University of Houston System

Ruling L Meng

Ching-Wu Chu

Yu-Yi Xue

Yuyi Xue

Diego Alberto Ramirez

Li Gao

Y Q Wang

Highly oriented HgBa,Ca,Cu,O,on Ni-tapes with a buffer layer of Cr/Ag or Cr/(Ag&mdash;Pd) have been described with a high transition temperature are described along with, one and two step methods of manufacture.

High temperature superconducting tape and method of manufacture

A trapped field magnet formed of a high temperature type II superconductor material is disclosed. The trapped field magnet is formed of a plurality of relatively small, single-grain superconductive elements. Optimal shaped of these elements is in a regular truncated cone wherein the half cone angle is 55.degree., and the optimal orientation of each single-grain superconducting elements is an angle of .phi..sub.m with respect to the axis perpendicular to the upper and lower surface of the element, wherein the .phi..sub.m =3 sin .theta. cos .theta./(3 cos.sup.2 .theta.-1) and .theta. determines the location of the element.

Strong high-temperature superconductor trapped field magnets

Highly oriented HgBa.sub.2 Ca.sub.2 Cu.sub.3 O.sub.8+.delta. on Ni-tapes with a buffer layer of Cr/Ag or Cr/(Ag--Pd) have been described with a high transition temperature are described along with, one and two step methods of manufacture.

The present invention is a controlled vapor/solid reaction process for the synthesis of samples of bulk compositions with a structure defined by the homologous series HgBa.sub.2 Ca.sub.n-1 Cu.sub.n O.sub.2n+2+.delta. [Hg-12(n-1)n] with n=2, 3, . . . with up to 75 to 90% Hg-1212 and 65 to 75% Hg-1223 by volume, which display sharp superconducting transitions up to 135 K.

Method for synthesis of high-temperature Hg-Ba-Ca-Cu-O (HBCCO)

A trapped field magnet formed of a high temperature type II superconductor material is disclosed. The trapped field magnet is formed of a plurality of relatively small, single-grain superconductive elements. Optimal shaped of these elements is in a regular truncated cone wherein the half cone angle is 55.degree., and the optimal orientation of each single-grain superconducting elements is an angle of .phi..sub.m with respect to the axis perpendicular to the upper and lower surface of the element, wherein the .phi..sub.m =3 sin.theta.cos.theta./(3 cos.sup.2 .theta.0-1) and .theta. determines the location of the element (FIG. 3a).

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Houston, TX, United States of America

Ruling L Meng