Title: Chapter 8: Rotational Motion
1Chapter 8 Rotational Motion
2Radians
- 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
10Angular 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
13Angular 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)
14Frequency and Period
- Frequency Revolutions per second
- Period Time for one complete revolution
- f w
- 2p
- T 1
- f
15Converting 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)
20Angular 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)
27Friction 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
29Torque
- 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
30Torque Sign Conventions
Counter-clockwise Torque is positive
Clockwise Torque is negative
31Torque 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
32Torque 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
34Torque 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).
36Torque 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)
40Moment 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?
41Deriving 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
43Moment 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
44Moment 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
45Moment 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?
59Translational 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
61Deriving the Rotational KE
- KE S½ mv2
- v rw
- KE S ½ m(rw)2
- KE S ½ mr2w2
- I S mr2
- KE ½ Iw2
62Calculating 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)
64Law 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
65Rotational 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
70Rotational 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)
77Conservation 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)
79The skater in more detail
- For now, lets just consider the skaters arms
- Arms out (initial) Arms in (final)
80Iiwi 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
81I 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
82Cons. 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
83Cons. 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)
86Vectors 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.
87Merry-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)