Prof. Dr-lng. Konstantin Meyl

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For example if the brightness decreases, if the experimenter touches the ground wire of the 

transmitter, he is now the receiver.

 

2.8 Conclusion

 

There is a feedback from the receiver to the transmitter, as can be observed here. With the 

transmission of radio waves no such feedback should be determined. Only with resonance 

between transmitter and receiver, scalar waves are developed. If the transmitter is unplugged 

or the generator frequency changes and leaves so the conditions of resonance, no more energy 

is transferred.

 

2.9 Consequences

 

Numerous interhuman effects are based on the principle shown in the feedback from the 

receiver to the transmitter. They are in this way for the first time physically modelled. At the 

same time it becomes clear that the as esoteric classified coherences are nothing else than scalar 

wave effects. These effects are wrongfully designated as para-science, because scalar waves 

are still unknown to the scientific world. The feedback shown in the experiment proves the 

existence of scalar waves!

 

2.10 Utilities:

 

Demo kit like in experiment 1.

 

Using the experimentation kit: pancake coil "A" with middle wire length

 

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- 1 3 -  

3rd experiment, subject: 

Proof of free energy

 

3.1

 

Experimentator: Prof. 

Dr.-Ing. Konstantin Meyl 

3.2

 

Place and date: 

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

3.3

 

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

It is a physical law, after which the field strength decreases with the square of the distance. As 

consequence of the law received power is generally smaller than the transmitted. The field 

strength continues to decrease quadratically with the distance.

 

3.4 Expectation according to the scalar wave theory by Konstantin Meyl

 

The transmission with scalar waves has no power attrition during transmission (quod vide 1st 

experiment). The dielectric between the two spherical electrodes is open and therefore able to 

interrelate with scalar wave fields from the environment. If such fields with appropriate 

frequency and phase position are present, efficiencies from over 100 % are not to be excluded, 

even expectable. Finally, it concerns an open system!

 

3.5 Experimental setup and carrying out the experiment

 

The transmission circuit is adjusted as described in experiment 2. The LED's at the transmitter 

coil are to be out, while at the receiving coil they have to shine. Further look first for the 

resonant frequency please (receivers shines) and then the amplitude has to be accordingly 

reduced. Subsequently, with the frequency controller, check again whether it is the correct 

point. There is the possibility that the receiver lamps light up at several frequency values, but 

only at the correct value the feedback to the transmitter is so strong that the transmitter lamps 

fade out completely.

 

3.6 Interpretation of the experimental results

 

Both coils should be identical (same numbers of turns, same wire length, same couple coil). 

Thus makes sure that the inductively coupled voltage should be larger than the receiptable 

under normal conditions. As a matter of fact it is vice versa. On the receiver side values over 

the threshold voltage of the LED (2 V) are reached, while on the transmitter side they are not, 

because the LED's on the receiver side shine, whether on the transmitter side they do not. The 

load by the LED's is identical in both cases, so that the higher voltage leads compellingly to a 

higher current and a higher power. That is, it will more power be received than the transmitter 

delivers.

 

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-14-

 

3.7 High frequency measurements

 

If the appropriate measuring technique is available, the into the transmission coil fed high 

frequency power and the received high frequency power can be measured directly. In addition 

a short laboratory cable replaces the shorting plug between waveform generator and the 

pancake coil and the current signal is measured with current measuring pliers (for high 

frequency measurements). The jumper is brought in central position. Thus the connector 

sockets on the left side are activated, where the voltage measurement can take place. Due to 

the fact that between current and voltage a phase angle arises, the instantaneous values must be 

multiplied with one another (the Scope must support this computation!). This results in a 

likewise sinusoidal output curve with double frequency, whose average value can be consulted 

as measure for the fed power.

 

The high frequency measurement on the receiver side takes place completely similarly. The 

jumper is put in central position and the voltage is measured. A resistor of 100 ohms is 

recommended as load. With the current-measuring pliers the current flowing through the load 

resistor is measured. By optimal impedance matching of the load resistance and with 

appropriate reduction of the amplitude the efficiency can be increased still further.

 

3.8 Interpretation of the high frequency measurements

 

Efficiencies of approximate 500% are measured. An appropriate measurement with a 200 MHz 

power measuring device is printed in the 2nd book from the book series "electromagnetic 

environmental compatibility" in chapter 19.11. A control survey took place at the technical 

university of Clausthal at the 6th of July 2000. In the Institut for electrical engineering an 

efficiency was measured with two Tektronix measuring devices, which averages 1000%. For 

the large astonishment of the research workers, the received Power at the middle pancake coil 

of the experimentation kit was ten times the power, which was transmitted.

 

3.9 Circuit analyzer measurements

 

Not each Institute has the necessary equipment, in order to be able to make high frequency 

power measurements. That applies especially to private researchers and schools. For this 

group, the third jumper position on the coil plates was designed (DC load). In this position the 

high frequency signal is applied to a bridge rectifier, and a condenser is loaded with the 

rectified voltage. On the right side of the plate are two sockets, at which DC voltage is 

impressed. It can be assumed that nearly everyone has a simple multimeter, which indicates the 

voltage level in DC position. The load resistor of 100 ohms is already on the plate, so that the 

converted power U

2

/100 ohm can be made directly out off the voltage measurement.

 

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