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    Quick Quiz (15 Minute)

    Jika masa mA=4kg, mB=2kg dan gesekan kinetiknyaadalah mkA=0.300 dan mkB=0.400 dan percepatangravitasi sebesar 9.8 m/s2. Tentukan (a) tegangan talipada sistem dan (b) percepatan dari sistem

    30O

    T

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    Circular Motion

    Setyawan P. Sakti

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    Some Example

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    Angular Displacement

    Recall for linear motion: displacement, velocity, acceleration

    Need similar concepts forobjectsmoving in circle (CD, merry-go-

    round, etc.) As before:

    need a fixed reference system (line)

    use polar coordinate system

    tva

    trvrrr if

    ,,

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    Angular Displacement

    Every point on the objectundergoes circular motion aboutthe point O

    Angles generally need to bemeasured in radians

    Note:

    r

    s

    3.572

    3601

    rad

    ]degrees[180]rad[

    length of arc

    radius

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    Angular Displacement

    The angular displacementisdefined as the angle the objectrotates through during some

    time interval

    Every point on the discundergoes the same angulardisplacement in any given timeinterval

    if

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    Angular Velocity

    The average angular velocity(speed), , of a rotating rigidobject is the ratio of theangular displacement to thetime interval

    ttt if

    if

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    Angular Speed

    The instantaneousangularvelocity (speed) is defined as thelimit of the average speed as thetime interval approaches zero

    Units of angular speed areradians/sec (rad/s)

    Angular speed will be positive if is increasing

    (counterclockwise)

    negative if is decreasing(clockwise)

    tt

    0lim

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    Angular Acceleration

    What if object is initially at restand then begins to rotate?

    The average angular acceleration,a, of an object is defined as theratio of the change in the angular

    speed to the time it takes for theobject to undergo the change:

    Units are rad/s

    Similarly, instant. angular accel.:

    ttt if

    if

    a

    tt

    a 0lim

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    Notes about angular kinematics:

    When a rigid object rotates about a fixed axis, everyportion of the object has the same angular speed andthe same angular acceleration

    i.e. ,, and a are not dependent upon r, distance formhub or axis of rotation

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    1. Bicycle wheel turns 240 revolutions/min. What is its angular

    velocity in radians/second?

    secradians1.25secradians8rev1

    rads2

    sec60

    min1

    min

    rev240

    2. If wheel slows down uniformly to rest in 5 seconds, what is the

    angular acceleration?

    2secrad5

    sec5

    secrad250

    t

    if a

    Examples:

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    Given:

    1. Angular velocity:

    240 rev/min

    2. Time t = 5 s

    Find:

    1. = ?

    3. How many revolution does it turn in those 5 sec?

    srevolution102

    rev1rad5.62)(

    rad5.62sec5secrad52

    1sec5secrad25

    2

    1

    2

    2

    0

    a

    rev

    tt

    Recall that for linear motion we had:

    Perhaps something similar for angular quantities?

    2

    02

    1attvx

    Examples:

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    Analogies Between Linear andRotational Motion

    Rotational Motion About aFixed Axis with Constant

    Acceleration

    Linear Motion withConstant Acceleration

    ti a

    2

    2

    1

    tti a

    a 222 i xavv i 222

    2

    2

    1

    attvx i

    atvv i

    R l i hi B A l d

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    Relationship Between Angular andLinear Quantities

    Displacements

    Speeds

    Accelerations

    r

    s

    vr

    ts

    rt

    1

    or

    1

    ra a

    R l ti hi B t A l d

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    Relationship Between Angular andLinear Quantities

    Displacements

    Speeds

    Accelerations

    Every point on therotating object has thesame angular motion

    Every point on the

    rotating object does nothave the same linearmotion

    rs

    rv

    ra a

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    Concept

    A ladybug sits at the outer edge of a merry-go-round, anda gentleman bug sits halfway between her and the axis ofrotation. The merry-go-round makes a complete revolutiononce each second.The gentleman bugs angular speed is

    1. half the ladybugs.2. the same as the ladybugs.3. twice the ladybugs.4. impossible to determine

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    Concept

    A ladybug sits at the outer edge of a merry-go-round, anda gentleman bug sits halfway between her and the axis ofrotation. The merry-go-round makes a complete revolutiononce each second.The gentleman bugs angular speed is

    1. half the ladybugs.2. the same as the ladybugs.3. twice the ladybugs.4. impossible to determine

    Note: both insects have an angular speed of 1 rev/s

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    Centripetal Acceleration

    An object traveling in a circle,even though it moves with aconstant speed, will have anacceleration (since velocity

    changes direction) This acceleration is called

    centripetal (center-seeking).

    The acceleration is directed

    toward the center of the circleof motion

    C t i t l A l ti d A l

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    Centripetal Acceleration and AngularVelocity The angular velocity and the linear

    velocity are related (v = r)

    The centripetal acceleration canalso be related to the angularvelocity

    t

    s

    r

    v

    at

    v

    sr

    vv

    r

    s

    v

    v

    a

    but,

    rar

    va CC

    22

    or

    Thus:

    Similar

    triangles!

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    Total Acceleration

    What happens if linearvelocity also changes?

    Two-componentacceleration: the centripetal component of

    the acceleration is due tochanging direction

    the tangential component of theacceleration is due to changingspeed

    Total acceleration can befound from thesecomponents:

    22

    Ct aaa

    slowing-down car

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    Vector Nature of Angular Quantities

    As in the linear case,displacement, velocityand acceleration arevectors:

    Assign a positive ornegative direction

    A more complete way isby using the right hand

    rule Grasp the axis of rotationwith your right hand

    Wrap your fingers in thedirection of rotation

    Your thumb points in thedirection of

    F C i C t i t l

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    Forces Causing CentripetalAcceleration Newtons Second Law says that the centripetal

    acceleration is accompanied by a force

    F stands for any force that keeps an object following acircular path

    Force of friction (level and banked curves)

    Tension in a string Gravity

    rmr

    v

    mmaF C2

    2

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    Example1: level curves

    Consider a car driving at 20 m/s (~45mph) on a level circular turn ofradius 40.0 m. Assume the carsmass is 1000 kg.

    1. What is the magnitude offrictional force experienced bycars tires?

    2. What is the minimum coefficientof friction in order for the car tosafely negotiate the turn?

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    Example1:

    Given:

    masses: m=1000 kg

    velocity: v=20 m/s

    radius: r = 40.0m

    Find:

    1. f=?

    2. m=?

    1. Draw a free body diagram, introduce

    coordinate frame and consider vertical

    and horizontal projections

    mgN

    mgNFy

    0

    Nm

    sm

    kgr

    v

    mmaf

    fmaFx

    4

    22

    100.140

    20

    1000

    2. Use definition of friction force:

    02.18.91000

    101.0

    thus,10

    2

    4

    42

    smkg

    N

    Nr

    vmmgf

    m

    m

    Lesson: m for rubber on dry concrete is 1.00!

    rubber on wet concrete is 0.2!

    driving too fast

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    Concept

    Is this static or kinetic friction is the car does not slide or skid?

    1. Static2. Kinetic

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    Example2: banked curves

    Consider a car driving at 20 m/s (~45mph) on a 30 banked circularcurve of radius 40.0 m. Assumethe cars mass is 1000 kg.

    1. What is the magnitude offrictional force experienced bycars tires?

    2. What is the minimum coefficientof friction in order for the car to

    safely negotiate the turn?

    A component of the normal force adds to thefrictional force to allow higher speeds

    rg

    v2

    tan

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    Given:

    masses: m=1000 kg

    velocity: v=20 m/s

    radius: r = 40.0m

    angle: a = 30

    Find:

    1. f=?

    2. m=?

    1. Draw a free body diagram,

    introduce coordinate frame and

    consider vertical and

    horizontal projections

    Nmgr

    vmf

    mgfr

    vmFx

    376030sin30cos

    30sin30cos

    2

    2

    NmgrvmN

    mgNr

    vmFy

    4

    2

    2

    103.130cos30sin

    30cos30sin

    2. Use definition of friction force:

    28.0

    101.3

    3760

    isminimalthus,

    4

    s

    N

    N

    N

    f

    Nf

    ss

    s

    m

    mm

    Lesson: by increasing angle of banking,

    one decreases minimal m or friction with

    which one can take curve!

    Example 2:

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    Example 3: Horizontal Circle

    The horizontal component ofthe tension causes thecentripetal acceleration

    tangaC

    E l 4

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    Example 4:

    7 m49 m

    http://www.gaydayatbuschgardens.com/rollercoaster.jpghttp://www.gaydayatbuschgardens.com/rollercoaster.jpghttp://www.gaydayatbuschgardens.com/rollercoaster.jpg
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    THE VIPER

    (Six Flags Over Magic Mountain)188 feet high

    70 mph

    One of the largestlooping roller coasters

    in the world

    Roller Coaster

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    Top Thrill Dragster(Cedar Point)

    420 feet tall

    120 mph0 to 120 mph in 4 sec

    free-falls back to Earth,reaching a speed of 120

    mph for the second time

    $ 25 million

    Which way do you perceive the

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    Perceived acceleration

    Which way do you perceive theacceleration for circular motion?

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    FORCE

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    FPerceived acceleration

    Circular motion:force is toward center of circle

    Note: the kid in the middle feels no acceleration!

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    look at the passengers!

    NASAs vomit comet

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    What has to be true about theacceleration a of the vomitcomet (if the apparent weightof the passengers is zero)?

    A. a points upward

    B. a points downward

    C. a points towards the

    center of their

    circular trajectory

    Clicker Question

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    You better believe in conservation of energy if you want tolive!

    Roller coasters

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    Most people find this sudden

    reduction in apparent weightterrifying.

    Note: this is not uniform circular motion!

    Forces in Accelerating Reference

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    Forces in Accelerating ReferenceFrames

    Distinguish real forces from fictitious forces

    Centrifugal force is a fictitious force

    Real forces always represent interactionsbetween objects

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    Newtons Law of Universal Gravitation

    Every particle in the Universe attracts every otherparticle with a force that is directly proportional tothe product of the masses and inverselyproportional to the square of the distancebetween them.

    2

    21

    r

    mm

    GF

    G is the universal gravitational constant

    G = 6.673 x 10-11 N m /kg

    This is an example of an inverse square law

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    Gravitation Constant

    Determined experimentally

    Henry Cavendish

    1798

    The light beam and mirror serve toamplify the motion

    E l

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    Example:

    Question: Calculate gravitational attraction between two students 1

    meter apart

    Nmkgkg

    kg

    mN

    r

    mm

    GF7

    22

    211

    2

    21

    102.41

    9070

    1067.6

    Extremely small

    Compare:

    NmgF 686

    Applications of Universal Gravitation 1: Mass of

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    Applications of Universal Gravitation 1: Mass ofthe Earth

    Use an example of anobject close to thesurface of the earth

    r ~ REGgRM EE

    2

    Applications of Universal Gravitation 2:

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    Applications of Universal Gravitation 2:Acceleration Due to Gravity

    g will vary with altitude

    2r

    MGg E

    mgrMGm

    rmMGF EE

    22

    Gravitational Potential

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    Gravitational PotentialEnergy

    PE = mgy is valid onlynear the earths surface

    For objects high above

    the earths surface, analternate expression isneeded

    Zero reference level isinfinitely far from theearth

    r

    mMGPE E

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    Escape Speed

    The escape speed is the speed needed for an objectto soar off into space and not return

    For the earth, vesc is about 11.2 km/s

    Note, v is independent of the mass of the object

    E

    Eesc

    R

    GMv

    2

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    Keplers Laws

    All planets move in elliptical orbits withthe Sun at one of the focal points.

    A line drawn from the Sun to any planet

    sweeps out equal areas in equal timeintervals.

    The square of the orbital period of any

    planet is proportional to cube of theaverage distance from the Sun to theplanet.

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    Keplers Laws, cont.

    Based on observations made by Brahe Newton later demonstrated that these laws

    were consequences of the gravitational force

    between any two objects together withNewtons laws of motion

    K l Fi L

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    Keplers First Law

    All planets move inelliptical orbits withthe Sun at onefocus.

    Any object bound toanother by aninverse square lawwill move in anelliptical path

    Second focus isempty

    K l S d L

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    Keplers Second Law

    A line drawn from theSun to any planet willsweep out equal areasin equal times

    Area from A to B and C toD are the same

    K l Thi d L

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    Keplers Third Law

    The square of the orbital period of anyplanet is proportional to cube of the averagedistance from the Sun to the planet.

    For orbit around the Sun, KS = 2.97x10-19 s2/m3

    K is independent of the mass of the planet

    32KrT

    K l Thi d L li ti

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    Keplers Third Law application

    Mass of the Sun or othercelestial body that hassomething orbiting it

    Assuming a circular orbit

    is a good approximation