Speed of Sound Lab
Transcript of Speed of Sound Lab
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PURPOSE STATEMENT:
The purpose of the experiment was to calculate the speed of sound by measuring and using the
time it took for an echo to travel down and back a tube (of a certain length) that was closed on
one end, using a Vernier microphone and a computer. The distance that the echo traveled divided
by the time it took to get back to the source would be used as the speed of sound.
DATA:
Important Data (premeasured):
Length of Tube (m) 0.610
Total Length to be Traveled by the Sound (m) 1.22
Temperature of Room (degrees Celsius) 24.5
Echo Test Trials: Time Intervals From Initial Source of Sound to Reception of Echo
Trial Total Travel Time (s)
1 0.00346
2 0.00344
3 0.00344
4 0.00348
5 0.00340
Average 0.00344
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CALCULATIONS:
1. The following is a calculation of the average travel time of sound, or average time
interval between the creation of a sound and the reception of its echo, based on the data
collected in the Echo Test Trials.
Average Time Interval = Time1+Time2+Time3+Time4+Time5
Number of Trials
Average Time Interval =
(0.00346 s )+(0.00344 s )+ (0.00344 s )+(0.00348 s )+(0.00340 s)+(0.00344 s)5Trials
Average Time Interval = 0.00344 s
2. The following is a calculation of the speed of sound based on experimental/measured
values. The average time interval is used as the time value in the calculation.
Speed of Sound = DistanceTraveled ( twicethe lengthof the tube)
TimeTaken(average timeinterval)
Speed of Sound = 2(0.610m)(0.00344 s)
Measured Speed of Sound = 355 m/s
3. The following is a calculation of the theoretical value for speed of sound at a the
temperature at which the experiment was conducted.
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Theoretical Speed of Sound = 331.5 + 0.607(T)
Theoretical Speed of Sound = 331.5 + 0.607(24.5°C)
Theoretical Speed of Sound (at 24.5°C) = 347 m/s
4. The following is a calculation of the percent difference between the measured value for
speed of sound and the theoretical value for the speed of sound at 24.5°C.
Percent Difference = vs ( experimental )−v s( theoretical)
vs (theoretical) x 100%
Percent Difference = (355m /s )−(347m /s)
(347m /s) x 100%
Percent Difference = 2.31 %
CONCLUSION:
The experiment seemed to be pretty successful, as the measured value for the speed of sound at
24.5°C was very close to the theoretical value of sound. The measured value for the speed of
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sound was 355 m/s whereas the theoretical value for speed of sound was 347 m/s. The small
percent difference between the measured value and the theoretical value (2.31%) is further
indication that the measured value for sound is relatively close to the theoretical value of sound.
The results for the trials conducted to measure the time intervals between the production of a
sound and the reception of an echo are supporting evidence for the precision of the experiment.
As can be noted, the values measured for the total travel time (time interval) for each trial were
relatively close to each other. In Trial 1, the total travel time was recorded as 0.00346 s; in Trial
2, the total travel time was recorded as 0.00344 s; in Trial 3, the total travel time was recorded as
0.00344 s; in Trial 4, the total travel time was recorded as 0.00348 s, and in Trial 5, the total
travel time was recorded as 0.00340 s. The largest difference of total travel times was between
the value recorded in Trial 4 (0.00348 s) and the value recorded in Trial 5 (0.00340 s), and the
difference between the values is only 0.00008 s, a very small number in comparison to the values
for total travel time. This thus indicates that the conduction of the experiment was very precise.
Despite the fact that the experimental/calculated values were very close to the
theoretical/accepted values, there are various sources of error that could have made the
experimental values inaccurate. For example, the measurement for the temperature of the room
could have been inaccurate if the temperature probe was not calibrated or did not have enough
time to adjust to room temperature. Also, the measuring stick used to measure the length of the
tube may not have been precise enough for the experiment. Because the sides of the stick were
worn out, the measured length of the tube may have been longer than the actual length. Another
important factor to consider is that the aluminum foil used to cover one end of the tube was not
perfectly flat, leading to a concave or convex wall for the sound the bounce off of. If the
aluminum foil made a concave wall, the actual distance traveled by the sound would be less than
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the measured value, and if the aluminum foil made a convex wall, the actual distance traveled by
the sound would be greater than the measured value. Besides measurement error, there are other
sources for error in the conduction of the experiment. An example of this would be if the tube
was not placed on a flat surface when the experiment was conducted. The sound could rebound
off the sides of the tube, giving an inaccurate measurement for the travel time of sound. Along
Additionally, the person making the sound could have placed his or hand too far away from or
too far into the tube, causing the actual distance traveled by the sound to be greater or less than
the recorded/measured value. There are other sources for error in the experiment, but these are
some of the most significant to the accuracy of the experiment.
SUMMARY:
A wave is a vibration or disturbance in frequency. Periodic waves are waves that repeat, and a
pulse wave is a single wave. There are many types of waves in the world, including earthquakes,
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light, ocean waves, radio waves, and sound. Probably the most important classification for a
wave, however, is whether it is a transverse wave or a longitudinal wave. In a transverse wave,
the particles are disturbed in a direction perpendicular to wave motion, whereas in longitudinal
waves, the particles are disturbed in a direction parallel to wave motion. Sound is an example of
the latter, a longitudinal wave.
Sound is a form of travelling wave that is an oscillation of pressure through a certain medium:
solid, liquid, or gas. Sound is composed of frequencies that are within the range of hearing and in
the threshold of hearing. The speed of waves is dependent on the medium or material the wave is
travelling through as well as the wave type, and sound is not an exception. The accepted speed
for sound at 0 °C and through air is about 331.5 m/s. According to the following formula for
speed of sound in air, the speed of sound increases with temperature:
v = 331.5 + 0.607(T) m/s, where T = Temperature
In addition, sound travels fastest through solids, slower through liquids, and slowest through
gases. The speed of the wave can be determined by a generic formula:
v= λT
∨v=λ f
where λ = wavelength, T = period, and f = frequency
Period, frequency, wavelength, pitch, intensity, loudness, amplitude, and decibel level are
essential properties of sound. The period is the time it takes for an entire wave to pass a certain
point. Frequency is the reciprocal of period, and it is a measure of the number of waves that pass
a certain point in 1 second. Wavelength is the length of an entire wave, usually from the crest of
one wave to another or the trough of one wave to another. Pitch is directly related to frequency:
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the higher the frequency, the higher the pitch, and the lower the frequency, the lower the pitch.
Pitch is a representation of the perceived fundamental frequency of a sound. It is in a sense, a
way to compare waves of different frequencies. Intensity is the rate that energy flows through a
given area. Since power is the rate at which energy flows, intensity can be given by the formula
below:
I = PA
where I = intensity, P = power, and A = area
If the wave is spherical, the area through which the wave travels is the surface area of a sphere,
4πr2. The units for intensity are in W/m2 (Watts per meter-squared).
Intensity of a sound is related to loudness and amplitude. If amplitude is increased, then the
loudness of the sound is increased, and vice versa. Intensity is proportional to the square of
amplitude of a sound, and in sound waves, the amplitude of a sound wave is the change in
pressure as the wave passes by. Decibel level, or relative intensity, is a form of measurement
related to intensity. The Decibel level or scale is a logarithmic scale used to compare the
intensity of all sounds to the intensity of the softest sound that a human being can hear. The
softest sound that a human can hear (I0) has an intensity of 1 x 10-12 W/m2. An increase in 10 dB
(Decibels) is equal to increasing the intensity of sound by a factor of 10. The Decibel level of a
sound can be given by the following formula:
β=10 log ( II 0)
where β = Decibel level, I = Intensity, and I0 = Threshold of Hearing = 1 x 10-12 W/m2
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The formula could also be manipulated to solve for Intensity:
I = 10β
10 (I0)
Also important to the concept of sound is interference, or when more than one wave is in the
same place at the same time and they combine. The combined effect is the sum of the individual
waves, and this phenomenon is called superposition. There are two types of interference:
constructive interference and destructive interference. In constructive interference, waves come
together to form a larger wave. In destructive interference, the opposite happens—waves come
together to make a smaller wave. Beats are a special type of interference effect, where two waves
of slightly different frequencies interfere and there is an alternation between constructive and
destructive interference. This creates a variation in amplitude, or loudness. The beat frequency is
the difference between the two different frequencies:
fbeat = f1 – f2
Standing waves are examples of another type of interference effect. In standing waves, a fixed
pattern of vibration forms when two identical waves traveling in opposite directions interfere.
Harmonics are sets of half-wavelengths that will travel in a certain length of space. For
longitudinal waves, air particles are free to move and so the frequency of the wave can be found
by:
fn = nv
2L n = 1, 2, 3…
where n = harmonic number, v = speed of wave, and L = length wave is traveling across
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Music is different from noise in that music is more structurally organized, and there are much
fewer harmonics in the playing of a note than in a “noise.” Noise usually has many harmonics,
and the pure tone and pitch of musical notes is not present.
To talk about: Doppler Effect