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Steam whistle

A steam whistle is a device used to produce sound in the form of a whistle using live steam, which creates, projects, and amplifies its sound by acting as a vibrating system.[1]

Operation edit

A recording of a mass blow of traction engine steam whistles

The whistle consists of the following main parts, as seen on the drawing: the whistle bell (1), the steam orifice or aperture (2), and the valve (9).

When the lever (10) is actuated (usually via a pull cord), the valve opens and lets the steam escape through the orifice. The steam will alternately compress and rarefy in the bell, creating the sound. The pitch, or tone, is dependent on the length of the bell; and also how far the operator has opened the valve. Some locomotive engineers invented their own distinctive style of whistling.

Uses of steam whistles edit

Steam whistles were often used in factories and similar places to signal the start or end of a work shift, etc. Steam railway locomotives, traction engines, and steam ships have traditionally been fitted with a steam whistle for warning and communication purposes. Large diameter, low-pitched steam whistles were used on light houses, likely beginning in the 1850s.[2]

The earliest use of steam whistles was as boiler low-water alarms[3] in the 18th century[4] and early 19th century.[5] During the 1830s, whistles were adopted by railroads[6] and steamship companies.[7]

Gallery edit

Railway whistles edit

Steam warning devices have been used on trains since 1833,[8] when George Stephenson invented and patented a steam trumpet for use on the Leicester and Swannington Railway.[9] Period literature makes a distinction between a steam trumpet and a steam whistle.[10] A copy of the trumpet drawing signed May 1833 shows a device about eighteen inches high with an ever-widening trumpet shape with a six-inch diameter at its top or mouth.[8] It is said that George Stephenson invented his trumpet after an accident on the Leicester and Swannington Railway where a train hit either a cart, or a herd of cows, on a level crossing and there were calls for a better way of giving a warning. Although no-one was injured, the accident was deemed serious enough to warrant Stephenson's personal intervention. One account states that [driver] Weatherburn had 'mouthblown his horn' at the crossing in an attempt to prevent the accident, but that no attention had been paid to this audible warning, perhaps because it had not been heard.

Stephenson subsequently called a meeting of directors and accepted the suggestion of the company manager, Ashlin Bagster, that a horn or whistle which could be activated by steam should be constructed and fixed to the locomotives. Stephenson later visited a musical instrument maker on Duke Street in Leicester, who on Stephenson's instructions constructed a 'Steam Trumpet' which was tried out in the presence of the board of Directors ten days later.

Stephenson mounted the trumpet on the top of the boiler's steam dome, which delivers dry steam to the cylinders. The company went on to mount the device on its other locomotives

Locomotive steam trumpets were soon replaced by steam whistles. Air whistles were used on some diesel and electric locomotives, but these mostly employ air horns.

Music edit

An array of steam whistles arranged to play music is referred to as a calliope.

In York, Pennsylvania, a variable pitch steam whistle at the New York Wire Company has been played annually on Christmas Eve since 1925 (except in 1986 and 2005) in what has come to be known as "York's Annual Steam Whistle Christmas Concert". On windy nights, area residents report hearing the concert as far as 12 to 15 miles away. The whistle, which is in the Guinness Book of World Records, was powered by an air compressor during the 2010 concert due to the costs of maintaining and running the boiler.[11][12][13][14][15][16]

Lighthouse fog signals edit

Beginning in 1869,[17] steam whistles began being installed at lighthouse stations as a way of warning mariners in periods of fog, when the lighthouse is not visible. 10" diameter whistles were used as fog signals throughout the United States for many years,[17] until they were later replaced by other compressed air diaphragm or diaphone horns.

Types of whistles edit

  • Plain whistle – an inverted cup mounted on a stem, as in the illustration above. In Europe, railway steam whistles were typically loud, shrill, single-note plain whistles. In the UK, locomotives were usually fitted with only one or two of these whistles, the latter having different tones and being controlled individually to allow more complex signalling. On railroads in Finland, two single-note whistles were used on every engine; one shrill, one of a lower tone. They were used for different signaling purposes. The Deutsche Reichsbahn of Germany introduced another whistle design in the 1920s called "Einheitspfeife", conceived as a single-note plain whistle which already had a very deep-pitched and loud sound, but if the whistle trigger is just pulled down half of its way an even lower tone like from a chime-whistle could also be caused. This whistle is the reason for the typical "long high - short low - short high" signal sound of steam locomotives in Germany.[18]
  • Chime whistle – two or more resonant bells or chambers that sound simultaneously. In America, railway steam whistles were typically compact chime whistles with more than one whistle contained within, creating a chord. In Australia the New South Wales Government Railways after the 1924 re-classification many steam locomotives either had 5 chimes whistles that sound similar to the Star Brass 5-chime fitted (this include many locomotives from the pre 1924 re-classification, or were built new with 5 chime whistles.[19] 3-chimes (3 compact whistles within one) were very popular, as well as 5-chimes, and 6-chimes. In some cases chime whistles were used in Europe. Ships such as the Titanic were equipped with chimes consisting of three separate whistles (in the case of the Titanic the whistles measured 9, 12, and 15 inches diameter). The Japanese National Railways used a chime whistle that sounds like a very deep single-note plain whistle, because the chords where just accessed in a simple parallel circuit if the whistle trigger is pulled down.[20]
  • Organ whistle – a whistle with mouths cut in the side, usually a long whistle in relation to diameter, hence the name. These whistle were very common on steamships, especially those manufactured in the UK.
  • Gong – two whistles facing in opposite directions on a common axis.[21] These were popular as factory whistles. Some were composed of three whistle chimes.
  • Variable pitch whistle – a whistle containing an internal piston available for changing pitch.[22] This whistle type could be made to sound like a siren or to play a melody. Often called a fire alarm whistle, wildcat whistle, or mocking bird whistle.
  • Toroidal or Levavasseur whistle – a whistle with a torus-shaped (doughnut-shaped) resonant cavity paralleling the annular gas orifice, named after Robert Levavasseur,[23] its inventor. Unlike a conventional whistle, the diameter (and sound level) of a ring-shaped whistle can be increased without altering resonance chamber cross-sectional area (preserving frequency), allowing construction of a very large diameter high frequency whistle. The frequency of a conventional whistle declines as diameter is increased. Other ring-shaped whistles include the Hall-Teichmann whistle,[24] Graber whistle,[25] Ultrawhistle,[26] and Dynawhistle.[27]
  • Helmholtz whistle – a whistle with a cross-sectional area exceeding that of the whistle bell opening, often shaped like a bottle or incandescent light bulb. The frequency of this whistle relative to its size is lower than that of a conventional whistle and therefore these whistles have found application in small gauge steam locomotives. Also termed a Bangham whistle.[28][29]
  • Hooter whistle - a single note whistle of greater diameter with a longer bell, resulting in a deeper “hoot” sound when blown. These found use in rail, marine, and industrial applications. In the United States, the Norfolk and Western Railway made extensive use of these kinds of whistles and were noted for the squeaks and chirps produced when blown in addition to their low pitch.

Whistle acoustics edit

Resonant frequency edit

A whistle has a characteristic natural resonant frequency[30] that can be detected by gently blowing human breath across the whistle rim, much as one might blow over the mouth of a bottle. The active sounding frequency (when the whistle is blown on steam) may differ from the natural frequency as discussed below. These comments apply to whistles with a mouth area at least equal to the cross-sectional area of the whistle.

  • Whistle length – The natural resonant frequency decreases as the length of the whistle is increased. Doubling the effective length of a whistle reduces the frequency by one half, assuming that the whistle cross-sectional area is uniform. A whistle is a quarter-wave generator, which means that a sound wave generated by a whistle is about four times the whistle length. If the speed of sound in the steam supplied to a whistle were 15936 inches per second, a pipe with a 15-inch effective length blowing its natural frequency would sound near middle C: 15936/(4 x 15) = 266 Hz. When a whistle is sounding its natural frequency, the effective length referred to here is somewhat longer than the physical length above the mouth if the whistle is of uniform cross-sectional area. That is, the vibrating length of the whistle includes some portion of the mouth. This effect (the “end correction”) is caused by the vibrating steam inside the whistle engaging vibration of some steam outside the enclosed pipe, where there is a transition from plane waves to spherical waves.[31] Formulas are available to estimate the effective length of a whistle,[30] but an accurate formula to predict sounding frequency would have to incorporate whistle length, scale, gas flow rate, mouth height, and mouth wall area (see below).
  • Blowing pressure – Frequency increases with blowing pressure,[32] which determines gas volume flow through the whistle, allowing a locomotive engineer to play a whistle like a musical instrument, using the valve to vary the flow of steam. The term for this was “quilling.” An experiment with a short plain whistle reported in 1883 showed that incrementally increasing steam pressure drove the whistle from E to D-flat, a 68 percent increase in frequency.[33] Pitch deviations from the whistle natural frequency likely follow velocity differences in the steam jet downstream from the aperture, creating phase differences between driving frequency and natural frequency of the whistle. Although at normal blowing pressures the aperture constrains the jet to the speed of sound, once it exits the aperture and expands, velocity decay is a function of absolute pressure.[34] Also, frequency may vary at a fixed blowing pressure with differences in temperature of steam or compressed air.[35][36][37] Industrial steam whistles typically were operated in the range of 100 to 300 pounds per square inch gauge pressure (psig) (0.7 - 2.1 megapascals, MPa), although some were constructed for use on pressures as high as 600 psig (4.1 MPa). All of these pressures are within the choked flow regime,[38] where mass flow scales with upstream absolute pressure and inversely with the square root of absolute temperature. This means that for dry saturated steam, a halving of absolute pressure results in almost a halving of flow.[39][40] This has been confirmed by tests of whistle steam consumption at various pressures.[41] Excessive pressure for a given whistle design will drive the whistle into an overblown mode, where the fundamental frequency will be replaced by an odd harmonic, that is a frequency that is an odd number multiple of the fundamental. Usually this is the third harmonic (second overtone frequency), but an example has been noted where a large whistle jumped to the fifteenth harmonic.[42] A long narrow whistle such as that of the Liberty ship John W. Brown sounds a rich spectrum of overtones, but is not overblown. (In overblowing the "amplitude of the pipe fundamental frequency falls to zero.")[43] Increasing whistle length increases the number and amplitude of harmonics, as has been demonstrated in experiments with a variable-pitch whistle. Whistles tested on steam produce both even-numbered and odd-numbered harmonics.[42] The harmonic profile of a whistle might also be influenced by aperture width, mouth cut-up, and lip-aperture offset, as is the case for organ pipes.[44]
  • Steam quality – The dryness of steam provided to a whistles is variable and will affect whistle tone frequency. Steam quality determines the velocity of sound, which declines with decreasing dryness due to the inertia of the liquid phase. The speed of sound in steam is predictable if steam dryness is known.[45] Also, the specific volume of steam for a given temperature decreases with decreasing dryness.[46][39] Two examples of estimates of speed of sound in steam calculated from whistles blown under field conditions are 1,326 and 1,352 feet per second.[47]
  • Aspect ratio – The more squat the whistle, the greater is the change in pitch with blowing pressure.[48][32] This may be caused by differences in the Q factor.[49] The pitch of a very squat whistle may rise several semitones as pressure is raised.[50] Whistle frequency prediction thus requires establishment of a set of frequency/pressure curves unique to whistle scale, and a set of whistles may fail to track a musical chord as blowing pressure changes if each whistle is of a different scale. This is true of many antique whistles divided into a series of compartments of the same diameter but of different lengths. Some whistle designers minimized this problem by building resonant chambers of a similar scale.[51]
  • Mouth vertical length (“cut-up”) – Frequency of a plain whistle declines as the whistle bell is raised away from the steam source. If the cut-up of an organ whistle or single bell chime is raised (without raising the whistle ceiling), the effective chamber length is shortened. Shortening the chamber drives frequency up, but raising the cut-up drives frequency down. The resulting frequency (higher, lower, or unchanged) will be determined by whistle scale and by competition between the two drivers.[52][53] The cut-up prescribed by whistle-maker Robert Swanson for 150 psig steam pressure was 0.35 x bell diameter for a plain whistle, which is about 1.45 x net bell cross-sectional area (subtracting stud area).[54] The Nathan Manufacturing Company used a cut-up of 1.56 x chamber cross-sectional area for their 6-note railway chime whistle.[55]
  • Cut-up in relation to mouth arc – A large change in cut-up (e.g., 4x difference) may have little impact on whistle natural frequency if mouth area and total resonator length are held constant.[30] For example, a plain whistle, which has a 360-degree mouth (that extends completely around the whistle circumference), can emit a similar frequency to a partial mouth organ whistle of the same mouth area and same overall resonator length (aperture to ceiling), despite an immensely different cut-up. (Cut-up is the distance between the steam aperture and the upper lip of the mouth.) This suggests that effective cut-up is determined by proximity of the oscillating gas column to the steam jet rather than by the distance between the upper mouth lip and the steam aperture.[56]
  • Steam aperture width – Frequency may rise as steam aperture width declines[53] and the slope of the frequency/pressure curve may vary with aperture width.[57]
  • Gas composition – The frequency of a whistle driven by steam is typically higher than that of a whistle driven by compressed air at the same pressure. This frequency difference is caused by the greater speed of sound in steam, which is less dense than air. The magnitude of the frequency difference can vary because the speed of sound is influenced by air temperature and by steam quality. Also, the more squat the whistle, the more sensitive it is to the difference in gas flow rate between steam and air that occurs at a fixed blowing pressure. Data from 14 whistles (34 resonant chambers) sounded under a variety of field conditions showed a wide range of frequency differences between steam and air (5 - 43 percent higher frequency on steam). Very elongate whistles, which are fairly resistant to gas flow differences, sounded a frequency 18 - 22 percent higher on steam (about three semitones).[58]

Sound pressure level edit

Whistle sound level varies with several factors:

  • Blowing pressure – Sound level increases as blowing pressure is raised,[59][60] although there may be an optimum pressure at which sound level peaks.[48]
  • Aspect ratio – Sound level increases as whistle length is reduced, increasing frequency. For example, depressing the piston of a variable-pitch steam whistle changed the frequency from 333 Hz to 753 Hz and raised the sound pressure level from 116 dBC to 123 dBC. That five-fold difference in the square of the frequency resulted in a five-fold difference in sound intensity.[61] Sound level also increases as whistle cross-sectional area is increased.[62] A sample of 12 single-note whistles ranging in size from one-inch diameter to 12-inches diameter showed a relationship between sound intensity and the square of the cross-sectional area (when differences in frequency were taken into account). In other words, relative whistle sound intensity can be estimated using the square of the cross-sectional area divided by the square of the wavelength.[61][63] For example, the sound intensity from a whistle bell of 6-inch diameter x 7.5-inch length (113 dBC) was 10x that of a 2 x 4-inch whistle (103 dBC) and twice that of a (lower frequency) 10 x 40-inch whistle (110 dBC). These whistles were sounded on compressed air at 125 pounds per square inch gauge pressure (862 Kilopascals) and sound levels were recorded at 100 feet distance. Elongate organ whistles may exhibit disproportionately high sound levels due to their strong higher frequency overtones. At a separate venue a 20-inch diameter Ultrawhistle (ring-shaped whistle) operating at 15 pounds per square inch gauge pressure (103.4 kilopascals) produced 124 dBC at 100 feet.[64][26] It is unknown how the sound level of this whistle would compare to that of a conventional whistle of the same frequency and resonant chamber area. By comparison, a Bell-Chrysler air raid siren generates 138 dBC at 100 feet.[65] The sound level of a Levavasseur toroidal whistle is enhanced by about 10 decibels by a secondary cavity parallel to the resonant cavity, the former creating a vortex that augments the oscillations of the jet driving the whistle.[66]
  • Steam aperture width – If gas flow is restricted by the area of the steam aperture, widening the aperture will increase the sound level for a fixed blowing pressure.[60] Enlarging the steam aperture can compensate for the loss of sound output if pressure is reduced. It has been known since at least the 1830s that whistles can be modified for low pressure operation and still achieve a high sound level.[7] Data on the compensatory relationship between pressure and aperture size are scant, but tests on compressed air indicate that a halving of absolute pressure requires that the aperture size be at least doubled in width to maintain the original sound level, and aperture width in some antique whistle arrays increases with diameter (aperture area thus increasing with whistle cross-sectional area) for whistles of the same scale.[56][60] Applying the physics of high pressure jets exiting circular apertures, a doubling of velocity and gas concentration at a fixed point in the whistle mouth would require a quadrupling of either aperture area or absolute pressure. (A quartering of absolute pressure would be compensated by a quadrupling of aperture area—the velocity decay constant increases approximately with the square root of absolute pressure in the normal whistle-blowing pressure range.) In reality, trading pressure loss for greater aperture area may be less efficient as pressure-dependent adjustments occur to virtual origin displacement.[34] Quadrupling the width of an organ pipe aperture at a fixed blowing pressure resulted in somewhat less than a doubling of velocity at the flue exit.[67]
  • Steam aperture profile – Gas flow rate (and thus sound level) is set not only by aperture area and blowing pressure, but also by aperture geometry. Friction and turbulence influence the flow rate, and are accounted for by a discharge coefficient. A mean estimate of the discharge coefficient from whistle field tests is 0.72 (range 0.69 - 0.74).[41]
  • Mouth vertical length (“cut-up”) – The mouth length (cut-up) that provides the highest sound level at a fixed blowing pressure varies with whistle scale, and some makers of multi-tone whistles therefore cut a mouth height unique to the scale of each resonant chamber, maximizing sound output of the whistle.[68] Ideal cut-up for whistles of a fixed diameter and aperture width (including single-bell chime compartments) at a fixed blowing pressure appears to vary approximately with the square root of effective length.[69] Antique whistle makers commonly used a compromise mouth area of about 1.4x whistle cross-sectional area. If a whistle is driven to its maximum sound level with the mouth area set equal to the whistle cross-sectional area, it may be possible to increase the sound level by further increasing the mouth area. .[70][71]
  • Frequency and distance Sound pressure level decreases by half (six decibels) with each doubling of distance due to divergence from the source, an inversely proportional relationship. (Distinct from the inverse square law, applicable to sound intensity, rather than pressure.) Sound pressure level also decreases due to atmospheric absorption, which is strongly dependent upon frequency, lower frequencies traveling farthest. For example, a 1000 Hz whistle has an atmospheric attenuation coefficient one half that of a 2000 Hz whistle (calculated for 50 percent relative humidity at 20 degrees Celsius). This means that in addition to divergent sound dampening, there would be a loss of 0.5 decibel per 100 meters from the 1000 Hz whistle and 1.0 decibel per 100 meters for the 2000 Hz whistle. Additional factors affecting sound propagation include barriers, atmospheric temperature gradients, and "ground effects.”[72][73][74]

Terminology edit

Acoustic length [75] or effective length [76] is the quarter wavelength generated by the whistle. It is calculated as one quarter the ratio of speed of sound to the whistle's frequency. Acoustic length may differ from the whistle's physical length,[77] also termed geometric length.[78] depending upon mouth configuration, etc.[30] The end correction is the difference between the acoustic length and the physical length above the mouth. The end correction is a function of diameter whereas the ratio of acoustic length to physical length is a function of scale. These calculations are useful in whistle design to obtain a desired sounding frequency. Working length in early usage meant whistle acoustic length, i.e., the effective length of the working whistle,[79] but recently has been used for physical length including the mouth.[80]

Loudest and largest whistles edit

Loudness is a subjective perception that is influenced by sound pressure level, sound duration, and sound frequency.[73][74] High sound pressure level potential has been claimed for the whistles of Vladimir Gavreau,[81] who tested whistles as large as 1.5 meter (59-inch) diameter (37 Hz).[82]

A 20-inch diameter ring-shaped whistle (“Ultrawhistle”) patented and produced by Richard Weisenberger sounded 124 decibels at 100 feet.[83] The variable pitch steam whistle at the New York Wire Company in York, Pennsylvania, was entered in the Guinness Book of World Records in 2002 as the loudest steam whistle on record at 124.1dBA from a set distance[clarify] used by Guinness.[84] The York whistle was also measured at 134.1 decibels from a distance of 23-feet.[12]

A fire-warning whistle supplied to a Canadian saw mill by the Eaton, Cole, and Burnham Company in 1882 measured 20 inches in diameter, four feet nine inches from bowl to ornament, and weighed 400 pounds. The spindle supporting the whistle bell measured 3.5 inches diameter and the whistle was supplied by a four-inch feed pipe.[85][86]

Other records of large whistles include an 1893 account of U.S. President Grover Cleveland activating the “largest steam whistle in the world,” said to be “five feet” at the Chicago World's Fair.[87][88]

The sounding chamber of a whistle installed at the 1924 Long-Bell Lumber Company, Longview, Washington measured 16 inches diameter x 49 inches in length.[89]

The whistle bells of multi-bell chimes used on ocean liners such as the RMS Titanic measured 9, 12, and 15 inches diameter.[90]

The whistle bells of the Canadian Pacific steamships Assiniboia and Keewatin measured 12 inches in diameter and that of the Keewatin measured 60 inches in length.[91][92]

A multi-bell chime whistle installed at the Standard Sanitary Manufacturing Company in 1926 was composed of five separate whistle bells measuring 5 x15, 7 x 21, 8x 24, 10 x 30, and 12 x36 inches, all plumbed to a five-inch steam pipe.[93]

The Union Water Meter Company of Worcester Massachusetts produced a gong whistle[clarify] composed of three bells, 8 x 9-3/4, 12 x 15, and 12 x 25 inches.[94] Twelve-inch diameter steam whistles were commonly used at light houses in the 19th century.[95]

It has been claimed that the sound level of an Ultrawhistle would be significantly greater than that of a conventional whistle,[96] but comparative tests of large whistles have not been undertaken. Tests of small Ultrawhistles have not shown higher sound levels compared to conventional whistles of the same diameter.[70]

See also edit

References edit

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  62. ^ Patent 2784693, Burrows, Lewis M., published 1957 , column 5, lines 30-34
  63. ^ Barry, Harry (2002). "Sound levels of my whistles". Horn and Whistle (98): 19.
  64. ^ Weisenberger, Richard (1983). "The loudest whistle". Horn and Whistle (6): 7–9.
  65. ^ Carruthers, James A. (1984). "More on loudest sounds". Horn and Whistle (10): 6.
  66. ^ Elias, I. (1962). "Evaluation and Applications of the Levavasseur Whistle". 1962 IRE National Convention. IEEE. pp. 36–42. doi:10.1109/irenc.1962.199221.
  67. ^ Außerlechner, Hubert J.; Trommer, Thomas; Angster, Judit; Miklós, András (2009-08-01). "Experimental jet velocity and edge tone investigations on a foot model of an organ pipe". The Journal of the Acoustical Society of America. 126 (2). Acoustical Society of America (ASA): 878–886. Bibcode:2009ASAJ..126..878A. doi:10.1121/1.3158935. ISSN 0001-4966. PMID 19640052.
  68. ^ Patent 2784693, Burrows, Lewis M., published 1957 , column 5, lines 20-28.
  69. ^ Rhodes, Tom (1984). Building a steamboat whistle. Live Steam, November:42-44.
  70. ^ a b Ommundsen, Peter (2008). "The Levavasseur toroidal whistle and other loud whistles". Horn and Whistle (119): 5.
  71. ^ Ommundsen, Peter (2009). "Whistle engineering questions". Horn and Whistle (121): 26–27.
  72. ^ Fagen, Edward (2005). "Whistles as Sound Sources". Horn and Whistle (107): 18–24.
  73. ^ a b Fagen, Edward (2005). "Whistles as Sound Sources, Part 2". Horn and Whistle (108): 35–39.
  74. ^ a b Piercy, J.E.; Tony F.W., Embleton (1979). "Sound propagation in the open air". In Harris, Cyril M. (ed.). Handbook of Noise Control (Second ed.). New York: McGraw-Hill.
  75. ^ Talbot-Smith, Michael (1999). Audio Engineer's Reference Book (2nd ed.). Oxford: Focal. ISBN 0-7506-0386-0.
  76. ^ Serway, Raymond A. (1990). Physics for Scientists and Engineers. Philadelphia: Saunders College Publishing. ISBN 0-03-005922-4.
  77. ^ Rossing, T.D. (1990). The Science of Sound. Addison-Wesley Publishing Company. ISBN 978-0-201-15727-7.
  78. ^ Fahy, F.J. (2000). Foundations of Engineering Acoustics. Elsevier Science. ISBN 978-0-08-050683-8.
  79. ^ Hadley, H.E. (1926). Everyday Physics. Macmillan and Company, limited.
  80. ^ Weisenberger, Richard (1986). Mathematics for the whistle builder. Horn and Whistle 23:10-16.
  81. ^ Altmann, Jürgen (2001). "Acoustic weapons ‐ a prospective assessment". Science & Global Security. 9 (3). Informa UK Limited: 165–234. Bibcode:2001S&GS....9..165A. doi:10.1080/08929880108426495. ISSN 0892-9882. S2CID 31795453.
  82. ^ Gavreau, V. (1968). "Infrasound". Science Journal (4): 33–37.
  83. ^ Weisenberger, Richard (1983). The loudest whistle. Horn and Whistle 6:7-9.
  84. ^ "Loudest whistle, steam". Guinness World Records. 2002-12-12.
  85. ^ The New York Times, May 26, 1882.
  86. ^ The Chronicle – a journal devoted to the interests of insurance. Vol xxix page 346 1882.
  87. ^ Crofford, Maurice (2001). The Rich Cut Glass of Charles Guernsey Tuthill. College Station: Texas A&M University Press. p. 64. ISBN 978-1-58544-148-8.
  88. ^ "FEATURES OF THE OPENING.; People Likely to Jump When the President Touches the Button at Chicago". The New York Times. April 27, 1893.
  89. ^ Drummond, Michael (1996) Steam whistle buffs abuzz over Big Benjamin. The daily News of Longview Washington, December 21, reprinted in Horn and Whistle 75:8-9.
  90. ^ Fagen, Ed (1997). Titanic’s whistle blow a bit less than titanic. Horn and whistle 75:8-11.
  91. ^ Barry, Harry (1983). The Assiniboia steam whistle. Horn and Whistle 4:13-14
  92. ^ Barry, Harry (1998). A survey of large whistles. Horn and Whistle 79:6-7
  93. ^ Louisville Herald, June 8, 1926.
  94. ^ Barry, Harry (2002). The twelve inch diameter, three bell Union Water meter gong whistle. Horn and Whistle 98:14-15.
  95. ^ Clarke, F.L. (1888). "Fog and fog signals on the pacific coast". Overland Monthly (12): 353.
  96. ^ For example, Weisenberger, Richard (1986). Build an eight inch super whistle: an introduction to the toroidal whistle. Horn and Whistle 25:4-6.

Further reading edit

  • Fagen, Edward A. (2001). The Engine's Moan: American Steam Whistles. New Jersey: Astragal Press. ISBN 1-931626-01-4.

steam, whistle, beer, brand, steam, whistle, brewing, steam, whistle, device, used, produce, sound, form, whistle, using, live, steam, which, creates, projects, amplifies, sound, acting, vibrating, system, contents, operation, uses, steam, whistles, gallery, r. For the beer brand see Steam Whistle Brewing A steam whistle is a device used to produce sound in the form of a whistle using live steam which creates projects and amplifies its sound by acting as a vibrating system 1 Contents 1 Operation 2 Uses of steam whistles 2 1 Gallery 2 2 Railway whistles 2 3 Music 2 4 Lighthouse fog signals 3 Types of whistles 4 Whistle acoustics 4 1 Resonant frequency 4 2 Sound pressure level 4 3 Terminology 5 Loudest and largest whistles 6 See also 7 References 8 Further readingOperation edit source source A recording of a mass blow of traction engine steam whistlesThe whistle consists of the following main parts as seen on the drawing the whistle bell 1 the steam orifice or aperture 2 and the valve 9 When the lever 10 is actuated usually via a pull cord the valve opens and lets the steam escape through the orifice The steam will alternately compress and rarefy in the bell creating the sound The pitch or tone is dependent on the length of the bell and also how far the operator has opened the valve Some locomotive engineers invented their own distinctive style of whistling Uses of steam whistles editSteam whistles were often used in factories and similar places to signal the start or end of a work shift etc Steam railway locomotives traction engines and steam ships have traditionally been fitted with a steam whistle for warning and communication purposes Large diameter low pitched steam whistles were used on light houses likely beginning in the 1850s 2 The earliest use of steam whistles was as boiler low water alarms 3 in the 18th century 4 and early 19th century 5 During the 1830s whistles were adopted by railroads 6 and steamship companies 7 Gallery edit nbsp High pitched plain whistle left and low pitched plain whistle right nbsp 3 bell multi tone chime whistle sounds a musical chord nbsp Single bell multi tone chime whistle with compartments of differing length and pitch tuned to a musical chord nbsp 6 note step top multi tone chime whistle with 6 compartments of differing length and pitch The mouth of each chamber is partially walled nbsp A partial mouth whistle organ whistle in which the mouth extends less than 360 degrees around the whistle circumference nbsp Gong chime whistle two whistles aligned on the same axis nbsp Variable pitch whistle note the internal piston used for adjusting pitch nbsp Ultrawhistle with ring shaped bell cavity nbsp Helmholtz whistle has a low pitch relative to its lengthRailway whistles edit Further information Train whistle Steam warning devices have been used on trains since 1833 8 when George Stephenson invented and patented a steam trumpet for use on the Leicester and Swannington Railway 9 Period literature makes a distinction between a steam trumpet and a steam whistle 10 A copy of the trumpet drawing signed May 1833 shows a device about eighteen inches high with an ever widening trumpet shape with a six inch diameter at its top or mouth 8 It is said that George Stephenson invented his trumpet after an accident on the Leicester and Swannington Railway where a train hit either a cart or a herd of cows on a level crossing and there were calls for a better way of giving a warning Although no one was injured the accident was deemed serious enough to warrant Stephenson s personal intervention One account states that driver Weatherburn had mouthblown his horn at the crossing in an attempt to prevent the accident but that no attention had been paid to this audible warning perhaps because it had not been heard Stephenson subsequently called a meeting of directors and accepted the suggestion of the company manager Ashlin Bagster that a horn or whistle which could be activated by steam should be constructed and fixed to the locomotives Stephenson later visited a musical instrument maker on Duke Street in Leicester who on Stephenson s instructions constructed a Steam Trumpet which was tried out in the presence of the board of Directors ten days later Stephenson mounted the trumpet on the top of the boiler s steam dome which delivers dry steam to the cylinders The company went on to mount the device on its other locomotivesLocomotive steam trumpets were soon replaced by steam whistles Air whistles were used on some diesel and electric locomotives but these mostly employ air horns Music edit An array of steam whistles arranged to play music is referred to as a calliope In York Pennsylvania a variable pitch steam whistle at the New York Wire Company has been played annually on Christmas Eve since 1925 except in 1986 and 2005 in what has come to be known as York s Annual Steam Whistle Christmas Concert On windy nights area residents report hearing the concert as far as 12 to 15 miles away The whistle which is in the Guinness Book of World Records was powered by an air compressor during the 2010 concert due to the costs of maintaining and running the boiler 11 12 13 14 15 16 Lighthouse fog signals edit Further information Foghorn Beginning in 1869 17 steam whistles began being installed at lighthouse stations as a way of warning mariners in periods of fog when the lighthouse is not visible 10 diameter whistles were used as fog signals throughout the United States for many years 17 until they were later replaced by other compressed air diaphragm or diaphone horns Types of whistles editPlain whistle an inverted cup mounted on a stem as in the illustration above In Europe railway steam whistles were typically loud shrill single note plain whistles In the UK locomotives were usually fitted with only one or two of these whistles the latter having different tones and being controlled individually to allow more complex signalling On railroads in Finland two single note whistles were used on every engine one shrill one of a lower tone They were used for different signaling purposes The Deutsche Reichsbahn of Germany introduced another whistle design in the 1920s called Einheitspfeife conceived as a single note plain whistle which already had a very deep pitched and loud sound but if the whistle trigger is just pulled down half of its way an even lower tone like from a chime whistle could also be caused This whistle is the reason for the typical long high short low short high signal sound of steam locomotives in Germany 18 Chime whistle two or more resonant bells or chambers that sound simultaneously In America railway steam whistles were typically compact chime whistles with more than one whistle contained within creating a chord In Australia the New South Wales Government Railways after the 1924 re classification many steam locomotives either had 5 chimes whistles that sound similar to the Star Brass 5 chime fitted this include many locomotives from the pre 1924 re classification or were built new with 5 chime whistles 19 3 chimes 3 compact whistles within one were very popular as well as 5 chimes and 6 chimes In some cases chime whistles were used in Europe Ships such as the Titanic were equipped with chimes consisting of three separate whistles in the case of the Titanic the whistles measured 9 12 and 15 inches diameter The Japanese National Railways used a chime whistle that sounds like a very deep single note plain whistle because the chords where just accessed in a simple parallel circuit if the whistle trigger is pulled down 20 Organ whistle a whistle with mouths cut in the side usually a long whistle in relation to diameter hence the name These whistle were very common on steamships especially those manufactured in the UK Gong two whistles facing in opposite directions on a common axis 21 These were popular as factory whistles Some were composed of three whistle chimes Variable pitch whistle a whistle containing an internal piston available for changing pitch 22 This whistle type could be made to sound like a siren or to play a melody Often called a fire alarm whistle wildcat whistle or mocking bird whistle Toroidal or Levavasseur whistle a whistle with a torus shaped doughnut shaped resonant cavity paralleling the annular gas orifice named after Robert Levavasseur 23 its inventor Unlike a conventional whistle the diameter and sound level of a ring shaped whistle can be increased without altering resonance chamber cross sectional area preserving frequency allowing construction of a very large diameter high frequency whistle The frequency of a conventional whistle declines as diameter is increased Other ring shaped whistles include the Hall Teichmann whistle 24 Graber whistle 25 Ultrawhistle 26 and Dynawhistle 27 Helmholtz whistle a whistle with a cross sectional area exceeding that of the whistle bell opening often shaped like a bottle or incandescent light bulb The frequency of this whistle relative to its size is lower than that of a conventional whistle and therefore these whistles have found application in small gauge steam locomotives Also termed a Bangham whistle 28 29 Hooter whistle a single note whistle of greater diameter with a longer bell resulting in a deeper hoot sound when blown These found use in rail marine and industrial applications In the United States the Norfolk and Western Railway made extensive use of these kinds of whistles and were noted for the squeaks and chirps produced when blown in addition to their low pitch Whistle acoustics editResonant frequency edit A whistle has a characteristic natural resonant frequency 30 that can be detected by gently blowing human breath across the whistle rim much as one might blow over the mouth of a bottle The active sounding frequency when the whistle is blown on steam may differ from the natural frequency as discussed below These comments apply to whistles with a mouth area at least equal to the cross sectional area of the whistle Whistle length The natural resonant frequency decreases as the length of the whistle is increased Doubling the effective length of a whistle reduces the frequency by one half assuming that the whistle cross sectional area is uniform A whistle is a quarter wave generator which means that a sound wave generated by a whistle is about four times the whistle length If the speed of sound in the steam supplied to a whistle were 15936 inches per second a pipe with a 15 inch effective length blowing its natural frequency would sound near middle C 15936 4 x 15 266 Hz When a whistle is sounding its natural frequency the effective length referred to here is somewhat longer than the physical length above the mouth if the whistle is of uniform cross sectional area That is the vibrating length of the whistle includes some portion of the mouth This effect the end correction is caused by the vibrating steam inside the whistle engaging vibration of some steam outside the enclosed pipe where there is a transition from plane waves to spherical waves 31 Formulas are available to estimate the effective length of a whistle 30 but an accurate formula to predict sounding frequency would have to incorporate whistle length scale gas flow rate mouth height and mouth wall area see below Blowing pressure Frequency increases with blowing pressure 32 which determines gas volume flow through the whistle allowing a locomotive engineer to play a whistle like a musical instrument using the valve to vary the flow of steam The term for this was quilling An experiment with a short plain whistle reported in 1883 showed that incrementally increasing steam pressure drove the whistle from E to D flat a 68 percent increase in frequency 33 Pitch deviations from the whistle natural frequency likely follow velocity differences in the steam jet downstream from the aperture creating phase differences between driving frequency and natural frequency of the whistle Although at normal blowing pressures the aperture constrains the jet to the speed of sound once it exits the aperture and expands velocity decay is a function of absolute pressure 34 Also frequency may vary at a fixed blowing pressure with differences in temperature of steam or compressed air 35 36 37 Industrial steam whistles typically were operated in the range of 100 to 300 pounds per square inch gauge pressure psig 0 7 2 1 megapascals MPa although some were constructed for use on pressures as high as 600 psig 4 1 MPa All of these pressures are within the choked flow regime 38 where mass flow scales with upstream absolute pressure and inversely with the square root of absolute temperature This means that for dry saturated steam a halving of absolute pressure results in almost a halving of flow 39 40 This has been confirmed by tests of whistle steam consumption at various pressures 41 Excessive pressure for a given whistle design will drive the whistle into an overblown mode where the fundamental frequency will be replaced by an odd harmonic that is a frequency that is an odd number multiple of the fundamental Usually this is the third harmonic second overtone frequency but an example has been noted where a large whistle jumped to the fifteenth harmonic 42 A long narrow whistle such as that of the Liberty ship John W Brown sounds a rich spectrum of overtones but is not overblown In overblowing the amplitude of the pipe fundamental frequency falls to zero 43 Increasing whistle length increases the number and amplitude of harmonics as has been demonstrated in experiments with a variable pitch whistle Whistles tested on steam produce both even numbered and odd numbered harmonics 42 The harmonic profile of a whistle might also be influenced by aperture width mouth cut up and lip aperture offset as is the case for organ pipes 44 Steam quality The dryness of steam provided to a whistles is variable and will affect whistle tone frequency Steam quality determines the velocity of sound which declines with decreasing dryness due to the inertia of the liquid phase The speed of sound in steam is predictable if steam dryness is known 45 Also the specific volume of steam for a given temperature decreases with decreasing dryness 46 39 Two examples of estimates of speed of sound in steam calculated from whistles blown under field conditions are 1 326 and 1 352 feet per second 47 Aspect ratio The more squat the whistle the greater is the change in pitch with blowing pressure 48 32 This may be caused by differences in the Q factor 49 The pitch of a very squat whistle may rise several semitones as pressure is raised 50 Whistle frequency prediction thus requires establishment of a set of frequency pressure curves unique to whistle scale and a set of whistles may fail to track a musical chord as blowing pressure changes if each whistle is of a different scale This is true of many antique whistles divided into a series of compartments of the same diameter but of different lengths Some whistle designers minimized this problem by building resonant chambers of a similar scale 51 Mouth vertical length cut up Frequency of a plain whistle declines as the whistle bell is raised away from the steam source If the cut up of an organ whistle or single bell chime is raised without raising the whistle ceiling the effective chamber length is shortened Shortening the chamber drives frequency up but raising the cut up drives frequency down The resulting frequency higher lower or unchanged will be determined by whistle scale and by competition between the two drivers 52 53 The cut up prescribed by whistle maker Robert Swanson for 150 psig steam pressure was 0 35 x bell diameter for a plain whistle which is about 1 45 x net bell cross sectional area subtracting stud area 54 The Nathan Manufacturing Company used a cut up of 1 56 x chamber cross sectional area for their 6 note railway chime whistle 55 Cut up in relation to mouth arc A large change in cut up e g 4x difference may have little impact on whistle natural frequency if mouth area and total resonator length are held constant 30 For example a plain whistle which has a 360 degree mouth that extends completely around the whistle circumference can emit a similar frequency to a partial mouth organ whistle of the same mouth area and same overall resonator length aperture to ceiling despite an immensely different cut up Cut up is the distance between the steam aperture and the upper lip of the mouth This suggests that effective cut up is determined by proximity of the oscillating gas column to the steam jet rather than by the distance between the upper mouth lip and the steam aperture 56 Steam aperture width Frequency may rise as steam aperture width declines 53 and the slope of the frequency pressure curve may vary with aperture width 57 Gas composition The frequency of a whistle driven by steam is typically higher than that of a whistle driven by compressed air at the same pressure This frequency difference is caused by the greater speed of sound in steam which is less dense than air The magnitude of the frequency difference can vary because the speed of sound is influenced by air temperature and by steam quality Also the more squat the whistle the more sensitive it is to the difference in gas flow rate between steam and air that occurs at a fixed blowing pressure Data from 14 whistles 34 resonant chambers sounded under a variety of field conditions showed a wide range of frequency differences between steam and air 5 43 percent higher frequency on steam Very elongate whistles which are fairly resistant to gas flow differences sounded a frequency 18 22 percent higher on steam about three semitones 58 Sound pressure level edit Whistle sound level varies with several factors Blowing pressure Sound level increases as blowing pressure is raised 59 60 although there may be an optimum pressure at which sound level peaks 48 Aspect ratio Sound level increases as whistle length is reduced increasing frequency For example depressing the piston of a variable pitch steam whistle changed the frequency from 333 Hz to 753 Hz and raised the sound pressure level from 116 dBC to 123 dBC That five fold difference in the square of the frequency resulted in a five fold difference in sound intensity 61 Sound level also increases as whistle cross sectional area is increased 62 A sample of 12 single note whistles ranging in size from one inch diameter to 12 inches diameter showed a relationship between sound intensity and the square of the cross sectional area when differences in frequency were taken into account In other words relative whistle sound intensity can be estimated using the square of the cross sectional area divided by the square of the wavelength 61 63 For example the sound intensity from a whistle bell of 6 inch diameter x 7 5 inch length 113 dBC was 10x that of a 2 x 4 inch whistle 103 dBC and twice that of a lower frequency 10 x 40 inch whistle 110 dBC These whistles were sounded on compressed air at 125 pounds per square inch gauge pressure 862 Kilopascals and sound levels were recorded at 100 feet distance Elongate organ whistles may exhibit disproportionately high sound levels due to their strong higher frequency overtones At a separate venue a 20 inch diameter Ultrawhistle ring shaped whistle operating at 15 pounds per square inch gauge pressure 103 4 kilopascals produced 124 dBC at 100 feet 64 26 It is unknown how the sound level of this whistle would compare to that of a conventional whistle of the same frequency and resonant chamber area By comparison a Bell Chrysler air raid siren generates 138 dBC at 100 feet 65 The sound level of a Levavasseur toroidal whistle is enhanced by about 10 decibels by a secondary cavity parallel to the resonant cavity the former creating a vortex that augments the oscillations of the jet driving the whistle 66 Steam aperture width If gas flow is restricted by the area of the steam aperture widening the aperture will increase the sound level for a fixed blowing pressure 60 Enlarging the steam aperture can compensate for the loss of sound output if pressure is reduced It has been known since at least the 1830s that whistles can be modified for low pressure operation and still achieve a high sound level 7 Data on the compensatory relationship between pressure and aperture size are scant but tests on compressed air indicate that a halving of absolute pressure requires that the aperture size be at least doubled in width to maintain the original sound level and aperture width in some antique whistle arrays increases with diameter aperture area thus increasing with whistle cross sectional area for whistles of the same scale 56 60 Applying the physics of high pressure jets exiting circular apertures a doubling of velocity and gas concentration at a fixed point in the whistle mouth would require a quadrupling of either aperture area or absolute pressure A quartering of absolute pressure would be compensated by a quadrupling of aperture area the velocity decay constant increases approximately with the square root of absolute pressure in the normal whistle blowing pressure range In reality trading pressure loss for greater aperture area may be less efficient as pressure dependent adjustments occur to virtual origin displacement 34 Quadrupling the width of an organ pipe aperture at a fixed blowing pressure resulted in somewhat less than a doubling of velocity at the flue exit 67 Steam aperture profile Gas flow rate and thus sound level is set not only by aperture area and blowing pressure but also by aperture geometry Friction and turbulence influence the flow rate and are accounted for by a discharge coefficient A mean estimate of the discharge coefficient from whistle field tests is 0 72 range 0 69 0 74 41 Mouth vertical length cut up The mouth length cut up that provides the highest sound level at a fixed blowing pressure varies with whistle scale and some makers of multi tone whistles therefore cut a mouth height unique to the scale of each resonant chamber maximizing sound output of the whistle 68 Ideal cut up for whistles of a fixed diameter and aperture width including single bell chime compartments at a fixed blowing pressure appears to vary approximately with the square root of effective length 69 Antique whistle makers commonly used a compromise mouth area of about 1 4x whistle cross sectional area If a whistle is driven to its maximum sound level with the mouth area set equal to the whistle cross sectional area it may be possible to increase the sound level by further increasing the mouth area 70 71 Frequency and distance Sound pressure level decreases by half six decibels with each doubling of distance due to divergence from the source an inversely proportional relationship Distinct from the inverse square law applicable to sound intensity rather than pressure Sound pressure level also decreases due to atmospheric absorption which is strongly dependent upon frequency lower frequencies traveling farthest For example a 1000 Hz whistle has an atmospheric attenuation coefficient one half that of a 2000 Hz whistle calculated for 50 percent relative humidity at 20 degrees Celsius This means that in addition to divergent sound dampening there would be a loss of 0 5 decibel per 100 meters from the 1000 Hz whistle and 1 0 decibel per 100 meters for the 2000 Hz whistle Additional factors affecting sound propagation include barriers atmospheric temperature gradients and ground effects 72 73 74 Terminology edit Acoustic length 75 or effective length 76 is the quarter wavelength generated by the whistle It is calculated as one quarter the ratio of speed of sound to the whistle s frequency Acoustic length may differ from the whistle s physical length 77 also termed geometric length 78 depending upon mouth configuration etc 30 The end correction is the difference between the acoustic length and the physical length above the mouth The end correction is a function of diameter whereas the ratio of acoustic length to physical length is a function of scale These calculations are useful in whistle design to obtain a desired sounding frequency Working length in early usage meant whistle acoustic length i e the effective length of the working whistle 79 but recently has been used for physical length including the mouth 80 Loudest and largest whistles editLoudness is a subjective perception that is influenced by sound pressure level sound duration and sound frequency 73 74 High sound pressure level potential has been claimed for the whistles of Vladimir Gavreau 81 who tested whistles as large as 1 5 meter 59 inch diameter 37 Hz 82 A 20 inch diameter ring shaped whistle Ultrawhistle patented and produced by Richard Weisenberger sounded 124 decibels at 100 feet 83 The variable pitch steam whistle at the New York Wire Company in York Pennsylvania was entered in the Guinness Book of World Records in 2002 as the loudest steam whistle on record at 124 1dBA from a set distance clarify used by Guinness 84 The York whistle was also measured at 134 1 decibels from a distance of 23 feet 12 A fire warning whistle supplied to a Canadian saw mill by the Eaton Cole and Burnham Company in 1882 measured 20 inches in diameter four feet nine inches from bowl to ornament and weighed 400 pounds The spindle supporting the whistle bell measured 3 5 inches diameter and the whistle was supplied by a four inch feed pipe 85 86 Other records of large whistles include an 1893 account of U S President Grover Cleveland activating the largest steam whistle in the world said to be five feet at the Chicago World s Fair 87 88 The sounding chamber of a whistle installed at the 1924 Long Bell Lumber Company Longview Washington measured 16 inches diameter x 49 inches in length 89 The whistle bells of multi bell chimes used on ocean liners such as the RMS Titanic measured 9 12 and 15 inches diameter 90 The whistle bells of the Canadian Pacific steamships Assiniboia and Keewatin measured 12 inches in diameter and that of the Keewatin measured 60 inches in length 91 92 A multi bell chime whistle installed at the Standard Sanitary Manufacturing Company in 1926 was composed of five separate whistle bells measuring 5 x15 7 x 21 8x 24 10 x 30 and 12 x36 inches all plumbed to a five inch steam pipe 93 The Union Water Meter Company of Worcester Massachusetts produced a gong whistle clarify composed of three bells 8 x 9 3 4 12 x 15 and 12 x 25 inches 94 Twelve inch diameter steam whistles were commonly used at light houses in the 19th century 95 It has been claimed that the sound level of an Ultrawhistle would be significantly greater than that of a conventional whistle 96 but comparative tests of large whistles have not been undertaken Tests of small Ultrawhistles have not shown higher sound levels compared to conventional whistles of the same diameter 70 See also editTrain horn Train whistleReferences edit nbsp Wikimedia Commons has media related to Steam whistles Chanaud Robert 1970 Aerodynamic whistles Scientific American 222 223 40 46 Bibcode 1970SciAm 222a 40C doi 10 1038 scientificamerican0170 40 Jones Ray 2003 The Lighthouse Encyclopedia Globe Pequot Press ISBN 0 7627 2735 7 Miller s Steam Boiler Alarm and Water Gage lincolnarchives us 2007 09 08 Archived from the original on 2008 03 28 Stuart Robert 1829 Historical and Descriptive Anecdotes of Steam Engines and of their Inventors and Improvers London Wightman and Cramp p 301 Ommundsen Peter 2007 Pre 1830 steam whistles Horn and Whistle 117 14 Wood Nicholas 1838 A Practical Treatise on Rail roads and Interior Communication in General Making of the modern world Longman Orme Brown Green amp Longmans p 340 a b Pringle R E Parkes J 1839 The causes and means of prevention of steam boat accidents Mechanics Magazine 31 262 a b Stretton C E 1903 The Locomotive Engine and Its Development A Popular Treatise on the Gradual Improvements Made in Railway Engines Between 1803 and 1903 Weale s scientific and technical series Crosby Lockwood Ross David 2004 The Willing Servant A History of the Steam Locomotive Tempus p 42 ISBN 0 7524 2986 8 Russell John Scott 1841 A Treatise on the Steam Engine Edinburgh Adam and Charles Black 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Patent 2755767 High power generators of sounds and ultra sounds US Patent 2678625 Resonant sound signal device US Patent 2013291784 Directional Isophasic Toroidal Whistle a b US Patent 4429656 Toroidal shaped closed chamber whistle US Patent 4686928 Toroidal whistle Fagen Ed 1996 Technical talk about flue pipes cavities and Helmholtz resonators Horn and Whistle 71 8 Bangham Larry 2002 The Resonator Whistle Steam in the Garden 66 and 67 via Horn and Whistle 101 12 15 a b c d Liljencrants Johan 2006 End correction at a flue pipe mouth Tohyama M 2011 Sound and Signals Berlin Springer Verlag 389 pp a b Ommundsen Peter 2003 Effects of pressure on whistle frequency Horn and Whistle 101 18 Science Magazine Volume 2 No 46 December 21 1883 page 799 a b BIRCH A D BROWN D R DODSON M G SWAFFIELD F 1984 The Structure and Concentration Decay of High Pressure Jets of Natural Gas Combustion Science and Technology 36 5 6 Informa UK Limited 249 261 doi 10 1080 00102208408923739 ISSN 0010 2202 Elliott Brian S 2006 Compressed Air Operations Manual New York McGraw Hill ISBN 0 07 147526 5 Crocker Malcolm J 1998 Handbook of Acoustics New York Wiley ISBN 0 471 25293 X Lerner L S 1996 Physics for Scientists and Engineers Physics Series Vol 1 Jones and Bartlett ISBN 978 0 86720 479 7 Heisler S I 1998 The Wiley Engineer s Desk Reference A Concise Guide for the Professional Engineer Wiley pp 266 267 ISBN 978 0 471 16827 0 a b Menon E Sashi 2005 Piping Calculations Manual New York McGraw Hill Ommundsen Peter 2012 Whistle steam and air consumption Horn and Whistle 127 4 a b Gilbert T M 1897 A test of the steam consumption of a locomotive whistle Sibley Journal of Engineering 11 108 110 a b Ommundsen Peter 2013 Steam whistle harmonics and whistle length Horn and Whistle 129 31 33 Fletcher N H 1974 08 01 Nonlinear interactions in organ flue pipes The Journal of the Acoustical Society of America 56 2 Acoustical Society of America ASA 645 652 Bibcode 1974ASAJ 56 645F doi 10 1121 1 1903303 ISSN 0001 4966 Fletcher N H Douglas Lorna M 1980 09 01 Harmonic generation in organ pipes recorders and flutes The Journal of the Acoustical Society of America 68 3 Acoustical Society of America ASA 767 771 Bibcode 1980ASAJ 68 767F doi 10 1121 1 384815 hdl 1885 213247 ISSN 0001 4966 Safarik Pavel Novy Adam Jicha David Hajsman Miroslav 2015 12 31 On the Speed of Sound in Steam Acta Polytechnica 55 6 Czech Technical University in Prague Central Library 422 doi 10 14311 ap 2015 55 0422 hdl 10467 67225 ISSN 1805 2363 Soo S L 1989 Particulates And Continuum Multiphase Fluid Dynamics Multiphase Fluid Dynamics Taylor amp Francis ISBN 978 0 89116 918 5 Ommundsen Peter 2017 Estimating speed of sound in steam Horn and Whistle 136 17 a b Pipe sensitivity Johan Liljencrants on organs pipes air supply 2011 10 30 Liljencrants Johan 2006 Q value of a pipe resonator Ommundsen Peter 2004 Whistle mouth area and lip height in relation to manifold pressure Horn and Whistle 103 7 8 Atchison Topeka and Santa Fe Railway 1925 engineering drawing published 1984 Horn and Whistle 13 12 13 Ommundsen Peter 2005 Effect of mouth size on frequency of a single bell chime whistle Horn and Whistle 110 29 30 a b Ommundsen Peter 2007 Observations on whistle cut up and frequency Horn and Whistle 116 4 7 Airchime Manufacturing Company May 15 1960 Steam Whistle Installation Adjustments Horn and Whistle Magazine No 25 page 37 July August 1986 Nathan Manufacturing Company 1910 December 3 General Information Pattern 30146 a b Ommundsen Peter 2007 Factors to consider in whistle slot width prescriptions Horn and Whistle 115 6 8 Ommundsen Peter 2006 Observations on whistle resonance frequency Horn and Whistle 112 7 8 Barry Harry and Peter Ommundsen 2012 Whistle frequency differences on steam vs compressed air Horn and Whistle 126 5 6 Patent 2784693 Burrows Lewis M published 1957 column 5 lines 29 31 a b c Ommundsen Peter 2005 Effect of slot width on whistle performance Horn and Whistle 109 31 32 a b Barry Harry and Peter Ommundsen 2015 Whistle sound levels revisited Horn and Whistle 133 4 5 Patent 2784693 Burrows Lewis M published 1957 column 5 lines 30 34 Barry Harry 2002 Sound levels of my whistles Horn and Whistle 98 19 Weisenberger Richard 1983 The loudest whistle Horn and Whistle 6 7 9 Carruthers James A 1984 More on loudest sounds Horn and Whistle 10 6 Elias I 1962 Evaluation and Applications of the Levavasseur Whistle 1962 IRE National Convention IEEE pp 36 42 doi 10 1109 irenc 1962 199221 Ausserlechner Hubert J Trommer Thomas Angster Judit Miklos Andras 2009 08 01 Experimental jet velocity and edge tone investigations on a foot model of an organ pipe The Journal of the Acoustical Society of America 126 2 Acoustical Society of America ASA 878 886 Bibcode 2009ASAJ 126 878A doi 10 1121 1 3158935 ISSN 0001 4966 PMID 19640052 Patent 2784693 Burrows Lewis M published 1957 column 5 lines 20 28 Rhodes Tom 1984 Building a steamboat whistle Live Steam November 42 44 a b Ommundsen Peter 2008 The Levavasseur toroidal whistle and other loud whistles Horn and Whistle 119 5 Ommundsen Peter 2009 Whistle engineering questions Horn and Whistle 121 26 27 Fagen Edward 2005 Whistles as Sound Sources Horn and Whistle 107 18 24 a b Fagen Edward 2005 Whistles as Sound Sources Part 2 Horn and Whistle 108 35 39 a b Piercy J E Tony F W Embleton 1979 Sound propagation in the open air In Harris Cyril M ed Handbook of Noise Control Second ed New York McGraw Hill Talbot Smith Michael 1999 Audio Engineer s Reference Book 2nd ed Oxford Focal ISBN 0 7506 0386 0 Serway Raymond A 1990 Physics for Scientists and Engineers Philadelphia Saunders College Publishing ISBN 0 03 005922 4 Rossing T D 1990 The Science of Sound Addison Wesley Publishing Company ISBN 978 0 201 15727 7 Fahy F J 2000 Foundations of Engineering Acoustics Elsevier Science ISBN 978 0 08 050683 8 Hadley H E 1926 Everyday Physics Macmillan and Company limited Weisenberger Richard 1986 Mathematics for the whistle builder Horn and Whistle 23 10 16 Altmann Jurgen 2001 Acoustic weapons a prospective assessment Science amp Global Security 9 3 Informa UK Limited 165 234 Bibcode 2001S amp GS 9 165A doi 10 1080 08929880108426495 ISSN 0892 9882 S2CID 31795453 Gavreau V 1968 Infrasound Science Journal 4 33 37 Weisenberger Richard 1983 The loudest whistle Horn and Whistle 6 7 9 Loudest whistle steam Guinness World Records 2002 12 12 The New York Times May 26 1882 The Chronicle a journal devoted to the interests of insurance Vol xxix page 346 1882 Crofford Maurice 2001 The Rich Cut Glass of Charles Guernsey Tuthill College Station Texas A amp M University Press p 64 ISBN 978 1 58544 148 8 FEATURES OF THE OPENING People Likely to Jump When the President Touches the Button at Chicago The New York Times April 27 1893 Drummond Michael 1996 Steam whistle buffs abuzz over Big Benjamin The daily News of Longview Washington December 21 reprinted in Horn and Whistle 75 8 9 Fagen Ed 1997 Titanic s whistle blow a bit less than titanic Horn and whistle 75 8 11 Barry Harry 1983 The Assiniboia steam whistle Horn and Whistle 4 13 14 Barry Harry 1998 A survey of large whistles Horn and Whistle 79 6 7 Louisville Herald June 8 1926 Barry Harry 2002 The twelve inch diameter three bell Union Water meter gong whistle Horn and Whistle 98 14 15 Clarke F L 1888 Fog and fog signals on the pacific coast Overland Monthly 12 353 For example Weisenberger Richard 1986 Build an eight inch super whistle an introduction to the toroidal whistle Horn and Whistle 25 4 6 Further reading editFagen Edward A 2001 The Engine s Moan American Steam Whistles New Jersey Astragal Press ISBN 1 931626 01 4 Retrieved from https en wikipedia org w index php title Steam whistle amp oldid 1195263374, wikipedia, wiki, book, books, library,

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