Spent most of the day catching up. Enjoyed Jibbguy's post regarding the internal multimeter functions and have to agree with him there. But at the same time, I find myself agreeing with .99 if an older style analog Galvanometer were used in place of the current sensing resistors, or specifically right between the B(-) terminal and all other components. In fact, one on each battery terminal would show if there were a 'leak' in the circuit. Swapping them between multiple tests would eliminate any calibration concerns. Nevertheless, either we trust the 3054 or we don't and I for one have no reason to doubt its results. My far inferior B&K Precision 1476 has a vertical precision of 0.02V/div with each division on the graticule subdivided into 5 equal parts. A well focused trace occupies about 50% or 2mV of screen just for the trace width. Therefore, the smallest accurate ripple that can be measured would be about 3mV, just enough to tell it is not a flat line. So even with my cheap scope, a 5mV signal would be a trustworthy signal. That being said, I can grab hold my scope probe and easily produce 800mV of AC energy from my fingers while the ground wire simple floats at the Scopes Chassis potential (which is tied to an 8 foot long 1/2 inch diameter copper rod driven into the earth right outside my office not more than 4 feet away. The 'Noise' envelope on that signal measures at about 200mV across a 10K resistor with various harmonics and a measurable fundamental that produces 11 cycles for 10 div set on 1 microsecond per division, or 1.1MHz. You can measure this 'Noise' by placing your probe connections across a 10K resistor and touching the probe end while not touching anything else. I put an alligator clip jumper wire on that point and placed the other end on my tongue to enhance the signal to the measured value. Now, we must stated then, conclusively, that the free energy 'noise' must have produced 200mV / 10K current in the resistor. That has to be 20 micro amps right? So, 4 micro-watts of power right there, free for the taking, even if it is buried in the 'noise'. One million resistors on a chip, touch one end to your tongue and the other to 'ground' and you have yourself a 4 Watt heater that runs on 'noise'


Is this enough to trigger the IRFPG50? Not according the specifications. The Fig3 on page 1117 of the Designers Manual shows zero drain current at 4 volts gate to source. But it then shows 500mA at 4.5V. Does the IRFPG50 do any strange things below 4V? I would have to say yes. The turn off time for the device is 130ns. So if the gate is fully charged and then depleted, it takes 130ns before the drain current ceases. This means that there is some residual charge dissipation occurring that causes it to stay on, and some of that is between four and zero volts. Down in that range we are really in uncharted territory and attempting to use the device in a way that it wasn't intended. So can the device self trigger down there? I think there is enough resistance in the circuit to prohibit it, but a floating gate pin is not the way to find out. The wirewound pot makes a good RF antenna for whatever frequency it is tuned to and that is pumped into the gate. So Aaron may have a keen little RF feedback oscillator when he removes the timer from the circuit. I would expect a little more conduction through the IRFPG50 if that were the case however. It is more likely that the noise we see is descriminated RF passed through the body diode and internal capacitance. It may be micropower, but it is still power and the scope reads it. This is somewhat evidenced by the signal which looks fully rectified (I would have expected to see halfwave instead)
Well here it is Sunday Evening and I haven't even fired up the circuit since Friday

BTW - Glen, your scope is waaaaaay fast enough to evaluate the original 140KHz aperiodic oscillations. I just hope my 10MHz scope is fast enough for these 'noise' oscillations


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