A New Chaotic Jerk Circuit

J. C. Sprott

ABSTRACT

Much recent interest has been given to simple chaotic oscillators based on jerk equations that involve a third-time derivative of a single scalar variable. The simplest such equation has yet to be electronically implemented. This paper describes a particularly elegant circuit whose operation is accurately described by a simple variant of that equation in which the requisite nonlinearity is provided by a single diode and for which the analysis is particularly straightforward.

(Manuscript received September 20, 2010; revised December 1, 2010; accepted January 26, 2011. Date of current version April 20, 2011.)

Ref: J. C. Sprott, IEEE Transactions on Circuits and Systems--II: Express Briefs 58, 240-243 (2011)

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Chaotic circuit schematicFig. 1. Chaotic circuit schematic.


Actual circuit in opeation

Fig. 2. Actual circuit in operation.


Frequency spectrum of the x
        output of the chaotic circuit
Fig. 3. Frequency spectrum of the x output of the chaotic circuit.


Numerically calculated phase
        space plot on the same scale as Fig. 2
Fig. 4. Numerically calculated phase space plot on the same scale as Fig. 2.


Numerically calculated
        waveforms of x and its successive derivatives
Fig. 5. Numerically calculated waveforms of x and its successive derivatives.


Poincare section in the x-y
        plane at the instant of maximum diode conduction
Fig. 6. Poincaré section in the x-y plane at the instant of maximum diode conduction.


Largest Lyapunov exponent and
        the value of x when x-dot is a local maximum vrsus the
        bifurcation parameter A in (6)
Fig. 7. Largest Lyapunov exponent and the value of x when dx/dt is a local maximum versus the bifurcation parameter A in (6).


Homoclinic orbit for A=0.7043Homoclinic
        orbit for A=0.3890
Fig. 8. Homoclinic orbits, with the upper for A = 0.7043 and the lower for A = 0.3890 in (6).