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experiment in which that energy is diverted and used without affecting the input magnetisation circuit. Then the recovery of energy upon demagnetisa- tion of that latter circuit will occur, but as it cannot take used energy back from a load, the polarising magnetic source simply has to do the work and so leave the quantising vacuum field in a cooler state. Rather than wait until I am ready to report such further progress, I thought it appropriate to inform you and, via you, the readers of your newsletter at this otaca tion was virtually constant. This was as expected from my theo- retical reasoning, but there was a sur- prise in that the transverse permeability was smaller than I expected, by a factor of ten. Now, if you are wondering what this means, note that my object is to store ‘reluctance’ energy by that transverse excitation, meaning energy that goes in THE SOLID-STATE ENERGY PROBE as inductance energy and is recovered EXPERIMENT without loss on the down quarter-cycle. By making that transverse oscillation Te: third experiment which tells stronger and stronger, the object is then | THREE EXPERIMENTS| ON 'FREE ENERGY' | Part 2 © Harold Aspden, 1993 me that I am on the verge of a_ to deflect the primary polarisation so breakthrough in penetrating the that the intrinsic ferromagnetic power barrier giving access to ‘free energy’ ina develops flux oscillations in the axis of solid-state device has yielded its own the primary coil. The aim is to tap encr- surprises. gy from that deflected ‘reluctance’ ener- Here I built a form of transformer that gy source, most of which is powered by is intended to serve as an exploratory the atomic spins in the ferromagnet, and test rig. I shall, owing to the developing _ use that energy on the up quarter-cycle. length of this communication, curtail This process then the constructional details and leave allows the polarising something for future reporting. bias, which could be The test involved setting up a DC that provided by a per- magnetic bias in the x-direction and an manent magnet, to AC transverse magnetic oscillation in reset as the transverse the y-direction. Again I used the above- current diminishes, but described technique of studying the the shortfall in the shape and form of the B-H loop devel- stored reluctance’ ener- oped by the AC flux. gy given back to the The AC excitation was of low mag- magnetising coil in that netic flux density amplitude so that the transverse direction has eddy-current losses should be negligi- then to be made up by ble, as should hysteresis loss. I was the magnet. operating in the flux rotation zone and The experiment I above the B-H knee where rotational report here goes no fur- hysteresis loss diminishes rapidly to ther than showing that zero. I expected the B-H ‘loop’ to show the transverse excita- as a line on my oscilloscope and, tion is a pure, virtually indeed, such a line did appear. Ihadto loss-free, inductive expand it off the range of the screen by process which involved increasing the x deflection sensitivity a characteristic mag- substantially in order to trace the small netic permeability indi- capacitive contribution of my circuit for cating a 30:1 ratio of integrating induced EMF to derive the B_ ferromagnetic power signal. I could find no trace of a loss. input compared with Moreover, the line was not curved: it external power input. was very straight, which meant that the That is the starting incremental permeability effective in point which will, I am s. ahh. the direction transverse to DC polarisa- sure, lead to the fourth 'THREE EXPERIMENTS. | ON 'FREE ENERGY' | Part 2 © Harold Aspden, 1993 THE SOLID-STATE ENERGY PROBE EXPERIMENT slage. CONCLUSION In summary, just as with the reluc- tance motor, one seeks to use a magnet to inject inductive energy into an air gap and then release that energy as mechani- cal work as the air gap closes, before NEXUS ¢53 APRIL - MAY 1994 ee