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Chapter 8: Rotational Motion

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Title: Chapter 8: Rotational Motion


1
Chapter 8 Rotational Motion
2
Radians
  • 1) 1 radian angle subtended by an arc (l)
    whose length is equal to the radius (r)
  • 2) q l
  • r
  • 3600 2p radians 1 rev
  • Radians are dimensionless

l
r
q
3
  • Convert the following
  • 20o to radians
  • 20o to revolutions
  • 5000o to radians
  • 0.75 rev to radians
  • 0.40 radians to degrees

4
  • A bird can only see objects that subtend an angle
    of 3 X 10-4 rad. How many degrees is that?
  • 3 X 10-4 rad 360o 0.017o
  • 2p rad

5
  • How small an object can the bird distinguish
    flying at a height of 100 m?
  • q l
  • r
  • l q r
  • l (3 X 10-4 rad)(100m)
  • l 0.03 m 3 cm

q
r
l (approx.)
6
  • How at what height would the bird be able to just
    distinguish a rabbit that is 30 cm long (and
    tasty)?
  • (ANS 1000 m)

q
r
l (approx.)
7
  • A tiny laser beam is aimed from the earth to the
    moon (3.8 X 108 m). The beam needs to have a
    diameter of 2.50 m on the moon. What is the
    angle that the beam can have?
  • (6.6 X 10-9 radians)

8
  • Convert
  • 0.0200 rev/s to radians/s (0.126 rad/s)
  • 30.0o/s to radians/s (0.534 rad/s)
  • 1.40 rad/s to rev/s (0.223 rev/s)
  • 3000 rpm to radians/s (314 rad/s)

9
  • The Mighty Thor swings his hammer at 400 rev/min.
    Express this in radians/s.
  • 400 rev 1 min 2p rad
  • 1 min 60 s 1 rev
  • 13.3p rad/s or
  • 41.9 rad/s

10
Angular Velocity
  • v Dx w Dq
  • Dt Dt
  • Angular Velocity radians an object rotates per
    second
  • All points on an object rotate at the EXACT same
    angular velocity
  • All points on an object DO NOT rotate with the
    same linear speed. (the farther out the faster)

11
  • Merry-Go-Round Example
  • wa wb
  • (both rotate through 3600 in the same time
    period)
  • va lt vb
  • (Point b travels a longer distance around the
    circle)

vb
va
a
b
12
  • If a person at point b flies off the
    merry-go-round, will they travel in a curve or
    straight line?

b
13
Angular Acceleration
  • a Dv a Dw
  • Dt Dt
  • The angular acceleration of all points on a
    circle is the same.
  • All points on an object DO NOT experience the
    same linear acceleration. (the farther out the
    more acceleration)

14
Frequency and Period
  • Frequency Revolutions per second
  • Period Time for one complete revolution
  • f w
  • 2p
  • T 1
  • f

15
Converting between Angular and Linear Quantities
atan
  • Linear Radius X Angular
  • v rw
  • atan ra
  • Note the use of atan to differentiate from
    centripetal acceleration, ac or ar

ar
16
  • One child rides a merry-go-round (2 revolutions
    per minute) on an inside lion 2.0 m from the
    center. A second child rides an outside horse,
    3.0 m from the center.
  • Calculate the angular velocity in rad/s. (0.209
    rad/s)
  • Calculate the frequency and the period. (0.0333
    Hz, 30 s)
  • Calculate the linear velocity of each rider.
    (0.419 m/s, 0.628 m/s)
  • Who has a higher angular velocity?

17
  • A clock has a seconds hand that is 7.00 cm long.
  • Calculate the angular velocity of the second hand
    in radians/s. (0.105 rad/s)
  • Calculate the frequency and period. (0.0167 Hz,
    60 s)
  • Calculate the angular velocity in degrees/s.
    (6o/s)
  • Calculate the linear velocity at the end of the
    seconds hand. (7.35 X 10-3 m/s)

18
  • A baseball bat is found to have a linear
    acceleration of 13.9 m/s2 at the sweet spot.
    The sweet spot is at 59 cm from the handle.
  • Calculate the angular acceleration in rad/s2 (a
    23.6 rad/s2)
  • Convert the angular acceleration to rev/s2 (3.75
    rev/s2)

19
  • A golf club has an angular acceleration of 20.0
    rad/s2 and is 114 cm long.
  • Calculate the tangential acceleration of the
    club. (22.8 m/s2)
  • Convert the angular acceleration to rev/s2.
    (3.18 rev/s2)
  • Calculate the force the club could give to a
    45.93 g golf ball. (1.05 N)
  • Calculate the velocity of the ball if the club is
    in contact with the ball for 50 cm. (4.77 m/s)

20
Angular Kinematics
  • vvo at wwo at
  • x vot ½ at2 q wot ½ at2
  • v2 vo2 2ax w2 wo2 2aq

21
  • A bike wheel starts at 2.0 rad/s. The cyclist
    accelerates at 3.5 rad/s2 for the next 2.0 s.
  • Calculate the wheels new angular speed (9.0
    rad/s)
  • Calculate the number of revolutions. (1.75)

22
  • A DVD rotates from rest to 31.4 rad/s in 0.892 s.
  • Calculate the angular acceleration. (35.2 rad/s2
    )
  • How many revolutions did it make? (2.23)
  • If the radius of the disc is 4.45 cm, find the
    linear speed of a point on the outside edge of
    the disc. (1.40 m/s)

23
  • A bicycle slows from vo 8.4 m/s to rest over a
    distance of 115 m. The diameter of each wheel is
    68.0 cm.
  • Calculate the angular velocity of the wheels
    before braking starts. (24.7 rad/s)
  • How many revolutions did each wheel undergo?
    (HINT calculate the circumference of the circle
    first) (53.8 rev)
  • Calculate the angular acceleration. (-0.903
    rad/s2)
  • Calculate the time it took the bike to stop (27.4
    s)

24
  • A spinning bike tire of radius 33.0 cm has an
    angular velocity of 50.0 rad/s. Twenty seconds
    later, its angular speed is 150.0 rad/s.
  • Calculate the angular acceleration. (5.00
    rad/s2)
  • Calculate the angular displacement over the 20 s.
    (2000 radians)
  • Calculate the revolutions travelled in the 20 s
    (318 rev)
  • Calculate the linear distance the tire travelled
    in 20 s. (660 m)

25
  • A pottery wheel turning with an angular speed of
    30.0 rev/s is brought to rest in 60.0
    revolutions.
  • Calculate the radians that the wheel travelled
    (377 rad)
  • Calculate the angular acceleration. (-47.1
    rad/s2)
  • Calculate the time required to stop. (4.00 s)
  • If the radius of the wheel is 12.0 cm, calculate
    the linear distance the outside of the wheel
    travelled. (45.2 m)

26
  • A game show wheel with a 90 cm radius is
    initially turning at 3.0 rev/s. A point on the
    outside of the wheel travels 147 meters before
    stopping.
  • Calculate how many revolutions it when through.
    (26 rev)
  • Calculate the angular deceleration. (1.09
    rad/s2)
  • Calculate how long it took to stop. (17.3 s)
  • Calculate the initial linear speed and linear
    acceleration on the outside of the wheel (17.0
    m/s, 0.98 m/s2)
  • Calculate the initial centripetal acceleration on
    a point at the edge of the wheel. (319 m/s2)

27
Friction and Rolling Wheels
  • Rolling uses static friction
  • A new part of the wheel/tire is coming in contact
    with the road every instant

B
A
28
  • Braking uses kinetic friction

Point A gets drug across the surface
A
29
Torque
  • Torque tendency of a force to rotate a body
    about some axis (the force is always
    perpendicular to the lever arm)
  • t Fr

r
pivot
F
30
Torque Sign Conventions
Counter-clockwise Torque is positive
Clockwise Torque is negative
31
Torque Example 1
  • A wrench is 20.0 cm long and a 200.0 N force is
    applied perpendicularly to the end. Calculate
    the torque.
  • t Fr
  • t (200.0 N)(0.20 m)
  • t 40.0 m-N

20.0 cm
200.0 N
32
Torque Example 2
  • Suppose that same 200.0 N force is now applied at
    a 60o angle as shown. Calculate the Torque. Is
    it greater or less?

20.0 cm
200.0 N
60o
33
  • First we need to resolve the Force vector into x
    and y components
  • Only Fy has any effect on the torque
    (perpendicular)
  • Fy Fsinq (200.0 N)(sin 60o) 173.2 N
  • t Fr (173.2 N)(0.20 m) 34.6 m-N

200.0 N
Fy
60o
Fx
34
Torque Example 3
  • The biceps muscle exerts a 700 N vertical force.
    Calculate the torque about the elbow.
  • Fr (700 N)(0.050 m)
  • 35 m-N

35
  • A force of 200 N acts tangentially on the rim of
    a wheel 25 cm in radius.
  • Calculate the torque.
  • Calculate the torque if the force makes an angle
    of 40o to a spoke of the wheel.
  • If the wheel is mounted vertically, draw a free
    body diagram of the wheel if the force is the one
    in (a).

36
Torque Example 4
  • Two wheels, of radii r1 30 cm and r2 50 cm
    are connected as shown. Calculate the net
    torque on this compound wheel when two 50 N force
    act as shown.

50 N
30o
r2
Note that Fx will pull the wheel
r1
50 N
37
  • First find the horizontal component of the top
    force
  • Fx (50 N)(cos 30o) 43 N
  • The top force is pulling clockwise (-) and the
    bottom force pulls counterclockwise ()
  • St F1r1 F2r2
  • St (50N)(0.30m) (43 N)(0.50 m) -6.5 m-N

38
  • Two children push on a merry-go-round as shown.
    Calculate the net torque on the merry-go-round if
    the radius is 2.0 m.
  • (1800 m N)

39
  • A 60.0 cm diameter wheel is pulled by a 500.0 N
    force.  The force acts at an angle of 65.0o with
    respect to the spoke.  Assume that a frictional
    force of 300.0 N opposes this force at a radius
    of 2.00 cm.  Calculate the net torque on the
    wheel. (130.0 Nm)

40
Moment of Inertia (I)
  • Measure of Rotational Inertia
  • An objects resistance to a change in angular
    velocity
  • Would it be harder to push a child on a
    playground merry-go-round or a carousel?

41
Deriving I
  • Consider pushing a mass around in a circle (like
    the child on a merry-go-round)
  • F ma t Fr
  • a ra t mrar
  • F mra t mr2a

F
r
m
42
  • I moment of inertia
  • I mr2
  • More properly
  • I Smr2 m1r12 m2r22 .
  • St Ia
  • Would it be harder (require more torque) to twirl
    a barbell in the middle (pt. M) or the end (Pt. E)

E
M
43
Moment of Inertia Example 1
  • Calculate the moment of inertia (I) for the
    barbell when rotated about point M. We will
    assume the barbell is 1.0 m long, and that each
    weight is a point mass of 45.4 kg.
  • I Smr2 (45.4 kg)(0.50 m)2 (45.4 kg)(0.50
    m)2
  • I 22.7 kg-m2

M
44
Moment of Inertia Example 2
  • Now calculate I assuming Mr. Fredericks uses his
    massive musculature to twirl the barbells from
    point E.
  • I Smr2 (45.4 kg)(0 m)2 (45.4 kg)(1 m)2
  • I 45.4 kg-m2

E
45
Moment of Inertia Example 3
  • Calculate I for Bouncing Boy (75 kg, radius 1.2
    m). Use the formulas from the book.
  • I 2/5 MR2
  • I (2)(75 kg)(1.2 m)2
  • 5
  • I 43.2 kg-m2

46
  • Calculate the moment of inertia of an 8.00 kg
    solid wheel with a radius of 25.0 cm.

47
  • A wheel has a moment of inertia of 0.50 kg m2.
  • Calculate the torque (St Ia) is required to give
    it an acceleration of 3 rad/s2. (1.5 mN)
  • Calculate its angular speed (from rest) after
    5.00 s. (15 rad/s)
  • Calculate the number of revolutions it goes
    through in 5.00 s. (37.5 rad, 5.97 rev)

48
  • A 15.0 N force is applied to a cord wrapped
    around a pulley of radius 33.0 cm. The pulley
    reaches an angular speed (w) of 30.0 rad/s in
    3.00 s.
  • Calculate the angular acceleration. (10.0 rad/s2)
  • Calculate the torque (4.95 m-N)
  • Calculate the moment of inertia of the pulley.
    (0.495 kg-m2)

33.0 cm
15.0 N
49
  • A 25.0 kg wheel has a radius of 40.0 cm. A 1.20
    kg mass is hung on the end of the wheel by a
    string and falls freely.
  • Calculate the moment of inertia of the wheel. (2
    kg m2)
  • Calculate the torque on the pulley. (4.70 mN)
  • Calculate the angular acceleration of the wheel.
    (2.35 rad/s2)
  • Calculate the tangential acceleration of the
    wheel (and bucket) (0.94 m/s2)
  • Calculate the tension in the string. (10.6 N)

50
  • A 15.0 N force is applied to a cord wrapped
    around a pulley of radius 33.0 cm. The pulley
    reaches an angular speed (w) of 30.0 rad/s in
    3.00 s. Since this is a real pulley, there is a
    frictional torque (tfr 1.10 m-N) opposing
    rotation.
  • Calculate net torque on the pulley. (3.85 m-N)
  • Calculate the moment of inertia of the pulley.
    (0.385 kg-m2)

33.0 cm
15.0 N
51
  • Using the same pulley as the previous problem
    (I0.385 kg m2), hang a 15.0 N bucket (1.53 kg)
    from the cord. There is a frictional torque of
    1.10 m-N opposing rotation. Calculate the
    angular and linear acceleration of the bucket.
    Also calculate FT.

33.0 cm
FT
52
  • We will break this problem into two parts
    pulley and bucket. Lets first look at the
    pulley
  • St FTr tfr
  • St Ia
  • Ia FTr tfr
  • (0.385)a FT(0.33) 1.10

tfr
33.0 cm
FT
53
  • Now we will deal with the bucket
  • SF mg FT
  • ma mg FT
  • 1.53a 15 FT
  • a ra
  • 1.53ra 15 FT
  • (1.53)(0.33)a 15 FT
  • 0.505a 15 FT
  • 0.385a 0.33FT 1.10
  • a 7.07 rad/s2, a 2.33 m/s2, FT 11.5 N

FT
mg
54
  • Now calculate the rotational speed of the pully
    (w) and the linear speed of the bucket after 3.00
    s.
  • wwo at
  • w 0 at (6.98 rad/s2)(3.00 s) 20.9 rad/s
  • vrw
  • v (0.330 m)(20.9 rad/s) 6.90 m/s

55
  • A 2.00 kg bucket is attached to a 1.00 kg, 4.00
    cm radius cylindrical pulley. The bucket is
    suspended 2.00 m above the floor.
  • Calculate the moment of inertia of the cylinder
    (1/2 MR2) (8X10-4 kgm2)
  • Calculate the acceleration of the bucket. (7.84
    m/s2)
  • Calculate the angular acceleration of the pulley.
    (196 rad/s2)
  • Calculate how long it takes to reach the floor.
    (0.714 s)

4.00 cm
FT
56
  • a) I 1/2 MR2 (1/2)(1.00 kg)(0.04 m)2
  • I 8 X 10-4 kgm2
  • Bucket Pulley
  • ma mg FT t FTR
  • 2a (2)(9.8) FT Ia FTR
  • 2a 19.6 FT a aR
  • Ia/R FTR
  • 8 X 10-4 a FT(0.04)
  • 0.04
  • a -7.84 m/s2

57
  • a aR
  • a a/R 7.84/0.04 196 rad/s2
  • y yo vt ½at2
  • y ½ at2
  • t v(2y/a) 0.714 s

58
  • A 1000 kg elevator is suspended by a 100 kg
    cylinder pulley of radius 50.0 cm.
  • Calculate the moment of inertia of the pulley.
    (12.5 kgm2)
  • Calculate the linear acceleration if the elevator
    drops. (9.33 m/s2)
  • Calculate the angular acceleration of the
    elevator. (18.7 rad/s2)
  • Calculate the tension in the cord. (470 N)
  • Are you glad you are not in the elevator?

59
Translational and Rotational Energy
  • Does a rotating helicopter blade have kinetic
    energy before the helicopter takes off?
  • How about afterwards?
  • Does all of the energy of the fuel go into moving
    the helicopter?

60
  • Translational Speed (v)
  • speed of the center of a wheel with respect to
    the ground
  • Can also be called linear speed
  • Use regular KE ½ mv2
  • Rotational speed (w)
  • angular speed of the wheel
  • Use KE ½ Iw2

61
Deriving the Rotational KE
  • KE S½ mv2
  • v rw
  • KE S ½ m(rw)2
  • KE S ½ mr2w2
  • I S mr2
  • KE ½ Iw2

62
Calculating Work
  • A pottery wheel of I 0.200 kgm2 is accelerated
    from rest to 500 rpm.
  • Calculate the final angular velocity in rad/s.
    (52.4 rad/s)
  • Calculate the change in kinetic energy (274 J)
  • How much work is done in the process (274 J)
  • If the wheel takes 30 seconds to get up to speed,
    calculate the angular acceleration (1.75 rad/s2)

63
  • Jupiter has a mass of 1.9 X 1027 kg and a radius
    of 7.0 X 107 m. Its day is only 9.92 hours long.
  • Calculate Jupiters moment of inertia, treating
    it as a sphere. (3.72 X 1042 kgm2)
  • Calculate Jupiters rotational speed in rad/s.
    (1.76 X 10-4 rad/s)
  • Calculate Jupiters kinetic energy of rotation.
    (5.76 X 1034 J)
  • Jupiter is 7.78 X 1011 m from the sun. Calculate
    Jupiters moment of inertia, assuming it is a
    point mass from the sun. (1.15 X 1051 kgm2)
  • Calculate Jupiters orbital speed around the sun
    if it takes11.9 year to orbit the sun. (1.67 X
    10-8 rad/s)
  • Calculate the kinetic energy about the sun. (1.60
    X 1035 J)

64
Law of Conservation of Mechanical Energy
  • (KEt KEr PEt)i (KEt KEr PEt)f
  • When using this equation, we will ignore
    friction.
  • Also the work done in rotating object is
  • W tDq

65
Rotational KE Example 1
  • What will be the translational speed of a log
    (100 kg, radius 0.25 m, I ½ mr2) as it rolls
    down a 4 m ramp from rest?

4 m
66
  • Calculate I
  • I ½ mr2 (1/2)(100 kg)(0.25m)2
  • I 3.125 kgm2
  • Law of Conservation of Energy
  • (KEt KEr PEt)i (KEt KEr PEt)f
  • (0 0 mgy)i ( ½ mv2 ½ Iw2 0)f
  • mgy ½ mv2 ½ Iw2
  • 3920 50v2 1.56w2
  • v wr w v/r w2 v2/r2
  • 3920 50v2 1.56v2/(0.25m)2
  • 3920 75v2 v 7.2 m/s

67
  • (KEt KEr PEt)i (KEt KEr PEt)f
  • (0 0 mgy)i ( ½ mv2 ½ Iw2 0)f
  • mgy ½ mv2 ½ Iw2
  • 2mgy mv2 Iw2 (multiplied both sides by 2)
  • v rw so w v/r
  • 2mgy mv2 Iv2
  • r2
  • I 1/2 mr2
  • 2mgy mv2 1mr2v2
  • 2r2

68
  • 2mgy mv2 1mr2v2
  • 2r2
  • 2gy v2 1v2
  • 2
  • 2gy 2v2 1v2
  • 2 2
  • 2gy 3v2
  • 2
  • v 4gy 4(9.8m/s2)(4.00 m) 7.23 m/s
  • 3 3

69
  • Now we can calculate the angular speed
  • v rw so w v/r
  • 7.23 m/s 29 rad/s
  • 0.25 m
  • 29 rad 1 rev 4.6 rev/s
  • s 2p rad

70
Rotational KE Example 2
  • What will be the translational speed of Bouncing
    Boy (75 kg, radius 1.2 m) as he rolls down a 3
    m ramp from rest? (Treat him as a sphere)

3 m
71
  • (KEt KEr PEt)i (KEt KEr PEt)f
  • (0 0 mgy)i ( ½ mv2 ½ Iw2 0)f
  • mgy ½ mv2 ½ Iw2
  • 2mgy mv2 Iw2 (multiplied both sides by 2)
  • v rw so w v/r
  • 2mgy mv2 Iv2
  • r2
  • I 2/5 mr2
  • 2mgy mv2 2mr2v2
  • 5r2

72
  • 2mgy mv2 2mr2v2
  • 5r2
  • 2gy v2 2v2
  • 5
  • 2gy 5v2 2v2
  • 5 5
  • 2gy 7v2
  • 5
  • v 10gy 10(9.8m/s2)(3.00 m) 6.50
    m/s
  • 7 7

73
  • Now we can calculate the angular speed
  • v rw so w v/r
  • 6.50 m/s 5.4 rad/s
  • 1.2 m
  • 5.4 rad 1 rev 0.86 rev/s
  • s 2p rad

74
  • What would his speed be if he just slid down the
    ramp?
  • (KEt KEr PEt)i (KEt KEr PEt)f
  • (0 0 mgy)i ( ½ mv2 0 0)f
  • mgy ½ mv2
  • gy ½ v2
  • v2 2gy
  • v \/2gy (2 X 9.8 m/s X 3.00 m)1/2
  • v 7.7 m/s
  • Why is this larger than if he rolls?

75
  • A wooden dowel (mass 0.50 kg, r 1.00 cm)
    rolls down a 1.25 m tall ramp.
  • Calculate the moment of inertia (2.5 X 10-5
    kgm2)
  • Calculate the linear speed at the bottom. (4.04
    m/s)
  • Calculate the angular speed at the bottom. (404
    rad/s, 64.3 rev/s)

76
  • A bike tire can be modeled as a thin hoop
    (Imr2). The wheel has a diameter of 66.0 cm and
    a mass of 2.00 kg. The wheel is allowed to roll
    down a ramp and has a linear (translational)
    speed of 2.00 m/s at the bottom of the ramp.
  • Calculate the moment of inertia of the wheel.
    (0.218 kgm2)
  • Calculate the height of the ramp (40.8 cm)

77
Conservation of Angular Momentum
  • The total angular momentum of a rotating body
    remains constant if the net torque acting on it
    is zero
  • Angular Momentum (L) is conserved
  • p mv (linear momentum)
  • L Iw (angular momentum)
  • Iiwi Ifwf

78
(No Transcript)
79
The skater in more detail
  • For now, lets just consider the skaters arms
  • Arms out (initial) Arms in (final)

80
Iiwi Ifwf I mr2 Her mass will not change
when she moves her arms mri2wi
mrf2wf ri2wi rf2wf Since rf will be smaller
(arms are in) wf must increase to compensate
81
I wanna go fast!
  • A child sits on a merry-go-round at point A. If
    the child wants to go faster, should he walk
    towards the center or the outside?

A
82
Cons. of Angular Momentum Ex. 1
  • A skater holds her arms at a length of 56 cm.
    She spins at 9.43 rad/s. What will be her new
    speed if she pulls her arms tight to her body, 20
    cm?
  • Iiwi Ifwf
  • I mr2
  • mri2wi mrf2wf
  • ri2wi rf2wf
  • wf ri2wi /rf2
  • wf (0.56 m)2(9.43 rad/s)/(0.20 m)2 74 rad/s

83
Cons. of Angular Momentum Example 2
  • A mass m is attached to the end of a string which
    passes through a hole in a table. Initially the
    r1 is 0.80 m and the block moves at 2.4 m/s.
    What will be the new speed as the radius of the
    string is reduced to 0.48 m?

84
  • Iiwi Ifwf
  • I mr2
  • mri2wi mrf2wf
  • ri2wi rf2wf
  • v rw so w v/r
  • ri2vi rf2vf
  • ri rf
  • rivi rfvf
  • vf rivi (0.80m)(2.4 m/s) 4.0 m/s
  • rf (0.48 m)

85
  • Old record players rotate at 33.3 rev/min.
    Assume a record has a radius of 15.24 cm and a
    mass of 100.0 grams.
  • Calculate the angular speed in rad/s (3.49
    rad/s)
  • Calculate the moment of inertia. (1/2 mr2) (1.16
    X 10-3 kgm2)
  • Calculate angular momentum of the record. (4.05 X
    10-3 kg m2/s)
  • A second record drops on top of the first.
    Calculate the new moment of inertia and new
    angular speed. (2.32 X 10-3 kg m2, 1.74 rad/s)

86
Vectors and Angular Momentum
  • Direction of the vector w is defined by the
    right-hand rule.
  • L Iw
  • L is defined as going in the same direction.

87
Merry-Go-Round
  • What will happen if you start to walk on a still
    merry-go-round? Can you walk around it without
    it moving?

88
  • Assume this merry-go-round is initially at rest
    (Ltotal 0)
  • As the man walks counter-clockwise, the platform
    spins counterclockwise
  • Total Angular Momentum is still zero.

89
  • What will happen if the student flips the bicycle
    wheel while standing on the merry-go-round?

90
  • A merry-go-round (500 kg) has a radius of 1.5 m.
    A 40.0 kg student is sitting on the
    merry-go-round as it spins at 30.0 rev/min.
  • Calculate the angular speed (3.14 rad/s)
  • Calculate the moment of inertia of the
    merry-go-round and student, assuming she sits at
    the edge. (652.5 kg m2)
  • Calculate the angular momentum. (2049 kgm2/s)
  • A second student (80.0 kg) now jumps on the
    merry-go-round. Calculate the new moment of
    inertia and angular speed. (832.5 kgm2, 2.46
    rad/s)

91
  • 2. RSun 6.5 X 105 km
  • 4. 2900 m
  • 6. 188 rad/s
  • 8. 1.9 rad/s2
  • 10. -260 rad/s2
  • 12. 3300 revolutions
  • 14. a) 1.99 X 10-7 rad/s b) 7.27 X 10-5 rad/s
  • 16. 3.6 X 104 rpm
  • 0.56 rad/s2
  • 22. a) -84 rad/s2 b) 150 rev
  • 24. 38 m

92
  • 22. a) -84 rad/s2 b) 150 rev
  • 24. 38 m
  • 26. a) 0.58 rad/s2 b) 12 s
  • 30. a) 38 m N b) 33 m N
  • 32. 650 m N
  • 34. 1.89 kg m2
  • 36. a) 6.1 kg m2 b) 0.61 kg m2
  • 38. a) 0.851 kg m2 b) 0.0720 m N
  • 1.99 X 10-3 kg m2 b) 0.0682 m N
  • 590 m N, 240 N
  • 46. 2250 kg m2, 8800 mN

93
  • 42. 590 m N, 240 N
  • 44. a) 7.5 m N b) 300 N
  • 46. 2250 kg m2, 8800 mN
  • 50. 94 J
  • 52. a) 2.6 X 1029 J b) 2.7 X 1033 J
  • a) 8.37 m/s, 41.8 rad/s b) 2.50 (mass
    independent)

94
  • 58. a) angular momentum conserved b) 1.6
  • 60. 0.77 kg m2 (pull arms close to body)
  • 62. a) 14 kg m2/s b) -2.7 m N
  • 66.a) 1.2 rad/s b) 2000 J, 1200 J (loss of
    800J, 40 loss)
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