Duffing Oscillator Northern Illnois UniversityDuffing振子北伊利诺斯大学.pptVIP

Duffing Oscillator Two Springs A mass is held between two springs. Spring constant k Natural length l Springs are on a horizontal surface. Frictionless No gravity Transverse Displacement The force for a displacement is due to both springs. Only transverse component Looks like its harmonic Purely Nonlinear The force can be expanded as a power series near equilibrium. Expand in x/l The lowest order term is non-linear. F(0) = F’(0) = F’’(0) = 0 F’’’(0) = 3 Quartic potential Not just a perturbation Mixed Potential Typical springs are not at natural length. Approximation includes a linear term Quartic Potentials The sign of the forces influence the shape of the potential. Driven System Assume a more complete, realistic system. Damping term Driving force Rescale the problem: Set t such that w02 = k/m = 1 Set x such that b = ka/m = 1 This is the Duffing equation Steady State Solution Try a solution, match terms Amplitude Dependence Find the amplitude-frequency relationship. Reduces to forced harmonic oscillator for A ? 0 Find the case for minimal damping and driving force. f, g both near zero Defines resonance condition Resonant Frequency The resonant frequency of a linear oscillator is independent of amplitude. The resonant frequency of a Duffing oscillator increases with amplitude. Hysteresis A Duffing oscillator behaves differently for increasing and decreasing frequencies. Increasing frequency has a jump in amplitude at w2 Decreasing frequency has a jump in amplitude at w1 This is hysteresis. * * k l m k l q s x s s x s l+d l+d hard soft double well trig identities A w Duffing oscillator Linear oscillator w = 1 A w2 w1 next