*GlowStick* 5
Learning from Particle 3 in the Fuel and other historical Rossi related data - and the recent work by Holmlid, this replications fuel will be Hunter AH50 + LiAlH4 + HTED-04 catalyst.
Good luck to Alan and Mark!
Learning from Particle 3 in the Fuel and other historical Rossi related data - and the recent work by Holmlid, this replications fuel will be Hunter AH50 + LiAlH4 + HTED-04 catalyst.
Good luck to Alan and Mark!
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Here's an image of the cell components before assembly:
None of the 5 Glowstick experiments so far have produced convincing results, with the maximum excess heat observed being less than the cumulative accuracy of calorimetry. They should therefore be considered null tests, but have served well for ongoing development and debugging of the apparatus.
The next iteration (GS5.2) is under construction, and we hope to begin calibrations next week. The focus for this test will be the hydrogen loading behavior of various Nickel powders, leading up to a longer-duration experiment with fuel prepared according to the Rossi patent.
We also considered that Rossi was stimulating his powders with RF based on the number of wires going into the system. A simple oscilloscope would have caught this but Rossi apparently prohibited their use. As to the frequency, we tried a number of things along those lines with numerous Ni systems on various supports and saw nothing. This was before LiAlH4 came into vogue, so we may have had the wrong materials.
In general, the answer is no. Inductive heating operates by means of a high Q L/C circuit, and high Q circuits typically have very narrow bandwidths which yield sinusoidal waveforms.
I also experimented previously with a PWM supply but found no difference in terms of excess heat (ie, none) compared to DC heating. However, the B-field strength for PWM is no where near as strong as for inductive heating, where hundreds of amps can flow through the work coil.
Inductive heating has the advantages you mention, but also presents challenges. For example, thermocouples exposed to the field would suffer from both induced voltage and induced heat, limiting their accuracy. And for direct heating of Ni fuel in powder form, the heating would be unpredictable unless the particle size is uniform and known, and would change significantly as the Ni exceeds its Curie temperature.
These problems can be mitigated by careful design and engineering, at the probable cost of added complexity and development time.
If you have solutions for these problems I'd be very happy to apply them to the Glowstick reactor. I've been testing a Class D power supply capable of sourcing arbitrary waveforms up to 30 kHz and 1200 watts. It can also be modified to use the 500 kHz chopped output without filtering.
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