The Duffing Equation. Introduction. We have already seen that chaotic behavior can emerge in a system as simple as the logistic map. In that case the.
26 A?u 2016 Keywords: Duffing equation cubic Duffing oscillator equation
The Duffing Equation is an externally forced and damped oscillator equation that exhibits a range of interesting dynamic behavior in its solutions.
1 Oca 2014 Abstract: In this article Differential transform method is presented for solving Duffing equations.We apply these method to three examples.
linear equation of motion including a cubic stiffness term. The Duffing equation is capable to show many phenomena of nonlinear vibrations
Hence. Duffing equation has been widely investigated by many researchers using several numerical methods. Among them one can mention: the improved Taylor
Keywords— Nonlinear Duffing Oscillator Chaos
We consider the periodic solutions of the Duffing equation which describes the nonlinear forced oscillation: (1.1) u"(t) + ?u'(t) + ?u(t) + au3(t) = /?(?)
is described by a single ordinary differential equation called the Duffing equation. In order to get chaos in such a simple system
The Duffing equation will be studied under a variety of different val- ues for the coupling parameters in the equation. The general expression.
The Duffing equation describes the motion of a classical particle in a double well potential We choose the units of length so that the minima are at x = ± 1 and the units of energy so that the depth of each well is at -1/4 The potential is given by VHxL = - x2 2 + x4
ENGI 9420 4 11 - Duffing’s Equation Page 4 65 4 11 Duffing’s Equation Among the simplest models of damped non-linear forced oscillations of a mechanical or electrical system with a cubic stiffness term is Duffing’s equation: 2 3 2 cos dx dx abxcxd dt dt +++= ?t (1) In section 4 01 we considered the simple undamped pendulum: 2 2 sin 0
The Duffing Oscillator Consider this system: T 7 E > T 6 E : G 5 G G 6 T 6 ; T L # O E J : × P ; This equation is the Duffing equation For this particular system the damping changes with the magnitude of x Consider for example the MEMS resonator below: The 2-beam suspension system is statically indeterminate For small
A Duffing equation with such coefficients has physical rele- vance: it is e g a simple model of the time dependence of a buckled beam undergoing forced lateral vibrations [8] Equation (1) possesses a great number of qualitatively different kinds of periodic solutions x(t) which depend on w
Duffing Equationv Clear confirmation of our prediction of elongation with increasing amplitude Soft Spring Model ü Introduction In the soft-spring model the spring force has the property that the force per unit extension becomes less as x increases This is modeled by the equation d2 x ÅÅÅÅÅÅÅÅÅÅÅÅÅÅ dt2 + x -x3 = 0