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Rotational Kinematics

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Rotational Kinematics

Angular Position q









Degrees and revolutions:

Angular Position q



Arc length s,

measured in radians:





s

q

r



q (radians)  q (degrees)  /180  q (rev) 2

Angular Velocity w

Sign of w

A small sphere attached to a light rigid rod rotates about an axis

perpendicular to and fixed to the other end of the rod. Relative to

the positive direction of the axis of rotation, the angular positions

of the sphere are negative, its angular velocity is negative, and its

angular acceleration is negative. The sphere is





1. rotating clockwise and

slowing down. 71%

2. rotating counterclockwise

and slowing down.

3. rotating clockwise and

speeding up.

4. rotating counterclockwise

and speeding up.

5. first rotating

counterclockwise and then 10% 10% 10%

clockwise.

0%



1 2 3 4 5

A small sphere attached to a light rigid rod rotates about an axis

perpendicular to and fixed to the other end of the rod. Relative to

the positive direction of the axis of rotation, the angular positions

of the sphere are negative, its angular velocity is negative, and its

angular acceleration is negative. The sphere is





1. rotating clockwise and

slowing down. 71%

2. rotating counterclockwise

and slowing down.

3. rotating clockwise and

speeding up.

4. rotating counterclockwise

and speeding up.

5. first rotating

counterclockwise and then 10% 10% 10%

clockwise.

0%



1 2 3 4 5

The angular speed of the minute

hand of a clock, in rad/s, is

35%

1



1. .

30%

1800

1 25%



2. 60 .





3. .

1



30

4. π.

5. 120π.

5% 5%







1 2 3 4 5

The angular speed of the minute

hand of a clock, in rad/s, is

35%

1



1. .

30%

1800

1 25%



2. 60 .





3. .

1



30

4. π.

5. 120π.

5% 5%







1 2 3 4 5

Connections Between

Linear & Rotational Quantities

Angular Acceleration a

Comparison to 1-D Kinematics



Angular Linear

a  constant a  constant

w  w0  a t v  v0  at

1 1 2

q  q 0  w0 t  a t 2 x  x0  v0t  at

2 2

w 2  w0 2  2a (q  q0 ) v2  v02  2a  x  x0 

And for a point at a distance R from the rotation axis:



x = Rq v = wR a = aR

By convention, q, w, a are positive if they are in the

counterclockwise direction.

Decelerating Windmill

As the wind dies, a windmill that had

been rotating at w = 2.1 rad/s begins to

slow down at a constant angular

acceleration of a = 0.45 rad/s2.

How long does it take for the windmill

to come to a complete stop?









w

a av 

t

w w f  wi (0)  (2.1 rad/s)

t     4.7 s

a av a (0.45 rad/s )

2

The fan blade shown is slowing down.

Which option describes a and w?



48%









24% 24%





1. w>0 and a>0

2. w>0 and a0

4. w0 and a>0

2. w>0 and a0

4. w<0 and a<0 1 2 3 4

Rotational Kinematics









If the angular

acceleration is

constant:

The graphs below show angular velocity as a

function of time. In which one is the magnitude of

the angular acceleration constantly decreasing?









1. a

53%



2. b 42%







3. c

4. d 5%





5. e

0% 0%



1 2 3 4 5

The graphs below show angular velocity as a

function of time. In which one is the magnitude of

the angular acceleration constantly decreasing?









1. a

53%



2. b 42%







3. c

4. d 5%





5. e

0% 0%



1 2 3 4 5

Thrown for a Curve

To throw a curve ball, a pitcher

gives the ball an initial angular

speed of 157.0 rad/s. When the

catcher gloves the ball 0.795 s

later, its angular speed has

decreased (due to air resistance)

to 154.7 rad/s.

(a) What is the ball’s angular acceleration, assuming it to be constant?

(b) How many revolutions does the ball make before being caught?





w  w0  a t

w  w0 (157.0 rad/s)  (154.7 rad/s)

a   3.03 rad/s 2

t (0.795 s)

q  w0t  1 a t 2

2



 (157.0 rad/s)(0.795 s)  1 ( 3.03 rad/s 2 )(0.795 s) 2

2



 123.9 rad  19.7 rev

Wheel of Misfortune

On a certain game show, contestants spin the

wheel when it is their turn. One contestant gives

the wheel an initial angular speed of 3.40 rad/s.

It then rotates through 1.25 revolutions and

comes to rest on BANKRUPT.

(a) Find the wheel’s angular acceleration,

assuming it to be constant.

(b) How long does it take for the wheel to

come to rest?





w 2  w02  2a q

w 2  w02 0  (3.40 rad/s) 2

a   0.736 rad/s 2

2q 2(2 rad/rev)(1.25 rev)

w  w0  a t

w  w0 0  (3.40 rad/s)

t   4.62 s

a (0.736 rad/s )

2

A Rotating Crankshaft

A car’s tachometer indicates the angular velocity w of the crank shaft in rpm. A

car stopped at a traffic light has its engine idling at 500 rpm. When the light turns

green, the crankshaft’s angular velocity speeds up at a constant rate to 2500 rpm

in a time interval of 3.0 s.



How many revolutions does the crankshaft make in this time interval?









wi  500 rpm  (2 rad/rev)/(60 s/min)=52.4 rad/s w f  2500 rpm  5wi  262.0 rad/s



w f  wi (262.0 rad/s  52.4 rad/s)

a   69.9 rad/s 2

t (3.0 s)

q f  qi  wi t  1 a  t 

2

2



1rev

 0  (52.4 rad/s)(3.0 s)  1 (69.9 rad/s 2 )  3.0 s   472 rad   75 rev

2

2

2 rad

Time to Rest

A pulley rotating in the counterclockwise direction is

attached to a mass suspended from a string. The mass

causes the pulley’s angular velocity to decrease with a

constant angular acceleration a = 2.10 rad/s2.

(a) If the pulley’s initial angular velocity is w0 = 5.40

rad/s, how long does it take for the pulley to come to

rest?

(b) Through what angle does the pulley turn during this

time?

(c) If the radius of the pulley is 5.0 cm, through what distance is the mass lifted?



w  w0  a t



t  (w  w0 ) / a  0  (5.40 rad/s) / (2.10 rad/s2 )  2.57 s



q  w0t  1 a t 2

2



 (5.40 rad/s)(2.57 s)  1 ( 2.10 rad/s 2 )(2.57 s) 2  6.94 rad

2





s  q r  6.94rad  5.0 cm  34.7cm

CD Speed

CDs and DVDs turn with a variable w

that keeps the tangential speed vt

constant.

Find the angular speed w and the

frequency that a CD must have in order

to give it a linear speed vt = 1.25 m/s

when the laser beam shines on the disk

(a) at 2.50 cm from its center, and

(b) at 6.00 cm from its center.



vt

w

r

(1.25 m/s) 50.0rad 1rev

r  2.50 cm: w     7.96 rps

(0.0250 m) s 2 rad

(1.25 m/s) 20.8 rad 1rev

r  6.00 cm: w     3.31 rps

(0.0600 m) s 2 rad

Rotational vs. Linear Kinematics

Analogies between linear and rotational kinematics:

Connections Between

Linear & Rotational Quantities

More Connections Between

Linear & Rotational Quantities

This merry-go-round has

both tangential and

centripetal acceleration.



at  ra acp  rw 2  vt2 / r



a  at2  acp

2

Speeding up





  tan 1

acp / at 

The Microhematocrit

Suppose the centrifuge is just starting up, and

that it has an angular speed of 8.00 rad/s and

an angular acceleration of 95.0 rad/s2.

(a) What is the magnitude of the centripetal,

tangential, and total acceleration of the

bottom of a tube?

(b) What angle does the total acceleration

make with the direction of motion?

2

v2  rad 

ac   w 2 r   8.00    9.07cm   580.5 s 2

cm

r  s 



 rad 

aT  a r   95 2   9.07cm   861.7 cm 2

 s  s



a  ac  aT 

2 2

580.5 cm s   861.7 cm s 

2 2 2 2

 1039 cm s 2

a   580.5 cm 

  tan  c

1



 

s2

  34  0.593rad

o



 aT   861.7 s 2 

cm





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