MODULE 5
ADVANCED MECHANICS
UNIFORM CIRCULAR MOTION
Uniform circular motion is circular motion
with a uniform tangential (orbital) speed. As an example of circular motion,
imagine you have a rock tied to a string and are whirling it around your head
in a horizontal plane. Because the path of the rock is in a horizontal plane,
as shown in the diagram, gravity plays no part in its motion. The Greek,
Aristotle, considered that circular motion was a perfect and natural motion,
but it is far from it. If you were to let go of the string, the rock would
fly off at a tangent to the circle - a demonstration of Newton's First Law of
Motion (an object continues in uniform motion in a straight line unless acted
upon by a force). In the case of our rock, the force keeping it within a
circular path is the tension in the string, and it is always directed back
towards the hand at the centre of the circle. Without that force the rock
will travel in a straight line (figure 1). Fig. 1. A force acting towards the centre of a
circle is necessary for an object to rotate in a circular path. If the magnitude of the velocity is
constant but its direction is changing, then the velocity must be changing,
so, the rock is accelerating. A force is required to accelerate the rock and
as stated above, this force is the tension in the string. This centre seeking
force is called the centripetal force .
The term centripetal force is only a label attached to real physical forces such as tension, gravitation or
friction. On force diagrams, you should show the real physical forces acting
and not the label centripetal force. The same is true of a spacecraft in
orbit around the Earth, or any object in circular motion - some force is
needed to keep it moving in a circle or accelerate it and that force is
directed towards the centre of the circle. In the case of the spacecraft, it
is the gravitational attraction between the Earth and the spacecraft that
acts to maintain the circular motion and keep it in orbit. The Moon obits
around the Earth and the Earth around the Sun because of the gravitational
force like the satellite shown in figure 2. Fig.2. A satellite is acted upon by the gravitation
force between the Earth and the satellite. The centripetal force is the
gravitational force. An object is shown moving between
two points (1) and (2) on a horizontal circle in figure 3. Its velocity has
changed from to .
The magnitude of the velocity is always the same, but the direction has
changed. Since velocities are vector quantities, we need to use vector
mathematics to work out the average change in velocity .
In this example, the direction of the average change in velocity is towards
the centre of the circle. This is always the case and thus true for
instantaneous acceleration. This acceleration is called the centripetal acceleration . Fig.
3. The direction of the change in
velocity (and acceleration) is directed towards the centre of the circle. For an object of mass ,
moving at a speed ,
in uniform circular motion of radius ,
the net force acting on is called the centripetal force and its magnitude is given by equation 1 (1) centripetal force This centripetal force is
responsible for the change in direction of the object as its speed is
constant. The resulting acceleration due to the change in direction is the
centripetal acceleration and its magnitude is given by equation 2.
The direction of the centripetal force and centripetal acceleration is
towards the centre of the circle (centripetal means centre seeking). (2) centripetal acceleration [WARNING: the equations given in the Physics Stage 6 Syllabus for
the centripetal force and centripetal acceleration are absolutely incorrect] It is important to understand that
centripetal force is not a new force that starts acting on something when it
moves in a circle. It is the sum of all forces acting on the object. This
resultant force results from all the other forces on the object. When the
rock in the example above is whirled in a vertical circle (instead of
horizontal), gravity interacts with the tension in the string to produce the
net force which we call centripetal force. Centripetal force is always the
net force. |
Period, frequency, angular frequency (speed) Consider
an object executing uniform circular motion with a radius r
and speed v . The time for one complete
revolution is known as the period T . The distance travelled by the
object in one period is simply the circumference of the circle .
The orbit speed ,
period and radius are connected by the equations
The frequency f and angular frequency (speed) are
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ENERGY and WORK Have
you wondered why the Earth just keeps going around the Sun year after a year,
in fact for many billions of years the Earth has been orbiting the Sun. The Earth is attracted to the Sun by the
gravitational force acting between the Earth and the Sun, but the Earth does
not lose energy, it just keeps orbiting the Sun. The
gravitational force acts as the centripetal force responsible for the uniform
circular motion of the Earth around the Sun (actually, the
motion of the Earth is only approximately circular, and its speed does vary
slightly in its orbit). The centripetal force always acts towards the centre
of the circle, but at each instant the displacement of the Earth is at right
angles to the centripetal force. Hence, zero work is done by the
gravitational force and there is zero change in potential or kinetic energies of the Earth in its orbit and the total
energy is constant. So, the Earth can just keep
orbiting. The work done by
the net force on an object equals its change in kinetic energy. For uniform
circular motion, the speed and hence kinetic energy do not change, Therefore,
the net force (centripetal force) does zero work on the object. Work done by the centripetal force
Note: The equation for angular speed given in the Physics Stage 6 Syllabus is . This expression should always be written as . This is another example of the incompetence of the people who put the Syllabus together. |
Ian Cooper School of Physics University of Sydney If you have any feedback, comments,
suggestions or corrections please email Ian Cooper ian.cooper@sydney.edu.au |