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Page 1
Voir dans le PDF(s’ouvre dans une nouvelle fenêtre)and the lambdoma diagram
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Page 2
Voir dans le PDF(s’ouvre dans une nouvelle fenêtre)Author(s): Barbara Hero
Source: Leonardo, Vol. 11, No. 4 (Autumn, 1978), pp. 301-303
Published by: The MIT Press
Stable URL: http://www.jstor.org/stable/1573956
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Page 3
Voir dans le PDF(s’ouvre dans une nouvelle fenêtre)Leonardo,Vol. 11, pp. 301-303.
c PergamonPressLtd. 1978. Printedin GreatBritain.
1001-0301$02.00/0
DRAWINGS BASED ON LASER LISSAJOUS
FIGURES AND THE LAMBDOMA DIAGRAM
Barbara Hero*
1.
recorded inputs. Two outputs from the amplifier,
corresponding to X and Y, drive two galvanometers for
laser scanning[3] (General Scanning, Watertown, Mass.).
One, rotating on a vertical axis, carries a mirror 7 x 7 mm;
the other, rotating on a horizontal axis, carries a mirror
7 x 11 mm. The mirrors oscillate to the beats of the
different frequencies received. The helium-neon laser
beam impinges on one mirror, is reflected to the next and
is finally reflected to a wall or a projection screen.
The power of a laser (0.5 mW) is sufficient to produce a
satisfactory image on a wall at a distance of 3-4.5 m. I
calibrate the system so that the Lissajous figures can be
analyzed, although I do not attempt to do so myself.
In an earlier article in Leonardo, I described some
nonfigurative paintings that I made whose patterns and
colors were related in arbitrary ways to relative pitch in
music [1]. A more extensive discussion of my work
relating visual art and music is given in my book,
Eyes + Ears = Ideas[2]. The starting point for the pictorial
compositions is the Lambdoma or Pythagorian diagram,
which dates back to Ancient Greece.
For recent works I use the following procedure: I select
a number of tones with the aid of the Lambdoma
diagram, produce the tones electronically and make
sketches of their Lissajous figures, which are produced by
means of a helium-neon laser scanner device and
projected onto a wall or screen. Finally, I make a drawing
based on the Lissajous figures with colors chosen
according to an arbitrary code that identifies colors with
3.
My aim is to produce Lissajous figures that are
aesthetically pleasing as well as meaningful. It is desirable
to minimize dissonances to obtain well delineated designs.
The absence of dissonance is assured when only
frequencies of the harmonic series are employed. The
numerical values of the frequencies of the harmonic series
are obtained by multiplying the frequency of the
fundamental tone (which I have chosen to be 352 Hz) by
the integers 1-16 and by dividing each of the products by
the integers 1-16. This calculation, which is realistically
restricted to integral multipliers and divisors below 17 to
provide frequencies covering eight octaves and which
roughly includes the frequency range of present-day
pianos, follows the plan of the Lambdoma diagram [1].
The results of the calculation can be tabulated conveniently as an array of 256 numbers (Fig. 1). The
notation for the harmonic series is shown below the array.
Figure 1 shows the tone notations corresponding to
each of the frequencies in the array. To determine the
frequency of a tone, one must read its coordinates x and y;
then multiply 352 by x and divide the result by y. For
example for g, read x = 4 and y = 7. The frequency is then
calculated to be 201 Hz. In Fig. 1, each of the 16
horizontal rows represents one overtone of the harmonic
series and each of the 16 vertical columns represents one
undertoneof the series. For convenience the first of the
harmonic series begins with the fundamental f1l (44) and
is followed by f, (88), an octave above it, then by the fifth c
(132), the third octave f (176), the third a (220), another
fifth c1 (264), the seventh e b (308), the octave fl (352),
g1 (396), a1 (440), bl (484), c11 (528), d11 (572), e bl1
(616), e11 (660) and f11 (704). The undertone series can be
traced in the same way downwards for four octaves,
starting at f1 (352) or f11 (704) up to f" (5632).
When a pure sine-wave tone is mixed with another, a
sum and a difference are produced. For example, if fl (352
Hz) is combined with its third harmonic cT1 (1056 Hz),
frequencies.
2.
A tone of a specific frequency is produced by an
electronic sine-wave oscillator (Eico 379 solid state
sine/square wave generator, Eico Electronic Instrument
Co, Brooklyn, N.Y.). Sinusoidal wave forms may be
produced in a frequency range from 20 Hz to 2m Hz, but I
do not exceed 1200 Hz. It is essential in my work that
tones have wave forms with a minimum of overtones of
the harmonic series. Therefore sinusoidal wave forms are
preferred to square and triangular ones.
I record the frequencies of the harmonic tones from the
Lambdoma diagram (Fig. 1), one of which is a fundamental, separately on each of two channels of a magnetic tape.
Later, using a second tape recorder, I make mixtures of
these tones, which I record on one channel of a magnetic
tape and different mixtures of tones on the second
channel. These two channels are used as input to the
scanners that produce the Lissajous figures [3,4].
The production of Lissajous figures in response to
music by means of a helium-neon laser beam scanner for
projection on a screen has been described in Leonardoby
Wagler [5]. He reported on the use of a Sonavision
projector manufactured by Sonavision, Ann Arbor,
Michigan. I employ a Metrologic laser (model ML-600,
0.5 mw, Metrologic Instruments, Bellmaur, N.J.).
The tape-recorded tones on two channels, called X and
Y are used as an input to an amplifier (Studio Standard
CA-2100, Fisher, Long Island City, N.J.) having four
outputs, two of which are speakers, enabling one to hear
as well as to see simultaneously the sum of the two tape*Artist, 48 LawrenceStrret, Boston, MA 02116, U.S.A.
(Received 19 Nov. 1977.)
Page 4
Voir dans le PDF(s’ouvre dans une nouvelle fenêtre)Barbara Hero
(O V ER TONES)
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an assumedfundamenta f (352
Fig. 1. Musical tones within8 octaves (4 octaves below and 4 octaves above
in the Lambdomadiagram.
sound
frequencies
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arranged
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the summation tone f1 1 (1408) and the differential tone
fl 1 (704) are produced. If one uses only the frequencies
that fall in the range of the harmonic series (Fig. 1), the
most clearly defined Lissajous figures seem to be
produced. The sums and differences of the harmonic
1
series are reinforced. This can be seen in Fig. 1 where fl
(1408) is found at x= 8, y=2 and fl1 (704) at x= 8, y=4.
That the changes in shapes of the figures are due to the
beats of the tones, indicating that beats are an acoustical
rather than a psychological phenomenon [6], should be
investigated further.
Most present-day synthesizers employ equal temperament, the division of the octave into 12 equal parts (semitones). The natural harmonic series (just intonation) is
based on pure overtones-that
is, if u is the frequency of a
tone, then 2u is the octave (first overtone), 3/2 u is the
interval of the fifth and 5/4 u is the interval of the major
third, none of which (except for the octave) corresponds
precisely to their equivalents in the equal temperament
system. The Pythagorean tones within an octave could
number as few as nine tones or as many as one could
conceive in a microtonal context, depending on how far
the table is enlarged beyond the audible 16 overtones and
undertones.
4.
Lissajous figures are made up of continuous closed
paths. The closed paths are produced when any two
frequencies are frequencies of the harmonic series. When
two sounds are almost the same frequency, the pattern is
elliptical. (Two tones of the same frequency produce a
closed circle.) The slope of the major axis of the ellipse is
related to the phase shift between the two tones. The two
tones fl and fP1, an octave apart, produce a figure-eight
pattern.
A high frequency tone combined with one of a lower
octave produces a multiplicity of lines in the figure-eight
Page 5
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Fig 3. Four tone patterns based on the location in the array (Fig.
4) of (1) thefirst harmonicand the second harmonic;(2) the third
harmonic; (3) the fifth harmonic and (4) the seventh harmonic.
overtones fl 1, fl 1, fl and f and its undertones f, f1, f1
and f 11. The resulting pattern of black squares I then use
to generate a drawing consisting of four quadrants in
which quadrant I of the drawing is the mirror image of the
tone pattern shown in Fig. 3 (bottom right). Then the
drawing is completed by producing in quadrants II and
III the mirror image of the quadrant pair I and IV. One
can make drawings in a similar way using the other three
tone patterns in Fig. 3.
If the Lambdoma diagram in Fig. 1 were continued
beyond the 16th harmonic series to higher and lower
frequencies, it would be found that the black square
patterns would be repeated. This repetition can be
detected in the picture reproduced in Fig. 5 (cf. color
plate), where I show the diagram extended to the 177th
overtone and the 90th undertone of the harmonic series.
The colors employed correspond to an arbitrary color
code that I established for certain tones [1].
References
pattern resembling a projection of the Mobius strip. A
fifth combined with a fundamental tone can produce
crown-like patterns. A low, barely audible tone, around
20 Hz, coupled with a harmonic tone produces welldefined figures.
The Lissajous figures serve me as a source of
inspiration. Figure 2 shows a drawing containing shapes
based on Lissajous figures and tone patterns, with bands
of colored squares, suggesting the Lambdoma array.
Four patterns are shown in Fig. 3; these are derived
from the array shown in Fig. 1, as indicated in Fig. 4. The
pattern for the first harmonic (Fig. 3, bottom right), for
example, was obtained as follows: I blackened all the
squares in Fig. 1 occupied by the fundamental fl and its
1. B. Hero, Paintings Based on Relative Pitch in Music,
Leonardo 8, 13 (1975).
2. B. Hero, Eyes+ Ears= Ideas (New York: Franklin Furnace,
1975).
3. P. G. Brosens and E. Grenda, Applications of
Galvanometers to Laser Scanning, paper presented at the
18th Ann. Tech. Mtg. of the Soc. of Photo-Optical
Instrumentation Engrs., San Diego, Calif., Aug. 1974.
4. G. Trythall, Principlesand Practice of ElectronicMusic (New
York: Grosset & Dunlap, 1973).
5. S. R. Wagler, Sonavision: A Visual Display of Sound,
Leonardo 3, 443 (1970). Also in Kinetic Art: Theory and
Practice, F. J. Malina, ed. (New York: Dover, 1974) p. 162.
6. W. Apel, Harvard Dictionary of Music, 2nd rev. ed.
(Cambridge, Mass.: Harvard Univ. Press, 1969).
Page 6
Voir dans le PDF(s’ouvre dans une nouvelle fenêtre)Top left: Barbara Hero. Untitled,felt pen on canvas, 90 x 140 cm, 1975. (Fig. 5, cf. page 303)
Top right: Naomi Boretz. 'Basedon Yellow',watercoloron paper, celluloseacetatefilm, 42.5 x 54.0 cm, 1973.
(Fig. 3, cf. page 294)
Center left: P. P. Konchalovsky.'Portraitof a Fiddler',oil on canvas, 143 x 105cm, 1918. (Fig. 6, cf. page 321)
Center right: Michele Andal. Untitled, black ink and acrylic paint on paper, 91 x 56 cm, 1977. (Fig. 8, cf.
page 272)
Bottom left: Tom Kelly. 'Marilyn Monroe', color photograph. (Copyright C Tom Kelly, 1978) (Fig. 6, cf.
page 316)
Bottom right: Anait A. Stephens. 'Eye', cylindrical white-light transmissionhologram (120?), dia. 40 cm,
height 26 cm, 1975. (Fig. 2, cf. page 306)
[facing page 292]