Superconductivity
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© 1998-2008 by Glenn Elert -- A Work in Progress
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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
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
- defects like …
- impurities
- grain boundaries
- stresses
- lattice ion vibrations
The latter cause results in "ordinary resistance". The former results in residual resistance. To get rid of the residual resistance …
- 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
- 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"
- "The resistance of pure mercury at helium temperatures." Comm. Leiden. 120b (28 April 1911).
- "The disappearance of the resistivity of mercury." Comm.
Leiden. 122b (27 May 1911).
- "On the sudden change in the rate at which the resistance of mercury disappears," Comm. Leiden. 124c (25 November 1911).
- "The imitation of an ampere molecular current or a permanent magnet by means
of a supraconductor." Comm. Leiden. 140b (Day Month 1914).
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 |
- The material must be cooled below a characteristic temperature, known as
its superconducting transition temperature or critical temperature (Tc).
- The magnetic field to which the material is exposed must be below a characteristic
value known as the critical magnetic
field (Hc).
- The current passing through a given cross-section of the material must be
below a characteristic level known as the critical
current density (Jc).
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:
- complete flux expulsion (field forced out when temperature drops below critical)
- complete flux exclusion (field can't penetrate when turned on below critical
temperature)
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".
- John Bardeen, Leon N. Cooper, J. Robert Schrieffer. "Microscopic Theory of Superconductivity." Physical Review. 108 (1957): 162-164.
- John Bardeen, Leon N. Cooper, J. Robert Schrieffer. "Theory of Superconductivity." Physical Review. 108 (1957): 1175-1204.
high temperature superconductors
three families of high-temperature, non-intermetallic superconductors
- cuprates
- bismuthades
- fullerites
high temperature superconductivity
Bednorz, Müller. Zeitschrift fur Physik. Condensed Matter. April 1986.
Which is correct?
- Liquid helium is 500 times more expensive than liquid nitrogen.
- With liquid nitrogen 50 times cheaper than helium and thus the promise of
commercial viability for the new materials. FERMILAB
liquid nitrogen is 50 times less expensive than helium (10 cents a liter
instead of $5 a liter). ORNL
- Michigan Technological University
"Posted on the door are Rules, Usual Procedures, Price ($0.75 / liter) …."
"The price for liquid helium from August 1, 2000 will be $3.25/liquid liter."
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
- magnetic resonance imaging (mri)
"Magnetic Resonance Imaging (MRI) is currently the most important market for
low temperature superconductors. MRI enables physicians to obtain detailed
images of the interior of the human body without surgery or exposure to ionizing
radiation. MRI devices are now available only at major hospitals and specialized
MRI centers. They are very bulky machines largely because of the amount of
thermal insulation required to keep the liquid helium from evaporating. The
amount of liquid helium to operate an MRI device costs about $30,000 per
year. It has been estimated that the use of liquid nitrogen superconducting
magnets could save $100,000 per year in overall operating costs for each
MRI device. In addition, the initial cost of the machines would be far lower,
and the physical size of the machines would be much smaller."
- microwave antennas
"Communications - Superconductors could improve capacity, coverage and quality
of service for personal communications devices, such as hand held communicators
to generate and read e-mail."
- magnetic levitation (maglev)
- maglev train
- magnetic bearings
- vibration isolation
- superconducting magnetic energy storage (SMES)
"energy is stored within a magnet that is capable of releasing megawatts of
power within a fraction of a cycle to replace a sudden loss in line power."
- fault current limiters
"A current limiter is designed to react to and absorb unanticipated power
disturbances in the utility grid, preventing loss of power to customers or
damage to utility grid equipment."
"They can limit the peak short-circuit current automatically by their transition
from the superconducting to the normal state. This means high short-circuit
capacity during normal operation and a limitation of the short-circuit currents
in case of a fault."
- power transmission cables
"Conduct electricity with little or no resistance and associated energy loss.
Can transmit much larger amounts of electricity than conventional wires of
the same size."
"Superconducting cables can provide 2 to 5 times more power than conventional
cables of the same size."
Increased capacity without the need to purchase new land for utility
right of way.
- electric motors
large industrial and marine motors over 1000 hp
"Conventional motors are made primarily of iron, which makes them heavy and
increases the frictional load seen by the motor bearings. All iron can be
eliminated when constructing superconducting electrical machines with HTS
windings. The removal of the iron teeth in the armature not only makes superconducting
motors lighter (with lower inertia), it also leaves more room for armature
copper, which lowers the electrical losses and also improves machine efficiency.
These reductions in losses result in lower operating costs than conventional
motors."
- Electric generators
lighter, higher efficiency
- transformers
"Improved energy efficiencies from smaller, lighter transformers. Reduced
environmental concerns from elimination of fire and environmental hazards.
Liquid nitrogen is safe, nonflammable, and environmentally friendly as it
is simply the liquid form of the most abundant element on earth. Using it
as a dielectric and coolant instead of oil eliminates the dangers of explosion
and contamination of the soil from leaks. An HTS transformer replaces the
copper wire coils in a conventional transformer with lower loss HTS wire.
Inexpensive and environmentally benign liquid nitrogen replaces the conventional
oil as the electrical insulation (dielectric) and provides the necessary
cooling for the HTS. More generated power can be utilized by consumers rather
than lost in the environment as heat."
"If all transformers in the United States equal to or greater than 100 MVA
were replaced with HTS transformers, the lifetime energy savings from conventional
transformer losses could account for 340 billion kWh or 10.2 billion dollars."
Summary
Problems
practice
- Write something.
- Write something.
- Write something.
- Write something completely different.
statistical
- 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.
Resources
- announcements
- ceramics
- Nobel Prize
in Physics 1987 to Bednorz & Müller "for their important
break-through in the discovery of superconductivity in ceramic materials",
Nobel Foundation
- Bulk superconductivity
at 36 K in La1.8Sr0.2CuO4.
R. J. Cava, R. B. van Dover, B. Batlogg, and E. A. Rietman. Physical
Review Letters. Vol. 58, No. 4 (26 January 1987):
408410.
- Superconductivity
at 93 K in a new mixed-phase Yb-Ba-Cu-O compound system at ambient
pressure. M. K. Wu, J. R. Ashburn, C. J. Torng, P. H. Hor, R.
L. Meng, L. Gao, Z. J. Huang, Y. Q. Wang, and C. W. Chu. Physical
Review Letters. Vol. 58 No. 9: 908-910. This was
the most cited scientific paper of 1987 and the 6th most cited of
the 1980s despite containing an intentional typo.
- Superconductivity
above 130 K in the Hg-Ba-Ca-Cu-O system. A. Schilling, et al., Nature. Vol. 363 (15 April 1993): 56-58.
- Superconductivity
up to 164 K in HgBa2Cam-1CumO2m+2+δ under quasihydrostatic pressures.
L. Gao, et al. Physical Review B. Vol. 50, No. 6
(1 August 1994) : 4260-4263.
- magnesium diboride
- commerce
- education
- magnetic leviation
- research
- miscellaneous
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