Title: Ch10-1 Angular Position, Displacement, Velocity and Acceleration
1Chapter 10 Rotational Kinematics and Energy
Ch10-1 Angular Position, Displacement, Velocity
and Acceleration Rigid body every point on the
body moves through the same displacement and
rotates through the same angle.
? CCW
2CT1A ladybug sits at the outer edge of a
merry-go-round, and a gentleman bug sits halfway
between her and the axis of rotation. The
merry-go-round makes a complete revolution once
each second. The gentleman bugs angular speed
is A. half the ladybugs. B. the same
as the ladybugs. C. twice the ladybugs. D.
impossible to determine.
3Angular Position
Counterclockwise is positive
4Radians
? s/r (a dimensionless ratio)
5Angular Displacement
6Chapter 10 Rotational Kinematics and Energy
? CCW
Ch2-1 Angular Velocity
Average angular velocity ?av angular
displacement / elapsed time ?av
??/?t Instantaneous angular velocity ? lim
??/?t ?t 0
7P10.9 (p.308)
8Chapter 10 Rotational Kinematics and Energy
? CCW
Ch2-1 Angular Acceleration
Average angular acceleration ?av angular
velocity / elapsed time ?av
??/?t Instantaneous angular acceleration ?
lim ??/?t ?t 0
9Chapter 10 Rotational Kinematics and Energy
? CCW
Ch2-2 Rotational Kinematics
10- CT2 Which equation is correct for the fifth
equation? - ? ?0 ???
- ?2 ?02 ???
- ?2 ?0 ???
- ?2 ?02 2???
11Equations for Constant Acceleration Only
- v v0 at ? ?0 ?t
- vav (v0 v) / 2 ?av (?0 ?) / 2
- x x0 (v0 v) t / 2 ? ?0 (?0 ?) t /
2 - x x0 v0 t at2/2 ? ?0 ?0 t ?t2/2
- v2 v02 2a(x x0) ?2 ?02 2?(? ?0)
- Assuming the initial conditions at t 0
- x x0 and ? ?0
- v v0 and ? ?0
- and a and ? are constant.
12- ? ?0 ?t
- ?av (?0 ?) / 2
- ? ?0 (?0 ?) t / 2
- ? ?0 ?0 t ?t2/2
- ?2 ?02 2?(? ?0)
P10.20 (p.309) P10.22 (p.309)
13Chapter 10 Rotational Kinematics and Energy
Ch2-3 Connections Between Linear and Rotational
Quantities s r? vt r? at r? acp v2/r
14CT3 A ladybug sits at the outer edge of a
merry-go-round, and a gentleman bug sits halfway
between her and the axis of rotation. The
merry-go-round makes a complete revolution once
each second. The gentleman bugs linear speed
is A. half the ladybugs. B. the same
as the ladybugs. C. twice the ladybugs. D.
impossible to determine.
15P10-29 (p.310)
16- CT4 P10.29c The force necessary for Jeffs
centripetal acceleration is exerted by - gravity.
- Jeff.
- the vine.
- air resistance.
17Chapter 10 Rotational Kinematics and Energy
Ch2-4 Rolling Motion v r? if no slipping ? 0
if no friction
18Rolling Without SlippingConstant v and ?d
vt2?r vt (2?/t)r v ?r v recall that ?r
vt
19P10.45 (p.311)
20- CT5 P10.45b If the radius of the tires had been
smaller, the angular acceleration of the tires
would be - greater.
- smaller.
- the same.
21Chapter 10 Rotational Kinematics and Energy
Ch2-5 Rotational Kinetic Energy and Moment of
Inertia For N particles I ?miri2 and K
I?2/2 Recall for translation K mv2/2 Both
translation and rotation K mv2/2 I?2/2
22Kinetic Energy of a Rotating Objectof Arbitrary
ShapeRigid Body of N Particles
23Table 10-1aMoments of Inertia for Uniform, Rigid
Objects of Various Shapes and Total Mass M
24Table 10-1bMoments of Inertia for Uniform, Rigid
Objects of Various Shapes and Total Mass M
25P10.52 (p.311)
26- CT6 P10.52b If the speed of the basketball is
doubled to 2v, the fraction of rotational kinetic
energy will - double.
- halve.
- stay the same.
27Chapter 10 Rotational Kinematics and Energy
Ch2-6 Conservation of Energy WNC ?E with K
mv2/2 I?2/2
28Problem 10-60
P10.60 (p.311)
29- CT7 P10.60b If the radius of the bowling ball
were increased, the final linear speed would - increase.
- decrease.
- stay the same.
30- CT8 In the race between the hoop and solid disk,
which will arrive at the base of the incline
first? - hoop.
- disk.
- neither, it will be a tie.