Hybrid phased array transmission
US-10103452-B2 · Oct 16, 2018 · US
US10498174B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10498174-B2 |
| Application number | US-201715837362-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 11, 2017 |
| Priority date | Dec 11, 2017 |
| Publication date | Dec 3, 2019 |
| Grant date | Dec 3, 2019 |
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Systems and methods for efficient coupling to low-loss eigenmodes of a spherical waveguide bounded by the Earth's surface and its ionosphere are disclosed. One or more eigenmodes of the Earth-ionosphere waveguide may be computed based on a mathematical model incorporating electrical properties of the terrestrial surface and plasma physics of the ionospheric layer. An array of electrically-connected waveguide-coupling elements may be configured for coupling to the one or more eigenmodes. By adjusting relative phases and/or amplitudes of the waveguide-coupler elements, as well as frequencies, the electrical size of the array may be made much larger than its physical size, and substantial electromagnetic energy may be targeted to preferentially excite the one or more eigenmodes. The adjustments may also account or compensate for non-homogeneous propagation properties of the ionosphere, and help reduce ohmic losses in the ionosphere.
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What is claimed: 1. An apparatus comprising: an electrically small array of waveguide coupling elements configured for coupling energy into a waveguide cavity; and a computer apparatus having one or more processors and memory storing instructions that, when executed by the one or more processors, cause the system to carry out operations including: determining an eigenmode of the waveguide cavity; and causing the electrically small array of coupling elements to generate an electromagnetic excitation that overlaps with the eigenmode, wherein causing the electrically small array of coupling elements to generate the electromagnetic excitation that overlaps with the eigenmode couples energy into the waveguide cavity. 2. The apparatus of claim 1 , wherein the waveguide cavity is a spherical waveguide cavity that is bounded by a terrestrial surface and an ionospheric layer. 3. The apparatus of claim 2 , wherein the spherical waveguide cavity is Earth. 4. The apparatus of claim 1 , wherein the electrically small array of coupling elements comprises at least one of: a driven element and a parasitic element. 5. The apparatus of claim 4 , wherein a discrete electrical element is electrically coupled to a driven element of the array. 6. The apparatus of claim 4 , wherein the at least one driven element is coupled to at least one power source, wherein the at least one power source comprises a coupling element, and wherein the at least one driven element is positioned within a coupling distance of the at least one power source. 7. The apparatus of claim 1 , wherein a separation distance between any two adjacent coupling elements of the array is less than a wavelength of the eigenmode. 8. The apparatus of claim 7 , wherein separation distance is on distance scales between 0.01λ, and 0.0001λ, where λ is the eigenmode wavelength of the eigenmode. 9. The apparatus of claim 1 , wherein the coupling elements are electrically small resonant elements. 10. The apparatus of claim 1 , wherein the apparatus is a helical coil resonator, and wherein turns of the helical coil resonator comprise the array of waveguide coupling elements. 11. The apparatus of claim 10 , wherein the helical coil is vertically oriented. 12. The apparatus of claim 10 , wherein a pitch of the helical coil is determined based on the eigenmode. 13. The apparatus of claim 10 , wherein the helical coil comprises at least one conductive material, wherein a type of the at least one conductive material is selected based on the eigenmode. 14. The apparatus of claim 10 , wherein a respective diameter of one or more turns of the helical coil is determined based on the eigenmode. 15. The apparatus of claim of claim 10 , wherein the helical coil is one of a resonator or a slow-wave waveguide coupling structure. 16. The apparatus of claim 1 , wherein causing the array of coupling elements to generate the electromagnetic excitation that overlaps with the eigenmode comprises driving each of the coupling elements with a respective signal that has a respective phase and a respective magnitude. 17. A method comprising: computing one or more eigenmodes of a spherical waveguide cavity encompassed by two boundaries; determining at least one of the one or more eigenmodes to use for wireless energy transmission in the spherical waveguide cavity; and causing an electrically small array of coupling elements to generate an electromagnetic excitation that overlaps the at least one eigenmode, wherein causing the electrically small array of coupling elements to generate the electromagnetic excitation that overlaps the at least one eigenmode couples energy wirelessly into the spherical waveguide cavity. 18. The method of claim 17 , wherein the computing is based on a mathematical model that incorporates respective properties of the two boundaries. 19. The method of claim 18 , wherein a first one of the boundaries is a terrestrial surface and a second one of the boundaries is an ionospheric layer, wherein the respective properties of the terrestrial surface are electrical properties, and wherein the respective properties of the ionospheric layer are properties based on plasma physics of the ionospheric layer. 20. An apparatus comprising: an electrically small array of coupling elements configured for extracting energy from a spherical waveguide cavity; and a controller configured to: determine an eigenmode of the spherical waveguide that is overlapped by an electromagnetic excitation generated by a transmitter; and receive a first signal from a first element of the array and a second signal from a second element of the array, wherein the first signal and the second signal correspond to the electromagnetic excitation that overlaps the eigenmode of the spherical waveguide cavity, and wherein said receiving extracts energy from the spherical waveguide cavity.
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