Lab 6 - Atwoods Machine and N2 Instructions

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Lab 6 – Atwood’s Machine & Newtons Second Law PHY110 Lab – General Physics Lab I Vernier/Video LAB Objectives 1. Measure the acceleration of the Atwood’s Pulley System using two different methods 2. Determine the total mass of the system by plotting the Net force vs. Acceleration 3. To verify Newtons Second Law stating that the Net force is proportional to the acceleration 4. Determine the friction that acts on the system
Equipment List: Vernier Software Atwood’s Machine – Full Video Vernier Data Files o Atwood’s Machine mass diff 4g o Atwood’s Machine mass diff 8g o Atwood’s Machine mass diff 12g o Atwood’s Machine mass diff 16g o Atwood’s Machine mass diff 20g o Atwood’s Machine mass diff 24g Stopwatch (easy touch-based stopwatch) Introduction Newtons Second Law of Motion can be modeled using a system called the Atwood’s Machine (as shown in Figure 1). It consists of two masses at the end of a thin string that passes over a pulley. Figure 1 – Atwood’s Machine Apparatus The difference in the two masses generates a net force on the system, causing the two masses to accelerate. According to Newtons Second Law, F net = m a (1) Where m is the mass of the system in kg, a is the acceleration in m/s 2 and F net is the net force in Newtons, the acceleration of the system is directly proportional to the Net force of the system. The Net Force of the system can be derived from the free-body diagram. Lets assume that m 2 is larger than m 1 . Therefore the resulting free-body diagram is modeled in Figure 2 where m 2 is pulling the system downward.
Figure 2 – The free-body diagram of m 1 and m 2 , assuming m 2 is pulling the system downward. T represents the tension in the string and the bottom force is the weight, or mg of each mass. The tension of the string is the same throughout, therefore the tension T in the free-body diagram for m 1 is the same as the tension in the free-body diagram for m 2 . The free body diagram gives the net force for each mass T m 1 g = m 1 a and m 2 g T = m 2 a (2) One can add the two equations simultaneously to eliminate the Tension variable (also unknown in the experiment) and to combine the equations into one m 2 g m 1 g = m 2 a + m 1 a (3) The expression can be reduced down to ( m 2 m 1 ) g = ( m 2 + m 1 ) a (4) Written this way, the expression models Newtons Second Law. The Net Force on the left is the difference in weight and on the right, the m is replaced by the combined masses ( m 2 + m 1 ) and a remains the net acceleration of the system. In the lab setting the masses can be measured with a triple beam balance or scale, and the acceleration can be measured either using kinematics or through Vernier Smart Pulley photogate measurement. The pulley will impart some friction on the system. We can rewrite equation 4 to incorporate the friction on the system with ( m 2 m 1 ) g f = ( m 2 + m 1 ) a (5) The friction can be added to the right side of the equation to model a linear relationship similar to y=mx + b. In this case, the y-axis will be the Net force, ( m 2 m 1 ) g , the x-axis will be a . This leaves the slope as the ( m 2 + m 1 ) or the total mass of the system and the y-intercept will represent the frictional force implied on the system. ( m 2 m 1 ) g = ( m 2 + m 1 ) a + f (6) The acceleration in this lab will be measured two ways. The first way is through the kinematic equation
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x = v i t + 1 2 at 2 (7) where x is the height from the bottom of the hanging mass of m 2 to the floor, vi is the initial velocity of the system which is zero, a is the acceleration and t is the time it takes for m 2 to reach the floor. The equation reduces to x = 1 2 at 2 (8) Figure 3 – Displacement, x , of m 2 . This remains fixed in the experiment. The time will change depending on the mass difference between m 1 and m 2 . Measuring the time (via stopwatch) and the distance, the acceleration can be calculated. Figure 3 gives a visual of the laboratory setup to measure x. The second way to measure the acceleration is the measure the change in velocity while the pulley is moving using a photogate as shown in Figure 4. The photogate has an infrared laser that passes through the spokes. The distance of the spokes and the time the laser is blocked is calibrated with the software, therefore, distance, time, velocity and acceleration can be measured using Logger Pro software.
Figure 4 – Photogate with the Vernier Smart Pulley in Lab. This lab will measure several accelerations for Atwood’s Machine for several different net forces ( m 2 m 1 ) g using a fixed mass total ( m 2 + m 1 ) . Because the pulley is not massless, some portion of the mass should be included in the total mass. Procedure Method 1 1. Open Video – Atwoods Machine – Full Video. Watch the prelab information if you haven’t completed it. At 4:00s in the video, the time trial data begins. https://qu.techsmithrelay.com/14IB 2. Using the video and a stopwatch, time how long it takes the heavier mass to reach the ground for the mass difference of 4g. Record the time in seconds. Note: Even though the instructor tries their best to coordinate a “3-2-1” and release, it may not be perfect. Be sure you start the stop at the point at which the instructor lets go of the masses. 3. Repeat this measurement two times for a total of three time trials. 4. Repeat this procedure with all of the mass differences and trials in the video. 5. Record all values in Data Table 2. 6. Calculate the average times 7. Convert the mass difference from grams kg. 1000g = 1kg. 8. Calculate the net force by Fnet = ( massdifference ( kg ) ) g 9. Calculate the acceleration by using the data from table 1 for delta x, and the average time from table 2 and the given kinematic equation ∆ x = 1 2 at avg 2 10. Plot the Net force on the y-axis and the Acceleration on the x-axis. Add the equation of the line and the R2. Label this graph as Method 1 Fnet vs Acc. 11. Record the slope of the graph. This represents the experimental total mass (m 1 + m 2 ) exp . 12. Record the intercept of the graph. This represents the frictional force in the pulley, f . 13. Record the R2 value. This represents the linear nature of your model. 14. Calculate the actual total mass (m 1 +m 2 ) act by using the data from Table 1. 15. Calculate the percent error of your total mass experimental and actual. % Error = Experimental Actual Actual * 100% Method 2 1. Open Logger Pro file “Atwoods Machine mass diff 4g”.
2. Using the Velocity vs. Time graph, highlight the section of the graph that represents a straight line. Ignore any other shapes the graph might make. Since there are two lines, you may do this one at a time, or do them both at once. 3. Select the “Linear Fit” Icon at the top of the screen to find the slope of the graph. 4. Select both Run 1 and Lastest. 5. Record the slope of the graph in Trial 1 and Trial 2 of Table 5. 6. Repeat for each file for each mass difference. 7. Calculate the average acceleration for the two values. 8. Calculate the net force of the system using the same equation as step 8 in Method 1. They are the same net force. 9. Graph the Net force on the y-axis and the Acceleration on the x-axis. Label this graph as Method 2 Fnet vs Acc. 10. Determine the graphical information listed on Table 6 similar to Method 1. Analysis Questions 1. What is the evidence for Newtons Second Law in a Net Force vs Acceleration graph? Do your graphs support the theory for Newtons Second Law in Method 1 and Method 2? CER 2. Which method was more accurate and why? CER 3. Friction becomes important when the percentage between friction and the net force are greater than 25%. Usually if the percentage were less than 5%, then the friction would be negligible and not a factor to consider when evaluating data. The frictional force comes from the y-intercept of your graph. The net force comes from the y-values of the graph. a. For each applied force, divide the frictional force to get a percentage for each method % Friction = friction force Net Force 100% Mass Diff (g) Net Force Percentage of friction Method 1 4 8 12 16 20 24
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Mass Diff (g) Net Force Percentage of friction Method 2 4 8 12 16 20 24 b. Analyze the percentage for each trial. i. Is there significant friction in one of the net forces? ii. This is the same pulley and ideally, you should see the same amount of percent friction in each method – do you see the same amount of friction percentages? 4. In the experiment, the mass was always transferred from one side of the pulley to the other side. Why was the procedure used instead of just adding mass to one side of the pulley to make a larger net force?