This invention relates in general to tapered slot antennas and, more particularly, to a method and apparatus for obtaining wideband performance in a tapered slot antenna.
During recent years, there has been an increase in the use of antennas that include an array of antenna elements, one example of which is a phased array antenna. Antennas of this type have many applications in commercial and defense markets, such as communication and radar systems. In many of these applications, broadband performance is desirable. In this regard, some of these antennas are designed so that they can be switched between two or more discrete frequency bands. Thus, at any given time, the antenna is operating in only one of these multiple bands. However, in order to achieve true broadband operation, an antenna needs to be capable of satisfactory operation in a single wide frequency band, without the need to switch between two or more discrete frequency bands.
One type of antenna element that has been found to work well in an array antenna is commonly referred to as a tapered slot antenna element. The spacing between antenna elements in an array antenna is inversely proportional to the frequency at which the antenna operates, and a tapered slot antenna element fits comfortably within the space available for antenna elements in many array antennas, including those which operate at high frequencies.
Tapered slot antenna elements typically have a bandwidth of about 3:1 or 4:1, although some very recent designs have achieved a maximum bandwidth of about 10:1, or in other words one decade. While these existing tapered slot antenna elements have been generally adequate for their intended purposes, they have not been satisfactory in all respects. In this regard, there are applications in which it is desirable for a tapered slot antenna element to provide good performance across a bandwidth in the range of approximately two to four decades, or even more. Existing designs and design techniques have not been able to provide a tapered slot antenna element which approaches this desired level of broadband performance.
From the foregoing, it may be appreciated that a need has arisen for a method and apparatus that contribute to a greater bandwidth than is currently available in pre-existing antenna elements. One form of the present invention relates to an apparatus which includes a slot section having electrically conductive material that defines a slot with first and second ends, an electrically conductive element extending generally transversely to the slot in the region of the first end thereof, and a balun portion communicating with the first end of the slot. The method and apparatus involve: configuring the balun portion to have a high impedance; and absorbing a selected degree of electromagnetic energy in the balun portion.
A better understanding of the present invention will be realized from the detailed description which follows, taken in conjunction with the accompanying drawings, in which:
Two filler layers 16 and 17 are provided above the ground plane layer 12, and are made from a material having a low dielectric constant. In the disclosed embodiment, the layers 16 and 17 are made from a foam which can be obtained commercially under the trademark AIREX from Baltek Corporation of Northvale, N.J., as catalog number R82. However, it would alternatively be possible to use any other suitable material. In the embodiment of
A layer or sheet 18 of a resistive material is provided between the foam layers 16 and 17, and is oriented parallel to the ground plane layer 12. In the disclosed embodiment, the resistive sheet 18 has a resistance of approximately 360 ohms per square, and provides a selected degree of absorption of electromagnetic energy, as discussed later. A suitable material for the sheet 18 can be obtained commercially from SV Microwave, Inc., of West Palm Beach, Fla., in the form of a resistance coated metal film on 2 mil Kapton. It would alternatively be possible to use any other suitable material that provides an appropriate degree of absorption of electromagnetic energy.
In the embodiment of
The array antenna 10 has a plurality of cylindrical openings extending vertically through the foam layers 16-17 and the resistive sheet 18, and three of these openings are visible at 21, 22 and 23 in
The array antenna 10 has, above the foam layer 17, a plurality of electrically conductive flare elements, three of which are designated by reference numerals 31, 32 and 33. In the embodiment of
In a top view, each flare element has the shape of a regular cross, with four identical legs. As evident from
Each of the slots in the array antenna 10 have a vertical center line, for example as indicated diagrammatically at 51-53 in
The cables 71 and 72 have respective center conductors 81 and 82, which are concentrically surrounded by respective sleeves 83 and 84 made of an insulating material. In the disclosed embodiment, the conductive metal material of each post and flare element serves as an outer shield for the coaxial cables. However, it would alternatively be possible to provide a separate outer shield, and an additional layer of insulation could be provided around the outer shield.
At the upper and outer end of each of the cables 71 and 72, the center conductor 81 or 82 has an end portion which extends horizontally across the lower end of a respective slot, closely adjacent the top surface of the foam layer 17. The tip of the outer end of each such center conductor is received within an opening in another flare element. For example, the cable 71 extends upwardly through the post 28 and then horizontally through the groove 76 in the flare element 31, and the tip of its center conductor 81 is received in an opening in the flare element 32. In the disclosed embodiment, the tip of each center conductor is secured in the associated opening of a flare element by solder, so as to electrically couple the flare element to the tip of the center conductor. The center conductor is the only portion of each cable which extends across one of the slots and into an opening in a flare element.
With reference to
A not-illustrated circuit of a known type is coupled to the lower end of the coaxial cable 71, and the cable 71 is matched in impedance to this circuit, so as to provide a substantially uniform impedance of approximately 50 ohms from the circuit through the cable 71 to the lower end of the slot 41. The slot 41 effects an impedance transformation from a value of approximately 50 ohms at its lower end (which is matched to the impedance of the cable 71), to a value of approximately 377 ohms at the upper end (which is effectively matched to the impedance of free space).
The balun 93 is configured to provide a relatively high impedance of at least several hundred ohms, which represents a relatively large discontinuity in relation to the 50 ohm impedance at the lower end of the slot 41. As noted above, electromagnetic fields generated by the center conductor 81 within the slot 41 will tend to want to split and travel both upwardly and downwardly within the slot 41. However, the large impedance discontinuity at the junction of the balun 93 and the lower end of the slot 41 will cause the majority of this electromagnetic energy to travel upwardly rather than downwardly within the slot 41, and to thus be transmitted upwardly through the slot and then into free space from the upper end of the slot.
In pre-existing systems, balun configurations were specifically designed with the intent of taking the energy received in a slot antenna element, and transmitting as much of this energy as possible through the slot and into free space. This was considered logical in order to maximize the efficiency of the antenna element. However, a feature of the present invention is the recognition that this also tended to limit the bandwidth of the antenna element, for example to a maximum bandwidth of approximately one decade. Consequently, a feature of the invention is that the balun 93 in
In particular, the foam layers 16 and 17 have a low dielectric constant and are thus effectively transparent to radio frequency (RF) energy. On the other hand, the resistive sheet 18 serves as a lossy material which is intentionally configured to absorb a predetermined portion of the energy introduced into the slot 41 from the center conductor 81. The amount of this energy which is absorbed by the sheet 18 is within a range of approximately 5% to 20%, and preferably within a range of approximately 9% to 15%. In the embodiment of
With respect to the increased bandwidth resulting from the absorption of energy by the sheet 18, an explanation of the underlying theory will be provided with reference to
In the case of pre-existing quarter-wave stub and open-circuit cavity balun designs, where the cavity load impedance ZL,cav is a short circuit, the equation for Zin,cav reduces to:
Zin,cav=jZo,cav tan(βLcav) (2)
The performance of a balun with the input cavity impedance given by Equation (2) is determined by the magnitude of the cavity characteristic impedance and the cavity length. However, it is clear that, for any finite characteristic impedance, it will be the case that Zin,cav=0 at Lcav=nλ/4, n=0,1,2 . . . Thus, baluns with a short-circuit termination possess both upper and lower limits on the operating frequency band.
In the case of a high-impedance balun, the cavity load impedance is no longer a short circuit. Ideally, it is desirable to set the load impedance so that it exactly equals the cavity characteristic impedance, which for this discussion is selected to be 377 Ω (the highest possible impedance in a square-lattice array). This reduces Equation (1) to:
Zin,cav=Zo,cav=377Ω (3)
As is evident from Equation (3), a matched-load balun termination eliminates the theoretical bandwidth limits on the balun performance. In an ideal world, it should theoretically be possible to terminate a balun with a high-impedance load and obtain limitless bandwidth. In the ideal case of a 377Ω load and a 50Ω system impedance, a high-impedance balun should transmit 88% of the incident power into the slot, and the remaining 12% should be either reflected at the junction, or dissipated in the high-impedance load.
The embodiment of
Although as mentioned above the bandwidth should ideally be limitless, practical limits in the materials and size of the balun load serve to effectively limit the bandwidth performance. Consequently, the disclosed embodiment provides a bandwidth in excess of approximately 35:1 at an efficiency in excess of 88%. However, electromagnetic effects (such as wave reflection off the air-load resistor interface) can be optimized in order to provide better than optimal performance within the band.
The present invention provides a number of advantages. One such advantage is the provision of a broadband balance-to-unbalanced transition that operates over a multi-decade frequency band. The bandwidth is at least two to four times as broad as the best known previous design. This is achieved through the provision of a lossy or absorbing material within a balun, so as to provide a high look-in impedance throughout a bandwidth of two or more decades.
Although one embodiment has been illustrated and described in detail, it will be understood that various substitutions and alterations are possible without departing from the spirit and scope of the present invention, as defined by the following claims.