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No Fear Translations of Shakespeare’s plays (along with audio!) and other classic works
Flashcards
Mastery Quizzes
Infographics
Graphic Novels
AP® Test Prep PLUS
AP® Practice & Lessons
My PLUS Activity
Note-taking
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Teaching Shakespeare to today's generation can be challenging. No Fear helps a ton with
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Testimonials from SparkNotes Customers
No Fear provides access to Shakespeare for students who normally couldn’t (or wouldn’t) read his plays. It’s also a very useful tool when trying to explain Shakespeare’s wordplay!
Erika M.
I tutor high school students in a variety of subjects. Having access to the literature translations helps me to stay informed about the various assignments. Your summaries and translations are invaluable.
Kathy B.
Teaching Shakespeare to today's generation can be challenging. No Fear helps a ton with understanding the crux of the text.
Kay H.
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An object in circular motion has an easily defined period, frequency and angular
velocity. Can circular motion be considered an oscillation?
Though circular motion has many similarities to oscillations, it can not truly
be considered an oscillation. Though we can see circular motion as moving back
and forth, in a sense, when we examine the forces involved in circular motion,
we see that they do not meet the requirements of oscillations. Recall that in
an oscillating system a force must always act to restore an object to an
equilibrium point. In circular motion, however, the force always acts
perpendicular to the motion of the particle, and does not act against
the displacement from a particular point. Thus circular motion cannot be
considered an oscillating system.
Problem :
What is the equilibrium point of a ball bouncing up and down elastically on a
floor?
Though this type of oscillation is not a traditional one, we can still find its
equilibrium point. Again, we use our principle that in an oscillating system
the force always acts to restore the object to its equilibrium point. Clearly
when the ball is in the air the force always points towards the ground. When it
does hit the ground, the ball compresses, and the elasticity of the ball
produces a force on the ball that causes it to rebound into the air. However,
the instant the ball hits the ground, there is no deformation of the ball, and
the normal force and the gravitational force cancel exactly, producing no net
force on the ball. This point, the instant the ball hits the ground must be the
equilibrium point of the system. Shown below is a diagram of the ball at
equilibrium, and displaced in both directions from the equilibrium point:
a) The ball at equilibrium b) the ball in the air, with net downward
force c) the ball deformed, with net upward force
Problem :
A mass on a spring completes one oscillation, of total length 2 meters, in 5
seconds. What is the frequency of oscillation?
The only piece of information we need here is the total time of one oscillation.
5 seconds is simply our period. Thus:
ν = = .2 Hz
Problem :
The maximum compression of an oscillating mass on a spring is 1 m, and during
one full oscillation the spring travels at an average velocity of 4 m/s. What
is the period of the oscillation?
Since we are given average velocity, and we want to find the time of travel of
one revolution, we must find the total distance traveled during the revolution.
Let's start our oscillation when the spring is fully compressed. It travels 1
meter to its equilibrium point, then an additional meter to its maximum
extension point. Then it returns to its initial state of maximum compression.
Thus the total distance traveled by the mass is 4 meters. Since t = x/v we can
calculate that T = x/v = 4 m/4 m/s = 1 second. The period of
oscillation is one second.