As it is, it delivers high voltage and current to the coil, plus the amplitude has excellent temperature stability.
This circuit contains no frequency-dependent components other than the resonant LC tank. The driving transistors are switched at the exact zero-crossing of the tank's current in perfect quadrature with the tank's voltage regardless of the resonant frequency. Just replace L and C and you get a perfect sine wave signal at any frequency. The ratio L/C must be kept between 15.000 and 120.000 (H/F).
Q9 senses the current through lower driving transistor Q6, R9 converts it to an amplified voltage and this is used to turn the upper driving transistor off. The same is applicable to Q7, Q8 and R12. The Schottky diodes prevent saturation that would delay the switching relative to the zero-crossing. If they're omited the quadrature is less than perfect but still very good and you get a 5% more power.
I share this circuit idea so that you guys can make it better, for example: making less dependent on resistor values and transistor tolerances by using op-amps, comparators etc. where appropriate.

This circuit contains no frequency-dependent components other than the resonant LC tank. The driving transistors are switched at the exact zero-crossing of the tank's current in perfect quadrature with the tank's voltage regardless of the resonant frequency. Just replace L and C and you get a perfect sine wave signal at any frequency. The ratio L/C must be kept between 15.000 and 120.000 (H/F).
Q9 senses the current through lower driving transistor Q6, R9 converts it to an amplified voltage and this is used to turn the upper driving transistor off. The same is applicable to Q7, Q8 and R12. The Schottky diodes prevent saturation that would delay the switching relative to the zero-crossing. If they're omited the quadrature is less than perfect but still very good and you get a 5% more power.
I share this circuit idea so that you guys can make it better, for example: making less dependent on resistor values and transistor tolerances by using op-amps, comparators etc. where appropriate.
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