Lecture 5 Limit of LEFM

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    CEE 770 Meeting 5

    Objectives of This Meeting

    Learn the limit of applicability of LEFM:

    K-dominance

    The process zone, and estimating its size

    Small-scale yielding, SSY

    Dimensional restrictions on process zone size

    The concept of Brittleness Number

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    LEFM predicts infinite stress at the crack front.

    This cannot be true for a real material.

    There must be a region near the crack front where nonlinear materialbehavior prevails. This behavior might be governed by elasto-plastic, or

    microcracking, or any other dissipative mechanisms.This region is called the fracture process zone.

    Process zone formation in Al-Cu-Mg alloy, From Broek,Elementary Engineering Fracture Mechanics, 3d Edit, 1982.

    Example of an elasto-plastic process zone

    Physical Observation

    See Computational Simulation

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    Lets Estimate rp

    First approximation, call it r*p:

    Ignore triaxiality, assume elastic-perfectly plastic behavior,fy = uniaxial yield stress, assume no stress redistribution, then

    *2 p

    Iyy

    r

    Kf

    ==

    x

    KIy

    2 =

    2

    2

    *

    2y

    f

    K

    r

    I

    p

    =

    yield

    x

    y

    x

    KIy

    2 =

    rp

    And an upper bound on r*p

    2

    2

    *

    2y

    f

    K

    rIc

    p=

    (62)Is this an upper or lowerbound to actual value?

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    Better Estimates forrp

    Include 1D stress redistribution:

    **2

    2

    yf

    Kr Icp

    =

    strainplanein32

    2

    y

    Icpf

    Kr

    =

    stressplanein2

    2

    y

    Icp

    f

    Kr

    =

    Include stress redistribution and allow for multiaxiality with the von Misesyield criterion:

    Why difference?

    Next, we want rp to be small. Compared to what? How small?

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    Small Compared to What? How Small?

    ForK, a linear-elastic concept, to dominate the solution, the

    process zone must be small compared to all significant dimensionsof the structure containing the crack.

    By convention and by reasonableness, small is accepted to meanless than about 1/25th.

    For example, we would want rp to be less than 1/25th of the crack

    length, a

    2

    2

    2

    5.23

    25

    y

    Ic

    y

    Ic

    f

    Ka

    f

    Ka or

    (63)

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    Necessary Geometrical Conditions for Validity of LEFM in Materials

    in Which Elasto-Plastic Process Zone Behavior Dominates

    W

    2a

    B

    Necessary Conditions:

    2

    ,,

    Y

    I

    fKaWBa c2.5>-

    100

    where

    KIc= Plane Strain Fracture Toughness

    fy= Uniaxial yield strength

    W-a = ligament

    If all these conditions are met, thenSSY conditions are said to prevail

    and LEFM applies.

    W-a

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    Brittleness Numbers

    An important concept that emerges from this simple calculation is that of theBrittleness Number.

    A material in a state with a high brittleness number has a small process zone, eg.

    statematerialplastic-elastofor2

    y

    Icp

    f

    Kr

    so the ratio of yield stress to plane strain fracture toughness, fy/KIc, can beinterpreted as a brittleness number for materials in which the process zone ispredominately dissipating energy in plastic strain energy.

    Similarly, brittleness numbers for materials which dissipate fracture energythrough other mechanisms have been defined, eg.

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