Beam Deflection Theory

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    r

    y (4)

    Compression

    Tension

    Neutral Axis

    strain

    stressE then

    The force acting on a differential area dA is dA

    y

    r

    E (5)

    from equation (5) ydAr

    EdA

    0

    ydAr

    EdA

    The internal bending moment must be

    equal to the external bending moment,M.

    dAyr

    EdAyM

    2

    dAyI2

    However, Neglecting (-)

    r

    EIM (6)or

    EI

    M

    r

    1

    dA dA The sum () of horizontal

    forces is zero.F

    Fy

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    EI

    M

    dx

    dy

    dx

    yd

    r

    2

    32

    2

    2

    1

    1

    Beam Deflection Equation:

    112

    3

    2

    dx

    dysince is small,

    dx

    dy

    EIM

    dxyd 2

    2

    (7)

    1cMdxdx

    dyEI (8)

    21 cxcMdxEIy (9)

    General Slope Equation

    General Curve Equation

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    y

    F

    L

    Solving Moment,Mat anyx location:

    Moment Diagram

    -FL0

    -FL0

    L

    x

    M

    usingEI

    M

    dx

    yd

    2

    2

    (7)

    xL

    M

    L

    FL

    )( xLFM or

    )(2

    2

    xLFMdx

    ydEI (10)

    1

    2

    2

    Cx

    FFLx

    dx

    dyEI (11)

    21

    32

    62CxC

    xF

    xFLEIy (12)

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    y

    F

    L

    (0,0)

    2

    2x

    FFLxEIdx

    dyEI General Slope Equation

    Also, whenx=0,y=0.

    62

    32x

    Fx

    FLEIy Elastic Curve Equation

    It can be seen that whenx=0, dy/dx==0.

    x

    1

    2

    2

    Cx

    FFLx

    dx

    dyEI (11) Thus, C1=0.

    21

    32

    62CxC

    xF

    xFLEIy (12)Thus, C2=0.

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    )3(662

    232

    xLFxx

    Fx

    FLEIy

    100mm

    F

    700mm

    Case 1

    100mm

    F

    700mm

    or

    ;Lx when

    3

    4109

    700.0

    1.010909.4101053

    m

    mmxPaxF

    Material:

    Diameter= 10mm;Length = 700mmy=100mm

    Implant Grade (ASTM F136 Titanium)Modulus of Elasticity,E= 105GPa

    Moment of Inertia, I

    41044

    10909.464

    )01.0(

    64

    mx

    mDI

    3

    3FLEIy

    kgfNF 60.408.45

    x

    x

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    100mm

    45.08N

    700mm

    x

    y

    )3(6

    2

    xLFx

    EIy

    -120

    -100

    -80

    -60

    -40

    -20

    0

    0 100 200 300 400 500 600 700 800

    x- Location of Fn (mm)

    y-deflection(mm)

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    y

    F

    L

    aCase 2

    C

    y

    F

    L

    (0,0)

    x

    2

    2x

    FFLxEIdx

    dyEI

    2

    2x

    LxFEI

    62

    32x

    Fx

    FLEIy

    xLFx

    EIy 36

    2

    A

    B

    Case 1

    x

    xLFx

    EIy BA 36

    2

    aL

    xaFxEIy BA 36

    2

    when

    ?CBEIy since B-C is still a straight line

    BBC

    2

    2FaEI B aLx CB

    )(23

    23

    aLFaFaxyEIy CBBBCB

    )3(6

    2

    aLFa

    EIy CB

    ax 0

    LxorLa

    aLx

    when ax 3

    3Fa

    EIyB

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    =

    +

    Method of Superposition

    Deflection or Slope(A)

    F1

    F2

    L

    a

    (A)

    F2

    a

    (B)

    F1

    L

    (C)

    Deflection or Slope(B)

    Deflection or Slope(C)

    =

    +

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    0

    5

    10

    15

    20

    25

    0 100 200 300 400 500 600 700 800

    x- Location of Fn (mm)

    y-defle

    ction(mm)

    +F1

    L

    xn

    +F2 +F3 +F4 +F5 +F6 +F7

    -F1 -F2 -F3 -F4 -F5 -F6 -F7

    Case 3

    Force,N -100 -100 50 -300 10 -6 120

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    -0.14

    -0.12

    -0.1

    -0.08

    -0.06

    -0.04

    -0.02

    0

    0.02

    0.04

    0.06

    0.08

    0 100 200 300 400 500 600 700 800

    x- Location of Fn (mm)

    y-deflection(mm)

    +F1

    L

    xn

    +F2 +F3 +F4 +F5 +F6 +F7

    -F1 -F2 -F3 -F4 -F5 -F6 -F7

    Force,N 100 -50 10 0 0.02 0 0.258

    Case 4

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    +F1

    L

    xn

    +F2 +F3 +F4 +F5 +F6 +F7

    -F1 -F2 -F3 -F4 -F5 -F6 -F7

    Force F1=? F2=? F3=? F4=? F5=? F6=? F7=?

    yn mm1 mm2 mm3 mm4 mm5 mm5 mm6

    Numerical Method for Solving Fn(xn, yn)

    xn mm1 mm2 mm3 mm4 mm5 mm5 mm6

    Solve