JP6071461B2 - Material deterioration diagnosis apparatus and material deterioration diagnosis method - Google Patents

Description

  Embodiments described herein relate generally to an electromagnetic ultrasonic oscillator, a material deterioration diagnosis device, and a material deterioration diagnosis method.

  Ultrasonic flaw detection is used for pipe thinning and corrosion inspection. In the ultrasonic flaw detection method, a probe that transmits and receives ultrasonic waves is pressed against the surface of a test object, and ultrasonic waves of various frequencies are propagated inside. And the ultrasonic wave which reflected and returned by the defect in a to-be-tested object and a back surface is received, and the state inside a to-be-tested object is grasped | ascertained. The defect position is measured from the time required from transmission to reception of the ultrasonic wave, and the size of the defect is obtained by measuring the intensity of the received echo and the range in which the defect echo appears.

  The ultrasonic inspection method is used in nuclear power plants to measure the thickness of materials and to detect welding defects such as lamination. In addition, such an inspection method is also used in the inspection of the weld opening that reinforces the nozzle opening, branch, and pipe joint around the reactor pressure vessel.

  It has been found that in power plants, thinning tends to occur easily in the elbow part of the piping, the downstream side of the orifice, and the like due to flow accelerated corrosion (FAC) and erosion. Based on such knowledge, a standard (JSME S CA1-2005) for pipe thinning management has been established by the Japan Society of Mechanical Engineers. As a standardized pipe thinning management technique, pipe thickness measurement using an ultrasonic thickness measuring instrument is performed. However, this method requires a great deal of time and cost because it is necessary to disassemble / restore the heat insulating material covering the pipe every time measurement is performed.

  Therefore, in order to realize low-cost thinning management, an embedded type fixed point measuring sensor has been developed. For example, an ultrasonic optical probe in which an electromagnetic ultrasonic transducer (EMAT) and an optical fiber vibration sensor are combined is known. The optical fiber vibration sensor is polyimide-coated and attached to the pipe surface using a polyimide-based adhesive. The electromagnetic ultrasonic oscillator directly excites the ultrasonic wave in the pipe by the action of electromagnetic force, and the resonance wave of the excited ultrasonic wave is detected by the optical fiber vibration sensor. Then, by analyzing the detection result, it is possible to obtain information on the pipe thickness and internal defects.

  A conventional embedded type fixed point measuring sensor has to install ultrasonic optical probes at thousands of points on the pipe surface. That is, thousands of electromagnetic ultrasonic oscillators and optical fiber vibration sensors have to be prepared and installed, resulting in an increase in installation cost.

Kiichiro Uchigasaki et al .: “Nuclear Power and Design Technology” Taiga Publishing (1980), pp.226-250

  The problem to be solved by the present invention is to provide a material deterioration diagnosis device with reduced installation cost, an electromagnetic ultrasonic oscillator used in the material deterioration diagnosis device, and a material deterioration diagnosis method.

  According to the present embodiment, the material deterioration diagnosis device responds to the oscillation provided in the surface of the metal material, the optical fiber provided on the surface of the metal material, and the vibration in the metal material. An optical interferometer that converts fluctuations of light transmitted through the optical fiber into an electrical signal, and a measurement / control that calculates the thickness of the metallic material based on the electrical signal and determines the degree of deterioration of the metallic material A section. The oscillator includes an electric coil and a magnet that is provided on the electric coil and applies a magnetic field along the surface direction of the metal material. The optical interferometer converts a change in light transmitted through the optical fiber according to vibration excited by the oscillator into an electric signal.

1 is a schematic configuration diagram of a material deterioration diagnostic apparatus according to an embodiment of the present invention. 1 is a schematic configuration diagram of an electromagnetic ultrasonic oscillator according to an embodiment of the present invention. The schematic block diagram of the optical fiber sensor part which concerns on embodiment of this invention. The figure which shows the example of installation of the material degradation diagnostic apparatus which concerns on embodiment of this invention. The figure explaining the material degradation diagnostic method which concerns on embodiment of this invention. The figure explaining the material degradation diagnostic method by a comparative example. The figure which shows the example of installation of the material deterioration diagnostic apparatus by a comparative example. The graph which shows the measurement result by this embodiment and a comparative example. The schematic block diagram of the electromagnetic ultrasonic oscillator by a modification. The schematic block diagram of the electromagnetic ultrasonic oscillator by a modification. The schematic block diagram of the electromagnetic ultrasonic oscillator by a modification. The schematic block diagram of the electromagnetic ultrasonic oscillator by a modification. The figure which shows the example of installation of the material deterioration diagnostic apparatus by a modification.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings.

  FIG. 1 shows a schematic configuration of a material deterioration diagnosis apparatus according to an embodiment of the present invention. The material deterioration diagnostic apparatus includes an electromagnetic ultrasonic oscillator (hereinafter referred to as EMAT) 1, an optical fiber sensor unit 2, a light source 3, an optical interferometer 4, a measurement / control unit 5, a waveform signal generator 6, and an amplifier 7. ing. The EMAT 1 and the optical fiber sensor unit 2 are arranged on the surface of the metal whose thickness is to be measured. The thickness measurement target is, for example, a piping of a nuclear power plant or a thermal power plant. The waveform signal generator 6 and the amplifier 7 supply a high-frequency current to the EMAT 1 based on the control of the measurement / control unit 5.

  FIG. 2 shows a schematic configuration of EMAT1. The EMAT 1 includes an electric coil 12 connected to the amplifier 7 and supplied with a high-frequency current, and a permanent magnet 11 placed on the electric coil 12. The permanent magnet 11 includes a cylindrical magnet 11A and a columnar magnet 11B provided inside the cylindrical magnet 11A.

  The material of the permanent magnet 11 is, for example, samarium cobalt. Since samarium cobalt has a demagnetization point between 350 and 400 ° C., it is preferably used in an environment of 350 ° C. or less. A samarium iron-based sintered magnet may also be used.

  The permanent magnet 11 may be plated (plated) to prevent oxidation and the electric coil 12 may be coated with polyimide. In this way, the oscillation power can be maintained even at high temperatures.

  The upper surface of the optical fiber sensor unit 2 is shown in FIG. 3A, and the side surface is shown in FIG. As shown in FIG. 3A, in the optical fiber sensor unit 2, the optical fiber 21 is spirally wound into a circular flat plate. One end on the inner side of the optical fiber 21 is connected to the optical interferometer 4, and the other end on the outer side is connected to the light source 3. The optical fiber 21 receives the reference laser light from the light source 3. Further, the optical interferometer 4 detects the fluctuation of the light transmitted through the optical fiber 21. The optical fiber 21 is coated with a metal such as gold or nickel, or silica.

  Although not shown, the connection relationship between the optical interferometer 4 and the light source 3 with respect to the optical fiber may be reversed.

  As shown in FIGS. 3A and 3B, the optical fiber 21 is attached to the sheet material 22 using an adhesive 23. For the sheet material 22, for example, a flexible sheet material that does not contain metal such as silicon foil, glass foil, ceramic foil, and the like can be used. The adhesive 23 for bonding the optical fiber 21 and the sheet material 22 differs depending on the material for coating the optical fiber 21. For example, when the optical fiber 21 is coated with gold, a gold paste is used for the adhesive 23. Further, when the optical fiber 21 is nickel-coated, a gold paste or a silver paste is used for the adhesive 23. Alternatively, when the optical fiber 21 is coated with silica, a glass paste is used for the adhesive 23.

  As shown in FIG. 3C, the optical fiber 21 may be sandwiched between the sheet material 22 and the resin sheet 24. The optical fiber 21 is fixed by filling the adhesive 23 between the sheet material 22 and the resin sheet 24. For the resin sheet 24, a heat-resistant resin sheet such as heat-resistant epoxy, polybenzimidazole, mica-reinforced polytetrafluoroethylene, and aromatic polyester can be used.

  4A and 4B show an example of attachment of the EMAT 1 and the optical fiber sensor unit 2 to the pipe 40. FIG. FIG. 4B is a cross-sectional view taken along the line II of FIG.

  As shown in FIGS. 4A and 4B, EMAT 1 has eight pieces (45 ° intervals) in the circumferential direction with respect to the cross section of the pipe 40, and a predetermined interval φ along the axial direction of the pipe 40 (φ is the pipe 40 (outer diameter length) is arranged with a gap.

  The optical fiber sensor unit 2 is provided between the surface of the pipe 40 and the EMAT 1. Two optical fiber sensor units 2 are arranged in the circumferential direction (at intervals of 180 °), and are arranged at an interval of 3φ along the axial direction of the pipe.

  The EMAT1 is fixed to the pipe 40 by the magnetic force of the permanent magnet 11, and the optical fiber sensor unit 2 is sandwiched and fixed between the surface of the pipe 40 and the EMAT1.

  In this embodiment, one optical fiber sensor unit 2 is provided for a plurality (12 in the example shown in FIGS. 4A and 4B) of EMAT1. 12 EMAT1 and one optical fiber sensor 2 are grouped so as to be surrounded by broken lines in FIGS. 4A and 4B, and one optical fiber sensor 2 is ultrasonic waves excited by EMAT1 of the same group. Is detected.

  Next, a method of measuring the thickness of the pipe 40 using the EMAT 1 and the optical fiber sensor unit 2 attached to the pipe 40 in this way will be described with reference to FIGS. FIG. 5A shows a cross section of the optical fiber sensor unit 2 and the EMAT 1 stacked on the pipe 40. FIG. 5B shows a cross section of EMAT 1 provided directly on the pipe 40. The surface of the pipe 40 is a curved surface, but is shown as a plane for convenience in FIGS. 5 (a) and 5 (b).

  As shown in FIGS. 5 (a) and 5 (b), when a high-frequency current flows through a circular flat-plate electric coil 12 wound in a spiral shape, a cylindrical magnet 11A and a columnar magnet arranged substantially concentrically with the electric coil. The magnetization direction of 11B becomes the opposite direction, a magnetic field is generated along the surface direction of the pipe 40, and the pipe 40 vibrates to generate electromagnetic ultrasonic waves. The frequency of the alternating current applied to the electric coil 12 is changed by the waveform signal generator 6 (see FIG. 1), and the frequency of the generated electromagnetic ultrasonic waves is swept in a desired frequency band.

  The vibration inside the pipe 40 (inside the pipe wall) is transmitted to the optical fiber sensor unit 2 on the same principle as the strain measurement of the high-temperature strain gauge. When vibration reaches the optical fiber sensor unit 2 in a state where the reference laser beam is input from the light source 3, the optical fiber 21 is slightly expanded and contracted, and the Doppler effect and the polarization plane change occur in the laser beam. The frequency of the ultrasonic wave propagating in the pipe 40 can be measured by the optical interferometer 4 converting the fluctuation (stretching speed) into a voltage value by photoelectric conversion.

  The frequency of vibration generated inside the pipe 40 can be selected by the waveform signal generator 6 from 1 Hz to 10 MHz in accordance with the thickness of the pipe 40. The measurement / control unit 5 detects vibration with a frequency of 1 Hz to 20 kHz and ultrasonic vibration with a frequency of 20 kHz to 10 MHz via the optical fiber 21 and the optical interferometer 4.

  When the frequency of the electromagnetic ultrasonic wave is swept and the relationship of λ = 2d is established between the thickness d of the pipe 40 and the wavelength λ of the electromagnetic ultrasonic wave, the incident wave and the reflected wave resonate, and the amplitude of the output wave is large. Become. This relationship can be expressed as f = v / 2d using the ultrasonic frequency f and sound velocity v. Therefore, the thickness of the pipe 40 can be obtained from the resonance frequency and the speed of sound. For example, in the case of a 9 mm thick steel plate, resonance occurs when an ultrasonic wave of 300 kHz is input.

  The EMAT 1 for passing a current through the electric coil 12 is sequentially switched by the measurement / control unit 5, and the corresponding optical fiber sensor unit 2 detects ultrasonic vibration. In the present embodiment, as shown in FIGS. 5A and 5B, by generating a magnetic field along the surface direction of the pipe 40, the SN ratio of resonance in the thickness direction of the pipe 40 is increased. Therefore, the optical fiber sensor unit 2 provided at a position away from the EMAT 1 can detect the resonance signal.

  (Comparative Example) FIG. 6 shows a cross section of the optical fiber sensor unit 200 and the EMAT 100 laminated on the pipe 40 according to a comparative example. The EMAT 100 according to the comparative example includes a cylindrical permanent magnet 110 and an electric coil 120. As shown in FIG. 6, when a high frequency current flows through the electric coil 120, a magnetic field along the thickness direction of the pipe 400 is generated. The optical fiber sensor unit 200 has the same configuration as the optical fiber sensor unit 2.

  Such an EMAT 100 and an optical fiber sensor unit 200 are arranged as shown in FIGS. 7A and 7B, and the EMATs 100_1 to 100_4 in the (n + 1) th column are sequentially oscillated and measured by the optical fiber sensor unit 200_1 in the nth column. The S / N ratio of resonance is shown in FIG. FIG. 7B is a cross-sectional view of a portion corresponding to the n-th column in FIG. The interval between the n-th column and the (n + 1) -th column is the outer diameter length φ of the pipe 400. The EMATs 100_1 to 100_4 are provided at positions shifted by 0 °, 40 °, 90 °, and 135 ° in the circumferential direction as viewed from the optical fiber sensor unit 200_1. Moreover, the result of having performed the same measurement by replacing the EMAT 100 and the optical fiber sensor unit 200 with the EMAT 1 and the optical fiber sensor unit 2 according to the present embodiment is also shown in FIG.

  From FIG. 8, by using the EMAT1 according to the present embodiment, an ultrasonic signal excited by the EMAT1 at a position shifted by φ in the axial direction and 90 ° in the circumferential direction as viewed from the optical fiber sensor unit 2 can be obtained with a sufficient SN ratio. It can be seen that it can be measured. On the other hand, in the EMAT 100 according to the comparative example, since a magnetic field is generated along the thickness direction of the pipe 40, the S / N ratio of resonance cannot be increased.

  As described above, according to the present embodiment, the single optical fiber sensor unit 2 can detect the resonance signals by the EMAT 1 that are located in the grouped regions of the axial direction ± φ and the circumferential direction ± 90 °. it can. Since only one optical fiber sensor unit 2 needs to be prepared for a plurality of EMATs 1, the installation cost of the material deterioration diagnosis apparatus can be reduced.

  In the said embodiment, it is preferable to install EMAT1 in the measuring point prescribed | regulated by piping thinning management standard. In the pipe thinning management standard, when the pipe size is 150A (outer diameter: about 165mm) or more, there are 8 measurement points (45 ° intervals) in the circumferential direction, and when the pipe size is less than 150A, the circumferential direction It is stipulated that four measurement points (90 ° intervals) are provided. Moreover, it is prescribed | regulated that the axial direction of piping provides a measurement point with the space | interval below the outer diameter length of piping.

  In the above embodiment, the permanent magnet 11 includes the cylindrical magnet 11A and the columnar magnet 11B provided inside the cylindrical magnet 11A. However, as shown in FIGS. Instead of the magnet 11A, a plurality of rectangular magnets 11C may be arranged circumferentially. FIG. 9A is a top view, and FIG. 9B is a cross-sectional view taken along the line II-II in FIG. 9A. The magnetization directions of the plurality of rectangular magnets 11C and the columnar magnet 11B are opposite to each other, and a magnetic field along the surface direction of the pipe 40 can be generated. Since the resonance signal can be detected with high accuracy in the optical fiber sensor unit 2 provided at a position away from the EMAT 1, it is sufficient to provide one optical fiber sensor unit 2 for a plurality of EMATs 1 and Installation cost can be reduced.

  10A and 10B, a high permeability material 11D such as an amorphous alloy may be provided between the cylindrical magnet 11A and the columnar magnet 11B. FIG. 10A is a top view, and FIG. 10B is a cross-sectional view taken along line III-III in FIG. By providing the high magnetic permeability material 11D, a stronger magnetic field can be generated along the surface direction of the pipe 40.

  Further, the permanent magnets 11 may be arranged in a Halbach array. For example, as shown in FIGS. 11A and 11B, a cylindrical magnet magnetized between a cylindrical magnet 11A and a columnar magnet 11B so that a magnetic field is directed from the inside to the outside or from the outside to the inside. 11E may be provided. 11A is a top view, and FIG. 11B is a cross-sectional view taken along the line IV-IV in FIG. 11A. With such a configuration, the magnetic field along the surface direction of the pipe 40 can be increased approximately twice without increasing the outer diameter of the permanent magnet 11.

  Further, as shown in FIGS. 12A and 12B, the structure may be simplified by omitting the cylindrical magnet 11A from the configuration shown in FIGS. 11A and 11B. 12A is a top view, and FIG. 12B is a cross-sectional view taken along line VV in FIG. 12A.

  In the above embodiment, the optical fiber sensor unit 2 is provided between the pipe 40 and the EMAT1, but the optical fiber sensor unit 2 may be disposed independently of the EMAT1 as shown in FIG. For example, the optical fiber sensor unit 2 is disposed at an intermediate point of the EMAT 1 adjacent to the pipe 40 in the axial direction. The optical fiber sensor unit 2 detects a resonance signal from the EMAT 1 located in the region of the axial direction ± φ and the circumferential direction ± 90 ° as viewed from the optical fiber sensor unit 2.

  According to at least one embodiment or modification described above, the installation cost of the material deterioration diagnosis apparatus can be reduced.

  Although the embodiment of the present invention has been described, this embodiment is presented as an example and is not intended to limit the scope of the invention. These novel embodiments can be implemented in various other forms, and various omissions, replacements, and changes can be made without departing from the scope of the invention. These embodiments and modifications thereof are included in the scope and gist of the invention, and are included in the invention described in the claims and the equivalents thereof.

1 EMAT
2 Optical fiber sensor unit 3 Light source 4 Optical interferometer 5 Measurement / control unit 6 Waveform signal generator 7 Amplifier 11 Permanent magnet 12 Electric coil 21 Optical fiber 40 Piping

Claims (7)

A plurality of oscillators provided at predetermined intervals on the surface of the metal material;
An optical fiber sensor unit comprising an optical fiber provided on the surface of the metal material and grouping a plurality of oscillators provided at a predetermined interval, and one provided for the grouped oscillators ; ,
An optical interferometer that converts fluctuations of light transmitted through the optical fiber that constitutes the optical fiber sensor unit in response to vibration in the metal material into an electrical signal;
The plurality of grouped oscillators that generate vibrations are sequentially switched, a resonance frequency is obtained based on the electrical signal, a thickness of the metal material is calculated based on the resonance frequency, and a deterioration degree of the metal material A measurement / control unit for determining
With
The oscillator includes an electric coil and a magnet that is provided on the electric coil and applies a magnetic field along a surface direction of the metal material,
The material interferometer, wherein the optical interferometer converts a fluctuation of light transmitted through the optical fiber according to vibration excited by a plurality of oscillators provided at the predetermined interval into an electric signal. The magnet
A cylindrical magnet;
A columnar magnet provided inside the cylindrical magnet;
The material deterioration diagnosis apparatus according to claim 1, wherein:   The material deterioration diagnosis apparatus according to claim 2, wherein a high permeability material is provided between the cylindrical magnet and the columnar magnet.   The material deterioration diagnosis apparatus according to claim 1, wherein the magnet is a Halbach array magnet.   5. The optical fiber according to claim 1, comprising x optical fibers (x is an integer equal to or greater than 1) and y oscillators (y is an integer satisfying y> x). The material deterioration diagnosis apparatus described. The oscillator is, across the optical fiber to the surface of a metallic material, or an electromagnetic ultrasonic oscillator is provided directly,
6. The material deterioration diagnosis apparatus according to claim 1 , further comprising: an electric coil; and a magnet that is provided on the electric coil and applies a magnetic field along a surface direction of the metal material. A plurality of second oscillators provided on the surface of the metallic material at predetermined intervals and including a magnet for applying a magnetic field along the surface direction of the metallic material; and the predetermined intervals provided on the surface of the metallic material. A material deterioration diagnosis method using a plurality of resonators provided in a group and an optical fiber sensor unit including an optical fiber provided for one of the grouped resonators ,
A step of sequentially switching and exciting vibrations in the metal material by the grouped oscillators, and a step of converting fluctuations of light transmitted through the optical fiber in response to the vibrations into electrical signals;
Obtaining a resonance frequency based on the electrical signal, and calculating a thickness of the metallic material corresponding to an installation position of the oscillator by the resonance frequency ;
A material deterioration diagnosis method comprising:

Images