期刊文献+

Numerical simulation and analysis of complex patterns in a two-layer coupled reaction diffusion system

Numerical simulation and analysis of complex patterns in a two-layer coupled reaction diffusion system
下载PDF
导出
摘要 The resonance interaction between two modes is investigated using a two-layer coupled Brusselator model. When two different wavelength modes satisfy resonance conditions, new modes will appear, and a variety of superlattice patterns can be obtained in a short wavelength mode subsystem. We find that even though the wavenumbers of two Turing modes are fixed, the parameter changes have influences on wave intensity and pattern selection. When a hexagon pattern occurs in the short wavelength mode layer and a stripe pattern appears in the long wavelength mode layer, the Hopf instability may happen in a nonlinearly coupled model, and twinkling-eye hexagon and travelling hexagon patterns will be obtained. The symmetries of patterns resulting from the coupled modes may be different from those of their parents, such as the cluster hexagon pattern and square pattern. With the increase of perturbation and coupling intensity, the nonlinear system will con- vert between a static pattern and a dynamic pattern when the Turing instability and Hopf instability happen in the nonlinear system. Besides the wavenumber ratio and intensity ratio of the two different wavelength Turing modes, perturbation and coupling intensity play an important role in the pattern formation and selection. According to the simulation results, we find that two modes with different symmetries can also be in the spatial resonance under certain conditions, and complex patterns appear in the two-layer coupled reaction diffusion systems. The resonance interaction between two modes is investigated using a two-layer coupled Brusselator model. When two different wavelength modes satisfy resonance conditions, new modes will appear, and a variety of superlattice patterns can be obtained in a short wavelength mode subsystem. We find that even though the wavenumbers of two Turing modes are fixed, the parameter changes have influences on wave intensity and pattern selection. When a hexagon pattern occurs in the short wavelength mode layer and a stripe pattern appears in the long wavelength mode layer, the Hopf instability may happen in a nonlinearly coupled model, and twinkling-eye hexagon and travelling hexagon patterns will be obtained. The symmetries of patterns resulting from the coupled modes may be different from those of their parents, such as the cluster hexagon pattern and square pattern. With the increase of perturbation and coupling intensity, the nonlinear system will con- vert between a static pattern and a dynamic pattern when the Turing instability and Hopf instability happen in the nonlinear system. Besides the wavenumber ratio and intensity ratio of the two different wavelength Turing modes, perturbation and coupling intensity play an important role in the pattern formation and selection. According to the simulation results, we find that two modes with different symmetries can also be in the spatial resonance under certain conditions, and complex patterns appear in the two-layer coupled reaction diffusion systems.
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2015年第4期491-496,共6页 中国物理B(英文版)
基金 Project supported by the National Natural Science Foundation of China(Grant No.11247242) the Young Scientists Fund of the National Natural Science Foundation of China(Grant No.51201057) the Natural Science Foundation of Hebei Province,China(Grant No.A2014208171)
关键词 Brusselator model pattern formation Turing mode INSTABILITY : Brusselator model, pattern formation, Turing mode, instability
  • 相关文献

参考文献25

  • 1Turing A M 1952 Philos. Trans. R. Soc. London B 237 37.
  • 2Steinbock O, Kasper E and Müller S C 1999 J. Phys. Chem. A 103 3442.
  • 3Gomes M G 1999 Phys. Rev. E 60 3741.
  • 4David G M, Milos D, Irving E and Alberto P M 2011 Phys. Rev. E 84 046210.
  • 5Gao Z, Hu B and Hu G 2002 Phys. Rev. E 65 055204.
  • 6Epstein T and Fineberg J 2008 Phys. Rev. Lett. 100 134101.
  • 7Pampaloni E, Residori S, Soria S and Arecchi F T 1997 Phys. Rev. Lett. 78 1042.
  • 8Dong L F, Fan W L, He Y F, Liu F C, Li S F, Gao R L and Wang L 2006 Phys. Rev. E 73 066206.
  • 9Cai M C, Pan J T and Zhang H 2012 Phys. Rev. E 86 016208.
  • 10Barrio R A, Varea C, Aragon J L and Maini P K 1999 Bull. Math. Biol. 61 483.

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部