Titlebook: Stabilization of Superconducting Magnetic Systems; V. A. Al’tov,V. B. Zenkevich,V. V. Sychev Book 1977 Springer Science+Business Media New

确定方向

Combined Conductors with Forced Coolingibution, or else in the presence of a temperature gradient) for the case in which the conductor is immersed in a liquid helium tank. However, there is one special case in which the combined conductor is made hollow and the helium passes along its inner surface.

DAFT

Equilibrium and Propagation of the Normal Zone in a Close-Packed Superconducting Coil the conductor is surrounded by a large volume of liquid helium, and in the second the conductor is wound fairly tightly and it is difficult for the helium to penetrate into the inner layers. An intermediate position between these two limiting cases is occupied by various kinds of loose windings con

Hyperopia

Stability of Superconductors of the Second Kind with Respect to Flux Jumpsed the safe and reliable operation of a superconducting magnetic system in the presence of certain acceptable perturbations. Only serious mechanical and electrical damage or the stoppage of the coolant can lead to failure or disorder in such a system. However, ensuring a high degree of reliability b

G-spot

Multiple-Core Straight Conductorsd use of a single-core superconducting wire involves serious difficulties. The number of individual superconducting strands in the conductor may vary from 10–20 to several hundreds or even thousands. In addition to this the combined conductor contains normal metal; this is either a pure metal with a

减至最低

Predigest

BRIDE

Equilibrium of the Normal Zone in Combined Conductors Under Isothermal ConditionsThermal (cryostatic) stabilization is the name given to a system of protective measures preventing the transition of a superconducting device into the normal state when a normal zone appears in the superconducting coil.

Mets552

surmount

978-1-4613-4117-8Springer Science+Business Media New York 1977

Constant

Protection of Superconducting Magnetic Systemsxtremely high value. Thus in the superconducting magnetic system of the bubble chamber of the Argonne National Laboratory (USA) the stored energy amounts to 80 MJ; in the magnetic system of the bubble chamber in the National Accelerator Laboratory of the USA the energy reaches 396 MJ.