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colloquiallyineffable
modified 10 years ago

Where to find negative dynamic resistance

5
5
314
06:35:21
I decided to revisit this idea because I've noticed a few oscillators out there that have this mechanism at heart, but try to trace their origins from elsewhere. I'm by no means an expert on the subject but I do feel capable of a competent explanation, so here we go. This circuit is more generally known as a type of Bistable Multivibrator; specifically, it is a Set/Reset Latch or SR Flip-flop. When it is being used as a bistable device, each of the bases act as an input (Set,Reset) and each of the collectors act as complementary outputs (Q,-Q). At the instant the circuit is powered, neither transistor has the advantage and the circuit exists in unstable equilibrium between states. Heavy regenerative feedback between the opposing transistors acts to reinforce any small imbalances that develop. Which ever transistor happens to conduct best first is rapidly driven into saturation(ON) and the other into cut-off(OFF). If an input pulse of sufficient magnitude either drives the base of the ON transistor low or the base of the OFF transistor high, the circuit will switch states. Now, suppose that if instead of using all that heavy feedback to switch between one of two stable states, you force the circuit to operate between states by placing an appropriate tuned RLC tank between your inputs(where I have the triangle and volt meter in this case). Once again, the circuit starts out in unstable equilibrium between states and any small imbalance is reinforced, but now, if either transistor saturates, the tank just swings the other way. The circuit as I have drawn it here is probably the most basic manifestation of the concept, but there are countless ways to reinvent it into working oscillators. The tank can be simple or complicated, the transistors can be npn, pnp, nMOS, pMOS, or combinations, the frequency can be almost anything.. So to sum it up, the simple bistable multivibrator possesses a characteristic region of negative dynamic resistance between its differential inputs (and outputs) when biased between states. Under normal operation it can be thought of as the force that drives the circuit into one of its stable states by reinforcing any existing or applied instability. I built this in EC 2.16 but that shouldn't matter. I hope someone out there still cares and will benefit from this.
published 10 years ago
hurz
10 years ago
Like the way you describe it in your own words, and you know much more about electronic, i m sure. And yes, the secret of this is the negative resistance. With a tank circuit its a nice LC oscillator. Keep it up please! http://everycircuit.com/circuit/6315802756644864
colloquiallyineffable
10 years ago
PS: As is, this circuit develops -272ohms. ∆V/∆I=4V/-0.0147A
hurz
10 years ago
One other field of use is as chua diode and build an chaotic oscillator - check this http://everycircuit.com/circuit/6748292855627776
colloquiallyineffable
10 years ago
In real life, a simple silicon pn rectifier diode produces white noise when reverse biased due to the random, statistical nature of the reverse leakage events. From white noise you can randomize whatever you want.
hurz
10 years ago
Yes, but chaos is not random noise. A chua oscillator is a chaotic one.

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