Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics
Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and p...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Khobragade, Sandip [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2019 |
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| Schlagwörter: |
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| Anmerkung: |
© The Minerals, Metals & Materials Society 2019 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 49(2019), 2 vom: 26. Nov., Seite 1194-1203 |
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| Übergeordnetes Werk: |
volume:49 ; year:2019 ; number:2 ; day:26 ; month:11 ; pages:1194-1203 |
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| DOI / URN: |
10.1007/s11664-019-07821-3 |
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| Katalog-ID: |
SPR021565546 |
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| 245 | 1 | 0 | |a Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
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| 520 | |a Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. | ||
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10.1007/s11664-019-07821-3 doi (DE-627)SPR021565546 (SPR)s11664-019-07821-3-e DE-627 ger DE-627 rakwb eng Khobragade, Sandip verfasserin aut Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2019 Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 Patel, Satyanarayan (orcid)0000-0002-4165-1040 aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2019), 2 vom: 26. Nov., Seite 1194-1203 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 https://dx.doi.org/10.1007/s11664-019-07821-3 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2019 2 26 11 1194-1203 |
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10.1007/s11664-019-07821-3 doi (DE-627)SPR021565546 (SPR)s11664-019-07821-3-e DE-627 ger DE-627 rakwb eng Khobragade, Sandip verfasserin aut Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2019 Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 Patel, Satyanarayan (orcid)0000-0002-4165-1040 aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2019), 2 vom: 26. Nov., Seite 1194-1203 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 https://dx.doi.org/10.1007/s11664-019-07821-3 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2019 2 26 11 1194-1203 |
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10.1007/s11664-019-07821-3 doi (DE-627)SPR021565546 (SPR)s11664-019-07821-3-e DE-627 ger DE-627 rakwb eng Khobragade, Sandip verfasserin aut Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2019 Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 Patel, Satyanarayan (orcid)0000-0002-4165-1040 aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2019), 2 vom: 26. Nov., Seite 1194-1203 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 https://dx.doi.org/10.1007/s11664-019-07821-3 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2019 2 26 11 1194-1203 |
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10.1007/s11664-019-07821-3 doi (DE-627)SPR021565546 (SPR)s11664-019-07821-3-e DE-627 ger DE-627 rakwb eng Khobragade, Sandip verfasserin aut Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2019 Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 Patel, Satyanarayan (orcid)0000-0002-4165-1040 aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2019), 2 vom: 26. Nov., Seite 1194-1203 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 https://dx.doi.org/10.1007/s11664-019-07821-3 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2019 2 26 11 1194-1203 |
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10.1007/s11664-019-07821-3 doi (DE-627)SPR021565546 (SPR)s11664-019-07821-3-e DE-627 ger DE-627 rakwb eng Khobragade, Sandip verfasserin aut Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2019 Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 Patel, Satyanarayan (orcid)0000-0002-4165-1040 aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 49(2019), 2 vom: 26. Nov., Seite 1194-1203 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 https://dx.doi.org/10.1007/s11664-019-07821-3 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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 49 2019 2 26 11 1194-1203 |
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Enthalten in Journal of electronic materials 49(2019), 2 vom: 26. Nov., Seite 1194-1203 volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 |
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Enthalten in Journal of electronic materials 49(2019), 2 vom: 26. Nov., Seite 1194-1203 volume:49 year:2019 number:2 day:26 month:11 pages:1194-1203 |
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Khobragade, Sandip @@aut@@ Patel, Satyanarayan @@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">SPR021565546</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331055415.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11664-019-07821-3</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR021565546</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11664-019-07821-3-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">Khobragade, Sandip</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</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">© The Minerals, Metals & Materials Society 2019</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Energy harvesting</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Olsen cycle</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">ferroelectric</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">lead-free materials</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Patel, Satyanarayan</subfield><subfield code="0">(orcid)0000-0002-4165-1040</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of electronic materials</subfield><subfield code="d">Warrendale, Pa : TMS, 1972</subfield><subfield code="g">49(2019), 2 vom: 26. 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|
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Khobragade, Sandip |
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Khobragade, Sandip misc Energy harvesting misc Olsen cycle misc ferroelectric misc lead-free materials Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
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Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics Energy harvesting (dpeaa)DE-He213 Olsen cycle (dpeaa)DE-He213 ferroelectric (dpeaa)DE-He213 lead-free materials (dpeaa)DE-He213 |
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misc Energy harvesting misc Olsen cycle misc ferroelectric misc lead-free materials |
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misc Energy harvesting misc Olsen cycle misc ferroelectric misc lead-free materials |
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misc Energy harvesting misc Olsen cycle misc ferroelectric misc lead-free materials |
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Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
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(DE-627)SPR021565546 (SPR)s11664-019-07821-3-e |
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Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
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Khobragade, Sandip Patel, Satyanarayan |
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Elektronische Aufsätze |
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Khobragade, Sandip |
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10.1007/s11664-019-07821-3 |
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thermal energy harvesting capabilities in lead-free $ ba_{0.85} %$ ca_{0.15} %$ ti_{0.9−x} %$ sn_{x} %$ zr_{0.10} %$ o_{3} $ ferroelectric ceramics |
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Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
| abstract |
Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. © The Minerals, Metals & Materials Society 2019 |
| abstractGer |
Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. © The Minerals, Metals & Materials Society 2019 |
| abstract_unstemmed |
Abstract The energy harvesting potential in bulk lead-free $ Ba_{0.85} %$ Ca_{0.15} $ $ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ (BCT–BZT-Sn) ferroelectric ceramic has been investigated. All the compositions (x = 0.01, 0.02, 0.04, and 0.06) were fabricated by the solid-state reaction route and possessed a single-phase perovskite structure, whereas a small amount of secondary phase was observed in the x = 0.06 sample. The Olsen cycle was used to estimate the enhanced thermal energy harvesting performance over a wide range of temperatures and electric field strengths. The energy conversion density increases up to x = 0.02 and decreases thereafter owing to a reduction in the hysteresis loop area. The maximum energy conversion density for the BCT–BZT-Sn composition were found to be 306 kJ/$ m^{3} $, 332 kJ/$ m^{3} $, 226 kJ/$ m^{3} $ and 167.6 kJ/$ m^{3} $ for x = 0.01, 0.02, 0.04 and 0.06, respectively, for a temperature range of 303–373 K and an electric field of 1–29 kV/cm. These values are three times higher than that of the soft $ PbZrTiO_{3} $ which has an almost equivalent piezoelectric performance as $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9} %$ Zr_{0.10} %$ O_{3} $ at room temperature. The obtained energy conversion is also higher than most other lead-based and lead-free ferroelectric bulk materials. © The Minerals, Metals & Materials Society 2019 |
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| title_short |
Thermal Energy Harvesting Capabilities in Lead-Free $ Ba_{0.85} %$ Ca_{0.15} %$ Ti_{0.9−x} %$ Sn_{x} %$ Zr_{0.10} %$ O_{3} $ Ferroelectric Ceramics |
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https://dx.doi.org/10.1007/s11664-019-07821-3 |
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Patel, Satyanarayan |
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| doi_str |
10.1007/s11664-019-07821-3 |
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2024-07-03T23:20:33.977Z |
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| score |
7.399658 |