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A Brief Introduction to Atonal Music Theory
for Scientists and Mathematicians
Paul Lombardi
A note produced
from an acoustic instrument has a rich series of overtones. For the
duration of this introduction, we will ignore the overtones and only
consider the fundamental pitch. Pitch has a frequency that is
measured in hertz. Two pitches sounded simultaneously or played in
succession produce an interval. The ratio of the two frequencies in
an interval determines whether the interval is consonant or
dissonant. Consonant intervals sound harmonious while dissonant
intervals sound harsh. Consider the interval from two pitches that
have a frequency ratio of 2:1 as shown in Figure 1.

When those two pitches are sounded
simultaneously, we hear their sum. Some other intervals are shown in
Figure 2, all of which are periodic.

As the resulting wave from the sum of
the two pitches becomes more complex, the interval becomes more
dissonant. The 2:1 interval is so consonant that we perceive the two
pitches as the same note, and it is called an octave. In adjacent
octaves, harmonic systems are related geometrically. For example, if
the note A has a frequency of 440 Hz, the A an octave
higher has a frequency of 880 Hz and the A an octave lower
has a frequency of 220 Hz.
In modern Western
Art Music, the octave is partitioned into twelve notes that aurally
sound equidistant from each other, which we call equal temperament.
A harmonic system of twelve divisions of the octave developed early
in the history of Western Art Music as a result of composers’
preference for consonance. If a pitch has a frequency of υ
in equal temperament, the next highest pitch has a frequency of
.
The interval of
is called a semitone. Consider the interval shown in Figure 3 that
spans 7 semitones.

The interval of 7 semitones in nearly
equal to the ratio of 3:2. The interval of 3:2 is perfectly in tune,
while the interval of
is slightly dissonant. Pythagoras said that musical ratios were the
same as the distances between the planets, all combined into a
beautiful harmony that he called Music of the Spheres. Plato
further elaborated on this concept where he said that the difference
between the musical intervals 3:2 and
is analogous to the orbits of the planets in that all of the planets
are never simultaneously in the same places. Plato knew that as
intervals of 3:2 are stacked to preserve consonance, the harmonic system
abruptly loses the equal temperament quantization.[1] Music early in the history of Western Art
Music used tunings that relied on consonant ratios such as 3:2, 4:3
and 5:4. As music incorporated more dissonances and modulations, a
system of equal temperament became necessary.[2] In a temperament system based on consonant
ratios, some of the intervals must be out of tune to compensate for
other notes to be in tune. For the remainder of this introduction,
we will assume equal temperament.
With
the advent of atonal music at the beginning of the Twentieth
Century, composers drastically changed their thinking about pitch.
This new thinking was soon coined as octave equivalence, which means
that a pitch in any octave has the same function, or a group of
pitches arranged in any order in any octave has the same function.
To simplify the understanding of atonal music, theorists use
integers to refer to pitches. In this introduction, we refer to the
twelve pitches of an octave with the integers 0-9 and A and B. The
integers as they correspond to the pitches on a keyboard are shown
in Figure 4.

A pitch class or PC refers to a pitch
without regards to which octave it’s in. For example, the PC 0
refers to any or all Cs regardless of which octave they’re in.
Pitch is linear, but since the equal tempered harmonic system
repeats every octave, a PC is cyclical; so we can understand PC in
mod 12 space like the face of a clock as shown in Figure 5. The
picture in Figure 5 is called a pitch-class wheel.

In this harmonic
system, intervals are the differences between PCs. Assuming octave
equivalence, there are two ways of examining intervals. An ordered
pitch-class interval is always computed in a positive clockwise
direction around a PC wheel. Some examples of ordered pitch-class
intervals are shown in Figure 6.

| (6 + 3)mod 12 = 9 |
(2 + 9)mod 12 = B |
(A + 6)mod 12 = 4 |
An interval class, or IC, is always
the shortest distance between 2 PCs regardless of the direction
around the PC wheel. Some examples of ICs are shown in Figure 7.

| (6 + 3)mod 12 = 9 |
(B + 3)mod 12 = 2 |
(A ± 6)mod 12 = 4 |
| (9 - 3)mod 12 = 6 |
(2 - 3)mod 12 = B |
|
A set of 3 or more
PCs is called a pitch-class set. Consider the PC set 236A. Here, the
4 PCs are sorted in increasing order, which is called ascending
form. An interval vector counts all of the interval classes between
the pairs of PCs in a set, as shown in Figure 8. The interval vector
for 236A is <101310> because there is one IC 1, zero IC 2, one
IC 3, three IC 4, one IC 5, and zero IC 6 between the pairs of PCs
in the set.
| 236A: |
(3-2)mod 12=1 |
(6-2)mod 12=4 |
(2-A)mod 12=4 |
1 2 3 4 5 6 |
|
(6-3)mod 12=3 |
(3-A)mod 12=5 |
|
< 1 0 1 3 1 0 > |
|
(A-6)mod 12=4 |
|
|
|
PC sets can be
transposed by adding a constant integer mod 12 to each PC. 2368 is
transposed as shown by the equations in Figure 9, where T indicates
transposition and the subscript indicates the distance of
transposition.
T2(2368) = 458A
T7(2368) = 9A13 = 139A
The first line shows a transposition
by 2 semitones, and the second line shows a transposition by 7
semitones. After each transposition, the PCs are resorted into
ascending form. PC sets can be inverted by reflecting the PCs around
an axis as shown in Figure 10.

I(2368) = A964 = 469A
Here, I indicates an axis that passes
through PCs 0 and 6 in the PC wheel. 2368 inverted around this axis
gives the PC set 469A, where 2 inverts to A, 3 inverts to 9, 6
inverts to 6, and 8 inverts to 4, and then the resulting set is
sorted into ascending form. Notice that the pairs of PCs are
complementary in base 12. PC sets can be inverted around other axes
by combining inversion with transposition. 2368 inverted around the
axis that passes through 1 and 7 is given by the equation shown in
Figure 11.

T2I(2368) = 0B86 = 068B>
Here, the PC set is transposed by 2
after being inverted around the 0/6 axis. Notice that the inverted
set has 2 PCs in common with the original set. Figure 12 shows the
TnI transformations for all axes of inversion. Notice
that the axis of inversion may be between PCs rather than passing
through them.

PC sets are
symmetrical when they have all common PCs under some Tn
or TnI transformation. An example of a common PC is
illustrated by the PC sets 247 and 348 that have PC 4 in
common. There are two types of symmetry: inversional and
transpositional. Inversionally symmetrical PC sets have all common
PCs at some TnI transformation. For example, 2457 is
symmetrical around the axis that passes between 4 and 5 as shown in
Figure 13.

| T9I(2457) = 7542 = 2457 |
T2I(159) = 195 = 159 |
|
T6I(159) = 519 = 159 |
|
TAI(159) = 951 = 159 |
Also shown in Figure 13, some PC sets,
such as 159, have more than one axis of symmetry. PC sets are
transpositionally symmetrical if they have all common PCs at some
transposition level other than T0. 159, shown in Figure
14, is transpositionally symmetrical because it has all common tones
at T4 and T8.

| T0(159) = 159 |
| T4(159) = 591 = 159 |
| T8(159) = 915 = 159 |
The ascending form
of PC sets can be rotated so that any of their PCs can be listed
first. The three rotations of 23B are 23B, 3B2, and B23 as shown in
Figure 15.
| 23B |
3B2 |
[B23] |
| (2 + 9)mod 12 = B |
(3 + B)mod 12 = 2 |
(B + 4)mod 12 = 3 |
In each of the rotations, the PCs
remain in a clockwise order around the PC wheel. For each of these
rotations, the interval between the first and last PCs is 9, B and 4
respectively. B23 has the smallest interval between its first and
last PCs, so B23 is the most compact rotation of the set. Therefore,
B23 is in normal form. When two rotations have the same interval
between their first and last PCs, the smaller interval between the
first and second-to-last PCs is used to determine normal form. For
any PC set, the most compact rotation of the ascending form is
called normal form. PC sets are given in square brackets when they
are in normal form.
A set class, or SC,
includes all transpositions and inversions of a PC set. Figure 16
shows all of the transpositions and inversions for the PC set [013],
all of which are members of the same SC. The 24 sets in this SC are
all listed in normal form.
| SC 3-2 (013): |
|
|
|
|
|
|
|
| T0[013] = [013] |
T6[013] = [679] |
T0I[013] = [9B0] |
T6I[013] = [356] |
| T1[013] = [124] |
T7[013] = [78A] |
T1I[013] = [A01] |
T7I[013] = [467] |
| T2[013] = [235] |
T8[013] = [89B] |
T2I[013] = [B12] |
T8I[013] = [578] |
| T3[013] = [346] |
T9[013] = [9A0] |
T3I[013] = [023] |
T9I[013] = [689] |
| T4[013] = [457] |
TA[013] = [AB1] |
T4I[013] = [134] |
TAI[013] = [79A] |
| T5[013] = [568] |
TB[013] = [B02] |
T5I[013] = [245] |
TBI[013] = [8AB] |
Of these 24 sets, only [013] and [023]
begin with PC 0. [013] is more normal than [023] (i.e. the interval
between the first and second-to-last PCs is smaller), so we say that
(013) is in prime form. Sets in prime form are given in parentheses.
Each SC has only one prime form.
SCs have been
cataloged differently by several theorists, but the catalog by Allen
Forte has become the standard. The Forte names for SCs include a
number that indicates the cardinality of the set, followed by the
catalog number. The PC sets shown in Figure 16 are all members of SC
3-2. The three indicates that the set has 3 PCs, and the 2 indicates
that the set is the second set in the catalog of sets with a
cardinality of 3. As shown in Figure 17, the complement of [013] in
base 12 is [2456789AB]. Complementary SCs have the same catalog
number, so the complement of SC 3-2 is SC 9-2.
| [013] |
[2456789AB] |
| 3-2 (013) |
9-2 (012345679) |
All PC sets in a SC
have the same interval vector. There are some sets that have the
same interval vector that are not members of the same SC. That is,
even though they have the same interval vector, they are not related
by transposition or inversion. Different SCs that have the same
interval vector are said to be Z-related, so a Z is included in
their Forte name. As shown in Figure 18, SCs 5-Z12 and 5-Z36 are
Z-related because they both have an interval vector of
<5222121>.
| 5-Z12 (01356) |
5-Z36 (01247) |
| <5222121> |
<5222121> |
So far in this
introduction, we have arranged sets in ascending, normal and prime
forms. In serial music, however, the order of the PCs is important.
Curly braces are used to indicate a series in a fixed order.
Serialism is not just limited to PCs, but any musical element may be
serialized such as duration, instrumentation, intensity, and
articulation. Twelve-tone music is a specific type of serialism that
makes use of a series that has one occurrence of each of the twelve
PCs. Figure 19 shows a twelve-tone series by Arnold Schoenberg
labeled P for prime.
| P |
{45716382B09A} |
 |
| R |
{A90B28361754} |
T8I |
| I |
{4317250698BA} |
 |
| RI |
{AB8960527134} |
|
The retrograde of the twelve-tone
series is labeled R. The inversion of the series is labeled I. Here,
the series is inverted around the axis that passes through PC 4
(T8I) so that P and I begin with the same PC. RI is the
retrograde of the inversion.
There are twelve
transpositions of each of P, R, I and RI. As shown in Figure 20, a
twelve-tone matrix is a handy way of compactly listing all of these
transpositions.

P is listed in the top row of the
matrix, and I is listed in the left column of the matrix. The twelve
transpositions of P are listed in the twelve rows of the matrix
reading from left to right. The twelve transpositions of I are
listed in the twelve columns reading from top to bottom. Likewise
the transpositions of R and RI are listed in the matrix as the
retrogrades of P and I. We can refer to any of the 48 forms of the
series as follows. The transposition of P beginning with PC 4 is
labeled P4, which is in the top row of the matrix. The
transposition of P beginning with PC 3 is labeled P3,
which is in the second row of the matrix. The retrograde of
P4 begins with PC A, and is labeled R4 and not
RA. This way, we can know that P4 and
R4 are retrogrades of each other without having to know
the last note in P4. The transpositions of I and RI are
handled similarly. For example, the third column of the matrix is
I7 and its retrograde is RI7. I7
begins with PC 7, while RI7 begins with PC 1. Frequently,
it is necessary to refer to elements within a series based on their
order position. So, we refer to a PC’s placement within the
series by using a coordinate system where the top left PC in the
matrix is coordinate 0,0. For example, the first PC of P4
is 4, which has an order position of 0; while the first PC of
R4 is A, which has an order position of B.
This introduction
rudimentarily discusses some basic topics of atonal music theory.
For a more detailed discussion of these topics, see Joseph
Straus’s Introduction to Post-Tonal
Theory.[3]
© 2007 Paul Lombardi
[1]
James Haar: ‘Music of the spheres’, Grove Music
Online ed. L. Macy (Accessed [15 January 2007]),
<http://www.grovemusic.com>.
[2]
Mark Lindley: ‘Equal temperament’, Grove Music
Online ed. L. Macy (Accessed [15 January 2007]),
<http://www.grovemusic.com>.
[3]
Joseph Straus, Introduction to Post-Tonal Theory, 3rd Ed.
Upper Saddle River, NY: Pearson Prentice Hall, 2005.
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