Accession No

6217


Brief Description

trombone for demonstrations of the interference of sound waves [acoustic interferometer], by Rudolph Koenig, French, 1889 (c)


Origin

France; Paris


Maker

Koenig, Rudolph


Class

sound; demonstration


Earliest Date

Jan. 1, 1889


Latest Date

Dec. 31, 1889


Inscription Date


Material

wood (?); metal (brass); paint


Dimensions

length (pipe not extended): 1060 mm; width: 280 mm; height: 235 mm


Special Collection


Provenance

Purchased from Trevor Philip & Sons, 75A Jermyn Street, St. James’s, London, SW1Y 6NP on or before 03/03/2008.


Inscription

“RUDOLPH KOENIG À PARIS” [stamped into top of wooden table]


Description Notes

Trombone by Rudolph Koenig for demonstrations of the interference of sound waves [Acoustic interferometer]; French; c.1889.

Wooden tabletop device with curved brass pipes, painted black, attached horizontally across the top. Table has brass levelling screw on one foot.

The pipes are curved into narrow U shapes and have a tap at each end. One pipe is stationary, whilst the other slides horizontally on the first one like a trombone slider. (Tap on stationary pipe is a modern replacement -- see conservation history). The sliding position is read off from a wooden scale (marked from 0-36 cm in 1mm intervals) attached to the top of the table.

The pipes each have 2 openings. A tuning fork is vibrated in front of one set of openings causing sound waves to enter the pipes. The length of the movable pipe can be varied by sliding it back and forth.

The sound is heard at the other set of openings. Depending upon the position of the movable pipe, constructive and destructive interference of the two sound waves can be created. This corresponds to maximum and minimum sound levels respectively.

Condition good.


References

Torben Rees; 'Trombone de Koenig'; Explore Whipple Collections online article; Whipple Museum of the History of Science; University of Cambridge; 2009: https://www.whipplemuseum.cam.ac.uk/explore-whipple-collections/acoustics/rudolph-koenig-pursuit-acoustic-perfection/trombone-de-koenig


Events

Description
This apparatus, reminiscent of a trombone, is for experiments and demonstrations relating to the interference of sound waves. From an original design by Sir John Herschel (1792-1881) this example was built by the Parisian physicist and acoustical scientific instrument maker Rudolph Koenig.

The apparatus consists of two metal tubes that bend in a U shape. A sound of definite pitch is produced by means of a tuning fork and Helmholtz resonator, which is then introduced to the two tubes by means of another Y shaped tube. The sound is then split in two identical sound waves, which travel along each main tube. The two sound waves may then be recombined at the other end. One of the tubes may be varied in length by means of sliding, rather like a trombone slide, and this variation can be measured precisely with the ruler fixed in place. As the length of the tube is changed constructive and destructive interference is observed at the opening by means of the ear or by using a manometric flame apparatus.

Interference occurs whenever two sound waves are combined. Sound waves are regular variations in air pressure that travel outwards from sound sources. The pressure at a given point, say at the ear of the observer, varies from higher than atmospheric to lower than atmospheric as the surrounding air is in turn compressed and rarefied. When two sound waves combine, the resulting air pressure is the sum of the two pressures at a given time and location. Sound waves may therefore act to reinforce each other (constructive interference) or to cancel each other out (destructive interference) depending on their frequency and phase (phase being the measure of where the wave is between its maximum and minimum pressures). By making two sound waves of identical frequency travel distances differing by one half of the wavelength it is possible to produce perfect destructive interference. This results in no sound being emitted.

Koenig’s apparatus can be used to determine the velocity of sound in air by using the equation, velocity = frequency x wavelength. If one introduces a sound of known frequency f and achieves destructive interference with a tube length difference of d, then we can find the velocity v by v=2fd (d being half a wavelength). The apparatus can also be used to determine the velocity of sound in other gases by filling the tubes with the gas under investigation.

The idea behind Koenig’s apparatus has been used to develop sound reduction systems in all kinds of areas. In particular, the idea of splitting and recombining out of phase sounds has been deployed in building silencers (mufflers) for automobiles.
28/05/2008
Created by: Dr. Torben Rees on 28/05/2008


FM:46689

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