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Drinking bird

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Drinking bird
Drinking bird about to dip its beak in the water
ClassificationHeat engines
ApplicationToy, scientific demonstration
Fuel sourceHeat transfer
ComponentsBulbs, tube, axle, support
Invented1945 / much earlier than 1920

Drinking birds, also known as dunking birds, drinky birds, water birds, or dipping birds[1][2][3] are toy heat engines that mimic the motions of a bird drinking from a water source. They are sometimes incorrectly considered examples of a perpetual motion device.[4]

Construction and materials

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A drinking bird consists of two glass bulbs joined by a glass tube (the bird's neck/body). The tube extends nearly all the way into the bottom bulb, and attaches to the top bulb but does not extend into it.

The space inside the bird contains a fluid, usually colored for visibility. (This dye might fade when exposed to light, with the rate depending on the dye/color).[5] The fluid is typically dichloromethane (DCM), also known as methylene chloride.[6][7] Earlier versions contained trichlorofluoromethane.[7] Miles V. Sullivan's 1945 patent suggested ether, alcohol, carbon tetrachloride, or chloroform.[8]

Air is removed from the apparatus during manufacture, so the space inside the body is filled by vapor evaporated from the fluid.[8] The upper bulb has a "beak" attached which, along with the head, is covered in a felt-like material.[8] The bird is typically decorated with paper eyes, a plastic top hat, and one or more tail feathers. The whole device pivots on a crosspiece attached to the body.

Heat engine steps

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Video of a Drinking Bird

The drinking bird is a heat engine that exploits a temperature difference to convert heat energy to a pressure difference within the device, and performs mechanical work. Like all heat engines, the drinking bird works through a thermodynamic cycle. The initial state of the system is a bird with a wet head oriented vertically.

The process operates as follows:[9]

  1. The water evaporates from the felt on the head.
  2. Evaporation lowers the temperature of the glass head (heat of vaporization).
  3. The temperature decrease causes some of the dichloromethane vapor in the head to condense.
  4. The lower temperature and condensation together cause the pressure to drop in the head (governed by Equations of state).
  5. The higher vapor pressure in the warmer base pushes the liquid up the neck.
  6. As the liquid rises, the bird becomes top heavy and tips over.
  7. When the bird tips over, the bottom end of the neck tube rises above the surface of the liquid in the bottom bulb.
  8. A bubble of warm vapor rises up the tube through this gap, displacing liquid as it goes.
  9. Liquid flows back to the bottom bulb (the toy is designed so that when it has tipped over the neck's tilt allows this). Pressure equalizes between top and bottom bulbs.
  10. The weight of the liquid in the bottom bulb restores the bird to its vertical position.
  11. The liquid in the bottom bulb is heated by ambient air, which is at a temperature slightly higher than the temperature of the bird's head.

If a glass of water is placed so that the beak dips into it on its descent, the bird will continue to absorb water and the cycle will continue as long as there is enough water in the glass to keep the head wet. However, the bird will continue to dip even without a source of water, as long as the head is wet, or as long as a temperature differential is maintained between the head and body. This differential can be generated without evaporative cooling in the head; for instance, a heat source directed at the bottom bulb will create a pressure differential between top and bottom that will drive the engine. The ultimate source of energy is the temperature gradient between the toy's head and base; the toy is not a perpetual motion machine.

Physical and chemical principles

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Video The Engineering of the Drinking Bird

The drinking bird is an exhibition of several physical laws and is therefore a staple of basic chemistry and physics education. These include:

  • The dichloromethane with a low boiling point (39.6 °C (103.3 °F) under standard pressure po = 105 Pa – as the drinking bird is first evacuated, partially filled and sealed, the pressure and thus the boiling point in the drinking bird will be different), gives the heat engine the ability to extract motion from low temperatures. The drinking bird is a heat engine that works at room temperature.
  • The combined gas law, which establishes a proportional relationship between temperature and pressure exerted by a gas in a constant volume.
  • The ideal gas law, which establishes a proportional relationship between number of gas particles and pressure in a constant volume.
  • The Maxwell–Boltzmann distribution, which establishes that molecules in a given space at a given temperature vary in energy level, and therefore can exist in multiple phases (solid/liquid/gas) at a single temperature.
  • Heat of vaporization (or condensation), which establishes that substances absorb (or give off) heat when changing state at a constant temperature.
  • Torque and center of mass.
  • Capillary action of the wicking felt.
  • Wet-bulb temperature: The temperature difference between the head and body depends on the relative humidity of the air.

The operation of the bird is also affected by relative humidity.[10][11]

By using a water-ethanol mixture instead of water, the effect of different rates of evaporation can be demonstrated.[12]

By considering the difference between the wet and dry bulb temperatures, it is possible to develop a mathematical expression to calculate the maximum work that can be produced from a given amount of water "drunk". Such analysis is based on the definition of the Carnot heat engine efficiency and the psychrometric concepts.[13]

The drinking bird may also be considered to be an entropy engine driven by the difference of the entropy of liquid water and the entropy of water vapor dispersed in air, that is, the sum of the entropy of evaporation of pure water plus the entropy of dilution of water vapor in air. The evaporation of water is an endothermic process requiring the input of thermal energy or a positive enthalpy flow from the environment. Since a spontaneous process requires a negative change in Gibbs free energy, the positive enthalpy has to be overcome by the large entropy increase.

History

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By the 1760s (or earlier) German artisans had invented a so-called "pulse hammer" (Pulshammer). In 1767 Benjamin Franklin visited Germany, saw a pulse hammer, and in 1768, improved it.[14] Franklin's pulse hammer consisted of two glass bulbs connected by a U-shaped tube; one of the bulbs was partially filled with water in equilibrium with its vapor. Holding the partially filled bulb in one's hand would cause the water to flow into the empty bulb.[15] In 1872, the Italian physicist and engineer Enrico Bernardi combined three Franklin tubes to build a simple heat motor that was powered by evaporation in a way similar to the drinking bird.[16]

In 1881 Israel L. Landis got a patent for a similar oscillating motor.[17] A year later (1882), the Iske brothers got a patent for a similar motor.[18] Unlike the drinking bird, the lower tank was heated and the upper tank just air-cooled in this engine. Other than that, it used the same principle. The Iske brothers during that time got various patents on a related engine which is now known as Minto wheel.

A Chinese drinking bird toy dating back to 1910s~1930s named insatiable birdie is described in Yakov Perelman's Physics for Entertainment.[1] The book explained the "insatiable" mechanism: "Since the headtube's temperature becomes lower than that of the tail reservoir, this causes a drop in the pressure of the saturated vapours in the head-tube ..."[1] It was said in Shanghai, China, that when Albert Einstein and his wife, Elsa, arrived in Shanghai in 1922, they were fascinated by the Chinese "insatiable birdie" toy.[19]

In addition, the Japanese professor of toys, Takao Sakai, from Tohoku University, also introduced this Chinese toy.[20]

Arthur M. Hillery got a US patent in 1945. Arthur M. Hillery suggested the use of acetone as working fluid.[21] It was again patented in the US by Miles V. Sullivan in 1946.[8] He was a Ph.D. inventor-scientist at Bell Labs in Murray Hill, NJ, USA.[8][22][4] Robert T. Plate got a US Design patent in 1947, that cites Arthur M. Hillery's patent.[23]

  • Israel L. Landis 1881[17]
    Israel L. Landis 1881[17]
  • Iske Brothers 1881[18]
    Iske Brothers 1881[18]
  • Arthur M. Hillery, 1944[21]
    Arthur M. Hillery, 1944[21]
  • Miles V. Sullivan 1945[8]
    Miles V. Sullivan 1945[8]
  • Robert T. Plate 1947
    Robert T. Plate 1947
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The drinking bird has been used in many fictional contexts. Drinking birds have been featured as plot elements in the 1951 Merrie Melodies cartoon Putty Tat Trouble and the 1968 science fiction thriller The Power. In S4E11 of the comedy series Arrested Development, a delusional character hears the voice of God speaking through a drinking bird.[24]

In Australian contemporary playwright John Romeril's play The Floating World, drinking birds are a symbolic prop which represent the progression of Les' insanity.[25]

In season 7 episode 7 of animated sitcom The Simpsons titled "King-Size Homer" Homer uses a drinking bird to press the Y key on his nuclear control computer, eventually leading to a nuclear meltdown. The bird eventually returns two seasons later in the episode "Das Bus".

Alternative design

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In 2003 an alternative mechanism was devised by Nadine Abraham and Peter Palffy-Muhoray of Ohio, USA, that utilizes capillary action combined with evaporation to produce motion, but has no volatile working fluid. Their paper "A Dunking Bird of the Second Kind",[26] was submitted to the American Journal of Physics, and published in June 2004. It describes a mechanism which, while similar to the original drinking bird, operates without a temperature difference. Instead it utilizes a combination of capillary action, gravitational potential difference and the evaporation of water to power the device.

This bird works as follows: it is balanced such that, when dry, it tips into a head-down position. The bird is placed next to a water source such that this position brings its beak into contact with water. Water is then lifted into the beak by capillary action (the authors used a triangular sponge) and carried by capillary action past the fulcrum to a larger sponge reservoir which they fashioned to resemble wings. When enough water has been absorbed by the reservoir, the now-heavy bottom causes the bird to tip into a head-up position. With the beak out of the water, eventually enough water evaporates from the sponge that the original balance is restored and the head tips down again. Although a small drop in temperature may occur due to evaporative cooling, this does not contribute to the motion of the bird. The device operates relatively slowly with 7 hours 22 minutes being the average cycle time measured.

See also

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References

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  1. ^ a b c Perelman, Yakov (1972) [1936]. Physics for Entertainment. Vol. 2. pp. 175–178. ISBN 978-1401309213.
  2. ^ American Physical Society (2012). "Insatiable Birdie". American Physical Society, with permission of the Hyperion(Reprint edition).
  3. ^ Exploratorium Teacher Institute (1993-07-27). "Exhibit-Based Energy Teaching at the Exploratorium" (PDF). US Department of Energy Office of Scientific and Technical Information: 3. doi:10.2172/6421909. Retrieved 2010-03-03. {{cite journal}}: Cite journal requires |journal= (help) (cover page URL)
  4. ^ a b "Miles V. Sullivan [..] is a member of the Photolithography Group in the Bipolar IC ... He is probably best known as the inventor of the “perpetually” drinking bird novelty." Bell Laboratories record: Volume 52 1974
  5. ^ Guy, The Souvenir (9 February 2015). "Drinking Birds and Hand Boilers – Why these Retro Souvenirs are Still So Popular". Souvenirbuyers.com. Retrieved 30 January 2022.
  6. ^ "How Does a Dippy Bird Work?". Science.howstuffworks.com. 5 April 2001.
  7. ^ a b "How the Drinking Bird Science Toy Works". Thoughtco.com.
  8. ^ a b c d e f U.S. patent 2,402,463
  9. ^ Güémez, J.; Valiente, R.; Fiolhais, C.; Fiolhais, M. (December 2003). "Experiments with the drinking bird" (PDF). American Journal of Physics. 71 (12): 1257–1263. Bibcode:2003AmJPh..71.1257G. doi:10.1119/1.1603272. hdl:10316/12328. Archived from the original (PDF) on 2011-07-01. Retrieved 2012-02-19.
  10. ^ "The Dipping Happy Bird" (PDF). Archived from the original (PDF) on 2021-08-01. Retrieved 2021-08-01.
  11. ^ Güémez, J.; Valiente, R.; Fiolhais, C.; Fiolhais, M. (December 2003). "Experiments with the drinking bird". American Journal of Physics. 71 (12): 1257–1263. Bibcode:2003AmJPh..71.1257G. doi:10.1119/1.1603272. hdl:10316/12328. Retrieved 30 January 2022.
  12. ^ "The Engineering of the Drinking Bird". Retrieved 30 January 2022 – via YouTube.
  13. ^ Flórez-Orrego, Daniel. "Three hand-solved thermodynamics exercises for fun". Flórez-Orrego, Daniel. Polytechnic School, University of Sao Paulo.
  14. ^ See:
  15. ^ For videos of Franklin's pulse hammer in operation, see YouTube examples:
  16. ^ See:
  17. ^ a b "Oscillating motor". Patents.google.com. Retrieved 30 January 2022.
  18. ^ a b "US253868A - Motor - Google Patents". Google.com.
  19. ^ Alice Calaprice and Trevor Lipscombe, Albert Einstein: A Biography (Greenwood Publishing Group, 2005):86–87.
  20. ^ 酒井高男 (Takao Sakai) (February 1977). おもちゃの科学 (in Japanese). 講談社. ISBN 4061179101.
  21. ^ a b U.S. patent 2,384,168
  22. ^ "Dr. Sullivan also holds patents on several novelty items such as the well-known drinking bird." Electrochemical technology: Volume 6 1968
  23. ^ "USD146744S - Design for an activated toy bird figure - Google Patents".
  24. ^ Mitch Hurwitz (Director), Troy Miller (Director), Mitch Hurwitz (Writer), Jim Vallely (Writer), Paul Rust (Story Editor), Jim Brandon (Story Editor), Brian Singleton (Story Editor), Will Arnett (Actor), Peter Jason (Voice) (May 26, 2013). Arrested Development S4E11 Original Cut "A New Attitude" (Television production). 4 (Original Cut ed.). Netflix. 07:37 minutes in.
  25. ^ "Reading Australia: 'The Floating World' by John Romeril". www.australianbookreview.com.au. Archived from the original on 18 June 2015. Retrieved 22 May 2022.
  26. ^ Abraham, Nadine; Palffy-Muhoray, Peter (June 2004). "A dunking bird of the second kind" (PDF). American Journal of Physics. 72 (6): 782–785. Bibcode:2004AmJPh..72..782A. doi:10.1119/1.1703543. Archived from the original (PDF) on 2012-07-10. Retrieved 2012-02-19.
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