Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field
Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-p...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zheng, Dianliang [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Schlagwörter: |
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| Anmerkung: |
© The Minerals, Metals & Materials Society 2021 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 50(2021), 8 vom: 17. Mai, Seite 4469-4479 |
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| Übergeordnetes Werk: |
volume:50 ; year:2021 ; number:8 ; day:17 ; month:05 ; pages:4469-4479 |
| Links: |
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| DOI / URN: |
10.1007/s11664-021-08970-0 |
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| Katalog-ID: |
SPR044402805 |
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| 245 | 1 | 0 | |a Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
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| 520 | |a Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. | ||
| 650 | 4 | |a Scaled measurement |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a absorbing material |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a tunable absorber |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a magnetorheological fluid |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Wei, Feiming |4 aut | |
| 700 | 1 | |a Xu, Yonggang |4 aut | |
| 700 | 1 | |a Chen, Teng |4 aut | |
| 700 | 1 | |a Dai, Fei |4 aut | |
| 700 | 1 | |a Liu, Ting |4 aut | |
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10.1007/s11664-021-08970-0 doi (DE-627)SPR044402805 (SPR)s11664-021-08970-0-e DE-627 ger DE-627 rakwb eng Zheng, Dianliang verfasserin aut Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2021 Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 Wei, Feiming aut Xu, Yonggang aut Chen, Teng aut Dai, Fei aut Liu, Ting aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 50(2021), 8 vom: 17. Mai, Seite 4469-4479 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 https://dx.doi.org/10.1007/s11664-021-08970-0 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 50 2021 8 17 05 4469-4479 |
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10.1007/s11664-021-08970-0 doi (DE-627)SPR044402805 (SPR)s11664-021-08970-0-e DE-627 ger DE-627 rakwb eng Zheng, Dianliang verfasserin aut Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2021 Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 Wei, Feiming aut Xu, Yonggang aut Chen, Teng aut Dai, Fei aut Liu, Ting aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 50(2021), 8 vom: 17. Mai, Seite 4469-4479 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 https://dx.doi.org/10.1007/s11664-021-08970-0 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 50 2021 8 17 05 4469-4479 |
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10.1007/s11664-021-08970-0 doi (DE-627)SPR044402805 (SPR)s11664-021-08970-0-e DE-627 ger DE-627 rakwb eng Zheng, Dianliang verfasserin aut Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2021 Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 Wei, Feiming aut Xu, Yonggang aut Chen, Teng aut Dai, Fei aut Liu, Ting aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 50(2021), 8 vom: 17. Mai, Seite 4469-4479 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 https://dx.doi.org/10.1007/s11664-021-08970-0 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 50 2021 8 17 05 4469-4479 |
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10.1007/s11664-021-08970-0 doi (DE-627)SPR044402805 (SPR)s11664-021-08970-0-e DE-627 ger DE-627 rakwb eng Zheng, Dianliang verfasserin aut Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2021 Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 Wei, Feiming aut Xu, Yonggang aut Chen, Teng aut Dai, Fei aut Liu, Ting aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 50(2021), 8 vom: 17. Mai, Seite 4469-4479 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 https://dx.doi.org/10.1007/s11664-021-08970-0 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 50 2021 8 17 05 4469-4479 |
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10.1007/s11664-021-08970-0 doi (DE-627)SPR044402805 (SPR)s11664-021-08970-0-e DE-627 ger DE-627 rakwb eng Zheng, Dianliang verfasserin aut Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2021 Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 Wei, Feiming aut Xu, Yonggang aut Chen, Teng aut Dai, Fei aut Liu, Ting aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 50(2021), 8 vom: 17. Mai, Seite 4469-4479 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 https://dx.doi.org/10.1007/s11664-021-08970-0 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 50 2021 8 17 05 4469-4479 |
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Enthalten in Journal of electronic materials 50(2021), 8 vom: 17. Mai, Seite 4469-4479 volume:50 year:2021 number:8 day:17 month:05 pages:4469-4479 |
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Zheng, Dianliang @@aut@@ Wei, Feiming @@aut@@ Xu, Yonggang @@aut@@ Chen, Teng @@aut@@ Dai, Fei @@aut@@ Liu, Ting @@aut@@ |
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In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. 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| author |
Zheng, Dianliang |
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Zheng, Dianliang misc Scaled measurement misc absorbing material misc tunable absorber misc magnetorheological fluid Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
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Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field Scaled measurement (dpeaa)DE-He213 absorbing material (dpeaa)DE-He213 tunable absorber (dpeaa)DE-He213 magnetorheological fluid (dpeaa)DE-He213 |
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Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
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Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
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Zheng, Dianliang |
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Zheng, Dianliang Wei, Feiming Xu, Yonggang Chen, Teng Dai, Fei Liu, Ting |
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Zheng, Dianliang |
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10.1007/s11664-021-08970-0 |
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design of a tunable scaled absorber using magnetorheological fluid under a magnetic field |
| title_auth |
Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
| abstract |
Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. © The Minerals, Metals & Materials Society 2021 |
| abstractGer |
Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. © The Minerals, Metals & Materials Society 2021 |
| abstract_unstemmed |
Abstract In order to achieve wideband scaled measurement of low observable object scattering characteristics, the scaling design of the related absorbing material has been within the scope of researchers over recent years. In this work, a tunable material was designed to meet the wideband and high-precision requirements for scaling measurements. The material was produced using magnetorheological (MR) fluid, composed of silicon rubber and flaky carbonyl iron particles (CIPs), and an electric magnet. According to the results, applying the magnetic field made the CIPs in the MR fluid aligned with respect to different parallelism depth. Furthermore, the larger the field strength, the lower the permittivity and the higher the permeability. Based on the Maxwell–Garnett mixing rule, two parameters could be interpolated within a frequency range of 18–40 GHz. Changing the magnetic field resulted in the tunable absorbing property of the composite at frequencies of 2–40 GHz and the adjustable reflection loss in the region of −22 dB to –3 dB. While the thickness of the full-size absorbing coating was 0.7–0.9 mm at 10 GHz and a scale factor of 4, the designed material was as thick as 0.8 mm, and the average radar cross-section (RCS) error of coating plates was less than 0.5 dB. In addition, the scaled frequency band could be tunable within a range of 36–40 GHz as the absorber was as thin as 2 mm, and the mean RCS error was found to be less than 0.6 dB. Therefore, the MR fluid was shown to be a promising candidate for scaled measurements. © The Minerals, Metals & Materials Society 2021 |
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Design of a Tunable Scaled Absorber Using Magnetorheological Fluid Under a Magnetic Field |
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https://dx.doi.org/10.1007/s11664-021-08970-0 |
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Wei, Feiming Xu, Yonggang Chen, Teng Dai, Fei Liu, Ting |
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10.1007/s11664-021-08970-0 |
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2024-07-04T00:30:36.447Z |
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| score |
7.3964148 |