The Physics of Music - Physics 15 University of California, Irvine ...
The Physics of Music - Physics 15 University of California, Irvine ...
The Physics of Music - Physics 15 University of California, Irvine ...
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<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
Lecture 10<br />
• <strong>Music</strong>al Notes and Scales<br />
• Scales and Timbre<br />
• Pythagorean Scale<br />
• Equal Temperament Scale<br />
• Unorthodox Scales<br />
Midterm<br />
<strong>The</strong> average score on the midterm was 64%. <strong>The</strong> average<br />
on the multiple choice section (73%) was higher than on<br />
the written sections (59%).<br />
This average corresponds to C+/B-, which is most likely<br />
where the final course average will end up and is normal<br />
for an intro physics course.<br />
I will be checking that the grades for the two versions<br />
are consistent, and make adjustments if necessary when<br />
calculating your final grade.<br />
Remember that the midterm contributes 25% to your<br />
final grade for the course (homework is 40%, the final is<br />
35%).<br />
Instructor: David Kirkby (dkirkby @uci.edu)<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 2<br />
Students HectorAleman and Claire Dreyer should see me<br />
after class today.<br />
Here are some<br />
distributions from<br />
the midterm grades:<br />
Drop Deadline<br />
<strong>The</strong> deadline to drop this course is Friday.<br />
For Drop Card signatures, see the <strong>Physics</strong> Undergrad<br />
Affairs Coordinator:<br />
Kirsten Lodgard<br />
klodgard@uci.edu<br />
137 MSTB<br />
Homework and midterm scores are posted on the web for<br />
your reference:<br />
http://www.physics.uci.edu/undgrad/coursescores.html<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 3<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 4<br />
Review <strong>of</strong> Lecture 9<br />
In the last lecture, we covered:<br />
• <strong>The</strong> perception <strong>of</strong> combination tones (difference<br />
tones)<br />
• Different modes <strong>of</strong> hearing (analytic/synthetic,<br />
harmonic/inharmonic)<br />
• <strong>The</strong> physical basis for dissonance<br />
• <strong>The</strong>ories <strong>of</strong> pitch perception (the relative importance<br />
<strong>of</strong> wavelength and frequency cues)<br />
Why does a piano<br />
have 7 white notes<br />
and 5 black notes<br />
per octave<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 5<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 6<br />
1
<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
<strong>Music</strong>al Scales<br />
<strong>The</strong>re is an infinite continuum <strong>of</strong> possible frequencies to<br />
use in music.<br />
But, in practice, most music uses only a small (finite)<br />
number <strong>of</strong> specific frequencies.<br />
We call each <strong>of</strong> these special frequencies a musical note,<br />
and call a set <strong>of</strong> notes a musical scale .<br />
Different cultures have adopted different scales. <strong>The</strong><br />
choice <strong>of</strong> scale is primarily aesthetic, but some aesthetic<br />
judgments are heavily influenced by physical<br />
considerations (e.g., dissonance).<br />
What can physics tell us about musical scales<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 7<br />
Harmonic Timbres<br />
Most musical sounds have overtones that are<br />
approximately harmonic (ie, equally spaced on a linear<br />
frequency axis).<br />
This is most likely due to a combination <strong>of</strong> two related<br />
factors:<br />
• <strong>The</strong> resonant frequencies <strong>of</strong> many naturally occurring<br />
resonant systems are approximately harmonic.<br />
• Your brain is optimized for listening to timbres that<br />
are approximately harmonic.<br />
Note that there are examples <strong>of</strong> naturally occurring<br />
inharmonic sounds (eg, a hand clap) but we do not perceive<br />
these as being musical.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 8<br />
Octaves Rule<br />
Two notes played together on instruments with harmonic<br />
timbres sound most consonant (least dissonant) when their<br />
fundamental frequencies are an exact number <strong>of</strong> octaves<br />
apart:<br />
frequency<br />
<strong>The</strong> correct answer to the octave test was #4, although<br />
most people prefer a slightly bigger octave with a<br />
frequency ratio <strong>of</strong> about 2.02:1 that corresponds to #6.<br />
This preference for slightly stretched octaves may be due<br />
to our familiarity with listening to pianos which are usually<br />
deliberately tuned to have stretched octaves (more about<br />
this in Lecture 14).<br />
In this sense, an octave is a special interval that we can<br />
expect will play a special role in any “natural” scale<br />
(although it is certainly possible to invent un-natural<br />
scales).<br />
Try this demonstration to see if you can pick out octaves.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 9<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 10<br />
Subdividing the Octave<br />
In practice, this means that if a particular frequency is<br />
included in a scale, then all other frequencies that are an<br />
exact number <strong>of</strong> octaves above or below are also included.<br />
<strong>The</strong>refore, choosing the set <strong>of</strong> notes to use in a scale<br />
boils down to the problem <strong>of</strong> how to subdivide an octave.<br />
Is the choice <strong>of</strong> how to subdivide an octave purely<br />
aesthetic, or are there physical considerations that<br />
prefer certain musical intervals<br />
Scales and Timbre<br />
<strong>The</strong> choice <strong>of</strong> a scale (subdivisions <strong>of</strong> an octave) is<br />
intimately related to the timbre <strong>of</strong> the instrument that<br />
will be playing the scale.<br />
<strong>The</strong> scale and timbre are related by dissonance: the notes<br />
<strong>of</strong> a scale should not sound unpleasant when played<br />
together.<br />
For example, most people listening to an “instrument” with<br />
no overtones (ie, a pure SHM sine wave) will have no<br />
preference for how to subdivide an octave (and the octave<br />
is no longer a special interval).<br />
Try these demonstrations to learn more about the<br />
connection between scales and timbre.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 11<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 12<br />
2
<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
However, most people listening to an instrument with<br />
harmonic timbre (ie, most “musical” instruments) will have<br />
a definite preference for certain intervals where<br />
overtones coincide exactly.<br />
Different instruments with harmonic timbres have<br />
different strengths for the various harmonics. <strong>The</strong>se<br />
differences affect how consonant the preferred intervals<br />
are but do not change their frequencies.<br />
<strong>The</strong>refore, there is a universal set <strong>of</strong> preferred<br />
subdivisions <strong>of</strong> the octave for instruments with harmonic<br />
timbres (based on a physical model <strong>of</strong> dissonance).<br />
How Finely to Chop the Octave<br />
Minimizing the dissonance <strong>of</strong> notes played together on<br />
instruments with harmonic timbres gives us some guidance<br />
on how to create a scale with a given number <strong>of</strong> notes, but<br />
not on how many notes to use.<br />
Some <strong>of</strong> the conventional choices are:<br />
• Pentatonic: octave is divided into 5 notes (eg, Ancient<br />
Greek, Chinese, Celtic, Native American music)<br />
• Diatonic, Modal: octave is divided into 7 notes (eg,<br />
Indian, traditional Western music)<br />
• Chromatic: octave is divided into 12 notes (modern<br />
Western music)<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 13<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 14<br />
A Primer on <strong>Music</strong>al Notation<br />
<strong>The</strong> white notes on the piano are named A,B,C,D,E,F,G.<br />
After G, we start again at A. This reflects the special role<br />
<strong>of</strong> the octave: we give two frequencies an octave apart the<br />
same note name.<br />
Going up in frequency (towards the right on the keyboard)<br />
from a white note to its adjacent black note gives a sharp:<br />
C goes to C # , D goes to D # , etc.<br />
Similarly, going down in frequency gives a flat: D goes to<br />
D b , E goes to E b , etc.<br />
D b<br />
E b<br />
C # D # F # G # A # C # D # F # G # A #<br />
G b A b B b D b E b G b A b B b<br />
C D E F G A B C D E F G A B C<br />
C D E F G A B C D E F G A B C<br />
C # and D b are necessarily the same note on the piano, but<br />
this is not generally true for all possible scales!<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby <strong>15</strong><br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 16<br />
Pentatonic Scales<br />
<strong>The</strong> usual choice <strong>of</strong> 5 notes in a pentatonic scale<br />
corresponds to the black notes on the piano:<br />
This scale includes the dissonant whole tone (9:8)<br />
interval, but leaves out the less dissonant major (5:4) and<br />
minor (6:5) third intervals. Why<br />
Other choices <strong>of</strong> 5 notes are also possible.<br />
Examples:<br />
• Indian music<br />
• Chinese music<br />
• Celtic music: Auld Lange Syne, My Bonnie Lies Over<br />
the Ocean<br />
Presumably because music limited to just 5 notes would<br />
be boring without some dissonance to create tension.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 17<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 18<br />
3
<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
Diatonic Scales<br />
<strong>The</strong> major and minor scales <strong>of</strong> Western music are diatonic<br />
scales, in which the octave is divided into 7 steps.<br />
<strong>The</strong> notes <strong>of</strong> the major scale correspond to the white<br />
notes on a piano, starting on C. <strong>The</strong> (natural) minor scale<br />
corresponds to the white notes starting on A.<br />
Diatonic scales can also start on any other white note <strong>of</strong><br />
the piano. <strong>The</strong> results are the modes with names like<br />
Dorian, Phrygian, Lydian, …<br />
Most Western music since the 17th century is based on<br />
major and minor scales.<br />
Earlier music was primarily modal.<br />
Example: Gregorian chants<br />
A<br />
C<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 19<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 20<br />
Chromatic Scales<br />
Although most Western music is based on diatonic scales,<br />
it frequently uses scales starting on several different<br />
notes in the same piece <strong>of</strong> music (as a device for adding<br />
interest and overall shape).<br />
A major scale starting on C uses only white notes on the<br />
piano, but a major scale starting on B uses all five black<br />
notes.<br />
<strong>The</strong> main reason for adopting a chromatic scale is to be<br />
able to play pieces based on different scales with the<br />
same instrument.<br />
An octave divided into twelve notes includes all possible<br />
seven-note diatonic scales.<br />
Not all instruments adopt this strategy. For example,<br />
harmonicas are each tuned to specific diatonic scales. To<br />
play in a different key, you need a different instrument<br />
(or else to master “bending” techniques).<br />
What exactly should be the frequencies <strong>of</strong> the 12 notes<br />
that make up a chromatic scale<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 21<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 22<br />
Is there an obvious way to subdivide an octave into twelve<br />
notes<br />
Yes: the notes should be equally spaced and include all <strong>of</strong><br />
the special consonant frequency ratios (3:2, 4:3, …).<br />
To what extent is this actually possible<br />
After the octave, the fifth (3:2) is the most consonant<br />
interval for harmonic timbres. <strong>The</strong> fourth (4:3) is really<br />
just a combination <strong>of</strong> the octave and fifth:<br />
4/3 = (3/2) x (1/2)<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 23<br />
<strong>The</strong> Circle <strong>of</strong> Fifths<br />
We can reach all 12 notes <strong>of</strong> the chromatic scale by<br />
walking up or down the piano in steps <strong>of</strong> a fifth (3:2):<br />
Going up, we reach all<br />
white notes <strong>of</strong> the piano<br />
except F, and then go<br />
through the sharps.<br />
Going down, we hit F first<br />
and then go through the<br />
flats.<br />
Either way, we eventually<br />
get back to a C (7 octaves<br />
away) if we start on a C.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 24<br />
4
<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
Using the circle <strong>of</strong> fifths, we can calculate the frequency<br />
<strong>of</strong> any note we reach going up as:<br />
starting<br />
note<br />
f = f 0 x (3/2) x (3/2) x … x (3/2) / 2 / 2 / … / 2<br />
Steps up in fifths<br />
Steps down<br />
in octaves<br />
A similar method works for each step down by a fifth:<br />
f = f 0 / (3/2) / (3/2) / … / (3/2) x 2 x 2 x … x 2<br />
Steps down in fifths<br />
Steps up<br />
in octaves<br />
What happens when we get back to our original note<br />
For example, after going 12 fifths up, we get back to a C<br />
that is 7 octaves up which corresponds to a note:<br />
f = f 0 x (3/2) 12 / (2) 7 = f 0 (531441/524288) = 1.014 f 0<br />
We end up close but not exactly where we started!<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 25<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 26<br />
Pythagorean Scale<br />
If we ignore this problem <strong>of</strong> not getting back to where we<br />
started, we end up with the set <strong>of</strong> notes corresponding to<br />
the Pythagorean scale.<br />
<strong>The</strong> Pythagorean scale has the feature that all octave and<br />
fifth intervals are exact (and therefore so are fourths).<br />
But the Pythagorean scale also has some shortcomings:<br />
• <strong>The</strong> frequencies we calculate for the black notes<br />
depend on whether we are taking steps up or down, so<br />
C # and D b are different notes!<br />
• <strong>The</strong> semitones from E to F and B to C are bigger than<br />
the semitones from C to C # and D b to D.<br />
• Frequency ratios for intervals other than 8ve, 4th, 5th<br />
depend on which note you start from, and can be far<br />
from the ideal ratios.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 27<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 28<br />
Alternative Scales<br />
Since the major (5:4) and minor (6:5) 3rd intervals are<br />
important for diatonic music, several alternative scales<br />
have been proposed that have these intervals better in<br />
tune (ie, closer to their ideal frequency ratios) without<br />
sacrificing the octave, fourth, and fifth too much.<br />
Some alternatives that I will not discuss are the meantone<br />
and just intonation scales (see Sections 9.3-9.4 in the<br />
text for details).<br />
<strong>The</strong>se scales both improve the tuning <strong>of</strong> intervals but<br />
sound differently depending on the choice <strong>of</strong> starting<br />
note for a diatonic scale (Beethoven described D b -major<br />
as “majestic” and C-major as “triumphant”). <strong>The</strong>y also give<br />
different frequencies for C # and D b , etc.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 29<br />
Equal Temperament Scale<br />
<strong>The</strong> scale that is most widely used today is the equal<br />
temperamentscale.<br />
This scale is the ultimate compromise for an instrument<br />
that is tuned infrequently and for which the performer<br />
cannot adjust the pitch during performance.<br />
<strong>The</strong> equal temperament scale gives up on trying to make<br />
any intervals (other than the octave) exactly right, but<br />
instead makes the 12 notes equally spaced on a logarithmic<br />
scale.<br />
Listen to the difference between equally-spaced notes on<br />
linear and logarithmic scales:<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 30<br />
5
<strong>The</strong> <strong>Physics</strong> <strong>of</strong> <strong>Music</strong> - <strong>Physics</strong> <strong>15</strong><br />
<strong>University</strong> <strong>of</strong> <strong>California</strong>, <strong>Irvine</strong><br />
Instructor: David Kirkby<br />
dkirkby@uci.edu<br />
Mathematically, each semitone corresponds to a frequency<br />
ratio <strong>of</strong> 2 1/12 = 1.059, so that 12 semitones exactly equals<br />
an octave.<br />
<strong>The</strong> equal temperament scale has the main advantage that<br />
all intervals sound the same (equally good or bad)<br />
whatever note you start from.<br />
<strong>The</strong>refore, diatonic scales played from different notes<br />
(eg, C-major, D-major, …) are mathematically identical<br />
except for their absolute frequency scale (which most<br />
people have no perception <strong>of</strong>).<br />
Unorthodox Scales<br />
Instead <strong>of</strong> dividing the octave into 12 equally spaced<br />
notes, we can divide it into any number <strong>of</strong> equally spaced<br />
notes.<br />
Listen to these scales with different numbers <strong>of</strong> notes:<br />
• 12 notes (standard equal-tempered chromatic scale)<br />
• 13 notes<br />
• 8 notes<br />
Why aren’t 13 and 8 note scales popular Because they are<br />
more dissonant than 12 note scales when two or more<br />
notes are played together with harmonic timbres.<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 31<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 32<br />
Unorthodox Instruments<br />
Some instruments designed to play unorthodox scales have<br />
actually been built and played:<br />
Unorthodox Instruments<br />
Although most real acoustic instruments have<br />
approximately harmonic timbres, artificial instruments can<br />
be electronically synthesized to have any timbres.<br />
Fokker organ designed<br />
to play a 31-note scale<br />
http://www.xs4all.nl/~huygensf/english/index.html<br />
In particular, we can create instruments that are less<br />
dissonant when played in non-standard scales.<br />
<strong>The</strong> results are interesting and easy to listen to<br />
(compared with the Fokker organ). For example:<br />
• 11-note scale:<br />
• 19-note scale:<br />
http://eceserv0.ece.wisc.edu/~sethares/mp3s/<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 33<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 34<br />
Frequency Standardization<br />
Most people have no perception <strong>of</strong> absolute pitch so it is<br />
not surprising that we managed for a long time without any<br />
standard definition <strong>of</strong> the frequency <strong>of</strong> middle C.<br />
In 1877, the A 4 pipes on organs reportedly ranged from<br />
374 - 567 Hz (corresponding to the modern range F-C # ).<br />
<strong>The</strong> modern standard is A 4 = 440 Hz and was adopted in<br />
1939.<br />
Summary<br />
We covered the following topics:<br />
• <strong>Music</strong>al Notes and Scales<br />
• Scales and Timbre<br />
• Pythagorean Scale<br />
• Equal Temperament Scale<br />
• Unorthodox Scales<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 35<br />
<strong>Physics</strong> <strong>of</strong> <strong>Music</strong>, Lecture 10, D. Kirkby 36<br />
6