Abstract:
A log-periodic antenna comprises two arrays of dimensionally tapered radiating elements disposed in the E-plane and each fed by a balanced line consisting of the inner conductors of two coaxial cables. In one embodiment the elements of each array are dipoles and in another embodiment are formed of continuous conductive strips in zig-zag patterns on non-conductive support members. Each array preferably has two sets of elements disposed in planes, respectively, which converge toward the smaller end of the array with vertically aligned radiating elements of each set projecting in opposite directions from the array axis. Periodic gain dropout anomalies across the antenna operating band are eliminated by use of a shielded feed line. In another embodiment having advantage in direction finding, the sets of elements of each array are located on associated opposite sides of a right rectangular pyramid. These pyramidal arrays are used in pairs for direction finding.

Description:
RELATED APPLICATION 
     This is a continuation of Ser. No. 309,874, filed Oct. 19, 1981, now abandoned. 
    
    
     BACKGROUND OF THE INVENTION 
     This invention relates to frequency independent antennas and more particularly to frequency independent log-periodic antenna arrays. 
     Log-periodic antennas, well known for their psuedo-frequency independent operation, are arrayed together to provide higher directivity and higher gain and also to adapt the antennas for use in direction finding and tracking applications. Such uses of arrayed log-periodic antennas provide independent error curves for either amplitude comparison of for sum and difference derivations. A problem with such arrays is the periodic occurrence of gain variations in the E-plane (horizontal) arrays of the antenna across the operating band. These periodic gain variations or &#34;dropouts&#34; are accompanied by pattern deteriorations and seriously adversely affect the performance of the antenna. When a conventional log-periodic dipole antenna was arrayed in the frequency independent manner in the E-plane, periodic gain dropouts of more than 10 dB over an active operating band were measured in spite of the fact that the individual antenna elements of the array provide frequency independent operation. 
     Attempts to decrease or eliminate such gain dropouts and pattern deteriorations have been attempted in the past. By using size-reduced dipoles as radiating elements as described in U.S. Pat. No. 3,732,572, the magnitude of the gain dropouts has been reduced but not completely eliminated. Another technique that has been proposed is wrapping of the two-wire transmission line with RF absorbing material, see &#34;A Study of TEM Resonances on a Class of Parallel Dipole Arrays&#34; by Tranquilla et al, Proceedings of the 1977 Antenna Applications Symposium, Electromagnetics Laboratory, University of Illinois, Urbana Champaign, Ill., Apr. 27-29, 1977. Such absorbing materials, however, produce substantial losses of approximately 4 to 6 dB at all frequencies and therefore is not an acceptable solution to the problem. 
     This invention is directed to a frequency independent antenna that overcomes this gain dropout anomaly. 
     OBJECTS AND SUMMARY OF THE INVENTION 
     A general object of the invention is the provision of a log-periodic antenna having arrays of elements in the E-plane operating over the frequency band of the antenna without gain dropouts. 
     A further object is the provision of such an antenna in which periodic gain dropouts are eliminated without otherwise detracting from the performance characteristics of the antenna. 
     These and other objects of the invention are achieved by utilizing a shielded balanced feed line for energizing log-periodic antenna elements arrayed in a frequency independent manner in the E-plane. A preferred form of the shielded feed line is the inner conductor of a coaxial cable. 
    
    
     DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a schematic plan view of a log-periodic dipole antenna embodying this invention. 
     FIG. 2 is a perspective view of one of the arrays of FIG. 1 with parts of the feed lines broken away to show details of construction. 
     FIG. 3 is a schematic plan view similar to FIG. 1 showing arrays having a zig-zag pattern of radiating elements. 
     FIG. 4 is an enlarged perspective view of one of the arrays of FIG. 3. 
     FIG. 5 is a greatly enlarged portion of FIG. 4 showing the connection of the feed lines to the radiating elements. 
     FIG. 6 is a greatly enlarged plan view of a portion of the zig-zag shaped conductive strip of FIGS. 3-5 showing design parameters. 
     FIG. 7 is a perspective view of an array of a log-periodic antenna designed for circularly polarized operation and embodying the invention. 
     FIG. 8 is an enlarged end view of the array taken on line 8--8 of FIG. 7. 
     FIG. 9 is a schematic representation of two of the arrays of FIG. 7 disposed to provide direction finding information. 
    
    
     DESCRIPTION OF PREFERRED EMBODIMENTS 
     Referring now to the drawings, FIG. 1 illustrates an antenna 10 embodying the invention and comprising dipole arrays 11 and 12 in a horizontal (E) plane, the axes 13 and 14 of arrays 11 and 12, respectively, forming an angle ε. Arrays 11 and 12 have feed lines 16 and 17, respectively, connected to hybrid T junctions 18 and 19, respectively, also known as magic T junctions. The outputs of the magic T junctions 18 and 19 are connected to a power divider 21 which in turn is connected to utility apparatus such as a receiver or transmitter. 
     Antenna arrays 11 and 12 are substantially identical in construction and accordingly only one of them, array 11, is shown in FIG. 2 and is described. Feed line 16 of array 11 comprises vertically stacked coaxial cables 23 and 24 having inner conductors 25 and 26, respectively, and outer conductors 27 and 28, respectively. The outer conductors are grounded as indicated at 29 and thus shield the inner conductors. Cables 23 and 24 are connected to magic T 18 which provides 180° phase reversal in the two lines as required for end fire radiation along array axis 13. 
     Radiating elements 30 are connected to the feed lines transversely of the array axis 13 such that element dimensions and interelement spacings decrease from a maximum at one end to a minimum at the other in increments of a predetermined ratio τ. These elements comprise a first set a, b, c, d and e connected to inner conductor 25 of cable 23 and a second set a&#39;, b&#39;, c&#39;, d&#39; and e&#39; connected to inner conductor 26 of cable 24. Each element extends through an opening in the outer conductor of the associated cable for direct electrical contact with the inner conductor thereof. The elements of each array are arranged in transversely extending pairs, each pair being designated by the same letter a-a&#39;, b-b&#39;, etc.) and each pair comprising one dipole. Inner conductors 25 and 26 are the balanced feed lines for the array and by connecting them to the radiating elements and by grounding outer conductors 27 and 28 as described, the feed lines are shielded from external radiation including the effects of mutual coupling between arrays 11 and 12. By use of these shielded feed lines, periodic gain variations across the operating band of the antenna are eliminated. 
     A log-periodic dipole antenna 10 constructed as described above had the following design parameters and performance characteristics: 
     
         ______________________________________Convergence angle ε                 26Taper angle α   20°τ                 0.9Smallest dipole       5&#34;Largest dipole        16&#34;Feed line impedance (Z.sub.0)                 100 ohmsFrequency band        470-900 MHz______________________________________ 
    
     The feeder impedance is 100 ohms because 50 ohm coaxial cables were used. This antenna provides pseudo-frequency independent performance similar to a log-periodic dipole antenna fed by conventional balanced lines. When two dipole arrays are arrayed in the frequency independent manner at relatively close spacing, i.e., 0.5 wavelength the antenna provided substantially frequency independent performance with no periodic gain dropouts or pattern deteriorations. The dipole antenna described above is constructed to operate at UHF frequencies readily but not at microwave frequencies due to the physical size of the balun and the manner in which the radiators are attached to the transmission lines. 
     The shielded feed lines described above as the inner conductors of coaxial cables achieve the objects of the invention efficiently and economically since standard commercially available cable is utilized. Practice of the invention, however, is not limited to this feed line which alternatively may take the form of twin spaced conductors within a single enclosing grounded shield having openings through which the dipoles extend for connection to the lines as described above. 
     Periodic gain dropouts and pattern deteriorations are not limited to E-plane arrays of the planar log-periodic dipole antennas of the type described above. Open structure types of log-periodic antennas comprising E-plane arrays with the radiating elements of each array in two planes converging to the feed point also have periodic gain dropouts when arrayed in the frequency independent manner. An example of such open type structure is illustrated in FIGS. 3 and 4 and comprises antenna 35 having substantially identical arrays 36 and 37, each array having two sets of radiating elements converging at an angle ψ in the H-plane (vertical). The angle ψ determines the H-plane beamwidth and the mean level of the input impedance of the antenna and distinguishes the &#34;open&#34; structure from the planar antenna. In other words, when the angle ψ approaches 0, a planar antenna comparable to the above described log-periodic dipole antenna results. 
     Arrays 36 and 37 have axes 38 and 39 respectively, which converge at an angle θ toward the feed points of the arrays, and in accordance with this invention, are fed by balanced lines 41 and 42, respectively. These arrays are substantially identical and accordingly only one of them, array 36, is described. Feed line 41 comprises the inner conductors 43a and 44a of coaxial cables 43 and 44, respectively, see FIGS. 4 and 5. Cables of lines 41 and 42 are connected to magic T couplers 45 and 46, respectively, which in turn are connected to a power divider 47 for connection to associated utility apparatus. Array 36 comprises a pair of conductive strips 50 and 51 in tapered zig-zag shapes forming triangularly shaped radiating elements. Strips 50 and 51 are mounted on elongated support members 52 and 53, respectively, composed of dielectric material such as epoxy fiberglass. The outer conductors of coaxial cables 43 and 44 are suitably grounded and the inner conductors 43a and 44a thereof are connected to strips 50 and 51, respectively, at the converging end of the array to constitute the feed point. 
     The triangular portions of strips 50 and 51 having the same spacing from the array feed point project equal distances and in opposite directions from supports 52 and 53, respectively, and constitute the radiating elements of the array. For example, segment 50a of strip 50 and segment 51a of strip 51 are equally spaced from the feed point and project equal distances and in opposite directions from supports 52 and 53, respectively. Segments 50a and 51a thus have equal lengths and constitute one radiating element of the array analogous to a dipole of array 11. 
     The continuous zig-zag shaped conductive strip is defined by two conventional log-periodic design parameters α see FIG. 6, and τ. An additional design parameter β defines the width of the zig-zag conductor. When the value of β approaches the value of α, the antenna structure approaches that of a zig-zag wire. As the value of β decreases, the width of the zig-zag conductor increases until β approaches 0. The array structure consisting of two of these zig-zag conductors performs similarly to the conventional log-periodic dipole array with the exception of a slight loss of gain due to the I 2  R loss. The exciting currents, instead of travelling straight on the metallic boom of the conventional antenna, follow the zig-zag conductor path before reaching the active region of the array. The loss is less than 1 dB. By decreasing the angle β this loss is minimized with the tradeoff of a slight increase in the amount of conductive material. The spacings l 0 , l 1 , l 2 , . . . l n  of the elements from the point of convergence as illustrated in FIG. 6 are related to each other log-periodically in accordance with the following formulae: 
     
         ______________________________________       l.sub.3 = √τ l.sub.4       l.sub.2 = √τ l.sub.3       l.sub.n-1 = √τ l.sub.η______________________________________ 
    
     A circularly polarized antenna embodying the invention was constructed by substituting a 90° coupler for the power divider 47 in FIG. 3 and such antenna had the following parameters: 
     
         ______________________________________α               20°β                7°√τ         0.9Length of smallest element                 0.3&#34;Length of largest element                 7.0&#34;Frequency band        1 to 12 GHz______________________________________ 
    
     No periodic gain dropout anomalies were observed during operation of the above antenna. 
     Another embodiment of the invention is shown in FIGS. 7, 8 and 9 depicting a circularly polarized antenna array 55 comprising four zig-zag conductive strips 56, 57, 58 and 59, similar to the strips shown in FIG. 6 and mounted on the plane sides of a pyramid-like dielectric support 60. Adjacent sides of support 60 are at right angles to each other and taper from a maximum dimension at one end to a minimum dimension at the other. Each of the strips is similarly tapered to the feed point of each at the end having the minimum dimension. The planes of adjacent strips are likewise perpendicular to each other as shown in FIGS. 7 and 8. 
     The array 55 is fed by the inner conductors 62, 63 and 64 and 65 of coaxial cables, the other conductors of which are connected to ground. Cables having conductors 62 and 64 are connected to magic T 67 and cables having conductors 63 and 65 are connected to magic T 68. Each magic T is connected to a 90° coupler 69 which in turn is connected to associated utility apparatus. The magic T junctions 67 and 68 and the 90° coupler 69 are enclosed in a broken line block 70 for convenience of explanation of FIG. 9. When two such circularly polarized arrays 55 and 55&#39; are arrayed together as shown in FIG. 9, the outputs of block 70 and identical block 70&#39; may be combined in magic T 71 to provide direction finding data. Since two pairs of zig-zag strips are in the E-plane when the structures are arrayed as shown in FIG. 9, the antenna is subject to the gain dropout anomaly when energized by conventional unshielded feed lines. In accordance with this invention, the use of shielded feed lines for each of the array structures shown in FIG. 9 eliminates this gain dropout anomaly. 
     An antenna shown in FIGS. 7, 8 and 9 was constructed and operated from 0.25 to 4.0 GHz. The smallest and largest radiating elements were 0.8 inches and 26 inches, respectively. This frequency independent array was used as a direction finding antenna and operated over the above band without any periodic gain dropout anomaly.