Boson beam enersend system

11476715 · 2022-10-18

    Inventors

    Cpc classification

    International classification

    Abstract

    Systems and methods are presented for wireless energy transfer by scalar-longitudinal electromagnetic propagating waves. The scalar wave beam antenna is further enhanced with additional active and parasitic resonant elements for increasing the penetrating and far field distance transfer of energy. A receiving antenna module is designed for effective capture of longitudinal and transverse waves. Presented are uses for this system to illuminate areas without the need for wires, powering electronic devices, charging batteries remotely, new style communications, and military applications.

    Claims

    1. A system comprising: a scalar wave beam antenna configured to transfer wireless energy through objects and walls, and at far-field distances, by a scalar electromagnetic propagating wave, not comprising electromagnetic propagation transverse waves, electromagnetic induction, and magnetic resonance coupling systems; wherein the scalar wave beam antenna comprises an omnidirectional signal antenna, connected to a radio frequency transmitter configured to radiate transverse electromagnetic propagating waves parallel to omnidirectional signal antenna axis, with an axis in line with an axis of a parabolic reflector, at a focal point of the parabolic reflector; wherein the scalar wave beam antenna is further configured to reflect the transverse electromagnetic propagating waves by the parabolic reflector with 180 degrees phase shift and then projected forward as transverse electromagnetic propagating waves now in a plane orthogonal to the axis of the parabolic reflector and in an axially spoke-like configuration around a central parabolic reflector axis; and wherein transverse electromagnetic propagating waves is comprised of collinear in-phase reflected transverse wave components all with a same polarity at an end of the axis of the parabolic reflector and the same polarity and an opposite polarity at an outer end of the transverse wave components, creating a focused central axial scalar forward propagating wave.

    2. The system of claim 1 wherein in a preferred configuration the parabolic reflector is two wavelengths at an operating frequency in diameter in the plane orthogonal to the axis of the parabolic reflector and through the focal point of the parabolic reflector, and one-half wavelength deep from the focal point of the parabolic reflector.

    3. The system of claim 1 wherein a focal point radiator is a half wave type, with an outward projecting element being of a quarter wavelength wire, and an inward projecting element a cone with a one quarter wavelength side wall.

    4. The system of claim 1 wherein a focal point radiator is a half wave dipole type, with an outward projecting element and inward projecting element both being of a quarter wavelength wire.

    5. The system of claim 1 wherein a focal point radiator is a half wave dipole type, with an outward projecting element and inward projecting element both being of sheets of conductive material and of various 3-dimensional forms.

    6. The system of claim 1 wherein a focal point radiator has a first end and a second end such that the first end is along the axis and away from a base of the parabolic reflector, the second end is insulated from the base of the parabolic reflector and connected to a one lead of a two-lead feedline from the radio frequency transmitter, the other lead of the radio frequency transmitter is connected to the base of the parabolic reflector.

    7. The system of claim 6 wherein a projecting from a base element of a focal point radiator has an additional element connected along it and which is connected at its other end to a base of the parabolic reflector.

    8. The system of claim 1 further comprising a scalar wave beam antenna receiving antenna structure using metal mass components at opposing positions along a one resonant wavelength long wire loop antenna.

    9. The system of claim 1 wherein the scalar wave beam antenna is configured as a receiver.

    10. The system of claim 1 configured for lighting and powering electronic devices and charging batteries.

    11. The system of claim 1 configured for radio communications on earth and in space.

    12. The system of claim 1 configured for military applications piercing walls and objects with high power.

    13. The system of claim 1 further comprising parasitic one wavelength resonant loop elements with a plane of the parasitic one wavelength resonant loop elements in a same plane as and surrounding a radiative and axially positioned feed point antenna for enhancing a beam.

    14. The system of claim 1 configured as a transmitting antenna and a receiving antenna.

    Description

    BRIEF DESCRIPTION OF DRAWINGS

    (1) One or more preferred embodiments that illustrate the best mode(s) are set forth in the drawings and in the following description. The claims particularly and distinctly point out and set forth the invention.

    (2) The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate various example methods, and other example embodiments of various aspects of the invention. It will be appreciated that the illustrated element boundaries (e.g., boxes, groups of boxes, or other shapes) in the figures represent one example of the boundaries. One of ordinary skill in the art will appreciate that in some examples one element may be designed as multiple elements or that multiple elements may be designed as one element. In some examples, an element shown as an internal component of another element may be implemented as an external component and vice versa. Furthermore, elements may not be drawn to scale.

    (3) FIG. 1 is a prior art illustration of standard transverse radio waves,

    (4) FIG. 2 illustrates the substantial reduction in power with transverse radio waves by wall structures.

    (5) FIG. 3 illustrates the scalar/longitudinal wave penetrating through wall-like structures.

    (6) FIG. 4 illustrates the diminutive scalar/longitudinal wave of standard antennas, due to their self-dissipating nature on the scalar/longitudinal wave component.

    (7) FIG. 5 illustrates a means for generating scalar/longitudinal waves using a parabolic reflector with an axially positioned feed element where center axis focused 180 degrees out of phase collinear transverse waves summate to axial and near-axial longitudinal longitudinal/scalar waves.

    (8) FIG. 6 illustrates a scalar wave receiver antenna, represented here at 1.2 GHz.

    (9) FIG. 7 illustrates dramatic attenuation of the transverse wave by metals and liquids, and pass-through penetration of these objects and materials by the longitudinal/scalar wave.

    (10) FIG. 8 illustrates enhancement of the scalar wave by transverse waves diffracting around the object in the propagation path.

    (11) FIG. 9 illustrates substantiating the central axial longitudinal wave showing reception by axially oriented antenna receivers and substantially reduced reception by orthogonally positioned transverse wave antenna receivers, whereas the sideward transverse wave has reception by orthogonally positioned transverse antenna receivers and substantially reduced reception by axially oriented antenna receivers.

    (12) FIG. 10 illustrates the scalar wave beam antenna used also as a receiver.

    (13) FIG. 11 illustrates the electromagnetic interacting fields of the enhanced scalar wave beam antenna.

    (14) FIG. 12 illustrates particularly the electromagnetic field components generated by the loop component of the feed element.

    (15) FIG. 13 illustrates the scalar wave receiving antenna with a metal sheet reflector.

    (16) FIG. 14 illustrates the scalar wave effectively penetrating a wall enhancing the diminished transverse wave that poorly penetrated the wall.

    (17) FIG. 15 illustrates efficient transfer of energy through walls of a building producing bright light at the scalar wave receiving antenna ˜55 feet away from the scalar wave transmitting beam antenna fed with only ˜5 watts.

    (18) FIG. 16 illustrates the scalar wave beam antenna sending energy to distances through walls to power electronic devices.

    (19) FIG. 17 illustrates the scalar wave beam antenna sending energy to distances through walls to charge batteries.

    (20) FIG. 18 illustrates use of this science and technology for penetrating and distance communications.

    (21) FIG. 19 illustrates high power military use of this science and technology penetrating substantial wall (like) structures.

    DETAILED DESCRIPTION OF THE INVENTION

    (22) Humans utilize energy for a multitude of things. And electrical energy delivery has historically been tied to wires. More recent developments allow transfer of energy without wired connection but only over short distances, and not through walls and objects.

    (23) Herein is the solution so desired by mankind, a method for sending and receiving energy across large distances and through walls and objects effectively and efficiently for a vast number of uses such as lighting, powering electronic devices directly, charging batteries, communications, and energy transfer for military applications; all these things on earth as well as in space and elsewhere.

    (24) To accomplish the above profoundly, the scalar wave beam antenna with its scalar/longitudinal wave needed to be invented and preferably enhanced in penetrating and energy over distance capabilities with a loop design added to the axial feed, and rings (‘suspended’ resonant loops) with the active and parasitic interactions resulting in high gain for size and diverse longitudinal and transverse waves, where the transverse waves enhance the scalar wave in diffracting around objects, and penetrating scalar waves enhance transverse waves more diminished in strength after traversing obstructions and walls.

    (25) FIG. 1 illustrates the standard transverse wave and FIG. 2 the substantial attenuation of the standard transverse wave through objects and walls.

    (26) FIG. 3 shows the anticipated penetrating properties of the longitudinal/scalar wave. Although there is the near field ‘immediacy’ of longitudinal waves from the high voltage point tip of a monopole and dipoles actively fed with radio frequency power, there is a dramatic degradation of that scalar energy component as the near and far fields of transverse waves are generated, as illustrated in FIG. 4.

    (27) Longitudinal waves are generated with a reflector illustrated in FIG. 5A with a single active element 501 and a parabolic reflector 502. The transverse waves generated by the axial element 501 propagate laterally toward the parabolic reflector inner walls and become collinear indicated by 503 and 504 and are 180 degrees out of phase, with the central near-axis components of these transverse waves being of the same polarity as the axial scalar wave in FIG. 5A which further illustrates this (near) axial summating of same polarities, producing a focused scalar wave 505; FIG. 5B a preferred example; FIG. 5C a dimensional view.

    (28) FIG. 6 illustrates a scalar wave receiving antenna which is tuned by dimensions to resonance at the transmitted energy frequency, effective in receiving transverse electromagnetic waves, and the summation of same-polarity components of transverse and longitudinal waves by nature of its geometric construct and particularly with its metal mass components 601 positioned somewhat laterally to the central axis scalar wave. The scalar wave receiving antenna with generated current and voltage can be used in producing light with an LED (Light Emitting Diode) 602 in circuit shown in FIG. 6 and to power electronic devices directly and to charge batteries.

    (29) Penetration of objects and metals and liquids by the longitudinal waves illustrated by 701 in FIG. 7 and substantial attenuation of the transverse waves illustrated by 702.

    (30) Mutually supportive scalar and transverse waves are shown by illustration in FIG. 8 with diffraction of the transverse wave 801 around the object 802 in the path of the signal from the scalar wave beam transmitter of FIG. 5, and by illustration in FIG. 8 showing by summation of like-polarities the enhanced scalar wave 803.

    (31) Substantiating the lack of transverse waves in the central axis radio frequency propagation pattern of the scalar wave beam and lack of longitudinal waves in the sideward propagation pattern, FIG. 9 illustrates the strong signal and light of the axial positioned receivers 901 and 902 in the central forward path of the scalar wave beam and low signal 903 and no light 904 with the transverse positioned receivers in that path, and strong signal and light with transverse positioned receivers 905 and 906 in the sideward path and low signal and no light with axial oriented receivers 907 and 908 in that propagation path.

    (32) Progressing to the enhanced scalar wave beam antenna adaptation for further enhancing penetrating and distance transfer of energy, FIG. 10 illustrates enhancing loop components and dimensions.

    (33) FIG. 11 and FIG. 12 illustrate the loop design 1107 add-on to the axial active element with near field magnetic 1201 and electric 1202 radio frequency field components. FIG. 11 illustrates the total transverse horizontally polarized electric far field 1101 that is generated by a combination of the ‘hot’ loop feed segment 1107 of FIG. 11 and FIG. 12, and reflected transverse waves produced to the sides 1003 of the axial ‘hot’ element segment. FIG. 11 further illustrates the field enhancing resonant rings (‘suspended’ loops) 1102 having electromagnetic 1103 parasitic interaction particularly with the axial segment of the feed element 1104, parasitic electromagnetic interaction between rings 1105, and increased at the horizon and near the horizon field signal strengths 1106.

    (34) The scalar wave component of the energy field of the enhanced scalar wave beam antenna penetrates objects and walls well 1401 as illustrated in FIG. 14; the transverse wave component penetrates poorly 1402, and residual transverse wave components are then enhanced 1403 by penetrating same-polarity scalar wave 1404.

    (35) FIG. 13 illustrates the ability to enhance penetrating and distance energy transfer capabilities with a metal reflector 1301 supplementing the scalar wave receiving antenna with directivity.

    (36) The effective penetrating transfer of energy at distances is efficient and substantial and novel to mankind. FIG. 15 illustrates bright light generated passing energy through walls to ‘ENERSEND RECEIVERS’ with LED's ˜55 feet away, where the transmitter is of only ˜5 watts of power. The light produced at the scalar wave beam receiver at substantially 55 feet with a total of 40 LED's where each LED is producing ˜5 lumens, for a total of ˜200 lumens, is substantially equal to the light generated by a 7-watt incandescent light bulb.

    (37) With this new ability to transfer energy through the air, through space, through objects, a number of applications exist including powering electronic devices directly as illustrated in FIG. 16, including soap dispensers, radios, cell phones, cordless phones, headphones and headsets, hand tools, toys, medical equipment, office equipment, remote systems, emergency and back-up systems, security systems, sensors.

    (38) The transferred energy may also be used to charge batteries remotely as illustrated in FIG. 17.

    (39) And new horizons in penetrating and distance communications is now realized as illustrated in FIG. 18.

    (40) FIG. 19 illustrates military applications particularly using high transmitted power resulting in substantial penetrating energy levels through substantial objects and walls.