Image:2 Helium.png|thumb|Liquid helium in a cup.
Helium exists in liquid form only at extremely low temperatures. The boiling point and critical point (thermodynamics)|critical point depend on the isotope of the helium; see the table below for values. The density of liquid helium-4 at its boiling point and 1 atm is approximately 0.125 g/mL 
Helium-4 was first liquefied on 10 July 1908 by Dutch physicist Heike Kamerlingh Onnes. Liquid helium-4 is used as a cryogenic refrigerant; it is produced commercially for use in superconducting magnets such as those used in Magnetic resonance imaging|MRI or Nuclear magnetic resonance|NMR. It is liquefied using the Hampson-Linde cycle.
The temperatures required to liquefy helium are low because of the weakness of the attraction between helium atoms. The interatomic forces are weak in the first place because helium is a noble gas, but the interatomic attraction is reduced even further by quantum effects, which are important in helium because of its low atomic mass. The zero point energy of the liquid is less if the atoms are less confined by their neighbors; thus the liquid can lower its ground state energy by increasing the interatomic distance. But at this greater distance, the effect of interatomic forces is even weaker.
Because of the weak interatomic forces, helium remains liquid down to absolute zero; helium solidifies only under great pressure. At sufficiently low temperature, both helium-3 and helium-4 undergo a transition to a superfluid phase (see table below).
Liquid helium-3 and helium-4 are not completely miscible below 0.9 K at the saturated vapor pressure. Below this temperature a mixture of the two isotopes undergoes phase separation into a lighter normal fluid that is mostly helium-3, and a denser superfluid that is mostly helium-4. (This occurs because the system can lower its enthalpy by separating.) At low temperatures, the helium-4 rich phase may contain up to 6% of helium-3 in solution, which makes possible the existence of the dilution refrigerator, capable of reaching temperatures of a few millikelvin above absolute zero.
|Properties of liquid helium||Helium-4||Helium-3|
|Critical temperature||5.2 K||3.3 K|
|Boiling point at 1 atm ||4.2 K||3.2 K|
|Minimum melting pressure||25 atm||29 atm at 0.3 K|
|Superfluid transition temperature at saturated vapor pressure||2.17 K ||1 m K in zero magnetic field |
- Expansion ratio
- Liquid nitrogen
- Liquid hydrogen
- Liquid air
- Liquid oxygen
References[edit | edit source]
- cite book|title=The Properties of Liquid and Solid Helium|author=J. Wilks|year=1967|place=Oxford|publisher=Clarendon Press|isbn=0-19-851245-7
- Freezing Physics: Heike Kamerlingh Onnes and the Quest for Cold , Van Delft Dirk (2007). Edita - The Publishing House Of The Royal Netherlands Academy of Arts and Sciences. ISBN 9789069845197.
[edit | edit source]
- He-3 and He-4 phase diagrams, etc.
- Helium-3 phase diagram, etc.
- Onnes's liquifaction of helium
- Polypedilum vanderplanki
Category:Noble gases|Helium, liquid Category:Coolants Category:Cryogenics Category:Helium
ar:الهيليوم السائل fr:Hélium liquide ko:액체 헬륨 no:Flytende helium pl:Ciekły hel ru:Жидкий гелий
- ^ Liquid Helium, accessed 2010-04-02
- ^ Wilks, p. 7
- ^ cite book|author=Daniel V. Schroeder|title=An Introduction to Thermal Physics|page=141|publisher=Addison Wesley Longman|year=2000|isbn=0201380277
- ^ a b c d Wilks, p. 1.
- ^ cite journal|author=D. O. Edwards, D. F. Brewer, P. Seligman, M. Skertic, and M. Yaqub|journal=Phys. Rev. Lett.|volume=15|page=773|year=1965|title=Solubility of He3 in Liquid He4 at 0°K|doi=10.1103/PhysRevLett.15.773
- ^ Wilks, p. 244.
- ^ Wilks, pp. 474-478.
- ^ Wilks, p. 289.
- ^ cite book|author=Dieter Vollhart and Peter Wölfle|title=The Superfluid Phases of Helium 3|page=3|publisher=Taylor and Francis|year=1990