DE102010052353A1 - Device for generating gravitational waves i.e. electromagnetic waves, has module for generating plasma to move ions of plasma in high-frequency vibrations, where ions are stimulated to high frequency vibrations by electric field - Google Patents

Abstract

The device (1) has a module for generating plasma to move ions (11) of the plasma in high-frequency vibrations with frequency. The ions are stimulated to high frequency vibrations by an electric field. Gravitational excitation of the ions is carried out such that a pattern of the gravitational waves is radiated with transverse quadruple characteristics. A vibration space (7) comprises a top electrode (8) and a bottom electrode (9) for applying alternating electrical voltage in order to generate an alternating electric field.

Description

The invention is directed to a device for generating gravitational waves.

Gravitational waves are generated by accelerated masses and manifest themselves in a change in the structure of space-time, which means that the acceleration of a system of several compact and heavy masses creates a so-called quadrupole moment, which causes gravitational radiation to be emitted. Although gravitational waves were predicted in 1916 by Albert Einstein in the context of his General Theory of Relativity, scientists worldwide have not been able to provide direct evidence for their existence. Although the astronomers Hulse and Taylor were awarded the Nobel Prize in Physics for calculations in 1993, the decrease in the orbital period of a double-stem system could be interpreted as energy loss due to the emission of gravitational waves; However, these studies are only an indirect proof.

Detecting gravitational waves and examining their properties would be invaluable to all science. On the one hand, this would provide a confirmation of the General Realtivity Theory; On the other hand, it would be possible to obtain important astrophysical information through the detection of natural gravitational waves, such as the Big Bang, the formation of the universe, pulsars, black holes, supernovae, and so on.

Conversely, if one were able to produce gravitational waves, they could be produced and examined in the laboratory; In addition, one could make these waves may be commercially useful, for example, to transmit information in areas that are intrusive to electromagnetic waves, for example, through the Earth's interior, etc. For if the assumption is true that gravitational waves in contrast to electromagnetic Waves hardly interact with the surrounding matter, they can pass this almost without loss of energy. Thus, one could imagine an information transport with the help of gravitational waves through, for example, planets, for example, on a direct route to a space station on the back of the moon.

As already mentioned above, an emphasis in the field of research on gravitational waves is the attempt to detect them. Among these are especially the works of Joseph Weber, who tried to detect gravitational waves by the use of tons of aluminum cylinders, which should serve as a resonator for incoming gravitational waves, cf. for example the US 3,722,288 , Since the effect of the natural gravitational waves is only very small, the proof by Weber's measuring setups has not yet been achieved or could not be repeated.

Another approach to the detection of gravitational waves is the use of interferometers, cf. for example the US 5646,728 However, these experimental setups bring some disadvantages and problems. The amplitudes as well as the frequencies to be measured are very small in relation to the possible disturbances. The directional dependence and external influences of the experimental environment, which distort the signal of gravitational waves, are difficult to control, and in some cases hardly possible with earthbound experiments.

The generation of gravitational waves is documented for example by work of Robert ML Baker (eg. US 6,417,597 ). These works have the disadvantage that no real gravitational waves are generated there, but rather an emulation is carried out by means of computer technology. The connected computer technology leads to signal-induced signal delays, which precludes the generation of measurable gravitational waves, so that no measurable effect can be achieved.

Furthermore, there are attempts in the Russian Federation to generate gravitational waves. In the RU 2 184 384 a generator for the generation of longitudinal gravitational waves is claimed, which has the disadvantage of too low a design power P _r and a much too small efficiency η << 1.

From the disadvantages of the prior art described above, the problem initiating the invention is to propose a device for generating gravitational waves, whereby gravitational waves of measurable power can be produced.

The solution to this problem is achieved by a device for generating a plasma, which puts its ions in high-frequency oscillations with a frequency f.

The inventor was led to this solution by the following considerations:
As a natural source of gravitational waves, binary star systems are generally considered to be stars rotating rapidly around a common center of gravity. Inspired by this idea, considerations were already made about the generation of gravitational waves. The idea of a rotating mass has already been used several times, cf. For example, Baker's proposals concerning large rotating masses.

Thorsten Fließbach examines in his textbook "General Theory of Relativity", 3rd edition 1998, chapter 36, p. 197 u. a , the gravitational wave power that can be generated by a rotator in the form of a rotating beam.

The mass and the distance of the rotating body exert a significant influence on the radiant power of such a rotating mass distribution. Here one can determine the exact moment of inertia of the mass distribution over an inertial tensor. Simplified, one can also use the formula according to Steiner's theorem for the model of a rotating rod, according to which the moment of inertia J of a mass m applies, relative to an axis of rotation at a distance L from the center of gravity: J = J _body + m · L ² (I)

For example, the moment of inertia of a solid sphere is: J _sphere = 0.4 · m · r ² (II)

For the principal moments of inertia J ₁ , J _{2 of} a dumbbell-shaped mass distribution with two balls of mass m of radius r at a distance d = 2L, this results in J ₁ = 2 × [J _sphere + m × L ² ] = = m × [0.8r ² + 2L ² ] (III) J ₂ = 2 * J _sphere = = m * 0.8 * r ² (IV)

This results in the mean moment of inertia I to I = [J ₁ + J ₂ ] / 2 = = m × [0.8 r ² + L ² ], ≈ m × L ² for L >> r (V) and the ellipticity ε of the mass distribution too ε = [J ₁ - J ₂ ] / [J ₁ + J ₂ ] = = 2 · L ² / [1,6r ² + 2L ² ] ≈ = 1 for L >> r (VI)

G

= Gravitationskonstante,

I

= Trägheitsmoment,

ε

= Elliptizität,

Ω

= Frequenz der oszillierenden Massenverteilung,

c

= Lichtgeschwindigkeit.

The radiant power P of a rotating mass distribution is P = 6.4 · G · I ² · ε ² · Ω ⁶ / c ⁵ , (VII) With

G

= Gravitational constant,

I

= Moment of inertia,

ε

= Ellipticity,

Ω

= Frequency of the oscillating mass distribution,

c

= Speed of light.

The frequency ω of the gravitational wave is ω = 2 Ω.

Substituting (V) and (VI) into (VII) yields: P = 6.4 · G · m ² · L ⁴ · Ω ⁶ / c ⁵ , (VIII)

It is clear from equation (VIII) that the mass m of the accelerated body whose distance d = 2L from each other and the rotational frequency Ω of the moving bodies can be possible setting knobs for achieving a high radiation power P, while G and c are constant.

The inventor, using suitable formulas for this system, came to the conclusion that it is only possible to achieve a measurable effect by generating very high-frequency acceleration rates. However, the inventor turns away from the idea of rotating massed bodies around a rotation axis, but oscillates ions in a plasma. In contrast to rotational movements in which the centrifugal forces with increasing rotational frequency Ω quickly increase in technically unmanageable dimensions, linear movements are not subject to such restrictions.

The oscillation of the ions in the plasma causes a radiation of gravitational waves with a frequency f = 2πω, which is preferably greater than f = 10 ¹⁰ s ^-1 , in particular greater than f = 3 · 10 ¹¹ s ^-1 . Only by generating superhigh-frequency oscillations of the ions formed in the plasma is it possible to generate gravitational waves with a measurable effect.

In terms of design, it makes sense to oscillate the ions generated in the plasma in an electrical alternating field of frequency f = 2πω. Only in the electric field is there such a rapid reversal of polarity that the charged particles formed in the plasma want to follow the electric field and therefore oscillate sufficiently quickly back and forth.

The vibrational excitation of the ionized plasma particles already described above must be done according to a specific pattern. The goal is to create only transverse gravitational waves with the experimental setup. It should be noted that gravitons have the spin 2 and the corresponding radiation comes about through a quadrupole characteristic of the vibrating body.

Furthermore, even ions at extremely high frequencies are barely able to follow the alternating electric field; For this reason, the "driving" electric field strength must be extremely large. In order that the electric field generating that field strength need not be extremely high, the invention proposes that the device in which the plasma is formed and vibrated is divided into small oscillation spaces.

In order for the plasma ions to oscillate without hindrance, the dimensions h _{1 of} these compartments in the direction of the ion oscillation must be greater than their oscillation amplitude, but at the same time it must be ensured that the dimension in question is smaller than the oscillation amplitude of the oscillation having the same frequency f Electrons, so that the electrons are collected by a preferably conductive wall of the respective compartment and thus withdrawn from the oscillation space, so that so swing only the positively charged plasma ions.

By setting the optimum geometric parameters for the individual compartments, the disadvantages known from the prior art are eliminated and thus a maximum power P _{r of} the resulting gravitational radiation is achieved.

A preferred height h ₁ for this purpose in the vertical housings of the device is thus calculated according to:

Further details on this can be found in the attached appendix.

It has proved favorable that the plasma to be formed consists of vaporized and ionized mercury. Hg has the advantage that it is a heavy metal (M = 200.59 g / mol) and thus the influence of the mass in equation (VIII) can be sufficiently taken into account. Furthermore, mercury is readily available not overly expensive and also easy to handle. Since it is liquid under normal conditions, it can be easily and accurately dosed into the chambers provided. Furthermore, mercury is easily volatile and easily distributed in the chambers with the involvement of a vacuum pump, in addition, the ionization potential IP ₁ = 10.44 eV of mercury is such that it is easy to plasma formation.

It is in accordance with the teachings of the invention that the electrodes used in the device should have particular properties. It makes sense in the course of the experiment if the material used for this purpose is such that there is a particularly high work function or that it is coated in such a way that a high work function must be performed. The high work function or a corresponding coating of the electrodes means that during the oscillation of the plasma it is not possible to reduce the resulting Hg ⁺ ions in the given time window fast enough. A back reduction within the experimental setup would disqualify them because the superhigh frequency oscillation of the system would be disrupted.

It has proven to be particularly advantageous if the electrode material used consists of a nickel alloy, in particular a Chromnickellegierung. A further increase in the work function at the electrode can be achieved if it is equipped in the Vorrfeld the experiment with an inert gas at the surface. For example, nitrogen adsorbed on the electrode additionally increases the work function. The use of other gases (for example noble gases) for adsorption is also conceivable, as long as they do not interact reactively with the resulting plasma.

The device according to the invention provides that at least two, but preferably a plurality of oscillation spaces in the direction of the high-frequency ion oscillation are connected in series to form a kind of oscillation column. The use of several successive rooms allows easier detection of the resulting gravitational waves, since their radiation performance can be increased. The gravitational radiation power of the device according to the invention corresponds in fact to the total mass Σm of the Hg in the plasma in all individual vibration chambers of the vibrating columns. (see appendix, treatise Klepach)

The functionality of the device is only guaranteed if at least two or more vibrating columns are used. For example, the mass used is calculated as follows: Σm (Hg) = 2 · * 2n · * M ₁ = 1.05 · 10 ^-2 kg (IV)

For optimum functioning of the device, neighboring oscillation columns should have a distance which is equal to or greater than half the wavelength Λ / 2 = c / 2f of the generated gravitational wave.

In the operation of the vibrating columns, it is advantageous if the ions are excited in adjacent vibrating columns to phase-shifted oscillations. As mentioned above, gravitational waves exhibit a quadrupole characteristic, that is to say they arise, for example, when two accelerated masses move in such a way that they oscillate quadrupolarly.

Polarisationen h₊ und h_x The polarizations of the gravitational wave can be understood as stretching and stretching the unit circle. There are two polarizations h ₊ and _hx :

Polarizations h ₊ and _hx

It should be noted that the polarization direction h _x is rotated by 45 ° relative to h ₊ . The superposition of the two polarizations results in a rotating ellipse. In this case, depending on the phase, the ellipse in the clockwise direction or counter-clockwise, alo counterclockwise, rotate.

Does the particle system under consideration in the plasma in the oscillation columns of a device according to the invention quadrupole oscillations in a plane, the propagation of the resulting gravitational waves takes place perpendicular to this plane, so that transverse gravitational waves arise.

On the other hand, two or more oscillation columns can also be arranged outside a common plane, that is to say obliquely or skewed so that the longitudinal axes of the oscillation columns do not run parallel to one another. In this case, the processing of a gravitational wave depends on the phase shift between the vibrating columns, based on the wavelength Λ of the gravitational wave and the distance of the vibrating columns.

Finally, it is the teachings of the invention to maintain certain predetermined geometric conditions for the device to physically enable generation of gravitational waves. The centers of adjacent vibrating columns should lie on a common midpoint line. The longitudinal axes of adjacent vibrating columns should lie in a common plane or intersect each other along the midpoint line at an angle of about 90 °.

Particularly with this predetermined geometry of the device, an optimal quadrupole moment can be generated by means of phase-offset oscillation excitation of the plasmas in the different oscillation columns, and thus detectable gravitational waves can be generated.

Further features, details, advantages and effects on the basis of the invention will become apparent from the following description of a preferred embodiment of the invention and from the drawing. Hereby shows:

1 a side view of the device according to the invention for generating gravitational waves, partially cut open;

2 an enlarged view of the detail II 1 to explain the structure of the device according to the invention; such as

3 a cut through the 2 along the line III-III.

In 1 is the device according to the invention 1 with two swinging towers 2 shown. The swinging towers 2 are preferably formed as elongated, hollow cuboid, wherein the cuboid having a preferably square base on one or each solid foundation 3 fixed, which must be able to the swinging towers 2 sufficiently stabilized during operation, even if it should lead to increased vibration. However, the operating frequency is far beyond all mechanical resonance frequencies of the arrangement, so that this danger arises mainly in case of malfunction.

The swinging towers 2 are placed parallel to each other and their vertical axes 4 are at a distance 2L to each other, wherein 2L may preferably be a multiple of the wavelength Λ of the gravitation waves to be generated. The two swinging towers 2 are each of an air and gas-tight housing 5 surrounded, whose interior preferably has a square base, for example. With an inner edge length b ₁ <L, preferably b ₁ ≤ L / 2, in particular b ₁ ≤ L / 4. The side length b _{1 of} the square base area is preferably divisible by the wavelength Λ.

The housing 5 is by about horizontal or transverse to the longitudinal axis 4 extending shelves 6 into a multitude of superimposed chambers 7 divided. Every chamber 7 is an upper electrode 8th assigned as well as a lower electrode 9 , The upper electrode in each case 8th located at the bottom of the relevant chamber 7 above final intermediate floor 6 while selecting the associated lower electrode 9 on the top of the relevant chamber 7 below final floor 6 located. All electrodes 8th . 9 are flat and horizontally aligned and preferably extend over the entire base of the relevant chamber 7 ; Preferably, they each have a square base area of the dimensions b ₁ × b ₁ , corresponding to the base of an intermediate floor 6 which also has the dimensions b ₁ × b ₁ . The attachment of the electrodes 6 and 7 on the substrate 8th is preferably carried out by welding or by vapor deposition, sputtering od. Like.

In each case under the electrode 9 a chamber 7 can with a bulge 10 for storing a Hg drop 11 be, for example, which can be effected by means of a metering syringe.

The electrodes 6 . 7 and / or the shelves 6 are heatable to the filled mercury 11 to evaporate. By further heating and / or by an electric field between the electrodes 6 . 7 becomes the Hg gas 11 ionizes to a plasma with positively charged Hg ⁺ ions and free electrons.

The cavities of all chambers 7 can have a conduit system 12 with each other and / or with one or more vacuum pumps 13 communicate, preferably on the lower base of a swinging column 2 connected.

A vacuum pump 13 serves to produce as complete a vacuum as possible within the connected chambers 7 before evaporating the Hg drop 11 (p≈0).

After evaporation of the Hg drop 11 the Hg pressure is greater than zero: p> 0. The vacuum pump can 13 be equipped with an autoregulation to the pressure p = kTm ₁ ε ₀ (ω / e ₁ ) ^{2 of} the working medium 11 in the swinging column 2 For example, depending on the desired amplitude a of the resonant vibrations of the Hg ⁺ ions of the frequency ω = 2πf one to the electrodes 8th . 9 connected electric generator 14 and of the mean free path w of a Hg ⁺ ion, preferably such that 2a <w.

In particular, must also for the height h of a chamber 7 be valid: 2a <h.

The electric generator 14 generates a frequency f of more than 1 MHz (megahertz = 1,000 kilohertz), preferably more than 10 MHz, in particular more than 100 MHz, or a radio frequency (HF) of more than 1 GHz (gigahertz = 1,000 megahertz), preferably from more than 10 GHz, in particular more than 100 GHz, or a superhigh frequency (SHF) of more than 1 THz (terahertz = 1,000 gigahertz), preferably more than 10 THz, in particular more than 100 THz.

The electric generator 14 is by wires 15 and 16 to the electrodes 8th . 9 connected. It should be noted that also the nominal lengths l _{1 of} the wires 15 and 16 should be exactly the same length, or a length difference corresponds to a multiple of the wavelength Λ, so that the ions of the working medium 11 in the two vibration towers 2 oscillate synchronously. The electrodes 8th . 9 in all chambers 7 a vibration tower 2 are in the same direction as the electric generator 14 connected, for example, by each of the upper electrodes 8th to a manifold 15 are connected and the bottom electrodes 9 each to the lower manifold 16 , However, it is important to ensure that the length difference Δl _i hiss two adjacent connection points of a common manifold 15 . 16 a multiple of the wavelength Λ corresponds to the ions of the working medium 11 in all chambers 7 oscillate synchronously with each other, in time with the frequency of the electro-oscillator 14 and parallel to the longitudinal axis 4 of the respective vibration tower 2 ,

However, the ions of the working medium should 11 in all chambers 7 of the other oscillation tower 2 swing anticyclically, ie, for example, each along the longitudinal axis 4 up, if at the same time the ions of the working medium 11 in all chambers 7 of the first vibration tower 2 swing straight down. For this purpose, the manifolds 15 . 16 from the electrodes 8th . 9 both Shung towers 2 with opposite polarity to the electric generator 14 connected, so that one pole thereof, for example. With the upper electrodes 8th a vibration tower 2 is connected and with the lower electrodes 9 of the other vibration tower 2 , while the second pole of the electric generator 14 with the remaining electrodes 9 . 8th connected is.

Due to the anti-cyclic mass movement of the ions of the plasma-shaped working medium 11 in the chambers 7 the two vibration towers 2 results in a total movement of all ions involved 11 in the manner of a quadrupole vibration capable of emitting a gravitational wave.

Since the free electrons have a much smaller mass than the porotonically charged ions of the working medium 11 , these are from the electrodes 8th . 9 captured. It is therefore by a suitable choice of the material of the electrodes 8th . 9 and / or by a geeingete coating thereof to pay attention that the work function for electrons from the electrodes 8th . 9 as high as possible, so that only a few electrons in the chamber 7 emerge where they would lead anticyclic movements to the there, positively charged ions.

For a more detailed description of the invention, in particular with the aid of further explanatory formulas, a mathematical treatise originating from the inventor is reproduced below:
The invention relates to the field of gravitational engineering and can be used for the excitation of quadrupole particle vibrations of the sampled medium, for information transmission in the electromagnetic wave opaque environment, as well as for experimental research of gravitational wave properties.

For example, binary star systems serve as a natural source of gravitational waves. These are simulated in the present arrangement by two systems - I and II - the mass M of the particles of the working medium (AM) - in the form of a fully ionized plasma. The centers of the masses M of systems I and II - the points S ₁ and S ₂ - move approximately on a circular line with radius L and are just held in the mutual distance 2L by the gravitational and centrifugal forces. The design power P _{r of} the gravitational emission of the mentioned natural analogue - the double star - forms the tiny part of the power P _{0 of} "producing" processes. However, the efficiency of the natural analogue - η ₀ = P _r / P ₀ ~ 10 ^-12 ([1] §105) - is several orders of magnitude higher than the efficiency η _{1 of} every imaginable artificial analog of the "dumbbell" type. The concentrated masses M of the "dumbbells" are held by electromagnetic forces at the mutual distance 2L and move on the circle with radius L at constant velocity v <0,1c, where c = 2,9979 · 10 ⁸ m / s - electrodynamic Constant. The moment of inertia I of the system I-II with respect to the axis of rotation, the angular velocity ω, the effort P ₁ , the design power P _{r of} the gravitational radiation ([1] §105) and the efficiency η ₁ = P _r / P _{1 of} the two-mass (imaginary) Analogs are: I = 2ML ² ; ω = v / L; P ₁ = ½Iω ² · ω ≡ ML ² ω ³ ; P _r = (2G / 5c ⁵ ) I ² ω ⁶ ≡ (8G / 5c ⁵ ) P ₁ ² ; η ₁ = (8G / 5c ⁵ ) P ₁ (1) where G = 6.67 × 10 ^-11 m ³ / kg × s ² - is the gravitational constant; The efficiency of the laboratory device with the power P ₁ = 10 ⁶ watts would be a trace quantity: η ₁ = 4.4 · 10 ^-47 .

A disadvantage of previously known proposals are the low values of the design power P _r and the efficiency η ₁ □ ₁ . The generator of longitudinal gravitational waves patented in Russia (Patent of the Russian Federation RU 2184384 ; 2001), neither an analogue nor a prototype, since in the present invention no longitudinal gravitational waves are to be generated, but always gravitational waves polarized transversely to the propagation direction ([1] §102).

The vibration systems I and II of the device according to the invention are supplemented by the following functional systems: III - a support system for generating a set temperature T and the pressure P of superheated steam of the working medium (AM); IV - a system for full ionization of the AM; V - a system for excitation of continuous ion oscillations in AM with a frequency ω = 2π c / Λ and an amplitude α <0,1 c / ω; VI - a system for compliance with the prescribed law of movement of the Center of mass AM.

Compared to other plasma species such as, for example, cesium plasma with an ion mass Cs ⁺ : m ₁ = 2.207 × 10 ^-25 kg, and a pressure p of the working medium AM of, for example, 300 atm: p = 3 × 10 ⁷ Pascal and a temperature of AM room temperature: T = 293 K, mercury is better suited.

The equations for the oscillatory motions of mercury ions (in the directions Ox _i ) in the field of the current wave falling on them ([1] §78) are as follows: d ² x _ij / dt ² + ω ₀ ² x _ij = (Ee ₁ / m ₁ ) cos (ωt + φ _ij ); φ _ij ≡ (i-1) π / 2 + 2πξ _ij / Λ; j = 0, 1, 2, ..., v = N ^1/3 b; ξ _ij ε [0; b]; (4) x _ij = (Ee ₁ / m ₁ ) (ω ₀ ² -ω ² ) ^-1 cos (ωt + φ _ij ) ≐ (Ee ₁ / 2m ₁ ωΔω) cos (ωt + φ _ij ); i = 1, 2; (5) r ₀ ≡ (x _1j ² + x _2j ² ) ^½ ≡ ζ (Ee ₁ / 2m ₁ ωΔω); ζ ≡ α / α ₁ <1, (6) where ζ - the coefficient of lowering of amplitude a of the oscillations of the center of the masses of the charged particle system in the periodic field E (ξ) = Ecos (2πξ / Λ) in comparison to the amplitude α _{1 of} the vibrations of the particle characterizing the considered device, which is at the distance ξ from the electrode plane, on the condition that the mutual arrangement of particles is chaotic.

In the non-relativistic approximation adopted in the theories of gravitational waves, the amplitude a coincides with the average value of the amplitudes α (ξ) in the field (4) ([1] §14, [2] §9): α (ξ) ≡ α ₁ cos (2πξ / Λ); α = b ^-1 ∫ b / 0α (ξ) d (ξ) ≡ (Λα ₁ / 2πb) sin (2πb / Λ); ζ = a / α ₁ ≡ (Λ / 2πb) sin (2πb / Λ) = 2.53 · 10 ^-5 . (7)

Suppose that at the electrodes 8th . 9 applied voltage u has an amplitude u = 10 ⁶ V and with respect to the above equations, we find out: E = 2u / b = 2 x 10 ⁶ V / m; r ₀ = 1.86 × 10 ^-8 m; I = Mr ₀ ² = 5.66 × 10 ^-13 kg × m ² ; P _r = (2G / 5c ⁵ ) I ² ω ⁶ = 3.26 W. (8)

The power P _p , which is dissipated in the collision of electrons and ions AM with the frequency ν _e , and the efficiency η _{2 of} the analog are: ν _e = ω; P _p = E ² Vε ₀ ν _e / 2 = 1.75 × 10 ¹⁴ W; η ₂ = P _r / P _p = 1.86 × 10 ^-14 . (9)

It turns out that the selected parameters (P _r , P _p , M, P, u) are unsuitable.

des vorgeschlagenen Gerätes sind:

The height h _{1 of} the ES and the function

of the proposed device are:

In the course of the explanation it is shown that the ratios (10) correspond to the maximum power of gravitational emission P _r .

On the - the overall view and the main elements of the presented invention are shown schematically.

The present institution ( ) contains two vertical housings arranged in the horizontal direction Ox ₂ with distance 2L (divisible by the wavelength Λ) and fixed on the hard foundation. The hollow shape of the housing has in cross section a square shape of the size b ₁ , which is divisible by the wavelength Λ. The sides of the square are parallel to the coordinate axes Ox ₁ and Ox ₂ , where: b ₁ ² << L ² .

On the walls of the cavity are supports h ₁ with a vertical extension 3h ₁ and a distance between two adjacent supports h ₁ (FIG. ) produced.

The left (or right) wall of the left (or right) housing is made detachable, with the possibility of mounting flat horizontal electrodes square shape b ₁ × b ₁ in the housing of the periodic system. The upper electrode and the lower electrode of a discharge gap (ES) are fixed on the entire substrate of size b ₁ × b ₁ (for example, by the method of burn-in). Upper (lower) substrate of each housing carries an electrode.

The housing and substrates of the vibration towers are preferably made of ceramic, which may be reinforced with metal mesh. The electrodes are made of a chrome nickel alloy.

Thus, the hollow shape of the housing is divided into 2n sections from the periodic system of the electrodes with the period h = 4h ₁ = Λ, where h _{1 is} the height of the ES. When connecting electrodes to the general source of the SHF voltage 2ucosωt with the wires of the specified nominal lengths l _i , divisible by the wavelength Λ, the phase of the potential of the i-electrode is independent of the index i; l _i = iΛ; ± ucos [ω (t - l _i / c)] = ± ucosωt; i = 1, 2, ..., n (11)

As AM of the submitted device superheated vapors of mercury are assumed, the atmospheric pressure P and the temperature T> T. i / H to fill the ES ([3] p. 194): P = 1 atm = 101325 Pa; T = 370 ° C = 643.15 K; T i / H = 3066 [7.752 - lg (P / 133.3)] ^-1 = 629.4 K (12)

T is the temperature of saturated Hg vapor at 1 atm pressure. The atomic mass unit of mercury A = 200.59.

The mass m _{1 of} the ion Hg ⁺ , the mass m _{2 of} the electron, its concentration N in the fully ionized plasma of the SHF discharge, ion ω ₁ and electron ω ₂ plasmas frequencies are: m ₁ ≐ Aμ = 3.3309 x 10 ^-25 kg; m ₂ = 9,1095 x 10 ^-31 kg; N = P / kT = 1.1411 x 10 ²⁵ m ^-3 ; ω ₁ = (Ne ₁ ² / m ₁ ε ₀ ) ^½ = 3.1515 · 10 ¹¹ s ^-1 ; ω ₂ = ω ₁ (m ₁ / m ₂ ) ^½ = 1.9057 · 10 ¹⁴ s ^-1 . (13)

The operating frequency ω, the wavelength Λ and the voltage 2u of the generator 14 are: ω ≐ ω ₁ ; Π ≡ 2πc / ω = 6 × 10 ^-3 m; h ₁ = Λ / 4 = 1.5 × 10 ^-3 m; 2u = 24V; u ε [u ₁ ; u ₂ ], (14) where u ₁ = 10.4 V, u ₂ = 14.5 V - the potentials of single-ionization of the atoms of mercury and the (adsorbed in the working plane of the electrode) atoms of nitrogen, u = 12 V is the amplitude value of the Electrode potential (11), which corresponds to the amplitude value E _{0 of} the voltage. E (t; ξ) = E ₀ cos (ωtΥ2πξ / Λ); ξ ε [0; h ₁ ]; E ₀ = [u - (-u)] / h ₁ = 1.6 × 10 ⁴ V / m; (15)

α₁ ≐ E₀e₁/πm₁ω₁Δω = 7,773·10^–5 m; α₂ ≐ –2E₀e₁(πm₂ω₂ ²)^–1 = –4,9·10^–14 m; α₁ω = 0,08c. (16) The orthogonal planes of the electrode of the deviation α _i (t; ξ) of ions (i = 1) and electrons (i = 2), which in the time instant t at the distance ξ from the plane of the electrode in the field E (t; ξ) (15), due to averaging on the range ξ ε [0; h ₁ ], taking into account the records (3) - (5), (10), (13), are presented in the following manner:

α ₁ ≐ E ₀ e ₁ / πm ₁ ω ₁ Δω = 7,773 · 10 ^-5 m; α ₂ ≐ -2E ₀ e ₁ (πm ₂ ω ₂ ² ) ^-1 = -4.9 × 10 ^-14 m; α ₁ ω = 0.08c. (16)

The pump controlled by the autoregulation system (ARS) supports the atmospheric pressure AMs P = kTm ₁ ε ₀ (ω / e ₁ ) ² (13) in all ESs, corresponding to the resonant vibrations of ions Hg ⁺ at the frequency ω of the generator 14: ω ₁ ≐ ω. The condition of the existence of the SHF discharge in ES is observed ([3] p. 158), - | α ₂ | << α ₁ <h _1/2 = 7.5 x 10 ^-4 m - (17) in which process the majority of charges from a field on electrodes is not conducted, but is accumulated in ES.

The calculation and description of the system VI.

The components I assigned to the Cartesian coordinate system Ox ₁ × ₂ × ₃ i / αβ of the steady-state tensor of the system of two masses M ₁ (2) concentrated in points S ₁ and S _2i , the vibrations coming in the plane x ₁ = 0 in the vertical direction Ox ₃ with distance L from the axis Ox ₃ ( ), are ([2] § 32): I i / 11 = 2M ₁ (L ² + z 2 / i); I i / 22 = 2M ₁ z 2 / i; I i / 33 = 2M ₁ L ² ; I i / 23 ≡ I i / 32 = -2M ₁ Lz _i ; i = 1, 2, ..., n = 50; (18) I i / 12 = I i / 21 = I i / 13 = I i / 31 = 0; z _i ≡ z _i (t) ≡ H / 2 - ih - α ₁ (t) α ... ₁ (t) = α ₁ ω ³ (sinωtΥcosωt); (19) Λ = 4h ₁ = 6.10 ^-3 m; b ₁ = 16Λ = 0.096 m; V ₁ = b ₁ ² h ₁ = 1.382 x 10 ^-5 m ³ ; M ₁ = NV ₁ m ₁ = 5.253 · 10 ⁵ kg, (20) where Υz _i - the vertical coordinate of the center of the masses of the i-section of the housing 1 (2) - the point S _1i (S _2i ), which performs the small vertical vibrations (16); V ₁ - volume ES; 2n - the number of sections in the housing.

sind die Ausdrücke von dritten zeitlichen Ableitungen der Komponenten I i / αβ und I_αβ der Trägheitsmoment-Tensoren des i-Massen-Teilsystems und entsprechend 2n Teilsysteme:

wobei die Annäherung İ₁₁ = İ₂₃ die bevorstehenden Berechnungen wesentlich vereinfacht, trägt aber die Abweichung bei etwa P_r/100.Considering the relations

are the terms of third time derivatives of components I i / αβ and I _{αβ of} the moment of inertia tensors of the i-mass subsystem and corresponding to 2n subsystems:

the approximation İ ₁₁ = İ ₂₃ considerably simplifies the forthcoming calculations, but carries the deviation at approximately P _r / 100.

D ... ≡ M₁Lnα ...₁(t) ≡ M₁Lα₁nω₃(sinωtϒcosωt); D ...² ≡ (M₁Lα₁nω³)²(1ϒsin2ωt). (24) The third time derivatives of the components of the tensor D _{αβ of} the quadrupole moment of the system 2n masses M ₁ ([1] § 96) are connected to the I _αβ Kronecker symbol:

D ... ≡ M ₁ Lnα ... ₁ (t) ≡ M ₁ Lα ₁ nω ₃ (sinωtΥcosωt); D ... ² ≡ (M ₁ Lα ₁ nω ³ ) ² (1Υsin2ωt). (24)

The densities Π _i (t), which are aligned parallel to the axes Ox _i of energy streams of the gravitational emission in the wave zone, ie at the distance R ~ 10L from the point O ([1] § 105), are: Π ₁ (t) = (Π ₀ / R ² ) [(D ... ₂₂ - D ... ₃₃ ) ^2/4 + D ... ₂₃ ² ] ≡ 5Π ₀ (D ... / R) ² ; Π ₂ (t) = (Π ₀ / R ² ) [(D ... ₁₁ - D ... ₃₃ ) ^2/4 + D ... ₁₃ ² ] ≡ Π ₀ (D ... / R) ² ; Π ₃ (t) ≡ 0; Π ₀ ≡ G / (πc ⁵ ) ^-1 = 8.77 × 10 ^-54 (W) ^-1 . (25)

wobei M₁ = 5,253·10^–5 kg (20); L = 0,6 m (21); α₁ = 7,773·10^–5 m (16); n = 50(18); (26) ω ≐ ω₁ (13); R = 6 m. The averaging of the expressions Π _i (t) after the time t taking into account (24) is:

in which M ₁ = 5.253 x 10 ^-5 kg (20); L = 0.6 m (21); α ₁ = 7.773 x 10 ^-5 m (16); n = 50 (18); (26) ω ≐ ω ₁ (13); R = 6 m.

The densities of energy Π _1,2 are perfectly sufficient for experimentation in the wave zone, - R τL πΛ, - corresponding to the range of applicability of formulas (25) ([1] § 105). Therefore, the further increase in the sizes L, H is hopeless.

entspricht der genügend kleinen summarischen Masse M des AMs in allen ES der zwei Gehäuse: M = 2·2n·M₁ = 1,05·10^–2 kg << M = 1637 kg. (28) The gravitational radiation power of the present facility ([1] § 105),

corresponds to the sufficiently small summary mass M of the AM in all the ES of the two housings: M = 2 · 2n · M ₁ = 1.05 · 10 ^-2 kg << M = 1637 kg. (28)

Back to the note to the record (10), we consider one in the term I i / 23 (18) implicitly ranked function of the argument h ₁ - the height ES: F (h ₁ ) ≡ M ₁ α (ξ) ≡ Nm ₁ b ₁ ² h ₁ (α ₁ / h ₁ ) ∫ h1 / 0cos (2πξ / Λ) dξ ≡ ≡ (2π) ^-1 ΛNm ₁ b ₁ ² α ₁ · sin (2πh ₁ / Λ) (29)

At h ₁ = Λ / 4, the function F (h ₁ ) and correspondingly the power P _r (27) is maximal.

Each point S _1i (S _2i ) of the lower (upper) half of the housing corresponds to the point S _2i (S _1i ) of the upper (lower) half of the housing ( ). The points S _1i and S _2i perform small vertical oscillations in opposite directions with the amplitudes Υα ₁ ( 16 ), ie that the bundle of sections S _1i S _2i (with the center at point O) makes torsional oscillations about the horizontal axis Ox _i in the preservation of horizontal projections 2L of sections S _1i S _2i ; i = 1, 2, ..., n = 50. Since α ₁ ² << b ₁ ² << L ² , it can be said that the elements of the considered system of point masses perform quadrupole oscillations which (mainly) coincide with the Components D _{23 of} the quadrupole mass moment tensor are characterized. As a result of (26), the densities Π _{i of} the energy flow of the gravitational emission in the directions Ox _i (where j = 1, 2, 3, x ₁ ≡ x, x ₂ ≡ y, x ₃ ≡ z) are measured at the distance 10L from Point O: Π ₁ = 5Π ₂ ≈ 18 W / m ² ; Π ₃ ≡ 0, - in accordance with the assertion that "... the gravitational waves are transverse waves" ([1] § 102), and that the particle system in the gravitational wave field performs quadrupole vibrations in a plane perpendicular to the direction wave propagation ([4] chapter 5) is used.

The last property can be used for the destruction of mines that have the low smoothing resistance.

The calculation of the effort P _v in the systems V and VI.

The mean thermal speed v _e and the free path length λ _e of electrons under the conditions ES are ([3] p. 190, 178): v _e = (8 kT / πm ₂₎ ^½ = 1.575 x 10 ⁵ m / s; λ _e = _(e0 λ / 760) T / T: / 0 = 8.555 · 10 ^-7 m; λ _e0 = 2.76 × 10 ^-4 m (30) where λ _e0 - the free electron path length at P ₀ = 1 Torr and T : / 0 = 273K is.

The frequencies ν _i of collision and mobility w _i ≡ qe ₁ / (m _i · ν _i ) ([3] p. 45) (where q ~ 1) of ions Hg ⁺ (i = 1) and electrons (i = 2 ) are associated with the ratio w ₂ / w ₁ = 18 / 0.045 ([3] pp. 191-192)); from this, considering (30) we find out: ν ₂ = ν _e / λ _e = 1.84 × 10 ¹¹ s ^-1 ; ν ₁ = (w ₂ / w ₁ ) ν ₂ m ₂ / m ₁ = 2.013 · 10 ⁸ s ^-1 . (31)

Without the special measures, the power P _v 'is unacceptably high: P _v '= 4n * E ₀ ² V ₁ ε ~ ₁ ε ₀ ω / 2 = 9.87 × 10 ⁵ W (13) - (15), (20), (32) where ε ~ = 1 - is the usual coefficient of relative electrical permeability (KRED) of the medium ES. However, in the case of the ion resonance (ω = ω ₁ ) of the discharge (17) in the SHF plasma, KRED is ε - an imaginary size ([3] pp. 85-86): ε ≡ 1 - (ω ₁ / ω) ² (1 + jv ₁ / ω) ≡ -jν ₁ / ω; j ≡ √ -1 ; P _A ≡ P _v '| ε / ε ~ ₁ | ≡ P _v 'ν ₁ / ω ≡ 2nE ₀ ² V ₁ ε ₀ ν ₁ = 630 W, (33) wherein (due to the ionic conduction of the plasma σ ≡ ε ₀ ν ₁ ), the active power P _{A is} substantially smaller than the reactive power P _P , which is scattered on the capacities of electrodes and wires.

We calculate the capacitance C ₁ "of the capacitor", which consists of two electrodes, of the substrate of thickness d ₁ , which is made of ceramic (KRED ε ₁ ), and the system n ' ₁ of titanium gratings 8 with transparency ψ which increase the durability of the substrate and reduce the capacity C ₁ : d ₁ = 4 x 10 ^-3 m; ε ₁ = 3.5; ψ = 0.5; n ' ₁ = 3; C ₁ = b ₁ ² ε ₀ ε ₁ ψ / d ₁ n ' ₁ = 1.19 × 10 ^-11 F (34)

The capacitance C2 of the wire 13 of the round section with the radius r (KRED of the insulation ε ₁ ) and the length l: l = 2Λ = 1.2 x 10 ^-2 m; r = 2.5 x 10 ^-4 m; C ₂ = 4πε ₀ ε ₁ l / ln (2l / r) = 1.024 x 10 ^-12 F. (35)

The capacity C _{3 of} the wire 14 of the round section of the radius r 'and the length l': L '= L - b is _1/2 - l + H = 1.14 m; r '= 1 x 10 ^-3 m; C ₃ = 4πε ₀ ε ₁ l '/ ln (2l' / r ') = 5.742 x 10 ^-11 F. (36)

The equivalent capacitances C _{C of} the section consisting of the successive and connected «capacitor» and the wires 13 and the system C _n of the 4n parallel connected sections are: C _c = (C ₁ ^-1 + 2 / C ₂ ) ^-1 = 4.909 x 10 ^-13 F; C _n = C _C · 4n = 9.818 · 10 ^-11 F. (37)

The wires from the electrodes of a vibration tower are connected in parallel with the wires from the other electrodes of the same vibration tower, by means of two supply wires ( ). The sewer lines (whose length is divisible by Λ) are connected to opposite poles of the generator.

By opposing connection of the central manifolds of both oscillation towers to the poles of the electric generator, as a result, the synchronous countermovements of the points S ₁ , and S ₂ , ( ) (i = 1, 2 ..., n = 50) without using appropriate SHF devices.

The equivalent capacity C of the system of 4n sections and four wires, the reactive power P _P and the full power P _{V of} the systems V-VI are: C = (C _n ^-1 + 4 / C ₃ ) ^-1 = 1.252 x 10 ^-11 F; P _P = C · (2u) ² ω = 2273 W; (14) P _V = P _A + P _P = 2903 W (38)

The description and calculation of the system III.

After removing the wall of a tower oscillation three drops of mercury mass M _{1/3 of} (20) (the diameter of the drop d _k = 1.35 mm <h ₁₎ in each ES (in a dent on the surface of the electrode 6) introduced a syringe, preferably automated.

Thereafter, the wall seals the cavity in the housing and the pump is turned on. After removing the air from all ES (through the air outlet ducts in the wall of the housing), the pump (by means of the automatic regulation system) is switched off and the generator is switched on to full power P _* = 10 ⁴ W.

As a result, the SHF potentials (11) heat the system of electrodes from the temperature T ₀ = 293 K to the temperature T = 643 K; the drops (located in the electrodes of the electrodes) are intensively vapourised and the AM vapors fill the cavities of the sections (and the air outlet channels) at the pressure P equal to the atmospheric pressure P _H = 1.0133 x 10 ⁵ Pascals. Considering that 1 Torr = 133.3 Pascal, we introduce the known dependence (12) in the following way: P (T) = 133.3 x exp {2.3026 [7.752 - 3066 / (T - T _Π )]}; T _Π = 13.6 K; Tε [573; 1193] K. (39) where T = 643K, P = P _H - the adjustment parameters ARS;
T _Π - the set temperature of overheating AM.

From the equation (39) it follows that the disturbances of the temperature ES ΔT = ± 1 K are accompanied by the disturbances of the pressure AM ΔP = ± 1800 Pascal, which are perfectly sufficient for the triggering of the sensor of the (reversible) pump 10.

The thicknesses d _i , the densities ρ _i and specific heat capacities C ~ _i the materials (chrome nickel alloy and ceramics), the masses M ~ ⁱ , the amounts n ~ ⁱ and heat content H ~ ₁ of electrodes (i = 0) and substrates (i = 1) in the device are: d ₀ = 2.5 x 10 ^-4 m; d ₁ = Λ -h ₁ -2d ₀ = 4 × 10 ^-3 m; ρ ₀ = 8300 kg / m ³ ; ρ ₁ = 3500 kg / m ³ ; M ~ ₀ = 1.9 x 10-2 kg; M ~ ₁ = 0.13 kg; C ~ ₀ = 460 J / kg · K; C ~ ₁ = 1400 J / kg · K; (40) n ~ ₀ = 400; n ~ ₁ = 200; H ~ _i = C ~ _i M ~ _i (T - T ₀ ) n ~ _i ; H ~ ₀ = 1.22 x 10 ⁶ J; H ~ ₁ = 1.27 × 10 ⁷ J; (Heat content of the AMH ~ ³ Joul must not be considered)

The thickness of the wall d ₂ , the mass of the housing M ~ ₂ and the heat content of two housings H ~ ₂ are: d ₂ = Λ = 6 × 10 ^-3 m; M ~ ₂ = _[(1 + b 2 d ₂₎ ² - ₁ ² b] Hρ ₁ = 5.14 kg; H ~ = ₂ ~ 2C ~ _{2 1} M (T - T ₀₎ = 5.04 x 10 ⁶ J (41)

The thermal conductivity λ and the thickness d _{3 of} the thermal insulation - the quartz fiber, the power P _{T of} the thermal losses of the housing surface area S _T and (conditional on the power P _{* of} the electric generator) duration t ₃ of Starts of the System III are: λ = 0.037 W / m · K; d3 = Λ; S _T = 2 [4 (b ₁ + 2d ₂ + 2d ₃ ) H + 2 (b ₁ + 2d ₂ + 2d ₃ ) ² ] = 0.63 m ² ; P _* = 10 ⁴ W; P _T = S _T (T - T ₀ ) λ / d ₃ = 1360 W; t ₃ = (Σ 2 / t = 0H ~ _i ) / (P _* -P _T ) = 2190 s = 36 min; η = P _r / P _* = 0.35, (42) wherein the efficiency of the device (9) η depends on the power of the generator 9 used.

The calculation of the system IV.

The probability W _{u of} the ionization of the mercury atom in the wake of collision depends on the potentials u, u1 (14) ([3] p. 186): Wu = A (u-u ₁ ) exp [(u ₁ -u) / B] = 1.354 x 10 ^-2 , A = 8.6 x 10 ^-3 V ^-1 , B = 100 V, u-u ₁ = 1.6 V. (43)

In those periods Δt where the potential of the electrode 5 (6) is ucosωt> u ₁ , the upper (lower) layer of the atoms AMs ionizes, and the ions Hg ⁺ are repelled downwardly (upward) from the electrode potential , The average frequency ν + positive ionization can be calculated as follows: cosωt ε (u ₁ / u 1]; Δt = ω ^-1 arccos (u ₁ / u) = 1.66 × 10 ^-12 s, ν + = ½W _u / Δt = 4 × 10 ⁹ s ^-1 (44 )

After a half cycle of oscillation π / ω = 10 ^-11 s, the polarity of the electrode changes, but the negative ionization of the atoms AM does not occur, because the emission of electrons from the nitrided surface of the electrode is u <u ₂ (14) is missing.

The frequency ν- of the recombination of ions Hg ⁺ and the formation of ions Hg ^- is proportional to the frequency ν ₂ (31) of collisions of the electrons with the sample particle and to the recombination probability W _p : W _p = 760 W ₀ T _H / T ~ 10 ^-4 ; W ₀ ~ 10 ^-6 ; ν- = W _p ν ₂ ~ 10 ⁷ S ^-1 ; (ν + / ν-) ~ 10 ² , (45) where W ₀ - the probability of recombination at pressure AM 1 Torr and at the temperature T _H = 273 K ([3] p. 189); the last result (45) corresponds to the total simple positive ionization AM in the time t ₃ (42), since the potential of double ionization of the atom of mercury u ² = 19 V> u would be.

Thus, systems III-IV operate on the power of the SHF generator with power P _* = 10 kilowatts. The drive powers of two pumps and the automatic regulation system are low compared to P _* .

literature

• 1. Landau Lev D. The classical theory of fields. Transl. from Russian. Oxford (among others), Pergamon Press, 1975 ,
• Second Landau Lev D. Mechanics. Braunschweig [ua], Vieweg [ua], 1969
• Third Lewitskij SM The tasks and calculations in physical electronics. (In Russian language) University publishing house. Kiev, 1964 ,
• 4th Chiu, Hong-yee. Gravitation and relativity, New York [ua], Benjamin, 1964 ,

LIST OF REFERENCE NUMBERS

1

contraption

2

oscillating tower

3

foundation

4

longitudinal axis

5

casing

6

false floor

7

chamber

8th

upper electrode

9

lower electrode

10

bulge

11

mercury drops

12

line system

13

pump

14

SHF generator

15

wires

16

wires

QUOTES INCLUDE IN THE DESCRIPTION

This list of the documents listed by the applicant has been generated automatically and is included solely for the better information of the reader. The list is not part of the German patent or utility model application. The DPMA assumes no liability for any errors or omissions.

Cited patent literature

• US 3,722,288 [0005]
• US 5646728 [0006]
• US 6417597 [0007]
• RU 2184384 [0008, 0063]

Cited non-patent literature

• "General Theory of Relativity", 3rd edition 1998, chapter 36, p. 197 u. a [0012]

Claims (19)

Contraption ( 1 ) for generating gravitational waves, characterized by means for generating a plasma and its ions ( 11 ) in high-frequency oscillations with a frequency f. Contraption ( 1 ) according to claim 1, characterized by an alternating electric field, which the ions ( 11 ) excites to high-frequency oscillations of the frequency f. Contraption ( 1 ) according to claim 1 or 2, characterized in that the vibrational excitation of the ions ( 11 ) is performed in such a pattern as to radiate therefrom a gravitational wave having a quadrupole transverse characteristic. Contraption ( 1 ) according to one of claims 1 to 3, characterized in that the plasma ( 11 ) in small oscillation spaces ( 7 ) whose extension (h ₁ ) in the direction of the ion oscillation is greater than twice the oscillation amplitude (a) of the ions oscillating at the frequency f ( 11 ), but smaller than the oscillation amplitude of the electrons vibrating at the same frequency f. Contraption ( 1 ) according to one of the preceding claims, characterized in that the plasma ( 11 ) consists of vaporized and ionized mercury. Contraption ( 1 ) according to one of the preceding claims, characterized in that a vibration space ( 7 ) two electrodes ( 8th . 9 ) for applying an electrical AC voltage for the purpose of generating an alternating electric field. Contraption ( 1 ) according to claim 6, characterized in that the electrodes ( 8th . 9 ) consist of a material with a particularly high work function and / or are coated with such a material. Contraption ( 1 ) according to one of claims 6 or 7, characterized in that the electrodes ( 8th . 9 ) consist of a nickel alloy, in particular a Chromnickellegierung. Contraption ( 1 ) according to one of claims 6 to 8, characterized in that the electrodes ( 8th . 9 ) have a nitrided surface. Contraption ( 1 ) according to one of the preceding claims, characterized in that two or more oscillation spaces ( 7 ) in the direction ( 4 ) of the high-frequency ion oscillation are connected in series, for example. To a kind of vibration column ( 2 ). Contraption ( 1 ) according to claim 10, characterized in that two or more vibration columns ( 2 ) are provided. Contraption ( 1 ) according to claim 11, characterized in that adjacent vibration columns ( 2 ) have a distance equal to or greater than half the wavelength Λ / 2 = c / 2f of the generated gravitational wave. Contraption ( 1 ) according to one of claims 11 or 12, characterized in that the ions ( 11 ) in adjacent vibration columns ( 2 ) are excited to temporally phase-shifted oscillations. Contraption ( 1 ) according to one of claims 11 to 13, characterized in that the centers of adjacent vibration columns ( 12 ) and / or the ions oscillating therein ( 11 ) lie on a common midpoint line. Contraption ( 1 ) according to one of claims 11 to 14, characterized in that the longitudinal axes ( 4 ) of adjacent vibration columns ( 12 ) lie in a common plane. Contraption ( 1 ) according to one of claims 11 to 15, characterized in that the longitudinal axes ( 4 ) of adjacent vibrating columns lie in planes which intersect each other along the midpoint line at an angle of about 90 °. Contraption ( 1 ) for generating gravitational waves (mainly with the superhigh frequency (SHF) ω = 2πc / Λ ≈ 3 · * 10 ¹¹ s ^-1 , where Λ ≈ 6 · * 10 ^-3 m is the wavelength and c is the electrodynamic constant), with a ) two systems (I and II) which contain masses of mobile particles of the working medium (for example vapors of mercury), their centers (of the mobile particle masses of the systems I and II) or centers of gravity (S ₁ and S ₂ ) At vertical distances L (x ₁ - x ₃ ), passing through point 0 (the center or center of gravity of the mobile masses of both systems I and II), of two vertical, preferably ceramic, thermally-insulated hermetically sealed housings ( 2 ) (preferably with the hollow shapes of square cross-section with the edge length b ₁ and the base b ₁ ² << L ² ) held; b) a system (III) for setting the target temperature (T) and the pressure (P) of the working medium; c) a system (IV) for full ionization of the working medium; d) a system (V) for generating undamped (continuous) ion oscillations in the (vertical) direction (x ₃ ) with a frequency ω = ω ₁ and an amplitude a ₁ <0.1 c / ω, where ω ₁ ≡ [Pe ₁ ² / (kTm ₁ ε ₀ )] ^{½ is} the natural frequency of the plasma oscillations of ions of mass m ₁ and the charge e ₁ , while k is the Boltzmann constant and ε _{0 is} the electrical constant; e) a system (VI) for compliance with a law of movement of the mass centers (M) around the points (S ₁ and S ₂ ); characterized in that with the aim of realizing torsional vibrations of the section (S ₁ -S ₂ ) about the (horizontal) axis (x ₁ ) with a frequency ω (at approximately constant length 2L of the horizontal projection of the section S ₁ -S ₂ ), and with the aim, in the wave zone, ie at distances R ~ 10L from the origin 0, a sufficiently high density Π, (x) of the (along the axis x ₁ ) oriented energy flow Π, (R)> 10 W / m ^{2 of} the gravitational waves realize the hollow shape of the housing ( 2 ) is divided by a periodic system of flat horizontal electrodes into n sections with the period h (the distance between similar elements of the adjacent sections), the period h being equal to the wavelength Λ: h = Λ = 4h ₁ , where h ₁ is the height of the discharge gap between adjacent electrodes (this discharge gap is designed to allow a drop of the working magnetization (eg mercury) of the given total mass M ₁ = M / n to be introduced therein), the upper (resp lower) electrodes of each section of a housing ( 2a ) in parallel with the lower (or upper) electrodes of each section of the other housing ( 2 B ) with the help of wires ( 15 . 16 ) of predetermined nominal lengths, which are divisible by the wavelength Λ, are connected, wherein the wires ( 15 . 16 ) each having a connection to one of the poles of a voltage source ( 14 ) are connected to the oscillating SHF voltage u (t) = u · cos (ωt), where u is the amplitude value of the electrode potential. Apparatus according to claim 17, characterized in that the electrodes (the thickness d ₀ ) in pairs at the intermediate levels of the entire ceramic substrate with a thickness d ₁ of each d ₁ = 3 Λ / 4 - d ₀ fixed by means of a reinforcing metal grid system of predetermined mesh size are. Apparatus according to claim 17 or 18, characterized in that (by combining the systems III and IV), nitrogen atoms are adsorbed on the working plane of an electrode made of a chromium nickel alloy, wherein the amplitude | u | of the electrode potential from the condition u ₁ <| u | <u ₂ and _{ui are} the potentials of simple positive ionization of the atoms of mercury (i = 1) and of nitrogen (i = 2).

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