The present invention relates generally to antennas, and more particularly to a compact antenna system with a reduced directional pattern in the backward hemisphere.
Global navigation satellite systems (GNSSs) can determine locations with high accuracy. Currently deployed GNSSs include the United States Global Positioning System (GPS) and the Russian GLONASS. Other GNSSs, such as the European GALILEO system, are under development. GNSSs are used in a wide range of applications, such as surveying, geology, and mapping.
In a GNSS, a navigation receiver receives and processes radio signals transmitted by satellites located within a line-of-sight of the navigation receiver. A critical component of a GNSS is the receiver antenna. Key properties of the antenna are bandwidth, multipath rejection, size, and weight.
High-accuracy navigation receivers typically process signals from two frequency bands. Two common frequency bands are a low-frequency band in the range of 1164-1300 MHz and a high-frequency band in the range of 1525-1610 MHz.
For portable navigation receivers, antennas with light weight and compact size are desirable. In surveying applications, for example, an antenna is mounted on a surveying pole. The dimensions of the antenna should be sufficiently small to accommodate mounting on a standard surveying pole. The weight of the antenna should also be small enough to ensure easy handling of the pole-mounted assembly: if the weight is excessive, the center-of-gravity is raised too high, and the pole-mounted assembly is unwieldy.
Navigation receivers achieve the highest accuracy when they receive only the direct, line-of-sight, radio signals from the satellites. Navigation receivers, however, typically operate in environments in which the radio signals reflect off environmental surfaces, such as earth and water, and objects, such as buildings, towers, and vehicles. Reflected signals that are detected by the navigation receiver are referred to as multipath signals. Multipath signals reduce the accuracy with which the position of the navigation receiver can be determined.
Antennas that reject or suppress the reception of multipath signals, therefore, are desirable. PCT International Publication No. WO 2004/027920 (I. Soutiaguine et al.), for example, describes an antenna system that operates over a wide bandwidth and reduces multipath reception of GPS signals.
The active micropatch antenna 120 includes the ground plane 102 and the radiating patch 104. The ground plane 102 and the radiating patch 104 are separated by the dielectric substrate 106. The radiating patch 104 is actively driven by the excitation pin 108.
The passive micropatch antenna 130 includes the ground plane 102 and the radiating patch 110. The ground plane 102 and the radiating patch 110 are separated by the dielectric substrate 112. The radiating patch 110 has no excitation pin and is driven by the field from the active micropatch antenna 120.
The fields of the micropatch antenna 120 and the micropatch antenna 130 are mutually suppressed in the backward hemisphere; consequently, the level of the directional pattern in the backward hemisphere is reduced. The antenna system 100, however, suppresses the multipath signal only within a narrow bandwidth; and the stacked antenna construction has the further disadvantages of heavy weight and large dimensions.
The operating bandwidth for the antenna system 100 is dependent on the distance between the radiating patch 104 and the ground plane 102. To reduce the antenna dimensions and expand the directional pattern in the forward hemisphere, the space between the radiating patch 104 and the ground plane 102 is filled with the dielectric substrate 106. Suitable dielectric materials over the operating frequency bands, however, have a high density; consequently, the weight of the antenna system increases significantly.
As discussed above, in surveying applications, an antenna is mounted on a surveying pole. Examples of pole-mounted GPS antennas are given in European Patent Application Publication No. EP 1503176 (F. Ohtomo et al.) and United States Patent Application Publication No. 20100211314 (Zhukov et al.). In both instances, the antenna extends considerably beyond the pole (particularly along lateral dimensions), and the configuration of outer mounting elements reduces the stability of the overall pole-mounted assembly.
A GNSS antenna with compact size, low weight, and high multipath rejection is therefore advantageous. An antenna that can operate over dual frequency bands and that can be readily mounted onto a standard surveying pole, while maintaining ease of handling, is further advantageous.
In an embodiment, an antenna system includes a ground plane, an active antenna disposed above the ground plane, and a passive antenna disposed below the ground plane. The ground plane is substantially flat, with a top surface, a bottom surface, a perimeter, and a normal axis substantially coincident with the antenna axis.
The active antenna includes a first conducting ring substantially parallel to the top surface of the ground plane and disposed above the top surface of the ground plane. A first radiating conductor passes through substantially the center of the first conducting ring; the ends of the first radiating conductor are electrically connected to the first conducting ring. An excitation pin is electrically connected to the first radiating conductor.
A first set of reactive impedance elements is electrically connected between the first conducting ring and the top surface of the ground plane. The first set of reactive impedance elements is disposed substantially parallel to the antenna axis.
The passive antenna includes a second conducting ring substantially parallel to the bottom surface of the ground plane and disposed below the bottom surface of the ground plane. A second radiating conductor passes through substantially the center of the second conducting ring; the ends of the second radiating conductor are electrically connected to the conducting ring. The passive antenna does not include an excitation pin.
A second set of reactive impedance elements is electrically connected between the second conducting ring and the bottom surface of the ground plane. The second set of reactive impedance elements is disposed substantially parallel to the antenna axis.
Embodiments of the antenna system can be configured for linearly-polarized radiation or circularly-polarized radiation. Embodiments of the antenna can be configured for single-frequency band or dual-frequency band operation. Embodiments of the antenna system can be inexpensively manufactured with flexible printed circuit boards. Embodiments of the antenna system are light weight and compact and can be readily integrated with a surveying pole for applications with global navigation satellite systems.
These and other advantages of the invention will be apparent to those of ordinary skill in the art by reference to the following detailed description and the accompanying drawings.
In
To quantitatively characterize the capability of an antenna to reject or suppress the reflected signal, the following ratio is commonly used:
The parameter DU(θ) (down/up ratio) is equal to the ratio of the antenna directional pattern (DP) level F(−θ) in the backward hemisphere to the antenna directional pattern level F(θ) in the forward hemisphere at the mirror angle, where F represents a voltage level. Expressed in dB, the ratio is:
DU(θ)(dB)=20 log DU(θ). (E2)
Compact, light-weight antenna systems with high rejection of multipath signals in the backward hemisphere are described below. Embodiments of the invention are described for antenna systems configured to receive or transmit electromagnetic radiation with the following characteristics: (1) single-frequency band, linearly-polarized radiation, (2) single-frequency band, circularly-polarized radiation, (3) dual-frequency band, linearly-polarized radiation, and (4) dual-frequency band, circularly-polarized radiation. An antenna system configured for electromagnetic radiation with specific characteristics refers to an antenna system configured to receive or transmit electromagnetic radiation with the specific characteristics. From the well-known antenna reciprocity theorem, antenna properties, such as directional pattern, in the transmit mode correspond to antenna properties in the receive mode.
Herein, an active antenna refers to an antenna whose radiating element has an excitation pin, and a passive antenna refers to an antenna whose radiating element has no excitation pin. In the transmit mode of the antenna, the excitation pin is coupled to the output of a transmitter, and the excitation pin is driven by signals from the transmitter. In the receive mode of the antenna, the excitation pin is coupled to the input of a receiver. Signals received by the active antenna are typically transmitted from the excitation pin to the input of a low-noise amplifier (LNA) in the receiver. There can be intermediate components, such as combiners and splitters, cables, and connector ports, between the excitation pin and the output of the transmitter or the input of the receiver.
Refer to
Inside the tubular dielectric substrate 312 is the planar dielectric substrate 322, such as a printed circuit board; single-sided or double-sided metallization can be used. On the planar dielectric substrate 322 are the radiating conductor 324 and the excitation pin 326. The excitation pin 326 is connected via a power line to an antenna port (not shown). A low-noise amplifier (not shown) is then connected to the antenna port. The position of the excitation pin 326 is specified to provide the desired matching input impedance.
The radiating conductor 324 is electrically connected to the conducting ring 314; for example, via the solder joint 328 and the solder joint 330. The planar dielectric substrate 322 is secured to the tubular dielectric substrate 312 via the fastener tabs 332. The planar dielectric substrate 322 provides structural reinforcement for the tubular dielectric substrate 312.
To reduce the cross-sectional dimensions of the antenna system, the set of impedance elements 318 is electrically connected to the conducting ring 314, and the set of impedance elements 320 is electrically connected to the conducting ring 316. Cross-sectional dimensions, also referred to as lateral dimensions, refer to dimensions measured orthogonal to the antenna axis 301. Axial dimensions, also referred to as vertical dimensions or height dimensions or longitudinal dimensions, refer to dimensions measured parallel to the antenna axis 301. More details of the impedance elements are described below.
Refer to
Inside the tubular dielectric substrate 312 is the planar dielectric substrate 352. On the planar dielectric substrate 352 is the radiating conductor 354; there is no excitation pin. The radiating conductor 354 is electrically connected to the conducting ring 344; for example, via the solder joint 358 and the solder joint 360.
To reduce the cross-sectional dimensions of the antenna system, the set of impedance elements 348 is electrically connected to the conducting ring 344, and the set of impedance elements 350 is electrically connected to the conducting ring 346. More details of the impedance elements are described below.
Details of the tubular dielectric substrate 312 are shown in
Herein, geometrical conditions are “substantially” satisfied if they are met within user-defined tolerances. User-defined tolerances include typical manufacturing tolerances and design tolerances within which the antenna system performance is acceptable to the user; here, “user” refers, for example, to an antenna design engineer. To simplify the terminology, unless otherwise stated, geometrical conditions (such as parallel, orthogonal, circular, and cylindrical) and values of dimensions (such as lengths and angles) are implicitly modified by the term “substantially”.
Refer to
When the tubular dielectric substrate 312 has a cross-section with a circular geometry, then the conducting ring 314 and the conducting ring 316 (
The geometries of the tubular dielectric substrate 342 are similar to those of the tubular dielectric substrate 312.
The longitudinal axis of the tubular dielectric substrate 312, the longitudinal axis of the tubular dielectric substrate 342, and the normal axis of the ground plane 302 are all aligned along the antenna axis 301. The plane of the planar dielectric substrate 322 is parallel to the antenna axis 301, and the antenna axis 301 lies on the plane of the planar dielectric substrate 322. Similarly, the plane of the planar dielectric substrate 352 is parallel to the antenna axis 301, and the antenna axis 301 lies on the plane of the planar dielectric substrate 352. The azimuthal angle, measured about the antenna axis 301, of the planar dielectric substrate 352 with respect to the planar dielectric substrate 322 is variable and set according to design specifications.
The geometries and dimensions of the tubular dielectric substrate 312, the tubular dielectric substrate 342, and the ground plane 302 are independently variable and set according to design specifications. In particular, the shape and the dimensions of the tubular dielectric substrate 312 and of the tubular dielectric substrate 342 are not necessarily the same. For example, an antenna system can be configured with a combination of a tubular dielectric substrate 312 with a circular cross-section, a tubular dielectric substrate 342 with a square cross-section, and a ground plane 302 with a hexagonal geometry. To simplify the discussion, in the examples below, the tubular dielectric substrate 312 and the tubular dielectric substrate 342 have circular cross-sections, and the ground plane 302 has a circular geometry.
The excitation efficiency of the passive antenna 340 by the active antenna 310 is a function of the lateral dimension of the ground plane 302. If the tubular dielectric substrates are cylinders with a diameter d1 and the ground plane is a circular disk with a diameter d2>d1, then the value a=(d2−d1)/2 is approximately 0.12-0.15 times the operating wavelength of the antenna. For a GPS antenna, a is approximately 25-35 mm. More detailed analysis of the optimum range of a is provided below.
As discussed above, in an embodiment, the tubular dielectric substrate 312 and the tubular dielectric substrate 342 are fabricated from flexible printed circuit boards that are then rolled into tubes.
Also shown in
The active antenna 310 shown in
The planar dielectric substrate 322, for example, can be eliminated if the radiating conductor 324 and the excitation pin 326 are fabricated from sheet metal that does not require a supporting substrate. The radiating conductor 324 and the excitation pin 326 can be fabricated as a single unit, or the excitation pin 326 can be soldered or mechanically fastened to the radiating conductor 324.
The tubular dielectric substrate 312, for example, can be eliminated if the conducting ring 314 is fabricated from metal wire or sheet metal that does not require a supporting substrate. The set of impedance elements can be fabricated from wires or pins integrally fabricated with, soldered to, or mechanically fastened to the conducting ring 314. The conducting ring 316 and the set of impedance elements 320 can be similarly fabricated. In some embodiments, the conducting ring 316 can be eliminated, and the set of impedance elements 320 can be soldered directly onto the ground plane 302.
In embodiments that have no dielectric substrates, the conducting ring 314 can be supported above the ground plane 302 with suitable dielectric posts. As described later in reference to
The various fabrication techniques described above for the active antenna 310 can be similarly applied, with appropriate modifications, for the passive antenna 340 and for the active and passive antennas described below.
In the receive mode, the excitation pin 726 is connected via the power line 784 passing through a hole in the ground plane 302 to the input port 794 of the quadrature combiner 790. Similarly, the excitation pin 746 is connected via the power line 782 passing through a hole in the ground plane 302 to the input port 792 of the quadrature combiner 790. There is a 90-degree phase shift between the input port 792 and the input port 794. The output port 796 of the quadrature combiner 790 is connected to an antenna port (not shown). A low-noise amplifier (not shown) is then connected to the antenna port. The positions of the excitation pins are specified to provide the proper matching input impedances. [Note, in the transmit mode, the antenna port is connected to a transmitter, and the quadrature combiner acts as a quadrature splitter.]
In addition to the structures in
On the planar dielectric substrate 752 is the radiating conductor 754. Similarly, on the planar dielectric substrate 772 is the radiating conductor 774. There are no excitation pins on the planar dielectric substrate 752 and the planar dielectric substrate 772. The azimuthal angle, measured about the antenna axis 301, of the planar dielectric substrate 752 and the planar dielectric substrate 772 with respect to the planar dielectric substrate 722 and the planar dielectric substrate 742 is variable and set according to design specifications. In one embodiment, the azimuthal angle is about 45 deg.
Refer to
Refer to
Refer to
Refer to
The geometries and dimensions of the dielectric substrates, slots, radiating conductors, conductive strips, and excitation pins are all independently variable and set according to design specifications.
The antenna system 800 includes the low-frequency (LF) active antenna 810, the LF passive antenna 830, the high-frequency (HF) active antenna 850, the HF passive antenna 870, and the ground plane 302. In operation, the LF active antenna 810 and the HF active antenna 850 face towards the sky, and the LF passive antenna 830 and the HF passive antenna 870 face towards the Earth.
Refer to
Inside the tubular dielectric substrate 812 is the planar dielectric substrate 822. On the planar dielectric substrate 822 are the radiating conductor 824 and the excitation pin 826. The radiating conductor 824 is electrically connected to the conducting ring 814.
The HF active antenna 850 includes the tubular dielectric substrate 852. At one end of the tubular dielectric substrate 852 is the conducting ring 854. At the other end of the tubular dielectric substrate 852 is the conducting ring 856. The HF active antenna 850 is stacked above the LF active antenna 810. The conducting ring 856 of the HF active antenna 850 is electrically connected to the radiating conductor 824 of the LF active antenna 810.
Inside the tubular dielectric substrate 852 is the planar dielectric substrate 862. On the planar dielectric substrate 862 are the radiating conductor 864 and the excitation pin 866. The radiating conductor 864 is electrically connected to the conducting ring 864.
The excitation pin 826 of the LF active antenna 810 is connected via a power line to a LF antenna port (not shown). The excitation pin 866 of the HF active antenna is connected via a power line to a HF antenna port (not shown). In the receive mode, a LF low-noise amplifier (not shown) is connected to the LF antenna port, and a HF low-noise amplifier (not shown) is connected to the HF antenna port. The positions of the excitation pins are specified to provide the proper matching input impedances.
Refer to
Inside the tubular dielectric substrate 832 is the planar dielectric substrate 842. On the planar dielectric substrate 842 is the radiating conductor 844; there is no excitation pin. The radiating conductor 844 is electrically connected to the conducting ring 834.
The HF passive antenna 870 is similar to the HF active antenna 850. The HF passive antenna 870 includes the tubular dielectric substrate 872. At one end of the tubular dielectric substrate 872 is the conducting ring 874. At the other end of the tubular dielectric substrate 872 is the conducting ring 876. The HF passive antenna 870 is stacked below the LF passive antenna 830. The conducting ring 876 of the HF passive antenna 870 is electrically connected to the radiating conductor 844 of the LF passive antenna 830.
Inside the tubular dielectric substrate 872 is the planar dielectric substrate 882. On the planar dielectric substrate 882 is the radiating conductor 884; there is no excitation pin. The radiating conductor 884 is electrically connected to the conducting ring 874.
The longitudinal axis of the tubular dielectric substrate 812, the longitudinal axis of the tubular dielectric substrate 852, the longitudinal axis of the tubular dielectric substrate 832, the longitudinal axis of the tubular dielectric substrate 872, and the normal axis of the ground plane 302 are all aligned along the antenna axis 801. The plane of the planar dielectric substrate 822 is parallel to the antenna axis 801, and the antenna axis 801 lies on the plane of the planar dielectric substrate 822. The plane of the planar dielectric substrate 862 is parallel to the antenna axis 801, and the antenna axis 801 lies on the plane of the planar dielectric substrate 862. The plane of the planar dielectric substrate 842 is parallel to the antenna axis 801, and the antenna axis 801 lies on the plane of the planar dielectric substrate 842. The plane of the planar dielectric substrate 882 is parallel to the antenna axis 801, and the antenna axis 801 lies on the plane of the planar dielectric substrate 882.
The planar dielectric substrate 822 and the planar dielectric substrate 862 are co-planar. The planar dielectric substrate 842 and the planar dielectric substrate 882 are co-planar. The azimuthal angle, measured about the antenna axis 801, of the planar dielectric substrate 822 and the planar dielectric substrate 862 with respect to the planar dielectric substrate 842 and the planar dielectric substrate 882 is variable and set according to design specifications.
To reduce the cross-sectional dimensions of the antenna system, sets of impedance elements are configured on the outer walls of the four tubular dielectric substrates. A representative example is referenced on the tubular dielectric substrate 812 (see
Refer to
Inside the tubular dielectric substrate 912 are the planar dielectric substrate 922 and the planar dielectric substrate 932. The planar dielectric substrate 922 and the planar dielectric substrate 932 are mounted orthogonal to each another. On the planar dielectric substrate 922 are the radiating conductor 924 and an excitation pin (not shown in this view, but shown in more detail below). The radiating conductor 924 is electrically connected to the conducting ring 914. On the planar dielectric substrate 932 are the radiating conductor 934 and an excitation pin (not shown in this view, but shown in more detail below). The radiating conductor 934 is electrically connected to the conducting ring 914.
The HF active antenna 970 includes the tubular dielectric substrate 972. At one end of the tubular dielectric substrate 972 is the conducting ring 974. At the other end of the tubular dielectric substrate 972 is the conducting ring 976. The HF active antenna 970 is stacked above the LF active antenna 910. The conducting ring 976 of the HF active antenna 970 is electrically connected to the radiating conductor 924 and the radiating conductor 934 of the LF active antenna 910.
Inside the tubular dielectric substrate 972 are the planar dielectric substrate 982 and the planar dielectric substrate 992. The planar dielectric substrate 982 and the planar dielectric substrate 992 are orthogonal to each other. On the planar dielectric substrate 982 are the radiating conductor 984 and an excitation pin (not shown in this view, but shown in more detail below). The radiating conductor 984 is electrically connected to the conducting ring 974. On the planar dielectric substrate 992 are the radiating conductor 994 and an excitation pin (not shown in this view, but shown in more detail below). The radiating conductor 994 is electrically connected to the conducting ring 974.
Refer to
Inside the tubular dielectric substrate 942 are the planar dielectric substrate 952 and the planar dielectric substrate 962. The planar dielectric substrate 952 and the planar dielectric substrate 962 are orthogonal to each other. On the planar dielectric substrate 952 is the radiating conductor 954; there is no excitation pin. The radiating conductor 954 is electrically connected to the conducting ring 944. On the planar dielectric substrate 962 is the radiating conductor 964; there is no excitation pin. The radiating conductor 964 is electrically connected to the conducting ring 944.
The HF passive antenna 9100 is similar to the HF active antenna 970. The HF passive antenna 9100 includes the tubular dielectric substrate 9102. At one end of the tubular dielectric substrate 9102 is the conducting ring 9104. At the other end of the tubular dielectric substrate 9102 is the conducting ring 9106. The HF passive antenna 9100 is stacked below the LF passive antenna 940. The conducting ring 9106 of the HF passive antenna 9100 is electrically connected to the radiating conductor 954 and the radiating conductor 964 of the LF passive antenna 940.
Inside the tubular dielectric substrate 9102 is are the planar dielectric substrate 9112 and the planar dielectric substrate 9122. The planar dielectric substrate 9112 and the planar dielectric substrate 9122 are orthogonal to each other. On the planar dielectric substrate 9112 is the radiating conductor 9114; there is no excitation pin. The radiating conductor 9114 is electrically connected to the conducting ring 9104. On the planar dielectric substrate 9122 is the radiating conductor 9124; there is no excitation pin. The radiating conductor 9124 is electrically connected to the conducting ring 9104.
To reduce the cross-sectional dimensions of the antenna system, sets of impedance elements are configured on the outer walls of the four tubular dielectric substrates. A representative example is referenced on the tubular dielectric substrate 912 (see
For a dual-frequency band antenna operating in the GPS L1 and L2 frequency bands, characteristic dimensions for an embodiment are the following:
diameter 915: 19 mm
diameter 925: 19 mm
diameter 911: 28 mm
diameter 921: 28 mm
length 917: 12 mm
length 927: 12 mm
length 913: 20 mm
length 927: 20 mm
a=(diameter 903-diameter 911)/2: 25 mm.
Approximate weights for embodiments of the antenna range from 10 to 30 grams.
In the receive mode, power lines connect the excitation pin 926 and the excitation pin 936 of the LF active antenna 910 to a LF quadrature combiner (not shown, but similar to the configuration shown in
Refer to
Refer to
Refer to
Refer to
As discussed above, cross-sectional dimensions of the antenna system can be reduced by configuring sets of impedance elements on the tubular dielectric substrates.
The dielectric substrate 1002 has a thickness 1001. The dielectric substrate 1002 has a front face 1002A, a rear face 1002B, a top face 1002C, a bottom face 1002D, a left face 1002E, and a right face 1002F. The designations of the faces are used strictly for descriptive reference with respect to the figures. When the dielectric substrate 1002 is rolled into a tube, the front face 1002A becomes the outer wall, and the rear face 1002B becomes the inner wall (compare
Refer to
The set of impedance elements 1018 is electrically connected to the conducting strip 1014, and the set of impedance elements 1020 is electrically connected to the conducting strip 1016. In this instance, the set of impedance elements 1018 and the set of impedance elements 1020 are interdigitated to form a set of capacitive elements separated by the gap 1019 with a gap spacing 1003.
Refer to
The conducting strip 1116 and the set of impedance elements 1120 are disposed on the front face 1102A. The conducting strip 1114 and the set of impedance elements 1118 are disposed on the rear face 1102B. Because the set of impedance elements 1120 and the set of impedance elements 1118 are separated by the dielectric substrate 1102, there are more degrees of freedom in configuring the sets of impedance elements than in the configuration shown in
The active antenna 1210 includes the tubular dielectric substrate 1212. At one end of the tubular dielectric substrate 1212 is the conducting ring 1214. At the other end of the tubular dielectric substrate 1212 is the conducting ring 1216, which is electrically connected to the ground plane 302. Inside the tubular dielectric substrate 1212, there are a pair of planar dielectric substrates. The planar dielectric substrate 1222 and the planar dielectric substrate 1232 are orthogonal to each other. On the planar dielectric substrate 1222 are the radiating conductor 1224 and the excitation pin 1226; as described below, the radiating conductor 1224 and the excitation pin 1226 operate over two frequency bands. The radiating conductor 1224 is electrically connected to the conducting ring 1214. On the planar dielectric substrate 1232 are the radiating conductor 1234 and the excitation pin 1236; as described below, the radiating conductor 1234 and the excitation pin 1236 operate over two frequency bands. The radiating conductor 1234 is electrically connected to the conducting ring 1214.
In this embodiment, in the receive mode, the excitation pin 1226 and the excitation pin 1236 are connected via power lines to input ports of a quadrature combiner. The output port of the quadrature combiner is connected to the input of a low-noise amplifier. The quadrature combiner and the low-noise amplifier have a wide enough bandwidth to process signals from two frequency bands.
The passive antenna 1240 is similar to the active antenna 1210. The passive antenna 1240 includes the tubular dielectric substrate 1242. At one end of the tubular dielectric substrate 1242 is the conducting ring 1244. At the other end of the tubular dielectric substrate 1212 is another conducting ring (not shown), which is electrically connected to the ground plane 302. Inside the tubular dielectric substrate 1212, there are a pair of planar dielectric substrates (not shown), similar to the pair of planar dielectric substrates in the active antenna 1210, except there are no excitation pins. The passive antenna 1240 is driven by the electromagnetic field from the active antenna 1210.
On the tubular dielectric substrate 1212, a set of impedance elements 1218 are electrically connected between the conducting ring 1214 and the conducting ring 1216. Similarly, on the tubular dielectric substrate 1242, a set of impedance elements 1248 are electrically connected between the two conducting rings. Dual-frequency operation of the active antenna 1210 and the passive antenna 1240 is achieved by a specific dependence of the impedance elements on frequency, as discussed in further detail below.
Frequency parameters of both the active antenna 1210 and the passive antenna 1240 can be estimated with the equivalent transmission line model shown in
The admittance Ys can be determined approximately as
Y
s=(N/2)Yi, (E3)
where Yi is the admittance of a single impedance element 1218 and N is the number of impedance elements 1218.
The resonance condition is determined by setting the sum of the admittance for the leg, Yi(f)=−iY0ctg(k(f)l), and the admittance Ys(f) to zero:
Im(Yl(f)+Ys(f))=0, (E4)
where Y0 is the wave admittance of the equivalent transmission line;
is the wave number; f is the frequency; and C is the speed of wave propagation. The frequency dependence of the admittance Ys(f) to satisfy condition (E4) must hold for two frequencies f1 and f2 corresponding to average frequencies of the HF and LF bands.
The required frequency dependence can be implemented if each impedance element is configured as a circuit element 1400 as shown in
is the central frequency, and λ0 is the wavelength in vacuum that corresponds to frequency f0. The argument of the functions is the relative frequency mismatch
From the plots, it is apparent that, for the frequencies corresponding to δf=±10%, Yl and Ys have equal values and opposite signs, and their sum Yl+YS at these frequencies is zero; that is, the resonance condition (E4) is satisfied. In the antenna system 1200 with the impedance element 1400, therefore, the resonance condition is satisfied at two frequencies f1 and f2 corresponding to average frequencies of the HF and LF bands, respectively.
Capacitors C1, C2, and inductance L1 can be fabricated in the form of lumped elements (discrete components) within miniature cases or printed elements configured on a dielectric substrate (flexible or rigid). Impedance elements can be attached via lead wires, for example, to the conducting ring 1214 and the ground plane 302. The conducting ring 1214 can be supported by the set of impedance elements, and a substrate (tubular or planar) is not required for support.
An embodiment of a dual-frequency band antenna system similar to the dual-frequency band antenna system 1200 can be configured for linearly-polarized radiation. The active antenna and the passive antenna are each outfitted with a single planar dielectric substrate.
The single-frequency band antenna system 700 (shown in
In
In
In
In
Herein, the reactive impedance elements, Z 1604, Z 1614, Z 1624, Z 1634, Z 1644, Z 1654, Z 1664, and Z 1674 are referred to as frequency-control reactive impedance elements.
An equivalent transmission line diagram for the dual-frequency band antenna is shown in
At the frequency f1, resonance of the parallel circuit 1710 occurs that corresponds to the idling mode (Z=∞) in the section Δl of the transmission line. At the frequency f2, the circuit impedance C1L1 has a capacitive characteristic. The series-connected inductor L2 1706 permits resonance to occur: it is equivalent to a short circuit in the section Δl of the transmission line. Therefore, at the frequency f1 the resonance length of the radiator remains unchanged and equal to l; however, at the frequency f2, the equivalent resonance length is reduced to l−Δl.
An embodiment of a dual-frequency band antenna system similar to the dual-frequency band antenna system just described above can be configured for linearly-polarized radiation. The active antenna and the passive antenna are each outfitted with a single planar dielectric substrate.
As discussed above, in surveying applications, an antenna is often mounted on a surveying pole. The compact, light-weight antenna systems described above can all be integrated with a surveying pole (also referred to as a geodetic pole).
The active antenna 910 and the active antenna 970 sit above the pole case 2002. The active antennas are covered by the antenna housing 2006, which terminates in the flange 2008. The flange 2008 mates with the flange 2004. For simplicity, various mounting hardware is not shown. The pole case 2002 and the antenna housing 2006 are fabricated from material that is substantially transparent to radio-frequency electromagnetic radiation. Examples of suitable materials include Xenoy 5220 and Lexan 143.
As discussed above, the excitation efficiency of a passive antenna is directly related to the distance a between the perimeter of the ground plane and the perimeter of the active antenna. The distance a also determines the maximum cross-sectional dimensions of the antenna system. Presented below is an analysis of the dependence of the operation of the antenna system on the distance a. Design rules are derived for minimizing the distance a while maintaining a high suppression of multipath signals reflected from the backward hemisphere.
As previously presented in (E1), to quantitatively characterize the capability of an antenna to reject or suppress the reflected signal, the following ratio is commonly used:
where θ is measured from the horizon. For satellite applications, the value for the angle θ=90° is often used as a characteristic parameter.
The analysis can be performed using a simplified two-dimensional radiator model, as shown in
Above the flat surface 2102 is the magnetic current with surface density jm1 2104 (referred to as the upper magnetic current), which simulates an active antenna. Below the flat surface 2102 is the magnetic current with surface density jm2 2106 (referred to as the lower magnetic current), which simulates a passive antenna. The surface densities of these currents are given by
Here U1 and U2 are the equivalent voltages in the area of the impedance elements (for example, the set of impedance elements 918 and the set of impedance elements 920 in the antenna system 900 shown in
Assume that the amplitude U1 is a known quantity. The passive antenna is a resonator formed by a set of conductors [for example, in the antenna system 900, the resonator is formed by the radiating conductor 964, the ground plane 302, and the sets of impedance elements on the tubular dielectric substrate 942 (see
y=0+ib. (E7)
The value b is determined by structural details of the passive antenna and can be varied according to parameters discussed below. In
The amplitude U2 characterizes the coupling between the top and bottom radiators:
Here Y12 is the mutual admittance between the upper and lower magnetic currents, and Y22 is the radiation admittance of the lower magnetic current.
The field of this system is a sum of the upper and lower magnetic current fields:
E=E(jm1)+E(jm2). (E9)
It then follows that:
F(θ)=U1F1(θ)+U2F2(θ). (E10)
Here F1(θ) is the directional pattern level of the source jm1 with U1=1 and U2=0; and F2(θ) is the directional pattern level of the source jm2 with U2=1 and U1=0.
As discussed above, the ratio DU(θ) at θ=90° is commonly used as a characteristic parameter in satellite applications; this parameter is designate as DU90. Then,
Now let
If the magnetic currents jm1 and jm2 are symmetrical relative to the flat surface 2102, then F1(90°)=F2(−90°) and F1(−90°)=F2(90°). It then follows that
From (E11), it then follows that
Assume that the antenna system is designed to minimize the value of DU90. Then, in (E14), the numerator needs to be minimized, and the denominator needs to be maximized (that is, the fields of the upper and lower sources need to be subtracted, not added, in the region near the nadir (θ=−90°). If the numerator is set to zero, then
The denominator can then be expressed as:
The denominator is maximized if
arg(A)=±π/2. (E17)
The condition (E15) cannot be fully satisfied, since there is no active component in (E7). The system parameters (the distance a and the reactivity b are therefore selected such that condition (E15) is satisfied as closely as possible.
Consider graphs of dependences for phase and modulus of the coefficient A when the distance a changes. The graphs were obtained by solving numerically the electro-dynamic problem using the moment method. In
The value
(condition E17) is reached at
An expression for the admittance of the passive antenna (E7) needed to tune the system and a achieve a minimum ratio DU90 is now derived. Substituting (E15) into (E8) yields
The active component of equation (E19) is negative; therefore, condition (E15) for the passive system cannot be satisfied. The active component, however, of the passive antenna admittance can be set to zero (E7). The condition for tuning the passive antenna is then:
In
The foregoing Detailed Description is to be understood as being in every respect illustrative and exemplary, but not restrictive, and the scope of the invention disclosed herein is not to be determined from the Detailed Description, but rather from the claims as interpreted according to the full breadth permitted by the patent laws. It is to be understood that the embodiments shown and described herein are only illustrative of the principles of the present invention and that various modifications may be implemented by those skilled in the art without departing from the scope and spirit of the invention. Those skilled in the art could implement various other feature combinations without departing from the scope and spirit of the invention.
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/RU2012/000652 | 8/9/2012 | WO | 00 | 3/10/2014 |