Carnegie Mellon University

The United States of America As Represented by the Department of Energy

U.S. Department of Energy

Spang, Inc.

Alex Leary

Michael McHenry

Paul Ohodnicki

Vladimir Keylin

Michael Paul Buric

Joseph Huth

Kevin Byerly

Samuel J Kernion

Paul R Ohodnicki, Jr

Satoru Simizu

Jagannath Devkota

Richard B Beddingfield

Richard Beddingfield

Derek Lau

Yuval Krimer

Michael E Mchenry

A method of thermally processing a material with a thermal processing system includes providing a material for treating in an in-line thermal process to a heating system, providing a force to the material at a portion of the material configured to be heated by the heating system, adjusting the heating system to a specified temperature value, and heating the portion of the material to the specified temperature value while the portion of the material is under the force to change a magnetic property in the portion of the material. The heating system is moveable from a first position that is away from a path of the material through the in-line thermal process to a second position in which the heating system is configured to heat the portion of the material to the specified temperature value. The heating system can include induction-based heating.

Thermal processing techniques for metallic materials

The invention provides a method for measuring the magnetic field of an electromagnetic component having the steps of: instrumenting one or more portions of an electromagnetic component by placing an optical fiber in electromagnetic communication with the one or more portions of said electromagnetic component; energizing the electromagnetic component; interrogating the optical fiber using light and an optical detector; and determining changes in the magnetic field incident on the optical fiber based on the detected changes in the light received by the optical detector.

Optical sensing of magnetic fields using magnetically sensitive materials

A method includes producing an amorphous precursor to a nanocomposite, the amorphous precursor comprising a material that is substantially without crystals not exceeding 20% volume fraction; performing devitrification of the amorphous precursor, wherein the devitrification comprises a process of crystallization; forming, based on the devitrification, the nanocomposite with nano-crystals that contains an induced magnetic anisotropy; tuning, based on one or more of composition, temperature, configuration, and magnitude of stress applied during annealing and modification, the magnetic anisotropy of the nanocomposite; and adjusting, based on the tuned magnetic anisotropy, a magnetic permeability of the nanocomposite.

Tunable anisotropy of co-based nanocomposites for magnetic field sensing and inductor applications

An OFDR based fiber-optics sensor for distributed real-time temperature rise monitoring of a transformer in operation has been disclosed. The fiber-optic sensor provides an effective solution to monitoring the physical structures of the transformer core, as well as accurately detecting the non-uniform temperature distribution inside the transformer, and thus provides innovative feedback to the transformer design by minimizing the core losses. Additionally, the method may be responsive to the presence of magnetic and electric fields, as well as responsive to various chemical species. The method allows novel approaches to real-time asset monitoring of power transformers while operational.

Distributed sensing of electromagnetic components using optical fiber based methods

A method includes producing an amorphous precursor to a nanocomposite, performing devitrification of the amorphous precursor, forming, based on the devitrification, the nanocomposite comprising an induced magnetic anisotropy, and for a first portion of the nanocomposite, determining a desired value of a magnetic permeability of the first portion, tuning, based on the desired value, the induced magnetic anisotropy for the first portion, and adjusting, based on the tuning of the induced magnetic anisotropy of the first portion, a first magnetic permeability value of the first portion of the nanocomposite, wherein the first magnetic permeability value is different from a second magnetic permeability value for a second portion of the nanocomposite.

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Pittsburgh, PA, United States of America

Alex Leary