CN105651215B - A kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition - Google Patents

A kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition Download PDF

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CN105651215B
CN105651215B CN201610165884.5A CN201610165884A CN105651215B CN 105651215 B CN105651215 B CN 105651215B CN 201610165884 A CN201610165884 A CN 201610165884A CN 105651215 B CN105651215 B CN 105651215B
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msub
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coating
sound
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CN105651215A (en
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林莉
张伟
马志远
罗忠兵
金士杰
雷明凯
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Dalian University of Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B17/00Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
    • G01B17/02Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness
    • G01B17/025Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness for measuring thickness of coating

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  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Abstract

A kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition, belongs to material ultrasonic non-destructive inspection techniques field.The measuring method includes the ultrasonic pulse-echo detecting system of reflectoscope, delay block probe, digital oscilloscope and the computer composition for installing MATLAB softwares using a set of.It is unknown and there is fluctuation under different technical parameters or heterogeneous conditions and cause the problem of coating layer thickness can not be measured for echo-signal aliasing, the velocity of sound during coating ultrasonic thickness measurement, using ultrasonic pulse-echo technology, inverting is carried out simultaneously to sample coatings thickness and velocity of ultrasonic sound with reference to ultrasonic sound pressure reflection coefficient amplitude spectral analysis method and Relative coefficient.The measuring method have the advantages that definite principle, be easily achieved, matching precision it is high, overcome that existing Gauss-Newton inversion method computing is complicated, initial value is chosen require limitation that is higher, being difficult to use in engineer applied, with good prospect for promotion and application.

Description

A kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition
Technical field
The present invention relates to a kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition, belong to the inspection of material ultrasonic non-destructive Survey technology field.
Background technology
Coating material is widely used to many necks such as Aero-Space, oil-gas transportation, automobile making and biomedical engineering Domain, occupies more and more consequence in field of engineering technology.In a series of indexs for characterizing coating performance, thickness is not only It is a parameter for characterizing coating itself physical dimension, and performance to coating and life-span have a significant impact, coating layer thickness Do not reach or be all unable to reach desired effects more than design load, and thickness is excessive or uneven is also possible to reduce its bond strength And service life, cause coating plasticity to be deteriorated and even result in coating localized delamination.Therefore, accurate measurement is carried out to thickness has turned into Ensure the important means of coating performance.
In existing coating thickness measurement technology, ultrasonic pulse-echo technology is due to definite principle, realizing simple, non-demolition Property and it is applied widely the advantages of, among the thickness measure for being widely used in layered medium material.When coating layer thickness compared with Greatly, its thickness can be surveyed by traditional ultrasonic transit time method when aliasing does not occur for coating surface ripple and interface echo Amount;When coating layer thickness is relatively thin, and the propagation time of ultrasonic wave in the coating is less than its pulse width, coating surface ripple and boundary wave Will occur aliasing, ultrasonic transit time method is no longer applicable.Will by sound pressure reflection coefficient amplitude spectral analysis method (URCAS) Time-domain signal, which transforms to frequency domain progress processing, can effectively solve this problem.However, found during ultrasonic thickness measurement, no matter It is that ultrasonic transit time method or URCAS signal processing methods are required to the velocity of sound of coating for known quantity, but due to by technique The influence of the factors such as parameter, Coating Non-Uniformity, the velocity of sound of coating is often to be unknown and there is certain fluctuation in diverse location. Zhao Yang, Lin Li etc. propose to use the Gaussian-Newton method progress inverting based on binary nonlinear equation, can be in the coating velocity of sound Its thickness and velocity of ultrasonic sound are determined in the case of unknown simultaneously, and it is excellent that this method has that local convergence speed is fast, matching precision is high etc. Point, but higher is required to the selection of initial value, if initial value selection is improper to this may result in only converging to locally optimal solution very Do not restrained to equation, it is impossible to obtain inversion result.It is real to coating sample present invention introduces the Relative coefficient in statistics Survey sound pressure reflection coefficient amplitude spectrum and apply shelf theory sound pressure reflection coefficient amplitude spectrum matrix in the range of ultrasound detection effective band The matching analysis is carried out one by one, and the thickness of thin layer and the velocity of sound of correspondence maximum correlation coefficient are optimal inversion result.
The content of the invention
It is an object of the invention to provide a kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition.This method is used It is a set of to include the ultrasound of reflectoscope, delay block probe, digital oscilloscope and the computer composition for installing MATLAB softwares Pulse echo detecting system.For echo-signal aliasing, the velocity of sound during coating ultrasonic thickness measurement it is unknown and different process ginseng There is fluctuation under number or heterogeneous conditions and cause the problem of coating layer thickness can not be measured, using ultrasonic pulse-echo technology, with reference to Ultrasonic sound pressure reflection coefficient amplitude spectral analysis method and Relative coefficient enter simultaneously to sample coatings thickness and velocity of ultrasonic sound Row inverting.This method have the advantages that definite principle, be easily achieved, matching precision it is high, overcome existing Gauss-Newton inverting side Method computing is complicated, requirement limitation that is higher, being difficult to use in engineer applied is chosen to initial value, with good popularization and application Prospect.
The technical solution adopted for the present invention to solve the technical problems is:A kind of painting thickness under velocity of ultrasonic sound unknown condition Measuring method is spent, using a set of including super supersonic detector, delay block probe, digital oscilloscope and installation MATLAB softwares Computer constitute ultrasonic pulse-echo detecting system;The measuring method uses the following steps:
(a) specimen surface is handled
Tested coating sample surface is handled using absolute ethyl alcohol or acetone cleaning agent, removes what specimen surface was present Greasy dirt, organic solvent pollution thing, are suitably polished, it is ensured that sample using the fine sandpaper position larger to specimen surface roughness Surfacing, and suitable couplant guarantee delay block probe and the good coupling being tested between coating sample are chosen according to coating characteristic Close;
(b) material properties are determined
Understand density, the velocity of sound of acoustic attenuation coefficient and probe delay block and base material, the density of tested sample coating Material properties, respective acoustic impedance is calculated according to the velocity of sound and density of probe delay block and base material;
(c) ultrasonic probe is chosen
Suitable delay block ultrasound is chosen according to tested sample coating layer thickness, acoustical damping properties and the requirement to accuracy of detection Probe, acoustic attenuation thin to coating layer thickness is small, accuracy of detection requires high, and thickness measuring precision is improved from high frequency probe;To coating layer thickness Greatly, acoustic attenuation is serious, accuracy of detection requires low, and echo-signal can not be known caused by avoiding high frequency attenuation serious from low-frequency probe Not;
(d) parameter setting is detected
Pulse recurrence frequency PRF, ENERGY E nergy, gain G ain, wave filter are arranged as required on reflectoscope Bandwidth detection parameter;
(e) data acquisition
According to step (a)-(d) completion specimen surfaces are handled, material properties are determined, probe is chosen and detection parameter is set Postpone, then delay block probe is placed in tested sample surface by one delay block time domain echo-signal of collection as reference signal, Digital oscilloscope gain, detecting way, average time, sampling frequency parameters are adjusted, complete, stable coating tim e- domain detection is obtained Signal;
(f) coating sound pressure reflection coefficient amplitude spectrum is calculated
The time-domain signal that digital oscilloscope is collected is imported in computer, and FFT is carried out to it using data processing software Conversion obtains the amplitude spectrum of reference signal | A (f) | and the amplitude spectrum of detection signal | A (f) |*, effective frequency is obtained according to formula (1) Bandwidth undercoating surveys sound pressure reflection coefficient amplitude spectrum | r (f;d,c2)|*
The material properties parameter obtained in step (b) is updated in formula (2) and obtains the internally coated theory of effective bandwidth Sound pressure reflection coefficient amplitude spectrum | r (f;d,c2)|:
In formula, subscript 1,2,3 represents probe delay block, coating and base material, r respectively12、r23To represent heterogeneous material It is thickness of thin layer, c to expect the sound pressure reflection coefficient at interface, d2It is respectively the rate of sound and attenuation of sound coefficient of coating with α (f);
(g) correlation coefficient matching method is analyzed
By assigning formula (2) coating thickness d and velocity of sound c2A series of consecutive variations values, obtain theoretical sound pressure reflection system Number amplitude spectrum matrix is as parent, and the reflectance magnitude obtained using formula (3) to theoretical calculation is composed | r (f) | and actual inspection The reflectance magnitude spectrum measured | r (f) |*Carry out the matching analysis, correlation coefficient r one by one in -6dB effective bandsp(d,c2) most Big position corresponding d and c2The as optimal inversion result of tested sample coating layer thickness and the velocity of sound:
Wherein, N represents data points of the time-domain signal after FFT in the range of effective band, and subscript i represents i-th Individual frequency values;|r(f;d,c2) | with | r (f;d,c2)|*The theoretical sound pressure reflection coefficient amplitude with actual measurement respectively in effective band Spectrum,WithThe theoretical arithmetic with the sound pressure reflection coefficient amplitude spectrum of actual measurement respectively in effective band Average value.
The invention has the advantages that:Coating thickness measurement method under this velocity of ultrasonic sound unknown condition is using a set of The ultrasonic pulse that computer including reflectoscope, delay block probe, digital oscilloscope and installation MATLAB softwares is constituted Echo detecting system, coating layer thickness is conjointly employed in by sound pressure reflection coefficient amplitude spectral analysis technology and Relative coefficient Among Ultrasonic NDT.The ultrasonic time domain echo-signal of coating is obtained using ultrasonic pulse-echo technology, sound pressure reflection is utilized Coefficient amplitude spectral analysis technology is extracted to ultrasonic feature parameter, by between actual measurement and theoretical sound pressure reflection coefficient amplitude spectrum Relevant matches are analyzed, and the binary nonlinear equation without solving complexity is anti-while coating layer thickness can be achieved with velocity of ultrasonic sound Drill, overcome complicated existing Gauss-Newton inversion method computing, initial value selection difficulty, the limitation for being difficult to use in engineer applied Property.This method have the advantages that definite principle, be easily achieved, matching precision it is high, with good prospect for promotion and application.
Brief description of the drawings
Patent of the present invention is described further with reference to the accompanying drawings and examples.
The hardware connection diagram of Fig. 1 ultrasonic pulse-echo detecting systems.
Fig. 2 reference signal y (t) and its corresponding amplitude spectrum | A (f) |.
Fig. 3 coatings detection signal y (t)*And its corresponding amplitude spectrum | A (f) |*
Fig. 4-6dB effective frequency belt widths undercoating surveys sound pressure reflection coefficient amplitude spectrum | r (f;d,c2)|*
Fig. 5 different-thickness combines corresponding correlation coefficient r with the velocity of soundp(d,c2)。
Fig. 6 is surveyed to be contrasted with the sound pressure reflection coefficient amplitude spectrum under optimal coupling condition.
In figure:1st, supersonic detector, 2, delay block probe, 3, coating, 4, base material, 5, digital oscilloscope, 6, meter Calculation machine.
Embodiment
USIP40 supersonic detectors, the delay block of the ultrasonic pulse-echo detecting system that this method is used as shown in Figure 1 Probe and the computer composition for being provided with MATLAB softwares.Laboratory sample in the present embodiment is magnetic loss type radar-wave absorbing Coating sample (absorbent is carbonyl iron dust, and binding agent main component is epoxy resin, and base material is flat aluminium alloy plate), coating Thickness and velocity of ultrasonic sound are unknown quantity, coating time domain echo-signal are obtained using ultrasonic pulse-echo technology, with reference to ultrasonic sound Pressure reflectance magnitude spectral analysis method and Relative coefficient carry out inverting simultaneously to sample coatings thickness and velocity of ultrasonic sound. Methods described uses the following steps:
(a) specimen surface is handled.Tested coating sample surface is handled using acetone, removing specimen surface may deposit The pollutant such as greasy dirt, organic solvent, suitably polished using the fine sandpaper position larger to specimen surface roughness, really Protect specimen surface smooth, and glycerine is chosen as couplant guarantee delay block probe according to coating characteristic and is tested between coating sample Good coupling.
(b) material properties are determined.Understand density, acoustic attenuation coefficient and probe delay block and the substrate of tested sample coating The material properties such as the velocity of sound, the density of material.Known coating species is magnetic loss type absorption coating, thickness is about 0.2mm, close Spend for 3290kg/m3, acoustic attenuation coefficient α (f)=1.47f+8.51E (- 4) f4;Delay block of material is epoxy resin, and the velocity of sound is 2316.6m/s, density is 1045.5kg/m3;Aluminum alloy substrate acoustic velocity of material is that 6480m/s, density are 2700kg/m3
(c) ultrasonic probe is chosen.Chosen according to tested sample coating layer thickness, acoustical damping properties and the requirement to accuracy of detection Suitable delay block ultrasonic probe.If coating layer thickness is relatively thin, acoustic attenuation is smaller, accuracy of detection requires high, high frequency should be selected Pop one's head in improve thickness measuring precision;If coating layer thickness is larger, acoustic attenuation is serious, accuracy of detection requires relatively low, low frequency should be selected Probe is with echo-signal None- identified caused by avoiding high frequency attenuation serious.Because acoustic attenuation is more serious in microwave absorbing coating, this Embodiment is from Olympus 5MHz monocrystalline ultrasonic probes and is equipped with a diameter of 6mm epoxy resin delay block and is detected.
(d) parameter setting is detected.Pulse recurrence frequency PRF is set on USIP40 reflectoscopes:500Hz, energy Energy:10 μ J, gain G ain:20dB, filter bandwidht:0-10MHz.
(e) data acquisition.According to step (a)-(d) completion specimen surfaces are handled, material properties are determined, probe is chosen A delay block time domain echo-signal y (t) is gathered first as reference signal with after detection parameter setting, then visits delay block Head is placed in tested sample surface, adjusts the gain of parameter such as digital oscilloscope gain, detecting way, average time, sample frequency complete Whole, stable coating tim e- domain detection signal y (t)*
(f) coating sound pressure reflection coefficient amplitude spectrum is calculated.The time-domain signal that digital oscilloscope is collected imports computer In, the amplitude spectrum that FFT obtains reference signal is carried out to it using data processing software | A (f) | and the amplitude of detection signal Spectrum | A (f) |*, -6dB effective frequency belt widths undercoating actual measurement sound pressure reflection coefficient amplitude spectrum is obtained according to formula (1) | r (f;d, c2)|*
The material properties obtained in step (b) are updated in formula (2) and obtain the internally coated theory of -6dB effective bandwidths Sound pressure reflection coefficient amplitude spectrum | r (f;d,c2)|:
In formula, subscript 1,2,3 represents probe delay block, coating and base material, r respectively12、r23To represent heterogeneous material It is thickness of thin layer, c to expect the sound pressure reflection coefficient at interface, d2It is respectively the rate of sound and attenuation of sound coefficient of coating with α (f).
(g) correlation coefficient matching method is analyzed.By assigning formula (2) coating thickness d and velocity of sound c2A series of consecutive variations Value, obtains theoretical sound pressure reflection coefficient amplitude spectrum matrix as parent, the reflectance factor obtained using formula (3) to theoretical calculation Amplitude spectrum | r (f) | and the actually detected reflectance magnitude spectrum arrived | r (f) |*Carry out matching point one by one in -6dB effective bands Analysis, correlation coefficient rpThe corresponding d of (d, c2) maximum position and c2 is tested sample coating layer thickness and the optimal inverting knot of the velocity of sound Really.
Wherein, N represents data points of the time-domain signal after FFT in the range of effective band, and subscript i represents i-th Individual frequency values;|r(f;d,c2) | with | r (f;d,c2)|*The theoretical sound pressure reflection coefficient amplitude with actual measurement respectively in effective band Spectrum,WithThe theoretical arithmetic with the sound pressure reflection coefficient amplitude spectrum of actual measurement respectively in effective band Average value.
As shown in table 1, absolute error is 5 μ between coating layer thickness inversion result and actual measurement parameter for inversion result and measurement error M-8 μm, relative error be 2.53%-3.72%, between the velocity of sound and actual value absolute error be 4.3m/s-6.4m/s, relative error For 2.51%-3.75%, engineering detecting requirement is met.
The microwave absorbing coating sample parametric inversion result of table 1 and error

Claims (1)

1. a kind of coating thickness measurement method under velocity of ultrasonic sound unknown condition, it is characterized in that:Visited using a set of including ultrasonic wave Hinder instrument, delay block probe, digital oscilloscope and the ultrasonic pulse-echo detection system that the computer of MATLAB softwares is constituted is installed System;The measuring method uses the following steps:
(a) specimen surface is handled
Tested coating sample surface is handled using absolute ethyl alcohol or acetone cleaning agent, the oil that specimen surface is present is removed Dirty, organic solvent pollution thing, is suitably polished, it is ensured that sample table using the fine sandpaper position larger to specimen surface roughness Face is smooth, and chooses suitable couplant guarantee delay block probe and the good coupling being tested between coating sample according to coating characteristic Close;
(b) material properties are determined
Understand the density, the velocity of sound of acoustic attenuation coefficient and probe delay block and base material, density material of tested sample coating Attribute, respective acoustic impedance is calculated according to the velocity of sound and density of probe delay block and base material;
(c) ultrasonic probe is chosen
Suitable delay block ultrasound is chosen according to tested sample coating layer thickness, acoustical damping properties and the requirement to accuracy of detection to visit Head, acoustic attenuation thin to coating layer thickness is small, accuracy of detection requires high, and thickness measuring precision is improved from high frequency probe;To coating layer thickness Greatly, acoustic attenuation is serious, accuracy of detection requires low, and echo-signal can not be known caused by avoiding high frequency attenuation serious from low-frequency probe Not;
(d) parameter setting is detected
Pulse recurrence frequency PRF, ENERGY E nergy, gain G ain, filter bandwidht are arranged as required on reflectoscope Detect parameter;
(e) data acquisition
According to step (a)-(d) completion specimen surfaces are handled, material properties are determined, probe is chosen and detection parameter setting Afterwards, a delay block time domain echo-signal is gathered as reference signal, and delay block probe is then placed in tested sample surface, adjusted Whole digital oscilloscope gain, detecting way, average time, sampling frequency parameters, obtain complete, stable coating tim e- domain detection letter Number;
(f) coating sound pressure reflection coefficient amplitude spectrum is calculated
The time-domain signal that digital oscilloscope is collected is imported in computer, and FFT is carried out to it using data processing software Obtain the amplitude spectrum of reference signal | A (f) | and the amplitude spectrum of detection signal | A (f) |*, effective band is obtained according to formula (1) wide Spend undercoating actual measurement sound pressure reflection coefficient amplitude spectrum | r (f;d,c2)|*
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The material properties parameter obtained in step (b) is updated in formula (2) and obtains the internally coated theoretical acoustic pressure of effective bandwidth Reflectance magnitude is composed | r (f;d,c2)|:
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In formula, subscript 1,2,3 represents probe delay block, coating and base material, r respectively12、r23To represent Bimaterial in terface Sound pressure reflection coefficient, d be thickness of thin layer, c2It is respectively the rate of sound and attenuation of sound coefficient of coating with α (f);
(g) correlation coefficient matching method is analyzed
By assigning formula (2) coating thickness d and velocity of sound c2A series of consecutive variations values, obtain theoretical sound pressure reflection coefficient width Spectrum matrix is spent as parent, the reflectance magnitude spectrum obtained using formula (3) to theoretical calculation | r (f) | arrived with actually detected Reflectance magnitude spectrum | r (f) |*Carry out the matching analysis, correlation coefficient r one by one in -6dB effective bandsp(d,c2) dominant bit Put corresponding d and c2The as optimal inversion result of tested sample coating layer thickness and the velocity of sound:
<mrow> <msub> <mi>r</mi> <mi>p</mi> </msub> <mrow> <mo>(</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>=</mo> <mfrac> <mrow> <msubsup> <mi>&amp;Sigma;</mi> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>N</mi> </msubsup> <mo>&amp;lsqb;</mo> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> <mo>-</mo> <mover> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>&amp;OverBar;</mo> </mover> <mo>&amp;rsqb;</mo> <mo>&amp;lsqb;</mo> <msup> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>*</mo> </msup> <mo>-</mo> <mover> <msup> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>*</mo> </msup> <mo>&amp;OverBar;</mo> </mover> <mo>&amp;rsqb;</mo> </mrow> <msqrt> <mrow> <msubsup> <mi>&amp;Sigma;</mi> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>N</mi> </msubsup> <msup> <mrow> <mo>&amp;lsqb;</mo> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> <mo>-</mo> <mover> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>&amp;OverBar;</mo> </mover> <mo>&amp;rsqb;</mo> </mrow> <mn>2</mn> </msup> <msubsup> <mi>&amp;Sigma;</mi> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>N</mi> </msubsup> <msup> <mrow> <mo>&amp;lsqb;</mo> <msup> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>*</mo> </msup> <mo>-</mo> <mover> <msup> <mrow> <mo>|</mo> <mi>r</mi> <mrow> <mo>(</mo> <mi>f</mi> <mo>;</mo> <mi>d</mi> <mo>,</mo> <msub> <mi>c</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> <mo>|</mo> </mrow> <mo>*</mo> </msup> <mo>&amp;OverBar;</mo> </mover> <mo>&amp;rsqb;</mo> </mrow> <mn>2</mn> </msup> </mrow> </msqrt> </mfrac> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>3</mn> <mo>)</mo> </mrow> </mrow>
Wherein, N represents data points of the time-domain signal after FFT in the range of effective band, and subscript i represents i-th of frequency Rate value;|r(f;d,c2) | with | r (f;d,c2)|*The theoretical sound pressure reflection coefficient amplitude spectrum with actual measurement respectively in effective band,WithThe theoretical arithmetic average with the sound pressure reflection coefficient amplitude spectrum of actual measurement respectively in effective band Value.
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