This application claims priority to India Patent Application No. 151/KOL/2005, filed Mar. 10, 2005, which is incorporated herein by reference.
Constant Altitude Plan Position Indicator (CAPPI) is a form of data presentation in weather radars. For CAPPI scanning, a horizontal slice is taken through the radar volume scan data at a constant altitude above the earth surface. The radar volume scan data is extracted from full 3-D scan data, and is converted to a 2-D format for presentation in polar coordinates on a computer display, paper printout, or any other two-dimensional surface.
CAPPI is a variant of the more general Plan Position Indicator (PPI) that displays weather parameters along radials from the radar as function of an azimuth scan angle. A radar antenna transmits and receives pulses at different elevation angles φ and at different azimuth angles θ by both performing a rotating scan operation in the azimuth and by varying the elevation angle. PPI data is generated and recorded by scanning a beam circularly at a constant elevation angle. A volume scan consists of multiple constant-elevation azimuth scans. PPI volume scan data at multiple elevation angles is used to produce CAPPI.
Near the radar site there is often ground clutter, which may interfere with obtaining a clean display of weather. In the beam position(s) with low elevation angle(s), clutter is often so strong that filtering the ground clutter also removes weather signals resulting in gaps in the weather display.
In PPI scanning, the radar beam may overshoot precipitation altitudes, for a part of the radial, and thereby not detect any precipitation at the corresponding ranges (i.e. distances from the radar).
Weather radar systems often deliberately degrade the time resolution for observation in order to improve signal quality and also to reduce the data handling specifications over long observation periods. The PPI volume scanning mode also degrades the spatial resolution by skipping certain elevation angles to reduce the time for scanning the region around the radar.
The maximum elevation of scan may be limited to a value less than 90° (i.e. vertical pointing), leaving a conical ‘blind zone’ over the radar location. This causes a circular hole to appear in the CAPPI, the hole being larger at higher altitudes.
Individual radars may be limited in their range coverage. To get a weather picture over a large geographical area, data may be combined from multiple radars that are spatially separated.
Combining CAPPI data from multiple radars may pose technical challenges. When a geographical area is covered by many radars, the coverage pattern is not uniform. Certain areas may not be covered at all (i.e. fall between coverage zones of individual radars), certain areas may have coverage only from a single radar, certain areas may have coverage from two radars, certain areas may be covered by three radars, and certain other areas may receive coverage from more than three radars. Such variability of coverage poses technical challenges in data combining.
CAPPI Data Generation
An elevation angle φ represents the angle at point D between the earth's surface (i.e. a tangent to the Earth's surface at point D) and the line CD. The specific elevation angle φ may have been skipped during the radar scan operation. In an example embodiment, gaps such as this may be filled using an interpolation scheme to potentially provide spatially continuous information of weather at the given altitude H. The elevation angle φ of the radar is computed for each increment in EC using equation set (2) and
Because the Earth is curved and the scan elevation interval may be between a minimum value and a maximum value, a point such as point C in
Embodiments may account for bending of the radar beam. The radar beam may bend as it passes through layers of air with different refractive indices. Under standard atmospheric conditions, the bending of the radar beam has a radius of curvature about four times the radius of the Earth. Thus, under normal conditions, a radar beam emitted horizontally and at other elevations would take paths that curve slightly below straight line paths.
In a volume scanning mode, an elevation angle φ of the antenna 101 is changed incrementally by a determined angle and a horizontally rotating scanning operation is performed along each incremented elevation angle. CAPPI data for point C may not be readily available in the volume scan data, and may be constructed from radar data gathered along other elevation angles and/or azimuth angles, in embodiments of the present invention. The CAPPI data at point C may be generated by interpolating the gathered radar data in elevation. Elevation angles φm and φm-1 denote the elevation angles of the radar scan that are closest to angle φ, on either side, as shown in
In
In the example embodiments, the CAPPI scan line data is generated by keeping EC constant and varying the azimuth angle θ of the radar from 0 to 2π (or a certain θmin to θmax for a sectoral CAPPI) clockwise or counter-clockwise depending on the direction of the radar scan. As discussed in more detail with regard to the process of
In the second step of the CAPPI construction, the CAPPI scan line data is presented to the PPI coordinate conversion, formatting and display mechanism.
Latitude-Longitude Coordinate System
The CAPPI radar data may be converted from the individual radar coordinates to a universal grid system as follows. Let Re denote the radius of the earth and H be the altitude above the Earth's surface 245 at which the mosaic is to be constructed. Coordinate (λmin, φi) may be the latitude-longitude location of the radar i on the earth's surface 245.
Coordinates ((λmin
The coordinates ((λmin,φmin), (λmax,φmax)) of the MBR for N radars may be calculated as arguments of the minimum and maximum values, respectively, where i=1, 2, . . . N.
λmin=arg mini=1,2, . . . ,Nλmin
λmax=arg maxi=1,2, . . . ,Nλmax
φmin=arg mini=1,2, . . . ,Nφmin
φmax=arg maxi=1,2, . . . ,Nφmax
A distance d between two latitude-longitude points (λ1,φ1) and (λ2,φ2) may be calculated as
d((λ1,φ1),(λ2,φ2))=Re cos−1(cos(λ1)cos(λ2)cos(φ1−φ2 )+sin(λ1)sin(λ2)) (9)
Mosaic For Multiple Radars
In this embodiment, there are 13 separate regions in the mosaic 250. The regions along with the overlapping radars are shown in Table I. Table I is indexed by region and shows the corresponding radars in that particular region. The region may or may not have overlapping radars. In the instance where there are at least two radars covering the region, there are overlapping radars. In the regions covered by three radars (e.g. regions 4, 5, 8, 9) or more than three radars (e.g. region 7), a three dimensional wind vector may be constructed. A two dimensional wind vector may be constructed for a region with two overlapping radars (e.g. regions 2, 6, 10, 12).
Flowcharts
At block 305 of
At block 320, an arc length EC (φm) may be calculated for each elevation angle φm of the radar. The interval for the elevation number m may be: 0≦m<M. The elevation number m may be incremented, by 1, for example, in the interval. The arc length EC may be calculated for each elevation angle φm with the formula:
EC(φm)=(Re+H)×[cos−1 (Re cos (φm)/(Re+H))−φm].
At block 330, a first mechanism of EC(φm) values in terms of the elevation number m of the radar may be generated using the values generated at block 320. The first mechanism may be a look up table indexed by elevation number m and/or elevation angle φm, a graph, an algorithm, a chart, and/or any other possible mechanism.
At block 335, the process of generating the first mechanism ends.
At block 401, the process 400 of
At block 405, the process 400 sets the value of the arc length EC, illustrated in
At block 410, the length EC is incremented by one step, which may be one (1) km or any other chosen value.
At block 415, the range CD and the corresponding angle φ may be calculated using equation (2). The range AC may be calculated using the equation: AC=CD×sin(φ−φM-1)/(cos(φM-1+β). The range DA may be calculated by solving for DA in the equation:
Optionally, for a given radar and scan cycle, instead of calculating the range DA, the values of range DA may be read from a pre-stored mechanism, such as a pre-stored look-up table LUTR, of range DA indexed by arc length EC. The pre-stored mechanism may be from a previous computation of the range DA for the same CAPPI altitude.
The azimuth angle θ may be incremented from θmin to θmax in steps of Δθ, where Δθ may be any degree, such as 1 degree. The radar data ZA may be retrieved at range DA, from the original scan data at elevation φM-1, for all θ values. The radar data ZA may be stored in a CAPPI scan line data buffer indexed by arc length EC and azimuth angle θ.
At block 420, the process 400 is queried as to whether EC is less than or equal to EC(φM-1). If the answer to the query is ‘yes’ then the process may proceed to block 410. If the answer to the query is ‘no’, then the process may proceed to block 425.
At block 425, m may be initialized to M-1 and the process may proceed to block 430 in
At block 430, the weights BC and AC may be calculated using the equations BC=CD×sin(φm−φ)/(cos(φm+β) and AC=CD×sin(φ−φm-1)/(cos(φm-1+β), where CD and φ are obtained using equation (2). Optionally, for a given radar and scan cycle, the values of weights BC and AC may be read from a pre-stored mechanism, such as a pre-stored look-up table LUTW, from a previous computation of BC and AC for the same CAPPI altitude.
At block 435, determine ranges DB and DA solving for DB and DA in the equations:
respectively. Optionally, for a given radar and scan cycle, the values of ranges DB and DA may be read from a pre-stored mechanism, such as the look-up table LUTR indexed by arc length EC, from a previous computation of ranges DB and DA for the same CAPPI altitude.
At block 440, CAPPI data is calculated at point C. Weather data ZA may be retrieved from the radar volume scan data for elevation φm-1 and range DA. Weather data ZB may be retrieved for elevation φm and range DB from the radar volume scan data. The weather data ZC at CAPPI data point C is the interpolation of ZA and ZB with weights BC and AC, and may be calculated according to the equation
At block 445, the length EC is incremented by one step.
At block 450, the process is queried as to whether EC is less than or equal to EC(φm-1). If the answer to the query is ‘yes’ then the process may proceed to block 430. If the answer to the query is ‘no’, then the process may proceed to block 455.
At block 455, m is decremented by 1.
At block 460, the process is queried as to whether m is equal to 1. If the answer to the query is ‘no’ then the process may proceed to block 430. If the answer to the query is ‘yes’, then the process proceeds to block 465. The process may proceed to block 465 in
At block 465, for a given arc length EC, calculate weight BC using the equation BC=CD×sin(φ1−φ)/(cos(φ1+β), then solve for range DB using the equation:
Angle θ may be incremented from θmin to θmax in steps of Δθ. The radar data ZB at range DB may be retrieved from the scan data at elevation φ1, for all θ values. The radar data ZB may be stored in CAPPI scan line data buffer indexed by length EC and angle θ. Optionally, for a given radar and scan cycle, the values of DB may be read from the pre-stored mechanism, such as the pre-stored look-up table LUTR indexed by EC, from a previous computation of range DB for the same CAPPI altitude.
At block 470, the length EC is incremented by one step.
At block 475, the process is queried as to whether EC is less than or equal to EC(φ0) at φ0=0°. If the answer to the query is ‘yes’ then the process proceeds to block 465. If the answer to the query is ‘no’, then the process proceeds to block 480.
At block 480, CAPPI scan line data generation ends.
At block 485, PPI display scan conversion occurs, as described herein. PPI scan converted CAPPI scan line data may be obtained and stored.
At block 490, the generated CAPPI radar data ZC along the surface 202 at the altitude H above the earth's surface may be displayed on the display 104 and/or printed.
Superposition of Scalar Data
The process 600 for constructing the mosaic of scalar data with data from N radars may begin at block 605.
At block 610 the Minimum Bounding Rectangle (MBR) coordinates ((λmin
At block 620, coordinates associated with the MBR for N radars ((λmin,φmin), (λmax,φmax)) may be determined using equation (8).
At block 630, grid resolution parameters (dimensions of latitude-longitude cell) δλ and δφ, may be set to any specified value. The latitude-longitude cell of dimension δλ and δφ at location (λmin,φmin) is chosen as the first of the latitude-longitude cells x within the MBR for N radars, obtained in block 620.
At block 640, a sum s of individual CAPPI data at x, from all weather radars observing cell x, is set to zero. A number of overlapping radars n is set to zero. The radar index i is set to 1. The index of cell x is set to 1.
At block 650, the process 600 queries as to whether designated conditions are met for radar i. If the answer to the query is no, the process proceeds to block 680 with s and n held at their current values. If the answer to the query is yes, the process proceeds to block 670.
For the latitude-longitude cell x at coordinates (λ, φ), the designated conditions include first checking if the inequality λmin
At block 670, the number of overlapping radars n is set to n+1. The sum of weather data s is set to (s+PPI scan-converted CAPPI scan line data from the ith radar at the cell x). The PPI scan-converted CAPPI scan line data from the ith radar at the cell x may be obtained by first computing the east-west distance dEWi and north-south distance dNSi using the formulae dEWi=d((λi,φ), (λi,φi)) and dNSi=d((λ,φi), (λi,φi)) respectively, of x from the ith radar location. The PPI scan converted data obtained and stored at block 485 of
At block 680, the process 600 is queried as to whether radar index i is less than or equal to the number of radars N. If the answer to the query is yes, the process proceeds to block 690. If the answer to the query is no, the process proceeds to block 700.
At block 690, the radar index i may be set to i+1. The process then proceeds to block 650 such that determinations may be made for each radar i.
At block 700, the process is queried as to whether the number of overlapping radars n is equal to zero. If the answer to the query is no, the process proceeds to block 720. If the answer to the query is yes, the process proceeds to block 730.
At block 720, weather data at cell x having coordinates (λ, φ), may be set to the sum s of individual radar CAPPI data, divided by the number of overlapping radars n. The process may proceed to block 735.
At block 730, there are no overlapping radars at cell x (λ, φ), and the weather/mosaic data at cell x (λ, φ), may be set to zero. The process may proceed to block 735.
At block 735, weather data for cell x, at (λ, φ), may displayed against the coordinates λ and φ. In case of reflectivity data, the data is converted from the linear Z scale to the logarithmic dBZ scale by using the formula dBZ=10 log10 (Z). The process may proceed to block 740.
At block 740, the process is queried as to whether each cell x of the MBR for the N radars has been determined. If the answer to the query is no, the process proceeds to block 745. If the answer to the query is yes, the process proceeds to block 750.
At block 745, the cell x may be set to cell x+1, and the process proceeds to block 640.
At block 750, the process ends.
Superposition of Vector Data
In the process 800 described in
At block 820, the Minimum Bounding Rectangle (MBR) coordinates ((λmin
At block 830, coordinates ((λmin,φmin), (λmax,φmax)) of the MBR for N radars may be determined using equation (8).
At block 840, the latitude and longitude interval between the coordinates ((λmin,φmin), (λmax,φmax)) may be divided into “D” rectangular display blocks of size k×p, i.e. there are “D” rectangular display blocks in the grid. Further, the grid resolution parameters (dimensions of latitude-longitude cell) δλ and δφ, may be set to any specified value.
At block 850, an index B of the current rectangular display block may be set to 0. At block 860, set B=1+B.
At block 870, the largest area within the display block B that is simultaneously observed by a given number of radars M may be determined. The wind vector for the display block B in
At block 880, the PPI scan-converted CAPPI scan line data from the ith radar for the cell located at (λ,φ) is obtained by first computing the east-west distance dEWi and north-south distance dNSi from the formulae dEWi=d((λi,φ),(λi,φi)) and dNSi=d ((λ,φi), (λi,φi)) respectively, of x from the ith radar location. The PPI scan converted Doppler wind velocity data obtained and stored at block 485 of
At block 900, the process 800 is queried as to whether the overlapping radars M may be equal to either 2 or 3. If the answer to the query is yes, the process proceeds to block 910. If the answer to the question is no, the process proceeds to block 920.
At block 910, the average wind velocity V may be obtained by solving the dot-product equation V·P(i)=A(i), where P(i) is the unit position vector from the origin of the radar i to the center of the block B, with i taking on the values corresponding to the radars covering the largest region within B. The process may proceed to block 950.
At block 920, the process is queried as to whether the overlapping radars M is less than 2. If the answer to the query is yes, the process proceeds to block 930. If the answer to the question is no, the process proceeds to block 940.
At block 930, there is not enough data to determine a 2-dimensional or 3-dimensional wind vector at block B. The vector data for this block B is not displayed.
At block 940, the average wind velocity V may be obtained by solving the dot-product equation V·P(i)=A(i) using the least squares method, where P(i) is the unit position vector from the origin of the radar i to the center of the block B, with i taking on the values corresponding to the radars covering the largest region within display block B. The process then proceeds to block 950.
At block 950, the wind vector is displayed as an arrow with its center located at the latitude and longitude coordinates corresponding to the center of the display block B. The process may proceed to block 960.
At block 960, the process is queried as to whether the wind vector for each block B has been determined. If the answer to the query is yes, the process proceeds to block 970. If the answer to the question is no, the process proceeds to block 860.
At block 970, the process ends.
The wind velocity may be extracted using radial velocities from two or more separately located radars scanning overlapping areas. The 3-dimensional velocity components of the wind may be obtained from the combination of three Doppler radars.
The position vector from the origin of the radar to the center of the block B may be calculated for the radars corresponding to the largest coverage region within display block B. The average of the values may be calculated independently for each radar covering that region. The dot product of the unit position vector and wind vector may give the radial component of velocity. However, because the vector is displayed over a display block, the radial component may be taken as the average of the values. These equations may be solved to obtain the actual vector in two or three dimensions depending on the number of overlapping radars. If the set of equations is written in matrix notation (equation (10)), then the least squares solution may be found by solving equation (11) where AT denotes the transpose of A.
AX=C (10)
ATAX=ATC (11)
In equations (10) and (11) X may represent a column vector for the wind velocity at display block B, A may be a matrix whose rows represent the unit position vectors of the radars observing display block B (i.e. the largest area within display block B), and C may be a column vector of the average values of the Doppler velocities for each radar over the display block B (i.e. the largest area within display block B).
Combined Scalar Data and Vector Data from Multiple Radars
Grids of multiple weather radars may generate data on scalar (reflectivity, spectrum width) as well as vector (wind velocity) parameters of the atmosphere. Because of the curvature of the earth's surface, the radar grid may not be co-planar. Scalar and vector data from multiple radars may be combined in a grid and displayed.
Computer System
Further, while a single machine is illustrated, the term “machine” shall also be taken to include any collection of machines that individually or jointly execute a set (or multiple sets) of instructions to perform any one or more of the methodologies discussed herein.
The example computer system 1001 includes the processor 103/1002 (e.g., a central processing unit (CPU), a graphics processing unit (GPU), or both), a main memory 1004 and a static memory 1006, which communicate with each other via a bus 1008. The computer system 1001 may further include a video display unit 1010 (e.g., a liquid crystal display (LCD) or a cathode ray tube (CRT)). The computer system 1001 also includes an input device 1012 (e.g., a keyboard), a cursor control device 1014 (e.g., a mouse), a disk drive unit 1016, a signal generation device 1018 (e.g., a speaker) and a network interface device 1020.
The disk drive unit 1016 includes a machine-readable medium 1022 on which is stored one or more sets of instructions (e.g., software 1024) embodying any one or more of the methodologies or functions described herein. The instructions 1024 may also reside, completely or at least partially, within the main memory 1004, the static memory 1006, and/or within the processor 1002 during execution thereof by the computer system 1001. The main memory 1004 and the processor 103/1002 also may constitute machine-readable media. In an additional embodiment, the mechanism (such as the look up table) is not stored, but rather a processor or additional processor is used to generate the weights substantially in real-time. This additional embodiment may be useful, e.g. where processing speed is more readily available as compared with memory.
The term “machine-readable medium” shall also be taken to include any medium that is capable of storing, encoding or carrying a set of instructions for execution by the machine and that cause the machine to perform any one or more of the methodologies of the present invention. The term “machine-readable medium” shall accordingly be taken to include, but not be limited to, solid-state memories, optical and magnetic media, and carrier wave signals.
The instructions 1024 may further be transmitted or received over a network 1026 via the network interface device 1020.
Embodiments may be utilized by running the program on a digital computer that receives the appropriate type of data (scalar and vector) from a number of overlapping radar fields to generate a CAPPI display on the monitor in quasi-real-time. Embodiments are also useful for generating CAPPI display from pre-recorded radar data available from public or private data archives. The display unit 1010 may be of any resolution and embodiments may be implemented without addition of any special hardware to a computer.
The mechanism(s) may also be implemented on a Digital Signal Processing (DSP) chip or any other computer board. The mechanism(s) is(are) implemented in a high level programming language for ease of coding, though they may also be implemented in other types of programming languages, e.g. in assembly or machine languages to achieve higher processing speed and reduced memory overheads. Due to the versatile nature of the mechanism, the technique may be embedded in hardware for CAPPI display of data from radar receiver during real-time operation.
Applications that may include the apparatus and systems of various embodiments broadly include a variety of electronic and computer systems. Some embodiments implement functions in two or more specific interconnected hardware modules or devices with related control and data signals communicated between and through the modules, or as portions of an application-specific integrated circuit. Thus, the example system is applicable to software, firmware, and hardware implementations.
Using the embodiments of methods and systems described herein, a horizontal slice is taken through the radar volume scan data at constant altitude above the earth surface using Constant Altitude Plan Position Indicator (CAPPI). Weather radar systems often deteriorate the spatial sampling of the scan volume by skipping certain elevation angles to reduce time used for scanning the region around the radar. This results in gaps in the CAPPI data, which have been filled in the embodiment using an interpolation scheme. Other CAPPI schemes may utilize a nearest neighbor approach, which may introduce artifacts into the display, including sharp jumps or boundaries between annular segments of the display. Embodiments determine the display parameter at the CAPPI surface by making a weighted interpolation of data from adjacent scan elevations to obtain a smoother and more accurate CAPPI display. The CAPPI scan line data constructed along each azimuth angle may be scan converted to computer display coordinates.
In systems described herein, the elevation from the ground of the CAPPI surface may be first specified, and CAPPI data for increments in EC between the vertical and the highest elevation angle of radar is taken from the radar volume scan data for the highest elevation angle. The CAPPI data for increments in EC between the lowest elevation angle and 0° (i.e. horizontal) is taken from the radar volume scan data for the lowest elevation angle. The length of the arc EC for each elevation angle is computed. These pre-computed arc lengths may be used for determining the adjacent elevation angles corresponding to each increment in EC; the scheme may avoid computation of adjacent elevation angles for each increment in EC. Further, interpolation may add little overhead due to calculation of weights and weighted average of weather data from adjacent elevation angles.
Coverage by multiple radars may help in improving the quality of scalar radar data such as reflectivity, which corresponds to rainfall intensity. Multiple Doppler radar coverage may also help in retrieving the wind vectors which may not be observed directly by single Doppler radars. The multi-radar data combining method or system may handle scalar data as well as vector data.
Any number of radar fields overlapping at a given point may be handled using the method(s) described herein. The number of overlapping radars at a given element may be determined dynamically using a distance measure bounded by a value depending on the altitude of the element from the surface of the Earth. For scalar data, the data from the overlapping radars may be averaged and displayed on a CAPPI (Constant Altitude Plan Position Indicator) projection. For vector data, the projections corresponding to the individual radar radial directions may be used to reconstruct a true vector at the radar resolution cell. The vector data may be averaged over a display box and may be represented by an arrow for each box. For two overlapping radars, the vector is calculated as a planar (2-D) vector. With 3 overlapping radars, an exact solution of the 3-D vector is obtained. If the overlapping radars are more than 3 then a 3-D vector is reconstructed on a least-squares basis. The software may automatically determine the number of overlapping radars and employ the appropriate reconstruction algorithm.
Individual radar data may be generated and archived in a radar-centric coordinate system. When combining data from multiple radars, the data may be converted to a universal coordinate system that may increase functionality and efficiency. In embodiments, a universal latitude-longitude grid for displaying the data generated at constant altitude may be used.
In embodiments described herein, a mechanism, such as a graph, a look-up table (LUT), a set of equations, and/or an algorithm may be used for calculating or storing the arc lengths EC for each radar beam elevation φ, and weights and ranges for each increment in EC for a given altitude H from ground. For ease of explanation, the mechanism is a look up table (LUT) in these embodiments. The LUT for ranges and weights (i.e. the second and third mechanisms) is implemented as one dimensional arrays indexed by the number of the increments in EC from the vertical, while the LUT for lengths of EC for each elevation angle is indexed by the elevation number. The LUT can be computed with minimal processing overhead and can be accessed quickly. The technique may be efficient because the memory used for storing the LUTs may be minimal and an efficient calculation of the lengths may add less processing overhead. This technique may not recompute the LUT unless the altitude or the elevation angles of the radar data change. Since the elevation angles of the radar data are less likely to change, multiple LUTs may be computed and stored for different altitudes. The use of LUTs enables high performance with minimal memory overhead and memory may be less expensive as compared to the increase of the processing speed of hardware. It also enables the CAPPI data computation to be carried on processors of lower capability such as those in airborne computers.
CAPPI may avoid issues associated with PPI by picking constant altitude data from different elevation scans. However, because CAPPI includes data from all elevation scans in the radar volume, processing in some embodiments may take considerably longer than PPI displays.
As described herein, the CAPPI data generation process described may be compatible with any PPI display algorithm or device that may handle any user-specified rotation, zooming, magnification, distance interval, and sector selection. This scheme may provide additional features for displaying CAPPI. The CAPPI data generated using these embodiments are indexed by the horizontal distance (along constant-height arc) from the vertical through the radar, and the azimuth angle, and may be converted to any other coordinate systems, e.g. latitude-longitude, Cartesian. Embodiments are suitable for generating CAPPI data for use with techniques superposing CAPPI data from overlapping radars, where the radar data should be converted from the individual radar coordinates to a universal grid system. CAPPI, generated using this interpolation scheme, suits viewing specifications and may be more accurate and continuous than data generated using another scheme, for example, a nearest neighbor scheme.
Embodiments described herein may be used with the presentation and display of weather radar data by users such as meteorologists, air traffic controllers, pilots, TV weather broadcasters, and disaster monitors. Embodiments can be licensed to companies working on general radars, weather radars, imaging radars, meteorological data products and PPI displays.
Overlapping radar sites may increase reliability and may fill the void of non-operational sites. Such an overlapping network may offer a superior quality of coverage and the observed information may be more precise. For example, a single radar may have a blind azimuth that an adjacent radar may cover. Multiple radars may provide continuity and redundancy in case of a failure. Where a single radar surveillance system may experience catastrophic failure, multiple radar systems may provide for graceful degradation of overall performance.
A large number of radar sites are distributed across the world, e.g. US Weather Surveillance Radar-1988 Doppler (WSR-88D), also known as Next Generation Radar (NEXRAD) network. These sites operate independently, but the ranges of these radar sites may overlap. The NEXRAD network may provide information associated with monitoring severe weather and issuing storm warnings, flash flood warnings.
Gridded data may allow various WSR-88D users to benefit from a wide-variety of products and displays (flexible horizontal or vertical cross sections) that may be easily extracted from multiple radar analysis grids. Further, data fusion, i.e. the process of combining radar data with information from other sources e.g. satellite, may be performed for gridded radar data. The gridded data may provide a more complete depiction of storm and precipitation events than using a single radar.
A mosaic of data combined with radar images may be constructed from overlapping radars into a single image to potentially render a more accurate display.
The following issues may be addressed using embodiments herein: Variability of the number of radar coverage volumes overlapping at a given location. These may range from 0 (no radar coverage) or 1 (coverage by a single radar) to coverage by several radars; variability of the size and orientation of the radar resolution volumes of multiple radars at a given location; the conical nature of the individual radar beam scanning surfaces for different elevation angles, and the non-overlap of these conical surfaces from adjacent radars; non-contiguous stacking of the scanning radar beams, i.e. presence of significant gaps between the scanning elevations of a radar, especially at the higher elevation angles; the curvature of the earth, which makes even the flat, zero-elevation scanning planes of adjacent radars to be non-overlapping, and uses additional formulation for transforming the coordinates from one radar to another, or to a common set of coordinates.
The following description includes terms, such as “up”, “down”, “upper”, “lower”, “first”, “second”, etc. that are used for descriptive purposes only and are not to be construed as limiting. The elements, materials, geometries, dimensions, and sequence of operations may all be varied to suit particular applications. Parts of some embodiments may be included in, or substituted for, those of other embodiments. While the foregoing examples of dimensions and ranges are considered typical, the various embodiments are not limited to such dimensions or ranges.
The Abstract is provided to comply with 37 C.F.R.§1.74(b) to allow the reader to quickly ascertain the nature and gist of the technical disclosure. The Abstract is submitted with the understanding that it will not be used to interpret or limit the scope or meaning of the claims.
The illustrations of embodiments described herein are intended to provide a general understanding of the structure of various embodiments, and they are not intended to serve as a complete description of all the elements and features of apparatus and systems that might make use of the structures described herein. Many other embodiments will be apparent to those of skill in the art upon reviewing the above description. Other embodiments may be utilized and derived therefrom, such that structural and logical substitutions and changes may be made without departing from the scope of this disclosure. The figures are merely representational and may not be drawn to scale. Certain proportions thereof may be exaggerated, while others may be minimized. Accordingly, the specification and drawings are to be regarded in an illustrative rather than a restrictive sense.
In the foregoing Detailed Description, various features are grouped together in a single embodiment for the purpose of streamlining the disclosure. This method of disclosure is not to be interpreted as reflecting an intention that the claimed embodiments have more features than are expressly recited in each claim. Thus the following claims are hereby incorporated into the Detailed Description, with each claim standing on its own as a separate embodiment. One skilled in the art will recognize that other configurations are available and other methods of manufacture may function as well without exceeding the scope of the disclosed subject matter.
While particular embodiments have been illustrated and described, they are merely examples and a person skilled in the art may make variations and modifications to the embodiments described herein without departing from the spirit and scope of the presently disclosed subject matter.
Number | Date | Country | Kind |
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Number | Date | Country | |
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20060202886 A1 | Sep 2006 | US |