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  • 8/6/2019 Microsoft Power Point - STATICS Handouts 3

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    V. Analysis of 3DForce Systems

    Most of the physical quantities in mechanics canbe expressed mathematically by means ofscalars and vectors

    A scalar quantity is characterized by a positiveor negative number, i.e., mass, volume andlength

    A vector quantity has both magnitude anddirection, i.e., force and moment

    Unit vector

    A unit vector is a vector having a magnitude of 1. If Ais a vector having a magnitude A 0, then a unitvector having the same direction as A is representedby

    where A represents the magnitude of and defines the direction

    and sense of

    Au

    Au

    A

    A

    =

    =

    A

    uA

    1

    Cartesian Unit Vectors

    In threedimensions, the setof Cartesian unitvectors I, j, k, isused to designatethe directions of thex, y, and z axe

    respectively,z

    y

    xi

    j

    k

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    Cartesian Vector Representation

    x

    z

    y

    Ayj

    Axi

    Azk

    j

    i

    k

    kAjAiA zyx++=

    Cartesian vector form of components:

    Magnitude of a Cartesian Vector

    x

    z

    y

    Ayj

    Axi

    Azk

    j

    i

    k

    ( ) ( ) ( )222

    zyx AAAA++=

    Ay

    Az

    Ax

    A

    Direction of a Cartesian Vector

    x

    z

    y

    Ayj

    Axi

    Azk

    A

    Ax=cosDirection cosines of A: , ,

    A

    Ay=cos A

    Az=cos

    kAjAiA

    kAjAiA

    Au

    kyiu

    kA

    Aj

    A

    Ai

    A

    A

    Au

    zyx

    A

    A

    zyxA

    ++=

    ++=

    =

    =++

    ++=

    ++=

    =

    coscoscos

    1coscoscos

    coscoscos

    222

    If magnitude and coordinate direction angles of A are given,the Cartesian vector form of A is,

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    Vector Operations

    x

    z

    y

    (Ax + Bx)i

    kAjAiA zyx ++=

    R

    B

    A

    (Az + Bz)k

    (Ay + By)j

    kBjBiBzyx ++=

    Given:

    ( ) ( ) ( )

    ( ) ( ) ( )kBAjBAiBAR

    kBAjBAiBAR

    zzyyxx

    zzyyxx

    ++==

    +++++=+=

    '

    Vector Addition:

    Vector Subtraction:

    Resultant of Force Systems

    Concurrent Force System

    The concept of vector addition may be generalizedand applied to a system of several concurrentforces.

    The force resultant is the vector sum of all the forcesin the system

    ZkYjXiFR ++==

    Problem 1

    Determine themagnitude andcoordinatedirection anglesof the resultantforce acting onthe ring.

    x

    y

    z

    F1 = {300i+400j}NF2 = {- 500i+1000j+1000k}N

    Problem 2

    Two forces act onthe hook. Specifythe coordinatedirection angles ofF2 so that theresultant force FRacts along thepositive x axis andhas a magnitude of

    800N

    y

    z

    x

    F2=700N

    F1=300N

    600

    450

    1200

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    Position vector

    x

    z

    y

    ( )zyxP ,,

    yj

    xi

    zk

    zkyjxir ++=

    The position vector r isdefined as a fixed vectorwhich locates a point inspace relative to another

    point.

    O

    The position vector may ne denoted from pointA to point B in space

    ( )AAA zyxA ,,

    x

    y

    z

    r

    rA

    rB

    ( )ixx AB

    ( ) ( )( ) ( ) ( )kzzjyyixxr

    kzjyixkzjyixrrr

    rrr

    ABABAB

    BBABBBAB

    BA

    ++=

    ++++==

    =+

    x

    z

    y

    A

    B

    ( )jyy AB

    ( )kzz AB

    Dot product

    The dot product of vectors A and B is defined asthe product of the magnitudes of A and B andthe cosine of the angle between their tails

    cosAB=

    A

    B

    Laws of Operation

    Commutative law

    Multiplication by a scalar

    Distributive law

    =

    ( ) ( ) ( ) ( )aaaa ===

    ( ) ( ) ( )DD =

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    The dot product of two general vectors A and Bexpressed in Cartesian vector form

    Applications

    Angle formed between two vectors or intersecting lines

    Components of a vector parallel and perpendicular to a line

    ( ) ( )

    zzyyxx

    zyxzyx

    BABABA

    kBjBiBkAjAiA

    ++=

    ++++=

    Cross Product

    The cross product of two vectors A and Byields the vector C,

    C = A x B

    The magnitude of C is defined as the productof the magnitudes of A and B and the sine ofthe angle between their tails

    C = AB sin

    Vector C has a direction perpendicular to

    the plane containing A and B

    C = A x B = (AB sin ) ucC

    BA

    ucC = AB sin

    Laws of Operation

    A x B = -B x A

    Multiplication by a scalar

    a(A x B) = (aA) x B = A x (aB) = (A x B)a

    Distributive law

    A x (B + D) = (A x B) + (A x D)

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    The cross product of two general vectors A andB expressed in Cartesian vector form

    The above equation may be expressed indeterminant form

    ( ) ( )

    ( ) ( ) ( )kBABAjBABAiBABA

    kBjBiBkAjAiA

    xyyxxzzxyzzy

    zyxzyx

    +=

    ++++=

    z

    z

    y

    y

    x

    x

    B

    A

    k

    B

    A

    j

    B

    A

    i

    =

    Moment of a Force

    The moment of a force F about point or, orabout the moment axis passing through O andperpendicular to the plane containing O and F,can be expressed using the vector crossproduct,

    FrMO =

    F

    MO

    OA r

    d

    Moment axis

    The magnitude of the above cross product

    ( ) FdrFrFMO

    === sinsin zyx

    kyxO

    FFF

    rrr

    ijk

    rxFM =

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    Equilibrium in Three Dimensions

    Support reactionsCable

    Smooth surface

    Roller

    Ball and socket

    Single smooth pin

    Single hinge

    Fixed supportFxFz

    Fy

    Mx

    My

    Mz

    Fx

    Fy

    Fz

    Conditions of Equilibrium

    0

    0

    0

    0

    0

    =

    =

    =

    =++=

    =++=

    z

    y

    x

    zyxO

    zyx

    F

    F

    F

    kMjMiMM

    kFjFiFF

    0

    0

    0

    =

    =

    =

    z

    y

    x

    M

    M

    M

    Problem

    Determine thetension incables BC andBD and thereactions atthe ball-andsocket joint Afor the mast

    shown.z

    y

    x

    F = 1KN

    6m

    6m

    6m 3m

    Solution program (Vector Analysis)

    Draw the FBD

    Represent each force on the FBD in vector form

    Apply the force equation of equilibrium

    Take moment about point A to eliminate theother unknowns

    Evaluate the cross product and combine liketerms and equate to zero to solve for the

    unknows.

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    { }

    ( ) ( )

    ( ) ( ) ( )

    ++

    ++=

    =

    +

    +=

    =

    ++=

    =

    222

    22

    zx

    zyx

    magnitude

    ctorpositionve

    z

    zy

    magnitude

    ctorpositionve

    BDyBDBD

    BDBDBD

    BD

    BD

    BD

    BDBD

    BCBCy

    BCBC

    BC

    BC

    BC

    BCBC

    zyx

    rrr

    krjrirT

    r

    rTT

    rr

    krjrT

    r

    rTT

    kAjAiAA

    NiF

    ( ) ( )

    03

    1

    2

    2

    0

    03

    2

    2

    2

    0

    03

    21

    0

    03

    1

    3

    2

    3

    2

    2

    2

    2

    2

    0

    0

    =

    =

    =

    =

    =+

    =

    =

    +

    +

    ++++

    =+++

    =

    BDBCz

    BDBCy

    BDx

    BDBDBDBCBCzyx

    BDBC

    TTA

    Z

    TTA

    Y

    TA

    X

    kTjTiTkTjTkAjAiAi

    TTAF

    F

    ( )

    ( ) ( )

    ( )

    046

    0

    0223

    0

    3

    1

    3

    2

    3

    2

    2

    2

    2

    26

    0

    0

    =

    =

    =

    =

    +

    +

    +

    =++

    =

    BD

    z

    BDBC

    x

    BDBDBDBCBC

    BDBCAB

    A

    T

    M

    TT

    M

    kTjTiTkTjTij

    TTFr

    M

    0

    5.1

    0

    707.02

    2

    5.1

    :

    =

    =

    =

    ==

    =

    z

    y

    x

    BC

    BD

    A

    KNA

    A

    KNT

    KNT

    Answer

    Problem

    Rod AB issubjected tothe 200N force.Determine thereactions at theball-and-socketjoint A and thetension incables BD and

    BE.

    A

    E

    B

    C

    D

    1.5m

    1.5m

    2m

    2m

    200N

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    Solution program (Vector Analysis)

    Draw the FBD

    Represent each force on the FBD in vector form

    Apply the force equation of equilibrium

    Take moment about point A to eliminate theother unknowns

    Expand the equation and equate to zero to solvefor the unknowns

    { }

    iTT

    kTT

    kAjAiAA

    NiF

    BDBD

    BEBE

    zyx

    =

    =

    +=

    = 200

    ( ) ( ) ( ) ( )

    0

    0

    200

    0200

    0

    0

    0

    0200

    0

    0

    =+

    =

    =

    =+

    =

    =+

    =

    =++++

    =+++

    =

    BEz

    y

    y

    BDx

    BDBEzyx

    BDBE

    TA

    Z

    NA

    A

    Y

    TA

    X

    iTkTkAjAiAj

    TTAF

    F( )

    ( ) ( ) ( ) ( )

    0200

    0

    022

    0

    0200

    0

    0222005.0

    0

    0

    =+

    =

    =+

    =

    =

    =

    =++++

    =++

    =

    BD

    z

    BDBE

    y

    BE

    x

    BDBE

    BDBEABAC

    A

    T

    M

    TT

    M

    T

    M

    iTkTkjijkji

    TTrFr

    M

    NA

    NATNAT

    Answers

    y

    xBD

    zBE

    200

    200200

    :

    =

    ==

    ==

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    Problem Set 2Problem Set 3

    Instructions for Problem Set

    Use short-size bondpaper as answer

    sheet

    Show complete solution

    Deadline of Submission: Monday, August

    15, 2011

    Problem

    The uniformconcrete slabhas a weight of25KN. Determinethe tension ineach of the threeparallelsupportingcables when theslab is held in the

    horizontal plane.

    8m

    y

    zx

    TC

    A

    B

    C

    TA

    TB

    Problem

    A vertical load P =3600N applied tothe tripod causes acompressive forceof 1200N in leg ABand a compressiveforce of 1300N inleg AC. Determinethe force in leg ADand the coordinatesxDand zDof its

    lower end D.

    3m

    2.4m

    2.4m

    1.8m

    xD

    zDO

    C

    A

    B

    D

    P

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