EP2531822A2 - Procédé de mesure de la profondeur d'une nappe d'eau - Google Patents
Procédé de mesure de la profondeur d'une nappe d'eauInfo
- Publication number
- EP2531822A2 EP2531822A2 EP11701634A EP11701634A EP2531822A2 EP 2531822 A2 EP2531822 A2 EP 2531822A2 EP 11701634 A EP11701634 A EP 11701634A EP 11701634 A EP11701634 A EP 11701634A EP 2531822 A2 EP2531822 A2 EP 2531822A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- reflector
- water
- radiation
- reflection
- emitted
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/12—Supports; Mounting means
- H01Q1/22—Supports; Mounting means by structural association with other equipment or articles
- H01Q1/225—Supports; Mounting means by structural association with other equipment or articles used in level-measurement devices, e.g. for level gauge measurement
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
- G01F23/284—Electromagnetic waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/88—Radar or analogous systems specially adapted for specific applications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/27—Adaptation for use in or on movable bodies
- H01Q1/28—Adaptation for use in or on aircraft, missiles, satellites, or balloons
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/27—Adaptation for use in or on movable bodies
- H01Q1/34—Adaptation for use in or on ships, submarines, buoys or torpedoes
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/14—Reflecting surfaces; Equivalent structures
- H01Q15/18—Reflecting surfaces; Equivalent structures comprising plurality of mutually inclined plane surfaces, e.g. corner reflector
Definitions
- the invention relates to a method for measuring the water level of a body of water and to a corresponding measuring system.
- the measurement of water levels of artificial and natural waters, e.g. Rivers, lakes and freshwater reservoirs are of particular importance today for monitoring both flood risk areas and areas of increasing water scarcity.
- water levels of bodies of water at locally distributed level stations on the ground are read by human personnel or electronically measured by the level stations and transmitted to central evaluation centers.
- Such gauges contain moving mechanics or active electronics and are therefore prone to failure.
- gauge stations are easily damaged or destroyed and are therefore no longer available for the very important water level monitoring during flooding.
- SAR Synthetic Aperture Radar
- the water level measurement described in these documents requires specific aquatic plants that protrude from the water surface and reflect radar waves. Such plants are rare worldwide.
- the method provides only relative readings and no absolute water level. Thus, a level station is still needed.
- the object of the invention is therefore to enable the measurement of the water level of a body of water easily and reliably without the use of level stations. This object is achieved by the method according to claim 1 or the measuring system according to claim 14 or the use of a reflector according to claim 16 or the reflector according to claim 17.
- a reflector which comprises a number (ie, at least one) of reflection surfaces for reflecting electromagnetic radiation in a predetermined wavelength range and provided in or on the body of water whose water level is to be measured.
- water body is to be understood broadly and includes any type of artificial or natural waters, in particular rivers, lakes, wetlands, reservoirs, marine areas, water reservoirs and reservoirs.
- the reflector is arranged in or on the body of water (for example on the edge or on the bank of the body of water) that an angle reflector is formed by the water surface of the body of water and one or more reflection surfaces of the reflector. That is, the reflection surface or reflection surfaces and the water surface, which form the angle reflector, are all substantially perpendicular to one another.
- electromagnetic radiation in the predetermined wave range is emitted by a jet device located above the water body.
- This radiation is incident on the reflector in such a way that this radiation is reflected back to the angle reflector formed by the reflection surfaces and the water surface, based on a multiple reflection involving the water surface.
- back reflection also referred to as retroreflection, it is meant that the incident radiation is reflected back substantially in the same direction as it falls on the angular reflector. According to the invention thus the radiation incidence the jet device and the angle reflector aligned so that this retro-reflection occurs.
- the water level of the water body is determined.
- This reflection center whose location is proportional to the water level, is formed by the intersection or cut edge between the reflective surface (s) of the reflector and the water surface.
- the point of intersection or the cut edge can also be an imaginary point or an imaginary edge, which result as a section between extensions of the reflection surface or reflection surfaces of the reflector and the water surface.
- An imaginary point of intersection or an imaginary cutting edge occur in particular in embodiments in which the reflector is positioned on the edge or on the bank of the watercourse.
- the distance measurement takes place via a transit time measurement of the radiation emitted by the jet device and, after back reflection at the angle reflector, received again at the location of the jet device. Over this period can be determined by the speed of light in a simple way, the distance between the jet and angle reflector. Taking account of corresponding position data relating to the position of the blasting device and the reflector, the water level can then be determined, as will be explained by way of example in the detailed description with reference to FIG. 1.
- the electromagnetic radiation emitted by the beam device can have different wavelengths or lie in different wavelength ranges.
- Radio-frequency radio waves having a frequency in the range between 1 GHz and 30 GHz, in particular 10 GHz and larger, are preferably used as the radiation.
- the angle of incidence of the radiation emitted by the radiation device can be in different angular ranges, in particular the radiation is incident on the angle reflector at an angle between 20 ° and 50 ° with respect to the vertical.
- the size of Refiexionsfizzen the reflector is between 30 cm and 3 m, in particular between 30 cm and 2 m or 30 cm and 50 cm.
- the edge length of the respective reflection surfaces thus lies in this order of magnitude.
- the reflection surface or reflection surfaces of the reflector are preferably metallic, in particular of aluminum and / or stainless steel.
- the reflector is fastened in particular by means of a suitable anchoring in or on the water, for example driven into the ground or embedded in concrete.
- a suitable anchoring in or on the water for example driven into the ground or embedded in concrete.
- the distance measurement is performed by radar and in particular by microwave radar, i. by means of radiation in the gigahertz range.
- the radiation incident on the reflector is thus emitted by a radar sensor, for which purpose a SAR radar sensor, for example, well-known from the prior art, e.g. TerraSAR-X, which allows highly accurate measurements.
- the radar sensor also takes over the measurement or detection of the backreflected radiation. From this, the duration of the radiation can be determined, from which, in turn, the water level can be determined.
- the radiation directed onto the reflector or angle reflector is emitted by a radiation device which is located on a moving flying object, in particular on a satellite or an aircraft or a helicopter.
- a radiation device which is located on a moving flying object, in particular on a satellite or an aircraft or a helicopter. In this way, by flying over a large area, the water levels of larger watering point by point at various points on appropriately provided reflectors are detected.
- the reflector used in the method according to the invention can be configured differently.
- the reflector comprises at least one pair of two mutually perpendicular, i. a right angle with each other forming reflection surfaces, wherein the water surface is perpendicular to each reflection surface of the at least one pair.
- a triple-angle reflector is formed by the water surface and the reflector, in which the retroreflection takes place via a threefold reflection at the angle reflector, including the water surface.
- the reflector has only one reflection surface, which is arranged in the water or in the vicinity of the water body.
- a double-angle reflector is formed by the reflection surface and the water surface, in which the retroreflection is effected by a reflection at the reflection surface and the water surface.
- the reflector includes two pairs of reflecting surfaces, wherein the reflecting surfaces of a respective pair are perpendicular to each other and the pairs are aligned in different directions, so that a water level measurement can be made from two directions or angular ranges of incident radiation.
- the pairs of reflection surfaces may, for example, be rotated by 180 ° relative to each other so that a respective reflection surface of the one pair is substantially perpendicular to a reflection surface of the other pair and parallel to the other reflection surface of the other pair.
- further reflection surfaces are preferably formed by the backs of the respective reflection surfaces, so that the angle reflector four, by 90 ° to each other twisted pairs of reflective surfaces.
- each pair of reflective surfaces is aligned with an ascending or descending trajectory of a satellite orbiting around the earth, for example, on a polar or near-polar orbit of a satellite.
- the radiation incident on the angle reflector is generated by a jet device on the satellite, wherein this beam device preferably comprises a radar sensor.
- a reflector is used, which comprises a damping device for damping water waves of the water body in the vicinity of the reflector. In this way, a suitable level measurement can be performed with sufficient accuracy even in heavy waves.
- the damping device comprises one or more screens transparent to electromagnetic radiation in the predetermined wave range, for example one or more Plexiglas panes.
- the water surface can be well shielded in the area of the reflector against wave motion.
- a respective screen extends between the reflecting surfaces of a pair of reflecting surfaces, especially between those edges of reflecting surfaces which are remote from the right angle formed between the reflecting surfaces of the pair.
- the damping device may also be formed in such a way that a cavity with at least one compensation opening or at least one compensation valve is provided in the region of the reflection surfaces, wherein the at least one compensation opening or the at least one compensation valve serves for the passage of air and / or water.
- the cavity can thus either an air cavity above the water surface or filled with water of the water Cavity below the water surface.
- pneumatic or hydraulic damping of shaft movements is achieved by a corresponding opening or a valve.
- the at least one compensation opening or the at least one compensation valve is provided in at least one cover closing the cavity, which is preferably transparent to the electromagnetic radiation of the jet device.
- the cover is arranged in the flow through the opening or the valve with water of the water below the water surface and in flowing through the opening or the valve with air above the water surface.
- a damping device is preferably combined with the above-described embodiment of a transparent screen.
- the cavity is formed by the at least one cover, one or more reflection surfaces of the reflector and at least one transparent screen.
- a three-dimensional position of the jet device and a two-dimensional position describing the position of the reflector in plan view of the earth surface are considered in a preferred variant, which are previously known or determined within the scope of the method .
- the three-dimensional and the two-dimensional position are determined in particular with respect to the same reference coordinate system.
- the two-dimensional position of the reflector can be determined via GPS or already present as GPS coordinates.
- a reference angle reflector for determining the water level of the water body, a reference angle reflector, the reflection surfaces of which do not comprise the water surface of the water, provided with a predetermined reference position in or on the body of water Duration of the emitted by the jet and At the reference angle reflector reflected radiation, the distance between the reference beam and the center of reflection of the angle reflector is measured. Since the actual distance is known on the basis of the previously known reference position of the reference angle reflector, an error compensation of the distance measurement with respect to the other reflector located in or on the water can thus take place with suitable methods.
- the invention further comprises a measuring system for measuring the water level of a body of water.
- This measuring system comprises a reflector comprising a number (ie, at least one) of reflection surfaces for reflecting electromagnetic radiation in a predetermined wave range and disposed in or on the body of water through the water surface of the body of water and one or more Reflection surfaces of the reflector, an angle reflector is formed.
- the measuring system further includes a radiation device located above the water body for emitting electromagnetic radiation in the predetermined wavelength range, so that the emitted radiation falls onto the reflector in such a way that the incident radiation is reflected back at the angle reflector based on a multiple reflection including the water surface ,
- the measuring system also includes a measuring device for measuring the distance between the beam device and the reflection center of the angle reflector over the duration of the emitted and reflected back radiation.
- an evaluation device for determining the water level of the water body is provided based on the measured distance.
- the reflector can be designed as a reflector with at least one pair of reflection surfaces.
- the reflector may comprise the damping device described above.
- a radar sensor can also be used for the measurement, in which case the jet device and the measuring device are integrated in this radar sensor.
- the evaluation device can be arranged at any location.
- a central evaluation device can be provided on which the measured data recorded by the measuring device are transmitted and evaluated there for determining the water level.
- the invention further relates to the use of a reflector comprising one or more reflecting surfaces for the reflection of electromagnetic radiation in a predetermined wave range in the method according to the invention described above or the measuring system according to the invention described above.
- the reflector may comprise any of the features described with respect to embodiments of the method according to the invention and the reflector.
- the reflector can be designed as a reflector with at least one pair of reflection surfaces and optionally comprise a damping device.
- the invention furthermore relates to a reflector which is particularly suitable for use in the method according to the invention or the measuring system according to the invention.
- This reflector which comprises one or more reflection surfaces for the reflection of electromagnetic radiation in a predetermined wave range, is characterized in that it further comprises a damping device for damping water waves of the water in the vicinity of the reflector and / or two pairs of reflection surfaces, wherein the reflection surfaces of a respective pair are perpendicular to each other and the pairs are aligned in different directions.
- a water level measurement can be carried out with stronger waves or from multiple beam directions of incident electromagnetic radiation.
- This reflector may also contain all other features described above relating to refinements of the reflector.
- FIG. 1 shows a schematic representation of an embodiment of a measuring system according to the invention for measuring the water level of a body of water
- FIG. 2 shows a first embodiment of a reflector used in the method according to the invention
- FIG. 3 shows a second embodiment of a reflector used in the method according to the invention
- FIG. 4 shows a third embodiment of a reflector used in the method according to the invention.
- FIG. 5 shows a fourth embodiment of a reflector used in the method according to the invention.
- FIG. 6 shows a fifth embodiment of a reflector used in the method according to the invention
- Fig. 7 shows a sixth embodiment of a reflector used in the method according to the invention.
- Fig. 1 shows a measuring arrangement for carrying out an embodiment of the method according to the invention.
- the water level of a body of water is determined whose water surface is indicated in Fig. 1 by a horizontal line W.
- the water level is measured with respect to a reference coordinate system whose coordinate origin is denoted by O and which encompasses the horizontal coordinate axes x, y and the vertical coordinate axis h.
- the representation of FIG. 1 shows in simplified form a planar Erdober lakegeometrie.
- the following calculation will be described based on this simplified geometry. However, the calculation can also be applied analogously to a curved earth oid surface are applied. In this case, the calculation is a little more complicated, but the same and exactly possible.
- the transfer of the calculation of a planar Erdober perennialgeometrie on curved geometries is within the scope of common expertise.
- FIG. 1 shows a schematic representation of a radar sensor 3 located on the satellite (in particular a SAR radar), which emits the radar radiation towards the water surface W.
- the reflector 1 is fixed in the water such that the two reflection surfaces 1a and 1b are perpendicular to the water surface W.
- the attachment of the reflector can be achieved by a suitable anchoring on the bottom of the water, for example, by Einbetonnieren or ramming.
- the reflector is further aligned with respect to the previously known and indicated by the arrow P satellite orbit such that the radar radiation of the radar 3 so falls on the reflector that a retroreflection of the radiation by a multiple reflection at the two reflection surfaces la and lb and the water surface W he follows.
- the reflector 1 thus forms, together with the water surface W, a triple-angle reflector for reflecting the radar radiation.
- the distance between the satellite 2 and the reflector 1, denoted by R, is measured over a transit time measurement of the radiation emitted by the radar sensor and reflected back on the reflector 1. This distance depends on the height H w of the water level, since in the retroreflection the water surface is included as a reflection surface and thus the measured distance R is greater, the lower the water level. In other words, via the retroreflection, the distance R between the water surface W and the reflector 1 formed corner and the radar sensor measured, the position of this corner depends on the height of the water level.
- the position of the satellite 2 above the earth's surface in the reference coordinate system is also known.
- the satellite 2 is just above the x-axis of the coordinate system at the position x s .
- the fixed installation position of the reflector 1 with respect to the earth's surface is known, and in the scenario of FIG. 1 this position also lies along the x-axis of the reference coordinate system and is given by the coordinate XR for reasons of simplicity.
- the satellite's altitude H Sat is known with respect to the reference plane spanned by the x-axis and y-axis of the reference coordinate system.
- the water level H w with respect to the position of the x-axis of the reference coordinate system can be determined in a simple manner as follows:
- the current position of the satellite is needed, which can be determined from the previously known satellite orbit.
- the (two-dimensional) position of the reflector is also previously known and given for example in GPS coordinates.
- the measurement accuracy of the water level measurement depends on the error of the satellite orbit determination and the term-based determination of the distance R and the angle of incidence of the radar radiation on the reflector 1, wherein this angle of incidence is designated in Fig. 1 with ⁇ .
- Absolute errors can now be achieved with modern satellite systems up to approx. 6 cm with an angle of incidence of the radar radiation of 45 °.
- the accuracy of the water level measurement can be further improved in a variant of the method according to the invention by a second, in three axes exactly measured conventional angle reflector (not shown) in the vicinity of the water whose water level is to be measured, for example, on the bank, positioned is. From this angle reflector, which now comprises three mutually perpendicular reflection surfaces, its three-dimensional position is precisely known. This reflector also reflects the radar radiation back to the radar sensor 3. Thus, based on the radiation reflected by this second angle reflector, the distance between this reflector and the sensor 3 can also be measured over a propagation time measurement and used as a comparison value. As a result, the error in the measurement of the distance R can be largely compensated and even accuracies in the determination of the water level in the sub-centimeter range can be achieved.
- the measuring method described with reference to FIG. 1 is used for determining the water level of any waters, such as large-area moist tissues or remote water surfaces. Likewise, the levels of reservoirs and rivers can be monitored. In general, arbitrary, both artificial and natural waters, possibly also artificially created pools, can be measured with the method described with reference to FIG.
- the description of the embodiment of the method according to the invention with reference to FIG. 1 is merely exemplary and suitable modifications for determining the water level of a body of water are conceivable.
- the radar sensor used for the distance measurement can also be replaced by a sensor which emits the transit time based on electromagnetic radiation in a different wavelength range than radar radiation.
- the senor does not have to be provided on a satellite, but it can also be arranged on an aircraft which overflies the water to be measured. In this case, when performing the measurement, the position of the aircraft must be known, and this position can be determined, for example, via GPS. Likewise, there is possibly the possibility that a stationary measurement of the water body is carried out by the sensor is arranged at a fixed, pre-determined position above the water surface.
- a reflector 1 which comprises two reflection surfaces 1a and 1b, wherein a triple-angle reflector is formed by reflection of the water surface as Refiexionsfiambae by the reflector when placed in the water.
- the reflector forms a single reflective wall, which is arranged in the water or on the bank of the water, that a double-angle reflector is formed by the reflective wall and the water surface, the suitable incident radiation through a reflection on the wall and the water surface in the same direction as the incident radiation strictlyfiekt.
- FIG. 2 shows a first embodiment of a reflector 1, which corresponds to the reflector in the measuring arrangement of FIG. 1.
- the reflector is shown in Fig. 2 and also in the other Fig. 3 to 7 in the intended position for the measurement in the water, the water surface W is indicated in perspective as a dotted area.
- the subsurface part of the reflector is shown by dashed lines. 2 shows in particular the right-angled arrangement of the two reflection surfaces 1a and 1b and the water surface W, which is represented by the three 90 ° angles illustrated.
- an angle reflector is formed by the water surface W and the two sections of the reflection surfaces 1a and 1b projecting from the water surface.
- the reflector 1 has no moving parts and reflects in interaction with the water surface in a relatively wide angular range, so that it can be observed from different positions in space or from the air.
- the reflector can optionally also be constructed on both sides, such a double-sided structure being shown in the embodiment according to FIG.
- the angle reflector 101 reproduced there comprises 2 the two reflection surfaces 1c and 1d, of which only the rear side thereof is visible in FIG. 3, are represented by the rectangular reflection surfaces 1a and 1b, which correspond to the reflection surfaces of the reflector of FIG.
- the reflection surface 1c is an extension of the reflection surface 1b and is perpendicular to the reflection surface 1a.
- the reflection surface ld is an extension of the reflection surface la and is perpendicular to the reflection surface lb.
- this reflector is again arranged in the water such that all reflection surfaces 1a to 1d are perpendicular to the water surface W.
- the reflector 101 thus achieves retroreflection from two angular ranges, namely from an angular range which is directed to the reflection surfaces 1a and 1b, and from an angular range which is directed to the reflection surfaces 1c and 1d. Since radiation from two sides can be detected with the reflector of FIG. 2, this embodiment is particularly suitable for evaluating radar signals from ascending and descending orbits of polar exploration satellites.
- the rear sides of the respective reflection surfaces 1a to 1d are also designed to be reflective and thus form further reflection surfaces.
- a reflector with four pairs of reflection surfaces is provided, which reflects back incident radiation from essentially all directions.
- FIG. 4 shows a further embodiment of a reflector according to the invention, which is designated by reference numeral 201.
- This reflector allows in the region of Refiexionsfizzen la and lb an attenuation of horizontal wave movements, which complicate the measurement of the back-reflected radiation.
- the attenuation is achieved by a dielectric water wave screen 4 which is transparent to the incident radiation and which is arranged in the illustrated reflector between the edges K of the reflection surfaces 1a and 1b.
- the part of the water wave screen 4 lying below the water surface is indicated by dashed lines.
- the wave shield or the wave shield can, in a preferred variant, be formed by a Plexiglas disk.
- FIG. 5 shows a modified embodiment of the reflector according to FIG.
- This wave reflector is designated by reference numeral 301 and substantially corresponds in structure to the reflector of FIG. 4.
- the embodiment of FIG. 5 also achieves a damping of water pressure waves. which penetrate from below over the opening formed by the reflection surfaces la and lb and the screen 4. These pressure waves can be reflected on the water surface in the region of the reflection surfaces 1a and 1b and thus falsify the measurement result.
- the attenuation of the pressure waves penetrating from below is achieved in accordance with FIG. 5 via a cover 5 provided on the upper side of the reflector with a corresponding opening 6 realized through an opening pipe, whereby an air cavity is formed which only allows a slow flow of air over the opening 6 allows.
- a penetrating into the cavity pressure wave is compensated. It thus forms in the reflector an undisturbed mean water level, which is insensitive to short-term fluctuations in the water level.
- Fig. 6 shows a modification of the embodiment of Fig. 5.
- this, designated by reference numeral 401 reflector allows damping of water wave movements in the cavity formed by the reflection surfaces la and lb and the screen 4.
- a cover 7 arranged below the water surface is used for this purpose with an opening 8 realized via an opening pipe. Due to the low flow rate of the water through the opening 8, this reflector is also insensitive to pressure waves penetrating from below, so that again a mean constant water level is formed in the space formed by the reflection surfaces 1a and 1b and the screen 4.
- FIG. 7 shows by way of example an embodiment of a reflector 501 which, analogous to the reflector of FIG. 3, comprises four mutually perpendicular reflection surfaces 1a to 1d. It should be- see the leading edges of the reflection surfaces la and lb analogous to the embodiment of Fig. 4, a transparent screen 4 is arranged. Furthermore, in analogy to the embodiment of FIG. 5, a cover 5 provided with opening 6 is provided on the upper side of the reflector and, analogous to the embodiment of FIG. 6, a cover 7 with opening 8 located below the water surface. With the embodiment of FIG. 7, an especially good damping against shaft movements is achieved for the angle reflector formed by the reflection surfaces 1a and 1b.
- the rear angle reflector formed by the reflection surfaces 1c and 1d may be analogous to the front angle reflector, ie it may also comprise a screen 4 and corresponding covers 5 and 7 with openings 6 and 8, respectively.
- the measuring method according to the invention described above has a number of advantages.
- the water levels of hard to reach waters can be measured without having to provide level stations with human or electronic reading on site. It is only once to install a corresponding reflector with known position in or on the water, and then can be determined by the retroreflection of radiation at the reflector, the water level.
- Radar sensors already in use in particular satellite-supported radar sensors, can be used to determine the water level, which can achieve very high distance accuracies of up to a few centimeters with corresponding calibrations. The accuracy can be further increased by the use of a reference angle reflector with accurate measurement and position.
- the radar beams which are reflected back from the reflector located in or on the water, appear as a bright pixel in the radar image. From the position of this pixel results in the oblique distance between the radar sensor and the Winkeleck between the reflecting surfaces of the reflector and the water surface. The (previously known) horizontal position of the reflector can then be derived from the oblique distance of the water level with high accuracy.
Landscapes
- Physics & Mathematics (AREA)
- Remote Sensing (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Radar, Positioning & Navigation (AREA)
- General Physics & Mathematics (AREA)
- Astronomy & Astrophysics (AREA)
- Aviation & Aerospace Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- Radar Systems Or Details Thereof (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
Abstract
L'invention concerne un procédé de mesure de la profondeur d'une nappe d'eau. Pour ce faire, on utilise un réflecteur (1, 101, 201, 301, 401, 501) qui comprend un certain nombre de surfaces réfléchissantes (1a, 1b) pour renvoyer un rayonnement électromagnétique situé dans une plage de longueurs d'ondes prédéterminée, et qui est disposé dans ou sur la nappe d'eau, de façon que la surface (W) de la nappe d'eau et au moins une surface réfléchissante (1a, 1b) du réflecteur (1, 101, 201, 301, 401, 501) forment un réflecteur à coin. Dans le cadre de ce procédé, un rayonnement électromagnétique qui est situé dans la plage de longueurs d'ondes prédéterminée et qui est émis par un dispositif de rayonnement (3) disposé au-dessus de la nappe d'eau, vient frapper le réflecteur (1, 101, 201, 301, 401, 501), de telle façon que le rayonnement incident est réfléchi par le réflecteur à coin sur la base d'une réflexion multiple tenant compte de la surface (W) de l'eau. La distance entre le dispositif de rayonnement (3) et le centre de réflexion du réflecteur à coin est mesurée pendant le temps de propagation du rayonnement incident et réfléchi puis, à partir de là, la profondeur (W) de la nappe d'eau est déterminée.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE201010001440 DE102010001440B4 (de) | 2010-02-01 | 2010-02-01 | Verfahren und Mess-System zur Messung des Wasserstands eines Gewässers |
| PCT/EP2011/050372 WO2011092056A2 (fr) | 2010-02-01 | 2011-01-13 | Procédé de mesure de la profondeur d'une nappe d'eau |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| EP2531822A2 true EP2531822A2 (fr) | 2012-12-12 |
Family
ID=44201209
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP11701634A Withdrawn EP2531822A2 (fr) | 2010-02-01 | 2011-01-13 | Procédé de mesure de la profondeur d'une nappe d'eau |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP2531822A2 (fr) |
| CA (1) | CA2787896C (fr) |
| DE (1) | DE102010001440B4 (fr) |
| WO (1) | WO2011092056A2 (fr) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| IT1401469B1 (it) * | 2010-06-28 | 2013-07-26 | Tele Rilevamento Europa T R E S R L | Apparato per la misura del movimento del suolo con immagini sar mediante almeno un riflettore di onde elettromagnetiche |
| CN105136073B (zh) * | 2015-08-14 | 2017-09-12 | 昆明理工大学 | 一种在边坡形变监测中的气象校正模型 |
| CN105182339A (zh) * | 2015-09-25 | 2015-12-23 | 昆明理工大学 | 一种基于角反射器的边坡形变监测环境影响校正方法 |
| EP3748313B1 (fr) | 2019-06-05 | 2024-11-06 | Rosemount Tank Radar AB | Évaluation de niveau de radar à l'aide d'un réflecteur en coin formé par la surface du produit et la paroi du réservoir |
| CN111983609B (zh) * | 2020-07-30 | 2022-02-08 | 中国科学院空天信息创新研究院 | 基于雷达遥感影像的湿芦苇提取方法 |
| CN113567981B (zh) * | 2021-06-28 | 2023-08-08 | 中国电建集团华东勘测设计研究院有限公司 | 一种基于sar影像的洪涝风险区自动提取方法 |
| DE102024118419B4 (de) | 2024-06-28 | 2026-01-08 | Deutsches Zentrum für Luft- und Raumfahrt e.V. | SAR-Satelliten-Konfiguration zur Bestimmung der Geo-Koordinaten von Radar-Punktzielen auf der Erdoberfläche und Verfahren unter Verwendung einer derartigen Satelliten-Konfiguration |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE889617C (de) * | 1950-05-13 | 1953-09-10 | Gasaccumulator Svenska Ab | Fuer Radarzwecke bestimmte Reflektoranlage |
| JP2001177335A (ja) * | 1999-12-20 | 2001-06-29 | Tootekkusu Kk | 電波反射用コーナーレフレクター |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3258737A (en) * | 1966-06-28 | Ciavaglia silent underwater beacon | ||
| US2823365A (en) * | 1945-07-18 | 1958-02-11 | Rines Robert Harvey | Electro-acoustic system and method |
| AU497632B2 (en) * | 1974-01-03 | 1978-12-21 | Commonwealth Of Australia, The | Ground plane corner reflectors |
| US4184155A (en) * | 1978-09-22 | 1980-01-15 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Radar target for remotely sensing hydrological phenomena |
| US4914734A (en) * | 1989-07-21 | 1990-04-03 | The United States Of America As Represented By The Secretary Of The Air Force | Intensity area correlation addition to terrain radiometric area correlation |
| CA2636235C (fr) * | 2006-01-03 | 2014-11-25 | Altamira Information, S.L. | Dispositif actif permettant de recevoir et d'emettre des ondes electromagnetiques |
| EP2283380B1 (fr) * | 2008-05-29 | 2014-08-06 | Telespazio S.p.A. | Détection de cible dans une zone marine dont une image est réalisée par un radar à synthèse d'ouverture |
| DE102008029771A1 (de) * | 2008-06-25 | 2009-12-31 | Endress + Hauser Gmbh + Co. Kg | Anordnung zur Füllstandsmessung |
-
2010
- 2010-02-01 DE DE201010001440 patent/DE102010001440B4/de not_active Expired - Fee Related
-
2011
- 2011-01-13 WO PCT/EP2011/050372 patent/WO2011092056A2/fr not_active Ceased
- 2011-01-13 EP EP11701634A patent/EP2531822A2/fr not_active Withdrawn
- 2011-01-13 CA CA2787896A patent/CA2787896C/fr not_active Expired - Fee Related
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE889617C (de) * | 1950-05-13 | 1953-09-10 | Gasaccumulator Svenska Ab | Fuer Radarzwecke bestimmte Reflektoranlage |
| JP2001177335A (ja) * | 1999-12-20 | 2001-06-29 | Tootekkusu Kk | 電波反射用コーナーレフレクター |
Non-Patent Citations (1)
| Title |
|---|
| See also references of WO2011092056A2 * |
Also Published As
| Publication number | Publication date |
|---|---|
| WO2011092056A3 (fr) | 2011-10-13 |
| CA2787896C (fr) | 2015-07-21 |
| DE102010001440B4 (de) | 2014-01-16 |
| WO2011092056A2 (fr) | 2011-08-04 |
| DE102010001440A1 (de) | 2011-08-04 |
| CA2787896A1 (fr) | 2011-08-04 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| DE102010001440B4 (de) | Verfahren und Mess-System zur Messung des Wasserstands eines Gewässers | |
| EP3803454B1 (fr) | Procédé radar à ouverture synthetique et dispositif radar à ouverture synthetique | |
| EP2130062B1 (fr) | Procédé d'exploration d'une zone glaciaire ou d'une zone sèche par échosondage par radar | |
| DE102013220259A1 (de) | Radarsensor mit Radom | |
| DE102016208508B4 (de) | Winkelreflektorvorrichtung mit einstellbarer Höhenmehrdeutigkeit für SAR-Anwendungen | |
| EP2875384A1 (fr) | Procédé de traitement de données brutes d'un radar rso en mode de saisie hyperfine obtenues en haute résolution et à protection spatiale | |
| EP1318414A2 (fr) | Méthode tomographique pour radar à aperture synthétique (SAR) basée sur aéronef ou satellite | |
| DE4344509B4 (de) | Verfahren zur Messung der akustischen Rückstreueigenschaft von Gewässerböden | |
| Vogelzang et al. | Mapping submarine sand waves with multiband imaging radar: 2. Experimental results and model comparison | |
| DE4037156A1 (de) | Radarantennenanordnung | |
| DE69630816T2 (de) | Doppler-radarhöhenmesser mit kompensierter verzögerung | |
| EP1515159B1 (fr) | Méthode pour réduire le centroide doppler pour des systèmes radar coherent à impulsion | |
| EP2290397B1 (fr) | Procédé de mesure destiné à l'analyse non destructive d'une couche de neige et dispositif de mesure destiné à l'exécution du procédé de mesure | |
| DE69838162T2 (de) | Verfahren zur Störungsabschwächung der Reflektionsstrahlungskeulen einer Radarantenne | |
| DE202019105270U1 (de) | System zur Herleitung von Seestatusparametern | |
| DE2619727A1 (de) | Fluidum-stroemungsmesser | |
| DE102018105431A1 (de) | Radarsystem und Verfahren zur Messung horizontal aufgelöster Windfelder in der Mesosphäre und/oder unteren Thermosphäre | |
| DE102023113349B4 (de) | Verfahren zum Bestimmen einer vertikalen Struktur eines halbtransparenten Mediums aus SAR-Daten eines SAR-Systems | |
| DE102005023787A1 (de) | Verfahren und Vorrichtung zum Korrigieren von Wetterdaten sowie Computerprogrammprodukt | |
| DE4005676A1 (de) | Absorber fuer elektromagnetische wellen | |
| DE102016224962B3 (de) | Synthetik-Apertur-Radarverfahren und Synthetik-Apertur-Radarsystem | |
| DE102021131933B4 (de) | Referenzstation zur Nutzung in der großflächigen Bestimmung der Bewegung der Erdoberfläche in SAR-Anwendungen | |
| EP1910785A2 (fr) | Dispositif de mesure d'un niveau | |
| DE102022133858B4 (de) | Verfahren zur rechnergestützten Verarbeitung von SAR-Rohdaten | |
| AT526218B1 (de) | Kompensationsverfahren zur Erlangung phasenkohärente Standbilder bei einem bistatischem Radar |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
| 17P | Request for examination filed |
Effective date: 20120831 |
|
| AK | Designated contracting states |
Kind code of ref document: A2 Designated state(s): AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR |
|
| DAX | Request for extension of the european patent (deleted) | ||
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: EXAMINATION IS IN PROGRESS |
|
| 17Q | First examination report despatched |
Effective date: 20170512 |
|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION HAS BEEN WITHDRAWN |
|
| 18W | Application withdrawn |
Effective date: 20181218 |