Impulse and Momentum The impulse-momentum theorem relates impulse, the average force applied to an object times the length of time the force is applied, and the change in momentum of the object: FAt = mvs - mv; Here, we will only consider motion and forces along a single line. The average force, F , is the net force on the object, but in the case where one force dominates all others, it is sufficient to use only the large force in calculations and analysis. For this experiment, a Dynamics Cart will roll along a level track. Its momentum will change as it collides with a hoop spring. The hoop will compress and apply an increasing force until the cart stops. The cart then changes direction and the hoop expands back to its original shape. The force applied by the spring is measured by a Dual-Range Force Sensor. The cart velocity throughout the motion is measured with a Motion Detector. You will then use data-collection software to find the impulse to test the impulse-momentum theorem. Figure 1 OBJECTIVES . Measure a cart's momentum change and compare it to the impulse it receives. . Compare average and peak forces in impulses. MATERIALS computer Vernier Dynamics Track Vernier computer interface Vernier Dynamics Cart Logger Pro Vernier Bumper and Launcher Kit Vernier Motion Detector Motion Detector Bracket Vernier Dual-Range Force SensorPRELIMINARY QUESTIONS 1. In a car collision, the driver's body must change speed from a high value to zero. This is true whether or not an airbag is used, so why use an airbag? How does it reduce injuries? Two playground balls, the type used in the game of dodgeball, are inflated to different levels. 2. One is fully inflated and the other is flat. Which one would you rather be hit with? Why? PROCEDURE 1. Measure the mass of the cart and record the value in the data table. 2. Attach the Motion Detector and bracket to one end of the Dynamics Track (see Figure 1). 3. Set the range switch on the Dual-Range Force Sensor to 10 N. Replace the hook end of the Dual-Range Force Sensor with the hoop spring bumper. Attach the Dual-Range Force Sensor to the bumper launcher assembly as shown in Figure 2. Then attach the bumper launcher assembly to the end of the track opposite the Motion Detector. Figure 2 Connect the Dual-Range Force Sensor to the bumper launcher assembly. Note: Shown inverted from how the sensor and assembly are attached to the track. 4. Place the track on a level surface. Confirm that the track is level by placing the low-friction cart on the track and releasing it from rest. It should not roll. If necessary, adjust the track to level it. 5. Set the Motion Detector sensitivity switch to Track. Connect the Motion Detector to a digital (DIG) port of the interface. Connect the Dual-Range Force Sensor to Channel 1 of the interface 6. Open the file "19 Impulse and Momentum" in the Physics with Vernier folder. 7. Remove all force from the Dual-Range Force Sensor. Click 8 Zero , select only the Dual- Range Force Sensor in the list, and click ok to zero the sensor. Part I Elastic collisions 8. Practice releasing the cart so it rolls toward the hoop spring, bounces gently, and returns to your hand. The Dual-Range Force Sensor must not shift, and the cart must stay on the track. Keep your hands away from the space between the cart and the Motion Detector. Physics with VernierImpulse and Momentum 9. Position the cart so that the front of the cart is approximately 50 cm from the spring. Click D Collect ; roll the cart so it bounces off the spring. 10. Study your graphs to determine if the run was useful. a. Inspect the force data. If the peak exceeds 10 N, then the applied force is too large. Roll the cart with a lower initial speed. b. Confirm that the Motion De lotion Detector detects the cart throughout its travel and that you can collection. see a region of constant velocity before and after the impact. If necessary, repeat data 11. Once you have made a run with good position, velocity, and force graphs, analyze your data. To test the impulse-momentum theorem, you need the velocity before and after the impulse. a. On the velocity vs. time graph, find an interval corresponding to a time before the impulse, when the cart was moving at approximately constant speed toward the Dual- Range Force Sensor. b. Select this interval and click Statistics, i. Record the average velocity for the initial velocity in your data table. C. In the same manner, choose an interval corresponding to a time after the impulse, when the cart was moving at approximately constant speed away from the Dual-Range Force Sensor. d. Select this interval and click Statistics, . Record the average velocity as the final velocity in your data table. 12. Calculate the impulse from the average force on your force vs. time graph. The impulse is the product of the average (mean) force and the length of time that force was applied, or FAt . a. Drag across the impulse, capturing the entire period when the force was non-zero. b. Find the average value of the force by clicking Statistics, , and record this value in your data table. c. Also read the duration of the time interval, At, over which your average force is calculated, which Logger Pro reports on the graph. Record this value in your data table. d. From the average force and time interval, determine the impulse, FAt , and record this value in your data table. 13. Repeat Steps 9-12 two more times to collect a total of three trials; record the information in your data table.mead. Part II Inelastic collisions 14. Replace the hoop spring bumper with one of the clay holders from the Bumper and Launcher Kit. Attach cone-shaped pieces of clay to both the clay holder and to the front of the cart, as shown in Figure 3. Figure 3 15. Remove all force from the Dual-Range Force Sensor. Click 8 zero ], select Dual-Range Force Sensor from the list, and click ok ] to zero the Dual-Range Force Sensor. 16. Practice launching the cart with your finger so that when the clay on the front of the cart collides with the clay on the Dual-Range Force Sensor, the cart comes to a stop without bouncing. 17. Position the cart so that the front of the cart is approximately 50 cm from the clay holder on the Bumper and Launcher Kit. Click D collect ; roll the cart so that the clay pieces impact one another. 18. Study your graphs to determine if the run was useful. a. Inspect the force data. If the peak exceeds 10 N, then the applied force is too large. Reshape the clay pieces and roll the cart with a lower initial speed. b. Confirm that the Motion Detector detects the cart throughout its travel and that you can see a region of constant velocity before and after the impact. If necessary, reshape the clay pieces and repeat data collection. 19. Once you have made a run with good position, velocity, and force graphs, analyze your data. To test the impulse-momentum theorem, you need the velocity before and after the impulse. a. On the velocity vs. time graph, select the interval corresponding to a time before the impact and click Statistics, . Record the average velocity for the initial velocity in your data table. b. In the same manner, select the interval corresponding to a time after the impact and click Statistics, . Record the average velocity as for the final velocity in your data table. 20. Calculate the impulse from the average force on your force vs. time graph. a. Select the impulse, click Statistics, , and record this value in your data table. b. Also record the length of the time interval, At, over which your average force is calculated. c. From the average force and time interval, determine the impulse, FAt , and record this value in your data table. 21. Repeat Steps 17-20 two more times to collect a total of three trials; record the information in your data table. Note: You will need to reshape the clay pieces before each trial. Physics with VernierImpulse and Momentum DATA TABLE kg Mass of cart 10.5 1177 kg % Final Initial Change Average Duration difference Trial velocity of Impulse Change in velocity force of momentum between VI velocity impulse FAt Vi (kg.m /s) or Impulse and (m/s) AV (m/s) (N) At (N.S) (s) (N.S) Change in (m/s) momentum Elastic 1 to-2358 6. 2944/ 0. 5302 1.27N 0 2 0.254 0. 27 5.90/0 2 -2.601 0 3099 0.57 1-338N 0-22 0. 294 0.29 0 010 3 8.2512 0.31130-56850-786IN|0-36 0.283 0-29 2410 Inelastic 1 O 6. 38590. 3859/ 6.82510.032 2 O 6 432 0.4320 3.324/10.08 6 159 3 O b. 41410 0.4140 4-87/10.046 ANALYSIS 1. Calculate the change in velocities and record the result in the data table. From the mass of the cart and the change in velocity, determine the change in momentum that results from the impulse. Make this calculation for each trial and enter the values in the data table. 2. If the impulse-momentum theorem is correct, the change in momentum will equal the impulse for each trial. Experimental measurement errors, along with friction and shifting of the track or Dual-Range Force Sensor, will keep the two from being exactly the same. One way to compare the two is to find their percentage difference. Divide the difference between the two values by the average of the two, then multiply by 100%. How close are your values, percentage-wise? Do your data support the impulse-momentum theorem? 3. Look at the shape of the last force vs. time graph. Is the peak value of the force significantly different from the average force? Is there a way you could deliver the same impulse with a much smaller force? 4. Revisit your answers to the Preliminary Questions in light of your work with the impulse- momentum theorem. ysics with VernierElastic 1 File Eda Erper sent Data Analyze Insan Options Page Help Force - 0.006 N 0.3 01- Position (m 01 O w - (41:0.20 Ax 0.000) Time (s) 0.4 0.2 Velocity (mis 0.0 02 0 (At:0.20 Av 0.000) Time (9) 1.5- 1.0 Force (i 0.5 0.0 (At:0.20 Ay:0.01) Time (s) More elastic trial 3 File Edit Experiment Data Analyze Insert Options Page Help but. Graphs FAQ Q V V/ / MONO Collect Force = 0.017 N 0.3- 0.1- Position (m) 01 (At:0.36 Ax:0.000) Time (s) 0.4 0.2 0.0- -0.2 0.4- 0 (At:0.36 Av:0.000) Time (s) 1.0 0.5 0.0Inelastic 1 Force -0.010 N E 08 0.4 02 0 2 0.787, 0.918) (41:1.004 Ax;0.000) Time (s) 1.5 1 10 05 0.0 05 0 (4t: 1 004 Av:0.00) Time (s) 10 5 Force (N 0 (At:1.004 Ay:0.00) Time (S) Inelastic trial 2 Logger Pro - 19 impulse and Momentum.ombl' File Edit Experiment Data Analyze Insert Options Page Help 1: Graphs AQQ F 1/ / NO Collect Force = 0.002 N 0.9 0.7- Position (m) 0.5- 03 (At:0,480 Ax:0.000) Time (S) 0.5 0.3 Velocity (m/s 0.1- -0.1- 0 2 (At:0.480 Av:0. 156) Time (s) orce (N)3 6 1.0 0.5- Velocity (mis 0.0 05 0 2 (At:1.004 4v:0.00) Time (s) 10 5- Force (N 0 (At:1.004 Ay:0.00) Time (9) Inelastic trial 2 Logger Pro - 19 Impute and Momentumanbit File Edit Experiment Date Analyze Insert Options Page Help 1: Graphs AQQ~ yz/ / XPOCollect Force = 0.002 N 0.9- E 0.7 Position 0.5 03- (At:0.480 4x:0,000) Time (S) 0.5 0.3 Velocity (mis 0.1- -0.1- 3 0 Time (S) (At:0.480 Av;0. 156) Force (N 0 Time (s) (At:0.480 Ay:0 00)Inelastic trial 3 68 : Graphs 10 0.8- 5 06- 2 0.4 02 2 3 (1.038, 0.928) (At:0 046 Ax:0.000) Time (s) 10 0.5 Velocity (m/s 00 0 Statistics for Latest | Velocity (4t:0.046 4v.0.009 2 0.3981 m 2.248 max. 0.4 Time (s) 10 5- Force (N min -0.8767 at 2 474 max. 9.904 8: 2 404 muart 4.870 median: 4 951 (At0.046 Ay:0.00) dev: 3.657 samples: 23 Time (s) By: 10.781