The present invention relates to communications systems, and more particularly, to radio frequency (RF) antennas and related methods.
For communications in the Very Low Frequency (VLF), Low Frequency (LF), and Medium Frequency (MF) ranges, for example, relatively large ground-based antenna towers are used for transmitting such signals. Such antenna configurations may include a tower several hundred feet in height connected to the ground at its base, with numerous guy wires connecting the tower to ground for stability.
One example medium wave antenna system is disclosed in U.S. Pat. No. 6,873,300 to Mendenhall. This patent discloses an antenna system including an electrically conductive radiating mast that extends generally vertical relative to earth ground. The mast has a lower end for receiving RF energy for radiation thereby at an operating RF frequency and an upper end. A plurality of N radial, electrically conductive, wires are provided with each having an inner end and an outer end. The inner ends of the radial wires are electrically connected together and located proximate to the vertical mast. The radial wires are elevated throughout their lengths above the level of earth ground and extend radially outward from the vertical mast. A tuning device, such as an adjustable inductor, is connected to the radial wires for adjusting the impedance thereof such that the radial wires resonate at the operating frequency.
Another example where large scale tower based antennas are used is low frequency transmission stations for navigation systems, such as the long range navigation (LORAN) system. LORAN was developed in the United States during World War II. Subsequent implementations provided for enhancements in accuracy and usefulness, including LORAN-C and the later enhanced LORAN (eLoran) implementations. More particularly, eLoran is a low frequency radio navigation system that operates in the frequency band of 90 to 110 kHz. Low frequency eLoran transmissions can propagate by ground wave, a type of surface wave that hugs the earth. Ionospheric reflections or sky waves are another significant mechanism of eLoran wave propagation. With typical low frequency antennas, the tower itself is used as a monopole antenna. Because of the height of the tower, which may be 600 feet or more as a result of the operating wavelength, many upper wires connect to the tower top forming a resonating capacitor. These wires, known as top loading elements (TLEs), may approximate a solid cone.
eLoran may operate at low frequencies such as 100 kHz, making transmit antenna physical size large and yet antenna electrical size small relative to wavelength. Physics may limit electrically small antenna fixed tuned bandwidth. One theory is the Chu Limit as described in the reference “Physical limitations of omni-directional antennas”, Chu, L. J. (December 1948), Journal of Applied Physics 19: 1163-1175, which is incorporated herein in its entirety by reference. The Chu Bandwidth Limit equation may Q=1/kr3, where Q is a dimensionless number relating to bandwidth, k is the wave number=2π/λ, and r is the radius of a spherical analysis volume enclosing the antenna. Antenna radiation bandwidth is a matter of considerable importance to eLoran as it enables sharp eLoran pulses with fast rise times to be transmitted.
With the rise of satellite based navigations systems such as the Global Positioning System (GPS), there has been relatively little development or investment in terrestrial-based navigation systems such as eLoran until recently. A renewed interest in such systems has arisen as a backup to satellite navigation systems, particularly since low frequency eLoran signals are less susceptible to jamming or spoofing compared to the relatively higher frequency GPS signals. As such, further developments in eLoran antenna systems may be desirable in certain applications.
An antenna may include a tower extending vertically upward from a ground location, a first set of elongate antenna elements extending outwardly from the tower at a first height above the ground location, and a second set of elongate antenna elements extending outwardly from the tower at a second height above the ground location and below the first height. The antenna may also include at least one elongate antenna element of the first and second sets of elongate antenna elements being electrically coupled to the ground location, and a radio frequency (RF) feed electrically coupled to the first and second sets of elongate antenna elements.
More particularly, the antenna may further include a plurality of buried ground conductors at the ground location, and the at least one elongate antenna element of the first and second sets of elongate antenna elements may be electrically coupled to the plurality of buried ground conductors. Moreover, the RF feed may also be electrically coupled to the plurality of buried ground conductors. Additionally, at least one of the first and second sets of elongate antenna elements may be arranged in a conical pattern. By way of example, the conical pattern may be defined by an angle from normal to the tower in a range of 10-90 degrees. In accordance with another example embodiment, at least one of the first and second sets of elongate antenna elements may be arranged in a planar pattern.
In accordance with an example implementation, the tower may comprise a conductive material, the first and second sets of elongate antenna elements may be electrically coupled to the tower, and the RF feed may be electrically coupled to the tower. In accordance with another example, the first and second sets of elongate antenna elements may be electrically insulated from the tower, and the antenna may further include an RF feed cable coupling the RF antenna feed to the first and second sets of elongate antenna elements.
By way of example, each of the first and second sets of elongate antenna elements may include at least ten elongate antenna elements. Furthermore, the first and second sets of elongate antenna elements may be configured to operate in the eLoran frequency range of 90 to 110 KHz, for example. Additionally, the tower may comprise a lattice tower in one example implementation.
A related method for making an antenna may include mounting a tower extending vertically upward from a ground location, mounting a first set of elongate antenna elements extending outwardly from the tower at a first height above the ground location, and mounting a second set of elongate antenna elements extending outwardly from the tower at a second height above the ground location and below the first height. The method may further include electrically coupling at least one elongate antenna element of the first and second sets of elongate antenna elements to the ground location, and electrically coupling a radio frequency (RF) feed to the first and second sets of elongate antenna elements.
The present description is made with reference to the accompanying drawings, in which exemplary embodiments are shown. However, many different embodiments may be used, and thus the description should not be construed as limited to the particular embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete. Like numbers refer to like elements throughout, and prime notation and multiple prime notation are used to indicate similar elements in different embodiments.
Referring initially to
By way of background, the eLoran navigation system utilizes low frequency signal pulses in a range of 90 to 110 KHz. Moreover, eLoran pulses are interleaved, and the sharper the pulses the more eLoran stations that can be deployed. An eLoran transmit tower needs to transmit rise times in approximately 55 microseconds or less to reject skywave, and with peak powers which are typically 100 KW or higher. While increased antenna bandwidth increases reported position accuracy, it is desirable to avoid long antenna smeared pulses as they degrade system performance.
Furthermore, typical eLoran antennas included a ground-mounted conductive (e.g., metal) tower mounted on a base insulator. The tower itself was used as a monopole antenna. As noted above, upper wires connect to the tower top forming a resonating capacitor, and these top loading elements may approximate a solid cone. The top loading wires do not extend to the ground electrically due to insulators in the wires. However, this antenna configuration develops only a low radiation resistance, so a transformer and inductors are needed in a building at the tower base. Moreover, this type of conventional eLoran antenna configuration provides a quadratic frequency response.
eLoran transmit antennas may be electrically small relative to wavelength or nearly so. As such, eLoran antenna fixed tuned bandwidth may be limited according to the Chu-Harrington Limit of 1/kr3, where k is the wave number 2n/λ and r is the radius of an spherical analysis volume enclosing the antenna.
In the illustrated example, the antenna 30 includes a mast or tower 31 extending vertically upward from a ground location (schematically shown as a line in
Generally speaking, ten or more elements may be used in the first and second sets of elongate antenna elements 32, 33, and more particularly up to about thirty-six elements for an eLoran implementation. The tower 31 may be mounted on a base insulator (not shown).
In addition, the antenna 30 also illustratively includes one or more ground return conductors or cables 34 coupled to respective elongate antenna elements 33 so that they are electrically coupled to the ground location. More particularly, in the illustrated embodiment a plurality of buried ground conductors 35 (e.g., a cage) is provided at the ground location, and the ground return cables 34 couple respective antenna elements 33 to the ground conductors. The first and second sets of antenna elements 32, 33 are fed by a radio frequency (RF) feed source 36 which, in the illustrated example, is coupled to the tower 31. The RF feed source 36 is also electrically coupled to the ground conductors 35 as schematically shown in
The ground return cables 34 advantageously increase tower resistance with respect to conventional eLoran antenna configurations. Furthermore, the more ground return cables 34 used, the higher the resistance. The ground return cables may be connected at different positions along the length of the antenna elements 33 (i.e., closer or further spaced from the tower 31). Generally speaking, the further the ground return cables 34 are out from the tower 31, the higher the resistance will be. This advantageously allows for direct impedance matching (e.g., 50 Ohm), so that no base transformer is needed as in conventional eLoran antenna configurations.
While the present approach is not bound to any particular theory of operation, the ground return cables 34 may carry antiparallel currents relative the tower 31. This means that that current flow in the ground return cables 34 may be in an opposite direction to the current flow on the tower 34. The opposite direction currents on the tower 31 and the ground return cables 34 in turn generate bucking induction fields to raise tower 31 base resistance. As well, in circuit equivalent terms the ground return cables 34 refer parallel inductance across the tower 31 base providing a method of raising antenna 30 driving resistance. Advantageously, the ground return cables 34 easily carry any high currents needed for large radio frequency (RF) feed source 36 power levels, and the ground return cables avoid the need for a transformer, helix or coil at the tower 31 base.
In accordance with an example implementation, the following steps may be performed: 1) sizing the first and second sets of antenna elements 32, 33 to place the antenna 30 slightly below resonance at the desired frequency of operating without the ground return cables 34 and then; 2) utilizing parallel inductance from the ground return cable(s) 34 to complete fine tuning for resonance at the desired frequency of operation.
In the illustrated example, both of the first and second sets of antenna elements 32, 33 are arranged in respective conical patterns. By way of example, the conical pattern may be defined by an angle α from normal to the tower in a range of 10-90 degrees, although both sets need not have the same angle. Furthermore, different antenna elements within the same set of elements may be at different angles relative to one another in some embodiments. Moreover, the angle α may be an upward angle for one or both sets of antenna elements 32, 33 in some embodiments, as opposed to the downward angle in the illustrated example. In accordance with one example eLoran implementation, the first height h1 may be approximately 650 feet, the second height h2 may be approximately 400 feet, and the first and second sets of antenna elements 32, 33 may extend laterally outward from the tower 31 approximately 300 feet. That is, the antenna may have a total width or “footprint” of about 600 feet (not including the grounding cage 35, which may extend wider than the antenna elements in some embodiments). Generally speaking, this footprint or diameter may be approximately 0.2-0.25 of the operating wavelength, for example.
Based upon the above-noted eLoran antenna dimensions, a 3000:1 scale model was built and tested in a lab with a vector network analyzer using solid sheet metal cones emulating the wire cage configurations shown in
As can be appreciated, the simple monopole antenna or conventional top loaded monopole may have quadratic, single VSWR dip at first resonance. The Chu size-bandwidth limit appears to have been worked for quadratic response antennas and not multiple tuned antennas such as in the present examples. The present approach may advantageously allow for smaller eLoran transmitting antennas.
The antenna 30 is not limited as to the use of only two sets of elongate antenna elements 32, 33. Three and more sets of elongate antenna elements are theoretically possible. For example, the upper limit for tuning order and increased passband ripple rate from a large plurality of elongate antenna elements may be 3π that of a single set of elongate antenna elements 32. A single set of elongate antenna elements will for example produce a quadratic frequency response without further compensation. Of course, as diminishing return sets in regarding bandwidth as more and more sets of elongate antenna elements are employed and more passband ripples are realized.
Embodiments of the antenna 30 may include using only one set of elongate antenna elements 32 with the one or more ground return cables 34. This embodiment provides a quadratic frequency response and an adjustable driving resistance at the base of the tower 31 such as 50 ohms. The ground return cables 34 provide a method of adjusting or raising antenna tower 31 base resistance increase with any number of elongate antenna elements 32 or “capacitive hats”, one or more.
Embodiments may also be used where two or more sets of elongate antenna elements may be used to obtain extended antenna 30 bandwidth without the use ground return cable(s) 34. In this embodiment, other approaches of adjusting or raising tower 30 base resistance may be employed, such as a common transformer with coil windings and an iron core (not shown), or a paralleled helix type inductor between the tower base and ground (not shown).
The realized gain response versus frequency of the antenna 30 may be approximately the reciprocal of the VSWR response versus frequency, although different amplitude scales will apply. Thus, where there is a VSWR minima the realized gain may be at maxima. The elevation plane radiation patterns of the antenna 30 is approximately the same sine function shape that a short monopole with a single set of elongate antenna elements 23 (not shown) exhibits, plus the ground effects. The radiation pattern bandwidth of antennas small versus wavelength antennas is quite stable over frequency, whereas impedance bandwidth may vary rapidly. The antenna 30 beneficially extends this impedance bandwidth. The realized gain of the antenna 30 is the product of directivity times efficiency. Efficiency depends upon factors including ground conductivity, which makes the number of ground conductors 35 important. For sufficiently conductive soils, estimates of directivity may be the small antenna directivity limit of 1.7 dBi with a 3 dBi directivity increase due to half space radiation, so 4.7 dB total. Radiation efficiency and realized gain may be computed for specific embodiments by the moment finite element methods using numerical computation.
The tuning of most to all low frequency antennas can drift over time, and this may include upward drifts in frequency due to soil freezing. Soil freezing reduces the soil relative permeability, and this reduces soil capacitive loading effects on a low frequency antennas. Low frequency antenna electric near fields (e.g. those of Gauss' Law) couple into any soil not shielded by the ground radial wire system. The antenna 30 may therefore be advantageous in areas subject to soil freezing and thawing, as the increased bandwidth can provide an increased margin against drift.
In the example of
In accordance with another example embodiment of the antenna 30″ now described with reference to
A related method for making the antenna 30 (or the antennas 30′, 30″) is now described with reference to the flow diagram 60 of
Many modifications and other embodiments will come to the mind of one skilled in the art having the benefit of the teachings presented in the foregoing descriptions and the associated drawings. Therefore, it is understood that the disclosure is not to be limited to the specific embodiments disclosed, and that other modifications and embodiments are intended to be included within the scope of the appended claims.
Number | Name | Date | Kind |
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3234948 | Stebbings | Feb 1966 | A |
3253279 | Tanner | May 1966 | A |
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3742511 | Smith et al. | Jun 1973 | A |
4149169 | Weber | Apr 1979 | A |
5467955 | Beyersmith | Nov 1995 | A |
6873300 | Mendenhall | Mar 2005 | B2 |
9571132 | Hershberger | Feb 2017 | B1 |
20090318094 | Pros et al. | Dec 2009 | A1 |
Number | Date | Country |
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5624818 | Mar 1981 | JP |
2017025675 | Feb 2017 | WO |
Entry |
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“Continental Electronics receives Patent Beneficial to Future eLoran Deployments” www.contelec.com; Dallas, Texas, Apr. 4, 2017; 1 pg. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Martin Ehrenfried “The terminated coaxial cage monopol (tc2m) a new design of broadband HF vertical antenna” RadCom: May 2014, pp. 13-16. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Martin Ehrenfried “A new design of broadband HF vertical antenna” RadCom: Jun. 2014, pp. 38-42. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Sarah Mahmood “Critical Infrastructure Vulnerabilities to GPS Disruptions” http://www.gps.gov/governance/advisory/meetings/2014-06/mahmood.pdf, Jun. 4, 2014, pp. 17. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Jansky & Bailey “The Loran-C system of navigation” http://www.loran-history.info/Loran-C/Jansky%20_%20Bailey%201962.pdf Feb. 1962, pp. 135. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Anonymous “Loran-C” https://en.wikipedia.org/wiki/Loran-C#eLORAN; retrieved from internet Jan. 3, 2018; pp. 13. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Koo et al. “Modified L-type eloran transmitting antenna for co-location with an AM antenna” 2016 International Symposium on Antennas and Propagation (ISAP); Abstract Only. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Stout et al. “Designing, Developing, and Deploying a Small Footprint eLoran System” Proceedings of the 2010 International Technical Meeting of The Institute of Navigation Jan. 25-27, 2010; Abstract Only. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Richard Degener “Loran navigation signal back on and better than before” Jun. 19, 2015 http://www.pressofatlanticcity.com/news/loran-navigation-signal-back-on-and-better-than-beforearticle_21d19298-16d0-11e5-9a69-1343edc2e90b.html, pp. 6. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Chu, L.J. “Physical limitations of omni-directional antennas” Journal of Applied Physics 19: Dec. 1948; 1163-1175. Abstract Only. See Priority U.S. Appl. No. 15/980,857, filed May 16, 2018. |
Number | Date | Country | |
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20200411999 A1 | Dec 2020 | US |
Number | Date | Country | |
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Parent | 15980857 | May 2018 | US |
Child | 17021204 | US |