# Free energy

 Название Free energy страница 4/7 Дата конвертации 13.09.2012 Размер 180.55 Kb. Тип Документы

## REALISATION

There are a lot of options in realization depends on core

1. on air (vacuum)

2. on bar ferromagnetic core

3. on toroid ferromagnetic core

4. on transformer ferromagnetic core

L1

L1

L1

L2

L2

L2

2

3

4

PROPERTIES (tested a lot of times for variety of cores)

The value of the total inductance LS does not change if to short one of the inductance components L1 or L2 (perhaps, the first time tested by Mr. Tesla in the 19th century).

APPLICATION

Energy generation based on asymmetrical process

1. Feed the total inductance LS by current I

2. To short one part of the inductance (for example, L1)

3. Drain off energy from L2 in a capacitor

4. After draining L2, to short it and drain energy from L1 in a capacitor

## QUESTION

Is it possible in such a way to get dual energy on the basis of asymmetry of the process, and if not, what is wrong?

^ AN ANSWER we need tests, and start from manufacturing the coils.

## THE EXAMPLES OF THE REAL COILS

A coil is wounded on transformer ferromagnetic core (size is not impotent) with permeability 2500 (not impotent) for power supply transformers. Each half-coil consists from 200 wounds (not impotent), wire is 0.33 mm in diameter (not impotent). The total inductance LS is about 2 mHn (not impotent).

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A coil is wounded on toroidal ferromagnetic core with permeability 1000 (not impotent). Each half-coil consists from 200 wounds (not impotent), wire is 0.33 mm in diameter (not impotent).

The total inductance LS is about 4 mHn (not impotent).

An ordinary transformer (based on iron core) for 50-60 Hz power supply (size is not impotent) with coils placed on its halfs, the total inductance LS is about 100 mHn (not impotent).

## ^THE TASK OF THE TESTS

To make tests confirmed with coils properties, make measurements of the LS inductance without shorted coil L2 and with shorted coil L2 and match results.

Remark all test will be done with toroidal coil (the other coils have the same properties), you can repeat tests and prove it by yourself.

## OPTION 1

The simplest inductance measurements with the help of an ordinary RLC – meter

#### An order of measurements

The total coil inductance LS was measured without shorted coils, the figures were stored. The L2 coil was shorted and inductance LS was measured, the figures were stored. After that, the figures of two measurements were matched.

The result

The inductance LS has no changes with accuracy about a percent.

## OPTION 2

A special sep up was used, consisted from an analogical oscilloscope, digital voltmeter and generator to measure a voltage on the inductance LS without shorted L2 and with shorted L2.

After measurements all results were matched.

Schematics of the setup

Generator

Oscilloscope

Voltmeter

100 Ohm

Frequency 10 kHz

L1

L2

#### An order of measurements

Voltage on resistor by oscilloscope was measured, and voltage on inductance by voltmeter was measured before and after shorting L2

#### The result

The voltages have no changes with occurrence about a percent.

Before the measurements, the voltage on L1 and L2 were measured. The voltage on both halfs was a half of the voltage on the total inductance LS.

#### Remark

The frequency about 10 kHz was chosen because a coil did not have parasitic resonances at this frequency and for low frequencies.

All measurements were repeated for coil with ferromagnetic transformer E - core. All results were the same.

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