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ANTIGRAVITATION
INTERACTION OF ROTATING MASSES
S.V. Plotnikov
The analogy between a stationary gravitational field and a stationary electromagnetic field is widely known / 1-7 /. In particular, the structure of the equation of the gravitational field in the local region repeats the equations of the electromagnetic field. This analogy is widely used in solving hydrodynamic problems / 2 /. Recently, a number of papers have attempted to obtain, by analogy with the well-known electrodynamic equations, new effects for the gravitational field [4-7].
In this paper, an attempt is made to combine all known laws into two general sets of fields of gravitational and electric charges. These two kinds of charges exist in a single space-time continuum and, therefore, the structure of the equations describing their behavior in space and time should have a similar structure. Indeed, the fields of stationary charges are described in the same way, for example, the force of interaction of electric charges is described by Coulomb's law, and gravitational - by the law of universal gravitation. We can talk about potential fields. In principle, there is a complete analogy in the equations of electrodynamics and the dynamics of gravitational masses.
Electric charges in mobile reference systems are described by equations of Maxwell type. It can be shown, based on the postulates of the theory of relativity and on the invariance of electric charge, that the magnetic interaction of electric charges is a consequence of Coulomb's law. It is logical to assume that equations similar to the electromagnetic field equations are valid for gravitational charges. VI Babetsky / 7 /, it is shown that the gravitational field of a thin rotating ring is analogous to the electromagnetic field of a turn with a current. Thus, we can say that in nature there are only two types of charges: electric and gravitational. Accordingly, two types of fields: electromagnetic and gravidynamic, the structure of which repeats each other. Consequently, there are only two types of interaction between particles: electromagnetic and gravidynamic.
Experiment
Measurements of gyroscope-earth interaction, gyroscope-gyroscope are carried out.
The standard gyro of aircraft autopilot was placed on the analytical balance of the 2nd class ADV-200M. The rotating part of the gyroscope was in a closed case, with all the structural holes being sealed. The weight of the gyro together with the body is 540 grams. The gyro was rigidly attached to the scales, and a spring system is provided to compensate for its weight. The gyro was powered by a voltage of 12 volts through a converter for 3 400V phases. The switch made it possible to change the direction of rotation of the gyroscope, Fig.
Fig.1 Scheme of the experiment
At the moment when the current is turned on for some time, when the gyroscope is untwisted, a sharp increase in weight occurs. Fig.2. As the set of revolutions, the weight gradually decreases and, finally, assumes a stationary value. When rotating the gyroscope counter-clockwise, the weight on the contrary decreases.
Figure 2. Gyro's weight as a function of time
When the gyro's power is turned off, its weight decreases sharply, then goes to a negative value and then becomes equal to the stationary value. Increasing the supply voltage of the gyro from 12V to 15V leads to an increase in the interaction force from 430mg to 540mg. Thus, if the direction of rotation of the gyroscope coincides with the direction of rotation of the Earth, its weight increases, and in the opposite direction decreases. When the gyro is suspended perpendicular to the weights, a similar change in weight is observed, but the stationary value is smaller, see Table 1.
Interaction of two gyroscopes
The interaction of two gyroscopes was investigated. In this case, the second analogous gyroscope was suspended at a distance of 1 cm from the first one. In this case, the distance from the centers of mass was about 3 cm.
Fig.3. Scheme of the experiment on the interaction of two gyroscopes.
When turning on the power of gyroscopes, the dependences of the weight of the second gyro are similar to those of the Earth-gyroscope interaction. But there are some features:
1. With the inclusion of one gyroscope, weight changes are not observed.
2. The perpendicular direction of the gyroscope axes does not change the weight of the gyroscope.
Gravidynamic interaction of nucleons
The nucleon field can be represented as a superposition of the electrostatic and gravidynamic field of a rotating mass. By analogy with a magnetic field, the gravidynamic field of a rotating mass at distances large in comparison with its dimensions is determined by pr (the gravidynamic dipole moment). In particular, the gravidynamic induction of the field of a flat contour of any shape at large distances has the form:
Where r is the distance from the contour to the given point of the field; - the angle between the direction of the vector Pr and the direction from the contour to the given point of the field; 
- gravidynamic constant.
The value of the gravidynamic constant is determined by analogy with electrodynamics.
Where 
- the gravitational constant, hence
A gravidynamic constant is mentioned in [8] without explaining its physical meaning.
The gravidynamic dipole moment has the dimension of the angular momentum and it can be assumed that for elementary particles 
Has the meaning of angular momentum 
. Then the induction of the gravidynamic field of the plane contour of the mass at large distances has the form:
On the contour axis, the expression takes the form:
Let us consider how two mass contours interact. For simplicity, suppose that the contour 1 creates a field, and the contour 2 is in this field.
The contour 2 is on the axis of the contour 1, and its angular momentum is with the axis of the angle 
. In this case, the force acting between the contours is 
Substituting (4), we obtain
"A" energy of interaction
It is seen from formulas 6 and 7 that the force of interaction between two contours of mass is inversely proportional to the fourth power of the distance between them, that is, it is a short-range force, the force depends on the angle between the contour axes. In the case of a parallel orientation of the angular momentum, an attractive force acts between them, while an antiparallel one has a repulsive force.
The magnitude of nuclear forces
From formula 7 we can find the interaction potential of two nucleons.
Let us consider what happens when two particles collide. In any case, "in addition to the frontal", the moment of momentum of the particle changes, but what is curious, no one has considered this question. In addition, it is interesting what will happen with the angular momentum if the linear velocity of points on the particle surface reaches the speed of light. The mass of the surface layers of the particle will increase, while it will take the form of a toroid and, accordingly, its angular momentum will increase.
Thus, the angular momentum of the nucleons may well acquire values other than h.
Let us find the value of the constant of the gravidynamic interaction of nucleons from the experimental data on p-p scattering at low energies.
The potential of p-p interaction can be written in the most general form
Knowing that the minimum in the scattering is observed at an energy T = 0.45 MeV, we can write
Hence, we obtain r = 2.133x10-15m, and k2 = 2.184x10-45 Mev * m3
It is interesting that the const of the gravidynamic interaction can be obtained from the const of the weak interaction
Then the gravidynamic moments of the nucleons are equal to
The potential of the pn interaction at large distances, if we assume conditionally that the scattering takes place centrally, has the form
And for np scattering
Considering that gravidynamic forces act between nucleons in the nucleus and, assuming that the nucleons interact with each other as mass contours, one can, by analogy with the interaction of turns with an electric current, derive the basic properties of nuclear forces.
1. Nuclear forces are short-range. The radius of their action is of the order of 10 -15 m. They depend on the distance as 1 / r4.
2. Nuclear forces are not central, and have the nature of electric dipole forces.
3. Nuclear forces depend on the direction of the spin of the nucleons, in the parallel direction of the spins they are attractive forces, while for antiparallel forces they are repulsive forces.
4. Nuclear forces have charge independence, i.e. Are symmetric with respect to the proton and neutron; Rotating masses interact.
5. Nuclear forces have the saturation property, i.e. The kernel can interact with a limited number of neighbors.
CONCLUSION
1. All phenomena in nature are due to the fundamental properties of the spirit of the kinds of charges-electric and gravitational.
2. The laws of the electromagnetic field are analogous to the laws of the gravidynamic field.
3. Strong interaction of elementary particles is due to gravidynamic forces.
4. Between the rotating masses act gravidynamic forces, analogous to which are the forces acting between two turns with a current in electrodynamics.
LITERATURE
1. J. Lense, H. Thirring, Phys. Zs.1.9.156.1918
2. R. Feynman, R. Leaton, M. Sands. Feynman lectures on physics. T.1-9, M. Mir, 1977
3. T. Kalutsa. To the problem of the unity of physics. / / Albert Einstein and the theory of gravitation. -M. Peace. 1973
4. Ya.B. Zeldovich. Analog of the Zeeman effect in the gravitational field of a rotating star. // Letters to JETP, 1, 40, 1965.
5. N.V. Mickiewicz, I.Pulido-Garcia. On the motion of test masses in the gravitational field of a rotating body. // DAN, Vol. 192, 6, p. 1263, 1970.
6. VI Babetsky. On the gravitational analog of the phenomenon of electromagnetic induction. // Izv. University. Physics, 10, 16, 1978.
7. VI Babetsky. To the problem of energy in the general theory of relativity, Izv. University. Physics, 10,20, 1978.
8. A.G. Joseph. Questions of the nuclear theory of electromagnetic and gravitational-inertial fields. Yerevan, 1959
9. A.Myslicki. Zeit. Nauk. WSP. Phys.11.56. 1963
10. CW Scott. Canad..Jour. Phys. 44,1147, 1966.
11. A.Z.Petrov. Gravitation and the theory of relativity. // Sat. Kazan
print version
Author: S. V. Plotnikov
PS The material is protected.
Publication date 17.04.2004гг
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