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PHY ion Force and Mot SICAL SER SCIENCE ACTIVITY 7 Rolling downhill M AT E R I A L S What happens to the velocity of a ball while it is rolling down a hill, instead of along a level track? Does its velocity change? Can you predict how it changes? For each group of 4 students OV E RV I E W A ball rolls down an incline. As it does so, its velocity changes. This activity introduces the concept of acceleration. By measuring the average speed of a ball rolling on an incline, students discover that the ball’s velocity increases with time; the longer it’s on the hill the faster it goes. Some students, who are ready to grasp proportional relationships, will see that when the slope is constant, the rate of change of velocity (the acceleration) is also constant. Graphs again are an effective way to describe motion and changes in motion. 1 or more copies Student Activity Sheet 7, Rolling downhill 1 long ramp system (see Appendix, item A-IV for assembly) including: 1 tripod base (A) 1 half-meter stick 1 height marker (B) 1 support bar (C) 1 ramp box (E) 2 tracks Students will: 1 large metal ball (3/4" diameter, approx. 2 cm) • time a rolling ball over various distances on a ramp 1 measuring tape or meter stick 1 stopwatch • calculate average velocity for four different segments of the ramp 2 sticky arrows or masking tape • graph velocity vs. time (optional) for opening demonstration: tennis ball, 2 one-meter sticks* • discover a relationship between velocity and how long the object has been accelerated • interpret graphs of a variety of motions * not in kit TIME 2 (50-minute) class periods This includes time for whole-class discussion on graphs at the conclusion of the activity. Some teachers allow more than two class periods to maximize the benefits of in-depth discussions and longer reflection time for students. B C FIGURE 7.1 E 107 A IES PHY ion Force and Mot SICAL SER SCIENCE IES S C I E N C E B A C KG R O U N D The physics of changing velocity. When velocity is not constant in time, we say that acceleration is taking place. The quantitative definition of acceleration is: acceleration = (final velocity 2 initial velocity) / elapsed time Acceleration is the rate of change of velocity; it’s an indication of how quickly or slowly velocity is changing. Like velocity, acceleration has a direction as well as a size. Here are some examples: before it hits floor after it hits floor • As a subway car pulls away from the station, its forward speed is increasing. Its initial velocity is zero, and so the car is accelerating forward. If it changes speed in a short time, the acceleration is large. • As a tired runner finishes the race and gradually slows down, her forward speed is decreasing. Her forward acceleration is negative; or we could say that the runner is accelerating backward. v v • When a basketball bounces off the floor, the direction of motion changes from down to up. Even though the speed might not change, there is a change in velocity that is directed away from the floor (up). The bounce doesn’t take very long, and so the acceleration is huge; it is also upward. S EE D FIGURE 7.2 • A falling object accelerates downward. In each successive interval of 0.1 second its speed is greater. TH E C When the direction of motion changes suddenly, there is a large acceleration, even if speed stays constant. 0.0 0.2 Meters Acceleration of falling objects. We all have a lot of experience with acceleration. A falling object is an interesting special case, because the acceleration is constant—it’s constantly increasing its speed. Figure 7.3 shows how a ball falls. The black circles represent the ball’s position every tenth of a second, starting at 0 sec when it’s released. The positions cluster together at the beginning, but then get farther and farther apart as it continues to accelerate. The light gray circle shows where the ball would be after only half a second—it has dropped more than a meter! change in velocity 0.4 0.6 0.8 FIGURE 7.3 1.0 108 The black dots show the position of a falling object every 1/10 second. PHY ion Force and Mot SICAL 5 Figure 7.4 graphs the motion of a ball dropping about 5 meters straight down. It takes only 1 second to fall about 5 meters. 4 The next graph, figure 7.5, shows a ball’s motion when you throw it up in 3 the air nearly 5 meters, and then watch it fall. The second half of this graph is exactly like the one we just looked at in 2 figure 7.4. On the first half of the graph, however, when the ball is on the way up, it travels a smaller distance in each suc1 cessive time interval. It is slowing down. On both parts of the ball’s trip, it is accelerating downward. When its veloc0 0.5 ity is upward, the speed is decreasing; Time (seconds) when its velocity is downward, the speed is increasing. Unfortunately, the acceleration of a falling object is too large for us to be able to study it with meter sticks and stopwatches. Your classroom ceiling is most likely less than 5 m (16 feet) high, and according to figure 7.4, SER SCIENCE IES FIGURE 7.4 Height (meters) Falling objects go farther in each successive time interval. 1 5 Height (meters) 4 3 FIGURE 7.5 2 When the ball is moving upward, its speed is decreasing; as it moves downward, its speed is increasing. 1 0.5 1.0 Time (seconds) 1.5 109 EE S any ball-dropping experiment you can do in the classroom would be over in less than a second, which can’t be timed accurately with a stopwatch. Although photogates or other kinds of electronic timers do get informative data with objects that fall only a few meters, we will, instead, study a ball rolling on a slightly inclined track. It accelerates much more slowly, enough so that we can measure it with a stopwatch. This activity does not directly measure the acceleration, because all we know is the average speed, which necessarily is less than the final speed. Dividing the average speed by the time on the ramp gives an 2.0 D 0 TH E C PHY ion Force and Mot SICAL SER SCIENCE IES EE S Calculating acceleration. Students are not asked to calculate acceleration in this module, but background information on how to do those calculations, and about the units of acceleration, is on the CD. D “acceleration” that is too small by a factor of 2. The data will show, however, that the average velocity increases in proportion to the time on the ramp, which implies that the acceleration is constant. TH E C FIGURE 7.6 In uniform motion, an object travels equal distances in equal time intervals. 40 cm 0 40 cm 40 cm 1.0 0.5 1.5 SCIENCE IN EVERYDAY LIFE. A car has a pedal called “the accelerator.” You “step on the gas” to go faster. A car, however, is not quite an isolated system, especially at high speeds where 0 0.5 it becomes hard to push the air out of the way fast enough, at which point “put the pedal to the metal” just means go fast, rather than accelerate constantly. Much more consistently we could call the brake pedal “the decelerator.” A practical application of acceleration is in the timing of your tennis serve. The ball should be thrown upward so that its highest point is right at the height where you can hit it, because that point is where it is moving 110 EE S Visualizing motion. Let’s compare visualizations of accelerated motion and uniform motion for systems like the ones you are using in these activities. Figure 7.6, which was also in the introduction to Activity 5, represents uniform motion. It shows the ball at fixed time intervals (every 0.5 second). Unlike the accelerating falling ball in figures 7.4 and 7.5, the uniformly moving ball covered equal distances in each time interval. In the present activity students will measure accelerated motion on an incline, as shown in figure 7.7. Again the ball is shown at equal time intervals (every 0.5 sec), but it covers more distance for each successive interval. Accelerated motion is not uniform motion. D Time (seconds) TH E C 1.0 1.5 Time (seconds) FIGURE 7.7 In accelerated motion, an object covers different distances in each equal time intervals. PHY SICAL SER SCIENCE IES 1.5 height (meters) its slowest. As shown in figure 7.8, the ball spends 0.2 seconds within 5 cm of the turn-around point—plenty of time to hit it. Throwing the ball too high sends it through the target region faster, and now you must time your swing more precisely. ion Force and Mot 1.0 0.5 G E T T I N G R E A DY The concluding discussion for this activity includes 0 several graphs for class interpretation. Look ahead 0.5 1.0 now to that discussion, and plan on devoting more time (seconds) time to it than you did for the conclusion of most of FIGURE 7.8 the previous activities. Hitting a tennis ball at the top of its Five parts in your kit (in addition to two sections of track) arc—where it is moving slowest—makes make up the long ramp system. See Appendix A, Item A-IV it easier to hit. for complete assembly instructions. Notice that the two tracks used in this activity are connected end to end to make the ramp. You G L O S S A RY will use no horizontal track. Figure 7.9 is the assembly diagram from the acceleration appendix. Students have used all but one of the pieces earlier. The new item is a small box labelled ‘E’ that supports the joint between the two balanced forces tracks. The track clips nestle in between the posts on the box. Notice that distance the top surface of the box (the top is where the 4 prongs point up) has a slight angle. This angle matches the ramp angle when the upper ramp median end is set at 6.5 cm. position Decide how you want to share the setup instructions with your stuspeed, average speed C dents (from Appendix A, item AB system IV). They can be distributed in print form to each group, time shown on the overhead projecuniform motion tor, or described as part of your activity introvelocity duction for the class. S EE D A TH E C E taller side of box faces uphill FIGURE 7.9 FIGURE 7.10 Assembly of the long ramp system When properly placed, the support box posts fit around the track joint where the two track sections connect 111 PHY ion Force and Mot SICAL SER SCIENCE To have a constant acceleration to measure, it’s very important that the inclines of the coupled track pieces are identical. A FIGURE 7.11 B To ensure that the inclines of the two ramp pieces are the same, set the height marker that supports the upper end of the higher track at 6.5 cm (be sure the half-meter stick is pushed all the way to the bottom of the tripod). The bottom end of the lower track must rest on the tabletop and not hang over the edge. The joint between the two tracks is supported by the box that fits exactly at the joint. These conditions produce a shallow and consistent incline angle that leads to good stopwatch data. Your students will likely want to experiment with steeper slopes. This can go on the question board for later open investigations, or on hold until Activity 9 when they will specifically look at the effect that steepness of the slope has on acceleration. As part of the concluding discussion you could include the visualizations comparing uniform to non-uniform motion (figures 7.6 and 7.7 on page 110). These figures offer a different way to visualize the same motions that students will be studying graphically. Showing this representation of uniform and non-uniform motion will be helpful for some students, but may overload others. I NTRODUCI NG TH E ACTIVITY Ask students why we used the ramp in the previous activities. Possible responses would be: “We wanted to get the ball going” or “It was speeding up on the ramp.” When students start saying “speeding up” or “go faster,” you can begin discussing the words accelerate, which means “to change velocity,” and acceleration, which is the rate of change of velocity (how quickly or slowly velocity changes). Below are two optional demonstrations. Kept brief, these can help the students shift from thinking about motion on a horizontal surface to motion on an incline, without reproducing the investigation they will do. In a place visible to the whole class, roll a tennis ball so that it moves uniformly across a few meters of a horizontal surface. Ask the students to tell you about the important features of its motion: Because it has constant speed and direction, it is moving uniformly. Now make a shallow V-shaped ramp by grasping two meter sticks side by side in one hand as shown in figure 7.12. Rest the bottom of 112 A is correct; both ramp sections have the same incline. B is wrong; the top half of the ramp is steeper than the bottom and the support box is not at the joint. IES PHY ion Force and Mot SICAL SER SCIENCE this V-ramp on the table, and hold the top of it only about 5 to 10 cm above the tabletop. Release the tennis ball at the top, and let it roll down the ramp. Ask the students how this motion is different. Is the motion uniform? Apparently not, since the ball is not moving at the very beginning and is moving later. What does happen after it starts rolling? It’s hard to tell by just watching, and so let’s study this in detail. Distribute or show instructions to students for assembling the ramp and ensuring that both of their ramp sections have the same incline. DOI NG TH E ACTIVITY Distribute materials and copies of Student Sheet 7, Rolling downhill, or pose an open-inquiry alternative. As you move around the room observing and talking with individuals and groups while they work, ask them to clarify what they are doing, what they see, and what they can conclude from it. Pose questions to help them solve any difficulties they encounter, and to get them to probe the underlying concepts or discuss how what they see connects with other things they have experienced. Challenge them to think of other ideas that their investigations lead to. Use the suggested responses below to guide student investigation and discussion. Keep in mind that investigation, objective observation, and ensuing scientific discussion are important to learning—as important as the answers themselves. This activity was designed for only a slight incline so that the timing can be done with stopwatches. What happens to the velocity when something is rolling down a hill? You can investigate this question by timing a ball rolling down the entire hill, and then timing it for shorter trips on only part of the slope. • Connect two track pieces together, and use them to make one long ramp. • Place the small ramp box under the joint between the two tracks. Turn the box so that its taller side faces uphill. It should hold the track prongs securely. • Set the high end of the ramp at 6.5 cm. • Make sure that the whole ramp has a uniform incline (no bend in the middle). 113 FIGURE 7.12 Making a V-ramp using two meter sticks SAFETY Caution students to keep control of the ball. If one falls to the floor, immediately pick it up so that it does not become a trip hazard. O P E N - I N Q U I RY A LT E R N AT I V E How does a ball’s velocity change as it rolls down a hill? Allow more time for this option. IES PHY Sketch figures 7.11 A and B in the “Getting Ready” section if you believe it will help students set up the system correctly. Setting the top end of the upper track at 6.5 cm and putting the ramp box at the joint between the two ramp pieces ensures that the inclines are uniform. Start ball and timer here Stop timing here for table 1 ion Force and Mot SICAL SER SCIENCE TEACH I NG TI P Before students start their data collection, make sure that the ramps are set up properly: ramp does not extend over the edge of the table, consistent incline (no bend in the middle); no jump or wobble of the ball at the joint or on any part of the ramp; and no movement or flexing of the track while the ball is rolling. A FIGURE 7.13 1. Time how long it takes the ball to go the full length of the ramp—from when you let it go at the top of the ramp to point A at the bottom. Mark the starting point so you start the ball in the same place each time. In table 1 record five good trials for the ball rolling from start to point A. Measure and record the distance the ball traveled. Enter the median time. Table 1: Time and distance for ball to roll full length of slope distance ball travels while being timed (cm) 110 (the total length of the ramp) trial number time (seconds) 1 2.57 2 2.47 3 2.43 4 2.54 5 2.50 median time: 2.50 The sticky arrows or masking tape are included in the materials list as a way for students to mark their start and end points. Instructions for doing this are minimal because students should already know from Activity 5 how to do this and why. Before collecting their data students should practice releasing the ball and starting the stopwatch consistently. Their practice timing efforts should not be recorded in the table. Data should not be entered in the table until students can comfortably repeat their ball release and timing so that the data is fairly consistent and not widely scattered. 114 TEACH I NG TI P Put a shallow box or lay a book at the end of the track just beyond measurement range to stop the balls before they fall off the table. IES PHY 2. Mark point B about three quarters of the way down the ramp. Release the ball just as you did in Question 1, and time how long it takes to go from start to B. Measure the distance from start to B. Complete table 2. B SICAL Make sure students always use the same start point— at the top of the ramp— for Questions 1 through 4. Always start the timer when the ball is released. Always do practice runs before collecting data. A FIGURE 7.14 Table 2: Time and distance for ball to roll down three quarters of the slope distance ball travels while being timed (cm) 85 trial number time (seconds) 1 2.12 2 2.16 3 2.22 4 2.18 5 2.15 median time: 2.16 Choosing a different ending point (B in the figure) may confuse some students. Help them understand that to study changes in velocity, we need to time the ball for different parts of its trip down the ramp. In the first table they timed it for the whole ramp. In this table they will time it for a shorter distance, only about three quarters of the ramp. They get to choose the point. It does not need to be exactly three quarters of the total ramp; anything close to that is fine. However, it is important to measure and record the distance they use. 115 SER SCIENCE TEACH I NG TI P Stop timing here for table 2 Start ion Force and Mot IES PHY ion Force and Mot SICAL 3. Mark point C about halfway down the ramp, as shown in the figure. Time the ball’s trip from start to C. Complete table 3. Stop timing here for table 3 Start C B A FIGURE 7.15 Table 3: Time and distance for ball to roll down half of the slope distance ball travels while being timed (cm) trial number 54 time (seconds) 1 1.75 2 1.75 3 1.71 4 1.87 5 1.72 median time: 1.75 4. Mark point D about one quarter of the way down the ramp from the top. Time the ball’s trip from start to D. Complete table 4. Start Stop timing here for table 4 D C B A FIGURE 7.16 116 SER SCIENCE IES PHY ion Force and Mot SICAL Table 4: Time and distance for ball to roll down the first quarter of the slope distance ball travels while being timed (cm) 15 trial number time (seconds) 1 1.35 2 1.38 3 1.22 4 1.34 5 1.28 median time: 1.34 5. Move your data for the distances and median times from tables 1 through 4 to the first two columns of table 5. Complete the last column by calculating the velocity of the ball for each ramp distance that you timed. Table 5: Average velocity of ball rolling on a slope for different periods of time. distance (cm) median time (seconds) average velocity (cm / sec) 110 2.50 44 85 2.16 39 54 1.75 31 30 1.34 22 0 0 0 Students will need to remember that dividing the distance traveled by the time gives the average velocity over the run. The ball is speeding up as it goes down the ramp, and so the final velocity is necessarily greater than the average velocity. For the case of constant acceleration (velocity increasing constantly with time, which it does in this case), the final velocity is exactly twice the average velocity. If we were to calculate acceleration, we would need the final velocity, rather than the average velocity, but this is harder to determine experimentally. We’ve chosen this simpler procedure (using average velocity) so that students can focus on the concepts and not get mired in the process. We added the (0,0) point because it is a legitimate data point; a part of what happened. The ball is released and the watch started at the same instant, and so at 0 seconds, it hasn’t gone anywhere and the velocity is zero. 117 SER SCIENCE IES 6. Key question: Use table 5 to make a line graph of average velocity vs. time. First you have to make the scale for the vertical axis. Include the point (0,0) on your graph, too. Make the line smooth, not jagged. It does not have to touch each data point, but it should go close to them. Average velocity (cm/s) PHY SICAL SER SCIENCE 50 40 30 20 10 0 S U M M A RY When the velocity of an object is changing, we say that it is accelerating. If the velocity is increasing, the object is accelerating forward; if the velocity decreases, it is accelerating backward, or decelerating. 7. Key question: From your graph what can you conclude about the motion of a ball traveling on a slope? The longer the ball is on the slope, the more its average velocity increases. This means the ball is accelerating. The line is straight, which means that the two variables—time on the slope and average velocity—are clearly related. If your students are ready, this is an excellent time to go into the proportional relationship implied by a linear graph. The average velocity is increasing proportionally to how long the ball is rolling. This certainly indicates that the actual velocity is increasing, too. In fact, the velocity at any specific time is proportional to how long it has been rolling, which means that the acceleration is constant. CO N C L U D I N G T H E A C T I V I T Y Question 7 includes the key concepts for this activity: • Acceleration is a description of how velocity changes. In this activity, there is acceleration because the speed changes. • A ball on a slope accelerates: The longer the ball is on the slope the faster it goes. • This is different from a ball rolling on a level track, where it does not speed up. The fact that the average velocity is proportional to the time is notable. It implies that acceleration is constant, and that the “instantaneous” velocity (the velocity at the particular time) is also proportional to how long the ball has been accelerating. It may be helpful to students if you draw sketches similar to figures 7.6 118 ion Force and Mot 1.0 2.0 Time (seconds) 3.0 FIGURE 7.17 Average velocity of a rolling ball on a slope vs. time it spends on the slope IES PHY and 7.7, visualizations comparing uniform to non-uniform motion. Transparencies 7.1 and 7.2 are graphs for students to interpret and discuss. They show a ball’s motion on ramps and level surfaces—accelerated and uniform motion. As you go through graphs A to F ask students to discuss how they could set up the ball-and-track systems they have been working with to produce each graph. Then go through the graphs again and ask students to describe an everyday situation that would produce each one. Graph D: Distance vs. time for the situation in Graph C. As the ball moves faster and faster, it can cover distances more quickly, so this graph is not linear. Graph E: Zero velocity for a period of time means it’s not moving. Then it starts speeding up linearly. This could be a graph of a ball held still on a ramp after the timer starts, and then the ball is released and accelerates. Velocity Time 0 Time Distance Graph C: The velocity is increasing with time. The ball is accelerating. This is what we just found for the motion of a ball rolling down a ramp in Activity 7, increasing in speed as it goes. 0 0 Time Velocity Graph B: If you used the same data from graph A but plotted distance vs. time instead of velocity vs. time, this is what it would look like. This is the same data that made graph A. As time increases, distance does too at the same rate. Distance Velocity Graph A: The velocity is not changing with time—it’s constant; the ball is not accelerating. This is what happens on a level horizontal track. Ask students what this same motion 0 Time plotted as distance vs. time would look like. Remind them that they made such a graph at the end of Activity 5. That’s the next graph, B. 0 Time 119 ion Force and Mot SICAL SER SCIENCE IES PHY ion Force and Mot SICAL SER SCIENCE 0 S EE G O I N G F U RT H E R Question Board The following are actual questions posed by students during this activity. They are not for display but rather are examples of the kinds of open-inquiry questions that students can generate and then pursue through hands-on investigations. • What if the ramp was not straight, and instead curved up? • What if we put a piece of tape right down the middle of the ramp? • What if we cover the ramp with a layer of tissue paper? • Is there a maximum speed where acceleration stops? Open-Inquiry Alternatives Instead of using the printed student activity, provide the same investigative materials and allow students to experiment with these. As they explore, ask them to develop and then pursue their own questions around the topic, “How does a ball’s velocity change as it rolls down a hill?” Other more specific questions offer a bit more guidance: What happens to the velocity of a ball while it is rolling down a hill? Does it change? How do you measure and show the change? Is the amount that it changes predictable? To provide even more guidance, prompt students to “measure how long it takes the ball to cover different lengths of a sloped track, and from that calculate its velocity along different parts of the slope.” 120 Time D Graph F: The ball accelerates for a period of time, and then the graph shows acceleration stops because velocity is constant. This could be the ball rolling down a ramp and then out onto a horizontal track. An everyday version of this graph would be the motion of a car on a city street. It starts from rest and speeds up until it is going at normal traveling speed. Imagine that it stays at constant speed until it gets to a stoplight. What would the graph look like if it were extended to show the car slowing down and stopping? More graphs are on the CD. Velocity An everyday version of this would be the motion of a car at a stoplight: It waits for the light to turn green, and then smoothly accelerates. It could also describe an apple that hangs in the orchard until one day it drops (now the direction of the velocity is down but we can still show the graph going up because the velocity is increasing). What would the distance vs. time graph look like for this motion? (It would be much like Graph D but would start with a horizontal line for the initial time period when it’s not moving.) TH E C IES PHY ion Force and Mot SICAL EXTENSIONS 1. Describe your velocity, and its changes, when riding your bike (or skateboard) on a level road, down a hill, and up a hill. 2. If we assume that the final velocity is twice the average velocity, we can calculate the acceleration of the rolling ball from acceleration = (final velocity — initial velocity) / time elapsed 4. Measure how long it takes for a car to get from a stop to 22 mph: 1 second, 5 seconds, or 20 seconds (assuming normal driving)? Measure how much longer it takes to change speed to 45 mph. And measure how much longer again it takes to get to 67 mph. And then measure how long it takes to slow the car back down from 67 mph to 45 mph, to 22 mph, and to a stop. Use the results to calculate the acceleration of the car for these six cases (note: 22 mph is 10 meters per second; 45 mph is 20 meters per second; and 67 mph is 30 meters per second). Finally, compare all of these to the acceleration for a falling object 9.8 (meters per second) per second. 5. Military aircraft and spacecraft can accelerate very fast. It becomes important to know whether the pilot can stand accelerations of 1 g, 2 g, or 5 g (meaning, 1, 2, or 5 times the acceleration of a freely falling object). How do these numbers compare with the accelerations we meet everyday, in elevators and cars? 121 EE TH E C D D TH E C S 3. (For students ready to grasp the mathematical representations of acceleration) When an elevator starts to move up or down, it has to accelerate: The velocity was zero, and now we want to go somewhere! But the passengers will get upset if the acceleration is more than a few meters per second per second. This limits how fast the elevator can be going after 10 seconds, and this in turn limits how far the elevator can go in this time. Halfway to its destination, the elevator must start slowing down again, too! So, about how far can an elevator go in 20 seconds? EE S The units for acceleration are “(meters per second) per second,” or m/sec2. You can calculate the acceleration of a falling object the same way, starting from the data gathered in Activity 1. The accelerations for the rolling ball and for the falling ball are very different. Both are constant but the falling object accelerates more quickly. SER SCIENCE IES PHY While the module does not address the idea of “g,” it is a logical extension from the basics of acceleration we have just covered. One g is the acceleration on Earth of a freely falling object—about 10 (m/sec)/sec. An accelerating car cannot get from 0 to 10 m/sec (22 mph) in one second, so its acceleration is much less than 10 (m/sec)/sec. One g is a panic stop made by slamming on the brakes in a car. Half a g is running a car going 20 mph into a bush that brings it to a stop in 1 meter—not quite the equivalent of running into a tree but close to it. 122 ion Force and Mot SICAL SER SCIENCE IES PHY Name ion Force and Mot SICAL SER SCIENCE Date STUDENT SHEET 7 Rolling downhill What happens to the velocity of a ball while it is rolling down a hill instead of along a level track? Does its velocity change? Can you predict how it changes? M AT E R I A L S 1 long ramp system 1 tripod base (A) 1 half-meter stick 1 height marker (B) 1 support bar (C) 1 ramp box (E) 2 tracks 1 metal ball 1 measuring tape or meter stick 1 stopwatch CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y 2 sticky arrows or masking tape What happens to the velocity when something is rolling down a hill? You can investigate this question by timing a ball rolling down the entire hill, and then timing it for shorter trips on only part of the slope. • Connect two track pieces together, and use them to make one long ramp. • Place the ramp box under the joint between the two tracks. Turn the box so that its taller side faces uphill. It should hold the track prongs securely. • Set the high end of the ramp at 6.5 cm. • Make sure that the whole ramp has a uniform incline (no bend in the middle). Start ball and timer here Stop timing here for table 1 A 123 IES PHY ion Force and Mot SICAL 1. Time how long it takes the ball to go the full length of the ramp— from when you let it go at the top of the ramp to point A at the bottom. Mark the starting point so that you start the ball in the same place each time. In table 1 record five good trials for the ball rolling from start to point A. Measure and record the distance the ball traveled. Enter the median time. Table 1: Time and distance for ball to roll full length of slope distance ball travels while being timed (cm) trial number time (seconds) 1 2 3 4 5 median time: CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y 2. Mark point B about three quarters of the way down the ramp. Release the ball just as you did in Question 1, and time how long it takes to go from start to B. Measure the distance from start to B. Complete table 2. Stop timing here for table 2 Start B Table 2: Time and distance for ball to roll down three quarters of the slope distance ball travels while being timed (cm) trial number time 1 2 3 4 5 median time: 124 (seconds) A SER SCIENCE IES PHY ion Force and Mot SICAL SER SCIENCE 3. Mark point C about halfway down the ramp, as shown in the figure above. Time the ball’s trip from start to C. Complete table 3. Stop timing here for table 3 Start C B A B A Table 3: Time and distance for ball to roll down half of the slope distance ball travels while being timed (cm) trial number time (seconds) 1 2 3 4 5 CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y median time: 4. Mark point D about one quarter of the way down the ramp from the top. Time the ball’s trip from start to D. Complete table 4. Start Stop timing here for table 4 D C Table 4: Time and distance for ball to roll down the first quarter of the slope distance ball travels while being timed (cm) trial number time 1 2 3 4 5 median time: 125 (seconds) IES PHY ion Force and Mot SICAL SER SCIENCE 5. Move your data for the distances and median times from tables 1 to 4 to the first two columns of table 5. Complete the last column by calculating the velocity of the ball for each of the four sloped ramp distances that you timed. Table 5: Average velocity of a ball rolling on a slope for different periods of time. distance (cm) median time (seconds) average velocity (cm / sec) 0 0 0 6. Key question: Use table 5 to make a line graph of average velocity vs. time. First you have to make the scale for the vertical axis. Include the point (0,0) on your graph, too. Make the line smooth, not jagged. It does not have to touch each data point, but it should go close to them. Average velocity (cm/s) CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y 50 Average velocity of a rolling ball on a slope vs. time it spends on the slope 40 30 20 10 0 1.0 2.0 Time (seconds) 3.0 S U M M A RY When the velocity of an object is changing, we say that it is accelerating. If the velocity is increasing, the object is accelerating forward; if the speed decreases, it is accelerating backward, or decelerating. 7. Key question: From your graph what can you conclude about the motion of a ball traveling on a slope? 126 IES 0 0 Distance Velocity CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y Distance Velocity PHY A. Time 0 C. Time 0 127 ion Force and Mot SICAL T R A N S PA R E N C Y 7. 1 B. Time D. Time SER SCIENCE IES CO P Y R I G H T © 2 0 0 6 , S A L LY S H A F E R A N D J O S E P H ST R A L E Y 0 Velocity Velocity PHY E. Time 0 128 ion Force and Mot SICAL T R A N S PA R E N C Y 7. 2 F. Time SER SCIENCE IES END OF SECTION INDEX NEXT