Tunable patch antenna

Abstract
A patch antenna is composed of a segmented patch and MEMS switches which are built on a substrate. The patch segments of the segmented patch can be electrically connected to each other by the MEMS switches to form a contiguous patch and optional tuning strips and to connect or block RF between the contiguous patch and the optional tuning strips. When RF is connected between the tuning strips and the contiguous patch, the tuning strips increase the effective length of the contiguous patch and lower the antenna's resonant frequency, thereby allowing the antenna to be frequency tuned electrically over a relatively broadband of frequencies. When the tuning strips are connected to the patch in other than a symmetrical pattern, the antenna pattern of the antenna can be changed. In another aspect of the invention, the optional tuning strips are continuous structures that are formed by connecting patch segments using switches. A planar inverted F antenna (PIFA) is also provided with one or more tuning strips spaced from the lid of the PIFA and with switches to connect or block RF between the lid of the PIFA and the tuning strips.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to patch antennas, and more particularly, to tunable patch antennas with a patch and switches to one or more tuning strips which when coupled to the patch by the switches adjust the antenna resonant frequency.




2. Description of Related Art




Many applications require small, light weight, efficient conformal antennas. Traditionally microstrip patch antennas have been a preferred type for many applications. These applications tend to be only over a narrow frequency band, since microstrip patch antennas typically are efficient only in a narrow frequency band. Otherwise, the advantages of these antennas of being mountable in a small space, of having high efficiency and of being capable of being constructed in a rugged form, have made them the antennas of choice in many applications.




Satellite communication (Satcom) systems and other similar communications systems require relatively broadband antennas. Typical military broadband applications include long range communication links for smart weapon targeting and real time mission planning and reporting. A variety of antenna designs, such as crossed slots, spirals, cavity-backed turnstiles, and dipole/monopole hybrids have been used for similar applications over at least the last 15 years. However, most of these antennas require large installation footprints, typically for UHF antennas, a square which is two to three feet on a side. When used on aircraft, these antennas intrude into the aircraft by as much as 12 inches and can-protrude into the airstream as much as 14 inches. For airborne Satcom applications, antennas of this size are unacceptably large, especially on smaller aircraft, and difficult to hide on larger aircraft, where it is undesirable to advertise the presence of a UHF Satcom capability. Therefore, there has been a need for small highly efficient broadband or frequency-reconfigurable narrowband antennas, not just in these applications, but in many other new and different commercial applications. For example, one possible application is a multiband multimode mobile phone that operates in the GSM 900 MHz, PCS 1900 MHz, and DES 1800 MHz bands, although not simultaneously.




SUMMARY OF THE INVENTION




A patch antenna is composed of a segmented patch and MEMS switches which are built on a substrate. The patch segments of the segmented patch can be electrically connected to each other by the MEMS switches to form a contiguous patch and optional tuning strips and to permit or block the flow of RF currents between the contiguous patch and the optional tuning strips. When RF is connected between the tuning strips and the contiguous patch, the tuning strips increase the effective length of the contiguous patch and lower the antenna's resonant frequency, thereby allowing the antenna to be frequency tuned electrically over a relatively broadband of frequencies. When the tuning strips are connected to the patch in other than a symmetrical pattern, the antenna pattern of the antenna can be changed. In another aspect of the invention, fine tuning in accordance with desired frequency, input impedance and/or polarization can be achieved by selectively connecting patch segments in reconfigurable patterns using switches. A planar inverted F antenna (PIFA) is also provided with one or more tuning strips spaced from the lid of the PIFA and with switches to connect or block RF between the lid of the PIFA and the tuning strips.











BRIEF DESCRIPTION OF THE DRAWINGS




These and other objects and advantages of the present invention will become apparent to those skilled in the art after considering the following detailed specification, together with the accompanying drawings wherein:





FIG. 1

is a perspective view of a prior art microstrip patch antenna;





FIG. 2

is a cross sectional view taken along the y-axis of FIG.


1


.





FIG. 3

is a top plan view of the antenna of

FIG. 1

showing the virtual radiating slots thereof;





FIG. 4

is a top plan view of a dual feed embodiment of the antenna of

FIG. 1

;





FIG. 5

is a partial diagrammatic plan view of an antenna constructed according to the present invention, showing a switch configuration thereof;





FIG. 6

is a top plan view showing how the tuning strips of an embodiment of the present invention can be connected to the patch thereof;





FIG. 7

is a graph of typical Frequency vs. Return Loss for various tuning states of the antenna of

FIG. 6

, where the frequency subscript designates the particular tuning strips electrically connected to the patch;





FIG. 8

is a graph of Frequency vs. Return Loss for the antenna of

FIG. 9

, which can be finely tuned;





FIG. 9

is a partial top plan view of the tuning strips and patch of an antenna constructed according to the present invention, showing how tuning strips are positioned and spaced when the antenna is to be finely tuned at frequencies near the resonant frequency of the patch alone;





FIG. 10

is a partial top plan view of the tuning strips and patch of an antenna constructed according to the present invention, showing how tuning strips are positioned and spaced when the antenna is to cover a broad RF frequency band;





FIG. 11

is a graph of Frequency vs. Return Loss for various tuning states of the antenna of

FIG. 10

;





FIG. 12

is a partial diagrammatic plan view of an antenna constructed according to the present invention, showing an alternate switch configuration thereof;





FIG. 13

is a partial diagrammatic plan view of an antenna constructed according to the present invention, showing an alternate switch configuration thereof that grounds the tuning strips rather than connects them to the patch, useful when the strips capacitively couple to the patch;





FIG. 14

is a top plan view of an antenna constructed according to the present invention, with its switch circuits, leads, and RF feeds;





FIG. 15

is a side cross-sectional view taken at line


15





15


of

FIG. 14

;





FIG. 16

is a circuit diagram of a switching circuit for connecting and disconnecting a tuning strip to the patch of the present antenna;





FIG. 17

is a circuit diagram of another switching circuit for connecting and disconnecting a tuning strip to the patch of the present antenna;





FIGS. 18 and 19

are equivalent circuit diagrams for the switching circuit of

FIG. 16

when the circuit is connecting the patch to the tuning strip;





FIGS. 20 and 21

are equivalent circuit diagrams for the switching circuit of

FIG. 16

when the circuit is disconnecting the patch from the tuning strip;





FIG. 22

is an equivalent circuit diagram for the switching circuit of

FIG. 17

showing how a tuned filter is formed thereby;





FIG. 23

is a top plan view of a broadband antenna being constructed according to the present invention with some of the switching circuits of

FIG. 16

being in place thereon;





FIG. 24

is an enlarged cross-sectional view of an alternate arrangement to form the switching circuit of

FIG. 16

on the antenna of

FIG. 23

;





FIG. 25A

is a top plan view of an antenna constructed according to the present invention with a two feed circular patch and segmented concentric tuning strips;





FIG. 25B

is a top plan view of a modified version of the antenna of

FIG. 25A

with an oval patch and segmented concentric tuning strips;





FIG. 26

is a top plan view of an antenna constructed according to the present invention with a center fed circular patch and concentric tuning strips;





FIG. 27

is a top plan view of an antenna constructed according to the present invention with a triple feed triangular patch and uneven numbers of tuning strips spaced from the edges of the patch;





FIG. 28

is a top plan view of a pair of antennas elements constructed according to the present invention positioned back-to-back to form a frequency tunable dipole antenna;





FIG. 29A

illustrates an integrated patch antenna with MEMS switches;





FIGS. 29B-G

illustrate various MEMs connection configurations to reconfigure a TPA, such as the one illustrated in greater detail in

FIG. 29A

, to achieve both coarse and fine tuning of desired operating frequency, input impedance, and polarization;





FIG. 30

illustrates a tunable planar inverted F antenna (PIFA); and





FIG. 31

illustrates a PIFA antenna with digitally related capacitive tuning bars.











DETAILED DESCRIPTION OF THE INVENTION




Referring to the drawings more particularly by reference numbers, number


20


in

FIG. 1

refers to a prior art patch antenna that includes a conducting ground plane


22


, a conducting patch


24


and a dielectric spacer


26


spacing the patch


24


parallel to and spaced from the ground plane


22


. Suitable feed means


28


electrically insulated from the ground plane


22


, extends therethrough and through the dielectric spacer


26


to feed RF energy to the patch


24


. Although the patch


24


is shown as square or rectangular in shape, it is also quite common to have circular patches either center fed or fed adjacent the edge as feed


28


is positioned. For any patch antenna operating in the lowest order mode, Tm


11


for a circular patch and the order mode TE


10


for a rectangular patch, a linearly polarized radiation pattern can be generated by exciting the patch


24


at a single feed point such as feed point


28


. For antenna


20


, which has a square patch that is a special case of a rectangular patch, the patch


24


generates a linearly polarized pattern with the polarization aligned with the y-axis. This can be understood by visualizing the antenna


20


as a resonant cavity


30


formed by the ground plane


22


and the patch


24


with open side walls as shown in FIG.


2


. When excited at its lowest resonant frequency, the cavity


30


produces a standing half wave


31


(λ/2) when operating at the lowest order mode as shown, with fringing electric fields


32


and


34


at the edges


36


and


38


that appear as radiating slots


40


and


42


(FIG.


3


). This electric field configuration has all field lines parallel with the y-axis and hence produces radiation with linear polarization. When a feed


44


is located on the x-axis as shown in

FIG. 4

, all electric field lines are aligned with the x-axis. If two feeds


28


and


44


are present simultaneously, one on the x-axis and the other on the y-axis as shown in

FIG. 4

, then two orthogonal electric fields are generated. Because the fields are orthogonal, they do not couple or otherwise affect each other and circular polarization results if the feeds are fed at 90° relative phase. With two feeds


28


and


44


, four polarization senses can be generated. When feed


44


alone is used, there is linear horizontal polarization. When feed


28


only is used, there is linear vertical polarization. When feeds


28


and


44


are activated with feed


28


90° in phase behind feed


44


, then the antenna


20


radiates RF signals with right hand circular polarization. When feed


28


is fed 90° ahead of feed point


44


, left hand circular polarization results. Therefore, with two feeds and the ability to switch between them, any of the four polarizations can be generated from a single antenna


20


.




As shown in

FIG. 2

, the maximum electric field is positioned at the edges


36


and


38


of the patch


24


whereas the minimum electric field occurs at the center


45


of the patch


24


. At some intermediate positions between the center


45


and the edges of the patch


24


, impedances occur that may match the characteristic impedance of the transmission line of feed


28


. The feeds


28


and


44


are preferably placed so the impedances perfectly match.




A simplified antenna


50


constructed according to the present invention is shown in

FIG. 5

with only one polarization shown for simplicity. The antenna


50


and other antennas constructed in accordance with the present invention to be described hereinafter, are shown on a planar ground plane even though all of the present antennas can be curved within reason to conform to curved or compound curved surfaces of air vehicles or other supporting structures on or in which they may be mounted. The antenna


50


includes a patch


51


with three equally-spaced tuning bars or strips


52


,


54


,


56


and


58


,


60


and


62


on opposite sides


64


and


66


of the patch


51


The resonant frequency of the antenna


50


is inversely proportional to the total effective patch length, that is the length of the patch


51


plus any of the strips


52


through


62


connected thereto. Therefore, the highest resonant frequency of the antenna


50


occurs when all of the strips


52


through


62


are disconnected from the patch


51


. Possible operating states that can be generated with antenna


50


include f


highest


(f


0


) for just the patch


51


, f


mid-high


(F


1


) for the patch


51


with strips


52


and


58


connected, f


highest


(f


21


) for the patch


51


with strips


52


,


54


,


58


and


60


connected and f


lowest


(f


321


) for the patch


51


with all of the strips


52


through


62


connected. However, the antenna


50


can be used with some of the outermost strips like


56


and


62


connected and the remaining strips disconnected (

FIG. 6

) to produce an operating frequency f


3


somewhat higher than f


lowest


(f


321


) as shown in

FIG. 7

, which is a graph of return loss versus frequency. Another possible configuration has the patch


51


connected to strips


54


,


56


,


60


and


62


but not strips


52


and


58


to produce a frequency f


32


just above f


lowest


. The extra frequencies that are possible by connecting different combinations of strips allow antennas of the present invention to be designed with fewer tuning strips and connecting components, while still providing continuous coverage over the frequency range of interest.




The tuning strips do not have to be equally spaced and fewer more widely spaced strips make the present antenna simpler and less costly to build. For the high frequency tuning states that employ only the innermost strips, these extra tuning states are less available. For example, if the frequency coverage shown in

FIG. 8

is required, a patch


70


of the antenna


71


with closely spaced tuning strips


72


,


73


,


74


and


75


can be used (FIG.


9


). The strips


72


and


74


must be located sufficiently close to the patch


71


that frequency f


1


is generated. Any combination of other strips located further from the patch


71


will generate an operating frequency lower than f


1


. Similarly, tuning strips


73


and


75


will generate the next lowest frequency f


2


. Therefore, a broadband design may appear as shown in

FIG. 10

by antenna


80


, which includes patch


81


and tuning strips


82


,


83


,


84


,


85


,


86


,


87


,


88


and


89


. Note the narrow spacing between the patch


81


and the strips


82


and


86


and then that the spacing increases outwardly as shown on

FIG. 11

, so a relatively even spread of frequencies can be obtained either by using individual strips or combinations, the frequencies being shown with subscript numbers indicating the connected strips counting outwardly from the patch


81


. The resonant frequency of patch


81


alone is f


0


.




As shown in

FIGS. 5

,


12


and


13


, the tuning strips


52


,


54


and


56


can be coupled to the patch


51


by different switching arrangements. In

FIG. 5

, switches


100


,


101


and


102


connect the tuning strips


52


,


54


and


56


in parallel to the patch


51


so that any combination can be connected thereto. If only the strips


52


,


54


, and


56


are connected to the patch


51


, the effect is to move the feed


103


percentage wise closer to the edge


66


to affect the antenna pattern and/or impedance match. In

FIG. 12

, switches


105


,


106


, and


107


connect the tuning strips


52


,


54


and


56


in series. In this configuration, an interior tuning strip cannot be skipped to tune between what would normally be tuning strip frequencies.




At high frequencies, the strips preferably are positioned very close together because they must be wide enough to carry the RF currents yet located at small distances from the patch. When they are positioned close to the patch, capacitance therebetween is high enough to couple RF between the strips and the patch and make the connection circuitry of

FIGS. 5 and 12

ineffective to isolate the strips from the patch. Therefore, as shown in

FIG. 13

, switches


108


,


109


and


110


are connected so they can ground the tuning strips


52


,


54


and


56


, which otherwise capacitively couple to the patch


51


. In some instances, the switch connections of FIG.


13


and either

FIGS. 5

or


12


may need to be combined to get desired coupling and decoupling of the strips and the patch.




A microstrip patch antenna


120


constructed according to the present invention, whose thickness is exaggerated for clarity, can be seen in FIG.


14


. The antenna


120


includes a conductive ground plane


122


and a square patch


124


supported and insulated from the ground plane


122


by a dielectric spacer


126


. The patch


124


is fed by two leads


128


and


130


, which are physically positioned at 90° to each other about the center hole


131


(

FIG. 15

) of the patch


124


. When the antenna


120


is transmitting, the leads


128


and


130


connect RF signals that are electrically 90° degrees apart in phase to the patch


124


to produce circular polarization. As previously discussed, this causes the polarization of the antenna


120


to be right hand circular if lead


128


is fed 90° ahead of lead


130


. If the phase difference of the leads


128


and


130


is reversed, the antenna


120


produces an output with left hand circular polarization. If the antenna


120


is oriented as shown in

FIG. 15

at 90° to the earth


131


, and only lead


130


is fed, then the antenna


120


produces an output signal with a linear horizontal polarization. When only lead


128


is feeding the antenna


120


, then an output signal with a linear vertical polarization is produced. As shown in

FIG. 15

, a suitable connector


132


is provided on each of the leads


128


and


130


for connection to RF producing or receiving means, the leads


128


and


130


being insulated or spaced from the ground plane


122


, as shown. Note that other connection means may be employed in place of the connector


132


, such as microstrip lines, coplanar waveguide, coupling apertures, and the like.




As aforesaid, relatively conventional patch antennas employing a patch


124


above a ground plane


122


and fed as described, are fairly conventional, efficient narrow frequency band devices. To increase the frequency coverage of the antenna


120


without affecting its antenna pattern, operation modes, or polarization, conductive frequency broadening strips are positioned on the spacer


126


parallel to and spaced from the patch


124


with strips


134


and


136


positioned near the lower edge


138


of the patch


124


, strips


140


and


142


positioned near the right edge


144


of the patch


124


, strips


146


and


148


positioned near the upper edge


150


of the patch


124


, and strips


152


and


154


positioned near the left edge


156


of the patch


124


.




When the strips


134


,


140


,


146


and


152


are connected by switch means


155


to the RF frequencies present at the patch


124


, they effectively enlarge the patch


124


without changing its shape and thereby lower its resonant frequency. If in addition strips


136


,


142


,


148


and


154


are also connected to the patch


124


, this further lowers the resonant frequency of the antenna


120


. Intermediate frequencies can be gained by connecting only strips


136


,


142


,


148


and


154


to the patch


124


which has the effect of lowering the resonant frequency of the antenna


120


but not so much as if all strips were connected. In addition to changing the resonant frequency, the pattern of the antenna


120


can be changed by connecting the patch


124


to only opposite pairs of strips or connecting only the strips on one edge, adjacent edges or three edges. This allows the antenna pattern to be directed in a chosen direction to reduce an interfering signal near or at the frequency of interest. With the symmetrical antenna


120


, in almost every combination, the connecting of the strips adjusts the resonant frequency of the antenna and/or adjusts its radiation pattern. With a non-symmetrical antenna of the present invention, it is difficult to change the resonant frequency without changing the antenna pattern.




The patch


124


can be connected to the strips


134


,


136


,


140


,


142


,


146


,


148


,


152


, and


154


by suitable means such as electronic switches, diodes, field effect transistors (FETs), EM relays and other electronic devices. Preferable circuits


159


and


160


are shown in

FIGS. 16 and 17

where PIN diodes are biased to either conduct or not conduct with a DC signal to connect or disconnect a strip to the patch


124


. A positive/negative DC power source


161


is used to bias diodes


162


and


164


either into conducting or nonconducting conditions. When both diodes


162


and


164


are biased by a positive current from the power source


161


to conduct, the strip


140


is connected to any RF signal on the patch


124


and acts to expand the length thereof and thus lower the resonant frequency of the patch


124


. The RF signal passes through a DC blocking capacitor


165


whose capacitance is chosen to act like a short to RF in the frequency band of interest. The RF signal then passes through the diode


164


(which when forward biased appears as a very low resistance of 0.5Ω), to the strip


140


, and through the diode


162


connected between the patch


124


and the strip


140


. Balancing resistors


166


and


168


are positioned in parallel to the diodes


162


and


164


respectively. Their resistances are chosen to be relatively high (typically 20 to 500 KΩ). They have no effect when the diodes


162


and


164


are conducting since the impedance of the diodes


162


and


164


is 40,000 times less, the equivalent circuit at RF being shown in FIG.


18


. Since the 0.5Ω diodes


162


and


164


are so much lower in impedance than the 20 KΩ resistors


166


and


168


, virtually all the RF current flows through the 0.5Ω diodes


162


and


164


, and the 20 KΩ resistors


166


and


168


act like open circuits as shown in FIG.


19


. However, when the power source


161


reverse biases the diodes


162


and


164


, the diodes


162


and


164


present a very high resistance of 1 MΩ or more, as shown in the equivalent circuits of FIG.


20


. The circuit is then a voltage divider. If the diodes


162


and


164


are identical in reverse bias impedance, then the resistors


166


and


168


are not needed because an equal voltage drop occurs across each diode


162


and


164


. However, economical bench stock diodes can have an impedance difference as much as 1 MΩ. Therefore, as shown in

FIG. 20

, the diodes


162


and


164


if mismatched, become components in an unbalanced impedance bridge, which might allow a RF signal to appear on the strip


140


. With diode


162


having a reverse bias impedance of 1 MΩ and diode


164


having a reverse bias impedance of 2 MΩ, the voltage division created may not be enough to keep diode


162


biased off when RF is fed to the patch


124


. The balancing resistors


166


and


168


avoid the problem by greatly reducing the effect of mismatched diodes since the parallel impedance of 1 MΩ diode


162


and 20 KΩ resistor


166


is 19.6 KΩ, whereas the parallel impedance of 2 MΩ diode


164


and 20 KΩ resistor


168


is 19.8 KΩ resulting in an insignificant voltage division of 49.75% to 50.25% across the diodes


162


and


164


respectively. An RF blocking coil


170


is used to complete the DC circuit to the power source


161


without allowing RF to ground out therethrough.




Another connection circuit


160


for connecting the patch


124


to strip


140


utilizing diodes


182


and


184


is shown in

FIG. 17

wherein PIN diodes


182


and


184


are connected oriented in the same direction in parallel between the patch


124


and the strip


140


to avoid voltage division there between. The circuit


160


includes a capacitor


186


of a capacitance chosen to be a short circuit at RF frequencies and an open circuit at DC and an inductor


188


chosen such that, when combined with the parasitic capacitances of the diodes


182


and


184


, the capacitor


186


and inductor


188


form a parallel resonant circuit


189


(FIG.


22


). The series connected capacitor


186


and inductor


188


are fed DC therebetween by a DC power source


190


similar to the source


161


, which can provide both positive and negative DC current thereto. The patch configuration is essentially the same for the parallel diode circuit


160


as for the series diode circuit


159


as to patch size, number of strips and strips facing. When forward biased by the power source


190


, the diodes


182


and


184


conduct from the strip


140


to the patch


124


in a DC sense, thereby forming a low resistance RF path. The advantage of circuit


160


over circuit


159


is that the resistors


166


and


168


are no longer required because the applied voltage is no longer divided between the two diodes


182


and


184


. Also, each diode


182


and


184


is reverse biased by the entire output of the power source


190


as opposed to approximately ½ as in the case of circuit


159


. This increases the bias voltage allowing the antenna to handle higher RF power or allows a more economical lower power source


190


to be employed.




The partially constructed antenna


200


of

FIG. 23

shows a typical embodiment of the present invention with the switching circuits


159


thereon. Like the aforementioned antennas, antenna


200


includes a patch


202


having feeds


204


and


206


symmetrically positioned at 90° with respect to each other and on the horizontal and vertical axis of the patch


202


. A plurality of spaced tuning strips


208


are symmetrically placed around the square patch


202


so that they can effectively increase its size when connected to the patch


202


by the switching circuits


159


, one of which switching circuits


159


having the appropriate component numbers indicated, for connecting tuning strip


209


to the patch


202


. Note that some of the leads


210


and


212


connecting to the tuning strip


209


extend outwardly beyond the tuning strip


209


. The stubs


214


and


216


that result allow fine tuning of the antenna


200


once it has been constructed and can be tested. The stubs


214


and


216


are intentionally made longer than needed and then trimmed off to raise the resonant frequency of the antenna


200


when the strip


209


is connected.




The tuning circuits


159


are connected to the power source


161


by suitable leads, such as lead


218


, which is shown extending through a center orifice


220


included for that purpose. As shown in

FIG. 24

, the lead


218


can also be fed through an insulator


222


that extends through the ground plane


224


and the patch


202


to connect to the capacitor


165


, the diode


164


and the resistor


168


. The lead


218


could also be an insulated plated-through hole.




As the patch


202


is effectively enlarged by the addition of tuning strips with similar enlargement of the electric field standing wave (see FIG.


2


), when the patch is enlarged uniformly, the impedance matches of the feeds


204


and


206


change. The original construction of the antenna


200


can be compromised for this by positioning the feeds


204


and


206


toward the strips so that a perfect impedance match occurs when some of the strips are connected symmetrically, or the strips can be connected asymmetrically so that as the effective patch size of the antenna increases, the effective center of the patch shifts away from the feed to keep its impedance matched. Additional strips


208


on the opposite edge from the feeds


204


and


206


can also be added so that strips can be asymmetrically added over the entire frequency band of the antenna. Which method is used for feed impedance matching in some measure depends on the ability of the connected transmitter or receiver to tolerate antenna feed mismatch and physical constraints that might prevent additional strips on sides opposite from the feeds


204


and


206


. Whether any correction for impedance match changes is needed depends on the bandwidth being covered. Experiments have shown that no correction is required for the Satcom band discussed above.




Although the invention has been described primarily with square patch antennas, other shapes are possible. For example, in

FIG. 25A

, a circular antenna


230


is shown mounted over a square dielectric spacer


232


and ground plane


234


. The antenna


230


includes a circular patch


236


with two feeds


238


and


240


for polarization control as in the square patch antennas previously described. Two rings of segmented concentric tuning strips


242


and


244


are used to lower the resonant frequency of the antenna


230


.

FIG. 25B

shows a similar antenna


230


′ where the patch


236


′ and rings of segmented tuning strips


242


′ and


244


′ are oval, showing that the shape of the patches


236


and


236


′ can be said to be shaped as a plane section of a right circular cone. Another configuration of a circular antenna


250


including the present invention is shown in FIG.


26


. The antenna


250


has a central feed


252


and concentric tuning rings


254


and


256


surrounding the patch


258


. The antenna


250


therefore has no means to vary the polarization or the antenna pattern, the tuning rings


254


and


256


only being useful in reducing the resonant frequency of the antenna


250


.




As shown in

FIG. 27

, almost any configuration of patches and tuning strips can be employed for special purposes. The antenna


270


of

FIG. 27

includes a triangular patch


272


with three feeds


274


,


276


and


278


positioned in the corners thereof. The feeds


274


,


276


and


278


can be fed out of phase or fed all in the same phase so that they act like a center feed. Note that the upper sides of the triangular patch


272


have associated single tuning strips


280


and


282


while two tuning strips


284


and


286


are provided at the lower edge


288


. This configuration would be used if low frequencies are only required with a directed antenna pattern.




The antenna


300


shown in

FIG. 28

is essentially two of the present antennas


302


and


304


positioned back-to-back to form a tunable dipole antenna


300


.





FIG. 29A

illustrates an integrated patch antenna with MEMS switches in accordance with certain aspects of the invention. As shown in

FIG. 29A

, antenna


400


includes segmented patch


402


composed of a grid or array of conducting (metallic) plates


404


which are connected to each other for communicating RF energy therebetween by a system of MEMS switches


406


which are fabricated on the same substrate


408


as plates


404


. Substrate


408


can be a semiconductor or other material, including circuit-board material such as alumina. Substrate


408


is disposed over a ground plane


410


. A coaxial or microstrip feedpoint


412


terminates on one of the plates


404


and thereby provides a feed for RF energy to the antenna


400


. In order to not obscure the invention, the control lines and the bias lines to the switches are not shown. With suitable means of addressing and controlling the individual MEMS switches, using techniques adapted from U.S. Pat. No. 6,061,025, for example, the integrated plates and switches of antenna


400


can be connected together to produce patch antennas of various sizes and shapes, to control antenna resonant frequency, polarization, input impedance, and to some degree antenna pattern shape.




It should be noted that the drawing in

FIG. 29A

is not necessarily to scale, particularly with respect to the size of the MEMS switches versus the plate size, separation between plates, etc. According to an aspect of the present invention for providing fine tuning of various parameters, however, the plate size is very small with respect to the wavelength of the desired antenna application, such as {fraction (1/10)} to {fraction (1/100)} of wavelength (i.e. λ


d


, or wavelength in the dielectric). Certain aspects of such fine tuning will be described hereinbelow.




While the plates


404


shown in

FIG. 29A

are of equal size, it should be appreciated that in alternative embodiments plates


404


can be of unequal size. For example, the length of each plate may depend on its distance from the center of the segmented patch. Additionally, while only one feedpoint is shown in

FIG. 29A

, it should be appreciated that in alternative embodiments there can be two or more feedpoints. For example, a dual polarized antenna can be constructed with antenna


400


that has two feed points.




While the plates


404


shown in

FIG. 29A

are in the shape of a square or rectangle, it should be appreciated that in alternative embodiments plates


404


can have arcuate or angular shapes such that structures such as those in

FIG. 25A

,

FIG. 25B

,

FIG. 26

,

FIG. 27

can be constructed by appropriately turning on switches.




It should be noted that, with appropriate control, certain of plates


404


can be coupled to non-adjacent plates. In this regard, although

FIG. 29A

shows all the plates being capable of being coupled to only adjacent plates using switches


406


, constructing connectors to provide interconnection and bias lines at different layers in a substrate is well understood in the art of semiconductor processing and need not be described here.




From this observation, it should be appreciated that the plates can be coupled together using switches


406


to make both a patch from a fraction of the plates and tuning strips displaced from the patch using certain of the remaining fraction of the plates. For example, plate


413




a


can be coupled to plate


414




a


and the plates in column


414


can be connected to each other to form the outer edge of a patch or alternatively plate


413




a


and the other plates in column


413


can be connected to each other to form the outer edge of a patch. For example, plate


413




b


can be coupled to plate


415




b


via an appropriate connector. Further, plate


413




c


can be coupled to plate


416




c


via an appropriate connector. In this manner, plates can singly or in pairs be used for fine control. Alternatively, various numbers of plates in column


415


can be coupled together or various numbers of plates in column


416


can be coupled together.




While in the description provided above, the patch and the tuning strips have straight edges, it should be appreciated that patches and tuning strips that are roughly arcuate in shape are encompassed by the teachings of this invention. For example, a patch can be in the general shape of a circle or an ellipse or some other curved shape. A tuning strip can be in the general shape of a ring or arcuate segments.





FIGS. 29B-G

illustrate various MEMs connection configurations to reconfigure a TPA, such as the one illustrated in greater detail in

FIG. 29A

, to achieve both coarse and fine tuning of desired operating frequency, input impedance, and polarization.

FIGS. 29B and 29C

illustrate that the input impedance of an antenna is affected by the distribution of patches around the feed point. For example, as shown in

FIG. 29C

, a row of patches further away from the feed point is not connected to the patches that are connected to the feed point, causing the impedance to increase relative to the configuration in

FIG. 29B

where a row of patches near the feed point is not connected to the patches that are connected to the feed point.




In

FIG. 29D

the operating frequency is increased relative to the configurations in

FIGS. 29B and 29C

by decreasing the size of the antenna (i.e., decreasing the number of patches connected to the feed point).





FIG. 29E

illustrates that the polarization may be changed by changing the dominant direction in which the patches are distributed relative to the feed point. It should be appreciated that the patches connected to the feed point are distributed more along the x-axis, resulting in a corresponding polarization in the x direction for the dominant mode. The operating frequency and input impedance are the same as in the configuration described in connection with

FIG. 29B

, but the polarization is in the x direction.





FIG. 29F

illustrates an asymmetrical distribution of connected patches around the feed point. Consequently, an elliptical polarization results. It should be appreciated that a circular polarization is also possible and that many other possible configurations are possible.





FIG. 29G

illustrates a technique for fine tuning both operating frequency and polarization by creating gaps or slots. By selectively disconnecting patches so as to create a gap or slot within a patch network, the operating frequency can be raised or lowered relative to the original network. Further, fine tuning of polarization in the y direction is also achieved. This technique can be used with any of the preceding

FIGS. 29B-F

.





FIG. 30

illustrates a tunable planar inverted F antenna (PIFA) according to certain other aspects of the present invention. As shown in

FIG. 30

, antenna


500


includes a PIFA lid


502


, a shorting wall


504


, a ground plane


506


, and tuning strips


507




a


,


507




b


, and


507




c


. RF energy is fed into antenna


500


through feed


512


. The direction of the dominant mode electric field is from ground plane


506


up to PIFA lid


502


, and standing waves run the length of the lid


502


, between shorting wall


504


and radiating aperture


508


. One of ordinary skill in the art would understand that the PIFA lid, shorting wall and feed can be together considered a radiating element, but a PIFA is typically used with a truncated ground plane, not much larger than the lid, in which case, the whole combination is the radiating element.




It should be noted that

FIG. 30

shows a shorting wall


504


that is coextensive with the patch or lid


502


for coupling the lid to the ground plane


506


, thereby permitting the resonant frequency of the antenna to be reduced without increasing the antenna size. However, other alternatives to the shorting wall


504


shown in

FIG. 30

are possible. For example, the wall need not be the same length as the edge of the lid to which it is coupled. As another example, the shorting element may be comprised of a plated through hole or via through the antenna dielectric layer that acts as a shorting pin between the lid and the ground plane.




Referring back to

FIG. 30

, switches


510


can selectively connect one or more of tuning strips


507




a


,


507




b


, and


507




c


to lid


502


, increasing the length of lid


502


and decreasing the resonant frequency of antenna


500


. Switches


510


components include PIN diodes, FETs, bulk switchable semiconductors, relays, mechanical switches, and microelectromechanical systems (MEMS) switches as described herein.




While in the description provided in connection with

FIG. 30

, lid


502


is a solid patch and the tuning strips each comprise a single solid segment, it should be appreciated that in an alternative embodiment, lid


502


and tuning strips


507




a


-


507




c


can be constructed in accordance with the description provided in connection with

FIG. 29A

where a segmented patch is used to make both a patch and a tuning strip. In a further alternative using patch segments, in place of a shorting wall, a shorting pin comprised of a via or plated through hole can be coupled between the ground plane and an arbitrary one of the patch segments.




It should be further noted that, although the tuning strips


507


in

FIG. 30

are shown as being the same size, the invention is not limited thereto, and strips of different sizes are possible.

FIG. 31

illustrates a top view of an alternative embodiment of a PIFA antenna such as that shown in FIG.


30


. In this example, PIFA lid


502


′ is coupled to tuning strips


507


′ by respective switches. In this example, the tuning strips


507


′ are digitally-related capacitive tuning bars, comprised of n conducting patches of sizes and positions such that


2




n


tuning states can be created by selecting and connecting the patches in accordance with a digital word. For example, 3 patches of relative areas


1


,


2


, and


4


(as shown in

FIG. 31

) (i.e. a first patch has a relative size of 1, another patch has a relative size of 2 times that of the first patch, and a third patch has a relative size of 4 times the first patch) may enable


8


tuning states corresponding to switch states “000” through “111,” where a “1” is a closed switch. For this, the smallest patch is selected to create a first small frequency shift, the next larger patch creates a larger shift, and the combination of these two results in an even larger shift, and so on. This arrangement provides certain additional advantages over the previously described tuning strips, such as simplified tuning and control.




Thus, there has been shown and described novel antennas which fulfill all of the objects and advantages sought therefor. Many changes, alterations, modifications and other uses and application of the subject antennas will become apparent to those skilled in the art after considering the specification together with the accompanying drawings. All such changes, alterations and modifications which do not depart from the spirit and scope of the invention are deemed to be covered by the invention which is limited only by the claims which follow.



Claims
  • 1. An antenna including:a ground plane that is electrically conductive; a segmented patch that is divided into patch segments and that is electrically conductive; a plurality of MEMS switches disposed between the patch segments; a dielectric layer positioned between said segmented patch and said ground plane; and a RF lead connected to one of the patch segments, none of the other patch segments being coupled to any other RF lead, wherein the MEMS switches couple at least two of the patch segments together for communicating RF energy therebetween including the one of the patch segments connected to the RF lead and wherein no other patch segrnent receives RF energy unless it is one of the coupled at least two patch segments.
  • 2. The antenna as defined in claim 1 wherein the at least two patch segments are disposed along an axis with certain other of the patch segments in between them.
  • 3. The antenna as defined in claim 1, wherein the patch segments have a substantially rectangular shape, the antenna has a desired wavelength, and the side of each rectangular patch segment is substantially less than {fraction (1/20)} of the desired wavelength.
  • 4. The antenna as defined in claim 1, wherein the patch segments are coupled to achieve a desired resonant frequency for the antenna.
  • 5. The antenna as defined in claim 1, wherein the patch segments are coupled to achieve a desired input impedance to the antenna.6.The antenna as defined in claim 1, wherein the patch segments are coupled to achieve a desired polarization for the antenna.
  • 7. An antenna including:a ground plane that is electrically conductive having a first side surface; a segmented patch that is divided into patch segments and that is electrically conductive, said patch segments having collectively a first side surface and outer boundaries that define four rectilinear edges; a dielectric layer positioned between said patch segments and said ground plane, said dielectric layer including: a first side surface in contact with said first side surface of said patch segments; and a second side surface in contact with said first side surface of said ground plane; an RF lead connected to one of the patch segments, none of the other-patch segments being coupled to any other RF lead; and a plurality of MEMS switches to individually electrically connect and disconnect RF energy from the RF lead among said patch segments, whereby one or more of a resonant frequency, a feed impedance, and a polarization of said antenna can be changed.
  • 8. The antenna as defined in claim 7 wherein the patch segments are spaced from each other by distances that increase in accordance with increasing distances of said patch segments from a point within the segmented patch, and wherein said first and second side surfaces of said dielectric layer are parallel.
  • 9. The antenna as defined in claim 7 wherein each of the patch segments have lengths that increase in accordance with a corresponding increase in a distance of patch segments from a point within the segmented patch.
  • 10. An antenna including:a ground plane that is electrically conductive having a first side surface; a segmented patch that is divided into patch segments and that is electrically conductive, said segmented patch being shaped as a segmented plane section of a right circular cone and having: an outer boundary defined by the outer edges of the outermost patch segments of the segmented patch; and a first side surface; a dielectric layer positioned between said first patch and said ground plane, said dielectric layer including: a first side surface in contact with said first side surface of said segmented patch; and a second side surface in contact with said first side surface of said ground plane; a plurality of spaced ring shaped tuning strips that are electrically conductive and that are positioned concentric to each other and said outer boundary of said segmented patch on said first side surface of said dielectric layer; an RF lead connected to one of said patch segments, none of the other patch segments being coupled to any other RF lead; and MEMS switches to individually-electrically connect and disconnect RF energy from the RF lead between said patch segments and said plurality of spaced ring shaped tuning strips, whereby a resonant frequency of said antenna can be changed.
  • 11. The antenna as defined in claim 10 wherein said plurality of spaced ring shaped tuning strips are formed in arcuate segments, said switch means controllably electrically connecting and disconnecting RF energy between said arcuate segments of said tuning strips and said patch segments, whereby a resonant frequency and an antenna polarization of said antenna can be changed.
  • 12. An antenna including:a ground plane that is electrically conductive; a first segmented patch that is divided into first patch segments and that is electrically conductive having: at least one outer boundary; means to electrically insulate and space said ground plane from said first segmented patch; a plurality of tuning strips that are electrically conductive spaced from said at least one outer boundary of said first segmented patch and said ground plane; an RF, lead connected to one of said first patch segments, none of the other patch segments being coupled to any other RF lead; and a plurality of MEMS switches to individually electrically connect and disconnect RF energy from the RF lead among said tuning strips and said first patch segments.
  • 13. The antenna as defined in claim 12 wherein said segmented patch is a planar patch oriented on a patch plane parallel to said ground plane, and said plurality of conductive tuning strips are positioned on said patch plane.
  • 14. The antenna as defined in claim 12, further comprising:a center hole through said first patch, said ground plane, and said means to electrically insulate and space said ground plane from said first patch; and lines that pass through said center hole for supplying a voltage to said plurality of MEMS switches.
  • 15. The antenna as defined in claim 12, wherein said plurality of tuning strips correspond to a plurality of frequencies covering a desired frequency band.
  • 16. An antenna including:ground plane that is electrically conductive; a first segmented patch that is divided into first patch segments and that is electrically conductive, said first segmented patch having an outline that is rectilinear and having: four linear edges; means to electrically insulate and space said ground plane from said first patch; an RF lead connected to one of said first patch segments, none of the other patch segments being coupled to any other RF lead; and a plurality of MEMS switches to individually electrically connect and disconnect RF energy from the RF lead between said first patch segments, whereby a resonant frequency of said antenna and an antenna polarization thereof can be changed.
  • 17. The antenna as defined in claim 16, wherein a fraction of said first patch segments are to be coupled by said MEMS switches into a contiguous patch driven by the RF lead.
  • 18. The antenna as defined in claim 17 wherein another fraction of said first patch segments are adapted to be coupled together by said MEMS switches into tuning strips which are spaced from each other by a distance that increases in accordance with increasing distances of said tuning strips from said contiguous patch.
  • 19. The antenna as defined in claim 17 wherein another fraction of said first patch segments are adapted to be coupled together by said MEMS switches into tuning strips which have lengths that increase in accordance with a corresponding increase of a distance of said tuning strip from said contiguous patch.
  • 20. The antenna as defined in claim 16 wherein a fraction of said first patch segments are adapted to be coupled together by said MEMS switches into a contiguous patch driven by the RF lead.
  • 21. The antenna as defined in claim 20, wherein another fraction if said first patch segments are adapted to be coupled together by said MEMS switches into a plurality of spaced ring shaped tuning strips that are alectrically condutive and that are positioned concentric to each other and said contiguous patch.
  • 22. The antenna as defined in claim 21 wherein said plurality of spaced ring shaped tuning strips are formed in segments, said plurality of switches controllably electrically connecting and disconnecting RF energy between said segments of said tuning strips and said contiguous patch, whereby a resonant frequency and a polarization of said antenna can be changed.
  • 23. An antenna including:a ground plane that is electrically conductive; a first segmented patch that is divided into first patch segments and that is electrically conductive, said first segmented patch being shaped as a plane section of a right circular cone; means to electrically insulate and space said ground plane from said first segmented patch; an RF lead connected to one of said first patch segments, none of the other patch segments being coupled to any other RF lead; a plurality of MEMS switches to individually electrically connect and disconnect RF energy from the RF lead among said first patch segments, whereby a resonant frequency of said antenna can be changed.
  • 24. In an antenna that includes a ground plane that is electrically conductive, a segmented patch that is divided into patch segments and that is electrically conductive and having at least one boundary, means to electrically insulate and space the ground plane from the patch, an RF lead connected to the segmented patch, none of the other patch segments being coupled to any other RF lead, and a plurality of MEMS switches to individually electrically connect and disconnect RF energy from the RF lead between respective ones of the tuning strips and the patch, the patch supporting a resonance at a first RF frequency, a fraction of said patch segments are coupled by said MEMS switches into a contiguous patch, the contiguous patch having at least one boundary, a plurality of conductive tuning strips spaced from the at least one boundary of the contiguous patch and the ground plane, a method of operation including the steps of:placing RF energy on the RF lead at a second RF frequency below the first RF frequency; after connecting RF energy to at least one of the tuning strips positioned and dimensioned with respect to the contiguous patch so that the contiguous patch and the connected at least one tuning strip together have a resonant frequency that is about the second RF frequency.
  • 25. The method as defined in claim 24 wherein said connecting step includes:connecting RF energy to at least two of the tuning strips and blocking RF energy from at least one of the tuning strips, said at least one blocked tuning strip being positioned between at least one of the at least two tuning strips and the contiguous patch.
  • 26. The method as defined in claim 24 wherein the contiguous patch has at least two edges and a plurality of tuning strips spaced from each edge, said connecting step including:connecting RF energy to more tuning strips spaced from one edge than the other to change a polarization of the antenna.
  • 27. The method as defined in claim 24 wherein the RF lead is connected to the patch nearer to the at least one edge than an opposite edge, said connecting step including:connecting RF energy to more tuning strips spaced from the opposite contiguous patch edge than to tuning strips spaced from the at least one contiguous patch edge so as to adjust an impedance match between the RF lead and the antenna.
  • 28. The method as defined in claim 24 wherein another fraction of said patch segments are coupled by said MEMS switches into a plurality of conductive tuning strips.
  • 29. The method as defined in claim 28 wherein said connecting step includes:connecting RF energy to at least two of the tuning strips and blocking RF energy from at least one of the tuning strips, said at least one blocked tuning strip being positioned between at least one of the at least two tuning strips and the contiguous patch.
  • 30. The method as defined in claim 28 wherein the RF lead is connected to the patch nearer to the at least one edge than an opposite edge, said connecting step including:connecting RF energy to more tuning strips spaced from the opposite contiguous patch edge than to tuning strips spaced from the at least one contiguous patch edge so as to adjust an impedance match between the RF lead and the antenna.
  • 31. The method as defined in claim 24 wherein the contiguous patch has at least two edges and a plurality of tuning,strips spaced from each edge, said connecting step including:connecting RF energy to more tuning strips spaced from one edge than the other to change a polarization of the antenna.
  • 32. An antenna comprising:a patch that is adapted to receive RF energy and that has a first edge; a shorting element coupled to the patch; an electrically conductive ground plane coupled to the shorting element; a plurality of n tuning strips that are electrically conductive spaced from said first edge of said patch and spaced from said ground plane, each of said n tuning strips having a respective size; an RF lead connected to said patch; and at least one switch to electrically connect and disconnect RF energy between said at least one turning strip and said patch, wherein n≧2 and each of said n tuning strips is connected to said patch by way of an associated one said at least one switch, wherein 2n tuning states are available by selecting and connecting the at least n tuning strips.
  • 33. The antenna as defined in claim 32 wherein said at least one switch includes at least one diode.
  • 34. The antenna as defined in claim 32 wherein said at least one switch includes at least one MEMS switch.
  • 35. The antenna as defined in claim 32 wherein the shorting element is comprised of a wall that is coupled at a first end to a second edge of the patch parallel to and opposite from the first edge and to the ground plane at a second end.
  • 36. The antenna as defined in claim 35 wherein the patch, shorting element and ground plane define a resonator having a radiating aperture.
  • 37. The antenna as defined in claim 35, wherein the first end of the wall is coextensive with the second edge of the patch.
  • 38. The antenna as defined in claim 32, wherein the shorting element is comprised of a plated through hole.
  • 39. An antenna comprising:a segmented patch divided into patch segments; a shorting element coupled to at least one of the patch segments; an electrically conductive ground plane coupled to the shorting element; an RF lead connected to one of the patch segments of said segmented patch, none of the other patch segments being coupled to any other RF lead; and switches to electrically connect and disconnect RF energy from the RF lead between said patch segments.
  • 40. The antenna as defined in claim 39 wherein a fraction of the patch segments are electrically connected by the switches into a contiguous patch having a first edge.
  • 41. The antenna as defined in claim 40, wherein another fraction of the patch segments are electrically connected by the switches into at least one tuning strip that is electrically conductive spaced from said first edge of said contiguous patch and spaced from said ground plane.
  • 42. The antenna as defined in claim 40 wherein the switches electrically connects the at least one tuning strip to the contiguous patch.
  • 43. The antenna as defined in claim 42, wherein said at least one tuning strip includes at least n tuning strips and n≧2 and each of said at least n tuning strips is connected to said patch by way of an associated one said at least one switch, wherein 2n tuning states are available by selecting and connecting the at least n tuning strips.
  • 44. The antenna as defined in claim 39, wherein the shorting element is comprised of a wall that is coupled at a first end to an edge of the patch and to the ground plane at a second end.
  • 45. The antenna as defined in claim 44, wherein the patch, shorting element and ground plane define a resonator having a radiating aperture.
  • 46. The antenna as defined in claim 44, wherein the first end of the wall is coextensive with the edge of the patch.
  • 47. The antenna as defined in claim 39, wherein the shorting element is comprised of a plated through hole.
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Entry
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