Bonded Terfenol-D composites with low eddy current loss and high magnetostriction
Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current l...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Tian, Jianjun [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Anmerkung: |
© Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 |
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| Übergeordnetes Werk: |
Enthalten in: Rare metals - Beijing : Yejin Gongye Chubanshe, 1989, 29(2010), 6 vom: 20. Nov., Seite 579-582 |
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| Übergeordnetes Werk: |
volume:29 ; year:2010 ; number:6 ; day:20 ; month:11 ; pages:579-582 |
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| DOI / URN: |
10.1007/s12598-010-0173-5 |
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| Katalog-ID: |
SPR026246686 |
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| 520 | |a Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. | ||
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| 650 | 4 | |a eddy current losses |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a density |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Zuo, Zhijun |4 aut | |
| 700 | 1 | |a Pan, De’an |4 aut | |
| 700 | 1 | |a Zhang, Shengen |4 aut | |
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10.1007/s12598-010-0173-5 doi (DE-627)SPR026246686 (SPR)s12598-010-0173-5-e DE-627 ger DE-627 rakwb eng Tian, Jianjun verfasserin aut Bonded Terfenol-D composites with low eddy current loss and high magnetostriction 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 Zuo, Zhijun aut Pan, De’an aut Zhang, Shengen aut Enthalten in Rare metals Beijing : Yejin Gongye Chubanshe, 1989 29(2010), 6 vom: 20. Nov., Seite 579-582 (DE-627)513219307 (DE-600)2238702-X 1867-7185 nnns volume:29 year:2010 number:6 day:20 month:11 pages:579-582 https://dx.doi.org/10.1007/s12598-010-0173-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2700 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2010 6 20 11 579-582 |
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10.1007/s12598-010-0173-5 doi (DE-627)SPR026246686 (SPR)s12598-010-0173-5-e DE-627 ger DE-627 rakwb eng Tian, Jianjun verfasserin aut Bonded Terfenol-D composites with low eddy current loss and high magnetostriction 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 Zuo, Zhijun aut Pan, De’an aut Zhang, Shengen aut Enthalten in Rare metals Beijing : Yejin Gongye Chubanshe, 1989 29(2010), 6 vom: 20. Nov., Seite 579-582 (DE-627)513219307 (DE-600)2238702-X 1867-7185 nnns volume:29 year:2010 number:6 day:20 month:11 pages:579-582 https://dx.doi.org/10.1007/s12598-010-0173-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2700 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2010 6 20 11 579-582 |
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10.1007/s12598-010-0173-5 doi (DE-627)SPR026246686 (SPR)s12598-010-0173-5-e DE-627 ger DE-627 rakwb eng Tian, Jianjun verfasserin aut Bonded Terfenol-D composites with low eddy current loss and high magnetostriction 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 Zuo, Zhijun aut Pan, De’an aut Zhang, Shengen aut Enthalten in Rare metals Beijing : Yejin Gongye Chubanshe, 1989 29(2010), 6 vom: 20. Nov., Seite 579-582 (DE-627)513219307 (DE-600)2238702-X 1867-7185 nnns volume:29 year:2010 number:6 day:20 month:11 pages:579-582 https://dx.doi.org/10.1007/s12598-010-0173-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2700 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2010 6 20 11 579-582 |
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10.1007/s12598-010-0173-5 doi (DE-627)SPR026246686 (SPR)s12598-010-0173-5-e DE-627 ger DE-627 rakwb eng Tian, Jianjun verfasserin aut Bonded Terfenol-D composites with low eddy current loss and high magnetostriction 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 Zuo, Zhijun aut Pan, De’an aut Zhang, Shengen aut Enthalten in Rare metals Beijing : Yejin Gongye Chubanshe, 1989 29(2010), 6 vom: 20. Nov., Seite 579-582 (DE-627)513219307 (DE-600)2238702-X 1867-7185 nnns volume:29 year:2010 number:6 day:20 month:11 pages:579-582 https://dx.doi.org/10.1007/s12598-010-0173-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2700 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2010 6 20 11 579-582 |
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10.1007/s12598-010-0173-5 doi (DE-627)SPR026246686 (SPR)s12598-010-0173-5-e DE-627 ger DE-627 rakwb eng Tian, Jianjun verfasserin aut Bonded Terfenol-D composites with low eddy current loss and high magnetostriction 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 Zuo, Zhijun aut Pan, De’an aut Zhang, Shengen aut Enthalten in Rare metals Beijing : Yejin Gongye Chubanshe, 1989 29(2010), 6 vom: 20. Nov., Seite 579-582 (DE-627)513219307 (DE-600)2238702-X 1867-7185 nnns volume:29 year:2010 number:6 day:20 month:11 pages:579-582 https://dx.doi.org/10.1007/s12598-010-0173-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2700 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 29 2010 6 20 11 579-582 |
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Enthalten in Rare metals 29(2010), 6 vom: 20. Nov., Seite 579-582 volume:29 year:2010 number:6 day:20 month:11 pages:579-582 |
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Enthalten in Rare metals 29(2010), 6 vom: 20. Nov., Seite 579-582 volume:29 year:2010 number:6 day:20 month:11 pages:579-582 |
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Tian, Jianjun @@aut@@ Zuo, Zhijun @@aut@@ Pan, De’an @@aut@@ Zhang, Shengen @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR026246686</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331232939.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2010 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12598-010-0173-5</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR026246686</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s12598-010-0173-5-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Tian, Jianjun</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Bonded Terfenol-D composites with low eddy current loss and high magnetostriction</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2010</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). 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Tian, Jianjun |
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Tian, Jianjun misc composites misc Terfenol-D misc magnetostriction misc eddy current losses misc density Bonded Terfenol-D composites with low eddy current loss and high magnetostriction |
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Bonded Terfenol-D composites with low eddy current loss and high magnetostriction composites (dpeaa)DE-He213 Terfenol-D (dpeaa)DE-He213 magnetostriction (dpeaa)DE-He213 eddy current losses (dpeaa)DE-He213 density (dpeaa)DE-He213 |
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misc composites misc Terfenol-D misc magnetostriction misc eddy current losses misc density |
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Bonded Terfenol-D composites with low eddy current loss and high magnetostriction |
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Bonded Terfenol-D composites with low eddy current loss and high magnetostriction |
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Tian, Jianjun Zuo, Zhijun Pan, De’an Zhang, Shengen |
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Tian, Jianjun |
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10.1007/s12598-010-0173-5 |
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bonded terfenol-d composites with low eddy current loss and high magnetostriction |
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Bonded Terfenol-D composites with low eddy current loss and high magnetostriction |
| abstract |
Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 |
| abstractGer |
Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 |
| abstract_unstemmed |
Abstract Bonded Terfenol-D composites, with high electrical resistivity and low eddy current loss, can be used in an alternating magnetic field with high frequency. However, the nonmagnetic binder impairs the magnetostriction of the composites. To achieve high magnetostriction and low eddy current loss, the mixture of the alloy powder and binder was compressed at low pressure in an oriented magnetic field. After this, the aligned samples were recompressed by cold isostatic pressing (CIP). Besides, the effect of particle size on the magnetostriction of the bonded Terfenol-D composites was also studied. The results showed that the bonded Terfenol-D composites had excellent magnetostriction when the particle size was 50–80 μm. The oriented magnetic field and CIP could improve the magnetostriction of the bonded composites, which reaches 1020×$ 10^{−6} $. The bonded Terfenol-D composites had good compact structure and high density (7.24 g/$ cm^{3} $). The magnetic loss of the bonded Terfenol-D composites was 192 mW/$ cm^{3} $ at a frequency of 100 kHz in a magnetic field of 960 A/m, which was about one third of that of casting Terfenol-D alloys. © Journal Publishing Center of University of Science and Technology Beijing and Springer Berlin Heidelberg 2010 |
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6 |
| title_short |
Bonded Terfenol-D composites with low eddy current loss and high magnetostriction |
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https://dx.doi.org/10.1007/s12598-010-0173-5 |
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| author2 |
Zuo, Zhijun Pan, De’an Zhang, Shengen |
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Zuo, Zhijun Pan, De’an Zhang, Shengen |
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| doi_str |
10.1007/s12598-010-0173-5 |
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2024-07-03T19:45:03.802Z |
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| score |
7.401026 |