Practical Guige to Free Energy Devices

Confirmation of the importance of the charge pack in the PAGD function of the present circuitry here considered,
comes from the fact that the size (the number of cells) and the intrinsic capacitance of the charge pack affect the
PAGD frequency dramatically (see Table 4): increasing the charge pack size of 29 cells to 31, by 7% leads to a
10-fold reduction in frequency; further increases in the number of charge pack cells extinguishes the
phenomenon. On the upper end of the scale, this effect appears to be tied in to restrictions that it places on the
ability of the larger charge packs to accept the discharge power output once the charge pack voltage exceeds the
PAGD amplitude potential. All of these measurements were conducted with the same 128 cm 2 plate PAGD
generator, at a pressure of 0.8 Torr and in the triode configuration (see Fig.9).
Other factors can also affect the frequency: the motion of external permanent magnetic fields oriented
longitudinally with the inter-electrode gap, external pulsed or alternating magnetic fields, external electrostatic or
electromagnetic fields, specific connections of the earth ground, and the presence of a parallel capacitative,
capacitative-inductive or self-inductive arm in the circuit, such as we have described for our electromechanical
PAGD transduction method as described in the “531” application.
Analysis of the modulation of PAGD amplitude is simpler than that of its frequency, because fewer factors affect
this parameter:
(1) magnitude of the applied potential,
(2) inter-electrode gap distance and
(3) the negative pressure, as shown in the “863” application, for "low" applied currents.
As the magnitude of the applied potential itself is limited by the gap and the pressure, to the desired conditions of
breakdown, the important control parameter for the PAGD amplitude is the pressure factor. This is shown in Fig.6
and Fig.7, respectively for "low" (5 mA) and "high" (about 500 mA) applied currents and for the same plate diode
configuration of a H34 Al 128 cm 2 plate PAGD generator (5 cm gap), in the simple circuit described in the “863”
application; it is apparent that both positive and negative components of the amplitude of these pulses in the
oscillograph, are a function of the pressure, but the maximum cut-off limit of our equipment, for the negative
component (at 240 volts for the "low" current experiment and at 120 volts for the "high" current), precluded us
from measuring the peak negative voltage of these pulses.
However, rms measurements of the pulse amplitude at the plates and DC measurements at the circuit output to
the charge pack indicate that the negative component increases with decreasing pressure to a maximum, for a
given arrangement of potential and gap distance; no pressure-dependent bell shape variation of the pulse
amplitude, as that seen for the positive component at "high" applied currents (Fig.7) is observed with the negative
amplitude component. For the typical range of 0.8 to 0.5 Torr, the rms value for pulse amplitude varies from 320
to 480 volts, for a 5.5 cm gap distance and applied DC voltages of 540 to 580 volts. PAGD amplitude is a critical
factor for the design of the proper size of the charge pack to be utilised in the optimal circuit.
The development of the circuits to be described stemmed from fundamental alterations to the principles implicit in
our previous methods of electromechanical transduction of AGD plasma pulses as described in the “531”
application. Whereas this electromechanical coupling (capacitative and self-inductive), utilised directly, energises
the AGD pulses inverted from the DC input by the vacuum generator, the purpose of the development that led to
the presently described experiments was to capture efficiently, in the simplest of ways, most of the pulse energy
in a closed circuit, so that power measurements for the energy transduction efficiency of the observed
endogenous pulsation could be carried out. Ideally, comparative DC power measurements would be performed at
both the input and output of the system, taking into account the losses generated across the components; this
would overcome the measurement problems posed by the myriad of transformations implicit in the variable
frequency, amplitude, crest factor and duty-cycle values of the PAGD regime, and necessitated some form of
rectification of the inverted tube output.
A - 576