Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption
Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Garg, Avesh [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Schlagwörter: |
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| Anmerkung: |
© The Minerals, Metals & Materials Society 2020 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 49(2020), 3 vom: 03. Jan., Seite 2233-2241 |
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| Übergeordnetes Werk: |
volume:49 ; year:2020 ; number:3 ; day:03 ; month:01 ; pages:2233-2241 |
| Links: |
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| DOI / URN: |
10.1007/s11664-019-07922-z |
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| Katalog-ID: |
SPR021566682 |
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| 245 | 1 | 0 | |a Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
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| 520 | |a Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. | ||
| 650 | 4 | |a Composite materials |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a sol–gel processes |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a magnetization |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a magnetic measurements |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Goel, Shivanshu |4 aut | |
| 700 | 1 | |a Kumari, Neelam |4 aut | |
| 700 | 1 | |a Dubey, Ashish |4 aut | |
| 700 | 1 | |a Eswara Prasad, N. |4 aut | |
| 700 | 1 | |a Tyagi, Sachin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Journal of electronic materials |d Warrendale, Pa : TMS, 1972 |g 49(2020), 3 vom: 03. Jan., Seite 2233-2241 |w (DE-627)324918739 |w (DE-600)2032868-0 |x 1543-186X |7 nnns |
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| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s11664-019-07922-z |z lizenzpflichtig |3 Volltext |
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10.1007/s11664-019-07922-z doi (DE-627)SPR021566682 (SPR)s11664-019-07922-z-e DE-627 ger DE-627 rakwb eng Garg, Avesh verfasserin aut Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2020 Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 Goel, Shivanshu aut Kumari, Neelam aut Dubey, Ashish aut Eswara Prasad, N. aut Tyagi, Sachin aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2020), 3 vom: 03. Jan., Seite 2233-2241 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2020 number:3 day:03 month:01 pages:2233-2241 https://dx.doi.org/10.1007/s11664-019-07922-z 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_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_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2020 3 03 01 2233-2241 |
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10.1007/s11664-019-07922-z doi (DE-627)SPR021566682 (SPR)s11664-019-07922-z-e DE-627 ger DE-627 rakwb eng Garg, Avesh verfasserin aut Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2020 Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 Goel, Shivanshu aut Kumari, Neelam aut Dubey, Ashish aut Eswara Prasad, N. aut Tyagi, Sachin aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2020), 3 vom: 03. Jan., Seite 2233-2241 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2020 number:3 day:03 month:01 pages:2233-2241 https://dx.doi.org/10.1007/s11664-019-07922-z 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_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_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2020 3 03 01 2233-2241 |
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10.1007/s11664-019-07922-z doi (DE-627)SPR021566682 (SPR)s11664-019-07922-z-e DE-627 ger DE-627 rakwb eng Garg, Avesh verfasserin aut Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2020 Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 Goel, Shivanshu aut Kumari, Neelam aut Dubey, Ashish aut Eswara Prasad, N. aut Tyagi, Sachin aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2020), 3 vom: 03. Jan., Seite 2233-2241 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2020 number:3 day:03 month:01 pages:2233-2241 https://dx.doi.org/10.1007/s11664-019-07922-z 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_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_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2020 3 03 01 2233-2241 |
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10.1007/s11664-019-07922-z doi (DE-627)SPR021566682 (SPR)s11664-019-07922-z-e DE-627 ger DE-627 rakwb eng Garg, Avesh verfasserin aut Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2020 Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 Goel, Shivanshu aut Kumari, Neelam aut Dubey, Ashish aut Eswara Prasad, N. aut Tyagi, Sachin aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2020), 3 vom: 03. Jan., Seite 2233-2241 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2020 number:3 day:03 month:01 pages:2233-2241 https://dx.doi.org/10.1007/s11664-019-07922-z 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_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_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2020 3 03 01 2233-2241 |
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10.1007/s11664-019-07922-z doi (DE-627)SPR021566682 (SPR)s11664-019-07922-z-e DE-627 ger DE-627 rakwb eng Garg, Avesh verfasserin aut Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2020 Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 Goel, Shivanshu aut Kumari, Neelam aut Dubey, Ashish aut Eswara Prasad, N. aut Tyagi, Sachin aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2020), 3 vom: 03. Jan., Seite 2233-2241 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2020 number:3 day:03 month:01 pages:2233-2241 https://dx.doi.org/10.1007/s11664-019-07922-z 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_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_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2020 3 03 01 2233-2241 |
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Garg, Avesh @@aut@@ Goel, Shivanshu @@aut@@ Kumari, Neelam @@aut@@ Dubey, Ashish @@aut@@ Eswara Prasad, N. @@aut@@ Tyagi, Sachin @@aut@@ |
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The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). 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Garg, Avesh |
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Garg, Avesh misc Composite materials misc sol–gel processes misc magnetization misc magnetic measurements Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
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Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption Composite materials (dpeaa)DE-He213 sol–gel processes (dpeaa)DE-He213 magnetization (dpeaa)DE-He213 magnetic measurements (dpeaa)DE-He213 |
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Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
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Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
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Garg, Avesh |
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Garg, Avesh Goel, Shivanshu Kumari, Neelam Dubey, Ashish Eswara Prasad, N. Tyagi, Sachin |
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Elektronische Aufsätze |
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Garg, Avesh |
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10.1007/s11664-019-07922-z |
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development of $ srfe_{12} %$ o_{19} $/$ ti_{3} %$ sic_{2} $ composites for enhanced microwave absorption |
| title_auth |
Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
| abstract |
Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. © The Minerals, Metals & Materials Society 2020 |
| abstractGer |
Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. © The Minerals, Metals & Materials Society 2020 |
| abstract_unstemmed |
Abstract Microwave absorbing composites containing strontium hexaferrite and titanium silicon carbide, $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ powder, were synthesized by mixing in different weight ratios. The strontium hexaferrite ($ SrFe_{12} %$ O_{19} $) particles were synthesized using low-temperature combustion. The ‘as synthesized’ strontium hexaferrite powder is observed to have low coercivity (255.09 G) and high saturation magnetization (45.1 emu/g). The titanium silicon carbide ($ Ti_{3} %$ SiC_{2} $) powder was synthesized by heat treatment of the precursors (Ti/Si/TiC) at 1100°C under argon atmosphere. A microwave absorbing composite is fabricated by mixing in a high-energy ball mill followed by heating of $ SrFe_{12} %$ O_{19} $ and $ Ti_{3} %$ SiC_{2} $ powders at 200°C. The maximum reflection loss of − 39.67 dB is observed at 9.46 GHz for the composite casted into pellets containing 20% $ Ti_{3} %$ SiC_{2} $ and 80% $ SrFe_{12} %$ O_{19} $ with 2-mm thickness. The bandwidth for less than − 10 dB loss is observed to be 2.77 GHz (66% of the total band). The developed magneto-dielectric composition confirmed its candidacy as a potential microwave absorbing material. © The Minerals, Metals & Materials Society 2020 |
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3 |
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Development of $ SrFe_{12} %$ O_{19} $/$ Ti_{3} %$ SiC_{2} $ Composites for Enhanced Microwave Absorption |
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https://dx.doi.org/10.1007/s11664-019-07922-z |
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Goel, Shivanshu Kumari, Neelam Dubey, Ashish Eswara Prasad, N. Tyagi, Sachin |
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Goel, Shivanshu Kumari, Neelam Dubey, Ashish Eswara Prasad, N. Tyagi, Sachin |
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10.1007/s11664-019-07922-z |
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2024-07-03T23:21:00.293Z |
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| score |
7.4018774 |