This invention relates generally to communications and more specifically to communications accomplished via spiral antennas. More specifically, the invention relates to utilizing a spiral antenna design that provides linear polarization. With greater specificity, but without limitation thereto, the invention relates to using two or more linearly polarized, conductor-backed, spiral antennas to simultaneously transmit upon the same frequencies without interfering with each other.
Typically, antennas transmitting simultaneously on the same frequency will interfere with one another. Depending on the relative intensities of the transmissions, one transmission can overwhelm or “drown out” the other transmission.
Certain prior art methods designed to use the frequency spectrum efficiently rely upon complex methods of interlacing messages by time (TDMA) or by coding (CDMA). Another method uses crossed-log periodic antennas. The crossed-log antennas have broad bands and are linearly polarized but are not physically compact. Typically, these antennas extend in the direction perpendicular to propagation on the order of 0.5 wavelength and are often several times the wavelength in size in the direction along the line of propagation. Crossed dipoles and patches are yet a further application. These are relatively compact and are linearly polarized, but are not broad band. Yet another scheme of enhancing communications can be found in the satellite communication field. Antennas used to communicate with satellites often use helices. The uplink signal is typically orthogonal to the downlink signal (e.g. right circularly polarization versus left circular polarization). Helical antennas are rarely compact. The cavity-backed spiral is another design that has been used in many antenna systems. The polarization of a cavity-backed spiral is typically circular and could be used in a dual transmitting mode by transmitting a right-circular polarized signal and receiving a left-circular polarized signal. In the cavity-backed spiral design, half the power utilized is absorbed in the cavity behind the spiral.
There is therefore a need within the art to provide an enhanced method of communicating that permits simultaneous transmission at the same frequencies from a relatively simple antenna system of efficient, compact and broad-band design.
The invention provides a method and apparatus in which two or more conductor-backed, spiral antennas are used to simultaneously transmit or receive upon the same frequencies without interference. The conductor-backed spirals are broad-band in operation, typically exhibiting a 9:1 ratio of maximum to minimum frequency. These spirals are also efficient, experiencing approximately a 6 dB advantage in gain on transmit and receive compared to a cavity-backed spiral.
The invention utilizes specifically designed conductor-backed spiral antennas shown to exhibit linear polarization. For these conductor-backed spiral antennas, a change in frequency is synchronized to a change in the polarization vector of the communication signal. The amplitude (change in dB) of the polarity change is related in general to the thickness of the dielectric layer between the radiating elements of the antenna and its conductor backing.
To permit simultaneous transmission on the same frequencies, two, for example, of the linearly polarized, conductor-backed spiral antennas can be spaced vertically, for example, and are oriented so that the feed points of one antenna are orthogonal to the feed points of the second antenna. Since the specifically designed spiral antennas will be both transmitting or both receiving at orthogonally arranged polarizations, the antennas will not interfere with each other, even though communication is upon substantially the same frequency.
Accordingly, it is an object of this invention to provide a communication method and apparatus that enhances the efficiency of communication.
A further object of this invention is to provide a communication method and apparatus that enhances the efficiency of communication by using an antenna of simple design.
Yet another object of this invention is to provide a communication method and apparatus that enhances the efficiency of communication by using an antenna of relatively compact design.
Still a further object of this invention is to provide a communication method and apparatus that enhances the efficiency of communication by using an antenna of broad-band design.
Still a further object of this invention is to provide a communication method and apparatus that enhances the efficiency of communication by using an efficient antenna of simple, compact and broad-band design incorporating spiral antenna elements.
Other objects, advantages and new features of the invention will become apparent from the following detailed description of the invention when considered in conjunction with the accompanying drawings.
Research conducted by the U.S. Navy on antennas has indicated that specific spiral antennas of conductor-backed design are linearly polarized over a broad frequency band. This polarization has been found to depend upon frequency, the number of turns of the spiral antenna elements and the thickness of a dielectric disposed between the spiral antenna elements and their corresponding conductor backing.
The Navy study found that increasing the number of turns of the spiral increases the occurrence of polarization changes (from horizontal to vertical and vice-versa) for a given frequency range. It was also learned that in general the thickness of the dielectric layer between the spiral radiating elements and the conductor backing determines the magnitude (change in dB) of the polarization effect. For a conductor-backed spiral antenna with a relatively thin dielectric layer (one that is small compared to the utilized wavelength), a small change in frequency can cause a relatively large change in polarization. The studies were conducted on two-arm spirals, however it is envisioned that similar effects may also be attributable to conductor-backed spiral antennas having more than two spiral arms.
Referring now to
The spiral antennas will be described in greater detail, however, as a general description, each of the antennas include at least a pair of spiral radiating elements or arms shown generally as 22 and 22′ and 24 and 24′.
Although antennas having two-armed spirals have been successfully employed to achieve desired polarization characteristics, it is also envisioned that spiral antennas containing a greater number of arms may also exhibit similar polarization performance characteristics. In the spiral antennas researched, the spiral radiating elements followed an Archimedean path and had two foot diameters of a variety of turns. As is well understood in the art of spiral antennas, the maximum diameter of the spirals and inner gap dimensions are determined by the minimum and maximum frequencies anticipated to be used with the antennas. Further, those skilled in the art will appreciate that other spiral configurations of the antenna elements of the invention may also be possible and still fall within the metes and bounds of the invention disclosed here.
Shown are conductor backings 26 and 28 for use with arrays 10 and 12, respectively. In conjunction with the two foot outer diameter spirals described here, a suitable conductor backing can take the configuration of a three foot by six foot rectangular plate. As can be seen the spiral radiating elements are separated from the conductor backings by a dielectric substrate 30, 30′ and 32, 32″ having substantially flat, opposite sides. A suitable dielectric for this purpose is marketed under the trademark name of DIVINYCELL and has a dielectric constant of approximately 1. Others materials with different dielectric constants could also be used to advantage.
In research conducted and as well be further explained, this substrate was varied in thickness to ascertain its affect on polarization performance. As a result of this research, it was learned that the degree (or change in dB) to which horizontal or vertical polarization dominates depends upon the distance between the spiral radiating elements and the ground plane. To enhance a change in polarization upon a change in transmitted/or received frequency, the distance between the spiral elements and the ground plane (conductor) should be a small fraction of a wavelength of the energy radiated or received.
Referring again to
Referring now to
The orthogonality of the polarization vector permits two signals with the same frequency to be transmitted and received without interference with each other. This is accomplished by orienting an imaginary line drawn through the separate feed points of the antennas to be mutually perpendicular.
Referring again to
Referring now to
Referring to
In the specific example presented, spiral elements 40 are made up of photolithically applied conductive metal traces 42 applied to a first substantially flat side 44 of a dielectric substrate 46. Attached to metal traces 42 is a coaxial cable 48. In this implementation of the invention, the outer braided grounding shield (not shown) of coaxial cable 48 is soldered to metal traces 42 at various points along the path of the traces. At outer end 50 of spiral elements 40, the inner conductor (not shown) of coax cable 48 is shorted to the outer braid of the cable. At inner end 52 of spiral elements 40, the inner conductor of the two arms are joined and are soldered to the outer braid of the coax cable.
In this embodiment, the radiating elements are center-fed by means of an infinite balun. Alternatively, it can be envisioned that the antenna could be edge-fed by a balun. Connector 54 provides an input/output to the antenna elements and also an energization point. As is known in the art of spiral antennas, the length of the radiating elements and accordingly their largest diameter and inner gap are a function of the frequency expected to be used. As this is well understood within the art, greater details of this aspect of the antennas will not be presented here. It should also be understood that the particular feed and antenna energizations schemes discussed herein as well as the design of the spiral elements disclosed could be replaced by other configurations known in the art and still fall within the spirit of the invention disclosed here providing that an orthogonal feed arrangement as discussed above is maintained.
As can also be seen in
A measure of the dominance of one polarization over another is known as an axial ratio. Referring to
The 6-inch thick spiral had a difference between maximum and minimum for an axial ratio of 17.15 dB. The 3-inch thick spiral had a corresponding difference of 30.45 dB. The difference for the 1-inch thick spiral was 42.59 dB. This data of course indicates that the thinner dielectric substrate provides the most profound change in gain between polarizations, suggesting that minimizing the substrate thickness will accentuate a change in polarization as frequency increases.
A factor that limits the number of signals that can be transmitted simultaneously is the frequency spectrum allotted to the application. Typically, providers pay huge sums of money to purchase the rights to use portions of the frequency spectrum. A broad band device that can double the number of users within a frequency band would be very advantageous.
The invention is a method and a device that uses the frequency spectrum more efficiently. The device described will at least double the number of users that can send signals within a particular frequency band. The invention includes a compact antenna with linear polarization and a broad frequency spectrum over which it can radiate efficiently. The conductor-backed spiral antenna described also has a 6 dB advantage in gain on transmit and receive over cavity-backed spiral antenna designs. These designs absorb half the power used via a lossy material in the cavity behind the spiral.
One feature of the conductor-backed spirals described is that if the thickness of the dielectric layer that separates the spiral antenna elements from the conductor is small compared to the utilized wavelength, the polarization of the antenna will be dependent on the frequency. The variation of the polarization depends upon both the thickness and the number of antenna element turns. This variation of the polarization with frequency presents the further advantage that two signals in the same antenna with slightly different frequencies will be somewhat isolated from each other. A given frequency band can thus be further divided into sub-bands using these antennas.
Obviously, many modifications and variations of the invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as has been described.
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