The charge separation. The analogue of the Tesla transformer
In this work, the author is one of the ways of separation of charge, which is able in some cases to replace the Tesla transformer. Based on the obtained effect can be effective to charge the capacitor, and even to transmit information or energy at a distance of non-classical way.
The science concerned with the problem of transfer spin currents, called spintronics . To obtain the separated spin-oriented charges it proposes to use heterostructures or some ferromagnetic materials, in particular, dzhozefsonovskikh transitions from an insulating ferromagnet, where you can control tunneling using an external magnetic field.
The author found an easier way of such a division. As it turned out, it is enough to set bandstop LC filter at the output of the sinusoid generator. The inductance of the filter should represent the coil core consists of two ferrite cups, with the obligatory gap, and its resonant frequency must be equal to the oscillator frequency.
Fig.1. The scheme of separation of spin-oriented charge (a) and devices based on it (b, c)
As is known from the theory of radio engineering, bandstop filter L1C1 does not pass on the XS1 output signal in the case where the resonance frequency equal to the frequency of the generator G1 (Fig. 1a). This means that in this case, ordinary radio signals will not affect the device connected to the output XS1. But as it turned out, this circuit is shared charges — about the same as it does in the Tesla transformer. Output ATT we get a spin-oriented charges that can be used for some unusual devices.
In figure 1b, to the output of the ATT, we connect the plug Avramenko, consisting of two diodes VD1 and VD2, the output of which is connected to the capacitor C1. Despite the fact that the second end of the device is connected to nowhere, we get the charge on the capacitor, the voltage many times exceeds the amplitude of the generator G1. The setup of this scheme is reduced to finding the maximum of the luminescence indicator of the electric field at the point the XS1. The same scheme is suitable for single-wire energy transmission.
Following the connection to ATT (Fig. 1c) even more interesting: the exit XS1 plug the antenna WA1 is a small piece of wire about a meter long and as receiver use the indicator of the second magnetic field. When you hit the frequency of the generator G1 are exactly in resonance bandstop filter (ZF), the led this indicator will light up when you than the selection of the resonant frequency of the core indicator is not required. Depending on the amplitude of the generator, thus, it is possible to wirelessly link up to 5-7 meters. Interestingly, the type of waves it will negritoski. If the scheme of the indicator to amplify the intermediate circuit with a resonant frequency of ZF, we obtain a new kind of radio to far greater distances!
Fig.2. The core of the two ferrite cups, with the gap h
Fig.3. Table ferrite cups
In the diagram in figure 1a a very important element is the inductance L1 represents the coil with two ferrite cups. Is also mandatory nachlichie gap between them. The author used a Cup P22/13 (Fig. 3), but this size is optional. It is important to observe a good quality filter than it will be more the better will manifest the effect. Consequently, the best way to wind the coil-the more turns the larger the wire diameter. For P22/13 optimal was 100 turns of wire with a diameter of 0.12 mm. the Clearance h (Fig. 2) ideally you want to pick up for each core — it multiplies the effect. It was established experimentally that for cups P22/13 he will be 0.4-0.5 mm. Clearance can be maintained by means of a ring of sturdy thin cardboard. Cups must be pulled between a non-magnetic bolt and nut.
The parameters of the ferrite cups for other sizes are given in the table in figure 3.
The materials used