Transcript Physics_U8

Unit 8:
Circular Motion
Section A: Angular Units
Corresponding Textbook Sections:
– 10.1
PA Assessment Anchors:
– S11.C.3.1
Angular Position
Defined as the angle, , that a line from
the axle to a spot on the wheel makes
with a reference line
Unit: Radian (rad)
[dimensionless]
Sign convention for angular
position:
If  > 0, counterclockwise rotation
If  < 0, clockwise rotation
Converting between degrees
and radians
1 revolution = 360 = 2 rad
1 rad = 57.3
Convert the same way you would
between any other units.
Section B:
Angular / Linear Relationships
Corresponding Textbook Sections:
– 10.3
PA Assessment Anchors:
– S11.C.3.1
Arc Length
The arc length is the distance from a
reference line to a spot of interest on a
circle.
Equation:
s = r
Angular Velocity
Symbol: 

 av 
t
Units: s-1 or 1/s
Sign Convention for 
If  > 0
Counterclockwise rotation
If  < 0
Clockwise rotation
Practice Problem #1
An old phonograph rotates clockwise at
33⅓ rpm. What is the angular velocity
in rad/s?
Practice Problem #2
If a CD rotates at 22 rad/s, what is its
angular speed in rpm?
Period
The period is the time it takes to
complete one revolution.
Units: seconds (s)
T
2

Practice Problem #3
Find the period of a record that is
rotating at 45 rpm.
Angular Acceleration
The change in angular speed of a
rotating object per unit of time.
Units: rad/s2


t
Practice Problem #4
As the wind dies, a windmill that was
rotating at 2.1 rad/s begins to slow
down with a constant angular
acceleration of 0.45 rad/s2. How long
does it take for the windmill to come to a
complete stop?
Section C:
Angular Kinematics
Corresponding Textbook Sections:
– 10.2
PA Assessment Anchors:
– S11.C.3.1
Relationship between angular
and linear quantities
Linear Quantity
Angular Quantity
x

v
ω
a
α
Based on these relationships, we can rewrite the
kinematics equations from 1-D and 2-D Kinematics
Angular Kinematics Equations
v  v o  at
 =  o  t
1 2
x  x o  v o t  at
2
1 2
 =  o   o t  t
2
v  v  2ax
    2
2
2
o
2
2
o
So, basically…
These are just variations of equations
we already know how to use.
They work the same way as the linear
equations.
We’ll use the same setup as before:
• Data table, equation, picture, etc…
Practice Problem #1
To throw a curveball, a pitcher gives the
ball an initial angular speed of 36 rad/s.
When the catcher gloves the ball 0.595
s later, its angular speed has decreased
to 34.2 rad/s. What is the ball’s angular
acceleration?
Practice Problem #2
Based on the last problem, how many
revolutions does the ball make before
being caught?
Practice Problem #2
Refer to Example 10-2 on page 280
Section D:
Torque
Corresponding Textbook Sections:
– 11.1, 11.2
PA Assessment Anchors:
– S11.C.3.1
What is Torque?
Torque is the rotational equivalent of
force
It depends on:
– Force applied
– Distance from the force to the axis of
rotation

More on Torque…
Equation:
  rF
Greek Letter “tau”
Units: Nm
Axis of Rotation
(where it turns)
Practice Problem #1
If the minimum required torque to open
a door is 3.1 Nm, what force must be
applied if:
– r = 0.94 m
– r = 0.35 m
Section E:
Moment of Inertia
Corresponding Textbook Sections:
– 10.5
PA Assessment Anchors:
– S11.C.3.1
What is “Moment of Inertia”?
The “rotational mass” of an object
– Rotational mass depends on actual mass,
radius, and distribution of mass
Useful for determining rotational KE:
1 2
KE  I
2
Moment of inertia
Practice Problem #1
What is the moment of inertia of a
hollow sphere with mass of 40 kg and
radius of 3 m?
Practice Problem #2
A grindstone with radius of 0.61 m is
being used to sharpen an axe. If the
linear speed of the stone relative to the
ax is 1.5 m/s, and the stones rotational
KE is 13 J, what is its moment of
inertia?