Lecture Module 4 Axial Loads

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    SOLID MECHANICS ISOLID MECHANICS I(BDA 10402)

    Lecture 4: Axial Loads

    Dr. Waluyo Adi SiswantoUniversity Tun Hussein Onn Malaysia

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    Deformation Under Axial Load

    From Hooke's Law

    =E =

    E=

    F

    A E

    Since can be obtain from the elongation

    =

    L =

    F L

    A Ethen

    If the bar is subjected to different axial forces

    =F L

    A E

    Lo

    Ao

    FF

    LA

    FF

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    BDA 10402 Dr. Waluyo Adi Siswanto 3

    Sign Convention

    Sign: tension and elongation

    ! Sign: com"ression and contraction

    AA # $ %

    & 4

    &

    !(

    !)

    *

    )

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    BDA 10402 Dr. Waluyo Adi Siswanto 4

    Strain Relative

    &

    !(

    !)

    A # $ %

    A /B=5 L

    AB

    AAB EB /C=

    3LBC

    ABCEC/D=

    7LCD

    ACDE

    A /C=5 L

    AB

    AAB E

    3LBC

    ABCE

    A /C=A/C

    LAC

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    More on Strain Energy Density

    Strain +nerg, %ensit, is based on the straincalculation

    Strain +nerg, %ensit, relates with the

    corres"onding strains

    +xam"les:A /B=

    5 LAB

    AAB E u A /B=

    1

    2 =

    1

    2

    5

    AAB

    A/ B

    L AB

    =1

    2

    52

    AABE

    In general u i=1

    2

    Fi

    2

    AiE

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    Approximation Approa!

    A1

    A2

    F F

    L1

    L2

    =FL

    1

    A1E

    FL2

    A2E

    A2

    A1

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    Statially Indeterminay

    Structures for which internal forces and reactions cannotbe determined from statics alone are said to be staticall,indeterminate-

    A structure will be staticall, indeterminate whene.er it isheld b, more su""orts than are re/uired to maintain itse/uilibrium-

    0edundant reactions are re"laced with unknown loadswhich along with the other loads must "roduce com"atibledeformations-

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    BDA 10402 Dr. Waluyo Adi Siswanto 8

    "riniple of S#perposition

    L

    R

    =L

    R=0

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    BDA 10402 Dr. Waluyo Adi Siswanto 9

    $!ermal Stress

    A change in tem"erature can cause material to change its dimensions-

    If the tem"erature increases 1 generall, the material ex"ands1 whereas if thetem"erature decreases1 the material will contract-

    T= T L

    T : the algebraic change in length of the member

    : a "ro"ert, of the material1 referred to as the linear coefficient of thermal

    ex"ansion

    23 : the change in tem"erature of the member

    L : the original length of the member

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    Example "ro%lem &'(

    (-4

    m

    (-4m

    3he A!( Steel column 5+67**89a is used tosu""ort the s,mmetric loads from the two floorsof a building-%etermine the loads 9; and 97 if A mo.esdownward ( mm and # mo.es downward 7-7&mm when the loads are a""lied-

    3he column has a cross!sectional area of;4-7& mm7-

    (Hibbeler, 7thd, !roble" #$%&

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    BDA 10402 Dr. Waluyo Adi Siswanto 11

    Example "ro%lem &')

    A reinforced concrete "edestal 5+67&*89aha.ing dimensions and loads as shown in the"icture-

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    Example "ro%lem &'+

    3he two circular rod segments1 one ofaluminum and the other one co""er1 are fixedto the rigid walls such that there is a ga" of *-7mm between them when 3; 6 ;&o$-+ach rod has a diameter of (* mm1@

    Al6 745;*!o$1 +

    al6 )* 89a

    @$