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Chap 03 - Mech Properties of Material

Jul 07, 2018

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    Mechanics of Materials ISKMM1113

    MECHANICAL PROPERTIESOF MATERIALS

    Instructor:

    Dr Muhammad Adil Khattak 

    (PhD,ME,MBA,BE)

    017-8272871

    [email protected]

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    hat!s It "#out$

    •  %his lecture is a#out the mechanical&ro&erties of materials

    • 'o( to measure them and use them.

    • It!s im&ortant for any material (hichis )oin) to #e su#*ected tomechanical forces in use.

    •  %hese forces cause the material todeform +i.e. chan)e sha&e, and maycause it to fail +i.e. #rea,.

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    Mechanical ro&erties in/esi)n

    • /esi)ners need to no( a#outmechanical &ro&erties

    • to choose the ri)ht material for a)ien com&onent +e.). a car!scranshaft, or structure +e.). a dam,.

    •  %hey need to mae sure that there(on!t #e too much deection underload and that the forces (on!t #ehi)h enou)h to cause failure.

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    45am&les of 6ailures

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    45am&les of 6ailures

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    /enin) and Measurin) Mechanical

    ro&erties

    •  %here are lots of mechanical&ro&erties in this lecture (e are *ust)oin) to loo at the sim&lest +and

    most im&ortant, ones (hich (e callthe 9static &ro&erties.

    •  %hese can #e measured usin) ery

    sim&le tests conducted on sam&lesof the material.

    •  %he most im&ortant test is the tensile

    test

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    Sim&le %ensile %est

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    Some racticalities

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     %he Stress;Strain

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     %y&ical =esults

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    Stress Strain /ia)ram

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     %y&ical Stress Strain>ehaiour

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    Stress Strain /ia)ram

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     %ensile S&ecimen ? %he

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    6racture 6eatures:

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    Im&ortant Mechanical ro&ertiesfrom a %ensile %est

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     %erminolo)y

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     %he stress;strain cure in more

    detail

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     ield Stren)th

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     %ensile Stren)th %S

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    StiAness

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    Bsin) StiAness

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    Bsin) StiAness

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     %ou)hness

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     %ou)hness

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    Strain hardenin)

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    Strain 'ardenin) +n K or <alues,

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    /uctility C4D

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    oisson 4Aect

    • hen a material is com&ressed in one direction itusually tends to e5&and in the other t(o directions&er&endicular to the direction of com&ression.

    •  %his &henomenon is called the oisson eAect.

    • oissonEs ratio +nu, is a measure of the oisson eAect.

    •  %he oisson ratio is the ratio of the fraction +or&ercent, of e5&ansion diided #y the fraction +or&ercent, of com&ression for small alues of these

    chan)es.

    long 

    lat vε 

    ε −=

    long 

    lat vε 

    ε −=

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    4n)ineerin) Stress

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    Shear Stress-strain

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    6ailure of Materials due to

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    'i)h %em&erature Material ro#lem

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    hat is

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    F#*ectie:

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    The gradual deterioration of a material that issubjected to time-varying loads.

    FTI!"#

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    Structures subjected to fatigue loading

    Jack-up structure

    Lifter   (photo courtesy

    P.M. Anderson)

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    $. The stresses have been repeated a

    very large number of times

    %. ctual ma&imum stresses were below

    the ultimate strength (even below theyield strength) of the material

    '. egins with a small crac at a point of

    discontinuity in the material.

    *. !ives no warning+ it is sudden and

    fatal.

    6ati)ue

    failure

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    'o( to reco)niHe fati)ue in a

    #roen &iece

    • each mars on the fracture surface &$%

    Indications of loading

    changes

    • /triations

    01 (/how indiv.2ycles)

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    45am&le 1

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    Solution

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    Solution

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    45am&le 2

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    Solution