Patent Grant
6914575
1. Statement of the Technical Field
The present invention relates to the field of antennas, and more particularly to switchable sub-reflector antenna system using fluidic dielectrics.
2. Description of the Related Art
Typical satellite antenna systems use either parabolic reflectors or shaped reflectors to provide a specific beam coverage, or use a flat reflector system with an array of reflective printed patches or dipoles on the flat surface. These “reflect array” reflectors used in antennas are designed such that the reflective patches or dipoles shape the beam much like a shaped reflector or parabolic reflector would, but are much easier to manufacture and package on a spacecraft.
However, satellites typically are designed to provide a fixed satellite beam coverage for a given signal and may be limited in bandwidth by the structure of the reflectors and sub-reflectors. For example, Continental United States (CONUS) beams are designed to provide communications services to the entire continental United States. Once the satellite transmission system is designed and launched, changing the beam patterns to improve the operational bandwidth would be difficult.
The need to change the beam pattern provided by the satellite has become more desirable with the advent of direct broadcast satellites that provide communications services to specific areas and possibly on different frequency ranges. Without the ability to change beam patterns and coverage areas as well as to flexibly use multiple frequency ranges, additional satellites must be launched to provide the services to possible future subscribers, which increases the cost of delivering the services to existing customers.
Some existing systems are designed with minimal flexibility in the delivery of communications services. For example, a symmetrical Cassegrain antenna that uses a movable feed horn, defocuses the feed and zooms circular beams over a limited beam aspect ratio of 1:2.5. This scheme has high sidelobe gain and low beam-efficiency due to blockage by the feed horn and the subreflector of the Cassegrain system. Further, this type of system splits or bifurcates the main beam for beam aspect ratios greater than 2.5, resulting in low beam efficiency values. Other systems attempt to alter beam width and gain by using multiple feed horns. In any event, most of these systems will have a main reflected signal that will be interfered with by a sidelobe of the radiator or feed horn.
In another system as shown in
More specifically,
In any event, a programmable array such as the reflector array 206 can be reconfigured on-orbit. Satellites using the reflector array 206 can be designed for use in clear sky conditions, and, when necessary, the beams emanating from the reflector array 206 can be shaped to provide higher gains over geographic regions having rain or other poor transmission conditions, thus providing higher margins during clear sky conditions.
It can be seen, then, that there is a need in the art for an antenna system that can be alternatively reconfigured in-flight without the need for complex systems. It can also be seen that there is a need in the art for a communications system that can be reconfigured in-flight that has high beam-efficiencies and high beam aspect ratios. There is also a need for an antenna that is able to simply switch a sub-reflector on and off for use with multiple feed horns and that can optionally have the advantages of the antenna of FIG. 1 and other advantages as will be further described below utilizing fluidic dielectrics in accordance with the present invention.
Two important characteristics of dielectric materials are permittivity (sometimes called the relative permittivity or ∈r) and permeability (sometimes referred to as relative permeability or μr). The relative permittivity and permeability determine the propagation velocity of a signal, which is approximately inversely proportional to √{square root over (με)}. The propagation velocity directly affects the electrical length of a transmission line and therefore the amount of delay introduced to signals that traverse the line.
Further, ignoring loss, the characteristic impedance of a transmission line, such as stripline or microstrip, is equal to √{square root over (L1/C1)} where L1 is the inductance per unit length and C1 is the capacitance per unit length. The values of L1 and C1 are generally determined by the permittivity and the permeability of the dielectric material(s) used to separate the transmission line structures as well as the physical geometry and spacing of the line structures.
For a given geometry, an increase in dielectric permittivity or permeability necessary for providing increased time delay will generally cause the characteristic impedance of the line to change. However, this is not a problem where only a fixed delay is needed, since the geometry of the transmission line can be readily designed and fabricated to achieve the proper characteristic impedance. Analogously, wave propagation delays and energy beam patterns through dielectric materials in reflector and/or sub-reflector based antenna systems are typically designed accordingly with a fixed dielectric permittivity or permeability. When various time delays are needed for specific energy shaping or beam forming requirements, however, such techniques have traditionally been viewed as impractical because of the obvious difficulties in dynamically varying the permittivity and/or permeability of a dielectric board substrate material. Accordingly, the only practical solution has been to design variable delay lines using conventional fixed length RF transmission lines with delay variability achieved using a series of electronically controlled switches. Such schemes would be impracticable and overly complicated for a reflector or sub-reflector based antenna.
The invention concerns an antenna utilizing a reflector and/or sub-reflector which includes at least one cavity and the presence, absence or mixture of fluidic dielectric in the cavity. A pump or a composition processor, for example, can be used to add, remove, or mix the fluidic dielectric to the cavity in response to a control signal. A sub-reflector can be selectively activated using the fluidic dielectric to reflect a first radiated signal or pass a second radiated signal. Additionally, a propagation delay or beam pattern or gain of a radiated signal through the antenna can be selectively varied by manipulating the fluidic dielectric through the cavity or cavities.
The fluidic dielectric can be comprised of an industrial solvent. If higher permeability or conductivity is desired, the industrial solvent can have a suspension of magnetic or conductive particles contained therein. The aforementioned particles can be formed of a wide variety of materials including those selected from the group consisting of ferrite, metallic salts, and organo-metallic particles.
In accordance with a first embodiment of the present invention, a selectable sub-reflector antenna system comprises a main reflector unit, a sub-reflector unit disposed apart from the main reflector unit and having at least one cavity, and at least one fluidic dielectric having a permittivity and a permeability. The system further comprises at least one composition processor adapted for dynamically changing a composition of the fluidic dielectric to vary at least one among the permittivity and permeability in at least one cavity among a plurality of cavities and a controller for controlling said composition processor to selectively vary at least one among permittivity and permeability in at least one cavity in response to a control signal.
In accordance with a second embodiment of the present invention, a selectable sub-reflector antenna system comprises a main reflector unit, a sub-reflector unit disposed apart from the main reflector unit and having at least one cavity, and at least one fluidic dielectric having a permittivity and a permeability. The system in accordance with this second embodiment further comprises at least one fluidic pump unit for moving the fluidic dielectric among at least one cavity and a reservoir for adding and removing said fluid dielectric to at least one cavity in response to a control signal.
In yet another embodiment of the present invention, a method for selectively activating a sub-reflector in a reflector antenna system comprises the steps of reflecting a first radiated signal from the sub-reflector from a first source toward a main reflector in a first mode wherein the sub-reflector is activated using at least a fluidic dielectric and transmitting a second radiated signal through the sub-reflector from a second source toward the main reflector in a second mode wherein the sub-reflector is inactivated at least in part by changing the fluidic dielectric.
Although the antenna of
Referring to
The cavity or cavities in the sub-reflector primarily serves to selectively activate the sub-reflector 111 by reflecting a first radiated signal from the sub-reflector 111 from a first source such as feed horn 119 toward a main reflector 101 in a first mode wherein the sub-reflector 111 is activated using at least a fluidic dielectric. In a second mode, the sub-reflector 111 allows a second radiated signal from a second source such as feed horn 109 to transmit through the sub-reflector 111 toward the main reflector 101 wherein the sub-reflector is inactivated at least in part by changing the fluidic dielectric. By changing the fluidic dielectric, it is meant to be understood that the fluidic dielectric in at least a cavity of the sub-reflector is either completely or partially removed or that the mixture of fluidic dielectric material within the cavity is changed. The main reflector unit 101 is preferably spaced apart from a feed horn or radiator 109 that radiates towards the main reflector unit 101 (and through the sub-reflector unit 111 in the second mode. The sub-reflector unit 111 is preferably placed between a second feed horn or radiator 119 and the feed horn 119. The sub-reflector unit 111 in the first mode reflects a radiated from the feed horn 119 towards the main reflector unit 101.
It should be noted that the main reflector unit 101 can be completely be composed of a solid dielectric material or can further comprise at least one cavity or a plurality of cavities 106 that can contain at least one fluidic dielectric having a permittivity and a permeability. The cavities 106 can be a plurality of concentric tubes such as quartz capillary tubes on the outer periphery of the sub-reflector unit 101, although the invention is not limited to such arrangement in terms of cavities and construction. The fluidic dielectric can be moved in and out of the respective cavities using feed lines 107 and the pump or composition processor 104 for example. As previously described, the fluidic dielectric used in the cavities of the sub-reflector 111 and as optionally used in the main reflector unit 11 can be comprised of an industrial solvent having a suspension of magnetic or conductive particles. The particles are preferably formed of a material selected from the group consisting of ferrite, metallic salts, and organo-metallic particles although the invention is not limited to such compositions.
Referring again to
For the purpose of introducing time delay or energy shaping in accordance with one aspect of the present invention, the exact size, location and geometry of the cavity structure as well as the permittivity and permeability characteristics of the fluidic dielectric can play an important role. The energy shaping features are particularly applicable to the main reflector unit 101 in the present invention since the sub-reflector 111 preferably operates as a switch either reflecting or allowing a radiated signal through. Even so, the energy shaping concepts may equally be applicable to the sub-reflector 111 in particular applications. The processor and pump or flow control device (102 and 104) can be any suitable arrangement of valves and/or pumps as may be necessary to independently adjust the relative amount of fluidic dielectric contained in the cavities 106. Even a MEMS type pump device (not shown) can be interposed between the cavity and a reservoir for this purpose. However, those skilled in the art will readily appreciate that the invention is not so limited as MEMS type valves and/or larger scale pump and valve devices can also be used as would be recognized by those skilled in the art.
The flow control device can ideally cause the fluidic dielectric to completely or partially fill any or all of the cavities 106 (or cavities 416 in FIGS. 4 & 5). The flow control device can also cause the fluidic dielectric to be evacuated from the cavity into a reservoir (not shown). According to a preferred embodiment, each flow control device is preferably independently operable by controller 102 so that fluidic dielectric can be added or removed from selected ones of the cavities 106 to produce the required amount of delay indicated by a control signal 105.
Propagation delay of signals in the antenna system 100 can be controlled by selectively controlling the presence and removal or mixture of fluidic dielectric from the cavities 106. Since the propagation velocity of a signal is approximately inversely proportional to √{square root over (με)}, the different permittivity and/or permeability of the fluidic dielectric as compared to an empty cavity (or a cavity having a different mixture with different dielectric properties) will cause the propagation velocity (and therefore the amount of delay introduced)) to be different.
According to yet another embodiment of the invention, different ones of the cavities 106 can have different types of fluidic dielectric contained therein so as to produce different amounts of delay for RF signals traversing the antenna 100. For example, larger amounts of delay can be introduced by using fluidic dielectrics with proportionately higher values of permittivity and permeability. Using this technique, coarse and fine adjustments can be effected in the total amount of delay introduced or in the desired energy shaping of the radiated signal.
As previously noted, the invention is not limited to any particular type of structure. The cavities do not necessarily need to be tubes or in concentric arrangements as shown, but can be formed in various arrangements to accomplish the objectives of the present invention.
Composition of the Fluidic Dielectric
The fluidic dielectric can be comprised of any fluid composition having the required characteristics of permittivity and permeability as may be necessary for achieving a selected range of delay. Those skilled in the art will recognize that one or more component parts can be mixed together to produce a desired permeability and permittivity required for a particular time delay or radiated energy shape. In this regard, it will be readily appreciated that fluid miscibility can be a key consideration to ensure proper mixing of the component parts of the fluidic dielectric.
The fluidic dielectric also preferably has a relatively low loss tangent to minimize the amount of RF energy lost in the antenna. Aside from the foregoing constraints, there are relatively few limits on the range of materials that can be used to form the fluidic dielectric. Accordingly, those skilled in the art will recognize that the examples of suitable fluidic dielectrics as shall be disclosed herein are merely by way of example and are not intended to limit in any way the scope of the invention. Also, while component materials can be mixed in order to produce the fluidic dielectric as described herein, it should be noted that the invention is not so limited. Instead, the composition of the fluidic dielectric could be formed in other ways. All such techniques will be understood to be included within the scope of the invention.
Those skilled in the art will recognize that a nominal value of permittivity (εr) for fluids is approximately 2.0. However, the fluidic dielectric used herein can include fluids with higher values of permittivity. For example, the fluidic dielectric material could be selected to have a permittivity values of between 2.0 and about 58, depending upon the amount of delay or energy shape required.
Similarly, the fluidic dielectric can have a wide range of permeability values. High levels of magnetic permeability are commonly observed in magnetic metals such as Fe and Co. For example, solid alloys of these materials can exhibit levels of μr in excess of one thousand. By comparison, the permeability of fluids is nominally about 1.0 and they generally do not exhibit high levels of permeability. However, high permeability can be achieved in a fluid by introducing metal particles/elements to the fluid. For example typical magnetic fluids comprise suspensions of ferro-magnetic particles in a conventional industrial solvent such as water, toluene, mineral oil, silicone, and so on. Other types of magnetic particles include metallic salts, organo-metallic compounds, and other derivatives, although Fe and Co particles are most common. The size of the magnetic particles found in such systems is known to vary to some extent. However, particles sizes in the range of 1 nm to 20 μm are common. The composition of particles can be selected as necessary to achieve the required permeability in the final fluidic dielectric. Magnetic fluid compositions are typically between about 50% to 90% particles by weight. Increasing the number of particles will generally increase the permeability.
Example of materials that could be used to produce fluidic dielectric materials as described herein would include oil (low permittivity, low permeability), a solvent (high permittivity, low permeability) and a magnetic fluid, such as combination of a solvent and a ferrite (high permittivity and high permeability). A hydrocarbon dielectric oil such as Vacuum Pump Oil MSDS-12602 could be used to realize a low permittivity, low permeability fluid, low electrical loss fluid. A low permittivity, high permeability fluid may be realized by mixing same hydrocarbon fluid with magnetic particles such as magnetite manufactured by FerroTec Corporation of Nashua, N.H., or iron-nickel metal powders manufactured by Lord Corporation of Cary, N.C. for use in ferrofluids and magnetoresrictive (MR) fluids. Additional ingredients such as surfactants may be included to promote uniform dispersion of the particle. Fluids containing electrically conductive magnetic particles require a mix ratio low enough to ensure that no electrical path can be created in the mixture. Solvents such as formamide inherently posses a relatively high permittivity. Similar techniques could be used to produce fluidic dielectrics with higher permittivity. For example, fluid permittivity could be increased by adding high permittivity powders such as barium titanate manufactured by Ferro Corporation of Cleveland, Ohio. For broadband applications, the fluids would not have significant resonances over the frequency band of interest.
For conductive fluids, a liquid metal such as mercury or a solvent-electrolyte mixture could be employed. A system which relies on the presence or absence of a conductive fluid must ensure that no conductive residue remains in/on the walls of the fluid channels when the radome needs to be in the “RF transparent” state. It is believed that cases exist which illustrate that this condition can be met, in some instances with a passive system. An example is a commonly used mercury thermometer. As the mercury, which is a conductive liquid, is drawn down the tube in response to decreasing temperature the surface tension of the fluid draws all material along and does not leave “residue” or particulate matter on the sides of the transport tube. For other conductive fluids which may consist of particles in solution or suspension, an active purging system may be employed which uses a non-conductive fluid to flush the channel of any remaining conductive particles.
The antennas of
In either case, once the controller has determined the updated configuration for each of the cavities necessary to implement the time delay, the controller can operate device 104 to implement the required delay. The required configuration can be determined by one of several means. One method would be to calculate the total time delay for each cavity or for all the cavities at once. Given the permittivity and permeability of the fluid dielectrics in the cavities, and any surrounding solid dielectric (108 in
As an alternative to calculating the required configuration for a given delay or energy shape, the controller 102 could also make use of a look-up-table (LUT). The LUT can contain cross-reference information for determining control data for fluidic delay units necessary to achieve various different delay times and energy shapes. For example, a calibration process could be used to identify the specific digital control signal values communicated from controller 102 to the cavities that are necessary to achieve a specific delay value or energy shape. These digital control signal values could then be stored in the LUT. Thereafter, when control signal 105 is updated to a new requested delay time, the controller 102 can immediately obtain the corresponding digital control signal for producing the required delay.
As an alternative, or in addition to the foregoing methods, the controller 102 could make use of an empirical approach that injects a signal at an RF input port and measures the delay to an RF output port. Specifically, the controller 102 could check to see whether the appropriate time delay or energy shape had been achieved. A feedback loop could then be employed to control the flow control devices (104) to produce the desired delay characteristic.
The present invention is ideally applicable to any sub-reflector type antenna. Operationally, the present invention enables a system designer to alter the size of the reflective surface for a given application or frequency range and allows the use of multiple feed horns that normally would not operate appropriately on a single system by using a switch mechanism facilitated by the use of fluidic dielectric. The present invention adds further flexibility by controlling the reflection off the surface of the reflectors by dynamically changing the size of the surface with the fluidic dielectric. In essence, the reflector size can be made to vary based on the frequency or application as opposed to existing systems that are constructed on the basis of fixed frequencies since feeds are frequency dependent generally. In this manner, sidelobes created by different feed horns can each be independently averted and not reflected as required by manipulating the size of the reflectors or sub-reflectors using the fluidic dielectric. In one embodiment, when the fluidic dielectric is present, the reflector or sub-reflector is effectively extended in size and when the fluidic dielectric is removed the reflector or sub-reflector is effectively reduced in size.
Those skilled in the art will recognize that a wide variety of alternatives could be used to adjust the presence or absence or mixture of the fluid dielectric contained in each of the cavities. Additionally, those skilled in the art should also recognize that a wide variety of configurations in terms of cavities and reflectors or sub-reflectors could also be used with the present invention. The reflector or sub-reflector of the present invention can be assembled in a configuration that resembles a reflector in forms such as parabolic, circular, flat, etc, depending on the desires of the designer for the available or desired beam patterns antenna. Accordingly, the specific implementations described herein are intended to be merely examples and should not be construed as limiting the invention.
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| Number | Date | Country | |
|---|---|---|---|
| 20050030240 A1 | Feb 2005 | US |
