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Tuning fork
Tuning fork
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Tuning fork by John Walker stamped with note (E) and frequency in hertz (659)

A tuning fork is an acoustic resonator in the form of a two-pronged fork with the prongs (tines) formed from a U-shaped bar of elastic metal (usually steel). It resonates at a specific constant pitch when set vibrating by striking it against a surface or with an object, and emits a pure musical tone once the high overtones fade out. A tuning fork's pitch depends on the length and mass of the two prongs. They are traditional sources of standard pitch for tuning musical instruments.

The tuning fork was invented in 1711 by British musician John Shore, sergeant trumpeter and lutenist to the royal court.[1]

Description

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Motion of an A-440 tuning fork (greatly exaggerated) vibrating in its principal mode

A tuning fork is a fork-shaped acoustic resonator used in many applications to produce a fixed tone. The main reason for using the fork shape is that, unlike many other types of resonators, it produces a very pure tone, with most of the vibrational energy at the fundamental frequency. The reason for this is that the frequency of the first overtone is about 52/22 = 25/4 = 6+14 times the fundamental (about 2+12 octaves above it).[2] By comparison, the first overtone of a vibrating string or metal bar is one octave above (twice) the fundamental, so when the string is plucked or the bar is struck, its vibrations tend to mix the fundamental and overtone frequencies. When the tuning fork is struck, little of the energy goes into the overtone modes; they also die out correspondingly faster, leaving a pure sine wave at the fundamental frequency. It is easier to tune other instruments with this pure tone.

Another reason for using the fork shape is that it can then be held at the base without damping the oscillation. That is because its principal mode of vibration is symmetric, with the two prongs always moving in opposite directions, so that at the base where the two prongs meet there is a node (point of no vibratory motion) which can therefore be handled without removing energy from the oscillation (damping). However, there is still a tiny motion induced in the handle in its longitudinal direction (thus at right angles to the oscillation of the prongs) which can be made audible using any sort of sound board. Thus by pressing the tuning fork's base against a sound board such as a wooden box, table top, or bridge of a musical instrument, this small motion, but which is at a high acoustic pressure (thus a very high acoustic impedance), is partly converted into audible sound in air which involves a much greater motion (particle velocity) at a relatively low pressure (thus low acoustic impedance).[3] The pitch of a tuning fork can also be heard directly through bone conduction, by pressing the tuning fork against the bone just behind the ear, or even by holding the stem of the fork in one's teeth, conveniently leaving both hands free.[4] Bone conduction using a tuning fork is specifically used in the Weber and Rinne tests for hearing in order to bypass the middle ear. If just held in open air, the sound of a tuning fork is very faint due to the acoustic impedance mismatch between the steel and air. Moreover, since the feeble sound waves emanating from each prong are 180° out of phase, those two opposite waves interfere, largely cancelling each other. Thus when a solid sheet is slid in between the prongs of a vibrating fork, the apparent volume actually increases, as this cancellation is reduced, just as a loudspeaker requires a baffle in order to radiate efficiently.

Commercial tuning forks are tuned to the correct pitch at the factory, and the pitch and frequency in hertz is stamped on them. They can be retuned by filing material off the prongs. Filing the ends of the prongs raises the pitch, while filing the inside of the base of the prongs lowers it.

Currently, the most common tuning fork sounds the note of A = 440 Hz, the standard concert pitch that many orchestras use. That A is the pitch of the violin's second-highest string, the highest string of the viola, and an octave above the highest string of the cello. Orchestras between 1750 and 1820 mostly used A = 423.5 Hz, though there were many forks and many slightly different pitches.[5] Standard tuning forks are available that vibrate at all the pitches within the central octave of the piano, and also other pitches.

Tuning fork pitch varies slightly with temperature, due mainly to a slight decrease in the modulus of elasticity of steel with increasing temperature. A change in frequency of 48 parts per million per °F (86 ppm per °C) is typical for a steel tuning fork. The frequency decreases (becomes flat) with increasing temperature.[6] Tuning forks are manufactured to have their correct pitch at a standard temperature. The standard temperature is now 20 °C (68 °F), but 15 °C (59 °F) is an older standard. The pitch of other instruments is also subject to variation with temperature change.

Calculation of frequency

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The frequency of a tuning fork depends on its dimensions and what it is made from. Using the Euler-Bernoulli beam model, the fundamental frequency of the tuning fork is:[7][8]

where

f is the frequency the fork vibrates at, (SI units: Hz or 1/s)
α1.875 is the smallest positive real solution to cos(α)cosh(α) = −1,[7] which arises from the boundary conditions of the prong's cantilevered structure.
L is the length of the prongs, (m)
E is the Young's modulus (elastic modulus or stiffness) of the material the fork is made from, (Pa or N/m2 or kg/(ms2))
I is the second moment of area of the cross-section, (m4)
ρ is the density of the fork's material (kg/m3), and
A is the cross-sectional area of the prongs (tines), (m2).

The ratio k2 = I/A in the equation above, where k is the radius of gyration for the prongs, can be rewritten as r2/4 if the prongs are cylindrical with radius r, and b2/12 if the prongs have rectangular cross-section of width b along the direction of motion.[9]

Uses

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Tuning forks have traditionally been used to tune musical instruments, though electronic tuners have largely replaced them. Forks can be driven electrically by placing electronic oscillator-driven electromagnets close to the prongs.

In musical instruments

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A number of keyboard musical instruments use principles similar to tuning forks. The most popular of these is the Rhodes piano, in which hammers hit metal tines that vibrate in the magnetic field of a pickup, creating a signal that drives electric amplification. The earlier, un-amplified dulcitone, which used tuning forks directly, suffered from low volume.

In clocks and watches

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Quartz crystal resonator from a modern quartz watch, formed in the shape of a tuning fork. It vibrates at 32,768 Hz, in the ultrasonic range.
A Bulova Accutron watch from the 1960s, which uses a steel tuning fork (visible in center) vibrating at 360 Hz.

The quartz crystal that serves as the timekeeping element in modern quartz clocks and watches is in the form of a tiny tuning fork. It usually vibrates at a frequency of 32,768 Hz in the ultrasonic range (above the range of human hearing). It is made to vibrate by small oscillating voltages applied by an electronic oscillator circuit to metal electrodes plated on the surface of the crystal. Quartz is piezoelectric, so the voltage causes the tines to bend rapidly back and forth.

The Accutron, an electromechanical watch developed by Max Hetzel[10] and manufactured by Bulova beginning in 1960, used a 360-hertz steel tuning fork as its timekeeper, powered by electromagnets attached to a battery-powered transistor oscillator circuit. The fork provided greater accuracy than conventional balance wheel watches. The humming sound of the tuning fork was audible when the watch was held to the ear.

Medical and scientific uses

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1 kHz tuning fork vacuum tube oscillator used by the U.S. National Bureau of Standards (now NIST) in 1927 as a frequency standard.

Alternatives to the common A=440 standard include philosophical or scientific pitch with standard pitch of C=512. According to Rayleigh, physicists and acoustic instrument makers used this pitch.[11] The tuning fork John Shore gave to George Frideric Handel produces C=512.[12]

Tuning forks, usually C512, are used by medical practitioners to assess a patient's hearing. This is most commonly done with two exams called the Weber test and Rinne test, respectively. Lower-pitched ones, usually at C128, are also used to check vibration sense as part of the examination of the peripheral nervous system.[13]

Orthopedic surgeons have explored using a tuning fork (lowest frequency C=128) to assess injuries where bone fracture is suspected. They hold the end of the vibrating fork on the skin above the suspected fracture, progressively closer to the suspected fracture. If there is a fracture, the periosteum of the bone vibrates and fires nociceptors (pain receptors), causing a local sharp pain.[citation needed] This can indicate a fracture, which the practitioner refers for medical X-ray. The sharp pain of a local sprain can give a false positive.[citation needed] Established practice, however, requires an X-ray regardless, because it's better than missing a real fracture while wondering if a response means a sprain. A systematic review published in 2014 in BMJ Open suggests that this technique is not reliable or accurate enough for clinical use.[14]

Non-medical and non-scientific uses

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Tuning forks also play a role in several alternative therapy practices, such as sonopuncture and polarity therapy.[15]

Radar gun calibration

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A radar gun that measures the speed of cars or a ball in sports is usually calibrated with a tuning fork.[16][17] Instead of the frequency, these forks are labeled with the calibration speed and radar band (e.g., X-band or K-band) they are calibrated for.

In gyroscopes

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Doubled and H-type tuning forks are used for tactical-grade Vibrating Structure Gyroscopes and various types of microelectromechanical systems.[18]

Level sensors

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Tuning fork forms the sensing part of vibrating point level sensors. The tuning fork is kept vibrating at its resonant frequency by a piezoelectric device. Upon coming in contact with solids, amplitude of oscillation goes down, the same is used as a switching parameter for detecting point level for solids.[19] For liquids, the resonant frequency of tuning fork changes upon coming in contact with the liquids, change in frequency is used to detect level.

See also

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
A tuning fork is a U-shaped acoustic device typically constructed from steel, featuring two prongs or tines extending from a central handle, which, when struck, vibrates at a precise, fixed frequency to generate a pure tone with minimal harmonics. This vibration arises from the simple harmonic motion of the prongs, creating alternating regions of compression and rarefaction in the surrounding air that propagate as sound waves. The frequency of oscillation depends on the fork's material, dimensions, and mass distribution, often standardized at pitches like 440 Hz for the musical note A4. Invented in 1711 by John Shore, an English trumpeter and lutenist in the service of the British royal court, the tuning fork was initially developed as a pitch standard for musicians to tune instruments accurately, offering stability that surpassed earlier methods like pipe organs or flutes affected by temperature and humidity. By the mid-19th century, its role expanded into scientific applications, where it functioned as a precision tool for acoustics research, enabling measurements of vibration types, sound speeds, and resonance phenomena through techniques such as resonance tubes and Lissajous figures. In medicine, its use began in the 19th century, evolving into diagnostic applications by the late 1800s for evaluating auditory function and peripheral nerve sensation, as seen in the 1834 work of Ernst Heinrich Weber on bone conduction and human vibration perception using the tuning fork. Today, tuning forks remain integral to diverse fields: in music for calibration and therapy, in physics laboratories for demonstrating wave principles and as timing references in early chronometry, and in clinical settings for non-invasive assessments like the Rinne test (comparing air and bone conduction) and Weber test (lateralizing hearing loss), as well as vibratory sense evaluation in neurological exams per U.S. regulatory standards. Their enduring utility stems from the device's low damping, ensuring prolonged, consistent vibrations, though modern variants include quartz crystal models for ultra-precise applications in cryogenics and force detection.

History

Invention and Early Development

The tuning fork was invented in 1711 by John Shore, a British musician, lutenist, and sergeant trumpeter to the court of Queen Anne. Shore designed the device as a reliable pitch standard for tuning musical instruments, particularly stringed ones like the lute and harpsichord, which required consistent intonation in performance settings. The instrument consisted of a two-pronged steel fork that, when struck, produced a clear, pure tone of fixed frequency, offering a more stable reference than variable organ pipes or other contemporary aids. Initially, the tuning fork's use was confined to elite musicians and court ensembles for maintaining pitch accuracy during rehearsals and performances, as inconsistencies in tuning could disrupt harmonic balance. By the 1750s, it saw broader adoption in emerging orchestras across Europe, where it helped standardize ensemble intonation amid the growing complexity of symphonic music. Shore himself tuned his original fork to approximately A=423.5 Hz, a pitch that became a reference for early users. Commercial production began in England during the mid-18th century, enabling wider distribution to professional musicians. Key early adopters included European royal courts and instrument makers, who valued the fork's precision for calibration. For instance, Shore gifted a fork to composer George Frideric Handel, tuned to A=422.5 Hz (equivalent to C=512 Hz), which survives in historical collections and exemplifies 18th-century craftsmanship. Such artifacts, including similar forks from the period held by institutions like the Smithsonian, demonstrate the device's role in establishing early pitch norms around 422 Hz. By the 19th century, the tuning fork began transitioning to scientific applications in acoustics and physiology.

Standardization and Evolution

In the 19th century, efforts to standardize pitch measurement advanced significantly through the work of Johann Heinrich Scheibler, a German acoustician who in 1834 invented the tonometer—a set of 56 precisely tuned forks spanning from 220 Hz to 440 Hz, enabling accurate vibration counting and beat detection to verify pitches in equal temperament. This innovation allowed for the deskilling of tuning processes, making equal temperament accessible beyond skilled luthiers by providing a portable, objective reference for musical intervals. Scheibler's device influenced subsequent standardization, as it demonstrated tuning forks' utility in resolving discrepancies in pitch across regions and instruments. Building on such precision, governmental and international bodies formalized pitch standards using tuning forks as benchmarks. In 1859, the French government decreed A=435 Hz as the official diapason normal through a commission's decree, establishing the first legally binding concert pitch to unify orchestral tuning amid rising "pitch inflation" in Europe. This was later revised internationally; in 1939, at the International Conference on Acoustics in London, delegates endorsed A=440 Hz, which the International Organization for Standardization (ISO) ratified as ISO 16 in 1955, solidifying its global adoption for music and acoustics. Concurrently, tuning forks played a key role in early sound recording; Édouard-Léon Scott de Martinville's 1857 phonautograph relied on them for calibration, with forks vibrating at known frequencies like 250 Hz to timestamp and synchronize graphical traces of sound waves. Material and design refinements enhanced tuning forks' reliability during this period. Initially forged from tempered steel, 19th-century forks transitioned to nickel-plated steel and alloys like nickel-silver, improving corrosion resistance and tonal stability for prolonged use in humid environments or scientific settings. By the 1870s, adjustable variants emerged, featuring sliding weights on the tines secured by thumb screws to fine-tune frequencies without remaking the fork, primarily for educational demonstrations of beats and interference. Hermann von Helmholtz further propelled their scientific application in the 1860s, employing electromagnetically driven tuning forks in experiments on tone sensation and vowel formants, as detailed in his 1863 treatise On the Sensations of Tone. Mass production accelerated in the late 1800s through workshops like that of Rudolph Koenig in Paris, who crafted extensive sets—such as his 1876 grand tonometer of over 600 forks—for acoustics laboratories, democratizing access to precision instruments. Into the 20th century, tuning forks endured despite electronic alternatives like quartz crystals in timekeeping devices, retaining their role in calibration and therapy due to the pure, stable tones of metal constructions. Koenig-inspired manufacturing proliferated, with firms producing standardized sets for phonautographs and early spectrographs, underscoring forks' versatility before quartz dominated precision timing in the mid-1900s.

Design and Physics

Physical Construction

A tuning fork is constructed as a U-shaped bar featuring two parallel prongs, referred to as tines, of equal length that extend from a central stem, forming the basic structure for producing sustained vibrations. The tines are typically rectangular in cross-section, measuring approximately 7 mm by 9 mm, with a separation of about 10 mm between them to minimize vibrational coupling between the prongs. For a standard model tuned to 440 Hz, the overall length is around 13.7 cm (5.4 inches), with the tines themselves spanning roughly 8-10 cm, though lengths vary inversely with frequency to achieve desired pitches. The primary materials used are elastic metals such as high-quality aluminum alloys or forged steel, selected for their ability to resonate with minimal damping and maintain structural integrity over repeated use. Aluminum alloys are favored in modern designs for their lightweight properties and corrosion resistance, while steel provides greater durability in heavier-duty applications. The tines are often slightly tapered toward the tips to optimize vibrational modes, and the stem, typically 2-4 cm long and cylindrical (about 8 mm in diameter), serves as a handle for manual striking or a mounting point for attachment to resonators. Optional components include dampers to halt vibrations quickly or wooden resonators, such as spruce boxes, to amplify the emitted sound through acoustic coupling. Standard tuning forks weigh between 50 and 100 grams, with a 440 Hz aluminum model typically at 54 grams. Manufacturing begins with forging or casting the U-shaped form from flat bar stock, followed by precision shaping of the tines via cutting or milling to establish the base dimensions. Tuning to the exact frequency involves iterative adjustment: historically, this was achieved by hand-filing the ends of the tines to shorten them and raise the pitch or filing the inner bases to lower it, using beat frequencies against a reference tone for accuracy. In contemporary production, computer numerical control (CNC) machining ensures consistent geometry, while laser etching or grinding refines the tines to within 0.1% of the target frequency, such as A=440 Hz. Adjustable models incorporate removable weights at the tine bases to fine-tune the resonance without permanent alteration.

Principles of Vibration

When a tuning fork is struck, the impact causes elastic deformation of its tines, initiating symmetric flexural waves that propagate along the length of each tine. These waves result in the tines bending toward and away from each other with equal amplitude, maintaining an antiphase motion where one tine moves outward while the other moves inward simultaneously. This symmetric deformation ensures minimal net force on the stem, preserving the purity of the vibration. The primary mode of vibration is the fundamental mode, characterized by the lowest frequency at which the tines flex in antiphase, producing the characteristic pure tone associated with the fork. Higher harmonics, or overtones, occur at approximately integral multiples of the fundamental frequency, but they are rapidly damped due to the fork's design, resulting in a nearly monochromatic sound. The antiphase nature of the fundamental mode isolates the vibration to the tines, reducing energy loss through the stem. Sound is generated as the vibrating tine tips displace surrounding air molecules, creating alternating regions of compression and rarefaction that propagate as longitudinal pressure waves. To minimize damping, the stem experiences negligible vibration, directing energy primarily to airborne sound radiation from the tine ends. The resonance quality, quantified by the Q-factor, reaches up to 1000 in air for typical metal tuning forks, enabling a sustained tone lasting 2-5 seconds before significant decay. The vibrational energy is stored as elastic potential within the deformed metal lattice of the tines during bending. Decay occurs primarily through internal friction, or hysteresis losses in the material, and air resistance, including viscous drag on the tines and acoustic radiation. Classical tuning forks rely solely on mechanical principles, without electrical components, to achieve this energy storage and dissipation.

Frequency Determination

The fundamental frequency of a tuning fork is calculated by modeling its tines as cantilever beams vibrating according to Euler-Bernoulli beam theory. The core equation for the fundamental mode is f(1.875)22πL2EIρA,f \approx \frac{(1.875)^2}{2\pi L^2} \sqrt{\frac{E I}{\rho A}},
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