METHOD FOR MEASURING THE BURIAL DEPTH OF A LINE AND DEVICE

Abstract

The invention relates to a method and device for measuring the burial depth of lines that are being laid increasingly under a soil surface on land and in water. In order to increase a measurement precision, more than one excitation or transmission coil is used, which extends in an xy plane, the transmission coils are positioned next to one another in a span extending essentially perpendicular to a center axis of the line and are moved over the line along this center axis; the transmission coils transmit electromagnetic pulses in a time-lagged fashion as a primary signal, and receiver coils are used, which are distributed across the array of transmission coils in the xy plane and measure in at least two axes extending orthogonally to one another; and all of the receiver coils measure secondary signals in reaction to the transmission of a primary pulse by the transmission coils.

Claims

1. A method for measuring a burial depth of a line buried underground, comprising: transmitting an electromagnetic pulse as a primary signal with a detector cell and receiving a secondary signal based on it; calculating a distance of the detector cell from the line, and measuring at the same time a height of the detector cell above the soil surface; calculating the difference between the distance and the height to determine the thickness of the covering; and wherein more than one excitation or transmission coil extending in an xy-plane of a Cartesian coordinate system is used, the transmission coils are positioned next to one another in a span extending perpendicular to a center axis of the line 24 and are moved over the line along this center axis being parallel to the y-axis of said Cartesian coordinate system; the transmission coils transmit time-lagged electromagnetic pulses as a respective primary signal, and receiver coils are used, which are arranged in an equally distributed fashion in the xy-plane across the array of transmission coils, where two respective receiver coils are combined with two axes or center axes extending in x-axis and z-axis of the Cartesian coordinate system respectively and all of the receiver coils measure secondary signals in reaction to the transmission of a respective primary pulse by the transmission coils.

2. The method according to claim 1, wherein the receiver coils measure the secondary signals over a certain time span only after a fixed time lag relative to a transmission of an electromagnetic pulse by the transmission coils.

3. The method according to claim 2, wherein a time lag in a range of 400 up to 550 s and preferably of approximately 498 s is used.

4. The method according to claim 1, wherein the measurement of the secondary signals is carried out for a time span of up to about 10 ms.

5. The method according to claim 1, wherein the receiver coils situated in a uniformly distributed fashion are used, which are all situated within the array composed of the transmission coils or a plane parallel to said array.

6. A device for measuring a thickness of a covering of a line, comprising: a detector cell, which is embodied to transmit an electromagnetic pulse as a primary signal and to receive a secondary signal; evaluation means for determining a distance of the detector cell from the line; means for determining a height of the detector cell above the soil surface; and means for determining a thickness of the covering by calculating the difference of the distance of the detector cell from the line and the height of the detector cell above the soil surface; and wherein more than one excitation or transmission coil extending in an xy plane of a Cartesian coordinate system is provided as means for transmitting the primary signal, the transmission coils are arranged next to one another in a span extending perpendicular to a center axis of the line and are movable along this center axis over the line being parallel to the y-axis of said Cartesian coordinate system; the transmission coils are embodied for transmitting electromagnetic pulses in a time-lagged fashion as a primary signal, and receiver coils are used, which are arranged in an equally distributed fashion in the xy plane across the array of transmission coils and where two respective receiver coils are combined with two axes or center axes extending in x-axis and z-axis of the Cartesian coordinate system respectively; and all of the receiver coils are embodied to measure respective secondary signals in reaction to the transmission of a respective primary pulse by the transmission coils.

7. The device according to claim 6, wherein a pair of receiver coils of said different axes are combined as a receiver unit, where receiver units are embodied inside the array composed of the transmission coils or a plane parallel to said array.

8. The device according to claim 6, wherein the transmission coils and receiver units are affixed to a wing-shaped support composed of an electrically nonconductive material.

9. The device according to claim 6, wherein each transmission coil is embodied as a rectangle with the edge lengths of approximately 1.5 m*approximately 1.41 m with a winding at a nominal current of approximately 170 A.

10. The device according to claim 6, wherein two receiver coils are combined as a pair extending orthogonally to one another to form a cube-like receiver unit.

11. The device according to claim 6 wherein the transmission coil are arranged in line forming a bar.

Description

[0017] Other features and advantages of embodiments according to the invention will be described in greater detail below in conjunction with exemplary embodiments based on the drawings. In the drawings:

[0018] FIG. 1: is a schematic top view of a device that is moved at a speed v centrally over a line extending under a sea bed surface in order to measure a thickness of a covering;

[0019] FIGS. 2a and 2b: show schematic depictions of a section extending in a plane II-II from FIG. 1 during the impact of electromagnetic pulses and during the emission of a secondary signal.

[0020] Throughout the different figures of the drawings, the same reference numerals are consistently used for the same elements. Further, a Cartesian coordinate system is used throughout all figures modelling an ideal situation of application, where the center axis of a line as well as a direction of motion of a device according to the present invention are parallel to the y-axis of said Cartesian coordinate system.

[0021] Because of the growing importance of so-called offshore wind farms for the production of renewable energy, it is very important to protect, monitor, and/or inspect a line network that is to be constructed and maintained for these wind farms. Without restricting a use field of the present invention, only on an inspection of such lines will be discussed below. Basically, related and alternative use fields in the realm of archeology, prospecting for natural resources, or locating pipelines and the like are not precluded from a use of the method and devices according to the invention.

[0022] The illustration in FIG. 1 shows a top view of a device 1, which is moved as a detector cell at a speed v centrally over a line 2 extending under a sea bed surface BO in order to measure a thickness of a covering. The device 1 in this case includes three excitation or transmission coils 3, 3, 3 extending in the xy plane, which are positioned next to one another in a span essentially perpendicular to a center axis M of the line 2. Being perpendicular to a center axis M of the line 2 is the best case in theory, but hard to be carried out exactly in reality. However, the method described has shown robust results even in case of deviations regarding said positioning. This is why the term essentially is used in this connection.

[0023] As shown in more detail in FIGS. 2a and 2b, the transmission coils 3, 3, 3 transmit electromagnetic pulses B, B, B that are time-lagged relative to one another as a primary signal.

[0024] These pulses B, B, B also penetrate the sea bed surface BO of the indicated sea bed and excite the flow of induced currents in the electrically conductive material of the line extending 2. These currents decay and in turn generate secondary electromagnetic signals B.sub.r.

[0025] Distributed in the xy plane across the array of transmission coils 3, 3, 3 is an arrangement of receiver coils 4 for receiving the secondary electromagnetic signals B.sub.r. In a manner not shown in the drawing, two respective receiver coils 4 are combined with two axes or center axes extending in x and z of the Cartesian coordinate system respectively. Thus, two receiver coils 4 are combined as a pair extending orthogonally to one another to form a cube-like receiver unit 5. As a matter of the fact that the line 2 under a sea bed surface BO as the target is lying parallel to the y-axis of said Cartesian coordinate system changes in this direction may be neglected in this embodiment of the invention.

[0026] In this embodiment, there are five cube-like receiver units 5 used distributed in a more or less equidistant manner within each of the transmission coils 3, 3, 3 and beyond. Receiver units 5 shown in dashed lines are cube-like receiver units in a somewhat staggered configuration, which still is regarded as a xy-plane configuration within the scope of the present invention reduce to deviations in real life showing very little effect to the method described in here. Thus, all cube-like receiver units 5 are regarded to be equal even in case of a deviation of their respective position. Said receiver units 5 are made to measure only the secondary signals B.sub.r in the receiver coils 4 of the receiver units 5 for evaluation after a specified time lag t from the transmission of primary pulses by the transmission coils 3, 3, 3. This may be achieved by switching means not further disclosed here. Approximately 498 s is used as the time lag t.

[0027] The illustration in FIG. 2a shows the measurement principle as a depiction of a section in a plane II-II from FIG. 1. According to it, the detector cell 1 is moved at a basically arbitrary depth under the surface of a body of water WO at a distance d above the surface of the sea bed BO of the indicated sea bed at the speed v; in this case, exactly in the direction of the y-axis and over the line 2. The distance d can be exactly determined by means of a sonar measurement or similar known devices that are also provided on the detector cell 1 without further disclosure. The transmission coils 3, 3, 3 and receivers 5 are affixed to a wing-shaped support composed of an electrically nonconductive material and can thus be moved as a unit and, using known means or drive units, can be corrected in their position relative to the line 2 for reasons that will be explained in greater detail below. However, this embodiment shows a way there the receiver units 5 are located within the array composed of the transmission coils 3, 3, 3 in about the same xy plane, if the certain height of the components and especially the receiver units 5 is kept in mind. However, an arrangement in parallel planes would do as well from electromagnetics point of view, where moving and positioning under water might get more difficult e.g. due to higher flow resistance.

[0028] The excitation coils 3, 3, 3 all lie in an xy plane and transmit electromagnetic pulses that are time-lagged relative to one another as a primary signal, as indicated by the different field lines B, B, and B in FIG. 2a.

[0029] The illustration in FIG. 2b shows the section extending in the plane II-II from FIG. 1 during the emission of a secondary signal B.sub.r in response to currents induced in an electrically conductive body of the line 2 buried under the surface or the seabed BO. Due to the general three-dimensional characteristic of a magnetic field this response signal B.sub.r is registered in different magnitude as well as significantly differing vectorial analysis depending form the position of the respective receiver units 5 within the detector cell 1.

[0030] Across the array of transmission coils 3, 3, 3, distributed in the xy plane, receiver units 5 are provided, which all measure the secondary signals B.sub.r, not shown in detail here, that are generated in response to the transmission of each primary pulse by one of the transmission coils 3, 3, 3. Since the receiver units 5 each have receiver coils 4 that measure in two axes x and z extending orthogonal to one another, reception signals are picked up simultaneously at different points of the detector cell 1 that are slightly offset from one another. For simple reasons of geometry, the receiver units 5 according to FIGS. 2a und 2b are each positioned at different angles and distances from the line 2. As a result, the respectively detected reception signals also differ from one another fundamentally. Based on these differences in the at least two spatial axes, a distance D of the detector cell 1 from the line 2 can be determined, the large number of measurement values making it possible to compensate for measuring inaccuracies. A thickness of a covering layer over the line 2 can thus be determined continuously along the line 2 as a simple difference between the distances d and D. Symmetries within the described arrangement help to check the plausibility of the measured values. For example, excitation by coils 3 and 3 results in a mirror-symmetric field, so that a comparable symmetry can also be expected in the response signals.

[0031] This effect may be used to reduce the influence of e.g. noise. Due to the longitudinal extension of the line 2 and a resulting form of the fields, the evaluation of response signals B.sub.r in this extension axis y is hardly informative. This means that measurement and calculation efforts can be saved here. In an exemplary embodiment, each transmission coil 3, 3, 3 is embodied as a rectangle with the edge lengths of approximately 1.5 m*approximately 1.41 m with a winding at a nominal current of approximately 170 A and a voltage between about 10 V to less than about 25 V. It can be shown, that in case of deviation regarding an axial offset as well as a coverage thickness the amplitudes clearly decrease from a situation with a low coverage thickness and a measurement position exactly over the center axis M of the line. Basically, however, the curve of an x component is always essentially point-symmetrical to the origin 0,0, the y component remains at about 0 due to symmetry of the line 2 and the detector cell 1 being torn at least parallel to the y-axis, while the z component has a curve that is axially symmetrical to the zero point.

[0032] Finally, a time decay at maximum amplitude for three different diameters of cables has been measured within the same field. Certainly, the best and strongest response is given from the cable having the largest diameter. However, over the measurements it was found that a response signal may be used up to 10 ms after switching of the primary signal. A time lag t in a range of 400 up to 550 s cutting away by appropriate switching means analysis of the data derived from a respective measurement still gives the chance to receive a strong and reliable result for measuring a thickness of a covering over the line 2 under examination.

REFERENCE NUMERAL LIST

[0033] 1 device/detector cell [0034] 2 line [0035] 3, 3, 3 excitation/transmission coil [0036] 4 receiver coil [0037] 5 cube-like receiver unit [0038] 5 cube-like receiver unit in a staggered configuration which still is regarded as a xy-plane configuration [0039] B, B, B electromagnetic excitation pulse, primary pulse [0040] B.sub.r secondary signal in response to currents induced in an electrically conductive body by a primary pulse B,B,B [0041] BO sea bed surface [0042] d height of the detector cell 1 above the sea bed surface BO [0043] D distance of the detector cell 1 from the line 2 [0044] M center axis of the line 2 [0045] v speed [0046] WO surface of the water [0047] x, y, z axes of a Cartesian coordinate system [0048] thickness of a covering over the line 2