Mechanical Waves
A wave pulse is a disturbance that moves through a medium. A
periodic wave is a periodic
disturbance that moves through a medium. The medium itself goes nowhere.
The individual atoms and molecules in the medium oscillate about their
equilibrium position, but their average position does not change. If the
displacement of the individual atoms or molecules is perpendicular to the
direction the wave is traveling, the wave is called a transverse wave. If the displacement is parallel to the
direction of travel the wave is called a longitudinal wave or a
compression wave.
Waves can transport energy and information. Examples of mechanical
waves are water waves, sound waves, and seismic waves. All waves are described
mathematically in terms of a wave function, and reflection,
refraction and diffraction and
interference a characteristic behaviors of all types of waves.
In this session you will study wave motion in one dimension only, to learn
about several of these characteristic behaviors. You will visualize
the patterns of pressure variations associated with different sounds traveling
through air and you will examine the frequency content of those patterns.
You will produce standing sound waves in a tube and measure the speed of sound
waves in air.
Equipment needed:
- sound sensor
- resonance tube
- tuning forks and rubber block
- thermometer
Open a Microsoft Word document to keep a log of your
experimental procedures, results and discussions. Address the points highlighted in blue. Answer all
questions.
Exploration
Use an on-line simulation from the University of Colorado PhET
group to explore the behavior of waves on a string.
Link to the simulation:
http://phet.colorado.edu/en/simulations/wave-on-a-string
(a) Explore the interface. Try the different controls.
(b) Investigate the behavior of a wave pulse.
- Start with the following settings:
- Pulse
- No End
- Amplitude: 0.5 cm
- Pulse Width: 0.5 s
- Damping: none
- Tension: high
- Ruler and timer: checked
- Observe this pulse and measure its speed in cm/s.
(You can start and stop the pulse and use slow motion.)
- Vary (one at a time) amplitude, pulse width, damping, and tension, and
describe what happens.
- Return to the original pulse but change the end first to a loose end and then
to a fixed end and describe what happens.
(c) Investigate the behavior of a traveling wave.
- Start with the following settings:
- Oscillate
- No End
- Amplitude: 0.5 cm
- Frequency: 1.5 Hz
- Damping: none
- Tension: high
- Ruler and timer: checked
- Observe this wave (wave 1) and make measurements. Enter your measurements into the table.
- Measure the amplitude of the wave in cm.
- Measure the wavelength in cm.
- Measure the period in s.
- Find the speed of the wave in cm/s.
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wave 1 |
wave 2 |
wave 3 |
wave 4 |
wave 5 |
amplitude A |
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wavelength λ |
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period T |
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frequency f |
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speed v |
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- Move the amplitude slider to 0.25 cm (wave 2)
and then to 0.75 cm (wave 3).
Make new measurements. Describe what changes.
- With the amplitude slider at 0.5 cm, move the frequency slider to 1 Hz (wave 4) and then to
2 Hz (wave 5).
Make new measurements. Describe what
changes.
- Discuss the relationships between wavelength and frequency, period and
frequency, amplitude and frequency and speed and frequency.
- Can you change the speed of the wave? What can you do to produce a
wave that moves with approximately 1/4 the speed of wave 1.
- Describe what happens when you include damping.
(d) Investigate the behavior of a standing wave.
- Start with the following settings:
- Oscillate
- No End
- Amplitude: 0.5 cm
- Frequency: 0.75Hz
- Damping: 1 notch
- Tension: high
- Ruler and timer: checked
- Describe the wave. What is its maximum amplitude in cm? Does
this maximum amplitude change when you change the frequency slider?
- Change the end to a fixed end.
- Slowly increase the frequency.
Wait several seconds to see what happens to the maximum displacement
from equilibrium of the wave for each frequency setting.
- For which frequencies between 0.75 Hz and 1.7 Hz is the maximum displacement from equilibrium
largest (larger than that of the traveling wave)? In other
words, for which frequencies do you hit resonance? What happens if you set
the damping to zero at those frequencies?
- What can you say about the wavelengths associated with those frequencies?
Sound
Experiment 1
Most sounds we hear are not single sound pulses but more complex sound
patterns. We will now explore some of those sound patterns.
(a) Compare the output of a sound sensor (microphone) for a clapping and a
humming sound. The sound sensor is an electrets condenser microphone which
converts pressure variations into voltage variations which can be recorded and
displayed by the computer.
- Make sure the Pasco 850 interface is turned on. Open the Capstone program.
- Plug the Pasco sound sensors into Analog Channel A of the interface.
- Click Hardware Setup, Analog Channel A and choose to add sound sensor.
- Set the sample rate to 10 kHz.
- Drag the "Graph" icon onto the page.
- In Continuous Mode, collect sensor voltage (Sound Intensity (V)) versus time data for a single clap
and for a continuous humming sound, for example "ahhhh".
Adjust the voltage and time scales to zoom in so you can see more details.
Paste your graphs into your Word document. How do the microphone voltage patterns
compare? Describe your observations.
(b) Compare the output of a sound sensor for a humming sound and the
sound produced by a tuning fork.
- Delete the "Graph" display and delete all data runs.
Drag the "Scope" icon onto the page. Measure sensor voltage
(Sound Intensity (V)) versus time.
- Reset the sample rate to 10 kHz. Choose Fast Monitor Mode.
- Press "Monitor" and again hum into the sensor.
- Adjust the "time and voltage scales until you get
a good display of several cycles of the signal.
- When you have a stable signal click the Stop button.
Paste your graph into your Word document. Does your humming sound wave have a
definite frequency? How do you justify your answer?
- Pick a tuning fork. Strike the tuning force against a rubber block. Never strike the fork
against a hard material. Monitor the sound produced by the tuning
fork with the sound sensor and display the output on the Scope.
- Adjust the "time and voltage scales until you get
a good display of several cycles of the signal.
- When you have a stable signal click the Stop button.
Paste your graph into your Word document. Does the tuning fork producing a pure
sine wave? How does the wave of the tuning fork sound compare to the waveform
of the humming sound?
(c) Any wave pattern can be produced by
superimposing the appropriate sinusoidal waves. Breaking up the
original sound wave into its sinusoidal components is called Fourier analysis. We can find the
frequencies and amplitudes of the sine and cosine waves that must be added to
produce our sound wave. We will choose the "Fast Fourier Transform" or FFT
display to let Capstone perform Fourier analysis on a sound.
- Drag the FFT icon onto the same page as the Scope. Choose to
measure the Sound Intensity (V).
- Reset the sample rate to 10 kHz. Choose Fast Monitor Mode.
- Click the Monitor button and then start humming.
- When you have a stable signal click the Stop button.
Paste your graphs into your Word document. What frequencies are strong in your
"ahhh" sound?
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Obtain a Fast Fourier Transform of the sine wave
signal.
What frequencies are present in this signal?
- Start humming the "ahhh" sound again and form the FFT
of this signal. Without changing the pitch of your voice, change the
sound from "ahhh" to "eee".
What happens to the frequencies shown in the FFT?
Experiment 2
When you produce a sound, air from the lungs is pushed
through the vocal folds. This produces a train of air pulses.
As you speak, muscles in your larynx tighten the vocal folds. When
air from your lungs passes through the folds, they vibrate.
Vibrations at the resonance frequencies have the largest amplitudes. The
tighter the vocal cords, the higher are the resonance frequencies and
the higher is the pitch of your voice.
The pulse train produced by the
vocal folds is shaped by the resonances of the vocal tract. The
vocal tract acts like a variable filter. It is a filter because it
amplifies certain frequencies and suppresses others. It is
variable because by changing the position of your tongue, jaw, lips,
etc. you can change the overall frequency response.
Link: The Human Voice
Develop a hypothesis to explain the frequency pattern observed when you make the "ahhh" sound.
You will now use a resonance in a tube as a variable filter.
The tube has one open and one closed end. The length of the tube can be
varied by moving a piston. You will produce resonances for a fixed
frequency by varying the length of the tube.
- Position the sound sensor close to the open end of a
resonance tube.
- Click the Monitor button and monitor the oscilloscope and the FFT display.
- Pick a tuning fork. The frequency f with which it oscillates is
stamped on the fork. Hold the rubber block still and strike the tuning
fork against it.
- Hold the fork near the open end of the resonance tube.
Start with a zero-length tube and move the piston
until you find the 1st harmonic.
You will hear the loudest sound and you will also see the maximum peak
voltage on the oscilloscope display.
- Record the tube length for the 1st harmonic in table 1.
- Does the frequency f of the sound you read of the FFT display agree with
the frequency stamped onto the tuning fork?
- Move the piston until you find the 3rd harmonic. Record the tube
length for the 3rd harmonic in table 1.
- Can you find the 5th harmonic? If yes, record the tube length for
the 5rd harmonic in table 1.
- Measure the air temperature and record it in table 1.
- Repeat the experiment with a different tuning fork.
Table 1 (tube length)
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1st harmonic |
3rd harmonic |
5th harmonic |
frequency (Hz) |
temperature oC |
fork 1 |
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fork 2 |
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Analyze your data and complete table 2.
Table 2
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frequency f |
wavelength λ |
temperature TC |
speed
v = λf |
fork 1 |
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fork 2 |
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Compare your experimentally obtained value for the speed of sound with the
value obtained from the formula
v = (331.4 + (0.6/oC)TC) m/s.
Experiment 3
In the previous experiment you measured the speed of sound
by measuring the wavelength and frequency of a sinusoidal wave and
using v = λf. In this experiment you will measure the speed of sound directly.
- Delete the Scope and the FFT display and drag the "Graph" icon onto the page.
- Reset the sample rate to 10 kHz. Choose Continuous Mode.
Move the piston as far as possible to one end of the
resonance tube. Set up the microphone at the open end of the tube.
Your goal is to record the sound of your fingers snapping and then the echo of
the snap after it has traveled the length of the tube and back.
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What data must you collect in this experiment to measure the speed of sound in the tube?
- Estimate the time interval between the original sound and the echo reaching the sensor.
- Using your collected data, calculate the speed of sound in the tube.
- Repeat your measurement at least five times. How do you use the five or more measurements to
determine your best experimental value for the speed of sound?
- How do you estimate the uncertainty in this value?
- Do you think your experimental value for the speed of sound would change if you heated up the air in the tube?
Convert your log into a lab report.
Name:
E-mail address:
Laboratory 11 Report
- In one or two sentences, state the goal of this lab.
- Make sure you completed the entire lab and answered all parts. Make
sure you show your work and inserted and properly labeled relevant tables
and plots.
- Add a reflection at the end of your report in a short essay format.
Save your Word document (your name_lab11.docx), go to Canvas, Assignments, Lab
11, and submit your document.