Lecture 2a Fracture - Theory

Embed Size (px)

Citation preview

  • 8/12/2019 Lecture 2a Fracture - Theory

    1/23

    Fracture Mechanics - Calculations

    Theory for calculations of severity of crack.

    FEM J integrals for plane problems.

    Special Finite Elements + video of crack process

    FEM J integrals for 3-D problems.

    1

  • 8/12/2019 Lecture 2a Fracture - Theory

    2/23

    Conclusion of continuum exercise

    At sharp edges there is a stress singularity

    The stresses go to infinity

    The strain energy density is limited

    The magnitude of the stress singularity determines the strain energydensity or the stress intensity factor K

    Stress intensity factors should not be confused with stress concentrationfactors.

    2

  • 8/12/2019 Lecture 2a Fracture - Theory

    3/23

    3

    Stress Intensity Factor for a small crack with a length of a:

  • 8/12/2019 Lecture 2a Fracture - Theory

    4/23

    The crack singularity - polar coordinates

    Stress state around crack (Continuum Mechanics)

    4

  • 8/12/2019 Lecture 2a Fracture - Theory

    5/23

    Mode I - Opening mode

    Stresses depend on inverse of squareroot of r - singularitySingularity dominates at the crack tip - C11 depends on external load

    Symmetric solution.

    5

  • 8/12/2019 Lecture 2a Fracture - Theory

    6/23

    Mode II - Shearing mode

    Stresses depend on inverse of squareroot of r - singularity

    Singularity dominates at the crack tip - C21 depends on external load

    Antimetric solution.

    6

  • 8/12/2019 Lecture 2a Fracture - Theory

    7/23

    Reformulation of parameters

    The D1 is the case with out-of-plane shear (torsion mode).

    7

  • 8/12/2019 Lecture 2a Fracture - Theory

    8/23

    How to find the singularity?

    Structure with crack is analysed by means of superposition

    8

  • 8/12/2019 Lecture 2a Fracture - Theory

    9/23

    Structure without crack + stresses on crack

    Crack is closed and stresses will be finite.

    The stresses on the crack is easily calculated (FEM hand calculation)

    9

  • 8/12/2019 Lecture 2a Fracture - Theory

    10/23

    Calculation of singularity

    10

  • 8/12/2019 Lecture 2a Fracture - Theory

    11/23

    Singular part - Infinite stresses

    The infinite stress state around the crack can be found by

    Analytically solution for a crack in an infinite plate subjected to

    - 2 opposite point forces (normal or shear direction)

    Integration of analytically solution

    In this way many analytical or semianalytical solutions have been found.

    11

  • 8/12/2019 Lecture 2a Fracture - Theory

    12/23

    J - integral

    The J integral is a very effective way of calculating the energy associatedwith the singularity.

    Numerical stable.

    Independent of material (can be plasticity).

    Easily programmed in a finite element context .

    Basically postprocessing of a Finite Element model with the crackmodelled.

    12

  • 8/12/2019 Lecture 2a Fracture - Theory

    13/23

    Idea of J - integral

    J Integral around a closed curve without singularities can be shown to be 0.

    13

  • 8/12/2019 Lecture 2a Fracture - Theory

    14/23

    Definition of J-integral

    J-integral is a contour integral of the strain energy (w) the stresses timesdisplacement gradients.

    14

  • 8/12/2019 Lecture 2a Fracture - Theory

    15/23

    Reformulation of solution in Cartesian coordinates

    The solution on the boundaries are simple.

    Depends on plane stress and plane strain. (kappa value)

    15

  • 8/12/2019 Lecture 2a Fracture - Theory

    16/23

    Physical interpretation

    Formulate the polar solution from Mode I in cartesian coordinates

    Insert the Mode I solution

    Calculation of strain energy, stresse and displacement gradients are

    relative easy.

    Integration around a contour gives

    16

  • 8/12/2019 Lecture 2a Fracture - Theory

    17/23

  • 8/12/2019 Lecture 2a Fracture - Theory

    18/23

    Crack driving force

    The crack driving force should for stable cracks be less than the materialparameter fracture thoughness

    18

  • 8/12/2019 Lecture 2a Fracture - Theory

    19/23

    J-integral in Ansys Plane Problem

    By Sren Heide Lambertsen, Ph.D. student,Department of Civil Engineering, Aalborg University

    19

  • 8/12/2019 Lecture 2a Fracture - Theory

    20/23

    Special elements - Improved convergence, accuracy

    Isoparametric elements with midside node in the quarter point containstrains with inverse squareroot singularity.

    Should only be used near crack tips.

    20

  • 8/12/2019 Lecture 2a Fracture - Theory

    21/23

    Triangular, isoparametric elements around crack

    Source: Cook et al., Concepts and Applications of Finite Element Analysis,Wiley.

    21

  • 8/12/2019 Lecture 2a Fracture - Theory

    22/23

    3-D effects

    Plane case: Difference between plane stress and plane strain.

    22

  • 8/12/2019 Lecture 2a Fracture - Theory

    23/23

    Video of crack proces in fiberreinforced concrete

    High speed video.

    Pattern recognition to identify different positions.

    Calculation of strains.

    23