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doi: 10.3934/dcdsb.2020344

Codimension one and two bifurcations in Cattaneo-Christov heat flux model

Zhouchao Wei 1,, , Wei Zhang 2, , Irene Moroz 3, and  Nikolay V. Kuznetsov 4,

1. 

School of Mathematics and Physics, China University of Geosciences, Wuhan, Hubei 430074, China, Zhejiang Institute, China University of Geosciences, Hangzhou, Zhejiang 311305, China
2. 

College of Mechanical Engineering, Beijing University of Technology, Beijing, 100124, China
3. 

Mathematical Institute, University of Oxford, Oxford OX2 6GG, England
4. 

Faculty of Mathematics and Mechanics, St. Petersburg State University, Peterhof, St. Petersburg, Russia, Faculty of Information Technology, University of Jyväskylä, Jyväskylä, Finland

* Corresponding author: weizhouchao@163.com

Received  May 2020 Revised  October 2020 Published  November 2020

Fund Project: The first author is supported by National Natural Science Foundation of China (Grant No. 11772306), Zhejiang Provincial Natural Science Foundation of China under Grant (No.LY20A020001), and the Fundamental Research Funds for the Central Universities, China University of Geosciences (CUGGC05). The second author is supported by National Natural Science Foundation of China (Grant No. 11832002). The last author is supported by the Russian Leading Scientific School (Center of Excellence) program (2624.2020.1)

Layek and Pati (Phys. Lett. A, 2017) studied a nonlinear system of five coupled equations, which describe thermal relaxation in Rayleigh-Benard convection of a Boussinesq fluid layer, heated from below. Here we return to that paper and use techniques from dynamical systems theory to analyse the codimension-one Hopf bifurcation and codimension-two double-zero Bogdanov-Takens bifurcation. We determine the stability of the bifurcating limit cycle, and produce an unfolding of the normal form for codimension-two bifurcation for the Layek and Pati's model.

Keywords: Cattaneo-Christov heat-flux model, Hopf bifurcation, Bogdanov-Takens bifurcation, limit cycle, homoclinic bifurcation.
Mathematics Subject Classification: Primary: 34D20, 34D45; Secondary: 34K18.
Citation: Zhouchao Wei, Wei Zhang, Irene Moroz, Nikolay V. Kuznetsov. Codimension one and two bifurcations in Cattaneo-Christov heat flux model. Discrete & Continuous Dynamical Systems - B, doi: 10.3934/dcdsb.2020344
References:
[1]

F. A. Carrillo, F. Verduzco and J. Delgado, Analysis of the Takens-Bogdanov bifurcation on m-parameter ized vector fields, International Journal of Bifurcation and Chaos, 20 (2010), 995-1005.  doi: 10.1142/S0218127410026277.  Google Scholar

[2]

C. C. Daumann and P. C. Rech, Hyperchaos in convection with the Cattaneo-Christov heat-flux model, European Physical Journal B: Condensed Matter and Complex Systems, 92 (2019), 1-5. Google Scholar

[3]

J. Guckenheimer and P. Holmes, Nonlinear Oscillations, Dynamical Systems and Bifurcations of Vector Fields, Springer, New York. 1983. doi: 10.1007/978-1-4612-1140-2.  Google Scholar

[4]

Yu. A. Kuznetsov, Numerical normalization techniques for all codim 2 bifurcations of equilibria in ODE's, SIAM Journal on Numerical Analysis, 36 (1999), 1104-1124.  doi: 10.1137/S0036142998335005.  Google Scholar

[5]

Yu. A. Kuznetsov, Elements of Applied Bifurcation Theory, 3rd Edition, Springer, New York, 2004. doi: 10.1007/978-1-4757-3978-7.  Google Scholar

[6]

G. C. Layek and N. C. Pati, Bifurcations and chaos in convection taking non-Fourier heat-flux, Physics Letters A, 381 (2017), 3568-3575.  doi: 10.1016/j.physleta.2017.09.020.  Google Scholar

[7]

E. N. Lorenz, Deterministic nonperiodic flow, Journal of the Atmospheric Sciences, 20 (1963), 130-141.  doi: 10.1175/1520-0469(1963)020<0130:DNF>2.0.CO;2.  Google Scholar

[8]

E. N. Lorenz, Irregularity: A fundamental property of the atmosphere, Tellus A: Dynamic Meteorology and Oceanography, 36 (1984), 98-110.  doi: 10.3402/tellusa.v36i2.11473.  Google Scholar

[9]

S. Moon, J. M. Seo, B.-S. Han, J. Park and J.-J. Baik, A physically extended Lorenz system, Chaos, 29 (2019), 063129. doi: 10.1063/1.5095466.  Google Scholar

[10]

L. Stenflo, Generalized Lorenz equations for acoustic-gravity waves in the atmosphere, Physica Scripta, 53 (1996), 83-84.  doi: 10.1088/0031-8949/53/1/015.  Google Scholar

[11]

J. Sotomayor, L. F. Mello and D. D. C. Braga, Bifurcation analysis of the Watt governor system, Computational and Applied Mathematics, 26 (2007), 19-44.  doi: 10.1590/S0101-82052007000100002.  Google Scholar

[12]

Z. Wei and W. Zhang, Hidden hyperchaotic attractors in a modified Lorenz-Stenflo system with only one stable equilibrium, International Journal of Bifurcation and Chaos, 24 (2014), 1450127, 14 pp. doi: 10.1142/S0218127414501272.  Google Scholar

show all references

References:
[1]

F. A. Carrillo, F. Verduzco and J. Delgado, Analysis of the Takens-Bogdanov bifurcation on m-parameter ized vector fields, International Journal of Bifurcation and Chaos, 20 (2010), 995-1005.  doi: 10.1142/S0218127410026277.  Google Scholar

[2]

C. C. Daumann and P. C. Rech, Hyperchaos in convection with the Cattaneo-Christov heat-flux model, European Physical Journal B: Condensed Matter and Complex Systems, 92 (2019), 1-5. Google Scholar

[3]

J. Guckenheimer and P. Holmes, Nonlinear Oscillations, Dynamical Systems and Bifurcations of Vector Fields, Springer, New York. 1983. doi: 10.1007/978-1-4612-1140-2.  Google Scholar

[4]

Yu. A. Kuznetsov, Numerical normalization techniques for all codim 2 bifurcations of equilibria in ODE's, SIAM Journal on Numerical Analysis, 36 (1999), 1104-1124.  doi: 10.1137/S0036142998335005.  Google Scholar

[5]

Yu. A. Kuznetsov, Elements of Applied Bifurcation Theory, 3rd Edition, Springer, New York, 2004. doi: 10.1007/978-1-4757-3978-7.  Google Scholar

[6]

G. C. Layek and N. C. Pati, Bifurcations and chaos in convection taking non-Fourier heat-flux, Physics Letters A, 381 (2017), 3568-3575.  doi: 10.1016/j.physleta.2017.09.020.  Google Scholar

[7]

E. N. Lorenz, Deterministic nonperiodic flow, Journal of the Atmospheric Sciences, 20 (1963), 130-141.  doi: 10.1175/1520-0469(1963)020<0130:DNF>2.0.CO;2.  Google Scholar

[8]

E. N. Lorenz, Irregularity: A fundamental property of the atmosphere, Tellus A: Dynamic Meteorology and Oceanography, 36 (1984), 98-110.  doi: 10.3402/tellusa.v36i2.11473.  Google Scholar

[9]

S. Moon, J. M. Seo, B.-S. Han, J. Park and J.-J. Baik, A physically extended Lorenz system, Chaos, 29 (2019), 063129. doi: 10.1063/1.5095466.  Google Scholar

[10]

L. Stenflo, Generalized Lorenz equations for acoustic-gravity waves in the atmosphere, Physica Scripta, 53 (1996), 83-84.  doi: 10.1088/0031-8949/53/1/015.  Google Scholar

[11]

J. Sotomayor, L. F. Mello and D. D. C. Braga, Bifurcation analysis of the Watt governor system, Computational and Applied Mathematics, 26 (2007), 19-44.  doi: 10.1590/S0101-82052007000100002.  Google Scholar

[12]

Z. Wei and W. Zhang, Hidden hyperchaotic attractors in a modified Lorenz-Stenflo system with only one stable equilibrium, International Journal of Bifurcation and Chaos, 24 (2014), 1450127, 14 pp. doi: 10.1142/S0218127414501272.  Google Scholar

Figure 1.  When $ \sigma = 10, r = 28, \delta = 15, b = 3 $ and initial condition is $ (5.1, 6.2, 7.3, 8.4, 9.5) $, chaotic attractors are shown and corresponding Lyapunov exponents are (0.9263, -0.0000, -11.8503, -14.3371, -14.7389): (a) X-Y-Z space; (b) Z-P-W space
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Figure 2.  (a) Let $ (\sigma, b) = (10, 8/3) $. The equilibrium $ O $ of system (1) is asymptotically stable in the green region; the equilibria $ E_{1,2} $ of system (1) is asymptotically stable in the yellow region
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Figure 3.  First Lyapunov coefficient $ l_1 $ will be negative for $ \sigma = 10, b = 8/3, 0<\delta <10/11 $
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Figure 4.  Stable periodic orbit near $ O $ of system (1) from Hopf bifurcation with parameter values $ (\sigma, b, r, \delta) = (10, 8/3, 0.53, 0.5) $, and initial values $ (0.002, 0.002, 0.001, 0.02, 0.001) $ : (a) stable periodic orbit; (b) time series of state variables
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Figure 5.  Stable periodic orbit near $ E_1 $ of system (1) from Hopf bifurcation with parameter values $ (\sigma, b, r, \delta) = (10, 8/3, 4.92, 0.5) $, and initial values $ (1.65, 1.6, 9, -6.5, 2.6) $: (a) stable periodic orbit; (b) time series of state variables
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Figure 6.  Stable periodic orbit near $ E_1 $ of system (1) from Hopf bifurcation with parameter values $ (\sigma, b, r, \delta) = (10, 8/3, 6.638712, 1.5268) $, and initial values $ (2.33,2.46,10.41,-10.90,9.59) $ : (a) stable periodic orbit; (b) time series of state variables
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Figure 7.  Bogdanov-Takens bifurcation of system (25)
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