CN104034287B - A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method - Google Patents

A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method Download PDF

Info

Publication number
CN104034287B
CN104034287B CN201410245535.5A CN201410245535A CN104034287B CN 104034287 B CN104034287 B CN 104034287B CN 201410245535 A CN201410245535 A CN 201410245535A CN 104034287 B CN104034287 B CN 104034287B
Authority
CN
China
Prior art keywords
thermal barrier
barrier coating
echo
power spectrum
metallic matrix
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.)
Active
Application number
CN201410245535.5A
Other languages
Chinese (zh)
Other versions
CN104034287A (en
Inventor
林莉
马志远
罗忠兵
李广凯
赵灿
雷明凯
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.)
Dalian University of Technology
Original Assignee
Dalian 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 Dalian University of Technology filed Critical Dalian University of Technology
Priority to CN201410245535.5A priority Critical patent/CN104034287B/en
Publication of CN104034287A publication Critical patent/CN104034287A/en
Application granted granted Critical
Publication of CN104034287B publication Critical patent/CN104034287B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Abstract

A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method, belongs to ultrasonic non-destructive inspection techniques field。It adopts and a set of includes the ultrasonic pulse-echo method C-scan thickness measuring system that ultrasonic C-scanning device, water logging point focusing probe, digital oscilloscope and computer collectively form, respectively to detected sample and reference coupon measurement。For elastic anisotropy metallic matrix thermal barrier coating sample ultrasound echo signal, correction factor Δ γ by definition, extract the ultrasound data of all of which Δ γ > 0, and calculate its normalized power spectrum Gm (f), read the resonant frequency fn in Gm (f) effective band, in conjunction with known thermal barrier coating longitudinal wave velocity c, bring sound pressure reflection coefficient power spectrum resonance frequency expression into and can realize elastic anisotropy metallic matrix thermal barrier coating thickness measure。The method effectively overcomes the phenomenons such as the ultrasonic waveform distortion owing to base elastomer anisotropy causes and frequency shift and causes the problem that thermal barrier coating ultrasonic thickness measurement result error is bigger。

Description

A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method
Technical field
The present invention relates to a kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method, it belongs to the technical field of Ultrasonic NDT。
Background technology
Adopting the operating temperature that thermal barrier coating improves the hot-end components such as engine blade is the very cost-effective technological approaches of one, and thermal barrier coating thickness and uniformity thereof directly influence final effect of heat insulation。At the scene in coating decoration and quality inspection process, it is desirable to the thermal barrier coating thickness of spraying reaches criterion of acceptability。Thermal barrier coating thickness non-destructive testing method is the urgent engineering demand in this field accurately and reliably。
Existing multiple lossless detection method can be used for the measurement of thermal barrier coating thickness, mainly has the methods such as eddy-current method, infrared method, microwave method and supercritical ultrasonics technology。Wherein eddy-current method is based between probe and matrix and is changed, by coating layer thickness, the Lift-off effect caused carries out thickness measuring, and thickness measuring result is bigger by the impact of tack coat。Infrared method is the infrared ray absorbing corresponding wavelength according to detected coating under ultrared irradiation, analyzes and processes absorbed intensity and coating just can carry out thickness measurement, and the factor such as thickness measuring precision exposure time, coating composition uniformity affects bigger。Microwave method is to be preferably suitable to the sensitiveest wave band of coating detection before detection, and by measuring the information of echo reflection coefficient phase and then calculating thick coating angle value, the method is still in the laboratory research stage。Ultrasonic method is measured thermal barrier coating thickness and is mainly included ultrasonic microscope, ultrasonic surface wave, three kinds of technology of ultrasonic pulse-echo。Ultrasonic microscope technology is to utilize high-frequency ultrasonic that specimen material top layer and internal structure are carried out the technology of lossless micro-imaging, and its testing cost is high, detect system complex, the method is higher to the requirement of coating surface flatness simultaneously。Ultrasonic surface wave technical basis sound wave dispersion equation in the coating, by measuring coating phase velocities dispersion curve, coating layer thickness is calculated then in conjunction with inversion technique, owing to thermal barrier coating thickness is many at some tens of pm to hundred micron dimensions, therefore the surface wave frequency excited needed for is many in 40MHz-200MHz scope, at present many exciting by laser, the factor such as low yet with optoacoustic conversion efficiency, echo-signal is weak and detection sensitivity is low limits its application。Traditional ultrasonic pulse-echo technology utilizes the path difference of interface reflected P-wave before and after coating or two adjacent resonant frequencies of corresponding frequency spectrum, realizes the measurement of coating layer thickness in conjunction with the longitudinal wave velocity of coating。Owing to longitudinal wave velocity is big, extremely short during propagation sound in coating, the method is measured thickness thermal barrier coating less than hundred microns and is typically required more than 40MHz bandwidth, thus causes ultrasonic radio-frequency component to be decayed by force, wave distortion etc., it is difficult to implement measurement。Lin Li etc. propose the technology of a kind of ultrasonic longitudinal wave low-angle incidence wave mode converted measurement thermal barrier coating thickness, experiment adopts the water logging point focusing probe of conventional dominant frequency 20MHz, to the yittrium oxide PSZ (Y of the thickness range 66~100 μm of preparation on stainless steel base2O3Partiallystabilizedzirconia, YSZ) coating carried out ultrasonic thickness measurement, and result is accurately and reliably。But, for the metallic matrix thermal barrier coating sample being representative with nickel base superalloy, owing to dendritic segregation and recrystallization can occur matrix in preparation process, cause that it exists elastic anisotropy, ultrasound wave communication process wherein can cause the phenomenon such as wave distortion and frequency shift, and then cause thermal barrier coating thickness measure to be forbidden。The problem that above method all can not effectively solve this type of elastic anisotropy metallic matrix thermal barrier coating thickness nondestructive measurement。
Summary of the invention
By ultrasonic pulse-echo method C-scan thickness measuring system, the anisotropy of elastic anisotropy metallic matrix is characterized, and define the correction factor Δ γ of an elastic anisotropy metallic matrix thermal barrier coating thickness measuring, Δ γ=γani-ciso-c。When Δ γ≤0, the elastic anisotropy of metallic matrix is bigger on the impact of coating thickness measuring, it is difficult to accurately measure coating layer thickness;As Δ γ > 0, metallic matrix elastic anisotropy is little on the impact of coating thickness measuring, extracts the Ultrasonic data of all Δ γ > 0, and calculates its normalized power spectrum Gm (f);Read the resonant frequency f in Gm (f) effective bandn, in conjunction with known thermal barrier coating longitudinal wave velocity c, bring sound pressure reflection coefficient power spectrum resonance frequency expression into and can realize thermal barrier coating thickness measure;The method overcome the problem that thermal barrier coating ultrasonic thickness measurement result error that metallic matrix elastic anisotropy causes is bigger。
The technical solution adopted for the present invention to solve the technical problems is: a kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method, it is characterized in that: it adopts the ultrasonic pulse-echo method C-scan thickness measuring system that a ultrasonic C-scanning device, water logging point focusing probe, digital oscilloscope and computer collectively form, respectively elastic anisotropy metallic matrix thermal barrier coating sample, elastic isotropy metallic matrix thermal barrier coating sample, elastic anisotropy metallic matrix sample being carried out ultrasound detection, concrete detecting step is as follows:
(1) first defining the correction factor Δ γ of an elastic anisotropy metallic matrix thermal barrier coating thickness measuring, expression formula is:
Δ γ=γani-ciso-c(1)
Wherein γani-cRepresent ultrasound echo signal power spectrum (hereinafter referred to as " power spectrum ") the frequency shift coefficient of elastic anisotropy metallic matrix thermal barrier coating sample, γiso-cRepresent that before and after coating, interface echo interferes the power spectrum frequency shift coefficient caused;Use γaniRepresenting the power spectrum frequency shift coefficient that elastic anisotropy metallic matrix causes, the expression formula of γ is:
γ = f i - f 0 f 0 - - - ( 2 )
Wherein fiFor tested sample power spectrum dominant frequency, f0Initial spike power spectrum dominant frequency for water logging point focusing probe;
(2) ultrasonic pulse-echo method C-scan thickness measuring system has been calibrated, water logging point focusing probe is placed in above elastic anisotropy metallic matrix sample, adjusting water immersion focusing probe makes Main beam axis vertical with specimen surface, by acoustic beam focal point in matrix surface, gather an initial spike as reference signal J, signal J is carried out Fourier transformation and obtains its power spectrum and read the dominant frequency f of correspondence0And the effective band that-6dB is corresponding;Then by acoustic beam focal point in matrix bottom surface, by the output gate locating of C-scan in matrix Bottom echo position, whole matrix sample is carried out C-scan detection;Gather the echo-signal that C-scan result difference grayscale position is corresponding, and the matrix Bottom echo in intercept signal carries out Fourier transformation, obtain the power spectrum M of its correspondence, add up dominant frequency fani, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingani
(3) water logging point focusing probe is placed in above elastic isotropy metallic matrix thermal barrier coating reference coupon, adjusts water logging point focusing probe and make Main beam axis vertical with specimen surface, by acoustic beam focal point in matrix bottom surface;By the output gate locating of C-scan in matrix Bottom echo position, whole sample is carried out C-scan detection;Then gathering corresponding echo-signal in C-scan result difference grayscale position, the matrix Bottom echo intercepted in all signals carries out Fourier transformation, obtains the power spectrum M of its correspondence and adds up the dominant frequency f of its correspondenceiso-c, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingiso-c
(4) water logging point focusing probe is placed in above elastic anisotropy metallic matrix thermal barrier coating sample, equally by the output gate locating of C-scan in matrix Bottom echo position, whole sample is carried out C-scan detection;Gather echo-signal corresponding to C-scan result difference grayscale position, and intercept matrix Bottom echo and carry out Fourier transformation, obtain the power spectrum M of its correspondence and add up the dominant frequency f of its correspondenceani-c, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingani-c;More resilient anisotropy metallic matrix thermal barrier coating sample diverse location γani-cγ with corresponding thickness elastomeric isotropism metallic matrix thermal barrier coating sampleiso-cValue;When Δ γ≤0, γani-cNot only include interface echo before and after coating and interfere the frequency shift caused, also include the frequency shift γ that base elastomer anisotropy causesani, now utilize normalization amplitude spectrum resonant frequency to carry out coating thickness measuring, resultant error is relatively big, and thickness measuring result is unreliable;As Δ γ > 0, γani-cMainly include interface echo before and after coating and interfere the frequency shift caused, extract the data of all Δ γ > 0 and carry out coating thickness measuring;
(5) data that step (4) is extracted carried out Fourier transformation and is normalized for benchmark with signal J, obtaining its normalized power spectrum Gm (f), reading the resonant frequency value f in Gm (f) effective bandn, it is known that the longitudinal wave velocity c of this thermal barrier coating, brings sound pressure reflection coefficient power spectrum resonance frequency expression (3) into:
f n = n × c 4 d - - - ( 3 )
Wherein n is resonant frequency exponent number, takes positive integer value, and d is thermal barrier coating thickness, can be calculated the coating layer thickness of correspondence by expression formula (3)。
The invention have the advantages that: elastic anisotropy metallic matrix thermal barrier coating sample, elastic isotropy metallic matrix thermal barrier coating sample, elastic anisotropy metallic matrix sample are carried out ultrasound detection by ultrasonic pulse-echo method C-scan thickness measuring system by this invention respectively。By the correction factor Δ γ of definition, extract the ultrasonic echo data of all Δ γ > 0 of elastic anisotropy metallic matrix thermal barrier coating, and calculate its normalized power spectrum Gm (f), read the resonant frequency f in Gm (f) effective bandn, in conjunction with known thermal barrier coating longitudinal wave velocity c, bring sound pressure reflection coefficient power spectrum resonance frequency expression into and can realize thermal barrier coating thickness measure。The method not only overcomes and is currently used for the ultrasonic microscope of thermal barrier coating thickness measuring, ultrasonic surface wave, the deficiencies such as detection frequency that requirement that three kinds of technology of ultrasonic pulse-echo exist is high and hardware configuration, testing cost height, system complex, and efficiently solve the problem that coating ultrasonic thickness measurement resultant error that metallic matrix elastic anisotropy causes is bigger。The method is low to detection System Hardware Requirement, and easy to operate, cost is low。
Accompanying drawing explanation
Below in conjunction with drawings and Examples, patent of the present invention is described further。
Fig. 1 is ultrasonic pulse-echo method C-scan thickness measuring system。
Fig. 2 is reference signal J time domain waveform and corresponding power spectrum。
Fig. 3 is the C-scan result of nickel base superalloy matrix sample。
Fig. 4 is the power spectrum M and dominant frequency coefficient of deviation γ of nickel base superalloy matrix sampleani
Fig. 5 is the C-scan result of the uniform stainless steel base YSZ coating sample of coating layer thickness 40~120 μm。
Fig. 6 is the frequency shift coefficient gamma of the uniform stainless steel base YSZ coating sample of coating layer thickness 40~120 μmiso-c
Fig. 7 is the C-scan result of nickel base superalloy matrix YSZ coating sample。
Fig. 8 is the dominant frequency coefficient of deviation γ of nickel base superalloy matrix YSZ coating sampleani-c
Fig. 9 is YSZ coating ultrasonic thickness measurement result and metallographic thickness measuring result。
Figure 10 is the electron scanning micrograph of YSZ coating sample cross section
Figure 11 is YSZ coating ultrasonic thickness measurement error analysis。
In Fig. 1: 1, computer, 2, DPO4O32 digital oscilloscope sample, 3, ultrasonic C-scanning device, 4, water logging point focusing probe, 5, sample, 6, sample bench。
Detailed description of the invention
This elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method adopts the ultrasonic pulse-echo method C-scan thickness measuring system shown in Fig. 1, and it is collectively formed by a SM-J38-300 ultrasonic C-scanning device, the water logging point focusing probe of nominal 25MHz, DPO4O32 digital oscilloscope and computer。Respectively to the nickel base superalloy matrix YSZ coating sample of nominal 60 μ m-thick, the uniform stainless steel base YSZ coating sample of coating layer thickness 40~120 μm, the measurement of nickel base superalloy matrix sample, the measuring process that it adopts is as follows:
(1) ultrasonic pulse-echo method C-scan thickness measuring system has been calibrated, nominal 25MHz water logging point focusing probe is placed in above nickel base superalloy matrix sample, adjusting water immersion focusing probe makes Main beam axis vertical with specimen surface, by acoustic beam focal point in matrix surface, gather an initial spike as reference signal J, see Fig. 2 (a)。It is carried out Fourier transformation obtain its power spectrum and see Fig. 2 (b), dominant frequency f0=23.25MHz, effective band corresponding for power spectrum-6dB is 13.75MHz~33.0MHz。Then by acoustic beam focal point in matrix bottom surface, by the output gate locating of C-scan in matrix Bottom echo position, whole elastic anisotropy metallic matrix sample being carried out C-scan detection, result is shown in Fig. 3;Gather echo-signal corresponding to C-scan result difference grayscale position, and intercept matrix Bottom echo and carry out Fourier transformation, obtain the power spectrum M of its correspondence, see Fig. 4 (a)。The dominant frequency f of statistics power spectrumani, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingani, such as Fig. 4 (b)。Figure can be seen that the frequency shift coefficient gamma of nickel base superalloy matrixaniBeing mainly distributed on-0.5~0 scope, matrix anisotropy causes ultrasound wave dominant frequency to low frequency offset。
(2) nominal 25MHz water logging point focusing probe is placed in above the uniform stainless steel base YSZ coating sample of coating layer thickness 40~120 μm, adjusting water logging point focusing probe makes Main beam axis vertical with specimen surface, by acoustic beam focal point in uniform stainless steel base bottom surface;By the output gate locating of C-scan in matrix Bottom echo position, whole sample being carried out C-scan detection, result is Fig. 5 such as。Then the echo-signal that C-scan result difference grayscale position is corresponding is gathered。Intercept matrix Bottom echo and carry out Fourier transformation, obtain the power spectrum M of its correspondence and add up the dominant frequency f of its correspondenceiso-c;The frequency shift coefficient gamma that coating layer thickness fluctuation 10% causes is calculated according to formula (2)iso-cScope, is shown in Fig. 6。The thickness measuring giving 23.25MHz probe in figure ranges for 40~90 μm。The thickness measuring that same method measures 15MHz probe is adopted to range for 60~120 μm。It is found that the method adopts low-frequency probe can measure bigger coating layer thickness, adopting high frequency probe can measure relatively thin coating layer thickness, the thickness measuring scope of other frequency probe needs to demarcate according to practical situation。
(3) nominal 25MHz water logging point focusing probe is placed in above the nickel base superalloy matrix YSZ coating sample of nominal 60 μ m-thick, equally by the output gate locating of C-scan in matrix Bottom echo position, whole sample is carried out C-scan detection, and result is Fig. 7 such as。Gather the echo-signal that arrow locations is corresponding in Fig. 7, and intercept matrix Bottom echo and carry out Fourier transformation, obtain the power spectrum M of its correspondence and add up the dominant frequency f of its correspondenceani-c;The frequency shift coefficient gamma of its correspondence is calculated according to formula (2)ani-cScope, is shown in Fig. 8;Relatively diverse location γani-cThe γ corresponding with 60 μ m thick in Fig. 6iso-ciso-c=0) value。If Δ γ≤0, γ is describedani-cNot only include interface echo before and after YSZ coating and interfere the frequency shift γ causediso-c, γ that matrix anisotropy causesaniAlso can not ignore, now utilize normalization amplitude spectrum resonant frequency to carry out coating thickness measuring, resultant error is bigger;If Δ γ > 0, it was shown that γani-cThe frequency shift γ caused is interfered essentially from interface echo before and after YSZ coatingiso-c, γ that matrix anisotropy causesaniCan ignore, extract the data of all Δ γ > 0 and carry out coating thickness measuring。
(4) data that step (3) is extracted carried out Fourier transformation and is normalized for benchmark with signal J, obtaining its normalized power spectrum Gm (f), reading Gm (f) resonant frequency value fn, it is known that this YSZ coating longitudinal wave velocity 4320m/s, brings sound pressure reflection coefficient power spectrum resonance frequency expression (3) into, can calculate the YSZ coating layer thickness of correspondence, see Fig. 9。Then dissecting sample, utilize metallographic method to determine YSZ coating layer thickness, the electron scanning micrograph of coating sample cross section is as shown in Figure 10。Figure 11 give the raw ultrasound method thickness measuring result of the nickel base superalloy matrix YSZ coating sample of nominal thickness 60 μm and revise after the ultrasonic method thickness measuring result absolute error corresponding with metallographic thickness measuring result, the bounded absolute error of raw ultrasound method thickness measuring result is-10.89~98.5 μm, statistical standard difference is 29.3 μm, and statistics relative error is 49.8%。After correction, the bounded absolute error of ultrasonic method thickness measuring result is-10.89~11.9 μm, and statistical standard difference is 5.07 μm, and statistics relative error is 9.9%。

Claims (1)

1. an elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method, it is characterized in that: it adopts the ultrasonic pulse-echo method C-scan thickness measuring system that a ultrasonic C-scanning device, water logging point focusing probe, digital oscilloscope and computer collectively form, respectively elastic anisotropy metallic matrix thermal barrier coating sample, elastic isotropy metallic matrix thermal barrier coating sample, elastic anisotropy metallic matrix sample being carried out ultrasound detection, concrete detecting step is as follows:
(1) first defining the correction factor Δ γ of an elastic anisotropy metallic matrix thermal barrier coating thickness measuring, expression formula is:
Δ γ=γani-ciso-c(1)
Wherein γani-cRepresent the ultrasound echo signal power spectrum frequency shift coefficient of elastic anisotropy metallic matrix thermal barrier coating sample, hereinafter referred to as " power spectrum frequency shift coefficient ", γiso-cRepresent that before and after coating, interface echo interferes the power spectrum frequency shift coefficient caused;Use γaniRepresenting the power spectrum frequency shift coefficient that elastic anisotropy metallic matrix causes, the expression formula of γ is:
γ = f i - f 0 f 0 - - - ( 2 )
Wherein fiFor tested sample power spectrum dominant frequency, f0Initial spike power spectrum dominant frequency for water logging point focusing probe;
(2) ultrasonic pulse-echo method C-scan thickness measuring system has been calibrated, water logging point focusing probe is placed in above elastic anisotropy metallic matrix sample, adjusting water immersion focusing probe makes Main beam axis vertical with specimen surface, by acoustic beam focal point in matrix surface, gather an initial spike as reference signal J, signal J is carried out Fourier transformation and obtains its power spectrum and read the dominant frequency f of correspondence0And the effective band that-6dB is corresponding;Then by acoustic beam focal point in matrix bottom surface, by the output gate locating of C-scan in matrix Bottom echo position, whole matrix sample is carried out C-scan detection;Gather the echo-signal that C-scan result difference grayscale position is corresponding, and the matrix Bottom echo in intercept signal carries out Fourier transformation, obtain the power spectrum M of its correspondence, add up dominant frequency fani, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingani
(3) water logging point focusing probe is placed in above elastic isotropy metallic matrix thermal barrier coating sample, adjusts water logging point focusing probe and make Main beam axis vertical with specimen surface, by acoustic beam focal point in matrix bottom surface;By the output gate locating of C-scan in matrix Bottom echo position, whole sample is carried out C-scan detection;Then gathering corresponding echo-signal in C-scan result difference grayscale position, the matrix Bottom echo intercepted in all signals carries out Fourier transformation, obtains its power spectrum M and adds up the dominant frequency f of its correspondenceiso-c, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingiso-c
(4) water logging point focusing probe is placed in above elastic anisotropy metallic matrix thermal barrier coating sample, equally by the output gate locating of C-scan in matrix Bottom echo position, whole sample is carried out C-scan detection;Gather echo-signal corresponding to C-scan result difference grayscale position, and intercept matrix Bottom echo and carry out Fourier transformation, obtain the power spectrum M of its correspondence and add up the dominant frequency f of its correspondenceani-c, calculate, according to formula (2), the frequency shift coefficient gamma that each sampling point position is correspondingani-c;More resilient anisotropy metallic matrix thermal barrier coating sample diverse location γani-cγ with corresponding thickness elastomeric isotropism metallic matrix thermal barrier coating sampleiso-cValue;When Δ γ≤0, γani-cNot only include interface echo before and after coating and interfere the frequency shift caused, also include the frequency shift γ that base elastomer anisotropy causesani;As Δ γ > 0, γani-cMainly include interface echo before and after coating and interfere the frequency shift caused, extract the data of all Δ γ > 0 and carry out coating thickness measuring;
(5) data that step (4) is extracted carried out Fourier transformation and is normalized for benchmark with signal J, obtaining its normalized power spectrum Gm (f), reading the resonant frequency value f in Gm (f) effective bandn, it is known that the longitudinal wave velocity c of this thermal barrier coating, brings sound pressure reflection coefficient power spectrum resonance frequency expression (3) into:
f n = n × c 4 d - - - ( 3 )
Wherein n is resonant frequency exponent number, takes positive integer value, and d is thermal barrier coating thickness, is calculated the coating layer thickness of correspondence by expression formula (3)。
CN201410245535.5A 2014-06-05 2014-06-05 A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method Active CN104034287B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410245535.5A CN104034287B (en) 2014-06-05 2014-06-05 A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410245535.5A CN104034287B (en) 2014-06-05 2014-06-05 A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method

Publications (2)

Publication Number Publication Date
CN104034287A CN104034287A (en) 2014-09-10
CN104034287B true CN104034287B (en) 2016-06-22

Family

ID=51465153

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410245535.5A Active CN104034287B (en) 2014-06-05 2014-06-05 A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method

Country Status (1)

Country Link
CN (1) CN104034287B (en)

Families Citing this family (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104457635A (en) * 2014-10-10 2015-03-25 北京理工大学 Ultra-thin coating thickness uniformity lossless detection method based on Welch method spectral estimation
CN105651215B (en) * 2016-03-19 2017-10-13 大连理工大学 A kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition
CN106205584A (en) * 2016-07-06 2016-12-07 南京大学 A kind of broadband noise elimination pipeline of Helmholtz resonator based on adjustable resonant frequency
CN107063143B (en) * 2017-04-28 2019-07-19 大连交通大学 A kind of high-precision ultrasonic displacement measurement system
CN109781041B (en) * 2019-02-28 2021-04-20 华中科技大学 Electromagnetic ultrasonic thickness measurement method based on frequency domain analysis
CN110398461B (en) * 2019-07-11 2021-07-27 上海交通大学 Method for realizing three-dimensional imaging of dendritic crystals in lithium metal battery by utilizing photoacoustic imaging
CN111442747B (en) * 2020-03-13 2021-11-30 中核武汉核电运行技术股份有限公司 Ultrasonic signal processing method
CN111947769B (en) * 2020-06-30 2023-03-28 核动力运行研究所 Resonant wave frequency determination method and device
CN112305077B (en) * 2020-10-27 2023-06-20 洛阳轴承研究所有限公司 Nondestructive testing method for bonding quality of bearing surface coating and substrate interface
CN113188489B (en) * 2021-04-29 2022-10-21 深圳市麒博精工科技有限公司 Ultrasonic reflectance spectrum method for detecting thickness consistency of thin flat plate material
CN117760347B (en) * 2024-02-22 2024-05-17 中国航发北京航空材料研究院 Method and device for detecting thickness of high-temperature alloy thermal barrier coating, storage medium and electronic equipment

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3570305A (en) * 1967-03-20 1971-03-16 Hitachi Ltd Apparatus for measuring depth of chilled layer on cast iron roll
CN103245311A (en) * 2013-05-11 2013-08-14 大连理工大学 Ultrasonic thickness measurement device and method for multilayered wave-absorbing coatings
CN103292753A (en) * 2013-05-29 2013-09-11 大连理工大学 Method of measuring thickness of thermal barrier coating by ultrasonic water-immersion focusing technology
CN103615996A (en) * 2013-11-14 2014-03-05 大连理工大学 Method for measuring thickness of coatings through ultrasonic signal spectrum filter technology in nondestructive mode

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3570305A (en) * 1967-03-20 1971-03-16 Hitachi Ltd Apparatus for measuring depth of chilled layer on cast iron roll
CN103245311A (en) * 2013-05-11 2013-08-14 大连理工大学 Ultrasonic thickness measurement device and method for multilayered wave-absorbing coatings
CN103292753A (en) * 2013-05-29 2013-09-11 大连理工大学 Method of measuring thickness of thermal barrier coating by ultrasonic water-immersion focusing technology
CN103615996A (en) * 2013-11-14 2014-03-05 大连理工大学 Method for measuring thickness of coatings through ultrasonic signal spectrum filter technology in nondestructive mode

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
基于超声声压反射系数相位谱法的热障涂层非均匀性表征;赵扬等;《无损检测》;20100731;第32卷(第7期);第485-489页 *
热障涂层喷涂质量微焦点CT检测;敖波等;《航空动力学报》;20130831;第28卷(第8期);第1777-1783页 *

Also Published As

Publication number Publication date
CN104034287A (en) 2014-09-10

Similar Documents

Publication Publication Date Title
CN104034287B (en) A kind of elastic anisotropy metallic matrix thermal barrier coating thickness ultrasonic measurement method
CN103292753B (en) Adopt the method for ultrasound wave water immersion focusing commercial measurement thermal barrier coating thickness
Gan et al. The use of broadband acoustic transducers and pulse-compression techniques for air-coupled ultrasonic imaging
Konstantinidis et al. The temperature stability of guided wave structural health monitoring systems
Potter et al. Nonlinear ultrasonic phased array imaging
CN101451944B (en) Coating density ultrasonic measurement method based on pressure reflection coefficient phase spectrum
CN101750454B (en) For ultrasound inspection methods and the related probes of noise founding materials
CN105004792A (en) Nonlinear ultrasonic phased array imaging method for micro-crack detection
CN110346453B (en) Method for rapidly detecting reflection echoes of small defect arrays in concrete structure
Michaels Ultrasonic wavefield imaging: Research tool or emerging NDE method?
In et al. A fully non-contact, air-coupled ultrasonic measurement of surface breaking cracks in concrete
CN103822971A (en) Resolution detecting and calibrating method for ultrasonic microscope
CN103148815A (en) Lamella thickness ultrasonic detecting method based on sound pressure reflection coefficient
CN102607479B (en) Method for measuring round-trip time of ultrasound in thin layered medium based on sound pressure reflection coefficient power spectrum
Sen et al. Ultrasonic thickness measurement for aluminum alloy irregular surface parts based on spectral analysis
CN106198739A (en) A kind of TOFD near surface blind region defect location detection method based on shape transformation
CN105424810A (en) Evaluation method for uniformity of fiber reinforcement ceramic matrix composite
Cao et al. A correlation-based approach to corrosion detection with lamb wave mode cutoff
Tang et al. Non-contact phase coded excitation of ultrasonic Lamb wave for blind hole inspection
Roy et al. A study on the efficacy of modal acoustic emission technique for health monitoring of structures with different geometries
Kang et al. Measurement of shallow defects using noncontact broadband leaky Lamb wave produced by pulsed laser with ultrasound microphone
Cong et al. Parameter design of linear frequency modulated excitation waveform for ultrasonic nondestructive testing of metallic materials
Murav’eva et al. Analysis of reflected signals in testing cylindrical specimens by the multiple reflection echo-shadow method
CN111665296A (en) Method and device for measuring three-dimensional radiation sound field of ultrasonic transducer based on EMAT
Hesse et al. A single probe spatial averaging technique for guided waves and its application to surface wave rail inspection

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