Failure Criteria for Isotropic Materials(1)

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    Failure criteria for laminated

    composites

    Defining failure is a matter of purpose.

    Failure may be defined as the first event thatdamages the structure or the point of structuralcollapse.

    For composite laminates we distinguish betweenfirst ply failure when the first ply is damagedand ultimate failure when the laminate fails tocarry the load.

    Ultimate failure requires progressive failureanalysis where we reduce the stiffness of failedplies and redistribute the load.

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    Failure criteria for isotropic layers

    Failure is yielding for ductile materials and fracture

    for brittle materials.

    Every direction has same properties so we prefer to

    define the failure based on principal stresses. Why?

    We will deal only with the plane stress condition,

    which will simplify the failure criteria. Then principal

    stresses are

    What about the third principal stress?

    2

    21,2

    2 2x y x y

    xy

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    Maximum normal stress criterion

    For ductile materials strength is same in

    tension and compression so criterion for

    safety is

    However, criterion is rarely suitable for ductile

    materials.

    For brittle materials the ultimate limits are

    different in tension and compression

    1 2,y yS S

    1 2,uc ut S S

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    Maximum strain criterion

    Similar to maximum normal stress criterion

    but applied to strain.

    Applicable to brittle materials so tension and

    compression are different.

    1 2,uc ut

    What is wrong with the figure?

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    Maximum shear stress (Tresca)

    criterion

    Henri Tresca (1814-1885) French ME

    Material yields when maximum shear stress

    reaches the value attained in tensile test.

    Maximum shear stress is one half of the

    difference between the maximum and

    minimum principal stress.

    In simple tensile test it is one half of the

    applied stress. So criterion is

    12 1 2 1 2 or and and

    2

    y

    y y y

    SS S S

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    Distortional Energy (von Mises)

    criterion

    Richard Edler von Mises (1883 Lviv, 1953

    Boston).

    Distortion energy (shape but not volume

    change) controls failure.

    Safe condition

    For plane stress reduces to

    2 2 2 2

    1 2 2 3 3 1

    1 1

    6 3d yU S

    E E

    2 2 2

    1 1 2 2 yS

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    Comparison between criteria

    Largest differences when principal strains have

    opposite signs

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    Maximum difference between Tresca and

    von Mises

    Define stresses as , 2 = , . For what do we get the maximum ratio between the twopredictions of critical value of ? Can assume|| 1. Why?

    1. Positive . Tresca gives = . Von Mises leadsto 2(1 + 2) =

    2. Maximum for =0.5, = 0.75 = 1.155

    2. Negative . Tresca leads to 1 = . Von

    Mises still same equation. Maximum ratio for=-1. = 0.5 , = 3

    Check!