Electromagnetic toroidal impeller

Abstract

The invention relates to an electromagnetic toroidal impeller in the field of physics applied to electromagnetism. The invention comprises a cylindrical arrangement of superconducting antennas (9) which are separated by a dielectric (8) over a superconducting cylindrical plate (7) and exposed in a resonant cavity (6). The radiation in the cavity is incident on the force ring having a superconducting surface (4) containing ferrite (11), the coolant (5) introduced through the pipes (1) flowing through the toroidal interior of same. The force received in the ring (4) is transmitted via the supporting members (3) to the support (2). The cavity is thermally insulated with insulation (12) and is cooled with the liquid (10) through the pipes (14). The invention provides a device capable of generating driving force from the conversion of the energy available in electromagnetic waves that are contained in a resonant cavity.

Claims

1. An electromagnetic drive capable of generating a driving force, characterized by emitting radiation on a force ring outside of a resonant cylindrical cavity, in which a driving force is generated and on whose inner surface, emitting antennas of electromagnetic waves are arranged.

2. The electromagnetic drive of claim 1, wherein the antennas thereof emit synchronized, horizontally polarized waves in the resonant cylindrical cavity.

3. The electromagnetic drive of claim 1, characterized by having a resonant cylindrical cavity with a conducting or superconducting cylindrical surface.

4. The electromagnetic drive of claim 1, characterized by having a force ring with a conducting or a superconducting surface.

5. The electromagnetic drive of claim 1, comprising functional components.

6. The electromagnetic drive of claim 1, wherein the force ring is a toroidal shape.

7. The electromagnetic drive of claim 1, wherein the emitting antennas comprise three or more emitting antennas.

8. The electromagnetic drive of claim 1, wherein the generated driving force includes Lorentz force.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The accompanying drawings, which are incorporated into and constitute a part of this specification, illustrate one or more example aspects of the present disclosure and, together with the detailed description, serve to explain their principles and implementations.

(2) FIG. 1 shows a photograph of the EmDrive, in accordance with aspects of the present disclosure.

(3) FIG. 2 shows an energy flux, in accordance with aspects of the present disclosure.

(4) FIG. 3 shows a photograph of the Cannae Drive, in accordance with aspects of the present disclosure.

(5) FIG. 4 shows a schematic diagram of the Cannae Drive, in accordance with aspects of the present disclosure.

(6) FIG. 5 shows a photograph of the Toroidal Electromagnetic Drive, in accordance with aspects of the present disclosure.

(7) FIG. 6 is a 3D diagram, in accordance with aspects of the present disclosure.

(8) FIG. 7 shows radiation without force ring, in accordance with aspects of the present disclosure.

(9) FIG. 8 shows an electric field in the cavity, in accordance with aspects of the present disclosure.

(10) FIG. 9 shows a magnetic field in the cavity, in accordance with aspects of the present disclosure.

(11) FIG. 10 shows a radiation pattern with the force ring, in accordance with aspects of the present disclosure.

(12) FIG. 11 shows clockwise and counter-clockwise currents in the force ring, in accordance with aspects of the present disclosure.

(13) FIG. 12 shows a net driving force, in accordance with aspects of the present disclosure.

(14) FIG. 13 shows a magnetic flux on the surface of the ring, in accordance with aspects of the present disclosure.

(15) FIG. 14 shows resonance behavior inside the cavity, in accordance with aspects of the present disclosure.

(16) FIG. 15 shows a control diagram, in accordance with aspects of the present disclosure.

DESCRIPTION OF THE INVENTION

(17) In accordance with the disclosed situation and given that there are technologically known techniques that allow high precision in construction processes as well as advances in power management in high-frequency electronics, the invention provides a different energy conversion that directly harnesses the available energy supplied by electromagnetic waves so that a resonant cavity can supply the desired driving force.

(18) The force that electric charges experience in an electromagnetic field is the force that is harnessed in the present invention. The Lorentz equation makes it possible to establish, as a vector, the force experienced by a charge q in an electromagnetic field, according to the equation:
F=qE+q(v×B)

(19) The general idea of the invention is to harness the energy of the radiated electrical field in order to impose a force that provides velocity to the electrical charges found on the surface of a superconducting ring. Said driven charges then receive the force provided by the energy of the magnetic field associated with the radiation. The geometry of the components in the present invention makes it possible to achieve significant power values given the resonance levels of the electromagnetic fields in the proposed cylindrical cavity.

(20) FIG. 5 shows a cross-section of the drive in a schematic diagram. According to FIG. 5, a cylindrical distribution of superconducting antennas (9) is provided, separated by a dielectric (8) located on a superconducting cylindrical plate (7), exposed in a resonant cavity (6). The radiation exposed by the cavity is incident on the force ring with superconducting surface (4) that contains the ferrite (11), the toroidal ring thereof containing the cooling liquid (5), which circulates through the ducts (1). The force received by the toroidal superconducting ring (4) is transmitted via the legs (3) to the support (2). The resonant cavity (6) is thermally insulated by the insulator (12) and is cooled through the ducts (14) by the cooling liquid (10).

(21) FIG. 6 shows a 3D representation of the antennas, the resonant cavity and the toroidal force ring.

(22) The invention manages to produce a net driving force, as a result of the forces exerted by electrons or Cooper pairs that move in the toroidal force ring. The aim is thus to generate, in an ordered fashion, the radiation of electric and magnetic fields that provide the characteristic of maximizing the Lorentz equation:
F=qE+q(v×B).
FIG. 7 shows the radiation pattern in the absence of the force ring. Said pattern is produced due to a synchronized signal in the antennas having a wavelength that approximates the diameter of the cavity.

(23) Proper polarization (electrical field in the x-y plane) allows the constructive interference of the emitted electromagnetic waves to produce in the resonant cavity the desired increase in the electric and magnetic fields. The electrical field (in the absence of the ring) in the plane (x-y) is shown in FIG. 8:

(24) Due to the contribution of each antenna, the cross-section of the cavity shows that the electrical field changes its counter-clockwise and clockwise rotation according to the phase change of the signal. FIG. 8 shows the electrical field for the cavity of which the diameter approximates the length of the emitted waves. A cross-section across the plane (x-y), exactly at the center of the cavity, is shown.

(25) FIG. 9 shows (in the absence of the ring), on the planes (y-z) and (x-z), the magnetic field for the same instant.

(26) Evidently, according to the direction of the observed radiation (z axis), it is logical to understand that the ring will receive in its electrons or Cooper pairs the force due to the electrical component of the Lorentz equation. This is F=q E, which is why a circulating electrical current generated by the energy of the electrical field is produced in the ring. This energy use reduces the radiation intensity observed in the vicinity of the ring as shown in FIG. 10:

(27) The currents circulating in the force ring (counter-clockwise and clockwise) are shown in FIG. 11. The change of direction of the electric current caused by the phase change in the signal of the antennas is, of course, simultaneous with the change in the direction of the magnetic flux.

(28) The Cooper pair electrons in motion then experience, in each cycle of the wave, the change in the direction of the velocity due to the energy contribution of the magnetic field, resulting in the driving force F=q (v×B), which is shown in FIG. 12.

(29) With the current circulating in the ring, it is clear that, according to the location of the ring on the z axis (not only is the direction of the magnetic field most parallel to the plane (x-y) sought, but also for there to be no induction that would generate a magnetic field opposite to the incident field), the optimal net resulting force (maximized on the z axis) is obtained, which is experienced in each phase always in the same direction, given that the corresponding electric and magnetic fields likewise change direction. A distance of Lambda/2, measured from the origin of coordinates, is proposed.

(30) It is easy to obtain the necessary thrust given the natural characteristics of the behavior of the electromagnetic fields in the proposed geometry. FIG. 13 shows the direction of the magnetic field, which follows the surface of the ring, thus optimizing the vector product that provides the force.

(31) Knowing that the invention proposes an ordered radiation, high power values can be obtained given the resonances in the cylindrical cavity (total efficiencies of more than 5000 have been achieved in the simulator). The capacities in the treatment of higher power levels in existing semiconductors and the capacity for producing soft ferrites with higher permeability values at high frequencies also contribute to achieving more significant forces.

(32) FIG. 14 shows that the proposed geometry provides the appropriate resonance behavior for different frequency values. Considerable efficiencies in the radiated power are obtained for the highest resonance frequency. The orange line in FIG. 14 shows the behavior of the accepted power for different frequency values.

(33) Based on the above, it is clear to understand that the achievement of the invention is to reproduce, in each phase of the radiated wave, the phenomenon observed in the fall of a magnet onto a copper conductor block, where the eddy currents (in this case, those that follow the circumference of the ring) are crossed by the incident magnetic field (in this case, the one in the plane of the ring).

(34) Likewise, the levitation phenomenon observed when a magnet is placed near a superconducting element, the currents generated on the surface of the superconductor do not cease due to zero resistance in the movement of the charges (Cooper pairs) on the superconducting surface (for this case, those that follow the circumference of the ring), whereby the magnetic field of the magnet is “deflected,” due to the known expulsion of the magnetic fields inside the superconductor. (In this case, the one in the plane of the ring).

(35) Because the net driving force is obtained by the force experienced by the electric charges on the surface of the ring, it is logical to find that in the case of using a non-superconducting ring, the energy losses due to the displacement of the charges are not very significant, given that the movement imparted to them is due to the incidence of the high-frequency clockwise/counter-clockwise electrical field that the ring experiences on its radiated surface.

(36) The opposite occurs with the walls of the resonant cavity, where the losses obtained by the circulation of the current due to the excitation of the antennas and the reflection of the waves are obviously minimized by the superconducting materials. The control diagram of the invention is shown in FIG. 15.