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Registered Member #1025
Joined: Sun Sept 23 2007, 07:53PM
Location: Czech Rep.
Posts: 566
I simplified the design (it is powered straight by non-rectified 220V AC mains) and increased the power of my single switch…
How it works: It employs three BUP314 transistors in parallel switched by TL494 followed by UCC37322/1 gate drive and GDT. The resonant frequency of the coil is 380KHz. The coil works in Class E and to achieve Class E at 2.5KW which the coil sucks from the wall needs a special trick. The PW of the switch pulses is very short (only 1us) and the switching frequency is only half the resonant frequency (180KHz). Big advantage of this concept is that through the opened transistor the C1 is discharged into the primary and this discharge has a very short peak (most of the energy goes within first 300ns). Thus, the turn off time of the transistors is not longer an issue and relatively slow IGBT type of transistor can be easily used. Such ultra short pulses are relatively easy to place to the zero voltage transitions of the L1/C2 resonator by simple tuning of the coil (at low input voltage). The huge C3 capacitor works as a non-inductive current limiter with very low resistance. It basically determines the AMP peak of the C1 discharge. The C3 is made of many PP capacitors (used in asynchronous motors) and by connecting and disconnecting some of the caps the power of the coil can be regulated.
Here is the video of the coil in action…
Comments welcomed
Red - secondary waves Black - driving pulses
BTW: Would be great if somebody could help me to solve a feedback for this coil - I'm sure it would increase the spark lenght...
Registered Member #1025
Joined: Sun Sept 23 2007, 07:53PM
Location: Czech Rep.
Posts: 566
Dr. Conner wrote ...
Looks like you reinvented the OLTC with an extra capacitor.
I don’t understand where you see similarities with an OLTC concept. I checked all the OLTC schemes on the internet and the only similarity I see, is that they are also connected to the wall plug-in. The OLTC concept as I understand it is a substitution of a spark gap a by a semiconductor. It means that the switch device is in parallel to the L/C. Next, the power source for a common OLTC is rectified mains with some kind of current limiter (a choke or transformer). The driving pulses for the OLTC transistor are completely unrelated to the resonant frequency of the coil, usually kept in low bps rate. None of these features are part of my coil – so why is it OLTC for you?
My coil has a transistor in series with primary and is in parallel with the resonant cap (class E concept). As a power source I use non-rectified mains and the driving pulses are exactly 1/2 of the resonant frequency of the coil (In case I’m out of tune, no or very little sparks appear).
Registered Member #1025
Joined: Sun Sept 23 2007, 07:53PM
Location: Czech Rep.
Posts: 566
GeordieBoy wrote ...
Just to avoid confusion, this circuit is not operating like a Class-E RF amplifier. If anything it is operating closer to a Class-C frequency doubler.
Class-E operation is characterised by a damped sinusoidal voltage waveform, where the switch turns on at zero-voltage and with zero-current.
Some info including waveshapes here:
-Richie,
Thanks for the link and the Class comment... I do not understand the Class C - how it works, whether it has also a resonant cap or not. Still, I believe the signal is actually damped - you can even see it on the osciloscope picture. The only thing which is different from classical classE operation is that I switch every second wave. I also tried to switch every negative wave (this means the full resonant frequency of the coil). It worked very well, but only two seconds - than I destroyed one of the transistors so I went back to the safe waters of the resonant freq/2 (BTW: paralleling of the transistors have the big advantage that you destroy only one, in case you make some mistake. The bridge design is never so generous...).
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