Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites
To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Fu, Jiyong [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
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2016transfer abstract |
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5 |
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| Übergeordnetes Werk: |
Enthalten in: Transient response and failure of medium density fibreboard panels subjected to air-blast loading - Langdon, G.S. ELSEVIER, 2021, Amsterdam |
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| Übergeordnetes Werk: |
volume:380 ; year:2016 ; number:20 ; day:29 ; month:04 ; pages:1788-1792 ; extent:5 |
| Links: |
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| DOI / URN: |
10.1016/j.physleta.2016.03.024 |
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ELV035333464 |
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| 245 | 1 | 0 | |a Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites |
| 264 | 1 | |c 2016transfer abstract | |
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| 520 | |a To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. | ||
| 520 | |a To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. | ||
| 650 | 7 | |a Magnetoelectric coupling |2 Elsevier | |
| 650 | 7 | |a Piezoelectric coupling |2 Elsevier | |
| 700 | 1 | |a Santa Rosa, Washington |4 oth | |
| 700 | 1 | |a M'Peko, Jean Claude |4 oth | |
| 700 | 1 | |a Algueró, Miguel |4 oth | |
| 700 | 1 | |a Venet, Michel |4 oth | |
| 773 | 0 | 8 | |i Enthalten in |n North-Holland Publ |a Langdon, G.S. ELSEVIER |t Transient response and failure of medium density fibreboard panels subjected to air-blast loading |d 2021 |g Amsterdam |w (DE-627)ELV006407811 |
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10.1016/j.physleta.2016.03.024 doi GBVA2016012000006.pica (DE-627)ELV035333464 (ELSEVIER)S0375-9601(16)30003-2 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Fu, Jiyong verfasserin aut Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. Magnetoelectric coupling Elsevier Piezoelectric coupling Elsevier Santa Rosa, Washington oth M'Peko, Jean Claude oth Algueró, Miguel oth Venet, Michel oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:20 day:29 month:04 pages:1788-1792 extent:5 https://doi.org/10.1016/j.physleta.2016.03.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 20 29 0429 1788-1792 5 045F 530 |
| spelling |
10.1016/j.physleta.2016.03.024 doi GBVA2016012000006.pica (DE-627)ELV035333464 (ELSEVIER)S0375-9601(16)30003-2 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Fu, Jiyong verfasserin aut Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. Magnetoelectric coupling Elsevier Piezoelectric coupling Elsevier Santa Rosa, Washington oth M'Peko, Jean Claude oth Algueró, Miguel oth Venet, Michel oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:20 day:29 month:04 pages:1788-1792 extent:5 https://doi.org/10.1016/j.physleta.2016.03.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 20 29 0429 1788-1792 5 045F 530 |
| allfields_unstemmed |
10.1016/j.physleta.2016.03.024 doi GBVA2016012000006.pica (DE-627)ELV035333464 (ELSEVIER)S0375-9601(16)30003-2 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Fu, Jiyong verfasserin aut Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. Magnetoelectric coupling Elsevier Piezoelectric coupling Elsevier Santa Rosa, Washington oth M'Peko, Jean Claude oth Algueró, Miguel oth Venet, Michel oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:20 day:29 month:04 pages:1788-1792 extent:5 https://doi.org/10.1016/j.physleta.2016.03.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 20 29 0429 1788-1792 5 045F 530 |
| allfieldsGer |
10.1016/j.physleta.2016.03.024 doi GBVA2016012000006.pica (DE-627)ELV035333464 (ELSEVIER)S0375-9601(16)30003-2 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Fu, Jiyong verfasserin aut Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. Magnetoelectric coupling Elsevier Piezoelectric coupling Elsevier Santa Rosa, Washington oth M'Peko, Jean Claude oth Algueró, Miguel oth Venet, Michel oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:20 day:29 month:04 pages:1788-1792 extent:5 https://doi.org/10.1016/j.physleta.2016.03.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 20 29 0429 1788-1792 5 045F 530 |
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10.1016/j.physleta.2016.03.024 doi GBVA2016012000006.pica (DE-627)ELV035333464 (ELSEVIER)S0375-9601(16)30003-2 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Fu, Jiyong verfasserin aut Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. Magnetoelectric coupling Elsevier Piezoelectric coupling Elsevier Santa Rosa, Washington oth M'Peko, Jean Claude oth Algueró, Miguel oth Venet, Michel oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:20 day:29 month:04 pages:1788-1792 extent:5 https://doi.org/10.1016/j.physleta.2016.03.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 20 29 0429 1788-1792 5 045F 530 |
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magnetoelectric coupling in lead-free piezoelectric li x (k0.5na0.5)1− x nb1− y ta y o3 and magnetostrictive cofe2o4 laminated composites |
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Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites |
| abstract |
To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. |
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To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. |
| abstract_unstemmed |
To replace lead zirconium titanate in magnetoelectric (ME) composites owing to concerns regarding its toxicity, we investigate the ME coupling in bilayer composites comprising lead-free Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 (LKNNT) (piezoelectric) and CoFe2O4 (magnetostrictive) phases. We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. The effect of the volume fraction and interface parameter on the ME coupling is also discussed. |
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Magnetoelectric coupling in lead-free piezoelectric Li x (K0.5Na0.5)1− x Nb1− y Ta y O3 and magnetostrictive CoFe2O4 laminated composites |
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We prepare the LKNNT ceramics and measure its piezoelectric coefficient d 31 , a crucial ingredient determining ME couplings, for several Li ( x = 0.03 , 0.035 , 0.04 ) and Ta ( y = 0.15 , 0.2 , 0.25 ) concentrations, and find that the highest d 31 occurs at y = 0.2 for all the values of x studied here. We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). 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We then evaluate both the transverse ( α E , 31 ) and the longitudinal ( α E , 33 ) low-frequency ME coupling coefficients of our composites, for each the above composition of ( x , y ). At x = 0.03 , we find the usual scenario of α E , 31 and α E , 33 , i.e., the strongest ME coupling occurs when d 31 is maximal, namely at y = 0.2 . On the other hand, interestingly, we also obtain the strongest ME coupling when the LKNNT layer has a relatively weaker d 31 , e.g., at y = 0.25 for x = 0.035 and y = 0.15 for x = 0.04 , following from the interplay of d 31 and other ingredients (e.g., dielectric constant). Our calculated ME couplings, with α E , 31 in magnitude around twice of α E , 33 , are comparable to those in lead-based composites. 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