02 force systems

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    2 Force Systems

    K L 2 1 0 3 , C L A S S 0 2

    S E M E S T E R I 2 0 1 2 / 2 0 1 3

    Force

    Force is a vector quantity. Its effect on a body or a

    direction of the force.

    Generally, a complete description of a force must

    include its magnitude, direction, andpoint ofapplication.

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    External and Internal Effects

    The effects of a force on a body (or structure) can bese arated into external and internal effects.

    External effects: reaction forces at the supports sothat the whole structure is in equilibrium (more onthis in Chapter 3).

    Internal effects: internal forces (will be discussed inCha ter and ) stress and deformation in the

    structure (will be discussed in Mechanics ofMaterials).

    Principle of Transmissibility

    A force may be applied at any point onits line of action without altering the

    resultant effects of the force external tothe body on which it acts.

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    Components of a Force

    Example 1

    The forces F1, F2, and F3act on pointA of the

    rac et as s own.

    Determine thexand y

    components of each ofthe three forces.

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    o

    1

    o

    1

    600 cos 35 491 N

    600sin 35 344 N

    x

    y

    F

    F

    4 2

    2

    5

    3500 300 N

    5

    x

    yF

    0.2800 358 NF

    2 2

    32 2

    0.2 0.4

    0.4800 716 N

    0.2 0.4

    x

    yF

    Resultant of Forces

    1 2

    1 2

    1 2

    x x x x

    y y y y

    R F F F

    R F F F

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    Example 2

    Combine the twoforces P and T into asingle equivalent forceR.

    o

    o

    o

    6sin60tan 0.866 40.9

    3 6cos60

    BD

    AD

    o

    o

    800 600cos 40.9 346 lb

    600sin 40.9 393 lb

    x xR F

    R F

    2 2

    1 o

    524 lb

    tan 48.6

    x y

    y

    x

    R R R

    R

    R

    Graphical solution:

    o

    525 lb

    49

    R

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    Moment about a Point

    Definition: tendency of the force torotate the body about the point.

    The magnitude of the moment isproportional to the magnitude ofthe force and to the momentarm d:

    M r F

    Varignons Theorem

    The moment of a force about any point is equal to

    force about the same point.

    OM Rd Pp Qq

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    Example 3

    Calculate themagnitude of themoment about the

    base point O of the600-N force indifferent ways.

    (i) Moment arm: o o4cos 40 2sin 40

    4.35 m

    d

    600 4.35 2610 N-m CWOM

    o

    1

    o

    2

    600 cos 40 460 N

    600sin 40 386 N

    F

    F

    (ii) Components ofF:

    460 4 386 2 2610 N-m CWOM

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    (iii)

    By principle of transmissibility,Fcan be moved to pointB or Cto eliminate the moment of componentF2 orF1, respectively.

    o

    14 2tan 40 5.68 md

    386 6.77 2610 N-mOM

    (iv)o

    22 4cot 40 6.77 md

    . -O

    o o2 4 600 cos40 sin 402610 N-m

    O

    M r F i j i j

    k

    (v) Using vector formulation:

    Couple

    Definition: the momentM F d ,

    opposite, andnoncollinear forces.

    The moment of a couplehas the same value atall points.

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    Equivalent Couples

    Changing the value ofFand ddoes not change acou le as lon as the roductFdremains the same.

    Likewise, a couple is not affected if the forces act in adifferent but parallel plane.

    In these four cases, the couples are equivalent:

    Example 4

    The rigid structuralmember is subjected to

    the two 100-N forces.Replace this couple by

    an equivalent coupleconsisting of the twoforces P and P, eachof which has amagnitude of 400 N.Determine the properangle .

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    The original couple is counterclockwise with magnitude of:

    100 0.1 10 N-mM

    The forces P and P produce a counterclockwise couple of:

    .

    10 16cos

    Solving for :

    1 o10cos 51.316

    Force Couple System

    Effect of a force acting on a body: Translation in the direction of the force.

    Rotation about any axis which does not intersect the line of theforce.

    Both effects can be represented by replacing a forceby a force and a couple.

    Reversing the process, we can combine a force couple system into a single, equivalent force.

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    Equivalent Force Systems

    A group or a system of forces can be replaced by theresultant.

    The resultant usually represents the simplest force couple combination without altering the externaleffect on the body.

    x xR F R = F

    y y

    R F

    M M Fd

    Equivalent Force Systems

    Two force systems are equivalent if the force

    systems are the same.

    1 2 1 2x xR R

    R = R

    1 2

    1 2

    y y

    M M

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    Equivalent Force Systems

    These four systemsare e uivalent:

    Example 5

    Replace the horizontal 80-lb

    equivalent system consisting ofa force at O and a couple.

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    Apply two equal and opposite 80-lb forces at O andidentify the counterclockwise couple:

    o80 9sin 60 624 lb-in.M

    Example 6

    Determine the

    four forces and onecouple which act

    on the plate shown.

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    (i) Equivalent force-couple at O:o o

    o o

    : 40 80cos30 60cos45 66.9 N

    : 50 80sin30 60sin 45 132.4 N

    x x x

    y y y

    R F RR F R

    2 2

    66.9 132.4 148.3 NR

    1 o132.4tan 63.2

    66.9

    o o: 140 50 5 60cos 45 4 60sin 45 7

    237 N-m CW

    O OM Fd M

    (ii) Single equivalent force

    148.3 237

    1.60 m

    ORd M d

    d

    237 1.792 m132.4

    y OR b M b

    In other form: