The invention relates to an antenna arrangement for the reception of circularly polarized satellite radio signals, in particular for satellite radio navigation.
Satellite radio signals are as a rule transmitted using circularly polarized electromagnetic waves due to polarization rotations on the transmission path and are used in all known satellite navigation systems. Modern navigation systems provide for an evaluation of simultaneously received radio signals of a plurality of satellite navigation systems, in particular for global availability in conjunction with high navigation accuracy in mobile navigation. Such systems that receive in combination are collected together under the name GNSS (global navigation satellite system) and include known systems such as GPS (global positioning system), GLONASS, Galileo and Beidou, etc. Satellite antennas for navigation on vehicles are as a rule configured on the electrically conductive outer skin of the vehicle body. Circularly polarized satellite reception antennas are used such as are known from DE 10 2009 040 910 A or DE 40 08 505 A. In particular those antennas that are characterized by a low construction height in conjunction with a cost-effective manufacturing capability are suitable for configuration on vehicles. They in particular include the ring line radiator known from DE 10 2009 040 910 A, designed as a resonant structure, and having a small construction volume that is in particular an absolute requirement for mobile applications. The antenna has a small base surface and is very low with a height of less than one tenth of the free space wavelength.
Patch antennas that are, however, more complex and/or expensive in design than antennas stamped from sheet metal are known in accordance with the prior art as further antennas for satellite navigation on vehicles. One challenge for the satellite antennas for GNSS comprises the demand for a large frequency bandwidth that is, for example, predefined for GPS by the frequency band L1 having the center frequency 1575 MHz (required bandwidth approximately 80 Hz) and by the frequency band L2 having the center frequency 1227 MHz (required bandwidth approximately 53 MHz). This requirement is, for example, covered by a separate antenna associated with a respective one of the frequency bands L1 and L2 or by a broadband antenna comprising both frequency bands. Systems for the simultaneous evaluation of signal content in the frequency bands L1 and L2 make particularly high demands on the antennas, and indeed with a small available construction space such as is above all always present in vehicle construction. The use of separate antennas located in close proximity to one another for the two frequency bands includes the problem of mutual electromagnetic coupling with the effect of influencing the radiation patterns and the polarization purity and in particular the cross polarization. Due to the signals of the position location satellites incident at low angles of elevation and even with sufficient gain in the desired, typically right hand circular polarization direction (RHCP), the suppression of the opposite polarization direction—the cross polarization—acquires crucial importance with respect to correct position location results. The accuracy of the position location result is thus particularly influenced by the ratio of the desired polarization direction to the cross polarization of the satellite reception antenna, that is by the cross-polarization spacing. On the other hand, the implementation of a satellite navigation antenna which covers both frequency bands with a bandwidth of approximately 360 MHz and in so doing satisfies the in part very strict demands on the cross-polarization spacing is technically difficult.
In particular satellite reception antennas having a small construction space are suitable for use on vehicles. Antennas of this kind in accordance with the prior art are known as patch antennas. They are, however, less powerful with respect to the reception at a low angle of elevation and are more complex and/or expensive in design. This disadvantage is remedied in part by ring line antennas such as are described in DE 10 2009 040 910 A. It is desirable, even for such antennas, to improve the cross-polarization spacing over the full bandwidth of the above-described frequency bands L1, L2 or L5.
Satellite reception antennas for satellite navigation are provided for installation on horizontal surfaces of the electrically conductive vehicle body. The substantially horizontal vehicle roof acts as a conductive base surface with respect to the antenna properties.
It is the underlying object of the invention to provide an antenna for the reception of circularly polarized satellite radio signals for satellite navigation which has a high cross-polarization spacing over a frequency range which is as large as possible and which is thus suitable for the acquisition of particularly accurate position location results in a vehicle with sufficient gain and also at low angles of elevation of the radiation characteristics.
This object is satisfied by the features of claim 1.
The advantage is associated with an antenna in accordance with the invention that it can be manufactured particularly inexpensively and is thus particularly suitable for mass production and for use in the mass production of vehicles.
In accordance with the invention an antenna 1 for the reception of circularly polarized satellite radio signals comprises at least one horizontally oriented conductor loop arranged above a conductive base surface 6, comprising an arrangement connected to an antenna connector 5 for the electromagnetic excitation of the conductor loop. The conductor loop is formed by a polygonal or circular closed ring line in a horizontal plane having a height h and extending over the conductive base surface 6. The ring line radiator 2 forms a resonant structure and is electrically excitable by electromagnetic excitation in a manner such that the current distribution of a propagating line wave is adopted on the ring line in a single revolving direction whose phase difference over one revolution amounts to exactly 2π.
Radiators 4, 4a-d that are galvanically coupled to the ring line radiator 2, that are vertical, and that extend toward the conductive base surface 6 are present at ring line coupling points 7 at the periphery of the ring line radiator 2, with the excitation of the conductive loop taking place via one of the radiators as the active radiator 4a and the other radiators are coupled as passive radiators 4b, 4c, 4d to the electrically conductive base surface 6.
At least two vertical passive radiations 4b, 4c, 4d are present which are galvanically coupled to the ring line radiator 2, which extend toward the conductive base surface 6 and of which N vertical radiators 40 are coupled to the electrically conductive base surface 6 over a reactance circuit having an active component 12 whose loss factor is greater than the value 0.1/N. At no point along the ring line radiator 2 are two of these N vertical radiators arranged adjacent to one another. All the remaining passive vertical radiators 4b, 4c are coupled to the base surface 6 via lossless reactance circuits 13. All the radiators are approximately evenly distributed along the ring line radiator 2 so that none of the spacings between mutually adjacent ring line coupling points 7 at the periphery of the ring line radiator 2 is smaller than half the spacing that would result with an equidistant distribution of all the radiators over the stretched length L of the ring line radiator (2).
Advantage embodiments will be explained in more detail in the following:
At least two of the part sections of the ring line radiator 2 that are respectively located between two adjacent ring line coupling points and that have mutually different wave impedances ZL1, ZL2 can be present.
The reactance circuit having the active component 12 for coupling N vertical radiators 4d to a ground connector 11 on the electrically conductive base surface 6 can be formed in each case by the serial connection of a capacitor 15 and a circuit having ohmic losses 12a and each of the remaining passive vertical radiators 4b, 4c can be provided with a lossless reactance circuit 13 realized as a capacitor 15 for coupling to a ground connector point 11 on the electrically conductive base surface 6.
The stretched length L of the ring line of the ring line radiator 2 in resonance can be shortened by the effect of the vertical radiators 4, starting from approximately the line wavelength λ down to approximately half the line wavelength λ.
The active vertical radiator 4a can be provided with a reactance circuit 13 implemented as a capacitor 15 for coupling to the antenna connector 5.
The circuit having ohmic losses 12a can be formed from an ohmic resistor 20.
A parallel oscillating circle—comprising a parallel capacitor 18 and a parallel inductor 17—having a resonant frequency in the vicinity of the frequency band center can be connected in parallel with the ohmic resistor 20 to expand the frequency bandwidth of the cross-polarization spacing.
A respective parallel oscillating circle—comprising a capacitor 18 and an inductor 17—can be connected in parallel with the ohmic resistor 20 and the lossless reactance circuits 13, to which the remaining passive vertical radiators 4b, 4c having the electrically conductive base surface 6 are coupled, can each be formed from the serial connection of a capacitor 15 and a parallel oscillating circle—comprising a parallel capacitor 18 and a parallel inductor 17—and the resonant frequency of the parallel oscillating circles can each be selected as approximately in proximity to the center of a predefined frequency band for expanding the frequency bandwidth of the cross-polarization spacing.
The parallel resonant circle in the lossless reactance circuit 13 and the parallel resonant circuit respectively connected in parallel with the ohmic resistor 20 can be coordinated in this manner such that a maximum of the cross-polarization spacing is adopted in the respective frequency band center of the two satellite navigation frequency bands L1 and L2.
N=1 vertical radiators 4d having a reactance circuit having the active component 12 for coupling to a ground connector 11 on the electrically conductive base surface 6 can be present and said ground connector can be arranged adjacent to the active vertical radiator 4a.
The ring line radiator 2 can be designed as a rectangle at whose corners a respective ring line coupling point 7 having a vertical radiator 4a-d galvanically connected there can be formed.
To support the unidirectionality of the wave propagation on the ring line radiator 2, a further part section of the ring line radiator 2 disposed opposite the first part section and having a wave impedance (ZL2) differing from the wave impedance (ZL1) of the remaining part sections of the ring line radiator 2 can be present.
The lossless reactance circuits 13 of the passive radiators implemented as capacitors 15 for coupling to the conductive base surface 6 or for coupling to the circuit having ohmic losses 12a coupled to the conductive base surface 6 and the capacitor 15 for coupling the active radiator 4a to the antenna connector 5 can be formed in a manner such that the vertical radiators 4, 4a-d are molded at their lower ends to form individually designed areal capacitor electrodes 32a, 32b, 32c, 32d and the capacitors 15 can be configured by interposition of a dielectric plate 33 between the areal capacitor electrodes 32a, 32b, 32c, 32d and the electrically conductive base surface 6 formed as an electrically conductively coated circuit board 35 for coupling the passive radiators 4b, 4c to the electrically conductive base surface 6.
An areal counter-electrode 34 insulated from this film can be configured for the capacitive coupling of the active vertical radiator 4a to the antenna connector 5 and for the capacitive coupling of a passive vertical radiator 4d adjacent to the active vertical radiator 4a to the circuit having ohmic losses 12a on the electrically conductive base surface 6.
The conductive structure, comprising the ring conductor 2 and the vertical radiators 4, 4a-d connected thereto, can be fixed by a dielectric support structure 36 such that the dielectric board 33 is implemented in the form of an air gap.
The associated Figures show in detail:
a)
an antenna in accordance with the invention having a ring line radiator 2 having vertical radiators 4a-4d galvanically coupled to ring line coupling points 7. The passive vertical radiator 4d which is arranged adjacent to the active vertical radiator 4a in the example shown is coupled via the ground connector point 11 to the conductive base surface 6 via the reactance circuit having an active component 12. The excitation of the ring line radiator 2 takes place via the active vertical radiator 4a that is connected to the antenna connector 5 via the lossless reactance circuit 13. The reactance circuits 13 and the reactance circuit having the active component 12 form the resonant structure together with the reactive properties of the ring line circuit 2 and of the vertical radiators 4 in a manner such that the current distribution of a propagating line wave is adopted on the ring line 2 in a single direction of revolution whose phase difference amounts to exactly 2π over one revolution;
b) an antenna in accordance with the invention as in Figure a), but with a changed arrangement of the vertical radiators at the periphery of the ring line radiator 2. Following a sense of revolution, a respective two vertical radiators interconnected with a lossless reactance circuit 13 are arranged between successive vertical radiators interconnected with a reactance circuit having an active component 12. The active radiator 4a is coupled to the antenna connector 5 via the lossless reactance circuit 13;
c) an antenna in accordance with the invention as in Figure b), but, following a sense of revolution, a respective only one vertical radiator interconnected with a lossless reactance circuit 13 is arranged between successive vertical radiators interconnected with a reactance circuit having an active component 12. The active radiator 4a is coupled both via the lossless reactance circuit 13 to the electrically conductive base surface 6 and to the antenna connector 5;
an antenna in accordance with the invention as in
a) an antenna in accordance with the invention as in
b) a circuit diagram of the reactance circuit having the active component 12 comprising the serial connection of the capacitor 15 and the circuit having ohmic losses 12a implemented by the ohmic resistor 20;
c) a circuit diagram of the reactance circuit having the active component 12 as in Figure b), but with a parallel resonant circuit, comprising the parallel capacitor 18 and the parallel inductor 17 in parallel connection with the resistor 20;
the course of the cross-polarization spacing and of the gain for the low incidence of the satellite signals at an angle of elevation of 20°, entered over the frequency in the satellite navigation frequency band L1;
a) implemented, extremely high cross-polarization spacing in dB;
b) an exemplary sufficient cross-polarization spacing in dB;
c) implemented antenna gain in dB;
a self-explanatory exploded diagram to explain the design of the antenna in accordance with the invention described in
an antenna in accordance with the invention similar to in
an antenna in accordance with the invention as in
in the Figure, the upper side of the circuit board 35 of an antenna 1 in accordance with the invention is shown onto which the electrical ring line radiator 2 has been placed. For the configuration of a dual band capable multiband antenna in accordance with the invention—for example for the frequency ranges L1 and L2—the resonance circuit 13 is respectively designed in a multifrequency manner such that both the resonance of the ring line radiator 2 and the required direction of propagation of the line wave on the ring line radiator 2 is given in the mutually separate frequency bands L1 and L2.
This is achieved in the example in
a dual band antenna in accordance with the invention as in
a) with a view of the upper side of the circuit board 35 having vias 16 on the counter-electrode 34 beneath the capacitor electrodes 32;
b) all the SMD circuit elements are correspondingly arranged on the rear side of the circuit board on pads 26 that are connected via vias 16.
The mode of operation of the suppression of the unwanted polarization direction LHCP of an antenna provided for RHCP can be compared to that of a bridge circuit or to a hybrid ring. Such a bridge can, however, only be completely compared for a specific frequency—generally approximately the center frequency of a frequency band. With frequencies differing therefrom, in addition to the wanted radiation in the RHCP mode, the unwanted radiation naturally arises in the opposite direction of rotation, that is the LHCP mode, on excitation at a gate, that is at the active vertical radiator 4a in
The interconnection of the radiator 4d adjacent to the excited radiator 4a and having a reactance circuit having the active component 12 influences the phasing of the voltage at this radiator in a manner such that the unwanted LHCP portion in the radiation is also largely compensated with a frequency offset from the center frequency. It is found in accordance with the invention in this respect that a substantially greater bandwidth of the required cross-polarization spacing can already be achieved with a simple combination of a serial connection of a capacitor 15 having an ohmic resistor 20, as shown in
The low-effort implementation of a reactance circuit having an active component 12 is advantageous in this respect. A particular advantage of the invention also comprises the improvement of the bandwidth of the cross-modulation spacing already being able to be achieved with only N=1, that is with only one single vertical radiator having a reactance circuit having an active component 12—whose loss factors is greater than 0.2. The ratio of the effective resistance/reactance with a serial specification or of the conductance/susceptance with a parallel specification of the reactance circuit is designated as the loss factor of the reactance circuit having the active component 12—analogously to the customary definition.
Provision is made in accordance with the invention, as described above, with N>1, to arrange a plurality of vertical radiators interconnected with the reactance circuit having the active component 12 along the periphery of the ring line radiator 2. Provision is made in accordance with the invention in this case to select the loss factor in accordance with the number N of each of the reactance circuits having the active component 12 as no smaller than 0.2/N.
The bandwidth of the cross-modulation spacing can be further increased by using more complicated circuits. The parallel connection of a parallel resonant circuit, comprising the parallel inductor 17 and the parallel capacitor 18, to the ohmic resistor 20 in
Number | Date | Country | Kind |
---|---|---|---|
10 2017 003 072 | Mar 2017 | DE | national |
Number | Name | Date | Kind |
---|---|---|---|
20110215978 | Lindenmeier et al. | Sep 2011 | A1 |
20120050120 | Lindenmeier et al. | Mar 2012 | A1 |
20140028512 | Lindenmeier | Jan 2014 | A1 |
20150123869 | Bit-Babik et al. | May 2015 | A1 |
20170047665 | Yang | Feb 2017 | A1 |
Number | Date | Country |
---|---|---|
4008505 | Sep 1991 | DE |
2296227 | Mar 2011 | EP |
2424036 | Feb 2012 | EP |
1105354 | Mar 1968 | GB |
6602498 | Aug 1967 | NL |
Entry |
---|
European Search Report for European Application No. 18163139.1 dated Aug. 6, 2018; 4 pages. |
Number | Date | Country | |
---|---|---|---|
20180294571 A1 | Oct 2018 | US |