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M1-6 Creep

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    MODULE 1 : ENGINEERING MECHANICS 6 hrs

    Statically determinate and indeterminate systems.Stress- strain relations.

    Variation of Stress and Strain.

    .

    Stress Concentration.

    Creep and Viscoelasticity.

    PP Benham, RJ Crawford, CG Armstrong, Mechanics of

    Engineering Materials, 2nd

    8/10/2011 Module 1

    pages 573-597 of the above book

    sections 21.1-14

    Originated from: A/P SHU DongWei

    6. Creep and Viscoelasticity

    ,

    turbines, nuclear processes, etc

    Creep = strain increases at constant stress.

    Thermoplastics susceptible at room

    .

    Part 1: Metals

    Part 2: Plastics

    Creep of metals0.3Tm, and 0.5Tm

    constant stress /load

    constant temperature

    Andrade 1910; test on lead at room temp

    long duration:4 stages

    initial elastic

    primary

    secondary (const

    ra e

    tertiary to fracture

    Empirical creep strain: general

    =f . f t . f T

    f1() = A1 ; A2 sinh(/0) ; A3 exp(/0)

    f2(t) = t1/3

    + t + t3

    f3(T) = exp(H/(RT))

    R universial gas constant

    T absolute temperature

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    Empirical Creep strain: Linear

    = + n

    Secondary creep strain

    Eqn 21.6

    0.5% strain at 100,000 hrsextrapolation

    Test results for

    different

    temperatures

    Temperature

    Plotted from previous graph and then

    extrapolate to 100,000

    21.3 Creep-Rupture test

    Used for selection of material for long term test

    Determine the rupture strength

    Applied varying stress sufficient to cause rupture, successive tests

    at constant T

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    21.5 Creep during beam bending

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    Creep under multi-axial stresses

    of the

    &

    are

    in

    Creep under multi-axial stresses

    Creep under multi-axial stresses

    E21.1

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    5

    4

    23

    4

    503

    Where th=time in hours

    Sub the design values:

    4.

    2. xpxxx

    p4=794.4x108

    p=530N/m2

    Time-dependent increase in strain at constant stress

    21.7 stress relaxation: thermal(Time-dependent decrease in stress at constant strain)

    tightening stress in

    bolts:

    Loosening of bolts

    in tension

    stress relaxation

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    21.8 stress relaxation in a bolt

    relaxation: variable stress/temp

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    Time-hardening hyp

    Creep rate = f(stress, t)

    Strain hardening hyp

    Strain rate = f(stress,p.strain)

    Creep and fatigue Creep and fatigue, Sa-Sm diagram(0.26% carbon steel at 400degc 100

    Points along

    x-axis=> creep.

    Points along

    y-axis=>

    Fati ue

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    21.11:Plastics material: viscoelasticity

    tf.viscoelasticity

    tf ,

    time-dependent

    strain, i.e. relaxation.

    When applied stress

    is remove, strain

    recovery over period

    of time.Can happen at

    ambient temp.

    Creep and recovery: Plastic material

    Creep curves/isometri/isochro Creep modulus

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    Creep modulus/temperature

    Effect of temp on the creep

    rate of plastic materials.

    T=(-30deg c) to (+40deg c)

    Creep/stress levels

    Designing for creep in

    plastic: Most acceptable

    approac pseu o-e as c

    design method.

    Use of published

    experimental creep data for

    the material

    Fig 21.18: Creep curves for

    acetal at 20deg C

    Creep/stress levelsfrom previous curves

    A solid circular acetal rod,

    0.15m long, clamped at one

    end and the other free end is

    25N. Determine a suitable

    diameter for the rod for a

    limiting strain of 2% in 1 year.What would be the max.

    deflection at this time.

    1 year Isochronous curve:

    allowable stress of 17.1MN/m2 is

    obtained at 2% strain limit.

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