89589540-Strength-of-Materials-by-S-K-Mondal-14.pdf

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    14. Strain Energy Method

    Theory at a Glance (for IES, GATE, PSU)1. Resilience (U) Resilience is an ability of a material to absorb energy when

    elastically deformed and to return it when unloaded.

    The strain energy stored in a specimen when stained within

    the elastic limit is known as resilience.

    2

    U = U =2 2

    2

    E V o lu m e o r V o lu m e

    E

    2. Proof Resilience Maximum strain energy stored at elastic limit. i.e. the strain energy stored in the body upto

    elastic limit.

    This is the property of the material that enables it to resist shock and impact by storing

    energy. The measure of proof resilience is the strain energy absorbed per unit volume.

    3. Modulus of Resilience (u)The proof resilience per unit volume is known as modulus of resilience. If is the stress due to

    gradually applied load, then

    2

    u = u =2 2

    2 E o r

    E

    4. Application

    2 22

    22

    3P .

    4 4= 2 2 (2 ) 2.4 4

    L L P

    P LU d AE d E E

    = +

    Strain energy becomes smaller & smaller as the cross sectional area of bar

    is increased over more & more of its length i.e. A , U

    5. Toughness This is the property which enables a material to be twisted, bent or stretched under impact

    load or high stress before rupture. It may be considered to be the ability of the material to

    LL/4

    2d

    P

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    hapter-14abso

    abso

    Toug

    The

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    Thestruc

    odulus of

    The

    to ab

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    that

    with

    Thediag

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    . Strain

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    Tota

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    bed after b

    hness is an

    bility to wi

    hness = str

    materialstures that

    Toughne

    ability of u

    sorb energy

    amount of

    the mat

    ut failure.

    rea under

    am is calle

    h is a meas

    bsorbed b

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    ures.

    nergy in

    2

    nergy per

    or,

    2=

    G

    Strain Ene

    12

    =

    s

    s

    U

    U

    or =sU

    s

    , sid shaft U

    ,llowshaft

    n the plas

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    ability to a

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    work per

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    modulus o

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    the unit

    mpact load

    shear a

    2

    s

    nit volume

    u2 = G

    rgy (U) for

    2

    12

    T

    T Lor

    GJ

    2max

    2

    22

    LG r

    2max

    4 =

    G

    2max

    4sU

    G=

    Strain Eic zone. T

    d upto the p

    sorb energ

    sional stre

    ility

    modulused to sudde

    of material

    ic range.

    nit volume

    withstand

    tress strain

    f toughness ,

    gy that can

    volume of

    ng before it

    d torsio

    s, (u )

    Shaft in T

    21 GJ2

    L

    2 d

    2 L

    ( 4 42

    D d

    D

    ergy Mete measure

    oint of frac

    in the plas

    ses above t

    of toughnen and impa

    orsion

    ) 2max4

    L

    G=

    od of toughn

    ure.

    tic range.

    he yield str

    ss are uset loads.

    U

    ( )2 22

    D d

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    +

    O

    T

    ss is the

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    d to make

    = u f

    Volume

    A

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    fracture.

    componen

    ndalsenergy

    ts and

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    Chapter

    7. Strai

    A

    S

    o r

    C

    I

    8. Cast

    14

    s = L

    hin walle

    here

    Conical sp

    Cantilever

    Helical sp

    n energy

    ngle subten

    rain energ

    =

    =

    0

    U2

    2

    L

    b

    b

    M

    E I

    ases

    o Canti

    o Simpl

    portant

    o For p

    o For n

    gliones= n

    n

    U P

    ,

    ngth of me

    stube U

    S, U

    =ring

    eam with l

    , =sing U

    in bendi

    ed by arc,

    stored in b

    2

    22

    2

    .x d xI

    d yd x

    lever beam

    y supporte

    ote

    re bending

    M is cons

    MLEI

    =

    =2

    2

    M LU

    EI

    n-uniform

    Strain en

    Strain en

    theorem

    Strai2

    4an centre li

    sLt G

    2 2

    0

    2

    P=

    2GJ

    n

    GJ d dx

    R

    oad 'p' at e

    2 3 P R nGJ

    ng.

    .= x M d EI eam.

    d x

    with a end l

    with a loa

    tant along t

    if Misknow

    bending

    ergy in she

    ergy in ben

    Energy M

    e

    2

    2

    ( var

    = GJ dx

    d R

    s

    3d, U

    5

    =

    ( 2= L

    2

    2

    d yd x

    oad P , bU

    P at centr

    he length L

    =2

    n2

    EIif

    L

    r is neglect

    ing is only

    ethod

    2

    0

    .

    ies with

    n PR R

    GJ

    2

    P LbhG

    ) Rn

    =

    ME I

    2 3

    6= P L

    EI

    ,2

    96=

    b

    PU

    curvature

    ed

    considered.

    . ( =d R

    3

    I

    / isknowL

    S K

    )adius

    n

    Mondals

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    Chapter-14 Strain Energy Method S K Mondals1 =

    x x

    M U M dx

    p EI p

    Note:

    o Strain energy, stored due to direct stress in 3 coordinates

    21 ( ) 2 2

    = x x y

    U E

    o = =If ,in case of equal stress in 3 direction thenx y z

    2 23 U= [1 2 ] (volume strain energy)

    2 2E k =

    Page 390 of 429