Musical Mathematics
on the art and science
of acoustic instruments
Order now and save 33% at Amazon.com
Also available from the publisher at Chronicle Books, San Francisco.
All rights reserved.
www.chrysalis-foundation.org
CHAPTER 12: ORIGINAL INSTRUMENTS
Section 12.12
The
Diamond Marimba in Plate 7 is based on a 13-limit tonality diamond.
Max F. Meyer (1873–1967) first described the concept of a two-dimensional tonality diamond in
his book The Musician’s Arithmetic, published in 1929.
On p. 22, Meyer shows the diagram of a 7-limit Tonality Diamond that includes 16 just
intoned frequency ratios. (See Chapter 10, Figure 57.) In 1946, Harry Partch (1901–1974) transformed and expanded
Meyer’s original design and built an 11-limit Diamond Marimba with 36 just intoned bars. (See Chapter 10, Figure 59.)
With respect to my Diamond Marimba, Figure 12.5 shows the 49 bars required by a 13-limit
tonality diamond. Here the frequency ratios of the
diagonals that ascend from left to right include odd numbers 1, 5, 3, 7, 9, 11, 13 — or
“octave-multiples” of these numbers — in the numerators; conversely, the frequency ratios of the diagonals that
descend from left to right include odd numbers 1, 5, 3, 7, 9, 11, 13 — or “octave-multiples” of
these numbers — in the denominators. A careful examination of
Meyer’s 7-limit, Partch’s 11-limit, and my 13-limit diamond reveals that the row
that runs through
the center of these designs represents a sequence of unisons.
For this reason, I refer to the center row as the
neutral axis. On the 11-limit and 13-limit Diamond
Marimbas, the neutral axis sounds the tone of the tonic, ratio 1/1, below all the bars in the
upper
halves of the diamonds. Furthermore, on the 13-limit Diamond Marimba, the neutral
axis produces the tone of the “octave,” ratio 2/1, above the following 15 bars in the
lower
half of the diamond: 14/13, 12/11,
10/9, 8/7, 14/11, 4/3 (12/9), 18/13, 10/7, 14/9, 8/5, 18/11, 5/3, 22/13, 12/7. And it produces the tone of the “double-octave,” ratio 4/1,
above the following 6 bars in the lower
half of the
diamond: 16/13, 16/11, 20/13, 16/9, 20/11, 24/13.
Now, a
bar that sounds the fundamental frequency, ratio 1/1, below the lowest bar, or below the “sharp
minor third,” ratio 16/13, is
not a part of the diamond. Also, a bar that sounds the “octave,” ratio 2/1, between the
“sharp minor seventh,” ratio 24/13, and the “sharp minor second,” ratio 14/13, is not included. Consequently, I decided to append the basic structure of the
diamond design. In the lower part of the instrument,
Figure
12.5 illustrates that I added a bar for the fundamental G3 at 196.0 cps, and a bar for the
“octave” G4 at 392.0 cps. The neutral axis now produces
the interval of the “double-octave” G5 at 784.0 cps above the fundamental. Figure
12.5 shows that I also included three more bars that
produce the intervals of the “fourth,” ratio 4/3, the “fifth,” ratio 3/2, and the “sharp minor
sixth,” ratio 13/8, above the fundamental. Therefore,
the Diamond Marimba in Plate 7 has a total number of 49 bars + 5 bars = 54 bars.
The
Diamond Marimba stand consists of six parts: a lower
base, four poles, and an upper platform. The Honduras
rosewood bars are mounted on a terraced platform that consists of fourteen rows of bars. Beginning with the second row, each succeeding row rises a
half inch above the previous row, so that the difference in height between the first
row and the last
row equals 13 × 1/2
in. = 6 1/2 in. Underneath the platform, I mounted a
quarter-wavelength resonator for each bar. (See Chapter 7, Sections 10–11.) The resonators are made from cast acrylic tubes, and the stand poles, from cast
acrylic rods. In Plate 7, note that the profile of the
fundamental bar in the first row shows the triple-arch design used to tune the first
three modes of vibration.
(See Chapter 6, Sections 10–14.) For the others,
I tuned the first two modes of the bars in the 16/13–7/5
range, and only the first or fundamental mode of the bars
in the 13/9–13/8 range. (See Chapter 6, Section 15.)