Superconductivity

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Discussion

discovery

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


[magnify]

The resistivity of copper deviates from a linear function at low temperature.


[magnify]

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.


[magnify]

Resistance has two causes

  1. defects like …
    1. impurities
    2. grain boundaries
    3. stresses
  2. lattice ion vibrations

The latter cause results in "ordinary resistance". The former results in residual resistance. To get rid of the residual resistance …

  1. use ultrapure mercury (instead of pure gold or platinum) which is easy to distill, cooled to make a wire instead of drawn (stressed) through a die
  2. cool it to reduce vibration

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

Superconducting Transition Temperatures for Selected Elements
element Tc (K)   element Tc (K)
aluminum 1.175   0.00037 rhodium
cadmium 0.517   3.722 tin
lead 7.196   0.39 titanium
mercury 4.154   0.015 tungsten
niobium 9.25   0.2 uranium
      0.85 zinc

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.

Meisner Effect:

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

bcs theory

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".

high temperature superconductors

three families of high-temperature, non-intermetallic superconductors

  1. cuprates
  2. bismuthades
  3. fullerites

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

organic superconductors

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

magnesium diboride

Milestone Superconducting Transition Temperatures
year Tc (K) material, comments
1911 4.154 Hg (superconductivity discovered)
Heike Kamerlingh-Onnes, Georg Holst
Universiteit Leiden
1913 7.196 Pb
Heike Kamerlingh Onnes
Universiteit Leiden
after
1932?
9.25 Nb (pure element with highest critical temperature)
who
where
1932 11.5 NbC
who
where
1941 16.10 NbN
E. Justi
Berlin
1953 17.1 V3Si
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.
1954 18.05 Nb3Sn
B.T. Matthias, T.H. Geballe, S. Geller, E. Corenzwit
Bell Telephone Laboratories
Physical Review. Vol. 95, No. 6 (September 1954): 1435.
1967 20.7?1? Nb3Al0.75Ge0.25
who
where
reference
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.
1988 105 Bi2Sr2CaCu2O8
H. Maeda, Y. Tanaka, M. Fukutomi, T. Asano
Tsukuba Magnet Laboratory
Japanese Journal of Applied Physics. Vol. 27 (January 1988): 209.
1988 120 Tl2Ba2Ca2Cu3O10
Z.Z. Sheng, A.M. Hermann
University of Arkansas
Nature. Vol. 332 (March 1988): 138.
1993 133 HgBa2Ca2Cu3O8
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.

superconducting technology

large scale vs. small scale

Summary

Problems

practice

  1. Write something.
    • Answer it.
  2. Write something.
    • Answer it.
  3. Write something.
    • Answer it.
  4. Write something completely different.
    • Answer it.

statistical

  1. Very Rough Idea. The temperature at which a metal becomes superconducting varies inversely as the square root of its molecular weight. Discovered independently by E. Maxwell of the National Bureau of Standards -- NBS (now the National Institute of Standards and Technology -- NIST) and Bernard Serin of Yale University in 1950.

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