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Video: Superconducting Levitating Train

superconductor wire What is a superconductor?

Superconductor applications

Glossary of Terms

Cross section of a 5% carbon-doped MgB2 wire taken with polarized light.
Courtesy of U.S. Dept. of Energy's Ames Laboratory

What is a superconductor?
Superconductors are materials that conduct electricity with no resistance. This means that, unlike the more familiar conductors such as copper or steel, a superconductor can carry a current indefinitely without losing any energy. They also have several other very important properties, such as the fact that no magnetic field can exist within a superconductor.

Superconductors already have drastically changed the world of medicine with the advent of MRI machines, which have meant a reduction in exploratory surgery. Power utilities, electronics companies, the military, transportation, and theoretical physics have all benefited strongly from the discovery of these materials.

A brief history of superconductors

The first discovery of a superconductive material took place in 1911 when a Dutch scientist named Heike Kammerlingh Onnes, who was also the first person to liquefy helium, and reached temperatures as low as 1.7 kelvin (K).

In the 1960s, two unrelated discoveries made closely together ushered in a new era in which practical superconducting devices were developed and commercialized: one was the discrovery of NbTi superconductor, which provided the first material for the practical manufacture of superconducting wire and shaped components; the second was the Josephson junction, which continues to provide the basis for a variety of unique electronic devices.

To this day, the largest successful applications of superconductors remains the powerful electromagnets used in Magnetic Resonance Imaging (MRI) systems (over 22,000MRI magnets made) and research magnets, and the RF accelerator cavities used in high energy physics experiments. Courtesy of Paul E. Debevec   Courtesy of Paul E. Debevec Courtesy of Paul E. Debevec

Despite the enormous success of NbTi and similar materials, even broader application of superconductors has been restricted by the requirement for cooling to very low temperatures (1.5 - 5K)using liquid helium.

In late 1986 J. Georg Bednorz and K. Alexander Müller, two researchers at IBM's Zurich Lab, discovered announced an oxide material that superconducted at 30K. These two researchers were awarded the Nobel Prize in Physics 1987 for their work. Then, in 1987, Paul Chu at the University of Houston discovered YBCO, which became a superconductor at just 90K. Because 90K can be reached using liquid nitrogen, a common industrial refrigerant, these discoveries opened up for the first time the potential for a much wider range of devices. Over the next several months, discoveries of BSCCO and TBCCO brought the transition temperature of superconductors up to 127K.

This discovery of these "High Temperature Superconductors" sparked vast interest, and an entire industry dedicated to the research and commercial development of these materials and their applications has emerged. Today, an enormous range of devices are under development for both low and high temperature superconductors.

International competition is strong in these materials, and current efforts involve many facets of the electronics, communications, power, medical technology, transportation, military, and materials processing industries.

Applications of Superconductivity
Legend:   Commercial Emerging
High Tc Low Tc Various Tcoptions    
Medical Magnet Resonance Imaging (MRI) MRI
Various Nuclear Magnetic Resonance (NMR) NMR (inserts)
Industrial MRI, NMR, etc.  
  Magnetic Separation Magnetic Separation
    Magnetic Shielding
    Sensors and Transducers
Electric Power   Power Cables
    Generators
    Motors
    Fault Current Limiters
    Flywheel Energy Storage
    Magnetic Energy Storage (SMES)
    Transformers
    Fusion Energy
Transportation   Magnetically levitated trains
    Marine Propulsion (motors)
    Marine Propulsion (magnetohydrodynamic)
Physics Particle Accelerators  
  Magnets  
  Plasma/Fusion Research  
Electronics SQUIDs SQUIDs
    High Speed Computing
    Quantum Computing
  Sensors  
    Circuitry
  Filters  

Glossary of Terms

1G First generation HTS wires, formed by extrusion of BSCCO, coated with metal.
2G Second generation HTS wires, formed by depositing YBCO onto a metal substrate.
AC Alternating current. Also ac.
Alpha channeling A cooling technique that removes alpha particles from a fusion reactor while capturing their energy.
Ampere Unit of electric current. Also Amp or A.
Anneal To heat and then slowly cool a material to reduce brittleness. Annealing of ceramic superconductors usually follows sintering and is done in an oxygen-rich atmosphere to restore oxygen lost during calcination. The oxygen content of a ceramic superconductor is critical. For example, YBCO with 6.4 atoms of oxygen will not superconduct. But YBCO with 6.5 atoms will. (from superconductors.org)
ASD Adjustable-speed drive
B Magnetic Flux Density, also referred to as magnetic field. In Units of Teslas. Related to H via B = mH.
BCS theory Theory developed to explain the properties of Type 1 superconductors by John Bardeen, Leon Cooper, and Robert Schrieffer. Key elements of the theory are Cooper Pairs of electrons. (from superconductors.org)
Bi-2212 Bi2Sr2CaCu2Ox. Also known as BSCCO – 2212. See BSCCO.
Bi-2223 (Bi, Pb)2Sr2Ca2Cu3Ox. Also known as BSCCO – 2223. See BSCCO.
Biaxially textured Textured along two axes.
Borocarbides Superconducting borocarbides are compounds containing both boron and carbon in combination with rare-earth and transition elements; some of which exhibit the unusual ability to return to a normal, non-superconductive state at temperatures below TC. (from superconductors.org)
BSCCO HTS compound containing Bi, Sr, Ca, Cu, O, and typically including Pb for the best possible TC . Also known as Bi-2223 or (Bi,Pb)2Sr2Ca2Cu3O10,. Used in 1G HTS wires.
BSCCO-2223 See Bi-2223
Buffer Material put in place between metal substrate and superconductor material to prevent contamination and provide texturing.
CCPPC Continuous Columnar Pinning Centers. Type of pinning center produced by radiation damage, gives continuous columns of damage. See Flux Pinning.
Ceramics Ceramic superconductors are inorganic compounds formed by reacting a metal with oxygen, nitrogen, carbon or silicon. Ceramics are typically hard, brittle, heat-resistant materials formed by a process known as solid-state reaction. (from superconductors.org)
Ceria CeO2 Cerium oxide. Buffer material for HTS. See buffer.
chemical solution deposition A technique for depositing thin films by dipping or spraying a substrate with a solution.
CIC Cable-in-conduit.
closed-cycle refrigeration Cooling system in which the cooling substance is recycled through the system and reused.
Coated conductor A superconductor formeby depositing a superconducting film layer on a substrate. See thin film and thick film.
conductor Conductors are materials that contain movable charges (electrons or holes) of electricity. When an electric potential difference is impressed across separate points on a conductor, the mobile charges within the conductor are forced to move, and an electric current between those points appears in accordance with Ohm's law. While many conductors are metallic, there are non-metallic conductors as well, including all plasmas.
Cooper pairs Two electrons in a material that couple together as a result of interacting with the lattice. Main cause of superconductivity in BCS theory.
Critical current Maximum current through a material that allows it to remain in the superconducting state. Also IC.
Critical fields Minimum and maximum magnetic fields between which a material is superconducting. Also Hc1 (minimum) and Hc2 (maximum)
Critical temperature Maximum temperature at which a material is superconducting. Also known as transition temperature.
CRT Composite reaction textured
Cryocooler Also see pulse tube cryocooler
Cryogenics A branch of physics and engineering that studies and produces very low temperatures (below –150 °C, –238 °F or 123 K) and the behavior of materials at those temperatures.
Current density Electrical current per cross-sectional area. Measured in Amps/m2. Also J. See JC.
CVD Chemical vapor deposition, A method of forming dense structural parts or coatings using the decomposition of relatively high vapor pressure gases.
DAC Diamond anvil cell, used to apply pressure to a sample in the laboratory, often to increase the TC of a superconductor. It is composed of 2 diamonds and a stainless steel gasket containing a small chamber full of fluid. Hydrostatic forces in excess of a million atmospheres can be brought to bear on a sample suspended within the fluid.
DC Direct current
DC sputtering A sputtering deposition in which direct current is applied to a cathode in a vacuum tube. Used for thin film deposition.
Defects Nano-particles, dislocations, stacking faults, or columnar defects in the crystal structure that can increase HTS critical current. See Flux Pinning.
Diamagnetism The ability of a material to repel a magnetic field. Superconductors exhibit strong diamagnetism below TC. In a few rare compounds, a material may become superconductive at a higher temperature than the point at which diamagnetism appears. But, as a rule, the onset of strong diamagnetism is one of the most reliable ways to ascertain when a material has become superconductive. (from superconductors.org)
Dilution refrigerator Cryogenic device using helium to cool systems to micro-Kelvin temperatures.
Doping A process of adding impurities to the crystal lattice of a semiconductor in order to control its properties. Some heavily-doped semiconductors are capable of superconductivity.
E-beam evaporation Electron beam evaporation. Method by which a substance is vaporized by bombarding it with electrons.
Electropolishing Sometimes called reverse electroplating, this is an electrochemical process which polishes a metal surface by removing a microscopic amount of material from the work piece. Used on some radio frequency particle accelerator cavities.
Expitaxial A thin film with the same crystal structure as the substrate it was grown on. The property of superconductor materials to grow this way is used to get films with good grain alignment.
Ex-situ "Out of place." In wire manufacturing, when the superconducting material is formed, then put into place. Compare In-situ.
Fault Current Limiter Device to reduce a fault current in an electrical power system.
FCL See fault current limiter
Flux lattice Magnetic flux lines in a superconductor arrange themselves into a regular lattice.
Flux lines Lines of magnetic flux inside a superconductor. Also known as vortices because the current spirals around them. These form a lattice structure, and flow through the material as the magnetic or electric field changes. The motion of flux lines dissipates energy and destroys the superconductor state. As the external magnetic field increases, the number of lines will increase, until the superconductor is full of them and the superconductor state is destroyed.
Flux Pinning Preventing the movement of flux lines within a superconductor. This prevents destruction of superconductivity, and can be achieved by defects in the superconductor structure.
Flux Qubit Micro-metre sized loops of superconducting metal interrupted by a number of Josephson junctions. Used to perform computations with qubits.
Fluxon Quantized line of magnetic flux.
Four-point Probe The most common method of determining the TC of a superconductor. Wires are attached to a material at four points with a conductive adhesive. Through two of these points a voltage is applied and, if the material is conductive, a current will flow. Then, if any resistance exists in the material, a voltage will appear across the other two points in accordance with Ohm’s law (voltage equals current times resistance). When the material enters a superconductive state, its resistance drops to zero and no voltage appears across the second set of points. By using the four-point method, instead of just two points, resistance in the adhesive and wires can be ignored; as the second set of points do not themselves conduct any current and can, therefore, only reflect what voltage exists across the body of the material. (from superconductors.org)
Free path length Mean distance a electron will travel through a material without interacting.
FRP Fiber-reinforced plastic
FWHM Full width at half maximum
giant flux creep Large thermal decay of current observed in high Tc superconductors (HTS).
Grain Single crystal of superconductor material.
Grain Alignment Orientation of grains to one another, less than 4o angle is best for superconductor.
Grain Boundary Boundary between superconductor grains.
GZO Gadolinium zirconium oxide, a buffering/texturing material used in some IBAD processes.
H Henry. Magnetic field strength in units of Amps/meter. Related to B (magnetic flux density in teslas) via B = mH.
Hastelloy Trade name of commercial Ni-based high temperature alloys.
Hc2 Upper critical field.
High-Temperature Superconductors High temperature superconductor – ceramic materials that superconduct with a Tc of 30 K or greater. Some examples are YBCO and BSCCO. Also known as HTS.
HOP Operating magnetic field.
HTS See High-temperature superconductors.
I Current expressed in amps
I2R Joule heating, the product of the current squared times the resistance of a conductor.
IBAD Ion beam assisted deposition. A technique for depositing thin superconductor films. An ion beam is directed at an angle towards the substrate to grow textured buffer layers.
IC See critical current.
Ic Critical current of a superconductor, the maximum amount of current that can flow below a fixed electric field or resistivity criterion.
IFL I = current, FL = full load. Full load current
Index value n The n-value describes the relationship of the voltage drop across the wire to the applied current. (from amsuper.com)
In-situ "In place." In wire manufacturing, when the precursors to the superconductor are put into place before being reacted to form the superconducting compound. Compare Ex-Situ.
IPP Independent power producer
IR Current times the resistance of a conductor; equals the voltage drop along the conductor.
Irreversibility line The line which separates the mixed state region of the H-T plane of a type 2 superconductor into two regions, below which the critical current density has a finite value and turns to zero.
ISD Inclined substrate deposition, Method for depositing a buffer onto a substrate at an angle in order to get good texturing.
I-V Current-voltage
Jc Critical current density. Maximum current density in a material that allows it to remain in the superconducting state.
JE Engineering critical current – critical current density calculated for the entire wire, not just the superconductor material. Includes effects of buffers, substrate.
Josephson Junction A thin layer of insulating material sandwiched between 2 superconducting layers. Electrons tunnel through this non-superconducting region via the Josephson effect. Key components in superconductor electronics and computing. (from superconductors.org)
Laser Ablation  
Large-grain HTS HTS produced in relatively large thicknesses, composed of large crystals. JC is much lower than in thin film coated conductors, although it can be increased with the use of chemically-created pinning centers. Large grain HTS is frequently used to make permanent magnets. It is difficult to make long lengths of large grain HTS, and it is therefore not a candidate for power transmission.
LHC Large Hadron Collider at CERN
LL Load losses
Lorentz microsuperconductoropy A simple method by which the domain walls of magnetic materials can be made visible in a qualitative fashion.
LPE Liquid phase epitaxy
LTS Low temperature superconductor, metallic materials with a TC of less than 30 K
Maglev Magnetic levitation, i.e. for trains. Some use electromagnets, there are superconductor magnet prototypes.
Magnesium diboride A cheap, "off-the-shelf" chemical compound that can be made into a superconductor. Magnesium diboride becomes superconducting at -234 °C (39K) - much higher than previously observed in relatively simple and readily available compounds, and between conventional LTS and HTS temperatures. Also MgB2.
Magnetic Field  
Magnetic Flux  
Magnetoencephalography Imaging of the electromagnetic field of the brain.
MCP Melt Cast Processed,
MEG See Magnetoencephalography – imaging of the electromagnetic field of the brain.
Meissner effect The Meissner effect is the effect by which a weak magnetic field decays rapidly to zero in the interior of a superconductor. The distance to which the field is active is known as the london penetration depth. This active exclusion of magnetic fields is distinct from perfect diamagnetism, as the magnetic field will be zero inside the superconductor regardless of what it was before the material became superconducting. The Meissner effect is one of the defining features of superconductivity, and its discovery served to establish that the onset of superconductivity is a phase transition. It was discovered by Walther Meißner and Robert Ochsenfeld in 1933. (wikipedia)
MFCL Matrix fault current limiter. See Fault Current Limiter.
M-G Motor-generator
MHD Magnetohydrodynamic – Having to do with the study of magnetic fluids, i.e. plasma.
MILD multiple-in-line-damage. See flux pinning.
MOCVD Metallorganic Chemical Vapor Deposition, producing a thin film by depositing a precursor material evaporated onto a substrate.
MOD Metal organic deposition. Precursor material deposited in liquid form onto substrate, baked to form YBCO.
MOV Metal oxide varistor
MPMG Melt powder melt growth
MRI Magnetic resonance imaging. The body is exposed to a strong magnetic field, which aligns hydrogen atoms in the body's water and fat molecules. Radio frequency pulses make the atoms absorb and release energy that can be detected and displayed graphically by a computer.
multi-plume A method for manufacturing superconducting materials where the superconductors are sprayed onto the metal substrate.
multi-turn A method for manufacturing superconducting wire where the process is sped up by applying the superconducting material to multiple turns of the wire at the same time.
Naming superconductors For cuprate superconductor. The scheme chosen uses four numbers. The first denotes the number of insulating layers between adjacent conducting blocks. The second represents the number of spacing layers between identical CuO2 blocks. The third gives the number of layers that separate adjacent CuO2 planes within the conducting block. And, the fourth is the number of CuO2planes within a conducting block.
Nano-structure A nanostructure is an intermediate size between molecular and microscopic (micrometer-sized) structures.
Nd-422 Nd4Ba2Cu2Ox
NLL No-load loss
NMR Nuclear magnetic resonance
NQR Nitrogen nuclear quadrupole resonance. The use of the resonant frequency of atoms to determine the molecular structure of a material.
OD Outer diameter
OPIT Oxide-powder-in-tube process for manufacturing 1G wire.
PCS Persistent current switch
PCS Power conditioning system
perovskites A family of Type 2 superconductor. These metal-oxide ceramics normally have a ratio of 2 metal atoms to every 3 oxygen atoms.
physical vapor deposition A fabrication technique for depositing a thin film upon a substrate. A conventional physical vapor deposition (PVD) technique is sputtering. In the sputtering method, materials are bombarded with an ionized inert gas, such as argon, and are deposited onto the substrate..
Pinning See Flux Pinning
PIT Powder in tube (conductor)
plasma In physics and chemistry, plasma is typically an ionized gas, and is usually considered to be a distinct phase of matter in contrast to solids, liquids, and gases because of its unique properties.
PLD See Pulsed laser deposition
Pulsed Laser Deposition An efficient method to produce thin films by utilizing a technique called laser ablation.
Pulse Tube Cryocooler A device which produces low temperatures. It is a closed system that uses an oscillating pressure at one end to generate an oscillating gas flow in the rest of the system. This gas flow can carry heat away from a low temperature point if the conditions are right. The prime advantage of Pulse Tube cryocoolers over Stirling cryocoolers is that they have no moving parts in the low temperature region.
p-YSZ Polycrystalline yttrium-stabilized zirconia
QMG Quench melt growth
Qubit Quantum bit. A unit of data stored physically in a quantum system.
quatratran quasiparticle trapping transistor - see supercurrent transistor
RABiTS Rolling assisted biaxially textured substrates. Method for creating textured metal substrate for 2G wires by adding a buffer layer between the nickel substrate and YBCO, in order to prevent the texture of the YBCO from being destroyed during processing under oxidizing atmospheres.
RE Rare earth element (such as La, Nd, Sm, Eu, Gd, etc.). Often added to superconductors to improve their flux pinning abilities.
RE-123 oxides 123 compound formed with a rare earth instead of yttrium. See YBCO.
Reactive sputtering A technique where a deposited film is formed by chemical reaction between the target material and a gas which is introduced into the vacuum chamber. Oxide and nitride films are often fabricated using reactive sputtering. The composition of the film can be controlled by varying the relative pressures of the inert and reactive gases. See thin film deposition.
Reel-to-reel Continuous wire manufacturing. (Can theoretically handle any length wire.)
rf Radio frequency
rms Root mean square
RFSQ Rapid Single Flux Quantum superconducting circuit.
SBCO Sm-Ba-Cu-O compound.
SBIR Small business innovative research program (From the US government.)
Self-epitaxial A material that grows on itself with the same crystal structure.
Self-field The self field is the magnetic field that is induced when there is finite current flowing in a wire. In the case of critical current measurements, the self field is the magnetic field that is induced in a straight piece of wire that is being measured.
SFCL Superconducting Fault Current Limiter,
SFQ Single flux quantum
Slot-die coating A method of applying a liquid material to a substrate. In this process, liquid is forced out from a reservoir through a slot by pressure and transferred to a moving web.
SMES Superconducting magnetic energy storage
sol-gel A colloidal suspension that can be gelled to form a solid. The resulting porous gel then is chemically purified and fired at high temperatures into high purity oxide materials. The gel can be modified with a number of dopants to produce unique properties in the resultant glass unattainable by other means. It can be used in ceramics manufacturing processes, as an investment casting material, or as a means of producing very thin films of metal oxides for various purposes.
Spin coating A procedure used to apply uniform thin films to flat substrates. An excess amount of solvent is placed on a substrate, which is then rotated at high speed in order to spread the fluid. Rotation is continued until the desired thickness of the film is achieved. The applied solvent is usually volatile, and evaporates as well as pouring off the edge of the substrate.
spray pyrolysis Liquid droplets containing precursors are injected into a thermal reactor. The solvent evaporates and the precursors react to form the product.
SPTL Superconducting power transmission line
Sputtering A process whereby atoms in a solid target material are ejected into the gas phase due to bombardment of the material by energetic ions. It is commonly used for thin-film deposition and analytical techniques.
SQUID Superconducting quantum interference device. A sensitive magnetic instrument usually used for medical diagnostics.
Substrate The surface or base layer on which a superconducting thin film is grown.
Superconductivity A state where a material exhibits no electrical resistance and excludes the inner magnetic field.
Superconductor An element, inter-metallic alloy, or compound that will conduct electricity without resistance below a certain temperature. Once set in motion, current will flow forever in a closed loop of superconducting material. This applies only to direct current (DC) electricity and to finite amounts of current. All known superconductors are solids. superconductor can be classified into Type 1 and Type 2, and can be categorized further by their dimensionality. Most are 3-D, but some compounds, like surface-doped NaWO3 and some organic superconductors are 2-D. Li2CuO2 and single-walled carbon nano-tubes have shown rare 1-D superconductivity. In addition to repelling magnetic fields, enhanced thermal conductivity, higher optical reflectivity and reduced surface friction are also properties of superconductors. (from superconductors.org)
Superconductor A material capable of displaying superconductivity.
Superconductor/PM Superconductor/permanent magnet
SuperconductorFCL Superconductive fault current limiter
supercurrent transistor The superconducting transistor, or quatratran, is made of very thin layers of the superconductor niobium, insulation, and aluminum, which is a non-superconducting metal. When a voltage is applied to one of the superconducting layers, the increase in energy causes electrons from the aluminum layer to stream into a superconducting layer, causing a gain, or change in current, 70 times larger than the amount of current applied.
synchronous condenser Fundamentally an AC synchronous motor that is not attached to any driven equipment. Its field is controlled by a voltage regulator to either generate or absorb reactive power as needed by the system. It operates at full leading power factor and puts VARs onto the network as required to support a system’s voltage or to maintain the system power factor at a specified level. The condenser’s installation and operation are identical to large electric motors.
T 1. Tesla, a unit for magnetic flux density. 2. May also refer to temperature, as in TC
TC See critical temperature.
TEM Transmission electron microscope or microscopy
Tesla Unit for magnetic flux density (B). Equal to one weber per square meter or one newton per ampere-meter.
Texturing Crystal grain alignment – a textured buffer layer is used to grow an aligned superconductor layer.
TFA Tri-flouro-acetate, a material used for MOD.
Thermal runaway A condition in which the current for a fully charged nickel-cadmium battery rises out of proportion to the impressed-voltage level. This condition is caused when heat from oxygen recombination causes the battery's voltage to drop as it gets hot.
Thick Film Coated Conductor 3 to 10 microns thick. A thick film coated conductor, say 7 microns thick would be expected to carry about 10 times the current carried by a thin film conductor, but it typically carries only a bit more current than thin film. Thin film coated conductor, about 1 micron thick, is the leading candidate for power transmission applications. It presently has Jc in the range of 1 to 2 Meg Amps per cm*2. A thin film tape, 1 cm wide and 1 micron thick might carry 100 Amps.
Thin Film Coated Conductor Thin film coated conductor, about 1 micron thick, is the leading candidate for power transmission applications. It presently has Jc in the range of 1 to 2 Meg Amps per cm*2. A thin film tape, 1 cm wide and 1 micron thick might carry 100 Amps.
Thin Film Deposition A method of fabricating ceramic superconductors to more precisely control the growth of the crystalline structure to eliminate grain boundaries and achieve a desired Tc. This can involve Pulsed-Laser Deposition (PLD) or Pulsed-Electron Deposition (PED) of the superconductor material onto a substrate. The substrate and possible buffer layers support the film and can increase the Jc of the HTS directly in contact with it. The part of the HTS nearest to the supporting layer carries high Jc. Further away from the support (less than a micron) Jc falls off very rapidly.A variation of this technique can be used to increase the Tc of a superconductor by growing it on a supporting material with a smaller interatomic spacing. The supporting material acts as a molecular "girdle" to compress the atomic lattice of the superconductor, thereby raising its transition temperature.Superconductive tape/wire is made using thin film deposition technology.(from superconductors.org)
Tl-1223 (Tl, Pb)(Ba, Sr)2Ca2Cu3Ox
Tokamak Fusion reactor design which uses a magnetic field to confine plasma to a closed torus.
Transport phenomena Any of various mechanisms by which particles or quantities move from one place to another. Three common examples of transport phenomena are diffusion, convection, and radiation.
Type 1 superconductor The Type 1 category of superconductors is mainly comprised of metals and metalloids that show some conductivity at room temperature. They require incredible cold to slow down molecular vibrations sufficiently to facilitate unimpeded electron flow in accordance with what is known as BCS theory. (from superconductors.org)
Type 2 superconductor Also known as the "hard" superconductors. They have higher TC than Type 1 and their transition from a normal to a superconducting state is gradual across a region of "mixed state" behavior. This allows some penetration of external magnetic fields. All metallic compounds or alloys (except for vanadium, technetium and niobium), including the perovskites, BSCCO.
Ultra-capacitor Sometimes called a supercapacitor, an ultra-capacitor is an electrochemical capacitor that has an unusually large amount of energy storage capability relative to its size. These are of particular interest for hybrid vehicles and as supplemental storage for battery electric vehicles.
Ultraconductor Materials known as ultraconductors™ display room-temperature resistance many orders of magnitude lower than the best metallic conductors. Examples of these materials include oxidized atactic polypropylene (OAPP) and other polymers. Since ultraconductor™ is a colloquial term, these materials might better be described as "hyperconductors". The Meissner effect cannot be confirmed in them, but strong (giant) diamagnetism is in evidence. Some of them may actually find acceptance in high-current applications ahead of superconductors as a result of their low losses at ambient temperatures and pressures.
vapor-liquid-solid (VLS) process A process for fabricating single crystal fibers such as silicon carbide with diameters ranging from 0.1-10 μm and lengths of 100 mm.
vortices See flux lines.
XLPE Cross-linked polyethylene (industry designation for dry insulated high voltage lines).
Y-123 YBa2Cu3Ox (see also YBCO)
Y-211 Y2BaCuO5
YBCO YBa2Cu3O7-d (also Y-123, YBCO-123, YBa2Cu3O7) A high temp superconductor material developed in 1991 by Fujikara. Used in 2G wires.
YSZ Yttrium-stabilized zirconia. A buffering/texturing material used in some IBAD processes.
Z Impedence (complex [ac] impedance of a circuit or component consisting of a resistive and a reactive part).

More superconductivity terms can be found at:

Superconductors.org Glossary

American Superconductor's HTS Wire Glossary

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