EP1807693A1 - Vorrichtung und verfahren zur elektromagnetischen akustischen materialprüfung und/oder dickenmessung an einem wenigstens elektrisch leitende und ferromagnetische materialanteile aufweisenden prüfobjekt - Google Patents
Vorrichtung und verfahren zur elektromagnetischen akustischen materialprüfung und/oder dickenmessung an einem wenigstens elektrisch leitende und ferromagnetische materialanteile aufweisenden prüfobjektInfo
- Publication number
- EP1807693A1 EP1807693A1 EP05801683A EP05801683A EP1807693A1 EP 1807693 A1 EP1807693 A1 EP 1807693A1 EP 05801683 A EP05801683 A EP 05801683A EP 05801683 A EP05801683 A EP 05801683A EP 1807693 A1 EP1807693 A1 EP 1807693A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- test object
- eddy current
- magnetic
- current coil
- technical surface
- 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- Withdrawn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
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B06—GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
- B06B—METHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
- B06B1/00—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
- B06B1/02—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
- B06B1/04—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with electromagnetism
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
- G01N27/72—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables
- G01N27/82—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables for investigating the presence of flaws
- G01N27/90—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables for investigating the presence of flaws using eddy currents
- G01N27/9006—Details, e.g. in the structure or functioning of sensors
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/22—Details, e.g. general constructional or apparatus details
- G01N29/24—Probes
- G01N29/2412—Probes using the magnetostrictive properties of the material to be examined, e.g. electromagnetic acoustic transducers [EMAT]
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/04—Wave modes and trajectories
- G01N2291/042—Wave modes
- G01N2291/0422—Shear waves, transverse waves, horizontally polarised waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/04—Wave modes and trajectories
- G01N2291/044—Internal reflections (echoes), e.g. on walls or defects
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/04—Wave modes and trajectories
- G01N2291/051—Perpendicular incidence, perpendicular propagation
Definitions
- the invention relates to a device and a method for material testing on an at least electrically conductive and ferromagnetic material having test object, which has at least one technical surface, with at least one electromagnetic ultrasonic transducer assembly (EMUS) having a permanent or electromagnet assembly with at least two of facing magnetic surface arranged magnetic poles of different magnetic polarity, as well as at least one in the projection on the technical surface between two magnetic poles medium or arranged directly relative to the technical surface eddy current coil provides.
- EUS electromagnetic ultrasonic transducer assembly
- Electromagnetic ultrasonic transducers are used in a manner known per se for purposes of non-destructive material testing and measurement of test specimens consisting of electrically conductive materials, which preferably also have ferromagnetic properties.
- two types of electromagnetic ultrasonic transducers can be distinguished, on the one hand those with which the generation of so-called horizontally polarized shear waves is possible, which are able to propagate mainly parallel to the coupling surface within the specimen, and on the other hand US converter for generating so-called freely in the specimen propagating ultrasonic waves, which preferably propagate perpendicular to the coupling surface within the sample body.
- the Excitation of ultrasound waves within a specimen attributable to the occurrence of magnetostriction and Lorenz adopted within the specimen material, which can be generated by the presence of a temporally largely constant magnetic field in superposition with a caused by an alternating electrical current electromagnetic alternating field.
- FIG. 5 a, b A typical structure for exciting ultrasonic waves according to the so-called EMUS principle can be taken from FIG. 5 a, b.
- Common EMUS converters 3 have a permanent magnet 1 and an eddy current coil 2, which are designed for common handling as a unit.
- the eddy current coil 2 is formed as a rectangular or spiral flat coil and attached to a magnetic pole side of the permanent magnet 1, so that the coil 2 is penetrated vertically by a permanent magnetic field.
- the normal to the test object surface propagating ultrasonic waves as well as the radially polarized shear waves along the Prüêtober Structure propagating ultrasonic waves are suitable according to the prior art for both error checking, such as crack testing within the test object and for Wand37n ⁇ or wall thickness measurement of the test object.
- DE 35 11 076 A1 discloses a test pig for electromagnetic tests on pipe walls made of steel, with which, for example in the context of a non-destructive test, wall weakenings can be examined and detected by rusting on pipeline walls.
- a pig member described in greater detail in the document is provided with uniformly distributed on the circumference of electromagnets, each having two axially aligned measuring heads, a yoke connecting the measuring heads and a magnetizing coil on these measuring heads.
- the field of each electromagnet runs parallel to the pipe center axis.
- an eddy current coil is arranged directly on at least one of the poles or magnetic heads, which is acted upon by strong and very steeply sloping current pulses.
- the pipelines formed as pipelines round seams are provided at the seams of two adjacent pipe sections that exert a shock load on the electromagnetic transducer in a continuous inspection of a passing over the seams with the above-mentioned flirtmolch, which also prevail through the existing existing between the electromagnet and the pipe wall magnetic forces is significantly increased.
- an electromagnetic ultrasonic transducer can be removed, which provides two separate eddy current coils for transmission and reception in or from an electrically conductive, ferromagnetic test specimen, which are preferably brought into coincidence with one another via an insulating layer.
- an EMUS transducer can be removed, in which for generating a permanent magnetic field, a U-shaped permanent magnet is used, both of which one end magnetic poles facing a test body to be examined. Between the bridge area of the U-shaped permanent magnet projecting surface area of the test object are each serving for ultrasonic generation and ultrasonic reception eddy current coils, which are each designed as meander coils provided.
- the invention is based on the object, an apparatus and a method for material testing on an at least electrically conductive and ferromagnetic Material-containing test objects based on electromagnetic ultrasonic excitation and using an electromagnetic ultrasonic transducer assembly (EMUS) to develop such that on the one hand ensures that the eddy current coil required for generating eddy current is subject to little or no fretting, on the other hand, the opportunity is offered to the test specimen in its entire depth or thickness and to carry out wall thickness measurements.
- the measures to be taken should be suitable for examining and measuring tubular and disk-shaped test specimen geometries.
- the proposed device allows one of the prevailing between the Permanent ⁇ or electromagnet assembly and the test object magnetic Attractively independent positioning of the at least one eddy current coil relative to the technical surface of the test object so that it is not subject to any Reibverschleiss that would result from a magnetkraftbeetzschlagte contact pressure of the eddy current coil on the technical surface of the test object to be examined.
- the eddy current coil is arranged in a region relative to the technical surface of the test object, which is penetrated by a longitudinally of the technical surface spaced from each other arranged magnetic poles resulting tangential magnetic field, ie the initiated by the permanent or electromagnet assembly within the test object magnetic field lines are largely parallel to the technical surface on or relative to the eddy current coil is arranged.
- the eddy current coil in which the eddy current coil is arranged directly to the magnetic pole face facing a test object, act in the inventive device no induced by external magnetic fields attractions between the eddy current coil and the test object to be examined.
- the at least one eddy current coil it is possible to firmly connect the at least one eddy current coil by providing a suitable holder with the permanent or electromagnet assembly.
- a suitable holder with the permanent or electromagnet assembly.
- Such a spatially fixed association between the permanent magnet or electromagnet arrangement and the at least one eddy current coil enables a uniform and simple handling of the electromagnetic ultrasonic transducer arrangement designed in accordance with the solution.
- an independent handling of permanent or electromagnet assembly and the at least one eddy current coil can offer advantageous applications, for example, in cases where the permanent or electromagnet assembly disposed on one side of a test object to be tested and the at least one eddy current coil on, the permanent or Electromagnet assembly facing away from the test object is positioned in a manner such that the at least one eddy current coil always comes to lie in projection on the technical surface between two magnetic poles of the permanent or electromagnet assembly.
- eddy current coils are to be provided, which are to be oriented in a suitable manner relative to the tangential magnetic field.
- the at least one eddy current coil within the test object in the area of the tangential magnetic field, it is necessary to create a spatial area in which an eddy current with an increased current density and with a uniform eddy current direction is formed.
- the at least one eddy current coil it is necessary to form the at least one eddy current coil and to arrange it in relation to the test object penetrated by the tangential magnetic field, so that within the test object a spatially delimitable area is created by the vortex coil geometry, in which a resulting eddy current field with an eddy current density increased compared to the surrounding spatial regions and forms a uniform eddy current direction.
- a preferred eddy current coil which satisfies the above requirements, provides an AC-supplyable electrical conductor arrangement, which has at least two or more sections, preferably a plurality of substantially parallel electrical conductors which are traversed in the same direction by the alternating current.
- two preferred embodiments are described for such an eddy current coil arrangement, one of which represents a three-dimensional eddy current coil and the other provides a two-dimensional interconnect arrangement which has at least two interconnect sections designed in the manner of a rectangular coil each, wherein the interconnect sections are arranged adjacent to one another in this way, that both rectangular coils, each having a rectangular coil section are arranged directly next to each other, which is interspersed with alternating current of the same orientation.
- the device according to the invention is capable of coupling free ultrasonic waves which propagate substantially perpendicularly to the technical surface, with respect to which the electromagnetic ultrasonic transducer is arranged.
- the ultrasound coupling is based on the type of test object and its magnetic saturation on the magnetostrictive effect or on Lorenz forces. Both ultrasonic injection mechanisms will be described in detail below with reference to the figures.
- the device according to the invention is based on a method for material testing on a test object having at least electrically conductive and ferromagnetic material components by way of electromagnetic ultrasonic wave generation within the test object having a technical surface, which itself distinguished by the following process steps in detail.
- an alternating current eddy current coil is provided relative to the technical surface for purposes of inducing an alternating magnetic field in the test object, wherein the alternating field induced by the eddy current coil comes into superposition with the tangential magnetic field.
- both magnetic fields it is necessary to make the orientation of both magnetic fields in such a way that their magnetic field lines are parallel to each other, but not necessarily rectified to each other.
- a resulting magnetic field within the range in which both magnetic fields are superimposed results, which results either from the addition or subtraction of the two magnetic field strengths.
- the AC excitation of the eddy current coil is preferably pulse-wise, it is possible to record wall thickness thicknesses of the test object in addition to the material test within the scope of transit time measurements. For this the transit times are detected, between ultrasonic wave generation and ultrasonic wave reception, wherein the generated ultrasonic waves are reflected at an interface or surface of the test object.
- the device according to the invention is particularly suitable for measuring the thickness of tubular test objects, such as, for example, remote pipelines or pipelines as well as disc-shaped test objects, such as railway wheels.
- the solution according to the device serves as an integral part of a scholarmolches, which is guided via a suitable drive in the interior along a pipeline, the pipeline checked for material defects and in particular their wall thickness is detected without having to take damage to the electromagnetic ultrasonic transducer.
- FIG. 3 is a schematic plan view of an eddy current coil formed according to the invention
- FIG. Fig. 4a, b is a schematic representation of an alternative trained
- FIG. 6a - c schematic representations for Faced-array control of a
- FIGs 1a to f different arrangement and training options of the device according to the invention are shown.
- a U-shaped permanent magnet assembly 1 is provided, the yoke-like spans the test object 4 and the front side with their magnetic poles N, S directly on the technical Surface of the test object 4 rests.
- the permanent magnet 1 feeds a tangential magnetic field in the region between the magnetic poles N, S within the test object 4, which is constant in time in the case of a permanent magnet 1.
- the permanent magnet 1 shown in Figures 1 it is also possible, instead of the permanent magnet 1 shown in Figures 1 to use an electromagnet in the same or similar configuration, which is able to feed a time-variable tangential magnetic field in the test object 4. In this case, care must be taken to ensure that the AC frequency required to form the tangential magnetic field is much lower than the AC frequency with which the at least one eddy current coil 2 is fed, which is on the technical surface 5 of the test object 4 in the region of the acting tangential magnetic field is arranged. In addition, it is assumed for the sake of simplicity that the magnet arrangement 1, as already explained above, is designed as a permanent magnet.
- the eddy current coil 2 is located on a surface of the test object 4 opposite the permanent magnet 1. In this case, it must be ensured that the tangential magnetic field coupled into the test object 4 by the permanent magnet 1 is present in the entire thickness of the test object 4 Test object 4 acts.
- the test object 4 is located between the two magnetic poles N 1 S, so that the tangential magnetic field is formed along the entire longitudinal extent of the test object 4.
- FIG. 1f shows a schematized plan view of the electromagnetic ultrasonic transducer arrangement, for example according to FIG. 1a, again, and makes it clear that the eddy current coil 2 is independent of the magnet arrangement along or transversely to the tangential magnetic field lines which are from the north pole to the south pole run, be moved. If necessary, an air gap between the eddy current coil 2 and the test object 4 can be adjusted or varied accordingly, if there are surface curvatures or unevenness, for example, due to weld overshoots, protruding over-rolling, corrosion, dirt or other unevenness.
- a U-shaped permanent magnet 1 for feeding in a temporally constant tangential magnetic field B t within the test object 4 is arranged in each case.
- the eddy current coil 2 is composed of a plurality of mutually parallel electrical conductors 7, which are traversed by an alternating current, each with the same current direction.
- Lorenz forces FL are generated perpendicularly to the technical surface 5. It is evident that the alternating Lorenz forces FL in each opposite effective direction depending on the AC direction longitudinal ultrasonic waves with a propagation direction perpendicular to the technical surface are able to generate.
- FIG. 3 shows a two-dimensional eddy current coil which provides a printed conductor arrangement simulated by a butterfly wing. It consists of two identical conductor track sections 8, 9, which are arranged side by side so that both arranged as rectangular coils conductor track sections are arranged directly adjacent to each other with a rectangular coil section, which is interspersed with alternating current of the same orientation (see the dashed bordered area and the arrow displays each indicating the direction of current flow).
- the dashed border area 10 is the so-called working zone, in which the electrical currents of the current-carrying electrical conductor track sections are always the same orientation.
- the eddy current density in the test object under the working zone 10 is thus significantly higher than in other areas, so that the ultrasound waves are best generated by this gradient at this point or at this area.
- FIGS. 4 a and b show another alternative three-dimensional eddy current coil 2 for exciting free ultrasonic waves.
- FIG. 4 a shows that the electrical conductor composing the eddy current coil 2 is wound around a cube-shaped coil holder 11.
- FIG. 4b shows a cross section through an electromagnetic ultrasonic transducer designed in this respect, in which the cube-shaped eddy current coil 2 is surmounted by the U-shaped permanent magnet 1.
- the individual eddy current coils 2 are to be controlled in a linearly delayed manner.
- test devices according to FIGS. 7 and 8 are to be combined with a corresponding movement kinematics, for example with a so-called test pig, in order to allow a forward movement along the tube.
- a plurality of individual eddy current coils 2 are arranged between two magnetic poles N, S, preferably in the form of a checkerboard pattern arrangement.
- the magnetic poles N, S can either be arranged side by side in the axial direction of the tube 12 or in a circular arrangement around the tube axis (see cross-sectional illustration in FIG. 7).
- the magnetic poles N, S are each annular and connected to each other via a common axis A.
- the annular or disc-like design of the magnetic poles N, S is adapted in each case to the internal geometry of the tube 12 to be examined.
- S brushes Preferably located at the peripheral edges of the magnetic poles N, S brushes, on the one hand to avoid jamming between the magnet assembly and the pipe inner wall and on the other hand to provide a cleaning purpose.
- a plurality of eddy current coils 2 along the peripheral edge of a disc assembly 14 is provided between both ring-shaped magnetic poles N, S.
- the disk assembly 14 is fixedly connected to the common magnetic axis A, which connects both magnetic poles N, S.
- the transducer assembly shown in Figure 8 is capable of detecting the entire inner circumference of a pipe section in the axial direction.
- the conventional design of the EMUS converter with a magnetization in the immediate area of the eddy current coil is, according to the solution, replaced by an arrangement in which a substantially larger area of the test object is magnetized with a tangentially extending magnetic field.
- the distance between the magnetic poles is significantly larger than the dimensions of the eddy current coils.
- One or more eddy current coils can be used.
- the eddy current coils can be positioned in any position over the magnetized area of the test object in any desired arrangement.
- the use of multiple eddy current coils, the so-called coil arrays, is preferred for testing large objects. In this way, a high test speed can be performed without time-consuming scanning of the test object.
- phased excitation of several eddy current coils can be sounded at selectable angles, which the detection of crack-like errors on the basis of appropriate regulations is possible.
- the stress of the eddy current coil due to magnetic attraction forces which are based on a force interaction between the magnet and the test object, is completely eliminated. This reduces the wear on the probe surface and reduces the life of the EMUS sensor.
- a fixed mechanical connection of the magnet and the eddy current coil can be omitted.
- the eddy current coil can move arbitrarily over the surface of the test object within the magnetized area. In particular, it is possible to move the eddy current coil independently of the surface profile of the test object and to unevenness, such as Curvatures, welds, etc. adapt.
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- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Health & Medical Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Electromagnetism (AREA)
- Life Sciences & Earth Sciences (AREA)
- Pathology (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102004053584A DE102004053584B4 (de) | 2004-11-05 | 2004-11-05 | Vorrichtung und Verfahren zur Materialprüfung und/oder Dickenmessung an einem wenigstens elektrisch leitende und ferromagnetische Materialanteile aufweisenden Prüfobjekt |
PCT/EP2005/011782 WO2006048290A1 (de) | 2004-11-05 | 2005-11-03 | Vorrichtung und verfahren zur elektromagnetischen akustische materialprünfung und/oder dickenmessung an einem wenigstens elektrisch leitende und ferromagnetische materialanteile aufweisenden prüfobjekt |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1807693A1 true EP1807693A1 (de) | 2007-07-18 |
Family
ID=35542239
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP05801683A Withdrawn EP1807693A1 (de) | 2004-11-05 | 2005-11-03 | Vorrichtung und verfahren zur elektromagnetischen akustischen materialprüfung und/oder dickenmessung an einem wenigstens elektrisch leitende und ferromagnetische materialanteile aufweisenden prüfobjekt |
Country Status (8)
Country | Link |
---|---|
US (1) | US8037764B2 (de) |
EP (1) | EP1807693A1 (de) |
CA (1) | CA2585823C (de) |
DE (1) | DE102004053584B4 (de) |
NO (1) | NO20072305L (de) |
RU (1) | RU2393468C2 (de) |
UA (1) | UA90117C2 (de) |
WO (1) | WO2006048290A1 (de) |
Families Citing this family (24)
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EP2084524B1 (de) * | 2006-11-01 | 2016-11-30 | Industry-academic Cooperation Foundation, Chosun University | Magnetsensorvorrichtung zum nachweis von defekten |
US20080315462A1 (en) * | 2007-06-25 | 2008-12-25 | General Electric Company | Systems and methods for monitoring a composite cure cycle |
GB2470054B (en) | 2009-05-07 | 2013-08-07 | Pii Ltd | Magnetising assembly |
US8319494B2 (en) | 2009-06-26 | 2012-11-27 | Tdw Delaware Inc. | Pipeline inspection tool with double spiral EMAT sensor array |
AT508478B1 (de) * | 2009-06-26 | 2012-01-15 | Tdw Delaware Inc | Sensorarray für die inspektion der innenwand eines rohres |
US8653811B2 (en) | 2009-06-26 | 2014-02-18 | Tdw Delaware Inc. | Pipeline inspection tool with oblique magnetizer |
DE102011018954B4 (de) * | 2011-04-29 | 2017-12-14 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Ultraschallprüfkopf und Verfahren zur zerstörungsfreien Prüfung eines flächig ausgebildeten Prüfkörpers |
JP5851783B2 (ja) * | 2011-09-27 | 2016-02-03 | 三菱重工業株式会社 | 渦電流探傷用プローブ |
CN103207239B (zh) * | 2013-03-29 | 2015-11-04 | 浙江大学 | 一种一体化可调节磁致伸缩纵向导波探头 |
CN103217481A (zh) * | 2013-04-02 | 2013-07-24 | 厦门大学 | 一种应用磁致伸缩的磁声成像探头 |
DE102013010824A1 (de) | 2013-06-28 | 2014-12-31 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Vorrichtung zum Erzeugen und/oder Nachweisen von Ultraschallwellen in Form von longitudinal polarisierten Volumenwellen |
FR3008187A1 (fr) * | 2013-07-05 | 2015-01-09 | Kontrolltechnik | Dispositif pour controler des tubes |
DE102014101368A1 (de) * | 2014-02-04 | 2015-08-06 | Rosen Swiss Ag | Inspektionsgerät zur Messung der Dicke einer Wand einer Rohrleitung |
GB201419219D0 (en) * | 2014-10-29 | 2014-12-10 | Imp Innovations Ltd | Electromagnetic accoustic transducer |
US10209223B2 (en) * | 2015-05-26 | 2019-02-19 | The Boeing Company | Real-time fusion of ultrasound and eddy current data during non-destructive examination |
US11009484B1 (en) | 2016-03-11 | 2021-05-18 | The University Of Tulsa | Velocity independent two-component magnetic flux leakage detective system |
CN107084692A (zh) * | 2017-06-30 | 2017-08-22 | 沈阳工业大学 | 电磁超声横波测厚换能器 |
CN107271572B (zh) * | 2017-07-31 | 2023-09-26 | 沈阳工业大学 | 电磁超声金属板材探伤换能器 |
JP7048028B2 (ja) * | 2017-09-27 | 2022-04-05 | 日立造船株式会社 | 渦電流探傷システムおよび渦電流探傷方法 |
CN108917805B (zh) * | 2018-08-08 | 2019-11-26 | 苏州博昇科技有限公司 | 电磁超声波双波换能器 |
DE102019206993B4 (de) * | 2019-05-14 | 2021-03-18 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Verfahren zur zerstörungsfreien Prüfung an über den Umfang von Bauteilen umlaufenden Wandungen |
DE102020108963A1 (de) * | 2020-03-31 | 2021-09-30 | Rosen Swiss Ag | Inspektionsvorrichtung zur Inspektion von sich flächig erstreckenden metallischen Gegenständen |
RU207258U1 (ru) * | 2021-04-09 | 2021-10-20 | Федеральное государственное бюджетное образовательное учреждение высшего образования "Кубанский государственный технологический университет" (ФГБОУ ВО "КубГТУ") | Внутритрубный магнитный локатор дефектов и повреждений труб |
CN113109430B (zh) * | 2021-04-14 | 2023-04-25 | 湖南大学 | 柔性差分涡流传感器、检测***及方法 |
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2004
- 2004-11-05 DE DE102004053584A patent/DE102004053584B4/de not_active Expired - Fee Related
-
2005
- 2005-11-03 UA UAA200706192A patent/UA90117C2/ru unknown
- 2005-11-03 EP EP05801683A patent/EP1807693A1/de not_active Withdrawn
- 2005-11-03 RU RU2007120757/28A patent/RU2393468C2/ru not_active IP Right Cessation
- 2005-11-03 WO PCT/EP2005/011782 patent/WO2006048290A1/de active Application Filing
- 2005-11-03 US US11/718,609 patent/US8037764B2/en not_active Expired - Fee Related
- 2005-11-03 CA CA2585823A patent/CA2585823C/en not_active Expired - Fee Related
-
2007
- 2007-05-04 NO NO20072305A patent/NO20072305L/no not_active Application Discontinuation
Non-Patent Citations (1)
Title |
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See references of WO2006048290A1 * |
Also Published As
Publication number | Publication date |
---|---|
DE102004053584A1 (de) | 2006-06-08 |
US8037764B2 (en) | 2011-10-18 |
US20090139335A1 (en) | 2009-06-04 |
WO2006048290A1 (de) | 2006-05-11 |
DE102004053584B4 (de) | 2006-08-31 |
RU2393468C2 (ru) | 2010-06-27 |
UA90117C2 (ru) | 2010-04-12 |
CA2585823A1 (en) | 2006-05-11 |
RU2007120757A (ru) | 2008-12-10 |
CA2585823C (en) | 2013-06-25 |
NO20072305L (no) | 2007-07-23 |
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