Forms
Liquid helium (He-4) is found in two forms: He-4 I and He-4 II, which share a sharp transition point at 2.1768 K at its vapor pressure. He-4 I (above this point) is a normal liquid, but He-4-II (below this temperature) is unlike any other known substance.
As it is cooled past 2.1768 K at its vapor pressure, the so-called lambda point, it becomes a superfluid known as liquid Helium II (as opposed to "normal" liquid Helium I) which has many unusual characteristics due to quantum effects; it was one of the first observed examples of quantum effects operating on a macroscopic scale. This transition takes place at much lower temperatures in Helium-3 than it does in Helium-4, as the effect relies on condensation of bosons but the nuclei of the former are fermions, which can't condense individually but must do so in bosonic pairs. Since the transformation is one of higher order, without latent heat at the lambda point, the two liquid forms never coexist.
Helium II has zero viscosity and has a heat conductivity much higher than any other substance. Furthermore, helium II exhibits a thermomechanical (fountain) effect; if two vessels containing helium II are connected by a narrow capillary and one of the two is heated a flow of helium toward the heated vessel will occur. Conversely, in the mechanocaloric effect, a forced flow of helium II through a capillary will result in cooling of the helium II leaving the capillary. Pulses of heat introduced into helium II will propagate through the liquid in the same manner as the density pulses of sound, a phenomenon which has been dubbed "second sound." Solid surfaces in contact with helium II are covered with a film 50 to 100 atoms thick, along which frictionless flow of the liquid can occur; as a result it is impossible to contain helium II in an open vessel without it flowing out over the edge. Mass transport through the helium II film takes place at a constant rate which only depends on temperature. Finally, a mass of helium II will not rotate as a unit; instead, attempts to set it rotating will induce small frictionless vortices throughout the liquid.
Precautions
Containers filled with gaseous helium at 5 to 10 K should be stored as if they contained liquid helium due to the large increase in pressure that results from warming the gas to room temperature.
External Links
Further Reading
- M. W. Wong. Prediction of a Metastable Helium Compound: HHeF.
- G. M. Chaban, J. Lundell, R. B. Gerber, J.Chem.Phys. 115 (2001) 7341. Lifetime and decomposition pathways of a chemically bound helium compound