


Frequency and Period
You’ve encountered frequency and period when dealing with
springs and simple harmonic motion, and you will encounter them
again in the chapter on waves. These terms are also relevant to
rotational motion, and SAT II Physics has been known to test the
relation between angular velocity and angular frequency and period.
Angular Frequency
Angular frequency, f,
is defined as the number of circular revolutions in a given time
interval. It is commonly measured in units of Hertz (Hz), where 1 Hz
= 1 s^{–1}. For example, the second
hand on a clock completes one revolution every 60 seconds
and therefore has an angular frequency of ^{1}
/_{60} Hz.
The relationship between frequency and angular velocity
is:
For example, the second hand of a clock has an angular
velocity of s. Plugging that value into the equation
above, we get
which we already determined to be the frequency of the
second hand of a clock.
Angular Period
Angular period, T,
is defined as the time required to complete one revolution and is
related to frequency by the equation:
Since we know that the frequency of the second hand is
^{1}/_{60} Hz,
we can quickly see that the period of the second hand is 60 s.
It takes 60 seconds for the second hand to complete
a revolution, so the period of the second hand is 60 seconds.
Period and angular velocity are related by the equation
Example

The question tells us that the Earth has a period of T = 365.25 days.
If we plug this value into the equation relating period and angular
velocity, we find:
Note, however, that this equation only gives us the Earth’s
angular velocity in terms of radians per day. In terms of radians
per second, the correct answer is:
Relation of Angular Variables to Linear Variables
At any given moment, a rotating particle has an instantaneous
linear velocity and an instantaneous linear acceleration. For instance,
a particle P that is rotating counterclockwise
will have an instantaneous velocity in the positive y direction
at the moment it is at the positive xaxis. In
general, a rotating particle has an instantaneous velocity that
is tangent to the circle described by its rotation and an instantaneous
acceleration that points toward the center of the circle.
On SAT II Physics, you may be called upon to determine
a particle’s linear velocity or acceleration given its angular velocity
or acceleration, or vice versa. Let’s take a look at how this is
done.
Distance
We saw earlier that the angular position, , of a rotating particle is related to the
length of the arc, l, between the
particle’s present position and the positive xaxis
by the equation = l/r,
or l = r. Similarly,
for any angular displacement, , we can say that the
length, l, of the arc made by a particle
undergoing that displacement is
Note that the length of the arc gives us a particle’s
distance traveled rather than its displacement, since displacement
is a vector quantity measuring only the straightline distance between
two points, and not the length of the route traveled between those
two points.
Velocity and Acceleration
Given the relationship we have determined between arc
distance traveled, l, and angular displacement, , we can now find expressions to relate
linear and angular velocity and acceleration.
We can express the instantaneous linear velocity of a
rotating particle as v = l/t, where l is
the distance traveled along the arc. From this formula, we can derive
a formula relating linear and angular velocity:
In turn, we can express linear acceleration as a
= v/t, giving us this formula relating linear and
angular acceleration:
Example

We know that the period of the Earth’s rotation is 24 hours,
or seconds. From the equation relating period, T,
to angular velocity, , we can find the angular
velocity of the Earth:
Now that we know the Earth’s angular velocity, we simply
plug that value into the equation for linear velocity:
They may not notice it, but people living at the equator
are moving faster than the speed of sound.
Equations of Rotational Kinematics
In Chapter 2 we defined the kinematic equations for bodies
moving at constant acceleration. As we have seen, there are very
clear rotational counterparts for linear displacement, velocity,
and acceleration, so we are able to develop an analogous set of
five equations for solving problems in rotational kinematics:
In these equations, is the object’s initial
angular velocity at its initial position, .
Any questions on SAT II Physics that call upon your knowledge
of the kinematic equations will almost certainly be of the translational
variety. However, it’s worth noting just how deep the parallels
between translational and rotational kinematics run.
Vector Notation of Rotational Variables
Angular velocity and angular acceleration are vector quantities;
the equations above define their magnitudes but not their directions.
Given that objects with angular velocity or acceleration are moving
in a circle, how do we determine the direction of the vector? It
may seem strange, but the direction of the vector for angular velocity
or acceleration is actually perpendicular to the plane in which
the object is rotating.
We determine the direction of the angular velocity vector
using the righthand rule. Take your right hand and
curl your fingers along the path of the rotating particle or body.
Your thumb then points in the direction of the angular velocity
of the body. Note that the angular velocity is along the body’s
axis of rotation.
The figure below illustrates a top spinning counterclockwise
on a table. The righthand rule shows that its angular velocity
is in the upward direction. Note that if the top were rotating clockwise,
then its angular velocity would be in the downward direction.
To find the direction of a rigid body’s angular acceleration,
you must first find the direction of the body’s angular velocity.
Then, if the magnitude of the angular velocity is increasing, the
angular acceleration is in the same direction as the angular velocity
vector. On the other hand, if the magnitude of the angular velocity
is decreasing, then the angular acceleration points in the direction
opposite the angular velocity vector.
