Prof. Dr-lng. Konstantin Meyl



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- 1 8 -

 

aware of that. The transmitter lamps continue to shine completely unaffected, what from the 



conclusion is to be drawn that this time no power is withdrawn. It has to be the wave, 

according to Hertz. For checking purposes the grounding on the transmitter coil is unplugged 

and plugged again. Whereas the receiver lamps fade out and shine, respectively. On the 

transmitter however no reaction can be recognized. The brightness of the lamps does not 

change at all.

 

4.7 Interpretation of the experiment



 

The missing feedback on the transmitter is an indication for radio waves, which only in close range 

can bring the receiver lamps to shine (law of the square-distance). Further indications are that at 

this point the receiver lamps do not shine more brightly than those of the transmitter and the degree 

of efficiency generally is below 100 %. If the distance to the transmitter is increased, the received 

power slowly fades out. Finally the transmitter can be put into a Faraday cage. The receiver lamps 

fade out immediately. Mostly it is sufficient to hold the hand before the receiver electrode in order 

to prevent the reception. Observations should be taken alternating at the two points of resonance, 

because particularly the direct comparison of the measured wave characteristics at the two points 

makes it clear, that with the low frequency (4-5 MHz) wave, according to Hertz is used, while with 

the high frequency (6-7 MHz) the scalar wave, according to Tesla is used.

 

4.8 Conclusion



 

The coil length and thus the wavelength were not changed, so that from a frequency change a 

change of the propagation speed follows directly. Both stand in direct proportionality to each 

other. If the frequency of the scalar wave is higher than those of radio waves, so that the 

frequency controller must be turned further toward the clockwise direction, then this wave is 

faster than light.

 

If a frequency counter is attached, it is recommended to note the two frequencies and compute 



afterwards the percentage of the larger (longitudinal) to the lower (transversal) frequency. The 

result is undoubtful: The scalar wave signal is approximately 1.4 to 1.6 times faster, than the 

electromagnetic radio wave. (typical values with the middle coil length are: Frequency of the 

scalar wave 6.7 MHz/radio wave 4.5 MHz =1.5 C/C the scalar wave has the factor 1.5 of light 

speed).

 

4.9 Consequences



 

Scalar waves are modulatable and can carry information. Therefore the acceptance, that light 

speed is the highest border for signal transmission, as Einstein insisted, is to be contradicted. It 

is still the correctly accomplished experiment that is able to show the physical reality and not 

any devious assumptions of a theoretical physicist.

 

4.10 Utilities



 

Demo kit, like in the experiment No. 1. Using the experimentation kit: first the coil with the 

middle wire length is used. With the other two coil sets the experiments can be repeated.

 



-19-

 

5th experiment, subject: Ineffective Faraday cage



 

5.1


 

Experimentator: 

Prof. Dr.-Ing. Konstantin Meyl 

5.2


 

Place and date: 

D-78112 St. Georgen, 21st of June 2000 

5.3


 

To the status of physics of electromagnetic waves (according to Heinrich Hertz) 

The Faraday cage is based on the principle that the inside of an electroconductive body remains 

field-free. It is used, in order to shield radio waves. Provided that the electromagnetic wave 

only consists of waves, according to Hertz, nothing may penetrate a Faraday cage. If the 

transmitter is outside, the inside of the cage is allegedly field-free. Is the transmitter inside the 

cage, e.g. a microwave oven, no wave should be provable outside.

 

5.4 Expectation according to the scalar wave theory by Konstantin Meyl



 

The scalar wave has characteristics, which empower it to penetrate a Faraday cage. The scalar 

wave is able to tunnel. It must be only sufficiently fast. Furthermore a resonance between 

transmitter and receiver is required.

 

5.5 Experimental setup



 

For this experiment we need a Faraday's cage, into the transmitter is to be put. For that, the 

provided metal suitcase is suitable, which is opened and placed unfold on a side.    The

 

 




In addition, a hamster cage made of metal or a microwave oven can be used. It is advised to 

pay attention, that lattice cages possess a certain critical frequency. The higher the frequency 

and therefore shorter the wavelength of an electromagnetic wave is, the closer must the lattice 

bars of the cage lie together. The wavelength of microwaves is approximately 5 millimeters. 

That corresponds to a frequency of approx. 60 GHz. The waveform generator produces 

frequencies of 1-20 MHz. Thus at least a percentage of the wavelengths from the waveform 

generator to the microwave oven of 3000:1 is given. That means, for our experiments, a cage 

with 3000 times larger lattice spacings would actually be sufficient. Using the microwave oven 

as shielding cage, which is prooved for high frequency impermeability, our experiments with 

relatively low frequencies are on the safe side. The power plug should have been pulled and 

the oven must not be activated in any case.

 

The cable connection has to be plugged into the receiver and has to be connected with the 



transmitter, wich has to be electroconductive connected to the cage (using a microwave oven 

for example, with the help of an alligator clip at metal parts). The aluminium suit-case is 

equipped with sockets on both sides.

 

- 2 0 -




-21- 

5.6 Carrying out the experiment

 

The amplitude controller is fully untwisted. It does not care whether the transmitter LED 



shines. Arbitrative for the success of the experiment is the fact alone whether a chance exists to 

bring the receiver LED to shine. For this purpose the frequency controller of the waveform 

generator is adjusted, till on the receiver side a maximum can be observed.

 

Who has doubts, the line cord to the waveform generator can radiate any high frequency, can 



use a 9-volt-battery in stead of the wall power supply , which is accommodated also in the cage. 

If the cage is closed, no more cable usher into the cage in this case. Only the cage itself is 

connected from outside with the receiving coil and from inside with the transmitter coil. Now 

the caged transmitter can swing as much as it wants. Outside of the cage nothing at all might 

arrive, according to educational books.

 

5.7 Interpretation of the experiment



 

If the lower frequency (the wave, according to Hertz) is adjusted, it is obviously recognizable 

that the smallest shielding leads already to the fact that the receiver lamps fade out. The higher 

frequency during a scalar wave transmission behaves substantially more resistant. A gap in the 

door or a cable, which leads out the suitcase, is adequate for a perfect coupling. In equally the 

small lamps on the receiver plate shine within a hamster cage or with a mouse lattice almost 

unimpressed. All previous experiments can be repeated and it is incidental that a transfer of 

energy, a feedback and even an increase in output are possible. Attention is payed to, that the 

resonant frequency between transmitters and receivers is affected by the cage, which makes a 

readjusting of the frequency necessary. The cage increases the surface and thus the capacity, so 

that the resonant frequency drops on substantially lower value (typical 4 to 5 MHz using the 

middle coil).

 

5.8 Conclusion



 

If the Faraday cage is not too close meshed, it does not represent a considerable barrier for the 

transfer of energy. Substantially at this result is the circumstance that a signal can escape from 

the cage. So somewhat is measurable, which may not be. This experiment reveals a completely 

substantial characteristic of the scalar wave.

 

5.9 Consequences



 

If the Faraday cage cannot affect scalar waves, no possibility is known to shield the scalar 

component of a wave. If during tunnel experiments the waves are confronted with a barrier, 

which should be actually insurmountable and if, albeit of this fact, signals behind the tunnel are 

measured, which are besides faster, as expected, then a scalar wave is received without doubt, 

(e.g. Professor Nimtz, 2nd physical Institute of the University of Cologne)

 

If architects sell their customers shielding mats against electromagnetic pollution, these mats 



shield only radio waves and no scalar waves. Which of both waves is biologically active and 

responsible for the electromagnetic pollution, has to be ascertained.

 

If somebody seeks shelter from scalar wave radiation, a scalar wave receiver is recommended, 



which is in resonance with the jammer and absorbs the sent energy. Whether such a device 

actually functions, can be recognized by the fact that a measurable output is perceivable: A 

small lamp shines or a component becomes hot.

 



 

Fig. 10: The closed aluminium suit-case with externally connected receiver

 

5.10 Utilities



 

Demo kit, like in experiment 1, additional the aluminium suit case as Faraday cage. 

Using the faraday cage, the experiments 1 to 4 are repeatable.

 

- 2 2 -




- 2 3 -

 

6th experiment, subject: 



Refutation of the near field interpretation

 

6.1



 

Experimentator: Prof. 

Dr.-Ing. Konstantin Meyl 

6.2


 

Place and date: 

D-78112 St. Georgen, 1st of July 2000 

6.3


 

To the status of physics of electromagnetic waves (according to Heinrich Hertz) 

For the refutation of the near field interpretation, it has to be calculated first, at which distance 

between transmitter and receiver the near field ends. This happens at 

 

6.4 Expectation according to the scalar wave theory by Konstantin Meyl



 

At 7 MHz it might therefore not be possible any longer, to bring a small lamp to shine, 

particularly because the near field is the scalar wave component. However, the computation of 

the near field and its range always takes place on the assumption of propagation with light 

speed. Scalar-wave can, against the doctrine, be faster. So that, according to the theory of Meyl, 

it can be expected that the transmission of energy is still possible over larger distance.

 

6.5 Experimental setup



 

The transmission circuit is set like in the experiments 1 to 3. The frequency is adjusted to the 

point of maximum luminosity of the receivers LED. The LED's on the transmitter side are 

unimportant for this experiment.

 

6.6 Carrying out the experiment



 

The connecting cable, which is designated by Tesla as "grounding", is lengthened to more than 

6 meters by an extension cord. The frequency is tracked and the maximum value has to be 

checked.


 

6.7 Interpretation of the experiment

 

It was always possible so far and the measurements will confirm it, that with distances of more 



than 6 meters the light emitting diodes on the receiver can be brought to light. Thus it has been 

shown that still outside of the near field a transfer of energy is possible. The finding of the 

maximum becomes more difficult. The longer the connection cable or the more potential 

receivers are connected (for example the heating installation or a water pipe), the rather the 

oscillation breaks away or the resonance breaks down. Then, immediately, no receipt is 

possible any longer. After such a break the distance must to be shortened, till the resonance is 

present. After than, the distance between receiver and transmitter can be extended again. 

In the course of the lecture alternative electrical engineering", students increased the distance 

to 60 meters and made measurements.

 

6.8 Conclusion



 

As it is possible to receive the full transmitted power, even at the tenfold distance, a frequently 

mentioned argument of high frequency technology is disposed of once and for all. 

The experiment can be expanded, if necessary, with the goal of showing the standing wave 

character as proof for the existence of longitudinal waves. As long as power is consumed, the

 



- 2 4 -

 

lines of flux are bundled at the receiver, whereby the standing wave character is lost. It is 



therefore recommended, that no jumper is set. Only measurement-devices with very high 

resistance, an oscillograph for example, should been used to control the voltage impressed at 

the coupling coil of the receiver. If the distance between the transmitter and the receiver is 

varied, the chance to proof the standing wave character exists by locating the nodal points.

 

6.9 Consequences



 

The near field of an antenna is the scalar component of a wave, whereas the scalar wave, vice 

versa, is more than the near field! It is an electrical longitudinal wave, which propagates 

towards the pointer of the electrical field.

 

6.10 Utilities



 

Demo kit, as in the experiment No. 1. Extension cords with different length. Using the 

experimentation kit: Coil with middle wire length.

 



- 2 5 -  

7. Experiments with the experimentation kit

 

First only the coil with the middle wire length was used in the experimentation kit. But still 



two further coil sets are provided, on the one hand a coil with the double wire length, 

recognizable by the high number of turns, on the other hand a coil with the half wire length. 

Using these coils, the experiments 1 to 5 can be repeated. Additional harmonic wave 

experiments are possible by combining the different coils. In this case attention should be paid 

to the fact that with the number of windings also the transmission ratio of the air cored 

transformer changes. The couple coil is identical at all variants with 5 windings. It can be 

modified, if necessary, on the lower surface, whereby an abbreviation to 4 turns is possible.

 

 



The waveform generator is only preset at the demo kit. The experimentation kit offers further 

adjustment possibilities. By turning-over the two switches form 1 and 2 to rectangle, the 

harmonic content can be significantly increased, which pulse-width is stepless adjustable. That 

can be helpful for experiments with mixed groups of coils, e.g. with a transmitter (high number 

of turns) and with two receivers (middle coil length).

 

Here is the fantasy of the experimenter in demand. Please write your own protocols and arrange 



them, given in the sample. We will try to reconstruct the experiment according to your 

description. We will, as the case may be with additions, collect your protocols together with 

others. We will send those protocols in a file to all buyers, who made own protocols. With this 

measure an incentive for own experiments is given and the feedback, which is important for us, 

has been motivated. For those, who do not deliver protocols, the collecting file and additional 

instructions are purchasable. Till the completion is finished, it can take some years. About 

stock availability, contents, extent and the price we will up-to-date inform on our homepage.

 



 

Fig. 12: The Receiver is draining visibly electrical power from the Transmitter.



 

-26-



 

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