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Dynamic magnetoelastic properties of TbxHo0.9−xNd0.1(Fe0.8Co0.2)1.93/epoxy composites
Tb Ho Nd (Fe Co /epoxy (0 ⩽ x ⩽ 0.40) composites are fabricated in the presence of a magnetic field. The structural and dynamic magnetoelastic properties are investigated as a function of both magnetic bias field H and frequency f at room temperature. The composites are formed as textured orientatio...
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Published in: | Materials science--Poland 2019-06, Vol.37 (2), p.257-264 |
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container_title | Materials science--Poland |
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creator | Shen, W.C. Lin, L.L. Shen, C.Y. Xing, S. Pan, Z.B. |
description | Tb
Ho
Nd
(Fe
Co
/epoxy (0 ⩽ x ⩽ 0.40) composites are fabricated in the presence of a magnetic field. The structural and dynamic magnetoelastic properties are investigated as a function of both magnetic bias field H
and frequency f at room temperature. The composites are formed as textured orientation structure of 1–3 type with 〈1 0 0〉 preferred orientation for x ⩽ 0.10 and 〈1 1 1〉-orientation for x ⩾ 0.25. The composites generally possess insignificant eddy-current losses for frequency up to 50 kHz, and their dynamic magnetoelastic properties depend greatly on H
. The elastic modulus (E
and E
) shows a maximum negative ΔE effect, along with a maximum d
, at a relatively low H
~ 80 kA/m, contributed by the maximum motion of non-180° domain-wall. The 1–3 type composite for x ⩾ 0.25 shows an enhanced magnetoelastic effect in comparison with 0 to 3 type one, which can be principally ascribed to its easy magnetization direction (EMD) towards 〈1 1 1〉 axis and the formation of 〈1 1 1〉-texture-oriented structure in the composite. These attractive dynamic magnetoelastic properties, e.g., the low magnetic anisotropy and d
as high as 2.0 nm/A at a low H
~ 80 kA/m, along with the light rare-earth Nd element existing in insulating polymer matrix, would make it a promising magnetostrictive material system. |
doi_str_mv | 10.2478/msp-2019-0027 |
format | article |
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Ho
Nd
(Fe
Co
/epoxy (0 ⩽ x ⩽ 0.40) composites are fabricated in the presence of a magnetic field. The structural and dynamic magnetoelastic properties are investigated as a function of both magnetic bias field H
and frequency f at room temperature. The composites are formed as textured orientation structure of 1–3 type with 〈1 0 0〉 preferred orientation for x ⩽ 0.10 and 〈1 1 1〉-orientation for x ⩾ 0.25. The composites generally possess insignificant eddy-current losses for frequency up to 50 kHz, and their dynamic magnetoelastic properties depend greatly on H
. The elastic modulus (E
and E
) shows a maximum negative ΔE effect, along with a maximum d
, at a relatively low H
~ 80 kA/m, contributed by the maximum motion of non-180° domain-wall. The 1–3 type composite for x ⩾ 0.25 shows an enhanced magnetoelastic effect in comparison with 0 to 3 type one, which can be principally ascribed to its easy magnetization direction (EMD) towards 〈1 1 1〉 axis and the formation of 〈1 1 1〉-texture-oriented structure in the composite. These attractive dynamic magnetoelastic properties, e.g., the low magnetic anisotropy and d
as high as 2.0 nm/A at a low H
~ 80 kA/m, along with the light rare-earth Nd element existing in insulating polymer matrix, would make it a promising magnetostrictive material system.</description><identifier>EISSN: 2083-134X</identifier><identifier>DOI: 10.2478/msp-2019-0027</identifier><language>eng</language><publisher>Sciendo</publisher><subject>dynamic magnetoelastic properties ; Laves phase ; magnetization process ; magnetostriction ; magnetostrictive composite</subject><ispartof>Materials science--Poland, 2019-06, Vol.37 (2), p.257-264</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Shen, W.C.</creatorcontrib><creatorcontrib>Lin, L.L.</creatorcontrib><creatorcontrib>Shen, C.Y.</creatorcontrib><creatorcontrib>Xing, S.</creatorcontrib><creatorcontrib>Pan, Z.B.</creatorcontrib><title>Dynamic magnetoelastic properties of TbxHo0.9−xNd0.1(Fe0.8Co0.2)1.93/epoxy composites</title><title>Materials science--Poland</title><description>Tb
Ho
Nd
(Fe
Co
/epoxy (0 ⩽ x ⩽ 0.40) composites are fabricated in the presence of a magnetic field. The structural and dynamic magnetoelastic properties are investigated as a function of both magnetic bias field H
and frequency f at room temperature. The composites are formed as textured orientation structure of 1–3 type with 〈1 0 0〉 preferred orientation for x ⩽ 0.10 and 〈1 1 1〉-orientation for x ⩾ 0.25. The composites generally possess insignificant eddy-current losses for frequency up to 50 kHz, and their dynamic magnetoelastic properties depend greatly on H
. The elastic modulus (E
and E
) shows a maximum negative ΔE effect, along with a maximum d
, at a relatively low H
~ 80 kA/m, contributed by the maximum motion of non-180° domain-wall. The 1–3 type composite for x ⩾ 0.25 shows an enhanced magnetoelastic effect in comparison with 0 to 3 type one, which can be principally ascribed to its easy magnetization direction (EMD) towards 〈1 1 1〉 axis and the formation of 〈1 1 1〉-texture-oriented structure in the composite. These attractive dynamic magnetoelastic properties, e.g., the low magnetic anisotropy and d
as high as 2.0 nm/A at a low H
~ 80 kA/m, along with the light rare-earth Nd element existing in insulating polymer matrix, would make it a promising magnetostrictive material system.</description><subject>dynamic magnetoelastic properties</subject><subject>Laves phase</subject><subject>magnetization process</subject><subject>magnetostriction</subject><subject>magnetostrictive composite</subject><issn>2083-134X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNotkE1Lw0AQhhdBsNQeveeoh6SzH8lm8STRWqHoJaC3sN2dlJSmG7IpNv_Asz_RX-IGncvM-x6egYeQGwoJEzJftr6LGVAVAzB5QWYMch5TLj6uyML7PYTJ8hQEnZH3x_Go28ZErd4dcXB40H4Isetdh_3QoI9cHZXb89pBon6-vs-vFhJ6u0JI8iJ07I4mii-xc-cxMq7tnG8G9NfkstYHj4v_PSfl6qks1vHm7fmleNjEnmZUxkKiYZRJXddqK8CAEMiUtkLnmWapxVrWUlqea6GMMKkVyqaSZ6hNKjTwObn_w37qw4C9xV1_GsNR7d2pP4bHFYVqclIFJ9XkpJqccMlYwPwCotRYlA</recordid><startdate>20190601</startdate><enddate>20190601</enddate><creator>Shen, W.C.</creator><creator>Lin, L.L.</creator><creator>Shen, C.Y.</creator><creator>Xing, S.</creator><creator>Pan, Z.B.</creator><general>Sciendo</general><scope/></search><sort><creationdate>20190601</creationdate><title>Dynamic magnetoelastic properties of TbxHo0.9−xNd0.1(Fe0.8Co0.2)1.93/epoxy composites</title><author>Shen, W.C. ; Lin, L.L. ; Shen, C.Y. ; Xing, S. ; Pan, Z.B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-s1617-47ec2127aff9b40c044e29ad4a86a25def7f77d38a49c4c5d49d5736eac54a03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>dynamic magnetoelastic properties</topic><topic>Laves phase</topic><topic>magnetization process</topic><topic>magnetostriction</topic><topic>magnetostrictive composite</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shen, W.C.</creatorcontrib><creatorcontrib>Lin, L.L.</creatorcontrib><creatorcontrib>Shen, C.Y.</creatorcontrib><creatorcontrib>Xing, S.</creatorcontrib><creatorcontrib>Pan, Z.B.</creatorcontrib><jtitle>Materials science--Poland</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shen, W.C.</au><au>Lin, L.L.</au><au>Shen, C.Y.</au><au>Xing, S.</au><au>Pan, Z.B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dynamic magnetoelastic properties of TbxHo0.9−xNd0.1(Fe0.8Co0.2)1.93/epoxy composites</atitle><jtitle>Materials science--Poland</jtitle><date>2019-06-01</date><risdate>2019</risdate><volume>37</volume><issue>2</issue><spage>257</spage><epage>264</epage><pages>257-264</pages><eissn>2083-134X</eissn><abstract>Tb
Ho
Nd
(Fe
Co
/epoxy (0 ⩽ x ⩽ 0.40) composites are fabricated in the presence of a magnetic field. The structural and dynamic magnetoelastic properties are investigated as a function of both magnetic bias field H
and frequency f at room temperature. The composites are formed as textured orientation structure of 1–3 type with 〈1 0 0〉 preferred orientation for x ⩽ 0.10 and 〈1 1 1〉-orientation for x ⩾ 0.25. The composites generally possess insignificant eddy-current losses for frequency up to 50 kHz, and their dynamic magnetoelastic properties depend greatly on H
. The elastic modulus (E
and E
) shows a maximum negative ΔE effect, along with a maximum d
, at a relatively low H
~ 80 kA/m, contributed by the maximum motion of non-180° domain-wall. The 1–3 type composite for x ⩾ 0.25 shows an enhanced magnetoelastic effect in comparison with 0 to 3 type one, which can be principally ascribed to its easy magnetization direction (EMD) towards 〈1 1 1〉 axis and the formation of 〈1 1 1〉-texture-oriented structure in the composite. These attractive dynamic magnetoelastic properties, e.g., the low magnetic anisotropy and d
as high as 2.0 nm/A at a low H
~ 80 kA/m, along with the light rare-earth Nd element existing in insulating polymer matrix, would make it a promising magnetostrictive material system.</abstract><pub>Sciendo</pub><doi>10.2478/msp-2019-0027</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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issn | 2083-134X |
language | eng |
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source | Free Full-Text Journals in Chemistry |
subjects | dynamic magnetoelastic properties Laves phase magnetization process magnetostriction magnetostrictive composite |
title | Dynamic magnetoelastic properties of TbxHo0.9−xNd0.1(Fe0.8Co0.2)1.93/epoxy composites |
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