Method of using a ferromagnet material having a high permeability and saturation magnetization at low temperatures

• US 4,894,360 A
• Filed: 05/19/1989
• Issued: 01/16/1990
• Est. Priority Date: 05/19/1989
• Status: Expired due to Fees

• Current Assignee: United States Of America As Represented By The Secretary Of The Army (Government of the United States of America)
• Original Assignee: The United States Of America As Represented By The Secretary Of The Army
• Inventors: Leupold, Herbert A.
• Primary Examiner(s): Harris, George
• Application Number:
  US07/355,582
• Time in Patent Office: 242 Days
• Field of Search: 335/216, 335/284, 505/1, 174/125.1
• US Class Current: 505/211
• CPC Class Codes: H01F 6/06 Coils, e.g. winding, insulating, terminating or casing arrangements therefor

Abstract

A ferromagnet material having a high permeability and saturation magnetizon at low temperatures is used to induce superconducting currents in a ring of a superconducting material where the ferromagnet material has a lower transition temperature than the superconductive material.

Claims

1. Method of using a ferromagnet material having a high permeability and saturation magnetization to induce superconducting currents in a ring of superconductive material where the ferromagnet material has a lower transition temperature than the superconductive material, said method including the steps of:

(A) placing a bar of a ferromagnet material in an annular ring of a superconductive material at a temperature above both the transition temperature of the ferromagnet material and the transition temperature of the superconductive material,

(B) applying an axial magnetic field of sufficient strength to saturate the ferromagnet when the ferromagnet is cooled below its transition temperature,

(C) cooling the ferromagnet to below its transition temperature without cooling the superconductive material so that the superconductive material does not become superconducting before the saturation of the ferromagnet,

(D) cooling the superconductive material to below its transition temperature,

(E) removing the ferromagnet and the applied field, and

(F) allowing the system to warm to a convenient operating temperature which must be below the transition temperature of the superconductive material.

2. Method according to claim 1 wherein the ferromagnet is cooled to below its transition temperature without cooling the superconductive material by combining heaters on the superconductive material, a thermal barrier between ferromagnet and superconductive material and refrigeration contacts on the ferromagnet.

3. Method according to claim 1 wherein the ferromagnet material is gadolinium.

4. Method according to claim 1 wherein the superconductive material is selected from the group consisting of YBa₂ Cu₃ O_7-y, Bi₂ (Ca,Sr)₃ Cu₂ O_8+y, and Tl₂ Ca₁.5 BaCu₃ O₈.5-y.

5. Method according to claim 4 wherein the superconductive material is YBa₂ Cu₃ O_7-y.

6. Method according to claim 4 wherein the superconductive material is Bi₂ (Ca,Sr)₃ Cu₂ O_8+y.

7. Method according to claim 4 wherein the superconductive material is Tl₂ Ca₁.5 BaCu₃ O₈.5-y.

8. Method of using a ferromagnet material, gadolinium, having a high permeability and saturation magnetization to induce superconducting currents in a ring of superconductive material, YBa₂ Cu₃ O_7-y, where the gadolinium has a lower transition temperature than the YBa₂ Cu₃ O_7-y, said method including the steps of:

(A) placing a bar of gadolinium in an annular ring of YBa₂ Cu₃ O_7-y at about 80°

K.,

(B) applying an axial magnetic field of several hundred gauss to saturate the gadolinium when the gadolinium is cooled below its transition temperature,

(C) cooling the gadolinium to below 50°

K. without cooling the YBa₂ Cu₃ O_7-y,

(D) cooling the YBa₂ Cu₃ O_7-y to below 70°

K.,

(E) removing the gadolinium and the applied field, and

(F) allowing the system to warm to about 60°

K.