The present invention is directed to radio frequency communication systems and more particularly to a method and apparatus to mitigate intermodulation effects from adjacent readers in RFID systems.
Fields of endeavor ranging from manufacturing to highway toll collection present a continuing challenge to monitor the movements of objects. There is thus a continuing goal to interrogate the location of objects in an inexpensive and streamlined manner.
One example of an identification system for monitoring the locations of objects uses an RF (radio-frequency) transponder device (commonly known simply as a “tag”) affixed to an object to be monitored, in which a reader or interrogator unit transmits an interrogation signal to the device. The tag receives the interrogation signal and then generates and transmits a responsive signal.
An example will be explained with reference to
Currently in the art, RFID systems use frequency separation and time domain multiplexing in combination to allow multiple readers to operate closely together within the bandwidth limitations imposed by radio regulatory authorities. In transportation and other applications, there is a compelling need for readers to operate in close proximity. In the example of a toll collection system, as seen in
Many technical obstacles limit system performance when readers are closely spaced. One of the major problems or technical obstacles is downlink interference at the tag. That occurs when a tag 104 receives the downlink signals DLS from two or more reader antennas 106, such that the downlink signals DLS interfere with one another. In systems using amplitude modulation such as on-off keying, such interference results in waveform distortion after detection.
Thus, an unaddressed need exists in the art to address the aforementioned deficiencies and inadequacies associated with waveform distortion after detection of the downlink signals from adjacent readers.
It is therefore an object of the present invention to provide an apparatus and method for mitigating intermodulation effects for adjacent readers in amplitude modulation RFID systems.
To achieve the above and other objects, a frequency-selective filter such as a low-pass filter is added at the output of the diode detector of the tag antenna. The raw signal from the detection of the interfering downlink signals includes components based on the frequency of each of the interfering signals, the difference in the frequencies, and the sum of the frequencies. Thus, given a difference in frequencies between adjacent ones of the reader antennas, an appropriate frequency-selective filter can be used to filter out undesired components of the signal.
During the design of the toll barrier or other facility at which the readers will be used, the frequencies are determined, so that the difference in frequencies between any two adjacent ones of the readers is known. That difference in frequencies is used to select the appropriate frequency-selective filter. Alternatively, if a particular frequency-selective filter is desired to be used, the design stage can include selection of the frequency difference accordingly.
A preferred embodiment of the present invention will be set forth in detail with reference to the drawings, in which:
A preferred embodiment of the present invention will be set forth in detail with reference to the drawings, in which like reference numerals refer to like elements throughout.
The tag 104 functions in the following manner. The antenna 300 receives an on-off keying RF signal from a reader, with interference from an adjacent reader. The detection circuitry 302 detects tat signal and outputs a baseband analog signal with a high level of interference. The low-pass filter 306 low-pass filters the signal to reduce the level of interference, in a manner to be explained below. The baseband analog signal with the reduced level of interference is applied to the limiter 308, which applies a digital signal to the baseband decoder and digital processing circuits 310.
The theory of operation of the tag 104 with the low-pass filter 306 will now be explained with reference to
Let:
Vd(t) be the envelope of the desired on-off keyed RF signal;
Vi(t) be the envelope of the interfering on-off keyed RF signal;
ωd be the frequency of the desired RF signal (microwave frequency);
ωi be the frequency of the interfering signal;
Vo be the output of the diode detector; and
Vin be the input to the diode detector.
Then the desired signal, shown in
Vd(t)*cos(ωdt),
while the interfering signal, shown in
Vi(t)*cos(ωit).
The signal received at the detector, shown in
Vin=Vd(t)*cos(ωdt)+Vi(t)*cos(ωit).
The detection process is often modeled as a second-order process, such that
Vo=Vin2.
Substituting from the above,
The first two terms in the equation above represent the output of the diode for the desired and interfering signals as if they were received separately, while the third term represents the results of the interference between those two signals. The effects of the interfering signal (the second term) cannot be removed by the tag. However, the effects of interference in the third term can be reduced as shown below.
Using the following well known identity from trigonometry:
cos A cos B=0.5(cos(A+B)+cos(A−B)),
the third term can be rewritten as
Vi(t)*Vd(t)*cos((ωd+ωi)t)+Vi(t)*Vd(t )*cos((ωd−ωi)t).
The first term is approximately twice the frequency of the desired signal, while the second component is at the difference frequency of the two components. The second component can be filtered out (removed) by attaching a low-pass filter 306 to the output of the diode detector and setting the cutoff frequency of that filter well below the difference frequency. The difference frequency will be much less than the sum of the two frequencies; thus, the filter will also remove the first term. The resulting filtered signal is shown in
Various design options for the low-pass filter 306 will now be described. The filter implementation is directly related to the frequency difference between the desired and interfering signals. When that frequency difference is large compared to the data rate (for example, 10 times) a simple RC low-pass filter can be used because the filter will not remove any of the frequency components of the desired signal.
An example of such a simple RC filter is shown in
When the frequency difference is comparable to the data rate, the low-pass filter implementation will require many components to achieve the same level of performance because the filter must roll off quickly to allow the desired signal to get through and yet attenuate the difference frequency. Various designs for low-pass filters are known in the art and can be used in the present invention.
While a preferred embodiment of the present invention has been set forth in detail above, those skilled in the art who have reviewed the present disclosure will readily appreciate that other embodiments can be realized within the scope of the invention. For example, the use of the present invention in a toll collection system is illustrative rather than limiting. Also, depending on the values of ωd+ωi and ωd−ωi, it may be necessary or desirable to use a high-pass filter instead of, or in addition to, the low-pass filter to remove the terms related to the interference effects without also filtering out the desired signal. Therefore, the present invention should be construed as limited only by the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
3866124 | Wycoff | Feb 1975 | A |
4665395 | Van Ness | May 1987 | A |
5128669 | Dadds et al. | Jul 1992 | A |
5164732 | Brockelsby et al. | Nov 1992 | A |
5525992 | Froschermeier | Jun 1996 | A |
5701127 | Sharpe | Dec 1997 | A |
5757288 | Dixon et al. | May 1998 | A |
5883575 | Ruby et al. | Mar 1999 | A |
6064320 | d'Hont et al. | May 2000 | A |
7109844 | Taki et al. | Sep 2006 | B2 |
Number | Date | Country | |
---|---|---|---|
20080117052 A1 | May 2008 | US |