Field of the Invention
The invention relates generally to a system and method for determining a location of an interfering signal source.
Background Information
Signals which interfere with GNSS receivers, whether unintentional or intentional, may cause significant degradation in performance of such receivers and, in some cases, may represent a serious threat. Some interfering signal sources are simply electronic devices which, through poor design or malfunction, are accidentally transmitting on GNSS frequencies of interest (e.g., L1 or L2). Other interfering signal sources are specifically designed to cause interference. For example, while illegal to sell, possess or use in the US, Canada and UK, handheld GNSS “personal privacy devices” (i.e., jammers) are widely available and inexpensive. Such jammers typically operate at power levels of 200-300 milliwatts and claim to be effective for a range of 5-10 meters. However, such jammers may adversely affect GNSS receivers at a range of more than 1 kilometer.
Determining the position of a jammer in real-time or near real-time is a challenging problem. A jammer's signal is typically wideband in nature and resembles a pulse or chirp with a period that is likely not known by a party (e.g., law enforcement) attempting to determine the location of the jammer. In addition, although a jammer's operating frequency band may be known or ascertained, its precise operating frequency is likely not known. Also, a jammer may vary its operating frequency over time further complicating the problem of determining its location.
In brief summary, the present invention provides a system and method for determining a location of a GNSS jammer with accuracy on the order of a few meters. The system includes three or more augmented GNSS receivers which are placed at known locations separated from one other by minimum distances. The receivers are networked with a server or other equipment which is capable of performing the necessary processing on data samples collected by the receivers.
Following initialization, each receiver simultaneously operates to collect raw I/Q data at GNSS frequencies of interest at a rate on the order of 5 megasamples per second. The collected data samples are filtered and downconverted to intermediate frequency (IF), digitized, and time tagged with the current time of the receiver which collected the samples. The collected samples may be stored locally by the receiver before they are transmitted over the network to the server.
The server initially processes the samples from a given one of the receivers in an effort to identify an interfering signal (or signals) whose power level exceeds a threshold that is considered significant. Assuming that at least one interfering signal is so identified, the server processes the samples to isolate a data set associated with the interfering signal. The server then proceeds to attempt to identify the same interfering signal within the collected data samples from at least two other receivers and isolate the associated data sets.
With at least three data sets collected from three different receivers, the server next performs a cross correlation of a pair of data sets in order to compute a time difference of arrival (TDOA) value which represents the time difference between when the interfering signal arrived at each of two different receivers. The cross correlation function is repeated for each unique pair of data sets.
In order to improve the accuracy of the location determination, the server processes the results of the cross correlations with a discriminator function. The discriminator function yields a significantly more precise computation of the TDOA, which results in greatly improved accuracy in determining the location of the jammer. Using the results of the discriminator function, the server computes a series of hyperbolic curves for each TDOA and, in turn, determines an intersection (or best fit) of such curves which represents the location of the jammer accurate to within a few meters.
The invention description below refers to the accompanying drawings, of which:
Server 106 may be implemented as, for example, a commercially available personal computer (PC), notebook or other computing device which has sufficient CPU, memory, mass storage and other resources to perform the data processing operations described herein. Alternatively, multiple servers (not shown) may be used to distribute the data processing load and improve performance.
Augmented GNSS receivers 102a-102e, network 104 and server 106 together form a system 110 for determining the location of an interfering signal source. An interfering signal source 108, whose location is initially unknown, is present in environment 100 and is transmitting one or more signals which interfere with the normal operations of augmented GNSS receivers 102a-102e. Interfering signal source 108 may represent, for example, a truck driver operating a handheld GNSS jammer.
A local PC 206 is coupled to front end 202 and a removable hard drive 208, and includes a network interface card (not shown) or other interface to network 104. Front end 202 includes an RF section 210, a Multiple Independent Nomadic Stargazer (MINOS) and processor section 212, an analog to digital (A/D) sampling section 214, and a digital section 216. Alternatively, augmented GNSS receiver 102a may be constructed without local PC 206 or removable hard drive 208 provided that sufficient random access memory (RAM) and appropriate network connectivity are provided, thereby enabling data samples collected by receiver 102a to be stored and forwarded to server 106.
GNSS antenna 200 may be implemented with a GPS-702-GG GNSS antenna available from NovAtel Inc. of Calgary, Alberta. GNSS front end 202 may be implemented with a Digital GNSS Front End (DGFE) also available from NovAtel Inc. Chip scale atomic clock 204 may be implemented with a Symmetricom Chip Scale Atomic Clock. Local PC 206 and removable hard drive 208 may be implemented with an Intel® Atom™ based PC board with a 1 TB removable hard drive, respectively. MINOS and processor section 212 may be implemented with an OEMV1DF also available from NovAtel Inc.
In general, augmented GNSS receiver 102a is capable of receiving signals in the GNSS bands including potentially interfering signals. Specifically, signals received by GNSS antenna 200, including L1 and L2, are passed to RF section 210 where they are filtered and downconverted to IF. The filtered and downconverted signals are then passed to A/D sampling section 214 which generates I/Q data samples at a rate preferably on the order of at least approximately 2.5 megasamples per second. Alternatively, higher sampling rates, up to at least approximately 20 to 30 megasamples per second, may be used provided that augmented GNSS receiver 102a is adequately provisioned to either store locally or store and forward the collected samples.
At a sampling rate of 5 megasamples per second, the time between successive samples is 200 ns or a distance equivalent of approximately 60 meters, which is not sufficiently precise for most applications. However, as described in detail below in connection with
The data samples are time-tagged by digital section 216 with the current time (e.g., the time indicated by chip scale atomic clock 204) of augmented GNSS receiver 102a. The time-tagged data samples may be stored by local PC 206 on removable hard drive 208 along with the phase and pseudorange for the GNSS satellites, and the position and clock offset information for augmented GNSS receiver 102a. The time-tagged data samples and related information are subsequently packetized for transmission over network 104 to server 106.
The above-described process of receiving signals, generating time-tagged samples and forwarding those samples to server 106 is carried out in parallel in each of augmented GNSS receivers 102a-102e (
The method begins at step 302 with the collection of time-tagged RF samples from each of augmented GNSS receivers 102a-102e and conversion of those samples to the frequency domain by way of a fast Fourier transform (FFT) function. Next, at step 304, the converted samples from a given one of receivers 102a-102e are analyzed in an effort to identify an interfering signal (or signals) having a power level above a threshold of interest. In general, an interfering signal would be expected to have a power level significantly higher than those of GNSS signals of interest. Further, if more than one interfering signal is present, each such signal will likely have at least one characteristic which will permit unique identification. For example, an interfering signal may have a unique frequency signature, power spike, signal transients, harmonics, angle of arrival at a given augmented GNSS receiver 102a-102e, or other characteristics.
Assuming that at least one interfering signal is identified at step 304, the method then continues to step 306 where converted samples associated with the interfering signal are located among the samples originating from at least two other augmented GNSS receivers 102a-102e, thereby creating a total of at least three data sets associated with the interfering signal.
Next, at step 308, for each of the at least three data sets associated with the interfering signal, all non-signal related FFT spectral frequencies are set to zero and the data sets are converted back to the time domain using an inverse FFT function. At step 310, by using the clock offset information previously received from augmented GNSS receivers 102a-102e as well as the time-tags, server 106 is able to perform a cross-correlation function with an initial pair of the (time domain) data sets which represent simultaneous observations by two augmented GNSS receivers 102a-102e. Through step 312, this processing is continued iteratively until all unique pairs of data sets have been cross-correlated.
At step 314, the cross-correlation for each pair of data sets is examined for the peak correlation value. As described in detail below in connection with
If the ratio of a correlation's peak value over the average correlation is above a specified tolerance, the computed TDOA may be corrected for the difference in each augmented GNSS receiver's clock offset.
Once a TDOA is computed for each unique pair of data sets, the method continues to step 316 at which hyperbolic curves are computed for each TDOA according to the following equation:
where (xi, yi) is the unknown location of the GNSS jammer
Results of the jammer location determination are reported or displayed (or both) at step 318. For example, in
The method of least squares is typically used to solve for the unknown location of a GNSS jammer (xi,yi) using a linearization of the TDOA equations for each combination of augmented GNSS receivers (AB, BC, AC). If the TDOAs computed using more than three augmented GNSS receivers are used in the least squares computation, the root mean squared of the residuals may be computed and compared against a tolerance to determine if the computed position is acceptable. Thus, the overall process of determining the location of a GNSS jammer (xi,yi) may be summarized as follows:
1. Solve for the TDOA using cross correlation and a discriminator function.
2. The TDOA equation is a hyperbolic line equation that can be written with TDOA as a function of the known augmented GNSS receiver coordinates and the unknown GNSS jammer coordinates. In least squares terms: 1=f(x), where 1=observations(TDOA) and x are the unknowns (GNSS jammer coordinates).
3. Linearize the TDOA function using Ax+w=1, where A is the design matrix formed by A=df/dx . . . derivative of TDOA equation with respect to the unknowns and w is the misclosure matrix (TDOA−TDOA′), where TDOA′ is computed using approximate coordinates (x0) for the GNSS jammer.
4. Using the least squares process solve for the corrections to x by:
Δ=(ATCl A)−1ATCl w
where C1 is the covariance matrix of the observations.
x=x0+Δ, where x0 are the approximate coordinates of the GNSS jammer.
5. Since the TDOA equation is non-linear, iterate steps 3 and 4. After updating x in step 4, reform A and w with the new approximate coordinates and then solve for A again, continuing until A (the corrections to the unknowns) falls below a certain tolerance (e.g., 1 mm).
As shown
For the case where Ye is less than YL, the value of Tos may be computed using the equation:
For the case where Ye is greater than YL, the value of Tos may be computed using the equation:
Through the use of the discriminator function described above, accuracy in the determination of a jammer's location may be improved from on the order of +/−60 meters to +/−3 meters.
If a jammer or other source of an interfering signal is moving, there will be an apparent Doppler shift of its frequency observed by augmented GNSS receivers 102a-102e (
The foregoing description has been directed to particular embodiments of this invention. It will be apparent, however, that other variations and modifications may be made to the described embodiments, with the attainment of some or all of their advantages. Also, the procedures, processes and/or modules described herein may be implemented in hardware, software, embodied as a computer-readable medium having program instructions, firmware, or a combination thereof.
Number | Name | Date | Kind |
---|---|---|---|
5008679 | Effland | Apr 1991 | A |
5936571 | Desjardins | Aug 1999 | A |
6882310 | Drentea | Apr 2005 | B1 |
7512492 | Irvin et al. | Mar 2009 | B2 |
8085201 | Ladd et al. | Dec 2011 | B2 |
8138975 | Bull et al. | Mar 2012 | B2 |
8446310 | Law et al. | May 2013 | B2 |
8558738 | Ladd et al. | Oct 2013 | B2 |
8587478 | Kang | Nov 2013 | B1 |
8743725 | Wigren | Jun 2014 | B2 |
9063215 | Perthold | Jun 2015 | B2 |
9172514 | Wigren | Oct 2015 | B2 |
20030112905 | Heinzl | Jun 2003 | A1 |
20050285781 | Park | Dec 2005 | A1 |
20120062426 | Tocker | Mar 2012 | A1 |
20140218240 | Kpodzo | Aug 2014 | A1 |
20150035699 | Yun | Feb 2015 | A1 |
Number | Date | Country |
---|---|---|
WO 9711383 | Mar 1997 | WO |
WO 0165271 | Sep 2001 | WO |
WO 2011160697 | Dec 2011 | WO |
WO 2014084512 | Jun 2014 | WO |
Entry |
---|
Bhatti J A et al., “Development and Demonstration of a TDOA-Based GNSS Interference Signal Localization System,” PLANS 2012—Proceedings of IEEE/ION Plans 2012, The Institute of Navigation, 8551 Rixlew Lane Suite 360 Manassas, VA 20109, Apr. 26, 2012, pp. 455-469. |
Oscar lsoz et al, “Development of a deployable low cost interference detection and localization system for the GNSS L1/E1 band” Satellite Navigation Technologies and European Workshop on GNSS Signals and Signal Processing (Navitec), 2010 5th ESA Workshop on, IEEE, Dec. 8, 2010, pp. 1-4. |
Lindstrom Jonas et al., “GNSS Interference Detection and Localization using a Network of Low Cost Front-End Modules” GNSS 2007—Proceedings of the 20th International Technical Meeting of the Satellite Division of the Institute of Navigation, 8551 Rixlew Lane Suite 360 Manassas, VA 20109, Sep. 28, 2007, pp. 1165-1172. |
Konstantin Gromov et al, “GIDL: Generalized Interference Detection and Localization System” GPS 2000—Proceedings of the 13th International Technical Meeting of the Satellite Division of the Institute of Navigation, 8551 Rixlew Lane Suite 360 Manassas, VA 20109, Sep. 22, 2000, pp. 447-457. |
European Search Report mailed Dec. 27, 2015 for European Patent Application No. 15172301.2-1812 for Novatel, Inc., 9 pages. |
Number | Date | Country | |
---|---|---|---|
20150369922 A1 | Dec 2015 | US |