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    Equilibrium and Torque

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    EquilibriumAn object is in Equilibrium when:

    1. There is no net force acting on the object

    2. There is no net Torque (well get to this later)

    In other words, the object is NOT experiencing

    linearacceleration or rotational acceleration.

    a v

    t 0

    t 0 Well get to this later

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    Static Equilibrium

    An object is in Static Equilibrium when it is

    NOT MOVING.

    v x

    t= 0

    a v

    t 0

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    Dynamic Equilibrium

    An object is in Dynamic Equilibrium when it is

    MOVING with constant linear velocity

    and/or rotating with constant angular velocity.

    a v

    t 0

    t 0

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    EquilibriumLets focus on condition 1: net force = 0

    The x components of force cancel

    The y components of force cancel

    F 0

    Fx 0

    Fy 0

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    Condition 1: No net Force

    We have already looked at situations where the net force = zero.Determine the magnitude of the forces acting on each of the

    2 kg masses at rest below.

    60

    3030 30

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    mg = 20 N

    N = 20 NFy = 0

    N - mg = 0N = mg = 20 N

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    Fy = 0

    T1 + T2 - mg = 0

    T1 = T2 = T

    T + T = mg

    2T = 20 N

    T = 10 N

    T1 = 10 N

    20 N

    T2 = 10 N

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    Condition 1: No net Force

    60

    mg =20 N

    f = 17.4 N N = 10 N

    Fx - f = 0

    f = Fx = mgsin 60

    f =17.4 N

    N = mgcos 60

    N = 10 N

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    3030

    mg = 20 N

    T1 = 20 N T2 = 20 N

    Fy = 0

    T1y + T2y - mg = 02Ty = mg = 20 N

    Ty = mg/2 = 10 N

    T2 = 20 N

    T2x

    T2y = 10 N

    30

    Ty/T = sin 30

    T = Ty/sin 30T = (10 N)/sin30

    T = 20 N

    Fx = 0

    T2x - T1x = 0

    T1x = T2x

    Equal angles ==> T1 = T2

    Note: unequal angles ==> T1 T2

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    Note:

    The y-components cancel, so

    T1y and T2y both equal 10 N

    3030

    mg = 20 N

    T1 = 20 N T2 = 20 N

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    30

    20 N

    T1 = 40 N

    T2 = 35 N

    Fy = 0

    T1y - mg = 0T1y = mg = 20 N

    T1y/T1 = sin 30

    T1 = Ty/sin 30 = 40 N

    Fx = 0

    T2- T1x = 0T2= T1x= T1cos30

    T2 = (40 N)cos30

    T2 = 35 N

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    Condition 1: No net Force

    Fx = 0 and Fy = 0

    Note:

    The x-components cancel

    The y-components cancel

    30

    20 N

    T1 = 40 N

    T2 = 35 N

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    3060

    Condition 1: No net Force

    A Harder Problem!

    a. Which string has the greater tension?

    b. What is the tension in each string?

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    a. Which string has the greater tension?

    Fx = 0 so T1x = T2x

    3060

    T1 T2

    T1 must be greater in order to have the same x-component as T2.

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    Fy = 0

    T1y + T2y - mg = 0

    T1sin60 + T2sin30 - mg = 0

    T1sin60 + T2sin30 = 20 N

    Solve

    simultaneous

    equations!

    Fx = 0

    T2x-T1x = 0

    T1x = T2xT1cos60 = T2cos30

    3060

    T1 T2

    Note: unequal angles ==> T1 T2

    What is the tension in each string?

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    EquilibriumAn object is in Equilibrium when:

    1. There is no net force acting on the object

    2. There is no net Torque

    In other words, the object is NOT experiencing

    linear accelerationorrotational acceleration.

    a v

    t 0

    t 0

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    What is Torque?

    Torque is like twisting force

    The more torque you apply to a wheel the

    more quickly its rate of spin changes

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    Math Review:

    1. Definition of angle in radians

    2. One revolution = 360 = 2 radians

    ex: radians = 180ex: /2 radians = 90

    s /r

    arc length

    radius

    s

    r

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    Linear vs. RotationalMotion

    Linear Definitions Rotational Definitions

    x

    v x

    t

    a v

    t

    in radians

    t

    in radians/sec or rev/min

    t in radians/sec/sec

    x

    xi xf

    i

    f

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    Linear vs. RotationalVelocity

    A car drives 400 m in20 seconds:

    a. Find the avg linear velocity

    A wheel spins thru an angle of400 radians in 20 seconds:

    a. Find the avg angular velocity

    v x

    t

    400m

    20s 20m /s

    t=

    400 radians

    20s

    20 rad/sec

    10 rev/sec

    600 rev/min

    x

    xi xf

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    Linear vs. Rotational

    Net Force ==> linear acceleration

    The linear velocity changes

    aFnet

    Net Torque ==> angular acceleration

    The angular velocity changes

    (the rate of spin changes)

    net

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    Torque

    Torque is like twisting force

    The more torque you apply to a

    wheel, the more quickly its rateof spin changes

    Torque = Frsin

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    Torque is like twisting force

    Imagine a bicycle wheel that can only spin about its axle.

    If the force is the same in each case, which case producesa more effective twisting force?

    This one!

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    Torque is like twisting force

    Imagine a bicycle wheel that can only spin about its axle.

    What affects the torque?1. The place where the force is applied: the distance r

    2. The strength of the force

    3. The angle of the force

    r

    F

    F// to r

    F to r

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    Torque is like twisting force

    Imagine a bicycle wheel that can only spin about its axle.

    What affects the torque?

    1. The distance from the axis rotation rthat the force is applied

    2. The component of force perpendicular to the r-vector

    r

    F

    F to r

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    Imagine a bicycle wheel that can only spin about its axle.

    Torque = (the component of force perpendicular to r)(r)

    r

    F

    F Fsin

    (F

    )(r)

    (Fsin)(r)

    Frsin

    Torque = Frsin

    Torque (F)(r)

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    Torque is like twisting force

    Imagine a bicycle wheel that can only spin about its axle.

    r

    F

    F Fsin

    (F

    )(r)

    (Fsin)(r)

    Frsin

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    (F )(r) Frsin

    r

    F

    F Fsin

    F

    r

    Since and are supplementary angle

    (ie : + = 180)sin = sin

    Cross r with F and choose any angle

    to plug into the equation for torque

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    Torque = (Fsin)(r)

    Two different ways of looking at torque

    r

    F

    F Fsin

    Torque = (F)(rsin)

    r

    F

    r

    r

    F Fsin

    r

    F

    Torque (F)(r)

    Torque (F)(r)

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    Imagine a bicycle wheel that can only spin about its axle.

    Torque = (F)(rsin)

    r

    F

    r

    r

    F

    r is called the "moment arm" or "moment"

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    EquilibriumAn object is in Equilibrium when:

    1. There is no net force acting on the object

    2. There is no net Torque

    In other words, the object is NOT experiencing

    linear accelerationorrotational acceleration.

    a vt

    0

    t 0

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    Condition 2: net torque = 0

    Torque that makes a wheel want to rotate clockwise is +

    Torque that makes a wheel want to rotate counterclockwise is -

    Positive Torque Negative Torque

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    Condition 2: No net Torque

    Weights are attached to 8 meter long levers at rest.Determine the unknown weights below

    20 N ??

    20 N ??

    20 N ??

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    Condition 2: No net Torque

    Weights are attached to an 8 meter long leverat rest.Determine the unknown weight below

    20 N ??

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    Condition 2: No net Torque

    F1 = 20 N

    r1 = 4 m r2 = 4 m

    F2 =??

    Ts = 0

    T2 - T1 = 0

    T2 = T1F2r2sin2 = F1r1sin1

    (F2)(4)(sin90) = (20)(4)(sin90)

    F2= 20 N same as F1

    Upward force

    from the fulcrum

    produces no torque

    (since r = 0)

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    Condition 2: No net Torque

    20 N 20 N

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    Condition 2: No net Torque

    20 N ??

    Weights are attached to an 8 meter long leverat rest.Determine the unknown weight below

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    Condition 2: No net Torque

    Ts = 0

    T2 - T1 = 0T2 = T1

    F2r2sin2 = F1r1sin1

    (F2)(2)(sin90) = (20)(4)(sin90)

    F2 = 40 NF2 =??

    F1 = 20 N

    r1 = 4 m r2 = 2 m

    (force at the fulcrum is not shown)

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    Condition 2: No net Torque

    20 N 40 N

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    Condition 2: No net Torque

    20 N ??

    Weights are attached to an 8 meter long leverat rest.Determine the unknown weight below

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    Condition 2: No net Torque

    F2 =??

    F1 = 20 N

    r1 = 3 m r2 = 2 m

    Ts = 0

    T2 - T1 = 0

    T2 = T1F2r2sin2 = F1r1sin1

    (F2)(2)(sin90) = (20)(3)(sin90)

    F2 = 30 N

    (force at the fulcrum is not shown)

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    Condition 2: No net Torque

    20 N 30 N

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    In this special case where

    - the pivot point is in the middle of the lever,

    - and 1 = 2

    F1R1sin1 = F2R2sin2

    F1R1= F2R2

    20 N 20 N

    20 N 40 N

    20 N 30 N

    (20)(4) = (20)(4)

    (20)(4) = (40)(2)

    (20)(3) = (30)(2)

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    More interesting problems

    (the pivot is not at the center of mass)

    Masses are attached to an 8 meter long leverat rest.

    The lever has a mass of 10 kg.

    Determine the unknown weight below.

    20 N ??

    CM

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    Trick: gravity applies a torque equivalent to(the weight of the lever)(Rcm)

    Tcm =(mg)(rcm) = (100 N)(2 m) = 200 Nm

    More interesting problems

    (the pivot is not at the center of mass)

    20 N??

    CM

    Weight of lever

    Masses are attached to an 8 meter long leverat rest.

    The lever has a mass of 10 kg.

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    Masses are attached to an 8 meter long leverat rest.

    The lever has a mass of 10 kg.

    Determine the unknown weight below.

    F1 = 20 N

    CM

    R1 = 6 m R2 = 2 m

    F2 = ??

    Rcm = 2 m

    Fcm = 100 N

    Ts = 0

    T2 - T1 - Tcm = 0T2 = T1 + Tcm

    F2r2sin2 = F1r1sin1 + FcmRcmsincm(F2)(2)(sin90)=(20)(6)(sin90)+(100)(2)(sin90)

    F2 = 160 N

    (force at the fulcrum is not shown)

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    Other problems:

    Sign on a wall#1 (massless rod)

    Sign on a wall#2 (rod with mass)

    Diving board (find ALL forces on the board)

    Push ups (find force on hands and feet)

    Sign on a wall, again

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    Sign on a wall #1

    Eat at Joes

    30

    A 20 kg sign hangs from a 2 meter long massless rod

    supported by a cable at an angle of 30 as shown.

    Determine the tension in the cable.

    30

    Pivot point

    T Ty = mg = 200N

    mg = 200N

    Ty/T = sin30

    T = Ty/sin30 = 400N

    We dont need to use torque

    if the rod is massless!

    (force at the pivot point is not shown)

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    Sign on a wall #2

    Eat at Joes

    30

    A 20 kg sign hangs from a 2 meter long rod that

    has a mass of 10 kgand is supported by a cable at an

    angle of 30 as shown. Determine the tensionin the cable FT

    30

    Pivot point

    FT

    mg = 200N

    Fcm= 100N

    (force at the pivot point is not shown)

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    Sign on a wall #2

    A 20 kg sign hangs from a 2 meter long rod that

    has a mass of 10 kgand is supported by a cable at an

    angle of 30 as shown. Determine the tension in the cable.

    30

    Pivot point

    FT

    mg = 200N

    Fcm = 100N

    T = 0

    TFT = Tcm + Tmg

    FT(2)sin30 =100(1)sin90 + (200)(2)sin90

    FT = 500 N

    (force at the pivot point is not shown)

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    Diving board

    bolt

    A 4 meter long diving board with a mass of 40 kg.a. Determine the downward force of the bolt.

    b. Determine the upward force applied by the fulcrum.

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    Diving board

    A 4 meter long diving board with a mass of 40 kg.

    a. Determine the downward force of the bolt.(Balance Torques)

    bolt

    Rcm = 1R1 = 1

    Fcm = 400 NFbolt = 400 N

    T = 0

    (force at the fulcrum is not shown)

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    Diving boardA 4 meter long diving board with a mass of 40 kg.

    a. Determine the downward force of the bolt.(Balance Torques)

    b. Determine the upward force applied by the fulcrum.

    (Balance Forces)

    bolt

    Fcm = 400 NFbolt = 400 N

    F = 800 N F = 0

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    Remember:

    An object is in Equilibrium when:

    a. There is no net Torque

    b. There is no net force acting on the object

    F 0

    0

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    Push-ups #1

    A 100 kg man does push-ups as shown

    Find the force on his hands and his feet

    1 m

    0.5 m

    30

    Fhands

    Ffeet

    CM

    Answer:

    Fhands = 667 N

    Ffeet = 333 N

    A 100 kg man does push ups as shown

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    A 100 kg man does push-ups as shown

    Find the force on his hands and his feet

    T = 0

    TH = Tcm

    FH(1.5)sin60 =1000(1)sin60

    FH = 667 N

    F = 0

    Ffeet + Fhands = mg = 1,000 N

    Ffeet = 1,000 N - Fhands = 1000 N - 667 N

    FFeet = 333 N

    1 m

    0.5 m

    30

    Fhands

    Ffeet

    CM

    mg = 1000 N

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    Push-ups #2

    A 100 kg man does push-ups as shown

    Find the force acting on his hands

    1 m

    0.5 m

    30

    Fhands

    CM90

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    Push-ups #2A 100 kg man does push-ups as shown

    T = 0

    TH = TcmFH(1.5)sin90 =1000(1)sin60

    FH = 577 N

    1 m

    0.5 m

    30

    Fhands

    CM

    90

    mg = 1000 N

    Force on hands:

    (force at the feet is not shown)

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    Sign on a wall, again

    A 20 kg sign hangs from a 2 meter long rod that

    has a mass of 10 kgand is supported by a cable at an

    angle of 30 as shown

    Find the force exerted by the wall on the rod

    Eat at Joes

    30 30

    FT = 500N

    mg = 200N

    Fcm = 100N

    FW = ?

    (forces and angles NOT drawn to scale!

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    Find the force exerted by the wall on the rod

    FWx = FTx = 500N(cos30)

    FWx= 433N

    FWy + FTy = Fcm +mg

    FWy = Fcm + mg - FTy

    FWy= 300N - 250

    FW 50N (forces and angles NOT drawn to scale!)

    Eat at Joes

    30 30

    FT = 500N

    mg = 200NFcm = 100N

    FW

    FWy= 50NFWx= 433N

    FW= 436N

    FW= 436N