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    DIGIT L IM GE CORREL TION

    ADEEL ZAFAR

    1

    CEE 498KUC Experimental Methods in Structures and Materials

    March 14th, 2008

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    DIGITAL IMAGE CORRELATION

    ABSTRACT

    Non-contact, optical technique for obtaining full-

    field deformation

    It uses image processing to go from severalimages of material, and to then calculate the

    deformation at any point in the field , and to then

    find deformation and strain values

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    OUTLINE Introduction to DIC

    History and Developments

    Concept and Approach

    Methodology

    Theoretical background Calibration

    DIC-3D

    Various Tests and Results

    Advantages and Disadvantages

    Applications

    Conclusion

    3

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    INTRODUCTION

    What is DIC?

    It is computer based process to obtain a 2-D full field

    information by recording deformation and motion of

    speckle patterns on a specimen surface before and

    after deformation of the body

    It takes advantage of the fact that applied stresseschange both the thickness and optical properties of

    materials, to determine displacement

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    INTRODUCTION

    Why need DIC?

    Although the bulk macroscale testing provides useful

    information about materials but many process occur at

    microscale and nanoscale. As a result testing methods

    are required to have that resolution and capture results

    at that level

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    HISTORY AND DEVELOPMENTS

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    HISTORY AND DEVELOPMENTS

    Developed in the early 80s at the University of South

    Carolina to measure full-field in-plane displacements

    and displacement gradientsof a strained body at the

    macroscale 1987Methodology to measure crack initiation mode

    & stress intensity factor in brittle materials

    1988Mixed-mode loading

    19923D effects near a crack tip

    1997Deformations measured in micron and

    nanometer scales

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    HISTORY AND DEVELOPMENTS

    1997Plastic deformation patterns in ductile

    materials

    1998Method to evaluate large deformations

    2002Professor Lambros constructed crack growthresistance curves for functionally graded materials

    Contd.

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    CONCEPT AND APPROACH

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    EQUIPMENT

    It is less demanding

    optically-ordinary incoherent

    light is sufficient and no

    need for optical components

    Requires one Hi resolutioncamera for 2D displacement

    and for 3D displacement, 2

    cameras

    A computer and frame

    grabbing circuit card to

    digitize the output

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    CONCEPT

    It is very simple in concept

    Digital camera takes picture

    of surface of the specimen

    Image is downloaded from

    camera to a frame grabbingcircuit card

    Analog signal from CCD

    array are then digitized The data is stored for

    subsequent processing

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    APPROACH

    Surface of specimen is sprayed

    with target pattern This is photographed before and

    after specimen is deformed

    Digital image of specimen

    contains intensitymeasurements at each pixel

    location on CCD (charge couple

    device-sensor) array before and

    after Using target features and their

    location, displacement field is

    generated

    Accuracy upto 0.02 pixels havebeen achieved

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    METHODOLOGY

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    LOCATING TARGET FEATURE

    Camera with CCD array(Has small

    photosensitive cells and high pixel count)

    records intensity of light falling on a pixel.

    Array in high resolution camera is

    rectangular with thousand or more pixels

    per line and a thousand or more lines perimage. (3x3 pixel)

    Signal from CCD array is digitized and

    gives a reading of the light intensity for

    each pixel. Intensity readings are shownas 0 from dark pixels and 100 for light

    pixel(Grey Scale)

    Storage of image into pixel and

    combination of pixel is calledCONVOLUTION

    100 0 100 100 100

    0 0 0 0 0

    100 0 100 100 100

    0

    50

    0

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    LOCATING TARGET FEATURE

    To locate the target from

    intensity data on pixel array,

    DIC uses intensity pattern

    matching method called

    CORRELATION This is done by defining the

    subset of pixels that

    surround the key feature on

    target

    Matching two patterns

    establishes target

    displacement

    100 100 100 100 100 100 100 100 100

    100 100 0 100 100 100 100 100 100

    100 0 0 0 100 0 0 100 100

    100 100 0 100 100 100 100 100 100

    100 100 100 100 100 100 100 100 100

    50 50

    0

    5050

    50

    50 50

    0

    50

    0

    50

    100

    100

    100

    100

    50

    100 100

    100 100

    100

    100 100

    100

    100

    50

    100

    50

    100

    100

    100

    0

    100

    100

    0

    50

    100 100

    100

    100

    100

    50

    100

    100

    Initial After

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    TARGET FEATURE REQUIREMENT

    If you have same type oftarget, then it would be

    impossible to distinguish

    between them

    Need to have unique shape

    for each point

    This is achieved with

    speckles Speckle should cover at

    least 3x3 pixel area

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    SPECKLE PATTERNS

    Techniques in creating speckles are :-

    For small speckles-Spraying white paint and sprinkling of carbon

    particles

    For moderate speckles-Spraying white paint and the black paint is

    sprayed with light pass

    For large speckles-Spraying white paint and brushing black paint For very high resolution- Fluorescent paint is used

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    SPECKLE MATCHING

    It is done based on

    algorithm for matching

    intensity field of many

    speckles because ofrichness of intensity data

    as compared to

    individual speckle

    matching

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    SPECKLES WITH RESPECT TO SCALE

    Macroscale Nanoscle

    Speckles must be custom made to fit the scale of

    observation. Thus, for the nanoscale, a smaller

    speckle pattern must be used than for the

    macroscale.

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    DIGITAL IMAGE

    Corresponding

    intensity profile

    as a surface plot

    Typical digital

    image captured

    by CCD camera

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    DIGITAL IMAGE PROCESSINGTHEORETICAL BACKGROUND

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    THEORETICAL BACKGROUND

    2-D deformation In-plane displacement

    Strain fields

    Known discretefunctions

    f(x,y)Undeformed

    g(x,y)Deformed

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    THEORETICAL BACKGROUND

    up

    vp

    Components of displacement vector of point p in

    x and y direction:

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    USING G(X,Y)

    Use above equations to solve for displacement

    vector :

    Position of any point can be defined by

    correlation functions:

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    MAPPING DISPLACEMENT(MATCHING)

    Correlation involves comparison of intensity data of

    two pixel fields. Mapping the coordinates between the

    two fields is accomplished by using:-

    X = x+u(x,y)

    Y= y+v(x.y) Matching process involves minimizing coefficient that

    measure how well both configuration compare

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    MATCHING PROCESS

    Two different coefficient have been used to compareaccuracy Least-square correlation coefficient

    Cross-correlation coefficient

    is a light intensity value (grayscale level)

    is corresponding intensity

    value of the same point q after deformation

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    LEAST-SQUARES

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    CROSS-CORRELATION

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    SMOOTHING THE INTENSITY DATA

    Digital Image contains thousands of pixels with

    different gray scale values. Usually they changeabruptly

    This produces mathematical difficulties when

    determining mapping parameter Therefore data is smoothed over the entire field in

    both images. Process is called INTERPOLATION

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    SMOOTHING THE INTENSITY DATA

    Interpolation over the intensityvalues of deformed configuration

    is needed to determine these

    sub-pixel location intensity

    values

    Following interpolation schemes

    are generally used;-

    Bilinear

    Cubic

    Both interpolations approximates

    intensity value of any point that

    lies between pixels

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    BICUBIC INTERPOLATION

    BILINEAR INTERPOLATION

    INTERPOLATIONS

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    DETERMINATION OF DISPLACEMENT VECTOR

    Two methods exist:- Coarse-Fine method. Brute force approach in which

    minimization coefficients are computed for a wide range of

    values and are minimized independently. Time consuming

    Newton-Raphson method . All coefficients are minimized

    simultaneously. Faster

    The process involves in obtaining optimum solution by

    searching over given range for the deformationparameters

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    CALIBRATION

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    CALIBRATION

    Determination of Magnification factorRelates to dimension on specimen to a

    corresponding dimension on the image plane of

    camera

    Location of lens center

    Center of camera lens should coincide with center

    of area of interest

    Lens Distortion

    Lens with long focal lengths are employed to

    minimize lens distortion

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    DIC - 3DOUT OF PLANE DISPLACEMENT

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    STEREO IMAGING TECHNIQUE

    Measurement of 3D

    component on aspecimen is much more

    difficult

    2 CCD cameras areemployed

    Procedure is to get

    image from both cameras

    and then develop stereoimaging equations before

    correlation process

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    TESTS AND RESULTS

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    PROCESS

    Deformation vector field Strain fieldLive field

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    TRANSLATION TEST

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    ROTATION TESTS

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    TENSION TESTS

    Contour plot of displacement

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    FRACTURE TEST

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    FRACTURE TEST

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    FRACTURE TEST

    Deformation vector field Strain fieldLive field

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    FRACTURE TEST

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    ADVANTAGES AND DISADVANTAGES

    ADVANTAGES

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    ADVANTAGES

    Preparation of the specimen is relatively simple as the speckle

    patterns used as unique targets are made by spray painting its

    surface. Ordinary white light is used to illuminate the surface of the

    specimen.

    Specimen size is not an issue as the method can be applied to

    both large and small specimens. Specimen size isaccommodated by changing the magnification used in

    recording the image.

    The method is not overly sensitive to vibration and a vibration

    isolation table is not necessary. However, it is essential thatboth the specimen and the camera be stable during the time

    required to record the image.

    Large strains or significant rigid body movement does not

    cause difficulties if the specimen does not move out of the fieldof view of the camera.

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    DISADVANTAGES

    Sensitive to fluctuation and nonuniformity of light

    intensity

    Measuring out of plain displacement requires more

    equipment and expertise

    Mathematics involved is challenging

    The calibration process is tedious

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    APPLICATIONS

    Professional development

    LaVisions StrainMaster

    Correlation Solution in Biomechanics

    Research development

    Velocity vectors in displacement zone

    of steel during cold-rolling process

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    SUMMARY

    DIC is a non-contact method for measuring whole field

    displacement Method involves interpolation to smooth gray scale levels and

    then applies coefficient to map the parameters to find strains

    Mathematics involved is challenging, but if computer code is

    available, mapping process becomes automatic Accuracy is often quoted as 0.02 pixels for each displacement

    component. Accuracy depends on:-

    Interpolation schemes

    Lens distortion Uniformity of light distribution

    Quality of speckle pattern

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    REFERENCES

    http://www.airframer.com/news_story.html?release=108

    http://en.wikipedia.org/wiki/Digital_image_correlation

    Thesis by JAY K. Patel on DIC for microscale and nanoscale

    deformation measurements

    Thesis by Jorge Luis Abanto-bueno on Fracture Modeling

    Structural Engineering Seminar by Prof Lambros

    http://www.airframer.com/news_story.html?release=108http://en.wikipedia.org/wiki/Digital_image_correlationhttp://en.wikipedia.org/wiki/Digital_image_correlationhttp://www.airframer.com/news_story.html?release=108
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    QUESTIONS