Monopole antennas are a common and inexpensive way to radiate an omnidirectional signal. The vertical radiator of a basic monopole antenna may include a ground to plane redirect a portion of the radiated electromagnetic energy over the surface of the earth. Otherwise a portion of the radiated energy may be lost, constructively cancelled, or dissipated. The ground plane may comprise the earth's surface or an artificial metallic or conductive plate that serves as an electromagnetic field reflector. The present disclosure, however, concerns an improvement to artificial ground planes. A monopole antenna having an artificial conductive plate ground plane, for example, simulates the function of a dipole antenna. Furthermore, the functionality of a monopole antenna with a sufficiently large ground plane approaches that of a dipole antenna.
Standard monopole antennas are vertically polarized elements that may produce an electromagnetic field over a ground plane. Monopole antennas produce null emissions at their zeniths, which make them ill suited for short range communications at high incident angles. The null at zenith also prevents full hemispherical coverage which is more important in airborne links from a ground station.
Previous techniques to fill null emission patterns included bending the monopole element. Unfortunately, this technique requires extraordinary precision and advanced manufacturing methods, especially at high frequencies. Bending of the monopole element also distorts the azimuthal symmetry of the pattern.
It is therefore an object of the present invention to provide a new antenna with a structure to partially obviate null emission patterns at its zenith.
It is further an object of the present invention to provide an existing antenna with a ground plane structure to at least partially fill otherwise null emission patterns at its zenith.
It is another object of the present invention to provide an antenna with an inexpensive mechanism to reduce null emission patterns at its zenith without bending the radiator element.
The present invention provides an antenna with the capability of filling a null at zenith. The invention takes advantage of slots in the ground plane which produce a measurable amount of circularly polarized radiation toward the zenith. The slots interrupt the currents and redirect energy into space.
The angle and the distance of the slots from the center of the monopole play a critical role in the amount of radial current redirected and the phase of the redirected energy respectively. A radial slot will not interrupt the radial current and will therefore not radiate; whereas slots perpendicular to the radius interrupt the most current and radiate the strongest. One embodiment utilizes an angle of forty-five degrees for the slots. In addition to the angle of the slots, this embodiment utilizes two slots that radiate vertically and two slots that radiate horizontally. The slots are spaced to cause a ninety degree phase difference. The ninety degree phase difference radiates circular polarization toward the zenith.
As there is no preferred azimuthal orientation, the circular polarization fills the null for all azimuthal orientations. The pattern at zenith corresponds to shorter ranges; therefore, a minimal gain of between −10 to −15 dB is useful at the zenith. In addition to reducing null depth by approximately 20 dB, the pattern of the monopole near the horizon is relatively unaffected. The present invention may be utilized while constructing a new antenna or in retrofitting or modifying an existing antenna.
Now referring to the drawings,
The slots 218 in the ground plane redirect induced currents in the ground plane which, in turn, stabilize an interference pattern in the signal 206 to redirect energy towards the zenith. The slots 218 may traverse a portion of the insulator thickness 216 or the entire thickness 216. For thin ground planes, the slot preferably runs the entire thickness of the ground plane. For thicker ground planes, it may be sufficient for the slots to only span a portion of the thickness to obtain a desired signal pattern. The angle of the slots 218 relative to a radius of the ground plane determines the extent of induced current flow in the ground plane and the amount of energy redirected. Radial slots do not interrupt radial EM emissions; while slots perpendicular to the radius interrupt a greater amount of EM emissions. Depending on the orientation of the slot angle, the EM emission may radiate horizontally or vertically. The number of slots 218 also may be varied to increase symmetry of the radiated signal.
In addition to the angle of the slots relative to a radius of the ground plane, the distance of the slots 218 from the radiator 202 determine the phase of the redirected EM emissions. Again referring to
The circular polarization 230; therefore, fills the null at the zenith 213. As there is no preferred azimuthal orientation at the zenith 213, the circular polarization is effective for filling the signal null at all azimuthal orientations. The gain needed at the zenith 213 corresponds to shorter ranges; hence only a minimal gain is needed at the zenith 213. A gain of −10 to −15 dB can provide sufficient gain while the pattern of the monopole antenna 200 is relatively unaffected. Any fill in the null is detrimental to side radial radiation and can be thought of a zero sum. Thus, any amount gained at the null is lost radially.
Now referring to
As detailed above, the number of slots, the angle of the slots relative to the ground plane radius, the distance of the slots, as well as the size and shape of the slots has an effect on the signal radiated by the slots. Each of the variables can be adjusted to develop a preferred particular embodiment for each antenna. Now referring to
The ground plane 404 further comprises a first slot 410, a second slot 412, a third slot 414 and a fourth slot 416, each having a long dimension and a short dimension. The slots 410, 412, 414 and 416 are positioned such that the slots make a forty five degree angle relative to the ground currents 408. The slots 410, 412, 414 and 416 interrupt the ground current 408 and produce a radiated polarization 420 perpendicular to the long dimension of the slots 410, 412, 414 and 416. The slots 410, 412, 414, and 416 are oriented such that two of the slots 410, 412, 414 and 416 radiate vertically and two of the slots 410, 412, 414, and 416 radiate horizontally. Slots 410 and 416 are further oriented such that they are perpendicular to slots 412 and 414.
Again referring to
Now referring to
The slots in the embodiments may be made during the initial construction of the monopole antenna or by retrofitting or modifying existing monopole antennas. The slots may be made separately or with the manufacture of the ground plane, by stamping, chemical material removal, cutting, laser cutting, plasma cutting, water-jet cutting, a circuit board manufacturing process, or any other similar or known processes. Furthermore, the ground plane may also be a layer on a substrate.
Having thus described the invention in connection with the several embodiments thereof, it will be evident to those skilled in the art that various revisions can be made to the several embodiments described herein with out departing from the spirit and scope of the invention. It is my intention, however, that all such revisions and modifications that are evident to those skilled in the art will be included with in the scope of the following claims. Any elements of any embodiments disclosed herein can be used in combination with any elements of other embodiments disclosed herein in any manner to create different embodiments.
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