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Perspectives of New Music
Some Compositional Uses of Projective GeometryAuthor(s): David LewinSource: Perspectives of New Music, Vol. 42, No. 2 (Summer, 2004), pp. 12-63Published by: Perspectives of New MusicStable URL: http://www.jstor.org/stable/25164553
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Some Compositional Uses
of
Projective Geometry
Le?7ta
David Lewin
Part
I: Introduction
to the
Projective
Plane;
Diatonic Modal
Examples
Imagine
a
school
that has
seven
students:
Ann, Bill, Carol,
Dan,
Eve,
Frank, and Gladys. Suppose the school offers seven courses: Latin,
Math,
Neurology, Psychology,
Quantum mechanics, Russian,
and
Span
ish.
Suppose
the enrollment of
students
in
courses
is
given by
Example
1.
On
the
example,
each
asterisk
indicates
that
the
student whose
initial
appears
to
the left
is
taking
the
course
whose
initial
appears
above.
Thus
Ann
is
taking
Math,
Neurology,
and
Quantum mechanics;
the students
enrolled
in
Spanish
are
Carol, Frank,
and
Gladys;
and
so
forth.
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ProjectiveGeometry
13
A
~B~
~C
~D
~E
~F~
~G
M
N
Q
R
EXAMPLE
1
Example
1
has the
following
properties:
1.
Any
two
students
have
just
one course
in
common.
2.
Any
two
courses
have
just
one
student
in
common.
3.
Every
course
has
at
least
three
students;
every
student is
taking
at
least three
courses.
4. It is
not
the
case
that
every
student
is
taking
every
course.
The
properties
manifest
a
structure
called
a
"projective
plane."
To
appreciate
the
geometric metaphor,
we can
replace
the word "student"
by
the
word
"point,"
the word
"course"
by
the word
"line,"
and
the
notion
of
a
student's
taking
a course
by
the notions
of
a
point's "lying
on"
a
line and
(equivalently)
of
the line's
"passing through"
the
point.
The properties above then translate as follows:
1.
Any
two
points
lie
on
just
one
line.
2.
Any
two
lines
pass
through just
one
point.
3.
Every
line
passes
through
at
least three
points;
every
point
lies
on
at
least
three
lines.
4. It is
not
the
case
that
every
point
lies
on
every
line.
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14
Perspectives
of
New Music
As
translated,
the
properties
suggest
things
we
apprehend
about
"plane geometry."
The
things
have
to
do in
particular
with incidence
relations
of
points
and lines.
Only
property
2
departs
from
Euclidean
intuition:
in
Euclidean
plane
geometxy^parallel
lines
do
not
pass
through
any
common
point. Projective
geometry,
unlike Euclidean
geometry
(or
"affine
geometry")
does
not
recognize
the
notion
of
parallel
lines.
To
turn
the
Euclidean
plane
into
a
projective plane
one can
adjoin
a
"line
at
infinity,"
comprising
formal
"points"
where
parallel
lines
meet.
In
the
Euclidean
plane
one
fixes
a
reference
line;
in
a
standard
Cartesian
coordinate
system
this could be the horizontal X axis. For each number a
between 0 inclusive
and
180
exclusive,
stipulate
a
corresponding
"point
at
infinity."
Each line in the Euclidean
plane
will
be
tilted
with
respect
to
the reference
line
at some
angle
a
degrees;
the
given
line
meets
the
line
at-infinity
at
point
a.
So
a
line
perpendicular
to
the
reference
line
meets
the
line-at-infinity
at
point
90.
A line
parallel
to
the
reference
line
meets
the
line-at-infinity
at
point
0. More
generally,
two
parallel
lines will both
be
tilted
the
same
amount
with
respect
to
the
reference
line;
if
the
com
mon tilt is a degrees, then the two linesmeet at infinite-point a. The
extended
structure
is called the "Real
Projective
Plane." The
reader
can
verify
that it satisfies
properties
1
through
4
above.1
A
projective plane
is
highly
structured,
and
that
structure
can
be musi
cally suggestive
in
various
contexts.
As
a
first
illustration,
let
us
return to
Example
1
and
now
read the
seven
"students"
as
the
seven
white-note
pitch
classes.
The
seven
"courses" then
become
a
family
of
seven
privi
leged
Chords,
the
Chords
L
through
S
displayed
in
Example
2.
The four
properties now read:
1.
Any
two notes
belong
to
just
one
Chord.
2.
Any
two
Chords
have
just
one common
tone.
3.
Every
Chord has
at
least
three
notes;
every
note
belongs
to
at
least
three Chords.
4. It
is
not
the
case
that
every
note
belongs
to
every
Chord.
L M
N
P
Q
R
S
EXAMPLE
2
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Projective Geometry
15
EXAMPLE
3
Indeed
in
this
particular
geometry
every
Chord
has
exactly
three
notes,
and
every
note
belongs
to
exactly
three
Chords.
Chords
L, M,
and
N,
taken
in
conjunction,
suggest
Phrygian modality;
Chord
P,
when
suitably
linearized,
is
appropriate
for
executing
a
melodic
Phrygian
cadence.
Obviously
I
constructed
the
example
with these features in
mind/ear.
Later
on,
I
shall show how
I
did
that.
Meanwhile
I
shall
present
a
Lehrst?ck
that
demonstrates
how
various
aspects
of
the
geometry
can
be
projected compositionally.
After
setting
up
the seven-note seven-chord
projective plane
as in
Examples
1 and
2,
to
build
a
species
of
"Phrygian
mode,"
I
decided
to
write
a
three-part
vocal
piece
where
every
three-note
verticality
would be
a
Chord.
I
decided
to
base this
piece
on a
cantus
firmus,
and had the idea
of
com
posing
the
cantus
as
a
twenty-one-note
tune
comprising
concatenated
linearizations
of the
seven
three-note
Chords.
Example
3 shows the
can
tus,
shaped
to
have
a
"Phrygian"
character
(and
somewhat
adjusted
as
the
composition
went
into later
stages).
As
shown
by
the brackets and
letters at the bottom of the
example,
the first three notes of the cantus
linearize
Chord
M,
the
next
three
linearize Chord
L,
and
so
on;
the
melodic cadence
is
achieved
through
a
linearized form of Chord
P.
Imagining
a
vocal
piece,
I
looked for
a
suitable
text.
I
tried
to
find
a
stylistically appropriate
twenty-one-syllable
text
that could be
sung
to
the
tune
of the
cantus
firmus.
Example
4,
setting
three
seven-syllable
verses
of
text,
seemed
apt. (I
modified
my
original
cantus
firmus
slightly,
the
better
to
accommodate
this
text.)
Ben
-
e
-
die
-
tus
qui
ven
-
it
in
no
-
mi
-
ne
Do
-
mi
-
ni,
in
no
-
mi
-
ne
Do
-
mi
-
ni.
EXAMPLE
4
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16
Perspectives
of
New
Music
I wanted to harmonize each note of the cantus firmuswith each of the
three
Chords
to
which
it
belongs. Example
5a
sketches the
idea.
Wsym
bolizes
the
note
of
the
cantus
firmus;
the lines
on
Example
5
a
indicate
the three Chords
containing
W,
that
is
{W,
XI,
X2],
{W,
Yl,
Y2\,
and
[W,Z1,Z2\.
a)
b)
c)
/W\ ,WV /Wl
W2
XI Yl Zl XI-Yl-Zl XI-Yl-W3
III
III II
XI Yl 72 X2?Y2-22 X2-Y2-W3
EXAMPLE
5
It is
not
hard
to
see
that
the
seven
"points"
of
Example
5a
must
be
the
seven
distinct
notes
of the
mode.2
One
naturally
hopes
to
be
able
to
arrange
matters
as
in
Example
5b,
so
that
{XI,
Yl,
Zl]
and
{X2,
T2,
Z2\
will
be
Chords
(i.e.,
"lines"
of the
geometry), projected
as
vocal lines in
the
two
accompanying
voices.
But
this
is
not
possible.
The line deter
mined
by
XI
and
Yl will
indeed contain
one
of
the
Z-points,
but that
same
Z-point
(not
the
other
one)
will also be the
third
point
on
the
X2
72 line.3
This feature
of
the
system suggests
the
compositional algorithm
sketched
by Example
5c.
Here Wl
symbolizes
the
present
note
of the
cantus
firmus,
and
W2
symbolizes
the
next
note
of
the
cantus.
(The
can
tus was
constructed
so
as
not to
have
repeated
notes.)
If
W3
is the
third
note
of
the Chord
containing
Wl
and
W2
(the
third
point
on
the
line
containing
Wl and
W2),
then the
X-notes
and
T-notes
can
be
arranged
so
that
X1-Y1-W3
is
a
geometric
line
(i.e.,
a
Chord),
and
X2-Y2-W3
is
also a geometric line (a Chord). Indeed, this arrangement isunique, up
to
contrapuntal
inversion of "voice
1"
and "voice
2,"
and/or
exchange
of
notes
Xn
with
notes
Tw.4
The basic
algorithm
of
Example
5
c
produced
the
compositional
study
of
Example
6.
Other
features
of
the
projective
geometry suggest
other
compositional
possibilities.
Consider for
instance the fact
that
every
pair
of distinct
notes
belongs
to
exactly
one
Chord,
to
which
exactly
one
other
note
also
belongs.
This
enables
one to
add
a
third
part automatically,
to
any two-part
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Projective
Geometry
17
nit,
ui
ve
-
-
-
nit,
n
m
mi
-
-
ni_
Do-mi
ni,_Do
-
mi
-
ni,
_
Do
- -
mi
-
ni,.
in_
no
-
-
mi
-
- -
ne inno
-
mi
-
ne
_
EXAMPLE
6
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18
Perspectives
of
New Music
example
7
diatonic
counterpoint
that does
not
contain
a
vertical
octave
or
unison.
Example
7
illustrates,
adding
a
third
part
to
an
example
from
Zarlino.5
The example illustrates his "third mode"; given our particular Chord
vocabulary,
it is
of
course
natural
to
select
a
two-part
model
from
one or
another E-final mode. The exercise could be made
more
elegant
if
it did
not
cling
so
doggedly
to
the
notion
that
every
three-note
verticality
had
to
be
a
Chord
of the
geometric
system;
protocols
for non-Chordal verti
calities
in
three
voices
could
of
course
be
worked
out.
Another
resource
for
composition
in
our
geometric
mode
is
"modula
tion"
to
secondary
modes. This
can
be
accomplished
in
several
ways. First,
the Chords of
Example
2
can
all
be
transposed by
a
fixed number of semi
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Projective
Geometry
19
a) b)
L'
W
N'
P'
?r
R' S' V
M' N' P'
Q
R'
S'
(M)
(Q)
(R)
(Q)
(P)
EXAMPLE
8
tones,
introducing
ficta
as
appropriate.
An
appropriate
interval
of
transpo
sition is
five
semitones
(Example
8a):
that
is
because
the
two
harmonic
triads
of
themode
are
related
by
T5;
also the
transposition
introduces
only
one ficta tone. The a-minor triad serves as
pivot:
Chord V of the trans
posed
mode
coincides with
Chord
M
of
the
original
mode.Example
8b
shows
the
original
mode
transposed
by
T2.
This introduces ficta
tones
F|
and
C|.
Chord
5'of the
transposed
mode
coincides with Chord
Q
of the
original
mode.
Example
8c
shows
a
particularly
idiomatic
pitch-class
inver
sion of
the
original
mode,
inversion-about-D. No
ficta
tones
are
intro
duced,
and
there
are
many
pivot-Chords:
P'and
il'coincide
with R and P
respectively;
Q
'coincides with
Q.
The
mode
of
Example
8c could be taken
in itself as a sort of
"Ionian/C-major"
structure.
That
suggests
another
sort
of
modulation
one can
make,
from the
original
mode
of
Example
2.
Namely,
one can
modulate
to
other diatonic
modes,
modes
given
by
other choices of
Chords,
to
realize
a
projective
plane
with the
seven
white
notes
as
"points."
One
can
easily
construct
large
numbers of such modes.
For
that
purpose,
the
abstract
configura
tion of
Example
9 is useful.
First
one
selects three basic
Chords,
which
one
might
think
of
as
"pri
mary." These are the Chords corresponding to lines 123, 345, and 561
on
the
figure.
The
primary
Chords
must
be
selected
so
that
any
two
of
them
have
exactly
one common
tone.
C-, G-,
and
F-major
triads could
not
be selected
as
the
three
Chords,
because the G
and the F triads
have
no
common
tone.
One
could,
however,
select
{C,
E,
G}, {F,A,
C},
and
{G, F,
B}.
Arranging
the
notes
to
suit
the
configuration
of
Example
9,
one
could take
C
=
1,
G
=
3,
F
=
5,
E
=
2,
B
=
4,
A
=
6. Then
the
remain
ing
note,
D,
would be
number 7 in
the
example.
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20
Perspectives
of
New Music
If
123, 345,
and
561
are
all
formal
"lines"
of
the
geometry,
then
so are
174,
376, 572,
and 246.
example
9
The choice of the "basic triangle" on Example 9 exhausts six notes of
the
mode.
The seventh
note
appears
at
the
center
of the
triangle.
It
must
be
the
case
that
174, 376,
and 572
are
all formal
"lines" of
the
geometry;
the
corresponding
notes
will then be
formal Chords
of
the
system.6
Finally,
it
must
be the
case
that 246 is
a
formal
"line";
the
corresponding
notes
then
form the
seventh
Chord.7
(a) (b)
(c)
"Ionian/Cmaj";
"Dorian";
primary "Mixolydian";
primary
Chords
CEG,
Chords
DFA, GBD,
primary
Chords
GBD,
FAC, GBF;
other
EGA;
other
Chords
DFA, GAC;
other
Chords
BCD,
DGA,
CDE, ABC, FGC,
Chords
CDE, EFG,
DEF,
EAB.
BEF.
EAB,
BCF.
EXAMPLE
10
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Projective Geometry
21
Example 10a shows themode generated by the "primary Chords" {C,
E,
G},
{F,A, C},
and
{G,
F,
B},
as
begim
above.
This
turns
out
to
be the
"Ionian/C-maj"
mode
encountered earlier in
Example
8c;
it
was
the
inversion
of
our
original
"Phrygian"
mode about
D.
Example
10b shows
a
"Dorian"
mode
generated by
taking
{D, F,
A},
{G, B, D},
and
{E,
G,
A}
as
primary
Chords.
Example
10b
inverts about D
to
yield
Example
10c,
a
"Mixolydian"
mode with
primary
Chords
{G, B, D},
{D,
F,
A},
and
{G,
A,
C}.
Chords
DFA,
GBD,
and
CDE
serve as
pivots
between
our
Dorian
and
Mixolydian modes;
FGC
pivots
as a
Chord
for
both
our
Phrygian
and
our
Dorian mode.
There
is
of
course
little
reason,
other than
historicist
sentimentality,
to
assign
special priority
to
harmonic
triads
as
Chords,
"primary"
or
other
wise,
in
constructing
any
formal
diatonic mode
(i.e.,
geometry).
Further
techniques
of
"modulation"
are
available.
Some mathemati
cally
idiomatic
ones
will
be
discussed
later,
"collineations"
in
particular.
* *
In
any
projective
plane,
there
are
many
ways
of
choosing
a
structure
almost
like that of
Example
9,
a
structure
consisting
of
seven
points
{1,2,
3, 4,
5,
6, 7}
in
which
123, 345, 561,
174, 376,
and
572
are
all
formal
"lines" of
the
geometry.
In
general,
246 need
not
be
a
formal
line.
We
shall
call
any
such
structure
a
"reference
quadrangle."
A
generic
reference
quadrangle
may
be
constructed
as
follows.
Given
any
projective plane
(whether
a
seven-point
plane
or
some
other),
select
"1" and "3" as any two distinct
points.
(Any line contains at least three
distinct
points.)
Since
not
all
points
of
the
plane
lie
on one
line,
select
"5"
as
any
point
not
on
the
line 13.
The
lines
13, 35,
and 15
are
all distinct.
(If
any
two
coincided,
then
points
1,3,
and 5 would all
be
collinear,
and
point
5
would lie
on
line
13,
contrary
to
construction.)
So,
in
particular,
lines
13 and 15
are
dis
tinct. Let
L
be
a
third line
passing
through
point
1.
(Every point
lies
on
at
least
three
distinct
lines.)
Take "4"
to
be the
point
where
line
L
meets
line 35. Point 4 isnot the same as point 3, since Lis distinct from line 13.
Point
4
is
not
the
same as
point
5,
since
L
is
distinct from
line
15.
Line L
contains
at
least three
distinct
points,
including
points
1
and 4.
Take "7"
to
be
a
third
point
on
line L.
Then 7
cannot
lie
on
any
of
the
other lines
so
far constructed
(13,
15,
or
35).
If
7
were on
line
13,
then
line
17,
which is
L,
would
be the
same
as
line 13?but L
was
taken
to
be
distinct from
line 13. If
7
were on
line
15,
then
line
17,
which
is
L,
would be
the
same as
line
15?but
L
was
taken
to
be
distinct
from
line
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12/53
22
Perspectives
of
New Music
Jl
=
[p2,p3, ql, ri} Kl
-
[pi, ri, s2, s3)
J2
=
[pi,
p3, q2,
r2\
K2
=
[p2,
r2, si,
s3}
J3
=
[plyp2,
q3,
r3]
K3
=
[p3,
r3,
si,
s2]
Ll
=
[pi, ql,
si,
t)
Ml
=
[q2, q3,
ri,
si)
L2
=
[p2,
q2,
s2, t)
M2
=
[ql,
q3,
r2,
s2\
L3
=
[p3, q3,
s3,
t]
M3
=
[ql,
q2,
r3,
s3)
N=[rl,r2,r3,t\
EXAMPLE
11
15. If 7
were on
line
35,
7 would be the
point
where
L
meets
line
35?
but that
point
is
point
4,
and
7
was
chosen
to
be
distinct
from
4.
Take
"2"
to
be the
point
where line 57
meets
line
13. Point
2
is
dis
tinct from
point
3: if2
=
3,
then line 25
=
line
35,
and
point
7 would lie
on
line 35?which it doesn't. Point 2 is distinct from
point
1:
if 2
=
1,
then line 25
=
line
15,
and
point
7 would lie
on
line 15?which
it
doesn't.
So
1, 2,
and 3
are
different
points
of line 13.
In like
manner,
taking
"6"
to
be the
point
where line 37
meets
line
15,
we see
that
1,
6,
and 5
are
distinct
points
of
line
15.
In
sum,
points
1
through
7
are
all
distinct; 123, 345,
561,
275,
471,
and
673
are
all dis
tinct lines.
In
the
general
projective
plane,
it
need
not
be the
case
that
points
2, 4,
and 6
are
collinear.
Part
II:
Some Other
Projective
Planes,
with
Musical Applications
A
generic thirteen-point projective plane
can
be
conceptualized
as
fol
lows. Let the
"points"
of
the
system
be
symbolized
as
pi, p2, p3, ql, q2,
q3,
rl, r2,
r3,
si,
s2,
s3,
and
t.
Then take
as
the thirteen "lines"
the
sets
of
points
J1,J2,
etc.
given by Example
11.
The given thirteenpoints, togetherwith the stipulated thirteen lines,form
a
projective plane.
The reader
may
check
the four
required properties:
1.
Any
two
points
lie
on
just
one
line.
2.
Any
two
lines
pass
through
just
one
point.
3.
Every
line
passes
through
at
least three
points;
every
point
lies
on
at
least
three lines.
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Projective Geometry
23
4. It is
not
the
case
that every point lies
on
every line.
In the
thirteen-point
plane,
every
point
lies
on
exactly
four lines and
every
line
passes
through
exactly
four
points.
The
thirteen-point plane
can
be used
to
structure
"chromatic"
modes,
if
one
adjoins
a
special
symbol
$
to
the
twelve
chromatic
pitch
classes.
The
special
symbol
could
be realized
musically
as
silence,
or as a non
pitched
event,
or as a
wild card.
Example
12
shows the
structure
of
one
such
mode.
pl=B,p2
=
G,p3=?, ql=D,
#2=Bt,
q3
=
G$,
ri=C, r2=E,
r3-Cf,
?i=Et,?2=Ff,.tf
=A,?
=
$.
/i={G,F,D,C}
tfi?{B,C,Ff,A}
J2
=
{B,
F,
Bt,
E}
K2
=
{G,
E,
Et,
A}
J3
=
{B,G,
Gf, Cf}
K3
-
{F,
Cf,
Et, Ff}
LI -
{B,
D,
Et,
$}
Ml =
{Bt,Gt,
C,
Et}
L2
=
{G,
Bt,
F|,
$}
M2
-
{D,
Gf,
E,
Ff}
L3
=
{F,
Gf,
A, $}
M3
=
{D,
Bt, C|,
A}
tf={C,E,Cf,$}
EXAMPLE
12
To
construct
the
mode of
Example
12
I
proceeded
as
follows.
I
decided
to
make the
special
symbol
$
the
point
t
of
Example
11. I
then
considered
the
four
lines
of
Example
11
that
would contain the
special
symbol
t
=
$.
These four
formal lines would be realized
in
the musical
mode
by
formal
Chords
thatwould each
comprise
three
"genuine
notes"
plus
the
special
effect.
I
decided
to structure
the mode
so
that those four
Chords
would be
transposed
or
inverted
forms,
each of
any
other.
I
spe
cificallydecided thatLI
=
[pi, ql, si, t)would be {B,D, Et, $}, that L2
=
[p2, q2,
s2,
t)
would be
{Ff,
G,
Bt,
$},
that L3
=
[p3,
q3,
s3,
t)
would be
{F,
Gf,
A,
$},
and
that
N
-
[rl,
r2,
r3,
t)
would be
{C,
Cf,
E,
$}.
Thus
the three
notes
B, D,
and
Et
would
be
assigned
in
some
order
as
the
points
pi,
ql,
and si
of
Example
11;
likewise the
three
notes
Ff,
G,
and
Bt
would
be
assigned
in
some
order
as
the
points
p2, q2,
and s2
of
Example
11,
and
so
forth.
Playing
around with
various
possibilities
for
those
assignments,
considering
the other
Chords
that
Example
11
would
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14/53
24
Perspectives
of
New Music
generate in each case, I arrived
at
themode of Example 12. Evidently
an
enormous
number of such modes
can
be
constructed.
(t-1-1)-1-p3-s3v
rl
r
-s
/-qJv pi-p
I-r3-(q3-q3-q3-q3)
rl-p
I-P3-(ql?ql-ql-ql)-J--ql
r3-ql-$3'
s2-rl-qV
si
EXAMPLE
13
Example
13 demonstrates
an
algorithm
for
harmonizing
certain
types
of
cantus
firmus.
The
example
supposes
the
succession
t,
q2, q3
as a
seg
ment of such a cantus firmus.All vertically aligned sets of four events in
the
example
are
Chords of the
generic
system.
At the
left,
the
cantus
fir
mus
event
tis harmonized
by
the four vertical Chords that contain it:
{t,
rl,
r2, r3}, {t,
si,
pi,
ql],
{t,
q3, p3,
s3],
and
(moving
onwards)
{t,
p2, q2,
s2).
The
voice
leading
can
be
arranged
so
that the three
accompanying
voices
of the first three chords all form formal lines with
q2,
the
next
event
of the
cantus
firmus. That
is?as
indicated
by
the horizontal and
diagonal
lines
in
Example
13?[rl,
si,
q3, q2)
is
a
formal
line;
so
is
\r2,
pi, p3, q2}y
and
so
is
[r3,
ql,
s3,
q2\. q2
now
takes
over as
cantus
firmus
event,
and it is first armonized
by
the
(unique)
chord that contains both
q2
and
t.
The
process
then
repeats,
aiming
at
q3,
the
next event
of
the
cantus
firmus.
Evidently,
in
this
arrangement,
it is
necessary
for
q3
not to
be
p2
or
s2?i.e.,
q3
must not
lie
on
the
line
defined
by
t
and
q2.
And
of
course
t
and
q2
must
be
distinct.
The
cantus
is thus
constrained
as
follows:
it
must
contain
no
immediately
repeated
events,
and
no
three consecutive
events
may
be collinear.
In
Example
13, the three initial lines of "alto," "tenor," and "bass"
voices,
under
t
in the
cantus
firmus,
become
verticalities when
q2
takes
over
the
cantus
role:
the
alto's initial
line
rl-sl-q3-q2
becomes the last
four-point
verticality
shown
in
the
example;
the tenor's
initial
line
r2-pl
p3-q2
becomes the fifth four-note
verticality,
and
so
forth. This
is
a
fea
ture
of the
algorithm.
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Projective
Geometry
25
* *
*
The
thirteen-point
plane
can
also be
applied
to
other musical
phenom
ena.
For
instance,
there
are
exactly
thirteen
of what
Larry Polansky
calls
"ternary
contours."8
These
are
illustrated
in
Example
14. The
thirteen
point
plane
will
organize
these
contours
into
mathematical
"lines,"
each
of
which
is
a
group
of
four
contours.
Example
11 will
help
the
reader
experiment
with
various modes
of
such
grouping, assigning
the
symbols
ply p2,
etc.
in
various
ways
to
the thirteen
symbols
of
Example
14.
EXAMPLE
14
* * *
There
is
a
twenty-one-point projective plane;
every
line therein has
exactly five points, and every point lies on exactly five lines. A generic
structure
for
the
plane
can
be
obtained
by
algebraic
techniques
to
be dis
cussed later. The
geometric
structure
could be
applied,
in various
"modes,"
to
the
family
of
twenty-one
diatonic unordered
dyads.
There is also
a
thirty-one-point projective plane;
every
line therein has
exactly
six
points,
and
every
point
lies
on
exactly
six
lines. The
structure
might
be of
interest
to
those who
are
interested in the
thirty-one-tone
scale;
the
geometry
would
single
out
a
privileged
family
of
thirty-one
hexachords
as
formal "lines" of the
system.
The
thirty-one privileged
hexachords
could be chosen
in
a
vast
variety
of
different
"modes."
Part
III: Algebraic
Structure
of the
Projective
Plane
There is
a
common
algebraic
structure
underlying
all
projective planes,
a
structure
which is
very
helpful
for
constructing
a
"generic" specimen
of
a
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16/53
26
Perspectives
of
New
Music
given plane, along the lines of Example 11 earlier. To grasp suchmatters,
one
must
first
nderstand the
notion
of
an
algebraic
"skew-field."
By
that
term,
a
mathematician
understands
a
set
F
of
objects
x,
y,
etc.,
upon
which
two
binary
combinations
are
defined.
The
combinations
are
usually
denoted
using
conventional
symbols
for
addition
and
multiplica
tion:
thus
objects
x
and
ymay
be
combined
so as
to
yield
a
formal
"sum"
x
+
y,
and
a
formal
"product"
xy.
In
order
to
constitute
a
"skew-field,"
the
system
must
satisfy requirements
1, 2,
and
3
following.
1. Pis
a
commutative
group
under addition.
The
identity
element is
denoted
by
0;
the additive
inverse
of
element
a;
is
denoted
"-#".
2.
The
non-zero
elements
of F
form
a
group
under
multiplication.
The
identity
element of the
group
is
denoted
by
1;
the
multiplicative
inverse of
a
non-zero
#is denoted
by
"aT1"
or
by
"1/V\
3.
Multiplication
distributes
over
addition,
according
to
the
laws
x(y
+
z)
=
xy
+
xz\ (x +y)z
=
xz
+yz.
If
multiplication
is
commutative,
the
skew-field
is
called
a
"field."
The
real
numbers
form
a
field.
So
do the rational
numbers?those
which
can
be
expressed
as
quotients
of
integers.
So
do
the numbers
of
form
a
+
b(Jl),
where
a
and
b
are
rational
numbers
and
Jl
is
the
(irrational)
square
root
of
2.
The
multiplicative
inverse
of
a non-zero a +
b(
Jl
)
is
(a
-b(j2))/(aa-
2bb)?the
denominator
cannot
vanish because
a2
cannot
possibly equal
2e2,
a
and b
being
rational and
not
both
zero.9
The integersmod 2 form a field. Those are the integers 0 and 1with
all
arithmetic reduced modulo
2?e.g.,
1
+
1
=
0. The
integers
mod 3
are
also
a
field,
that is the
symbols
0,
1,
and
2
with
arithmetic
reduced
mod
ulo
3:
2
+
1
=
0,
2 2
=
1
(4
is
one
more
than
some
multiple
of
3),
and
so
forth.
The
integers
mod 5
are a
field,
that is
the
symbols
0,1, 2, 3,
and
4,
with
all arithmetic reduced
modulo
5.
(4
3,
for
instance,
=
2,
since
12
is
two
more
than
some
multiple
of
5.)
In
general,
for
any
prime
number
p,
the
integers
mod
p
form
a
field.
There
are
other
finitefields
as
well. For
instance,
there is
a
field
of four
elements which
one can
denote
as
0,1,
a,
and
a
+
1. In
this
field,
anything
added
to
itself
produces
0,
and
a2
equals
a +
1.
These
properties
enable
one
to
carry
out
the
necessary arithmetic,
to
verify
that
the
structure
is
a
field. For
instance,
a(a
+
1)
=
a2
+
al
=
(a
+
I)
+
a
=
I
+
a
+
a
=
1.
Then
(a
+
l)(a
+
1)
=
a(a+
1)
+
l(a+
1)
=
(I)
+
(a
+
1)
=
1
+
1
+
a
=
a.
The
cardinality
of the field
just
studied,
four,
is
not
a
prime
number,
but it
is
a
power
of
a
prime.
In
general,
for
any
prime
number
p
and
any
positive integer
?,
there will be
a
field
of
cardinality
p^.
Furthermore, any
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Projective Geometry
27
finite fieldmust be one of those. Indeed, any finite skew-field must be
one
of
those,
since
a
remarkable theorem shows
that
any
finite skew-field
must
be
a
field.
* * *
Now
we are
ready
to
construct
a
generic projective plane.
Let
F
be
some
skew-field
(any
skew-field).
Consider the
family
of all
ordered
triples
formed from members
bl, b2,
and b3 of F.
We
stipulate
that
two
such
triples,
say
and
,
are
"left-equivalent"
if
there is
some non-zero
number k in
F
such that bl'
=
k
-
bl,
b2'
=
k
-
b2,
and b3'
=
k b3. This
in
indeed
an
equivalence
relation
among
the
triples.
The relation is
reflexive
(bj-
1
bj,forj
=
1, 2,
3);
it is
symmetric
(if
bj'=
k
-
bj,
then
bj
=
(l/k)
bjy,
the relation is also
transitive
(if
bj"
=
h
bj',
then
bj"
=
(hk)
bj).
The
points
of the F
Projective
Plane
are
labeled
by
the
non-zero
left
equivalence-classes
of
F-triples.
That
is,
is excluded
as a
"point"
of
the
geometry,
but
every
other
F-triple
represents
a
point;
among
those
triples
and
represent
the
same
point
if
and
only
if
there
is
some
non-zero
?in F such
that
cj
=
k-
?/for
each
y
=
1,2,3.
We shall label the
formal lines
of the
F
Projective
Plane
by
the
non
zero
right equivalence-classes
of
F-triples,
which
we
shall write
using
square
brackets:
the
triple
[XI, X2, X3]
is
r^i-equivalent
to
the
triple
[XI
',
T, X_H
if there is
some non-zero
k in
_Fsuch that
Xj'
=
Xj
k,
for
each
j
=
1,
2,
3.
Every
non-zero
triple
represents
a
line; among
those
triples [XI, X2, X3] and [Tl, T2, T3] represent the same line ifand
only
if there is
some non-zero
k in _Fsuch that
Yj
=
Xj-
k,
for each
j
=
1,2,3.
The
point
b=
lies
on
the line
X=
[XI,
X2,
X3]
if
and
only
if
he sixnumbers
atisfy
he
equation (bl)(Xl)
+
(b2)(X2)
+
(b3)(X3)
=
0 in the skew-field
F.
One
sees
that if b'
is
left-equivalent
to
b,
and/or
right-equivalent
to
X,
the numbers
?y'and Xj'wi? satisfy
the
same
equa
tion. Hence the relation
"? lies
on
_?" is
well-defined for
points
and lines.
The known
algebraic
behavior of such
equations
in
skew-fields
guaran
tees that the "points" and "lines" of the "F Projective Plane," as defined
above,
do indeed constitute
a
projective
plane.
That is:
1.
Any
two
points
lie
on
just
one
line.
2.
Any
two
lines
pass
through just
one
point.
3.
Every
line
passes
through
at
least
three
points;
every
point
lies
on
at
least three lines.
4. It isnot the case that every point lies on every line.
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28
Perspectives
of
New
Music
The Property of Desargues (discussed in note 1) also obtains. Remark
ably
enough,
every
projective plane
(i.e.,
every
aggregation
of
formal
points
and
formal
lines
satisfying
the
four
properties
above
and the
Prop
erty
of
Desargues)
can
be
labeled
by
numbers from
some
F
Projective
Plane
so as
to
realize the
algebraic
structure
described
above.
That
is,
every
Desarguesian) Projective
Plane
"is"
in
fact
an
F
Projective
Plane,
for
some
suitable F.
If
the
Pis
finite
(and
hence
a
field)
we
can
count
the
number of
points
in
the
F
Projective
Plane.
Say
the
cardinality
of Pis
q,
where
q
is
a
power
of
some
prime
p
(as
earlier).
The
number
of
F-triples
is
then
q3,
and the
number of
non-zero
F-triples
is
q3
-
1.
Of
those,
each
is
equivalent
to
q
1
others,
since each
triple
can
be
multiplied
by
any
of
the
q
-
1
non-zero
members of F
to
form
an
equivalent
triple.
The
number
of
non-zero
equivalence
classes
is then
q*
-
1
divided
by
q
-
1.
That
number is
equal
to
1
+
q
+
q2,
which
will
be the
number of
points
in
the
corresponding
projective plane.
If
#
=
2,l
+
#
+
#2
=
l+2
+
4
=
7;
the
mod-2
projective
plane
is
our
seven-point
"diatonic"
plane.
If
#=3,
1
+
^
+
^
=
1
+
3
+
9
=
13;
themod-3
projective plane
is our
thirteen-point
"chromatic"
or
"ternary
contour"
plane.
If
q
=
4,
we
obtain
the
twenty-one-point
plane;
if
q
=
5,
we
obtain
the
thirty-one-point
plane.
Six is
not
a
prime
power;
there is
no
six-element
(skew-)field,
so
there is
no
forty-three-point
pro
jective
plane.
But
there
is
a
seven-element
field,
so
there
is
a
fifty-seven
point
projective
plane. Eight
and nine
are
each
prime
powers,
so
there
is
a
seventy-three-point
plane,
and
a
ninety-one-point plane.
Part
IV:
Applications?Mathematical
and
Musical?of Part
III
to
the
Twenty-One-Point
Plane
21
=
1+4+16;
the
twenty-one-point
projective plane
"is"
in
fact the
F4
Projective
Plane,
where F4 is
the four-element
field
discussed in
Part III.
F4
=
(0,1,?,#+1};
anything
added
to
itself
is
0;
a +
1
=
02.
One
verifies
that
0(0
+
1)
=
(0
+
1)0
=
03
=
1;
(0
+
l)2
=
0;
(0
+
l)3
=
1.
1
+
(0
+
1)
[= 1 + 1 + 0]
=
a, and so forth.
Given
a
twenty-one-point projective
plane,
we
shall
now see
how it
manifests
the
structure
of
the F4
Projective
Plane.
Using
the
method
dis
cussed
at
the
end of
Part
I
earlier,
we
select
any
"reference
quadrangle"
in
the
plane;
let its
points
and
lines be
denoted
as
in
Example
15:
points
pi,
p2,
p3,
q,
rl,
r2,
and
r3\
lines
Jl,
J2,
J3,
Ml, M2,
and
M3,
each line
containing
inter
alia
the
points specified
on
the
figure.
Now,
using
numbers
from
F4,
we
label
pi
=
,
p2
=
,
p3
=
,
and
q
=
. The
algebraic
structure
of the F4 Plane
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Projective
Geometry
29
Jl=[p2,p3,rl,
J2
=
[p3,pl,r2,
J3
=
[pl,p2,r3,
Ml
=
[pl,
q,
rl,
M2
=
[p2, q, r2,
M3
=
[p3,
q,
r3,
EXAMPLE
15
tells
us
what
the
line coordinates for
Jl
will
be. Both
p2
and
p3
have
first
coordinate
equal
to
zero.
That
is,
both
are
points
b
=
satisfy
ing the equation bl
-
0. Thus, both points satisfythe equation (bl)(Xl)
+
(b2)(X2)
+
(b3)(X3)
=
0,
where
XI
=
1,
X2
=
0,
and
X3
=
0. We
know,
from
the
algebraic
structure
developed
in Part
III,
that
the
coordinates
for
Jl
will
then
be
[1,
0, 0]:
Jlis
that line
containing exactly
such
points
b
as
satisfy
bl =0
(more
explicitly,
bl
1,
plus
b2
0,
plus
b3
0
equals
0).
Similarly,
J2
=
[0,1,
0];
J2
contains
just
those
points
b
satisfying
b2
=
0.
And
J3
=
[0, 0, 1];
J3
contains
just
those
points
b
satisfying
b3
?
0.
Example
16
updates Example
15
to
display
the
new
information.
pl
-
,
pl=,p3
=
q-
/Z-[1,0,0]
J2
=[0,1,0]
J3
=
[0,0,1]
Ml=[pl,q,rl,.
M2
=
[ply
q,
rl,
.
M3
=
[p3y
}
r3,
.
EXAMPLE
16
[pl,p3,rl,..
[p3,pl,rl,..
[pl
l(W-O)
.K*2-0)
p2yv3y...
}(b3=0)
Next
we
shall find
the line
coordinates
for
Ml
in
F4.
The
lineMl
=
[XI,
X2,
X3]
passes
through
the
points pl
=
and
q
=
.
Accordingly,
we
must
have
1 XI
plus
0
X2
plus
0
X3
equal
to
0
(since
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30
Perspectives
of
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Music
pi lies onMl), and also 1 XI plus 1 X2 plus 1 X3 equal to 0 (since q
lies
on
Ml).
That
is,
we
must
have
XI
=
0,
XI
+
X2
+
X3
=
0. Or: XI
=
0,
X2
=
X3.
Accordingly
Ml
=
[0,
1,
l].10
In similar
fashion,
we see
thatM2
=
[1, 0, 1],
and
that
M3
=
[1,
1, 0].
The
new
information
is
displayed
in
Example
17.
pi
=
,
p2
=
,
p3
=
,
q
=
/i-
[1,0,0]
/2
=
[0,1,0]
J3
=
[0,0,1]
{p2,p3,rl,.
[p3,pl,r2,.
\pl,p2,r3,.
?fi-[0,1,1]:
{?I,
ft ri,.
?I?
-
[1, 0,1]:
{?2,
ftr2,.
M3-[l,l,0]:f^,ftr3,.
(M-0)
(?2=0)
(W-0)
(b2
=
b3)
(bl=b3)
(bl=b2)
EXAMPLE 17
Now
we
shall find the
point
coordinates
for
point
rl.
Suppose
those
coordinates
are
. Since rl lies
on
line/i
=
[1,
0,
0],
we
have
bl
=
0. Since
rl
lies
on
lineMl
=
[0,
1,
1],
we
have b2
+
b3
=
0,
whence b2
=
b3
(in F4).
In
sum:
bl
=
0;
b2
=
?3.
ri is
then labeled
by
the
triple
.
Similarly,
r2
is
labeled
by
the
triple
,
and
r3 is
labeled
by
the
triple
.
Example
18
updates
Example
17
with
the
new
information.
In the
particular
field
F4,
1 + 1 = 0.
Therefore,
in the
particular
sys
tem
we are now
considering,
the
sum
of rl's
three coordinates
is
zero.
So
is the
sum
of r2's
three
coordinates,
and
so
is the
sum
of
r3,s
three
coor
dinates. That
is,
the
points
rl, r2,
and
r3 all
satisfy
the
equation
bl
+
b2
+
b3
=
0.
(This
would
not
be
the
case
in
a
field where
things
added
to
themselves
were
not
zero.)
Hence
the three
r-points
all lie
on
the line
L
=
[1,
1, 1].
Example
19
updates Example
18 with the
new
information.
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Projective
Geometry
31
pl
=
,
p2
=
,
p3
=
,
q
=
rl
=
,
r2
=
,
r3
=
Jl
=[1,0,0]:
[p2,p3,rl,.
J2
=
[0,1,0]:
[p3,pl,
r2,
.
J3
=
[0,0,1]:
[pl,p2,r3,.
Ml
=[0,1,1]:
[pl,q,rl,.
M2
=
[1,0,1]:
[P2,q,r2,.
M3 =
[1,1,0]:
[p3,q,r3,.
(bl=0)
(b2=0)
(b3
=
0)
(b2
=
b3)
(bl=b3)
(bl=b2)
EXAMPLE
18
Example
19,
we
now
see,
realizes
a
seven-point plane
embedded
within
the
twenty-one-point
plane.
That
is
because the two-element field
F2
=
{0, 1}
is
a
subfield
of F4. The
seven
points
and
seven
lines of
Example 19 are exactly those points and lineswhose coordinates can be
written
using
only
numbers from F2.
Since
our
original
choice of refer
ence
quadrangle
was
arbitrary,
we can
pause
to
note
the
interesting
fact:
any
choice
of reference
quadrangle
in
the
twenty-one-point projective plane
realizes the
seven-point
plane.
The visual
image
of
Example
19,
on
the
Euclidean
plane
of
the
page,
begins
to
be
deceptive
now?for
instance
it does
not
show
us
that
rl, r2,
and r3
are
collinear.11
So
we
shall continue onwards
from
Example
19
purely algebraically, adjoining
other
points
and
lines
of
the
twenty-one
point plane using number-triples
of F4. The
coordinates
of
our new
points
and lines
will
all
involve numbers of
F4 that
are
not
numbers of
F2;
thus
they
will all involve
the
number
a
of F4.
Example
20 lists the
twenty-one
points
of the
plane,
identifying
them
with
twenty-one
non-equivalent
number-triples
from F4. And
Example
21
lists the
twenty-one
lines
of the
plane, giving
their line coordinates
in
square brackets;
Example
21
also
shows
which
points
of
Example
20 lie
on
which of
those
lines.
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32
Perspectives of
New Music
pi
=
,
p2
=
,
p3
=
,
q
=
ri
?
,
r2
=
,
r3
=
Jl=[l,0,0]:{p2,p3,rl,..
J2
=
[Q,l,0]:{p3,pl,r2,..
J3
=
[0,0,1]:
[pl,p2,r3,.
.
L-[l,
1,1]:
[ri, r2,r3,...
Ml=[0,l,l]:[pl,q,rl,..
M2
=
[l,Q,l]:{p2,q,r2,..
M3
=
[l,l,0]:{p3,q,r3,..
.}(W-0)
.}(f?-0)
.}(f??0)
}(M
+
*2
+
*3-0)
. }(t?-*3)
,
}(M-*3)
.
)(W-t?)
EXAMPLE
19
?i=,
ri=l>)
si
=,
ii'
=
,
tl
=,
fi'
=
7/23/2019 Lewin - Some Compositional Uses of Projective Geometry
23/53
Projective Geometry
33
Jl
=[1,0,0]
J2
=
[0,1,0]
/5
=
[0,0,1]
?
=
[1,1,1]:
Ml
=[0,1,1]
Ml-
[1,0,1]
M3
=
[1,1,0]
M
=[0,0,1]
#2
=
[0,0,1]
N3
=
[0,1,0]
ATi'
-[0,*
+
l,l]
N2'
=
[0 +1,0,1]
AT3'
=
[0
+
1,1,0]
?-[^,1,1]
K2-[1,*>1]
K3-[l,l,*]
Kl'
=[0
+
1,1,1]
Kl' =[1,0 + 1,1]
K3'
=[1,1,0
+
1]
G
=
[l,0,0
+
1]:
#=[1,0
+
1,0]:
[p2yP3ytlySlySV\
[plyp3yrlyslysi]
[pl,pl,r3,s3,s3'}
[rly
rly r3y
u,
v)
[plyqyTlytlyt?]
[pl,
qy
rly tly
ti
}
[p3y
y
r3y 3y
3'
)
[Ply
Sly
t?
yt3yU)
[flySlyt? yt3yV)
[p3y
3y ly
t?
y
U)
[plySl'
ytlyt3' yV)
[fly
S?
y
lyt3'
y
U)
[p3yS3'
ytlyti yV)
[rlySlyS3y
i'
yt? }
[Tly
ly
S3'
y
i'
y
3'
}
[r3ySl'
y
?
yti yti
[rly
S?
y
3'
y
ly
t3\
[rlyS3ySly tly t3\
[r3,
Sly
Sly
tly
tl\
[sly
i
y
3'
y
} u)
[Sly
S3y
S?
y
,
V)
(arithmetic nF4(\))
(W-0)
(?2-0)
(?5=0)
(bl+bl
+
b3
=
0)
(bl
=
b3)
(bl=b3)
(bl-bl)
(b3-a-bl)
(b3?a-bl)
(bl-a-bl)
(b3-(a
+
l)-bl)
(b3
=
(a
+
l)-
bl)
(bl=(a
+
l)-bl)
(a-bl-bl
+
b3)
(a-bl-bl+bJ)
(a-b3
=
bl+bl)
((a
+
l)bl=bl
+
b3)
((a + l)bl
=
bl+b3)
((a
+
l)b3-bl+b2>)
(bl+a(bl)
+
(a
+
l)b3=0)
(bl+(a
+
l)bl
+
a(b3)
=
0)
EXAMPLE
21
points listed in Example 20. One strategy?not the only one ?is to
begin
with
a
reference
quadrangle.
Example
22
assigns
to
Example
19
the values
pl
=
{CE},
pl
=
{FA},
p3
=
{GB},
r3
=
{EG},
rl
=
{DA},
r2
-
{BFU
=
{AC}.
EXAMPLE
22
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34
Perspectives
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New Music
These assignments give
a
"C-major"
sort
of reference
to
thequadrangle?a
feature evident
in
Example
23a,
where the bracketed
segments
are
collinear.
pi
r3
pi
rl
p3
rl
pi
pi
q
rl
r3
q
p3 p2
q
r2 r3
rl
p3
rl
pi
EXAMPLE 23
Example
23b
projects
the
same
formal
"lines"
as
verticalities,
indicat
ing
another
textural
possibility.
No
rhythm
is
indicated.
I
have
not
exer
cised
any
special
control
over
the
voice
leading
here,
simply
trying
to
project
vaguely Stravinskyish spacings
of the
dyad-triples.
Example
23
illustrates how the reference
quadrangle
of
Example
22
yields
a
seven-point subplane
of the
twenty-one-point plane. In the
present
context,
it is natural
to
arrive
at
the full
plane
by
"diminuting"
Example
23a. To
see
what that
means,
consider the first three
dyads
of
Example
23a. These
dyads,
playing
the roles of
pi,
r3,
and
p2,
all lie
on
line
J3
of the
full
plane,
but
they
do
not
constitute the
entire
line
J3
of
that
plane.
The
full line
J3,
as we see
in
Example
21,
contains
not
only
the
points
pi,
r3,
and
r2,
but
also the
points
s3 and
s3',
points
not
appearing
on
the reference
quadrangle.
We
can
naturally
imagine
dyads
s3 and
s3',
in
this
context,
appearing
"in
passing"
to
elaborate the
pro
gression pi,
r3,
p2
of
Example
23a. The
first
phrase
of
Example
24a
materializes
that
notion.
In
that
phrase,
the
progression pi,
r3,
p2,
which
began
Example
23a,
is
diminuted
by
transitional
dyads
{CG}
and
{EB}
that
appear
on
the off
beat
eighths.
To subsume those
dyads
onto
line
J3,
we
assign
them the
point-values
s3
and
s3',
the other
points
of line
J3.
The first
ive
dyads
of
Example
24a will then
project
line
J3
in
its
entirety.
In
like
spirit,
the
second five
dyads
of
Example
24a take the
progression
p2,
rl,
p3
from
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Projective
Geometry
35
pi
r3
p2 p2
rl
p3 p3
r2
pi pi
q
ri r3
q
p3
p2
q
r2 r2
r3
rl
s3 s3'
si si'
s2 s2'
tl tl'
t3 t3' t2
t2'
v u
EXAMPLE
24
Example
23a,
and diminute
it
by
inserting
transitional
dyads
{FG}
and
{CD}
on
the
off-beat
eighths;
the
transitional
dyads
are
then
assigned
as
points
si and
si',
so
the
phrase
as a
whole
projects
line
Jl
=
{p2,
p3,
rl,
si,
si'}
in
its
entirety.
Example
24a
proceeds
in
the
same
spirit through
out.
It
turns
out
(in
this
plane )
that
every
remaining point
of the
plane
will be referenced exactly once, by diminuting Example 23a in such a
way.
One
can
see
that
by
inspecting
Example
21;
there
one
sees
that the
lines
Jl,
J2, J3,
L, Ml, M2,
and M3
collectively
reference
point
u,
point
v,
each
?-point,
each s'
-point,
each
i-point,
and each t'
-point
exactly
once.
And those
are
the lines
which
appear
in
part
on
Example
23a,
as
progres
sions
to
be
"diminuted."
Example
24b
realizes the
five-dyad
lines
as
verticalities,
elaborating
the
three-dyad
verticalities of
Example
23b.
The
new
dyads
are
shown with
filled-in
noteheads.
Orchestration
and/or
other
compositional
means
(dynamics,
order of
entrance
and
exit,
amount
of
sustained
time,
etc.)
could
be used
to
project
the
idea that the
open-notehead
parts
of each
sonority
is
more
in
the
nature
of
a
Zentralklang,
while
the filled-in
noteheads
project
Akzidentien}2
On the
other
hand,
a
composer
might
not
choose
to
project
explicitly
the
"referentiality"
of
Example
23b,
treating
that
only
as
a
work
ing
method
to
arrive
at
the full
twenty-one-point
structure.
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36
Perspectives
of
New
Music
DEFGABEFGABFGAB
CCCCCCDDDDDEEEE
si'
pi
t3' s3
q
tT t2' s2' t3 rl t3
u
r3
v
s3'
G
A B A B B
F F F G G A
si
p2
r2 s2
p3
t2
EXAMPLE
25
Example
25 shows
the
assignment
of
dyads
to
points,
that
eventuates
from the diminutions of
Example
24. In
working
out
those
diminutions,
it is
helpful
of
course to
keep
a
running log
of
Example
25
as
it
develops,
to
be
sure
that each
dyad
is
used,
and used
only
once.
Now
that
we
have
assigned
a
dyad
to
each formal
point
of
Example
20,
we
automatically
know
the formal lines of
Example
21?in
particular
the
fourteen lines of that example not yet involved in the constructions of
Example
24.
t3 si
u
tT
pi
v
t3'
tl
pi
si' rl
si
s3 t3' tT
EXAMPLE
26
Example
26a
projects
lines
Nl,
Nlf,
and
Kl
of
Example
21 into
the
musical
texture
of
Examples
23a and
24a,
loosening
up
the
rhythm
and
"bowing"
a
bit.
Example
26b
imagines
a more
flexible
texture
than
any
so
far
presented;
in that
texture
it
projects
lines
J3,
G,
and
if
as
indicated.
The interested reader, taking hints from this example, will quickly dis
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Projective
Geometry
37
cover
many
other
textures
inwhich
to
project formal
lines
of the plane,
and
many
other
musical
resources
for
linking
the lines
together.
Many,
many
other "modes"
are
of
course
available for
assigning
dia
tonic
dyads
to
the formal
points
of
Example
20. The
choice of
our
"C
major"
mode
was
only
to
facilitate
hearing
for
the
first
such
mode
to
be
studied.
Within
a
composition,
one
could
"modulate"
between
different
such
modes,
particularly
if
they
have formal
lines
in
common,
with
which
to
"pivot."
Or
one
could
transpose
a
mode via
any
number of
semitones,
introducing
new
tones.
Example
24a,
using
a
ficta
F|
within
our
mode,
suggests
one
such
possibility.
Finally
one
can use
mathematical transfor
mations that
are
particularly
characteristic for
projective planes.
Part
V: Collineations
in the
Projective
Plane
It is
time
now
to
bring
such
transformations
into the
picture.
A
collinea
tion
is
a
function f that
permutes
the
points
of
a
projective plane
among
themselves in such fashion
that,
whenever
points
p,
q,
and r are
collinear,
so are
?(p),
?(q),
and
f(r).
Loosely
speaking,
a
collineation
is
an
operation
on
points
that
"preserves
lines."
If
point
p
varies
along
line
L,
then
f(L),
the
locus of the
points f(p),
will
itself be
a
line.
f(Z)
may
or
may
not
be
the
same
line
as
L.
Obviously,
collineations
are
particularly
idiomatic
sorts
of
transforma
tions
to
consider,
given
the
points
of
a
projective plane.
The
collineations
form
a
group
of
operations.13
Here is the basic theorem concerning collineations: letpl, p2, p3, and
p4
be
points,
no
three of which
are
collinear;
let
pi, p2',
p3',
and
p4'
also
be
such
a
quartet
of
points;
then there exists
a
collineation
f
such
that
f(pl) =pl',
f(p2)
=
pi, f(p3)
=
p3',
and
?(p4)
=
p4'.
In
this
context
the
p'
-points
may
all
be distinct from the
^-points,
or
various of
the
p'
-
points
may
be the
same as
various
of the
^-points;
the
theorem obtains
in
any
case.14
As
one
intuits from
the
theorem,
there
are a
"large
number" of
col
lineations
on a
given plane. To sharpen that intuition, letus examine col
lineations
on
the
seven-point plane.
For that
purpose
Example
27
essentially
reproduces
an
earlier
sche
matic for the
plane.
Points
1,
3,
and 5 of the
example
are
non-collinear;
we
can
take them
as
the
generic
"pl,
p2,
and
p3"
of
the
theorem.
We
are
also
to
consider
a
generic
"?>4"
not
lying
on
line
13,
or on
line
35,
or
on
line
51.
Point 7 is
the
only possible
such
p4,
for this
plane.
Given
points
pi,
pi,
p3',
and
p4'
as
stipulated,
let
us
find
a
collineation f
as
in the
theorem.
We
know that
any
such
f
must
satisfyf(l)
=
pl ', f(3)
=
pi, f(5)
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38
Perspectives
of
New
Music
A
seven-point plane:
123, 345,
and
561
are
all formal "lines" of the
geometry;
so are
174, 376, 572,
and 246
example
27
=
p3', f(7)
=
p4'. Subject
t