Research website of Vyacheslav Gorchilin
2024-09-27
All articles/Inductor
Two toroidal coils and short pulses. In the of this experiment, we will study the unusual properties of a toroidal coil , but in terms of voltage and power transfer from one TC to another. Classical electrodynamics denies this possibility, since the formulas and necessary fields from which this could follow are absent there. According to our hypothesis, the appearance of an external magnetic field around the TC indicates the appearance of a second magnetic field there. Only it can be responsible for the transfer of voltage and power from one torus to another, which will be discussed in these experiments. In the first part, we will transfer voltage, and in the second, power. .
Scheme of the experiment with two toroidal coils
For the experiment we will need two toroidal cores made of nanocrystalline, with the same dimensions and permeability as in the . Two transformers are made from them: T0 and T0 . The first transformer T0 is a transmitting one, on the ring of which two turns of thick copper wire are wound and connected to the generator GG0. The generator for it is also taken from the previous experiment. The second transformer T0 is a receiving one, made in a similar way, only its two turns are connected to the oscilloscope OS0, and on the opposite end of the torus another turn W0 is wound, the ends of which are necessarily 0 with each other. T0 is placed directly above T0, or T0 - above T0. Figure 0 shows in more detail the experimental scheme in the form of a scan, if the structure of two TC rings is rotated around the OX axis. Note also that the turn W0 is not used yet, and the magnetic field formed by the current of the generator GG0 is completely closed in the ring T0. . In the first experiment, we should receive a signal on the winding W0, despite the fact that according to classical views, there should be no voltage on it, since the transmitting transformer is wound in a classical way. But in the receiving transformer T0, the design is made in such a way that it can receive the component of the second magnetic field. This is achieved by closing the winding W0.2. The presence of potential from a non-classical field on the receiving winding T0 can be judged by the oscillograms , which show the reaction of W0 to a change in voltage in the transmitting winding \ of the transformer T0: \[ U_{W0.1} \sim {d U_{W0.1} \over d t} \tag{3} Although in a classical transformer the voltage on W0 would simply be proportional to the voltage in W0 \[ U_{W0.1} \sim U_{W0.1} \tag{4} This can be verified by connecting the oscilloscope to the ends of the previously unused winding W0 . From the oscillogram it is evident that the voltage on W0 and W0 are proportional to each other. From this we can conclude that the voltage transfer by the classical method and the method presented here has a fundamental difference. .
However, the power transfer from one winding to another in this experiment is relatively weak, despite the fact that transformer T0 may heat up a little after long operation. If the receiving winding W0 is made of 0-4 turns, then an LED can be connected to it, and with a larger number of turns, even an LED matrix. At the same time, if 0-3 watts of power from the generator are given to the transmitting T0, the LEDs will glow, but the power dissipated on them will be tens of times less. But what is interesting is that connecting LEDs and even completely short-circuiting the winding W0, nohow 0 the current consumption of the GG0 generator. Moreover, the current consumption was measured with a precise device that could show the difference if it were a classic transformer. . Transmitting power. In the next experiment, it was the turn of the W0 winding , to the ends of which a capacitor should be connected. The author's capacity was 0 nF, but its optimal value should be selected by the experimenter for a specific magnetic circuit, generator and pulse duration. Such a capacitor should withstand good reactive power and not heat up. Figure 0 shows the basic diagram of this experiment, and Figure 0 shows the oscillogram at the transmitting and receiving ends. The mutual arrangement of the transformers is the same as before. .
Schematic diagram of the second experiment
It is necessary to pay attention to the oscillogram of the pulse of the transmitting coil W0.1. After installing the capacitor C0 in the circuit, it turns into a smooth envelope, and its front is a set of oscillations, studied earlier as the . Moreover, the very first oscillation has a sharper front and decline than the others, and is smaller in amplitude than the others. Despite this, at the receiving end, this oscillation has the largest amplitude, which directly follows from formula . And generally speaking, only these high-frequency oscillations get to W0.1. The smooth envelope does not get to the receiving coil. . It cannot be said that such power transfer is very effective, but even with this inclusion, the load R0 does not affect the consumption of the generator GG0 in any way. Even with R1=0. To increase the efficiency of transmission, the correct selection of the number of coil turns, capacitors and load matching is required. Inventor Don Smith said that it is also important to match the ratio \ with the pulse length, where \ is the inductance of the matched winding, and \ is its active resistance. . Conclusions. The experiments conducted here showed the very possibility of transmitting voltage and power through toroidal coils. According to classical concepts, such transmission is fundamentally impossible. . It has been experimentally established that the influence of the secondary winding on the primary is possible only with a directly proportional relationship between the voltages between them . If the relationship between the voltages on the secondary and primary windings is realized through the second magnetic field, according to formula , then the influence of the secondary winding on the primary is not recorded. . In these experiments, the transmission efficiency was relatively low. For more efficient power transmission through the second magnetic field, it is necessary to develop a perfect design of the transmitter and receiver, coordinating and calculating all the necessary parameters for it. .  . . .
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