A Singularity Analysis Approach to the Solutions of Duffing’s Equation

  • T. Bountis
  • M. Bier
  • V. Papageorgiou
Conference paper
Part of the Research Reports in Physics book series (RESREPORTS)

Abstract

The singularity structure of Duffing’s equation in the complex t-plane is investigated analytically and numerically. A series expansion for the general solution around each singularity t* = tR+itI is given, and is subsequently used to approximate the locations of singularity “spirals” t * (n) , n = 1,2,…, around every t*. The main “chimney” patterns—on which singularities are observed to accumulate—are explained by deriving a simple expression for the distances between singularities on the “walls” of these chimneys |t*−t * (1) |∼Q−1/4exp(−tI/2), Q being the amplitude of the (periodic) driving force. Thus, singularity patterns are seen to further “condense”, as Q increases and the motion becomes globally more chaotic in real t. These results suggest that series expansions near singularities in the complex t-plane can provide useful representations of the general solution of Duffing’s equation.

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References

  1. [1]
    U. Frisch and R. Morf, Phys. Rev. A23 (5) (1981) 2673.ADSGoogle Scholar
  2. [2]
    M. Tabor and J. Weiss, Phys. Rev. A24 (1981) 2157.ADSGoogle Scholar
  3. [3]
    Y. F. Chang, M. Tabor and J. Weiss, J. Math. Phys. 23(4) (1982) 531; see also Y. F. Chang et al., Physica 8D (1983) 183.MathSciNetADSMATHCrossRefGoogle Scholar
  4. [4]
    T. Bountis in Singularities and Dynamical Systems, ed. S. Pnevmatikos (North Holland, Amsterdam, 1985 ).Google Scholar
  5. [5]
    A. Ramani, B. Grammatieos and B. Dorizzi, J. Math. Phys. 24 (1983) 2282; see also J. Math. Phys. 25 (1984) 481.MathSciNetADSCrossRefGoogle Scholar
  6. [6]
    T. Bountis, H. Segur and F. Vivaldi, Phys. Rev. A25 (1982) 1257.MathSciNetADSGoogle Scholar
  7. [7]
    T. Bountis, A. Ramani, B. Grammatieos and B. Dorizzi, Physica 128A (1984) 268.Google Scholar
  8. [8]
    S. L. Ziglin, Funct. Anal. Appl. 16 (1983) 181; also Funct. Anal. Appl. 17 (1983) 6.MATHCrossRefGoogle Scholar
  9. [9]
    S. L. Ziglin, Trans. Moscow Math. Soc. 1 (1982) 283.Google Scholar
  10. [10]
    H. Yoshida, Celestial Mech. 31 (1983) 363–379, 381–399; see also Physica 21D (1986) 18.MathSciNetADSMATHCrossRefGoogle Scholar
  11. [11]
    H. Ito, Kodai Math. J. 8 (1985) 120.MathSciNetMATHCrossRefGoogle Scholar
  12. [12]
    D. Rod, “On an Example of Ziglin in Hamiltonian Dynamics,” Conf. Proc. of Canad. Math. Soc. Vol. 8, ( AMS, Providence, R.I., 1987 ).Google Scholar
  13. [13]
    T. Bountis, V. Papageorgiou and M. Bier, Physica 24D (1987) 292.Google Scholar
  14. [14]
    A. Ramani, B. Grammatieos and T. Bountis, “The Painleve Property and Singularity Analysis of Integrable and Non-Integrable Systems,” Phys. Rep. 180 (3) (1989) 160.ADSCrossRefGoogle Scholar
  15. [15]
    M. Bier, Ph.D. Thesis, Department of Mathematics, Clarkson University, Potsdam, NY (1987).Google Scholar
  16. [16]
    H. T. Davis, Introduction to Nonlinear Differential and Integral Equations ( Dover, London, 1962 ).MATHGoogle Scholar
  17. [17]
    M. Lieberman and A. Lichtenberg, Regular and Stochastic Motion ( Springer, Berlin, 1983 ).MATHGoogle Scholar
  18. [18]
    E. T. Copson, An Introduction to the Theory of Functions of a Complex Variable (Oxford Press, 1935 ).Google Scholar
  19. [19]
    J. D. Fournier, G. Levine and M. Tabor, J. Phys. A: Math. Gen. 21 (1988) 33.MathSciNetADSMATHCrossRefGoogle Scholar

Copyright information

© Springer-Verlag Berlin Heidelberg 1990

Authors and Affiliations

  • T. Bountis
    • 1
  • M. Bier
    • 2
  • V. Papageorgiou
    • 2
  1. 1.Department of MathematicsUniversity of PatrasPatrasGreece
  2. 2.Department of Mathematics and Computer ScienceClarkson UniversityPotsdamUSA

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