Superconducting wires are electrical wires made of superconductive material. When cooled below their transition temperatures, they have zero electrical resistance. Most commonly, conventional superconductors such as niobium–titanium are used, but high-temperature superconductors such as YBCO are entering the market.
Superconducting wire's advantages over copper or aluminum include higher maximum current densities and zero power dissipation. Its disadvantages include the cost of refrigeration of the wires to superconducting temperatures (often requiring cryogens such as liquid nitrogen or liquid helium), the danger of the wire quenching (a sudden loss of superconductivity), the inferior mechanical properties of some superconductors, and the cost of wire materials and construction.
Its main application is in superconducting magnets, which are used in scientific and medical equipment where high magnetic fields are necessary.
The construction and operating temperature will typically be chosen to maximise:
Critical temperature Tc, the temperature below which the wire becomes a superconductor
Critical current density Jc, the maximum current a superconducting wire can carry per unit cross-sectional area (see images below for examples with 20 kA/cm2).
Superconducting wires/tapes/cables usually consist of two key features:
The superconducting compound (usually in the form of filaments/coating)
A conduction stabilizer, which carries the current in case of the loss of superconductivity (known as quenching) in the superconductoring material.
The current sharing temperature Tcs is the temperature at which the current transported through the superconductor also starts to flow through the stabilizer. However, Tcs is not the same as the quench temperature (or critical temperature) Tc; in the former case, there is partial loss of superconductivity, while in the latter case, the superconductivity is entirely lost.
Low-temperature superconductor (LTS) wires are made from superconductors with low critical temperature, such as Nb3Sn (niobium–tin) and NbTi (niobium–titanium).
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Les oxydes mixtes de baryum, de cuivre et d'yttrium, notés YBaCuO ou YBCO, sont des céramiques connues pour être des supraconducteurs à haute température et ont été les premiers matériaux identifiés présentant un phénomène de supraconductivité au-dessus de la température d'ébullition de l'azote liquide, soit (). Ils ont été découverts en 1986 par Johannes Georg Bednorz et Karl Alexander Müller. La plupart de ces oxydes ont pour formule générale , souvent notée Y123, mais d'autres présentent des rapports Y:Ba:Cu différents, tels que (Y124), (Y247), ou encore (Y222).
Un supraconducteur à haute température (en anglais, high-temperature superconductor : high- ou HTSC) est un matériau présentant une température critique de supraconductivité relativement élevée par rapport aux supraconducteurs conventionnels, c'est-à-dire en général à des températures supérieures à soit . Ce terme désigne en général la famille des matériaux de type cuprate, dont la supraconductivité existe jusqu'à . Mais d'autres familles de supraconducteurs, comme les supraconducteurs à base de fer découverts en 2008, peuvent aussi être désignées par ce même terme.
A superconducting magnet is an electromagnet made from coils of superconducting wire. They must be cooled to cryogenic temperatures during operation. In its superconducting state the wire has no electrical resistance and therefore can conduct much larger electric currents than ordinary wire, creating intense magnetic fields. Superconducting magnets can produce stronger magnetic fields than all but the strongest non-superconducting electromagnets, and large superconducting magnets can be cheaper to operate because no energy is dissipated as heat in the windings.
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