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US5041419A Expired / Lapsed US ⏱️ 0.0 years remaining

High energy product radially oriented toroidal magnet and method of making

Assignee: United States Department of the Army
•
Filing: 1990-04-30
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Granted: 1991-08-20
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Expires: 2010-04-30
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Abstract

Abstract An improved high energy product radially oriented toroidal magnet is made om an iron cylinder toroid by a method including the steps of: (A) sandwiching the iron cylinder toroid between two disc toroids of a superconductive material at a temperature above the transition temperature of the superconductive material at which temperature the superconductive material does not have superconducting properties and therefor cannot affect the magnetic state of the iron toroid, (B) aligning the iron radially with a small applied field so that flux lines go through the toroidal magnet in a radial direction and in response to which the magnetic dipoles of the iron align themselves with those flux lines, (C) cooling the superconductive material to below the transition temperature of the superconductive material thereby trapping magnetic flux in the iron cylinder toroid, and (D) removing the small applied field from the iron cylinder toroid that does not affect the radial magnetization of the iron as the radial magnetization of the iron is now sustained by the superconducting toroid.

Inventors

  • 👤 Herbert A. Leupold

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-09 07:02
CPC Classifications
H; H01; H01F; H01F41/00; H01F41/02; H01F41/0253; H01F41/0273; H01F41/028; Y; Y10; Y10T; Y10T29/00; Y10T29/49; Y10T29/49002; Y10T29/49014; Y10T29/4902; Y10T29/49075; Y10T29/49076

Claims Analysis

Total Claims: 3
Claim 1
Independent Claim 190 words
Method of making a high energy product radially oriented toroidal magnet from an iron cylinder toroid, said method including the steps of: (A) sandwiching an iron cylinder toroid between two disc toroids of a superconductive material at a first temperature above a transition temperature of the superconductive material, at which first temperature the superconductive material does not have superconducting properties and therefor cannot affect the magnetic state of the iron cylinder toroid, (B) aligning the iron radially by applying a small field of several hundred to several thousand gauss to the iron cylinder toroid, so that flux lines go through the iron cylinder toroid in a radial direction and magnetic dipoles of the iron align themselves with those flux lines, (C) cooling the superconductive material to below the transition temperature of the superconductive material, thereby making the disc toroids superconducting, and thereby trapping magnetic flux in the iron cylinder toroid, and (D) removing the small applied field from the iron cylinder toroid, whereby radial magnetization of the iron is not affected by removing the applied field, since the radial magnetization of the iron is now sustained by the superconducting toroids.
Claim 2
Dependent Claim 190 words
Method of making a high energy product radially oriented toroidal magnet from an iron cylinder toroid, said method including the steps of: (A) sandwiching an iron cylinder toroid between two disc toroids of a superconductive material at a first temperature above a transition temperature of the superconductive material, at which first temperature the superconductive material does not have superconducting properties and therefor cannot affect the magnetic state of the iron cylinder toroid, (B) aligning the iron radially by applying a small field of several hundred to several thousand gauss to the iron cylinder toroid, so that flux lines go through the iron cylinder toroid in a radial direction and magnetic dipoles of the iron align themselves with those flux lines, (C) cooling the superconductive material to below the transition temperature of the superconductive material, thereby making the disc toroids superconducting, and thereby trapping magnetic flux in the iron cylinder toroid, and (D) removing the small applied field from the iron cylinder toroid, whereby radial magnetization of the iron is not affected by removing the applied field, since the radial magnetization of the iron is now sustained by the superconducting toroids.
Claim 3
Dependent Claim 18 words
The method according to claim 1 wherein the superconductive material is YBa 2 Cu 3 O 7-y .

References Cited (Backward Citations)

US2188091A Cited
US2849312A Cited
US4205430A Cited
JPS57155706A Cited
US4457851A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1994-08-19 1995-02-18 1995-08-20 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1998-08-19 1999-02-18 1999-08-20 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 2002-08-19 2003-02-18 2003-08-20 $7700.00 Window Closed / Lapsed

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