Non-linear dynamics of a shallow arch under periodic excitation —I.1:2 internal resonance

Abstract The weakly non-linear resonance response of a two-degree-of-freedom shallow arch subjected to simple harmonic excitation is examined in detail for the case of 1:2 internal resonance . The method of averaging is used to yield a set of autonomous equations of the first-order approximations to the response of the system. The averaged equations are then examined to determine their bifurcation behavior. Our analysis indicates that by varying the detuning para- meters from the exact external and internal resonance conditions, the coupled mode response can undergo a Hopf bifurcation to limit cycle motion. It is also shown that the limit cycles quickly undergo period-doubling bifurcation, giving rise to chaos. In order to study the global bifurcation behavior, the Melnikov method is used to determine the analytical results for the critical parameter at which the dynamical system possesses a Smale horseshoe type of chaos.

[1]  M. H. Lock,et al.  Snapping of a shallow sinusoidal arch under a step pressure load. , 1966 .

[2]  Ali H. Nayfeh,et al.  Modal Interactions in Dynamical and Structural Systems , 1989 .

[3]  G. Kovačič,et al.  Orbits homoclinic to resonances, with an application to chaos in a model of the forced and damped sine-Gordon equation , 1992 .

[4]  John W. Miles,et al.  Resonant, nonplanar motion of a stretched string , 1984 .

[5]  N. Sri Namachchivaya,et al.  Chaotic motion of a shallow arch , 1988 .

[6]  N. Bogolyubov,et al.  Asymptotic Methods in the Theory of Nonlinear Oscillations , 1961 .

[7]  Neil Fenichel Persistence and Smoothness of Invariant Manifolds for Flows , 1971 .

[8]  Anil K. Bajaj,et al.  Amplitude modulated and chaotic dynamics in resonant motion of strings , 1989 .

[9]  J. Humphreys,et al.  On dynamic snap buckling of shallow arches. , 1966 .

[10]  Jerrold E. Marsden,et al.  A partial differential equation with infinitely many periodic orbits: Chaotic oscillations of a forced beam , 1981 .

[11]  Z. C. Feng,et al.  Global bifurcation and chaos in parametrically forced systems with one-one resonance , 1990 .

[12]  A. Maewal Chaos in a Harmonically Excited Elastic Beam , 1986 .

[13]  L. P. Šil'nikov,et al.  A CONTRIBUTION TO THE PROBLEM OF THE STRUCTURE OF AN EXTENDED NEIGHBORHOOD OF A ROUGH EQUILIBRIUM STATE OF SADDLE-FOCUS TYPE , 1970 .

[14]  P. R. Sethna Coupling in Certain Classes of Weakly Nonlinear Vibrating Systems , 1963 .

[15]  P. Holmes,et al.  A nonlinear oscillator with a strange attractor , 1979, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[16]  C. Hsu,et al.  Stability of Shallow Arches Against Snap-Through Under Timewise Step Loads , 1968 .

[17]  Jerrold E. Marsden,et al.  Horseshoes in perturbations of Hamiltonian systems with two degrees of freedom , 1982 .

[18]  Anil K. Bajaj,et al.  Period-Doubling Bifurcations and Modulated Motions in Forced Mechanical Systems , 1985 .

[19]  P. R. Sethna,et al.  Non-linear phenomena in forced vibrations of a nearly square plate: Antisymmetric case , 1992 .

[20]  Jerrold E. Marsden,et al.  Melnikov’s method and Arnold diffusion for perturbations of integrable Hamiltonian systems , 1982 .