Video Transcript
In this video, we will learn how to
describe the motion of oscillating objects. An example of an oscillating object
is a playground swing. At first, the swing will hang
straight down, with the rope of the swing vertical. If we left the swing like this, it
wouldn’t move. It would stay in this position
forever. We call this position the
equilibrium position of the swing.
But what would happen if we were to
give the swing a push? If we were to push on the back of
the swing, the swing would start to move to the right of the equilibrium
position. Eventually, it will reach its
rightmost point. Then, it’ll change direction and
start moving back towards equilibrium. Once it reaches equilibrium, it’ll
keep moving towards the left. Eventually, it’ll reach the
leftmost point.
At this point, it’ll change
direction again and move towards equilibrium. Once the swing reaches equilibrium,
it keeps moving back towards the right, and the whole process starts again. The swing will continue to move
back and forth repeatedly. Each time it swings, it passes
through its original equilibrium position, where the rope is vertical. When an object repeatedly moves
back and forth through an equilibrium position, we can describe its motion as
oscillatory.
Lots of different objects can have
oscillatory motion. In physics, we often talk about an
object called a pendulum. A pendulum consists of a bob
suspended from a piece of string. A pendulum is very similar to the
playground swing that we just talked about. When left to its own devices, the
pendulum will hang straight down in its equilibrium position. But if we were to move the bob to
one side of the equilibrium position and then let go, the pendulum will begin to
swing back and forth through its equilibrium position. In other words, the pendulum will
oscillate, just like a playground swing.
Pendulums can oscillate back and
forth for a long time, so they’re useful tools for observing oscillatory motion. In particular, we can look at the
displacement of the pendulum’s bob at different times in its oscillation. The displacement of the pendulum’s
bob refers to its distance from the equilibrium position in a particular direction,
left or right. Let’s imagine that the pendulum is
stationary and hanging straight downwards. Here, the pendulum is at its
equilibrium position. So, its displacement from its
equilibrium position is zero.
Now let’s imagine that we were to
move the bob to the left-hand side like this. We have now given the bob some
displacement to the left of the equilibrium position. If we were to let go of the bob and
allow the pendulum to oscillate, the pendulum would never move further to the left
than this. It’ll return to this point, but
it’ll never go past it. So, this is the pendulum’s maximum
displacement to the left. When the pendulum swings, it’ll
move through the equilibrium position to the right until it reaches its rightmost
point. Here, it has its maximum
displacement to the right.
There is something important we
should notice about the positions we have labeled maximum displacement. The displacement of the rightmost
point has the same magnitude as the displacement of the leftmost point. So, the maximum displacement of the
pendulum has the same magnitude on either side of the equilibrium position. For the pendulum to do one complete
oscillation, it has to travel back and forth through every point of its swing and
return to the position that it started from.
For example, if we wanted to
observe one complete oscillation of the pendulum starting from its maximum
displacement to the left, we would watch the pendulum move through the equilibrium
position to the right until it reaches its rightmost point. Then, we’d watch it change
direction, move back through equilibrium position to the left until it reaches the
point where it started from. At this point, the pendulum has
completed one single oscillation.
So far, we have seen that when an
object oscillates, its displacement changes in a regular and repeated way. The speed of the pendulum also
follows a repeated and regular pattern. The pendulum has the greatest speed
when it passes through the equilibrium position. It doesn’t matter whether the
pendulum is moving to the left or to the right. When it’s at the equilibrium
position and so has zero displacement, it always has the same maximum speed.
When the pendulum has the maximum
displacement from the equilibrium position, its speed is always zero. The pendulum has to have zero speed
for a very brief moment in order for it to change direction and move back towards
equilibrium. Again, it doesn’t matter whether
the pendulum is to the left of the equilibrium or to the right. When its displacement has the
maximum possible magnitude, its speed is always zero.
Since the speed and displacement of
the pendulum follow a regular and repeated pattern, it makes sense that the time it
takes for the pendulum to swing does not change. If the pendulum isn’t affected by
air resistance, it will take the same amount of time for the pendulum to complete
each oscillation. Again, the direction of the
pendulum’s motion does not affect the amount of time it takes for the pendulum to
swing. For example, let’s say it takes one
second for the pendulum to complete half an oscillation and move from its leftmost
point to its rightmost point. It would also take the pendulum one
second to complete half an oscillation traveling in the opposite direction from its
rightmost point to its leftmost point.
So, by looking at the oscillation
of a pendulum, we have seen that oscillation is a regular, repeated motion through
an equilibrium position. We have also seen that the
displacement of the pendulum, the speed of the pendulum, and the time taken for the
pendulum to complete an oscillation all follow regular and repeated patterns.
We need to be careful not to
confuse oscillatory motion with periodic motion. Periodic motion is also regular and
repeated. But periodic motion does not have
all of the same properties as oscillatory motion.
For example, consider a bouncy
ball. If we placed the ball on the
ground, it wouldn’t move. So, the ground is the ball’s
equilibrium position. Let’s imagine that we drop the ball
from a height. It’ll fall to the ground. Then, it’ll change direction and
start to move upwards. If the ball doesn’t lose any
energy, it’ll return to its initial maximum height and continue to bounce in this
way. This is periodic motion, but it’s
not oscillatory. The ball has an equilibrium
position, but it’s impossible for the ball to pass through it. The ball is only ever above the
ground and never below it. This is not consistent with our
earlier descriptions of oscillation.
Oscillation is repeated motion
through an equilibrium position. Plus, in order for the ball to
reverse direction when it hits the ground, it must momentarily have zero speed. So, when the ball is at its
equilibrium position, its speed is zero. But an oscillating object has its
maximum speed when it passes through the equilibrium position. So, for our bouncy ball, the
relationship between speed and displacement is not consistent with oscillatory
motion.
However, there are objects other
than pendulums that can have oscillatory motion. An example of such an object is a
spring. Here we have a spring, where one
end is fixed in place and the other end is free to move. At the moment, this spring is at
rest, so the spring isn’t moving, and nothing is being done to the spring to change
its length. This is the spring’s equilibrium
position. If the spring is left like this,
it’ll stay like this. But we can apply forces to the
spring to change its length.
If we push on the free end of the
spring, the spring will get shorter. We say that the spring is
compressed. When we compress the spring, the
spring will start to exert a reaction force to resist being compressed. When we let go of the spring, this
force will cause the spring to spring back to its original length. But the spring won’t just spring
back to its original length. It’ll actually keep moving,
stretching itself out, and making itself longer. Again, once the spring has begun to
stretch, it’ll start to exert a force on itself to resist this stretching. This will cause the spring to move
back to its original length. But again, it won’t stop once it’s
reached its original length. It’ll keep moving until it has
returned to its compressed position, and the process will continue.
This is an example of oscillatory
motion. Here, we have drawn one complete
oscillation of the spring. We know that the spring is
oscillating because the spring follows a regular repeated pattern of motion through
an equilibrium position. The speed and displacement of the
spring also have all the properties of oscillatory motion. When the spring is fully
compressed, it has maximum displacement to the left of the equilibrium position. When the spring is fully stretched,
it has a displacement of the same magnitude to the right. And the speed of the spring is
greatest when it is moving through equilibrium. The spring momentarily has zero
speed when it has its maximum displacement.
The two examples of oscillatory
motion that we have discussed in this video, the spring and the pendulum, may seem
very different, but we can compare the two. Compressing the spring is
equivalent to moving the pendulum bob to the left of its equilibrium. When the pendulum is released, it
moves through equilibrium and then keeps moving towards the right. This is just like a spring, which
returns to its original length but then keeps moving until the spring is stretched
out. We know that the pendulum will then
change direction and pass through equilibrium before moving back towards the
left. This is just like the spring
returning to its original length before compressing again.
Now we know how to identify
oscillatory motion, let’s take a look at some example questions.
A pendulum swings freely from left
to right. At which two of the positions shown
is the pendulum equally far from its equilibrium position? (A) I and III, (B) I and IV, (C) II
and III, or (D) II and IV.
To answer this question, we need to
determine which two positions of the pendulum are equally far from the equilibrium
position. First, let’s make sure we know what
is meant by the pendulum’s equilibrium position. The equilibrium position of an
object is the position where the object will not move unless a force acts on it to
make it move. A pendulum is at its equilibrium
position when the bob is hanging straight down, with its string vertical. This corresponds to position II in
the diagram.
So, we need to find out which two
positions are equally displaced from position II in the diagram. We can rule out any answer options
which contain position II straightaway, since position II cannot be equally far away
from itself and another point. So, we know that answer options (C)
and (D) aren’t correct.
To help us decide which of the
remaining options is right, we can label the displacement of positions I, III, and
IV on the diagram. Recall that the displacement of the
pendulum from its equilibrium position is its distance from equilibrium in a given
direction. Let’s label the displacement of
position I. Position I has a displacement to
the left of the equilibrium. The magnitude of this displacement
is shown by the length of this blue arrow. Both positions III and IV have a
displacement to the right of the equilibrium, which again we can represent like
this.
To compare the magnitude of the
displacement at each position, we simply compare the length of these arrows. We can see that the arrows
corresponding to positions I and IV are the same length. But the arrow corresponding to
position III is much shorter. This tells us that positions I and
IV have the same magnitude of displacement from the equilibrium position. So, the correct answer to this
question is option (B).
Let’s take a look at another
example.
A pendulum swings from left to
right and back again. The pendulum oscillates without
dissipating energy. At which of the following positions
is the speed of the pendulum greatest? (A), (B), or (C).
In this question, we need to work
out which of these three positions shows the pendulum when it has the greatest
speed. We are told that the pendulum
oscillates without dissipating energy. This means that the speed of the
pendulum will continue to change according to the same repeated pattern, regardless
of how many times the pendulum has oscillated.
Option (A) shows the pendulum at
its equilibrium position. Option (B) shows the pendulum when
it has its maximum displacement to the left. Option (C) shows the pendulum when
it has its maximum displacement to the right.
We can recall that the speed of an
oscillating object is related to the distance of the object from the equilibrium
position. When an object has its maximum
displacement, either to the left or to the right of equilibrium, its speed is
momentarily zero. This is because the object is about
to change direction and start moving back towards equilibrium. On the other hand, any time an
object is passing through the equilibrium position, its speed always has the maximum
possible value. So, we can say right away that the
correct answer to this question is option (A), as option (A) shows the pendulum
passing through its equilibrium.
In fact, it doesn’t really matter
what positions are shown in options (B) and (C). Any two nonequilibrium positions
would still always correspond to a lower speed. So, the correct answer to this
question is option (A).
Let’s look at one more example,
this time about a spring.
A spring attached to a wall is
pushed until it reaches the red line, and then it is released. The diagrams show how the length of
the spring changes after it is released. The spring oscillates without
dissipating energy. The blue line shows the equilibrium
position of the spring. How does the distance between the
red and blue lines compare to the distance between the green and blue lines?
The diagram is showing us the
oscillatory motion of the spring. The spring is first compressed to
the red line. Then, it’s allowed to oscillate
back and forth through the equilibrium position, the blue line. The furthest distance that it
stretches to is indicated by the green line. The red and green lines represent
the furthest nonequilibrium positions of the spring. We are told that the spring does
not dissipate energy while it oscillates. So the spring will continue to
oscillate between these two positions.
To answer this question, we need to
recall that when an object undergoes oscillatory motion, the magnitude of its
maximum displacement should be the same on either side of its equilibrium
position. When the spring is at its
equilibrium position, the end of the spring is in line with the blue line. When the spring is maximally
compressed, it has its maximum displacement to the left of equilibrium. This happens when the end of the
spring is in line with the red line. When the spring is maximally
stretched, it has its maximum displacement to the right of equilibrium. This happens when the end of the
spring is in line with the green line.
We know that the magnitude of the
spring’s maximum displacement is the same on either side of its equilibrium
position. So, we’re ready to answer the
question of how the distance between the red and blue lines compares to the distance
between the green and blue lines. We know that the distance between
the blue line and the red line is the same as the distance between the blue line and
the green line. The answer to this question is
therefore “The distances are the same.”
Now let’s finish up this video by
summarizing some key points. Oscillatory motion is regular,
repeated motion through an equilibrium position. The magnitude of the maximum
displacement of an oscillating object is the same on either side of the equilibrium
position. The speed of an oscillating object
is zero at the furthest nonequilibrium positions and maximum at the equilibrium
position. The time it takes for an
oscillating object to move through one complete oscillation is the same every
time. Examples of objects which can
undergo oscillatory motion are pendulums and springs.