SU17500A1 - Device for the technical use of the phenomenon of polarization of dielectrics by passing an electric current through them - Google Patents

Description

The present invention is based on the open, the applicant and the publicly distributed by him together with W.C. Ron% enoM in 1923 (Annalen der Physik, TV Folge, Bd 72, S. 472) the phenomenon consisting of that atom when passing through a dielectric; Normal current crystals with naparasevia up to 10,000 volts and higher are crystal fields and the electromotive force of polarization reaches the value of the potential. Accordingly, a polarized dielectric can then serve as a source of high-current voltage. Experience has established that only a thin dielectric layer adjacent to the electrode on the cathode side of VTOKa is subjected to polarization, while the remaining thickness of the dielectric does not affect the degree of polarization of the layer. Further studies have shown that perfectly other dielectric insulators, or semiconductors, behave in a very similar manner to dielectric crystals. Even non-crystalline, with the indispensable condition, however, that. they

must be firm, y.chie viscous consistency. For example, very satisfactory results were obtained with the use of calcium carbonate, aluminum phosphate, alumina, cement, drying oil, and other dielectrics.

According to the invention, to use the phenomenon of polarization of a dielectric, a device is proposed in which the following objectives are used: electrical engineering system of alternating thin-layers of solid or viscous dielectric or long-conductor and one in the same thin metal st; layers of dielectric and metal, as an independent whole, can be used to accumulate electrical energy as a high-voltage battery. In this case, the metallic layers are interconnected in parallel through one, forming two groups of metal spacers in a layered dielectric. 1E, each of which, during the process of polarization (charging), is connected to one

from the position of the voltage. So, for example, the deposition of colloidal stones, bonded with viscous organic matter, or cement, in thin layers of approximately 0.01 g, between aluminum layers of equal thickness and charge, preferably when heated to temperatures above 100 ° C, up to several tens of thousands of volts, it is then possible to get most of the electricity transmitted during a voltage that continuously decreases

from the maximum of the electric voltage applied to zero energy, high voltage delivered by the battery, can | be transformed to low incidence

conventional methods.

A diagram of such an battery is shown in the attached drawing.

 Including a high-voltage armature cable with a DC machine and; |: And with a rectified alternating current, you can use it as an equalizer1 (G voltage.

High voltage battery can

also listen as a capacitor of a very large capacity and a very high fractional voltage.

Coating wire of high distribution:, depending on the magnitude of the latter, one dielectric layer, the external surface of which 9 has a zero potential; , or by means of 1; 1; edec | rik, n |) chambered metal, assessing, with the pedestal of the outer surface of such a cover, to zero, it is necessary to destroy the external electrical fraction of the conductor and thereby protect it. from the discharge, and from the possibility of a short circuit. So, for example, according to the author, a layer of drying oil of 0.05 mm should destroy a conductor's field of 15,000 volts without a breakdown. To protect a conductor carrying a current of 100,000 volts, seven layers of dielectric C with six metal layers would be required accordingly. Secretly, high-voltage insulators can be arranged. Once polished, onk; keep the charged body from being charged.

Finally, taking into account that the attraction of the electrode to the polarization layer reaches several tenths: -E. D.:,; . -

For thousands of atmospheres, the applied diedectrique can be used to obtain a lot of mechanical forces and peeling when attracted to the polar layer ..,

Thin layers of dielectric material were obtained in various ways. 1) by applying the substance in a viscous or colloidal state, followed by drying or, by heating,

2) alternately deposition of dielectrics and metal by sublimation in vacuum or in a gas, which, reacting with the precipitate, gives the required dielectric,

3) electrolysis, sometimes followed by a reaction, 4) cathode mechanical sputtering.-fe) separating out solution or colloid, 6) others and giving sufficiently thin layers, such as: pressing, rolling, etc.

The subject of the patent.

1. Device for the technical use of the phenomenon of polarization of dielectrics by passing through them an elec- trographic current, which is characteristic of. using, for the purpose of accumulating electrical energy or protecting the charge-carrying conductors from the discharge OR: short circuit, alternating thin thin fields, black solid layers or a viscous dielectric or semiconductor and such metallic thin layers.

2. When used as described in l. 1 device for high voltage electric battery nsf parallel connection alternating: e layers of metal with the aim to produce two piles of metal spacers in a layered dielectric, each group charging the battery, respectively, to one of the high voltage source positions. ,,

3. Application of high-voltage electric battery built-in. according to p / 1, as a large-capacity and high-punching cotsdensatr

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4. Application of a dielectric in accordance with claim 1 of the dielectric to obtain large mechanical forces and bonding when attracted to the polarized layer.

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Patent A.f lIoffe M 17500

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