๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Temperature rise in a superconducting cable during overload

โœ Scribed by P.H. Melville


Publisher
Elsevier Science
Year
1975
Tongue
English
Weight
391 KB
Volume
15
Category
Article
ISSN
0011-2275

No coin nor oath required. For personal study only.

โœฆ Synopsis


Approximate calculations are presented for the temperature rise and temperature fluctuation in an ac superconducting cable during current overload. The calculations are for a cable, which it is intended will remain superconducting throughout the overload. These show that because of the low value of T c and low Jc niobium-titanium is not a suitable material to use. Niobium-zirconium with a 1 mm copper backing will carry continuous overloads of up to x 9 and a first cycle overload of up to x 11 provided it is fully stabilized against flux jumps. (Normal surface current rating = 4 x 104 A m-1). Niobium-tin can in principle carry very large overloads, but the limiting factors are its poor mechanical properties, the difficulty in producing thick layers of the material, and stabilization.

Temperature rise in a superconducting cable during overload P. H. Melville

Under normal operating conditions the hysteresis losses for most designs of ac superconducting cable are not sufficient to raise the conductor temperature much above the temperature of the supercritical helium used for cooling. However, when the cable is carrying an overload, the conductor temperature can rise appreciably. Obviously if the cable is to remain superconducting throughout the overload the temperature cannot be permitted to rise too far. In the work reported here estimates are given for the temperature rise for various overloads to establish the maximum overload that can be carried by different types of superconductor.


๐Ÿ“œ SIMILAR VOLUMES


Instability in kiloamp class a.c. superc
โœ K. Funaki; M. Nakashima; M. Iwakuma; M. Takeo; K. Yamafuji ๐Ÿ“‚ Article ๐Ÿ“… 1991 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 356 KB

In kiloamp (kA) class superconducting cables for a.c. use, where each strand does not have an insulation layer, the quench current in 60 Hz operation was found to be no more than 50% of the d.c. critical current, even on the load line. The degradation in the 60 Hz quench current of the kA class cabl

Temperature rise in biological tissue du
โœ R. Marchesini; S. Andreola; H. Emanuelli; E. Melloni; A. Schiroli; P. Spinelli; ๐Ÿ“‚ Article ๐Ÿ“… 1985 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 603 KB

Few data are available about temperature distribution in tissue during Nd:YAG laser irradiation. To study the heat distribution that produces tissue coagulation, we used a thermographic camera aimed orthogonally to the laser beam axis to obtain thermal maps. Immediately after surgical resection, spe

Temperature rise inside pastes during hy
โœ A.M. Alshamshi ๐Ÿ“‚ Article ๐Ÿ“… 1994 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 450 KB

This paper examines the influence of 30% fly ash and 60% ground granulated blast-furnace slag (ggbs) as partial cement replacement materials on temperature evolution during hydration at three different ambient temperatures as follows: 20ยฐC, 35~ and 4ffC. The apparatus was designed to allow for dissi

Electromagnetic properties of large capa
โœ Kazuo Funaki; Masataka Iwakuma; Masakatsu Takeo; Norio Takahashi; T. Fujii; Taka ๐Ÿ“‚ Article ๐Ÿ“… 1992 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 371 KB

We have designed and fabricated a 1000 kVA-class power transformers with iron core in a room-temperature space to test the electromagnetic properties of kA-class superconducting cables as the secondary winding. The test cable is a triply-stacked multi-strand (6x6x6) type. The elementary strand has 1