Effect of stress on the law of approach to saturation magnetization in carbon steels

In high fields where the magnetization is approaching saturation, the resolved magnetic polarization I can be expressed by a power series of the inverse of external field H as: I=I/sub s/-b/H/sup 2/-c/H/sup 3/ . . ., or alternatively in terms of the reversible permeability mu /sub rev/=1+(2b/H/sup 3...

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Veröffentlicht in:IEEE transactions on magnetics 1991-05, Vol.27 (3), p.3420-3425
Hauptverfasser: Utsunomiya, T., Nishizawa, H., Kaneta, K.
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Kaneta, K.
description In high fields where the magnetization is approaching saturation, the resolved magnetic polarization I can be expressed by a power series of the inverse of external field H as: I=I/sub s/-b/H/sup 2/-c/H/sup 3/ . . ., or alternatively in terms of the reversible permeability mu /sub rev/=1+(2b/H/sup 3/+3c/H/sup 4/+ . . .)/ mu /sub 0/ where I/sub s/ is the spontaneous magnetic polarization and b, c, are constants. These equations express the law of approach to saturation magnetization. The coefficient b for a cubic crystal has been deduced as b=0.0762/I/sub s/(K+1.5( lambda /sub 100/- lambda /sub 111/) sigma )/sup 2/, where sigma is the applied stress and others are magnetic constants. The values of reversible permeability mu /sub rev/ under biasing field H were measured for carbon steels with applied stresses. The results showed that the square root of 2b changed linearly with the applied stress, The values of magnetic constant K and lambda /sub 100/ - lambda /sub 111/ were calculated, They agreed with the standard values, but were affected by chemical composition and heat treatment of materials, especially in lambda /sub 100/- lambda /sub 111/.< >
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These equations express the law of approach to saturation magnetization. The coefficient b for a cubic crystal has been deduced as b=0.0762/I/sub s/(K+1.5( lambda /sub 100/- lambda /sub 111/) sigma )/sup 2/, where sigma is the applied stress and others are magnetic constants. The values of reversible permeability mu /sub rev/ under biasing field H were measured for carbon steels with applied stresses. 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These equations express the law of approach to saturation magnetization. The coefficient b for a cubic crystal has been deduced as b=0.0762/I/sub s/(K+1.5( lambda /sub 100/- lambda /sub 111/) sigma )/sup 2/, where sigma is the applied stress and others are magnetic constants. The values of reversible permeability mu /sub rev/ under biasing field H were measured for carbon steels with applied stresses. 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Metallurgy</topic><topic>Permeability measurement</topic><topic>Physics</topic><topic>Polarization</topic><topic>Saturation magnetization</topic><topic>Steel</topic><topic>Stress measurement</topic><topic>Studies of specific magnetic materials</topic><toplevel>online_resources</toplevel><creatorcontrib>Utsunomiya, T.</creatorcontrib><creatorcontrib>Nishizawa, H.</creatorcontrib><creatorcontrib>Kaneta, K.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>METADEX</collection><collection>Materials Research Database</collection><jtitle>IEEE transactions on magnetics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Utsunomiya, T.</au><au>Nishizawa, H.</au><au>Kaneta, K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of stress on the law of approach to saturation magnetization in carbon steels</atitle><jtitle>IEEE transactions on magnetics</jtitle><stitle>TMAG</stitle><date>1991-05-01</date><risdate>1991</risdate><volume>27</volume><issue>3</issue><spage>3420</spage><epage>3425</epage><pages>3420-3425</pages><issn>0018-9464</issn><eissn>1941-0069</eissn><coden>IEMGAQ</coden><abstract>In high fields where the magnetization is approaching saturation, the resolved magnetic polarization I can be expressed by a power series of the inverse of external field H as: I=I/sub s/-b/H/sup 2/-c/H/sup 3/ . . ., or alternatively in terms of the reversible permeability mu /sub rev/=1+(2b/H/sup 3/+3c/H/sup 4/+ . . .)/ mu /sub 0/ where I/sub s/ is the spontaneous magnetic polarization and b, c, are constants. These equations express the law of approach to saturation magnetization. The coefficient b for a cubic crystal has been deduced as b=0.0762/I/sub s/(K+1.5( lambda /sub 100/- lambda /sub 111/) sigma )/sup 2/, where sigma is the applied stress and others are magnetic constants. The values of reversible permeability mu /sub rev/ under biasing field H were measured for carbon steels with applied stresses. The results showed that the square root of 2b changed linearly with the applied stress, The values of magnetic constant K and lambda /sub 100/ - lambda /sub 111/ were calculated, They agreed with the standard values, but were affected by chemical composition and heat treatment of materials, especially in lambda /sub 100/- lambda /sub 111/.&lt; &gt;</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/20.79084</doi><tpages>6</tpages></addata></record>
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subjects Applied sciences
Chemicals
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Equations
Exact sciences and technology
Heat treatment
Magnetic field measurement
Magnetic materials
Magnetic properties and materials
Metals. Metallurgy
Permeability measurement
Physics
Polarization
Saturation magnetization
Steel
Stress measurement
Studies of specific magnetic materials
title Effect of stress on the law of approach to saturation magnetization in carbon steels
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