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Liquid air is air that has been cooled to very low temperatures (cryogenic temperatures), so that it has condensed into a pale blue mobile liquid. It is stored in specialized containers, such as vacuum flasks, to insulate it from room temperature. Liquid air can absorb heat rapidly and revert to its gaseous state. It is often used for condensing other substances into liquid and/or solidifying them, and as an industrial source of nitrogen, oxygen, argon, and other inert gases through a process called air separation (industrially referred to as air rectification.).
Properties
Liquid air has a density of approximately 870 kg/m (870 g/L; 0.87 g/cm). The density of a given air sample varies depending on the composition of that sample (e.g. humidity & CO2 concentration). Since dry gaseous air contains approximately 78% nitrogen, 21% oxygen, and 1% argon, the density of liquid air at standard composition is calculated by the percentage of the components and their respective liquid densities (see liquid nitrogen and liquid oxygen). Although air contains trace amounts of carbon dioxide (about 0.03%), carbon dioxide solidifies from the gas phase without passing through the intermediate liquid phase, and hence will not be present in liquid air at pressures less than 5.1 atm (520 kPa).
The boiling point of air is −194.35 °C (78.80 K; −317.83 °F), intermediate between the boiling points of liquid nitrogen and liquid oxygen. However, it can be difficult to keep at a stable temperature as the liquid boils, since the nitrogen will boil off first, leaving the mixture oxygen-rich and changing the boiling point. This may also occur in some circumstances due to the liquid air condensing oxygen out of the atmosphere.
Liquid air starts to freeze at approximately 60 K (−213.2 °C; −351.7 °F), precipitating nitrogen-rich solid (but with appreciable amount of oxygen in solid solution). Unless the oxygen is previously accommodated in the solid solution, the eutectic freezes at 50 K.
Preparation
Principle of production
The constituents of air were once known as "permanent gases", as they could not be liquified solely by compression at room temperature. A compression process will raise the temperature of the gas. This heat is removed by cooling to the ambient temperature in a heat exchanger, and then expanding by venting into a chamber. The expansion causes a lowering of the temperature, and by counter-flow heat exchange of the expanded air, the pressurized air entering the expander is further cooled. With sufficient compression, flow, and heat removal, eventually droplets of liquid air will form, which may then be employed directly for low temperature demonstrations.
The main constituents of air were liquefied for the first time by Polish scientists Karol Olszewski and Zygmunt Wróblewski in 1883.
Devices for the production of liquid air are not commercially available, and not easily fabricated.
Process of production
The most common process for the preparation of liquid air is the two-column Hampson–Linde cycle using the Joule–Thomson effect. Air is fed at high pressure (>75 atm (7,600 kPa; 1,100 psi)) into the lower column, in which it is separated into pure nitrogen and oxygen-rich liquid. The rich liquid and some of the nitrogen are fed as reflux into the upper column, which operates at low pressure (<25 atm (2,500 kPa; 370 psi)), where the final separation into pure nitrogen and oxygen occurs. A raw argon product can be removed from the middle of the upper column for further purification.
Air can also be liquefied by Claude's process, which combines cooling by Joule–Thomson effect, isentropic expansion and regenerative cooling.
Application
In manufacturing processes, the liquid air product is typically fractionated into its constituent gases in either liquid or gaseous form, as the oxygen is especially useful for fuel gas welding and cutting and for medical use, and the argon is useful as an oxygen-excluding shielding gas in gas tungsten arc welding. Liquid nitrogen is useful in various low-temperature applications, being nonreactive at normal temperatures (unlike oxygen), and boiling at 77 K (−196 °C; −321 °F).
Transport and energy storage
Main article: Cryogenic energy storageBetween 1899 and 1902, the automobile Liquid Air was produced and demonstrated by a joint American/English company, with the claim that they could construct a car that would run a hundred miles on liquid air.
On 2 October 2012, the Institution of Mechanical Engineers said liquid air could be used as a means of storing energy. This was based on a technology that was developed by Peter Dearman, a garage inventor in Hertfordshire, England to power vehicles.
See also
- Liquid nitrogen
- Liquid oxygen
- Cryogenic energy storage
- Industrial gas
- Liquefaction of gases
- Liquid nitrogen vehicle
References
- Babbage (Oct 15, 2012). "Difference Engine: End of the electric car?". The Economist. Retrieved Oct 21, 2012.
- Armarego, W. L. F.; Perrin, D. D. (16 October 1996). Purification of Laboratory Chemicals (4th ed.). Butterworth-Heinemann. ISBN 978-0750628396. LCCN 97109714. OCLC 762966259. OL 722457M.
- Kochenburger, Thomas M.; Grohmann, Steffen; Oellrich, Lothar R. (2015). "Evaluation of a Two-stage Mixed Refrigerant Cascade for HTS Cooling Below 60 K". Physics Procedia. 67: 227–232. Bibcode:2015PhPro..67..227K. doi:10.1016/j.phpro.2015.06.039.
- "Air liquefaction, "Linde Air", rectification: into new markets with new research findings". The Linde Group. Archived from the original on 27 September 2007. Retrieved 9 August 2007.
- https://uspas.fnal.gov/materials/10MIT/Lecture_2.1.pdf
- "Liquid air 'offers energy storage hope'". BBC News. 2012-10-02.
External links
- 2013-05-20 MIT Technology Review article on liquid air developments for transportation and grid energy storage