By Jan Pajak
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Extra resources for ADVANCED MAGNETIC PROPULSION SYSTEMS (UFOs, Magnocraft, Free Energy Devices)
After an analysis of the Johnson motor it becomes obvious that the greatest value of the telekinetic force P' is released just above the magnets of the stator (3) where the acceleration of magnetic circuits is the largest. e. a stator (3), a Telekinetic Effect activator (1) and a rotor (2). In such a three-part motor the mutual interactions between the stator and the field activator are only to release the Telekinetic Effect. But the force P' of this Effect is intercepted by the rotor, which then feeds a part of the impulse just received back onto the activator - to sustain its motion.
The thick closed line passing through magnets (1) and (3) represents the path of the magnetic circuits (force lines) that join both of these parts. The operation of this motor begins with stage (a) in which magnetic circuits are in an equilibrium position. But the inertial motion of the activator (1) in the direction "V" causes these circuits to jump into the position shown in part (b) of this Figure. During such a jump, the magnetic circuits are accelerated. This acceleration releases the telekinetic force "P".
But the motion of the material copy of this object in our world must obey the Conservation of Energy Principle. Because the cause of the telekinetic motion does not provide the energy required to satisfy this Principle, the material part of the object moved must achieve this by itself. e. absorb or release heat). The necessity for this exchange is called the "postulate of spontaneous heat exchange between the telekinetically moved objects and the environment". This postulate must have two consequences: (1) it produces a change in the environmental temperature during telekinetic motion, and (2) it produces a faint glow emitted from the matter (space) surrounding the telekinetically moved objects, called the "extraction glow".
ADVANCED MAGNETIC PROPULSION SYSTEMS (UFOs, Magnocraft, Free Energy Devices) by Jan Pajak