CN111398057A - Heterogeneous material crack stress intensity factor calculation method applying DIC technology - Google Patents

Heterogeneous material crack stress intensity factor calculation method applying DIC technology Download PDF

Info

Publication number
CN111398057A
CN111398057A CN202010185995.9A CN202010185995A CN111398057A CN 111398057 A CN111398057 A CN 111398057A CN 202010185995 A CN202010185995 A CN 202010185995A CN 111398057 A CN111398057 A CN 111398057A
Authority
CN
China
Prior art keywords
integral
crack
subunits
stress intensity
intensity factor
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
CN202010185995.9A
Other languages
Chinese (zh)
Other versions
CN111398057B (en
Inventor
黄培彦
李稳
陈展标
郭馨艳
杨怡
郑小红
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.)
South China University of Technology SCUT
Original Assignee
South China University of Technology SCUT
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 South China University of Technology SCUT filed Critical South China University of Technology SCUT
Priority to CN202010185995.9A priority Critical patent/CN111398057B/en
Publication of CN111398057A publication Critical patent/CN111398057A/en
Application granted granted Critical
Publication of CN111398057B publication Critical patent/CN111398057B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N3/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N3/20Investigating strength properties of solid materials by application of mechanical stress by applying steady bending forces
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N3/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N3/08Investigating strength properties of solid materials by application of mechanical stress by applying steady tensile or compressive forces
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2203/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N2203/0058Kind of property studied
    • G01N2203/006Crack, flaws, fracture or rupture
    • G01N2203/0067Fracture or rupture
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2203/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N2203/0058Kind of property studied
    • G01N2203/0069Fatigue, creep, strain-stress relations or elastic constants
    • G01N2203/0075Strain-stress relations or elastic constants
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2203/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N2203/02Details not specific for a particular testing method
    • G01N2203/06Indicating or recording means; Sensing means
    • G01N2203/0641Indicating or recording means; Sensing means using optical, X-ray, ultraviolet, infrared or similar detectors
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2203/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N2203/02Details not specific for a particular testing method
    • G01N2203/06Indicating or recording means; Sensing means
    • G01N2203/067Parameter measured for estimating the property
    • G01N2203/0682Spatial dimension, e.g. length, area, angle

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)

Abstract

The invention discloses a heterogeneous material crack stress intensity factor calculation method applying DIC technology, which comprises the following steps: preparing a standard compression or tension test piece of the heterogeneous material, and performing unidirectional compression or tension to obtain the elastic modulus and the Poisson ratio; preparing a standard fracture test piece of a heterogeneous material with cracks, and preparing speckles for DIC test on the surface of a region around the cracks; carrying out a fracture experiment on the test piece to obtain a displacement field and a crack size of an area near the tip of the crack under different loads; selecting different integral paths, dividing subunits in the integral area, and calculating J-integral values of the subunits; filtering the J-integral value, then superposing the J-integral value to obtain the J-integral value on an integral path, and converting the J-integral value into a stress intensity factor K; and repeating the steps, and calculating J-integral values under different loads/displacements to obtain the stress intensity factor K at each loading moment. The invention has the characteristics of high efficiency, high precision, strong universality and the like.

Description

Heterogeneous material crack stress intensity factor calculation method applying DIC technology
Technical Field
The invention relates to the technical field of fracture mechanics and engineering thereof, in particular to a calculation method of a crack stress intensity factor of a heterogeneous material by using DIC technology.
Background
The stress intensity factor K of the crack problem in the complex structure is difficult to calculate by using a theoretical expression, but if the displacement field or the stress field of the area near the crack tip in the complex structure is obtained by other methods, the stress intensity factor K of the crack can be calculated, in recent years, the stress intensity factor of the crack in the complex structure can be calculated by using a Digital Image Correlation (DIC) method, which has the advantages of high precision, simplicity in use, non-contact, post-processing of displacement data, and the like.
Disclosure of Invention
The invention aims to overcome the defects of the prior art and provides a calculation method of a crack stress intensity factor of a heterogeneous material by using DIC technology. According to the method, a displacement field of a region near a crack of the heterogeneous material is measured through DIC technology, then a program is programmed to calculate J-integral on an integral path around the crack, and after the calculated value is filtered, the J-integral is converted into a stress intensity factor K.
The purpose of the invention can be realized by the following technical scheme:
a stress intensity factor calculation method for a crack problem in a heterogeneous material comprises the following steps:
preparing a standard compression or tension test piece of the heterogeneous material, and performing a unidirectional compression or tension experiment on the standard test piece to obtain the elastic modulus E and the Poisson ratio mu of the heterogeneous material;
preparing a standard fracture test piece of a heterogeneous material with cracks, and preparing speckles which are in black and white phase and are appropriate in size and uniformly distributed on the surface of a region around the cracks; the area around the crack is an area which takes the tip of the prefabricated crack as the center of a circle and takes 5-7 times of the length of the prefabricated crack as the radius; the maximum speckle of the speckle is no more than 6 pixels;
performing a fracture experiment on the test piece, synchronously recording the deformation of the area (speckle) around the crack in the loading process by adopting a CCD (charge coupled device) camera, and obtaining the displacement field U and the crack size of the area near the tip of the crack under different loads after the processing by DIC (digital computer) software;
selecting different integration paths, compiling a calculation program according to the obtained elastic modulus E and the displacement field U, dividing subunits in the integration regions, and calculating J-integral values of the subunits on the different paths;
carrying out filtering processing on the calculated J-integral value;
superposing the J-integral values of the remaining subunits after filtering to obtain the J-integral value on the integral path, and converting the J-integral value into a stress intensity factor K under the same load/displacement;
and repeating the steps of calculating the J-integral values of all the subunits on different paths, filtering the integral values, converting the integral values into stress intensity factors K, calculating the J-integral values under different loads/displacements, and filtering to obtain the stress intensity factors K at all the loading moments.
Preferably, the heterogeneous material is concrete, composite, fiber reinforced composite (FRP), rock, or the like.
Preferably, the standard fracture test piece is a unidirectional tensile Central Crack (CCT) test piece, a Compact Tension (CT) test piece, or a three-Point Bending (3-Point Bending) test piece.
Specifically, the method for dividing the sub-units in the integration area comprises the following steps: and dividing the subunits in the integration region in a triangular unit or quadrilateral unit mode according to the principle that the subunits are full, do not overlap and completely cover the whole integration region.
Specifically, the calculation formula of the J-integral value after superposition of each subunit on different paths is as follows:
Figure BDA0002414209340000031
in the formula, n is the number of subunits divided by the annular integral domain; gp represents the number of Gaussian integration points in each subunit; u. ofiDisplacement field, σ, measured for DIC methodsijFor the stress on each subunit node, i, j is 1, and 2 represents x and y directions respectively; omega is the strain energy density; q. q.s1Take 0 at the outer boundary and 0 at the inner boundary0Taking 1 above;1jis the kronecker tensor; x is the number ofk、ηkThe coordinates of the real parameter unit and the form parameter unit are respectively, and k represents the x direction and the y direction;
Figure BDA0002414209340000032
is the weight coefficient of the gaussian integration point.
Specifically, the J-integrated values of the subunits to be filtered are classified into the following two types:
j-integrated value J of sub-unit near the removed crackedge
Filtering out J-integral singular value J of subunit satisfying formula (2) by applying 3 sigma-5 sigma principle of probability theorysingular
Figure BDA0002414209340000041
In the formula, JAIIs the J-integral value of the subunit; e is JAIExpected value (mean value) of; d is JAIThe variance of (a); the value of the coefficient n is 3-5 (3 is taken when 3 sigma is adopted, and 5 is taken when 5 sigma is adopted).
Preferably, the crack-near subunit is a subunit having a shortest distance between the centroid and the crack boundary of 1 to 4 mm.
Compared with the prior art, the invention has the following beneficial effects:
1. according to the method, a Digital Image Correlation (DIC) technology is combined with a J-integral calculation method, a displacement field of a region around a crack is extracted through the DIC technology, the numerical integration idea of finite element discretization is combined, the concussion of the displacement field of the surface of a heterogeneous material/component and the error of the displacement field of the free boundary of an object measured through DIC are considered, and the calculation of J-integral and a stress intensity factor K is achieved through Matlab programming. The method combines the DIC technology with the J-integral calculation method and the filtering technology, has the characteristics of high efficiency, high precision, strong universality and the like, and is suitable for calculating the J-integral and the stress intensity factor K of crack problems in various structures or components containing heterogeneous materials.
Drawings
FIG. 1 is a schematic view of a three-point bending test piece.
FIG. 2 is a schematic illustration of a speckle pattern of a concrete surface.
FIG. 3 shows the displacement field U in the X-direction of the region around the crackXCloud pictures.
FIG. 4 is a schematic diagram of the closed-loop integration domain (integrator rail) and subunits of a crack.
FIG. 5 is a diagram illustrating the J-integration values of the sub-units in the integration domain.
Fig. 6 is a schematic diagram of the sub-unit in the vicinity of the crack.
Fig. 7 is a graph of the stress intensity factor K as a function of the load point displacement v.
Fig. 8 is a graph comparing the calculated value of the stress intensity factor K with the theoretical value.
Detailed Description
The present invention will be described in further detail with reference to examples and drawings, but the present invention is not limited thereto.
Examples
A stress intensity factor calculation method for a crack problem in a heterogeneous material comprises the following steps:
(1) preparing a standard compression or tension test piece of the heterogeneous material, and carrying out a unidirectional compression or tension experiment on the standard test piece to obtain the elastic modulus E and the Poisson ratio mu of the heterogeneous material.
Before calculating the J-integral of the crack problem in the heterogeneous material, the mechanical parameters of the material need to be obtained. Therefore, in this embodiment, taking a concrete material as an example, a standard compression test piece is prepared according to general concrete mechanical property test method standard (GB/T50081-2002), and the standard compression test piece is unidirectionally compressed, so that the mechanical parameters of the concrete material test piece are: the elastic modulus E is 33.73GPa, and the Poisson ratio mu is 0.2.
(2) Preparing a standard fracture test piece of a heterogeneous material with cracks, and preparing speckles which are black and white and alternate, have the maximum spot size not more than 6 pixels and are uniformly distributed on the surface of a region around the cracks. The area around the crack is an area which takes the tip of the prefabricated crack as the center of a circle and takes 5-7 times of the length of the prefabricated crack as the radius.
FIG. 1 shows the preparation of three-point bend concrete test pieces containing type I pre-cracks. The test piece has a span S of 600mm, a width w of 150mm, a height h of 150mm, and an initial crack height a of 1/3h of 50 mm. Before the three-point bending experiment is carried out, speckles for DIC test need to be manufactured in the area around the crack on the surface of the test piece, and the manufacturing method comprises the following steps: and (3) uniformly coating white putty powder on the area around the crack, and spraying black matte paint after the area is dried to form a layer of uniformly distributed black spots. The speckle size is required to be moderate to ensure the measurement accuracy of DIC, and the speckle obtained by the manufacturing method is shown in figure 2.
(3) And (3) performing a fracture experiment on the test piece, synchronously recording the deformation of the area (speckle) around the crack in the loading process by adopting a CCD (charge coupled device) camera, and obtaining the displacement field U of the area near the tip of the crack under different loads and the size of the crack after the processing by DIC (digital computer) software.
In the process of the three-point bending experiment, a CCD camera of the DIC device is adopted to synchronously acquire displacement information of the concrete surface of the area around the crack in the loading process, and the height of the crack is tracked and determined. The loading speed in this embodiment is 0.005mm/s and the acquisition frequency of the camera is set to 1 Hz. Utilizing DIC system software to process displacement information of a certain moment (a certain picture) collected by a CCD camera so as to obtain a displacement field on the surface of the test area at the moment, wherein the displacement field U in the X directionXAs shown in fig. 3.
(4) Selecting different integration paths, compiling a calculation program according to the obtained elastic modulus E and the displacement field U, dividing subunits in the integration regions, and calculating J-integration values of the subunits on the different paths.
After the displacement field of the concrete in the area around the crack is determined, the J-integral value of each subunit AI in a certain integral path is calculated, and the concrete solving process is as follows:
fig. 4 shows a schematic diagram of a closed-loop integration domain (i.e., an integral peripheral path) and subunits of the crack in this embodiment.
Setting the node coordinate, the node displacement and the q function of a certain subunit as follows:
Figure BDA0002414209340000061
wherein m is the number of nodes in the unit, a triangle unit when m is 3, a quadrangle unit when m is 4, and qmTaking 0 at the outer boundary of the integration path (the envelope), and taking 0 at the inner boundary0Get 1 above.
The coordinate, the displacement and the function q of any point of the subunit are obtained by an interpolation method, and the function q is as follows:
[x y u v q]=N[x y u v q](4)
in the formula, N can be represented as:
N=[N1N2… Nm](1)
Figure BDA0002414209340000071
wherein i is 1,2, …, m, ξiThe coordinates of the form parameter units are ξ and η, and the coordinates a, b and c are coordinate constants.
The derivative is:
Figure BDA0002414209340000072
Figure BDA0002414209340000073
the jacobian matrix is:
Figure BDA0002414209340000074
Figure BDA0002414209340000075
the derivative of the shape function to the coordinates is:
Figure BDA0002414209340000076
according to the displacement field U measured by DIC on the unit node, the strain field can be obtained as follows:
Figure BDA0002414209340000081
Figure BDA0002414209340000082
similarly, the partial derivative of the function q can also be found as:
Figure BDA0002414209340000083
at this time, the stress at the gaussian integration point is:
Figure BDA0002414209340000084
in the formula:
Figure BDA0002414209340000085
the strain energy density can be expressed as:
Figure BDA0002414209340000086
the J-integral within a certain subunit AI can be calculated by:
Figure BDA0002414209340000087
in the formula (I), the compound is shown in the specification,
Figure BDA0002414209340000091
with gaussian integration, the J-integral of the subunit is:
Figure BDA0002414209340000092
wherein GP is the number of Gaussian integration points, ξP、ηPThe coordinates of the gaussian integration points. For a triangle unit, GP is generally taken to be 3; the unit of quadrilateral generally takes GP 4. The coordinate of the two-dimensional Gaussian integral point and the corresponding weight coefficient can be obtained by looking up the weight function table
Figure BDA0002414209340000093
Therefore, the method comprises the following steps:
Figure BDA0002414209340000094
thus, the J-integral over the entire integration domain (the corridor) is:
Figure BDA0002414209340000095
in the formula, n is the number of subunits in the crack periphery annular integral domain (surrounding channel).
(5) Carrying out filtering processing on the calculated J-integral value;
triangular subunits are divided by using a Delaunay triangulation algorithm in Matlab, the triangular subunits are divided into 1165 subunits in an annular integral domain (enclosed road), each subunit contains 3 Gaussian integral points, and the J-integral value J of each subunit can be obtained by using the formulas (3) to (21)AIAs shown in fig. 5.
The crack-neighborhood subunits within the integral domain (the corridors) are shown in fig. 6. Since the DIC method cannot accurately measure the displacement field of subunits near the crack in the integral domain (enclosed channel), the J-integral value J of the subunits needs to be determinededgeAnd deleted. In the present embodiment, the crack vicinity subunit is defined as: the shortest distance from the centroid of the triangular unit to the crack edge was 2 mm. By this definition, the calculated J-integral of 9 subunits is filtered outedgeThe center (○) point in FIG. 5, the filtered J-integral value is denoted as J2The method comprises the following steps:
J2=ΣJedge(23)
for J-integral singular value J3J for each subunit using the 5 σ principle and equation (2)AIWhen the judgment is made, the singularities (points of triangle (△) in fig. 5) appearing in the J-integrated values of 6 subunits are found and filtered out.
After removing the J-integrated values of the 9 subunits near the crack and the J-integrated singular values of the 6 subunits, the J-integrated values (the solid square (■) points in fig. 5) for the remaining 1150 subunits can be calculated using the following formula:
J=J1-J2-∑Jsingular(24)
equation (24) is the J-integral calculation equation in a certain integral path (enclosed road) obtained by the method of the present invention.
And processing the displacement picture acquired by the CCD camera at each moment, and calculating the J-integral value in the integral domain (the enclosed channel) according to the method to obtain a relation graph of the displacement v-J-integral of the loading point of the test piece.
(6) Superposing the J-integral values of the remaining subunits after filtering to obtain the J-integral value on the integral path, and converting the J-integral value into a stress intensity factor K under the same load/displacement;
(7) and (5) repeating the steps (4) to (6), calculating J-integral values under different loads/displacements, and performing filtering treatment to obtain a stress intensity factor K at each loading moment.
In addition, because the number of displacement pictures acquired by the CCD camera is large, it is sometimes difficult to avoid environmental interference during the acquisition process, and therefore, smoothing (filtering) processing needs to be performed on the stress intensity factor K converted in step (6). The specific calculation and processing method is as follows:
from the J-integral value obtained above, the stress intensity factor K of the crack front can be obtained by the following formulaorign
Figure BDA0002414209340000111
In the process of loading the test piece, if the collection frequency of DIC is h Hz, h displacement pictures can be collected every second, and each picture corresponds to 1 stress intensity factor Korign. Invoking smooth filter function of Matlab to obtain stress intensity factor K at all loading momentsorignPerforming smoothing (filtering) treatment, i.e.
K=smooth(Korign,span) (26)
A final stress intensity factor K versus load point displacement v can be obtained as shown in fig. 7.
In the formula (26), span is a filtering window, and is generally 150 to 250, and in this embodiment, is 200.
The method for calculating the stress intensity factor K of the crack problem in the heterogeneous material is described above.
In order to verify the effectiveness of the method of the present invention, the stress intensity factor K obtained from 4 different integration paths (corridors) shown in fig. 8 is compared with the stress intensity factor K calculated by using the linear elastic fracture theory.
According to the theory of linear elastic fracture (stress intensity factor handbook), the theoretical calculation formula of the stress intensity factor K of the three-point bending test piece is as follows:
Figure BDA0002414209340000112
wherein P is load, S is test piece span, h is test piece height, B is test piece thickness, α is crack relative height a/h, a is crack height, β is span-height ratio S/h, and geometric modification factor kβ(α) is:
Figure BDA0002414209340000113
in the three-point bending test, the crack height a at each time was measured by the DIC system, and the theoretical value of the stress intensity factor of the I-type crack in the concrete three-point bending test piece was obtained by using the equations (27) and (28), as shown in fig. 8.
As can be seen from fig. 8, in the initial loading stage, since the load is small, the deformation of the test piece is also small, which results in the test result of the DIC and the calculation result of K having an error; in addition, in the stage of crack destabilization and propagation (the stress intensity factor K is larger than the fracture toughness K of the material)IC1.4 MPam), the crack is rapidly expanded, and the testing precision is difficult to ensure by adopting a DIC method. In addition to the two special stages described above, the mean relative error of the stress intensity factor K calculated by the method of the invention (i.e. the integral peripheral 1) from its theoretical value is about 5% when the crack is steadily propagating. In addition, the fracture toughness K obtained by calculating the integral surrounding road 1-4ICThe relative errors from their experimental values were 3.2%, 4.3%, 3.7% and 3.0%, respectively. This indicates to adoptThe method of the present invention is effective and feasible for calculating the stress intensity factor K of the crack problem in heterogeneous materials, and the characteristics of the J-integral value independent of the integral path are also demonstrated again.
The above embodiments are preferred embodiments of the present invention, but the present invention is not limited to the above embodiments, and any other changes, modifications, substitutions, combinations, and simplifications which do not depart from the spirit and principle of the present invention should be construed as equivalents thereof, and all such changes, modifications, substitutions, combinations, and simplifications are intended to be included in the scope of the present invention.

Claims (9)

1. A heterogeneous material crack stress intensity factor calculation method applying DIC technology is characterized by comprising the following steps:
preparing a standard compression or tension test piece of the heterogeneous material, and performing a unidirectional compression or tension experiment on the standard test piece to obtain the elastic modulus and the Poisson ratio of the heterogeneous material;
preparing a standard fracture test piece of a heterogeneous material with cracks, and preparing speckles with black and white phases and proper sizes on the surface of a region around the cracks;
performing a fracture experiment on the test piece, synchronously recording the deformation of the area around the crack in the loading process by adopting a CCD (charge coupled device) camera, and obtaining the displacement field of the area near the tip of the crack under different loads and the size of the crack after the processing by DIC (digital computer) software;
selecting different integral paths, compiling a calculation program according to the obtained elastic modulus and displacement field, dividing subunits in the integral regions, and calculating J-integral values of the subunits on the different paths;
carrying out filtering processing on the calculated J-integral value;
superposing the J-integral values of the remaining subunits after filtering to obtain the J-integral value on the integral path, and converting the J-integral value into a stress intensity factor K under the same load/displacement;
and repeating the steps of calculating the J-integral values of all the subunits on different paths, filtering the integral values, converting the integral values into stress intensity factors K, calculating the J-integral values under different loads/displacements, and filtering to obtain the stress intensity factors K at all the loading moments.
2. The method of claim 1, wherein the heterogeneous material is concrete, composite, fiber reinforced composite, or rock.
3. The method of claim 1, wherein the standard fracture specimen is a unidirectional tensile center crack specimen, a compact tensile specimen, or a three point bend specimen.
4. The method of claim 1, wherein the sub-cell division method in the integration area is: and dividing the subunits in the integration region in a triangular unit or quadrilateral unit mode according to the principle that the subunits are full, do not overlap and completely cover the whole integration region.
5. The method of claim 1, wherein the J-integral value of the superposed subunits on different paths is calculated by the formula:
Figure FDA0002414209330000021
in the formula, n is the number of subunits divided by the annular integral domain; gp represents the number of Gaussian integration points in each subunit; u. ofiDisplacement field, σ, measured for DIC methodsijFor the stress on each subunit node, i, j is 1, and 2 represents x and y directions respectively; omega is the strain energy density; q. q.s1Take 0 at the outer boundary and 0 at the inner boundary0Taking 1 above;1jis the kronecker tensor; x is the number ofk、ηkThe coordinates of the real parameter unit and the form parameter unit are respectively, and k represents the x direction and the y direction;
Figure FDA0002414209330000022
is the weight coefficient of the gaussian integration point.
6. The method of claim 1, wherein J-integrated values of subunits to be filtered are classified into the following two categories:
j-integrated value J of sub-unit near the removed crackedge
Filtering out J-integral singular value J of subunit satisfying the following formula by applying 3 sigma-5 sigma principle of probability theorysingular
Figure FDA0002414209330000023
In the formula, JAIIs the J-integral value of the subunit; e is JAIThe expected value of (d); d is JAIThe variance of (a); the value of the coefficient n is 3-5.
7. The method of claim 6, wherein the crack-near subunits are subunits having a shortest distance between the centroid and the crack boundary of 1-4 mm.
8. The method according to claim 1, wherein the CCD camera acquires a large number of displacement pictures, which are sometimes inevitably interfered by the environment during the acquisition process, and therefore the stress intensity factor K after conversion needs to be smoothed, and the specific calculation and processing method is as follows:
from the J-integral value obtained, the stress intensity factor K of the crack front can be obtained by the following formulaorign
Figure FDA0002414209330000024
In the process of loading the test piece, if the collection frequency of DIC is h Hz, h displacement pictures can be collected every second, and each picture corresponds to 1 stress intensity factor Korign(ii) a Invoking smooth filter function, and applying stress intensity factor K at all loading momentsorignIs subjected to a smoothing treatment, i.e.
K=smooth(Korign,span)
In the formula, span is a filtering window, and the span is 150-250.
9. The method according to claim 1, wherein the area around the crack is an area which takes the tip of the prefabricated crack as a center of a circle and takes 5-7 times of the length of the prefabricated crack as a radius; the maximum speckle for said speckle is no more than 6 pixels.
CN202010185995.9A 2020-03-17 2020-03-17 Heterogeneous material crack stress intensity factor calculation method applying DIC technology Active CN111398057B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010185995.9A CN111398057B (en) 2020-03-17 2020-03-17 Heterogeneous material crack stress intensity factor calculation method applying DIC technology

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010185995.9A CN111398057B (en) 2020-03-17 2020-03-17 Heterogeneous material crack stress intensity factor calculation method applying DIC technology

Publications (2)

Publication Number Publication Date
CN111398057A true CN111398057A (en) 2020-07-10
CN111398057B CN111398057B (en) 2021-06-08

Family

ID=71430915

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010185995.9A Active CN111398057B (en) 2020-03-17 2020-03-17 Heterogeneous material crack stress intensity factor calculation method applying DIC technology

Country Status (1)

Country Link
CN (1) CN111398057B (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112903442A (en) * 2021-01-26 2021-06-04 北京市理化分析测试中心 Method for testing I-type fracture toughness of bonding interface of composite material bonding structure
CN113008669A (en) * 2021-01-22 2021-06-22 天津大学 Method for dynamically monitoring stress intensity factor of crack tip
CN113029817A (en) * 2021-01-14 2021-06-25 华南理工大学 Unilateral J-integration method for interface cracks
CN113158465A (en) * 2021-04-23 2021-07-23 中国石油大学(华东) Nano SiO based on crack failure mechanism2Nano SiO in modified composite material2Preferred method of content
CN114169209A (en) * 2021-12-24 2022-03-11 哈尔滨工业大学 Numerical method for extracting tip parameters of heterogeneous material mixed type dispersion cracks
CN114818340A (en) * 2022-04-29 2022-07-29 西北核技术研究所 Method for obtaining physical equivalent strength of heterogeneous rock under strong impact load
DE102021124940A1 (en) 2021-09-27 2023-03-30 Technische Universität Bergakademie Freiberg, Körperschaft des öffentlichen Rechts Method for determining the fracture-mechanical stress of at least one crack when a component is loaded, computer program product and device for carrying out the method, and their use
CN116046533A (en) * 2023-01-10 2023-05-02 中国人民解放军陆军工程大学 Crack tip stress intensity factor measuring method based on DIC and stress field reconstruction

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104390860A (en) * 2014-11-27 2015-03-04 西安交通大学 Determination method for failure parameters of materials with complex defects
CN104502198A (en) * 2015-01-05 2015-04-08 大连理工大学 Method for measuring J integration of cracks on basis of digital-image correlation
CN110174315A (en) * 2019-06-05 2019-08-27 南京理工大学 The contactless crack opening displacement measuring device and method of bend fracture test

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104390860A (en) * 2014-11-27 2015-03-04 西安交通大学 Determination method for failure parameters of materials with complex defects
CN104502198A (en) * 2015-01-05 2015-04-08 大连理工大学 Method for measuring J integration of cracks on basis of digital-image correlation
CN110174315A (en) * 2019-06-05 2019-08-27 南京理工大学 The contactless crack opening displacement measuring device and method of bend fracture test

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
蒋玮 等: "基于数字图像相关的积分测量方法", 《机械强度》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113029817A (en) * 2021-01-14 2021-06-25 华南理工大学 Unilateral J-integration method for interface cracks
CN113008669A (en) * 2021-01-22 2021-06-22 天津大学 Method for dynamically monitoring stress intensity factor of crack tip
CN112903442A (en) * 2021-01-26 2021-06-04 北京市理化分析测试中心 Method for testing I-type fracture toughness of bonding interface of composite material bonding structure
CN113158465A (en) * 2021-04-23 2021-07-23 中国石油大学(华东) Nano SiO based on crack failure mechanism2Nano SiO in modified composite material2Preferred method of content
CN113158465B (en) * 2021-04-23 2022-05-27 中国石油大学(华东) Optimal selection method of content of nano SiO2 in nano SiO2 modified composite material based on crack failure mechanism
DE102021124940A1 (en) 2021-09-27 2023-03-30 Technische Universität Bergakademie Freiberg, Körperschaft des öffentlichen Rechts Method for determining the fracture-mechanical stress of at least one crack when a component is loaded, computer program product and device for carrying out the method, and their use
WO2023046751A1 (en) 2021-09-27 2023-03-30 Technische Universität Bergakademie Freiberg Method for determining the fracture mechanical load of at least one crack when a component is loaded, computer program product and device for carrying out the method, and use thereof
CN114169209A (en) * 2021-12-24 2022-03-11 哈尔滨工业大学 Numerical method for extracting tip parameters of heterogeneous material mixed type dispersion cracks
CN114818340A (en) * 2022-04-29 2022-07-29 西北核技术研究所 Method for obtaining physical equivalent strength of heterogeneous rock under strong impact load
CN116046533A (en) * 2023-01-10 2023-05-02 中国人民解放军陆军工程大学 Crack tip stress intensity factor measuring method based on DIC and stress field reconstruction
CN116046533B (en) * 2023-01-10 2023-09-22 中国人民解放军陆军工程大学 Crack tip stress intensity factor measuring method based on DIC and stress field reconstruction

Also Published As

Publication number Publication date
CN111398057B (en) 2021-06-08

Similar Documents

Publication Publication Date Title
CN111398057B (en) Heterogeneous material crack stress intensity factor calculation method applying DIC technology
Sutton et al. Advances in two-dimensional and three-dimensional computer vision
Turkan et al. Tracking of secondary and temporary objects in structural concrete work
Armesto et al. FEM modeling of structures based on close range digital photogrammetry
CN109099852B (en) Structural fault detection method and system for measuring relative deformation of wind turbine blade
Yang et al. Deformation behavior analysis of composite structures under monotonic loads based on terrestrial laser scanning technology
CN103926025B (en) A kind of test unit for measuring coating unrelieved stress and method
CN104325462B (en) The method in robot motion space is built under a kind of inherent constraint
Poozesh et al. A multi-camera stereo DIC system for extracting operating mode shapes of large scale structures
CN113870366B (en) Calibration method and calibration system of three-dimensional scanning system based on pose sensor
CN108824816A (en) A kind of big inter-network frame sliding location and installation in high-altitude and monitoring method
CN112785654A (en) Calibration method and device for track geometry detection system
CN114970240A (en) Method and equipment for rapidly evaluating load state of multi-phase composite structure image
Cabaleiro et al. A case study of measurements of deformations due to different loads in pieces less than 1 m from lidar data
CN107014313A (en) The method and system of weighted least-squares phase unwrapping based on S-transformation ridge value
CN104897065A (en) Measurement system for surface displacement field of shell structure
JP2022545247A (en) Imposing quality requirements on 3D models with support structures
JP5795095B2 (en) Phase analysis method of lattice image using weighting
Chen et al. Applications of digital correlation method to structure inspection
CN113899746B (en) DIC-based steel structure fatigue crack growth morphology measurement method
JP4877105B2 (en) Vehicle 3D shape model data creation method
Colabella et al. A monitoring system for wooden post-formed gridshells
Toyoshi Residual displacement and residual strain measurement for steel frame under seismic load by integrated dot centroid tracking method
CN111912356A (en) Method and device for measuring three-dimensional surface shape of object based on L-K local optical flow
Zhang et al. Digital photogrammetry applying to reverse engineering

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