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Effects of Anisotropy Field and easy axis dispersions on square-ness ratio for HDDR-processed NdFeB powders
NdFeB magnetic powders that are produced by a hydrogenation decomposition desorption recombination (HDDR) process consist of small grains with highly anisotropic energy [1]-[3]. Therefore, HDDR-processed NdFeB magnet powders are expected to have a high squareness ratio and high coercivity (H_{c}) to...
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description | NdFeB magnetic powders that are produced by a hydrogenation decomposition desorption recombination (HDDR) process consist of small grains with highly anisotropic energy [1]-[3]. Therefore, HDDR-processed NdFeB magnet powders are expected to have a high squareness ratio and high coercivity (H_{c}) to obtain the high maximum energy product (BH _{max}) that is required in highly efficient motors of hybrid or electric vehicles. The squareness ratio is defined as the value of the magnetic field at 90% of the remanent magnetization divided by H_{c}. However, the squareness ratio is much lower than the expected value of 1.0, and the H_{c} is lower than a third of the average anisotropy fields. A previous study using a micromagnetic simulator has shown that when an anisotropy field (H_{k}) dispersion of grains was assumed to be a Gaussian distribution with a coefficient variation (\sigma H_{k} {/\lt \mathrm {H}} _{k} \gt ) of 30%, the squareness ratio corresponded with an experimental value [4]. However, Nishio et al. showed that the H_{k} of a single crystal was 7600 kA/m [5]. Therefore, when the \sigma H_{k} {/\lt \mathrm {H}} _{k} \gt is 30%, the \lt H_{k} \gt + 3 \sigma H_{k} is unrealistically higher than the H_{k} of a single crystal. In this study, the H_{k} dispersion of the grains was assumed to be a horizontally flipped lognormal distribution, and the effects of the H_{k} dispersion of the grains on the squareness ratio were investigated by using a micromagnetic simulator. Moreover, Nishio et al. showed that an easy axis (c-axis) inclination angle was distributed within ± 20° [6], so we also investigated the effects of the c-axis dispersion on the squareness ratio. |
doi_str_mv | 10.1109/INTMAG.2018.8508047 |
format | conference_proceeding |
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Therefore, HDDR-processed NdFeB magnet powders are expected to have a high squareness ratio and high coercivity (H_{c}) to obtain the high maximum energy product (BH _{max}) that is required in highly efficient motors of hybrid or electric vehicles. The squareness ratio is defined as the value of the magnetic field at 90% of the remanent magnetization divided by H_{c}. However, the squareness ratio is much lower than the expected value of 1.0, and the H_{c} is lower than a third of the average anisotropy fields. A previous study using a micromagnetic simulator has shown that when an anisotropy field (H_{k}) dispersion of grains was assumed to be a Gaussian distribution with a coefficient variation (\sigma H_{k} {/\lt \mathrm {H}} _{k} \gt ) of 30%, the squareness ratio corresponded with an experimental value [4]. However, Nishio et al. showed that the H_{k} of a single crystal was 7600 kA/m [5]. Therefore, when the \sigma H_{k} {/\lt \mathrm {H}} _{k} \gt is 30%, the \lt H_{k} \gt + 3 \sigma H_{k} is unrealistically higher than the H_{k} of a single crystal. In this study, the H_{k} dispersion of the grains was assumed to be a horizontally flipped lognormal distribution, and the effects of the H_{k} dispersion of the grains on the squareness ratio were investigated by using a micromagnetic simulator. Moreover, Nishio et al. showed that an easy axis (c-axis) inclination angle was distributed within ± 20° [6], so we also investigated the effects of the c-axis dispersion on the squareness ratio.</description><identifier>EISSN: 2150-4601</identifier><identifier>EISBN: 1538664259</identifier><identifier>EISBN: 9781538664254</identifier><identifier>DOI: 10.1109/INTMAG.2018.8508047</identifier><language>eng</language><publisher>IEEE</publisher><subject>Conferences ; Magnetics</subject><ispartof>2018 IEEE International Magnetics Conference (INTERMAG), 2018, p.1-1</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/8508047$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,780,784,789,790,23930,23931,25140,27925,54555,54932</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/8508047$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Akagi, F.</creatorcontrib><creatorcontrib>Shirai, T.</creatorcontrib><creatorcontrib>Kariya, R.</creatorcontrib><title>Effects of Anisotropy Field and easy axis dispersions on square-ness ratio for HDDR-processed NdFeB powders</title><title>2018 IEEE International Magnetics Conference (INTERMAG)</title><addtitle>INTMAG</addtitle><description>NdFeB magnetic powders that are produced by a hydrogenation decomposition desorption recombination (HDDR) process consist of small grains with highly anisotropic energy [1]-[3]. Therefore, HDDR-processed NdFeB magnet powders are expected to have a high squareness ratio and high coercivity (H_{c}) to obtain the high maximum energy product (BH _{max}) that is required in highly efficient motors of hybrid or electric vehicles. The squareness ratio is defined as the value of the magnetic field at 90% of the remanent magnetization divided by H_{c}. However, the squareness ratio is much lower than the expected value of 1.0, and the H_{c} is lower than a third of the average anisotropy fields. A previous study using a micromagnetic simulator has shown that when an anisotropy field (H_{k}) dispersion of grains was assumed to be a Gaussian distribution with a coefficient variation (\sigma H_{k} {/\lt \mathrm {H}} _{k} \gt ) of 30%, the squareness ratio corresponded with an experimental value [4]. However, Nishio et al. showed that the H_{k} of a single crystal was 7600 kA/m [5]. Therefore, when the \sigma H_{k} {/\lt \mathrm {H}} _{k} \gt is 30%, the \lt H_{k} \gt + 3 \sigma H_{k} is unrealistically higher than the H_{k} of a single crystal. In this study, the H_{k} dispersion of the grains was assumed to be a horizontally flipped lognormal distribution, and the effects of the H_{k} dispersion of the grains on the squareness ratio were investigated by using a micromagnetic simulator. Moreover, Nishio et al. showed that an easy axis (c-axis) inclination angle was distributed within ± 20° [6], so we also investigated the effects of the c-axis dispersion on the squareness ratio.</description><subject>Conferences</subject><subject>Magnetics</subject><issn>2150-4601</issn><isbn>1538664259</isbn><isbn>9781538664254</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2018</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><recordid>eNotUF9LwzAcjILgnPsEe8kX6PwlaZr0ce4_zAkyn0fa_ALR2dSkov32K7ing-PuuDtCpgxmjEH5tDscX-abGQemZ1qChlzdkAcmhS6KnMvylow4k5DlBbB7MknpAwB4oYXmMCKfK-ew7hINjs4bn0IXQ9vTtcezpaaxFE3qqfnziVqfWozJh2ZQNzR9_5iIWYMp0Wg6H6gLkW6Xy7esjaEeaLT0YNf4TNvwawfnI7lz5pxwcsUxeV-vjotttn_d7BbzfeaZkl0mqqFRZZSS0shaVo6jgsIxxUocNoBEWXOQFgvuOHOGK1bnAmypVZXnAsWYTP9zPSKe2ui_TOxP12_EBSJiWU8</recordid><startdate>201804</startdate><enddate>201804</enddate><creator>Akagi, F.</creator><creator>Shirai, T.</creator><creator>Kariya, R.</creator><general>IEEE</general><scope>6IE</scope><scope>6IL</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIL</scope></search><sort><creationdate>201804</creationdate><title>Effects of Anisotropy Field and easy axis dispersions on square-ness ratio for HDDR-processed NdFeB powders</title><author>Akagi, F. ; Shirai, T. ; Kariya, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i175t-3bfecba7755a5c5bf2e706f1719e60105e5c205de62f21fa271c430d987b443e3</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Conferences</topic><topic>Magnetics</topic><toplevel>online_resources</toplevel><creatorcontrib>Akagi, F.</creatorcontrib><creatorcontrib>Shirai, T.</creatorcontrib><creatorcontrib>Kariya, R.</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan All Online (POP All Online) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP All) 1998-Present</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Akagi, F.</au><au>Shirai, T.</au><au>Kariya, R.</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Effects of Anisotropy Field and easy axis dispersions on square-ness ratio for HDDR-processed NdFeB powders</atitle><btitle>2018 IEEE International Magnetics Conference (INTERMAG)</btitle><stitle>INTMAG</stitle><date>2018-04</date><risdate>2018</risdate><spage>1</spage><epage>1</epage><pages>1-1</pages><eissn>2150-4601</eissn><eisbn>1538664259</eisbn><eisbn>9781538664254</eisbn><abstract>NdFeB magnetic powders that are produced by a hydrogenation decomposition desorption recombination (HDDR) process consist of small grains with highly anisotropic energy [1]-[3]. Therefore, HDDR-processed NdFeB magnet powders are expected to have a high squareness ratio and high coercivity (H_{c}) to obtain the high maximum energy product (BH _{max}) that is required in highly efficient motors of hybrid or electric vehicles. The squareness ratio is defined as the value of the magnetic field at 90% of the remanent magnetization divided by H_{c}. However, the squareness ratio is much lower than the expected value of 1.0, and the H_{c} is lower than a third of the average anisotropy fields. A previous study using a micromagnetic simulator has shown that when an anisotropy field (H_{k}) dispersion of grains was assumed to be a Gaussian distribution with a coefficient variation (\sigma H_{k} {/\lt \mathrm {H}} _{k} \gt ) of 30%, the squareness ratio corresponded with an experimental value [4]. However, Nishio et al. showed that the H_{k} of a single crystal was 7600 kA/m [5]. Therefore, when the \sigma H_{k} {/\lt \mathrm {H}} _{k} \gt is 30%, the \lt H_{k} \gt + 3 \sigma H_{k} is unrealistically higher than the H_{k} of a single crystal. In this study, the H_{k} dispersion of the grains was assumed to be a horizontally flipped lognormal distribution, and the effects of the H_{k} dispersion of the grains on the squareness ratio were investigated by using a micromagnetic simulator. Moreover, Nishio et al. showed that an easy axis (c-axis) inclination angle was distributed within ± 20° [6], so we also investigated the effects of the c-axis dispersion on the squareness ratio.</abstract><pub>IEEE</pub><doi>10.1109/INTMAG.2018.8508047</doi><tpages>1</tpages></addata></record> |
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title | Effects of Anisotropy Field and easy axis dispersions on square-ness ratio for HDDR-processed NdFeB powders |
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