MDB Lecture Simple Strain

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    ** If the unit stress is variale, the unit strain is:

    HOOKES LAW: AXIAL DEFORMATION

    - 0he unit stress is directl1 2ro2ortional to the unit strain u2 to the elasticlimit.

    Solving for then sustituting to

    0herefore, ut

    So, the general formula of deformation is:

    Where:e = is the deformation in mm" = is the a3ial load in 4L = is the original length in mm = is the cross-sectional area in mmE = is the &oung5s 6odulus, or 6odulus of Elasticit1 in 6"a

    7hich isal7a1s constant

    Retri!ti"n in #in$ t%e &"r'#(a "& )e&"r'ati"n:

    Engr. erome !. !amadico "age %of $%ndSemester S.&. %'#(-%'#)

    =

    eL

    =

    dedL

    * =

    e = L

    e=

    8LE

    e=

    "LE

    =8E

    8=

    "

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    #. 0he load must e a3ial.

    %. 0he ar must have a constant cross section and e homogenous.

    (. 0he stress must not e3ceed the 2ro2ortional limit.

    Shearing deformation:- n element su9ect to shear does not change the length of its sides, ut

    undergoes a change in sha2e from a rectangle to 2arallelogram as sho7nin the figure.

    Where: = is the shearing forces = is the shearing area; = modulus of rigidit1

    Engr. erome !. !amadico "age (of $%ndSemester S.&. %'#(-%'#)

    e=

    L

    s;

    Figure 1: ShearDeformation

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    TERMS RELATED TO STRAIN:

    Engr. erome !. !amadico "age )of $%ndSemester S.&. %'#(-%'#)

    Figure 2: Stress-strainDiagram

    Figure 3: Comparative Stress-strain Diagrams fordifferent materials

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    %. n luminum tue is fastened et7een a steel rod and a rone rod as sho7n.3ial loads are a22lied at the 2ositions indicated. !ind the value " that 7ill note3ceed a ma3imum overall deformation of %mm or a stress in the steel of #)'64?m%, in the luminum of D' 64?m%, or in the rone of #%' 64?m%. ssume thatthe asseml1 is suital1 raced to 2revent ucCling and that ES= %'' 3 #'

    (6"a, El= B' 3 #'(6"a, and E/= D( 3 #'

    (6"a.

    (. 0he rigid ars sho7n are se2arated 1 a roller at and 2inned at and F. steelrod at / hel2s su22ort the load of >' C4. om2ute the vertical dis2lacement of theroller at .

    Engr. erome !. !amadico "age @of $%ndSemester S.&. %'#(-%'#)

    /

    (> C4

    F

    #> C4 (' C4 #' C4

    '.D m #.' m '.@ m

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    ). 0he rigid ar /, attached to t7o vertical rods as sho7n is horiontal efore theload " is a22lied. If the load " = >'C4, determine its vertical movement.

    STATICALL INDETERMINATE MEMBERS:

    - If the anal1sis could not e done 1 2lain a22lication of the three La7s ofStatic, the memer is said to e indeterminate.

    - F.= /0 - F1= /0 - M = /

    Engr. erome !. !amadico "age Bof $%ndSemester S.&. %'#(-%'#)

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    MECHANICS OF DEFORMABLE BODIESLecture Notes # 4

    - We need to a22l1 2rinci2le such as DEFORMATIONto determine theother unCno7ns.

    Pra!ti!e Pr"+(e':

    >. horiontal eam hinged at and carries a concentric load " = (' C4 at end F.0he eam is su22orted 1 t7o timer columns of the same material ut of differentcross-section. om2ute the value of the force at su22orts.

    @. s sho7n, a rigid eam 7ith negligile mass is 2inned at one end and su22orted1 t7o rods. 0he eam as initiall1 horiontal efore load " 7as a22lied. !ind thevertical movement of " if " = #%' C4.

    B. homogenous rod of constant cross-section is attached to un1ielding su22orts. Itcarries an a3ial load " as sho7n. om2ute the value of the reactions.

    Engr. erome !. !amadico "age Dof $%ndSemester S.&. %'#(-%'#)

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