CN103150449A - Design method of electromagnetic ultrasonic body wave transducer - Google Patents

Design method of electromagnetic ultrasonic body wave transducer Download PDF

Info

Publication number
CN103150449A
CN103150449A CN201310099541XA CN201310099541A CN103150449A CN 103150449 A CN103150449 A CN 103150449A CN 201310099541X A CN201310099541X A CN 201310099541XA CN 201310099541 A CN201310099541 A CN 201310099541A CN 103150449 A CN103150449 A CN 103150449A
Authority
CN
China
Prior art keywords
wave transducer
bulk wave
electromagnetic
electromagnetic acoustic
permanent magnet
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
CN201310099541XA
Other languages
Chinese (zh)
Other versions
CN103150449B (en
Inventor
翟国富
汪开灿
王亚坤
蒋韬
邱玉
王吉宇
蒋川流
康磊
王淑娟
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.)
Harbin Institute of Technology
Original Assignee
Harbin Institute 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 Harbin Institute of Technology filed Critical Harbin Institute of Technology
Priority to CN201310099541.XA priority Critical patent/CN103150449B/en
Publication of CN103150449A publication Critical patent/CN103150449A/en
Application granted granted Critical
Publication of CN103150449B publication Critical patent/CN103150449B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Abstract

The invention discloses a design method of an electromagnetic ultrasonic body wave transducer, relating to a design method of an electromagnetic ultrasonic body wave transducer, solving the problems of the weak excited body wave signal of the existing electromagnetic ultrasonic body wave transducer and more wave modes in the excited body wave signal. The design method comprises the main steps of: defining parameters required by modeling; establishing a geometric model of each part; setting material attributes; dividing a physical field solving region; modeling an emitting process; modeling a receiving process; partitioning a net of a finite element and solving the finite element; and finding out key parameters influencing induction voltage signal strength and sound wave mode purity in an electromagnetic ultrasonic body wave transducer coil 2, calculating a transducer parameter when the signal of the electromagnetic ultrasonic body wave transducer is strongest and the sound wave mode is optimal, and designing the electromagnetic ultrasonic body wave transducer. The design method has the characteristics that the simplicity is achieved in operation and the influence of the parameters of the electromagnetic ultrasonic body wave transducer to the induction voltage signal is easily analyzed. The design method can be widely applied to the design of the infinite element of any electromagnetic ultrasonic body wave transducer.

Description

Electromagnetic acoustic bulk wave transducer designs method
Technical field
The present invention relates to a kind of method for designing of electromagnetic acoustic bulk wave transducer.
Background technology
Electromagnetic acoustic bulk wave transducer can inspire ultrasonic bulk wave effectively in metal specimen, be widely applied in electromagnetic acoustic Non-Destructive Testing and nondestructive evaluation field.For convenience of producing and receiving the bulk wave signal, electromagnetic acoustic bulk wave transducer general work pattern is the transceiver pattern, and namely an electromagnetic acoustic bulk wave transducer not only produces bulk wave but also receive the bulk wave echoed signal.Electromagnetic acoustic bulk wave transducer winding form mainly contains three kinds of spiral winding, runway coil and butterfly shaped coilses, and multi-form coil need to be equipped with corresponding magnetic field and effectively excites bulk wave.Wherein to be equipped with the electromagnetic acoustic bulk wave transducer dimensions of cylindrical permanent magnet little, simple in structure for spiral winding, excites bulk wave to be distributed symmetrically, and uses also the most extensive.But, compare with the piezoelectric supersonic technology, the bulk wave signal that electromagnetic acoustic bulk wave transducer excites a little less than, and in the bulk wave signal that excites, wave mode is more, has affected effective judgement of flaw echoes.
Summary of the invention
The present invention is for a little less than solving existing electromagnetic acoustic bulk wave transducer and exciting the bulk wave signal and excite the more problem of wave mode in the bulk wave signal, and a kind of electromagnetic acoustic bulk wave transducer designs method that proposes.
The present invention solves the problems of the technologies described above the technical scheme of taking to be:
A kind of electromagnetic acoustic bulk wave transducer designs method, described method for designing are based on that the transducer model that comprises permanent magnet, electromagnet ultrasonic changer coil, metal specimen to be measured, refinement layer, defective and air far field carries out; Described permanent magnet is cylindrical permanent magnet; Described electromagnet ultrasonic changer coil is helical coil structure, is used for producing in metal specimen and receiving bulk wave; Described refinement layer is positioned at electromagnetic acoustic bulk wave transducer winding below metal specimen to be measured; Described defective is cylindrical defective, is positioned at bottom metal specimen to be measured;
The detailed process of described method for designing is:
Step 1: the needed parameter of definition modeling, wherein major parameter comprises diameter d and the height h of permanent magnet, the spacing a of wire in the electromagnet ultrasonic changer coil, width w and number of turn n;
Step 2: set up the geometric model comprise permanent magnet, electromagnet ultrasonic changer coil, metal specimen, refinement layer, defective and air far field;
Step 3: set material properties; Permanent magnet is set as magnetic material; The electromagnet ultrasonic changer coil is set as enameled wire; Metal specimen is set as metal material to be measured; Refinement layer is set as metal material to be measured; Defective and air far field are set as air;
Step 4: divide the physical field Domain; Described physical field comprises that electromagnet ultrasonic changer transmits and receives two physical fields---structure field and the electromagnetic field that relates in process; Described structure field Domain comprises metal specimen and refinement layer; Described electromagnetic field Domain comprises permanent magnet, electromagnetic acoustic bulk wave transducer winding, metal specimen, refinement layer, defective and air far field;
Step 5: emission process modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet magnetic field direction is vertical direction; Described electromagnetic acoustic bulk wave transducer receiving coil passes into the Tone-Burst signal of certain frequency; Described refinement layer is the physical load applying zone of structure field, and physical load is the Lorentz force that Electromagnetic Calculation obtains;
Step 6: receiving course modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet magnetic field direction is vertical direction; Described refinement layer is the velocity response zone of electromagnetic field, and namely the ultrasonic vibration cutting magnetic line of structure field induces voltage signal in electromagnetic acoustic bulk wave transducer winding;
Step 7: finite element meshing; The ultrasonic bulk wave transducer winding of described permanent magnet electromagnetic, metal specimen, refinement layer, defective and air far field employing tetrahedron element carry out subnetting; Carry out mesh refinement during described refinement layer subnetting, increase the model computational accuracy;
Step 8: finite element solving; Described structure field and electromagnetic field adopt finite element method, calculate the induced voltage signal that causes in eddy current, Lorentz force, ultrasound wave distribution and the electromagnetic acoustic bulk wave transducer winding in metal specimen;
Step 9: the diameter d and the height h that change permanent magnet, the spacing a of wire in the electromagnet ultrasonic changer coil, width w and number of turn n, the electromagnetic acoustic bulk wave transducer of setting up different parameters transmits and receives the process complete model, and finds the solution the induced voltage signal that causes in electromagnetic acoustic bulk wave transducer winding;
Step 10: the relation of induced voltage signal intensity and acoustic wave mode purity in acquisition electromagnetic acoustic bulk wave transducer major parameter and electromagnetic acoustic bulk wave transducer winding;
Step 11: find out the key parameter that affects induced voltage signal intensity and acoustic wave mode purity in electromagnetic acoustic bulk wave transducer winding from the relation that step 10 provides, calculate the strongest and acoustic wave mode of electromagnetic acoustic bulk wave transducer signal transducer parameters when optimum, electromagnetic acoustic bulk wave transducer is designed.
The invention has the beneficial effects as follows:
The ultrasonic bulk wave transducer designs of a kind of electromagnet of the present invention method transmits and receives the process complete basis that is modeled as with electromagnetic acoustic bulk wave transducer, finally realizes the design of electromagnetic acoustic bulk wave transducer; Electromagnetic acoustic bulk wave transducer of the present invention transmits and receives the complete modeling of process and contains electromagnetic field and structure field, the description that the electromagnet ultrasonic changer course of work is accurate complete out, and modeling process is simple, can change flexibly electromagnetic acoustic bulk wave transducer parameters, induced voltage signal in electromagnetic acoustic bulk wave transducer winding 2 under calculating different parameters condition; Electromagnetic acoustic bulk wave transducer designs of the present invention can be analyzed the relation of induced voltage signal intensity and acoustic wave mode purity in electromagnetic acoustic bulk wave transducer parameters and electromagnetic acoustic bulk wave transducer winding 2, calculate the strongest and acoustic wave mode of electromagnetic acoustic bulk wave transducer signal transducer parameters when optimum, realize electromagnetic acoustic bulk wave transducer designs.The ultrasonic bulk wave transducer designs of a kind of electromagnet method that the present invention proposes has simple to operate, and is easy to analyze electromagnetic acoustic bulk wave transducer parameters to the characteristics of induced voltage signal impact.The present invention can be widely used in the Finite element design of any electromagnetic acoustic bulk wave transducer.
Description of drawings
Fig. 1 is the model schematic diagram of realizing the ultrasonic bulk wave transducer designs of the described a kind of electromagnet of the application method; Fig. 2 is the structural representation of electromagnetic acoustic bulk wave transducer winding 2, in figure * the vertical paper of expression current direction is inside, and the vertical paper of expression current direction is outside; 2-1 is respectively two groups of identical wire combinations of current direction with 2-2; Fig. 3 is the Tone-Burst signal schematic representation that electromagnetic acoustic bulk wave transducer winding 2 passes into; Fig. 4 is the induced voltage signal that in embodiment two, electromagnetic acoustic bulk wave transducer winding 2 receives; Fig. 5 is the impact of parameter analysis phase different conductor width w on the reception induced voltage in embodiment two.
Embodiment
Embodiment one: present embodiment is described in conjunction with Fig. 1 and Fig. 2, the described a kind of novel electromagnetic acoustic bulk wave transducer modeling and optimization method for designing of present embodiment, realize that described method for designing need to transmit and receive process to electromagnetic acoustic bulk wave transducer and carry out complete modeling, the accurate description electromagnetic acoustic bulk wave transducer course of work, analyze the impact that ripple signal intensity and acoustic wave mode purity are regained in different transducer parameters docking, thereby obtain the transducer parameters combination of performance parameter optimum, electromagnetic acoustic bulk wave transducer is designed; Described model mainly comprises permanent magnet 1, electromagnet ultrasonic changer coil 2, metal specimen to be measured 3, refinement layer 4, defective 5 and air far field 6; Described permanent magnet 1 is cylindrical permanent magnet; Described electromagnet ultrasonic changer coil 2 is helical coil structure, is used for producing in metal specimen 3 and receiving bulk wave; Described refinement layer 4 is positioned at electromagnetic acoustic bulk wave transducer winding 2 below metal specimen 3 to be measured; Described defective 5 is cylindrical defective, is positioned at metal specimen to be measured 3 bottoms;
The ultrasonic bulk wave transducer designs of described a kind of electromagnet process is completed by following steps:
Step 1: the needed parameter of definition modeling, wherein major parameter comprises diameter d and the height h of permanent magnet 1, the spacing a of wire in electromagnet ultrasonic changer coil 2, width w and number of turn n;
Step 2: set up the geometric model comprise permanent magnet 1, electromagnet ultrasonic changer coil 2, metal specimen 3, refinement layer 4, defective 5 and air far field 6;
Step 3: set material properties; Permanent magnet 1 is set as magnetic material; Electromagnet ultrasonic changer coil 2 is set as enameled wire; Metal specimen 3 is set as metal material to be measured; Refinement layer 4 is set as metal material to be measured; Defective 5 and air far field 6 are set as air;
Step 4: divide the physical field Domain; Described physical field comprises that electromagnet ultrasonic changer transmits and receives two physical fields---structure field and the electromagnetic field that relates in process; Described structure field Domain comprises metal specimen 3 and refinement layer 4; Described electromagnetic field Domain comprises permanent magnet 1, electromagnetic acoustic bulk wave transducer winding 2, metal specimen 3, refinement layer 4, defective 5 and air far field 6;
Step 5: emission process modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet 1 magnetic direction is vertical direction; Described electromagnetic acoustic bulk wave transducer receiving coil 2 passes into the Tone-Burst signal of certain frequency; Described refinement layer 4 is the physical load applying zone of structure field, and physical load is the Lorentz force that Electromagnetic Calculation obtains;
Step 6: receiving course modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet 1 magnetic direction is vertical direction; The velocity response zone that described refinement layer 4 is electromagnetic field, namely the ultrasonic vibration cutting magnetic line of structure field induces voltage signal in electromagnetic acoustic bulk wave transducer winding 2;
Step 7: finite element meshing; Described permanent magnet 1, electromagnetic acoustic bulk wave transducer winding 2, metal specimen 3, refinement layer 4, defective 5 and air far field 6 adopt tetrahedron elements to carry out subnetting; Carry out mesh refinement during described refinement layer 4 subnetting, increase the model computational accuracy;
Step 8: finite element solving; Described structure field and electromagnetic field adopt finite element method, calculate the induced voltage signal that causes in eddy current, Lorentz force, ultrasound wave distribution and the electromagnetic acoustic bulk wave transducer winding 2 in metal specimen 3;
Step 9: the diameter d and the height h that change permanent magnet 1, the spacing a of wire in electromagnet ultrasonic changer coil 2, width w and number of turn n, the electromagnetic acoustic bulk wave transducer of setting up different parameters transmits and receives the process complete model, and finds the solution the induced voltage signal that causes in electromagnetic acoustic bulk wave transducer winding 2;
Step 10: the relation of induced voltage signal intensity and acoustic wave mode purity in analysis electromagnetic acoustic bulk wave transducer major parameter and electromagnetic acoustic bulk wave transducer winding 2; Induced voltage signal intensity and acoustic wave mode purity are the indexs of electromagnetic acoustic bulk wave transducer; Electromagnetic acoustic bulk wave transducer major parameter is influential to these two indexs;
Step 11: find out the key parameter (some parameter in electromagnetic acoustic bulk wave transducer major parameter) that affects induced voltage signal intensity and acoustic wave mode purity in electromagnetic acoustic bulk wave transducer winding 2, calculate the strongest and acoustic wave mode of electromagnetic acoustic bulk wave transducer signal transducer parameters when optimum, electromagnetic acoustic bulk wave transducer is designed.
Embodiment two: in present embodiment, in step 5, the frequency of the Tone-Burst signal of described certain frequency is 1~10MHz.Other step is identical with embodiment one.
Embodiment: in conjunction with Fig. 1 to Fig. 5, the present embodiment is described, the present embodiment is for adopting the specific embodiment of a kind of described novel electromagnetic acoustic bulk wave transducer designs method of embodiment one;
it is the cylindrical aluminium block of 45mm that metal specimen 3 adopts thickness, permanent magnet 1 adopts NdFeB material, with the distance of electromagnetic acoustic bulk wave transducer winding 2 be 1mm, the diameter d of permanent magnet 1 is 25mm, height h is 30mm, in electromagnet ultrasonic changer coil 2, the spacing a of wire is 1mm, width w is 0.5mm, number of turn n is 16, electromagnetic acoustic bulk wave transducer winding 2 is 0.5mm apart from the distance of metal specimen 3, defective 5 is highly 15mm, width is 2mm, distance model central axis distance is 2mm, it is 10A that electromagnetic acoustic bulk wave transducer winding 2 passes into Tone Burst current signal peak value, frequency is 2MHz, pulse width is 3.5 μ s.The described modeling and optimization method for designing of the application can obtain induced voltage signal in electromagnetic acoustic bulk wave transducer winding 2 by step 1 to step 8, as shown in Figure 4.Flaw echoes 8 and the end face echoed signal 9 that electromagnetic acoustic bulk wave transducer winding 2 receives after main impact signal 7 in Fig. 4.Change conductor width w in electromagnetic acoustic bulk wave transducer winding 2, obtain the variation of induced voltage in electromagnetic acoustic bulk wave transducer winding 2 by step 9 to step 11, as shown in Figure 5.Can get conductor width w and wire pitch a ratio is less from Fig. 5, the induced voltage amplitude is larger, so electromagnetic acoustic bulk wave transducer winding 2 should adopt the thin wire producing of trying one's best.
Above content is in conjunction with concrete preferred implementation further description made for the present invention, can not assert that concrete enforcement of the present invention is confined to these explanations.For this person of an ordinary skill in the technical field, without departing from the inventive concept of the premise, can also make some simple deduction or replace, all should be considered as belonging to the definite scope of patent protection of claims that the present invention submits to.

Claims (2)

1. electromagnetic acoustic bulk wave transducer designs method, described method for designing are based on that the transducer model that comprises permanent magnet (1), electromagnet ultrasonic changer coil (2), metal specimen to be measured (3), refinement layer (4), defective (5) and air far field (6) carries out; Described permanent magnet (1) is cylindrical permanent magnet; Described electromagnet ultrasonic changer coil (2) is helical coil structure, is used for producing in metal specimen (3) and receiving bulk wave; Described refinement layer (4) is positioned at electromagnetic acoustic bulk wave transducer winding (2) below metal specimen to be measured (3); Described defective (5) is cylindrical defective, is positioned at bottom metal specimen to be measured (3);
It is characterized in that: the detailed process of described method for designing is:
Step 1: the needed parameter of definition modeling, wherein major parameter comprises diameter d and the height h of permanent magnet (1), the spacing a of wire in electromagnet ultrasonic changer coil (2), width w and number of turn n;
Step 2: set up the geometric model that comprises permanent magnet (1), electromagnet ultrasonic changer coil (2), metal specimen (3), refinement layer (4), defective (5) and air far field (6);
Step 3: set material properties; Permanent magnet (1) is set as magnetic material; Electromagnet ultrasonic changer coil (2) is set as enameled wire; Metal specimen (3) is set as metal material to be measured; Refinement layer (4) is set as metal material to be measured; Defective (5) and air far field (6) are set as air;
Step 4: divide the physical field Domain; Described physical field comprises that electromagnet ultrasonic changer transmits and receives two physical fields---structure field and the electromagnetic field that relates in process; Described structure field Domain comprises metal specimen (3) and refinement layer (4); Described electromagnetic field Domain comprises permanent magnet (1), electromagnetic acoustic bulk wave transducer winding (2), metal specimen (3), refinement layer (4), defective (5) and air far field (6);
Step 5: emission process modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet (1) magnetic direction is vertical direction; Described electromagnetic acoustic bulk wave transducer receiving coil (2) passes into the Tone-Burst signal of certain frequency; Described refinement layer (4) is the physical load applying zone of structure field, and physical load is the Lorentz force that Electromagnetic Calculation obtains;
Step 6: receiving course modeling; The initial magnetic vector potential of described electromagnetic field Domain is 0; Described structure field Domain initial displacement and initial velocity are 0; Described permanent magnet (1) magnetic direction is vertical direction; Described refinement layer (4) is the velocity response zone of electromagnetic field, and namely the ultrasonic vibration cutting magnetic line of structure field induces voltage signal in electromagnetic acoustic bulk wave transducer winding (2);
Step 7: finite element meshing; Described permanent magnet (1), electromagnetic acoustic bulk wave transducer winding (2), metal specimen (3), refinement layer (4), defective (5) and air far field (6) adopt tetrahedron element to carry out subnetting; Carry out mesh refinement during described refinement layer (4) subnetting, increase the model computational accuracy;
Step 8: finite element solving; Described structure field and electromagnetic field adopt finite element method, calculate the induced voltage signal that causes in eddy current, Lorentz force, ultrasound wave distribution and the electromagnetic acoustic bulk wave transducer winding (2) in metal specimen (3);
Step 9: the diameter d and the height h that change permanent magnet (1), the spacing a of wire in electromagnet ultrasonic changer coil (2), width w and number of turn n, the electromagnetic acoustic bulk wave transducer of setting up different parameters transmits and receives the process complete model, and finds the solution the induced voltage signal that causes in electromagnetic acoustic bulk wave transducer winding (2);
Step 10: the relation that obtains the middle induced voltage signal intensity of electromagnetic acoustic bulk wave transducer major parameter and electromagnetic acoustic bulk wave transducer winding (2) and acoustic wave mode purity;
Step 11: find out the key parameter that affects the middle induced voltage signal intensity of electromagnetic acoustic bulk wave transducer winding (2) and acoustic wave mode purity from the relation that step 10 provides, calculate the strongest and acoustic wave mode of electromagnetic acoustic bulk wave transducer signal transducer parameters when optimum, electromagnetic acoustic bulk wave transducer is designed.
2. a kind of electromagnetic acoustic bulk wave transducer designs method according to claim 1, it is characterized in that: in step 5, the frequency of the Tone-Burst signal of described certain frequency is 1~10MHz.
CN201310099541.XA 2013-03-26 2013-03-26 Design method of electromagnetic ultrasonic body wave transducer Expired - Fee Related CN103150449B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310099541.XA CN103150449B (en) 2013-03-26 2013-03-26 Design method of electromagnetic ultrasonic body wave transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310099541.XA CN103150449B (en) 2013-03-26 2013-03-26 Design method of electromagnetic ultrasonic body wave transducer

Publications (2)

Publication Number Publication Date
CN103150449A true CN103150449A (en) 2013-06-12
CN103150449B CN103150449B (en) 2015-10-07

Family

ID=48548525

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310099541.XA Expired - Fee Related CN103150449B (en) 2013-03-26 2013-03-26 Design method of electromagnetic ultrasonic body wave transducer

Country Status (1)

Country Link
CN (1) CN103150449B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104122336A (en) * 2014-07-16 2014-10-29 哈尔滨工业大学 Electromagnetic ultrasonic surface wave transducer and design method thereof
CN108760899A (en) * 2018-08-03 2018-11-06 广东工业大学 Ultrasonic transducer model manufacturing method and device
CN110287617A (en) * 2019-06-28 2019-09-27 中北大学 A kind of design and relevant parameter method for solving of high power altrasonic transducer
CN112268954A (en) * 2020-08-31 2021-01-26 北京工业大学 L based on electromagnetic ultrasonic phased array sensorCRWave sound beam deflection regulating and controlling method
CN114101016A (en) * 2021-11-04 2022-03-01 之江实验室 Magnetic control flexible ultrasonic transducer

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101701810A (en) * 2009-11-13 2010-05-05 哈尔滨工业大学 Electromagnetic ultrasonic transducer capable of reducing echo of magnet

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101701810A (en) * 2009-11-13 2010-05-05 哈尔滨工业大学 Electromagnetic ultrasonic transducer capable of reducing echo of magnet

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
康磊: "用于铝板检测的电磁超声导波换能器优化设计技术研究", 《万方数据企业知识服务平台》 *
李智超: "基于洛伦兹力机理的电磁超声换能器建模及仿真研究", 《万方数据企业知识服务平台》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104122336A (en) * 2014-07-16 2014-10-29 哈尔滨工业大学 Electromagnetic ultrasonic surface wave transducer and design method thereof
CN108760899A (en) * 2018-08-03 2018-11-06 广东工业大学 Ultrasonic transducer model manufacturing method and device
CN108760899B (en) * 2018-08-03 2021-01-29 广东工业大学 Ultrasonic transducer model manufacturing method and device
CN110287617A (en) * 2019-06-28 2019-09-27 中北大学 A kind of design and relevant parameter method for solving of high power altrasonic transducer
CN110287617B (en) * 2019-06-28 2022-09-27 中北大学 Design of high-power ultrasonic transducer and related parameter solving method
CN112268954A (en) * 2020-08-31 2021-01-26 北京工业大学 L based on electromagnetic ultrasonic phased array sensorCRWave sound beam deflection regulating and controlling method
CN114101016A (en) * 2021-11-04 2022-03-01 之江实验室 Magnetic control flexible ultrasonic transducer
CN114101016B (en) * 2021-11-04 2022-08-23 之江实验室 Magnetic control flexible ultrasonic transducer

Also Published As

Publication number Publication date
CN103150449B (en) 2015-10-07

Similar Documents

Publication Publication Date Title
CN103150449A (en) Design method of electromagnetic ultrasonic body wave transducer
CN108802185B (en) Metal material defect detection sensor based on pulse eddy current and electromagnetic ultrasound
US11774409B2 (en) Electromagnetic acoustic transducer (EMAT) for corrosion mapping
Liu et al. Development of omnidirectional A0 mode EMAT employing a concentric permanent magnet pairs with opposite polarity for plate inspection
Liu et al. A direction-tunable shear horizontal mode array magnetostrictive patch transducer
CN103711474B (en) A kind of cross-dipole acoustic-electric combination well detecting Instrument
Liu et al. Obliquely incident EMAT for high-order Lamb wave mode generation based on inclined static magnetic field
Ratnam et al. Generation and detection of higher-order mode clusters of guided waves (HOMC-GW) using meander-coil EMATs
CN104090034A (en) Electromagnetic ultrasonic Lamb wave transducer for guided wave tomography
CN106540872B (en) A kind of coil autoexcitation electromagnetic acoustic Lamb wave energy converter
CN103308609A (en) Lamb wave mode control method based on electromagnetic ultrasonic emission transducer
CN108680652B (en) Full-directional S0 modal lamb wave electromagnetic ultrasonic transducer
CN204052095U (en) A kind of horizontal shear mode magneto strictive sensor
CN202757915U (en) Multi-main-frequency combined SH0-mode electromagnetic acoustic transducer
CN102175767B (en) Electromagnetic ultrasonic signal superposition method
CN103323531A (en) Nondestructive plate testing method with Lamb wave mode control based on electromagnetic ultrasonic receiving transducer
CN106824736A (en) A kind of electromagnetic acoustic Lamb wave transducer based on magnetostriction mechanism
CN103217481A (en) Magnetoacoustic tomography-with-magnetic-induction probe applying magnetostriction
CN103226630B (en) Electromagnetic ultrasonic surface wave receiving transducer method for designing
CN102636571B (en) Measuring method of horizontal shear guided wavelength in steel plate and electromagnetic ultrasonic transducer using same
RU2660770C1 (en) Acoustical method of determination of elastic constants of current-conducting solids
CN104122336A (en) Electromagnetic ultrasonic surface wave transducer and design method thereof
CN102608220B (en) Multi-basic frequency combined SH0 model electromagnetic acoustic transducer
Tu et al. A new magnetic configuration for a fast electromagnetic acoustic transducer applied to online steel pipe wall thickness measurements
Kang et al. A new surface-wave EMAT design of enhanced transduction efficiency

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20151007

Termination date: 20170326

CF01 Termination of patent right due to non-payment of annual fee