Practical Guige to Free Energy Devices

Solutions to this problem were explored using the circuit shown in Fig.9, which still maintains the necessary
communication link for the quasi-sinusoidal oscillation of the capacitatively stored charges at the input and outputs
of the rectification bridge, but integrated the functions of capacitor C4 into the single rectification circuit, in the
form of an asymmetric capacitative bridge C7a and C7b placed transversally to the capacitative bridge formed by
C3 and C5 and in parallel with the charge pack CP at the output from the rectification bridge D5, D6, D2, D3.
This second capacitative bridge is so disposed as to have its centre point connected to the anode A through
capacitor C5. If the axial member of the Tube T were to connect to the junction of D2 and D3 instead of at the
junction D5-D6, the function of bridge C7a and C7b would be connected to the cathode C through capacitor C3.
The capacitative bridge is insulated from the charge pack whose voltage it stabilises, by rectifiers D7 and D8,
which also prevent leakage of charge across C7a and C7b.
The anode and cathode oscillations generated by the electrostatic charge transduction through C3 and C5 into
the poles of the charge pack are trapped by the transversal transduction of the C7 bridge, at the outputs from the
rectification bridge, of which the oscillation has to become split between the bridge inputs into half-waves, for
electrostatic transduction and full wave rectification to occur. In fact, under these conditions, removal of the C7
bridge will suppress the PAGD phenomenon, unless other circuit variables are also altered. The transversal
bridge is thus an essential piece of this novel circuit. Variations in the circuit as shown in Fig.10 were then
studied, the first two being selectable utilising switch S2 (Fig.9).
The presence of the capacitative bridge effectively reduces the dynamic impedance of the charge pack CP so that
the output circuit approximates to a characteristic in which it presents a very high impedance to the tube T at
potentials below a certain level, and a very low impedance at potentials above that level.
With this modified circuit, more effective recovery of the energy produced by collapse of the PAGD pulses is
possible, with more effective isolation from the input circuit utilised to trigger the pulses. Under these conditions,
the energy captured by this circuit at the output, is not directly related to that utilised in triggering the pulses from
the input. The attainment of this condition critically depends on the large capacitance of the transversal bridge
being able to transfer the output energy from the tube T into the charge pack CP. Under these conditions, we
have found, as will be shown below, that the large peak pulse currents released by collapse of the PAGD pulses
released more energy than is used to trigger them, and these findings appeared to tally with other observations
(abnormal volt-ampere characteristics and anomalous pulse currents, etc.) associated with the anomalous
cathode reaction forces that accompany the auto-electronic emission-triggered PAGD regime. Experiments so far
indicate that the power output can be increased proportionately to the series value of C3, C5 and the two identical
C7 capacitors.
A - 578