The present invention is directed to precise local positioning systems, and more particularly to a method and system for self-surveying of ground transmitters.
Local positioning systems that employ a set of ground transmitters (pseudolites) require pre-survey of the location of each of the ground transmitters at a centimeter-level of accuracy for initializing the precise positioning capabilities of each ground transmitter. The precise relative or absolute positioning of ground transmitters often requires surveying techniques that employ GPS Real Time Kinematic (RTK) solutions. However, a GPS RTK solution may not be possible when ground transmitters are placed at locations with poor or no access to GPS satellites. For example, a GPS RTK solution may not be achievable in a mining pit.
According to another approach, the location of a given ground transmitter can be determined using information on the geometric motion of an array of ground transmitters. However, such an approach requires the ground transmitters to move relative to each other for self-surveying of their relative locations.
According to another approach, ground transmitters can self-survey their locations by tracking each other's multi-frequency carrier signals for resolving integer biases in a cascaded manner with little or no geometric motion information. However, the ground transmitters are required to transmit and track multi-frequency carrier signals, which adds to undesired complexity.
Thus, in view of the above problems, there is a need for a method and system to allow ground transmitters to self-survey their location at a centimeter-level of accuracy without resorting to requiring geometric motion information on the ground transmitters and without requiring the ground transmitters to transmit and track multi-frequency carrier signals.
According to one aspect of certain non-limiting embodiments, a position solution can be determined using an array of ground transmitters. Each ground transmitter of the array is capable of self-surveying its own location relative to the location of other ground transmitters in the array by generating ranging signals associated with a wideband code modulation with a chipping rate of faster than 30 MHz, and by tracking other ranging signals generated by the other ground transmitters in the array.
Each ground transmitter in array 100 can transmit and receive wideband signals 110. According to certain embodiments, the receiver section and the transmitter section of each ground transmitter of array 100, are clocked by the single common oscillator clock, such as clocks 102e, 104e, 106e, and 108e.
In an array of two ground transmitters, each ground transmitter is capable of determining their relative distance to the other ground transmitter in the array. In an array of three ground transmitters, each ground transmitter is capable of determining its 2-D location. If an array of at least four ground transmitters is deployed over a local area of interest, the ground transmitters are capable of determining their 3-D relative locations, and together, the ground transmitters in the array can provide a 3-D positioning solution to a given rover.
In the case of an array with more than four ground transmitters, it is not necessary for all the ground transmitters to have line of sight (LOS) to all the other ground transmitters in the array. If a particular ground transmitter in the array has LOS to at least three other ground transmitters in the array, then the particular ground transmitter can be self-surveyed relative to the ground transmitters that are in the line of sight.
At block 202 of
At block 208, each ground transmitter that has received wideband ranging signals measures the code phases of the received wideband ranging signals. At block 210, the code phase measurements measured by the ground transmitters are collected at a central unit. The central unit may reside in one of the ground transmitters in the array, according to certain embodiments. In other embodiments, the central unit may reside elsewhere.
At block 212, the collected phase measurements are used in formulating a matrix equation. The formulation of such a matrix equation is described in greater detail herein. At block 214, the matrix equation of block 212 is solved for cross ranges and/or relative clock biases. The solution of such a matrix equation is described in greater detail herein. At block 216, the relative location of each ground transmitter can be determined based on the resolved cross ranges.
Thus, the array of ground transmitters as described with reference to
The code phase measurements that are measured by the ground transmitters in the array include information on cross ranges and clock biases. For example, in an array comprising four ground transmitters, such as in
Code phase measurements at ground transmitter, GT1, can be modeled mathematically as:
Φ12=R1-2+T2−T1+ε12
Φ13=R1-3+T3−T1+ε13
Φ14=R1-4+T4−T1+ε14
where,
Φ12: Code phase of signal transmitted by GT2 and measured at GT1
Φ13: Code phase of signal transmitted by GT3 and measured at GT1
Φ14: Code phase of signal transmitted by GT4 and measured at GT1
R1-2: Cross range between GT1 and GT2
R1-3: Cross range between GT1 and GT3
R1-4: Cross range between GT1 and GT4
T1: Clock bias of GT1
T2: Clock bias of GT2
T3: Clock bias of GT3
T4: Clock bias of GT4
ε12: Noise of signal transmitted by GT2 and measured at GT1
ε13: Noise of signal transmitted by GT3 and measured at GT1
ε14: Noise of signal transmitted by GT4 and measured at GT1
The noise (ε) includes line biases that may be pre-calibrated.
Code phase measurements at ground transmitter, GT2, can be modeled mathematically as:
Φ21=R1-2+T1−T2+ε21
Φ23=R2-3+T3−T2+ε23
Φ24=R2-4+T4−T2+ε24
where,
Φ21: Code phase of signal transmitted by GT1 and measured at GT2
Φ23: Code phase of signal transmitted by GT3 and measured at GT2
Φ24: Code phase of signal transmitted by GT4 and measured at GT2
R1-2: Cross range between GT1 and GT2
R2-3: Cross range between GT2 and GT3
R2-4: Cross range between GT2 and GT4
T1: Clock bias of GT1
T2: Clock bias of GT2
T3: Clock bias of GT3
T4: Clock bias of GT4
ε21: Noise of signal transmitted by GT1 and measured at GT2
ε23: Noise of signal transmitted by GT3 and measured at GT2
ε24: Noise of signal transmitted by GT4 and measured at GT2
Code phase measurements at ground transmitter, GT3, can be modeled mathematically as:
Φ31=R1-3+T1−T3+ε31
Φ32=R2-3+T2−T3+ε32
Φ34=R3-4+T4−T3+ε34
where,
Φ31: Code phase of signal transmitted by GT1 and measured at GT3
Φ32: Code phase of signal transmitted by GT2 and measured at GT3
Φ34: Code phase of signal transmitted by GT4 and measured at GT3
R1-3: Cross range between GT1 and GT3
R2-3: Cross range between GT2 and GT3
R3-4: Cross range between GT3 and GT4
T1: Clock bias of GT1
T2: Clock bias of GT2
T3: Clock bias of GT3
T4: Clock bias of GT4
ε31: Noise of signal transmitted by GT1 and measured at GT3
ε32: Noise of signal transmitted by GT2 and measured at GT3
ε34: Noise of signal transmitted by GT4 and measured at GT3
Code phase measurements at ground transmitter, GT4, can be modeled mathematically as:
Φ41=R1-4+T1−T4+ε41
Φ42=R2-4+T2−T4+ε42
Φ43=R3-4+T3−T4+ε43
where,
Φ41: Code phase of signal transmitted by GT1 and measured at GT4
Φ42: Code phase of signal transmitted by GT2 and measured at GT4
Φ43: Code phase of signal transmitted by GT3 and measured at GT4
R1-4: Cross range between GT1 and GT4
R2-4: Cross range between GT2 and GT4
R3-4: Cross range between GT3 and GT4
T1: Clock bias of GT1
T2: Clock bias of GT2
T3: Clock bias of GT3
T4: Clock bias of GT4
ε41: Noise of signal transmitted by GT1 and measured at GT4
ε42: Noise of signal transmitted by GT2 and measured at GT4
ε43: Noise of signal transmitted by GT3 and measured at GT4
The network-based approach allows the formulation of all the code phase measurements from the array of ground transmitters into a single matrix as follows:
The above matrix equation can be solved for cross ranges and relative clock biases as follows:
The code-based cross ranges and relative clock biases are observable at each measurement epoch. The use of wideband signals can provide the accuracy of code-based cross ranges at about 15 cm in typical multi-path environments. Averaging may help achieve better accuracy.
Once all the cross ranges are resolved, the relative locations of the ground transmitters can be determined in local array fixed coordinates. For example, local Cartesian coordinates are defined as the first ground transmitter at the origin, the second ground transmitter on the X-axis, the third ground transmitter on the X-Y plane with positive Y. If needed, the local coordinates can be mapped to other coordinates (e.g., GPS WGS84) when at least three of the ground transmitters are determined in the desirable coordinates.
If the ground transmitters need to be synchronized, the estimate of the relative clocks (Ti−Tj) can be used as feedback to steer the relative clock biases to zero.
The relative clock bias estimate can be broadcast to rovers for transmitter clock bias corrections, as described herein with reference to
Each ground transmitter includes a transceiver antenna, such as transceiver antennas 302a, 304a, 306a, and 308a. The transceiver antennas are capable of both receiving and transmitting ranging signals. Further, each ground transmitter comprises: 1) an optional wireless data modem, such as modems 302b, 304b, 306b, and 308b, 2) a transmitter section, such as transmitter sections 302c, 304c, 306c, and 308c, 3) a receiver section, such as receiver sections 302d, 304d, 306d, and 308d, and 4) a clock, such as 302e, 304e, 306e, and 308e. Each ground transmitter broadcasts clock bias estimates 316 to rover 312 as correction data. Further, each ground transmitter in array 300 can transmit and receive wideband ranging signals 310. According to certain embodiments, the receiver section and the transmitter section of each ground transmitter of array 300, are clocked by a single common oscillator clock, such as clocks 302e, 304e, 306e, and 308e.
In the foregoing specification, embodiments of the invention have been described with reference to numerous specific details that may vary from implementation to implementation. The specification and drawings are, accordingly, to be regarded in an illustrative rather than a restrictive sense. The invention is intended to be as broad as the appended claims, including all equivalents thereto.
Number | Name | Date | Kind |
---|---|---|---|
5381798 | Burrows | Jan 1995 | A |
6449558 | Small | Sep 2002 | B1 |
20030164794 | Haynes et al. | Sep 2003 | A1 |
20050159891 | Cohen et al. | Jul 2005 | A1 |
20060022843 | Zimmerman | Feb 2006 | A1 |
20060022869 | Zimmerman et al. | Feb 2006 | A1 |
20060022870 | Zimmerman et al. | Feb 2006 | A1 |
20060022871 | Zimmerman | Feb 2006 | A1 |
20060022872 | Zimmerman | Feb 2006 | A1 |
Number | Date | Country |
---|---|---|
WO 9963358 | May 1999 | WO |
WO 2005012935 | Feb 2005 | WO |
Number | Date | Country | |
---|---|---|---|
20080036660 A1 | Feb 2008 | US |