[go: up one dir, main page]
More Web Proxy on the site http://driver.im/

CN110823117A - A single-step phase-shift electron speckle interferometry method, system, device and storage medium - Google Patents

A single-step phase-shift electron speckle interferometry method, system, device and storage medium Download PDF

Info

Publication number
CN110823117A
CN110823117A CN201911037596.1A CN201911037596A CN110823117A CN 110823117 A CN110823117 A CN 110823117A CN 201911037596 A CN201911037596 A CN 201911037596A CN 110823117 A CN110823117 A CN 110823117A
Authority
CN
China
Prior art keywords
phase
image
phase shift
shift
images
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
CN201911037596.1A
Other languages
Chinese (zh)
Other versions
CN110823117B (en
Inventor
蔡长青
黄永辉
陈慧敏
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.)
Guangzhou University
Original Assignee
Guangzhou University
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 Guangzhou University filed Critical Guangzhou University
Priority to CN201911037596.1A priority Critical patent/CN110823117B/en
Publication of CN110823117A publication Critical patent/CN110823117A/en
Application granted granted Critical
Publication of CN110823117B publication Critical patent/CN110823117B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B9/00Measuring instruments characterised by the use of optical techniques
    • G01B9/02Interferometers
    • G01B9/02094Speckle interferometers, i.e. for detecting changes in speckle pattern
    • G01B9/02095Speckle interferometers, i.e. for detecting changes in speckle pattern detecting deformation from original shape
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/16Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge
    • G01B11/161Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge by interferometric means
    • G01B11/162Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge by interferometric means by speckle- or shearing interferometry

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

本发明公开了一种单步相移电子散斑干涉测量方法、系统、装置和存储介质,所述的测量方法是在传统相移电子散斑干涉测量法的基础上增加插值计算这一概念,通过插值计算的方法,获得被测物体变形前所需的多幅相移图像和物体变形后所需的多幅相移图像,代替传统测量方法中逐个采集的物体变形前和物体变形后多个相移图像,消除在物体变形前后状态下对多幅相移图像的需要,从而解决现有相移电子散斑干涉测量法只能在静态或准静态测量中使用的问题,实现动态测量;并且,本发明专利不需要增加使用额外的光学器材或布置,只需利用传统相移电子散斑干涉测量装置,便能够实现动态测量。本发明可应用于光学测量技术领域。

The invention discloses a single-step phase-shift electronic speckle interferometry method, system, device and storage medium. The measurement method adds the concept of interpolation calculation on the basis of traditional phase-shift electronic speckle interferometry. Through the method of interpolation calculation, multiple phase-shift images required before the deformation of the object to be measured and multiple phase-shift images required after the object is deformed are obtained, instead of the multiple phase-shift images before and after the deformation of the object collected one by one in the traditional measurement method. Phase-shifted images, eliminating the need for multiple phase-shifted images before and after the object is deformed, thereby solving the problem that the existing phase-shifting electronic speckle interferometry can only be used in static or quasi-static measurement, and realizing dynamic measurement; and , the patent of the present invention does not need to increase the use of additional optical equipment or arrangement, and only needs to use the traditional phase-shift electronic speckle interferometry device to realize dynamic measurement. The present invention can be applied to the technical field of optical measurement.

Description

一种单步相移电子散斑干涉测量方法、系统、装置和存储介质A single-step phase-shift electron speckle interferometry method, system, device and storage medium

技术领域technical field

本发明涉及光学测量领域,尤其是一种单步相移电子散斑干涉测量方法、系统、装置和存储介质。The invention relates to the field of optical measurement, in particular to a method, system, device and storage medium for single-step phase-shift electron speckle interferometry.

背景技术Background technique

电子散斑干涉术(ESPI)法因具有全场、非接触、高精度、实时性和抗振性好等特点而被广泛应用于材料弹性模量测量、表面粗糙度评价、应力应变分析、振动分析和无损检测等领域。电子散斑干涉测量法是一种常用的全场表面位移测量的光学实验技术,表面位移的范围从几十纳米到几微米,这种全场测量具有广泛的实际应用,包括汽车工业中的机械应力评估,机械部件振动模式的研究,微机电系统的质量测试和生物样本的健康监测。Electron Speckle Interferometry (ESPI) is widely used in material elastic modulus measurement, surface roughness evaluation, stress-strain analysis, vibration analysis and non-destructive testing. Electron speckle interferometry is a commonly used optical experimental technique for full-field surface displacement measurements ranging from tens of nanometers to several microns. This full-field measurement has a wide range of practical applications, including mechanical Stress assessment, study of vibration modes of mechanical components, quality testing of MEMS and health monitoring of biological samples.

电子散斑干涉测量法通过对记录在光学粗糙表面上观察到的干涉图案来得到需要测量的信息。一种常见的方法是在物体变形之前采用四步相移得到的四幅图像,并在变形之后采用四步相移得到的另外四幅图像;相移通常使用压电致动镜完成,对所测量的相移图像内的强度变化的分析使得能够在相应的像素处确定相位变化并因此确定表面位移。Electron speckle interferometry obtains the information to be measured by recording the interference pattern observed on an optically rough surface. A common approach is to use four images obtained with a four-step phase shift before the object is deformed, and another four images obtained with a four-step phase shift after the deformation; Analysis of the intensity changes within the phase-shifted image enables the determination of the phase changes and thus the surface displacements at the corresponding pixels.

电子散斑干涉测量法的现有技术由于通常需要在被测物变形前后分别采集多组散斑图像,相移图像的需要通常限制了传统相移电子散斑干涉测量法只能在静态或准静态测量中使用。如果在图像采集期间表面显着移动,则除了由相移引起的相位变化之外还发生相位变化。基于多个波长,频率扫描或使用多相机系统等方法可以测量振动和动态运动,但这些方法需要复杂且昂贵的光学布置。The existing technology of electronic speckle interferometry usually needs to collect multiple sets of speckle images before and after the deformation of the measured object. Used in static measurements. If the surface moves significantly during image acquisition, a phase change occurs in addition to the phase change caused by the phase shift. Vibration and dynamic motion can be measured based on methods such as multiple wavelengths, frequency sweeps, or the use of multi-camera systems, but these methods require complex and expensive optical arrangements.

发明内容SUMMARY OF THE INVENTION

为了解决上述至少一个技术问题,本发明的目的在于提供一种单步相移电子散斑干涉测量方法、系统、装置和介质。In order to solve at least one of the above technical problems, the purpose of the present invention is to provide a single-step phase-shift electron speckle interferometry method, system, device and medium.

本发明所采取的技术方案是:一方面,本发明实施例包括一种单步相移电子散斑干涉测量方法,包括:The technical solution adopted in the present invention is: on the one hand, the embodiment of the present invention includes a single-step phase-shift electronic speckle interferometry method, including:

采集被测物体的电子散斑图像;Collect the electronic speckle image of the measured object;

从第一时刻采集所得的所述电子散斑图像中提取一幅第一相移图像;extracting a first phase shift image from the electronic speckle image acquired at the first moment;

从第二时刻采集所得的所述电子散斑图像中提取一幅第二相移图像;extracting a second phase-shift image from the electronic speckle image acquired at the second moment;

对第一相移图像和第二相移图像进行插值计算;performing interpolation calculation on the first phase-shift image and the second phase-shift image;

根据插值计算的结果,生成所述第一相移图像的至少一幅子图像;generating at least one sub-image of the first phase-shift image according to the result of the interpolation calculation;

根据插值计算的结果,生成所述第二相移图像的至少一幅子图像;generating at least one sub-image of the second phase-shift image according to the result of the interpolation calculation;

对第一相移图像、第一相移图像的子图像、第二相移图像和第二相移图像的子图像进行分析,计算并提取得到第一时刻与第二时刻之间的相位差;所述相位差用于描述被测物体的表面位移的变化。Analyzing the first phase-shift image, the sub-image of the first phase-shift image, the second phase-shift image and the sub-image of the second phase-shift image, and calculating and extracting the phase difference between the first moment and the second moment; The phase difference is used to describe the change of the surface displacement of the measured object.

进一步地,所述对第一相移图像和第二相移图像进行插值计算这一步骤,具体包括:Further, the step of performing interpolation calculation on the first phase-shift image and the second phase-shift image specifically includes:

从所述电子散斑图像中提取前相移图像组和后相移图像组;所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;所述目标相移图像分别为第一相移图像和第二相移图像;A pre-phase-shift image group and a post-phase-shift image group are extracted from the electronic speckle image; the pre-phase-shift image group includes a plurality of phase-shift images extracted before the target phase-shift image, and the post-phase-shift image The group includes a plurality of phase-shift images extracted after the target phase-shift image; the target phase-shift images are respectively a first phase-shift image and a second phase-shift image;

利用提取得到的所述前相移图像组和所述后相移图像组,进行插值计算。Interpolation calculation is performed using the extracted pre-phase-shift image group and the post-phase-shift image group.

进一步地,所述插值计算是通过以下公式执行的:Further, the interpolation calculation is performed by the following formula:

Figure BDA0002251959220000021
Figure BDA0002251959220000021

Figure BDA0002251959220000022
Figure BDA0002251959220000022

Figure BDA0002251959220000023
Figure BDA0002251959220000023

式中,In2、In3、In4分别为所述目标相移图像的子图像,In-6、In-5、In-3、In-2、In-1组成所述前相移图像组;In+1、In+2、In+3、In+5、In+6组成所述后相移图像组。In the formula, I n2 , I n3 , and I n4 are respectively the sub-images of the target phase-shift image, and I n-6 , I n-5 , I n-3 , I n-2 , and I n-1 form the Front phase-shift image group; In +1 , In +2 , In +3 , In +5 , In +6 form the post-phase-shift image group.

进一步地,一种单步相移电子散斑干涉测量方法还包括:Further, a single-step phase-shift electron speckle interferometry method further includes:

采集被测物体在多个时刻的电子散斑图像;Collect electronic speckle images of the measured object at multiple times;

对于任意第一时刻和第二时刻的电子散斑图像按照单步电子散斑干涉测量方法进行处理以输出第一时刻和第二时刻之间的相位差;所述相位差用于描述被测物体的表面位移的变化。The electronic speckle images at any first moment and second moment are processed according to the single-step electronic speckle interferometry method to output the phase difference between the first moment and the second moment; the phase difference is used to describe the measured object change in surface displacement.

另一方面,本发明实施例还包括一种单步相移电子散斑干涉测量系统,包括:On the other hand, the embodiment of the present invention also includes a single-step phase-shift electronic speckle interferometry system, including:

采集模块,用于采集被测物体的电子散斑图像;The acquisition module is used to acquire the electronic speckle image of the measured object;

提取模块,用于从第一时刻采集所得的所述电子散斑图像中提取一幅第一相移图像,和从第二时刻采集所得的所述电子散斑图像中提取一幅第二相移图像;an extraction module, configured to extract a first phase shift image from the electronic speckle image acquired at the first moment, and extract a second phase shift image from the electronic speckle image acquired at the second moment image;

计算模块,用于对第一相移图像和第二相移图像进行插值计算;a calculation module for performing interpolation calculation on the first phase-shift image and the second phase-shift image;

生成模块,用于根据插值计算的结果,生成第一相移图像的至少一幅子图像;和生成第二相移图像的至少一幅子图像;a generating module for generating at least one sub-image of the first phase-shifted image according to the result of the interpolation calculation; and generating at least one sub-image of the second phase-shifted image;

处理模块,用于对第一相移图像、第一相移图像的子图像、第二相移图像和第二相移图像的子图像进行分析,计算并提取得到第一时刻与第二时刻之间的相位差;所述相位差用于描述被测物体的表面位移的变化;The processing module is used for analyzing the first phase-shift image, the sub-image of the first phase-shift image, the second phase-shift image and the sub-image of the second phase-shift image, and calculating and extracting the difference between the first moment and the second moment. The phase difference between; the phase difference is used to describe the change of the surface displacement of the measured object;

输出模块,用于输出提取得到的相位差。The output module is used to output the extracted phase difference.

进一步地,所述计算模块包括:Further, the computing module includes:

提取单元,用于从采集得到的被测物体的电子散斑图像中提取前相移图像组和后相移图像组,所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;所述目标相移图像分别为第一相移图像和第二相移图像;The extraction unit is used for extracting a pre-phase-shift image group and a post-phase-shift image group from the collected electronic speckle images of the measured object, the pre-phase-shift image group including a plurality of images extracted before the target phase-shift image a phase-shift image, the post-phase-shift image group includes a plurality of phase-shift images extracted after the target phase-shift image; the target phase-shift images are respectively a first phase-shift image and a second phase-shift image;

计算单元,用于利用提取得到的所述前相移图像组和所述后相移图像组,进行插值计算。A calculation unit, configured to perform interpolation calculation by using the pre-phase-shift image group and the post-phase-shift image group obtained by extraction.

进一步地,所述处理模块包括:Further, the processing module includes:

分析单元,用于分析第一相移图像、第一相移图像的子图像、第二时刻的第二相移图像和第二相移图像的子图像;an analysis unit, configured to analyze the first phase-shift image, the sub-image of the first phase-shift image, the second phase-shift image at the second moment, and the sub-image of the second phase-shift image;

计算单元,用于计算第一时刻与第二时刻之间的相位差;a calculation unit for calculating the phase difference between the first moment and the second moment;

提取单元,用于提取计算得到的相位差。The extraction unit is used to extract the calculated phase difference.

另一方面,本发明实施例还包括一种单步相移电子散斑干涉测量装置,包括:激光器、摄像机和计算机,其中,所述激光器用于照射被测物体从而产生电子散斑图像;所述摄像机用于采集电子散斑图像;所述计算机用于执行单步相移电子散斑干涉测量方法以对采集到的电子散斑图像进行处理。On the other hand, the embodiment of the present invention also includes a single-step phase-shift electronic speckle interferometry device, including: a laser, a camera and a computer, wherein the laser is used to irradiate the measured object to generate an electronic speckle image; The camera is used for collecting electronic speckle images; the computer is used for executing a single-step phase-shifting electronic speckle interferometry method to process the collected electronic speckle images.

另一方面,本发明实施例还包括一种存储介质,其中存储有处理器可执行的指令,所述处理器可执行的指令在由处理器执行时用于执行单步相移电子散斑干涉测量方法。On the other hand, an embodiment of the present invention further includes a storage medium, in which processor-executable instructions are stored, and when executed by the processor, the processor-executable instructions are used to perform single-step phase-shift electronic speckle interferometry Measurement methods.

本发明的有益效果是:实施例中提出一种单步相移电子散斑干涉测量方法,其中主要是利用插值计算的方法获得测量所需的多幅相移图像,代替现有测量方法中逐个采集的多个相移图像;从而解决了现有相移电子散斑干涉测量法只能在静态或准静态测量中使用的问题,实现动态测量;并且,本发明专利不需要额外的光学器材或布置,只需利用传统相移电子散斑干涉测量装置,便能够实现动态测量。The beneficial effects of the present invention are as follows: a single-step phase-shift electronic speckle interferometry method is proposed in the embodiment, wherein the interpolation calculation method is mainly used to obtain multiple phase-shift images required for measurement, instead of one by one in the existing measurement method. A plurality of phase-shifted images collected; thus solving the problem that the existing phase-shifting electronic speckle interferometry can only be used in static or quasi-static measurement, and realizing dynamic measurement; and the patent of the present invention does not require additional optical equipment or Arrangement, dynamic measurement can be achieved only by using the traditional phase-shift electronic speckle interferometry device.

附图说明Description of drawings

图1为本发明实施例中所述单步相移电子散斑干涉测量方法的步骤流程图;Fig. 1 is the step flow chart of the single-step phase-shift electron speckle interferometry method described in the embodiment of the present invention;

图2为本发明实施例中所述单步相移电子散斑干涉测量系统的结构框图;2 is a structural block diagram of the single-step phase-shift electronic speckle interferometry system described in the embodiment of the present invention;

图3为本发明实施例中所述利用插值计算获得的每个时刻的四幅相移图的分布情况。FIG. 3 is the distribution of four phase shift maps at each moment obtained by interpolation calculation according to the embodiment of the present invention.

具体实施方式Detailed ways

现有的相移电子散斑干涉测量方法具体如下所示:The existing phase-shift electron speckle interferometry methods are as follows:

测量图像内的每个像素处的光强度I可以表述为:The light intensity I at each pixel within the measured image can be expressed as:

I=A+Bcosφ,I=A+Bcosφ,

其中A为背景光强,B为调制度,φ为随机相位。Where A is the background light intensity, B is the modulation degree, and φ is the random phase.

在静态物体或准静态上进行相移电子散斑干涉测量方法是在物体变形前先采集四幅相移图像,相移步长为

Figure BDA0002251959220000041
可以表达为:Phase-shifted electron speckle interferometry on a static object or quasi-static method is to collect four phase-shifted images before the object is deformed, and the phase-shift step size is
Figure BDA0002251959220000041
can be expressed as:

I01=A+BcosφI 01 =A+Bcosφ

Figure BDA0002251959220000042
Figure BDA0002251959220000042

I03=A+Bcos(φ+π)I 03 =A+Bcos(φ+π)

Figure BDA0002251959220000043
Figure BDA0002251959220000043

式中,下角标01、02、03、04中的0表示物体变形前的某一时刻,编号为0,下角标01、02、03、04中的1、2、3、4表示物体变形前某一时刻的第一、第二、第三、第四幅相移图像,所述四幅相移图像都是通过相移电子散斑干涉测量方法采集得到的。In the formula, 0 in the subscripts 01, 02, 03, and 04 represents a certain moment before the object is deformed, and the number is 0, and 1, 2, 3, and 4 in the subscripts 01, 02, 03, and 04 represent the object before deformation. The first, second, third, and fourth phase-shift images at a certain moment, the four phase-shift images are all acquired by the phase-shift electron speckle interferometry method.

然后在感兴趣的物体变形发生之后采集另外四幅相移图像,可以表达为:Then four additional phase-shifted images are acquired after the deformation of the object of interest occurs, which can be expressed as:

I11=A+Bcos(φ+Δ)I 11 =A+Bcos(φ+Δ)

Figure BDA0002251959220000044
Figure BDA0002251959220000044

I13=A+Bcos(φ+Δ+π)I 13 =A+Bcos(φ+Δ+π)

Figure BDA0002251959220000045
Figure BDA0002251959220000045

式中,下角标11、12、13、14中的1表示物体变形后的某一时刻,编号为1,下角标11、12、13、14中的1、2、3、4表示物体变形后某一时刻的第一、第二、第三、第四幅相移图像,所述四幅相移图像也都是通过相移电子散斑干涉测量方法采集得到的。In the formula, 1 in the subscripts 11, 12, 13, and 14 indicates a certain moment after the object is deformed, and the number is 1, and 1, 2, 3, and 4 in the subscripts 11, 12, 13, and 14 indicate that the object is deformed. The first, second, third, and fourth phase-shift images at a certain moment, the four phase-shift images are also acquired by the phase-shift electron speckle interferometry method.

其中Δ可由下式进行求解:where Δ can be solved by the following equation:

Figure BDA0002251959220000046
Figure BDA0002251959220000046

式中,Δ为物体变形前和物体变形后之间的相位差,所述相位差可用于描述被测物体的表面位移的变化,I01、I02、I03、I04、I11、I12、I13、I14分别为采集得到的物体变形前的四幅相移图像和物体变形后的四幅相移图像。In the formula, Δ is the phase difference between the object before and after the object is deformed, and the phase difference can be used to describe the change of the surface displacement of the measured object, I 01 , I 02 , I 03 , I 04 , I 11 , I 12 , I 13 , and I 14 are the acquired four phase-shift images before the object is deformed and the four phase-shift images after the object is deformed, respectively.

在物体变形前和变形后采集四幅相移图像时,物体都要在静态或者准静态情况下,这限制了现有的相移电子散斑干涉测量方法只能用于静态测量。When the four phase-shifted images are collected before and after the deformation of the object, the object must be in a static or quasi-static state, which limits the existing phase-shifted electron speckle interferometry methods to only be used for static measurement.

实施例1Example 1

如图1所示,一种单步相移电子散斑干涉测量方法,该方法具体包括以下步骤:As shown in Figure 1, a single-step phase-shift electron speckle interferometry method specifically includes the following steps:

S1.采集被测物体的电子散斑图像;S1. Collect the electronic speckle image of the measured object;

S2.从第一时刻采集所得的所述电子散斑图像中提取一幅第一相移图像;S2. Extract a first phase shift image from the electronic speckle image collected at the first moment;

S3.从第二时刻采集所得的所述电子散斑图像中提取一幅第二相移图像;S3. Extract a second phase-shift image from the electronic speckle image acquired at the second moment;

S4.对第一相移图像和第二相移图像进行插值计算;S4. Interpolate the first phase-shift image and the second phase-shift image;

S5.根据插值计算的结果,生成所述第一相移图像的至少一幅子图像;S5. generate at least one sub-image of the first phase-shift image according to the result of the interpolation calculation;

S6.根据插值计算的结果,生成所述第二相移图像的至少一幅子图像;S6. generate at least one sub-image of the second phase-shift image according to the result of the interpolation calculation;

S7.对第一相移图像、第一相移图像的子图像、第二相移图像和第二相移图像的子图像进行分析,计算并提取得到第一时刻与第二时刻之间的相位差;所述相位差用于描述被测物体的表面位移的变化。S7. Analyze the first phase-shift image, the sub-image of the first phase-shift image, the second phase-shift image and the sub-image of the second phase-shift image, calculate and extract the phase between the first moment and the second moment difference; the phase difference is used to describe the change of the surface displacement of the measured object.

作为本测量方法实施例的优选实施方式,所述步骤S4,也就是对第一相移图像和第二相移图像进行插值计算这一步骤,具体包括:As a preferred implementation of the embodiment of the measurement method, the step S4, that is, the step of performing interpolation calculation on the first phase-shift image and the second phase-shift image, specifically includes:

S401.从所述电子散斑图像中提取前相移图像组和后相移图像组;所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;所述目标相移图像分别为第一相移图像和第二相移图像;S401. Extract a pre-phase-shift image group and a post-phase-shift image group from the electronic speckle image; the pre-phase-shift image group includes a plurality of phase-shift images extracted before the target phase-shift image, and the post-phase-shift image group The shift image group includes a plurality of phase shift images extracted after the target phase shift image; the target phase shift images are respectively a first phase shift image and a second phase shift image;

S402.利用提取得到的所述前相移图像组和所述后相移图像组,进行插值计算。S402. Perform interpolation calculation by using the pre-phase-shift image group and the post-phase-shift image group obtained by extraction.

作为本测量方法实施例的优选实施方式,步骤S402中所述插值计算是通过以下公式执行的:As a preferred implementation of the embodiment of the measurement method, the interpolation calculation in step S402 is performed by the following formula:

Figure BDA0002251959220000051
Figure BDA0002251959220000051

Figure BDA0002251959220000052
Figure BDA0002251959220000052

Figure BDA0002251959220000053
Figure BDA0002251959220000053

式中,In2、In3、In4分别为所述目标相移图像的子图像,所述目标相移图像分别为第一相移图像和第二相移图像;In-6、In-5、In-3、In-2、In-1组成所述前相移图像组;In+1、In+2、In+3、In+5、In+6组成所述后相移图像组。例如,提取的第一相移图像为I71时,则I72、I73、I74分别为通过插值计算得到的第一相移图像的子图像,I1、I2、I3、I4、I5、I6组成所述前相移图像组,即第一相移图像的前6幅相移图像,I8、I9、I10、I11、I12、I13组成所述后相移图像组,即第一相移图像的后6幅相移图像;而提取的第二相移图像为I81时,则I82、I83、I84分别为通过插值计算得到的第二相移图像的子图像,I2、I3、I4、I5、I6、I7组成所述前相移图像组,即第二相移图像的前6幅相移图像,I9、I10、I11、I12、I13、I14组成所述后相移图像组,即第二相移图像的后6幅相移图像。In the formula, I n2 , I n3 , I n4 are respectively the sub-images of the target phase-shift image, and the target phase-shift image is the first phase-shift image and the second phase-shift image respectively; I n-6 , I n -5 , I n-3 , I n-2 , I n-1 form the pre-phase shift image group; I n+1 , I n+2 , I n+3 , I n+5 , I n+6 The post-phase-shift image group is composed. For example, when the extracted first phase-shift image is I 71 , then I 72 , I 73 , and I 74 are respectively the sub-images of the first phase-shift image obtained by interpolation calculation, I 1 , I 2 , I 3 , and I 4 . , I 5 , I 6 form the front phase-shift image group, that is, the first six phase-shift images of the first phase-shift image, and I 8 , I 9 , I 10 , I 11 , I 12 , I 13 form the back The phase-shifted image group, that is, the last six phase-shifted images of the first phase-shifted image; and when the extracted second phase-shifted image is I 81 , then I 82 , I 83 , and I 84 are respectively the second phase-shifted images obtained by interpolation. The sub-images of the phase-shift image, I 2 , I 3 , I 4 , I 5 , I 6 , and I 7 form the pre-phase-shift image group, that is, the first six phase-shift images of the second phase-shift image, I 9 , I 10 , I 11 , I 12 , I 13 , and I 14 form the post-phase-shift image group, that is, the post-phase-shift images of the second phase-shift image.

本实施例中,所述步骤S1,也就是采集被测物体的电子散斑图像这一步骤具体包括:利用传统相移电子散斑干涉测量装置生成并采集电子散斑图像,其中,采集方法是采用图像之间相移量保持递增

Figure BDA0002251959220000061
的方式,使用摄像机连续采图;即如果采集的第一时刻图像相位步长为0,则第二时刻图像相位步长为
Figure BDA0002251959220000062
第三时刻图像相位步长为π,第四时刻图像相位步长为
Figure BDA0002251959220000063
第五时刻图像相位步长为0,第六时刻图像相位步长为
Figure BDA0002251959220000064
以后依次类推。In this embodiment, the step S1, that is, the step of collecting the electronic speckle image of the measured object specifically includes: using a traditional phase-shift electronic speckle interferometry device to generate and collect the electronic speckle image, wherein the acquisition method is: Use the phase shift between images to keep increasing
Figure BDA0002251959220000061
The way of using the camera to continuously capture images; that is, if the phase step of the image at the first moment of acquisition is 0, the phase step of the image at the second moment is
Figure BDA0002251959220000062
The image phase step size at the third moment is π, and the image phase step size at the fourth moment is
Figure BDA0002251959220000063
The image phase step size at the fifth moment is 0, and the image phase step size at the sixth moment is
Figure BDA0002251959220000064
And so on.

本实施例中,只需在物体变形前先采集一幅相移图像,即第一相移图像,另外三幅可以根据插值计算得到。同样地,只需在感兴趣的变形发生之后采集另外一幅相移图像,即第二相移图像,其余三幅也同样可以根据插值计算得到。In this embodiment, only one phase-shift image, ie, the first phase-shift image, needs to be collected before the object is deformed, and the other three images can be obtained by interpolation. Similarly, only another phase-shift image, ie, the second phase-shift image, needs to be acquired after the deformation of interest occurs, and the remaining three images can also be calculated by interpolation.

本实施例中,所述步骤S4中对第一相移图像进行插值计算这一步骤,需要先提取前相移图像组和后相移图像组;所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;例如,如果采集得到的第一相移图像为I71,则对第一相移图像进行插值计算之前,需要从所述电子散斑图像中提取前相移图像组,即在第一相移图像之前的6幅相移图像,分别表示为I1、I2、I3、I4、I5、I6,并且需要从所述电子散斑图像中提取后相移图像组,即在第一相移图像之后的6幅相移图像,分别为I8、I9、I10、I11、I12、I13。然后再利用插值计算公式,计算得到第一时刻的另外三幅相移图像,分别为I72、I73和I74,其具体计算过程如下:In this embodiment, in the step of performing interpolation calculation on the first phase-shift image in step S4, it is necessary to first extract the pre-phase-shift image group and the post-phase-shift image group; the pre-phase-shift image group is included in the target phase-shift image group. Multiple phase-shift images extracted before the image, and the post-phase-shift image group includes multiple phase-shift images extracted after the target phase-shift image; for example, if the first phase-shift image acquired is I 71 , then Before performing the interpolation calculation on the first phase-shift image, it is necessary to extract the pre-phase-shift image group from the electronic speckle image, that is, the 6 phase-shift images before the first phase-shift image, which are respectively expressed as I 1 , I 2 , I 3 , I 4 , I 5 , I 6 , and the post-phase-shift image group needs to be extracted from the electronic speckle image, that is, the 6 phase-shift images after the first phase-shift image, which are I 8 , I 9 , I 10 , I 11 , I 12 , I 13 . Then use the interpolation calculation formula to obtain the other three phase-shifted images at the first moment, which are I 72 , I 73 and I 74 respectively. The specific calculation process is as follows:

Figure BDA0002251959220000065
Figure BDA0002251959220000065

Figure BDA0002251959220000066
Figure BDA0002251959220000066

Figure BDA0002251959220000071
Figure BDA0002251959220000071

同样地,本实施例中,所述步骤S4中对第二相移图像进行插值计算这一步骤,需要先提取前相移图像组和后相移图像组;所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;例如,假设采集得到的第二相移图像为I81,则对第二相移图像进行插值计算之前,需要从所述电子散斑图像中提取前相移图像组,即在第一相移图像之前的6幅相移图像,分别表示为I2、I3、I4、I5、I6、I7,并且需要从所述电子散斑图像中提取后相移图像组,即在第一相移图像之后的6幅相移图像,分别为I9、I10、I11、I12、I13、I14。然后再利用插值计算公式,计算得到第二时刻的另外三幅相移图像,分别为I82、I83和I84,其具体计算过程如下:Similarly, in this embodiment, in the step of performing interpolation calculation on the second phase-shift image in step S4, it is necessary to first extract the pre-phase-shift image group and the post-phase-shift image group; the pre-phase-shift image group includes the The multiple phase-shift images extracted before the target phase-shift image, and the post-phase-shift image group includes multiple phase-shift images extracted after the target phase-shift image; for example, it is assumed that the collected second phase-shift image is I 81 , before performing the interpolation calculation on the second phase-shift image, it is necessary to extract the pre-phase-shift image group from the electronic speckle image, that is, the 6 phase-shift images before the first phase-shift image, respectively denoted as I 2 , I 3 , I 4 , I 5 , I 6 , I 7 , and the post-phase-shift image group needs to be extracted from the electronic speckle image, that is, the 6 phase-shift images after the first phase-shift image, which are respectively I 9 , I 10 , I 11 , I 12 , I 13 , I 14 . Then, by using the interpolation calculation formula, the other three phase-shift images at the second moment are obtained by calculation, which are I 82 , I 83 and I 84 respectively. The specific calculation process is as follows:

Figure BDA0002251959220000072
Figure BDA0002251959220000072

Figure BDA0002251959220000073
Figure BDA0002251959220000073

Figure BDA0002251959220000074
Figure BDA0002251959220000074

利用插值计算的方法,得到第一时刻所需的四幅相移图像分别为I71、I72、I73、I74,其中,I71是从采集得到的电子散斑图像中提取得到的,I72、I73、I74是利用插值计算得到的,同样地,利用插值计算的方法,可得到第二时刻所需的四幅相移图像分别为I81、I82、I83、I84,其中I81是从采集得到的电子散斑图像中提取得到的,I82、I83、I84是利用插值计算得到的。然后利用现有的相移电子散斑干涉测量方法,利用插值计算的方法得到的I71、I72、I73、I74、I81、I82、I83、I84,计算得到第一时刻和第二时刻的相位差,所述相位差可用于描述被测物体的表面位移的变化。Using the method of interpolation calculation, the four phase-shifted images required to obtain the first moment are I 71 , I 72 , I 73 , and I 74 , respectively, where I 71 is extracted from the collected electron speckle images, and I 72 , I 73 , and I 74 are obtained by interpolation calculation. Similarly, by means of interpolation calculation, the four phase-shifted images required at the second moment can be obtained respectively as I 81 , I 82 , I 83 , and I 84 , wherein I 81 is extracted from the collected electron speckle image, and I 82 , I 83 , and I 84 are calculated by interpolation. Then, using the existing phase-shift electron speckle interferometry method, and using the interpolation calculation method to obtain I 71 , I 72 , I 73 , I 74 , I 81 , I 82 , I 83 , I 84 , the first moment is obtained by calculation and the phase difference at the second moment, the phase difference can be used to describe the change of the surface displacement of the measured object.

综上所述,本实施例中所述的单步相移电子散斑干涉测量方法具有以下优点:To sum up, the single-step phase-shift electron speckle interferometry method described in this embodiment has the following advantages:

通过利用插值计算的方法,获得被测物体变形前所需的多幅相移图像和物体变形后所需的多幅相移图像,代替现有相移电子散斑干涉测量方法中逐个采集的物体变形前和物体变形后多个相移图像,消除在物体变形前后状态下对多幅相移图像的需要,从而解决现有相移电子散斑干涉测量方法只能在静态或准静态测量中使用的问题,实现动态测量;并且,本实施例中所述的测量方法是在现有相移电子散斑干涉测量法的基础上增加插值计算这一概念,因此不需要增加使用额外的光学器材或布置,只需利用现有相移电子散斑干涉测量装置,便能够实现动态测量,最终计算得到相位差,从而能够描述被测物体表面位移的变化。By using the interpolation calculation method, multiple phase-shift images required before the deformation of the measured object and multiple phase-shift images required after the object is deformed are obtained, instead of the objects collected one by one in the existing phase-shift electronic speckle interferometry method Multiple phase-shift images before and after the object is deformed, eliminating the need for multiple phase-shift images before and after the object is deformed, thus solving the problem that the existing phase-shift electron speckle interferometry method can only be used in static or quasi-static measurement In addition, the measurement method described in this embodiment is to add the concept of interpolation calculation on the basis of the existing phase-shift electronic speckle interferometry, so there is no need to increase the use of additional optical equipment or The arrangement can realize dynamic measurement only by using the existing phase-shift electronic speckle interferometry device, and finally calculate the phase difference, so that the change of the surface displacement of the measured object can be described.

实施例2Example 2

一种单步相移电子散斑干涉测量方法,包括以下步骤:A single-step phase-shift electron speckle interferometry method, comprising the following steps:

采集被测物体在多个时刻的电子散斑图像;例如,采集t1、t2……t100等一百个时刻的电子散斑图像。Collect electron speckle images of the object to be measured at multiple times; for example, collect electron speckle images at one hundred times such as t1, t2...t100.

选取t1、t2……t100时刻中的任意两个时刻的为所述第一时刻和第二时刻,提取第一时刻和第二时刻的相移图像,执行实施例1所述单步相移电子散斑干涉测量方法以输出第一时刻和第二时刻之间的相位差;所述相位差用于描述被测物体的表面位移的变化。即本实施例中所述的单步相移电子散斑干涉测量方法可以获取任一时刻所需的4幅相移图像,并按实际需要计算得到任一两个时刻之间的相位差,从而实现动态测量并获取被测物体的表面位移的变化信息。Select any two of the time t1, t2...t100 as the first time and the second time, extract the phase shift images of the first time and the second time, and execute the single-step phase-shift electronic method described in Embodiment 1. The speckle interferometry method is used to output the phase difference between the first moment and the second moment; the phase difference is used to describe the change of the surface displacement of the measured object. That is, the single-step phase-shift electronic speckle interferometry method described in this embodiment can obtain 4 phase-shift images required at any moment, and calculate the phase difference between any two moments according to actual needs, so that Realize dynamic measurement and obtain the change information of the surface displacement of the measured object.

本实施例中所述的单步相移电子散斑干涉测量方法具有以下优点:The single-step phase-shift electron speckle interferometry method described in this embodiment has the following advantages:

通过利用插值计算的方法,可以获得任一时刻测量所需的多幅相移图像,即可获得被测物体变形前所需的多幅相移图像和物体变形后所需的多幅相移图像,代替现有相移电子散斑干涉测量方法中逐个采集的物体变形前和物体变形后多个相移图像,消除在物体变形前后状态下对多幅相移图像的需要,从而解决现有相移电子散斑干涉测量方法只能在静态或准静态测量中使用的问题,实现动态测量;并且,本实施例中所述的测量方法是在现有相移电子散斑干涉测量法的基础上增加插值计算这一概念,因此不需要增加使用额外的光学器材或布置,只需利用现有相移电子散斑干涉测量装置,便能够实现动态测量,最终计算得到相位差,从而能够描述被测物体表面位移的变化。By using the method of interpolation calculation, it is possible to obtain multiple phase-shift images required for measurement at any moment, that is, to obtain multiple phase-shift images required before the deformation of the measured object and multiple phase-shift images required after the object is deformed , instead of the multiple phase-shift images before and after the object is deformed, which are collected one by one in the existing phase-shift electronic speckle interferometry method, eliminating the need for multiple phase-shift images in the state before and after the object is deformed, so as to solve the problem of the existing phase-shift images. The problem that the shifting electron speckle interferometry method can only be used in static or quasi-static measurement can realize dynamic measurement; and the measurement method described in this embodiment is based on the existing phase shifting electron speckle interferometry method. The concept of interpolation calculation is added, so there is no need to increase the use of additional optical equipment or arrangements, just use the existing phase-shift electronic speckle interferometry device to achieve dynamic measurement, and finally calculate the phase difference, which can describe the measured Changes in the displacement of the surface of an object.

实施例3Example 3

参照图2,本实施例包括一种单步相移电子散斑干涉测量系统,包括采集模块、提取模块、计算模块、生成模块、处理模块和输出模块6个模块组成。Referring to FIG. 2 , this embodiment includes a single-step phase-shift electronic speckle interferometry system, including an acquisition module, an extraction module, a calculation module, a generation module, a processing module and an output module.

所述采集模块是采用图像之间相移量保持递增的方式,使用摄像机连续采图,采集得到被测物体的电子散斑图像;所述采集模块可根据实际需要采集多个时刻的电子散斑图像,例如可采集t1、t2……t100等一百个时刻的电子散斑图像,且所述采集模块在某一时刻只需采集一幅电子散斑图像,例如,在t1时刻只需采集一幅电子散斑图像,在t2时刻,也只需采集一幅电子散斑图像,在t3、t4……t100的时刻也都只需各采集一幅电子散斑图像。The acquisition module adopts the phase shift amount between the images to keep increasing The electronic speckle image of the object to be measured is obtained by using the camera to continuously capture images; the acquisition module can collect electronic speckle images at multiple times according to actual needs, such as t1, t2...t100, etc. An electronic speckle image at a time, and the acquisition module only needs to collect one electronic speckle image at a certain time. For an electronic speckle image, only one electronic speckle image needs to be collected at the time t3, t4...t100.

所述提取模块用于用于从采集所得的所述电子散斑图像中提取测量所需的电子散斑图像,例如,指定t7时刻为第一时刻,t8时刻为第二时刻,提取在t7时刻采集所得的电子散斑图像为第一相移图像,提取在t8时刻采集所得的电子散斑图像为第二相移图像,其具体操作如下:The extraction module is used to extract the electronic speckle image required for measurement from the collected electronic speckle image, for example, specifying time t7 as the first time, time t8 as the second time, and extraction at time t7 The collected electron speckle image is the first phase shift image, and the electron speckle image collected at time t8 is extracted as the second phase shift image. The specific operations are as follows:

将所述采集模块利用摄像机采集得到t1、t2……t100等一百个时刻的各一幅电子散斑图像;The acquisition module uses a camera to acquire an electronic speckle image at one hundred times such as t1, t2...t100;

将所述电子散斑图像形成视频信号;forming the electronic speckle image into a video signal;

将所述形成的视频信号连接到计算机监视器的输入端;connecting the formed video signal to an input of a computer monitor;

利用计算机提取在t7时刻采集所得的电子散斑图像为第一相移图像和提取在t8时刻采集所得的电子散斑图像为第二相移图像。The electronic speckle image collected at time t7 is extracted by a computer as the first phase shift image and the electronic speckle image collected at time t8 is extracted as the second phase shift image.

所述计算模块用于对第一相移图像和第二相移图像进行插值计算这一步骤,具体包括:The calculation module is used to perform interpolation calculation on the first phase-shift image and the second phase-shift image, and specifically includes:

利用计算机分析接收到的第一相移图像和第二相移图像;Using a computer to analyze the received first phase-shifted image and the second phase-shifted image;

从采集得到的电子散斑图像中提取第一相移图像的前6幅相移图像,即分别提取在t1、t2、t3、t4、t5、t6时刻采集的电子散斑图像组成前相移图像组,并从采集得到的电子散斑图像中提取第一相移图像的后6幅相移图像,即分别提取在t8、t9、t10、t11、t12、t13时刻采集的电子散斑图像组成后相移图像组;Extract the first six phase-shift images of the first phase-shift image from the collected electron speckle images, that is, extract the electron-speckle images collected at t1, t2, t3, t4, t5, and t6 respectively to form the pre-phase-shift images group, and extract the last six phase-shift images of the first phase-shift image from the collected electronic speckle images, that is, extract the electronic speckle images collected at t8, t9, t10, t11, t12, and t13. Phase shift image group;

同样地,从采集得到的电子散斑图像中提取第二相移图像的前6幅相移图像,即分别提取在t2、t3、t4、t5、t6、t7时刻采集的电子散斑图像组成前相移图像组,并从采集得到的电子散斑图像中提取第二相移图像的后6幅相移图像,即分别提取在t9、t10、t11、t12、t13、t14时刻采集的电子散斑图像组成后相移图像组;Similarly, the first six phase-shift images of the second phase-shift image are extracted from the collected electronic speckle images, that is, the electronic speckle images collected at t2, t3, t4, t5, t6, and t7 are extracted before the composition Phase shift image group, and extract the last 6 phase shift images of the second phase shift image from the collected electron speckle images, namely extract the electron speckle collected at t9, t10, t11, t12, t13, t14 respectively Phase-shifted image group after image composition;

根据预先设计的插值计算的公式程序分别计算得到第一相移图像对应的另外三幅相移图像和第二相移图像对应的另外三幅相移图像。The other three phase-shift images corresponding to the first phase-shift image and the other three phase-shift images corresponding to the second phase-shift image are respectively calculated according to the pre-designed interpolation calculation formula program.

所述生成模块,用于根据插值计算的结果,生成第一时刻所需要的包括第一相移图像在内的四幅相移图像;和生成第二时刻所需要的包括第二相移图像在内的的四幅相移图像。The generating module is used for generating four phase-shift images including the first phase-shift image required at the first moment according to the result of the interpolation calculation; and generating the second phase-shift image required at the second moment including the second phase-shift image of four phase-shifted images.

所述处理模块,用于对所述生成模块生成的第一时刻所需要的四幅相移图像和第二时刻所需要的四幅相依图像进行分析,并按照预先设计的现有电子散斑干涉测量方法中相位差的计算公式程序计算并提取得到第一时刻与第二时刻之间的相位差;所述相位差可用于描述被测物体的表面位移的变化。The processing module is configured to analyze the four phase-shifted images required at the first moment and the four dependent images required at the second moment generated by the generation module, and analyze the four phase-shifted images required at the second moment, and measure them according to a pre-designed existing electronic speckle interferometry method. The calculation formula of the phase difference in the program calculates and extracts the phase difference between the first moment and the second moment; the phase difference can be used to describe the change of the surface displacement of the measured object.

所述输出模块,用于输出提取得到的相位差。The output module is used for outputting the extracted phase difference.

进一步作为优选的实施方式,所述计算模块包括:Further as a preferred embodiment, the computing module includes:

提取单元,用于从采集得到的被测物体的电子散斑图像中提取前相移图像组和后相移图像组,所述前相移图像组包括在目标相移图像之前提取得到的多幅相移图像,所述后相移图像组包括在目标相移图像之后提取得到的多幅相移图像;所述目标相移图像分别为第一相移图像和第二相移图像。例如,利用摄像机采集得到t1、t2……t100等一百个时刻的各一幅电子散斑图像,指定t7时刻为第一时刻,t8时刻为第二时刻,提取在t7时刻采集所得的电子散斑图像为第一相移图像,提取在t8时刻采集所得的电子散斑图像为第二相移图像,分别提取在t1、t2、t3、t4、t5、t6时刻采集的电子散斑图像组成第一相移图像前相移图像组,分别提取在t8、t9、t10、t11、t12、t13时刻采集的电子散斑图像组成第一相移图像后相移图像组;同样地,分别提取在t2、t3、t4、t5、t6、t7时刻采集的电子散斑图像组成第二相移图像前相移图像组,分别提取在t9、t10、t11、t12、t13、t14时刻采集的电子散斑图像组成第二相移图像后相移图像组。The extraction unit is used for extracting a pre-phase-shift image group and a post-phase-shift image group from the collected electronic speckle images of the measured object, the pre-phase-shift image group including a plurality of images extracted before the target phase-shift image Phase-shifted images, the post-phase-shifted image group includes multiple phase-shifted images extracted after the target phase-shifted images; the target phase-shifted images are respectively a first phase-shifted image and a second phase-shifted image. For example, use a camera to collect one electron speckle image at one hundred times such as t1, t2...t100, specify time t7 as the first time, time t8 as the second time, and extract the electron speckle images collected at time t7. The speckle image is the first phase shift image, and the electronic speckle image collected at time t8 is extracted as the second phase shift image. For a pre-phase-shift image group, extract the electronic speckle images collected at t8, t9, t10, t11, t12, and t13 respectively to form the first phase-shift image post-phase-shift image group; The electronic speckle images collected at t3, t4, t5, t6, and t7 form the second phase-shift image pre-phase-shift image group, and the electronic speckle images collected at t9, t10, t11, t12, t13, and t14 are extracted respectively. The second phase-shifted image post-phase-shifted image group is formed.

计算单元,用于利用提取得到的所述前相移图像组和所述后相移图像组,根据预先设计的插值计算的公式程序进行插值计算。例如,利用提取得到的t1、t2、t3、t4、t5、t6时刻组成的前相移图像组,和t8、t9、t10、t11、t12、t13时刻组成的后相移图像组,按照预先设计的插值计算的公式程序进行插值计算,得到第一时刻的第一相移图像对应的另外三幅相移图像;利用提取得到的t2、t3、t4、t5、t6、t7时刻组成的前相移图像组,和t9、t10、t11、t12、t13、t14时刻组成的后相移图像组,按照预先设计的插值计算的公式程序进行插值计算,得到第二时刻的第二相移图像对应的另外三幅相移图像。The calculation unit is configured to perform interpolation calculation according to a pre-designed interpolation calculation formula program by using the pre-phase-shift image group and the post-phase-shift image group obtained by extraction. For example, the pre-phase-shift image group composed of the extracted time t1, t2, t3, t4, t5, and t6, and the post-phase-shift image group composed of the time t8, t9, t10, t11, t12, and t13, are used according to the pre-designed The formula program of the interpolation calculation is performed by interpolation calculation, and the other three phase-shift images corresponding to the first phase-shift image at the first moment are obtained. The image group, and the post-phase-shift image group formed at t9, t10, t11, t12, t13, and t14, are interpolated according to the pre-designed interpolation calculation formula program to obtain the second phase-shift image corresponding to the second time. Three phase-shifted images.

进一步作为优选的实施方式,所述处理模块包括:Further as a preferred embodiment, the processing module includes:

分析单元,用于分析第一相移图像、第一相移图像的子图像、第二相移图像和第二相移图像的子图像,也就是分析第一时刻所需要的包括第一相移图像在内的四幅相移图像,和第二时刻所需要的包括第二相移图像在内的的四幅相移图像;An analysis unit, configured to analyze the first phase-shift image, the sub-image of the first phase-shift image, the second phase-shift image, and the sub-image of the second phase-shift image, that is, the first phase-shift image required for analyzing the first moment includes the first phase-shift image Four phase-shifted images including the image, and four phase-shifted images including the second phase-shifted image required at the second moment;

计算单元,用于根据预先设计的现有电子散斑干涉测量方法中相位差的计算公式程序计算第一时刻与第二时刻之间的相位差;a calculation unit, configured to calculate the phase difference between the first moment and the second moment according to a pre-designed calculation formula program of the phase difference in the existing electronic speckle interferometry method;

提取单元,用于提取计算得到的相位差。The extraction unit is used to extract the calculated phase difference.

综上所述,本实施例中所述的单步相移电子散斑干涉测量系统具有以下优点:To sum up, the single-step phase-shift electron speckle interferometry system described in this embodiment has the following advantages:

通过利用插值计算的方法,获得被测物体变形前所需的多幅相移图像和物体变形后所需的多幅相移图像,代替现有相移电子散斑干涉测量方法中逐个采集的物体变形前和物体变形后多个相移图像,消除在物体变形前后状态下对多幅相移图像的需要,从而解决现有相移电子散斑干涉测量方法只能在静态或准静态测量中使用的问题,实现动态测量;并且,本实施例中所述的测量方法是在现有相移电子散斑干涉测量法的基础上增加插值计算这一概念,因此不需要增加使用额外的光学器材或布置,只需利用现有相移电子散斑干涉测量装置,便能够实现动态测量,最终计算得到相位差,从而能够描述被测物体表面位移的变化。By using the interpolation calculation method, multiple phase-shift images required before the deformation of the measured object and multiple phase-shift images required after the object is deformed are obtained, instead of the objects collected one by one in the existing phase-shift electronic speckle interferometry method Multiple phase-shift images before and after the object is deformed, eliminating the need for multiple phase-shift images before and after the object is deformed, thus solving the problem that the existing phase-shift electron speckle interferometry method can only be used in static or quasi-static measurement In addition, the measurement method described in this embodiment is to add the concept of interpolation calculation on the basis of the existing phase-shift electronic speckle interferometry, so there is no need to increase the use of additional optical equipment or The arrangement can realize dynamic measurement only by using the existing phase-shift electronic speckle interferometry device, and finally calculate the phase difference, so that the change of the surface displacement of the measured object can be described.

本实施例还包括一种单步相移电子散斑干涉测量装置,包括激光器、摄像机和计算机,其中,所述激光器用于照射被测物体从而产生电子散斑图像;所述摄像机用于采集电子散斑图像;所述计算机用于执行所述单步相移电子散斑干涉测量方法以对采集到的电子散斑图像进行处理。This embodiment also includes a single-step phase-shift electronic speckle interferometry device, including a laser, a camera and a computer, wherein the laser is used to irradiate the measured object to generate an electronic speckle image; the camera is used to collect electronic speckle images. A speckle image; the computer is configured to execute the single-step phase-shift electronic speckle interferometry method to process the collected electronic speckle image.

本实施例还包括一种存储介质,其中存储有处理器可执行的指令,所述处理器可执行的指令在由处理器执行时用于执行本实施例所述单步相移电子散斑干涉测量方法。This embodiment further includes a storage medium, in which processor-executable instructions are stored, and when executed by the processor, the processor-executable instructions are used to perform the single-step phase-shift electronic speckle interferometry described in this embodiment. Measurement methods.

当本实施例中所述单步相移电子散斑干涉测量系统是使用计算机等终端运行相应的程序执行时,所述介质是指计算机等终端中的存储模块。这些方法、介质的功能被实现时,可以实现与本实施例单步相移电子散斑干涉测量系统相同的技术效果。When the single-step phase-shift electronic speckle interferometry system in this embodiment is executed by using a terminal such as a computer to run a corresponding program, the medium refers to a storage module in the terminal such as a computer. When the functions of these methods and media are implemented, the same technical effect as the single-step phase-shift electronic speckle interferometry system of this embodiment can be achieved.

图3为本发明实施例中所述利用插值计算获得的每个时刻的四幅相移图的分布情况;其中,*符号表示的是从采集所得的所述电子散斑图像中提取的相移图像的图像强度,实心点表示的是通过插值计算得到的相移图像的图像强度;本图是通过所述单步相移电子散斑干涉测量方法,根据光学测量原理,以相移量为0时为例,测量得到的每个时刻的四幅相移图的分布情况;其具体过程如下:Fig. 3 is the distribution of four phase shift images at each moment obtained by interpolation calculation in the embodiment of the present invention; wherein, the * symbol represents the phase shift image extracted from the collected electron speckle image The image intensity of , the solid point represents the image intensity of the phase-shifted image calculated by interpolation; this figure is based on the single-step phase-shift electron speckle interferometry method, according to the principle of optical measurement, when the phase shift amount is 0 For example, the distribution of the four phase shift maps obtained at each moment is measured; the specific process is as follows:

以相移量为0时为例,从采集所得的所述电子散斑图像中提取的相移图像为k=1,5,9,13,这些图像的强度应该遵循平滑曲线,则对应的子图像k=2,3,4,k=6,7,8,k=10,11,12,k=14,15,16都可以通过插值计算的方式得到;即只需采集并提取某一时刻的一幅相移图像,其余三幅相移图像可以通过插值计算的方式获得。插值结果可以表达为:Taking the phase shift amount of 0 as an example, the phase shift images extracted from the collected electron speckle images are k=1, 5, 9, 13, the intensity of these images should follow a smooth curve, then the corresponding sub- Images k=2, 3, 4, k=6, 7, 8, k=10, 11, 12, k=14, 15, and 16 can be obtained by interpolation; that is, only a certain moment needs to be collected and extracted One phase-shift image of , and the remaining three phase-shift images can be obtained by interpolation. The interpolation result can be expressed as:

Imod(k-1,4)+1,k=Ik I mod(k-1,4)+1, k =I k

Figure BDA0002251959220000111
Figure BDA0002251959220000111

其中,当m=mod(k-1,4)+1=1时,从采集所得的所述电子散斑图像中提取的相移图像对应为0°相位步长,其中mod(,)是模或余数函数;类似地,当m=mod(k-1,4)+1=2,3,4时,对应为90°,180°,270°相位步长的相移图像。也就是说,m=mod(k-1,4)+1为I的第一个下标,当m=mod(k-1,4)+1等于1时,表示0°相位步长,m=mod(k-1,4)+1等于2时,表示90°相位步长,m=mod(k-1,4)+1等于3时,表示180°相位步长,m=mod(k-1,4)+1等于4时,表示270°相位步长。I的第二个下标k指的是帧号;需要注意的是,该插值计算过程需要在所需测量的目标相移图像之前和之后分别采集六个“额外”相移图像,即前相移图像组和后相移图像组,其中目标相移图像是从采集所得的所述电子散斑图像中提取得到,前相移图像组和后相移图像组也是从采集所得的所述电子散斑图像中提取得到。Wherein, when m=mod(k-1,4)+1=1, the phase shift image extracted from the collected electron speckle image corresponds to a 0° phase step, where mod(,) is the modulo or the remainder function; similarly, when m=mod(k-1,4)+1=2, 3, 4, it corresponds to a phase-shifted image with phase steps of 90°, 180°, and 270°. That is to say, m=mod(k-1, 4)+1 is the first subscript of I, when m=mod(k-1, 4)+1 is equal to 1, it means 0° phase step, m When =mod(k-1,4)+1 is equal to 2, it represents a 90° phase step, and when m=mod(k-1,4)+1 is equal to 3, it represents a 180° phase step, m=mod(k When -1,4)+1 equals 4, it represents a 270° phase step. The second subscript k of I refers to the frame number; it should be noted that this interpolation calculation process requires the acquisition of six "extra" phase-shift images before and after the target phase-shift image to be measured, i.e. the pre-phase A group of shifted images and a group of post-phase shifted images, wherein the target phase shifted image is extracted from the acquired electron speckle images, and the pre-phase shifted image group and the post-phase shifted image group are also obtained from the acquired electron speckle images. extracted from the spot image.

使用上式,可以得到图3中实心圆所示的通过插值计算得到的相移图像的图像强度,即通过插值计算得到的其余三幅相移图像。通过这种方式,在每次图像测量时可获得任一时刻所需的四幅相移图像,其中一幅图像直接测量,另外三幅通过插值计算得到。参照图3中相位步长为0°的曲线,当从采集所得的所述电子散斑图像中提取的相移图像为k=1,5,9,13时,则对应的子图像k=2,3,4,k=6,7,8,k=10,11,12,k=14,15,16都可以通过插值计算的方式得到,其中,k=1,5,9,13时的从采集所得的所述电子散斑图像中提取的相移图像的图像强度用*符号表示,k=2,3,4,k=6,7,8,k=10,11,12,k=14,15,16的通过插值计算得到的相移图像的图像强度用实心点表示;同样地,参照图3中相位步长为90°的曲线,当从采集所得的所述电子散斑图像中提取的相移图像为k=2,6,10,14时,则对应的子图像k=3,4,5,k=7,8,9,k=11,12,13,k=15,16,17都可以通过插值计算的方式得到,其中,k=2,6,10,14时的从采集所得的所述电子散斑图像中提取的相移图像的图像强度用*符号表示,k=3,4,5,k=7,8,9,k=11,12,13,k=15,16,17的通过插值计算得到的相移图像的图像强度用实心点表示;同样地,参照图3中相位步长为180°的曲线,当从采集所得的所述电子散斑图像中提取的相移图像为k=3,7,11,15时,则对应的子图像k=4,5,6,k=8,9,10,k=12,13,14,k=16,17,18都可以通过插值计算的方式得到,其中,k=3,7,11,15时的从采集所得的所述电子散斑图像中提取的相移图像的图像强度用*符号表示,k=4,5,6,k=8,9,10,k=12,13,14,k=16,17,18的通过插值计算得到的相移图像的图像强度用实心点表示;同样地,参照图3中相位步长为270°的曲线,当从采集所得的所述电子散斑图像中提取的相移图像为k=4,8,12,16时,则对应的子图像k=5,6,7,k=9,10,11,k=13,14,15,k=17,18,19都可以通过插值计算的方式得到,其中,k=4,8,12,16时的从采集所得的所述电子散斑图像中提取的相移图像的图像强度用*符号表示,k=5,6,7,k=9,10,11,k=13,14,15,k=17,18,19的通过插值计算得到的相移图像的图像强度用实心点表示。按照此类方法,便可得到每个时刻的四幅相移图的分布情况。Using the above formula, the image intensities of the phase-shifted images shown by the solid circles in Fig. 3 obtained by interpolation can be obtained, that is, the remaining three phase-shifted images obtained by interpolation. In this way, four phase-shifted images required at any moment can be obtained during each image measurement, one of which is directly measured, and the other three are calculated by interpolation. Referring to the curve with a phase step of 0° in FIG. 3 , when the phase shift images extracted from the collected electronic speckle images are k=1, 5, 9, and 13, the corresponding sub-images are k=2 , 3, 4, k=6, 7, 8, k=10, 11, 12, k=14, 15, 16 can be obtained by interpolation, where k=1, 5, 9, 13 The image intensities of the phase-shifted images extracted from the acquired electron speckle images are indicated by the * symbol, k=2, 3, 4, k=6, 7, 8, k=10, 11, 12, k= 14, 15, 16 The image intensities of the phase-shifted images obtained by interpolation are represented by solid dots; similarly, referring to the curve with the phase step size of 90° in Fig. 3, when the electron speckle images obtained from the acquisition are When the extracted phase shift images are k=2, 6, 10, 14, the corresponding sub-images are k=3, 4, 5, k=7, 8, 9, k=11, 12, 13, k=15, 16 and 17 can be obtained by means of interpolation calculation, wherein, the image intensity of the phase-shifted image extracted from the collected electron speckle image when k=2, 6, 10, 14 is represented by the symbol *, k = 3, 4, 5, k = 7, 8, 9, k = 11, 12, 13, k = 15, 16, 17 The image intensities of the phase-shifted images calculated by interpolation are indicated by solid dots; similarly, Referring to the curve with the phase step size of 180° in FIG. 3 , when the phase shift images extracted from the collected electron speckle images are k=3, 7, 11, and 15, the corresponding sub-images are k=4 , 5, 6, k=8, 9, 10, k=12, 13, 14, k=16, 17, 18 can be obtained by interpolation, where k=3, 7, 11, 15 The image intensities of the phase-shifted images extracted from the acquired electron speckle images are denoted by the * symbol, k=4, 5, 6, k=8, 9, 10, k=12, 13, 14, k= 16, 17, 18 The image intensities of the phase-shifted images calculated by interpolation are represented by solid dots; similarly, referring to the curve with the phase step size of 270° in Fig. 3, when the electron speckle images obtained from the acquisition are When the extracted phase shift images are k=4, 8, 12, 16, the corresponding sub-images k=5, 6, 7, k=9, 10, 11, k=13, 14, 15, k=17, 18 and 19 can be obtained by means of interpolation calculation, wherein, the image intensity of the phase-shifted image extracted from the collected electron speckle image when k=4, 8, 12, 16 is represented by the symbol *, k =5, 6, 7, k=9, 10, 11, k=13, 14, 15, k=17, 18, 19 The image intensities of the phase-shifted images calculated by interpolation are indicated by solid dots. According to this method, the distribution of the four phase shift maps at each moment can be obtained.

以上所述,只是本发明的较佳实施例而已,本发明并不局限于上述实施方式,只要其以相同的手段达到本发明的技术效果,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明保护的范围之内。在本发明的保护范围内其技术方案和/或实施方式可以有各种不同的修改和变化。The above are only preferred embodiments of the present invention, and the present invention is not limited to the above-mentioned embodiments, as long as it achieves the technical effect of the present invention by the same means, all within the spirit and principle of the present invention, do Any modification, equivalent replacement, improvement, etc., should be included within the protection scope of the present invention. Various modifications and changes can be made to its technical solutions and/or implementations within the protection scope of the present invention.

Claims (9)

1. A single-step phase-shifted electronic speckle interferometry method, comprising:
collecting an electronic speckle image of a measured object;
extracting a first phase shift image from the electronic speckle image acquired at a first moment;
extracting a second phase-shift image from the electronic speckle image acquired at the second moment;
performing interpolation calculation on the first phase shift image and the second phase shift image;
generating at least one sub-image of the first phase shift image according to the result of the interpolation calculation;
generating at least one sub-image of the second phase-shift image according to the result of the interpolation calculation;
analyzing the first phase shift image, the sub-image of the first phase shift image, the second phase shift image and the sub-image of the second phase shift image, and calculating and extracting to obtain a phase difference between the first moment and the second moment; the phase difference is used to describe the change in surface displacement of the object being measured.
2. The single-step phase-shifted electronic speckle interferometry method according to claim 1, wherein the step of performing interpolation calculation on the first phase-shifted image and the second phase-shifted image comprises:
extracting a front phase-shift image group and a rear phase-shift image group from the electronic speckle images; the front phase shift image group comprises a plurality of phase shift images extracted before the target phase shift image, and the rear phase shift image group comprises a plurality of phase shift images extracted after the target phase shift image; the target phase shift images are respectively a first phase shift image and a second phase shift image;
and performing interpolation calculation by using the extracted front phase shift image group and the extracted rear phase shift image group.
3. The single-step phase-shifted electronic speckle interferometry method according to claim 2, wherein said interpolation calculation is performed by the following formula:
Figure FDA0002251959210000011
Figure FDA0002251959210000012
in the formula In2、In3、In4Sub-images, I, respectively, of the phase-shifted image of the objectn-6、In-5、In-3、In-2、In-1Forming the front phase shift image group; i isn+1、In+2、In+3、In+5、In+6And forming the post phase shift image group.
4. A single-step phase-shift electronic speckle interferometry method is characterized by comprising the following steps:
collecting electronic speckle images of a measured object at multiple moments;
performing the measurement method of any one of claims 1 to 3 for the electronic speckle image at any first and second time instants to output a phase difference between the first and second time instants; the phase difference is used to describe the change in surface displacement of the object being measured.
5. A single-step phase-shifted electronic speckle interferometry system, comprising:
the acquisition module is used for acquiring an electronic speckle image of a measured object;
the extraction module is used for extracting a first phase shift image from the electronic speckle images acquired at a first moment and extracting a second phase shift image from the electronic speckle images acquired at a second moment;
the calculation module is used for carrying out interpolation calculation on the first phase shift image and the second phase shift image;
the generating module is used for generating at least one sub-image of the first phase shift image according to the result of the interpolation calculation; and generating at least one sub-image of the second phase-shifted image;
the processing module is used for analyzing the first phase shift image, the sub-image of the first phase shift image, the second phase shift image and the sub-image of the second phase shift image, calculating and extracting the phase difference between the first moment and the second moment; the phase difference is used for describing the change of the surface displacement of the measured object;
and the output module is used for outputting the extracted phase difference.
6. The system of claim 5, wherein the computing module comprises:
the device comprises an extraction unit, a phase shift unit and a phase shift unit, wherein the extraction unit is used for extracting a front phase shift image group and a rear phase shift image group from an acquired electronic speckle image of a measured object, the front phase shift image group comprises a plurality of phase shift images extracted before a target phase shift image, and the rear phase shift image group comprises a plurality of phase shift images extracted after the target phase shift image; the target phase shift images are respectively a first phase shift image and a second phase shift image;
and the computing unit is used for carrying out interpolation computation by utilizing the extracted front phase shift image group and the extracted rear phase shift image group.
7. The system of claim 5, wherein the processing module comprises:
an analysis unit for analyzing the first phase-shifted image, the sub-image of the first phase-shifted image, the second phase-shifted image at the second time, and the sub-image of the second phase-shifted image;
a calculation unit for calculating a phase difference between the first time and the second time;
and the extraction unit is used for extracting the calculated phase difference.
8. A single-step phase-shift electronic speckle interferometry device is characterized by comprising a laser, a camera and a computer, wherein the laser is used for irradiating a measured object so as to generate an electronic speckle image; the camera is used for collecting electronic speckle images; the computer is configured to perform the method of any one of claims 1-3 to process the acquired electronic speckle images.
9. A storage medium having stored therein processor-executable instructions, which when executed by a processor, are configured to perform the method of claims 1-3.
CN201911037596.1A 2019-10-29 2019-10-29 Single-step phase-shift electronic speckle interferometry method, system, device and storage medium Active CN110823117B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201911037596.1A CN110823117B (en) 2019-10-29 2019-10-29 Single-step phase-shift electronic speckle interferometry method, system, device and storage medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201911037596.1A CN110823117B (en) 2019-10-29 2019-10-29 Single-step phase-shift electronic speckle interferometry method, system, device and storage medium

Publications (2)

Publication Number Publication Date
CN110823117A true CN110823117A (en) 2020-02-21
CN110823117B CN110823117B (en) 2021-06-01

Family

ID=69551089

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201911037596.1A Active CN110823117B (en) 2019-10-29 2019-10-29 Single-step phase-shift electronic speckle interferometry method, system, device and storage medium

Country Status (1)

Country Link
CN (1) CN110823117B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114485448A (en) * 2022-01-25 2022-05-13 上海大学 An adaptive speckle interferometry method and system

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7079257B1 (en) * 2002-04-08 2006-07-18 Providence Health System Methods and apparatus for evaluating mechanical and thermal strains in electronic materials, semiconductor materials, and other structures
CN102353332A (en) * 2011-06-28 2012-02-15 山东大学 Electronic speckle-interference digital-compensating method and system thereof
CN104268837A (en) * 2014-09-26 2015-01-07 天津工业大学 Method for extracting phase position information of electronic speckle interference fringe pattern
CN104280139A (en) * 2014-10-27 2015-01-14 广州飞拓优视光电科技有限公司 Dynamic phase measuring device and method
CN105300307A (en) * 2015-11-20 2016-02-03 北京理工大学 Device and method for optical mirror distortion measurement of relevant techniques of two-dimensional digital speckling

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7079257B1 (en) * 2002-04-08 2006-07-18 Providence Health System Methods and apparatus for evaluating mechanical and thermal strains in electronic materials, semiconductor materials, and other structures
CN102353332A (en) * 2011-06-28 2012-02-15 山东大学 Electronic speckle-interference digital-compensating method and system thereof
CN104268837A (en) * 2014-09-26 2015-01-07 天津工业大学 Method for extracting phase position information of electronic speckle interference fringe pattern
CN104280139A (en) * 2014-10-27 2015-01-14 广州飞拓优视光电科技有限公司 Dynamic phase measuring device and method
CN105300307A (en) * 2015-11-20 2016-02-03 北京理工大学 Device and method for optical mirror distortion measurement of relevant techniques of two-dimensional digital speckling

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
蔡长青 等: "基于四步相移的相位差提取方法", 《华南理工大学学报(自然科学版)》 *

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114485448A (en) * 2022-01-25 2022-05-13 上海大学 An adaptive speckle interferometry method and system
CN114485448B (en) * 2022-01-25 2022-11-15 上海大学 Self-adaptive speckle interferometry method and system
WO2023142628A1 (en) * 2022-01-25 2023-08-03 上海大学绍兴研究院 Adaptive speckle interferometry method and system

Also Published As

Publication number Publication date
CN110823117B (en) 2021-06-01

Similar Documents

Publication Publication Date Title
CN110108348B (en) Micro-amplitude vibration measurement method and system for thin-walled parts based on motion-amplified optical flow tracking
Chen et al. Modal identification of simple structures with high-speed video using motion magnification
JP6574989B2 (en) Stress measuring apparatus, stress measuring system and stress measuring method
Stanislas et al. Main results of the third international PIV challenge
JP4883223B2 (en) Motion vector generation apparatus and motion vector generation method
Timoner et al. Multi-image gradient-based algorithms for motion estimation
WO2013136620A1 (en) Phase distribution analysis method and device for fringe image using high-dimensional brightness information, and program therefor
CN110268222B (en) Three-dimensional shape measuring device, three-dimensional shape measuring method, and storage medium
JP2014002744A (en) Event-based image processing apparatus and method using the same
TW201243484A (en) Resolution test device and method thereof
JP5669071B2 (en) Time correlation camera
Dorn et al. Efficient full-field vibration measurements and operational modal analysis using neuromorphic event-based imaging
US20150369589A1 (en) Positional shift amount measurement method, correction table generation apparatus, imaging apparatus, and projecting apparatus
CN114577444A (en) Detection method and detection device for modulation transfer function
JP2008216127A (en) Distance image generation device, distance image generation method, and program
CN110823117B (en) Single-step phase-shift electronic speckle interferometry method, system, device and storage medium
Morlier et al. Virtual vibration measurement using KLT motion tracking algorithm
Wei et al. Interferometric-scale full-field vibration measurement by a combination of digital image correlation and laser vibrometer
JP5219024B2 (en) Image processing apparatus, imaging apparatus, and image processing program
CN105593635A (en) Measurement method, measurement device, measurement program, and computer-readable recording medium recording measurement program
Li et al. Super-sensitivity full-field measurement of structural vibration with an adaptive incoherent optical method
CN116595344A (en) Signal reconstruction method and device based on visual structure vibration mode identification under environmental excitation
Liang et al. Vibration Measurement of a Metal Sheet Using Single‐Camera Digital Image Correlation with Projection Components
JP2021005206A (en) Image processing device, image processing method, and program
Price A comparison of Operating Deflection Shape and Motion Amplification Video Techniques for Vibration Analysis

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