The state in which liquid helium creeps up the walls of a beaker and siphons itself out
A Rollin film about 30 nanometres thick flows over any barrier at the same rate.
Science · Physics
Discovered 1937
Physics — low-temperature and condensed matter physics
Superfluidity is the state in which a liquid flows with exactly zero viscosity, so that once set moving it never stops. It was found in helium-4 cooled below 2.17 K, the lambda point, in experiments completed in 1937 and published simultaneously in January 1938 by Pyotr Kapitsa in Moscow and by John F. Allen and Don Misener in Cambridge. The liquid does impossible-looking things: it climbs the walls of its container in a film and siphons itself out, it squeezes through pores no ordinary liquid can enter, it conducts heat so well that it stops boiling and goes glassy, and it can be made to squirt upwards in a fountain when a heater is switched on. Helium-3, whose atoms are fermions, becomes superfluid too, but only at around two thousandths of a degree above absolute zero.
The state in which liquid helium creeps up the walls of a beaker and siphons itself out
A Rollin film about 30 nanometres thick flows over any barrier at the same rate.
Reached below the lambda point of 2.17 K, where the liquid suddenly stops bubbling
Its thermal conductivity becomes so enormous that no hot spots form to nucleate bubbles.
Demonstrated by the fountain effect, where a heater makes the liquid spurt upward (1938)
The thermomechanical effect: heat drives flow through a fine capillary.
Found in 1937 by Kapitsa in Moscow and by Allen and Misener in Cambridge at the same time (1937)
Their papers appeared back to back in Nature on 8 January 1938.
In the rarer helium isotope it requires about 2.5 millikelvin and paired fermionic atoms (1972)
Osheroff, Lee and Richardson found it at Cornell; Cooper-like pairs make bosons of fermions.
What cools the 1,232 dipole magnets of CERN's biggest ring to 1.9 K
Its huge heat conductivity carries away energy no ordinary coolant could.