ENGR221 Lecture 13

Embed Size (px)

Citation preview

  • 8/4/2019 ENGR221 Lecture 13

    1/33

    Trusses and Machines

    ENGR 221

    February 26, 2003

  • 8/4/2019 ENGR221 Lecture 13

    2/33

    Lecture Goals

    7-2 Plane Trusses

    7-3 Space Trusses

    7-4 Frames and Machines

  • 8/4/2019 ENGR221 Lecture 13

    3/33

    Example ProblemThe axis of the three-hinged arc ABC is a parabola with

    vertex B. Knowing that P = 20 kN and Q =0 determine a) the

    reactions at C, b) the components of the force exerted at on

    segment AB.

  • 8/4/2019 ENGR221 Lecture 13

    4/33

    Example Problem

    What is a hinge?

    At a hinge the moment is

    zero and can translate theforces across the point.

  • 8/4/2019 ENGR221 Lecture 13

    5/33

    Example Problem

    Draw the free-body

    diagram of the arch.

    x Ax Cx

    y Ay Cy

    Ay Cy

    A Cy

    Cy

    Ay

    0

    0 20 kN

    20 kN

    0 10 m 20 kN 3 m

    6 kN

    14 kN

    F R R

    F R R

    R R

    M R

    R

    R

  • 8/4/2019 ENGR221 Lecture 13

    6/33

    Example Problem

    Draw the free-body

    diagram of the arch at B.

    x Ax Cx

    B Ay Ax

    Ax

    Ax

    Cx

    0

    0 5 m 20 kN 2 m 2.5 m

    2.5 m 14 kN 5 m 20 kN 2 m

    12 kN

    12 kN

    F R R

    M R R

    R

    R

    R

  • 8/4/2019 ENGR221 Lecture 13

    7/33

    ZeroForce members

    When only two members form a non-collinear truss joint

    and no external load or support reaction is applied to the

    joint then the members must be zero-force members.

    When three members form a truss joint for which two of the

    members are collinear and the third is forms an angle with

    the first two, then the non-collinear member is a zero-force

    member provided no external force or support reaction isapplied to the joint, The collinear members carry equal

    loads.

  • 8/4/2019 ENGR221 Lecture 13

    8/33

    ZeroForce members

    Is there a zero force

    member in the truss?

  • 8/4/2019 ENGR221 Lecture 13

    9/33

    ZeroForce members

    Is there a zero force

    member in the truss?

  • 8/4/2019 ENGR221 Lecture 13

    10/33

    Example Problem

    The awning structure

    is supported by ball

    and socket joints at A

    and C and by a short

    link at B. The 750 N

    force is parallel to the

    z-axis. Determine the

    support reactions andthe force in each

    member of the space

    truss.

    EGAD!

    3-D Trusses!

  • 8/4/2019 ENGR221 Lecture 13

    11/33

    3-D Trusses

    The difference between 2-D and 3-D is that there

    are three more equations we will be concerned

    with and will require a bit more bookkeeping.

    Instead of just

    use the 6 sets of equations

    x y z0 0 0F F M

    x y z

    x y z

    0 0 0

    0 0 0

    F F F

    M M M

  • 8/4/2019 ENGR221 Lecture 13

    12/33

    Simple Truss

    A truss is analysis by using m=3*j-6, where m is

    number of members, j represents the number of

    joints and 6 represents the external supportreactions.

  • 8/4/2019 ENGR221 Lecture 13

    13/33

    Simple Truss

    If m< 3j-6, then the truss is unstable and will

    collapse under load.

    If m> 3j-6, then the truss has more unknowns

    than know equations and is an indeterminate

    structure.

    If m= 3j-6, ensures that a simple space truss is

    rigid and solvable, it is neither sufficient nor

    necessary to ensure that a non-simple plane truss

    is rigid and solvable.

  • 8/4/2019 ENGR221 Lecture 13

    14/33

    Example Problem

    The awning structure

    is supported by ball

    and socket joints at A

    and C and by a shortlink at B. The 750 N

    force is parallel to the

    z-axis. Determine the

    support reactions andthe force in each

    member of the space

    truss.

  • 8/4/2019 ENGR221 Lecture 13

    15/33

    Example Problem

    Draw the free body diagram

    A C B

    x Ax Cx

    y Ay Cy B

    Ay Cy B

    z Az Cz

    Az Cz

    0 750 N

    0

    0

    0 750 N

    750 N

    F R R R j k

    F R R

    F R R R

    R R RF R R

    R R

  • 8/4/2019 ENGR221 Lecture 13

    16/33

    Equilibrium ProblemExample

    Take the moment about A.

    A AW 1 AB B AC C0M r W r R r R

    1

    1

    AW

    AW 1

    4.0 m 5.0 m 0.0 m

    4.0 m 5.0 m 0.0 m

    0 0 750 N

    3750 N-m 3000 N-m 0

    r i j k

    i j k

    r W

    i j k

    AB

    AB B

    B

    B B

    4.0 m 0.0 m 4.0 m

    4.0 m 0.0 m 4.0 m

    0 0

    4.0 m 0 4.0 m

    r i j k

    i j k

    r R

    R

    R i j R k

  • 8/4/2019 ENGR221 Lecture 13

    17/33

    Equilibrium ProblemExample

    Take the moment about A.

    A AW 1 AB B AC C0M r W r R r R

    AC

    AC C

    Cx Cy Cz

    Cz Cy

    8.0 m 0.0 m 0.0 m

    8.0 m 0.0 m 0.0 m

    0 8 m 8 m

    r i j k

    i j k

    r R

    R R R

    i R j R k

  • 8/4/2019 ENGR221 Lecture 13

    18/33

    Equilibrium ProblemExample

    Using the summations of moments about A and look at the

    components.

    B B

    Cz Cz

    B Cy Cy

    component

    3750 N-m 4.0 m 0 937.5 N

    component

    3000 N-m 8.0 m 0 375 N

    component

    4.0 m 8.0 m 0 468.75 N

    i

    R R

    j

    R R

    k

    R R R

  • 8/4/2019 ENGR221 Lecture 13

    19/33

    Equilibrium ProblemExample

    Using the summations of forces about

    A and look at the components. The

    results are

    Unfortunately, RAx and RCx could notbe computed.

    Ay

    Az

    component

    468.75 N

    component

    375 N

    j

    R

    k

    R

  • 8/4/2019 ENGR221 Lecture 13

    20/33

  • 8/4/2019 ENGR221 Lecture 13

    21/33

    Equilibrium ProblemExampleUsing the method of joints look at joint A

    A AB AB AD AD

    x Ax AB AD

    y AD

    AD

    z AB

    AB

    Ax

    0

    0 0.7071 0.6247

    0 468.75 N 0.7809

    600.3 N

    0 375 N 0.7071

    530.33 N

    750 N

    F R T T

    F R T T

    F T

    T

    F T

    T

    R

    So the bars are in compression

    multiply by the unit vector to get the

    final set of forces.

  • 8/4/2019 ENGR221 Lecture 13

    22/33

    Equilibrium ProblemExampleUsing the method of joints look at joint C and the

    values will be same due to symmetry.

    C CB CB CD AD

    x Cx CB CD

    y CD

    CD

    z CB

    CB

    Cx

    0

    0 0.7071 0.6247

    0 468.75 N 0.7809

    600.3 N

    0 375 N 0.7071

    530.33 N

    750 N

    F R T T

    F R T T

    F T

    T

    F T

    T

    R

    So the bars are in compression multiply by the unit

    vector to get the final set of forces.

  • 8/4/2019 ENGR221 Lecture 13

    23/33

    Equilibrium ProblemExampleUsing the method of joints look at joint D

    z DB

    DB

    0 750 N 0.6247

    1200.6 N

    F T

    T

    Look at the y component of joint D

    DB

    2 2 2

    DB

    DB

    0 m 5 m 4 m

    0 m 5 m 4 m 6.403 m

    0 m 5 m 4 m6.403 m 6.403 m 6.403 m

    0.0 0.7809 0.6247

    r i j k

    r

    i j k

    i j k

  • 8/4/2019 ENGR221 Lecture 13

    24/33

    3-D Trusses - Class Problem

    The space truss is supported by ball and socket joints at D and

    by a short link at A and C. Determine the support reactions

    and the force in each member of the space truss.

  • 8/4/2019 ENGR221 Lecture 13

    25/33

    Frames -Definition

    Frames are structures that

    always contain at least one

    member acted on by forces

    at three or more points.Frames are constructed and

    supported so as to prevent

    any motion. Frame like

    structures that are not fully

    constrained are called

    machines or mechanisms.

  • 8/4/2019 ENGR221 Lecture 13

    26/33

    Frames

    In order to determine the

    internal forces holding the

    various parts of a frame

    together we mustdismember the frame and

    draw a free-body diagram

    for each of the component

    parts.

  • 8/4/2019 ENGR221 Lecture 13

    27/33

    FramesExample

    For the marine crane, which is

    used in offshore drilling

    operations, determine (a) the

    force in link CD (b) the force inbrace AC and ( c) the force

    exerted at on boom AB

  • 8/4/2019 ENGR221 Lecture 13

    28/33

    Frames

    Example

    Draw the free-body diagram

    x Ax

    Ax

    3 2

    y Ay

    Ay

    0

    0 N

    0 90 x10 kg 9.81 m/s

    882900 N or 882.9 kN

    F R

    R

    F D R

    D R

    RAxRAyD

    W

  • 8/4/2019 ENGR221 Lecture 13

    29/33

    Frames

    Example

    Take the moment about A

    A

    Ay

    0

    15 m 882.9 kN 38 m

    2236.68 kN

    R 3119.58 kN

    M

    D

    D

    RAxRAyDW

  • 8/4/2019 ENGR221 Lecture 13

    30/33

    Frames

    Example

    Cut along CD

    A

    CD

    CD CD

    0

    15 m 882.9 kN 38 m

    2236.68 kN 2236.68 kN T

    M

    T

    T T

    TCD

  • 8/4/2019 ENGR221 Lecture 13

    31/33

    Frames

    Example

    Look at joint A

    FACFAB

    1 o

    1 o

    18 mtan 50.19

    15 m

    58 mtan 55.4135 m

  • 8/4/2019 ENGR221 Lecture 13

    32/33

  • 8/4/2019 ENGR221 Lecture 13

    33/33

    Homework (Due 3/5/03)

    Problems:

    7-58, 7-60, 7-66, 7-68