Maxwell Wheel PHYS101 Past Paper PDF 2015

17-Nov-2015 PHYS101 - 10 MAXWELL WHEEL Objective To test the conservation of energy in a system with gravitational, translational and rotational energies. Introduction A wheel is suspended by two cords wr...

17-Nov-2015 PHYS101 - 10 MAXWELL WHEEL Objective To test the conservation of energy in a system with gravitational, translational and rotational energies. Introduction A wheel is suspended by two cords wrapped on its axis. After being released from rest, it unrolls from its cords and moves downward in the gravitational field. Figure 1 shows the initial stage. As time increases, more and more of the initial gravitational potential energy Ug of the system is converted to translational kinetic energy KT and rotational kinetic energy KR. Adjusting Screw Motion Sensor s0 ~ 20 cm Cord Initial Position Maxwell Wheel Spindle Figure 1 © KFUPM – PHYSICS 1 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 The total energy E = Ug + KT + KR of the system is conserved if friction is negligible. This implies that E = Einitial That is, Ug + KT + KR = Ugi + KTi + KRi If the system starts from rest, then its initial linear velocity v0 and initial angular velocity 0 are zero. This implies that KTi = ½ m v02 = 0 KRi = ½ I 02 = 0 where, m is the mass of the Maxwell wheel-spindle system and I is its moment of inertia about the axis of rotation. Therefore, Ug + KT + KR = Ugi This means that if there are no friction losses, the energy of the system at any point will remain constant and be equal to its potential energy at the start. Now, we want to express KT = ½ m v2 and KR = ½ I 2 in terms of variables that can be easily measured in this lab. We will release the wheel with zero initial velocity, and the center of mass of the wheel goes down with constant linear acceleration a. Therefore, from v2 = v02 + 2 a y v2 = 2 a y Furthermore, if the radius of spindle of the wheel is r, see Figure 2, then v  r Therefore, 1 KT  m v2  m a y 2 1 I KR  I 2  2 a y 2 r Note that as y increases, both kinetic energies increase. © KFUPM – PHYSICS 2 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 Spindle 2r Figure 2 Initial Position s yref Reference Position Ug = 0 y = ss0 Figure 3 © KFUPM – PHYSICS 3 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 The gravitational potential energy of the system can be expressed as U g  m g ( yref  y) where, y is the vertical distance traveled, see Figure 3, and we have set the value of the gravitational potential energy to zero at y = yref. That is, Ug = 0 at y = yref. The motion sensor measures the distance away from it as positive, and since the sensor is mounted above the moving object the downward direction will be taken as positive by the sensor. Therefore, Ug = mg(yref – y), and not mg(y –yref). Note that as y increases, the potential energy decreases. In this lab, you will use a motion sensor with DataStudio for collecting data and Excel for analyzing the data. You will verify that the linear acceleration of the system is constant. You I will notice that r being very small compared to the radius of the wheel, 2 is much greater r than m and thus KT is very small compare to KR. You will also verify that all three energy terms are linearly proportional to the vertical displacement y and the potential energy reference is entirely arbitrary. That is, only the changes in potential energy are physically meaningful, and hence you can add a constant to the potential energy without affecting the physics. Part 1 – Finding the constant acceleration a In this exercise, you will determine the acceleration by fitting position versus time graph to a quadratic function, Y = A t2 + B t + C. The second derivative of the function is the acceleration, which is equal to 2 A. 1. Download the file Maxwell Wheel.ds from the link in phys101 homepage and save it on the desktop. This file has been preconfigured for optimum experimental parameters such as position and time scales. 2. From the Start batton, go to All Program → DataStudio → English. This will open DataStudio. Click on Open Activity, navigate to the folder desktop and to the file Maxwell Wheel.ds, and open it. This will open the position-time graph. 3. Make sure the motion sensor is connected to a computer through the USB interface, and its range switch is set to work with the (short range) option. Also make sure the Ultrasonic Transducer is horizontal. You can use the Rotating Head to adjust the angle of the sensor, if needed. This alignment is very important for getting good results. © KFUPM – PHYSICS 4 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 4. Make sure the wheel is hanging horizontally. If not, use the adjusting screw to make it horizontal. Carefully roll up the wheel on its cords until it is about 20 cm from the sensor. This is important because the motion sensor cannot detect any object within 15 cm. Be sure that the cord winding runs inward (see Figure 1), so that the wheel will descend smoothly. If at any time the wheel begins to wobble and move erratically, you must gently catch it and do a proper job of rewinding. 5. Release the system from rest and click the start button in DataStudio simultaneously. This step should preferably be done by the same person. Click the stop button just before the system unwinds completely. 6. Your data will look like the red curve in Figure 4. Click on the Fit button in DataStudio and then select Quadratic Fit. The blue curve in Figure 5 shows the fit. The fitting parameter A is related to the acceleration a of the system, through a = 2 A. Note that a perfect quadratic fit would confirm the constant acceleration. Make sure the initial slope (parameter B) is zero (or very close to zero), which confirms v0 = 0. If not, repeat the experiment. The magnitude of the value of B from the quadratic fit should be < 0.01 to ensure initial speed is very close to zero. 7. Write down the acceleration in your report. Figure 4 © KFUPM – PHYSICS 5 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 Part 2 – Testing conservation of energy In this exercise, you will test the conservation of energy by plotting KT, KR, Ug and E versus y. 1. The diameter of the spindle is measured to be 6.0 mm. record this value in your report. 2. Export your data of Exercise 1 from DataStudio to Excel. To do this, choose Export Data…, from File menu. You will be presented with the Export Data box. Make sure you have chosen position data from the list and then click OK button. Save the data as text file in the desktop with an appropriate name (e.g. position.txt) 3. Now open Microsoft Excel. Click the office button and click Open. Navigate to the folder where you have saved the position.txt data file and open that file. (If you don’t see the file, choose All files(*.*) in the files of type). This will bring up the text import wizard – step 1 of 3. Just click the Finish button. 4. The first column of the data is time in seconds and the second column is the position (s) of the wheel, in meters, relative to the sensor. To find y, the vertical distance travelled, the initial-position value s0 should be subtracted from the position values. Do this in column C. Follow the instructions from Step 1 to Step 2 in the Appendix at the end of this write up and then return here to Step 5. 5. Now you have to input the values of radius of the spindle r, reference point for potential energy yref, mass m, moment of inertia I, acceleration a and define names for them. Choose the yref as the final y-value of your data. Follow the instructions from Step 4 to Step 7 in the Appendix and then return here to Step 6. 6. Calculate in Excel KT, KR, Ug, and E using the equations given in the Introduction section. Record these values in columns D, E, F, and G respectively. To do this, follow the instructions from Step 9 to Step 10 in the Appendix and then return here to Step 7. 7. To plot KT, KR, Ug, and E as a function of y on the same graph, select the values, including the labels, in columns C, D, E, F, and G, and insert scatter plot. Answer the following depending on the plot generated using Excel: a) Describe the behavior of the translational kinetic energy KT. b) Describe the behavior of the rotational kinetic energy KR. c) Describe the behavior of the gravitational potential energy Ug. d) Describe the behavior of the total mechanical energy E. © KFUPM – PHYSICS 6 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 8. In fact E decreases slightly as y increases, suggesting the presence of non- conservative force such as rolling friction between the cord and spindle. Since the change in mechanical energy is the work done by the non-conservative forces on the system, the slope of the E versus y graph represents the rolling friction. Find the linear trendline of the E versus y graph. The absolute value of the slope is the magnitude of friction. Note that it is very small. Write down the magnitude of the force of friction. Part 3 – Reference for gravitational potential energy is arbitrary In this exercise, you will confirm that physics does not change by changing the reference for gravitational potential energy. 1. In your Excel worksheet of Exercise 2, choose the yref as the initial y-value (zero) of your data, type 0 in cell J3, and press Enter key. This will automatically change Ug values in column F and re-plot the graph. Note that although the appearance of the graph has changed, the physics is not. a. Describe the behavior of the translational kinetic energy KT. b. Describe the behavior of the rotational kinetic energy KR. c. Describe the behavior of the gravitational potential energy Ug. d. Describe the behavior of the total mechanical energy E. e. Write down the magnitude of the force of friction. 2. Repeat Step 1 for another value of yref , say the middle y-value of your data. 3. Save your Excel worksheet using Save As  Excel Workbook from File menu and send this file by email to your instructor. 4. Write down a suitable conclusion for this experiment. © KFUPM – PHYSICS 7 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 APPENDIX Using Excel to do the calculations 1. Type the heading y(m) in cell C2 and type the formula =B3-$B$3 in cell C3 and Enter. This makes the position y=0 at t=0. 2. To write other values of y, click on cell C3 and use the left mouse button to press on the small square at the lower right corner of the cell and drag it down to the last data to be entered in that column. Note that $B$3 remains the same in all the cells and therefore, it is called absolute reference. In this way, you make sure always s0 is subtracted from s to find the corresponding y. 3. Return to step 5 in Exercise 2 of the write-up. 4. Type radius (m) in cell I2, yref (m) in cell J2, m (kg) in cell K2, I (kg.m2) in cell L2, and a (m/s2) in cell M2 as shown below. Also enter the values of m (0.450 kg) and I (0.00100 kg.m2) in cells K3 and L3, respectively. 5. In cell I3 type in your measured value of the radius (diameter/2) of the spindle in meters. In cell J3 type in the last data of column C. This puts zero reference level for the potential energy at the end position of the Maxwell wheel. In cell M3 type in the value of a you found in Exercise 1. 6. Select cell I3 and type radius in the Name box area and Enter. This defines the value of radius to be the value in the cell I3. © KFUPM – PHYSICS 8 Department of Physics revised 17/05/2017 Dhahran 31261 17-Nov-2015 PHYS101 - 10 7. Then select J3 and type yref in the Name box area and Enter. This defines the value of yref to be the value in the cell J3. Similarly give the names m, I and a for the cells K3, L3 and M3, respectively. 8. Return to step 6 in Exercise 2 of the write-up. 9. Type in the headings in the 2nd row and the formulas in 3rd row of columns D, E, F and G as shown below: 10. To write other values of KT, KR, Ug, and E, select the four cells D3 to G3 in row 3 and use the left mouse button to press on the small square at the lower right corner of the cell G3 and drag it down to the last data to be entered. 11. Return to step 7 in Exercise 2 of the write-up. © KFUPM – PHYSICS 9 Department of Physics revised 17/05/2017 Dhahran 31261