[go: up one dir, main page]

CN112147235A - An electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection - Google Patents

An electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection Download PDF

Info

Publication number
CN112147235A
CN112147235A CN202011151891.2A CN202011151891A CN112147235A CN 112147235 A CN112147235 A CN 112147235A CN 202011151891 A CN202011151891 A CN 202011151891A CN 112147235 A CN112147235 A CN 112147235A
Authority
CN
China
Prior art keywords
circuit board
printed circuit
flexible printed
double
coils
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.)
Granted
Application number
CN202011151891.2A
Other languages
Chinese (zh)
Other versions
CN112147235B (en
Inventor
刘素贞
郝煜朝
张闯
金亮
杨庆新
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hebei University of Technology
Original Assignee
Hebei University of Technology
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hebei University of Technology filed Critical Hebei University of Technology
Priority to CN202011151891.2A priority Critical patent/CN112147235B/en
Publication of CN112147235A publication Critical patent/CN112147235A/en
Application granted granted Critical
Publication of CN112147235B publication Critical patent/CN112147235B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating 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
    • G01N29/34Generating the ultrasonic, sonic or infrasonic waves, e.g. electronic circuits specially adapted therefor
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
    • B06B1/04Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with electromagnetism
    • B06B1/045Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with electromagnetism using vibrating magnet, armature or coil system
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating 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
    • G01N29/04Analysing solids
    • G01N29/12Analysing solids by measuring frequency or resonance of acoustic waves
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B2201/00Indexing scheme associated with B06B1/0207 for details covered by B06B1/0207 but not provided for in any of its subgroups
    • B06B2201/50Application to a particular transducer type
    • B06B2201/52Electrodynamic transducer
    • B06B2201/53Electrodynamic transducer with vibrating magnet or coil

Landscapes

  • Physics & Mathematics (AREA)
  • Biochemistry (AREA)
  • Analytical Chemistry (AREA)
  • Pathology (AREA)
  • Immunology (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • General Health & Medical Sciences (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Mechanical Engineering (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Abstract

本发明为一种用于管道导波混频检测的电磁超声激励装置,该装置包括由柔性制版技术制作的双层柔性印刷电路板和片状橡胶钕铁硼磁体,双层柔性印刷电路板的底层和顶层所印制的回折型多簇线圈的相邻簇线间距不同,顶层和底层线圈中心在同一位置;双层柔性印刷电路板粘贴在片状橡胶钕铁硼磁体的一面上,检测时双层柔性印刷电路板位于磁体与被测试件外表面之间。该装置安装拆卸便捷,结构简单紧凑,体积较小,具有柔性,能适应弯曲表面及狭窄环境,可以对管道微裂纹进行有效检出与定位。

Figure 202011151891

The invention relates to an electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection. The device includes a double-layer flexible printed circuit board and a sheet-shaped rubber NdFeB magnet made by flexible plate-making technology. The back-folded multi-cluster coils printed on the bottom layer and the top layer have different spacings between adjacent cluster lines, and the centers of the top layer and bottom layer coils are in the same position; the double-layer flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet. A two-layer flexible printed circuit board is located between the magnet and the outer surface of the DUT. The device is easy to install and disassemble, has a simple and compact structure, is small in size, and has flexibility, can adapt to curved surfaces and narrow environments, and can effectively detect and locate micro-cracks in pipes.

Figure 202011151891

Description

一种用于管道导波混频检测的电磁超声激励装置An electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection

技术领域technical field

本发明属于电磁超声检测领域,具体是一种用于管道导波混频检测的电磁超声激励装置。The invention belongs to the field of electromagnetic ultrasonic detection, in particular to an electromagnetic ultrasonic excitation device used for pipeline guided wave mixing detection.

背景技术Background technique

超声导波检测技术作为无损检测领域的重要分支,近年来被广泛应用于管道无损检测领域。对管道微裂纹进行检出与定位可以有效避免因损伤扩展造成的安全隐患。但传统的超声无损检测技术是利用超声波传播过程中遇到缺陷时声波的反射、散射等线性特征进行缺陷检测,难以对尺寸小于检测声波波长二分之一的缺陷及与周围介质的声阻抗差别小的缺陷进行有效检测。为了对管道微裂纹进行有效检测,可采用非线性超声检测技术。非线性超声检测技术能够从本质上反映材料微小缺陷对超声波传播过程的影响,可检测出传统超声检测不可检的微小缺陷。As an important branch in the field of non-destructive testing, ultrasonic guided wave testing technology has been widely used in the field of non-destructive testing of pipelines in recent years. Detecting and locating micro-cracks in pipelines can effectively avoid potential safety hazards caused by damage expansion. However, the traditional ultrasonic nondestructive testing technology is to use the linear features such as reflection and scattering of sound waves to detect defects during the ultrasonic propagation process. Small defects can be effectively detected. In order to effectively detect pipeline micro-cracks, nonlinear ultrasonic testing technology can be used. Non-linear ultrasonic testing technology can essentially reflect the influence of small defects in materials on the ultrasonic propagation process, and can detect small defects that cannot be detected by traditional ultrasonic testing.

由于在发射/接收系统(如放大器,换能器和耦合介质)中不可避免地会出现非线性失真,因此在实践中,非线性高次谐波法会由于测试系统引起的非线性出现虚警等问题。为克服这些局限性,可采用非线性超声混频检测技术,混频检测技术基于以下事实:当两列波在含有闭合裂纹等非线性源的非线性区域内相遇时,将发生相互作用,在频域内会观察到新的频率成分。由此可实现对材料损伤的检出,并且可以通过控制波混位置,对新的频率成分进行相应分析,实现对材料损伤情况的定位。Since nonlinear distortions inevitably occur in transmit/receive systems such as amplifiers, transducers, and coupling media, in practice, the nonlinear high-harmonic method will give false alarms due to nonlinearities caused by the test system And other issues. To overcome these limitations, nonlinear ultrasonic mixing detection techniques can be employed, which are based on the fact that when two waves meet in a nonlinear region containing nonlinear sources such as closed cracks, an interaction occurs, and the New frequency components are observed in the frequency domain. In this way, the detection of material damage can be realized, and the new frequency components can be analyzed correspondingly by controlling the wave mixing position, so as to realize the location of the material damage.

在管道上进行非线性超声混频检测,可以使用电磁超声换能器(EMAT),EMAT是非接触式换能器,不需要通过耦合剂接触被测材料,抑制了额外的非线性,对被测管道试件表面上常见的包裹层及油、污垢、水、氧化物及油漆不敏感,因而适合用于管道超声检测。超声混频检测需要两个激励换能器,现有检测方法通常使用使用间隔一定距离的两个多簇线圈分别激励不同频率的两列超声波,这种结构使得整体换能装置轴向长度较长,体积较大,不同位置磁通密度差别较大。目前EMAT通常采用螺线管电磁铁或刚性永磁体提供偏置磁场,螺线管电磁铁需要额外电源且在管道结构上安装复杂,永磁体需要使用铁轭和铰链等固定装置在管道表面进行固定。由于体积大,安装较复杂,电磁铁及刚性永磁体在管道电磁超声换能器上的应用均有局限。因此,将电磁超声混频检测技术应用于管道上时,需要对激励装置进行设计。针对这一需求,本发明提出了一种适合用于曲面类管道试件的电磁超声混频激励装置。For nonlinear ultrasonic mixing testing on pipelines, electromagnetic ultrasonic transducers (EMAT) can be used. EMAT is a non-contact transducer that does not need to contact the tested material through a couplant, which suppresses additional nonlinearity. The coating and oil, dirt, water, oxides and paints commonly found on the surface of pipeline specimens are not sensitive, so they are suitable for ultrasonic testing of pipelines. Ultrasonic mixing detection requires two excitation transducers. Existing detection methods usually use two multi-cluster coils separated by a certain distance to excite two columns of ultrasonic waves of different frequencies respectively. This structure makes the overall transducer device longer in axial length. , the volume is larger, and the magnetic flux density varies greatly at different positions. At present, EMAT usually uses solenoid electromagnets or rigid permanent magnets to provide bias magnetic fields. Solenoid electromagnets require additional power and are complicated to install on the pipeline structure. Permanent magnets need to be fixed on the surface of the pipeline with fixing devices such as iron yokes and hinges. . Due to its large size and complicated installation, the applications of electromagnets and rigid permanent magnets in pipeline electromagnetic ultrasonic transducers are limited. Therefore, when the electromagnetic ultrasonic mixing detection technology is applied to the pipeline, the excitation device needs to be designed. In response to this demand, the present invention proposes an electromagnetic-ultrasonic mixing excitation device suitable for curved-surface pipeline specimens.

发明内容SUMMARY OF THE INVENTION

本发明的目的为设计一种安装拆卸便捷,结构简单紧凑,体积较小,具有柔性,能适应弯曲表面及狭窄环境,可以对管道微裂纹进行有效检出与定位的电磁超声管道导波混频激励装置。The purpose of the present invention is to design an electromagnetic ultrasonic pipeline guided wave mixing with convenient installation and disassembly, simple and compact structure, small volume, flexibility, adaptability to curved surfaces and narrow environments, and effective detection and positioning of pipeline micro-cracks. Incentive device.

为实现上述目的,本发明采用的技术方案是:For achieving the above object, the technical scheme adopted in the present invention is:

一种用于管道导波混频检测的电磁超声激励装置,包括由柔性制版技术制作的双层电路板、片状橡胶钕铁硼磁体,双层柔性印刷电路板的底层和顶层所印制的回折型多簇线圈的相邻簇线间距不同,顶层和底层线圈中心在同一位置;双层柔性印刷电路板粘贴在片状橡胶钕铁硼磁体的一面上,检测时双层柔性印刷电路板位于磁体与待检测试件外表面之间。An electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection, comprising a double-layer circuit board made by flexible plate-making technology, a sheet rubber NdFeB magnet, and a double-layer flexible printed circuit board printed on the bottom layer and the top layer. The distance between the adjacent cluster lines of the back-folded multi-cluster coils is different, and the top and bottom coil centers are in the same position; the double-layer flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet, and the double-layer flexible printed circuit board is located at the detection time. Between the magnet and the outer surface of the test piece to be tested.

所述片状橡胶钕铁硼磁体是以橡胶作为粘结剂,钕铁硼粉末为填料并进行厚度方向充磁的柔性片状永磁材料,上表面极性单一,下表面极性单一。与柔性印刷电路板粘接为一体并包覆于管道时可提供沿管道径向的磁感应强度。磁体的沿轴向的宽度大于双层柔性印刷电路板的宽度,使电路板上的线圈完全置于磁场中,优选顶层与底层线圈的上下设置可以适应单一方向充磁磁体宽度不能大于50mm的磁体尺寸。The sheet-shaped rubber NdFeB magnet is a flexible sheet-shaped permanent magnet material that uses rubber as a binder, NdFeB powder as a filler and is magnetized in the thickness direction. The upper surface has a single polarity and the lower surface has a single polarity. It can provide magnetic induction along the radial direction of the pipe when it is bonded to the flexible printed circuit board and wrapped around the pipe. The axial width of the magnet is larger than the width of the double-layer flexible printed circuit board, so that the coil on the circuit board is completely placed in the magnetic field. size.

双层柔性印刷电路板的每层线圈相邻簇间所通电流方向相反,顶层线圈与底层线圈分别通入不同频率的激励电流信号,每层线圈的相邻簇间距均为对应激励频率下所需模态导波波长λ的一半。The direction of current passing between adjacent clusters of each layer of the double-layer flexible printed circuit board is opposite, the top coil and the bottom coil are respectively fed with excitation current signals of different frequencies, and the distance between adjacent clusters of each layer of coils is the same as that at the corresponding excitation frequency. Half of the modal guided wave wavelength λ is required.

本发明的检测过程是:The detection process of the present invention is:

根据被测试件的频散曲线选定当前被测试件的某种模态导波作为激励信号:纵向模态导波具有多模态和频散特性,在管道中激发纵向导波时,在低频段有L(0,1)与L(0,2)模态共存,在同一频率下换能器会同时激发这2种波模态,视具体管道频散曲线确定某一种模态为所需模态。当某簇线圈所激发的振动以相速度cp传播至λ/2远处时,即可与相邻簇线圈引发的同向质点振动产生相长干涉,使所需模态导波强度增大,并抑制其他模态导波。According to the dispersion curve of the tested piece, a certain modal guided wave of the tested piece is selected as the excitation signal: the longitudinal modal guided wave has multi-modal and dispersion characteristics. There are L(0,1) and L(0,2) modes coexisting in the frequency band. At the same frequency, the transducer will excite these two wave modes at the same time. Depending on the specific pipeline dispersion curve, a certain mode is determined as the desired mode. Modal required. When the vibration excited by a cluster coil propagates to a distance of λ/2 at the phase velocity c p , it can constructively interfere with the vibration of the same direction particle caused by the adjacent cluster coil, so that the required modal guided wave intensity increases , and suppress other modal guided waves.

进行检测时将柔性印刷电路板粘贴在片状橡胶钕铁硼磁体的一面上,以多簇线圈沿周向展开的形式包覆在被测试件上,柔性印刷电路板位于磁体与管道外表面之间,顶层与底层的回折线圈间隔一段时间分别通入不同频率的交变电流,交变电流在试件中感应出涡流,在橡胶钕铁硼磁体提供的偏置磁场下产生交变的洛伦兹力引发质点振动,振动会以纵向导波的形式沿管道轴向传播,从而产生两列导波;When testing, the flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet, and wrapped around the test piece in the form of multi-cluster coils unfolding in the circumferential direction. The flexible printed circuit board is located between the magnet and the outer surface of the pipe. During the period, alternating currents of different frequencies are respectively fed into the top and bottom layers at intervals of time. The alternating current induces eddy currents in the specimen and generates alternating Loran under the bias magnetic field provided by the rubber NdFeB magnets. This force induces particle vibration, and the vibration propagates along the axis of the pipeline in the form of longitudinal guided waves, resulting in two columns of guided waves;

线圈中所通入的电流是正弦脉冲信号,顶层线圈通入频率为f1的激励电流,底层线圈通入频率为f2的激励电流,两层线圈激励的导波的群速度分别为c1和c2,群速度是波的包络传播的速度,根据群速度通过控制两层线圈中通入激励电流的时间差即可使两列波同时到达管道某一位置。The current passed into the coil is a sinusoidal pulse signal. The top coil is fed with an excitation current of frequency f 1 , the bottom coil is fed with an excitation current of frequency f 2 , and the group velocities of the guided waves excited by the two-layer coils are c 1 respectively. and c 2 , the group velocity is the velocity of the envelope propagation of the wave. According to the group velocity, the two waves can reach a certain position of the pipeline at the same time by controlling the time difference of the excitation current in the two layers of coils.

如果管道中没有微裂纹,则不会有和频、差频非线性分量的出现;如果中存在微裂纹,则会出现两个基频的和频、差频分量,当两列波同时到达了微裂纹位置,此时的和频、差频分量幅值最大,据此,可以完成对微裂纹的检出与定位。If there are no micro-cracks in the pipeline, there will be no nonlinear components of sum and difference frequencies; if there are micro-cracks, the sum and difference components of the two fundamental frequencies will appear. When the two waves arrive at the same time At the position of the micro-crack, the amplitudes of the sum-frequency and difference-frequency components are the largest at this time, according to which, the detection and positioning of the micro-crack can be completed.

本发明与现有技术相比,具有以下优点和突出性效果:Compared with the prior art, the present invention has the following advantages and outstanding effects:

1)本发明中超声混频非线性检测所需的两个基频信号分别由顶层与底层的线圈激发,相较于平行放置的双激发换能器混频检测方式,轴向长度很小,有利于混频激励装置的小型化,且在磁体下方的区域内线圈不同簇位置磁通密度差别小。超声混频非线性检测可以对微裂纹进行有效检测,并对系统非线性不敏感,混频技术还可以通过采用不同延时控制两列波混合的位置对区域进行扫查,本发明安装与拆卸比较便捷,且对换能器体积控制较好,具有超声混频检测的优势,又对其短板进行了较好的控制。1) In the present invention, the two fundamental frequency signals required for the nonlinear detection of ultrasonic mixing are respectively excited by the coils on the top layer and the bottom layer. Compared with the dual-excitation transducer mixing detection method placed in parallel, the axial length is very small, It is beneficial to the miniaturization of the frequency mixing excitation device, and the difference in magnetic flux density between different cluster positions of the coil is small in the area below the magnet. The ultrasonic mixing nonlinear detection can effectively detect micro-cracks, and is not sensitive to the nonlinearity of the system. The mixing technology can also scan the area by using different delays to control the position where the two waves are mixed. The installation and disassembly of the present invention It is more convenient, and has better control over the volume of the transducer, has the advantages of ultrasonic mixing detection, and has better control over its shortcomings.

2)本发明针对管道的弯曲曲面设计,片状橡胶钕铁硼磁体具有轻薄柔性特点,与刚性永磁体相比不需要笨重的紧固件即可包覆于管道表面,不需要进行打磨等表面处理即可以和各种管径的试件良好贴合。此外磁体和电路板柔性的设计使其能够良好贴合在任意待测试件上,可以在周向上包裹管道侧面,也可以包裹周向非封闭的弯曲面。2) The present invention is designed for the curved surface of the pipeline. The sheet rubber NdFeB magnet has the characteristics of lightness, thinness and flexibility. Compared with the rigid permanent magnet, it can be covered on the surface of the pipeline without heavy fasteners, and the surface does not need to be polished. After processing, it can fit well with specimens of various pipe diameters. In addition, the flexible design of the magnet and the circuit board enables it to fit well on any piece to be tested. It can wrap the side of the pipe in the circumferential direction, or wrap the non-closed curved surface in the circumferential direction.

3)回折型多簇线圈相邻簇间距等于激励频率下所需模态导波的半波长,可以提高每个线圈激励频率下所需模态导波振动强度,并抑制产生其他模态,使混频波信号接收效果更好;回折型多簇线圈通过柔性印刷电路板的方式制作,与缠绕导线相比成本低,且便于精确地控制线圈相邻簇间距,使用时不需要绕制,直接随橡胶永磁体贴合于管道表面即可,便于安装与拆卸。3) The distance between adjacent clusters of the turn-back multi-cluster coil is equal to the half wavelength of the required modal guided wave at the excitation frequency, which can improve the vibration intensity of the required modal guided wave at the excitation frequency of each coil, and suppress the generation of other modes, so that the The mixing wave signal reception effect is better; the folded-back multi-cluster coil is made by a flexible printed circuit board, which is low in cost compared with winding wires, and it is easy to accurately control the spacing between adjacent clusters of the coil. It can be attached to the surface of the pipe with the rubber permanent magnet, which is convenient for installation and disassembly.

4)所采用的双层柔性印刷电路板的总厚度为0.13mm+/-0.03mm比一般的双层PCB版薄,线圈提离距离短,激励效果较好,且其底层与顶层距离很小,因此位于每层的线圈激励效果相近。4) The total thickness of the double-layer flexible printed circuit board used is 0.13mm+/-0.03mm, which is thinner than the general double-layer PCB version, the coil lift-off distance is short, the excitation effect is better, and the distance between the bottom layer and the top layer is very small, Therefore, the excitation effect of the coils located in each layer is similar.

附图说明Description of drawings

图1为本发明用于管道导波混频检测的电磁超声激励装置安装在管道上的结构示意图;1 is a schematic structural diagram of an electromagnetic ultrasonic excitation device used for pipeline guided wave mixing detection installed on a pipeline according to the present invention;

图2为本发明用于管道导波混频检测的电磁超声激励装置的激励过程原理示意图;2 is a schematic diagram of the excitation process principle of the electromagnetic ultrasonic excitation device used for pipeline guided wave mixing detection according to the present invention;

图3为本发明的双层柔性印刷电路板的打开状态示意图;3 is a schematic diagram of an open state of the double-layer flexible printed circuit board of the present invention;

图4为外径45mm壁厚1mm的铝合金管道纵向模态导波的相速度和群速度频散曲线;Figure 4 shows the phase velocity and group velocity dispersion curves of the longitudinal modal guided wave of an aluminum alloy pipe with an outer diameter of 45mm and a wall thickness of 1mm;

图5为激励频率为900kHz与1300kHz时接收信号;Figure 5 shows the received signal when the excitation frequency is 900kHz and 1300kHz;

图6为接收信号频域图;6 is a frequency domain diagram of a received signal;

图7为本发明装置应用于非封闭曲面被测试件的示意图;7 is a schematic diagram of the device of the present invention applied to a non-closed curved surface test piece;

图中,1为磁体、2为双层柔性印刷电路板、3为试件。In the figure, 1 is a magnet, 2 is a double-layer flexible printed circuit board, and 3 is a test piece.

具体实施方式Detailed ways

下面结合实施例及附图进一步解释本发明,但并不以此作为对本申请保护范围的限定。The present invention is further explained below with reference to the embodiments and accompanying drawings, but this is not intended to limit the protection scope of the present application.

如图1所示,本发明用于管道导波混频检测的电磁超声激励装置,应用于管道导波混频检测,由片状橡胶钕铁硼磁体1、顶层与底层分别印刷有线圈的双层柔性印刷电路板2构成;进行检测时将双层柔性印刷电路板粘贴于片状橡胶钕铁硼磁体的一面,将此整体包覆于被测管道试件3外表面,使得双层柔性印刷电路板的多簇线圈沿周向展开,磁体的沿轴向的宽度大于双层柔性印刷电路板的宽度,使双层柔性印刷电路板上的线圈完全置于磁场中。线圈采用回折型多簇线圈形式,位于顶层与底层的回折线圈中心位置相同,即两层线圈打开状态时同轴线,两层线圈的整体宽度可以不同,但上下印制在电路板上时轴线对齐,也就是中心位置相同。顶层线圈和底层线圈分别通入不同频率的交变电流,利用激励源的双输出通道和输出延迟功能激发出两列纵向导波。通过控制两层线圈中通入激励电流的时间差即可使两列波同时到达管道某一位置,采用一系列延时控制两列波混合的位置,观察和频、差频分量幅值,从而对区域进行扫查。As shown in Figure 1, the electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection of the present invention is applied to pipeline guided wave mixing detection. Layer flexible printed circuit board 2 is formed; when testing, the double-layer flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet, and the whole is covered on the outer surface of the pipeline test piece 3 to be tested, so that the double-layer flexible printed circuit board is printed The multi-cluster coils of the circuit board are extended in the circumferential direction, and the axial width of the magnet is larger than the width of the double-layer flexible printed circuit board, so that the coils on the double-layer flexible printed circuit board are completely placed in the magnetic field. The coils are in the form of foldback multi-cluster coils, and the center positions of the foldback coils on the top layer and the bottom layer are the same, that is, when the two layers of coils are open, they are coaxial, and the overall width of the two layers of coils can be different, but when the upper and lower layers are printed on the circuit board, the axis Aligned, that is, the same center position. The top coil and the bottom coil are respectively fed with alternating currents of different frequencies, and two columns of longitudinal guided waves are excited by the dual output channels and output delay function of the excitation source. By controlling the time difference between the excitation currents in the two-layer coils, the two waves can reach a certain position of the pipeline at the same time. A series of delays are used to control the mixing position of the two waves, and the amplitudes of the sum frequency and difference frequency components can be observed to determine the Scan the area.

如图2所示,为本发明用于管道导波混频检测的电磁超声激励装置的激励原理示意图。印刷于双层电路板的底层与顶层的线圈分别通入高频大功率激发电流Jm1和Jm2,其中Jm1频率较高。如图2中(a),先激发电流Jm1,在管道趋肤深度内感生出涡流Je1,涡流在磁场的作用下将受到洛伦兹力的作用,引发表面质点的高频振动产生一列纵向导波。如图2中(b),一段时延后激发电流Jm2,感生出涡流Je2,同理得到第二列纵向导波,第二列纵向导波将与第一列纵向导波在某位置相遇,通过控制通入两组线圈激发电流Jm1和Jm2的时间差控制波混合的位置。As shown in FIG. 2 , it is a schematic diagram of the excitation principle of the electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection according to the present invention. The coils printed on the bottom layer and the top layer of the double-layer circuit board are respectively supplied with high-frequency and high-power excitation currents J m1 and J m2 , wherein the frequency of J m1 is higher. As shown in (a) in Figure 2, the current J m1 is first excited, and the eddy current J e1 is induced in the skin depth of the pipeline. The eddy current will be affected by the Lorentz force under the action of the magnetic field, causing the high-frequency vibration of the surface particles to generate a series of Longitudinal guided waves. As shown in (b) in Figure 2, after a period of time delay, the current J m2 is excited, and the eddy current J e2 is induced. Similarly, the second row of longitudinal guided waves will be obtained. The second row of longitudinal guided waves will be at a certain position with the first row of longitudinal guided waves. When they meet, the position of the wave mixing is controlled by controlling the time difference between the excitation currents J m1 and J m2 of the two sets of coils.

双层柔性印刷电路板结构如图3所示,图中双层柔性印刷电路板整体为4,印刷于底层的回折型线圈即底层线圈为5,印刷于顶层的回折型线圈即顶层线圈为6,每层线圈的相邻簇间距均为对应激励频率下所需模态导波波长λ的一半,即cp/2f,其中cp为导波的相速度,f为导波的频率。顶层线圈和底层线圈的相邻簇间距不等。The structure of the double-layer flexible printed circuit board is shown in Figure 3. In the figure, the double-layer flexible printed circuit board as a whole is 4, the back-folded coil printed on the bottom layer, that is, the bottom coil is 5, and the back-folded coil printed on the top layer, that is, the top coil is 6. , the adjacent cluster spacing of each layer of coils is half of the required modal guided wave wavelength λ at the corresponding excitation frequency, that is, cp /2f, where cp is the phase velocity of the guided wave, and f is the frequency of the guided wave. The top and bottom coils have unequal spacing between adjacent clusters.

图7所示,被测试件为半圆管壁试件,如2为双层柔性印刷电路板,3为被测试件。As shown in FIG. 7 , the test piece is a semicircular tube wall test piece, such as 2 is a double-layer flexible printed circuit board, and 3 is a test piece.

实施例:Example:

以检测外径45mm壁厚1mm的6061铝合金管道微裂纹为例。Take the detection of microcracks in 6061 aluminum alloy pipes with an outer diameter of 45mm and a wall thickness of 1mm as an example.

图4为外径45mm壁厚1mm的6061铝合金管道纵向模态导波的相速度和群速度频散曲线。根据管道的频散曲线,L(0,2)模态导波在较低频率下有几乎非频散的特性,使得信号的解释更加容易,且其传播速度快,易与其他模态区分,故采用L(0,2)模态导波作为激励信号。根据频散曲线,0.9MHz的L(0,2)模态导波的相速度为5288m/s,故其波长λ1为5.876mm,半波长为2.938mm,1.3MHz的L(0,2)模态导波的相速度为5192m/s,波长λ2为3.994mm,半波长为1.997mm。双层柔性印刷电路板顶层线圈的相邻簇线间距为2.938mm,底层线圈的相邻簇线间距为1.997mm,均为12簇线圈,线圈的单簇长度为125mm,接近管直径,忽略端部连接细节后可认为绕管道一周。为了较强的激励效果,顶层线圈通入0.9MHz的激励信号,底层线圈通入1.3MHz的激励信号。Figure 4 shows the phase velocity and group velocity dispersion curves of the longitudinal modal guided waves of a 6061 aluminum alloy pipe with an outer diameter of 45mm and a wall thickness of 1mm. According to the dispersion curve of the pipeline, the L(0,2) mode guided wave has almost non-dispersive characteristics at lower frequencies, which makes the interpretation of the signal easier, and its propagation speed is fast and easy to distinguish from other modes. Therefore, the L(0,2) modal guided wave is used as the excitation signal. According to the dispersion curve, the phase velocity of the L(0,2) mode guided wave at 0.9MHz is 5288m/s, so its wavelength λ1 is 5.876mm , the half wavelength is 2.938mm, and the L(0,2) at 1.3MHz The phase velocity of the modal guided wave is 5192 m/s, the wavelength λ 2 is 3.994 mm, and the half wavelength is 1.997 mm. The spacing between adjacent cluster lines of the top coil of the double-layer flexible printed circuit board is 2.938mm, and the spacing between adjacent cluster lines of the bottom coil is 1.997mm, both of which are 12-cluster coils. It can be considered as a circle around the pipe after connecting the details. For a strong excitation effect, the top coil is connected to a 0.9MHz excitation signal, and the bottom coil is connected to a 1.3MHz excitation signal.

双层柔性印刷电路板使用0.5OZ覆铜,这种叠层结构的总厚度为0.13mm+/-0.03mm,而顶层与底层的距离约为0.074mm。片状橡胶钕铁硼磁体厚度为5mm,宽度为50mm,长度为140mm,下表面为N极,剩余磁通密度800mT。The double layer flexible printed circuit board uses 0.5OZ copper cladding, the total thickness of this laminated structure is 0.13mm+/-0.03mm, and the distance between the top layer and the bottom layer is about 0.074mm. The thickness of the sheet rubber NdFeB magnet is 5mm, the width is 50mm, the length is 140mm, the lower surface is N pole, and the residual magnetic flux density is 800mT.

在检测时设双层柔性印刷电路板上的印制线圈中心位置为0,超声接收探头位置在300mm处。激励装置与接收探头之间某处存在微裂纹。根据群速度频散曲线,1.3MHz的L(0,2)模态导波的群速度为4799m/s,0.9MHz的L(0,2)模态导波的群速度为5139m/s,故底层线圈激励信号不设延时,顶层线圈激励信号延时时间为t,以两列波在接收探头位置相遇时的延时为最大延时,根据计算,最大延时为4.1微秒,为实现损伤定位,采用从0到4.1微秒之间不同延时对区域进行扫查,采用的扫查时间步长越小则定位精度越高。实验中以0.455微秒时间步长进行扫查,则扫查次数为10,误差为±16.7mm,实验中第5次扫查,即延时时间t为2.275微秒时,和频、差频分量幅值之和最大。经过计算可知微裂纹位置在167mm±16.7mm处。实际测量后裂纹在163mm处,在设计误差范围内。图5为延时时间t为2.275微秒时的接收信号,时间中包括了波在超声接收探头(超声接收探头不属于本申请激励装置,属于外接设备)中的传播时间。图6为对此接收信号进行傅里叶变换后的频域图,其中7和8是0.9MHz与1.3MHz基频分量,9是两个基频的差频分量,10是两个基频的和频分量。上述实例佐证本发明可以完成对微裂纹的检出与定位。During detection, the center position of the printed coil on the double-layer flexible printed circuit board is set to 0, and the position of the ultrasonic receiving probe is set to 300mm. There is a microcrack somewhere between the excitation device and the receiving probe. According to the group velocity dispersion curve, the group velocity of the L(0,2) mode guided wave at 1.3MHz is 4799m/s, and the group velocity of the L(0,2) mode guided wave at 0.9MHz is 5139m/s, so There is no delay for the excitation signal of the bottom coil, and the delay time of the excitation signal of the top coil is t. The maximum delay is the delay when the two waves meet at the receiving probe position. According to the calculation, the maximum delay is 4.1 microseconds. For damage location, different delays from 0 to 4.1 microseconds are used to scan the area. The smaller the scan time step used, the higher the location accuracy. In the experiment, the scan was performed with a time step of 0.455 microseconds, the number of scans was 10, and the error was ±16.7mm. The fifth scan in the experiment, that is, when the delay time t was 2.275 microseconds, the sum frequency and difference frequency The sum of the magnitudes of the components is the largest. After calculation, it can be known that the position of the micro-crack is at 167mm±16.7mm. After the actual measurement, the crack is at 163mm, which is within the design error range. Figure 5 shows the received signal when the delay time t is 2.275 microseconds, and the time includes the propagation time of the wave in the ultrasonic receiving probe (the ultrasonic receiving probe does not belong to the excitation device of the present application, but belongs to an external device). Figure 6 is the frequency domain diagram after Fourier transform of the received signal, in which 7 and 8 are the 0.9MHz and 1.3MHz fundamental frequency components, 9 is the difference frequency component of the two fundamental frequencies, and 10 is the two fundamental frequencies. and frequency components. The above examples prove that the present invention can complete the detection and localization of micro-cracks.

本发明未述及之处适用于现有技术。What is not described in the present invention applies to the prior art.

Claims (7)

1.一种用于管道导波混频检测的电磁超声激励装置,其特征在于,该装置包括由柔性制版技术制作的双层柔性印刷电路板和片状橡胶钕铁硼磁体,双层柔性印刷电路板的底层和顶层所印制的回折型多簇线圈的相邻簇线间距不同,顶层和底层线圈中心在同一位置;双层柔性印刷电路板粘贴在片状橡胶钕铁硼磁体的一面上,检测时双层柔性印刷电路板位于磁体与被测试件外表面之间。1. an electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection, characterized in that the device comprises a double-layer flexible printed circuit board and a sheet rubber NdFeB magnet made by flexographic plate-making technology, and the double-layer flexible printing The back-folded multi-cluster coils printed on the bottom and top layers of the circuit board have different spacings between adjacent cluster lines, and the top and bottom coil centers are in the same position; the double-layer flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet , the double-layer flexible printed circuit board is located between the magnet and the outer surface of the test piece during detection. 2.根据权利要求1所述的装置,其特征在于,所述片状橡胶钕铁硼磁体是以橡胶作为粘结剂,钕铁硼粉末为填料并进行厚度方向充磁的柔性片状永磁材料。2 . The device according to claim 1 , wherein the sheet-like rubber NdFeB magnet is a flexible sheet-like permanent magnet with rubber as a binder and NdFeB powder as a filler and magnetized in the thickness direction. 3 . Material. 3.根据权利要求1所述的装置,其特征在于,磁体的沿轴向的宽度大于双层柔性印刷电路板的宽度,使双层柔性印刷电路板上的线圈完全置于磁场中。3 . The device according to claim 1 , wherein the width of the magnet in the axial direction is larger than the width of the double-layer flexible printed circuit board, so that the coils on the double-layer flexible printed circuit board are completely placed in the magnetic field. 4 . 4.根据权利要求1所述的装置,其特征在于,双层柔性印刷电路板的每层线圈相邻簇间所通电流方向相反,顶层线圈与底层线圈分别通入不同频率的激励电流信号,每层线圈的相邻簇间距均为对应激励频率下所需模态导波波长λ的一半。4. The device according to claim 1, wherein the direction of current passing between adjacent clusters of each layer of coils of the double-layer flexible printed circuit board is opposite, and the top coil and the bottom coil are respectively connected to excitation current signals of different frequencies, The spacing between adjacent clusters of each layer of coils is half of the required modal guided wave wavelength λ at the corresponding excitation frequency. 5.根据权利要求1所述的装置,其特征在于,所述双层柔性印刷电路板的总厚度为0.13mm+/-0.03mm;顶层线圈与底层线圈的距离为0.074mm。5 . The device according to claim 1 , wherein the total thickness of the double-layer flexible printed circuit board is 0.13mm+/-0.03mm; the distance between the top coil and the bottom coil is 0.074mm. 6 . 6.根据权利要求1所述的装置,其特征在于,检测过程是:获取被测试件的频散特性,确定该待检测试件的某一种纵向模态为所需模态,根据被测试件的频散曲线选定当前被测试件的某种模态导波作为激励信号;6 . The device according to claim 1 , wherein the detection process is: obtaining the frequency dispersion characteristics of the test piece, determining that a certain longitudinal mode of the test piece to be tested is the required mode, and according to the test piece. 7 . The dispersion curve of the component selects a certain modal guided wave of the current tested component as the excitation signal; 进行检测时将双层柔性印刷电路板粘贴在片状橡胶钕铁硼磁体的一面上,以多簇线圈沿周向展开的形式包覆在被测试件上,柔性印刷电路板位于磁体与被测试件外表面之间,顶层与底层的回折线圈间隔一段时间分别通入不同频率的交变电流,交变电流在试件中感应出涡流,在橡胶钕铁硼磁体提供的偏置磁场下产生交变的洛伦兹力引发质点振动,振动会以纵向导波的形式沿管道轴向传播,从而产生两列导波;When testing, the double-layer flexible printed circuit board is pasted on one side of the sheet rubber NdFeB magnet, and wrapped around the test piece in the form of multi-cluster coils unfolding in the circumferential direction. The flexible printed circuit board is located between the magnet and the test piece. Between the outer surfaces of the specimens, alternating currents of different frequencies are respectively fed into the top and bottom folded coils for a period of time. The variable Lorentz force causes particle vibration, and the vibration will propagate along the pipe axis in the form of longitudinal guided waves, thereby generating two columns of guided waves; 线圈中所通入的电流是正弦脉冲信号,顶层线圈通入频率为f1的激励电流,底层线圈通入频率为f2的激励电流,两层线圈激励的导波的群速度分别为c1和c2,根据群速度设定两层线圈中通入激励电流的时间差,在该时间差下使两列波同时到达管道某一位置;The current passed into the coil is a sinusoidal pulse signal. The top coil is fed with an excitation current of frequency f 1 , the bottom coil is fed with an excitation current of frequency f 2 , and the group velocities of the guided waves excited by the two-layer coils are c 1 respectively. and c 2 , according to the group velocity, set the time difference of the excitation current in the two layers of coils, and make the two waves reach a certain position of the pipeline at the same time under this time difference; 如果管道中没有微裂纹,则不会有和频、差频非线性分量的出现;如果中存在微裂纹,则会出现两个基频的和频、差频分量,当两列波同时到达了微裂纹位置,此时的和频、差频分量幅值最大,据此,能完成对微裂纹的检出与定位。If there are no micro-cracks in the pipeline, there will be no nonlinear components of sum and difference frequencies; if there are micro-cracks, the sum and difference components of the two fundamental frequencies will appear. When the two waves arrive at the same time At the position of the micro-crack, the amplitudes of the sum-frequency and difference-frequency components are the largest at this time, according to which, the detection and positioning of the micro-crack can be completed. 7.根据权利要求1所述的装置,其特征在于,所述被测试件为管道、非封闭的弯曲面。7 . The device according to claim 1 , wherein the tested piece is a pipe, a non-closed curved surface. 8 .
CN202011151891.2A 2020-10-23 2020-10-23 Electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection Active CN112147235B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011151891.2A CN112147235B (en) 2020-10-23 2020-10-23 Electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011151891.2A CN112147235B (en) 2020-10-23 2020-10-23 Electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection

Publications (2)

Publication Number Publication Date
CN112147235A true CN112147235A (en) 2020-12-29
CN112147235B CN112147235B (en) 2024-07-09

Family

ID=73954907

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011151891.2A Active CN112147235B (en) 2020-10-23 2020-10-23 Electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection

Country Status (1)

Country Link
CN (1) CN112147235B (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113466347A (en) * 2021-06-16 2021-10-01 西安交通大学 Semi-flexible electromagnetic ultrasonic probe for detecting defects of pipeline type components
CN114113337A (en) * 2021-12-07 2022-03-01 西安交通大学 Electromagnetic ultrasonic flexible array probe for detecting defects of curved surface structure and detection method
CN119492801A (en) * 2024-11-29 2025-02-21 北京交通大学 Axle defect detection guided wave transducer and axle defect detection device
CN119972487A (en) * 2025-04-14 2025-05-13 西南交通大学 A piezoelectric transducer and method for directional excitation and reception of non-dispersive torsional guided waves

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB0109440D0 (en) * 1999-02-02 2001-06-06 Csi Technology Inc Enhanced detection of vibration
KR100430385B1 (en) * 2003-06-04 2004-05-10 (주) 이우티이씨 A magnetic locator for locating buried objects by using magnetic markers
US20090078049A1 (en) * 2007-09-25 2009-03-26 The Regents Of The University Of California Non-contact feature detection using ultrasonic lamb waves
US7560920B1 (en) * 2005-10-28 2009-07-14 Innovative Materials Testing Technologies, Inc. Apparatus and method for eddy-current scanning of a surface to detect cracks and other defects
US8013600B1 (en) * 2007-11-19 2011-09-06 Sandia Corporation Mountable eddy current sensor for in-situ remote detection of surface and sub-surface fatigue cracks
DE102011016083A1 (en) * 2011-04-05 2012-10-11 Sciknowtec Gmbh Method for transmitting modulated radio frequency (RF) signals from transmitting station through RF-proof wall to receiving station, involves transforming data signals into waveform to overcome wall by overlay/Heterodyn transponder
CN104198594A (en) * 2014-06-11 2014-12-10 北京工业大学 Multiple-main-frequency combined torsional-mode electromagnetic acoustic array sensor
CN109765562A (en) * 2018-12-10 2019-05-17 中国科学院声学研究所 A three-dimensional forward looking audio-visual sonar system and method
CN110193460A (en) * 2019-05-29 2019-09-03 北京工业大学 A kind of omni-directional magnetic concentrator formula Lamb wave electromagnetic sound transducer
CN111157628A (en) * 2020-01-22 2020-05-15 河北工业大学 An electromagnetic ultrasonic excitation device for depth stress detection
CN213302105U (en) * 2020-10-23 2021-05-28 河北工业大学 Electromagnetic ultrasonic excitation device for pipeline guided wave frequency mixing detection

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB0109440D0 (en) * 1999-02-02 2001-06-06 Csi Technology Inc Enhanced detection of vibration
KR100430385B1 (en) * 2003-06-04 2004-05-10 (주) 이우티이씨 A magnetic locator for locating buried objects by using magnetic markers
US7560920B1 (en) * 2005-10-28 2009-07-14 Innovative Materials Testing Technologies, Inc. Apparatus and method for eddy-current scanning of a surface to detect cracks and other defects
US20090078049A1 (en) * 2007-09-25 2009-03-26 The Regents Of The University Of California Non-contact feature detection using ultrasonic lamb waves
US8013600B1 (en) * 2007-11-19 2011-09-06 Sandia Corporation Mountable eddy current sensor for in-situ remote detection of surface and sub-surface fatigue cracks
DE102011016083A1 (en) * 2011-04-05 2012-10-11 Sciknowtec Gmbh Method for transmitting modulated radio frequency (RF) signals from transmitting station through RF-proof wall to receiving station, involves transforming data signals into waveform to overcome wall by overlay/Heterodyn transponder
CN104198594A (en) * 2014-06-11 2014-12-10 北京工业大学 Multiple-main-frequency combined torsional-mode electromagnetic acoustic array sensor
CN109765562A (en) * 2018-12-10 2019-05-17 中国科学院声学研究所 A three-dimensional forward looking audio-visual sonar system and method
CN110193460A (en) * 2019-05-29 2019-09-03 北京工业大学 A kind of omni-directional magnetic concentrator formula Lamb wave electromagnetic sound transducer
CN111157628A (en) * 2020-01-22 2020-05-15 河北工业大学 An electromagnetic ultrasonic excitation device for depth stress detection
CN213302105U (en) * 2020-10-23 2021-05-28 河北工业大学 Electromagnetic ultrasonic excitation device for pipeline guided wave frequency mixing detection

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
郝煜朝: "基于电磁超声导波的管道微裂纹检测", 《硕士电子期刊》, 16 January 2023 (2023-01-16), pages 3 *

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113466347A (en) * 2021-06-16 2021-10-01 西安交通大学 Semi-flexible electromagnetic ultrasonic probe for detecting defects of pipeline type components
CN114113337A (en) * 2021-12-07 2022-03-01 西安交通大学 Electromagnetic ultrasonic flexible array probe for detecting defects of curved surface structure and detection method
CN114113337B (en) * 2021-12-07 2024-02-20 西安交通大学 Electromagnetic ultrasonic flexible array probe for detecting defects of curved surface structure and detection method
CN119492801A (en) * 2024-11-29 2025-02-21 北京交通大学 Axle defect detection guided wave transducer and axle defect detection device
CN119972487A (en) * 2025-04-14 2025-05-13 西南交通大学 A piezoelectric transducer and method for directional excitation and reception of non-dispersive torsional guided waves

Also Published As

Publication number Publication date
CN112147235B (en) 2024-07-09

Similar Documents

Publication Publication Date Title
CN112147235A (en) An electromagnetic ultrasonic excitation device for pipeline guided wave mixing detection
CN107790363B (en) Array type multi-angle spiral SH guided wave electromagnetic ultrasonic transducer
Hirao et al. An SH-wave EMAT technique for gas pipeline inspection
CN101354380B (en) Vortex flow and electromagnetic ultrasonic combined type nondestructive detection method
Liu et al. Longitudinal mode magnetostrictive patch transducer array employing a multi-splitting meander coil for pipe inspection
Nakamura et al. Mode conversion and total reflection of torsional waves for pipe inspection
Liu et al. A flexible and noncontact guided-wave transducer based on coils-only EMAT for pipe inspection
Ma et al. Excitation and detection of shear horizontal waves with electromagnetic acoustic transducers for nondestructive testing of plates
Kwun et al. Long-range guided wave inspection of structures using the magnetostrictive sensor
CN104198594A (en) Multiple-main-frequency combined torsional-mode electromagnetic acoustic array sensor
CN209745873U (en) An electromagnetic-acoustic composite non-destructive testing device and system
CN106768283A (en) A kind of pipe ultrasonic guided wave on-line measuring device and detection method based on long range waveguide
CN213302105U (en) Electromagnetic ultrasonic excitation device for pipeline guided wave frequency mixing detection
CN113155977A (en) Electromagnetic ultrasonic surface wave transducer for high-temperature metal detection and detection method
CN108426948A (en) A kind of electromagnet ultrasonic changer and its working method of the single mode Lamb wave of excitation
CN109470774A (en) Ultrasonic guided wave focusing transducer based on aluminum plate defect detection
CN115824330A (en) Device and method for synchronously measuring pipeline defects and fluid flow in the pipeline
Cai et al. Enhancement of Lamb-EMAT signal using a modified one-side pitch-catch design
US20240125742A1 (en) Defect sizing combining fixed wavelength and variable wavelength guided waves
Xu et al. An improved longitudinal mode guided wave received sensor based on inverse magnetostrictive effect for open end pipes
CN208383812U (en) A kind of electromagnet ultrasonic changer exciting single mode Lamb wave
Chaboty et al. Propagation of low frequency ultrasonic guided waves through welded lap joint
Gao et al. Defect detection in the dead zone of magnetostrictive sensor for pipe monitoring
JPH0587780A (en) Method and apparatus for nondestructive inspection of metal pipes
Hou et al. Novel design of an effective pneumatic magnetostrictive patch transducer based on the ultrasonic guided wave for application of fast pipe health inspection

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant