US 5,495,258 AGrant

Multiple Beam Antenna System for Simultaneously Receiving Multiple Satellite Signals

Issue Date:1996-02-27

•9 Claims

•11 Drawing Sheets

Abstract

A multiple beam array antenna system including a first group of right-handed circularly polarized subarrays and a second group of left-handed circularly polarized subarrays. Combined signals from the right-handed subarrays are output via low noise amplifiers to a first electromagnetic lens while the outputs of the left-handed circularly polarized subarrays are sent via low noise amplifiers to a second steering electromagnetic lens. A satellite selection matrix output block allows a user to tap into signals from right-handed circularly polarized satellites, left-handed circularly polarized satellites, and linearly polarized satellites. A plurality of satellites (e.g. right-handed satellite "A" and linearly polarized satellite "B") may be accessed simultaneously thus allowing the user to utilize both signals at the same time.

Metadata

Assignee

Muhlhauser; Nicholas L.

Inventors

Nicholas L. Muhlhauser
Scott A. Townley
Thomas C. Weakley

Application Information

Application Number:US 2993767

Filing Date:1994-09-01

Priority Date:1994-09-01

Art Unit:254

Classifications

IPC:

H01Q 1906

Field of Search:

343342753;789;895;754;844;850;853361;362;375;371;372;373

Patent Drawings (11 sheets)

Description

This invention relates to an array antenna system. More particularly, this invention relates to a multiple beam array antenna system of relatively high directivity helical elements including a plurality of electromagnetic lenses and multiple antenna element subarrays, each subarray being of either the right or left handed circularly polarized type.

Background of the Invention

High gain antennas are widely useful for communication purposes such as radar, television receive-only (TVRO) earth station terminals, and other conventional sensing/transmitting uses. In general, high antenna gain is associated with high directivity, which in turn arises from a large radiating aperture.

High gain antenna systems are often used in connection with TVRO systems such as those in the circularly polarized direct broadcast (DBS) band and in other linearly polarized systems. TVRO systems have been available since the early 1980s to those desiring to watch television via satellite delivered signals in their homes. A common method for achieving a large radiating aperture in TVRO applications is by the use of parabolic reflectors fed by a feed arrangement located at the focal point or focus of the parabolic reflector. Typically, large mesh or solid parabola-type antennas (i.e. backyard dishes) are placed in the yard of the consumer. Such parabolic dishes are often motorized so as to enable rotational movement along particular spatial arcs in which satellites are disposed thereby allowing the homeowner or consumer to view any one of a number of different satellites, one at a time. Unfortunately, movement of such parabolic antennas via the motor from one satellite to another is time consuming (i.e. it may take up to two minutes or more in some instances for the motor to move a typical parabola dish-type antenna from one extreme of the arc of satellites to the other) and subject to mechanical breakdown.

Motorized parabolic antenna systems also tend to be bulky, noisy, and subject to high maintenance requirements due to their abundance of moving parts. As stated above, most such parabolic antennas can only receive one satellite signal at a time. This is because typically a parabolic antenna reflects and concentrates the received signal to its focal point. A feed is mounted at the focal point to receive the signal and direct it to an amplifier/down converter which then directs the signal to the receiver in the home. Thus, depending upon what direction the dish is oriented, one satellite signal is focused into the focal point feed at a time.

Some prior art parabolic antennas have included multiple feeds near the center of the dish so as to enable the homeowner to receive multiple satellite signals simultaneously. Unfortunately, the angular range of such multi-feed systems is limited and such multi-feed antennas typically experience a signal loss because the multi-feeds are not directly in the center (i.e. focal center) of the dish but are only in its general proximity. Additionally, parabolic antennas often suffer structure required to support the feed, this often adversely affecting the illumination of the aperature and thereby perturbing the far-field radiation pattern.

Modern antenna systems have found increasing use of antenna arrays for high gain purposes. Phased array antennas often consist of a single output port and a plurality of stationary antenna elements which are fed coherently and use variable phase or time-delay control at each element to scan a beam to given angles in space. Such systems are highly expensive and are generally for this reason not used in TVRO applications. Variable amplitude control is sometimes also provided for pattern shaping. Single beam phased arrays are sometimes used in place of fixed aperture parabolic antennas, because the multiplicity of antenna elements allows more precise control of the radiation pattern thus resulting in lower side lobes and precise pattern shaping. The primary reason for the widespread use of such phased array antennas is to produce a directive beam that can be repositioned (scanned) electronically as opposed to the mechanical repositioning requirements of motorized parabolic antennas.

While phased arrays often have a single output port, multiple beam antenna systems have a multiplicity of output ports, each corresponding to a beam with its peak at a different angle in space. Typical systems utilizing such multiple beam technology and needing simultaneous, independent beams include multiple-access satellite systems and a variety of ground-based height-finding radars. Generally, multiple beam array antenna systems utilize a switching network that selects a single beam or a group of beams as required for specific applications via a generic lens or reflector. Other applications for multiple beam arrays include their use in the synthesis of shaped patterns where the beams are the constituent beams that combine to make up the shaped pattern, as in the commonly known Woodward-Lawson procedure. In still other cases, multiple beam arrays are used as one component of scanning systems such as the use of a multiple beam array feed for a reflector or lens system.

With the advent of higher power Ku band and direct broadcast satellites (DBS), it has become possible to manufacture array antennas having a diameter of less than about one meter. DBS is a term generally used for direct satellite to home transmissions. Such small high gain antennas have clear aesthetic advantages over bulky parabolic antennas.

Array antennas generally include an array (or plurality of elements or of subarrays of elements) of ordinarily identical antenna elements, each of which has a lower gain than the gain of the array. The antennas (or elements) are arrayed together and fed with an amplitude and phase distribution which establishes the far-field radiation pattern. Since the phase and power applied to each element of the array can be individually controlled, the direction of the beam (transmitting and receiving) can be controlled by controlling the amplitude and phase applied to each element in phased array systems. In multiple beam systems, reflectors or lenses are used to control the beam. A salient advantage of array antennas is clearly the ability to scan the beam or beams electronically without moving the mass of a reflector as is required in prior art parabolic-type antennas. A widespread problem of conventional phased array antennas and parabolic-type antennas is that they are limited to viewing one satellite at a time without experiencing reduced power or gain.

Existing satellites currently in orbit generally transmit two different and distinctive types of signals, namely circularly polarized (right and left-handed), and linearly polarized (horizontal and vertical). Accordingly, typical helical antenna elements making up array antennas may be wound in either the right-handed or left-handed directions. Helical antenna elements having right-handed windings or turns thereon may receive right-handed circularly polarized signals from right-handed satellites, but are eternally blind to left-handed circularly polarized satellite signals. This is also the case with left-handed helical antenna elements, such elements having the ability to received left-handed circularly polarized signals from satellites but being blind to satellite emitting right-handed circularly polarized signals.

Thus, conventional array antennas having only a plurality of left-handed circularly polarized antenna elements are blind to right-handed transmitting satellites, and arrays having only right-handed wound elements are blind to satellites transmitting left-handed circularly polarized signals. Therefore, consumers, in view of the limitations of the prior art, must decide whether they wish to view right-handed or left-handed circularly polarized signals in determining which type of antenna array to purchase (i.e. right-handed or left-handed) because conventional arrays are generally either right or left-handed.

While conventional multiple beam array antenna systems can receive beams from different satellites, such antennas cannot simultaneously receive signals from different satellites at substantially the same frequency where the satellites have different polarizations such as those of right and left handed circular polarization.

Accordingly, the need arises for an array antenna system having the ability to receive both right-handed and left-handed circularly polarized satellite signals, as well as linearly polarized signals (horizontal and vertical). Additionally, it would satisfy a long felt need in the art if such an antenna system were to be able to simultaneously receive signals from multiple satellites without substantial reduction in antenna directivity or gain, the received signals being any combination of right-handed, left-handed, or linear polarizations.

Currently, communication satellites re-broadcasting television signals to television receive-only (TVRO) earth stations from geostationary orbits over the equator are spaced apart by predetermined degrees of longitude (e.g. 4.degree.). Such angular spacing between satellites places severe requirements on TVRO antennas. In order to satisfactorily discriminate against interference from adjacent satellites that are re-using the same frequency band and polarization, antennas having high directivity and narrow beamwidths are required. Satisfying such requirements with conventional parabolic antennas necessitates the use of reflectors having very large diameters, this, of course, being undesirable. Clearly, there is also a need for a small, cost effective, array antenna system that is highly responsive to signals arriving from a primary receiving direction (e.g. satellite) but which can effectively nullify signals and noise arriving from other directions which differ from the primary receiving direction by a very small angle.

U.S. Pat. No. 4,845,507 discloses a modular radio frequency array antenna system including an array antenna and a pair of steering electromagnetic lenses. The antenna system of this patent utilizes a large array of antenna elements (of a single polarity) implemented as a plurality of subarrays driven with a plurality of lenses so as to maintain the overall size of the system small while increasing the overall gain of the system. Unfortunately, the array antenna system of this patent cannot simultaneously receive both right-hand and left-handed circularly polarized signals, and furthermore cannot simultaneously receive signals from different satellites wherein the signals are right-handed circularly polarized, left-handed circularly polarized, linearly polarized, or any combination thereof.

U.S. Pat. No. 5,061,943 discloses a planar array antenna assembly for reception of linear signals. Unfortunately, the array of this patent, while being able to receive signals in the fixed satellite service (FSS) and the broadcast satellite service (BSS) at 10.75 to 11.7 GHz and 12.5 to 12.75 GHz, respectively, cannot receive signals (without significant power loss and loss of polarization isolation) in the direct broadcast (DBS) band, as the DBS band is circular (as opposed to linear) in polarization.

U.S. Pat. No. 4,680,591 discloses an array antenna including an array of helices adapted to receive signals of a single circular polarization (i.e. either right-handed or left-handed). Unfortunately, because satellites transmit in both right and left-handed circular polarizations to facilitate isolation between channels and provide efficient bandwidth utilization, the array antenna system of this patent is blind to one of the right-handed or left-handed polarizations because all elements of the array are wound in a uniform manner (i.e. the same direction).

It is apparent from the above that there exists a need in the art for a multiple beam array antenna system (e.g. of the TVRO type,) which is small in size, cost effective, and modular so as to increase gain without significantly increasing cost. There also exists a need for such a multiple beam array antenna system having the ability to receive each of right-handed circularly polarized signals, left-handed circularly polarized signals, and linearly polarized signals. Additionally, the need exists for such an antenna system having the potential to simultaneously receive signals from different satellites, the different signals received being of the right-handed circularly polarized type, left-handed circularly polarized type, linearly polarized typed, or combinations thereof. It is the purpose of this invention to fulfill the above-described needs in the art, as well as other needs apparent to the skilled artisan from the following detailed description of this invention.

Those skilled in the art will appreciate the fact that array antennas are reciprocal transducers which exhibit similar properties in both transmission and reception modes. For example, the antenna patterns for both transmission and reception are identical and exhibit approximately the same gain. For convenience of explanation, descriptions are often made in terms of either transmission or reception of signals, with the other operation being understood. Thus, it is to be understood that the array antennas of the different embodiments of this invention to be described below may pertain to either a transmission or reception mode of operation. Those of skill in the art will also appreciate the fact that the frequencies received/transmitted may be varied up or down in accordance with the intended application of the system.

Those of skill in the art will also realize that right and left-handed circular polarization may be achieved via properly summing horizontal and vertical linearly polarized elements.

Summary of the Invention

Generally speaking, this invention fulfills the above-described needs in the art by providing a multiple beam array antenna system for simultaneously receiving/transmitting signals of different polarity, the system comprising:

beams for receiving/transmitting both linearly and circularly polarized signals at substantially the same frequencies; and

means for simultaneously receiving/transmitting at least two of: (i) right-handed circularly polarized signals; (ii) left-handed circularly polarized signals; and (iii) linearly polarized signals.

In certain further preferred embodiments of this invention, the means for simultaneously receiving/transmitting both linearly and circularly polarized signals at substantially the same frequency includes a first time delay electromagnetic lens coupled to a group of right-handed circularly polarized subarrays, and a second time delay electromagnetic lens coupled to a group of left-handed circularly polarized subarrays.

In still further preferred embodiments of this invention, the system further includes means for summing adjacent output ports on said first and second time delay lenses so as to split the step size of the lenses.

This invention further fulfills the above-described needs in the art by providing a multiple beam array antenna system for receiving electromagnetic polarized signals from different satellites, the system comprising:

first and second subarrays of circularly polarized helical antenna elements, the first subarray of antenna elements being right-handed circularly polarized and the second subarray of antenna elements being left-handed circularly polarized;

first and second signal summing waveguides, the received electromagnetic signals from the first subarray being summed in the first waveguide and the received electromagnetic signal from the second subarray being summed in the second waveguide;

first and second low noise amplifiers, the summed signal from the first subarray and the first waveguide being amplified by the first amplifier and the sum signal from the second subarray and the second waveguide being amplified by the second amplifier;

first and second electromagnetic lenses for allowing multiple signals to be received by the multiple beam array antenna system, the summed right-handed circularly polarized signal amplified by the first amplifier being sent to the first electromagnetic lens and the summed left-handed circularly polarized signal amplified by the second amplifier being sent to the second electromagnetic lens whereby the first lens acts upon received right-handed circularly polarized signals and the second lens acts upon received left-handed circularly polarized signals so that the system can receive both right and left-handed circularly polarized signals and thereafter output their contents.

This invention will now be described with respect to certain embodiments thereof, accompanied by certain illustrations, wherein:

In the Drawings

FIG. 1 is an exploded perspective view of the multiple beam array antenna system of a first embodiment of this invention.

FIG. 2 is a side cross-sectional view of a single antenna element of the array coupled to a combining waveguide according to a second embodiment of this invention. This FIG. 2 embodiment is equivalent to the first or FIG. 1 embodiment except that elements 7 and 9 of FIG. 2 are formed of a single piece of milled aluminum in the FIG. 1 embodiment.

FIG. 3 is a perspective view of an antenna element of the first or second embodiment of this invention.

FIG. 4 is a bottom view of the antenna element of FIG. 3.

FIG. 5 is a front or rear cross-sectional view of a subarray of antenna elements positioned adjacent their corresponding combining subarray waveguide according to the FIG. 2 embodiment of this invention.

FIG. 6 is a top elevational view of the plurality of antenna elements making up the plurality of subarrays of the array antenna of either the first or second embodiment of this invention.

FIG. 7 is a side elevational view of either of the electromagnetic lenses of the FIG. 1 (or FIG. 2) embodiment of this invention, with the lens rotated about 90.degree. from its position illustrated in FIG. 1.

FIG. 8 is an exploded cross-sectional front view of the electromagnetic lens of FIG. 7 illustrating the layers making up the lens.

FIG. 9(a) is a schematic diagram of the FIG. 1 (of FIG. 2) embodiment of this invention illustrating the different subarrays, combining waveguides, low noise amplifiers, electromagnetic lenses, and satellite selection output matrix block.

FIGS. 9(b)-9(e) are schematic diagrams illustrating different scenarios of the electromagnetic lenses being manipulated by the output block in order to view particular satellite(s).

FIG. 10 is a side elevational view of the output matrix block according to the first or second embodiment of this invention.

FIG. 11 is a front elevational view of the output block of FIG. 10, this view illustrating the output block inputs enabling electrical connection via transmission lines between the output block and the electromagnetic lenses.

FIG. 12 is a rear elevational view of the output block of FIGS. 10-11, this view illustrating the block outputs which enable the homeowner or consumer to choose particular satellite(s) for view.

FIG. 13 is an electric diagram of the low noise amplifiers (LNAs) according to the FIG. 1 (or FIG. 2) embodiment of this invention, where a single LNA is enlarged.

FIG. 14 is a graph illustrating a normalized theoretical radiation pattern of an antenna element and the array pattern according to the first or second embodiment.

FIG. 15 is a graph illustrating a computed array radiation pattern from a measured antenna element pattern according to the first or second embodiment.

Detailed Description of Certain Embodiments of This Invention

Referring now more particularly to the accompanying drawings in which like reference numerals indicate like parts throughout the several views.

FIG. 1 is an exploded perspective view of the multiple beam array antenna system according to a first embodiment of this invention. The system is adapted to receive signals in about the 10.70-12.75 GHz range in this and certain other embodiments. The multiple beam array antenna system of this embodiment takes advantage of restrictions in scan coverage in order to produce a high gain scanning system with few phase controls. Electromagnetic lenses (described below) are provided in combination with a switching network so as to allow the selection of a single beam or group of beams as required for specific applications.

The multiple beam array antenna systems of the different embodiments may be used in association with, for example, DBS and TVRO applications. In such cases, a beam array of relatively high directivity helical elements is provided and designed for a limited field of view. The system when used in at least DBS applications provides sufficient G/T to adequately demodulate digital or analog television downlink signals from high powered Ku band DBS satellites in geostationary orbit. Other frequency bands may also be transmitted/received. The field of view may be about .+-.12 degrees in certain embodiments, but may be greater or less in certain other embodiments.

With respect to the term "G/T" mentioned above, this is the figure of merit of an earth station receiving system and is expressed in dB/K. G/T=G.sub.dBi -10 log T, where G is the gain of the antenna at a specified reference point and T is the receiving system effective noise temperature in kelvin.

The array antenna portion includes a plurality of helical subarrays made up of antenna elements 1, element or antenna mounting plate 3, signal combining waveguides 5 (one waveguide 5 per subarray), and protective housing or radome 8. Protective housing 8 slides over antenna elements 1 and is affixed to element mounting plate 3 during use of the system so as to protect antenna elements 1. Housing 8 provides environmental protection to elements 1 and is transparent to the frequency fields (e.g. radio frequency fields) existing at the antenna aperture. Antenna elements 1, mounting plate 3, and waveguides 5 are illustrated in more detail in FIGS. 2-5.

FIG. 2 is a cross-sectional side view of a single antenna element 1 in a subarray illustrating its connection to mounting plate 3 and signal summing or combining subarray waveguide 5. In this FIG. 2 embodiment, mounting plate 3 is shown as being made up of two separate members, portion 7 defining waveguide 5 and portion 9 which is a conductive ground plane defining cup aperture 11 in which element 1 is mounted. Members 7 and 9 are affixed to one another. Alternatively, and as shown in the FIG. 1 embodiment, elements 7 and 9 defining mounting plate 3 may be made of a single piece of milled aluminum or the like wherein waveguides 5 and cup apertures 11 are milled out of the aluminum piece or block making up mounting plate 3. Other conventional metals or plastics may be used instead of aluminum. Thus, the only difference between the first embodiment and the FIG. 2 embodiment is that in the FIG. 2 embodiment plate 3 is made up of two members (7 and 9) instead of one.

Antenna element 1 as shown in FIG. 2 includes tapered dielectric rod or mandrel 13 which is made of an injection moldable plastic material or the like having a substantially low loss tangent. A material suitable for use in forming and making dielectric cone-shaped mandrel 13 is Delrin. A single wire or foil conductor 15 is wound around dielectric mandrel 13 in a helical fashion so as to define an electrically conductive helix located on the exterior surface of dielectric mandrel 13. Wire conductor 15 performs the primary electrical receiving (and transmitting) function of antenna element 1.

The material Delrin chosen for making dielectric mandrel 13 of element 1 has the advantages of being a plastic with a low loss tangent and being injection moldable. Any other conventional dielectric material having such characteristics or the like may also be used as dielectric mandrel or rod 13.

Conductive member 15 wound around dielectric 13 is made of copper foil including an adhesive backing in certain embodiments of this invention, the adhesive being for affixing the conductive foil 15 to dielectric mandrel 13. Such copper foil used as conductive helical member 15 may be about 2-3 mils thick and in the form of about a 50 mil strip in certain embodiments of this invention. Alternatively, copper wire or the like may instead be used as conductive helical member 15 on dielectric 13.

As shown, conductive wire (or foil) 15 is wound down from the apex or zenith of tapered mandrel 13 toward the base to a point 17 where wire 15 meets and is conductively attached to wire portion 19 disposed within dielectric 13. Wire 19 extends from the outer periphery of mandrel 13 (at point 17 where it is conductively attached to wire 15) to wire element output probe 21. Element output probe 21 extends from the base of element 1 (where it is conductively connected to wire 19) into signal summing waveguide 5. All elements 1 in the array are similar to the illustrated element portrayed in FIGS. 2-4.

In certain embodiments of this invention, a small notch is cut in dielectric mandrel 13 immediately adjacent wire 15 as it extends down and around mandrel 13. This notch (not shown) scribed in mandrel 13 winds around the mandrel from its apex to its base always adjacent wire 15. This notch is for alignment purposes with respect to conductor 15.

A plurality of elements 1 make up the plurality of subarrays making up the overall array. The array geometry is designed so as to provide sufficient gain for satellite downlink. Sufficient gain may be taken to mean a minimum of about 31 dBi for typical Ku band TVRO satellites in certain embodiments. A gain of from about 27-37 dBi may be utilized, and more preferably a gain of about 30-31 dBi may be achieved in certain embodiments. However, this gain may change in accordance with the application of the system in other embodiments. Additionally, the array is designed so as to obtain adequate G/T for applicable downlink situations.

Many different array lattices may be used to obtain satisfactory gain (e.g. about 31 dBi) in the different embodiments of this invention. In certain preferred embodiments, non-symmetrical subarrays (as will be described below and shown for example in FIG. 6) are formed so as to generate a fan type beam(s) with the fan direction oriented substantially perpendicular to the geostationary orbital satellite belt in the case of DBS applications. Fan shaped beam(s) have the advantage of reducing intersatellite interference in the absence of polarization and frequency band diversity for multiple beam earth stations.

The structural design of elements 1 is important for suppressing the grating lobes formed by the relatively sparse element spacings used in certain embodiments of this invention. The sparsely populated array in certain embodiments reduces the number of components and therefore total cost, but introduces certain radiation maxima which need to be suppressed or eliminated in order to realized substantially full array gain. Accordingly, elements 1 are designed so as to have sufficient directivity over the full DBS bandwidth so that a null (or greatly reduced radiation intensity) is produced for all angles equal to or greater than the closest approaching grating lobe. This angle is dependent upon the element 1 spacing and the maximum desired steering angle. Elements 1 spacing with respect to wavelength will be discussed below.

Furthermore, elements 1 are designed to have sufficiently low directivity over the full DBS bandwidth such that the element 1 radiation intensity at the angle corresponding to maximum steer is as high as possible (i.e. minimum pattern roll-off from maximum). Elements 1 are efficient over the full bandwidth to an extent so that they do not substantially dominate the system G/T. The input impedances of elements 1 over the full bandwidth are substantially similar and are at a convenient value of resistive impedance (e.g. about 25-100 ohms, and more preferably about 50 ohms).

In accordance with the above design requirements, in certain embodiments of this invention, tapered mandrel 13 of each element 1 may have a base diameter of about 0.321 inches at its base adjacent base 29 of cup aperture 11 (or the top surface of portion 7 as shown in FIG. 2) and a top diameter of about 0.229 inches at its apex 23. Additionally, the above-mentioned notch scribed in mandrel 13 adjacent helical wire 15 may be about 1 mil deep, the spiral spacing between wire or foil 15 along the exterior periphery of mandrel 13 (i.e. between turns) may be about 0.245 inches, and the axial length of dielectric mandrel 13 may be about 4.41 inches in certain embodiments of this invention. In these embodiments, there are about 18 turns of wire or conductor 15 from apex 23 to the base of dielectric mandrel 13. Also, wire 19 connecting helical conductor 15 to element output probe 21 within element 1 may have about a 160-200 mil diameter in certain embodiments.

With respect to antenna element spacing, helical antenna elements 1 within particular subarrays are spaced apart about 1.6.lambda. and the elements 1 of adjacent (right-handed and left-handed) subarrays are spaced apart about 1.2.lambda. in certain embodiments of this invention. Element spacings may however be from about 1.0-1.8 with respect to wavelength in certain other embodiments. When the multiple beam array antenna system is designed to receive frequencies in the range of from about 10.7 GHz to 12.75 GHz, .lambda. (wavelength) is defined in the middle of this band (i.e. at about 11.8 GHz).

While the above listed numerical parameters are illustrative for certain embodiments of this invention, they are not limiting upon the scope of the invention. Accordingly, different element 1 parameters than those listed above may be utilized in accordance with the intended scope and need of the array antenna system in certain embodiments of this invention.

Alternatively, instead of using wire 19 to connect helical conductor 15 to probe 21, a notch may be cut in the base portion of dielectric 13 so as to allow helical winding (e.g. foil) 15 to extend into the notch to the axial center of dielectric 13 where an electrical connection may be made between wire probe 21 and winding 15. Thus, probe 21 and wire 15 may be conductively attached in the notch at the axial center of dielectric 13 without the need for wire 19 according to this alternative. Additionally, if such a notch is provided, wire 19 may extend straight upwardly from probe 21 so as to meet and connect to conductor 15.

The dielectric mandrel 13 of each antenna element 1 includes a cylindrical extension portion 25 protruding from its base so as to allow each mandrel 13 to be affixed to element mounting plate 3 (or portion 7 thereof as in the FIG. 2 embodiment). An aperture is defined in mounting plate 3 (or portion 7 in the FIG. 2 embodiment) so as to allow extension 25 of mandrel 13 to extend thereinto thus allowing the mandrel to be mounted on mounting plate 3 and fixedly disposing element output probe 21 within the confines of rectangular signal summing waveguide 5. Extension 25 also provides an impedance match between the helix and probe 21.

Conductive cup aperture 11 is defined around each antenna element 1 in mounting plate 3 (or grounding plane 9 in the FIG. 2 embodiment) for radiation mode suppression purposes as is known in the art. Each conductive ground plane cup aperture 11 adjacent each antenna element 1 in the array (and subarrays) includes a base portion 29 immediately adjacent the base of mandrel 13, a substantially circular sidewall portion 27 defining aperture 11, and a central aperture in the base portion for allowing extension 25 of mandrel 13 to extend. As shown in FIG. 2, sidewall 27 of the conductive cup may extend upward at an angle substantially perpendicular to base portion 29 of the cup. Alternatively, but not shown, sidewall 27 of the conductive cup may extend from base portion 29 toward apex 23 of mandrel 13 with linearly increasing diameter as sidewall 27 extends toward apex 23. Thus, the diameter of the cup adjacent base portion 29 will be smaller than its diameter adjacent the exterior portion of the cup closest to apex 23 of mandrel 13.

For impedance matching purposes, the height of sidewalls 27 defining cup aperture 11 is about one-half (1/2) .lambda. and the diameter of cup aperture 11 is about three-quarter (3/4) .lambda. in certain embodiments of this invention. Accordingly, .lambda. at, for example, 11.8 GHz is about 1 inch. Therefore, at 11.8 GHz, the diameter of cup 11 is about three-quarters inch and the height of cup 11 is about one-half inch in certain embodiments.

FIG. 3 is a perspective view of a single antenna element 1 including winding 15. FIG. 4 is a bottom view of an element 1 illustrating the base portion of mandrel 13, extension 25, and wire output probe 21.

The output probe 21 of each element 1 which extends into the appropriate subarray signal combining waveguide 5 may be made of copper wire having a diameter of about 0.031 inches in certain embodiments. Alternatively, any conventional conductive wire will suffice.

As shown in FIGS. 1 and 6, the antenna array of certain embodiments is made up of a plurality of subarrays, each subarray having its own signal summing waveguide 5 (see FIGS. 5-6). Each subarray is made up of four (4) similarly wound (either right-handed circularly polarized or left-handed circularly polarized) helical antenna elements 1 in certain embodiments. As is known in the art, the direction of polarization of each element 1 depends upon the direction of winding 15.

The antenna system includes twenty-four separate non-symmetrical subarrays in certain embodiments as shown in FIG. 6 in order to form the above described fan shaped beam(s), the twenty-four subarrays being made up of twelve right-handed circularly polarized subarrays and twelve left-handed circularly polarized subarrays interleaved with one another. Thus, subarrays R1, L1, R2, L2 . . . R12, and L12 are defined on the front or signal receiving surface of antenna element mounting plate 3 (subarrays R1, R2, etc. referring to right-handed subarrays and subarrays L1, L2, etc. referring to left-handed circularly polarized subarrays). It is noted that the number and symmetry of the subarrays may vary in accordance with the intended use of the system.

The provision of both right-handed and left-handed circularly polarized subarrays allows the phased array antenna system of certain embodiments of this invention to receive signals from satellites emitting either righthanded circularly polarized signals, left-handed circularly polarized signals, or linearly polarized (horizontal or vertical) signals as will be discussed below.

While FIG. 2 is a side cross-sectional view illustrating an antenna element 1 and its corresponding signal summing waveguide 5, FIG. 5 is a front or rear cross-sectional view illustrating a complete subarray having four antenna elements 1 associated with a single summing waveguide 5. As shown in FIG. 6, which is a top view of the array antenna, each subarray (i.e. R1, L1, R2, L2, . . . , R11, L11, R12, and L12) has its own signal summing waveguide 5 in which the electromagnetic signals received by each of the four elements 1 of a subarray are combined and output via subarray output probe 31 typically made of a conductive wire.

The subarray output probe 31 for each subarray (and each waveguide 5), extends from the waveguide 5 through an aperture in cover plate 33. Cover plate 33 seals the rear or lens side of the plurality of signal summing waveguides 5 of the different subarrays. The apertures in plate 33 through which probes 31 extend are filled with dielectric material 35 so as to insulate, support, and to impedance transform wire probes 31.

Cover plate 33 is made of a conductive metal in certain embodiments of this invention. Alternatively, plate 33 may be made of a plastic material with the surface adjacent waveguides 5 being coated with a conductive metal.

The signal summing waveguide 5 of each subarray may be lined with a conductive metal such as aluminum or nickel. In the FIG. 1 embodiment, waveguide 5 is milled out of a solid piece of aluminum which defines all walls of each waveguide 5 save the single wall of each waveguide 5 defined by cover plate 33. This milled aluminum member of the first embodiment also defines all of the conductive walls of the plurality of cup apertures 11.

Alternatively, portion 7 in the FIG. 2 embodiment may be made of an injected molded plastic with the walls of the cups defining apertures 11 and waveguides 5 being defined by deposited conductive metal.

With respect to the dimensions of waveguides 5, all waveguides 5 preferably have the same rectangular dimensions. For example, each waveguide 5 may be about 0.75 inches deep, about 0.40 inches wide, and about 5.55 inches long in certain embodiments of this invention.

Each element output probe 21 from the different antenna elements 1 is designed so that each probe 21 contributes, in part, to the overall electromagnetic field conditions which exist within the enclosed volume of each subarray waveguide 5. Thus, each element output probe 21 in the subarray contributes to the electromagnetic field condition which exists at output probe 31 in waveguide 5, there being only one output probe 31 for each waveguide 5 (and subarray). The net effect is that the accumulative effect of each element output probe 21 in a subarray contributes to a linear superposition of electromagnetic fields caused to exist within the spatial volume of the subarray waveguide 5. Therefore, the waveguide output signal via probe 31 is related in strength to the linear summation of the different input probe 21 signal strengths accompanied by a very small loss in strength due to ohmic and mismatched losses.

The waveguide output probe 31 of each subarray passes through cover plate 33 and is connected electrically to a low noise amplifier (LNA) circuit on printed circuit board (PCB) 37. The LNA circuit on PCB 37 is an active circuit and provides signal strength amplification for the summed signal of each subarray with very low quantities of noise or other unwanted spurious signals added to the amplified signal.

PCB 37 includes a plurality of low noise amplifiers (LNAs), each output probe 31 having its own LNA 39 on PCB 37. LNAs 39 have sufficient gain in order to overcome any losses following the LNA circuit (e.g. lens losses) and low enough noise figures to not affect the system noise temperature to any great extent.

As described above, the output from waveguides 5 is sent via output probes 31 to LNAs 39 on PCB 37 within LNA housing 41. LNA housing 41 is affixed to plate 33 and includes a walled portion 43 defining sidewalls of the housing and a cover 45. PCB 37 with LNAs 39 defined thereon is placed within the confines of housing 43 and is sealed therein by cover board or plate 45. LNAs 39 are illustrated electrically in more detail in FIG. 13.

The output 111 of each LNA 39 is sent via a conventional transmission line 51 to either electromagnetic lens 53 or 55. Lenses 53 and 55 are also known in the art as parallel plate Rotman lenses. Electromagnetic lens 53 receives the output from all LNAs 39 associated with right-handed circularly polarized subarrays (R1, R2, R3, . . . ) while electromagnetic lens 55 receives all outputs of low noise amplifiers 39 associated with left-handed circularly polarized subarrays (L1, L2, L3, . . . ). Lenses 53 and 55 are non-symmetrical in certain embodiments, this meaning that the beam port arc and the feed port arc are not identical (i.e. the lens curve(s) from which the LNA inputs are fed is not equivalent to the lens arc which is connected to satellite selection matrix block 69).

FIG. 7 is a rear or front elevational view of electromagnetic lens 53 (or 55), while FIG. 8 is an exploded cross-sectional view of lens 53 (or 55). Electromagnetic lens 53 includes conductive circuit element 57, a pair of conventional dielectric substrates 59, and a pair of conductive ground planes 61. Lenses 53 and 55 are substantially identical. Conductive circuit 57 of lens 53 (and circuit 57 of lens 55) is sandwiched between dielectrics 59 with the dielectric/conductive combination being disposed between opposing ground planes 61.

Each lens 53 and 55 includes a plurality of input connectors 63 for allowing conductive circuit element 57 to be electrically connected to the low noise amplifier 39 outputs via transmission lines 51. Input connectors 63 are affixed via screws or the like to the curved input side of each lens 53 and 55. Additionally, each lens 53 and 55 includes a plurality of output connectors 65 affixed on the other curved or arc-shaped periphery thereof so as to allow the output of the lenses to be connected via transmission lines 67 to satellite selection matrix output block 69.

Connectors 63 and 65 each include a conductive portion 66 electrically connected to conductive circuit element 57 of the lens so as to allow conductivity between inputs 63 and outputs 65. Any conventional connections may be made regarding connectors 63 and 65 as well as transmission lines 51 and 67. There are twelve inputs 63 and twelve outputs 65 on each lens 53 and 55 in the embodiments of this invention which utilized twenty-four subarrays. In other words, the number of lens inputs corresponds to the number of subarrays in certain embodiments, with the number of lens 53 input ports corresponding to the number of right-handed subarrays and the number of lens 55 input ports 63 corresponding to the number of left-handed subarrays. The number of lens output ports may vary in accordance with the intended use of the system. Of course, those of ordinary skill in the art will recognize that the number of inputs 63 and outputs 65 may vary in accordance with the intended use of the system.

The arc of lenses 53 and 55 on which ports 65 are disposed may have a substantially constant radius while the curve on which ports 63 are located may not in certain embodiments.

With respect to electromagnetic lens (53 and 55) loss, lens loss may be compensated for by LNA 39 gain in a limited manner since LNAs 39 precede lenses 53 and 55. Either air or other dielectrics may be utilized in lenses 53 and 55. With respect to lens dielectric materials, air, Teflon, and FR-4 are suitable in different embodiments.

A design parameter of electromagnetic lenses 53 and 55 (i.e. Rotman lenses) is the angular increment of beam scan. This angular increment is driven by the spacing between satellites of a constellation from an earth point of view and the beamwidth of the array radiation pattern in the scanning plane. Furthermore, in order to achieve maximum gain from each independent beam in the multiple beam antenna systems of this invention, adjacent beam cross-coupling should be eliminated or substantially reduced. Ports 63 and 65 may be designed so that the angular increment of beam scan of each lens is about 4.degree. in certain embodiments. This increment may, of course, change in accordance with the application of the system.

Lenses 53 and 55 are designed based at least in part upon the principles set forth in "Wide-Angle Microwave Lens for Line Source Applications" by Rotman and Turner (1962), the disclosure of which is incorporated herein by reference. The focal angle of each lens 53 and 55 is about 60 degrees and lens parameter "g" (see Rotman-Turner) is about 1 in certain embodiments of this invention.

By combining the use of lenses 53 and 55, the user may receive satellite signals from anywhere in the scanning range of either lens in any polarization sense. The scanning capability of the system is bounded by the capability of the lenses and the array. Electromagnetic or microwave lenses 53 and 55 are time-delay devices designed to scan on the basis of optical path lengths, their radiated or scanned beams being substantially fixed in space. Lenses 53 and 55 may also be termed as "constrained" lenses in certain embodiments in reference to the manner in which the electromagnetic energy passes through the lens face. Constrained lenses 53 and 55 include a plurality of radiators to collect energy at the lens "back face" and to re-radiate energy from the "front face." Within lenses 53 and 55, electromagnetic energy is constrained by transmissions lines thus allowing tailoring of scanning characteristics.

In accordance with the above described lens designs, lenses 53 and 55 in combination of the multiple beam antenna systems of this invention allow the systems to select a single beam or a group of beams for reception (i.e. home satellite television viewing). Due to the design of the antenna array and matrix block 69, right-handed circularly polarized satellite signals, left-handed circularly polarized satellite signals, and linearly polarized satellite signals within the scanned field of view may be accessed either individually or in groups. Thus, either a single or a plurality of such satellite signals may be simultaneously received and accessed (e.g. for viewing, etc.).

The multiple beam array is configured in a 4.times.12 fashion in the first embodiment of this invention, the number 4 representing the number of helical elements in a subarray and the number 12 representing the number of subarrays corresponding to a particular polarity (either right-handed or left-handed). The non-symmetrical aspect of such a 4.times.12 array necessitates the above described fan-shaped beam from the array which is narrow in one direction (i.e. the East-West direction) and wider in another direction (i.e. the North-South direction). The fan-shaped beam of the antenna at half-power beamwidth is about 3.degree. in the East-West direction and about 10.degree. in the North-South direction as a result of this non-symmetrical arrangement of subarrays in certain embodiments of this invention. While the 4.times.12 parameter of subarrays is used as an example, other configurations may also be utilized, the parameters being determined in accordance with the intended use of the system.

Beam forming may be accomplished in certain other embodiments by varying the amplitude and/or phase of elements of symmetrical or asymmetrical arrays.

FIG. 14 is a graph illustrating the theoretical directivity of the 4.times.12 phased array antenna of the first embodiment of this invention, and the directivity of a single tapered antenna element 1. Side lobes and grating lobe(s) are also illustrated. It is noted that elements 1 of the multi-beam array of certain embodiments of this invention are tapered or conical in shape so as to position the immediate side lobes at least about 20 dB down with respect to the main lobe.

The graph for the azimuth plane in FIG. 14 (and FIG. 15) is indicative of the fan-shaped beam in the East-West direction and the elevation plane is indicative of the North-South direction. As shown, the beam is at least about twice as wide in the elevation plane as in the azimuth plane in this embodiment. This is because as described above satellites are typically positioned in orbit along an arc defined in the azimuth plane. Therefore, the thin profile of the beam in the East-West direction (or in the satellite arc) allows reduced interference between satellites.

As shown in FIG. 14, the main lobe in the East-West (or azimuth plane) extends about 3.degree. from normal (0.degree.) at about 20 dB down while the main lobe in the elevation plane extends about 7.degree.-8.degree. from normal. Multiple side lobes are shown for both planes from about 4.degree.-35.degree. in the azimuth plane and from about 9.degree.-50.degree. in the elevation plane. Additionally, a grating lobe in the azimuth plane is shown beginning at about 51.degree. reaching a peak at the element pattern and ending at about 63.degree..

FIG. 15 illustrates computed array patterns from an actual measured element pattern, this figure illustrating the array antenna system having a directivity of about 30.45 dBi. This graph was based upon the measured characteristics of a particular element 1 which were input into a simulation program for simulating a 4.times.12 array design of the first embodiment. The main lobes and numerous side lobes are shown in both the elevation and azimuth planes and in addition a grating lobe is shown in the elevation plane starting at about 30.degree.. The element pattern derived in coming up with the graph of FIG. 15 was taken at a frequency of about 11.95 GHz. For the ideal pattern, grating lobes are suppressed if they are positioned just outside of the element pattern. It is noted that FIGS. 14 and 15 were derived using a 1.6.lambda. (or 1.6 inch) element spacing within subarrays (in the Y direction) and a 1.2.lambda. or 1.2 inch spacing in the X direction (adjacent subarrays).

Directivity is a function of the number of elements 1 employed and the area over which they are positioned. Larger directivities require larger element areas in general and typically more elements. However, for limited scan applications such as the first embodiment of this invention, the element lattice may be sparsely populated and still achieve a high level of directivity, with the tradeoff involving ensuring that no or substantially no grating lobes are formed at any steering angle of the array. Grating lobe formation reduces the array directivity in the pertinent direction as is known in the art.

Grating lobes exist in an array when more than one possible field pattern maximum exists. Grating lobes can be completely prevented by selecting an array element spacing of 0.5.lambda. or less. Alternatively, and as carried out in the first embodiment, grating lobes are suppressed by utilizing helical elements 1 in making up the array and subarrays wherein each element 1 has an element in such a case pattern which is relatively small or reduced in regions where the grating lobes exist. Accordingly, in such a pattern multiplication necessitates that the array grating lobes are reduced in intensity to the level of element sidelobes or lower and therefore do not adversely impact the array gain. Thus, each element 1 is designed so as to provide a null (or at least about a 20 dB reduction in relative radiation intensity) at the angular position corresponding to grating lobe position(s).

FIG. 9(a) is a schematic diagram of the multi-beam array antenna system of certain embodiments (e.g. the first embodiment) of this invention. As shown, the signal is received by either the right-handed or left-handed subarray elements 1, or both. Thereafter, the signals received by elements 1 in a particular subarray are summed in a waveguide 5, the combined signals of each subarray then being sent to a low noise amplifier 39. After amplification, the signals from the left-handed subarrays are sent to lens 55 while the signals from the right-handed subarrays are sent to lens 53. Satellite selection matrix output block 69 then allows the user to select from which satellite(s) he wishes to receive signals.

Output block 69 accommodates the location of the user and the constellation of the satellites of interest to user. Because satellite spacing of a given constellation is different in different regions or viewing angles, block 69 may be adjusted so as to allow the user to view certain satellite(s), the adjustment of block 69 being a function of the region and constellation of satellites of interest in which the system is to be located.

FIG. 9(b) illustrates the case where the user manipulates satellite selection matrix output block 69 to simply pick up the signal from a particular satellite which is transmitting a right-handed circularly polarized signal. In such a case, the path length in lens 53 is adjusted so as to tap into the signal of the desired satellite. In FIG. 9(b), no left-handed circularly polarized signals or linear signals from other satellites are received in output block 69.

FIG. 9(c) illustrates the case where a plurality of received outputs from lens 55 (left-handed circularly polarized) are summed or combined in amplitude and phase. Summing adjacent ports of lens 55 (or 53) splits the steps size of the lens. The signals from two adjacent outputs 65 are combined at summer 71 so as to split the beams from the adjacent output ports 65. Thus, if the viewer wishes to view a satellite disposed angularly between adjacent output ports 65, output block 69 takes the output from the adjacent ports 65 and sums them at summer 71 thereby "splitting" the beam and receiving the desired satellite signal. It is noted that a small loss of power may occur when signals from adjacent ports 65 are summed in this manner.

For example, when the granularity of the array is 4.degree. apart, the step size of lenses 53 and 55 could be designed conveniently to be about 4.degree. in certain embodiments. When two satellites are spaced 6.degree. apart, the signal from one satellite may be received via one port 65. However, the signal from the second satellite is received by summing adjacent ports 65 so as to split their beam and obtain a signal disposed in the middle thereof.

FIG. 9(d) illustrates the case where outputs 65 from both lenses 53 and 55 are tapped so as to result in the receiving of a signal from a satellite having linear polarization. Output from port 65 from right-handed lens 53 is adjusted in phase at phase shifter 73 and thereafter combined with the signal from lens 55 at summer 71. Thus, the output from matrix output block 69 is indicative of the linearly polarized signal received from a particular satellite, the position of the satellite being determined by the ports of lenses 53 and 55 tapped and thus the lens path lengths.

FIG. 9(e) illustrates the case where it is desired to access a satellite disposed between the beams of adjacent ports 65 wherein the satellite emits a signal having linear polarization. Adjacent ports 65 are accessed in each of lenses 53 and 55 and are summed accordingly at summers 75. Thereafter, phase shifter 73 adjusts the phase of the signal from lens 53 and the signals from lenses 53 and 55 are combined at summer 71 thereafter outputting a signal from output block 69 indicative of the received linearly polarized signal.

Thus, the provision of electromagnetic lenses 53 and 55 allows the user to use the same array antenna elements 1 making up the overall array to view beams from different satellites. Additionally, lenses 53 and 55 allow the user to use the same elements 1 to simultaneously view plural beams from different satellites with substantially no reduction in power. In other words, matrix output block 69 and lenses 53 and 55 allow a user or consumer to tap into signals from a plurality of satellites simultaneously, the different signals received being of the right-handed circularly polarized-type, left-handed circularly polarized-type, linearly polarized-type, or different combinations thereof.

Therefore, the design of the multi-beam array antenna system of certain embodiments of this invention allows the user to, for example, simultaneously view signals from satellites A and B, where satellite A outputs a right-handed circularly polarized signal and satellite B outputs a left-handed circularly polarized signal. Matrix output block 69 may simultaneously access the two signals via lenses 53 and 55 and output the two signals over different paths to the user or consumer.

Alternatively, the user may simultaneously receive signals from satellites C and D where satellite C emits a linearly polarized signal and satellite D emits a right-handed circularly polarized signal. The reception of such signals simultaneously is carried out as described above with output block 69 accessing appropriate outputs or ports 65 from lenses 53 and 55 in accordance with the particular satellites to which viewing is desirable.

The multiple electromagnetic lenses utilized provide the necessary wave propagation control to vary the spacial position of the array apertures multiple directions of sensitivity. While two such lenses 53 and 55 are utilized in the above-described embodiments, more such lenses may be added in accordance with the intended use of the system. In such a case, output block 69 still acts to select the specific spacial and polarization characteristics of signals that will be transferred from the lenses to the receiver/user.

FIGS. 10-12 illustrate different views of satellite selection block 69. FIG. 10 is a top view illustrating inputs 75 which allow the switching matrix within block 69 to control and access the output ports of lenses 53 and 55. Outputs 77 are also shown, these outputs allowing the user to tap into desired satellite signals.

FIG. 13 is a circuit diagram of printed circuit board 37 and the multiplicity of low noise amplifiers 39 (LNA) thereon. Printed circuit board 37 may be manufactured by either Rodgers, Arlon, or Taconics Corp. and may have the following characteristics in certain embodiments: 0.020 inches thick; both sides copper clad with 1/2 oz. copper; and PTEE E.sub.r 2.2.

Each LNA 39 receives an input 81 from the waveguide 5 of a particular subarray (either right-handed or left-handed). One such LNA in FIG. 13 is enlarged so as to show different circuit elements thereof, each LNA 39 being substantially similar to the enlarged LNA illustrated.

Each LNA 39 is driven from power supply 83 which is a 14-24 volt DC source in certain embodiments. The LNA assembly and power regulation thereof includes 12 volt regulator 85 and 0.3 .mu.F capacitors 87. Each LNA 39 includes 0.1 .mu.F capacitor 89, 1,000 ohm (and one-eighth watt) resistor 91, 100 pF capacitor 93, one-quarter wave open stub 95 having an impedance of about 30 ohms, output matching network 97, one-quarter wave grounded or closed stub 99 having an impedance of about 200 ohms, noise matching system 101, high electron mobility transistor (HEMT) 103, one-quarter wave open stub 105 having an impedance of about 30 ohms, 100 pF capacitor 107, 25 ohm (and one-eighth watt) resistor 109, and output 111 which leads to one of electromagnetic lenses 53 and 55. Trace 98 is a quarter wave trace having an impedance of about 200.OMEGA.. HEMT 103 may be NEC Part No. 42484A; NEC Part No. 76083 (GaAs FET); or conventional Mitsubishi or Fujitsu HEMTS in certain embodiments.

The above-described LNA parameters are illustrative of one embodiment of this invention. It will be recognized by those of skill in the art that the parameters and sometimes the design of LNAs 39 may be varied in certain other embodiments.

Alternatively, instead of the illustrated single stage LNA, a double-stage LNA may instead be used so as to increase the carrier to noise ratio and help the G/T.

An advantage of the array antenna systems of the different embodiments of this invention is their modular characteristics. While the antenna array of the FIG. 1 embodiment includes twenty-four separate subarrays, additional subarrays may be stacked on top of (or adjacent to in certain embodiments) the existing subarrays of the FIG. 1 embodiment so as to increase signal strength. The signals output from the newly added subarrays are combined with existing subarray signals prior to the LNA input so as to save cost. Thus, the gain of the antenna may be significantly increased (e.g. doubled) simply by stacking additional subarrays on top of the existing subarrays without significantly increasing the cost of the system. The modular advantages of the system are particularly useful in regions requiring access to direct broadcast television satellites. Such satellites exhibit different signal strengths in different regions. Therefore, the need for increased gain is present in regions experiencing low strength signals from the satellites. Accordingly, in such regions in need of increased gain, additional subarrays may be stacked upon the existing ones so as to satisfy such customers.

In a typical operation of the multiple beam array antenna system of the first embodiment of this invention, travelling electromagnetic waves (e.g. from satellites) are incident upon windings 15 of antenna elements 1 making up the different subarrays of the array antenna. Additionally, the travelling electromagnetic waves are incident on conducting ground plane 9 and cup apertures 11. These waves cause electrical signal currents to be passed through windings 15 on mandrel 13 and via wires 19 (one per mandrel) to element output probes 21.

Elements 1 of right-handed subarrays (R1, R2, R3, . . .) receive right-handed circularly polarized waves from satellites while elements 1 of left-handed subarrays (L1, L2, L3, . . .) receive left-handed circularly polarized signals along with linearly polarized signals. The signals from these waves proceed as described above to probe outputs 21 disposed within subarray waveguides 5.

In waveguides 5, the electromagnetic waves from the plurality of elements 1 making up each subarray are combined or summed in a subarray waveguide 5 thus forming a summed electromagnetic wave bounded by the waveguide conductive walls. The bounded electromagnetic wave within each waveguide 5 exists in spacial close proximity to waveguide output probe 31 thus causing the combined signal currents to flow through probe 31 to a corresponding low noise amplifier 39 disposed on circuit board 37. The output from each waveguide 5 is sent to a different LNA 39.

The summed signal output from each subarray waveguide 5 proceeds to its own LNA input 81 and is thereafter amplified by the amplifier. The output of each LNA proceeds to a corresponding electromagnetic lens input 63. The combined signals from the right-handed circularly polarized subarrays (and their LNAs) proceed to electromagnetic lens 53 while the signals from the left-handed circularly polarized subarrays (and their LNAs) go to electromagnetic lens 55. Lenses 53 and 55 are substantially identical in design.

Now, let us assume that the user wishes to receive a television signal from a single satellite in orbit, this satellite transmitting right-handed circularly polarized signals. In such a case, the user manipulates satellite selection matrix output block 69 so as to access the signals of only this particular satellite. When matrix output block 69 receives such instructions, it accesses the particular output(s) 65 on right-handed lens 53 so as to "tap into" the signal of this particular satellite. Thus, only the signal from this particular right-handed satellite is presented to the viewer via block 69 for viewing.

Let us now assume that the user wishes to simultaneously access signals from two different satellites in orbit, the first satellite "A" transmitting linearly polarized waves and the second satellite "B" transmitting left-handed circularly polarized waves. In such a case, the user manipulates output block 69 so as to tap into the signals of both satellites "A" and "B" simultaneously via lenses 53 and 55. The matrix within output block 69 in order to allow the user to tap into the linearly polarized satellite signals from satellite "A" accesses corresponding outputs 65 from both lenses 53 and 55 as shown in FIG. 9(d). Thereafter, the signal from lens 53 (or alternatively lens 55) is phase shifted at shifter 73 with the phase shifted signal and the ordinary signal from lens 55 being combined at summer 71 so as to form the output in accordance with satellite "A". Simultaneously, a different output port 65 from lens 55 is accessed via the matrix within block 69 so as to tap into the received left-handed polarized signal of satellite "B". Both signals may simultaneously be output from block 69 so that the user may utilize both signals at the same time. If both satellites "A" and "B" are of the television transmitting type, then the user is able to view two different programs simultaneously, one from satellite "A" and one from satellite "B". In other circumstances, when, for example, satellite "B" is outputting music signals, the user is able to simultaneously access the television signal from satellite "A" and the music signal (or other data signal) from satellite "B".

In yet another embodiment of this invention horizontal and vertical linearly polarized antenna elements are utilized and manipulated (instead of the right and left-handed circularly polarized elements of the previous embodiments) for receiving each of the right-handed circularly polarized signals, left-handed circularly polarized signals, and linearly (horizontal and vertical) polarized signals.

The above-described and illustrated elements of the various embodiments of this invention are manufactured and connected to one another by conventional methods commonly used throughout the art unless otherwise specified.

Once given the above disclosure, therefore, various other modifications, features or improvements will become apparent to the skilled artisan. Such other features, modifications, and improvements are thus considered a part of this invention, the scope of which is to be determined by the following claims.

Claims

We claim:

1. A multiple beam array antenna system for receiving electromagnetic polarized signals from different satellites, said system comprising: first and second subarrays of circularly polarized helical antenna elements, said first subarray of antenna elements being right-handed circularly polarized and said second subarray of antenna elements being left-handed circularly polarized; first and second signal summing waveguides, the received electromagnetic signals from said first subarray being summed in said first waveguide and the received electromagnetic signals from said second subarray being summed in said second waveguide; first and second low noise amplifiers, the summed signal from said first subarray and said first waveguide being amplified by said first amplifier and the summed signal from said second subarray and said second waveguide being amplified by said second amplifier; first and second electromagnetic lenses for allowing multiple signals to be received by said multiple beam array antenna system, said summed right-handed circularly polarized signal amplified by said first amplifier being sent to said first electromagnetic lens and said summed left-handed circularly polarized signal amplified by said second amplifier being sent to said second electromagnetic lens whereby said first lens acts upon received right-handed circularly polarized signals and said second lens acts upon received left-handed circularly polarized signals so that said system can receive both right and left handed circularly polarized signals and thereafter output their content.

2. The antenna system of claim 1, wherein said first subarray includes at least four right-handed helical antenna elements and said second subarray includes at least four left-handed helical antenna elements and wherein each of said first and second subarrays are non-symmetrical so as to radiate or receive fan-shaped beams, and said first and second subarrays operate at substantially equal frequencies.

3. The antenna system of claim 2, wherein each of said antenna elements of said first and second subarrays includes a tapered dielectric mandrel with a conductive winding wound around its outer periphery in a helical manner, and wherein each of said antenna elements of said first and second subarrays is mounted on a mounting plate within a conductive cup aperture.

4. The antenna system of claim 3, wherein each of said mandrels includes an impedance matching extension portion protruding from its base for insertion into one of a plurality of mounting apertures defined within said mounting plate, and wherein a conductive member extends from said conductive winding on the mandrel outer periphery through said extension portion and said mounting aperture and into or adjacent the waveguide for the subarray so as to allow the received signals to make their way from said conductive winding into said waveguide.

5. The antenna system of claim 3, wherein said antenna elements of said first subarray are spaced apart from about 0.5.lambda. to 2.0.lambda. and said antenna elements of said second subarray are also spaced apart from about 0.5.lambda. to about 2.0.lambda., and wherein said first subarray antenna elements are spaced from said second subarray antenna elements by about 0.5.lambda. to 2.0.lambda..

6. The antenna system of claim 1, wherein said antenna elements making up said firsthand second subarrays are designed to receive satellite television signals from about 10.7-13 GHz, and wherein said system can simultaneously receive two of: (i) right-handed circularly polarized signals; (ii) left-handed circularly polarized signals; and (iii) linearly polarized signals.

7. The antenna system of claim 6, wherein said system scans a fan-shaped beam extending from about 2.degree.-5.degree. in the East-West direction and from about 5.degree.-10.degree. in the North-South direction, and wherein the array of antenna elements has a directivity of from about 29-32 dBi.

8. An array antenna receiving system comprising: a first group of right-handed circularly polarized subarrays, each such subarray having a plurality of right-handed circularly polarized helical antenna elements; a second group of left-handed circularly polarized subarrays, each such left-handed subarray having a plurality of left-handed circularly polarized helical antenna elements; wherein said subarrays of said first and second groups are arranged in an interleaved or alternating fashion and receive substantially the same frequencies; a first electromagnetic lens for receiving signals from said first group of subarrays and a second electromagnetic lens for receiving signals from said second group of subarrays; and means for manipulating said first and second electromagnetic lenses so as to enable said system to receive right-handed circularly polarized signals, left-handed circularly polarized signals, and linearly polarized signals within the scanning field of the system.

9. The system of claim 8, further including means for simultaneously receiving both circularly polarized signals and linearly polarized signals and outputting said simultaneously received signals to a user.

Patent Citations (32)

Patent	Date	Inventor
US2847672	1958-08-01	Giffin et al.
US2863148	1958-12-01	Gammon et al.
US2953781	1960-09-01	Donnellan et al.
US2977594	1961-03-01	Marston et al.
US2982959	1961-05-01	Hanneken
US3017633	1962-01-01	Marston et al.
US3135960	1964-06-01	Kaiser, Jr.
US3170158	1965-02-01	Rotman
US3509572	1970-04-01	Barbano
US3623118	1971-11-01	Monser et al.
US3718932	1973-02-01	Ikrath et al.
US4123759	1978-10-01	Hines et al.
US4315266	1982-02-01	Ellis, Jr.
US4400703	1983-08-01	Shiokawa et al.
US4427984	1984-01-01	Anderson
US4494117	1985-01-01	Coleman
US4680591	1987-07-01	Axford et al.
US4785302	1988-11-01	Ma et al.
US4791428	1988-12-01	Anderson
US4845507	1989-07-01	Archer et al.
US5041842	1991-08-01	Blaese
US5053786	1991-10-01	Silverman et al.
US5061943	1991-10-01	Rammos
US5117240	1992-05-01	Anderson et al.
US5146234	1992-09-01	Lalezari
US5227807	1993-07-01	Bohlman et al.
US5243358	1993-09-01	Sanford et al.
US5255004	1993-10-01	Berkowitz et al.
US5258771	1993-11-01	Praba
US5345248	1994-09-01	Hwang et al.
JPX56-141602	1981-11-01
JPX58-187003	1983-11-01

Non-Patent Literature (17)

Broadband Quasi-Taper Helical Antennas by J. L. Wong and H. E. King, IEEE, Jan. 1979, pp. 72-78.
Grating Lobe Control in Limited Scan Arrays by Mailloux et al, IEEE, Jan. 1979, pp. 79-85.
Short Helical Antenna Array Fed from a Waveguide by Nakano et al, IEEE, Aug. 1984, pp. 836-840.
Radiation from a Sheath Helix Excited by a Circular Waveguide: A Wiener-Hopf Analysis by Fernandes et al, Oct. 1990.
Low-Profile Helical Array Antenna Fed from a Radial Waveguide by Nakano, et al, IEEE, Mar. 1992, pp. 279-282.
Wave Propagation on Helical Antennas by Cha, IEEE, Sep. 1972, pp. 557-560.
A Study of the Sheath Helix with a Conducting Core and its Application to the Helical Antenna, by Neureuther, IEEE Mar. 1967, pp. 204-209.
Wave Propagation on Helices by Mittra, IEEE, Sep. 1963, pp. 585-586.
Review of Radio Frequency Beam Forming Techniques for Scanned and Multiple Beam Antennas by Hall, IEEE Oct. 1990, pp. 293-304.
Design Trades for Rotman Lenses by Hansen, IEEE Apr. 1991, pp. 464-472.
Design of Compact Low-Loss Rotman Lenses by Rogers, IEEE, Oct. 1987, pp. 448-456.
Focusing Characteristics of Symmetrically Configured Bootlace Lenses by Shelton, IEEE, Jul. 1978.
Design Considerations for Ruze and Rotman Lenses by Smith, The Radio and Electronic Engineer vol. 52, No. 4, pp. 181-187, Apr. 1982.
Amplitude Performance of Ruze and Rotman Lenses by Smith et al, The Radio and Electronic Engineer, vol. 53, No. 9, pp. 329-337, Sep. 1983.
Microstrip Port Design and Sidewall Absorption for Printed Rotman Lenses by Musa et al, IEEE, Feb. 1989, pp. 53-58.
Wide-Angle Microwave Lens for Line Source Applications by Rotman et al, IEEE, Nov. 1962, pp. 623-632.
Short Helical Antenna Array Fed from a Waveguide by Nakano et al, IEEE, Nov. 1983, pp. 405-408.

Abstract

Description