Nonlinear Dynamics of an Axially Translating Viscoelastic String With Parametric And Exact Internal Resonance
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Abstract
The subject of axially translating string has widespread engineering and industrial
newlineapplications which can be studied both theoretically and experimentally. It belongs to
newlineclass of travelling continua involving inherent coriolis force which renders the system
newlinegyroscopic and induces dynamic instabilities depending on the characteristics of the
newlinesystem and travelling velocity including its fluctuations.The time dependency present in
newlineaxial velocity causes parametric instabilities (resonances) characterized by vibration in a
newlinedirection orthogonal to the direction of unsteady velocity.The study of these parametric
newlineinstabilities has practical concern as well as of immense fundamental interest. The
newlineaxially travelling string exhibits wide range of linear and nonlinear dynamic behaviour
newlinedepending on the system parameters. Nonlinear modal interaction in the form of internal
newlineresonance also influences the system behaviour.
newlineIn the present dissertation, the nonlinear characterstics of a pulley supported axially
newlinetranslating string subjected to parametric resonance with exact internal resonance is
newlinestudied through analytical-numerical method. The translating string with initial axial
newlinetension is on pulley supports with variable stiffness. The cubic geometric nonlinearity in
newlinethe system is due to elongation of the string. The system has parametric excitation
newlineassociated with the travelling velocity having harmonic fluctuation about a steady mean
newlinevalue leading to parametric resonance. The third mode frequency is three times the
newlinefundamental frequency leading to 3:1 exact internal or autoparametric resonance
newlinebetween the third and first mode for this cubic nonlinear system. The multiple-scale
newlineanalysis approach is employed directly on the equation of motion to obtain approximate
newlinesolutions and analyse the system dynamics. The principal parametric resonance of first
newlinemode, combination parametric resonance of first and third mode, principal parametric
newlineresonance of third mode, combination parametric resonance of first and second mode are
newlinediscusse