V. ROSCHIN & S. M. GODIN SEG Testing of Small Prototype to Investigate Searl's Effect.pdf

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V. V. ROSCHIN & S. M. GODIN

Searl Effect Generator

New Energy Technologies, Vol. 2, pp. 242-245

Testing of Small Prototype to Investigate Searl's Effect

S. M. Godin and V.V. Roschin

The authors go further in the research of possibility to receive free energy by means of

rotating constant magnets (Searl’s Effect).

The aim of generator compact model (GCM) testing was studying of possibility to produce a

small and maximum cheap model, which uses the ceramic magnets. Laboratory research of

this model of generator was aimed at the discovery of self-generation effects and effects of

weight change, which were already achieved on the full-size generator [1].

A general view of GCM is shown in Figure 1. The generator represented a mechanical system

consisting of general construction as a cylinder made of stainless steel divided by it height in

approximately two equal parts. The direct current motor with collector was situated in the

lower part; windings of stator and rotor were connected in series.

Figure 1

In the upper part of the construction on the axis of motor the rotor is situated as a cylindrical

ceramic magnet with a central hole made on the base of cobalt-samarium mix. The magnet is

magnetized vertically and inserted into the steel fixture, which preserves the magnet from

destruction during the quick rotation. Small magnetic rollers also made of ceramic magnets

and magnetized along the axis of rotation were placed around the rotor. All 12 rollers were

placed into the aluminum cylinders, which preserve their brittle ceramics from mechanical

impact during the work in emergency conditions. The main idea of such construction consists

in the fact that in initial state the rollers were attracted by the magnet of rotor to the side face.

Due to the repulsion of the rollers from each other, the distance between them appeared

automatically. With this distance they uniformly distributed along the entire perimeter of the

rotor. During acceleration of the rotor the rollers diverge from the rotor step by step and begin

to run in the outside cylindrical fixture, which is placed around the rotor at the distance of 1.5

mm from the external surface of rollers in the initial states. The height of the rotor magnet is

24 mm, the diameter of the inside hole is 40 mm. All other geometrical sizes and ratios are

given in Figure 2.

Figure 2

It was supposed that with a certain acceleration of rotation the rollers would begin to rotate

inside the outside fixture with self-acceleration and would carry metal surface of rotor device.

This mode will be easy to discover due to the possible decrease of the current consumed by

the electric motor. Thus, the aim of GCM testing was an attempt to find the features of energy

transformation of environment which lies in the self-acceleration of the rotor device or other

characteristic effects concentric magnetic walls around the device and fall of temperature)

discovered already. The program of device testing included registration of dependence of

rotational speed of the rollers along the outside fixture from rotation speed of the motor.

Appearance of GCM is shown in Figure 3, when this device is ready to test in laboratory

conditions. GCM was placed on the massive grounded steel plate. The power supply made in

the form of controlled transformer, isolating transformer, bridge diode rectifier and capacitive

filter were placed on the right. Besides, the generator of reference frequency G3-112 and

frequency meter C3-54 were placed here.

Figure 3

The 2-channel oscilloscope C1-99, digital combined unit TSH300 applied for the

measurement of consumption current and power supply TEC-88 (0-30 V, 0-2.5 A) applied for

power supply of the optoelectronic sensor of device rotation were placed on the left. The

measurement of rotation speed of the rollers was made with an induction-type sensor, which

was placed at the height of the rollers, on the reverse side of the aluminum fixture. The rollers

after they separated from the rotor, rolled along this fixture. During the passing of every roller

by the induction-type sensor, the impulse of voltage with the amplitude of about 1V was

produced. This voltage was supplied to one of the inputs of 2-channel oscilloscope for direct

observation on the screen. A signal from the reference generator connected with the frequency

meter was supplied to the second input of the oscilloscope.

Synchronization of scanning of the oscilloscope was provided from the same reference signal.

The frequency of the signal on the reference generator was set to provide the most stable

immovable pattern on both channels of the oscilloscope. An accurate measurement was made

according to the data from the frequency meter. Such method of measurement was chosen

because the applied collector motor of direct current ad permanent deviations of rotation rate

due to the change of voltage in the mains, heating of bearings, collector and other reasons. All

this hampered the reception of an accurate value of average rotation rate directly from the

readings of the frequency meter. It was necessary to divide the readings of frequency meter by

12 to receive the real value of rotation rate in rates per second (rate of running around the

fixture) of the rollers.

Measurement of rotation rate of the rotor was made in an analogous way, but as a sensor we

used the self-made sensor on the base of optic pair IR emitter-receiver with an open optic

channel. The sensor was assembled on the textolite baseplate and attached to the upper

plexiglass head of GCM by means of usual plasticine. Using this sensor we could quickly and

effectively adjust the necessary operating gap between the surface of optoelectronic couple

and surface of special metal disk with 25 dark and 25 light sectors applied on it. Thus, during

one rotation period of the rotor the photon-coupled sensor gave 25 impulses of voltage, which

were transferred to the oscilloscope for immediate observation. The appearance of photon-

coupled sensor or rotations attached to the upper plexiglass head of the GCM unit is shown in

Figure 4.

Figure 4

In Figure 5 you can see the oscillograms of signal from the photon-coupled sensor of rotation

(upper beam) and harmonic signal from the reference generator in the moment of coincidence

of frequencies with a one-phase accuracy. The real rotation rate of the rotor was determined

as a measured frequency (rate) of generator divided by 25 (number of dark and light sectors

on the disk of rate controller).

Figure 5

To receive reliable information on the characteristics of the electromechanical system ‘motor-

permanent magnet of the rotor’ there were made several bare measurements without

installation of the rollers. Measurements were made with the placing of magnet north up and

vice versa.

As we can see from the diagrams of dependence of the motor consumption current from the

applied voltage of power supply, the strength of consumption current increases with the

voltage of power supply and reaches its maximum at 0.31 A with the minimal possible

rotation rate of the rotor. The strength of consumption current does not depend on the polarity

of installation of the magnet in the limits of experimental accuracy. For the given motor there

is an area of minimal consumption current, which lies in the diapason from 40 to 80 W.

We got similar curves of rotation speed for the cases of different location of magnets of the

rotor, which means the independence of rotation speed from the polarity of the magnet of the

rotor.

The results of measurements of rotation speeds of the rotor and rollers (given separately) are

presented in Table 1.

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