fig.1Another possible purpose for the horseshoe configuration, especially if the plastic blocks are indeed ELECTRETS might be to reduce the impedance of the wiring coiled around the horseshoe legs, which would of course improve the current output.
Yet another possible reaction might be to double the oscillating frequency of the rectifier section of the circuit, particularly as there can be seen on some of the photographs of the Testatika machines a coil (or two coils) of different coloured wire around the horseshoe legs at the very bottom of the coilings of red wire, and these coilings would be connected to the outer plates of the plastic-blocks / electret setup for just such a mechanism (using the DC voltage from the electret) to operate (see fig.1 and the circuits below).
The thick wiring seen around the horseshoe, and at other places in the circuit is normal for high-voltage high-frequency circuits, whereby the electric current moves on the outer surface of the wire rather inside it. This 'skin effect' is counteracted by the use of multi-strand "Litz" wire or by using thick tubing (of 1/8" or 3mm dia).
Suitable parallels to Methernitha’s electronic principles, as can be seen from the circuit layouts included below, belong to a by-gone era of experimental radio electronics.


fig.2One of the techniques used in the early days of radio was a magnetic amplifier, to reduce the impedance of the coil-windings, to thereby increase the CURRENT in the circuit. The two coils L1 and L2 are wound in PARALLEL over the iron core and shunted across an oscillating current A. Coil L3 is connected to a DC source and regulated by resistance OR. The increase in current, using fairly simple circuitry, was 400%. ("Radio Telephony" Alfred N. Goldsmith (1918) p195-7; and see "Magnetic-Amplifier Circuits" William A Geyger (1954) p82)


fig.3A very similar circuit was discovered which doubled or trebled the original frequency when a coil of DC current controlled the transformer core; to prevent the frequency increase but still control the original circuit a reactance coil is coupled to either the primary or the secondary. (From "Increasing Frequency by Static Transformers" by S.M. Powell in "The Electrical Review" Vol 73 Aug 29 (1913) p823)


fig.4Various effects can be had from inserting a capacitor between two transformers. In this case, which resembles the Methernitha set-up, the coils are wound in such a way that the DC winding (E1 & E2) joins the two primary currents (P1 & P2) which lag 180° apart, and effectively doubles the frequency ("Radio Frequency Changers" by A.N. Goldsmith in "Proceedings of IRE" Vol 3 (1915) p74/5).


fig.5Volta's contact law


When differing metals are brought into contact (dry) a difference of potentials exists between them.

The metals to the left exhibit positive potential when touched by any of the metals to the right in both the lists above (ie in a combination of copper/zinc - zinc would be positive, copper negative. Also, the pd between lead and gold would be greater than between iron and copper). For the voltage effect between two metals to be at its highest the surfaces of the metals must be smooth and clean (preferably cleaned with fine emery cloth) (also see "Electronic Influence Machines" by John Gray (1903) p191 and p201 about zinc / copper combinations and proportionally increasing voltages).




 

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All articles in this series copied with permission from Paul E. Potters excellent website

other pages concerning the Testatika in this series.

The index and information page for this series of pages

check out the webmasters original article on the swiss ml
Some interesting comments and ideas on the Free energy machine Swiss ML or Testatika Thestica Distakica
Electrets vs Dielectric Absorbers
Eguchi Electrets
Horseshoe Magnets and the Testatika
The electron field generator
The electron cascade effect
Some free electric notes
The Principle Experiments
Testatika demonstration 1999 report
Methernitha Testatika News
Testatika Machine ML converter pictures
A transcript from the Testakica video

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