CN111965651A - Method for testing plate thickness - Google Patents

Method for testing plate thickness Download PDF

Info

Publication number
CN111965651A
CN111965651A CN202010783247.0A CN202010783247A CN111965651A CN 111965651 A CN111965651 A CN 111965651A CN 202010783247 A CN202010783247 A CN 202010783247A CN 111965651 A CN111965651 A CN 111965651A
Authority
CN
China
Prior art keywords
waves
wave
compression
plate
different
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
CN202010783247.0A
Other languages
Chinese (zh)
Other versions
CN111965651B (en
Inventor
胡新发
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to CN202010783247.0A priority Critical patent/CN111965651B/en
Publication of CN111965651A publication Critical patent/CN111965651A/en
Application granted granted Critical
Publication of CN111965651B publication Critical patent/CN111965651B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S15/00Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems
    • G01S15/02Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems using reflection of acoustic waves
    • G01S15/06Systems determining the position data of a target
    • G01S15/08Systems for measuring distance only

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Acoustics & Sound (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Abstract

The invention discloses a method for testing plate thickness, which is characterized in that compression waves, shear waves and Rayleigh waves which are transmitted to the periphery are generated in stress waves excited by initial excitation, the Rayleigh waves occupy most of energy, the shear waves are second, the energy carried by the compression waves is minimum, the energy is attenuated in the process that all the waves are transmitted to the periphery at different speeds by taking an excitation point as a circle center, but the attenuation rate is the slowest with the Rayleigh waves, and because the energy of echo signals of the compression waves after being reflected by the bottom of a plate is very small, the influence of stimulated signaling is avoided. In order to avoid the influence of different wave velocities of compression waves of different concrete plates on a detection result due to different matching ratios, strengths, ages and the like, avoid the influence of different wave velocities of the compression waves on the detection result due to different plate sizes and different compression wave wavelengths and reduce the error of the detection result, the invention provides a method for measuring the plate thickness independent of the wave velocities of the compression waves of the plates.

Description

Method for testing plate thickness
Technical Field
The invention relates to the technical field of concrete plate thickness testing, in particular to a method for testing plate thickness.
Background
Concrete slabs, slabs made of reinforced concrete materials, are basic components in house buildings and various engineering structures, are commonly used as roof covers, floor systems, platforms, walls, retaining walls, foundations, terraces, pavements, pools and the like, have extremely wide application range, are divided into square slabs, circular slabs and special-shaped slabs according to planar shapes, are divided into unidirectional slabs and bidirectional slabs according to the stress action mode of the structure, are most commonly provided with the unidirectional slabs, the four-side supported bidirectional slabs and beamless flat slabs supported by columns, and need to be subjected to thickness detection before the completion of the engineering acceptance of the concrete slabs.
The invention provides a method for separating an excitation signal from an echo signal in a time domain and a method for measuring the plate thickness irrelevant to the compression wave velocity of a plate, aiming at the problems that the thickness of the structure such as the concrete plate is thin, the excitation signal and the echo signal are often interwoven together and cannot be separated in the time domain, the echo signal is separated by using a frequency spectrum analysis means such as FFT (fast Fourier transform algorithm), the effect is not ideal generally, the compression wave velocity of the concrete is preset according to experience, but the wave velocities of different concretes are not constant values, and the error caused by the fixed value is large.
In order to solve the problems, innovative design based on the original method for testing the thickness of the plate is urgently needed.
Disclosure of Invention
The invention solves the problems that the concrete slab and other structures are thin in thickness, excitation signals and echo signals of an acoustic echo method are often interwoven together and cannot be separated in a time domain, the echo signals are separated by means of frequency spectrum analysis means such as FFT (fast Fourier transform algorithm) and the like, but the effect is not ideal generally, the compression wave velocity of the concrete is preset according to experience, but the wave velocities of different concretes are not constant, and the error is large.
In order to solve the above technical problems, the present invention provides a method for measuring a sheet thickness, wherein a compression wave, a shear wave and a rayleigh wave are generated in a stress wave excited by an initial excitation, the rayleigh wave occupies most of energy, the shear wave has the lowest energy, the energy carried by the compression wave is the smallest, the energy is attenuated when each wave is transmitted to the periphery at different speeds with the excitation point as a center, but the attenuation rate is the slowest with the rayleigh wave, and the propagation speeds of the compression wave (P wave), the shear wave (S wave) and the rayleigh wave (R wave) are respectively:
velocity of compressional wave
Figure BDA0002620978840000021
Shear wave velocity
Figure BDA0002620978840000022
Wave velocity of Rayleigh wave
Figure BDA0002620978840000023
Wherein E-is the modulus of elasticity of the concrete;
g-shear modulus of concrete;
mu-Poisson's ratio of concrete, generally 0.2;
rho-mass density of the concrete,
the wave velocity is related to cP>cS>cR
Because the excitation energy occupied by the compression wave is very small, the longitudinal motion speed of the particle is mainly influenced by the shear wave and Rayleigh wave, the excitation point and the receiving point are positioned on the same side of the plate, and in order to ensure that the receiving point R is positioned on the same side of the plate1Firstly, receiving an echo signal of a P wave reflected by a plate bottom, and then receiving an S wave signal propagated along a surface, wherein the following steps are required:
Figure BDA0002620978840000024
where a-is the excitation point and the reception point R1The distance of (d);
h is the thickness of the plate,
and then have
Figure BDA0002620978840000031
The Poisson's ratio of concrete can be generally 0.2, but various special concretes are continuously emerged at present, and the Poisson's ratio of concrete is 0.10-0.30 calculated according to the formula (1) and the formula (2) in conclusion of previous researches
Figure BDA0002620978840000032
Is between 0.535 and 0.667, formula (5) can be simplified as:
a>1.8h (6)
for plates of other media, which typically have a Poisson ratio greater than 0.1, the above formula is also applicable,
from the equation (6), it can be seen that, as long as the distance between the excitation point and the receiving point is greater than 1.8 times the plate thickness, the receiving point receives the P-wave echo signal first, and separates the P-wave echo signal from the excitation signal, and for a material with a known poisson's ratio, for example, a steel plate with a poisson ratio of 0.25, according to the above calculation, the distance between the excitation point and the receiving point is greater than 1.5 times the plate thickness,
solves the problem of separating the excitation signal from the echo signal in the time domain, provides a method for testing the thickness of the plate,
excitation point and 1# receiving point R1A distance from the 2# reception point R2Has a distance of ka, k > 1, of
Figure BDA0002620978840000033
Figure BDA0002620978840000034
In the formula, t1、t2Respectively receiving points R1、R2The travel time of the echo signal of the P wave reflected by the bottom of the plate is received,
is represented by the formulae (7) and (8)
Figure BDA0002620978840000035
Further comprise
4(t2 2-t1 2)h2=(k2t1 2-t2 2)a2 (10)
Let λ be t2/t1Is provided with
Figure BDA0002620978840000041
From the formula (11), the plate thickness h is only related to the receiving-transmitting distance ratio k and the ratio lambda of the travel time of the two compression waves, and is not related to the wave velocity, so that the influence of different compression wave velocities of different concrete plates on the detection result due to different matching ratios, strengths, ages and other factors is avoided, and the influence of different compression wave velocities on the detection result due to different plate sizes and compression wave wavelengths is also avoided.
Has the advantages that: the method for testing the plate thickness avoids the influence of different wave velocities of the compression waves of different concrete plates on the detection result due to different matching ratios, strengths, ages and the like, also avoids the influence of different wave velocities of the compression waves on the detection result due to different plate sizes and compression wave wavelengths, improves the accuracy of the plate thickness test, and reduces the error of the detection result.
Detailed Description
The present invention will be further illustrated below with reference to specific embodiments, which are to be understood as merely illustrative and not limitative of the scope of the present invention.
A method for testing plate thickness is disclosed, wherein compression waves, shear waves and Rayleigh waves which propagate to the periphery are generated in stress waves excited by initial excitation, the Rayleigh waves occupy most of energy, the shear waves are the second order, the energy carried by the compression waves is the smallest, the energy is attenuated when each wave is transmitted to the periphery at different speeds by taking an excitation point as a circle center, but the attenuation rate is the slowest by the Rayleigh waves, and the propagation speeds of the compression waves (P waves), the shear waves (S waves) and the Rayleigh waves (R waves) are respectively as follows:
velocity of compressional wave
Figure BDA0002620978840000042
Shear wave velocity
Figure BDA0002620978840000043
Wave velocity of Rayleigh wave
Figure BDA0002620978840000051
Wherein E-is the modulus of elasticity of the concrete;
g-shear modulus of concrete;
mu-Poisson's ratio of concrete, generally 0.2;
rho-mass density of the concrete,
the wave velocity is related to cP>cS>cR
Because the excitation energy occupied by the compression wave is very small, the longitudinal motion speed of the particle is mainly influenced by the shear wave and Rayleigh wave, the excitation point and the receiving point are positioned on the same side of the plate, and in order to ensure that the receiving point R is positioned on the same side of the plate1Firstly, receiving an echo signal of a P wave reflected by a plate bottom, and then receiving an S wave signal propagated along a surface, wherein the following steps are required:
Figure BDA0002620978840000052
where a-is the excitation point and the reception point R1The distance of (d);
h is the thickness of the plate,
and then have
Figure BDA0002620978840000053
The Poisson's ratio of concrete can be generally 0.2, but various special concretes are continuously emerged at present, and the Poisson's ratio of concrete is 0.10-0.30 calculated according to the formula (1) and the formula (2) in conclusion of previous researches
Figure BDA0002620978840000054
Is between 0.535 and 0.667, formula (5) can be simplified as:
a>1.8h (6)
for plates of other media, which typically have a Poisson ratio greater than 0.1, the above formula is also applicable,
from the equation (6), it can be seen that, as long as the distance between the excitation point and the receiving point is greater than 1.8 times the plate thickness, the receiving point receives the P-wave echo signal first, and separates the P-wave echo signal from the excitation signal, and for a material with a known poisson's ratio, for example, a steel plate with a poisson ratio of 0.25, according to the above calculation method, the distance between the excitation point and the receiving point is greater than 1.5 times the plate thickness,
solves the problem of separating the excitation signal from the echo signal in the time domain, provides a method for testing the thickness of the plate,
excitation point and 1# receiving point R1A distance from the 2# reception point R2Has a distance of ka, k > 1, of
Figure BDA0002620978840000061
Figure BDA0002620978840000062
In the formula, t1、t2Respectively receiving points R1、R2The travel time of the echo signal of the P wave reflected by the bottom of the plate is received,
is represented by the formulae (7) and (8)
Figure BDA0002620978840000063
Further comprise
4(t2 2-t1 2)h2=(k2t1 2-t2 2)a2 (10)
Let λ be t2/t1Is provided with
Figure BDA0002620978840000064
From the formula (11), the plate thickness h is only related to the receiving-transmitting distance ratio k and the ratio lambda of the travel time of the two compression waves, and is not related to the wave velocity, so that the influence of different compression wave velocities of different concrete plates on the detection result due to different matching ratios, strengths, ages and other factors is avoided, and the influence of different compression wave velocities on the detection result due to different plate sizes and compression wave wavelengths is also avoided.
The method for testing the plate thickness has the following advantages:
the method for testing the plate thickness avoids the influence of different wave velocities of the compression waves of different concrete plates on the detection result due to different matching ratios, strengths, ages and the like, also avoids the influence of different wave velocities of the compression waves on the detection result due to different plate sizes and compression wave wavelengths, improves the accuracy of the plate thickness test, and reduces the error of the detection result.
The foregoing illustrates and describes the principles, general features, and advantages of the present invention. It will be understood by those skilled in the art that the present invention is not limited to the embodiments described above, which are described in the specification and illustrated only to illustrate the principle of the present invention, but that various changes and modifications may be made therein without departing from the spirit and scope of the present invention, which fall within the scope of the invention as claimed. The scope of the invention is defined by the appended claims and equivalents thereof.

Claims (1)

1. A method of testing sheet thickness, characterized by: in the stress wave excited by the initial excitation, bulk waves (compression waves and shear waves) and rayleigh waves propagating to the periphery are generated, the rayleigh waves occupy most of energy, the shear waves are the second order, the energy carried by the compression waves is the minimum, and in the process that all the waves are transmitted to the periphery at different speeds by taking an excitation point as a circle center, the energy is attenuated, but the attenuation rate is the slowest by the rayleigh waves, and the propagation speeds of the compression waves (P waves), the shear waves (S waves) and the rayleigh waves (R waves) are respectively:
velocity of compressional wave
Figure FDA0002620978830000011
Shear wave velocity
Figure FDA0002620978830000012
Wave velocity of Rayleigh wave
Figure FDA0002620978830000013
Wherein E-is the elastic modulus of the concrete;
g-shear modulus of concrete;
mu-Poisson's ratio of concrete, generally 0.2;
rho-the mass density of the concrete,
the wave velocity relationship is as follows: c. CP>cS>cR
Because the excitation energy occupied by the compression wave is very small, the longitudinal motion speed of the particle is mainly influenced by the shear wave and Rayleigh wave, the excitation point and the receiving point are positioned on the same side of the plate, and in order to ensure that the receiving point R is positioned on the same side of the plate1Firstly, receiving an echo signal of a P wave reflected by a plate bottom, and then receiving an S wave signal propagated along a surface, wherein the following steps are required:
Figure FDA0002620978830000014
wherein a-is the excitation point and the receiving point R1The distance of (d);
h-is the thickness of the plate,
and then have
Figure FDA0002620978830000021
The Poisson's ratio of concrete can be generally 0.2, but various special concretes are continuously emerged at present, and the Poisson's ratio of concrete is 0.10-0.30 calculated according to the formula (1) and the formula (2) in conclusion of previous researches
Figure FDA0002620978830000022
Is between 0.535 and 0.667, formula (5) can be simplified as:
a>1.8h (6)
for plates of other media, which typically have a Poisson ratio greater than 0.1, the above formula is also applicable,
from the equation (6), it can be seen that, as long as the distance between the excitation point and the receiving point is greater than 1.8 times the plate thickness, the receiving point receives the P-wave echo signal first, and separates the P-wave echo signal from the excitation signal, and for a material with a known poisson's ratio, for example, a steel plate with a poisson ratio of 0.25, according to the above calculation method, the distance between the excitation point and the receiving point is greater than 1.5 times the plate thickness,
solves the problem of separating the excitation signal from the echo signal in the time domain, provides a method for testing the thickness of the plate,
excitation point and 1# receiving point R1A distance from the 2# reception point R2Has a distance of ka, k > 1, of
Figure FDA0002620978830000023
Figure FDA0002620978830000024
In the formula, t1、t2Respectively receiving points R1、R2The travel time of the echo signal of the P wave reflected by the bottom of the plate is received,
is represented by the formulae (7) and (8)
Figure FDA0002620978830000025
Further comprise
4(t2 2-t1 2)h2=(k2t1 2-t2 2)a2 (10)
Let λ be t2/t1Is provided with
Figure FDA0002620978830000031
From the formula (11), the plate thickness h is only related to the receiving-transmitting distance ratio k and the ratio lambda of the travel time of the two compression waves, and is not related to the wave velocity, so that the influence of different compression wave velocities of different concrete plates on the detection result due to different matching ratios, strengths, ages and other factors is avoided, and the influence of different compression wave velocities on the detection result due to different plate sizes and compression wave wavelengths is also avoided.
CN202010783247.0A 2020-08-06 2020-08-06 Method for testing plate thickness Active CN111965651B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010783247.0A CN111965651B (en) 2020-08-06 2020-08-06 Method for testing plate thickness

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010783247.0A CN111965651B (en) 2020-08-06 2020-08-06 Method for testing plate thickness

Publications (2)

Publication Number Publication Date
CN111965651A true CN111965651A (en) 2020-11-20
CN111965651B CN111965651B (en) 2022-05-13

Family

ID=73364615

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010783247.0A Active CN111965651B (en) 2020-08-06 2020-08-06 Method for testing plate thickness

Country Status (1)

Country Link
CN (1) CN111965651B (en)

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5663502A (en) * 1994-10-18 1997-09-02 Hitachi, Ltd. Method and apparatus for measuring thickness of layer using acoustic waves
EP1505252A1 (en) * 2003-08-08 2005-02-09 Services Petroliers Schlumberger Multimode acoustic imaging in cased wells
TWI231362B (en) * 2002-04-12 2005-04-21 Yi-Ching Lin Method for measuring speed of longitudinal wave and thickness inside concrete plate by using stress wave
US20090007678A1 (en) * 2005-07-06 2009-01-08 Hiroyuki Fukutomi Method and apparatus for measuring flaw height in ultrasonic tests
US20150309007A1 (en) * 2014-04-29 2015-10-29 NLA Diagnostics LLC Apparatus and method for non-destructive testing of concrete
US20160363561A1 (en) * 2014-02-26 2016-12-15 Sintef Tto As Methods and systems for measuring properties with ultrasound
CN107192624A (en) * 2017-03-22 2017-09-22 国家电网公司 A kind of concrete strength detecting method based on impact elasticity ripple
CN110133105A (en) * 2019-05-31 2019-08-16 水利部交通运输部国家能源局南京水利科学研究院 A kind of non-contact non-destructive testing method of water logging concrete strength
US20200096330A1 (en) * 2016-12-22 2020-03-26 Posco Apparatus for measuring crystal grain size of steel sheet

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5663502A (en) * 1994-10-18 1997-09-02 Hitachi, Ltd. Method and apparatus for measuring thickness of layer using acoustic waves
TWI231362B (en) * 2002-04-12 2005-04-21 Yi-Ching Lin Method for measuring speed of longitudinal wave and thickness inside concrete plate by using stress wave
EP1505252A1 (en) * 2003-08-08 2005-02-09 Services Petroliers Schlumberger Multimode acoustic imaging in cased wells
US20090007678A1 (en) * 2005-07-06 2009-01-08 Hiroyuki Fukutomi Method and apparatus for measuring flaw height in ultrasonic tests
US20160363561A1 (en) * 2014-02-26 2016-12-15 Sintef Tto As Methods and systems for measuring properties with ultrasound
US20150309007A1 (en) * 2014-04-29 2015-10-29 NLA Diagnostics LLC Apparatus and method for non-destructive testing of concrete
US20200096330A1 (en) * 2016-12-22 2020-03-26 Posco Apparatus for measuring crystal grain size of steel sheet
CN107192624A (en) * 2017-03-22 2017-09-22 国家电网公司 A kind of concrete strength detecting method based on impact elasticity ripple
CN110133105A (en) * 2019-05-31 2019-08-16 水利部交通运输部国家能源局南京水利科学研究院 A kind of non-contact non-destructive testing method of water logging concrete strength

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
向阳等: "板状混凝土结构波速测量和板厚测量的研究", 《武汉理工大学学报(交通科学与工程版)》 *
崔德密等: "基于冲击回波法的混凝土厚度测试研究与评价", 《人民黄河》 *
杜正聪等: "高炉炉衬厚度检测技术性能分析与改进算法研究", 《中国测试》 *

Also Published As

Publication number Publication date
CN111965651B (en) 2022-05-13

Similar Documents

Publication Publication Date Title
Kelder et al. Observation of the Biot slow wave in water-saturated Nivelsteiner sandstone
Pyrak-Nolte et al. Elastic interface waves propagating in a fracture
Chekroun et al. Analysis of coherent surface wave dispersion and attenuation for non-destructive testing of concrete
Le Clézio et al. The interaction of the S0 Lamb mode with vertical cracks in an aluminium plate
LeBlanc et al. Sonar attenuation modeling for classification of marine sediments
CN103926315A (en) Method for obtaining elastic property of isotropous sheet material based on simplex method
Leclaire et al. Observation of two longitudinal and two transverse waves in a frozen porous medium
CN111965651B (en) Method for testing plate thickness
CN101915602B (en) Method for measuring sound velocities in elastic solids
Xu et al. Lamb wave dispersion compensation in piezoelectric wafer active sensor phased-array applications
WO1988001054A1 (en) Measuring metal hardness utilizing ultrasonic wave time-of-flight
Tallavó et al. New methodology for source characterization in pulse velocity testing
Crispin et al. Thickness-resonance waves in underlays of floating screed
CN106597546A (en) Method for detecting river bottom surface sediment physical properties
Aggelis et al. AE Applied to Fresh Concrete
Egle et al. Considerations for the detection of acoustic emission waves in thin plates
Massaad et al. Acoustic design of a transducer array for ultrasonic clamp-on flow metering
Aggelis et al. Acoustic emission characterization of fresh cement-based materials
Kautz Ray propagation path analysis of acousto-ultrasonic signals in composites
Maji et al. Improved impact-echo technique by signal processing
Gu et al. Interdigitated PVDF transducer for Lamb wave generation and reception
Ortiz-Osornio et al. Physical modeling of the reflectivity and transmissivity dependence on tilt and azimuth of a material with orthorhombic symmetry
Anisimkin A new type of acoustic modes of vibration of thin piezoelectric plates: Quasi-longitudinal normal modes
Cui et al. Anomalous dispersion of flexural guided waves in clad rods
Prosser et al. Propagation of flexural mode AE signals in GR/EP composite plates

Legal Events

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