Vocal resonation

McKinney defines vocal resonance as "the process by which the basic product of phonation is enhanced in timbre and/or intensity by the air-filled cavities through which it passes on its way to the outside air."[1] Throughout the vocal literature, various terms related to resonation are used, including: amplification, enrichment, enlargement, improvement, intensification, and prolongation. Acoustic authorities would question many of these terms from a strictly scientific perspective. However, the main point to be drawn from these terms by a singer or speaker is that the result of resonation is to make a better sound.

Human resonating chambers

The voice, like all acoustic instruments such as the guitar, trumpet, piano, or violin, has its own special chambers for resonating the tone. Once the tone is produced by the vibrating vocal cords, it vibrates in and through the open resonating chambers, or the vocal tract, activating the four primary colors (resonances): chest, mouth, nasal (or "mask"), and head.

The various resonances can represent vocal colors in a continuous spectrum, from dark or chest resonance to bright or head/nasal resonance. We may call this spectrum a resonance track. In the lower range, the chest resonance or dark color predominates; in the middle range, the mouth-nasal resonance is dominant; in the higher range, the head-nasal resonance (bright color) predominates. The objective is to have command of all the colors of the spectrum, which allows greater scope of emotional expression. The emotional content of the lyric or phrase suggests the color and volume of the tone and is the personal choice of the artist.

There are some singers who are recognized by their pronounced nasal quality and others noted for a deep, dark and chesty sound and still others for their breathy or heady sound, and so on. In part, such individuality depends on the structure of the singer's vocal instrument, that is, the inherent shape and size of the vocal cords and of the vocal tract.

The quality or color of a voice also depends on the singer's ability to develop and use various resonances by controlling the shape and size of the chambers through which the sound flows. It has been demonstrated electrographically in the form of "voice-prints" that, like fingerprints, no two voices are exactly alike.[2]

Sympathetic and conductive resonance

In a technical sense resonance is a relationship that exists between two bodies vibrating at the same frequency or a multiple thereof. In other words, the vibrations emanating from one body cause the other body to start vibrating in tune with it. A resonator may be defined as a secondary vibrator which is set into motion by the main vibrator and which adds its own characteristics to the generated sound waves.[3]

There are two kinds of resonance: sympathetic resonance (or free resonance) and conductive resonance (or forced resonance)[4] The essential difference between both types is what causes the resonator to start vibrating. In sympathetic resonance there is no physical contact between the two bodies. The resonator starts functioning because it receives vibrations through the air and responds to them sympathetically. In conductive resonance the resonator starts vibrating because it is in physical contact with a vibrating body.[5]

Both types of resonance are at work in the human voice during speaking and singing. Much of the vibration felt by singers while singing is a result of conductive resonance. The waves originated by the airflow modulated by the vibrating vocal folds travel along the bones, cartilages, and muscles of the neck, head, and upper chest, causing them to vibrate by forced resonance. There is little evidence that these vibratory sensations make any significant contribution to the external sound.[6]

These same conductive vibrations, however, are good sensation guides for the singer, regardless of their effect on the external sound. These sensations provide evidence to the singer that his vocal folds are forming strong primary vibrations which are being carried from them to the head and chest. Thus these vibratory sensations can supply sensory feedback about the efficiency of the phonatory process to the singer.

In contrast, the sound a person hears listening to a singer is a product of sympathetic resonance. Vibrations created by the vocal cords travel through air from the larynx into the cavities of the throat and head, setting them into vibration. This is sympathetic resonance, without physical contact between these cavities and the vocal cords. The vocal resonator is not a sounding board, comparable with stringed instruments, but rather a column of air, with a shape that is not only complex, but highly variable. Vennard says:

Thus it may vibrate as a whole or in any of its parts. It should not be too hard to think of it as vibrating several ways at once. Indeed most vibrators do this, otherwise we would not have timbre, which consists of several frequencies of different intensities sounding together. Air is fully as capable of this as any other medium; indeed, the sounds of many diverse instruments are carried to the ear by the same air, are funnelled into the same tiny channel, and can still be heard as one sound or as sounds from the individual sources, depending upon the manner in which we give attention.[5]

Factors affecting resonators

There are a number of factors which determine the resonance characteristics of a resonator. Included among them are the following: size, shape, type of opening, composition and thickness of the walls, surface, and combined resonators. The quality of a sound can be appreciably changed by rather small variations in these conditioning factors.[6]

In general, the larger a resonator is, the lower the frequency it will respond to; the greater the volume of air, the lower its pitch. But the pitch also will be affected by the shape of resonator and by the size of opening and amount of lip or neck the resonator has.[3]

A conical shaped resonator, such as a megaphone, tends to amplify all pitches indiscriminately. A cylindrical shaped resonator is affected primarily by the length of the tube through which the sound wave travels. A spherical resonator will be affected by the amount of opening it has and by whether or not that opening has a lip.[6]

Three factors relating to the walls of a resonator will affect how it functions: the material it is made of, the thickness of its walls, and the type of surface it has. The resonance characteristics of a musical instrument obviously will vary with different materials and the amount of material used will have some effect.[3]

Of special importance to singing is the relationship of the surface of a resonator to its tonal characteristics. Resonators can be highly selective-meaning that they will respond to only one frequency (or multiples of it)-or they can be universal-meaning that they can respond to a broad range of frequencies. In general, the harder the surface of the resonator, the more selective it will be, and the softer the surface, the more universal it will become. "[A] hard resonator will respond only when the vibrator contains an overtone that is exactly in tune with the resonator, while a soft resonator permits a wide range of fundamentals to pass through un-dampened but adds its own frequency as on overtone, harmonic or inharmonic as the case may be."[5]

Hardness carried to the extreme will result in a penetrating tone with a few very strong high partials. Softness carried to the extreme will result in a mushy, non-directional tone of little character. Between these two extremes lies a whole gamut of tonal possibilities.[3]

The final factor to be mentioned is the effect of joining two or more resonators together. In general the effect of joining two or more resonators is that the resonant frequency of each is lowered in different proportions according to their capacities, their orifices, and so forth. The rules governing combined resonators apply to the human voice, for the throat and mouth and sometimes the nose function in this manner.[3]

The vocal resonators in detail

Chest anatomy

There are seven areas that may be listed as possible vocal resonators. In sequence from the lowest within the body to the highest, these areas are the chest, the tracheal tree, the larynx itself, the pharynx, the oral cavity, the nasal cavity, and the sinuses.[6]

The chest

The chest is not an effective resonator. Although strong vibratory sensations may be experienced in the upper chest, and although numerous voice books refer to chest resonance, the chest, by virtue of its structure and location, can make no significant contribution to the resonance system of the voice. The chest is on the wrong side of the vocal folds and there is nothing in the anatomy of the lungs that could serve to reflect sound waves back toward the larynx.[3]

The tracheal tree

throat diagram

The tracheal tree makes no significant contribution to the resonance system except for a negative effect around its resonant frequency. The trachea and the bronchial tubes combine to form an inverted Y-shaped structure known as the tracheal tree. It lies just below the larynx, and, unlike the interior of the lungs, has a definite tubular shape and comparatively hard surfaces. The response of the tracheal tree is the same for all pitches except for its own resonant frequency. When this resonant frequency is reached, the response of the subglottic tube is to act as an acoustical impedance or interference which tends to upset the phonatory function of the larynx. Research has placed the resonant frequency of the subglottal system or tracheal tree around the E-flat above "middle C" for both men and women, varying somewhat with the size of the individual.[7]

The larynx

Due to its small size, the larynx acts as a resonator only for high frequencies. Research indicates that one of the desirable attributes of good vocal tone is a prominent overtone lying between 2800 and 3200 hertz, with male voices nearer the lower limit and female voices nearer the upper. This attribute is identified as brilliance, or more frequently as ring or the singer's formant. There are several areas in or adjacent to the larynx which might resonate such a high pitch. Among them are the collar of the larynx, the ventricles of Morgani, the vallecula, and the pyriform sinuses. The larynx is not under conscious control, but whatever produces "ring" can be encouraged indirectly by awareness on the part of the student and the teacher of the sounds which contain it.

The pharynx

The pharynx is the most important resonator by virtue of its position, size, and degree of adjustability. It is the first cavity of any size through which the product of the laryngeal vibrator passes; the other supraglottal cavities have to accept whatever the pharynx passes on to them. Greene states:

"The supraglottic resonators being in the main muscular and moveable structures must be voluntarily controlled to produce conditions of optimal resonance either by varying degrees of tension in their walls, or by alterations in the size of their orifices and cavities during the articulatory movements."

The oral cavity

The oral cavity is the second most effective resonator.

The nasal cavity

The nasal cavity is the third most effective resonator.

References

  1. ↑ McKinney, James (1994) The Diagnosis and Correction of Vocal Faults, Nashville, TN: Genovex Music Group.
  2. ↑ Austin, Howard (2007). Born To Sing (6th ed.). Music World. ISBN 0-9727194-9-0.
  3. 1 2 3 4 5 6 McKinney, James C. (1994). The Diagnosis and Correction of Vocal Faults. Nashville, Tennessee: Genovex Music Group. ISBN 978-1-56593-940-0. LCCN 97209575.
  4. ↑ McCoy, Scott (2004) Your Voice: An Inside View. Princeton, NJ: Inside View Press.
  5. 1 2 3 Vennard, William (1967). Singing: the Mechanism and the Technic (4th ed.). New York: Carl Fischer. ISBN 978-0-8258-0055-9. OCLC 1011087.
  6. 1 2 3 4 Greene, Margaret Cicely Langton; Lesley Mathieson (2001). The Voice and its Disorders (6th ed.). London; Philadelphia: Whurr; John Wiley & Sons. ISBN 978-1-86156-196-1.
  7. ↑ Van den Berg, J.W. (December 1963). "Vocal Ligaments versus Registers". The NATS Bulletin. 19: 18.

Further reading

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