CN115047079A - Ultrasonic phased array rapid focusing method for multilayer composite board - Google Patents

Ultrasonic phased array rapid focusing method for multilayer composite board Download PDF

Info

Publication number
CN115047079A
CN115047079A CN202210986070.3A CN202210986070A CN115047079A CN 115047079 A CN115047079 A CN 115047079A CN 202210986070 A CN202210986070 A CN 202210986070A CN 115047079 A CN115047079 A CN 115047079A
Authority
CN
China
Prior art keywords
point
multilayer composite
ultrasonic
ultrasonic beam
composite board
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
CN202210986070.3A
Other languages
Chinese (zh)
Other versions
CN115047079B (en
Inventor
邓川
范祥祥
郭思进
祁帅
汤伟伟
刘鹏程
曹羽
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.)
NANTONG UNION DIGITAL TECHNOLOGY DEVELOPMENT CO LTD
Original Assignee
NANTONG UNION DIGITAL TECHNOLOGY DEVELOPMENT CO LTD
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 NANTONG UNION DIGITAL TECHNOLOGY DEVELOPMENT CO LTD filed Critical NANTONG UNION DIGITAL TECHNOLOGY DEVELOPMENT CO LTD
Priority to CN202210986070.3A priority Critical patent/CN115047079B/en
Publication of CN115047079A publication Critical patent/CN115047079A/en
Application granted granted Critical
Publication of CN115047079B publication Critical patent/CN115047079B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/22Details, e.g. general constructional or apparatus details
    • G01N29/221Arrangements for directing or focusing the acoustical waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/02Indexing codes associated with the analysed material
    • G01N2291/023Solids
    • G01N2291/0231Composite or layered materials
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/02Indexing codes associated with the analysed material
    • G01N2291/028Material parameters
    • G01N2291/0289Internal structure, e.g. defects, grain size, texture

Landscapes

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

Abstract

The invention relates to an ultrasonic phased array rapid focusing method for a multilayer composite board, which is characterized in that an incident point R of an ultrasonic beam on the surface of the multilayer composite board is set 1 And obtaining the difference between the theoretical focusing point and the appointed focusing point through simple trigonometric function operation, and appointing the incidence point R again according to the difference 1 The actual incident point R is realized by the mode whether the horizontal coordinate range reaches the specified precision or not 1 And (4) obtaining. Then passes through the actual incident point R 1 The transmission time of the wafer and the relative delay time between the excitation signals of the wafers are obtained by the coordinate calculation, so that the delay excitation of the wafers is realized, and the aim of focusing the ultrasonic beam on a theoretical focus point is fulfilled. Compared with the existing calculation method, the method has the advantages that the ultrasonic beams emitted by the ultrasonic phased array are focused, the calculated amount is greatly simplified, and the focusing efficiency is higher.

Description

Ultrasonic phased array rapid focusing method for multilayer composite board
Technical Field
The invention relates to a focusing method of an ultrasonic phased array, in particular to a rapid focusing method of the ultrasonic phased array for a multilayer composite board.
Background
The concept of the ultrasonic phased array detection technology comes from the modern phased array radar technology, and the ultrasonic phased array detection technology can control ultrasonic beams to be synthesized by using multi-channel electron beams, so that different focusing or deflection forms of the synthesized beams are realized. The probe of the ultrasonic phased array is composed of a large number of piezoelectric ceramic wafers, and each wafer is independent from each other and can independently complete the transmission and the reception of ultrasonic waves. They are arranged according to a certain form to form a phased array ultrasonic transmitting and receiving array. The theoretical basis of the ultrasonic phased array detection technology is the Huygens Fresnel principle. According to the explanation of the principle, coherent waves can generate interference phenomena in the medium, thereby forming a stable sound field. Therefore, by controlling the time for generating the ultrasonic wave by each wafer in the phased array transducer, the ultrasonic wave can form a stable ultrasonic field, and the excitation pulse time of each wafer is accurately controlled (namely, each wafer is delayed to be de-excited according to a certain focusing algorithm), so that the ultrasonic field can realize the characteristics of focusing or deflection and the like.
At present, in the phased array ultrasonic flaw detection of a common single-layer plate, the system can conveniently calculate the pulse excitation delay time of each wafer through the positions of the wafers and the focus points so as to realize the accurate focusing of an ultrasonic wave array surface. However, in actual flaw detection, in order to protect the expensive phased array probe and change the effective coverage of the sound field of the probe, a wedge block is usually installed on the phased array probe. After the wedge block is additionally arranged, due to the fact that ultrasound refracts between the wedge block and a workpiece, the calculation formula of the excitation pulse time is complex, the direct solving difficulty is high, and the efficiency is low. The system can obtain an incidence point through dichotomy approximation, and then obtain the delay time of each wafer from the incidence point. For another example, the calculation method disclosed in chinese patent publication No. 106383171 entitled transverse wave full-focus ultrasonic imaging detection method for crack defects in steel plate welds is complex and inefficient.
In addition, for the multilayer composite board formed by parallel stacking and pressing of multilayer plates, due to different materials of each layer, ultrasonic waves can be sequentially refracted in each layer, the calculation difficulty of delay time is exponentially increased, for example, from a single-layer board to a k-layer board, and the upper bound of the time complexity of the conventional bisection method is defined by
Figure DEST_PATH_IMAGE001
Directly rise to
Figure 394085DEST_PATH_IMAGE002
Thereby greatly reducing the flaw detection efficiency.
Disclosure of Invention
In order to solve the technical problems, the invention aims to provide a simple ultrasonic phased array rapid focusing method with high focusing efficiency for a multilayer composite board.
The invention relates to an ultrasonic phased array rapid focusing method for a multilayer composite board, which comprises the steps of attaching an ultrasonic phased array probe with a wedge block at the front end to the surface of the multilayer composite board, and the ultrasonic phased array rapid focusing method for the multilayer composite board further comprises the following steps;
s1, in the section of the multilayer composite board passing through the appointed focus point, taking the direction parallel to the surface of the multilayer composite board as the abscissa direction, and taking the direction vertical to the abscissa as the ordinate direction;
s2, selecting an incidence point R on the boundary line of the wedge block and the multilayer composite board in the section 1 Incident point R 1 Abscissa R of 1x In the range of
Figure DEST_PATH_IMAGE003
And is and
Figure 655433DEST_PATH_IMAGE004
wherein the incident point R 1 For the point of incidence of the ultrasonic beam on the surface of the multilayer composite panel, E x Abscissa of point E of the wafer, F x The abscissa of the designated focus point F;
s3, taking incident point R 1 Has the coordinates of (R) 1x ,R 1y ) Wherein R is 1x =(R min +R max )/2,R 1y The longitudinal coordinate value of the surface of the multilayer composite board is equal to;
s4, according to the coordinate value of the wafer E and the incident point R in the step S3 1 Calculating the incident angle of the ultrasonic beam emitted by the wafer on the surface of the multilayer composite board
Figure DEST_PATH_IMAGE005
S5, from the incident angle obtained in the step S4
Figure 513799DEST_PATH_IMAGE005
And calculating the refraction angle of the ultrasonic beam in the first laminate by the law of refraction
Figure 518795DEST_PATH_IMAGE006
S6, the incident point R of the ultrasonic beam on the surface of the multilayer composite board in the step S3 1 The angle of refraction obtained in step S5
Figure 677375DEST_PATH_IMAGE006
Calculating the incident point position of the ultrasonic beam on the surfaces of the second layer plate and the Nth layer plate and the refraction angle of the ultrasonic beam in the second layer plate and the Nth layer plate in sequence, wherein the Nth layer plate is a plate layer where the designated focus point is located;
s7, an incident point R of the ultrasonic beam on the surface of the Nth plate obtained in the step S6 N Angle of refraction
Figure DEST_PATH_IMAGE007
And the distance h between the designated focus point F and the surface of the Nth layer plate f Calculating the coordinate of a theoretical focusing point F';
s8, comparing the difference Delta between the specified focus point F and the theoretical focus point F' in the horizontal coordinate direction, wherein,
Δ=F x -
Figure 844046DEST_PATH_IMAGE008
Figure 720866DEST_PATH_IMAGE008
is the abscissa of the theoretical focus point F';
if Δ>0, reassigning the incident point R in step S2 1 Range of abscissa
Figure DEST_PATH_IMAGE009
If Δ<0, reassigning the incident point R in the step S2 1 Range of abscissa
Figure 998394DEST_PATH_IMAGE010
If Δ =0, the incident point R in step S2 is reassigned 1 Range of abscissa
Figure DEST_PATH_IMAGE011
If abs (
Figure 745902DEST_PATH_IMAGE012
) When the specified accuracy range is reached, the incident point R selected in step S3 is used 1 The coordinate of the ultrasonic beam is the actual incident point coordinate of the ultrasonic beam on the surface of the multilayer composite board, and the transmission time of the ultrasonic beam from the wafer position to the appointed focus point is calculated;
if abs (
Figure 83473DEST_PATH_IMAGE012
) If the specified precision range is not reached, the incidence point R is used 1 The re-designated abscissa range repeats steps S3 through S8 until abs (S) ((S))
Figure 306644DEST_PATH_IMAGE012
) Reaching the specified precision range;
wherein abs is an absolute value function;
s9, calculating the transmission time of the ultrasonic beams from the wafer position to the appointed focus point of all the wafers in the ultrasonic phased array according to the calculation method of the steps S2 to S8;
s10, acquiring the relative delay time between the pulse excitation signals of the wafers according to the transmission time of each wafer of the ultrasonic phased array;
s11, the ultrasonic phased array wafers are time-delayed and excited by the relative delay time acquired in the step S10 to achieve focusing.
Further, the method for rapidly focusing the ultrasonic phased array for the multilayer composite board of the invention comprises the following steps of sequentially calculating the incident point position of the ultrasonic beam on the surfaces of the second layer board to the Nth layer board and the refraction angle of the ultrasonic beam in the second layer board to the Nth layer board in step S6;
step S61 of obtaining incident point from incident point R n Angle of refraction
Figure DEST_PATH_IMAGE013
And the layer height h of the nth layer plate of the multilayer composite plate n Calculating the incident point R of the ultrasonic beam on the surface of the (n + 1) th layer plate of the multilayer composite plate n+1
Step S62 of obtaining a refraction angle, an incident angle on the surface of the (n + 1) th layer plate by an ultrasonic beam
Figure 856705DEST_PATH_IMAGE014
And calculating the refraction angle of the ultrasonic beam in the (n + 1) th layer plate according to the law of refraction
Figure DEST_PATH_IMAGE015
Wherein
Figure 599665DEST_PATH_IMAGE014
=
Figure 170454DEST_PATH_IMAGE013
Where N =1, 2 … … N, N is the nth plate where the specified focus point F is located.
The ultrasonic phased array rapid focusing method for the multilayer composite board has the advantage that the ultrasonic phased array rapid focusing method for the multilayer composite board is used for setting the incident point R of an ultrasonic beam on the surface of the multilayer composite board 1 And obtaining the difference between the theoretical focusing point and the appointed focusing point through simple trigonometric function operation, and appointing the incidence point R again according to the difference 1 The abscissa range of (a). Then whether the range of the abscissa reaches the specified precision or not realizes the actual incident point R 1 And (4) obtaining. Then passes through the actual incident point R 1 The transmission time of the wafer and the relative delay time between the excitation signals of the wafers are obtained by the coordinate calculation, so that the delay excitation of the wafers is realized, and the aim of focusing the ultrasonic beam on a theoretical focus point is fulfilled. Compared with the existing calculation method, the method has the advantages that the ultrasonic beams emitted by the ultrasonic phased array are focused, the calculated amount is greatly simplified, and the focusing efficiency is higher.
The above description is only an overview of the technical solutions of the present invention, and in order to make the technical means of the present invention more clearly understood and to implement the technical means in accordance with the content of the description, the embodiments of the present invention are described in detail below.
Drawings
FIG. 1 is a schematic illustration of the propagation of an ultrasonic beam within a multilayer composite panel;
FIG. 2 is a flow chart of the calculation of the wafer to specified focus transit time;
fig. 3 is a flow chart of the calculation of the relative excitation time.
Detailed Description
The following detailed description of embodiments of the present invention is provided in connection with the accompanying drawings and examples. The following examples are intended to illustrate the invention but are not intended to limit the scope of the invention.
Referring to fig. 1 to 3, the ultrasonic phased array fast focusing method for a multilayer composite board of the present embodiment includes a step of attaching an ultrasonic phased array probe having a wedge at a front end to a surface of the multilayer composite board, and further includes the following steps;
s1, in the section of the multilayer composite board passing through the appointed focus point, taking the direction parallel to the surface of the multilayer composite board as the abscissa direction, and taking the direction vertical to the abscissa as the ordinate direction;
in this embodiment, in the probe of the ultrasonic phased array, a plurality of crystals are arranged in a linear array on the cross section, and an ultrasonic beam emitted by each crystal is transmitted in the cross section and refracted by the wedge and the multilayer composite board to reach a focus point at a specified depth.
Wherein, the abscissa direction can be directly selected from the surfaces of the multilayer composite boards, and at the moment, the ordinate of the surfaces of the multilayer composite boards is 0; the origin of coordinates can be arranged at the joint of the bottom corner of the wedge block and the multilayer composite board.
S2, selecting an incidence point R on the boundary line of the wedge block and the multilayer composite board in the section 1 Incident point R 1 Abscissa R of 1x In the range of
Figure 21867DEST_PATH_IMAGE003
And is and
Figure 500253DEST_PATH_IMAGE004
wherein the incident point R 1 For the point of incidence of the ultrasonic beam on the surface of the multilayer composite panel, E x Is the abscissa of point E on the wafer, F x The abscissa of the designated focus point F;
according to the snell's law of refraction, the abscissa of all incident points should be located at the wafer E and the focus point
Figure 776948DEST_PATH_IMAGE016
At a position in between, thus setting the point of incidence R here 1 Abscissa R of 1x Range
Figure 315377DEST_PATH_IMAGE004
The coordinates of the wafer E are determined by the installation position of the ultrasonic phased array wafer and the attributes of the wedge block, and specific numerical values of the wafer E can be obtained according to product description, measurement or calculation and stored in a system memory.
The coordinates of the designated focusing point F are designated by a system during detection, the number of the layers of the plate where the system is located can be calculated through the thickness of each layer of the plate of the multilayer composite plate, and the description is omitted here.
S3, taking incident point R 1 Has the coordinates of (R) 1x ,R 1y ) Wherein R is 1x =(R min +R max )/2,R 1y Equal to the surface of the multilayer composite boardThe longitudinal coordinate value of the position;
here, R is 1x Is arranged as (R) min +R max ) 2, i.e. at the point of incidence R 1 Selecting a midpoint thereof as an incident point R within the range of the abscissa 1 The coordinates of (a).
When the abscissa is set on the surface of the multilayer composite board, R 1y =0;
S4, according to the coordinate value of the wafer E and the incident point R in the step S3 1 Calculating the incident angle of the ultrasonic beam emitted by the wafer on the surface of the multilayer composite board
Figure 919665DEST_PATH_IMAGE005
Specifically, as can be seen from the arctan function,
Figure 873845DEST_PATH_IMAGE005
=arctan( | R 1x -E x | ÷ |R 1y -E y | )。
s5, from the incident angle obtained in the step S4
Figure 716031DEST_PATH_IMAGE005
And the law of refraction, calculating the refraction angle of the ultrasonic beam in the first laminate
Figure 222098DEST_PATH_IMAGE006
In particular, angle of refraction
Figure 782524DEST_PATH_IMAGE006
=arcsin(sin
Figure 274816DEST_PATH_IMAGE005
N) where n is the relative refractive index of the first ply, which is determined by the particular type of sheet material.
S6, the incident point R of the ultrasonic beam on the surface of the multilayer composite board in the step S3 1 The angle of refraction obtained in step S5
Figure 96142DEST_PATH_IMAGE006
And law of refraction, in turnCalculating the incident point position of the ultrasonic beam on the surfaces of the second layer plate and the Nth layer plate and the refraction angle of the ultrasonic beam in the second layer plate and the Nth layer plate, wherein the Nth layer plate is a plate layer where the designated focus point is located;
s7, an incident point R of the ultrasonic beam on the surface of the Nth plate obtained in the step S6 N Angle of refraction
Figure 648477DEST_PATH_IMAGE007
And the distance h between the designated focus point F and the surface of the Nth layer plate f Calculating the coordinate of a theoretical focusing point F';
specifically, let the coordinate of the theoretical focus F' be: (
Figure DEST_PATH_IMAGE017
) Then, then
Figure 571564DEST_PATH_IMAGE008
=R Nx +h f × tan
Figure 601969DEST_PATH_IMAGE007
Figure 808959DEST_PATH_IMAGE018
=R Ny +h f
S8, comparing the difference delta between the specified focus point F and the theoretical focus point F' in the horizontal coordinate direction, wherein,
Δ=F x -
Figure 1037DEST_PATH_IMAGE008
Figure 129530DEST_PATH_IMAGE008
is the abscissa of the theoretical focus point F';
if Δ>0, reassigning the incident point R in step S2 1 Range of abscissa
Figure 494783DEST_PATH_IMAGE009
Here,. DELTA.>0 means F x >
Figure 900488DEST_PATH_IMAGE008
I.e. the calculated theoretical focus point is located at the left side of the designated focus point, the actual incident point R 1 The abscissa is necessarily located at the set incident point R 1 Between the abscissa and the abscissa of the designated focus point F, the incident point R set in the next round of calculation is set 1 Range of abscissa
Figure 388101DEST_PATH_IMAGE009
If Δ<0, reassigning the incident point R in the step S2 1 Range of abscissa
Figure 3890DEST_PATH_IMAGE010
Similarly, the actual point of incidence R at this time 1 The abscissa is necessarily located between the abscissa of the wafer E and the set incident point R 1 Between the abscissas, hence the incidence point R set in the next calculation round 1 Range of abscissa
Figure 376097DEST_PATH_IMAGE010
If Δ =0, the incident point R in step S2 is reassigned 1 Range of abscissa
Figure 292100DEST_PATH_IMAGE011
At this time, the actual incident point is set to be as set R 1 Coincident, thus set, incident point R 1 Range of abscissa
Figure 560402DEST_PATH_IMAGE011
At this time abs: (
Figure 929066DEST_PATH_IMAGE012
)=0。
If abs (
Figure 839385DEST_PATH_IMAGE012
) When the specified accuracy range is reached, the incident point R selected in step S3 is used 1 The coordinate of the ultrasonic beam is the actual incident point coordinate of the ultrasonic beam on the surface of the multilayer composite board, and the transmission time of the ultrasonic beam from the wafer position to the appointed focus point is calculated;
the specific value of the transmission time can be obtained by removing the transmission speed of the ultrasonic beam in the wedge block or a certain layer of composite board, the value of the transmission speed is determined by the type of the medium, and the transmission distance can be calculated by trigonometric theory, which is not repeated herein.
If abs (
Figure 609894DEST_PATH_IMAGE012
) If the specified precision range is not reached, the incidence point R is used 1 The re-designated abscissa range repeats steps S3 through S8 until abs (S) ((S))
Figure 173731DEST_PATH_IMAGE012
) Reaching the specified precision range;
wherein abs is an absolute value function;
the specified precision range can be manually set according to the precision requirement of flaw detection, the flaw detection precision is usually less than 0.001mm, and the system can be manually adjusted according to the specific requirement in specific implementation.
S9, calculating the transmission time of the ultrasonic beams from the wafer position to the appointed focus point of all the wafers in the ultrasonic phased array according to the calculation method of the steps S2 to S8;
s10, acquiring the relative delay time between the pulse excitation signals of the wafers according to the transmission time of each wafer of the ultrasonic phased array;
the calculation of the relative delay time is based on that the ultrasonic beams emitted by each wafer can be stably interfered to form wave fronts with corresponding shapes and focus on the appointed focus point F, and the specific calculation process is a conventional technique in the field, and reference may be made to related documents such as "research on ultrasonic phased array sector scanning detection imaging technology" published by the university of harbinge industry, which is not described herein again.
S11, the ultrasonic phased array wafers are time-delayed and excited by the relative delay time acquired in the step S10 to achieve focusing.
The invention relates to an ultrasonic phased array rapid focusing method for a multilayer composite board, which is characterized in that an incident point R of an ultrasonic beam on the surface of the multilayer composite board is set 1 And obtaining the difference between the theoretical focusing point and the appointed focusing point through simple trigonometric function operation, and appointing the incidence point R again according to the difference 1 The abscissa range of (a). Then whether the range of the horizontal coordinate reaches the specified precision or not is judged, and the actual incident point R is realized 1 And (4) obtaining. Then passes through the actual incident point R 1 The transmission time of the wafer and the relative delay time between the excitation signals of the wafers are obtained by the coordinate calculation, so that the delay excitation of the wafers is realized, and the aim of focusing the ultrasonic beam on a theoretical focus point is fulfilled. Compared with the existing calculation method, the method has the advantages that the ultrasonic beams emitted by the ultrasonic phased array are focused, the calculated amount is greatly simplified, and the focusing efficiency is higher.
Preferably, in step S6, the method for calculating the incident point position of the ultrasonic beam on the surface of the second to nth plates and the refraction angle of the ultrasonic beam in the second to nth plates in sequence comprises the following steps;
step S61 of obtaining incident point from incident point R n Angle of refraction
Figure 905058DEST_PATH_IMAGE013
And the layer height h of the nth layer plate of the multilayer composite plate n Calculating the incident point R of the ultrasonic beam on the surface of the (n + 1) th layer plate of the multilayer composite plate n+1
Step S62 of obtaining a refraction angle, an incident angle on the surface of the (n + 1) th layer plate by an ultrasonic beam
Figure 743701DEST_PATH_IMAGE014
And calculating the refraction angle of the ultrasonic beam in the (n + 1) th layer plate according to the law of refraction
Figure 712925DEST_PATH_IMAGE015
Wherein
Figure 713242DEST_PATH_IMAGE014
=
Figure 790919DEST_PATH_IMAGE013
N =1, 2 … … N, where N is the nth layer plate where the designated focus point F is located;
the calculation methods of the incident point position and the refraction angle of the ultrasonic beam on the second layer plate to the Nth layer plate are similar, and the second layer plate is taken as an example.
From the point of incidence R 1 Angle of refraction
Figure 43040DEST_PATH_IMAGE006
And the layer height h of the first laminate 1 Calculating the incident point R of the ultrasonic beam on the surface of the second layer plate of the multilayer composite plate 2 The method comprises the following steps:
R 2x =R 1x +h 1 × tan
Figure 256984DEST_PATH_IMAGE006
,
R 2y =R 1y +h 1 ;
angle of incidence of ultrasonic beam on second layer plate surface
Figure DEST_PATH_IMAGE019
And calculating the refraction angle of the ultrasonic beam in the second laminate by the law of refraction
Figure 303568DEST_PATH_IMAGE020
Because the upper and lower surfaces of each layer of the multilayer composite board are parallel, the multilayer composite board has the advantages of simple structure, low cost and high reliability
Figure 602963DEST_PATH_IMAGE019
=
Figure 393195DEST_PATH_IMAGE006
Figure DEST_PATH_IMAGE021
2 =arcsin(sin
Figure 337012DEST_PATH_IMAGE019
N2) where n2 is the relative refractive index of the second layer sheet.
The calculation method from the third layer plate to the Nth layer plate is similar to that of the first layer plate, and the description is omitted here.
The above description is only a preferred embodiment of the present invention, which is used to assist those skilled in the art to implement the corresponding technical solutions, and is not used to limit the protection scope of the present invention, which is defined by the appended claims. It should be noted that, for those skilled in the art, on the basis of the technical solution of the present invention, several modifications and variations can be made equivalent thereto, and these modifications and variations should also be regarded as the protection scope of the present invention. Also, it should be understood that although the present description has been described in terms of the above embodiments, not every embodiment may include only a single embodiment, and such description is for clarity only, and those skilled in the art will recognize that the description is taken as a whole, and that the embodiments may be suitably combined to form other embodiments as will be appreciated by those skilled in the art.

Claims (2)

1. The ultrasonic phased array rapid focusing method for the multilayer composite board comprises the step of attaching an ultrasonic phased array probe with a wedge block at the front end to the surface of the multilayer composite board, and is characterized in that: the ultrasonic phased array rapid focusing method for the multilayer composite board further comprises the following steps;
s1, in the section of the multilayer composite board passing through the appointed focus point, taking the direction parallel to the surface of the multilayer composite board as the abscissa direction, and taking the direction vertical to the abscissa as the ordinate direction;
s2, selecting an incidence point R on the boundary line of the wedge block and the multilayer composite board in the section 1 Incident point R 1 Abscissa R of 1x In the range of
Figure DEST_PATH_IMAGE002
And is and
Figure DEST_PATH_IMAGE004
wherein the incident point R 1 For the point of incidence of the ultrasonic beam on the surface of the multilayer composite panel, E x Is the abscissa of point E on the wafer, F x The abscissa of the designated focus point F;
s3, taking incident point R 1 Has the coordinates of (R) 1x ,R 1y ) Wherein R is 1x =(R min +R max )/2,R 1y The longitudinal coordinate value of the surface of the multilayer composite board is equal to;
s4, according to the coordinate value of the wafer E and the incident point R in the step S3 1 Calculating the incident angle of the ultrasonic beam emitted by the wafer on the surface of the multilayer composite board
Figure DEST_PATH_IMAGE006
S5, from the incident angle obtained in the step S4
Figure 116650DEST_PATH_IMAGE006
And calculating the refraction angle of the ultrasonic beam in the first laminate by the law of refraction
Figure DEST_PATH_IMAGE008
S6, the ultrasonic beam is incident on the surface of the multilayer composite board at the incident point R in the step S3 1 Coordinates of (d), the refraction angle acquired in step S5
Figure 50102DEST_PATH_IMAGE008
Calculating the incident point position of the ultrasonic beam on the surfaces of the second layer plate and the Nth layer plate and the refraction angle of the ultrasonic beam in the second layer plate and the Nth layer plate in sequence, wherein the Nth layer plate is a plate layer where the designated focus point is located;
s7, an incident point R of the ultrasonic beam on the surface of the Nth plate obtained in the step S6 N Angle of refraction
Figure DEST_PATH_IMAGE010
And specifying the focal points F and NDistance h of the surface of the laminate f Calculating the coordinate of a theoretical focusing point F';
s8, comparing the difference delta between the specified focus point F and the theoretical focus point F' in the horizontal coordinate direction, wherein,
Δ=F x -
Figure DEST_PATH_IMAGE012
Figure 467656DEST_PATH_IMAGE012
is the abscissa of the theoretical focus point F';
if Δ>0, reassigning the incident point R in the step S2 1 Range of abscissa
Figure DEST_PATH_IMAGE014
If Δ<0, reassigning the incident point R in the step S2 1 Range of abscissa
Figure DEST_PATH_IMAGE016
If Δ =0, the incident point R in step S2 is reassigned 1 Range of abscissa of
Figure DEST_PATH_IMAGE018
If abs (
Figure DEST_PATH_IMAGE020
) When the specified accuracy range is reached, the incident point R selected in step S3 is used 1 The coordinate of the ultrasonic beam is the actual incident point coordinate of the ultrasonic beam on the surface of the multilayer composite board, and the transmission time of the ultrasonic beam from the wafer position to the appointed focus point is calculated;
if abs: (
Figure 380642DEST_PATH_IMAGE020
) If the specified precision range is not reached, the incidence point R is used 1 The re-designated abscissa range repeats steps S3 to S8,up to abs: (
Figure 867118DEST_PATH_IMAGE020
) Reaching the specified precision range;
wherein abs is an absolute value function;
s9, calculating the transmission time of the ultrasonic beams from the wafer position to the appointed focus point of all the wafers in the ultrasonic phased array according to the calculation method of the steps S2 to S8;
s10, acquiring the relative delay time between the pulse excitation signals of the wafers according to the transmission time of each wafer of the ultrasonic phased array;
s11, the ultrasonic phased array wafers are time-delayed and excited by the relative delay time acquired in the step S10 to achieve focusing.
2. The ultrasonic phased array rapid focusing method for the multilayer composite board according to claim 1, characterized in that: in step S6, a method of sequentially calculating the incident point position of the ultrasonic beam on the surface of the second to nth plates and the refraction angle of the ultrasonic beam in the second to nth plates includes the following steps;
step S61 of obtaining incident point from incident point R n Angle of refraction
Figure DEST_PATH_IMAGE022
And the layer height h of the nth layer plate of the multilayer composite plate n Calculating the incident point R of the ultrasonic beam on the surface of the (n + 1) th layer plate of the multilayer composite plate n+1
Step S62 of obtaining a refraction angle, an incident angle on the surface of the (n + 1) th layer plate by an ultrasonic beam
Figure DEST_PATH_IMAGE024
And calculating the refraction angle of the ultrasonic beam in the (n + 1) th layer plate according to the law of refraction
Figure DEST_PATH_IMAGE026
Wherein
Figure 987783DEST_PATH_IMAGE024
=
Figure 130183DEST_PATH_IMAGE022
N =1, 2 … … N, N being the nth layer plate where the specified focus point F is located.
CN202210986070.3A 2022-08-17 2022-08-17 Ultrasonic phased array rapid focusing method for multilayer composite board Active CN115047079B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210986070.3A CN115047079B (en) 2022-08-17 2022-08-17 Ultrasonic phased array rapid focusing method for multilayer composite board

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210986070.3A CN115047079B (en) 2022-08-17 2022-08-17 Ultrasonic phased array rapid focusing method for multilayer composite board

Publications (2)

Publication Number Publication Date
CN115047079A true CN115047079A (en) 2022-09-13
CN115047079B CN115047079B (en) 2022-10-21

Family

ID=83168399

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210986070.3A Active CN115047079B (en) 2022-08-17 2022-08-17 Ultrasonic phased array rapid focusing method for multilayer composite board

Country Status (1)

Country Link
CN (1) CN115047079B (en)

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB9622833D0 (en) * 1995-03-23 1997-01-08 Anderson John E Electromagnetic energy directing method and apparatus
WO2014086322A1 (en) * 2012-12-07 2014-06-12 Tsinghua University Ultrasonic imaging method and system for detecting multi-layered object with synthetic aperture focusing technique
CN104359982A (en) * 2014-11-19 2015-02-18 哈尔滨工业大学 Method for ultrasonic phased array detection of sheet weld joint by wedge block
CN111855809A (en) * 2020-07-20 2020-10-30 大连理工大学 Crack morphology reconstruction method based on compound mode full focusing
CN113049092A (en) * 2021-03-26 2021-06-29 中北大学 Method and system for calculating radiation sound field of ultrasonic array radiator under constraint condition
CN113899816A (en) * 2021-09-10 2022-01-07 国营芜湖机械厂 Ultrasonic nondestructive testing device and method for T-shaped composite structure and R-region testing method and device
CN114430106A (en) * 2022-01-05 2022-05-03 航天恒星科技有限公司 Sub-array assembly of phased array antenna and phased array antenna
CN114674928A (en) * 2022-03-21 2022-06-28 大连理工大学 Method for suppressing blind area in ultrasonic TOFD (time of flight diffraction) detection of thin plate structure based on second-order mode wave

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB9622833D0 (en) * 1995-03-23 1997-01-08 Anderson John E Electromagnetic energy directing method and apparatus
WO2014086322A1 (en) * 2012-12-07 2014-06-12 Tsinghua University Ultrasonic imaging method and system for detecting multi-layered object with synthetic aperture focusing technique
CN104359982A (en) * 2014-11-19 2015-02-18 哈尔滨工业大学 Method for ultrasonic phased array detection of sheet weld joint by wedge block
CN111855809A (en) * 2020-07-20 2020-10-30 大连理工大学 Crack morphology reconstruction method based on compound mode full focusing
CN113049092A (en) * 2021-03-26 2021-06-29 中北大学 Method and system for calculating radiation sound field of ultrasonic array radiator under constraint condition
CN113899816A (en) * 2021-09-10 2022-01-07 国营芜湖机械厂 Ultrasonic nondestructive testing device and method for T-shaped composite structure and R-region testing method and device
CN114430106A (en) * 2022-01-05 2022-05-03 航天恒星科技有限公司 Sub-array assembly of phased array antenna and phased array antenna
CN114674928A (en) * 2022-03-21 2022-06-28 大连理工大学 Method for suppressing blind area in ultrasonic TOFD (time of flight diffraction) detection of thin plate structure based on second-order mode wave

Also Published As

Publication number Publication date
CN115047079B (en) 2022-10-21

Similar Documents

Publication Publication Date Title
CN111175381B (en) Composite member interface rapid imaging quantitative detection method based on full matrix data
CN108169331B (en) Sheet grid wing structure welding seam phased array ultrasonic detection device and detection method
CN110007003B (en) Partitioning method for ultrasonic detection of sound velocity non-uniform metal thick plate welding line phased array
US20170284972A1 (en) Total focusing method adaptively corrected by using plane wave
US20140216158A1 (en) Air coupled ultrasonic contactless method for non-destructive determination of defects in laminated structures
CN100424506C (en) Phased-array ultrasonic wave apparatus and its detection method
CN108490079B (en) Beam forming method based on ultrasonic transducer
CN109490419B (en) Acoustic beam calibration method for full-focus imaging
KR102291701B1 (en) Ultrasonic flaw detector, ultrasonic flaw detection method, manufacturing method of welded steel pipe, and quality control method of welded steel pipe
US6792808B1 (en) Ultrasonic inspection method
CN202710519U (en) Compound probe for detecting defects of weld joints of workpieces
CA2893044C (en) Device and method for the non-destructive control of metal profiles
CN102980947A (en) A system and method suitable for calibrating a phased array system configured to inspect square bars
CN111024825A (en) Thin plate corner structure detection device and method and wedge block optimization method thereof
CN115047079B (en) Ultrasonic phased array rapid focusing method for multilayer composite board
CN108020598A (en) Become the adaptive linear phased array of wall thickness curved surface member and focus on scan method and detection method
Hinrichs et al. Lamb waves excited by an air-coupled ultrasonic phased array for non-contact, non-destructive detection of discontinuities in sheet materials
US4604897A (en) Multitransducer ultrasonic probe with transducers of different sizes
CN115856087B (en) Full-focusing imaging method based on longitudinal wave transmitting-receiving ultrasonic phased array probe
CN112924557A (en) Weld joint full-focusing probe device based on direct longitudinal wave and double linear arrays and detection method
AU2010297455B2 (en) Method and device for measuring a profile of the ground
CN110006995B (en) Phased array ultrasonic detection method for welding seam of metal thick plate with gradient acoustic velocity non-uniformity
CN113049092B (en) Method and system for calculating radiation sound field of ultrasonic array radiator under constraint condition
RU2697024C1 (en) Ultrasound separately-combined converter
CN114002323B (en) Imaging detection method and system for interface debonding of solid rocket engine II

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