, On the connectedness of attractors for dynamical systems, J. Differential Equations, 133 (1997), 1-14.  doi: 10.1006/jdeq.1996.3166.  Google Scholar

[6]

O. V. Kapustyan, P. O. Kasyanov and J. Valero, Structure and regularity of the global attractor of a reacction-diffusion equation with non-smooth nonlinear term, Discrete Contin. Dyn. Syst. Ser. A, 34 (2014), 4155-4182.  doi: 10.3934/dcds.2014.34.4155.  Google Scholar

[7]

O. V. Kapustyan, P. O. Kasyanov, J. Valero and M. Z. Zgurovsky, Structure of uniform global attractors for general non-autonomous reaction-diffusion systems, in Continuous and Distributed Systems. Theory and Applications, M.Z.Zgurovsky and V.A. Sadovnichiy eds, 211 (2014), 163-180, Cham, Springer. doi: 10.1007/978-3-319-03146-0_12.  Google Scholar

[8]

F. Huang and R. Pan, Convergence rate for compressible Euler equations with damping and vacuum, Arch. Rational Mech. Anal., 166 (2003), 359-376.  doi: 10.1007/s00205-002-0234-5.  Google Scholar

[9]

Y. Kim and K. Li, Time-periodic strong solutions of the 3D Navier-Stokes equations with damping, Electron. J. Differential Equations, 2017 (2017), 1-11.   Google Scholar

[10] O. A. Ladyzhenskaya, Attractors for Semigroups and Evolution Equations, Cambridge University Press, Cambridge, New-York, 1991.  doi: 10.1017/CBO9780511569418.  Google Scholar
[11]

J. L. Lions, Quelques Méthodes de Résolution des Problèmes Aux Limites Non Linéaires, Gauthier-Villar, Paris, 1969.  Google Scholar

[12]

A. A. Linninger, M. Xenos, D. C. Zhu, M. R. Somayaji, S. Kondapali and R. D. Penn, Cerebrospinal fluid flow in the normal and hydrocefalic human brain, IEEE Trans. Biomed. Eng., 54 (2007), 291-302.   Google Scholar

[13]

V. S. Valero and J. Melnik AND, On attractors of multi-valued semi-flows and differential inclusions, Set-Valued Anal., 6 (1998), 83-111.  doi: 10.1023/A:1008608431399.  Google Scholar

[14] J. Robinson, Infinite-dimensional Dynamical Systems, Cambridge University Press, Cambridge, 2001.  doi: 10.1007/978-94-010-0732-0.  Google Scholar
[15]

X. Song and Y. Hou, Attractors for the three-dimensional incompressible Navier-Stokes equations with damping, Discrete Contin. Dyn. Syst. Ser. A, 31 (2011), 239-252.  doi: 10.3934/dcds.2011.31.239.  Google Scholar

[16]

X. Song and Y. Hou, Uniform attractors for the three-dimensional Navier-Stokes equations with nonlinear damping, J. Math. Anal. Appl., 422 (2015), 337-351.  doi: 10.1016/j.jmaa.2014.08.044.  Google Scholar

[17]

X. Song, F. Liang and J. Wu, Pullback D-attractors for three-dimensional Navier-Stokes equations with nonlinear damping, Bound. Value Probl., 2016 (2016), 15PP.  doi: 10.1186/s13661-016-0654-z.  Google Scholar

[18]

R. Temam, Navier-Stokes Equations, North-Holland, Amsterdam, 1979.  Google Scholar

[19]

R. Temam, Infinite-dimensional Dynamical Systems in Mechanics and Physics, SpringerVerlag, New York, 1988. doi: 10.1007/978-1-4684-0313-8.  Google Scholar

[20]

J. Valero, On locally compact attractors of dynamical systems, J. Math. Anal. Appl., 237 (1999), 43-54.  doi: 10.1006/jmaa.1999.6446.  Google Scholar

[21]

H. Versteeg and W. Malalasekra, An Introduction to Computational Fluid Dynamics: The Finite Volume Method, Prentice Hall, New York, 2007. Google Scholar

[22]

W. Wang and G. Zhou, Remarks on the regularity criterion of the Navier-Stokes equations with nonlinear damping, Math. Probl. Eng., 2015 (2015), Art. ID 310934, 5 pp. doi: 10.1155/2015/310934.  Google Scholar

[23]

Z. Zhang, X. Wu and M. Lu, On the uniqueness of strong solution to the incompressible Navier-Stokes equations with damping, J. Math. Anal. Appl., 377 (2011), 414-419.  doi: 10.1016/j.jmaa.2010.11.019.  Google Scholar

[24]

X. Zhong, Global well-posedness to the incompressible Navier-Stokes equations with damping, Electron. J. Qual. Theory Differ. Equ., 62 (2017), 1-9.   Google Scholar

[25]

Y. Zhou, Regularity and uniqueness for the 3D incompressible Navier-Stokes equations with damping, Appl. Math. Letters, 25 (2012), 1822-1825.  doi: 10.1016/j.aml.2012.02.029.  Google Scholar

Figure 1.  Flow domain
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Figure 2.  Flow velocity $u$ for the steady state in the $xy$-section at $z = 0$. The darker areas mean lower fluid flow speed. The initial velocity $u_{0}$ is identically zero. Left panel parameters: $\alpha = 0.2;\, \beta = 1$. Right panel parameters: $\alpha = 0.5;\, \beta = 1$
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Figure 3.  Flow velocity $u$ for the steady state in the $xy$-section at $z = 0$. The darker areas mean lower fluid flow speed. The initial velocity $u_{0}$ is identically zero. Left panel parameters: $\alpha = 0.2;\, \beta = 2$. Right panel parameters: $\alpha = 0.5;\, \beta = 2$
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Figure 4.  Flow velocity $u$ for the steady state in the $xy$-section at $z = 0$. The darker areas mean lower fluid flow speed. The initial velocity $u_{0}$ is identically zero. Left panel parameters: $\alpha = 0.2;\, \beta = 4$. Right panel parameters: $\alpha = 0.5;\, \beta = 4$
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Figure 5.  Flow velocity $u$ in the $xy$-section at $z = 0$ for $\alpha = 0.2$ and $\beta = 1$. The darker areas mean lower fluid flow speed. The initial velocity $u_{0} = (1, 0, 0)$. Left panel: state when $t = 0.1$. Right panel: steady state ($t$ large enough)
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