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Chap 3 -Stress Mechanical Behavoir 4511

Jul 06, 2018

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    MECHANICAL BEHAVIOR

    OF MATERIALS

     

    strain & Stress

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    Introduction

     The two principal responses ofmaterials to external forces aredeformation and fracture.

      The deformation may beelastic, plastic, or creep (time-dependent plastic deformation).Fracture may occur suddenly orafter repeated application of

    loads (fatigue).

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    Introduction

    Fracture is the breaing of amaterial into two or morepieces. !f fracture occurs before

    much plastic deformationoccurs, we say that thematerial is brittle . !n contrast, ifthere has been extensi"eplastic deformation preceding

    fracture, the material is

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    Introduction

    uctile and Brittle material 

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    Introduction

    Ductile Fracture Brittle Fracture

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    Stress

    !f the state of stress is the

    same e"erywhere in a body

    Stress, #, is defined as theintensity of force at a point$

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    Stress

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    Stress• % normal stress

    (compressi"e or tensile)

    is one in which the forceis normal to the area onwhich it acts.

    # yy  & F y  '%y 

    • % shear stress , theforce is parallel to thearea on which it acts.  # y  

    & F y  '%  is the shearstress caused by a shearforce in the y-directionacting on a plane normal

    to .

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    Stress

    The nine components o stress actin! on anin"nitesimal element# The normal stresscomponents are σxx, σyy, and σzz. The shearstress components are σyz, σzx, σxy, σzy, σxz, and

    σyx.

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    Stress $ transormationo a%es

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    Stress

    rincipal stresses!t is always possible to nd a set of axes (*, +, ) alongwhich theshear stress components "anish. !n this case the normal

    stresses, σ 1, σ 2, and σ 3, are called principal stresses

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    Stress

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    Stress

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    Stress

    • Mohr(s circle, named after

    hristian tto /ohr, is a two-dimensionalgraphical representation of the stress tensor.

    •  The /ohr circle is used to determinegraphically the stress components acting on

    a rotated coordinate system.

    https://en.wikipedia.org/wiki/Christian_Otto_Mohrhttps://en.wikipedia.org/wiki/Circlehttps://en.wikipedia.org/wiki/Circlehttps://en.wikipedia.org/wiki/Christian_Otto_Mohr

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    Stress

    • )ra*in! Mohr(s circle$

    • 0raw the artesian coordinate system (σn , τn)with a horiontal σ-axis and a "ertical τ-axis.

    • 1lot two points %(σx , -τxy)and 2 (σy , +τxy) in the

    space corresponding to the nown stresscomponents on both perpendicular planes.

    • 0raw the diameter of the circle by 3oiningpoints % and 2 with a straight line %2.

    • 0raw the /ohr ircle. The centre of thecircle is the midpoint of the diameter line%2 , which corresponds to the intersection of

    this line with the σn axis.

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    Stress+'lane stress,

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    Stress+'lane stress,

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    rientations

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    Sample problem+'lanestress,

    • body is loaded under stresses #x & 45 /1a,

    #y & *5 /1a, 6 xy & -*4 /pa.

    Find$

    • the three principal stresses.

    • the largest shear stress in the body.

    • rientation of the principal stresses the

    largest shear stress.• Sol"e the problem using setch of /ohr7s

    circle diagram for this stress state.

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    Sample problem+'lanestress,

    • %t a point of interest on the free surfaceof an engineering component, thestresses with respect to a con"enient

    coordinate system in the plane of thesurface are #x & 84, #y & +4, and 6xy &+5/1a. 0etermine the principal normaland shear stresses and their coordinate

    system rotations. %lso determine themaximum normal stress and themaximum shear stress.

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    Solution

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    Sample problem

    -od. is loaded under stresses:

    Find:-the three principalstresses./the lar!est shear stress

    in the -od.#-Orientation of the principal stresses thelargest shear stress.

    -ol!e the pro"lem usings#etch of Mohr0s circle

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    9xercises

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    Strain

    • %n innitesimal normal strain isdened by the change of length, :, ofa line$ 

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    Strain

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    Strain

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    Strain

    •  There are se"eral reasons that true strainsare more con"enient than engineeringstrains.

    *. True strains for e;ui"alent amounts ofdeformation in tension and compressionare e;ual except for sign.

    +. True strains are additi"e. For a

    deformation consisting of se"eral steps,the o"erall strain is the sum of the strainsin each step.

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    Strain

    • Due to a loading, the plate is deformed into the

    dashed shape shown in Figure below. Determine• (a) the average normal strain along the side !,

    • (b) the average shear strain in the plate at relative to

    the x and y axes.

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    Strain

    • Part (a). "ine !, #oin#ident with the y axis,

     be#omes line !$ after deformation, as shown

    in Figure below.%he length of !$ is

    he average normal strain for ! is therefore

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    Strain

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    Strain• Small strains $

    Normal strain+1 ),

    Strain

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    Strain

    • Shear strain+1 ),

    The total engineering shear strain,

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    Strain

    Small strains can -e treated astensors

    St i

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    Strain

    • Mohr0s strain circles