Meta data: Data logging, for the teacher, English, friction, energy, work Friction forces – static friction and sliding friction (for the teacher) Level of difficulty: easy Summary This experiment demonstrates the friction between a small wooden block and a horizontal surface – both static and kinetic friction. The experiment employs a force sensor and a data logger to demonstrate the frictional force as a function of time. It is also possible to add a position sensor for a closer view of the transition between static and kinetic friction. Theory (Theoretical background) In this experiment a wooden block is pulled along a horizontal surface by means of a force working horizontally. Contact forces operating between the block and the underlying surface will offer resistance. These forces are termed friction forces or just friction. For as long as the block is lying still (non-moving) this friction is known as static friction. While the block is moving, the friction between the moving surfaces is known as kinetic friction, also known as sliding friction or dynamic friction. The magnitude of the friction depends to a great extent on the nature of the materials moving against one another. F = pulling force R = friction As long as the block moves at constant speed, the sum of the forces acting upon it equals zero, i.e. F = 0. This is an expression of Newton’s first law. Only two forces act upon the block: the pulling force (F) and the friction force (R). If we apply an even pulling force (F) and maintain a slow, even speed, the pulling force will be equal to the friction (R), both while the block is stationary as well as when it is moving. According to Newton’s 1st law: F = F + R = 0 R = - F. The two forces R and F are equal in size, but they work in opposite directions. Just when the block starts moving, its speed does change; a small acceleration (a) occurs. At the commencement of the movement, and according to Newton’s 2nd law there will be a small excess of force in the same direction as the movement, since F = ma. (F = F + R = ma > 0 F > - R). When the speed is low the acceleration will be small enough that we may assume F = - R throughout the experiment. This experiment is set up to measure the force F and observe how the friction may change as a function of time and the movement of the block. Dette verk er lisensieret under en Creative Commons Navngivelse 3.0 Norge Lisens. Les mere om projektet på www.dlis.eu. Page 1 of 5 Meta data: Data logging, for the teacher, English, friction, energy, work Technical considerations This experiment only requires a force sensor for the data logger, but a position sensor may also be used. As the pulling force (and the position) will change rapidly over time, the data logger should be adjusted to read data 25 – 50 times per second. The logger should also be adjusted to ensure that the force sensor registers the pulling force as positive (i.e. not pushing). Equipment - Wooden block with a small eye screw. NB! It is also possible to use a block from material other than wood. - Cotton thread and scissors - A horizontal surface (may be an ordinary table) - Data logger with force sensor, possibly a position sensor as well. - Possibly a computer with software compatible with the data logger. Arranging the equipment The equipment should be arranged as shown in the photo: The cotton thread connects the block (via the eye screw) to the force sensor. Important: The force sensor will only return correct data if it works parallel to the surface and in line with the cotton thread. The force sensor must be reset to zero before each set of measurements. The sensor has a reset button. Dette verk er lisensieret under en Creative Commons Navngivelse 3.0 Norge Lisens. Les mere om projektet på www.dlis.eu. Page 2 of 5 Meta data: Data logging, for the teacher, English, friction, energy, work Procedure Start recordings while the cotton thread is still slightly slack. Move the sensor slowly and at constant speed (1 – 3 cm/s) until the thread is tense, and then for a further 10 – 20 cm at the same, constant speed. Stop recordings. Examine the graph on the data logger set to show the friction (= the pulling force) as a function of time. Arrangement and procedure if the position sensor is also used Arrange the equipment as shown in the photo: In this arrangement the position sensor measures the distance to the rear surface to the block only. Important: The logger must be adjusted to record data from both sensors with equal frequency! Dette verk er lisensieret under en Creative Commons Navngivelse 3.0 Norge Lisens. Les mere om projektet på www.dlis.eu. Page 3 of 5 Meta data: Data logging, for the teacher, English, friction, energy, work In the computer the two graphs may look like the graphs below: Questions for discussion - Discuss these graphs section by section. In the illustrations above, section 1 would cover the period from 0- about 2 seconds, section 2: from 2-4 seconds, section 3: from 4-9 seconds, and section 4: after 9 seconds. What was taking place in each of these time sections? - The red graph is not quite flat between 4.5 – 9 seconds. Discuss what might be the reason(s). - Calculate the average sliding friction. The data logger will do this very easily, just remember to mark the relevant area of the graph (between 4.5 – 9 seconds in the graph above) for calculating this average. Hint: Select Tools Statistics Dette verk er lisensieret under en Creative Commons Navngivelse 3.0 Norge Lisens. Les mere om projektet på www.dlis.eu. Page 4 of 5 Meta data: Data logging, for the teacher, English, friction, energy, work - Discuss why the red graph has a very obvious maximum value immediately before the block starts moving. Read the value for maximum friction at rest, and compare it with the average sliding friction. - If a position sensor was used: Is it possible to observe from the (green) graph whether the block was moving at constant speed? Is it possible to see evidence of acceleration? Variations on the experiment - Repeat the experiment a number of times as identically as possible. Compare the results of recordings of maximum friction at rest and average sliding frictions between the different experiments. - Repeat the experiment, but pull the block at different speeds. The speed still needs to be as constant as possible every time. Compare the results of average sliding frictions at different speeds. - Repeat the experiment with a view to record an average sliding friction, but apply varying loads to the block. First record the mass (m) of the block with different loads by weighing on electronic scales, and then work out the gravity (G) using the formula G = mg, in which g = 9.81 N/kg. Experiment with at least 3 different loads. Before you start, invite the students to agree on a hypothesis for predicting results. Draw a graph to demonstrate how the gravity (G) relates to the sliding friction (R). - Look up the term friction coefficient () in a text book, or an encyclopedia. Check whether the formula R = ∙ N agrees with your findings. But first, what is N? When measuring friction, it is customary to use the force between the body and the surface, called the normal force (N), in calculations. This force acts at right angles (perpendicular) to the surface, pointing upward. On a horizontal surface, N will be equal to the gravity G. (This follows from Newton’s first law, as seen when only the forces G and N are at work.) - Try to calculate the friction (R) and the friction coefficient () when using surface materials of different quality. - If you used a position sensor: In this experiment, the position sensor was used only to measure the distance to the block over time. The data logger is also able to calculate the average speed (v) for each experiment. Request a v-t graph for each set of data which are already stored in the data logger. Dette verk er lisensieret under en Creative Commons Navngivelse 3.0 Norge Lisens. Les mere om projektet på www.dlis.eu. Page 5 of 5