FIGURE B:
chua's diode resistance graph
Chua's circuit can be modelled by a set of nonlinear differential equations where x, y and z are plotted against time, commonly represented as follows.
Chua equations: ẋ = α(y-x-g(x)) ẏ = x-y+z ż = -βy
These represent the voltages across capacitors C1, C2 and the current of the inductor respectively, as denoted in the schematic above. α and β depend on the actual circuit components. g(x) is a piecewise-linear function representing the change in resistance vs. current across the Chua Diode:
g(x) = {m0x+m0-m1, if x≤-1 {m1x, if -1≤x≤1 {m0x+m1-m0, if 1≤xHere m1 is the slope of the middle segment and m0 is the slope of the two outer segments.
We can, however, represent these explicitly as functions of components, voltages and resistance in the actual circuit as below:
̇v1 = [ 1/(R*C1) ]( (v2-v1)-R*g(v1) ) ̇v2 = [ 1/(R*C2) ]( v1 -v2+R*iL ) ̇iL = [ 1/(L) ]( -v2 ) g(v1) = {m0 v1 + (m0-m1)E1, if v1 ≤ -E1 {m1v1, if -E1 < v1 < E1 {m0 v1 + (m1-m0)E1, if E1 ≤ v1