This application claims the benefit, under 35 U.S.C. §119 of French Patent Application 1261642, filed Dec. 5, 2012.
The present invention relates to the field of radio frequency devices realised on circuit boards comprising a dielectric substrate. The invention relates more specifically to devices for transmitting and/or receiving radio frequency signals comprising at least one antenna and/or one filter realised in printed circuit technology on a substrate of dielectric material.
To obtain a high level of integration, radio frequency devices are traditionally realised on one or more printed circuit boards having a dielectric substrate. In such devices, the antenna is traditionally realised by a layer of conductive material of appropriate geometric form which is placed on the dielectric substrate. The conductive layer can be formed by one or more radiating strands of a particular form or by a conductive plate provided with slots. These devices also traditionally comprise filters. These filters can be realised, entirely or partially, by conductive lines, for example microstrip lines, arranged on the dielectric substrate.
It is known that the behaviour of these antennae and/or filters is strongly linked to the electrical and mechanical properties of the dielectric material of the substrate. It is also known that, in the field of consumer electronics devices, the material commonly used to manufacture the substrate is of FR4 type which is a low-cost material. The disadvantage of this material is that it has a relatively high dispersion in terms of dielectric permittivity values. This range of variation in the permittivity is larger or smaller according to the manufacturers. Generally, the more expensive the material, the more the range of variation in the permittivity is reduced.
This dispersion of the permittivity can impact several critical functions of the reception and/or transmission channel of the radio frequency devices, notably the behaviour of the antennae and filters realised with this dielectric substrate. More specifically, it creates frequency drifts in the response of the filters and causes the impedance of the antennae to drift thus leading to a degradation in performance thereof.
Currently, manufacturers of radio frequency devices on printed circuits have two options to prevent these drifts:
1) they use a dielectric substrate having a low variation in permittivity, which incurs an additional cost for the device; or
2) they modify the technical characteristics of the device to take into account this potential variation in the permittivity of the substrate by increasing the bandwidth of the antennae, for example, but this leads to a degradation in performance of the device.
The invention proposes another solution making it possible to continue to use a low-cost dielectric material without degrading performance of the antenna or of the filter of the radio frequency device.
According to the invention, it is proposed to equip the radio frequency device with a circuit for measuring a value linked to the permittivity of the dielectric substrates and with circuits making it possible to adjust the frequency response of the filter and the impedance of the antenna according to the measured permittivity value.
For this purpose, the invention relates to a device for transmitting and/or receiving radio frequency signals comprising at least one antenna and/or one filter realised in printed technology on a dielectric substrate, characterised in that it further comprises a circuit for measuring a value linked to the dielectric permittivity of the substrate able to deliver a measured value linked to the permittivity and adjustment means able to adjust the impedance of the antenna and/or the frequency response of said filter according to said measured value.
Thus, according to the invention, the impedance of the antenna and/or the frequency response of the filters of the device are adjusted by taking into account the real value of the permittivity of the substrate. The mismatching of the antenna and/or the frequency drifts in the response of the filter linked to the dispersion of the permittivity of the substrate are thus avoided.
According to a particular embodiment, the adjustment means comprise:
According to one embodiment, the impedance matching network comprises an adjustable capacitor digitally controlled by said at least one digital control signal. The variable-capacitance element inside said at least one filter is a varactor diode.
According to a particular embodiment, the circuit measuring a value linked to the permittivity comprises:
According to a particular embodiment, said resonator is a ring resonator. According to a variant, the resonator is a resonator comprising a rectilinear microstrip line having a length substantially equal to
where λg is the radio frequency signal wavelength.
Advantageously, the resonator is designed to have a resonance frequency close to the frequency of the radio frequency signals transmitted or received.
According to a particular embodiment wherein the device comprises at least two transmission and/or reception channels operating at different operating frequencies and each comprising at least one antenna and/or at least one filter realised in printed technology on a single dielectric substrate and further comprises a circuit measuring a value linked to the permittivity for measuring the relative permittivity of said dielectric substrate, the resonator of the measuring circuit is designed to have a resonance frequency close to the highest operating frequency which is generally the frequency most sensitive to the drifts caused by the dispersion of the permittivity of the substrate.
The purpose of the invention is also a method for adjusting the impedance of an antenna and/or the frequency response of a filter of a device such as previously defined, which comprises the following steps:
Advantageously, this method is implemented only once when the device is first switched on.
Other advantages may also occur to those skilled in the art upon reading the examples below, illustrated by the annexed figures, given by way of illustration:
This figure shows that a relative permittivity dispersion ∈r of around ±10% can lead to a frequency drift of ±200 MHz, which is unacceptable in many fields, notably in the field of transmission and reception of multimedia signals, such as 2.4 & 5 GHz Wi-Fi, DECT, 3G, Bluetooth, ZigBee or GPS signals.
The higher the frequency, the more the impact of the dispersion of the relative permittivity value ∈r of the substrate impacts the response of the filter, and this is true regardless of the type of filter (band-rejection, band-pass, low-pass, high-pass).
The dispersion of the relative permittivity of the substrate likewise impacts the impedance of antennae realised in printed technology on dielectric substrate.
According to the invention, it is therefore proposed to adjust the frequency response of the filter and/or the impedance of the antenna of radio frequency devices according to the effective value of the relative permittivity ∈r of the dielectric substrate on which they are realised.
According to the invention, it is proposed to measure a value linked to the relative permittivity ∈r of the substrate then to adjust the frequency response of the filter and/or the impedance of the radio frequency device according to the measured value.
The relative permittivity ∈r of the dielectric substrate of a printed circuit board can be measured according to different known techniques. One of them consists in realising, on the circuit board for which the permittivity of the substrate is to be measured, a ring resonator, for example with microstrip lines, then determining the resonance frequency of this ring. Such a resonator is shown diagrammatically in
In the case of a resonator circuit with microstrip lines, the electromagnetic waves propagate in a heterogeneous medium formed from substrate, microstrip lines and air. The dielectric permittivity of this heterogeneous medium, commonly called effective dielectric permittivity ∈r eff, is determined by the following equations:
where l is the circumference of the ring of the resonator and is equal to
λg is the wavelength of radio frequency signals propagating in said heterogeneous medium at the resonance frequency f, r is the radius of the ring of the resonator and λ0 is the wavelength of radio frequency signals propagating in the vacuum at the resonance frequency f;
If equations (1) and (2) are combined, the following equation is obtained:
where f is the resonance frequency of the ring and c is the speed of light in the vacuum (3.108 m/s).
The preceding equations show the relationships between the resonance frequency f of the resonator and the effective dielectric permittivity ∈r eff. This latter is linked to the relative permittivity ∈r of the substrate by the following relationship:
where h represents the thickness of the substrate and w is the width of the microstrip line forming the ring.
The relative permittivity ∈r of the substrate is therefore obtained by the following relationship:
Thus, by determining the resonance frequency f of the ring, it is possible to deduce very precisely the effective relative permittivity ∈r eff using equation (3) then the relative permittivity ∈r of the substrate using equation (5).
Determining the resonance frequency f consists in determining the signal frequency for which the power delivered by the resonator is maximum.
As can be seen in this figure, the response of the resonator has an amplitude peak at the resonance frequency f (around 5.25 GHz in the present case) and at its harmonics.
Detecting this amplitude peak makes it possible to determine the resonance frequency f of the resonator and to deduce the relative permittivity ∈r of the substrate using equations (3) and (5), the parameters n, l, h and w being known parameters.
To determine the relative permittivity ∈r of the substrate, the circuit measuring a value linked to the permittivity must therefore not only comprise a resonator such as defined in
In reference to
The circuit measuring a value linked to the permittivity also comprises a memory 16 connected to the microcontroller 14 for storing at least temporarily the power values measured by the power measuring circuit 13.
The generator 11 sequentially delivers a plurality of radio frequency signals in a frequency band to be analysed. As indicated above, this frequency band to be analysed includes the so-called nominal resonance frequency of the resonator obtained for a nominal relative permittivity value provided by the manufacturer of the substrate (for example, ∈r=4.55) and the frequencies around this nominal resonance frequency corresponding to the drifts of the resonance frequency which would be due to the dispersion of the relative permittivity of the substrate.
For example, if we consider a resonator realised on a substrate of FR4 type having a nominal relative permittivity ∈r equal to 4.5 liable to vary by around ±10%, that is to say between 4.05 and 4.95, whose resonance frequency varies between 5.3 GHz and 5.7 GHz as shown in the diagram of
The frequency band is swept over with a predetermined value step, for example 100 KHz. The smaller this step, the more accurately the resonance frequency of the resonator will be determined.
The resonator 12 is successively supplied with each of the signals generated by the generator 11. The amplitude of the signal delivered thereby thus has a maximum as the resonance frequency of the resonator is approached.
At the output of the resonator 12, the power measuring circuit 13 measures the power of the signal delivered by the resonator 12. The diagram of an example of a logarithmic power measuring circuit is shown in
The microcontroller 14 stores the power values measured by circuit 13 in the memory 16 then determines the maximum power value for a full sweep of the frequency band to be analysed.
The microcontroller 14 then determines the frequency of the signal supplied to the resonator giving this maximum power. This frequency corresponds to the resonance frequency f of the resonator.
The microcontroller 14 supplies this resonance frequency value f to the processor 15 which calculates, by means of equations (3) and (5), the relative permittivity value ∈r of the substrate.
Once this relative permittivity value is calculated, the circuit 10 measuring a value linked to the permittivity, by the intermediary of the processor 15, supplies this value to an adjustment control circuit 20 able to control adjustment means intended to adjust the impedance of antennae and/or the frequency response of filters of a radio frequency device.
In
A device for transmitting and/or receiving radio frequency signals according to the invention is shown in
This transmission/reception channel comprises an antenna 31, a band-pass filter 32a for filtering the RF signals received by the antenna, a low noise amplifier 33a for amplifying the signals output from the filter 32a and a processing circuit 34 for processing the RF signals delivered by the amplifier 33a. This circuit 34 is notably able to convert the received RF signals into baseband signals. The channel also comprises a power amplifier 33b for amplifying the RF signals to be transmitted generated by the processing circuit 34 and a high-pass filter 32b for filtering the signals amplified by the amplifier 33b. A switching circuit 35 is also placed between filters 32a and 32b and the antenna 31 in order to connect the antenna 31 selectively to filter 32a (reception) and filter 32b (transmission).
For the implementation of the invention, the device 30 also comprises a measuring circuit and a control circuit 20 as previously described and a matching network 36 for adjusting the impedance of the antenna to a predetermined value, for example 50 ohms, according to the measured relative permittivity. Moreover, filters 32a and 32b are filters whose frequency response is adjustable according to the measured relative permittivity.
The adjustment control circuit 20 delivers three control signals:
The matching network 36 is for example formed by one or more elementary impedance networks having an L or a Pi topology. This network comprises at least one DTC (Digitally Tunable Capacitor) constructed from a plurality of switched capacitors digitally controlled by a plurality of bits b1 . . . bi of the control signal C1 as shown in
In this figure, the matching network 36 comprises two elementary LC networks having an L topology. Each elementary network comprises an inductor Lp between the input and the output of the elementary network and 3 parallel switched capacitors Cp between the input of the elementary network and the earth. Each of the switched capacitors is controlled by a bit of the control signal C1. In this example, the control signal C1 therefore comprises 6 bits to vary the impedance of the antenna 31, that is to say 64 possible values.
Likewise, filters 32a and 32b each comprise at least one DTC or one varactor diode to vary their frequency response according to control signals C2 and C3.
The different control signals C1, C2, C3 necessary to obtain the different possible adjustments are defined in advance and are stored in the look-up table 20.
During operation, when the measuring circuit 10 delivers a relative permittivity value of the substrate, this latter is transmitted to the look-up table 20 which delivers the appropriate control signals C1, C2, C3 to adjust the matching network 36 and filters 32a and 32b.
This adjustment of the matching network and filters is preferably carried out only once when the radio frequency device is first switched on.
In reference to
The device of the invention can only comprise one transmission channel or one reception channel. In contrast, it can also comprise a plurality of transmission/reception channels as shown in
The first channel for transmitting/receiving 5 GHz Wi-Fi signals is identical to that of
The second channel for transmitting/receiving 2.4 GHz Wi-Fi signals comprises an antenna 301′, a matching network 306′, a band-pass filter 302a′, a low noise amplifier 303a′, a low-pass filter 302b′ and a power amplifier 303b′ arranged in the same way as the corresponding elements of the first transmission/reception channel. Note, however, that the high-pass filter (302b) in the first transmission/reception channel is replaced by a low-pass filter (302b′) in the second transmission/reception channel.
Device 300 also comprises a switching circuit 305 and a processing circuit 304 common to the two reception channels. The switching circuit 305 selectively connects filters 302a and 302b to antenna 301 via matching network 306 and filters 302a′ and 302b′ to antenna 301′ via matching network 306′. Processing circuit 304 carries out the conversion of the radio frequency signals into baseband signals and vice versa.
In this embodiment, control circuit 200 produces control signals C1, C2, C3, C1′, C2′ and C3′ for controlling respectively the adjustable elements 306, 302b, 302a, 306′, 302b′ and 302a′.
The adjustment of the adjustable elements of the device is performed as previously described for the device of
According to a variant embodiment, the device comprises only one resonator to reduce the space occupied by the measuring circuit. In this particular embodiment, we preferably choose a resonator having a resonance frequency close to the highest working frequency of the device, in the present case 5 GHz, in order to further minimise the space occupied by the resonator.
This matching of the frequency response of the filter and of the impedance of the antennae is therefore particularly useful in the case of a multi-radio device realised on low-cost substrates, for example substrates of FR4 type.
Although the invention has been described in relation to two particular embodiments, it is obvious that it is in no way restricted and that it comprises all the technical equivalents of the means described together with their combinations if the latter fall within the scope of the invention.
Naturally, resonators of types other than ring resonators can be used, notably resonators comprising a rectilinear microstrip line having a length substantially equal to
The invention is applicable to a device which comprises only one transmission channel or only one reception channel. It is also applicable to a device wherein only the impedance of the antenna is adjusted (without modifying the frequency response of the filters) or wherein only the frequency response of the filters is adjusted (without modifying the impedance of the antenna).
Number | Date | Country | Kind |
---|---|---|---|
12 61642 | Dec 2012 | FR | national |
Number | Name | Date | Kind |
---|---|---|---|
7834813 | Caimi | Nov 2010 | B2 |
8618817 | Jakoby | Dec 2013 | B2 |
20060281423 | Caimi et al. | Dec 2006 | A1 |
20080186239 | Itsuji | Aug 2008 | A1 |
20100148804 | Jakoby | Jun 2010 | A1 |
20100168817 | Yamamoto et al. | Jul 2010 | A1 |
Number | Date | Country |
---|---|---|
101496222 | Jul 2009 | CN |
102301530 | Dec 2009 | CN |
0971227 | Jan 2000 | EP |
1112485 | Dec 2009 | EP |
2006275687 | Oct 2006 | JP |
2011087380 | Aug 2011 | KR |
Entry |
---|
Search Rept: dated Jun. 17, 2013. |
Janezic et al. “ Broadband Complex Permittivity Measurements of Dielectric Substrates using a Split-Cylinder Resonator”, 2004 IEEE MTT-S Digest, 2004, p. 1817-1820, IEEE, Boulder, CO. |
Semouchkina et al. “High Frequency Permittivity Determination by Spectra Simulation and Measurement of Microstrip Ring Resonators”, Electronics Letters, May 25, 2005, vol. 36, No. 11, p. 956-958, University Park, PA. |
Number | Date | Country | |
---|---|---|---|
20140159987 A1 | Jun 2014 | US |