straight bending beam

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  • 8/10/2019 Straight Bending Beam

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    Bending of straight beams

    In mechanics of materials we cover symmetricalcross sections and bending in one plane. Now

    we will consider the more general case

    Moment perpendicular to a plane at an angle phi

    from x-z plane (plane of loads). Centroidal axes.

    Cantilever beam with an arbitrary cross section subjected to pure bending

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    Shear loading

    We assume for now pure bending with notwist. This implies shear forces passing

    through shear center

    Cantilever beam with an arbitrary cross section subjected to shear loading

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    Symmetrical bending

    Moments of inertia

    Moments of inertia also a tensor so has

    principal axes

    AdxyI

    AdrJ

    AdxI

    AdyI

    xy

    y

    x

    ==

    =

    =

    2

    2

    2

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    Symmetrical and anti-symmetrical

    cross sections

    Are these also principal axes?

    Equilateral triangle Open channel section

    Z- sectionAngle section

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    Symmetrical bending

    Euler-Bernoulli beam theory, Leonhard Euler(1707-1783) and Daniel Bernoulli (1700-1782)

    What are the assumptions?

    For symmetrical cross section

    Neutral axis

    X

    X

    Y

    Yzz

    I

    yM

    I

    xM+=

    0=zz

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    Rectangular cross section

    Maximum bending stress

    2max

    ||6

    bh

    MX

    =

    Cantilever beam with rectangular cross section

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    Unsymmetrical bending

    Equations of equilibrium

    Plane sections remain plane

    Combining it all

    =

    =

    =

    dAxM

    dAyM

    dA

    zzy

    zzx

    zz

    0

    cybxaE

    ycxba

    zz

    zzzz

    zz

    ++=

    =

    ++=

    yIII

    IMIMxIII

    IMIMxyyx

    xyyyx

    xyyx

    xyxxyzz

    ++

    += 22

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    Moments

    Moment is perpendicular to the plane of the

    loads. If the plane of the loads makes an angle with the x-axis,

    cotcot

    cossin

    xy

    x

    y

    yx

    MMM

    M

    MMandMM

    ==

    ==

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    Neutral axis

    For bending stress to be zero

    cot

    cottan

    tan

    tan

    xyy

    xxy

    xyyyx

    xyxyx

    xyyyx

    xyxyx

    zz

    II

    II

    IMIM

    IMIM

    xxIMIMIMIM

    =

    +

    +=

    =

    ++=

    Pure bending of a nonsymmetrically loaded

    cantilever beam

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    Example 7.3 A cantilever beam of length 3m as shown in the figure

    has a channel section. A concentrated load P=12.0 kN

    lies in the plane with an angle =/3 with the x-axis.

    The plane of the loads passes through the shear center

    C. Locate points of maximum tensile and compressive

    stresses and find the magnitude of stresses.

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    Location of max stresses

    460

    462

    10x73.300.82

    010x69.3610000

    :

    mmImmy

    ImmImmA

    propertiesSection

    y

    xyx

    ==

    ===

    rad

    I

    I

    II

    II

    AxisNeutralLocate

    y

    x

    xyy

    xxy

    6407.07457.0tan

    5774.0

    3

    sin

    3cos

    3cot

    3

    cotcot

    cottan

    :

    ==

    =

    =

    =

    =

    =

    mkNMM

    mkNPM

    Moments

    x .18.31sin

    .0.3600.3

    :

    ==

    ==

    Since moment is negative, the part

    above N.A is in tension and the bottom

    part is in compression. Therefore

    maximum tensile stress occurs at

    point A and maximum compressive

    stress at point B.

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    Maximum stresses

    ( )

    ( )( )

    ( )( )

    x

    x

    x

    Stress at A(-70,-118)

    M tan

    tan

    M 118 70 tan133.7MPa

    tan

    Stress at B(70,82)M 82 70 tan

    105.4MPatan

    zz

    x xy

    Ax xy

    B

    x xy

    y x

    I I

    I I

    I I

    =

    = =

    = =

    .

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    Deflections

    Determine separatelyxand y

    components of displacement.

    Here we show ycomponent

    Curvature

    )()tan(

    11

    22

    2

    2

    2

    xyyx

    xyyyx

    xyx

    x

    yy

    zz

    y

    IIIE

    IMIM

    IIE

    M

    dz

    vd

    dz

    vd

    Rwhere

    RR

    +=

    =

    =

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    Total displacement

    cos

    tan

    22 vvu

    vu

    =+=

    =

    Components of deflection of a

    nonsymmetrically loaded beam.

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    Example 7.6

    A simply supported beam of length 3m has a channel section. A

    concentrated load P= 35.0 kN applied at the center of the beam, lies in

    a plane with an angle = 5/9 with the x-axis. Locate points ofmaximum tensile and compressive stresses and magnitude of

    stresses. Find the maximum deflection. E=72 GPa.

    46

    0

    462

    10x73.300.82

    010x69.3610000

    :

    mmImmy

    ImmImmA

    propertiesSection

    y

    xyx

    ==

    ===

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    Solution

    MPaII

    M

    MPaII

    M

    II

    xyM

    xyx

    xB

    xyx

    xA

    xyx

    xzz

    2.87tan

    )tan)70(82(

    8.63tan

    )tan)70(118(

    tan

    )tan(:Stress

    =

    =

    =

    =

    =

    Locate Neutral Axis:

    tan cot 5 9

    tan 0.2277 0.2239

    = =

    = =

    x

    y

    I

    I

    rad

    mmvvu

    mmvu

    mmEI

    PLv

    EI

    x

    95.6cos

    54.1tan

    78.648

    sin48

    PL

    :beamsupportedSimplyDeflection

    22

    3

    3

    ==+=

    ==

    ==

    =

    mkNMM

    mkNPL

    M

    x .85.25sin

    .25.264

    :Moment

    ==

    ==

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    Reading assignment

    Sections 7.3-5: Question: Consider a horizontal cantilever

    beam under a tip vertical load. What condition is required so

    that tip will move both down and sideways?

    Source: www.library.veryhelpful.co.uk/ Page11.htm