The present invention relates, in general, to an antenna and, more specifically, to a phased array antenna including multiple radiating elements arranged in a cloverleaf pattern. The phased array operates over multi-octave bandwidths, subtends a wide field-of-view, and responds to any desired polarization in space. The phased array is amenable to conformal installation and may transmit at high peak and high average power.
Significant advances in broadband solid-state power generation have placed a new emphasis on phased arrays to efficiently combine the power of individual devices into high-power transmissions by exploiting the magnification property of phased arrays, known as the “array factor”. Commensurate with this trend, the demands for high transmitted effective radiated power (ERP) have increased by as much as an order of magnitude. In addition, operating frequency range has been lowered into the HF/VHF region.
Along with the high effective radiated power, the multi-functional performance characteristics associated with phased arrays, such as multi-octave bandwidths, wide field-of-view, instantaneous multiple beams and polarization agility, must also be maintained.
Within the context of these requirements, emphasis must now be given to issues related to power handling within the array aperture, as well as the entire corporate feed structure. Power handling encompasses not only the capacity to sustain peak and average (CW) power demands, but also to be able to operate in adverse temperatures on the phased array.
The present application is related to U.S. Pat. No. 6,992,632 issued to Mohuchy on Jan. 31, 2006, entitled “Low Profile Polarization-Diverse Herringbone Phased Array”, and U.S. Pat. No. 6,853,351 entitled “Compact High-Power Reflective-Cavity Backed Spiral Antenna”, issued to Mohuchy on Feb. 8, 2005. The entire contents of both patents are incorporated herein by reference.
To meet this and other needs, and in view of its purposes, the present invention provides a phased array antenna including a substrate, and multiple radiating elements conformally mounted as micro-strips on the substrate. Each of the radiating elements is of a triangular shape, and four of the radiating elements are arranged to form a crossed bowtie cloverleaf radiator.
The four radiating elements form two pairs of radiating elements, and the two pairs of radiating elements are orthogonal to each other. Moreover, the radiating elements are disposed on a front surface of the substrate, and a RF center conductor is orthogonally oriented toward a rear surface of the substrate and connected to each of the radiating elements for feeding a RF signal to the radiating element.
The phased array antenna has the radiating elements disposed on a front surface of the substrate. A metallic ground layer is disposed facing a rear surface of the substrate, and a fluted core layer is sandwiched between the metallic ground layer and the substrate for channeled passage of coolant.
Each of the triangular shaped radiating elements includes a launch point disposed adjacent a vertex formed by two equal sides of an isosceles triangle. A pair of triangular shaped radiating elements are arranged to have the launch point of one of the radiating elements to be adjacent to the launch point of the other radiating element to form a first bowtie configuration. Another pair of triangular shaped radiating elements are arranged to have the launch point of one of the radiating elements of the other pair to be adjacent to the launch point of the other radiating element of the other pair to form a second bowtie configuration. The first bowtie configuration is arranged to be orthogonal to the second bowtie configuration.
A scan axis is included for the phased array antenna. A line may be formed extending from the vertex and intersecting a midpoint of a base of the isosceles triangle. This line forms a 45 degree angle with respect to the scan axis.
The phased array antenna includes a RF center conductor orthogonally oriented to one of the radiating elements for feeding a RF signal to the one radiating element. The RF center conductor includes a coaxial center conductor at one end, remote from the one radiating element, and a thinned center conductor at the other end, adjacent to the one radiating element. The RF center conductor also includes a wide center conductor extending between the thinned center conductor and the coaxial center conductor. The thinned center conductor has a diameter that is smaller than the wide center conductor. The thinned center conductor is connected to a launch point of the one radiating element with a screw inserted into a threaded receptacle of the thinned center conductor. Additionally, the wide center conductor includes an axial core for receiving the coaxial center conductor, and the coaxial center conductor is positively connected to the wide center conductor by way of a set screw inserted radially into the axial core for contacting the coaxial center conductor. The coaxial center conductor passes transversely through a metallic ground layer. The wide center conductor and the thinned center conductor are a single RF conductor, which passes transversely through a fluted core layer sandwiched between the metallic ground layer and the substrate.
Another embodiment of the present invention is a phased array antenna having a substrate, and multiple crossed bowtie cloverleaf radiators conformally mounted as micro-strips on the substrate. Each crossed bowtie cloverleaf radiator is shaped as identical first and second bowtie configurations, and the first and second bowtie configurations are oriented orthogonally to each other. Each of the first and second bowtie configurations includes two radiating elements. Each radiating element has a shape of an isosceles triangle, with a launch point disposed adjacent to a vertex opposite to a base of the isosceles triangle, and the respective launch points of the two radiating elements oriented proximate to each other, and the respective bases oriented remote from each other.
In addition, four RF center conductors are orthogonally oriented to one of the crossed bowtie cloverleaf radiators. Two of the four RF center conductors are connected to the first bowtie configuration, and the other two of the four RF center conductors are connected to the second bowtie configuration. A plurality of sets of four RF center conductors are orthogonally oriented to the multiple crossed bowtie cloverleaf radiators. Two of a set of four RF center conductors are connected to a respective first bowtie configuration, and the other two of the set of four RF center conductors are connected to a respective second bowtie configuration.
Still another embodiment of the present invention is a phased array antenna including multiple crossed bowtie cloverleaf radiators mounted on a first dielectric layer. Cooling channels are disposed within a second dielectric layer, and a metallic ground is formed on a third layer. The first, second and third layers are disposed in a sequence of first, second and third layers, and each of the crossed bowtie cloverleaf radiators includes a set of four radiating elements arranged in a cross-configuration. This phased array antenna includes multiple RF center conductors, where each of the RF center conductors is coupled to a respective one of the four radiating elements in the set.
It is understood that the foregoing general description and the following detailed description are exemplary, but are not restrictive, of the invention.
The invention is best understood from the following detailed description when read in conjunction with the accompanying drawing. Included in the drawing are the following figures:
Referring to
λ/s=1+sin θ
where:
The orthogonal pairs of radiating elements 8 are positioned at 45 degrees relative to a scan axis of the phased array antenna, generally designated as 5. Although the scan axis is shown oriented along the X-axis, it will be appreciated that the scan axis may be oriented along the Y-axis, or any other angular orientation. The scan axis, for example, may also be of a conical scan orientation.
The substrate 11 is mounted on a fluted core layer of dielectric material, designated as core 9. The layer of core 9 is supported by a reflective, metallic ground plane, designated as 10. For discussion purposes,
The cloverleaf structure is shown in more detail in
Coaxial conductors 21A and 22A each forms one end of RF center conductors 21 and 22; wide center conductors 21B and 22B each forms a central portion of RF center conductors 21 and 22; and thinned center conductors 21C and 22C each forms the other end of RF center conductors 21 and 22. It will be understood that the coaxial conductor of the coaxial portion, the wide center conductor and the thinned center conductor form one continuous RF conduction path for coupling the RF signal from the input side to the output side of the radiating elements.
The RF signal is received via the four RF center conductors 21, 22, 23 and 24 (only RF center conductors 21 and 22 are visible in
The four RF center conductors 21, 22, 23 and 24 extend sequentially through metallic ground plane 10, fluted core 9 and substrate 11, as shown in
As best shown in
The multiple radiating elements 8 are chemically etched on copper clad dielectric material, which forms substrate layer 11, in the manner depicted in
It will be appreciated that a portion of fluted core 9 is removed in the area of the four RF center conductors 21, 22, 23 and 24 to preclude contact with the core material and permit convective cooling. The core material is removed in area 40 of
The RF center conductor, as shown in
The four RF center conductors for a given crossed bowtie cloverleaf radiator are arranged as a balanced twin-lead transmission line pair. Each RF center conductor has a varying cross-sectional diameter along its length, so that it is thinner at its output end adjacent each radiating element 8. This thinning of the RF center conductor advantageously allows matching the excitation ports of the bowtie radiators with respect to a driving point impedance desired to achieve minimum signal reflection. The socket set screw 51 caps thinned center conductor 21C, 22C, 23C, 24C for a positive connection to a bowtie radiator input.
The fluted core 9 in
A proof-of-concept phased array antenna, as embodied in the above described figures, was fabricated and measured in the 670-2000 MHz frequency band. The baseline for the phased array radiating aperture was determined using the general guidelines for biconical antennas, as outlined in Kraus, “Antennas”, Second Edition, published by McGraw-Hill Book Co, 1988, chapter 8. Chapter 8 is incorporated herein by reference in its entirety. The initial dimensions were then optimized using a three-dimensional method-of-moments (MOM) tool that allowed construction of an array of crossed bowtie cloverleaf radiators. The resulting radiation patterns and driving port impedances, taking into consideration mutual impedance contributions, were computed.
The element dimensions were specifically optimized for a maximum operating bandwidth over a 120 degree field-of-view. The main tradeoff parameters, as shown in
From a network point of view, the length L behaves as an inductive component, while the width W and the adjacent element gap G represent capacitance. The combined effect is a tank circuit which may be optimized for maximum operating bandwidth.
It will be appreciated that this optimization must include the entire field-of-view, because mutual coupling between adjacent elements varies significantly with the scan angle. A practical solution may be to focus on all scanned angles up to +/−45 degrees. Beyond the 45 degree scan coverage may be provided by pattern beam broadening effects.
A good indicator of array performance is the array VSWR (Voltage Standing Wave Ratio) for both the input to the array from the RF feed and the return loss seen by an incoming plane wave into the array. The desired figure of merit for both conditions is to operate a broadband array with a VSWR under 2:1. Practice, however, allows operating the array up to a 3:1 ratio, without significantly degrading the overall array operating efficiency.
ρ=(σ−1)/(σ+1)
where: ρ is Return Loss in voltage ratio
The aperture dimensions derived from the optimization are:
The center to center element spacing in both the Azimuth and Elevation directions is 2.307 inches.
The center RF conductors, shown in
The calculated impedance at the feed points of the bowtie (or pair of radiating elements 8) is 160 ohms. The RF coaxial connectors 60, when used as a pair, effectively represent 100 ohms. The resultant impedance then becomes 126 ohms, which corresponds to a wide center conductor (21B, for example) having a diameter of 0.34 inches. The center RF conductor (21, for example) is stepped down to 0.22 inch diameter forming the thinned center conductor (21C, for example) for approximately one fourth of the total length of center conductor 21. This dimension corresponds to the diameter of set screw 51 used to couple the bowtie input to the respective center RF conductor as a means of eliminating any possibility of RF corona between the set screw and the center RF conductor.
The fluted core shown in
Sample array patterns shown in
The sample radiation patterns in
Having described an embodiment of this invention, it is evident that other embodiments incorporating these concepts may be used. For example, frequency scaling of the dimensions may be used to operate in other frequency bands. The types of fasteners, connectors or dielectrics may be varied, with the appropriate electrical compensation. The array may be a planar or a conformally shaped structure deployed to any aspect ratio commensurate with the spatial coverage required.
Accordingly, although the invention has been described with a certain degree of particularity, it is understood that the present description is made only by way of example and that numerous changes in the details of construction, combination and arrangement of parts may be made without departing from the spirit and the scope of the invention.
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