The resistivity of a conductor decreases with decreasing temperature. In the case of copper, the relationship between resistivity and temperature is approximately linear over a wide range of temperatures
The resistivity of copper deviates from a linear function at low temperature.
The resistivity of copper does not vanish at absolute zero. Instead, it levels off in what is known as the residual resistance. Copper has a residual resistance of 0.020 nΩ m.
Resistance has two causes
The latter cause results in "ordinary resistance". The former results in residual resistance. To get rid of the residual resistance …
Heike Kamerlingh Onnes, Leiden, 1911
Surprise, surprise, surprise. At low temperatures, instead of zero residual resistance Kammerlign-Onnes discovered zero resistance; now know as superconductivity (originally called supraconductivity). Kammerlign-Onnes thought his equipment was experiencing a short circuit. Second paper of 1913 introduced the word "supraconductivity"
About half the elements are superconducting under the right conditions: low temperature, high pressure, amorphous phase, thin films. Elements that are good conductors are not superconductors. The element with the highest transition temperature is niobium 9.25 K. Rhodium is the superconductor with the lowest known transition temperature of 325 μK. Neither gold nor bismuth is superconducting, but Au2Bi is at 1.8 K
Persistent current: no decrease of induced current could be observed in the superconductive state for the duration of the experiment (1 hour)
It is uncanny to see the influence of these "permanent" currents on a magnetic needle. You can feel almost tangibly how the ring of electrons in the wire turns around, around, around — slowly and almost without friction.
Find a good quote from Onnes' Nobel speech
Magnetism destroys superconductivity
Type I vs. Type II superconductors,
Demonstration of the Meisner Effect. Superconductors are also superdiamagnetic. Superdiamagnetism: Fritz, Heinz London, Oxford explained the Meisner effect in terms of surface current, produced a magnetic field within the superconductor that opposed the field imposed from outside
|element||Tc (K)||element||Tc (K)|
BCS Theory, Cooper Pairs, two electrons with an attractive interaction always form a bound pair (in the presence of a filled Fermi sphere). Worked out of a cramped office on the 3½ floor in an annex of the Institute for Advanced Studies. They jokingly called it the "Institute for Retarded Studies".
three families of high-temperature, non-intermetallic superconductors
high temperature superconductivity
Bednorz, Müller. Zeitschrift fur Physik. Condensed Matter. April 1986.
Which is correct?
In addition to the savings in cost resulting from the displacement of liquid helium by liquid nitrogen for cooling, it is now apparent that superconductivity applications with more inexpensive refrigerants — or eventually no refrigerant at all — are possible. The race for new superconductors with higher Tc continues. The current record (1997) is for a the mercury barium calcium copper oxide (HBCCO) compound which superconducts at about 134 K without pressure. Under hydrostatic pressure, this compound superconducts at 164 K, which is Freon temperature
Doping C60 with alkali metals like potassium or rubidium leads to superconducting compounds with transition temperatures of 18-20 K and 20-30 K, respectively, 1991 may people, 20 hexagons and 12 pentagons like a football (soccer ball), 60 carbon atoms
|year||Tc (K)||material, comments|
|1911||4.154||Hg (superconductivity discovered)
Heike Kamerlingh-Onnes, Georg Holst
Heike Kamerlingh Onnes
|9.25||Nb (pure element with highest critical temperature)
G.F. Hardy and J.K. Hulm
University of Chicago
Physical Review. Vol. 89 No. 4 (February 1953): 884.
Physical Review. Vol. 93 No. 5 (March 1954): 1004–1016.
B.T. Matthias, T.H. Geballe, S. Geller, E. Corenzwit
Bell Telephone Laboratories
Physical Review. Vol. 95 No. 6 (September 1954): 1435.
|1973||23.2||Nb3Ge (classical superconductor with highest critical temperature)
J.R. Gavaler, M.A. Janocko, C. J. Jones
Westinghouse Research Laboratories
Applied Physics Letters. Vol. 23 No. 8 (October 1973): 480-482.
Journal of Applied Physics. Vol. 46 (July 1974): 3009-3013.
|1986||30||La1.85Ba0.15CuO4 (high temperature superconductivity discovered)
Johann Georg Bednorz, Karl Alex Müller
IBM Zurich Research Laboratory
Zeitschrift für Physik B. Vol. 64 (September 1986): 189-193.
|1987||93||YBa2Cu3O7 (liquid nitrogen barrier broken)
Wu, Ashburn, Torng, Hor, Meng, Gao, Huang, Wang, and Chu
University of Alabama and University of Houston
Physical Review Letters. Vol. 58 No. 9 (March 1987): 908-910.
H. Maeda, Y. Tanaka, M. Fukutomi, T. Asano
Tsukuba Magnet Laboratory
Japanese Journal of Applied Physics. Vol. 27 (January 1988): 209.
Z.Z. Sheng, A.M. Hermann
University of Arkansas
Nature. Vol. 332 (March 1988): 138.
A. Schilling, M. Cantoni, J.D. Guo, H.R. Ott
Laboratorium für Festkörperphysik
Nature. Vol. 363 (May 1993): 56-58.
|1995||138||Hg0.8Tl0.2Ba2Ca2Cu3O8.33 (highest critical temperature of any material)
P. Dai, B.C. Chakoumakos, G.F. Sun, K.W. Wong, Y. Xin, and D.F. Lu
University of Kansas, Lawrence
Physica C. Vol. 243 No. 3&4 (February 1995): 201-206.
|1994||164||HgBa2Ca2Cu3O8 (under 30 GPa pressure)
Gao, Xue, Chen, Xiong, Meng, Ramirez, Chu, Eggert, and Mao
University of Houston
Physical Review B. Vol. 50 No. 6 (August 1994): 4260–4263.
large scale vs. small scale
Pyotr Kapitsa, Soviet Union
Helium I vs. helium II. Helium II is a different phase than helium I
Helium liquefies under normal pressures at 4.2 K. From 4.2 K to 2.17 K it behaves like many other liquids, although it has an exceptionally low surface tension and is extremely transparent. Below 2.2 K it behaves quite differently.
The mechanisms for this phase transition, and the details of the superfluidity in 4He and 3He, are very different. 4He has an even number of constituent particles (protons, electrons, and neutrons), which makes it a boson, meaning it is governed by Bose-Einstein statistics. At low temperatures, all the bosons in a sample will want to occupy the same quantum-mechanical ground state, forming a Bose-Einstein condensate. This condensate is responsible for the superfluid behavior of 4He below Tλ = 2.17 K.
In contrast, 3He is a fermion, since it has one less neutron than 4He. Fermions obey the Pauli exclusion principle, which says that in a sample of many identical fermions, no two can occupy the same quantum-mechanical state. Bose-Einstein condensation is ruled out for 3He, so another mechanism is needed to explain its superfluid behavior. That mechanism is provided by the Bardeen-Cooper-Schrieffer (BCS) theory.