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  • 7/25/2019 Design Course Notes

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    MecE 360: Engineering Design II

    Section 4: Loading & Stress AnalysisDay 2

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    Class Notifications

    Pick up bearing catalogue in machine shop von Mises next day with failure discussion

    Office Hours: Extended 5:00 to 6:00 meeting

    times for Feb meetings May change further depending on sign-up

    trends

    Project: How to convey information on design

    1 page template with key information?

    Currently have final report posted for one, in

    process of getting reports from Chen

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    Objectives

    1. Stress concentration for fatigue2. Deflections and slopes for loaded beams

    Many long examples

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    SCF for Cyclic Loading (p.4-25)

    Brittle materials are more susceptible to stress

    concentration (SC) than ductile materials

    Ductile materials deform if local equivalent stresses

    exceed yield strength

    Brittle materials fail if stress reaches Sut(no yield)

    Components under cyclic loading often fail

    in a brittle manner

    Ductile materials that plastically deform are work

    hardened and become brittle

    Cracks propagate with each cycle in a brittle material

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    SCF for Cyclic Loading

    Fatigue SCF (Kf) Static (theoretical) SCF (Kt)

    If the material being cycled is rittle

    Kf=Kt and Kfs =Kts(tensile) (shear)

    Brittle materials are more sensitive to

    notches and stress concentrations

    Need to define a characteristic that relates the

    level of sensitivity to change in geometry and SCF for

    cyclic loading

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    Notch sensitivity q and qs provide relationship between

    fatigue SCF and theoretical SCF

    For very brittle materials q = 1 and qs = 1

    1

    1

    t

    f

    K

    K

    q 1

    1

    ts

    fs

    s K

    K

    q

    SCF for Cyclic Loading

    Known/given/from last day Known/given

    unknown unknown

    MaterialProperty, in

    charts/graphs

    MaterialProperty, in

    charts/graphs

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    Graphically find q or qs based on Sutand notch radius

    For qs , add 20 kpsi to Sut, then find q

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 0.05 0.1 0.15 0.2notch radius, r (in)

    q

    240/1656

    200/1379

    160/1103

    140/965

    120/827

    100/689

    80/552

    70/483

    60/41450/345

    Dd

    M Mr

    TT

    SCF for Cyclic Loading

    Sut[kpsi/MPa]

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    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 0.05 0.1 0.15 0.2

    notch radius, r (in)

    q

    240/1656

    200/1379

    160/1103

    140/965

    120/827

    100/689

    80/552

    70/483

    60/414

    50/345

    Example: Sut = 120 kpsi, r= 0.1 in

    q 0.86

    SCF for Cyclic Loading

    Sut[kpsi/MPa]

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    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 0.05 0.1 0.15 0.2

    notch radius, r (in)

    q

    240/1656

    200/1379

    160/1103

    140/965

    120/827

    100/689

    80/552

    70/483

    60/414

    50/345

    SCF for Cyclic Loading

    Sut[kpsi/MPa]

    Example: Sut = 120 kpsi, r= 0.1 in

    For qs use

    Sut+ 20 kpsi

    = 140 kpsi

    qs 0.89

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    nafa K

    1

    1

    t

    f

    K

    Kq

    SCF for Cyclic Loading

    For alternating stress

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 0.05 0.1 0.15 0.2notch radius, r (in)

    q

    240/1656

    200/1379

    160/1103

    140/965

    120/827

    100/689

    80/552

    70/483

    60/414

    50/345

    Shaft with groove in bending

    1

    2

    3

    4

    5

    0 0.1 0.2 0.3

    r/d

    Kt

    D/d= D/d=2 D/d=1.5 D/d=1.3

    D/d=1.15 D/d=1.1 D/d=1.05 D/d=1.01

    DdM M

    r

    Nominal stress

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    For mean stressnmfmm

    K

    Approach to solve for Kfm:

    SCF for Cyclic Loading

    Nominal stress

    If ynf SK max then: ffm KK

    If yf SK n max then:

    n

    n

    m

    afy

    fm

    KSK

    Ifyf

    SKnn

    2minmax then: 0

    fmK

    Most common case

    Ductile to brittle

    transition at notch

    Compression and tension;

    yielding occurs;

    mean stress has little effect

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    Example 4-3 (p.4-30)

    Dd

    MM

    r

    TT

    The 50 mm diameter shaft shown has fully reversed

    bending (100 Nm) and fluctuating torsion (50 25 Nm).

    The small diameter is dis 40 mm and the radius of

    curvature of the groove is 5 mm. The shaft is made of

    AISI 1018 cold-drawn steel with Sut= 440 MPa, Sy = 370MPa.

    Calculate mean and alternating bending and torsional

    stresses

    Given: The theoretical tensile and shear SCF are 1.75and 1.5, respectively.

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    Solution

    from last day.

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    Solution

    Sut[kpsi/MPa]

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    Solution

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    Solution Contd

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    Solution Final

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    Shaft Deflection ( p.4-32)

    Besides strength considerations, it is usually

    also important to examine component deflection

    We will investigate shaft deflections

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    Shaft Deflection

    Note that a shaft is usually stepped to

    accommodate gears and bearing.

    It is necessary to account for changes in loading

    and geometry along the length of the shaft.

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    21

    0 00

    1

    00

    2

    2

    2

    2 1

    CxCdxEI

    Mdx

    dx

    dyy

    CdxEI

    Mdx

    dx

    yd

    dx

    dy

    EI

    M

    dx

    yd

    x xx

    xx

    :deflection

    :slope

    :curvatureofradius

    where

    dxVM

    dxqV

    :moment

    :shear

    Shaft Deflection

    Need to solve deflection equations (see CivE 270)

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    Some functions to

    integrate/differentiate

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    Use of singularity functions, which are on/off

    type equations (brackets: < >)

    Value of a singularity function

    Integration:

    a-xa,xif

    0x,aif

    ax

    axax

    1nif1

    0nif

    1

    1

    n

    n

    n

    n

    ax

    ax

    ax

    If n < 0, then x - an = 0

    Shaft Deflection

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    Singularity functions are applied to the different

    shaft loads when defining shear flow equation

    Distributed load (w), shear flow (q), [N/m]

    Force (F), shear (V), [N]

    Couple/moment (M), [Nm]

    a is the position where the loading appears on the shaft

    2

    ax

    0

    ax 1

    ax

    Shaft Deflections

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    Left reaction (RL

    ) @ a = 0m

    R1 @ a = 0.025m

    M@ a = 0.025m

    R2 @ a = 0.075m

    Right reaction (RR) @ a = 0.1m

    Shaft Deflection

    10

    x

    1025.0 x

    2025.0

    x

    1075.0

    x

    11.0

    x

    R1

    =100N

    x

    R2=75N

    y

    z

    R11

    2

    R2

    100mm

    75mm

    25mm

    M=10Nm

    RL

    RR

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    Shaft Deflection

    11

    2

    21

    1

    1

    1.0075.0

    025.0025.0)(

    xRxR

    xMxRxRxq

    R

    L

    Integrate shear flow q twice with respect to xto find M(x).

    Use M(x) to find slope (x) and deflection y(x).

    R1

    =100N

    x

    R2=75N

    100mm

    75mm

    25mm

    M=10Nm

    RL

    RR

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    22 ABtotalABtotal zytotal

    22

    zy ABtotalABtotal

    Shaft Deflection

    y-deflection z-deflection

    Resultant deflection from all forces at critical

    position

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    Example 4-4

    Find the equations for deflection and slope at any point on the

    beam.

    Example in notes package

    E l P bl Si l it

    http://localhost/var/www/apps/conversion/tmp/MecE360_Fall2010/Resources/Section%201%20example.jnthttp://localhost/var/www/apps/conversion/tmp/MecE360_Fall2010/Resources/Section%201%20example.jnt
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    Example Problem- Singularity

    Functions

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    Solution

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    Solution

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    Example Problem

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    Solution

    45.469 N

    R2y=- R1y +P1y+ q (0.025)

    =- 45.469+50 +50 N/m (0.025m)

    R2y= 5.78125

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    Solution

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    Soln contd- x-y plane

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    Solution- Slope and Deflection

    Solution Solve Constants with

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    Solution- Solve Constants with

    Boundary Conditions

    - 0.014909

    Solution Slopes and

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    Solution- Slopes and

    Deflections in x-y plane

    C1/EI

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    x-z plane- Fast Forward

    Slope and Deflection Fast

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    Slope and Deflection-Fast

    Forward

    Solving Boundary Conditions

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    Solving Boundary Conditions-

    Fast Forward

    Boundary Conditions Fast

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    Boundary Conditions- Fast

    Forward

    Slopes and Deflections Fast

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    Slopes and Deflections- Fast

    Forward

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    Total Deflection and Slope

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    Whats next

    Section 5: Material Failure

    von Mises equivalent stress

    Design criteria

    Failure modes

    Influential factors