The (unnormalized) state equations are:
with
Dimensionless state equations can be derived from the original ones scaling time, voltages, and currents.
In the original paper [1], where the circuit was extensively analyzed, time, voltages, and currents are scaled by RC2, Bp, and BpG, respectively. The new state variables become:
and the normalized time is given by:
With these assumptions, we obtain the following dimensionless state equations:
with
where
The applet uses a different set of dimensionless state equations, as indicated below. Assume Ga - the slope of the inner segment of the nonlinear resistor characteristic - is negative and set Ra = -1/Ga > 0 . Then scale time, voltages, and currents by C1Ra , Bp , and Bp/Ra , respectively. If we use as state variables:
with normalized time given by:
the following dimensionless state equations are obtained:
with
and where
After this scaling, the nonlinear resistor has breakpoints for X = ±1 and the slopes of the piecewise linear characteristic are -1 in the inner segment and -b in the outer segments. Finally, note that the case = 0 corresponds to the (classical) Chua’s circuit, where R0 = 0.