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Chapter 4 Macromechanical Analysis of a Laminate Laminate Analysis: Example Dr. Autar Kaw Department of Mechanical Engineering University of South Florida, Tampa, FL 33620 Courtesy of the Textbook Mechanics of Composite Materials by Kaw
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  • Chapter 4 Macromechanical Analysis of a Laminate Laminate Analysis: Example

    Dr. Autar Kaw

    Department of Mechanical Engineering University of South Florida, Tampa, FL 33620

    Courtesy of the Textbook

    Mechanics of Composite Materials by Kaw

    http://autarkaw.com/books/composite/index.htmlhttp://autarkaw.com/books/composite/index.htmlhttp://autarkaw.com/books/composite/index.html

  • Fiber Direction

    θ

    x

    z

    y

  • A [0/30/-45] Graphite/Epoxy laminate is subjected to a load of Nx = Ny = 1000 N/m. Use the unidirectional properties from Table 2.1 of Graphite/Epoxy. Assume each lamina has a thickness of 5 mm. Find

    a) the three stiffness matrices [A], [B] and [D] for a three ply [0/30/-45] Graphite/Epoxy laminate.

    b) mid-plane strains and curvatures. c) global and local stresses on top

    surface of 300 ply. d) percentage of load Nx taken by

    each ply.

    0o

    30o

    -45o

    5mm

    5mm

    5mm

    z = -2.5mm

    z = 2.5mm

    z = 7.5mm z

    z = -7.5mm

  • A) The reduced stiffness matrix for the Oo Graphite/Epoxy ply is

    0

    Pa)10(

    7.1700

    010.352.897

    02.897181.8

    = [Q] 9

  • Pa)10(

    7.1700

    010.352.897

    02.897181.8

    = ]Q[ 90

    Pa)10(

    36.7420.0554.19

    20.0523.6532.46

    54.1932.46109.4

    = ]Q[ 930

    Pa)10(

    46.5942.87-42.87-

    42.87-56.6642.32

    42.87-42.3256.66

    = ]Q[ 945-

    Qbar Matrices for Laminas

  • The total thickness of the laminate is h = (0.005)(3) = 0.015 m. h0=-0.0075 m h1=-0.0025 m h2=0.0025 m h3=0.0075 m

    0o

    30o

    -45o

    5mm

    5mm

    5mm

    z = -2.5mm

    z = 2.5mm

    z = 7.5mm z

    z = -7.5mm

    Coordinates of top & bottom of plies

  • (-0.0075)]-[(-0.0025) )10(

    7.1700

    010.352.897

    02.897181.8

    = [A] 9

    (-0.0025)]-[0.0025 )10(

    36.7420.0554.19

    20.0523.6532.46

    54.1932.46109.4

    + 9

    0.0025]-[0.0075 )10(

    46.5942.87-42.87-

    42.87-56.6642.32

    42.87-42.3256.66

    + 9

    )h - h( ]Q[ = A 1 -k kkij3

    1 =k ij ∑

    )(][ 13

    1h - h Q = A k - kkij

    k = ij ∑

  • m- Pa)4.525(10)1.141(10)5.663(10)1.141(10)4.533(10)3.884(10

    )5.663(10)3.884(10)1.739(10 = [A]

    887

    888

    789

    −−

  • )h - h( ]Q[ 21 = B 2 1 -k 2kkij

    3

    1 =k ij ∑

    )] )(-0.0075 - )[(-0.0025 )10( 7.17

    00

    010.352.897

    0

    2.897181.2

    21 = [B] 229

    [ ])(-0.0025 - )(0.0025)10( 36.7420.0554.19

    20.0523.6532.46

    54.1932.46109.4

    21 + 229

    ])(0.0025 - )[(0.0075 )10( 46.5942.8742.8742.8756.6642.3242.8742.3256.66

    21 + 229

    −−−−

  • ( ) ( ) ( )( ) ( ) ( )( ) ( ) ( )

    2

    566

    665

    656

    108559100721100721100721101581108559100721108559101293

    m Pa.........

    [B] = −

    −−−−−

  • )h - h( ]Q[ 31 = D 3 1 -k 3kkij

    3

    1 =k ij ∑

    [ ]339 )00750()00250()10(17700035108972089728181

    31 . .

    ...

    .. [D] = −−−

    [ ]339 )00250()00250()10(743605201954052065234632195446324109

    31 . .

    ...

    ...

    ... + −−

    [ ]339 )00250)00750()10(594687428742874266563242874232426656

    31 . - (.

    .........

    +

    −−−−

  • ( ) ( ) ( )( ) ( ) ( )( ) ( ) ( )

    3

    333

    333

    334

    m- Pa107.663105.596105.240105.596109.320106.461105.240106.461103.343

    = [D]

    −−−−

  • κ

    κ

    κ

    γ

    ε

    ε

    )(.)(.-)(.-)(.)(.-)(.-

    )(.-)(.)(.)(.-)(.)(.

    )(.-)(.)(.)(.-)(.)(.-

    )(.)(.-)(.-)(.)(.-).

    )(.-)(.)(.)(.-)(.).

    )(.-)(.)(.-)(.)(.).

    =

    xy

    y

    x

    xy

    y

    x

    0

    0

    0

    333566

    333665

    334656

    566887

    665888

    656789

    106637105965102405108559100721100721

    105965103209104616100721101581108559

    102405104616103433100721108559101293

    10855910072110072110525410141110(6635

    10072110158110855910141110533410(8843

    10072110855910129310663510884310(7391

    0

    0

    0

    0

    1000

    1000

    Setting up the 6x6 matrix

  • /m

    .

    .

    .

    m/m

    .

    .

    .

    =

    κ

    κ

    κ

    γ

    ε

    ε

    xy

    y

    x

    xy

    y

    x

    1

    )10(1014

    )10(2853

    )10(9712

    )10(5987

    )10(4923

    )10(1233

    4

    4

    5

    7

    6

    7

    0

    0

    0

  • )(.

    )(.-

    )(.

    ) . + (-

    ) (.-

    ) (.

    ) (.

    =

    γ

    ε

    ε

    -

    -

    -

    -

    -

    -

    xy

    y

    x

    , top 101014

    102853

    109712

    00250

    105987

    104923

    101233

    4

    4

    5

    7

    6

    7

    300

    m/m

    )(.-

    )(.

    )(.

    =

    -

    -

    -

    107851

    103134

    103802

    6

    6

    7

    0o

    30o

    -45o

    5mm

    5mm

    5mm

    z = -2.5mm

    z = 2.5mm

    z = 7.5mm z

    z = -7.5mm

  • γ xy

    Ply # Position εx εy

    1 (00) Top Middle Bottom

    8.944 (10-8) 1.637 (10-7) 2.380 (10-7)

    5.955 (10-6) 5.134 (10-6) 4.313 (10-6)

    -3.836 (10-6) -2.811 (10-6) -1.785 (10-6)

    2 (300) Top Middle Bottom

    2.380 (10-7) 3.123 (10-7) 3.866 (10-7)

    4.313 (10-6) 3.492 (10-6) 2.670 (10-6)

    -1.785 (10-6) -7.598 (10-7) 2.655 (10-7)

    3(-450) Top Middle Bottom

    3.866 (10-7) 4.609 (10-7) 5.352 (10-7)

    2.670 (10-6) 1.849 (10-6) 1.028 (10-6)

    2.655 (10-7) 1.291 (10-6) 2.316 (10-6)

  • )101.785(-

    )104.313(

    )102.380(

    )10(

    36.7420.0554.19

    20.0523.6532.46

    54.1932.46109.4

    =

    τ

    σ

    σ

    6-

    6-

    -7

    9

    xy

    y

    x

    top,300

    Pa

    )103.381(

    )107.391(

    )106.930(

    =

    4

    4

    4

    Global stresses in 30o ply

  • Ply # Position σx σy τxy

    1 (00) Top Middle Bottom

    3.351 (104) 4.464 (104) 5.577 (104)

    6.188 (104) 5.359 (104) 4.531 (104)

    -2.750 (104) -2.015 (104) -1.280 (104)

    2 (300) Top Middle Bottom

    6.930 (104) 1.063 (105) 1.434 (105)

    7.391 (104) 7.747 (104) 8.102 (104)

    3.381 (104) 5.903 (104) 8.426 (104)

    3 (-450) Top Middle Bottom

    1.235 (105) 4.903 (104) -2.547 (104)

    1.563 (105) 6.894 (104) -1.840 (104)

    -1.187 (105) -3.888 (104) 4.091 (104)

  • 2)/ 101.785(-

    )104.313(

    )102.380(

    0.50000.43300.4330-

    0.8660-0.75000.2500

    0.86600.25000.7500

    =

    /2γ

    ε

    ε

    6-

    6-

    -7

    12

    2

    1

    m/m

    .

    .

    .

    =

    γ

    ε

    ε

    -

    -

    -

    )10(6362

    )10(0674

    )10(8374

    6

    6

    7

    12

    2

    1

  • Ply # Position ε1 ε2 γ12

    1 (00) Top Middle Bottom

    8.944 (10-8) 1.637 (10-7) 2.380 (10-7)

    5.955(10-6) 5.134(10-6) 4.313(10-6)

    -3.836(10-6) -2.811(10-6) -1.785(10-6)

    2 (300) Top Middle Bottom

    4.837(10-7) 7.781(10-7) 1.073(10-6)

    4.067(10-6) 3.026(10-6) 1.985(10-6)

    2.636(10-6) 2.374(10-6) 2.111(10-6)

    3 (-450) Top Middle Bottom

    1.396(10-6) 5.096(10-7)

    -3.766(10-7)

    1.661(10-6) 1.800(10-6) 1.940(10-6)

    -2.284(10-6) -1.388(10-6) -4.928(10-7)

  • )103.381(

    )107.391(

    )106.930(

    0.50000.43300.4330-

    .8660-0.75000.2500

    .86600.25000.7500

    =

    τ

    σ

    σ

    4

    4

    4

    12

    2

    1

    Pa

    )101.890(

    )104.348(

    )109.973(

    =

    4

    4

    4

    Local stresses in 30o ply

  • Ply # Position σ1 σ2 τ12

    1 (00) Top Middle Bottom

    3.351 (104) 4.464 (104) 5.577 (104)

    6.188 (104) 5.359(104) 4.531 (104)

    -2.750 (104) -2.015 (104) -1.280 (104)

    2 (300) Top Middle Bottom

    9.973 (104) 1.502 (105) 2.007 (105)

    4.348 (104) 3.356 (104) 2.364 (104)

    1.890 (104) 1.702 (104) 1.513 (104)

    3 (-450) Top Middle Bottom

    2.586 (105) 9.786 (104) -6.285 (104)

    2.123 (104) 2.010 (104) 1.898 (104)

    -1.638 (104) -9.954 (103) -3.533 (103)

  • Portion of load Nx taken by 00 ply = 4.464(104)(5)(10-3) = 223.2 N/m Portion of load Nx taken by 300 ply = 1.063(105)(5)(10-3) = 531.5 N/m Portion of load Nx taken by -450 ply = 4.903(104)(5)(10-3) = 245.2 N/m The sum total of the loads shared by each ply is 1000 N/m, (223.2 + 531.5 +

    245.2) which is the applied load in the x-direction, Nx.

    0o

    30o

    -45o

    5mm

    5mm

    5mm

    z = -2.5mm

    z = 2.5mm

    z = 7.5mm z

    z = -7.5mm

  • Percentage of load Nx taken by 00 ply Percentage of load Nx taken by 300 ply Percentage of load Nx taken by -450 ply

    % 22.32 =

    1001000223.2 ×=

    % 53.15 =

    100 1000531.5 ×=

    % 24.52 =

    100 1000245.2 ×=

  • EML 4230 Introduction to Composite MaterialsLaminate Stacking SequenceProblemSolution ������ ����Calculating [A] matrixThe [A] matrixCalculating the [B] MatrixThe [B] MatrixCalculating the [D] matrixThe [D] matrixB) Since the applied load is Nx = Ny = 1000 N/m, the mid-plane strains and curvatures can be found by solving the following set of simultaneous linear equationsMid-plane strains and curvaturesC) The strains and stresses at the top surface of the 300 ply are found as follows. The top surface of the 300 ply is located at z = h1 = -0.0025 m. Global strains (m/m)Slide Number 17Global stresses (Pa)The local strains and local stress as in the 300 ply at the top surface are found using transformation equations asLocal strains (m/m)Slide Number 21Local stresses (Pa)D) Portion of load taken by each plySlide Number 24END


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