Orchestration (cont.)

Mixing the Woodwind instruments

 

The sole function of the ryûteki and hichiriki is to present the melody, the most important element of the music. The two instruments typically voiced in octave, play in heterophony. On the other hand, the sole function of the shô is to provide the harmonic support, a function it fulfills in combination with the two string instruments. The lowest note of the shô’s aitake is considered to be its melodic tone.  Figure 2 shows the correspondence between the written pitches of the three-woodwind instruments. It demonstrates that for the most part, the shô’s aitakes fill up the octave space between the hichiriki and the ryûteki.

 

 

Correspondence between the pitches of the three-woodwind instruments

Figure 2

 

Although the ryûteki and hichiriki are united in their function and voiced in octave that is filled up with a harmonic structure, they do not fuse into a single sonority. In fact, the sound of the three-woodwind instruments usually creates a stratified texture where each instrument is clearly distinguishable. Moreover, the overall dynamics of the woodwind instrument is invariably loud contributing to create an overall monochromatic color, suggesting that the beauty of kangen music may lie beyond its overall sonority. Sections 1 and 2 aim at explaining why the sound of the three-woodwind instruments do not non-blend and why their dynamics is constantly loud.

 

1. Sound fusion

Our ability to hear separate parts is increased when instruments are not rhythmically synchronized, hence the traditional presentation of the melody by the ryûteki and hichiriki in heterophony diminishes their blending potential. Moreover, an examination of the acoustical properties of the three-woodwind instruments suggests
 that an important reason for their non-blending quality is 
intrinsic to the instruments themselves.

Indeed, fusion is facilitated when the sound of the instruments to be mixed is homogeneous, but already the three different types of embouchure of the woodwind instruments work against sonic fusion. Also the characteristically constant microtonal transformations of the hichiriki’s sound prevent any possible fusion, as demonstrated with Figure 3.  The spectra of the hichiriki (in blue) and ryûteki (in red) playing ff a D5 and D6, respectively, have been analyzed over a time-lap of about 2.5 seconds. The larger peaks of the hichiriki indicate that its sound fluctuates substantially during this time-lap. It also explains why the peaks of the two instruments do not align well in spite of the fact that they are in octave. Hence, Figure 3 shows that the acoustical properties of the two instruments do not favor their fusion since two tones blend better when more of their partials coincide.

FocusHicD5RyuD6.jpg

Spectra of the hichiriki (in blue) and ryûteki (in red) playing ff a D5 and D6, respectively.

Figure 3

2. Dynamics

The overall steady loud dynamics of the woodwind instruments is the outcome of a domino effect between the three instruments. The explanation of this sequence of events is divided up into three steps. It starts with an investigation of the effect of dynamics on the spectral envelope.

Step 1: The effect of dynamics on the Japanese woodwind instruments is different from their Western counterparts. Typically, the effect of dynamics on Western instruments is twofold involving a change of volume and a displacement on the frequency scale of the sound’s main energy. For instance, a decrescendo is characterized by a reduction in volume and a switch of energy towards the lower partials, as illustrated with the spectra on the left hand-side of Figure 4, which represents the sound of the clarinet playing a D5, ff (in blue), mf  (in red), and pp (in green), respectively.  On the other hand, the spectra on the right hand-side of Figure 4 are the shô’s also playing a D5 at the same three dynamics. While the reduction in volume is noticeable when comparing its spectra from the ff (in blue) to pp (in green), the energy displacement towards the lower partials is much less accentuated, it appears rather that the spectral envelop keeps more or less its shape and that the change of volume is proportionally spread over the entire envelop. Consequently, the transformation of the shô’s sound over a change of dynamics is much more discrete, hence less perceptible.

 

Cla-D5-Dynamics.jpg

Sho-D5-Dynamics.jpg

Change of the clarinet’s spectral envelop as it plays a D5, ff, mf, pp, respectively.

Change of the shô’s spectral envelop as it plays a D5, ff, mf, pp, respectively.

Figure 4

 

Figure 5 shows the transformation of the spectral envelops over the same three dynamics for the ryûteki and hichiriki playing a D6 and D5, respectively. It demonstrates the ryûteki’s response to a dynamic change is similar to the shô’s but that the hichiriki’s is comparable to the clarinet’s response. The importance of this acoustical phenomenon will be further commented on in Step #3.

 

Ryu-D6-Dynamics.jpg

Hic-D5-Dynamics.jpg

Change of the ryûteki’s spectral envelop as it plays a D6, ff, mf, pp, respectively.

Change of the hichiriki’s spectral envelop as it plays a D5, ff, mf, pp, respectively.

Figure 5

 

Step 2:  Because the hichiriki and ryûteki work together to present the melody, it is important to look at how dynamics affect their combined sounds. Figure 6 shows the spectra of the hichiriki (in blue) and ryûteki (in red) playing ff a D5 and D6, respectively. The last spectrum shows the combined two sounds and it reveals that the ryûteki must matched the hichiriki’s dynamics to avoid being masked.

 

HicD5RyuD6.jpg

Spectra of the hichiriki (in blue) and ryûteki (in red) playing ff a D5 and D6 respectively, and their combination.

Figure 6

 

Step 3: Figure 7 shows the spectra of the hichiriki (in blue) and ryûteki (in green) playing respectively a written D4 and D5, and the shô (in red) playing its aitake hô, which is based on D5: pp on the left-hand side and ff on the right-hand side. It also shows the combination of the three sounds. The importance of the phenomenon described under Step #1 comes to bear when comparing the pp and ff sounds of the hichiriki (in blue) with the shô (in red).

This comparison suggests that a move from ff to pp has a much stronger effect on the sound of the hichiriki than on the sound of the shô, to the point that the former could potentially be masked by the latter as they move towards a softer dynamics. Hence, to avoid being masked by the shô, the hichiriki must keep its dynamics on the loud side, and as explained in Step #2, the ryûteki must matched the hichiriki dynamic level to avoid being masked by it.

 

  3Inst2Dynamics.jpg

 

WWMix-pp.jpg

WWMix-ff.jpg

Spectra of the hichiriki (in blue),

shô (in red) and ryûteki (in green)

and their combination,

playing the written pitches pp

Spectra of the hichiriki (in blue),

shô (in red) and ryûteki (in green)

and their combination,

playing the written pitches ff

Figure 7

3. The beauty of kangen music

Although the overall steady loud dynamic of kangen music is obvious, it would be a mistake to conclude that this music has no dynamic shape. As a matter of fact, the transformation of dynamics in kangen music has a direct impact on the sophisticated and refined timbral shifts of the music. Typically, the shô’s part moves in waves of crescendo and decrescendo. The sound of the shô is not much sensitive to dynamic changes, so these dynamic-waves are in fact produced by the addition and subtraction of pitches, called te-utsuri (see the chapter: Woodwinds/Sho). Based on the phenomenon described in Step #3, we can predict that this pitch expansion and contraction will influence the overall timbre. We can indeed expect the sound of the hichiriki to come forward as the number of pitches of the shô decreases, and to slightly fade away as the number of pitches increases. This timbral transformation is clearly perceptible on the next sound example from Sandaien IchiguJo-Section A performed by the ensemble Reigakusha.

 

Sound example: Sandaien IchiguJo-Section A – (no score)

 

These intricate dynamics/timbral waves are clearly audible because of the stratified sound of the woodwind instruments that facilitates the perception of such minute timbral changes, but also because they coincide with the phrase structure. Theoretically, the Japanese melody divides the phrase structure into two symmetric parts. The first half of the phrase is characterized by melodic motion that is primarily conjunct, wave-like, and contained within the range of an octave. Moreover, the speed is essentially slow since the rhythmic subdivision of the melodies rarely goes beyond the eight-notes, with a metronome marking usually under quater-note = 54. Typically, this melody is then followed by a sustained-tone beginning at the phrase’s half-point, in phase with the meeting point of the three percussion instruments.  Example 2 shows the melody of the first phrase of Etenraku’s Section A.  In measures 1-2 the melodic motion of the ryûteki and hichiriki represents the foreground, while the shô’s two aitakes are background material, conversely to measures 3-4 where the single aitake as the woodwind instruments’ sustained-tone moves to the background. Note that sustained-tones in kangen music also have foreground quality since they are always ornamented has shown in Example 2 with the D acting as lower-neighbor tone to the E. This example is an excerpt from a recording by the ensemble Reigakusha.

 

 

Etenraku: Simplified version of the 1st phrase of Section A (measure 9-12), Woodwind and Percussion instruments only

Example 2