The Tom Bearden Free Energy Collector Principle
Jean Louis Naudin

 

Original version

 

 

Source : http://jnaudin.free.fr/html/tbfrenrg.htm

In the paper " The Final Secret of Free Energy " wrote in February 9, 1993, Tom Bearden has described the principle of a device which seems able to tap Free Energy from the energy flow ( the Poynting S-Flow ) in the vaccum during the short transient phase ( the relaxation time in a conductor ) when a source is connected to a resistive load. In this paper, I am trying to clarify a bit, the basic concept of this principle.

Tom Bearden claims that when a Source ( a dipole ) is connected to a resistive load, the most important part of the principle is the information transfered to the load at the speed of light by the S-Flow. The S-Flow is pure EM energy which flows through the space and outside the conductor. This energy is Free and only this part must be used as a "free lunch". Just after this very short time, after that the switch is closed ( the transient phase ), the current begins to flow in the circuit. This transient phase is named the Relaxation Time. In copper, the relaxation time is incredibly rapid, it's about 1.5 x 10-19 sec. When the current flows ( the permanent phase ), the circuit consumes power from the Source and dissipates energy by Joule's Effet, this phase must not be used in our case.

So, according to Tom Bearden, for tapping Free Energy, the purpose is to charge a " Collector " during its relaxation time and then, to switch this Collector to a common resistive load, just before that the electrons begin to flow in the circuit.

" We took some trapped EM energy density (a chunk of potential gradient, a "voltage" before current flows) from the source, by switching that potential gradient (energy density, which is joules per coulomb) onto a collector (containing a certain number of coulombs of trapped charges) where the potential gradient activates/potentializes/couples-to these temporarily non translating electrons. So the finite collector collected a finite amount of excess energy [joules/coulomb x collecting (trapped) coulombs] on its now-excited (activated) free electrons. Then, before any current has yet flowed from the source, we switched that potentialized collector (with its temporarily restrained but potentialized electrons; with their finite amount of excess trapped EM energy) away from the source and directly across the load. Shortly thereafter, the relaxation time in the collector expires. The potentialized electrons in the collector are freed to move in the external load circuit, consisting of the collector and the load, and so they do so. " has said Tom Bearden.

For the Collector it is necessary to use a conductive material which has a longer relaxation time than in the copper. This is only for the electronic circuit design and the limitation of its components. So, Tom Bearden has used " a Degenerate Semiconductor " which has a relaxation time of about 1 ms. The Collector is made with 98% Aluminum and 2% Iron.

Degenerate semiconductor :

Relaxation time :

  • A conductor contains large number of loosely bound electrons which we call free electrons or conduction electrons. The remaining material is collection of heavy positive ions called lattice. These ions keeps on vibrating about their mean positions. The average amplitude of vibration depends upon temperature. Occasionally, a free electron collides interacts in some other fashion with the lattice. The speed and direction of electron changes randomly at each such event. As a result electrons moves in a zig-zag path....The average time between two successive collisions in a conductor is called the relaxation time. ( see at : http://www.schooljunction.com/current.htm ) >>

The Bearden's Collector is charged by using a Stepwise Charging method with a ramp voltage generator, this is commonly used in high efficiency and low power consumption CMOS systems which use an Adiabatic Charging method ( see Charge Recycling Clocking for Adiatbatic Style Logic by Luns Tee, Lizhen Zheng ). With this Stepwise Charging method very few energy is required for charging the Collector. If the Collector is a common capacitor the efficiency is nearly close to 100%. With the Bearden's Collector, this method is used only for transfering the potential. The ramp duration of the voltage must be less than the relaxation time of the Collector used. So, there is no current flow in the circuit ( dQ/dt ~ 0 ) during the charging sequence. When the Collector is fully charged, all the free electrons are "potentialized", they have their own kinetic energy gained by the potential only produced by the S-Flow. The next step is to use these "potentialized electrons "by switching the circuit on the Load, now, the Collector acts as a Free Source of Energy, it acts as a dipole energized by only the S-Flow of the original source ( V1 in the diagram below).....

Meg diagram
( This diagram has been updated on July 11, 2001 according to the latest comments from Tom Bearden

I hope that, with this short description, I have been able to clarify a bit the Tom Bearden's " Final Secret of Free Energy ". Now, only a real working device will prove if his claim can be more than a simple overunity dream...

Good thinking and explorations,

Jean-Louis Naudin
July 10, 2001

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