High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices

The ceramics, (0.65 + y)Pb(Zr0.47Ti0.53)–(0.35 − y)Pb[(Ni1−xZnx)1/3Nb2/3]O3 have a morphotropic phase boundary (MPB) of pseudo‐cubic and tetragonal structures. Their ε33T/ε0 value considerably decreased on the pseudo‐cubic side of the MPB composition, but the d33 and kp slowly decreased on both side...

Ausführliche Beschreibung

Gespeichert in:

Bibliographische Detailangaben
Veröffentlicht in:	Journal of the American Ceramic Society 2011-11, Vol.94 (11), p.3629-3631
Hauptverfasser:	Seo, In-Tae, Cha, Yu-Joung, Kang, In-Young, Choi, Jae-Hong, Nahm, Sahn, Seung, Tae-Hyun, Paik, Jong-Hoo
Format:	Artikel
Sprache:	eng
Schlagworte:	Ceramics Coefficients Crystal structure Crystallography Devices Dielectric constant Electric properties Energy density Energy harvesting Harvesting Joining Permittivity Phase boundaries Piezoelectric ceramics Piezoelectricity Polycrystals
Online-Zugang:	Volltext
Tags:	Tag hinzufügen Keine Tags, Fügen Sie den ersten Tag hinzu!

container_end_page	3631
container_issue	11
container_start_page	3629
container_title	Journal of the American Ceramic Society
container_volume	94
creator	Seo, In-Tae Cha, Yu-Joung Kang, In-Young Choi, Jae-Hong Nahm, Sahn Seung, Tae-Hyun Paik, Jong-Hoo
description	The ceramics, (0.65 + y)Pb(Zr0.47Ti0.53)–(0.35 − y)Pb[(Ni1−xZnx)1/3Nb2/3]O3 have a morphotropic phase boundary (MPB) of pseudo‐cubic and tetragonal structures. Their ε33T/ε0 value considerably decreased on the pseudo‐cubic side of the MPB composition, but the d33 and kp slowly decreased on both sides of the MPB. Therefore, the maximum transduction coefficient (d33 * g33) was obtained from the composition on the pseudo‐cubic side of the MPB, because g33 is given by d33/ε33T. This result could be applied to other systems containing an MPB of pseudo‐cubic and tetragonal structures. Furthermore, a d33 * g33 value of 20 056 × 10−15 m2/N, which is the highest value reported so far for polycrystalline ceramics, was obtained from the 0.68Pb(Zr0.47Ti0.53)O3–0.32Pb(Ni0.6Zn0.4)1/3Nb2/3O3 ceramic.
doi_str_mv	10.1111/j.1551-2916.2011.04817.x
format	Article
fullrecord	<record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_1692385158</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1010927481</sourcerecordid><originalsourceid>FETCH-LOGICAL-c5777-c57ba87e5c0ef973f5815e1055d7a90d93512f3ad7b8914e10673b2d21c32c263</originalsourceid><addsrcrecordid>eNqNkUFvEzEQha0KJELhP6x64rJbj72O7QtStU27LVUhUhFHy3Fmg8Nmt9hJm_TX10toD1yID_ZY872n0TxCMqAFpHO6LEAIyJmGccEoQEFLBbLYHpHRa-MNGVFKWS4Vo-_I-xiX6QtalSNS137xM5t0GBa77By76Ne77JvHpx5bdOvgXVZhsCvvYtb04YWsbXjAuPbdIokevMP4gbxtbBvx49_3mHy_mNxVdX7z9fKqOrvJnZBSDvfMKonCUWy05I1QIBCoEHNpNZ1rLoA13M7lTGkoU2cs-YzNGTjOHBvzY_Jp73sf-t-bNINZ-eiwbW2H_SYaGGvGlQChDkBLxphWUv4fpUA1k2m1B6GDpRxmPfkHXfab0KX1GE1LrjiHMkFqD7nQxxiwMffBr2zYJSczRGyWZkjSDEmaIWLzJ2KzTdLPe-mjb3F3sM5cn1WToUwG-d7AxzVuXw1s-GXS2qUwP24vDZ3W1fl0eme-8GfD1bhr</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>904383314</pqid></control><display><type>article</type><title>High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices</title><source>Access via Wiley Online Library</source><creator>Seo, In-Tae ; Cha, Yu-Joung ; Kang, In-Young ; Choi, Jae-Hong ; Nahm, Sahn ; Seung, Tae-Hyun ; Paik, Jong-Hoo</creator><contributor>Priya, S. ; Priya, S.</contributor><creatorcontrib>Seo, In-Tae ; Cha, Yu-Joung ; Kang, In-Young ; Choi, Jae-Hong ; Nahm, Sahn ; Seung, Tae-Hyun ; Paik, Jong-Hoo ; Priya, S. ; Priya, S.</creatorcontrib><description>The ceramics, (0.65 + y)Pb(Zr0.47Ti0.53)–(0.35 − y)Pb[(Ni1−xZnx)1/3Nb2/3]O3 have a morphotropic phase boundary (MPB) of pseudo‐cubic and tetragonal structures. Their ε33T/ε0 value considerably decreased on the pseudo‐cubic side of the MPB composition, but the d33 and kp slowly decreased on both sides of the MPB. Therefore, the maximum transduction coefficient (d33 * g33) was obtained from the composition on the pseudo‐cubic side of the MPB, because g33 is given by d33/ε33T. This result could be applied to other systems containing an MPB of pseudo‐cubic and tetragonal structures. Furthermore, a d33 * g33 value of 20 056 × 10−15 m2/N, which is the highest value reported so far for polycrystalline ceramics, was obtained from the 0.68Pb(Zr0.47Ti0.53)O3–0.32Pb(Ni0.6Zn0.4)1/3Nb2/3O3 ceramic.</description><identifier>ISSN: 0002-7820</identifier><identifier>EISSN: 1551-2916</identifier><identifier>DOI: 10.1111/j.1551-2916.2011.04817.x</identifier><identifier>CODEN: JACTAW</identifier><language>eng</language><publisher>Columbus: Blackwell Publishing Ltd</publisher><subject>Ceramics ; Coefficients ; Crystal structure ; Crystallography ; Devices ; Dielectric constant ; Electric properties ; Energy density ; Energy harvesting ; Harvesting ; Joining ; Permittivity ; Phase boundaries ; Piezoelectric ceramics ; Piezoelectricity ; Polycrystals</subject><ispartof>Journal of the American Ceramic Society, 2011-11, Vol.94 (11), p.3629-3631</ispartof><rights>2011 The American Ceramic Society</rights><rights>Copyright American Ceramic Society Nov 2011</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c5777-c57ba87e5c0ef973f5815e1055d7a90d93512f3ad7b8914e10673b2d21c32c263</citedby><cites>FETCH-LOGICAL-c5777-c57ba87e5c0ef973f5815e1055d7a90d93512f3ad7b8914e10673b2d21c32c263</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1111%2Fj.1551-2916.2011.04817.x$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1111%2Fj.1551-2916.2011.04817.x$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27924,27925,45574,45575</link.rule.ids></links><search><contributor>Priya, S.</contributor><contributor>Priya, S.</contributor><creatorcontrib>Seo, In-Tae</creatorcontrib><creatorcontrib>Cha, Yu-Joung</creatorcontrib><creatorcontrib>Kang, In-Young</creatorcontrib><creatorcontrib>Choi, Jae-Hong</creatorcontrib><creatorcontrib>Nahm, Sahn</creatorcontrib><creatorcontrib>Seung, Tae-Hyun</creatorcontrib><creatorcontrib>Paik, Jong-Hoo</creatorcontrib><title>High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices</title><title>Journal of the American Ceramic Society</title><addtitle>J. Am. Ceram. Soc</addtitle><description>The ceramics, (0.65 + y)Pb(Zr0.47Ti0.53)–(0.35 − y)Pb[(Ni1−xZnx)1/3Nb2/3]O3 have a morphotropic phase boundary (MPB) of pseudo‐cubic and tetragonal structures. Their ε33T/ε0 value considerably decreased on the pseudo‐cubic side of the MPB composition, but the d33 and kp slowly decreased on both sides of the MPB. Therefore, the maximum transduction coefficient (d33 * g33) was obtained from the composition on the pseudo‐cubic side of the MPB, because g33 is given by d33/ε33T. This result could be applied to other systems containing an MPB of pseudo‐cubic and tetragonal structures. Furthermore, a d33 * g33 value of 20 056 × 10−15 m2/N, which is the highest value reported so far for polycrystalline ceramics, was obtained from the 0.68Pb(Zr0.47Ti0.53)O3–0.32Pb(Ni0.6Zn0.4)1/3Nb2/3O3 ceramic.</description><subject>Ceramics</subject><subject>Coefficients</subject><subject>Crystal structure</subject><subject>Crystallography</subject><subject>Devices</subject><subject>Dielectric constant</subject><subject>Electric properties</subject><subject>Energy density</subject><subject>Energy harvesting</subject><subject>Harvesting</subject><subject>Joining</subject><subject>Permittivity</subject><subject>Phase boundaries</subject><subject>Piezoelectric ceramics</subject><subject>Piezoelectricity</subject><subject>Polycrystals</subject><issn>0002-7820</issn><issn>1551-2916</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqNkUFvEzEQha0KJELhP6x64rJbj72O7QtStU27LVUhUhFHy3Fmg8Nmt9hJm_TX10toD1yID_ZY872n0TxCMqAFpHO6LEAIyJmGccEoQEFLBbLYHpHRa-MNGVFKWS4Vo-_I-xiX6QtalSNS137xM5t0GBa77By76Ne77JvHpx5bdOvgXVZhsCvvYtb04YWsbXjAuPbdIokevMP4gbxtbBvx49_3mHy_mNxVdX7z9fKqOrvJnZBSDvfMKonCUWy05I1QIBCoEHNpNZ1rLoA13M7lTGkoU2cs-YzNGTjOHBvzY_Jp73sf-t-bNINZ-eiwbW2H_SYaGGvGlQChDkBLxphWUv4fpUA1k2m1B6GDpRxmPfkHXfab0KX1GE1LrjiHMkFqD7nQxxiwMffBr2zYJSczRGyWZkjSDEmaIWLzJ2KzTdLPe-mjb3F3sM5cn1WToUwG-d7AxzVuXw1s-GXS2qUwP24vDZ3W1fl0eme-8GfD1bhr</recordid><startdate>201111</startdate><enddate>201111</enddate><creator>Seo, In-Tae</creator><creator>Cha, Yu-Joung</creator><creator>Kang, In-Young</creator><creator>Choi, Jae-Hong</creator><creator>Nahm, Sahn</creator><creator>Seung, Tae-Hyun</creator><creator>Paik, Jong-Hoo</creator><general>Blackwell Publishing Ltd</general><general>Wiley Subscription Services, Inc</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>201111</creationdate><title>High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices</title><author>Seo, In-Tae ; Cha, Yu-Joung ; Kang, In-Young ; Choi, Jae-Hong ; Nahm, Sahn ; Seung, Tae-Hyun ; Paik, Jong-Hoo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c5777-c57ba87e5c0ef973f5815e1055d7a90d93512f3ad7b8914e10673b2d21c32c263</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Ceramics</topic><topic>Coefficients</topic><topic>Crystal structure</topic><topic>Crystallography</topic><topic>Devices</topic><topic>Dielectric constant</topic><topic>Electric properties</topic><topic>Energy density</topic><topic>Energy harvesting</topic><topic>Harvesting</topic><topic>Joining</topic><topic>Permittivity</topic><topic>Phase boundaries</topic><topic>Piezoelectric ceramics</topic><topic>Piezoelectricity</topic><topic>Polycrystals</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Seo, In-Tae</creatorcontrib><creatorcontrib>Cha, Yu-Joung</creatorcontrib><creatorcontrib>Kang, In-Young</creatorcontrib><creatorcontrib>Choi, Jae-Hong</creatorcontrib><creatorcontrib>Nahm, Sahn</creatorcontrib><creatorcontrib>Seung, Tae-Hyun</creatorcontrib><creatorcontrib>Paik, Jong-Hoo</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of the American Ceramic Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Seo, In-Tae</au><au>Cha, Yu-Joung</au><au>Kang, In-Young</au><au>Choi, Jae-Hong</au><au>Nahm, Sahn</au><au>Seung, Tae-Hyun</au><au>Paik, Jong-Hoo</au><au>Priya, S.</au><au>Priya, S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices</atitle><jtitle>Journal of the American Ceramic Society</jtitle><addtitle>J. Am. Ceram. Soc</addtitle><date>2011-11</date><risdate>2011</risdate><volume>94</volume><issue>11</issue><spage>3629</spage><epage>3631</epage><pages>3629-3631</pages><issn>0002-7820</issn><eissn>1551-2916</eissn><coden>JACTAW</coden><abstract>The ceramics, (0.65 + y)Pb(Zr0.47Ti0.53)–(0.35 − y)Pb[(Ni1−xZnx)1/3Nb2/3]O3 have a morphotropic phase boundary (MPB) of pseudo‐cubic and tetragonal structures. Their ε33T/ε0 value considerably decreased on the pseudo‐cubic side of the MPB composition, but the d33 and kp slowly decreased on both sides of the MPB. Therefore, the maximum transduction coefficient (d33 * g33) was obtained from the composition on the pseudo‐cubic side of the MPB, because g33 is given by d33/ε33T. This result could be applied to other systems containing an MPB of pseudo‐cubic and tetragonal structures. Furthermore, a d33 * g33 value of 20 056 × 10−15 m2/N, which is the highest value reported so far for polycrystalline ceramics, was obtained from the 0.68Pb(Zr0.47Ti0.53)O3–0.32Pb(Ni0.6Zn0.4)1/3Nb2/3O3 ceramic.</abstract><cop>Columbus</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1111/j.1551-2916.2011.04817.x</doi><tpages>3</tpages></addata></record>
fulltext	fulltext
identifier	ISSN: 0002-7820
ispartof	Journal of the American Ceramic Society, 2011-11, Vol.94 (11), p.3629-3631
issn	0002-7820 1551-2916
language	eng
recordid	cdi_proquest_miscellaneous_1692385158
source	Access via Wiley Online Library
subjects	Ceramics Coefficients Crystal structure Crystallography Devices Dielectric constant Electric properties Energy density Energy harvesting Harvesting Joining Permittivity Phase boundaries Piezoelectric ceramics Piezoelectricity Polycrystals
title	High Energy Density Piezoelectric Ceramics for Energy Harvesting Devices
url	https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-26T19%3A51%3A01IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=High%20Energy%20Density%20Piezoelectric%20Ceramics%20for%20Energy%20Harvesting%20Devices&rft.jtitle=Journal%20of%20the%20American%20Ceramic%20Society&rft.au=Seo,%20In-Tae&rft.date=2011-11&rft.volume=94&rft.issue=11&rft.spage=3629&rft.epage=3631&rft.pages=3629-3631&rft.issn=0002-7820&rft.eissn=1551-2916&rft.coden=JACTAW&rft_id=info:doi/10.1111/j.1551-2916.2011.04817.x&rft_dat=%3Cproquest_cross%3E1010927481%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=904383314&rft_id=info:pmid/&rfr_iscdi=true