Motion Characteristics for Circular Motion
Student Extras
Need to see it? View the Inertia and the Right Hand Turn animation from the Multimedia Physics Studios.
Flickr PhysicsVisit The Physics Classroom's Flickr Galleries and enjoy a visual overview of the topic of circular motion
Shockwave StudiosThink you get the idea? Try the Race Track activity from the Shockwave Studios.
Physics of RacingA physicist and race car driver presents the argument of the fictional nature of a centrifugal force.
Teacher's Guide
Thinking Physics! Present your students with this short decision-making challenge.
PBS TeachersView a lesson plan from PBS Teachers on the topic of centripetal acceleration and force.
Shockwave StudiosGive your students a challenge with the Race Track activity from the Shockwave Studios.
Curriculum CornerLearning requires action. Give your students this sense-making activity from The Curriculum Corner.
The Forbidden F-Word
When the subject of circular motion is discussed, it is not uncommon to hear mention of the word centrifugal. Centrifugal, not to be confused with centripetal, means away from the center or outward. The use of or at least the familiarity with this word centrifugal, combined with the common sensation of an outward lean when experiencing circular motion, often creates or reinforces a common student misconception. The common misconception, believed by many physics students, is the notion that objects in circular motion are experiencing an outward force. "After all," a well-meaning student may think, "I can recall vividly the sensation of being thrown outward away from the center of the circle on that roller coaster ride. Therefore, circular motion must be characterized by an outward force." This misconception is often fervently adhered to despite the clear presentation by a textbook or teacher of an inward force requirement. As discussed previously in Lesson 1, the motion of an object in a circle requires that there be an inward net force - the centripetal force requirement. There is an inward-directed acceleration that demands an inward force. Without this inward force, an object would maintain a straight-line motion tangent to the perimeter of the circle. Without this inward or centripetal force, circular motion would be impossible.
So why then is this student misconception
of an outward or centrifugal force so prevalent and so
stubbornly adhered to? Perhaps like all misconceptions, the
notion of a centrifugal force as lodged in a person's head
has a particularly lengthy history. Part of that history is
certainly attributable to the experience of a circular
motion - either as a passenger or driver in an automobile or
perhaps on an amusement park ride. Even learned physics
types would admit that circular motion leaves the moving
person with the sensation of being thrown outward from the
center of the circle. But before drawing hasty conclusions,
ask yourself three probing questions:
- Does the sensation of being thrown outward from the center of a circle mean that there was definitely an outward force?
- If there is such an outward force on my body as I make a left-hand turn in an automobile, then what physical object is supplying the outward push or pull?
- And finally, could that sensation be explained in other ways that are more consistent with our growing understanding of Newton's laws?
If you can answer the first of these questions with "No" then you have a chance. But if you quickly conclude that the outward feeling means there is an outward force, then you at least must admit that your conclusion is contrary to all that has been discussed in Lesson 1 and that you don't believe that Newton's laws accurately describe circular motion. The sensation of being thrown outward is attributable to the idea of inertia, rather than the idea of force. When making that left-hand turn in the car, your tendency to be thrown rightward across the seat (that would be outward or away from the center of the circle) was not due to a force. It was due to your tendency to travel in a straight line while the car seat was making its turn. In fact, you were not thrown rightward at all; you moved in a perfectly straight line. If an airborne camera had collected the motion on film from above and we could watch the instant replay, then it would be a no-brainer - the car turned left and your body kept going straight. Finally, your body hits the door on the right side of the car and the door provides an inward push on your body to cause your body to begin moving in circular motion. But until hitting the door, your body's tendency was to follow its inertial path.
A
common physics demonstration involves using a flat
whiteboard with a tennis ball on top of it. The whiteboard
is carried along in a straight-line path; the ball rest on
top of the whiteboard and follows the same straight-line
path. Then suddenly, the board is turned leftward to begin a
circular motion; yet the ball keeps moving straight.
Ultimately, the ball rolls off the right-edge of the board
and continues in its straight-line inertial path. Without an
unbalanced force on the ball, the ball continues in its
original motion. The whiteboard merely moved out from under
the ball as it makes its turn. If you could watch carefully,
then you could view the ball's path from the perspective of
an airborne camera. It's a no brainer - the ball moves
straight while the whiteboard turns. And finally, the ball
travels off the "outside edge" of the whiteboard. Relative
to the circular motion of the whiteboard, the ball moves
away from the center of the circle. But explaining the
motion of the ball does not require that we imagine or dream
up the existence of an outward or centrifugal force. The
motion of the ball is explained by the tendency of an object
in motion to continue in motion in the same direction.
INERTIA!
Now
suppose that a block is attached to the top of the
whiteboard on the "outside" of the ball with such an
orientation that it would apply an inward force upon the
ball. When the whiteboard is turned, the block would turn as
well and supply the centripetal force required to move the
ball in a circle. Without the block, the ball would have
moved along the straight-line path, moving to position 1
after say 0.1 seconds, then to position 2 after 0.2 seconds,
then to position 3 after 0.3 seconds, and so on. But with
the block supplying an inward force, the ball moves inward
towards the center of the circle relative to its
straight-line path. Instead of being at position 1, the ball
is closer to the center at position 1'. And instead of being
at position 2 after 0.2 seconds, the ball is forced inwards
towards position 2'. And instead of being at position 3
after 0.3 seconds, the ball is forced inwards towards
position 3'. The inward net force accelerates the ball
inward, causing it to deviate from its straight-line path
that is directed tangent to the circle.
If you were the tennis ball in the first
example above, then you might feel like you were being
pushed outwards. After all, you would travel through the
outside door of the whiteboard. Yet it is clear from
the diagram and the discussion that you are not deviating
from any straight-line path. It is merely that the
whiteboard
is moving inward relative to your path and you are moving
outward relative to the whiteboard's path. But this
sensation of relative motion does not give reason for
supposing that an outward force exists. This notion of an
outward force is merely fictitious. Newton's law of inertia
- "an object in motion continues in motion with the same
speed and in the same direction unless acted upon an
unbalanced force" - provides a more reasonable explanation
for the sensations experienced by those who are in circular
motion. A centrifugal or outward net force simply does not
exist. No physical object could ever be identified that was
pushing you outwards. And if there was a physical object
pushing or pulling you outwards (e.g., in the rightwards
direction when taking a left-hand turn), then you certainly
would not turn in the circle that you are turning in.
An object moving n circular motion is at all times moving tangent to the circle; the velocity vector for the object is directed tangentially. To make the circular motion, there must be a net or unbalanced force directed towards the center of the circle in order to deviate the object from its otherwise tangential path. This path is an inward force - a centripetal force. That is spelled c-e-n-t-r-i-p-e-t-a-l, with a "p." The other word - centrifugal, with an "f" - will be considered our forbidden F-word. Simply don't use it and please don't believe in it.

