- 6 -
0.7 Description of the frequency counter (experimentation kit)
With the frequency counter also a period measurement or an event counting can be made apart
from the frequency measurement. Thereto the jumper 1 and 2 must be set accordingly. The
function-table is imprinted on the plate. Also the gate time is selectable with the jumpers 3 to 5.
0.8 Safety instructions
The entire arrangement is operated by the enclosed low-voltage wall power supply with test
seal (respectively batteries) and thus with a low and harmless operating voltage. A danger of
an electric shock is therefore impossible with the original kit (and the provided wall power
supply). Nevertheless it is to be made certain that short-circuits (e.g. by metallic objects or
lines) on the plates are avoided. This can entail the overheating of components or the
destruction of the device. Besides no liability for damage of any kind is assumed, which was
caused due to inappropriate treatment and/or use and/or the use of other respectively additional
components, not contained in the kit and their combination with the kit!
-7-
Experiments with scalar wave transmission
1st experiment, subject:
Energy transfer
1.1
Experimentator: Prof. Dr.-Ing. Konstantin Meyl
1.2
Place and date: D-78112 St. Georgen, 21st of June 2000
1.3
To the status of physics of electromagnetic waves (according to Heinrich Hertz)
It is a physical law, after which the field strength of waves according to Hertz (radio
communication and radio waves) decreases with the square of the distance. If the distance
between transmitters and receivers is doubled, then thereby the power of the receiver decreases
to a quarter.
1.4 Expectation according to the scalar wave theory by Konstantin Meyl
The wave equation says that beside the wave according to Hertz still another further wave, the
scalar wave, must exist. In contrast to the wave according to Hertz, the scalar wave spreads not
with constant speed, and also not evenly in all directions. Only a middle velocity of
propagation can be indicated, which can deviate from light speed substantially. A scalar wave
aligns itself with the receiver, were the streamlines of the field bundles themselves again.
Without dispersion the received power in case of resonance should correspond approximately
to the sent power. Therefore it should be possible to transmit both: information and energy.
-8-
Now the waveform generator must be attached with the help of two short circuiting plugs to the
couple coil of the pancake coil. These coil works as transmitter in this system. Now the
connection of the provided wall power supply is put into the socket designated for it on the
waveform generator plate and connected with a 230V wall outlet. The red control lamp signals
that voltage is impressed on the plate and that the generator is working.
Fig. 5: Connection of the waveform generator to one of the two pancake coils.
The other pancake coil with mounted spherical electrode is used as receiver and loaded with the
light emitting diodes. The jumper must be put both on the transmitter, and on the receiver on
position LED. The distance between transmitter and receiver should be selected first
consciously quite small (approx. 50 cm). The points of grounding, that are the outside ends of
the pancake coils, are to be connected by a laboratory cable. 6 meters black cable is designated
for it.
1.6 Carrying out the experiment
It can be assumed, that the frequency controller is not in the right position first and no self-
resonance is reached. The amplitude controller is untwisted, until the threshold voltage of the
light emitting diodes is crossed by 2 V and the LEDs on the transmitter plate brightly shine.
Now, the "rough" frequency controller ("fine" potentiometer in central position, sine form,
amplitude fully untwisted, frequency range: HI) is adjusted, until the
on the receiver mounted
light emitting diodes begins to shine. The power maximum is set, when the light emitting
diodes shine brightest. The shining of the receiver diodes proves that a energy transmission
- 9 -
takes place. If the one LED should shine somewhat more brightly as the other one, then this
signals a little unbalance of the sinusoidal supply voltage, because the positive half wave is
used by one - and the negative half wave by the other diode. This can be during an
asymmetrical load.
The distance between transmitter and receiver can now be increased. The distance can be
quadrupled for example, as the receiver is continually pulled away from the transmitter. It
could be that now on the receiver side less or nothing at all can be recognized, which is a
corollary of the changed resonance frequency of the system due to the larger distance. This has
to be compensated by adjusting the controller, until an power maximum is to be observed. The
small lamp will shine as brightly as in the experiment with the small distance, which contradicts
the law of square declension of the received energy conditional on the larger distance.
1.7 Interpretation of the experimental results
According guidelines of Tesla transmitter and receiver are operated grounded. The better the
grounding and the better the coupling over the grounding connection, the more simply it is to
find the point of resonance. The grounding wire used within the experiment is therefore
primarily an easement for the operator. This can be determined very fast, as a worse
connection is tried out e.g. over the central heating, over the earthing contact of the power line
or with a direct connection to earth outside. It can come to the fact that at such a grounding
inadvertently still different more "receivers" (e.g. biological systems) hang, which go into
resonance and withdraw the transmitter's energy.
This problem can be avoided by connecting the points of grounding by a cable directly. Even if
the grounding connection should
be understood as conductor, then, for a closed electric circuit,
the other conductor is missed. That is formed in this experiment by the transmission line. The
Shining of the small lamps proves that energy has been transmitted.
If it would have been waves according to Hertz, only the sixteenth part of the power might have
arrived by the quadrupled distance. (1/4)
2
= (1/16). Whereas it can be observed that the
received power with increasing distance does not decrease. For very large distances it might
happen that the resonance is missed and the oscillation fades out. If several receivers go into
resonance, it comes to an allocation of the emitted power or more distant receivers receive less
power respectively.