Installation and procedure for obtaining nuclear, gravitational and inertial polarization of bodies

Description

[0001] INSTALLATION AND PROCEDURE FOR OBTAINING NUCLEAR, GRAVITATIONAL AND INERTIAL POLARIZATION OF BODIES

[0002] Background

[0003] The existence of the magnetic moment of electrons, protons and neutrons is known and used in the current technique, among other things, by the magnetic polarization of some materials in a magnetic field. The magnetic field exists as such in nature in the form of magnets, i.e. permanently magnetically polarized materials. The generation of the magnetostatic field is achieved using coils of conductors through which electric currents pass.

[0004] Moreover, the presence of the spin kinetic moment of the particles determines the precession of the magnetic moments of these particles when they are in a magnetic field, according to Larmour's theorem.

[0005] In "A Unitary Theory of Nuclear, Electromagnetic and Gravitational Fields" published by Baltateanu Traian (ISBN 978-973-0-38954-8), the author demonstrates that the nuclear interactivity of elementary particles is induced by the circulation of a photon on a contc JI and the induced field , is dipolar.

[0006] The elementary particles that compound matter: the electron, the proton, and the neutton, have magnetic moment, spin kinetic moment, and nuclear moment.

[0007] Nuclear polarization, similar to magnetic polarization, can be induced in bodies in the presence of a technologically induced macroscopic nuclear field.

[0008] In the same work it is demonstrated that the precession of nuclear moments induces a ponderal interactivity, responsible, macroscopically, for the inertia and gravity of the bodies. In the same cited paper, it is demonstrated that a ponderal polarized body, through the precession of the components in the nuclear field, becomes gravitationally and inertial anisotropic.

[0009] If the ponderal polarization is in the direction of the gravitational field, but opposite to it, the w .-jight of the body decreases in proportion to the degree of polarization.

[0010] A ppnderal polarized body has a reduced inertia in the direction perpendicular to the direction of polarization, proportional to the degree of ponderal polarization.

[0011] If the technologically generated magnetic field can be used to change the trajectory of electric charges (in magnetic traps for example), similarly, a macroscopic nuclear field can be used to change the propagation path of photons.

[0012] The gravitational effect and the inertial effect of the technologically produced nuclear field is one of the purposes of this invention.

[0013] The use of the nuclear field for its interaction with photons and neutral particles is the second purpose of this invention.

[0014] The technological production of a nuclear field is not currently known and is the main object and claim of this invention, together with its use.

[0015] For the production of a macroscopic nuclear field, it is proposed to use some turns of optical fiber crossed by a laser beam.

[0016] Appl'crition domain

[0017] The invention aims to use the macroscopic nuclear interaction for its effects on matter.

[0018] The fields in which the invention is useful are: nuclear physics, transportation and medicine. Macroscopic nuclear field induction.

[0019] Induction of a macroscopic nuclear field can be induced by a flux of photons from a guided laser beam:

[0020] - in a fiber optic coil, or

[0021] - between two concentric cylindrical surfaces with a small space between them, covered with a material that reflects the laser beam used.

[0022] Lase coil installation, construction and mode of use

[0023] The installation consists of a fiber optic coil, consisting of turns with a radius that does not affect the transparency of the optical fiber. The optical fiber must support the transport of optical energies as high as possible, i.e. have as little diffusion or absorption losses as possible.

[0024] The two ends of the fiber are glued in extension after inserting a Y-shaped splitter through which a laser beam can enter as close as possible to the inner tangent to the coil, without obscuring the continuous transmission of the beam in the closed circuit in the coil.

[0025] The laser beam must be continuous wave.

[0026] The coil is immersed in a cooling medium to take over the thermal energy dissipated by energy losses when the laser beam passes through the fiber.

[0027] Inside the coil is inserted a body made of a material that allows nuclear polarization as high as possible in an external nuclear field (with gnas high as possible).

[0028] Principle of operation and value calculations

[0029] The effect of the closed-loop circulation of the photons in the laser beam is the induction oi a macroscopic nuclear field inside the propagating loop. The intensity of the induced field is calculated according to the formulas derived in [1], namely, according to the nuclear Biot-Savart-Laplace Law, for n turns.

[0030] Where: n is the number of turns in the coil, the current of photons (laser) in the coil is c

[0031] Um ~ Nqem N is the number of photons circulating through the coil in unit

[0032] 2itRSpire time, equal to the ratio between the energy of the laser beam in unit time and the energy of a photon in the beam,

[0033] Qem the electromagnetic charge of a photon, the same for any photon frequency, and the distance from the photons to a point located at the distance z from the center of the coil of radius R on the axis of the coil is d = Vz2+ R2

[0034] We are interested in the intensity of the field in the center of each turn, on the axis of the coil at z=0, so d=R radius of coil turn. The induced nuclear field at the center of the coil will be:

[0035] Where: N is the number of photons per unit time, constantly circulating in the coil.

[0036] For this number to be constant, the number of photons continuously injected through the splitter must be equal to the number of photons dissipated, (scattered) into the optical fiber over a distance equal to the total length of the fiber over the entire coil.

[0037] The number of photons initially injected through the splitter is greater than the number of photons continuously circulating in the coil, due to dissipation in the fiber. Photons that reenter the circuit, undissipated, accumulate to photons that are permanently injected. The number of photons dissipated is a percentage of the number of photons circulating in the coil. The photon flux in the coil will stabilize when the number of photons dissipated equals the number of photons injected.

[0038] If we Know the ratio between the number of photons dissipated and the number of photons circulating (dissipation coefficient) at a single pass through the coil and, equating the number of photons dissipated with the number of photons injected, we can calculate the number of photons constantly circulating in the coil (after stabilization) depending on the number of injected photons and the dissipation coefficient.

[0039] The dissipation coefficient is determined separately, as the ratio between the power drop and the output power of the laser beam injected into the coil in a single pass.

[0040] CdjssialiOnwith Pi input power and Pfoutput power.

[0041] The number of photons constantly circulating in the coil, equal, after stabilization, to the number of injected photon

[0042] The number of photons remaining, constantly circulating in the coil after stabilization, which form the inductive photon current of the nuclear field in the coil is:

[0043] This number of photons pass in one second, but a single pass through all n turns of the coil takes2irncRcon / seconds.

[0044] The nuclear field inside the coil becomes:

[0045] In an example of the installation, we use the experimental values:

[0046] ^■las ir - 10.6 ■ 10-6m, for the carbon dioxide laser,

[0047] Plaser = 100W,

[0048] ^dissipation = 0.5 is, the photon dissipation coefficient in the entire coil

[0049] 7?coii= 0.1m, is radius of coil the number of turns in the coil n=100.

[0050] Kobina = 1- 6587 - 109JJ (1.3)

[0051] The first fraction depends only on the constructive characteristics of the installation, i.e. of tne coil and the laser used, and the second fraction is a universal constant: the photcn charge.

[0052] The nuclear field required to achieve gravity cancellation by induction of a macroscopic ponderal dipole was calculated in (13.1.10) in [1].

[0053] The values of the parameters in this expression are:

[0054] 9n = 2, taking the minimum value for the gyro-nuclear factor (in the case of liquid hydrogen in this practical example),

[0055] A=0.267 from (1.3), cos cp = 1, in the case of alignment in opposite direction, p = 1.57 - 10-11din [1], c = 3 ■ 108,

[0056] Z= 120 7T, = 1.602 ■ 10"19, = RBohr = 52900 / m = 0.529 • 1O“10, odyi = Rcou = 0.1, in this example

[0057] The ( adulations above are for liquid hydrogen where the estimated gyro-nuclear factor equals 2.

[0058] The value of this ratio pnrepresents the ratio between the force (artificial weight) generated by the field of the coil and the natural weight of the body. This force (artificial weight) can be oriented in the same direction as the natural weight, in the opposite direction, or at different angles, to obtain a resultant with the desired orientation.

[0059] There are many other variables that can influence the values of the macroscopic nuclear fields 0coUinduced by the laser beam installation, some of the constructive nature of the installation, others of the structural nature of the body inside the coil.

[0060] The differences can be of the order of several orders of magnitude.

[0061] The choice of the "core" of the coil, the type of optical fiber, the type of laser, the influence of the gravitational field at the moment of starting the laser beam and the initial position of the axis of the coil in relation to the direction of the gravitational field is also important.

[0062] Applications of the macroscopic nuclear field

[0063] Nuclear field induction by a laser-type photonic current loop can be used to interact with particles with no electric charge, and no magnetic field (or with negligible magnetic field, such as neutrons, neutrinos, etc.). Interaction involves acceleration or deceleration, such as nuclear traps for neutral particles. A nuclear polarized body also acquires inhomogeneous inertial and gravitational properties.

[0064] For a partially polarized macroscopic body:

[0065] ‘ - In a direction parallel to the direction of polarization the inertia increases.

[0066] - In the direction perpendicular to the polarization direction, the inertia decreases.

[0067] - In the direction parallel to the direction of polarization the weight of the body decreases.

[0068] In the direction perpendicular to the direction of polarization the weight of the body increases.

[0069] The increase or decrease in inertia or weight is proportional to the number of particles oriented by polarization (intensity of polarization).

[0070] The effect of weight polarization of a body in an external nuclear field is the relativistic change of internal cycle times and dimensions along the direction of polarization.

[0071] A device that induces a nuclear field with a body inside can be used as a kind of antigravity engine. Two or three such devices placed at an angle or in a pyramid, with a variable angle between them, but with the bisector in the direction of the gravitational field, can be a variable lift antigravity engine.

[0072] Bibliography

[0073] 1 . Baltateanu Traian; A Unified Theory of Nuclear, Electromagnetic, and Gravitational Fields, 2023 - ISBN 978-973-0-38954-8.

Claims

CLAIMS1 . The use of a laser UHEREIN: the laser beam is guided on a circular trajectory, with the aim of obtaining inside, nuclear interaction or the effect on the weight and inertia of a body positioned inside. a. Using a laser in conjunction with an optical fiber UHEREIN: the optical fiber forms a coil and is used for the properties of the nuclear field inside the coil or for the effect on the weight and inertia of a body positioned inside. b. Using a laser beam together with two concentric reflective cylinders UHEREIN; the beam is oriented through the space between the cylinders to propagate on a circular contour and is used for the properties of the nuclear field inside, or for the effect on the weight and inertia of a body positioned inside. c. The use of a laser beam guided on a circular trajectory, UHEREIN; it is used to increase, decrease or reverse the gravitational attraction, or to increase or decrease the inertia when accelerating bodies. d. The use of a laser beam guided on a circular trajectory, UHEREIN; it is used to relativistically modify the duration of internal cycles or the relativistic size of bodies.

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