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Chaotic relaxation

From cornish semiconductor corporation
Revision as of 21:35, 24 August 2026 by Cornish semiconductor (talk | contribs) (Created page with "500px|right This circuit is one of the ones I'm most pleased with, as it's a design that I've come up with from a pair of simple relaxation oscillators that is capable of producing very complex sounds. Each oscillator is modulating the others pulse width, and there are two possibilities for disrupting the circuit with crystal diode clipping, the input signal is fed into the circuit and there is a breakout jumper so multiple of these modules can...")
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This circuit is one of the ones I'm most pleased with, as it's a design that I've come up with from a pair of simple relaxation oscillators that is capable of producing very complex sounds. Each oscillator is modulating the others pulse width, and there are two possibilities for disrupting the circuit with crystal diode clipping, the input signal is fed into the circuit and there is a breakout jumper so multiple of these modules can be chained for more complex feedback. I haven't tried much of this yet.

It slightly bends the variscan synthesis rules in that it works in an interesting way without a crystal in the circuit. This makes it more forgiving in a live setup, but I think it does exhibit differences between different semiconducting minerals when they are used.

Licenced under the CERN Open Hardware Licence Version 2 – Strongly Reciprocal

Inputs

  • Choice of two locations for a crystal diode: X1 limits the buffering like a soft clipper (needs connecting to work when not in use) and X2 hard clips the input to the first oscillator.
  • CV input
  • Audio input feeds into the circuit.
  • Breakout location to chain multiple chaotic relaxation oscillators together.

Controls

  • OSC 1 pitch
  • OSC 2 pitch

Outputs

  • Audio signal

Schematic

PCB layout

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