By I. A. Parinov
The major positive factors of high-temperature superconductors (HTSC) that outline their homes are intrinsic brittleness of oxide cuprates, the layered anisotropic constitution and the supershort coherence size. bearing in mind those positive factors, this treatise provides learn into HTSC microstructure and houses, and likewise explores the probabilities of optimization of the education suggestions and superconducting compositions. The "composition-technique-experiment-theory-model," hired the following, assumes enormous HTSC defectiveness and constitution heterogeneity and is helping to attract a accomplished photograph of contemporary representations of the microstructure, energy and the comparable structure-sensitive homes of the fabrics thought of. targeted realization is dedicated to the Bi-Sr-Ca-Cu-O and Y-Ba-Cu-O households, which at present provide the main promising functions. together with quite a few illustrations and references, this monograph addresses scholars, post-graduate scholars and experts, enjoying the improvement, training and learn of recent fabrics. the hot version were up to date intensively, in particular experimental investigations and modeling conductive and elastic homes of HTC superconductors were added.
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Additional resources for Microstructure and Properties of High-Temperature Superconductors
In this case, application areas of low-temperature electronics may be sufficiently broad and include analogous-digital and digital-analogous transducers, digital SQUIDs, digital autocorrelators, generators of pseudo-accidental signals and applications connected with high levels of radiation. One of the possible directions of the superconductive quantum computer application will be connected with existence of quantum algorithm which allow effective modeling different Hamiltonians describing coupling of electrons (for example, Bardeen– Cooper–Schrieffer (BCS) Hamiltonian) on quantum computer by using NMR.
8). Then, within and outside of the sphere, T must satisfy Laplace’s equation: DT ðr Þ ¼ 0; ð1:7Þ at the boundary conditions: Tþ ¼ T À ; r ¼ R; r1 n Á ðrTÞþ ¼ r2 n Á ðrTÞÀ ; T ¼ ÀE0 Á r; ð1:8Þ r ¼ R; ð1:9Þ r ! 1; ð1:10Þ where T+ and T- are the limits of T on the sphere surface r = R taken from the outside and inside, respectively. Similarly (rT)+ and (rT)- are the limits of rT at r = R from the outside and inside, respectively, where n = r/r is the unit vector of normal. The solution of Eqs. 10) for T can be found by using the separation of variables technique .
However, there is one type of the current limiters without these shortcomings, namely superconductive fault current limiters with biasing magnetic core. Superconducting winding holds the magnetic core in magnetized state. In waiting regime, an inductivity of the system is small till will be initiated short circuit and through power winding a current flows of high amplitude. In this case, the magnetic core goes out steady state, inductivity rises leading to restriction of alternating current in net.
Microstructure and Properties of High-Temperature Superconductors by I. A. Parinov