Chua's oscillator circuit -- Intuitive picture

[Filip Larsen]

For a chaotic model, a single 'blip', at the appropriate place can completely change the behaviour - hence 'the butterfly effect'.

"Completely change the behavior" sounds wrong to me.

The truncation and rounding errors in numerical method are considered a small perturbation as well, that is, the resulting long-term (chaotic) trajectory for a given initial condition will eventually diverge from such trajectory calculated by any other method. So it makes more sense to define dynamical "behavior" of a chaotic system not from its precise trajectory, but from measures of the strange attractor the trajectory produces, like the Luapunov exponent or the geometry of the stable and unstable manifolds [1]. In that way "behavior" can be defined in terms of how the phase space is mixed and folded, which is a necessary dynamics for chaos.

[1] https://www.bohrium.com/en/sciencep...stable_and_unstable_manifolds_of_chaotic_sets - This site is new to me, but at first glance the description here sounds valid. The topic is treated in many text books on chaos.

 

[sophiecentaur]

So it makes more sense to define dynamical "behavior" of a chaotic system not from its precise trajectory, but from measures of the strange attractor the trajectory produces,

That's a good point. Chaotic systems need a different approach from standard deterministic (right word?) systems. I've heard this sort of comment about weather forecasting models which identify which way they're going and switch from one mode to another when it ;looks like a chaotic pattern is approaching.

So you want to build a real electronic Chua oscillator, to generate a real random sequence? Then how will you implement Chua's diode with real components?

Why are you getting combative about this? There a millions of circuits which will never display chaotic behaviour and your average simulator is well suited to them. There will always be a good mapping between reality and simulation there. But is it true that any randomly chosen chaotic system will behave the same as the simulation unless the relevant simulation parameters are all included and not 'assumed' when the simulator enters its stock values?
If you remember, You took exception to my comment about simulations 'not being real' but (unless we are living in 'The Matrix') it is valid. It wasn't a criticism; I was just introducing a caveat.

 

[Baluncore]

Why are you getting combative about this?

It is you who is combative.

 

[Filip Larsen]

Chaotic systems need a different approach from standard deterministic (right word?) systems.

Indeed.

Regarding the name you could call them non-chaotic, classical or perhaps quasi-linear deterministic systems. For dissipative systems these are systems with only the simple phase space attractors you also see for linear systems, such as isolated fix-points (e.g. hard non-linear die tossing) or limit-cycles (e.g. a near-linear driven damped oscillator).

 

[sophiecentaur]

It is you who is combative.

Well, I get cross when someone refuses to accept a perfectly valid comment about the limitations of Simulators. Your comment about simulating a random signal generator with LTSpice is clearly nonsense and I never suggested it. I will calm down when you acknowledge that a simulation is not 'real' in the sense that it is only valid under certain conditions. You want it to be a panacea?

 

[Baluncore]

I will calm down when you acknowledge that a simulation is not 'real' in the sense that it is only valid under certain conditions. You want it to be a panacea?

This thread is about Chua's Oscillator, what do you not understand?

 

[Swamp Thing]

I have installed ngspice (RPi-5), but haven't got around to experimenting with it. However, it's possible to do thought experiments and refine one's ideas while doing other life stuff.

This has led me to discard the idea that there should be a momentary increase in disspiation exactly while the system is passing from one lobe of the attractor to the other (crossing over the separatrix ??).

The motivation for such an idea was the fact that the oscillation needs to regrow itself after those lobe-to-lobe transitions. However, it now seems to me that the dissipation could be occurring during the overshoot after crossing the separatrix (or whatever the barrier between lobes is called). This overshoot takes us into the region where the negative resistance of Chua's diode drops ( --> less gain) while the positive resistance of the conventional resistor of course remains fixed (--> same loss).

I hope to test this using suitable probes and computed plots in a day or two.

Edit: All this thinking about an oscillation quenching and regrowing in sync with a lower frequency square wave has just reminded me of the venerable superregenerative receiver. Could it be that electronic chaos and attractors have been lurking in our midst since the vacuum tube era? Wait, didn't someone mention 1911 in this thread?

 

[Baluncore]

However, it now seems to me that the dissipation could be occurring during the overshoot after crossing the separatrix (or whatever the barrier between lobes is called). This overshoot takes us into the region where the negative resistance of Chua's diode drops ( --> less gain) while the positive resistance of the conventional resistor of course remains fixed (--> same loss).

That is correct.
Energy increases until it climbs out of one attractor, then from the crest of the saddle, it overshoots the destination attractor, encountering the far soft wall, that attenuates or dumps some energy. It is then shepherded between that wall and the saddle, until it can again escape from the local attractor.

 

[Baluncore]

I hope to test this using suitable probes and computed plots in a day or two.

It should be possible with SPICE to plot the sum of all energy circulating or stored in L or C.
Ea = ½⋅L₁⋅I(L₁)² ; Eb = ½⋅C₂⋅V(C₂)² ; Ec = ½⋅C₁⋅V(C₁)²

For some reason that does not seem to work. I get a minimum energy sum on the saddle. Maybe zero potential is relative to the local attractor, rather than the high-ground.