How Does the Change in Force Applied to a Piano Key Alter its
Pitch?
Background | Statement | Hypothesis | Method | Diagram | Variable | Data | Calculations | Conclusion | Limitations | Cites | Bibliography | Go Up
Background:
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The piano is an instrument invented around the year 1700,
and it creates sound through the striking of hammers on strings(Piano
Facts). The sounds are produced by the frequencies of the strings, and a perfectly tuned note “A4” on the piano have the
frequency of 440Hz (Physics of Music). Frequency is defined through the equation , where v is the wave
speed and λ is the wavelength. Wave speed can be calculated through , where T is tension
and σ is linear density(Giancoli). Since the linear density and wavelength of a piano string is
constant, it seems like a change in the tension of the string can alter its frequency.
The tension can potentially be changed by an increase in the force applied to
the string, such as the hammer hitting the string harder, increasing its
amplitude and as a result tension. Therefore, I will be attempting to
investigate whether the force applied to the key will affect its pitch. Pitch is the quality of sound governed by the frequency
producing it, and it is measured in Hertz. Instead of measuring the frequency
of a note directly, the unit of measurement that I will be using is cents.
Cents is the measurement of musical interval, and it represents how “off” the
note’s pitch is in relationship to the absolute perfect pitch(Cents).
Frequencies can later be converted from cents through an equation shown in the
calculations part of this investigation.
Statement of the Problem: Go Up
The purpose of this investigation is to answer
the research question: “How does the change in force applied to a piano key
alter its pitch?”
Hypothesis:
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I believe that as the amount of force applied to the piano key
increases, the pitch of the note should become sharper. This is due to the
increase in the force of the hammer hitting the string, and thus increasing the
amplitude and tension of the string, causing it to vibrate faster and increase
the pitch.
Frequency is wavelength divided by wave speed, and the wave
speed is the square root of tension over linear density. Therefore, when the
hammer hits the string, it stretches it, increasing its tension and as a result
frequency as well.
Method: Go Up
To conduct the experiment, I gathered all the
equipments needed, including a tuner, weights measuring 100, 150, 200, 250,
300, and 350 grams, and a piano.
The tuner will be placed right above the
string of the piano to ensure an accurate recording of the note.
The mass will be placed .2m above the key of A4
so that when released, it would hit the key right at the edge.
When the mass hits the edge, the mechanism of
the piano will cause a hammer to strike the string, producing the note and be
recorded by the tuner for its pitch in cents.
This process will be repeated five times with
each mass (30 times total).
Diagram of Setup: Go Up
Variables:
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Controlled: The piano note A4
is used as the controlled variable throughout the experiment.
The height at which the mass is dropped will
stay constant at .2m, and since all the masses had enough impact force to
depress the piano key completely, the distance traveled by the mass after striking
the key is a constant .01m.
Independent variable: Mass in grams.
Dependent variable: The amount of deviation of the notes’
pitches in cents.
Raw Data Collected: Go
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Trials |
Mass in grams |
Pitch in cents (±0.5 cents) |
1 |
100 |
18 |
2 |
100 |
18 |
3 |
100 |
19 |
4 |
100 |
18 |
5 |
100 |
18 |
6 |
150 |
18 |
7 |
150 |
19 |
8 |
150 |
19 |
9 |
150 |
19 |
10 |
150 |
19 |
11 |
200 |
19 |
12 |
200 |
19 |
13 |
200 |
19 |
14 |
200 |
19 |
15 |
200 |
19 |
16 |
250 |
20 |
17 |
250 |
19 |
18 |
250 |
20 |
19 |
250 |
20 |
20 |
250 |
20 |
21 |
300 |
20 |
22 |
300 |
20 |
23 |
300 |
21 |
24 |
300 |
21 |
25 |
300 |
21 |
26 |
350 |
21 |
27 |
350 |
21 |
28 |
350 |
20 |
29 |
350 |
21 |
30 |
350 |
21 |
Calculations: Go Up
I calculated the forces by first finding out the impact
velocity of the masses using the formula . I then calculated the impact force using the “work formula” w =
F/d. By the time the mass reaches the piano key, all of its potential energy
has converted to kinetic energy. Calculating the kinetic energy using the
impact velocity and dividing by the travel distance of the mass after striking
the keys, I could find the impact force on the keys. Since many of the
calculated frequencies are the same across different force applied, I have
taken the average of all the frequencies that was outputted from one set of
mass.
To calculate the percentage uncertainty of the frequency, I
took the max frequency, subtract it with the lowest frequency, divide the
average frequency, and multiply it by 100.
%
Force in N |
Frequency in Hz (±0.15%) |
19.62 |
444.6500134 |
29.43 |
444.804144 |
39.24 |
444.8555209 |
49.05 |
445.0611471 |
58.86 |
445.2668625 |
68.67 |
445.3182988 |
Conclusion:
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From analyzing the graph, it is certain that my hypothesis
was correct. As the force applied to a key increases, its frequency increases
therefore the pitch becomes sharper. This is demonstrated by the slow but
definitely noticeable increase of frequency in the graph. Just like the
equations from the background and hypothesis, I believe that this was caused by
the increased force hitting the string, increasing the amplitude and therefore
tension of the string; and as the string was released and begins to vibrate,
the increased amplitude and tension caused the string to vibrate faster,
creating a higher frequency and pitch. It is also interesting to know that
despite the force applied have an direct impact on the
pitch, the change is so miniscule that it will not be detected by the human
ear. In the end, as the force applied to piano keys increases, so does the
frequency, but the change is insignificant and will not affect the sounds
produced in a noticeable way.
Limitations:
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There were definitely major limitations of this experiment.
One of which was the high uncertainty of the frequencies. This might be caused
by the possibilities of inaccuracies when the mass was dropped. When the mass
hits the part of the key on the piano that is farther from the edge, the hammer
will generate less force on the string as τ = rF, which can in
turn make the frequencies produced inaccurate. Furthermore, determining the
frequencies of the note in this experiment took two steps: recording the pitch
in cents and later calculating the frequencies through an equation. Since the
values of the cents in the experiment ranged between 18 and 21 while the
frequencies ranged between tenths or even hundredths of a unit, there could
potentially be great uncertainties lost during the calculation.
Since most of the values of the cents and frequencies
altered very little throughout all the trials, I believe that repeating more
trials would do little to the validity of the data, especially with the
limitations.
To improve the experiment, it could be possible to utilize
an actual frequency measurer rather than a tuner. It would eliminate an entire
step and also the potential of uncertainty and error associated with recording
the cents.
Related Cites: Go Up
https://en.wikipedia.org/wiki/Cent_(music) - Learn what pitch is and how it
applies to music.
https://pages.mtu.edu/~suits/notefreqs.html - Find out the frequencies of
various notes on a piano.
https://en.wikipedia.org/wiki/Impact_(mechanics)
– Learn about impact force.
https://www.youtube.com/watch?v=vFXBIFyG4tU
– See the mechanics of how a piano works.
https://en.wikipedia.org/wiki/Torque
- Learn about torque, a major part of the mechanics of a piano.
Bibliography:
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“Piano Facts.” Math, Softschools.com,
www.softschools.com/facts/music_instruments/piano_facts/3058/.
Giancoli, Douglas C. Physics: Principles with Applications. Upper Saddle River, NJ:
Pearson/Prentice Hall, 2009. Print.
“Physics of Music - Notes.” Frequencies of
Musical Notes, A4 = 440 Hz, pages.mtu.edu/~suits/notefreqs.html.
“Cents.” The Use of Cents for Expressing Musical
Intervals, Softschools.com, hyperphysics.phy-astr.gsu.edu/hbase/Music/cents.html.