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Ronan Nopp
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Power Electronics Projects

Plasma Toroid Lamp

This is an implementation of a HFSSTC (High Frequency Solid State Tesla Coil) circuit. The key component is a high current(50A) MOSFET. This acts as a self-oscillating switch. The circuit parameters are tuned to create a 15MHz frequency at the primary coil. High voltage excites low pressure Xenon gas, and the precise frequency couples the plasma with the primary coil, creating an effective secondary coil that appears as a ring of plasma.

Built on a small solderable breadboard, with a CPU fan for MOSFET cooling.
Primary Coil is made from leftover copper fridge coolant tubes
Plasma behavior when the circuit is resonating at the wrong frequency


1.2MV Tesla Coil

I designed and built this tesla coil from first principals, modeling the two coupled RLC systems as damped harmonic oscillators. Matching the resonant frequency of the secondary and primary coils is critical. The coupling coefficient between the two coils is a central design constraint that determines the maximum voltage possible. A low coefficient (<0.05) allows significant energy to be wasted in the primary coil, while a high coefficient (>0.2) allows energy to transfer too quickly, causing the spark gap to fire more frequently, and loose more energy doing so. I used Barton B. Anderson’s JavaTC program to tune the geometry of my Tesla coil for a coupling coefficient of ~0.1.

Winding the secondary(1350 turns) with a makeshift lathe
A view of the spark gap, primary coil hookup, transformer, and capacitor bank
The sheet metal manifold on the right focuses air from a large fan onto the spark gap
Finished Building! Note the ring above the primary coil. This is an insurance measure to make sure any discharges from the top load don’t strike the primary coil (could harm the transformer)
A fluorescent bulb is powered wirelessly in the background!

Some factors make the real world tesla coil behave differently from my model. One such factor is the capacitive loading of the spark gap itself. This is rather complicated to model, but can be accounted for by “detuning” the frequency of the primary coil. For this reason the hookup on one side of my primary inductor can be moved along the coil, allowing the inductance to be increased, accounting for the spark gap and empirically tuning for maximum performance.

The spark gap itself also requires some tuning, as the exact voltage breakdown of the system is dependent on many environmental factors, including surface oxidation of the copper pipes used, and small changes in the spark gap width due to imprecise construction. Besides reducing erosion/wear of the spark gap, utilizing many smaller spark gaps allows me to adjust the voltage by using alligator clips to short one or more of the spark gaps. When starting the tesla coil for the first time, it is often necessary to short all but two of the spark gaps to break through oxidation buildup, before a more gaps can be opened to increase the voltage. In the future I would like to explore the design of a solid state switching mechanism, as it allows for more convenient tuning of the system.

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