P09_Waves

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Old Dominion University Physics 111/226/231/261 Lab Manual 1 OLD DOMINION UNIVERSITY PHYS 111 PHYS 226/231/261 P09 – WAVES Submitted By: 1. 2. 3. Submitted on Date Lab Instructor
2 Experiment P09: Waves Waves Experiment P09 Objective Study the formation of standing waves on a vibrating string Materials Digital Function Generator Digital Scale String Vibrator Mass Hanger, Large, 50 g Large C-Clamp Banana-Banana Cable, x2 (1 red, 1 black) Elastic Wave String Slotted Mass Set Pulley w/Table Clamp Meter Stick Power Cable Theory A standing wave is one that oscillates with time but remains fixed in its location. In a string of length L that is tied down at both ends, standing waves are visible on the string if the string is vibrated. The standing waves have a sinusoidal appearance equal displacement above and below a zero-amplitude line. The points on a standing wave that remain fixed (zero displacement) are called nodes , and the points of maximum displacement are called anti-nodes . The frequency of a standing wave is equal to the number of complete waves that pass a fixed reference point in one second . The wavelength of a standing wave is equal to the distance between consecutive anti-nodes . The velocity of a wave traveling along a string depends only on the properties of the string, not on the frequency or wavelength of the wave. The velocity of a wave traveling on a string is given by: v = Tension mass per unitlength = F σ (1) where v is velocity, F is the weight (in Newtons) of the mass m hanging from the string, and σ (sigma) is the linear density of the string in units of kilograms/meter. The velocity v , frequency f , and wavelength of a wave are related by: λ v = (2) For standing waves on a string, the wavelength, is λ twice the distance between nodes ( = 2d). λ However, because the period T and frequency f are related by: T = 1 f (3) we can express also wavelength as: λ λ = vT (4)
Old Dominion University Physics 111/226/231/261 Lab Manual 3 The linear density (mass per unit length) of the string is found by: σ = M L (5) where M is the mass of the string in kilogram, and L is the length of the string in meter. Procedure In this experiment, you will use a frequency generator (Pasco Digital Function Generator) to drive a speaker that vibrates one end of a string. The other end of the string passes over a pulley and has a slotted mass hanging from it to provide tension in the string. The tension ( F ), in Equation (1) is the weight (in Newton) of the slotted mass ( m ), hanging from the string. The linear density ( σ ) is in kilogram/meter (kg/m). For standing waves on a string, the wavelength ( ), is twice the distance λ between nodes ( = 2d). λ Equipment Setup 1. Measure the length of the elastic wave string. ( Note: all knots must be removed!) Use a digital scale to measure the mass of the elastic wave string. Record the values in Data Table 2. 2. Take the large C-shaped clamp and use it to secure the String Vibrator to the table. There is even a spot on the vibrator that says, “Clamp Here”. 3. Plug one red and one black banana-banana cable into the red/black ports on the Function Generator and then plug the other end into the string vibrator. 4. Attach the Pulley table clamp to the opposite edge of the lab table. 5. a) Tie a small loop on the end of the elastic wave string hanging over the pulley assembly. b) Attach a 50 g mass hanger to the elastic wave string hanging over the pulley. Then add 450 grams to the hanger. Figure P09.2: Pulley Figure P09.1: String Vibrator
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4 Experiment P09: Waves 6. a) Align the position of the string vibrator and pulley assembly so that the elastic wave string forms a straight line when viewed from above. b) Adjust the height of pulley so that the elastic wave string forms a horizontal line with respect to the table. Data Collection 1. Turn-on the function generator and adjust the frequency knob to reduce the frequency to between 7-10 Hz . Set the function generator to produce a sinusoidal (~) waveform (the top choice). 2. Adjust the frequency to find the first harmonic standing wave in the string (you will see one antinode with a node on each end). Finely tune the ‘frequency’ knob as necessary until you get the largest antinode possible. The amplitude knob should probably be somewhere in the middle of its range. 3. Measure the distance between nodes for the first harmonic standing wave and note the frequency. Record these values in Data Table 1. 4. Slowly increase the function generator frequency until the string vibrates at the second harmonic standing wave (2 antinodes, 3 nodes ) . Make slight adjustments to the frequency and amplitude controls to obtain the maximum amplitude of antinodes. Measure the distance between all adjacent nodes and record the frequency. Record the values in Data Table 1. 5. Find as many consecutive harmonics (# of antinodes) as you can see on the string until you have reached the tenth harmonic (10 antinodes). Measure the distance between all adjacent nodes and note the frequency for each harmonic found. Record the values in Data Table 1. 6. For each harmonic, calculate the average distance between the nodes and then calculate the wavelength of the standing wave. Record the values in Data Table 1. Show your work for the third harmonic. 7. For each harmonic, use Equation (2) to calculate the velocity of each standing wave. Record the values in Data Table 1. Show your work for the third harmonic in the data section of your lab report. For the linear density of the string use the value σ = 0.00295 kg / m . Because our string is elastic, and stretches as we add tension, the linear density is not constant. We have obtained this average value from previous semesters and should work well for your experiment. 8. Find the average of all your wave velocities and record this in Data Table 2 as υ ave . 9. Use F=ma to calculate the tension in the string (don’t forget to include the mass of the hanger along with any mass you added), and then use Equation (1) to calculate the theoretical velocity of waves on the string. Record the value in Data Table 2 as υ theoretical . Show this calculation in your lab report.
Old Dominion University Physics 111/226/231/261 Lab Manual 5 10. Calculate the percent error between the velocity of the waves on the string from the graph and the theoretical velocity calculated from Equation (1). Record the value in Data Table 2. Show your work in the data section of your lab report. % error = | theoretical velocity measured velocity theoretical velocity | × 100 Graphing vs T λ 11. In a spreadsheet program of your choice, create two columns: one column with your frequency data and one with your wavelength data. 12. In a third column, have your program calculate the period T of the wave at each frequency. This comes from equation (3). 13. Create a plot of wavelength versus the period. Be sure to correctly label the axes of the graph and include units. 14. Add a linear trendline to the data and display the equation on the chart. 15. Use the slope of the data, in conjunction with Equation (4), to determine the velocity with which the waves travel along the string. How does this value for the wave velocity compare to the value you found before and the theoretical value?
6 Experiment P09: Waves Data Table – Experiment P09 Data Table 1 Standing Waves on a String Harmonic (# Anti-nodes) H Distance Between Nodes d n Sum of d n = d tot Average Distance Between Nodes (m) Frequency of Harmonic f (Hz) Wavelength of Harmonic λ = 2 d ave (m) Velocity of the Wave v = (m/s) 1 m 2 m m 3 m m m 4 m m m m 5 m m m m m 6 m m m m m m 7 m m m m m m m 8 m m m m m m m m 9 m m m m m m m m m 10 m m m m m m m m m m Data Table 2
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Old Dominion University Physics 111/226/231/261 Lab Manual 7 Standing Waves on a String – Velocity Comparison Linear Density of String ( σ ) 0.00295 kg/m Mass of Hanging Object ( m ) kg Tension on the String ( F ) N Average Wave Velocity ( υ ave ) m/s Theoretical Wave Velocity ( υ theoretical ) m/s % Difference ( υ ave Vs υ theoretical ) % What to Turn In Full lab report Data Tables 1 and 2 Graph of vs T λ Do not turn in the questions listed below. However, these questions can be used as a guideline for the types of things to consider when writing your report. However, do NOT directly rewrite and answer them. Questions to Consider Examine the velocity graph you plotted. Did your data points fall nicely on a straight line? Based on the percent error you found, what were the possible sources of error that that affected your results? If you added additional mass to the string, what variable in equation (1) would this affect and how would this affect the frequency of the harmonics you found? How would your results have changed if the string had a higher linear density? How does the velocity of the waves on the string compare to the velocity of a car (in m/s), on a highway or with the velocity of sound waves (in m/s), in the air? If you set up a standing wave of 6 antinodes, how many antinodes will occur in if you triple the frequency? How many wavelengths will there be? Explain your answer.