Yttrium barium
copper oxide, often
abbreviated YBCO, is a family of crystalline chemical compounds, famous for
displaying "High-temperature superconductivity". It includes the
first material ever discovered to become superconducting above the boiling
point of liquid nitrogen (77 K) at about 90 K. Many YBCO compounds have the
general formula YBa2Cu3O7x (also known as
Y123), although materials with other Y:Ba:Cu ratios exist, such as YBa2Cu4Oy
(Y124) or Y2Ba4Cu7Oy (Y247).
All materials
developed before 1986 became superconducting only at temperatures near the
boiling points of liquid helium (Tb = 4.2 K) or liquid hydrogen (Tb = 20.28 K) — the highest being Nb3Ge at 23 K. The significance of the
discovery of YBCO is the much lower cost of the refrigerant used to cool the
material to below the critical temperature.
Many possible applications of this and related high temperature superconducting materials have been discussed. For example, superconducting materials are finding use as magnets in magnetic resonance imaging, magnetic levitation, and Josephson junctions. (The most used material for power cables and magnets is BSCCO.)
YBCO has yet to be used in many applications involving superconductors for two primary reasons:
It should be noted that cooling materials to liquid nitrogen temperature (77 K) is often not practical on a large scale, although many commercial magnets are routinely cooled to liquid helium temperatures (4.2 K).
…. the properties
of YBCO are influenced by the crystallization methods used… However, new
possibilities have been opened since the discovery that trifluoroacetic acid (TFA)),
a source of fluorine, prevents the formation of the undesired barium carbonate
(BaCO3). Routes such as CSD (chemical solution
deposition) have opened a wide range of possibilities, particularly in the
preparation of long length YBCO tapes. This route lowers the temperature
necessary to get the correct phase to around 700 °C. This, and the lack of
dependence on vacuum, makes this method a very promising way to get scalable
YBCO tapes.
Although YBa2Cu3O7 is a well-defined chemical compound with a specific structure and
stoichiometry, materials with fewer than seven oxygen atoms per formula unit
are non-stoichiometric compounds. The structure of these materials depends on
the oxygen content. This non-stoichiometry is denoted by the YBa2Cu3O7-x in the chemical formula. When x = 1, the O(1) sites in the Cu(1)
layer are vacant and the structure is tetragonal. The tetragonal form of YBCO
is insulating and does not superconduct. Increasing the oxygen content slightly
causes more of the O(1) sites to become occupied.
Applications
Many possible applications of this and related high temperature superconducting materials have been discussed. For example, superconducting materials are finding use as magnets in magnetic resonance imaging, magnetic levitation, and Josephson junctions. (The most used material for power cables and magnets is BSCCO.)
YBCO has yet to be used in many applications involving superconductors for two primary reasons:
- First, although single crystals of YBCO have
a very high critical current density, polycrystals have a very low
critical current density: only a small current can be passed while
maintaining superconductivity. This problem is due to crystal grain
boundaries in the material. When the grain boundary angle is greater than
about 5°, the supercurrent cannot cross the boundary. The grain boundary
problem can be controlled to some extent by preparing thin films via CVD
or by texturing the material to align the grain boundaries.
- A second problem limiting the use of this
material in technological applications is associated with processing of
the material. Oxide materials such as this are brittle, and forming them
into wires by any conventional process does not produce a useful
superconductor. (Unlike BSCCO, the powder-in-tube process does not give
good results with YBCO.)
It should be noted that cooling materials to liquid nitrogen temperature (77 K) is often not practical on a large scale, although many commercial magnets are routinely cooled to liquid helium temperatures (4.2 K).
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