**Uniform Circular Motion Lab**

This experiment investigates how the force necessary to maintain a body in uniform circular motion (i.e. in a circle of constant radius and with a constant speed) is related to the speed of the object experiencing UCM. You should note that there are other possibilities for the independent variable. We are keeping all of the possible independent variables fixed save the applied force.

Your apparatus, shown in figure 1, consists of a glass tube,
some string, a rubber stopper, and an alligator clip. The force that keeps the rubber
stopper traveling in a circle at constant speed is supplied by the string. The source of
the force is gravity pulling down on a mass attached to the lower end of the string. If we
ignore the friction of the string on the glass tube, the force downward on the mass due to
gravity is the same as the force inward on the stopper. Hence the force is M_{hanging}
g and the velocity can be calculated by measuring the time for thirty complete circles,
calculating the distance traveled (30 times the circumference), and then the average
speed.

Before you begin your experiment, check your glass tube for chipped edges.

- Measure the mass of your stopper. (You won't need it until the end, but measuring it now makes sure you don't forget to do it.)
- Thread the string through the tube.
- Attach the stopper to one end and 150 g of mass to the lower end.
- Stretch the apparatus out on your lab table and position the stopper so that the distance between the middle of the stopper and the top of the tube is 50 cm.
- Attach the alligator clip about 2 cm below the bottom of the tube.
- Holding the tube in one hand, start swinging the stopper slowly in a circle above your head. As you swing faster, the clip will rise. This happens because the suspended mass can't supply enough force to keep the stopper from moving out. Thus, the radius increases and the force needed to maintain UCM will then decrease (due to the larger radius the needed acceleration is smaller). After a little practice, you should be able to maintain the alligator clip about 2 cm below the bottom of the tube.
- Have a partner start a stopwatch and time the amount of time needed for thirty complete revolutions. You should concentrate on trying to keep the alligator clip in a steady position 2 cm below the bottom of the tube.
- Once the time has been measured, record your data in a table (similar to the example below) and proceed on to other masses.
- You should acquire additional data for hanging masses of: 20, 30, 50, 100, 200, 250, and 280 grams.

For each case, we know the radius of the circle is equal to the value set earlier, and that the applied force is the weight of the hanging mass. Calculate the force applied, and the resulting velocity for each case and complete a table like the one shown in your notebook.

M |
Time (s) |
v (m/s) |
F |

Once your table is complete, plot a graph of velocity vs. applied force. What is the shape of the graph? If it is straight, draw in the best fit straight line and determine the equation for the best fit line. If the graph is not straight, use its shape to figure out how to re-plot the graph in such a manner as to obtain a straight (or straighter) line. Draw in the best fit line for this graph and determine the equation which describes the line.

Use Newton's second law (*with the net force being the
weight of the suspended mass) *and your knowledge of circular motion to predict what
the slope of your line should be. (*i.e. solve for v in terms of F _{net}. * Calculate
this theoretical slope. Compare this theoretical slope with the slope that you
got from your best fit line. How well do they agree? Make a verbal comparison
and also calculate the percentage difference between the experimental and theoretical
slopes. Which slope is larger? What are some possible experimental reasons that the two
might not agree? For one of the possible sources of errors

*Barney Taylor
Physics Dept.
Miami University - Hamilton
1601 University Blvd., Hamilton, OH 45011
(513) 785-3016
taylorbe@miamioh.edu *

*last modified Aug, 2013 *