Tonewood refers to specific wood varieties used for woodwind or acoustic stringed instruments. The word implies that certain species exhibit qualities that enhance acoustic properties of the instruments, but other properties of the wood such as esthetics and availability have always been considered in the selection of wood for musical instruments. According to Mottola's Cyclopedic Dictionary of Lutherie Terms, tonewood is:

Wood that is used to make stringed musical instruments. The term is often used to indicate wood species that are suitable for stringed musical instruments and, by exclusion, those that are not. But the list of species generally considered to be tonewoods changes constantly and has changed constantly throughout history.^[1]

Varieties of tonewood

As a rough generalization it can be said that stiff-but-light softwoods (i.e. from coniferous trees) are favored for the soundboards or soundboard-like surface that transmits the vibrations of the strings to the ambient air. Hardwoods (i.e. from deciduous trees) are favored for the body or framing element of an instrument. Woods used for woodwind instruments include African blackwood, (Dalbergia melanoxylon), also known as grenadilla, used in modern clarinets and oboes. Bassoons are usually made of Maple, especially Norway maple (Acer platanoides). Wooden flutes, recorders, and baroque and classical period instruments may be made of various hardwoods, such as pear (Pyrus species), boxwood (Buxus species), or ebony (Diospyros species).

Mechanical properties of tonewoods

Some of the mechanical properties of common tonewoods, sorted by density. See also Physical properties of wood.

Carbon-fiber/Epoxy, glass, aluminum, and steel added for comparison, since they are sometimes used in musical instruments.

Density is measured at 12% moisture content of the wood, i.e. air at 70 °F and 65% relative humidity.^[8] Most professional luthiers will build at 8% moisture content (45% relative humidity), and such wood would weigh less on average than that reported here, since it contains less water.

Data comes from the Wood Database,^[9] except for 𝜈_LR, Poisson's ratio, which comes from the Forest Product Laboratory, United States Forest Service, United States Department of Agriculture.^[10] The ratio displayed here is for deformation along the radial axis caused by stress along the longitudinal axis.

The shrink volume percent shown here is the amount of shrinkage in all three dimensions as the wood goes from green to oven-dry. This can be used as a relative indicator of how much the dry wood will change as humidity changes, sometimes referred to as the instrument's "stability". However, the stability of tuning is primarily due to the length-wise shrinkage of the neck, which is typically only about 0.1% to 0.2% green to dry.^[11] The volume shrinkage is mostly due to the radial and tangential shrinkage. In the case of a neck (quarter-sawn), the radial shrinkage affects the thickness of the neck, and the tangential shrinkage affects the width of the neck. Given the dimensions involved, this shrinkage should be practically unnoticeable. The shrinkage of the length of the neck, as a percent, is quite a bit less, but given the dimension, it is enough to affect the pitch of the strings.

The sound radiation coefficient is defined^[12] as:

${\displaystyle R={\sqrt {\cfrac {E}{{\rho }^{3}}}}}$

where ${\displaystyle E}$ is flexural modulus in Pascals (i.e. the number in the table multiplied by 10⁹), and ρ is the density in kg/m³, as in the table.

From this, it can be seen that the loudness of the top of a stringed instrument increases with stiffness, and decreases with density. The loudest wood tops, such as Sitka Spruce, are lightweight and stiff, while maintaining the necessary strength. Denser woods, for example Hard Maple, often used for necks, are stronger but not as loud (R = 6 vs. 12).

When wood is used as the top of an acoustic instrument, it can be described using plate theory and plate vibrations. The flexural rigidity of an isotropic plate is:

${\displaystyle D={\cfrac {EH^{3}}{12(1-\nu ^{2})}}}$

where ${\displaystyle E}$ is flexural modulus for the material, ${\displaystyle H}$ is the plate thickness, and ${\displaystyle \nu }$ is Poisson's ratio for the material. Plate rigidity has units of Pascal·m³ (equivalent to N·m), since it refers to the moment per unit length per unit of curvature, and not the total moment. Of course, wood is not isotropic, it's orthotropic, so this equation describes the rigidity in one orientation. For example, if we use 𝜈LR, then we get the rigidity when bending on the longitudinal axis (with the grain), as would be usual for an instrument's top. This is typically 10 to 20 times the cross-grain rigidity for most species.

The value for ${\displaystyle D}$ shown in the table was calculated using this formula and a thickness ${\displaystyle H}$ of 3.0mm=0.118″, or a little less than 1/8".

When wood is used as the neck of an instrument, it can be described using beam theory. Flexural rigidity of a beam (defined as ${\displaystyle EI}$) varies along the length as a function of x shown in the following equation:

${\displaystyle \ EI{dy \over dx}\ =\int _{0}^{x}M(x)dx+C_{1}}$

where ${\displaystyle E}$ is the flexural modulus for the material, ${\displaystyle I}$ is the second moment of area (in m⁴), ${\displaystyle y}$ is the transverse displacement of the beam at x, and ${\displaystyle M(x)}$ is the bending moment at x. Beam flexural rigidity has units of Pascal·m⁴ (equivalent to N·m²).

The amount of deflection at the end of a cantilevered beam is:

${\displaystyle w_{C}={\tfrac {PL^{3}}{3EI}}}$

where ${\displaystyle P}$ is the point load at the end, and ${\displaystyle L}$ is the length. So deflection is inversely proportional to ${\displaystyle EI}$. Given two necks of the same shape and dimensions, ${\displaystyle I}$ becomes a constant, and deflection becomes inversely proportional to ${\displaystyle E}$—in short, the higher this number for a given wood species, the less a neck will deflect under a given force (i.e. from the strings).

Read more about mechanical properties in Wood for Guitars.^[13]

Selection of tonewoods

In addition to perceived differences in acoustic properties, a luthier may use a tonewood because of:

• Availability
• Stability
• Cosmetic properties such as the color or grain of the wood
• Tradition
• Size (Some instruments require large pieces of suitable wood)

Sources

Many tonewoods come from sustainable sources through specialist dealers. Spruce, for example, is very common, but large pieces with even grain represent a small proportion of total supply and can be expensive. Some tonewoods are particularly hard to find on the open market, and small-scale instrument makers often turn to reclamation,^[14][15] for instance from disused salmon traps in Alaska, various old construction in the U.S Pacific Northwest, from trees that have blown down, or from specially permitted removals in conservation areas where logging is not generally permitted.^[16] Mass market instrument manufacturers have started using Asian and African woods, such as Bubinga (Guibourtia species) and Wenge (Millettia laurentii), as inexpensive alternatives to traditional tonewoods.

The Fiemme Valley, in the Alps of Northern Italy, has long served as a source of high-quality spruce for musical instruments,^[17] dating from the violins of Antonio Stradivari to the piano soundboards of the contemporary maker Fazioli.

Preparation

Tonewood choices vary greatly among different instrument types. Guitar makers generally favor quartersawn wood because it provides added stiffness and dimensional stability. Soft woods, like spruce, may be split rather than sawn into boards so the board surface follows the grain as much as possible, thus limiting run-out.

For most applications, wood must be dried before use, either in air or kilns.^[18] Some luthiers prefer further seasoning for several years. Wood for instruments is typically used at 8% moisture content (which is in equilibrium with air at 45% relative humidity). This is drier than usually produced by kilns, which is 12% moisture content (65% relative humidity). If an instrument is kept at a humidity that is significantly lower than that at which it was built, it may crack. Therefore, valuable instruments must be contained in controlled environments to prevent cracking, especially cracking of the top.

Some guitar manufacturers subject the wood to rarefaction, which mimics the natural aging process of tonewoods. Torrefaction is also used for this purpose, but it often changes the cosmetic properties of the wood. Guitar builders using torrefied sound boards claim improved tone, similar to that of an aged instrument. Softwoods such as Spruce, Cedar, and Redwood, which are commonly used for guitar sound boards, are easier to torrefy than hardwoods, such as Maple.

On inexpensive guitars, it is increasingly common to use a product called "Roseacer" for the fretboard, which mimics Rosewood, but is actually a thermally-modified Maple.

"Roasted" Maple necks are increasingly popular as manufacturers claim increased stiffness and stability in changing conditions (heat and humidity). However, while engineering tests of the ThermoWood method indicated increased resistance to humidity, they also showed a significant reduction in strength (ultimate breaking point), while stiffness (flexural modulus) remained the same or was slightly reduced.^[19][20] Although the reduction in strength can be controlled by reducing the temperature of the process, the manufacturer recommends not using its product for structural purposes. However, it is perhaps possible to compensate for this loss of strength in guitars by using carbon-fiber stiffeners in necks and increased bracing in tops.

References

External links

• Commercial article on woods used for woodwind instruments
• Guitarbench's database of tonewood species
• Alan Arnold Interactive Tonewood guide
• The Heretics Guide to Tonewoods
• More about Guitar Wood
• Tonewoods for guitars
• Taylor acoustic guitar woods