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    Chapter: 9

    Mechanical Properties

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    ISSUES TO ADDRESS...ISSUES TO ADDRESS...ISSUES TO ADDRESS...ISSUES TO ADDRESS... Stress and strain: What are they and why are

    they used instead of load and deformation?

    MECHANICAL PROPERTIES

    Elastic behavior: When loads are small, how muchdeformation occurs? What materials deform least?

    Plastic behavior: At what point do dislocations

    cause permanent deformation? What materials are

    most resistant to permanent deformation?

    Toughness and ductility: What are they and how

    do we measure them?

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    Introduction

    To know the characteristics of material

    To design the member To avoid the failure

    To concern to variety of parties

    To study distributions

    To study the requirement

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    bondsstretch

    return toinitial

    1. Initial 2. Small load 3. UnloadELASTIC DEFORMATION

    F

    Elastic means reversible!

    F

    Linear-

    elasticNon-Linear-elastic

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    1. Initial 2. Small load 3. Unload

    planes

    stillsheared

    bondsstretch

    & planesshear

    PLASTIC DEFORMATION (METALS)

    Plastic means permanent!

    F

    linearelastic

    linearelastic

    plastic

    F

    elastic + plastic plastic

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    Tensile stress, : Shear stress, :

    Area, A

    Ft

    Area, A

    Ft

    Fs

    F

    ENGINEERING STRESS

    Ft =

    FtA

    ooriginal areabefore loading

    FtF

    Fs

    =Fs

    AoStress has units:

    N/m2 or lb/in2

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    Simple tension: cable

    =F

    Ao = cross sectionalArea (when unloaded)

    FF

    COMMON STATES OF STRESS

    o

    Simple shear: drive shaft

    o =

    Fs

    A

    Note: = M/AcR here.

    Ski lift (photo courtesy P.M. Anderson)

    M

    M Ao

    2R

    Fs

    Ac

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    Simple compression:

    Ao

    OTHER COMMON STRESS STATES (1)

    Canyon Bridge, Los Alamos, NM

    Balanced Rock, ArchesNational Park o =

    F

    A

    Note: compressive

    structure member( < 0 here).

    (photo courtesy P.M. Anderson)

    (photo courtesy P.M. Anderson)

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    Bi-axial tension: Hydrostatic compression:

    OTHER COMMON STRESS STATES (2)

    Fish under waterPressurized tank

    z > 0

    > 0

    < 0h

    (photo courtesy

    P.M. Anderson)

    (photo courtesy

    P.M. Anderson)

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    Tensile strain: Lateral strain:

    /2

    /2

    Lowo =

    Lo L =

    L

    wo

    ENGINEERING STRAIN

    Shear strain:/2

    /2

    /2 -

    /2

    LL

    = tan Strain is always

    dimensionless.

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    Typical tensile specimen Typical tensile

    test machineload cell

    extensometerspecimen

    Adapted from Fig. 6.2,

    Callister 6e.

    STRESS-STRAIN TESTING

    Other types of tests:--compression: brittle

    materials (e.g., concrete)

    --torsion: cylindrical tubes,

    shafts.

    gaugelength

    (portion of sample withreduced cross section)

    =

    moving cross head

    Adapted from Fig. 6.3, Callister 6e.

    (Fig. 6.3 is taken from H.W. Hayden,

    W.G. Moffatt, and J. Wulff, The

    Structure and Properties of

    Materials, Vol. III, Mechanical

    Behavior, p. 2, John Wiley and Sons,

    New York, 1965.)

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    Shear test

    Shear and flexural test are performed bythree-point or four point beam

    tested is subjected to a concentrated load

    The experiment may be conducted on UTM

    and Tensometer using suitable attachments,or on a machine specially meant for it.

    M/I=E/R=f/y =VQ/bIzz

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    Torsion tests

    T

    Ability of material to resist twisting

    moment is determine by a torsion test

    G/L=T/J=/r

    = 16T/d3

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    Geometric Considerations of the Stress

    State

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    Geometric Consideration of the Stress

    State

    CED

    2

    2'

    )

    2

    21('

    SinCosSinSin

    BE

    BEBCSinBE

    CosCos

    BE

    BCCosBCBE

    ====

    +===

    AB

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    Modulus of Elasticity, E:(also known as Young's modulus)

    Hooke's Law: = E

    Poisson's ratio, : L

    F

    Linear-elastic

    1

    E

    LINEAR ELASTIC PROPERTIES

    metals: ~ 0.33

    ceramics: ~0.25

    polymers: ~0.40

    = L

    1-

    Fsimpletension

    testUnits:

    E: [GPa] or [psi]

    : dimensionless

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    Non-linear and Interatomic relation ME

    temp

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    Force versus interatomic separation

    Fc or Ft=-F=dP/dr where P= - A/rn+B/rm

    Hence A,B, m and n are constant in whichm>n

    E-dF/dr=d2P/dr2

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    Linear Strain and shear strain

    ,2

    1)

    1(

    2

    1)

    2

    1)(

    2

    1(

    451'1)1(

    =

    =

    AB

    BB

    AB

    BB

    BD

    CosBB

    BD

    BB

    BD

    BDDBd

    B1 B C1C

    q

    B

    ( )

    )1(2

    1

    .221

    +=

    +=

    +=

    ==

    GE

    Eqd

    E

    q

    E

    qd

    Gqd

    AD

    q

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    ANELASTICITY

    Time dependent elastic behavior is knownas anelasticity

    Time dependent microscopic and atomstic

    processes that are attendant to thedeformation

    For metal normally small and is often

    neglected however for some polymericmaterials its magnitude is significant

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    Elastic Shear

    modulus, G:

    1

    G

    = G

    M

    M

    simple

    torsion

    test

    OTHER ELASTIC PROPERTIES

    modulus, K:

    P= -KVVo

    V

    1-K

    Vo

    Special relations for isotropic materials:

    P P

    G =

    E

    2(1+ ) K =

    E

    3(1 2)

    pressure

    test: Init.

    vol =Vo.Vol chg.

    = V

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    Platinum

    Silver, Gold

    Tantalum

    Zinc, Ti

    Steel, Ni

    Molybdenum

    Si crystal

    Si nitrideAl oxide Carbon fibers only

    Aramid fibers only

    80100

    200

    600

    80010001200

    400

    Cu alloys

    Tungsten

    Si carbide

    Diamond

    AFRE fibers *

    CFRE(|| fibers)*

    Metals

    Alloys

    Graphite

    Ceramics

    Semicond

    PolymersComposites

    /fibers

    E(GPa)

    Eceramics

    > Emetals>> Epolymers

    YOUNGS MODULI: COMPARISON

    0.2

    8

    0.6

    1

    Magnesium,

    um num

    Graphite

    -

    Concrete

    PC

    Wood( grain)

    AFRE( fibers)*

    CFRE*

    GFRE*

    Glass fibers only

    Epoxy only

    0.4

    0.8

    2

    4

    6

    10

    20

    40

    60

    Tin

    PTFE

    HDPE

    LDPE

    PP

    Polyester

    PSPET

    CFRE( fibers)*

    GFRE( fibers)*

    GFRE(|| fibers)*

    109 Pa

    ,

    Callister 6e.Composite data based on

    reinforced epoxy with 60 vol%

    of aligned

    carbon (CFRE),

    aramid (AFRE), or

    glass (GFRE)

    fibers.

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    Simple tension:

    = FLoEA

    o

    L

    = FwoEA

    o

    /2

    F

    Ao

    Simple torsion:

    M=moment =angle of twist

    =2MLoro

    4G

    USEFUL LINEAR ELASTIC RELATIONS

    /2

    L/2

    L/2

    Lowo

    2ro

    Lo

    Material, geometric, and loading parameters all

    contribute to deflection.

    Larger elastic moduli minimize elastic deflection.

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    Simple tension test:

    (at lower temperatures, T < Tmelt/3)

    tensile stress,

    Elastic+Plastic

    at larger stress

    PLASTIC (PERMANENT) DEFORMATION

    engineering strain,

    initiallypermanent (plastic)after load is removed

    p

    plastic strain

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    Stress at which noticeableplastic deformation has

    occurred.

    when p = 0.002tensile stress,

    y

    YIELD STRENGTH, y

    engineering strain,

    p = 0.002

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    Graphite/Ceramics/Semicond

    Metals/Alloys

    Composites/fibers

    Polymers

    y(MPa

    )

    cursbeforeyield.

    400

    500600700

    1000

    2000

    Steel (1020)cdSteel (4140)a

    Steel (4140)qt

    Ti (5Al-2.5Sn)aW (pure)

    Mo (pure)Cu (71500)cw

    ,

    composites,si

    nce

    rsbeforeyield.

    y(ceramics)

    >>y(metals)

    >> y(polymers)

    YIELD STRENGTH: COMPARISON

    Yieldstrength,

    PVC

    Hardtomeasu

    re

    sinceintensio

    n,

    fractureusually

    oc

    Nylon 6,6

    LDPE

    70

    20

    40

    60

    50

    100

    10

    30

    200

    Tin (pure)

    Al (6061)a

    Al (6061)ag

    Cu (71500)hrTa (pure)Ti (pure)aSteel (1020)hr

    Hardtomeas

    ur

    inceramicmatrixandepoxyma

    trix

    intension,

    fractureusuallyo

    cc

    HDPEPP

    humid

    dry

    PC

    PET

    oom va ues

    Based on data in Table B4,

    Callister 6e.

    a = annealed

    hr = hot rolled

    ag = aged

    cd = cold drawncw = cold worked

    qt = quenched & tempered

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    Maximum possible engineering stress in tension.

    Adapted from Fig. 6.11,

    Callister 6e.

    TENSILE STRENGTH, TS

    eering

    ess

    TS

    Metals: occurs when noticeable necking starts.

    Ceramics: occurs when crack propagation starts.

    Polymers: occurs when polymer backbones are

    aligned and about to break.

    strain

    engin

    st

    Typical response of a metal

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    Graphite/Ceramics/Semicond

    Metals/Alloys

    Composites/fibers

    Polymers

    TS(MP

    a)

    300

    1000

    Al (6061)ag

    Cu (71500)hr

    Ti (pure)a

    Steel (1020)

    Steel (4140)a

    Steel (4140)qt

    Ti (5Al-2.5Sn)aW (pure)

    Cu (71500)cw

    2000

    3000

    5000

    Al oxide

    Diamond

    Si nitride

    GFRE(|| fiber)CFRE(|| fiber)

    AFRE(|| fiber)

    E-glass fib

    C fibersAramid fib TS(ceram)

    ~TS(met)

    ~ TS(comp)

    >> TS(poly)

    TENSILE STRENGTH: COMPARISON

    Si crystal

    Tensilestrength

    ,

    PVC

    Nylon 6,6

    10

    100 Al (6061)a

    a pure

    LDPE

    PP

    PC PET

    20

    3040

    Graphite

    Concrete

    Glass-soda

    HDPE

    wood( fiber)

    wood(|| fiber)

    1

    GFRE( fiber)CFRE( fiber)AFRE( fiber)

    Based on data in Table B4,

    Callister 6e.

    a = annealed

    hr = hot rolled

    ag = aged

    cd = cold drawn

    cw = cold workedqt = quenched & tempered

    AFRE, GFRE, & CFRE =

    aramid, glass, & carbon

    fiber-reinforced epoxy

    composites, with 60 vol%

    fibers.

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    Plastic tensile strain at failure:

    Engineeringtensilestress,

    smaller %EL

    (brittle if %EL5%)

    Another ductility measure:

    %AR =

    Ao A f

    Aox100

    Note: %AR and %EL are often comparable.--Reason: crystal slip does not change material volume.

    --%AR > %EL possible if internal voids form in neck.

    Adapted from Fig. 6.13,

    Callister 6e.

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    Resilience

    Capacity of material to absorbenergy when it is deformed

    elastically and then, upon

    un oa ng, to ave t s energy

    recovered.

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    Energy to break a unit volume of material

    Approximate by the area under the stress-strain

    curve.

    Engineeringtensile

    smaller toughness (ceramics)

    larger toughness

    TOUGHNESS

    smaller toughness-unreinforcedpolymers

    Engineering tensile strain,

    , ,

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    Resistance to permanently indenting the surface.

    Large hardness means:--resistance to plastic deformation or cracking in

    compression.--better wear properties.

    e.g.,apply known force(1 to 1000g)

    measure sizeof indent after

    HARDNESS

    mm sp ere

    removing load

    dDSmaller indentsmean largerhardness.

    increasing hardness

    mostplastics

    brassesAl alloys

    easy to machinesteels file hard

    cuttingtools

    nitridedsteels diamond

    Adapted from Fig. 6.18, Callister 6e. (Fig. 6.18 is adapted from G.F. Kinney, Engineering Properties

    and Applications of Plastics, p. 202, John Wiley and Sons, 1957.)

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    An increase in y due to plastic deformation.

    large hardening

    small hardening

    ad

    ad

    y0

    y1

    HARDENING

    Curve fit to the stress-strain response:

    u

    nl

    re

    lo

    T = C T( )

    n

    true stress (F/A) true strain: ln(L/Lo)

    hardening exponent:n=0.15 (some steels)to n=0.5 (some copper)

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    Design uncertainties mean we do not push the limit.

    Factor of safety, N

    working=

    y

    N

    Often N is

    between

    1.2 and 4

    Ex: Calculate a diameter, d, to ensure that yield does

    DESIGN OR SAFETY FACTORS

    .

    factor of safety of 5.

    1045 plaincarbon steel:

    y=310MPa

    TS=565MPa

    F = 220,000N

    d

    Loworking =

    y

    N

    220,000N d2/ 4

    5

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    Stress and strain: These are size-independent

    measures of load and displacement, respectively.

    Elastic behavior: This reversible behavior oftenshows a linear relation between stress and strain.

    To minimize deformation, select a material with a

    large elastic modulus (E or G).

    SUMMARY

    Plastic behavior: This permanent deformationbehavior occurs when the tensile (or compressive)

    uniaxial stress reaches y.

    Toughness: The energy needed to break a unit

    volume of material. Ductility: The plastic strain at failure.

    Note: For materials selection cases related to

    mechanical behavior, see slides 22-4 to 22-10.

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    Room T behavior is usually elastic, with brittle failure.

    3-Point Bend Testing often used.--tensile tests are difficult for brittle materials.

    FL/2 L/2

    cross section

    Rd

    Adapted from Fig.

    12.29, Callister 6e.

    MEASURING ELASTIC MODULUS

    9

    deflection

    rect. circ.

    Determine elastic modulus according to:

    E =F

    L3

    4bd3

    =F

    L3

    12R4rect.cross

    section

    circ.cross

    section

    Fx

    linear-elastic behavior

    F

    slope =

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    3-point bend test to measure room T strength.

    FL/2 L/2

    cross section

    Rb

    d

    rect. circ.

    Adapted from Fig.

    12.29, Callister 6e.

    MEASURING STRENGTH

    10

    Flexural strength:

    rect.

    fs = mfail =

    1.5FmaxL

    bd

    2=

    FmaxL

    R

    3

    xF

    Fmax

    max

    Typ. values:Material fs(MPa) E(GPa)

    Si nitride

    Si carbideAl oxide

    glass (soda)

    700-1000

    550-860275-550

    69

    300

    430390

    69Data from Table 12.5, Callister 6e.

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    Elevated Temperature Tensile Test (T > 0.4 Tmelt).

    creep test

    x

    slope = ss = steady-state creep rate.

    MEASURING ELEVATED T RESPONSE

    11

    Generally,

    time

    ssceramics < ss

    metals

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    Ceramic materials have mostly covalent & someionic bonding.

    Structures are based on:

    --charge neutrality--maximizing # of nearest oppositely charged neighbors.

    Structures may be predicted based on:

    SUMMARY

    12

    -- .

    Defects--must preserve charge neutrality

    --have a concentration that varies exponentially w/T.

    Room T mechanical response is elastic, but fracture

    brittle, with negligible ductility. Elevated T creep properties are generally superior to

    those of metals (and polymers).