CN111964601B - Speckle interference multi-parameter measuring system and method based on Taffy optical path - Google Patents

Speckle interference multi-parameter measuring system and method based on Taffy optical path Download PDF

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CN111964601B
CN111964601B CN202010758589.7A CN202010758589A CN111964601B CN 111964601 B CN111964601 B CN 111964601B CN 202010758589 A CN202010758589 A CN 202010758589A CN 111964601 B CN111964601 B CN 111964601B
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deformation
speckle interference
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顾国庆
王艳芳
邱成春
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Yancheng Institute of Technology
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    • 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
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Abstract

本发明涉及一种基于达菲光路的散斑干涉多参数测量系统及测量方法,激光器发射的激光经过第一反射镜在第一分光棱镜中分束为透射光波和反射光波,透射光波经过光学粗糙参考表面后在第二反射镜中形成一束参考光波;反射光波沿着光轴方向照射至被测物体表面后被分成第一物光波和第二物光波,第一物光波、第二物光波各自产生错位并分别形成两束剪切物光波,这四束剪切物光波与一束参考光波同时通过第二分光棱镜后共同成像在单色CCD相机靶面上,形成耦合散斑干涉图像;本发明能够实现对被测物体的变形、应变等多参数信息的同步动态测量,不仅测量系统结构简单,而且测量方法容易。

Figure 202010758589

The invention relates to a speckle interference multi-parameter measurement system and measurement method based on Duffy optical path. After referring to the surface, a beam of reference light waves is formed in the second reflector; the reflected light waves are irradiated to the surface of the object to be measured along the direction of the optical axis and are divided into the first object light wave and the second object light wave, the first object light wave and the second object light wave. Displacement occurs and two shearing object light waves are respectively formed. These four shearing object light waves and a reference light wave pass through the second beam splitting prism at the same time and are jointly imaged on the target surface of the monochromatic CCD camera to form a coupled speckle interference image; The invention can realize the synchronous dynamic measurement of the deformation, strain and other multi-parameter information of the measured object, not only the structure of the measurement system is simple, but also the measurement method is easy.

Figure 202010758589

Description

基于达菲光路的散斑干涉多参数测量系统及测量方法Speckle interference multi-parameter measurement system and measurement method based on Duffy optical path

技术领域technical field

本发明涉及一种基于达菲光路的散斑干涉多参数测量系统及测量方法,属于光学测量技术领域。The invention relates to a speckle interference multi-parameter measurement system and a measurement method based on the Duffy optical path, belonging to the technical field of optical measurement.

背景技术Background technique

散斑干涉是一种具有高灵敏度、高精度、实时、全场非接触测量等优点的现代光学测量方法,近年来已被广泛应用在航空航天、机械制造、汽车工程等领域先进材料测试与分析中。散斑干涉系统可以直接测量结构变形信息,却不能直接测量变形一阶导数,即应变信息。根据不同变形测量需求,散斑干涉系统一般可分为面内变形测量系统和离面变形测量系统。通常,应变信息可以通过散斑干涉测量变形信息经数值微分得到,或者通过剪切散斑干涉系统测量获得;但是剪切散斑干涉又不能直接测量变形,而且数值微分计算往往又会造成随机误差扩散传输。在实际工程应用中,承载结构质量安全评估和使用寿命预测都离不开变形和应变信息的同时获得,因此,设计开发能够同时测量变形和多个应变信息的散斑干涉系统以满足实际应用中多参数同步测量需求就显得至关重要。Speckle interferometry is a modern optical measurement method with the advantages of high sensitivity, high precision, real-time, full-field non-contact measurement. In recent years, it has been widely used in advanced material testing and analysis in aerospace, mechanical manufacturing, automotive engineering and other fields. middle. The speckle interferometry system can directly measure the structural deformation information, but cannot directly measure the first derivative of the deformation, that is, the strain information. According to different deformation measurement requirements, speckle interferometry systems can generally be divided into in-plane deformation measurement systems and out-of-plane deformation measurement systems. Usually, strain information can be obtained by numerical differentiation of deformation information by speckle interferometry, or by shear speckle interferometry; however, shear speckle interferometry cannot directly measure deformation, and numerical differential calculation often causes random errors Diffusion transmission. In practical engineering applications, the quality safety assessment and service life prediction of load-bearing structures are inseparable from the simultaneous acquisition of deformation and strain information. Therefore, a speckle interferometry system that can measure deformation and multiple strain information at the same time is designed and developed to meet practical applications. The need for simultaneous multi-parameter measurement is crucial.

现有能够实现变形和应变测量的散斑干涉系统一般可以分成两类:第一类是将散斑干涉系统和剪切散斑干涉系统简单组合形成整体系统分别测量变形和应变信息。该组合系统通过依次切换不同光路可以实现独立测量变形和应变信息,但是不能实现同时测量,且组合系统结构复杂,测量过程极不方便,不适合动态测量;第二类是在基于迈克尔逊(Michelson)式剪切散斑干涉系统中引入参考光波进而实现变形和应变的同时测量。该系统是目前最为常见的变形和应变同步测量系统,利用空间相移技术只需在一幅耦合散斑干涉图中即可同步解调出变形和应变信息,而且系统空间结构简单,测量方法便捷,适合动态测量。但是,该系统视场会受到迈克尔逊剪切装置限制,通常需要增加光学4f系统进行改进,而且,空间载频调制与剪切量控制相互不独立,难以完全分离出有用频谱信息;此外,无论是组合测量系统还是迈克尔逊式系统都只能测量变形和单个应变分量。Existing speckle interferometry systems that can measure deformation and strain can generally be divided into two categories: the first type is to simply combine the speckle interferometry system and the shear speckle interferometry system to form an overall system to measure deformation and strain information respectively. The combined system can achieve independent measurement of deformation and strain information by switching different optical paths in turn, but it cannot achieve simultaneous measurement, and the combined system has a complex structure, the measurement process is extremely inconvenient, and it is not suitable for dynamic measurement; the second type is based on Michelson (Michelson) ) type shear speckle interferometry system is introduced into the reference light wave to realize the simultaneous measurement of deformation and strain. This system is currently the most common deformation and strain synchronous measurement system. Using the spatial phase shift technology, the deformation and strain information can be synchronously demodulated only in a coupled speckle interferogram, and the system has a simple spatial structure and convenient measurement methods. , suitable for dynamic measurement. However, the field of view of this system is limited by the Michelson shear device, which usually needs to be improved by adding an optical 4f system. Moreover, the spatial carrier frequency modulation and the shear amount control are not independent of each other, so it is difficult to completely separate the useful spectral information; Either the combined measurement system or the Michelson-type system can only measure deformation and a single strain component.

发明内容SUMMARY OF THE INVENTION

本发明提供一种基于达菲光路的散斑干涉多参数测量系统及测量方法,能够实现对被测物体的变形、应变信息的同步动态测量,不仅测量系统结构简单,而且测量方法容易。The invention provides a speckle interference multi-parameter measurement system and measurement method based on Duffy optical path, which can realize synchronous dynamic measurement of deformation and strain information of a measured object, not only the measurement system has a simple structure, but also the measurement method is easy.

本发明解决其技术问题所采用的技术方案是:The technical scheme adopted by the present invention to solve its technical problems is:

一种基于达菲光路的散斑干涉多参数测量系统,以激光器为照射光源,其发射的激光经过第一反射镜在第一分光棱镜中按照5:5分束为透射光波和反射光波;A speckle interference multi-parameter measurement system based on the Duffy optical path, using a laser as an illumination light source, the emitted laser beam is divided into transmitted light waves and reflected light waves according to 5:5 in a first beam splitting prism through a first reflecting mirror;

前述透射光波经过光学粗糙参考表面后形成空间漫反射光波,空间漫反射光波顺次经过第一孔径光阑以及第二反射镜后形成一束参考光波;The aforementioned transmitted light waves pass through the optically rough reference surface to form spatial diffuse reflection light waves, and the spatial diffuse reflection light waves pass through the first aperture diaphragm and the second reflector in sequence to form a beam of reference light waves;

前述反射光波沿着光轴方向照射至被测物体表面后被分成第一物光波和第二物光波,第一物光波、第二物光波分别与光轴之间的夹角相同,其中第一物光波顺次经过第二孔径光阑、第三反射镜、全反直角棱镜、渥拉斯顿剪切装置形成两束剪切物光波,第二物光波顺次经过第三孔径光阑、第四反射镜、全反直角棱镜、渥拉斯顿剪切装置形成两束剪切物光波;The aforementioned reflected light wave is irradiated to the surface of the object to be measured along the direction of the optical axis, and is divided into a first object light wave and a second object light wave. The object light wave passes through the second aperture diaphragm, the third mirror, the all-inverse right-angle prism, and the Wollaston shearing device in sequence to form two sheared object light waves, and the second object light wave passes through the third aperture diaphragm, Four reflection mirrors, all-inverting right-angle prisms, and Wollaston shearing device form two beams of shearing object light waves;

四束剪切物光波与一束参考光波同时通过第二分光棱镜后共同成像在单色CCD相机靶面上;Four shearing object light waves and one reference light wave pass through the second beam splitting prism at the same time and are imaged together on the target surface of the monochromatic CCD camera;

其中,第二孔径光阑、第三孔径光阑相对光轴对称设置,第三反射镜、第四反射镜相对光轴对称设置,被测物体、第一分光棱镜、全反直角棱镜、渥拉斯顿剪切装置、第二分光棱镜以及单色CCD相机均依次分布在光轴上,第三反射镜与第四反射镜垂直于光轴的中心线的中心位置上布设全反直角棱镜;Among them, the second aperture diaphragm and the third aperture diaphragm are symmetrically arranged relative to the optical axis, the third reflecting mirror and the fourth reflecting mirror are symmetrically arranged relative to the optical axis, the object to be measured, the first beam splitting prism, the all-inverse right-angle prism, the Wola The ston shearing device, the second beam splitting prism and the monochromatic CCD camera are all distributed on the optical axis in turn, and an all-reverse right-angle prism is arranged at the center position of the third reflecting mirror and the fourth reflecting mirror perpendicular to the center line of the optical axis;

第一反射镜、第一分光棱镜以及光学粗糙参考表面形成的连接线与光轴垂直;The connecting line formed by the first reflecting mirror, the first beam splitting prism and the optical rough reference surface is perpendicular to the optical axis;

作为本发明的进一步优选,第一物光波经过渥拉斯顿剪切装置错位后的两束剪切物光波相互干涉形成第一剪切散斑干涉图像,第二物光波经过渥拉斯顿剪切装置错位后的两束剪切物光波相互干涉形成第二剪切散斑干涉图像;As a further preference of the present invention, two shearing object light waves after the first object light wave is displaced by the Wollaston shearing device interfere with each other to form a first shearing speckle interference image, and the second object light wave passes through the Wollaston shearing device. The two shearing object light waves after the dislocation of the cutting device interfere with each other to form a second shearing speckle interference image;

参考光波与剪切物光波相互干涉形成混合散斑干涉图像,混合散斑干涉图像分别与第一剪切散斑干涉图像、第二剪切散斑干涉图像再次发生干涉在单色CCD相机靶面形成耦合散斑干涉图像;The reference light wave and the shearing object light wave interfere with each other to form a mixed speckle interference image. The mixed speckle interference image interferes with the first shearing speckle interference image and the second shearing speckle interference image respectively on the target surface of the monochromatic CCD camera. form a coupled speckle interference image;

一种基于上述任意所述的基于达菲光路的散斑干涉多参数测量系统的测量方法,A measurement method based on any of the above-mentioned Duffy optical path-based speckle interference multi-parameter measurement systems,

第一步:被测物体加载变形前,通过激光器提供激光光源,单色CCD相机采集变形前的第一剪切散斑干涉图像;Step 1: Before the measured object is loaded and deformed, the laser light source is provided by the laser, and the monochromatic CCD camera collects the first sheared speckle interference image before the deformation;

第二步:对变形前的第一剪切散斑干涉图像进行傅里叶变换,获取变形前的第一剪切散斑干涉图像的空间频谱;Step 2: Fourier transform is performed on the first sheared speckle interference image before deformation, and the spatial spectrum of the first sheared speckle interference image before deformation is obtained;

第三步:对获取的变形前的第一剪切散斑干涉图像的空间频谱通过设置滤波窗口提取含有相位信息的高频项;The third step: extracting high-frequency terms containing phase information by setting a filter window for the obtained spatial spectrum of the first sheared speckle interference image before deformation;

第四步:对获取的变形前的第一剪切散斑干涉图像的高频项进行相位提取,得到变形前第一剪切散斑干涉图像含有变形、应变信息的相位信息;The fourth step: extracting the phase of the high frequency term of the obtained first sheared speckle interference image before deformation, to obtain phase information containing deformation and strain information in the first sheared speckle interference image before deformation;

第五步:加载装置对被测物体加载变形,按照第一步至第四步的步骤获取变形后第一剪切散斑干涉图像含有变形、应变信息的相位信息;Step 5: The loading device loads and deforms the measured object, and obtains the phase information of the deformation and strain information in the first sheared speckle interference image after deformation according to the steps from the first to the fourth step;

第六步:将被测物体变形前后的第一剪切散斑干涉图像的相位信息进行实时相减,得到第一剪切散斑干涉图像中与变形、应变有关的相位差;Step 6: Subtract the phase information of the first sheared speckle interference image before and after the deformation of the measured object in real time to obtain the phase difference related to deformation and strain in the first sheared speckle interference image;

第七步:按照第一步至第六步的方式,分别获取第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差;Step 7: Obtain the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the hybrid speckle interference image respectively according to the methods of the first step to the sixth step;

第八步:对前述获取的第一剪切散斑干涉图像中与变形、应变有关的相位差、第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差分布图像分别进行滤波处理,对滤波处理后的相位差分布图像进行解包裹处理,获取光滑连续的相位分布;通过获取的光滑连续的相位差分布计算获得被测物体的变形和应变;Step 8: Compare the phase difference related to deformation and strain in the first shearing speckle interference image obtained above, the phase difference related to deformation and strain in the second shearing speckle interference image, and the mixed speckle interference image. The phase difference distribution images related to deformation and strain are filtered respectively, and the filtered phase difference distribution image is unwrapped to obtain a smooth and continuous phase distribution; the measured object is obtained by calculating the obtained smooth and continuous phase difference distribution. deformation and strain;

作为本发明的进一步优选,As a further preference of the present invention,

第一步中,第一物光波经过渥拉斯顿剪切装置错位后的两束剪切物光波,变形前的被测物体在单色CCD相机靶面相互干涉形成第一剪切散斑干涉图像,其光强表示为In the first step, the first object light wave passes through the two shearing object light waves after the dislocation of the Wollaston shearing device, and the measured object before deformation interferes with each other on the target surface of the monochromatic CCD camera to form the first shearing speckle interference. image, whose light intensity is expressed as

I1(x,y)=[u11(x,y)+u12(x+△x,y)]·[u11(x,y)+u12(x+△x,y)]* (1)I 1 (x,y)=[u 11 (x,y)+u 12 (x+△x,y)]·[u 11 (x,y)+u 12 (x+△x,y)] * (1 )

其中,u11(x,y)为第一物光波错位后的一束剪切物光波的复振幅,u12(x+△x,y)为第一物光波错位后的另一束剪切物光波的复振幅,

Figure BDA0002612405610000031
为u11(x,y)的复共轭,
Figure BDA0002612405610000032
为u12(x+△x,y)的复共轭,Δx为被测物体经过渥拉斯顿剪切装置后沿x方向物面剪切量;Among them, u 11 (x, y) is the complex amplitude of a beam of shearing object light waves after the first object light wave is dislocated, and u 12 (x+△x, y) is another beam of shearing objects after the first object light wave is dislocated the complex amplitude of a light wave,
Figure BDA0002612405610000031
is the complex conjugate of u 11 (x,y),
Figure BDA0002612405610000032
is the complex conjugate of u 12 (x+△x,y), and Δx is the shearing amount of the measured object along the x-direction after passing through the Wollaston shearing device;

作为本发明的进一步优选,第二步中,对变形前的第一剪切散斑干涉图像进行傅里叶变换,获取变形前的第一剪切散斑干涉图像的空间频谱表示为As a further preference of the present invention, in the second step, Fourier transform is performed on the first sheared speckle interference image before deformation, and the spatial spectrum of the obtained first sheared speckle interference image before deformation is expressed as:

Figure BDA0002612405610000033
Figure BDA0002612405610000033

其中,

Figure BDA0002612405610000034
代表空间频谱中含有背景光的低频项频谱,
Figure BDA0002612405610000035
表示频域中卷积运算符,C*(fx-f0,fy)和C(fx+f0,fy)是互为共轭的高频项频谱,其含有x方向剪切的相位信息;fx为空间频谱的横坐标,fy为空间频谱的纵坐标,f0是由孔径光阑引入的载波频率;in,
Figure BDA0002612405610000034
represents the spectrum of the low-frequency term containing the background light in the spatial spectrum,
Figure BDA0002612405610000035
Represents the convolution operator in the frequency domain, C * (f x -f 0 , f y ) and C(f x +f 0 , f y ) are mutually conjugated high-frequency term spectra, which contain x-direction clipping The phase information of ; f x is the abscissa of the spatial spectrum, f y is the ordinate of the spatial spectrum, and f 0 is the carrier frequency introduced by the aperture diaphragm;

第三步中,选择截止频率,设置滤波窗口提取含有相位信息的高频项,具体的,利用设置的以(f0,0)为中心,以截止频率fr(fr<f0)为半径的圆形滤波窗口提取频谱作为含有x方向剪切的相位信息的频谱,对其进行移中处理并作逆傅里叶变换;In the third step, select the cutoff frequency, set the filter window to extract high-frequency terms containing phase information, specifically, use the set (f 0 , 0) as the center, and the cut-off frequency fr (f r < f 0 ) as The circular filter window of the radius extracts the spectrum as the spectrum containing the phase information clipped in the x-direction, and performs center-shift processing and inverse Fourier transform on it;

作为本发明的进一步优选,第四步中,获取被测物体变形前的第一剪切散斑干涉图像含有变形、应变信息的相位信息,其表示为As a further preference of the present invention, in the fourth step, the first sheared speckle interference image obtained before the deformation of the measured object contains phase information of deformation and strain information, which is expressed as

Figure BDA0002612405610000041
Figure BDA0002612405610000041

其中,Im为取虚部运算符,Re为取实部运算符,u11(x,y)为第一物光波错位后的一束剪切物光波的复振幅,u12(x+△x,y)为第一物光波错位后的另一束剪切物光波的复振幅,

Figure BDA0002612405610000042
为u12(x+△x,y)的复共轭;Among them, Im is the operator for taking the imaginary part, Re is the operator for taking the real part, u 11 (x, y) is the complex amplitude of a shearing object light wave after the first object light wave is dislocated, u 12 (x+△x, y) is the complex amplitude of another shearing object light wave after the dislocation of the first object light wave,
Figure BDA0002612405610000042
is the complex conjugate of u 12 (x+△x,y);

第五步中,按照第一步至第四步的步骤获取变形后第一剪切散斑干涉图像含有变形、应变信息的相位信息,具体为φ1a(x+△x,y);In the fifth step, the first sheared speckle interference image after deformation is obtained according to the steps from the first step to the fourth step and contains the phase information of the deformation and strain information, specifically φ 1a (x+Δx,y);

第六步中,将被测物体变形前后的第一剪切散斑干涉图像的相位信息进行实时相减,得到第一剪切散斑干涉图像中与变形、应变有关的相位差In the sixth step, the phase information of the first sheared speckle interference image before and after the deformation of the measured object is subtracted in real time to obtain the phase difference related to deformation and strain in the first sheared speckle interference image.

Figure BDA0002612405610000043
Figure BDA0002612405610000043

其中,

Figure BDA0002612405610000044
为第一剪切散斑干涉图像中与变形、应变有关的相位差,φ1a(x+△x,y)为变形后第一剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA0002612405610000045
为变形前第一剪切散斑干涉图像含有变形、应变信息的相位信息;in,
Figure BDA0002612405610000044
is the phase difference related to deformation and strain in the first shearing speckle interference image, φ 1a (x+△x,y) is the phase information that contains deformation and strain information in the first shearing speckle interference image after deformation,
Figure BDA0002612405610000045
is the phase information containing deformation and strain information for the first sheared speckle interference image before deformation;

作为本发明的进一步优选,第七步中,获取第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差分别为As a further preference of the present invention, in the seventh step, the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the hybrid speckle interference image are obtained as:

Figure BDA0002612405610000046
Figure BDA0002612405610000046

其中,

Figure BDA0002612405610000047
为第二剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000048
为混合散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000049
为变形后第二剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA00026124056100000410
为变形前第二剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA00026124056100000411
为变形后混合散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA00026124056100000412
为变形前混合散斑干涉图像含有变形、应变信息的相位信息;in,
Figure BDA0002612405610000047
is the phase difference related to deformation and strain in the second sheared speckle interference image,
Figure BDA0002612405610000048
is the phase difference related to deformation and strain in the mixed speckle interference image,
Figure BDA0002612405610000049
is the phase information of the deformation and strain information of the second sheared speckle interference image after deformation,
Figure BDA00026124056100000410
is the phase information containing the deformation and strain information of the second sheared speckle interference image before deformation,
Figure BDA00026124056100000411
is the phase information of the deformed mixed speckle interference image containing deformation and strain information,
Figure BDA00026124056100000412
Phase information containing deformation and strain information for the mixed speckle interference image before deformation;

作为本发明的进一步优选,通过获取的光滑连续的相位差分布计算被测物体的变形和应变,表示为As a further preference of the present invention, the obtained smooth and continuous phase difference distribution is used to calculate the deformation and strain of the measured object, which are expressed as

Figure BDA0002612405610000051
Figure BDA0002612405610000051

其中,w为被测物体的离面变形,

Figure BDA0002612405610000052
为被测物体的面内应变分量,
Figure BDA0002612405610000053
分别为被测物体的离面应变分量,△x为被测物体经过渥拉斯顿剪切装置后沿x方向物面剪切量,λ为系统所用激光光源波长,θ为系统观察方向与法线方向夹角,
Figure BDA0002612405610000054
为第一剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000055
为第二剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000056
为混合散斑干涉图像中与变形、应变有关的相位差。Among them, w is the out-of-plane deformation of the measured object,
Figure BDA0002612405610000052
is the in-plane strain component of the measured object,
Figure BDA0002612405610000053
are the out-of-plane strain components of the measured object, respectively, △x is the shearing amount of the measured object along the x-direction after passing through the Wollaston shearing device, λ is the wavelength of the laser light source used by the system, and θ is the observation direction and method of the system. Line direction angle,
Figure BDA0002612405610000054
is the phase difference related to deformation and strain in the first sheared speckle interference image,
Figure BDA0002612405610000055
is the phase difference related to deformation and strain in the second sheared speckle interference image,
Figure BDA0002612405610000056
is the phase difference related to deformation and strain in the mixed speckle interference image.

通过以上技术方案,相对于现有技术,本发明具有以下有益效果:Through the above technical solutions, with respect to the prior art, the present invention has the following beneficial effects:

1、本发明仅需使用一个激光器作为照射光源、一个单色CCD相机记录图像,包含多个独立共存的光路,使得测量系统结构得到简化,降低了测量成本;1. The present invention only needs to use one laser as the illumination light source and one monochromatic CCD camera to record the image, including multiple independent coexisting optical paths, which simplifies the structure of the measurement system and reduces the measurement cost;

2、本发明提供的测量系统中,设置了多个可调孔径光阑实现空间载波,利用傅里叶变换对单幅耦合散斑干涉图像进行频域处理,并使用频域滤波直接提取对应变形和多个应变分量的相位信息,实现了多参数动态同时进行测量;2. In the measurement system provided by the present invention, a plurality of adjustable aperture diaphragms are set to realize the space carrier, the single coupled speckle interference image is processed in the frequency domain by the Fourier transform, and the corresponding deformation is directly extracted by the frequency domain filtering. and the phase information of multiple strain components, realizing multi-parameter dynamic simultaneous measurement;

3、本发明使用渥拉斯顿剪切装置,同时实现两条独立的共光路剪切路径,使得系统抗干扰能力强,稳定性较好。3. The present invention uses the Wollaston shearing device to realize two independent common optical path shearing paths at the same time, so that the system has strong anti-interference ability and good stability.

附图说明Description of drawings

下面结合附图和实施例对本发明进一步说明。The present invention will be further described below in conjunction with the accompanying drawings and embodiments.

图1是本发明提供的基于达菲光路的散斑干涉多参数测量系统构成示意图。FIG. 1 is a schematic diagram of the structure of a speckle interference multi-parameter measurement system based on the Duffy optical path provided by the present invention.

图中:1为激光器,2为被测物体,3为第一反射镜,4为第一分光棱镜,5为光学粗糙参考表面,6为第一孔径光阑,7为第二反射镜,8为第二分光棱镜,9为第二孔径光阑,10为第三反射镜,11为第三孔径光阑,12为第四反射镜,13为全反直角棱镜,14为渥拉斯顿剪切装置,15单色CCD相机。In the figure: 1 is the laser, 2 is the object to be measured, 3 is the first mirror, 4 is the first beam splitting prism, 5 is the optical rough reference surface, 6 is the first aperture diaphragm, 7 is the second mirror, 8 is the second beam splitting prism, 9 is the second aperture diaphragm, 10 is the third reflecting mirror, 11 is the third aperture diaphragm, 12 is the fourth reflecting mirror, 13 is an all-inversion right angle prism, and 14 is the Wollaston scissors Cut device, 15 monochrome CCD cameras.

具体实施方式Detailed ways

现在结合附图对本发明作进一步详细的说明。这些附图均为简化的示意图,仅以示意方式说明本发明的基本结构,因此其仅显示与本发明有关的构成。The present invention will now be described in further detail with reference to the accompanying drawings. These drawings are all simplified schematic diagrams, and only illustrate the basic structure of the present invention in a schematic manner, so they only show the structures related to the present invention.

为了实现对被测物体2的变形、应变信息的同步动态测量,本发明提供一种基于达菲光路的散斑干涉多参数测量系统,该系统如图1所示,包括激光器1、第一反射镜3、第二反射镜7、第三反射镜10、第四反射镜12、第一分光棱镜4、第二分光棱镜8、渥拉斯顿剪切装置14、全反直角棱镜13、第一孔径光阑6、第二孔径光阑9、第三孔径光阑11以及单色CCD相机15,图中,被测物体2、第一分光棱镜4、全反直角棱镜13、渥拉斯顿剪切装置14、第二分光棱镜8以及单色CCD相机15均依次分布在光轴上,第三反射镜10与第四反射镜12垂直于光轴的中心线的中心位置上布设全反直角棱镜13,第一反射镜3与光学粗糙参考表面5形成的连接线与光轴垂直,同时第一分光棱镜4位于此连接线上,第二孔径光阑9、第三孔径光阑11相对光轴对称设置,第三反射镜10、第四反射镜12相对光轴对称设置;In order to realize the synchronous dynamic measurement of the deformation and strain information of the measured object 2, the present invention provides a speckle interference multi-parameter measurement system based on the Duffy optical path. As shown in FIG. 1, the system includes a laser 1, a first reflection Mirror 3, second reflector 7, third reflector 10, fourth reflector 12, first beam splitter prism 4, second beam splitter prism 8, Wollaston shearing device 14, all-inversion right angle prism 13, first Aperture diaphragm 6, second aperture diaphragm 9, third aperture diaphragm 11 and monochromatic CCD camera 15, in the figure, measured object 2, first beam splitting prism 4, all-inverting right angle prism 13, Wollaston shear The cutting device 14, the second beam splitting prism 8 and the monochromatic CCD camera 15 are all distributed on the optical axis in turn, and an all-inversion right angle prism is arranged at the center position of the third reflecting mirror 10 and the fourth reflecting mirror 12 perpendicular to the center line of the optical axis. 13. The connecting line formed by the first reflecting mirror 3 and the optical rough reference surface 5 is perpendicular to the optical axis, while the first beam splitting prism 4 is located on this connecting line, and the second aperture stop 9 and the third aperture stop 11 are relative to the optical axis. Symmetrically arranged, the third reflecting mirror 10 and the fourth reflecting mirror 12 are symmetrically arranged relative to the optical axis;

此测量系统中,以激光器1为照射光源,其发射的激光经过第一反射镜3在第一分光棱镜4中按照5:5分束为透射光波和反射光波;透射光波经过光学粗糙参考表面5后形成空间漫反射光波,空间漫反射光波顺次经过第一孔径光阑6以及第二反射镜7后形成一束参考光波;反射光波沿着光轴方向照射至被测物体2表面后被分成第一物光波和第二物光波,第一物光波、第二物光波分别与光轴之间的夹角相同,其中第一物光波顺次经过第二孔径光阑9、第三反射镜10、全反直角棱镜13、渥拉斯顿剪切装置14形成两束剪切物光波,第二物光波顺次经过第三孔径光阑11、第四反射镜12、全反直角棱镜13、渥拉斯顿剪切装置14形成两束剪切物光波;In this measurement system, the laser 1 is used as the illumination light source, and the laser light emitted by it passes through the first reflecting mirror 3 and is split into the transmitted light wave and the reflected light wave according to 5:5 in the first beam splitting prism 4; the transmitted light wave passes through the optical rough reference surface 5 Then a spatial diffuse reflection light wave is formed, and the spatial diffuse reflection light wave passes through the first aperture diaphragm 6 and the second mirror 7 in sequence to form a beam of reference light waves; The first object light wave and the second object light wave, the first object light wave and the second object light wave are respectively at the same angle with the optical axis, wherein the first object light wave passes through the second aperture diaphragm 9 and the third mirror 10 in sequence , the all-reverse right-angle prism 13, and the Wollaston shearing device 14 form two beams of shearing object light waves, and the second object light wave passes through the third aperture diaphragm 11, the fourth mirror 12, the all-reverse right-angle prism 13, and the second object light wave in sequence. The Ruston shearing device 14 forms two sheared object light waves;

也就是说,第一物光波、第二物光波经过渥拉斯顿剪切装置14,各自产生错位并分别形成两束剪切物光波,这四束剪切物光波与一束参考光波同时通过第二分光棱镜8后共同成像在单色CCD相机15靶面上,形成耦合散斑干涉图像,其中,第一幅图像为第一物光波经渥拉斯顿剪切装置14错位后的两束剪切物光波相互干涉形成的剪切散斑干涉图像,第二幅图像为第二物光波经渥拉斯顿剪切装置14错位后的另两束剪切物光波相互干涉形成的剪切散斑干涉图像;这两幅剪切散斑干涉图像分别在单色CCD相机15靶面两侧成像,相互之间不发生重叠干扰;第三幅图像为参考光波与剪切物光波相互干涉形成的混合散斑干涉图像;在单色CCD相机15的靶面上,混合散斑干涉图像分别与前两幅剪切散斑干涉图像再次发生干涉形成耦合散斑干涉图像,最终可实现变形及多个应变分量的同时测量。That is to say, when the first object light wave and the second object light wave pass through the Wollaston shearing device 14, they are respectively dislocated and form two shearing object light waves respectively, and these four shearing object light waves and one reference light wave pass through at the same time The second beam splitting prism 8 is then jointly imaged on the target surface of the monochromatic CCD camera 15 to form a coupled speckle interference image, wherein the first image is the two beams of the first object light wave after being displaced by the Wollaston shearing device 14 The shearing speckle interference image formed by the mutual interference of the shearing object light waves, the second image is the shearing speckle interference image formed by the mutual interference of the other two shearing object light waves after the second object light wave is displaced by the Wollaston shearing device 14 Speckle interference images; the two sheared speckle interference images are imaged on both sides of the target surface of the monochromatic CCD camera 15 respectively, and there is no overlapping interference with each other; the third image is formed by the mutual interference of the reference light wave and the sheared object light wave Mixed speckle interference image; on the target surface of the monochromatic CCD camera 15, the mixed speckle interference image and the first two sheared speckle interference images respectively interfere again to form a coupled speckle interference image, which can finally achieve deformation and multiple Simultaneous measurement of strain components.

接着,基于上述测量系统,本申请提供了一种测量方法,其原理主要是利用加载装置对被测物体2进行加载使其发生变形,分别采集单色CCD相机15靶面上的被测物体2变形前后的耦合散斑干涉图像,对采集到的两幅耦合散斑干涉图像进行傅里叶变换,获得多参数散斑干涉图像的频谱(即被测物体2变形前后的混合频谱),设置合适频率范围对混合频谱中含有变形和应变信息的频谱区域分别设置滤波窗口进行提取,分别获得含有变形及多应变信息的光波复振幅频谱部分,并对其分别进行逆傅里叶变换,分别获得含有变形及多应变信息的光波复振幅,通过复振幅相位提取,分别得到对应变形及多应变信息的相位分布;将被测物体2在变形前后的与变形有关的相位信息进行实时相减,得到表征被测物体2表面变形的相位差(包括被测物体2的离面变形相位信息和含有应变信息的混合相位信息),将含有应变信息的混合相位信息进行几何运算,从而进一步获得变形测量结果;按照单个相位信息相减的做法,将被测物体2在变形前后的多个应变相位信息进行实时相减,得到表征被测物体2表面多个应变的相位差,并对与应变有关的混合相位信息进行几何运算得到独立的应变相位信息,从而得到被测物体2表面多个应变的测量结果。Next, based on the above measurement system, the present application provides a measurement method, the principle of which is mainly to use a loading device to load the measured object 2 to deform it, and to collect the measured object 2 on the target surface of the monochrome CCD camera 15 respectively. For the coupled speckle interference images before and after deformation, Fourier transform is performed on the two collected coupled speckle interference images to obtain the spectrum of the multi-parameter speckle interference image (that is, the mixed spectrum of the measured object 2 before and after deformation), and the settings are appropriate. The frequency range is to set filter windows for the spectral regions containing deformation and strain information in the mixed spectrum, respectively, to obtain the spectral parts of the complex amplitude of the light wave containing deformation and multi-strain information, and perform inverse Fourier transform on them to obtain the spectral regions containing deformation and multi-strain information. The optical wave complex amplitude of deformation and multi-strain information, through the complex amplitude phase extraction, the phase distribution corresponding to the deformation and multi-strain information are obtained respectively; the phase information related to the deformation of the measured object 2 before and after the deformation is subtracted in real time to obtain the characterization The phase difference of the surface deformation of the measured object 2 (including the out-of-plane deformation phase information of the measured object 2 and the mixed phase information containing the strain information), and the mixed phase information containing the strain information is subjected to geometric operations, thereby further obtaining the deformation measurement results; According to the method of subtracting the single phase information, the multiple strain phase information of the measured object 2 before and after the deformation is subtracted in real time, and the phase difference characterizing the multiple strains on the surface of the measured object 2 is obtained, and the mixed phase related to the strain is obtained. The information is subjected to geometric operations to obtain independent strain phase information, thereby obtaining measurement results of multiple strains on the surface of the object to be measured 2 .

按照图1提供的测量系统,本申请提出的基于达菲光路的散斑干涉多参数测量系统的测量方法,具体包括以下步骤,According to the measurement system provided in FIG. 1, the measurement method of the speckle interference multi-parameter measurement system based on the Duffy optical path proposed in this application specifically includes the following steps:

第一步:被测物体2加载变形前,通过激光器1提供激光光源,单色CCD相机15采集变形前的第一剪切散斑干涉图像;即第一物光波经过渥拉斯顿剪切装置14错位后的两束剪切物光波,变形前的被测物体2在单色CCD相机15靶面相互干涉形成第一剪切散斑干涉图像,其光强表示为Step 1: Before the measured object 2 is loaded and deformed, the laser light source is provided by the laser 1, and the monochromatic CCD camera 15 collects the first sheared speckle interference image before the deformation; that is, the first object light wave passes through the Wollaston shearing device 14 The two shearing object light waves after dislocation and the measured object 2 before deformation interfere with each other on the target surface of the monochromatic CCD camera 15 to form the first shearing speckle interference image, and its light intensity is expressed as

I1(x,y)=[u11(x,y)+u12(x+△x,y)]·[u11(x,y)+u12(x+△x,y)]* (1)I 1 (x,y)=[u 11 (x,y)+u 12 (x+△x,y)]·[u 11 (x,y)+u 12 (x+△x,y)] * (1 )

其中,u11(x,y)为第一物光波错位后的一束剪切物光波的复振幅,u12(x+△x,y)为第一物光波错位后的另一束剪切物光波的复振幅,

Figure BDA0002612405610000071
为u11(x,y)的复共轭,
Figure BDA0002612405610000072
为u12(x+△x,y)的复共轭,Δx为被测物体2经过渥拉斯顿剪切装置14后沿x方向物面剪切量。Among them, u 11 (x, y) is the complex amplitude of a beam of shearing object light waves after the first object light wave is dislocated, and u 12 (x+△x, y) is another beam of shearing objects after the first object light wave is dislocated the complex amplitude of a light wave,
Figure BDA0002612405610000071
is the complex conjugate of u 11 (x,y),
Figure BDA0002612405610000072
is the complex conjugate of u 12 (x+Δx, y), and Δx is the shearing amount of the measured object 2 along the x-direction after passing through the Wollaston shearing device 14 .

第二步:对变形前的第一剪切散斑干涉图像进行傅里叶变换,获取变形前的第一剪切散斑干涉图像的空间频谱;获取的变形前的第一剪切散斑干涉图像的空间频谱表示为Step 2: Fourier transform is performed on the first sheared speckle interference image before deformation, and the spatial spectrum of the first sheared speckle interference image before deformation is obtained; the obtained first sheared speckle interference before deformation is obtained The spatial spectrum of the image is expressed as

Figure BDA0002612405610000073
Figure BDA0002612405610000073

其中,

Figure BDA0002612405610000074
代表空间频谱中含有背景光的低频项频谱,
Figure BDA0002612405610000075
表示频域中卷积运算符,C*(fx-f0,fy)和C(fx+f0,fy)是互为共轭的高频项频谱,其含有x方向剪切的相位信息;fx为空间频谱的横坐标,fy为空间频谱的纵坐标,f0是由孔径光阑引入的载波频率。in,
Figure BDA0002612405610000074
represents the spectrum of the low-frequency term containing the background light in the spatial spectrum,
Figure BDA0002612405610000075
Represents the convolution operator in the frequency domain, C * (f x -f 0 , f y ) and C(f x +f 0 , f y ) are mutually conjugated high-frequency term spectra, which contain x-direction clipping The phase information of ; f x is the abscissa of the spatial spectrum, f y is the ordinate of the spatial spectrum, and f 0 is the carrier frequency introduced by the aperture diaphragm.

第三步:对获取的变形前的第一剪切散斑干涉图像的空间频谱通过设置滤波窗口提取含有相位信息的高频项;具体的,选择截止频率,设置滤波窗口提取含有相位信息的高频项,利用设置的以(f0,0)为中心,以截止频率fr(fr<f0)为半径的圆形滤波窗口提取频谱作为含有x方向剪切的相位信息的频谱,对其进行移中处理并作逆傅里叶变换。Step 3: Extract high-frequency terms containing phase information from the obtained spatial spectrum of the first sheared speckle interference image before deformation by setting a filter window; specifically, select a cutoff frequency, set a filter window to extract high-frequency terms containing phase information Frequency term, using the set circular filter window with (f 0 , 0) as the center and the cutoff frequency fr (f r < f 0 ) as the radius to extract the spectrum as the spectrum containing the phase information clipped in the x direction, for It is center-shifted and inverse Fourier transformed.

第四步:对获取的变形前的第一剪切散斑干涉图像的高频项进行相位提取,得到变形前第一剪切散斑干涉图像含有变形、应变信息的相位信息,其表示为The fourth step: extract the phase of the high frequency term of the obtained first sheared speckle interference image before deformation, and obtain the phase information of the first sheared speckle interference image before deformation containing deformation and strain information, which is expressed as:

Figure BDA0002612405610000081
Figure BDA0002612405610000081

其中,Im为取虚部运算符,Re为取实部运算符,u11(x,y)为第一物光波错位后的一束剪切物光波的复振幅,u12(x+△x,y)为第一物光波错位后的另一束剪切物光波的复振幅,

Figure BDA0002612405610000082
为u12(x+△x,y)的复共轭。Among them, Im is the operator for taking the imaginary part, Re is the operator for taking the real part, u 11 (x, y) is the complex amplitude of a shearing object light wave after the first object light wave is dislocated, u 12 (x+△x, y) is the complex amplitude of another shearing object light wave after the dislocation of the first object light wave,
Figure BDA0002612405610000082
is the complex conjugate of u 12 (x+Δx,y).

第五步:加载装置对被测物体2加载变形,按照第一步至第四步的步骤获取变形后第一剪切散斑干涉图像含有变形、应变信息的相位信息,具体为φ1a(x+△x,y)。Step 5: The loading device loads and deforms the measured object 2, and obtains the phase information of the deformation and strain information in the first sheared speckle interference image after deformation according to the steps from the first to the fourth step, specifically φ 1a (x+ Δx,y).

第六步:将被测物体2变形前后的第一剪切散斑干涉图像的相位信息进行实时相减,得到第一剪切散斑干涉图像中与变形、应变有关的相位差Step 6: Subtract the phase information of the first sheared speckle interference image before and after the deformation of the measured object 2 in real time to obtain the phase difference related to deformation and strain in the first sheared speckle interference image

Figure BDA0002612405610000083
Figure BDA0002612405610000083

其中,

Figure BDA0002612405610000084
为第一剪切散斑干涉图像中与变形、应变有关的相位差,φ1a(x+△x,y)为变形后第一剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA0002612405610000085
为变形前第一剪切散斑干涉图像含有变形、应变信息的相位信息。in,
Figure BDA0002612405610000084
is the phase difference related to deformation and strain in the first shearing speckle interference image, φ 1a (x+△x,y) is the phase information that contains deformation and strain information in the first shearing speckle interference image after deformation,
Figure BDA0002612405610000085
Phase information containing deformation and strain information for the first sheared speckle interference image before deformation.

第七步:按照第一步至第六步的方式,分别获取第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差;Step 7: Obtain the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the hybrid speckle interference image respectively according to the methods of the first step to the sixth step;

获取第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差分别为The phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the hybrid speckle interference image are obtained as

Figure BDA0002612405610000091
Figure BDA0002612405610000091

其中,

Figure BDA0002612405610000092
为第二剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000093
为混合散斑干涉图像中与变形、应变有关的相位差,
Figure BDA0002612405610000094
为变形后第二剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA0002612405610000095
为变形前第二剪切散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA0002612405610000096
为变形后混合散斑干涉图像含有变形、应变信息的相位信息,
Figure BDA0002612405610000097
为变形前混合散斑干涉图像含有变形、应变信息的相位信息。in,
Figure BDA0002612405610000092
is the phase difference related to deformation and strain in the second sheared speckle interference image,
Figure BDA0002612405610000093
is the phase difference related to deformation and strain in the mixed speckle interference image,
Figure BDA0002612405610000094
is the phase information of the deformation and strain information of the second sheared speckle interference image after deformation,
Figure BDA0002612405610000095
is the phase information containing the deformation and strain information of the second sheared speckle interference image before deformation,
Figure BDA0002612405610000096
is the phase information of the deformed mixed speckle interference image containing deformation and strain information,
Figure BDA0002612405610000097
Phase information containing deformation and strain information for mixed speckle interference images before deformation.

第八步:由于公式(4)和(5)得到的相位差分布图像含有大量的随机噪声,会影响后续的变形和应变计算,为此选择适当的滤波算法对前述获取的第一剪切散斑干涉图像中与变形、应变有关的相位差、第二剪切散斑干涉图像中与变形、应变有关的相位差以及混合散斑干涉图像中与变形、应变有关的相位差分布图像分别进行滤波处理,对滤波处理后的相位差分布图像进行解包裹处理,获取光滑连续的相位分布;通过获取的光滑连续的相位差分布计算获得被测物体2的变形、应变,可表示为Step 8: Since the phase difference distribution images obtained by formulas (4) and (5) contain a large amount of random noise, which will affect the subsequent deformation and strain calculations, an appropriate filtering algorithm is selected for this purpose. The phase difference related to deformation and strain in the speckle interference image, the phase difference related to deformation and strain in the second shearing speckle interference image, and the phase difference distribution image related to deformation and strain in the hybrid speckle interference image are filtered respectively. processing, the filtered phase difference distribution image is unwrapped to obtain a smooth and continuous phase distribution; the deformation and strain of the measured object 2 are obtained by calculating the obtained smooth and continuous phase difference distribution, which can be expressed as

Figure BDA0002612405610000098
Figure BDA0002612405610000098

其中,w为被测物体2的离面变形,

Figure BDA0002612405610000099
为被测物体2的面内应变分量,
Figure BDA00026124056100000910
分别为被测物体2的离面应变分量,△x为被测物体2经过渥拉斯顿剪切装置14后沿x方向物面剪切量,λ为系统所用激光光源波长,θ为系统观察方向与法线方向夹角,
Figure BDA00026124056100000911
为第一剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA00026124056100000912
为第二剪切散斑干涉图像中与变形、应变有关的相位差,
Figure BDA00026124056100000913
为混合散斑干涉图像中与变形、应变有关的相位差。Among them, w is the out-of-plane deformation of the measured object 2,
Figure BDA0002612405610000099
is the in-plane strain component of the measured object 2,
Figure BDA00026124056100000910
are the out-of-plane strain components of the measured object 2, respectively, Δx is the shearing amount of the measured object 2 along the x direction after passing through the Wollaston shearing device 14, λ is the wavelength of the laser light source used by the system, and θ is the system observation the angle between the direction and the normal direction,
Figure BDA00026124056100000911
is the phase difference related to deformation and strain in the first sheared speckle interference image,
Figure BDA00026124056100000912
is the phase difference related to deformation and strain in the second sheared speckle interference image,
Figure BDA00026124056100000913
is the phase difference related to deformation and strain in the mixed speckle interference image.

在本申请提供的实施例中,通过调整测量系统的观察方向、渥拉斯顿剪切装置的剪切方向,也可以获取其他所需的应变分量。In the embodiments provided in this application, other required strain components can also be obtained by adjusting the observation direction of the measurement system and the shearing direction of the Wollaston shearing device.

本技术领域技术人员可以理解,除非另外定义,这里使用的所有术语(包括技术术语和科学术语)具有与本申请所属领域中的普通技术人员的一般理解相同的意义。还应该理解的是,诸如通用字典中定义的那些术语应该被理解为具有与现有技术的上下文中的意义一致的意义,并且除非像这里一样定义,不会用理想化或过于正式的含义来解释。It will be understood by one of ordinary skill in the art that, unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs. It should also be understood that terms such as those defined in general dictionaries should be understood to have meanings consistent with their meanings in the context of the prior art and, unless defined as herein, are not to be taken in an idealized or overly formal sense. explain.

本申请中所述的“和/或”的含义指的是各自单独存在或两者同时存在的情况均包括在内。The meaning of "and/or" described in this application means that each of them exists alone or both are included.

本申请中所述的“连接”的含义可以是部件之间的直接连接也可以是部件间通过其它部件的间接连接。The meaning of "connection" described in this application may be a direct connection between components or an indirect connection between components through other components.

以上述依据本发明的理想实施例为启示,通过上述的说明内容,相关工作人员完全可以在不偏离本项发明技术思想的范围内,进行多样的变更以及修改。本项发明的技术性范围并不局限于说明书上的内容,必须要根据权利要求范围来确定其技术性范围。Taking the above ideal embodiments according to the present invention as inspiration, and through the above description, relevant personnel can make various changes and modifications without departing from the technical idea of the present invention. The technical scope of the present invention is not limited to the contents in the specification, and the technical scope must be determined according to the scope of the claims.

Claims (7)

1. A speckle interference multi-parameter measurement system based on a Taffy optical path is characterized in that: the laser is used as an irradiation light source, and laser emitted by the laser is split into transmission light waves and reflection light waves in a first light splitting prism according to the ratio of 5:5 through a first reflector;
the transmitted light waves form spatial diffuse reflection light waves after passing through the optical rough reference surface, and the spatial diffuse reflection light waves form a beam of reference light waves after sequentially passing through the first aperture diaphragm and the second reflector;
the reflected light waves are irradiated to the surface of a measured object along the direction of an optical axis and then are divided into first object light waves and second object light waves, included angles between the first object light waves and the optical axis are the same as included angles between the second object light waves and the optical axis, the first object light waves sequentially pass through a second aperture diaphragm, a third reflector, a full-inverse right-angle prism and a Wollaston shearing device to form two shear object light waves, and the second object light waves sequentially pass through the third aperture diaphragm, a fourth reflector, the full-inverse right-angle prism and the Wollaston shearing device to form two shear object light waves;
the four beams of shear light waves and one beam of reference light waves simultaneously pass through a second light splitting prism and then are imaged on a target surface of a monochromatic CCD camera;
the device comprises a first aperture diaphragm, a second aperture diaphragm, a third reflector, a fourth reflector, a measured object, a first spectroscope, a full-reflection right-angle prism, a Wollaston shearing device, a second spectroscope and a monochromatic CCD camera, wherein the second aperture diaphragm and the third aperture diaphragm are symmetrically arranged relative to an optical axis;
a connecting line formed by the first reflector, the first beam splitter prism and the optical rough reference surface is vertical to the optical axis;
two shear object light waves of the first object light wave after dislocation of the Wollaston shearing device are mutually interfered to form a first shear speckle interference image, and two shear object light waves of the second object light wave after dislocation of the Wollaston shearing device are mutually interfered to form a second shear speckle interference image;
the reference light waves and the shearing object light waves are mutually interfered to form a mixed speckle interference image, and the mixed speckle interference image respectively interferes with the first shearing speckle interference image and the second shearing speckle interference image again to form a coupling speckle interference image on the target surface of the monochromatic CCD camera;
filtering the phase difference related to deformation and strain in the obtained first shearing speckle interference image, the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference distribution image related to deformation and strain in the mixed speckle interference image respectively through a filtering algorithm, and unwrapping the phase difference distribution image after filtering to obtain smooth and continuous phase distribution; and calculating to obtain the deformation and the strain of the measured object through the obtained smooth and continuous phase difference distribution.
2. A measuring method of the speckle interference multi-parameter measuring system based on the Taffy optical path is characterized in that:
the first step is as follows: before a measured object is loaded and deformed, a laser source is provided through a laser, and a monochromatic CCD camera collects a first shearing speckle interference image before deformation;
the second step is that: fourier transformation is carried out on the first shearing speckle interference image before deformation, and a spatial frequency spectrum of the first shearing speckle interference image before deformation is obtained;
the third step: extracting a high-frequency item containing phase information from the acquired space frequency spectrum of the first shearing speckle interference image before deformation by setting a filter window;
the fourth step: performing phase extraction on the high-frequency item of the acquired first shearing speckle interference image before deformation to obtain phase information of the first shearing speckle interference image before deformation, wherein the phase information contains deformation and strain information;
the fifth step: the loading device loads deformation on the measured object, and phase information containing deformation and strain information of the deformed first shearing speckle interference image is obtained according to the steps from the first step to the fourth step;
and a sixth step: subtracting phase information of the first shearing speckle interference image before and after the measured object is deformed in real time to obtain a phase difference related to deformation and strain in the first shearing speckle interference image;
the seventh step: respectively acquiring the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the mixed speckle interference image according to the modes from the first step to the sixth step;
eighth step: filtering the phase difference related to deformation and strain in the obtained first shearing speckle interference image, the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference distribution image related to deformation and strain in the mixed speckle interference image respectively, and unwrapping the phase difference distribution image after filtering to obtain smooth and continuous phase distribution; and calculating and obtaining the deformation and the strain of the measured object through the obtained smooth and continuous phase difference distribution.
3. The measuring method of the speckle interference multi-parameter measuring system based on the duffy optical path as claimed in claim 2, wherein:
in the first step, the two shear object light waves after the first object light wave passes through the Wollaston shearing device and is staggered, a measured object before deformation interferes with each other on a target surface of a monochromatic CCD camera to form a first shear speckle interference image, and the light intensity of the first shear speckle interference image is expressed as
I1(x,y)=[u11(x,y)+u12(x+Δx,y)]·[u11(x,y)+u12(x+Δx,y)]* (1)
Wherein u is11(x, y) is the complex amplitude of a shearer wave after dislocation of the first object wave, u12(x + Deltax, y) is the complex amplitude of another shear object wave after the dislocation of the first object wave,
Figure FDA0003295282920000021
is u11(x, y) in the presence of a complex conjugate,
Figure FDA0003295282920000031
is u12And (x + Deltax, y) complex conjugation, wherein Deltax is the object surface shearing quantity of the object to be measured along the x direction after the object passes through the Wollaston shearing device.
4. The measuring method of the speckle interference multi-parameter measuring system based on the duffy optical path as claimed in claim 3, wherein:
in the second step, Fourier transform is carried out on the first shearing speckle interference image before deformation, and the space frequency spectrum of the first shearing speckle interference image before deformation is obtained and expressed as
Figure FDA0003295282920000032
Wherein,
Figure FDA0003295282920000033
representing the spectrum of low frequency terms in the spatial spectrum with background light,
Figure FDA0003295282920000034
representing convolution operators in the frequency domain, C*(fx-f0,fy) And C (f)x+f0,fy) Is a mutually conjugated high-frequency term spectrum containing phase information sheared in the x direction; f. ofxIs the abscissa, f, of the spatial frequency spectrumyIs the ordinate, f, of the spatial frequency spectrum0Is the carrier frequency introduced by the aperture stop;
in a third step, the cut-off frequency is selected, the filtering window is set to extract the high frequency term containing the phase information, in particular by setting (f)00) centered on the cut-off frequency fr(fr<f0) The spectrum is extracted for a circular filter window of radius as the spectrum containing phase information clipped in the x-direction, shifted and inverse fourier transformed.
5. The measuring method of the speckle interference multi-parameter measuring system based on the Taffy optical path as claimed in claim 4, wherein:
in the fourth step, phase information containing deformation and strain information of the first shearing speckle interference image before the measured object is deformed is obtained and expressed as
Figure FDA0003295282920000035
Wherein Im is an operator of taking an imaginary part, Re is an operator of taking a real part, and u11(x, y) is the complex amplitude of a shearer wave after dislocation of the first object wave, u12(x + Deltax, y) is the complex amplitude of another shear object wave after the dislocation of the first object wave,
Figure FDA0003295282920000041
is u12(x + Δ x, y) complex conjugation;
in the fifth step, phase information containing deformation and strain information of the deformed first shearing speckle interference image is obtained according to the steps from the first step to the fourth step, and the phase information is phi1a(x+Δx,y);
In the sixth step, the phase information of the first shearing speckle interference image before and after the measured object is deformed is subtracted in real time to obtain the phase difference related to deformation and strain in the first shearing speckle interference image
Figure FDA0003295282920000042
Wherein,
Figure FDA0003295282920000043
is the phase difference related to deformation and strain in the first shearing speckle interference image, phi1a(x + Deltax, y) is the phase information of the deformed and strain information contained in the deformed first shearing speckle interference image,
Figure FDA0003295282920000044
the first shearing speckle interference image before deformation contains phase information of deformation and strain information.
6. The measuring method of the speckle interference multi-parameter measuring system based on the duffy optical path as claimed in claim 5, wherein:
in the seventh step, the phase difference related to deformation and strain in the second shearing speckle interference image and the phase difference related to deformation and strain in the mixed speckle interference image are respectively obtained
Figure FDA0003295282920000045
Wherein,
Figure FDA0003295282920000046
the phase difference related to deformation and strain in the second shearing speckle interference image,
Figure FDA0003295282920000047
in order to mix the phase difference related to deformation and strain in the speckle interference image,
Figure FDA0003295282920000048
the deformed second shearing speckle interference image contains phase information of deformation and strain information,
Figure FDA0003295282920000049
the second shearing speckle interference image before deformation contains phase information of deformation and strain information,
Figure FDA00032952829200000410
the deformed mixed speckle interference image contains phase information of deformation and strain information,
Figure FDA00032952829200000411
the mixed speckle interference image before deformation contains phase information of deformation and strain information.
7. The measuring method of the speckle interference multi-parameter measuring system based on the duffy optical path as claimed in claim 6, wherein: calculating the deformation and strain of the measured object by the obtained smooth and continuous phase difference distribution, and expressing as
Figure FDA0003295282920000051
Wherein w is the out-of-plane deformation of the object to be measured,
Figure FDA0003295282920000052
is the in-plane strain component of the object to be measured,
Figure FDA0003295282920000053
respectively is an out-of-plane strain component of a measured object, deltax is the object plane shearing quantity of the measured object along the x direction after passing through the Wollaston shearing device, lambda is the wavelength of a laser light source used by the system, theta is the included angle between the observation direction of the system and the normal direction,
Figure FDA0003295282920000054
the phase difference related to deformation and strain in the first shearing speckle interference image,
Figure FDA0003295282920000055
the phase difference related to deformation and strain in the second shearing speckle interference image,
Figure FDA0003295282920000056
the phase difference related to deformation and strain in the speckle interference image is mixed.
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