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    SYSTEM AND METHOD FOR MONITORING WIND CHARACTERISTICS IN A VOLUME, LASER ANEMOMETER, SYSTEM AND METHOD TO CONTROL THE OPERATION OF MULTIPLE WIND TURBINESThe present invention relates to systems and methodologies for monitoring wind characteristics, particularly useful in association with wind turbine installations. The system comprises a plurality of non-coherent laser anemometers (100, 200, 300, 350) operational to measure wind characteristics in a plurality of corresponding subvolumes 10 located within said volume and a data processing subsystem (102, 212, 312, 362) operational to receive data from said plurality of anemometers (100, 200, 300, 350) a Iaser not coherent and to provide output data that represent said wind characteristics in said volume.
    公开号:BR112012006806A2
    申请号:R112012006806-7
    申请日:2010-09-28
    公开日:2020-08-18
    发明作者:Sagie Tsadka；Nathan Sela
    申请人:Pentalum Technologies Ltd.；
    IPC主号:
    专利说明:

    "SYSTEM AND METHOD FOR MONITORING WIND CHARACTERISTICS IN A VOLUME, LASER ANEMOMETER, SYSTEM AND METHOD TO CONTROL THE OPERATION OF MULTIPLE WIND TURBINES" Field of Invention 5 The present invention relates to systems and methodologies to particularly monitor wind characteristics , useful in association with wind turbine installations.
    Background of the Invention The following publications are believed to represent the state of the art and are hereby incorporated by reference: US6,320,272 patents: US5,796,471; US7,311,000; US6,946,751; US7,342,323; US7,221,438; US7,281,891; US6,646,725; US7,391,506; US6,687,036: and US4,651,017; Published patent applications US2007 / 0158493; US2008 / 0210881; US2009 / 0099702; and US2009 / 0046289; Japanese patents JP 11271350 and jP11133049; Mayor et al., Two-Dimensional Vector Wind Fields from Volume lmaging Lidar Data, Journal of App / ied Meteorology 40: 1,331 to 1-346 (2001); Piironen et al, Accuracy Analysis of Wind Profiles Calculated from Volume lmaging Lidar Data, Joumal of Geophysical Reseamh 100: 25,559 to 25,567; and Vaughn et al, Laser Doppler Velocimetry Applied to the Measurement of Local and Global Wind, Wind Engineer / ng 13: 1 to 15.
    William T- Buttler et al, Remote sensing of three dimensional winds with elastic Lidar: explanation of maximum cross-correlation method, Boundary-Layer Meteorology 101: 305 to 328, 2001 lchiro Matsui et al, Wind profiling by a conical-scanning time correlation Lidar, Japanese journal of applied physics, Vol 29, n ° 2, February 1990, pgs. 441 to 444.
    Nobuo Sugimoto et al, An improved method for wind measurement with a conical-scanning correlation Lidar, Japanese Journal of applied physics, Vol 37 (1998), pgs. 5,598 to 560.
    Ting-i Wang, G. R. Ochs and R. S. Lawrence, Wind 5 measurements by the temporal cross-correlation of the optical scintillations Applied Optics, Vol. 20, question 23, pgs. 4,073 to 4,081 (1981).
    Description of the Invention The present invention seeks to provide improved systems and methodologies for monitoring wind characteristics, particularly useful for wind turbine installations. Accordingly, a system for monitoring wind characteristics in a volume that includes a number of non-coherent laser anemometers operational to measure wind characteristics in a plurality of corresponding sub-volumes located within the volume is provided according to a preferred embodiment of the present invention. and an operational data processing subsystem for receiving data from the plurality of non-coherent laser anemometers and for providing output data that represent wind characteristics in the volume.
    Preferably, the plurality of non-coherent laser anemometers and the data processing subsystem are operational to provide three-dimensional wind velocity vectors over the entire volume at an update rate of at least one per second. In addition, the system also includes operational modeling functionality to calculate maximum output power and ideal locations for a plurality of wind turbines. Also provided in accordance with another preferred embodiment of the present invention is a laser anemometer which includes a tunable laser, a scanner, which receives a tunable laser output and which provides laser beam outputs in various scanning directions, and at least one detector to receive signals from retro-designed Iaser beam outputs.
    Preferably, the tunable laser is a tunable wavelength laser and the scanner is a responsive 5-wavelength scanner that receives output at multiple wavelengths and provides the laser beam outputs in various scan directions according to the multiple wavelengths. In addition, the laser anemometer also includes an operational anemometer transmission controller to provide timed control outputs for the tunable Iaser.
    According to a preferred embodiment of the present invention, the control outputs include a power level, timing and a wavelength of the tunable laser pulse outputs. In addition, the Iaser anemometer also includes an optical amplifier. Additionally or alternatively, the Iaser anemometer also includes a wavelength division multiplexer coupled to the tunable laser. Alternatively, the at least one detector includes an array of detectors. In addition, the laser anemometer also includes an optical filter. Preferably, the laser anemometer also includes a set of operative correlation circuits for correlating signals received through at least one detector. In addition, in accordance with yet another preferred embodiment of the present invention, a laser anemometer includes a laser, an optical switch responsive to a control signal to provide laser beams in various scanning directions which are non-coherent when colliding with particles in the atmosphere, and at least one detector to receive signals from the retro-designed laser beam outputs that are non-coherent.
    In addition, the laser anemometer also includes an optical amplifier.
    Alternatively, the at least one detector includes an array of detectors. Preferably, the Iaser anemometer also includes an optical filter. Preferably, the laser anemometer also includes a set of operative correlation circuits for correlating signals received through at least one detector.
    In addition, according to yet another preferred embodiment of the present invention, a laser anemometer includes a laser, an optical switch that has no moving parts and is responsive to a control signal to provide laser beam outputs in several scanning directions, and at least one detector to receive signals from the retro-designed laser beam outputs. Preferably, the laser anemometer also includes an optical amplifier. Alternatively, the at least one detector includes an array of detectors. Preferably, the laser anemometer also includes an optical filter. Preferably, the laser anemometer also includes a set of operative correlation circuits for correlating signals received through at least one detector. Also provided in accordance with another preferred embodiment of the present invention is a laser anemometer that includes a laser, a MEMS optical switch (MEMS - Micro electro mechanical Systems) that is responsive to a control signal to provide laser beam outputs at various scanning directions, and at least one detector for receiving retro-designed laser beam output signals. Preferably, the laser anemometer also includes an optical amplifier. Alternatively, at least one detector includes an array of detectors. Preferably, the laser anemometer also includes an optical filter. Preferably, the laser anemometer also includes a set of operative correlation circuits for correlating signals received through at least one detector. In addition, in accordance with yet another preferred embodiment of the present invention, a laser anemometer including laser,
    a laser beam splitter to provide laser beam outputs simultaneously in the plurality of scan directions, and a plurality of detectors to receive signals from the rear projection of the laser beam outputs.
    Preferably, the laser anemometer also includes an optical amplifier.
    5 The laser anemometer preferably also includes an optical filter. Preferably, the laser anemometer also includes a set of operative correlation circuits to correlate signals received by the detector.
    In addition, a system for controlling the operation of multiple wind turbines, which includes a plurality of operational anemometers for measuring wind characteristics in at least a plurality of locations, is also provided according to another preferred embodiment of the present invention. operational data to receive data from the plurality of anemometers and to provide output data representing the wind characteristics in the plurality of locations, and a control subsystem that receives the output data from the data processing subsystem and that provides control signals from wind turbine for a plurality of wind turbines located at least in general proximity to the plurality of locations.
    According to a preferred embodiment of the present invention, the plurality of anemometers includes a plurality of laser anemometers. Preferably, the plurality of laser anemometers includes at least one non-coherent laser anemometer.
    In addition, the data processing subsystem receives data from the plurality of anemometers through a wireless communication link. Preferably, the plurality of anemometers includes at least one anemometer oriented in a horizontal direction.
    In addition, the plurality of anemometers includes at least one anemometer oriented in a vertical direction.
    Preferably, the wind turbine control signals include at least one of a rotor alignment signal, a paddle step signal and a rotor lock signal. In addition, the data processing subsystem is operational to receive data at an update rate of at least one update per second, and the control subsystem is operational to provide wind turbine control signals at an update rate between one update per second and one update for several minutes. Preferably, the data processing subsystem is operational to perform aerodynamic calculations to provide data output. Also provided in accordance with another preferred embodiment of the present invention is a laser anemometer system for monitoring wind speed that includes at least one Iaser that directs at least one laser illumination beam out of at least one location, at least at least one laser illumination receiver that receives reflections from the laser illumination of particles in the atrnosphere located at various distances from at least one location, and set of operative correlation circuits to correlate outputs from at least one laser illumination that represent reflections of different of the various distances from at least one location, thereby providing an indication of wind speed output along at least one direction approaching the location.
    According to a preferred embodiment of the present invention, the correlation circuitry is operational to generate a correlation graph. Preferably, the correlation graph is a graph of the C (T) correlation function mathematically described as follows: C (r) _- F- E: = ¢ [lÁ (t, + r) - T,] [lB (t,) - TJ 1iE: = Q! A (t,) - Í, j] 2, g: = g [l6 (tt) - ís] 2 where: | a and | b are the intensities of reflected laser beams of locations A and B in space, respectively, as a function of time; tj marks one of the n time points at which the 5 reflex samples are recorded: / a and Íb are the average intensity of the reflexes at locations A and B respectively over n samples recorded at the n time points: er is a difference parameter of time for which the correlation function is being calculated and t can be positive or negative.
    Additionally, according to yet another preferred embodiment of the present invention, a method for monitoring wind characteristics in a volume that includes using a plurality of non-coherent laser anemometers to measure wind characteristics in a plurality of corresponding sub-volumes located within the volume , and use a data processing subsystem to receive data from the plurality of non-coherent laser anemometers to provide output data that represent the wind characteristics in the volume.
    Preferably, the plurality of non-coherent laser anemometers and the data processing subsystem are operational to provide three-dimensional wind velocity vectors over the entire volume at an update rate of at least one per second. In addition, the method also includes calculating the maximum output power and the ideal locations for a plurality of wind turbines.
    A method for controlling the operation of multiple wind turbines that includes using a plurality of anemometers to measure wind characteristics in at least a plurality of locations, using a wind processing subsystem, is further provided according to yet another preferred embodiment of the present invention. data to receive data from the plurality of anemometers and to provide output data representing the wind characteristics in the plurality of locations, and to use a control subsystem to receive the output data from the data processing subsystem and to provide control signals from wind turbine 5 for a plurality of wind turbines located at least in general proximity to the plurality of locations.
    According to a preferred embodiment of the present invention, the plurality of anemometers includes a plurality of laser anemometers.
    Preferably, the plurality of laser anemometers includes at least one non-coherent laser anemometer. In addition, the data processing subsystem receives data from the plurality of anemometers through a wireless communication link. Preferably, the plurality of anemometers includes at least one anemometer oriented in a horizontal direction. In addition, the plurality of anemometers includes at least one anemometer oriented in a vertical direction. Preferably, the wind turbine control signals include at least one of a rotor alignment signal, a paddle step signal and a rotor lock signal. In addition, the data processing subsystem is operational to receive data at an update rate of at least one per second, and the control subsystem is operational to provide wind turbine control signals at an update rate between one per second and one for several minutes. Preferably, the data processing subsystem is operational to perform aerodynamic calculations to provide data output.
    Also provided in accordance with another preferred embodiment of the present invention is a laser anemometer method for monitoring wind speed which includes using at least one laser to direct at least one laser illumination beam out of at least one location, using at least at least one laser illumination receiver to receive reflections from the laser illumination of particles in the atmosphere located at different distances from at least one location, and use a set of correlation circuits to correlate outputs from at least one laser illumination representing 5 reflections of different from the various distances from at least one location, thereby providing an indication of wind speed output along at least one direction approaching the location.
    According to a preferred embodiment of the present invention, the correlation circuitry is operational to generate a correlation graph. Preferably, the correlation graph is a graph of the C (r) mathematical correlation function described as follows: E: = c [lÀ (t, -t I) - TJ [lB (t,) - LI C (" ) =, } E = Õ jjt,) - L] 'E:' = o [l8 (t,) - íj 'where: | a and | b are the intensities of Iaser beams reflected from locations A and B in the space, respectively, as a function of time; tj marks one of the n points in time at which the reflexes samples are recorded; / a and / b are the average intensities of the reflexes from locations A and B respectively over n samples recorded at n points in time; et is a time difference parameter for which the correlation function is being calculated and t can be positive or negative.
    BRIEF DESCRIPTION OF THE DRAWINGS The present invention will be understood and observed more fully from the following detailed description, taken in conjunction with the drawings, in which:
    Figure 1 is a simplified, partly schematic and partly illustrative illustration of a systenia to control the operation of multiple wind turbines based on monitored wind characteristics, built and operational according to an embodiment
    5 preferred of the present invention: Figure 2 is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics for short range wind vector forecast,
    constructed and operational in accordance with a preferred embodiment of the present invention; Figure 3 is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics for use in assessing wind resources available at a variety of locations at a prospective wind farm,
    constructed and operational in accordance with a preferred embodiment of the present invention;
    Figure 4 is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics for use in wind turbine planning placement, built and operational in accordance with a preferred embodiment of the present invention:
    Figures 5A and 5B are simplified, partly schematic and partly illustrative of the structure and operation of a non-coherent Iaser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide wind speed output indications. ;
    Figures 6A and 6B are simplified, partly schematic and partly illustrative of the structure and operation of an alternative embodiment of a non-coherent laser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide speed output indications. wind;
    Figures 7A and 7B are simplified illustrations, partially
    5 schematic and partially illustrative of the structure and operation of another alternative embodiment of a non-coherent Iaser anemometer for monitoring wind characteristics that includes set of operative correlation circuits to provide wind speed output indications;
    Figures 8A and 8B are simplified, partly schematic and partly illustrative of the structure and operation of yet another alternative embodiment of a non-coherent laser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide output indications. wind speed;
    Figure 9 is a simplified, partly schematic and partly illustrative illustration of the structure and operation of yet another alternative embodiment of a non-coherent laser anemometer for monitoring wind characteristics that includes set of operative correlation circuits to provide output indications. wind speed;
    Figure 10 is a simplified flowchart that illustrates the operation of the set of correlation circuits of the system of Figures 5A to 9 for laser beams in general and vertically directed pulses; Figure 11 is a simplified pulse laser beam correlation diagram useful in understanding the operation of the functionality of Figure 10; Figure 12 is a simplified flowchart that illustrates the operation of the system correlation circuitry of figures 5A to 9 for laser beams in direct pulse generated! and horizontally; and
    Figure 13 is a simplified pulse laser beam correlation diagram useful in understanding the operation of the functionality of Figure 12; e Figure 14 is a typical correlation graph produced by the 5 set of correlation circuits of the non-coherent laser anemometer in Figures 5A to 9. Description of the Invention's Achievements Reference is now made to Figure 1, which is a simplified illustration, partially schematic and partially illustrative of a system for controlling the operation of multiple wind turbines based on monitored wind characteristics, built and operational in accordance with a preferred embodiment of the present invention.
    The preferred system includes a plurality of anemometers 100 operational to measure wind characteristics in various locations, preferably at least one wind data processing subsystem (WDP - Wind Data Processing) 102, operational to receive data from the plurality of anemometers 100 and to provide output data representing the wind characteristics at the various locations and preferably at least one control subsystem 104, which receives the output data from the wind data processing subsystem 102 and which provides turbine control signals wind for a plurality of wind turbines 106 located at least in general proximity to the plurality of anemometers.
    As seen in figure 1, anemometers 100 are preferably laser anemometers, each of which provides an output that indicates wind speed at various locations along a geometry axis 110. The outputs of the plurality of laser anemometers 100 are supplied for at least one wind data processing subsystem 102 via wireless or wired communication links,
    respectively designated by reference numbers 112 and 114. At least one control subsystem 104, in turn, can provide control inputs for the plurality of wind turbines 106, via wireless or wired communication links, respectively designated by reference numbers 5 116 and 118. It is noted that laser anemometers 100 can be located in various positions, such as on the ground or in nacelles of wind turbines 106.
    The control inputs supplied to wind turbines 106 through at least one control subsystem 104 include data representing the anticipated wind characteristics in the intermediate proximity of each of the wind turbines 106, the data of which is used to align the rotor of each of the wind turbines. wind turbines 106 in a plane generally perpendicular to the direction of the incoming wind, thus maximizing the amount of wind power that is effective in rotating the rotor of each of the wind turbines 106, in turn, thus maximizing the amount of electricity that can be generated by the wind turbine 106. The alignment of a rotor is preferably carried out by a yaw motor provided with each of the wind turbines 106.
    Additionally, the data is used to control the pitch of each of the rotor blades of each of the wind turbines 106, thus maximizing the amount of electricity that can be generated by each of the wind turbines 106 while balancing the load on each of the wind turbines. rotor blades. The data can also be used by each of the wind turbines 106 to lock the rotor, thereby preventing it from rotating, when the wind is too weak to generate significant rotor rotation or when the wind is too strong to safely operate the turbine without to be damaged, It is a particular feature of an embodiment of the present invention that the plurality of laser anemometers 100 includes anemometers a (aser non-coherent. Non-coherent laser anemometers provide multiple mutually non-coherent laser beams in an anemometer measurement volume 120. The anemometer measurement volume is typically a cone, centered around a geometry axis 110, which typically extends up to 300 meters and extends below an opening angle of approximately 14 degrees. laser beams typically extend along the periphery of the cone. It is a particular feature of the present invention that the wind data processing subsystem 102 be operational to receive data from the plurality of laser anernometers 100 and to provide output data that represent the wind characteristics at various points to the control unit 104, as illustrated in figure 1.
    More particularly, it is a particular feature of the present invention that the at least one wind data processing subsystem 102 can provide three-dimensional wind speed measurements to the control unit 104, preferably at an update rate of at least one per second, and for this feature to provide control for the turbines at an update rate between one per second and one for several minutes.
    Reference is now made to figure 2, which is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics by forecasting the wind vector in space, time and / or short range, constructed and operational according to a preferred embodiment of the present invention. For example, such a short-range wind vector forecast is particularly useful for predicting the power that will be generated by a wind farm within the next several tens of seconds, minutes or hours, and thus facilitates optimal integration of the power output. wind farm within a larger-scale electricity grid. In addition, this forecast allows the optimization of the operation of wind turbines at the wind farm in response to anticipated wind characteristics. The system in figure 2 preferably includes a pIurality of 5 anemometers 200 operational to measure wind characteristics in different locations distributed by an entire forecast volume 202, which can be considered to be overlaid by a three-dimensional network 204.
    Typically, the size of the forecast volume 202 is at least on the order of cubic kilometers and the length of individual network units is at least on the order of tens of meters, however, additional anemometers may be located up to several kilometers away from the wind farm. and provide data on wind characteristics that are anticipated to arrive at the station at later times.
    Preferably, at least one wind data processing subsystem 212 is operational to receive data from the plurality of anemometers 200 and by performing aerodynamic calculations on the data to provide output data representing predicted wind characteristics at the various locations, and optionally at least one control subsystem 214, which receives output data from at least one wind data processing subsystem 212 and based on the predicted wind characteristics that provide wind turbine control signals for a plurality of localized wind turbines 216 at least in general proximity to the plurality of anemometers 200. The output data provided by the data processing subsystem 212 is also useful in providing forecast of the amount of electrical power anticipated to be generated by the wind farm, which is useful in facilitating transactions and sale of the power generated in the local electricity market.
    As seen in figure 2, anemometers 200 are preferably laser anemometers, each of which provides an output that indicates wind speed in various locations along a 220 measurement axis. The outputs of the pIurality of laser anemometers 200 are supplied to at least one wind data processing subsystem 212 through wireless or wired communication links, respectively designated by reference numbers 222 and 224. The at least one control subsystem 214, in turn , can provide control inputs for the plurality of wind turbines 216, via wireless or wired communication links, respectively designated by reference numbers 226 and 228. It is noted that laser anemometers 200 can be located in various positions , such as on the ground or in nacelles of wind turbines 216.
    The control inputs supplied to wind turbines 216 by at least one control subsystem 214 include data representing the wind characteristics predicted in the intermediate proximity of each of the wind turbines 216 whose data are used to align the rotor of each of the wind turbines 216 in a plane generally perpendicular to the direction of the incoming wind, thus maximizing the amount of wind power that is effective in rotating the rotor of each of the wind turbines 216, in turn, thus maximizing the amount of electricity that can be generated by wind turbine 216. The alignment of a rotor is preferably carried out by a yaw motor provided with each of the 216 wind turbines.
    Additionally, the data is used to control the pitch of each of the rotor blades on each of the 216 wind turbines, thus maximizing the amount of electricity that can be generated by each of the 216 wind turbines while balancing the load on each of the wind turbines. rotor blades. The data can also be used by each of the 216 wind turbines to lock the rotor, thus preventing rotation, when the wind is too weak to generate significant rotation of the rotor or when the wind is too strong to safely operate the turbine without damage it. It is a particular feature of an embodiment of the present invention that the plurality of laser anemometers 200 includes non-coherent laser anemometers. Non-coherent laser anemometers provide multiple mutually non-coherent laser beams in an anemometer measurement volume 230. The anemometer measurement volume is typically a cone, centered around a 220 measurement geometric axis, which typically extends across up to 300 meters and extends below an opening angle of approximately 14 degrees. The multiple laser beams typically extend along the periphery of the cone. It is a particular feature of the present invention that the wind data processing subsystem 212 is operational to receive data from the plurality of anemometers to Iaser 200 and to provide output data representing the wind characteristics at various points in the network 204 of the volume of forecast 202, which may cover one or more wind farms, as shown in figure 2.
    More particularly, it is a particular feature of the present invention that the at least one wind data processing subsystem 212 can provide three-dimensional wind speed vectors over the entire forecast volume 202, preferably at a refresh rate of at least one per second. Such predicted velocity vectors are preferably provided for each point on the three-dimensional network 204 and may represent real-time velocity vectors and / or measured predicted velocity vectors. This feature allows flexible placement of Iaser 200 anemometers that can be located on the ground and not necessarily in the nacelles of wind turbines 216, thus allowing easier positioning and integration of 200 laser anemometers in an existing wind station. Reference is now made to Figure 3, which is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics for use in assessing wind resources available at a variety of locations at a prospective, constructed and constructed wind farm. operational according to a preferred embodiment of the present invention.
    The system of figure 3 preferably includes a plurality of operational anemometers 300 for measuring wind characteristics in various locations spread across a potential wind farm.
    At least one wind data processing subsystem 312 is operational to receive data from the plurality of anemometers 300 and to provide output data representing the wind characteristics at the various locations whose output data is useful in assessing available wind resources within of the potential wind farm.
    As seen in figure 3, anemometers 300 are preferably laser anemometers, each of which provides an output that indicates wind speed at various locations along a 320 measurement axis. The outputs of the plurality of laser anemometers 300 are supplied to at least one wind data processing subsystem 312 via wireless or wired communication links, respectively designated by reference numbers 322 and 324. Note that laser anemometers 300 can be located in various positions within the potential wind farm. It is a particular feature of an embodiment of the present invention that the plurality of laser anemometers 300 includes non-coherent laser anemometers. Non-coherent laser anemometers provide multiple, mutually non-coherent laser beams in an anemometer measurement volume 330. The anemometer measurement volume is typically a cone, centered around the 320 measurement geometric axis, which typically extends up to 300 meters and extends below an angle 5 of approximately 14 degrees. The multiple laser beams typically extend along the periphery of the cone. It is another particular feature of the present invention that the wind data processing subsystem 312 is operational to receive data from the plurality of laser anemometers 300 and to provide data related to the wind resources available to a user. The wind data processing subsystem can be located within the potential wind farm or at a location that is remote from the potential wind farm. It is yet another particular feature of the present invention that the wind data processing subsystem 312 can use data received from the plurality of laser anemometers 300 to calculate several important parameters such as wind crossing and wind deviation at the wind farm, as well as the intensity of wind turbulence at the wind farm and locations within the wind farm that have stronger gusts or a higher turbulence flow that can negatively affect the performance of wind turbines that will be placed at such locations. Reference is now made to Figure 4, which is a simplified, partly schematic and partly illustrative illustration of a system for monitoring wind characteristics for placing wind turbines, constructed and operational in accordance with a preferred embodiment of the present invention.
    The system of figure 4 preferably includes a plurality of anemometers 350 operational to measure wind characteristics in various locations spread over a volume of potential wind farm 352, which can be considered to be overlaid by a three-dimensional network 354. Typically, the volume size of potential wind farm 352 is at least in the order of cubic kilometers and the length 5 of individual grid units is at least in the order of tens of meters. At least one wind data processing subsystem 362 is operational to receive data from the plurality of anemometers 350 and to provide output data representing the wind characteristics in the various locations whose output data is useful in the design and placement of a plurality of 366 future wind turbines, shown in rows. As seen in figure 4, anemometers 350 are preferably laser anemometers, each of which provides an output that indicates wind speed at various locations along a 370 measurement axis. The outputs from the plurality of anemometers a Iaser 350 are supplied for at least one wind data processing subsystem 362 via wireless or wired communication links, respectively designated by reference numbers 372 and 374, Note that the laser anemometers 350 can be located at various positions within the volume of potential wind farm 352.
    It is a particular feature of an embodiment of the present invention that the pIurality of laser anemometers 350 includes non-coherent Iaser anemometers. Non-coherent laser anemometers provide multiple, mutually non-coherent laser beams in an 380 anemometer measurement volume. The anemometer measurement volume is typically a cone, centered around the 370 measurement geometry axis, which typically extends up to 300 meters and extends below an angle of approximately 14 degrees. The multiple laser beams typically extend along the periphery of the cone.
    It is a particular feature of the present invention that the wind data processing subsystem 362 is operational to receive data from the plurality of laser anemometers 350 and to provide output data that represent the wind characteristics at various points in the network 354 of the
    5 potential wind farm volume 352, as illustrated in figure 4. More particularly, it is a particular feature of the present invention that the at least one wind data processing subsystem 362 can provide three-dimensional wind speed vectors across the entire volume of wind forecast 352, preferably at a refresh rate of at least one per second.
    Such predicted velocity vectors are preferably provided for each point in the three-dimensional network 354 and can represent real-time velocity vectors and / or measured predicted velocity vectors.
    Such a three-dimensional wind speed map within the volume of prospective wind station 352 can support a mathematical model that calculates ideal potential locations of the plurality of future wind turbines 366 within the volume of potential wind station 352, based on the maximum output power that future wind turbines 366 can potentially produce when operational under the measured and predicted wind vectors accumulated at tenong long by the data processing subsystem 362. Reference is now made to figures 5A and 5B, which are simplified, partly schematic and partly illustrations illustrating the structure and operation of an implementation of a non-coherent laser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide wind speed output indications, and figures 6A and 6B, which are simplified illustrations, partly schematic and partly illustrative of the structure ture and operation of an alternative realization of a non-coherent Iaser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide wind speed output indications.
    As seen in figures 5A to 6B, an anemometer transmission controller 400, which includes a master oscillator and set of 5 time setting circuits, provides time-controlled control outputs for a tunable laser 402, such as a tunable laser 3205-D or 3206-D, commercially available from JDS Uniphase Corporation of Milpitas, California, USA. The control outputs preferably control the power level, timing and wavelength of the 402 tunable laser pulse outputs. The 402 tunable laser pulse outputs are typically carried by an optical fiber to an optical amplifier 404, such as as a High Power Variable Gainkixed Gain EDFA, commercially available from Israel's Red-C Optical Networks Ltd. It is noted that any other suitable optical amplifier can be employed. It is also noted that the optical amplifier 404 can be excluded where the laser 402 generates sufficient power. Alternatively, any other suitable tunable laser or set of lasers with individual fixed wavelengths can be employed. For example, the four individual lasers shown in Magnification A of figures 5A to 6B provide laser output beams with four different wavelengths Àj, À2, À3 and À4. Preferably, 32 different wavelengths are employed. All of these alternatives are collectively included in the term "tunable laser" as used throughout the document. An amplified laser output from the optical amplifier 404 is preferably carried by an optical fiber to a 406 wavelength division multiplexer (WDM - Waveiength Division Multiplexer), such as a 100 GHz Athermal Arrayed Waveguide Grating from Gemfire Corporation of Fremont , California, USA.
    The outputs of the multiplexer 406 are a plurality of pulse beams, each of a different wavelength, each of which is preferably carried by a separate optical fiber. Preferably, a group 408 of 32 separate optical fibers 410 is employed to carry a corresponding number of laser output pulse beams with different wavelengths. The ends of the individual fibers 410 of the group 408 sit in the focal plane 412 of a lens 414 in a desired preferred circular configuration arranged to provide an optical output of lens 414 which has 32 non-mutually coherent pulse beams arranged around a conical surface . Alternatively, a cascade of lenses can be provided instead of lens 414. Magnification B, taken at focal plane 412, as designated by the lines of section BB, directed towards lens 414, shows fibers 410 and lens 414, in which the circular arrangement of the fibers is centered on the optical axis of Lens 412, which is designated by reference number 416. It is a particular additional feature of the embodiments of figures 5A to 6B that multiple pulse laser outputs are performed using a tunable laser whose output is coupled to a wavelength division multiplexer.
    It is also a particular additional feature of the realizations of figures 5A to 6B that the pulse laser outputs are distributed and arranged in a channel according to their wavelength by an apparatus, such as a wavelength division multiplexer, which does not it has moving parts and is therefore suitable for use in difficult and relatively inaccessible environments. It is noted that any suitable desired pattern or structure of pulse laser beam outputs can be realized in this way by properly arranging the ends of the fibers 410 in the focal plane 412 of a suitable lens 414. It is also noted that the ends of the fibers 410 in the focal plane 412 of lens 414 can be angled in a way that enhances the ability of lens 414 to collect light emission from the plurality of fibers 410, thus allowing lens 414 to be of relatively simple design and inexpensive, which in turn allows for a more robust and cheaper anemometer design and is therefore better suited for mass use on the market.
    The optical output of lens 412 typically collides with one or more folding mirrors that direct the pulse beams outward around a conical surface that has a central geometric axis (not shown). Pulse beams typically collide with particles, such as air molecules or molecules, or aerosols in the air, and are reflected thereby.
    Alternatively, the folding mirrors can be excluded and / or the lens can be replaced by one or more mirrors with optical power.
    As shown in figures 5A and 5B, the refection set optical elements, preferably incorporated in a mirror 422, receive reflections from the Iaser beams in the aerosol pulse in the air and optionally direct them through optical focusing elements 424, which typically comprise at least one lens, preferably for a 426 detector, typically an lnGaAs APDs detector or a lnGaAs PIN diode detector operating between 1,100 and 1,700 nanometers, both commercially available from Laser Components lG lnc. Hudson, New Hampshire, USA. Alternatively, as shown in figures 6A and 6B, optical focusing elements 424 can be excluded and an array of detectors 427 can be employed instead of detector 426. It is noted that the embodiments described in figures 5A to 6B may include a filter optical filtering light from wavelengths outside the fixed wavelengths generated by the anemometer before such light reaches detector 426 or array of detectors 427, thereby reducing the amount of background noise received by detector 426 or array of detectors 427.
    An amplified output of one or more detectors 426 is supplied 5 through an ND 428 converter (ADC - ND Converter) for the set of correlation circuits 429, which is operational to correlate signals derived from reflexes of the pulse beams varying in order to to provide information such as direction and speed of movement of aerosols in the air, whose information represents the speed of the wind. Correlation circuitry 429 is preferably incorporated into software residing on a programmable processor chip, such as an FPGA (Field Programmable Gate Array). In addition, other processing components such as a DSP (Digital Signal Processor) or a CPU (Central Processing Unit) can be employed to perform at least part of the required correlation calculations in real time. It is a particular feature of the present invention that the 429 correlation circuitry is operational to correlate between reflexes received from locations at the same or different distances along a single pulse beam and at locations at the same or different distances in different pulse beams and at different time intervals that represent a range of wind speeds that are to be measured. Preferably, a result of the correlation performed according to a preferred embodiment of the present invention is a vector at each location along the geometric axis of the tapered volume on which the wind speed is measured, which indicates the wind speed. It is another particular feature of the present invention that the correlation is performed on pulse laser beams that are not mutually consistent. This allows the use of a laser and optical elements in the anemometer, which are substantially much less expensive and can operate at lower signal-to-noise ratios than lasers and optical elements currently employed in conventional Doppler laser anemometers.
    5 Reference is now made to Figures 7A and 7B, which are simplified, partly schematic and partly illustrative of the structure and operation of another alternative embodiment of a non-coherent laser anemometer to monitor wind characteristics that includes a set of operative correlation circuits for provide wind speed output indications, and figures 8A and 8B, which are simplified, partly schematic and partly illustrative of the structure and operation of another alternative embodiment of a non-coherent laser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide wind speed output indications.
    As seen in figures 7A to 8B, an anemometer transmission controller 430, which includes a master oscillator and set of time setting circuits, provides timed control outputs for a 432 laser, such as a ULT laser commercially available from Eopsys SA de Lannion, France. The control outputs preferably control the power level and timing of the 432 laser pulse outputs. The 432 laser pulse outputs are typically carried by an optical fiber to a 434 optical amplifier, such as a High Power Variable Gain / Fixed Gain EDFA, commercially available from Red-C Optical Networks Ltd. of Israel, It is noted that any other suitable optical amplifier can be employed. It is also noted that the optical amplifier 434 can be excluded where the laser 432 generates sufficient power.
    An amplified laser output from the 434 optical amplifier is preferably carried by an optical fiber to a 436 switch, such as a Fast Fiber Optic 1x32 Switch, commercially available from SercA1O Microtechnology Ltd. of Schaan, Liechtenstein. Switch 436 is controlled by controller 430 so that the laser output of optical amplifier 434 is channeled to any of the output ports of switch 436 5 according to a command provided by controller 430. The outputs of switch 436 are one plurality of pulse beams, each of which is preferably carried by a separate optical fiber. Preferably, a group 438 of 32 separate optical fibers 440 is employed to carry a corresponding number of laser output pulse beams controlled by the control outputs provided by the controller
    430. The ends of the individual fibers 440 of the group 438 rest on the focal panel 442 of a Lens 444 in a desired preferential circular configuration arranged to provide an optical output from the lens 444 that has 32 pulse beams not mutually coherent arranged around a conical surface. Alternatively, a cascade of lenses can be provided instead of lens 444. Arrangement A, taken in focal plane 442, as designated by section lines AA, which faces lens 444 shows fibers 440 and lens 444, in that the circular arrangement of the fibers are centered on the optical axis of the lens 442, which is designated by the reference number 446. It is a particular additional feature of this embodiment of the present invention that the multiple pulse laser outputs are realized with the use of a laser whose output is coupled to a fiber optic switch- It is also a particular additional feature of the realizations of figures 7A to 8B that the pulse laser outputs can be distributed and arranged in channel according to control outputs provided by controller 430, by device, such as a switch, which has no moving parts and is therefore suitable for use in difficult and relatively inaccessible environments. Alternatively, pulse outputs from Iaser can be distributed and channeled by other mechanisms, such as through a rotation mirror or MEMS technologies.
    It is noted that any suitable desired arrangement of 5 pulse laser outputs can be carried out in this way through the appropriate arrangement of the ends of the fibers 440 in the focal plane 442 of a suitable lens 444. It is also noted that the ends of the fibers 440 in the focal plane 442 of lens 444 can be tilted in a way that enhances the ability of lens 444 to collect light emission from the plurality of fibers 440, thus allowing lens 444 to be of a relatively simple and inexpensive design, which in turn instead, it allows an anemometer design to be more robust and less expensive to manufacture and, therefore, better suited for use in the mass market.
    The optical output of lens 444 typically strikes one or more folding mirrors that direct the pulse beams outward around a conical surface that has a central geometric axis (not shown).
    Pulse beams typically collide into particles, such as air molecules or molecules or aerosols in the air, and are reflected thereby.
    Alternatively, the folding mirrors can be excluded and / or the lens can be replaced by one or more mirrors with optical power. As shown in figures 7A and 7B, the optical elements of the reflection set, preferably incorporated in a mirror 452, receive reflections from the laser beams in the aerosol pulse in the air and optionally direct them through optical focusing elements 454, which typically comprise at least one lens, preferably for a 456 detector, typically an InGaAs APDS detector or a lnGaAs PIN diode detector operating between 1,100 and 1,700 nanometers, both commercially available from Laser Components lG lnc. from Hudson, New
    Hampshire, USA. Alternatively, as shown in figures 8A and 8B, the focusing optical elements 454 can be excluded and an array of detectors 457 can be employed instead of detector 456.
    It is noted that the achievements described in figures 7A to 8B 5 may include an optical filter that filters light from wavelengths outside the range of wavelengths generated by the anemometer before such light reaches detector 456 or the array of detectors 457, thereby reducing the amount of antecedent noise received by detector 456 or detector arrangement 457.
    An amplified output from one or more detector 456 is supplied through an A / D converter 458, for the set of correlation circuits 459, which is operational to correlate signals derived from reflexes of the pulse beams that are variably directed to provide information such as direction and speed of movement of aerosols in the air, whose information represents the speed of the wind. The 459 correlation circuitry is preferably incorporated into software residing on a programmable processor chip, such as an FPGA. In addition, other processing components such as a DSP or a CPU can be employed to perform at least part of the required correlation calculations in real time. It is a particular feature of the present invention that the 459 correlation circuitry is operational to correlate between reflections received from locations at the same or different distances along a single pulse beam and at locations at the same or different distances in different pulse beams and at different time intervals that represent a range of wind speeds that will be measured- Preferably, a result of the correlation performed according to a preferred embodiment of the present invention is a vector at each location! along the geometric axis of the tapered volume on which the wind speed is measured, which indicates the wind speed. It is another particular feature of the present invention that the correlation is performed on pulse laser beams that are not mutually coherent. This allows the use of a laser and optical elements in the anemometer that are substantially much less expensive and that can operate at lower signal-to-noise ratios than lasers and optical elements currently employed in conventional Doppler laser anemometers. Reference is now made to Figure 9, which is a simplified, partly schematic and partly illustrative illustration of the structure and operation of yet another alternative embodiment of a non-coherent laser anemometer to monitor wind characteristics that includes set of operative correlation circuits to provide wind speed output indications- Conforrne seen in figure 9, an anemometer transmission controller 460, which includes a master oscillator and the timing set circuitry, provides timed control outputs for a 462 laser, such as a KULT commercially available from Keopsys SA of Lannion, France - The control outputs preferably control the power level and timing of the 462 laser pulse outputs. The 462 laser pulse outputs are typically carried by an optical fiber to a 464 optical amplifier, such as a High Power Variable Gain / Fixed Gain EDFA, commercially available from Re d-C Optical Networks Ltd.
    Israel. It is noted that any other suitable optical amplifier can be employed. An amplified laser output from the 464 optical amplifier is preferably carried by an optical fiber to a 466 splitter, such as a PLC-based splitter.
    The outputs of divider 466 are a plurality of simultaneous pulse beams, each of which is preferably simultaneously transported by a separate optical fiber. Preferably, a group 468 of 32 separate optical fibers 470 is employed to carry a corresponding number of beams in laser output pulse with identical wavelengths. The ends of the individual fibers 470 of the group 468 lie on the focal plane 472 of a lens 474 in a desired preferential circular configuration arranged to provide an optical output of the lens 474 with 32 non-mutually coherent pulse beams arranged around a conical surface, Alternatively, a cascade of lenses can be provided instead of lens 474. Magnification A, taken in focal plane 472, as designated by section lines A - A, which faces lens 474 shows fibers 470 and lens 474 , in which the circular arrangement of the fibers is centered on the optical axis of the lens 474, which is designated by reference number 476. It is a particular additional feature of this embodiment of the present invention that the multiple Iaser outputs on the pulse are realized with the use of a laser whose output is coupled to a divider. It is also a particular feature of the realization of figure 9 that the pulse laser outputs are generated by the device, such as a divider, which has no moving parts and is therefore suitable for use in difficult and relatively inaccessible environments.
    It is noted that any suitable desired arrangement of pulse laser outputs can be carried out in this way through the proper arrangement of the ends of the fibers 470 in the focal plane 472 of the lens 474. It is also noted that the ends of the fibers 470 in the focal plane 472 of the 474 lens can be tilted in a way that enhances the 474 lens’s ability to collect light emission from the 470 fiber naturality,
    thus allowing the 474 lens to be of an inexpensive and relatively simple design, which, in turn, allows an anemometer design to be more robust and cheaper and, therefore, better suited for use in the mass market.
    5 The optical output of the 474 lens typically strikes one or more folding mirrors that direct the pulse beams outward around a conical surface that has a central geometric axis (not shown).
    Pulse beams typically collide in particles, such as air molecules or molecules or aerosols in the air, and are thereby reflected.
    Alternatively, the folding mirrors can be excluded and / or the lens can be replaced by one or more mirrors with optical power.
    As shown in figure 9, the optical elements of the reflection set, preferably incorporated in a mirror 482, receive reflections from the laser beams in the aerosol pulse in the air and direct them preferably to a 487 array of detectors, preferably a detector for each of the pulse laser beams, typically an APDS lnGaAs detector or a PÍN diode detector that operates between 1,100 and 1,700 nanometers, both commercially available from the Laser Components lNc. Hudson, New Hampshire, USA.
    It is observed that the achievements described in figure 9 may include an optical filter that filters light of wavelengths outside the range of wavelengths generated by the anemometer before such light reaches the array of detectors 487, thus reducing the amount of noise received by the array of detectors 487.
    An amplified output from array 487 of detectors is supplied through an array 488 of 32 ADC converters corresponding to the 32 pulse beams, for the set of correlation circuits 489, which is operational to correlate signals derived from reflexes of the variously directed pulse beams in order to provide information such as direction and speed of movement of aerosols in the air, whose information represents the speed of the wind. The correlation circuitry 489 is preferably incorporated into software residing on a programmable processor chip, 5 such as an FPGA. In addition, other processing components such as a DSP or a CPU can be employed to perform at least part of the required correlation calculations in real time. It is a particular feature of the present invention that the 489 correlation circuitry is operational to correlate between reflections received from Iocais at the same or different distances along a single pulse beam and at locations at the same distances or at different distances in different pulse beams and at different time intervals that represent a range of wind speeds that will be measured. Preferably, a result of the correlation performed according to a preferred embodiment of the present invention is a vector at each location along the geometric axis of the tapered volume in which the wind speed is measured, which indicates the wind speed. It is another particular feature of the present invention that the correlation is performed on pulse laser beams that are not mutually consistent. This allows the use of a laser and optical elements in the anemometer which are substantially much less expensive and which can operate at signal ratios for lower noise, than lasers and optical elements currently employed in conventional Doppler laser anemometers.
    Reference is now made to figure 10, where a simplified flowchart illustrates the operation of the system correlation circuitry of figures 5A to 9, and figure 11 is a simplified pulse laser beam correlation diagram useful in understanding the operation of the system of figures 5A to 9 for pulse laser beams directed generally and vertically.
    As described above in this document with reference to Figures 5A to 9, a plurality of pulse laser beams, preferably 32 5 in number, is directed along a centralized conical surface and a geometric axis 490. The geometric axis 490 can be directed in any suitable direction. Typically, when a laser anemometer is located on a ground surface, the 490 geometry axis is directed vertically. When an Iaser anemometer is located in a nacelle of a wind turbine, the 490 geometry axis is typically in a horizontal plane.
    In the illustrated example, described below in this document, the geometric axis 490 is vertical. Figure 11 shows four typical pulse laser beams, designated in the present context by the letters, A, L, P and R, which are arranged along a conical surface around the 490 geometric axis. As shown in the simplified flowchart in the figure 10 in block 502, initially the signals representing the laser radiation of the plurality of Iaser beams retro-designed by aerosols in the air at various distances from the laser anemometer, which represent various vertical heights.
    are collected for a predetermined measurement time. Subsequently, as shown in block 504, a certain vertical height at which the measurement of a wind speed vector is chosen.
    Subsequently, as shown in block 506, the initial correlations of signals received at locations in different pairs of beams, which are at the same distance from the anemometer, are performed. Where the 490 geometry axis is vertical, these correlations are generally between locations that are generally on the same horizontal plane. This is based on a consideration that the wind is generally horizontal. Such correlations are preferably initially performed between some, but not all, pairs of laser pulse beams, typically the A, L. P and R beams shown in Figure 11. Graph I reveals the signal received from location A 13, Graph ll reveals signal 5 received from location A12 and Graph | j reveals signal received from location L13. A typical correlation graph is designated as the correlation graph I and shows the correlation between signals received from location L13 and signals received from Location A13, where locations L13 and A13 are typically separated by 25 meters. A maximum correlation between the signals received from the two locations is expected in the time it takes for the wind to flow from L13 to A13. The Correlation Graph l shows that the maximum correlation between the signals received from the two locations is received in a time shift of 5 seconds, q which means that the average horizontal wind speed between Iocais L13 and A13 is 5 meters per second.
    Based on the results of various correlations between different pairs of pulse laser beams, typically A, L, P and R at the same height, an approximate indication of the direction and amplitude of a horizontal projection of a wind speed vector is checked against that height.
    Subsequently, as shown in block 508, additional correlations are conducted, using selected beams that generally lie in proximity to the trajectory of the horizontal projection of the wind speed vector, over a range of displaced times that rest around the displaced time represented by the correlation peak, such as that in correlation graph I. These additional correlations provide an enhanced resolution correlation in terms of direction and in terms of displaced time, thereby providing an enhanced resolution horizontal projection of the vector of wind speed at the given height.
    Subsequently, as shown in block 510, additional correlations are performed between locations at different distances from the laser anemometer, that is, at different heights. A typical correlation is shown in figure 11 between locations L13 and A 12.
    5 A typical correlation graph for such additional correlation is designated as the ll correlation graph, and shows the correlation between signals received from location L13 and signals received from location A12, locations L13 and A12 that are typically 27 meters apart. A maximum correlation between the signals received from the Iocais is expected in the time it takes for the wind to flow from L13 to A12. As seen in the ll correlation graph, this maximum correlation is higher than the maximum correlation shown in graph I, which indicates that the true wind vector is not exactly horizontal, but preferably in the direction from L13 to A12. The Correlation Graph ll also shows that the correlated peak is received in a time shift in the 5 second time shift, which means that the average wind speed between L13 and A12 is 5.4 m / s.
    Based on the results of various correlations between the different pairs of pulse laser beams, typically A, L, P and R at different heights in the vicinity of the height at which the horizontal correlations were performed, an indication of a vector velocity. wind is checked against that height.
    As shown in block 512, the above procedure is repeated for all relevant heights at which a wind speed vector is to be measured and is preferably repeated over time. The predicted velocity vectors are stored and used as appropriate. Reference is now made to Figure 12, which is a simplified flowchart illustrating the operation of the system correlation circuitry of Figures 5A to 9, and Figure 13, which is a useful simplified pulse laser beam correlation diagram. in understanding the operation of the system of figures 5A to 9 for laser beams in general and horizontally oriented pulses. As described above in this document in reference 5 to Figures 5A to 9, a plurality of pulse laser beams, preferably 32 in number, is directed along a conical surface centered on a geometric axis 690. The geometric axis 690 can be directed in any suitable direction. Typically, when a laser anemometer is located on a ground surface, the 690 geometry axis is directed vertically. When a laser anemometer is located in a nacelle of a wind turbine, the 690 geometry axis typically rests on a horizontal plane.
    In the illustrated example, described below in this document, the geometric axis 690 is horizontal. Figure 13 shows four typical pulse laser beams, designated in the present context by the letters, A, L, P and R, which are arranged along a conical surface around the geometric axis
    690.
    As indicated in the simplified flowchart of figure 12 in block 702, initially the signals that represent the laser radiation of the plurality of laser beams retro-projected by aerosols in the air at various distances from the laser anemometer, which represent several generally horizontal distances from the laser anemometer , are collected over a predetermined measurement time. Subsequently, as shown in block 704, a determined distance from the laser anemometer over which the measurement of a wind speed vector is chosen.
    Subsequently, as shown in block 706, the initial correlations of signals received from different locations at approximately the given distance along a particular beam are performed, preferably, for some, but not all, pulse laser beams, typically the bundles A, L, P, and R shown in figure 13. This is based on a consideration that the wind is generally horizontal. Graph I reveals the 5 signal received from site A12, Graph | reveals the signal received from site A11, Graph III reveals the signal received from site AlO and Graph IV reveals the signal received from site R9.
    A typical correlation graph is designated as the correlation graph I and shows the correlation between the signals received from the Local AlO and the signals received from the A12 site, where the AlO and A12 sites are typically separated by 20 meters. A maximum correlation between the signals received from the two locations is expected in the time it takes for the wind to flow from AlO to A12. The Correlation Graph] shows that the maximum correlation between the signals received from the two locations is received in a time shift of 2 seconds, which means that the average wind speed between the AlO and A12 locations is 10 meters per second.
    Based on the results of various correlations between locations at approximately the given distance along a particular beam from some pulse laser beams, typically A, L, P and R, an approximate indication of the direction and amplitude of a horizontal projection of a wind speed vector is verified in relation to the distance determined along beam A.
    Subsequently, as shown in block 708, additional correlations are conducted, using selected beams that generally lie in proximity to the trajectory of the horizontal projection of the wind speed vector, over a range of displaced times that rest around the displaced time represented by the correlation peak, such as that in the correlation graph I. These additional correlations provide an enhanced resolution correlation result in both direction and displaced time, thereby providing an enhanced resolution horizontal projection of the wind speed vector at the given distance.
    5 Subsequently, as shown in block 710, additional correlations are performed between locations in different bundles.
    A typical correlation graph for such additional correlation is designated in Figure 13 as the correlation graph ll, and shows the correlation between signals received from site R9 and signals received from site A11, where sites R9 and A11 are typically separated by 25 meters. A maximum correlation between the signals received from the locations is expected at the time it takes for the wind to flow from R9 to A11. As seen in the correlation graph |, this maximum correlation is higher than the maximum correlation shown in graph I, which indicates that the true wind speed is not along beam A, but preferably in the direction from R9 to A11. The Correlation Graph ll also shows that the peak in the correlation is received in a time shift of 2 seconds, which means that the average wind speed between locations R9 and A11 is 12.5 meters per second.
    Based on the results of various correlations between different pairs of pulse laser beams, typically A, L, P, and R, an indication of a wind speed vector is obtained at the distance determined along the horizontal geometric axis 690 .
    As shown in block 712, the above procedure is repeated for all relevant distances from the laser anemometer in which a wind speed vector is measured and is preferably repeated over time. The predicted velocity vectors are stored and used as appropriate.
    Reference is now made to figure 14, which is a typical correlation graph produced by the set of correlation circuits of the non-coherent laser anemometer in figures 5A to 9.
    A C (t) correlation function can be mathematically described as follows: E = C [lÀ (t, + _t) - Í4] [IB (t,) - Ll C ('") = | u" i ) '4E; = õ! LA (t,) _ Ti]' E: = e [l8 't; _ Íg] "where: | a and | b are the intersections of reflected laser beams from locations A and B in space, respectively, as a function of time; tj marks one of the n time points at which the samples of reflexes are recorded; ÍLj and Íb are the average intensities of reflexes from locations A and B respectively over n samples recorded at n points in time; et is a time difference parameter for which the correlation function is being calculated, t can be positive or negative. As seen in figure 14, the correlation function C reaches a peak at a time difference of Tp which represents the time it takes for the specific reflection pattern to move from Iocal A to B in space, thus creating a peak correlation between the intensities of the reflected laser beams measured at location A and location B within that time difference, whereas the displacement of the reflection pattern in space is almost unchanged with the Iocal wind vector (at least by a period of temp the short, which is the same order of magnitude as Tp. The correlation peak actually measures the time it takes for the wind to transport the reflective particles from location A to location B and,
    therefore, the peak correlation time is directly proportional to the average wind speed between locations A and B in space. As described above in this document in relation to figures 11 and 13, the construction of multiple correlation functions between multiple locations in the space and then the analysis of the peaks resulting from the different correlation functions generally facilitates the accurate calculation of both the velocity of the wind and the direction of the wind in space.
    As is known to those skilled in the art, and as shown by Ting-i Wang et. al incorporated as a reference in this document, additional methods are available to calculate a wind vector from a correlation function. Such methods include measuring the slope of the correlation function around a time difference of Tp = 0, measuring the width of an autocorrelation function that is a correlation between location A and location A and / or measuring the crossing point the autocorrelation function and the correlation function. All of these parameters provide generally accurate calculations of the wind speed being measured by the laser anemometer between at least two locations in space. It will be appreciated by those skilled in the art that the present invention is not limited by what has been particularly shown and described above in this document. Preferably, the invention also includes various combinations and sub-combinations of the features described above in this document, as well as modifications and variations thereof, which would occur to those skilled in the art upon reading the background and which are not in the prior art.
    权利要求:
    Claims (10)
    [1]
    1. SYSTEM FOR MONITORING WIND CHARACTERISTICS IN A VOLUME, characterized by the fact that it comprises: a plurality of laser anemometers (100, 200, 300, 350) 5 not coherent operational to measure wind characteristics in a plurality of corresponding localized subvolumes within said volume: and a data processing subsystem (102, 212, 312, 362) operational to receive data from said anemometers (100, 200, 300, 350) to Iaser non-coherent and to provide output data that represent said wind characteristics in said volume.
    [2]
    2. SYSTEM FOR MONITORING WIND CHARACTERISTICS IN A VOLUME, according to claim 1, characterized by the fact that it also includes operational modeling functionality to calculate maximum output power and ideal locations of a plurality of wind turbines (106, 2 ' 16).
    [3]
    3. LASER ANEMOMETER, characterized by the fact that it comprises: a tunable Iaser (402): a scanner, which receives an output from said tunable laser (402) and which provides laser beam outputs in several scanning directions; at least one detector (426, 456) for receiving retro-designed laser beam output signals; and wherein said tunable laser (402) is a laser with tunable wavelength and said scanner is a wavelength responsive scanner, which receives said output at multiple wavelengths and which provides said beam outputs of taser in several scanning directions according to said multiple wavelengths.
    [4]
    4. LASER ANEMOMETER, characterized by the fact that it comprises: 5 an Iaser; an optical switch responsive to a control signal to provide laser beams in various scanning directions that are inconsistent when they collide with particles in the atmosphere; and at least one detector (426, 456) for receiving signals from overhead projected laser beam outputs that are non-coherent.
    [5]
    5. LASER ANEMOMETER, according to claim 4, characterized by the fact that it also comprises a set of correlation circuits (429, 489) operational to correlate signals received by said at least one detector (426, 456).
    [6]
    6. LASER ANEMOMETER, according to claim 4, characterized by the fact that it comprises an optical switch that has no moving parts.
    [7]
    7. LASER ANEMOMETER, according to claim 4, characterized by the fact that the optical switch is a MEMS optical switch.
    [8]
    8. LASER ANEMOMETER, characterized by the fact that it comprises: a laser; a laser beam splitter to provide laser beam outputs simultaneously in a plurality of scanning directions; and a plurality of detectors (426, 456) for receiving signals from the rear projection of said laser beam outlets.
    [9]
    9. LASER ANEMOMETER, according to claim 8, characterized by the fact that it also comprises a set of correlation circuits (429, 489) operational to correlate signals received by said detector (426, 456) - 5
    [10]
    10. SYSTEM TO CONTROL THE OPERATION OF MULTIPLE WIND TURBINES, characterized by the fact that it comprises: a plurality of anemometers (100, 200, 300, 350) operational to measure wind characteristics in at least a plurality of locations; a data processing subsystem (102, 212, 312, 362) operational to receive data from said plurality of anemometers (100, 200, 300, 350) and to provide output data representing said wind characteristics in said plurality of locations; a control subsystem (104, 214) which receives said output data from said data processing subsystem (102, 212, 312, 362) and which provides wind turbine control signals (106, 216) for a plurality of wind turbines (106, 216) located at least in general proximity to said plurality of locations; and wherein said plurality of anemometers (100, 200, 300, 350) comprises a plurality of laser anemometers (100, 200, 300, 350).
    11. SYSTEM, according to claim 10, characterized by the fact that said plurality of laser anemometers (100, 200, 300, 350) comprises at least one non-coherent laser anemometer (100, 200, 300, 350) -
    12. SYSTEM, according to claim 10, characterized by the fact that said data processing subsystem (102, 212, 312, 362) receives said data from said plurality of anemometers (100, 200, 300, 350) through a wireless communication link (112, 116. 222, 226, 322, 372).
    13. SYSTEM, according to claim 10, 5 characterized by the fact that said plurality of anemometers (100, 200, 300, 350) includes at least one anemometer (100, 200, 300, 350) oriented in a horizontal direction .
    14. SYSTEM, according to claim 10, characterized by the fact that said plurality of anemometers (100, 200, 300, 350) includes at least one anemometer (100, 200, 300, 350) oriented in a vertical direction.
    15. SYSTEM, according to claim 10, characterized by the fact that said wind turbine control signals (106, 216) comprise at least one of a rotor alignment signal, a paddle step signal and a signal rotor lock.
    16. METHOD FOR MONITORING WIND CHARACTERISTICS IN A VOLUME, characterized by the fact that it comprises: using a plurality of non-coherent laser anemometers (100, 200, 300, 350) to measure wind characteristics in a plurality of corresponding sub-volumes located within said volume; and using a data processing subsystem (102, 212, 312, 362) to receive data from said plurality of non-coherent laser anemometers (100, 200, 300, 350) to provide output data representing said characteristics of wind in said volume.
    17. METHOD TO CONTROL THE OPERATION OF MULTIPLE WIND TURBINES, characterized by the fact that it comprises:
    use a plurality of anemometers (100, 200, 300, 350)
    to measure wind characteristics in at least a plurality of locations;
    use a data processing subsystem (102, 212,
    312, 362) to receive data from said plurality of anemometers (100, 200, 300, 350) and to provide output data representing said wind characteristics in said plurality of locations; use a control subsystem (104, 214) to receive said output data from said data processing subsystem (102,
    212, 312, 362) and to provide wind turbine control signals for a plurality of wind turbines (106, 216) located at least in general proximity to said plurality of locations; and in which the said plurality of anemometers (100, 200, 300,
    350) comprises a plurality of laser anemometers (100, 200, 300, 350).
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    同族专利:
    公开号 | 公开日
    EP2483698A4|2013-02-20|
    CN104101731B|2017-04-12|
    WO2011036553A1|2011-03-31|
    EP2483698B1|2015-07-08|
    CN104101731A|2014-10-15|
    US20110106324A1|2011-05-05|
    US8701482B2|2014-04-22|
    CA2775222A1|2011-03-31|
    AU2010299566A1|2012-05-03|
    EP2483698A1|2012-08-08|
    ZA201202760B|2012-12-27|
    CN102667495A|2012-09-12|
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    法律状态:
    2020-09-01| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
    2020-09-08| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
    2020-12-22| B11B| Dismissal acc. art. 36, par 1 of ipl - no reply within 90 days to fullfil the necessary requirements|
    2021-11-03| B350| Update of information on the portal [chapter 15.35 patent gazette]|
    优先权:
    申请号 | 申请日 | 专利标题
    US24617409P| true| 2009-09-28|2009-09-28|
    US61/246,174|2009-09-28|
    US28599109P| true| 2009-12-13|2009-12-13|
    US61/285,991|2009-12-13|
    US35197610P| true| 2010-06-07|2010-06-07|
    US61/351,976|2010-06-07|
    US35239610P| true| 2010-06-08|2010-06-08|
    US61/352,396|2010-06-08|
    PCT/IB2010/002434|WO2011036553A1|2009-09-28|2010-09-28|Methods, devices and systems for remote wind sensing|
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