METHODS AND SYSTEMS FOR USE IN REMOTE SENSING
20190310365 ยท 2019-10-10
Inventors
Cpc classification
G01S15/58
PHYSICS
G01S17/58
PHYSICS
Y02A90/10
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
G01S15/582
PHYSICS
Y02E10/72
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
International classification
G01S15/58
PHYSICS
G06F17/11
PHYSICS
G01S7/481
PHYSICS
Abstract
A measurement configuration of a remote sensing device for use in implementing a remote sensing measurement campaign is improved. One method includes adjusting a scan geometry configuration of the remote sensing device during the measurement campaign based on measurement data acquired in a previous scan geometry configuration. In another method, the remote sensing device is configured in a scan geometry configuration having a plurality of scan geometries, and following acquisition of a measurement data set by the remote sensing device at a first time interval, one of the scan geometries indicative of an improved or optimal scan geometry at the first time interval is selected. The remote sensing device forms part of a remote sensing system and includes an optical source emitting a probe as a light beam along different lines of sight. The remote sensing device includes or is operatively associated with a receiver for detecting the reflected probe.
Claims
1. A method for use in remote sensing, the method comprising: receiving measurement data acquired previously during a remote sensing measurement campaign; determining from the received measurement data an adjustment in a measurement configuration of the remote sensing device, wherein said adjustment to the measurement configuration of the remote sensing device comprises a change in a scan geometry configuration of the remote sensing device; and providing an output indicative of the change to the scan geometry configuration of the remote sensing device for use in adjusting the remote sensing device during said measurement campaign.
2. The method of claim 1, comprising adjusting the measurement configuration of the remote sensing device by changing, during said measurement campaign, the scan geometry configuration of the remote sensing device based on the output.
3. The method of claim 1, wherein at least one of: the measurement data acquired previously during the remote sensing measurement campaign comprises measurement data acquired by the remote sensing device in a previous scan geometry configuration of the remote sensing device during said measurement campaign; and the measurement data acquired previously during the remote sensing measurement campaign comprises measurement data acquired by another remote sensing device or other sensing or measurement device during said measurement campaign.
4-6. (canceled)
7. The method of claim 1, wherein determining the change in the scan geometry configuration comprises determining a measurement of interest from the received measurement data acquired previously during the measurement campaign and determining from the measurement of interest a scan geometry configuration of the remote sensing device which is indicative of an improved or optimal scan geometry configuration of the remote sensing for said measurement of interest.
8. The method of claim 7, comprising adjusting the measurement configuration of the remote sensing device by changing, during said measurement campaign, the scan geometry configuration of the remote sensing device based on the output, wherein adjusting the measurement configuration of the remote sensing device comprises changing the scan geometry configuration of the remote sensing device according to the improved or optimal scan geometry configuration of the remote sensing for said measurement of interest during the measurement campaign.
9. The method of claim 7, comprising outputting the measurement of interest.
10. (canceled)
11. The method of claim 1, comprising a direction tracking operation.
12-17. (canceled)
18. The method of claim 1, comprising a volume tracking operation.
19-21. (canceled)
22. The method of claim 1, comprising a convergent scan geometry operation.
23-26. (canceled)
27. The method of claim 1, wherein the scan geometry configuration comprises scan geometry information comprising at least one of: timing information; information relating to the time at which the probe is emitted; information relating to the time the probe interacts with the fluid under investigation; and information relating to the time the probe is detected.
28-29. (canceled)
30. The method of claim 1, wherein the scan geometry configuration of the remote sensing device comprises a simple scan geometry element or arrangement.
31. (canceled)
32. The method of claim 1, wherein the scan geometry configuration of the remote sensing device comprises a complex scan geometry element or arrangement.
33. The method of claim 1, wherein the scan geometry configuration of the remote sensing device comprises a compound scan geometry element or arrangement.
34. (canceled)
35. The method of claim 1, wherein the measurement data comprises at least one of: fluid velocity data; fluid speed data; fluid direction data; fluid turbulence data; fluid compositional data.
36. A method for use in remote sensing, the method comprising: adjusting a measurement configuration of a remote sensing device for use in implementing a remote sensing measurement campaign during said remote sensing measurement campaign, wherein said adjustment to the measurement configuration of said remote sensing device comprises changing a scan geometry configuration of the remote sensing device based on measurement data acquired previously during the measurement campaign.
37. A system for use in remote sensing, the system comprising: a controller configured to receive measurement data acquired previously during a remote sensing device measurement campaign, the controller configured to determine from the received measurement data an adjustment in a measurement configuration of the remote sensing device, wherein said adjustment to the measurement configuration of the remote sensing device comprises a change in a scan geometry configuration of the remote sensing device, wherein the controller is configured to provide an output indicative of the change to the scan geometry configuration of the remote sensing device for use in adjusting the remote sensing device during said measurement campaign.
38. The system of claim 37, comprising a remote sensing device.
39-43. (canceled)
44. The system of claim 38, wherein the remote sensing device comprises a Lidar sensing device, a sodar sensing arrangement or an Acoustc doppler current profiler (ADCP).
45-46. (canceled)
47. The system of claim 37, comprising one or more energy capture devices.
48-49. (canceled)
50. The system of claim 37, comprising a control system, wherein the control system may be configured to adjust a position of the energy capture device.
51. (canceled)
52. A method for use in remote sensing, the method comprising: receiving measurement data acquired by a remote sensing device in a first scan geometry configuration at a first time interval, the first scan geometry configuration comprising a plurality of scan geometries; determining, from the received measurement data, one of the plurality of scan geometries which is indicative of an improved or optimal scan geometry at the first time interval; and providing an output indicative of a measurement of interest the improved or optimal scan geometry at the first time interval.
53. The method of claim 52, comprising multiple passes through the acquired data, a first pass for determining the prevailing conditions relevant for the selection of the optimal scan geometry for a given iteration of the compound scan geometry and a second pass for deriving a measurement of interest from the acquired data.
54. The method of claim 52, wherein the plurality of scan geometries of the first scan geometry configuration comprise a plurality of distinct and valid individual scan geometries which together form a compound scan geometry.
55-56. (canceled)
57. The method of claim 52, wherein the first scan geometry configuration comprises a Velocity Azimuth Display scan (VAD scan) operation.
58. (canceled)
59. The method of claim 52, wherein the scan geometry configuration of the remote sensing device comprises scan geometry information comprising at least one of: positional information; information relating to the location of a probe volume within a measurement volume; information relating to the distribution of probe volumes within a measurement volume; information relating to the orientation of a probe volume relative to the direction or line of sight along which a probe signal is emitted; information relating to the orientation of a probe volume relative to the direction along which the probe signal is detected. information relating to the azimuth angle of a probe volume relative to the direction along which the probe signal is detected; and information relating to the elevation angle of a probe volume.
60. The method of claim 52, wherein the scan geometry configuration comprises scan geometry information comprising at least one of: timing information; information relating to the time at which the probe is emitted; information relating to the time the probe interacts with the fluid under investigation; and information relating to the time the probe is detected.
61-62. (canceled)
63. The method of claim 52, wherein the scan geometry configuration of the remote sensing device comprises a simple scan geometry element or arrangement.
64. (canceled)
65. The method of claim 52, wherein the scan geometry configuration of the remote sensing device comprises a complex scan geometry element or arrangement.
66. The method of claim 52, wherein the scan geometry configuration of the remote sensing device comprises a compound scan geometry element or arrangement.
67. (canceled)
68. The method of claim 52, wherein the measurement data comprises at least one of: fluid velocity data; fluid speed data; fluid direction data; fluid turbulence data; and fluid compositional data.
69. A system for use in remote sensing comprising: a controller configured to determine, from a measurement data set acquired by the remote sensing device in a first scan geometry configuration at a first time interval, one of a plurality of scan geometries which is indicative of an improved or optimal scan geometry at the first time interval.
70. The system of claim 69, comprising a remote sensing device operable to implement a remote sensing measurement campaign.
71. A processing system configured to implement the method or system of one of claims 1, 36, 52, or 69.
72-77. (canceled)
78. A computer program product configured such that when processed by a suitable processing system configures the processing system to implement the method or system of one of claims 1, 36, 52, or 69.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0274] These and other aspects of the present invention will now be described, by way of example only, with reference to the accompanying drawings, in which:
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DETAILED DESCRIPTION OF THE DRAWINGS
[0299] Referring first to
[0300] As shown in
[0301] Beneficially, embodiments of the invention permit an optimal or at least improved remote sensing measurement campaign to be implemented under changing conditions by actively adjusting the measurement configuration of the remote sensing device during the measurement campaign. This is effected by adapting the scan geometry configuration of the remote sensing device during the measurement campaign based on measurement data acquired earlier during the same measurement campaign; in contrast to conventional RSDs which offer only a single scan geometry configuration during a measurement campaigntypically the default setting of the particular remote sensing device or one which is based on the initial objectives of the measurement campaign and projections of prevailing conditions made prior to commencing the measurement campaign. Embodiments of the present invention may adapt the configuration of the remote sensing device, and in particular the configuration of its scan geometry, during the measurement campaign to match the circumstances and conditions in which the measurements are acquired, which may vary significantly and repeatedly over time. Embodiments of the present invention thereby mitigate or eliminate inaccuracies which may otherwise arise in conventional systems and techniques due to measurement biases resulting from the, often significant, periods of time when measurements obtained are not fit for purpose or are relevant only for part of a given measurement campaign.
[0302] Referring now to
[0303] As shown in
[0304] The system 10 further comprises a remote sensing device 24 which, in the illustrated embodiment, is disposed on a platform 26 provided around the tower 14 of the wind turbine 12. It will be recognized, however, that the remote sensing device 24 may be provided at other suitable locations, such as a remote location, on the nacelle 16, on the ground or on one or more other turbine (not shown).
[0305] The remote sensing device 24 comprises a Lidar device having an optical source 28in the illustrated embodiment a laser source for transmitting a probe 30 in the form of a light beam to a region of interest 32 within the overall measurement volume V. The remote sensing device 24 further comprises or is operatively associated with a receiver 34in the illustrated embodiment an optical antenna for detecting the reflected probe 30. Referring now also to
[0306] Following acquisition of the first data set, an improved or optimal second scan geometry configuration is determined from the acquired first data set. The determination of the optimal scan geometry configuration may depend on the specific objectives of the measurement campaign. For example, upwind data may be required, and the scan geometry adjusted to always point upwind as the wind direction changes from one period of data acquisition to the next. The direction to the target volume may change as the platform rotates, for example, a wind turbine nacelle, in which case the scan geometry is adjusted to direct the lines of sight as required. In the illustrated embodiment, the second scan geometry configuration is formed by a second subset 40 of the possible lines of sight 36. The remote sensing device 24 is then reconfigured from the first scan geometry configuration as shown in
[0307] The remote sensing device 24 is then operated in the second scan geometry configuration to acquire a second data set relating to the region of interest 30. In this embodiment, the determination of the optimum or improved scan geometry configuration of the remote sensing device 24 is carried out during the measurement campaign and more particularly between each data acquisition. However, it will be recognized that the determination of the optimum or improved scan geometry configuration may alternatively be carried out during the measurement campaign but only after a selected number of data acquisitions or where the level of adjustment determined exceeds a selected threshold.
[0308] Referring now to
[0309] As shown in
[0310] The system 110 further comprises a remote sensing device 124 which, in the illustrated embodiment, is disposed on a platform 126 provided around the tower 114 of the wind turbine 112. It will be recognized, however, that the remote sensing device 124 may be provided at other suitable locations, such as a remote location, on the nacelle 116, on the ground or on one or more other turbine (not shown).
[0311] In this embodiment, the remote sensing device 124 comprises a Sodar device having an acoustic source 128 for transmitting a probe 130 in the form of a beam to a region of interest 132 within the overall measurement volume V. The remote sensing device 124 further comprises or is operatively associated with a receiver 134in the illustrated embodiment an acoustic antenna for detecting the reflected probe 130.
[0312] Operation of the system 110 is similar to that of the system 10 and will be described with reference to
[0313] As shown in
[0314] Referring now to
[0315] As shown in
[0316] The system 210 further comprises a remote sensing device 224 which, in the illustrated embodiment, is disposed on a platform 226 provided around the tower 214 of the turbine 212. It will be recognized, however, that the remote sensing device 224 may be provided at other suitable locations, such as a remote location, on the nacelle 216, on the seabed, a platform or on one or more other turbine (not shown).
[0317] In this embodiment, the remote sensing device 224 comprises an ADCP device having an acoustic source 228 for transmitting an acoustic probe 230 to a region of interest 232 within the overall measurement volume V. The remote sensing device 224 further comprises or is operatively associated with a receiver 234 - in the illustrated embodiment an acoustic antenna for detecting the reflected probe 230.
[0318] Operation of the system 210 is similar to that of the systems 10, 110 and will be described with reference to
[0319] As shown in
[0320] Referring now to
[0321] As shown in
[0322] Beneficially, this embodiment permits an optimal or at least improved remote sensing measurement campaign to be implemented under changing conditions by passively adjusting the scan geometry configuration of the remote sensing device during the measurement campaign by selecting the optimal scan geometry from the plurality of scan geometries available of which the first scan geometry is comprised, during processing of data acquired over multiple time steps; in contrast to conventional RSDs which offer only a single scan geometry configurationtypically the default setting of the particular remote sensing deviceor one geometry configuration which is configured prior to commencing a measurement campaign and which is based on the initial objectives of the measurement campaign, such that an optimal scan geometry cannot be selected with reference to variation of wind conditions during the measurement campaign.
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[0324] The system 310 comprises a wind turbine system including a wind turbine 312 having a tower 314, a nacelle 316 and a hub 318 having a plurality of radially extending blades 320. The hub 318 is operatively coupled to an electrical generator 322 via a drive shaft (not shown). In use, the kinetic energy of wind W impinging on the blades 320 drives rotation of the hub 318 relative to the nacelle 316, this kinetic energy being transmitted to the electrical generator 322 where it is converted into electricity.
[0325] The system 310 comprises a remote sensing device 324 which, in the illustrated embodiment, is disposed on a platform 326 provided around the tower 314 of the wind turbine 312. It will be recognized, however, that the remote sensing device 324 may be provided at other suitable locations, such as a remote location, on the nacelle 16, on the ground or on one or more other turbine (not shown).
[0326] The remote sensing device 324 comprises a Lidar device having an optical source 326in the illustrated embodiment a laser source for transmitting a probe 330 in the form of a light beam over a region of interest 332 within the overall measurement volume V'. The remote sensing device 324 further comprises or is operatively associated with a receiver 334in the illustrated embodiment an optical antenna for detecting the reflected probe 330.
[0327] Referring now also to
[0328] In this embodiment, the scan geometry configuration comprises a compound scan geometry encompassing a plurality of scan geometries and, in the illustrated embodiment, each of the 1st to nth data sets includes data for the entire region of interest 332.
[0329] Following data acquisition, each data set is analysed. A first pass of each data set determines which one of the scan geometries from the plurality of scan geometries is indicative of an improved or optimal scan geometry at each of the given time intervals t1 . . . tn. In
[0330] In this embodiment, the determination of the optimum or improved scan geometry configuration of the remote sensing device 324 is carried out after data acquisition, rather than between each data acquisition as in the first embodiment.
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[0332] The system 410 comprises a wind turbine system including a wind turbine 412 having a tower 414, a nacelle 416 and a hub 418 having a plurality of radially extending blades 420. The hub 418 is operatively coupled to an electrical generator 422 via a drive shaft (not shown). In use, the kinetic energy of wind W impinging on the blades 420 drives rotation of the hub 418 relative to the nacelle 416, this kinetic energy being transmitted to the electrical generator 422 where it is converted into electricity. The system 410 comprises a remote sensing device 424 which, in the illustrated embodiment, is disposed on a platform 426 provided around the tower 414 of the wind turbine 412. It will be recognized, however, that the remote sensing device 424 may be provided at other suitable locations, such as a remote location, on the nacelle 416, on the ground or on one or more other turbine (not shown).
[0333] In this embodiment, the remote sensing device 424 comprises a Sodar device having an acoustic source 426 for transmitting a probe 430 in the form of a beam over a region of interest 432 within the overall measurement volume V. The remote sensing device 424 further comprises or is operatively associated with a receiver 334in the illustrated embodiment an acoustic antenna for detecting the reflected probe 430.
[0334] Referring now also to
[0335] As in the previous embodiment, the scan geometry configuration comprises a compound scan geometry encompassing a plurality of scan geometries and, in the illustrated embodiment, each of the 1st to nth data sets includes data for the entire region of interest 432.
[0336] Following data acquisition, each data set is analysed. A first pass of each data set determines which one of the scan geometries from the plurality of scan geometries is indicative of an improved or optimal scan geometry at each of the given time intervals t1 . . . tn. In
[0337] Referring now to
[0338] As shown in
[0339] The system 510 further comprises a remote sensing device 524 which, in the illustrated embodiment, is disposed on a platform 526 provided around the tower 514 of the turbine 512. It will be recognized, however, that the remote sensing device 524 may be provided at other suitable locations, such as a remote location, on the nacelle 516, on the seabed, a platform or on one or more other turbine (not shown).
[0340] In this embodiment, the remote sensing device 524 comprises an ADCP device having an acoustic source 528 for transmitting a sonic probe 530 to a region of interest 532 within the overall measurement volume V. The remote sensing device 524 further comprises or is operatively associated with a receiver 534in the illustrated embodiment an acoustic antenna for detecting the reflected probe 530.
[0341] Referring now also to
[0342] As in the previous embodiment, the scan geometry configuration comprises a compound scan geometry encompassing a plurality of scan geometries and, in the illustrated embodiment, each of the 1st to nth data sets includes data for the entire region of interest 532.
[0343] Following data acquisition, each data set is analysed. A first pass of each data set determines which one of the scan geometries from the plurality of scan geometries is indicative of an improved or optimal scan geometry at each of the given time intervals t1 . . . tn. In
[0344] More details relating to the operation and analysis techniques employed in each of the above embodiments will now be described with reference to
[0345] As described above, the scan geometry configuration of the remote sensing devices is used to acquire the measurement data from which characteristics of the fluid under investigation can be determined and the scan geometry configuration may include, amongst other things, the locations and distribution of probe volumes within the measurement volume (defined in Cartesian co-ordinates x, y, z); the orientation of the probe volumes in terms of the directions along which the probe is emitted and detected (defined in terms of azimuth and elevation angles (, )); and the times at which the probes are emitted, interact with the fluid under investigation, and are subsequently detected (t).
[0346] With regard to the location of the probe volumes, in the illustrated embodiments the range is determined by measuring the back-scatter of light radiation which is reflected by natural aerosols carried by the wind, such as dust, water droplets, pollution, pollen, salt crystals or the like. The emissions are back-scattered and detected and the Doppler shift imposed on the frequency of the laser emissions by the motion of the aerosol particles is analysed to infer characteristics of the fluid motion. In addition, the strength of the detected signal can indicate the concentration of the aerosol particles at the point where the interaction occurred. Polarization effects are also sometimes observed. The detection of various effects of the interaction with the fluid allows investigation of various properties in addition to its motion, such as the fluid's composition. The Doppler shift is proportional to the component of the fluid velocity vector aligned with the line of sight (LoS) along which the laser emissions are directed, that is, the radial velocity. It will therefore depend on the angle between the LoS and the direction of the fluid velocity. The fluid velocity vector components can thus be inferred from observations of radial velocities along various lines of sight if the relationship between the wind velocity vectors witnessed in each probe volume can be deduced from the observations. For example, in the simplest case, the wind velocity vector can be inferred if each probe volume used in the calculation witnesses the same wind velocity vector. This is the case under conditions of uniform flow.
[0347] With regard to the orientation of the probe volume, where this is determined by the line of sight along which the probe is emitted and the radial distance r of the probe alone this line of sight is known, then (r, , ) can be stated and (x, y, z) omitted since the location and orientation is fully described in polar co-ordinates.
[0348] With regard to the timing information, this may be necessary to take account of the dimensions and characteristics of the probe volume itself. For example, the response of the probe may not be symmetrical within the probe volume and may give rise to effects which must be accommodated using the time information, such as unsteady features in fluid flow in time and/or where coherent fluid structures in space advected through the measurement volume are occurring and are being observed Timing information is also important if the measurements in each probe volume happen in a sequence rather than simultaneously, for example, as a result of the acquisition of measurements along a single line of sight or direction which is then scanned between a series of different orientations, rather than along multiple lines of sight which are implemented simultaneously.
[0349] It should be understood that the embodiment described herein is merely exemplary and that various modifications may be made thereto without departing from the scope of the invention.
[0350] For example, while the scan geometries in the illustrated embodiments comprises divergent scan geometries whereby multiple lines of sight under consideration may radiate and diverge from the location of a single RSD in order to fulfil the requirement for multiple angles relative to the fluid velocity direction, the scan geometries may take a number of different forms, as illustrated in