study of time dependence

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    Presented By:

    Swati Sharma

    TIME DEPENDENT PROPERTIES

    OF FIBRES

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    Time dependent properties study of different

    properties of the fibres with respect to the time.

    Time dependent study is important because it

    provides means of predicting behavior in real

    situation.

    INTRODUCTION

    2

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    Creep: long times, from 1 minute to 1 month.

    Stress relaxation: medium to long times, from 1 second

    to 1 hour.

    Stressstrain curves, including impact methods: short to

    medium times, from 1/100 second to 10 minutes.

    Dynamic testing: short times, from 0.1 millisecond to 1

    second.

    METHODS USED AT DIFFERENT TIME

    SCALES ARE AS FOLLOW

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    Creep is time dependent deformation under constant load

    for a long time.

    The total extension under applied load may therefore bedivided into three parts:

    Immediate elastic deformation , which is instantaneous and

    recoverable (a-b and d-e).

    Primary creep, which is recoverable in time (e-f) . The secodary creep, which is non-recoverable(g-h) .

    CREEP

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    CREEP UNDER CONSTANT LOAD AND

    RECOVERY UNDER ZERO LOAD

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    PRIMARY AND SECONDARY CREEP

    OF VISCOSE RAYON AT 60% R.H

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    The creep of viscose rayon at various loads shows a

    certain regularity when the elongation divided by the

    stress was plotted against the time

    The creep curves obtained at various loads and can be

    fitted to a single master curve by vertical and lateral

    shift and by multiplying the elongation scale by an

    appropriate factor

    GENERALIZED CREEP CURVES

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    GENERALISED CREEP CURVES FOR

    VISCOSE RAYON AT 6% R.H .

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    Humidity:

    Creep increases with the humidity. The change is small

    below 40% r.h. but considerable at higher humidity.

    Temperature:

    Creep of fibre increases as the temperature increased

    INFLUENCE OF VARIOUS FACTORS ON

    CREEP

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    Progressive loss of stress

    (load) over time under

    constant strain(deformation)

    is known as stress

    relaxation.

    Both linear elastic and

    viscous fluid behaviors are

    present.

    The material does notcompletely recover. There

    is both elasticity and

    plasticity

    STRESS RELAXATION

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    Stressstrain tests take some time, and consequentlythere is an opportunity for creep to occur.

    The slower the test, the more time there is available,

    and thus the greater the extension at a given load

    Because of creep, the slower curves are nearer to thestrain axis than the faster curves. There are two reasonsfor this:

    1. Near the end of the test, there has beenmore time for creep

    2. above the yield point the rate of creep isgreater

    STRESSSTRAIN CURVES

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    Stressstrain curves at various rates of

    extension viscose rayon

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    DIFFERENCE BETWEEN CRE AND CRL

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    The stressstrain curves obtained for a fibre thus

    depend on the time taken in the test and on the way in

    which the time is distributed

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    Technique used to s tudy and characterize materials

    One way is to use an impact test. In this method, amoving large mass is engaged with one end of thespecimen, while the other end is held fixed andconnected to a load-measuring device.

    The dynamic tests explained here are of two types

    (1) cyclic loading

    (2) tests in such a short time that the propagation of thestress wave means that the s tress cannot be regarded asconstant along the specimen

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    DYNAMIC TESTING

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    Let at ant time t ,stress is = f and strain = e at time t

    A sinusoidal strain is applied and the stress in the

    material is measured.

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    where em is the strain amplitude, and is the angular frequency in

    radians/second

    where fm is the stress amplitude and is the angular phase

    difference

    http://en.wikipedia.org/wiki/Sinusoidalhttp://en.wikipedia.org/wiki/Sinusoidal
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    Dynamic structures and

    steady-state response:

    (a) imposed sinusoidal

    strain variation;

    (b) stress variation for

    linear viscoelastic material;

    (c) Stressvariation for a non-linear

    material, showing also a

    longer-term trend

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    The subject is complicated by the number of ways inwhich the dynamic behavior can be represented

    1) modulus from ratio of amplitudes = fm/em

    2) phase angle or loss angle =

    3) in-phase modulus (usually termed dynamic modulus)

    4) It is a measure of how well a material can get rid ofenergy and is reported as the tangent of the phase anglealso known as diss ipation factor.

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    Direct observation of stressstrain loop:

    impose cyclic loading or extension and to record the

    stressstrain loop

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    METHODS OF DYNAMIC TESTING

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    Free vibrations :

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    Contd..

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    Forced resonant vibrations:

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    Direct observation Forced resonant vibrations:

    Rheovibron tester

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    Velocity of sound: continuous transmission

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    THANK

    YOU