Multilayer transducer transfer matrix formalism
A complete formulation of direct and inverse 4 /spl times/ 4 transfer matrices for parallel and series, electrically connected, mechanically stacked, 1-D thickness mode multilayer piezoelectric transducers is presented. Complex coefficients account for the mechanical, dielectric, and piezoelectric l...
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Veröffentlicht in: | IEEE transactions on ultrasonics, ferroelectrics, and frequency control ferroelectrics, and frequency control, 2002-09, Vol.49 (9), p.1300-1311 |
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description | A complete formulation of direct and inverse 4 /spl times/ 4 transfer matrices for parallel and series, electrically connected, mechanically stacked, 1-D thickness mode multilayer piezoelectric transducers is presented. Complex coefficients account for the mechanical, dielectric, and piezoelectric losses. The direct or inverse 4 /spl times/ 4 transfer matrix transfers quantities at the top surface into their values at the bottom surface or vice versa, respectively. The 4 /spl times/ 4 transfer matrices derive from the 3 /spl times/ 3 transfer matrices, which follow from the 3 /spl times/ 3 matrix for the general three-port. For both parallel and series connections, the 3 /spl times/ 3 and 4 /spl times/ 4 direct and inverse transfer matrices are interrelated through transformation symmetries; also, the inverse matrix can be obtained from the direct matrix by changing the sign of both the piezoelectric coefficient and the explicitly occurring complex variable, j. For the electrically parallel connected case, explicit voltage orientation reversals occur at successive piezoelectric layers. Cascading the 4 /spl times/ 4 matrices yields the sum of the currents through the piezoelectric layers for the electrically parallel-connected case and the sum of the voltage differences across the layers for the electrically series-connected case. The resultant matrices are calculated for the cascading of n identical piezoelectric layers connected in parallel and series. |
doi_str_mv | 10.1109/TUFFC.2002.1041547 |
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Complex coefficients account for the mechanical, dielectric, and piezoelectric losses. The direct or inverse 4 /spl times/ 4 transfer matrix transfers quantities at the top surface into their values at the bottom surface or vice versa, respectively. The 4 /spl times/ 4 transfer matrices derive from the 3 /spl times/ 3 transfer matrices, which follow from the 3 /spl times/ 3 matrix for the general three-port. For both parallel and series connections, the 3 /spl times/ 3 and 4 /spl times/ 4 direct and inverse transfer matrices are interrelated through transformation symmetries; also, the inverse matrix can be obtained from the direct matrix by changing the sign of both the piezoelectric coefficient and the explicitly occurring complex variable, j. For the electrically parallel connected case, explicit voltage orientation reversals occur at successive piezoelectric layers. Cascading the 4 /spl times/ 4 matrices yields the sum of the currents through the piezoelectric layers for the electrically parallel-connected case and the sum of the voltage differences across the layers for the electrically series-connected case. The resultant matrices are calculated for the cascading of n identical piezoelectric layers connected in parallel and series.</description><identifier>ISSN: 0885-3010</identifier><identifier>EISSN: 1525-8955</identifier><identifier>DOI: 10.1109/TUFFC.2002.1041547</identifier><identifier>PMID: 12243581</identifier><identifier>CODEN: ITUCER</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Acoustics ; Biomedical transducers ; Cascading ; Dielectric losses ; Electric potential ; Exact sciences and technology ; Fundamental areas of phenomenology (including applications) ; Impedance ; Inverse ; Mathematical analysis ; Mathematics ; Matrices ; Models, Theoretical ; Multilayers ; Nonhomogeneous media ; Physics ; Piezoelectric materials ; Piezoelectric transducers ; Piezoelectricity ; Postal services ; Surface treatment ; Transducers ; Transduction; acoustical devices for the generation and reproduction of sound ; Transfer matrices ; Ultrasonics ; Voltage</subject><ispartof>IEEE transactions on ultrasonics, ferroelectrics, and frequency control, 2002-09, Vol.49 (9), p.1300-1311</ispartof><rights>2002 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2002</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c505t-5a5d08e675c8c047b53c008e290c612eb8ed9018a431cabb41fe5b3b724e7f13</citedby><cites>FETCH-LOGICAL-c505t-5a5d08e675c8c047b53c008e290c612eb8ed9018a431cabb41fe5b3b724e7f13</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1041547$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27922,27923,54756</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/1041547$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=13893651$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/12243581$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Bloomfield, P.E.</creatorcontrib><title>Multilayer transducer transfer matrix formalism</title><title>IEEE transactions on ultrasonics, ferroelectrics, and frequency control</title><addtitle>T-UFFC</addtitle><addtitle>IEEE Trans Ultrason Ferroelectr Freq Control</addtitle><description>A complete formulation of direct and inverse 4 /spl times/ 4 transfer matrices for parallel and series, electrically connected, mechanically stacked, 1-D thickness mode multilayer piezoelectric transducers is presented. Complex coefficients account for the mechanical, dielectric, and piezoelectric losses. The direct or inverse 4 /spl times/ 4 transfer matrix transfers quantities at the top surface into their values at the bottom surface or vice versa, respectively. The 4 /spl times/ 4 transfer matrices derive from the 3 /spl times/ 3 transfer matrices, which follow from the 3 /spl times/ 3 matrix for the general three-port. For both parallel and series connections, the 3 /spl times/ 3 and 4 /spl times/ 4 direct and inverse transfer matrices are interrelated through transformation symmetries; also, the inverse matrix can be obtained from the direct matrix by changing the sign of both the piezoelectric coefficient and the explicitly occurring complex variable, j. For the electrically parallel connected case, explicit voltage orientation reversals occur at successive piezoelectric layers. Cascading the 4 /spl times/ 4 matrices yields the sum of the currents through the piezoelectric layers for the electrically parallel-connected case and the sum of the voltage differences across the layers for the electrically series-connected case. The resultant matrices are calculated for the cascading of n identical piezoelectric layers connected in parallel and series.</description><subject>Acoustics</subject><subject>Biomedical transducers</subject><subject>Cascading</subject><subject>Dielectric losses</subject><subject>Electric potential</subject><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Impedance</subject><subject>Inverse</subject><subject>Mathematical analysis</subject><subject>Mathematics</subject><subject>Matrices</subject><subject>Models, Theoretical</subject><subject>Multilayers</subject><subject>Nonhomogeneous media</subject><subject>Physics</subject><subject>Piezoelectric materials</subject><subject>Piezoelectric transducers</subject><subject>Piezoelectricity</subject><subject>Postal services</subject><subject>Surface treatment</subject><subject>Transducers</subject><subject>Transduction; acoustical devices for the generation and reproduction of sound</subject><subject>Transfer matrices</subject><subject>Ultrasonics</subject><subject>Voltage</subject><issn>0885-3010</issn><issn>1525-8955</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><sourceid>EIF</sourceid><recordid>eNqFkV1LwzAUhoMobk7_gIKIoF51OycfbXIpw6kw8WZehzRLoaNdZ9KC-_e2rjLxQq9yCM_7Hg4PIecIY0RQk8XbbDYdUwA6RuAoeHJAhiioiKQS4pAMQUoRMUAYkJMQVgDIuaLHZICUciYkDsnkpSnqvDBb569qb9Zh2djvMWuH0tQ-_7jKKl-aIg_lKTnKTBHcWf-OyGL2sJg-RfPXx-fp_TyyAkQdCSOWIF2cCCst8CQVzEL7QRXYGKlLpVsqQGk4Q2vSlGPmRMrShHKXZMhG5G5Xu_HVe-NCrcs8WFcUZu2qJmgFiWqjLG7J2z_JhCJIlfwPUsmBxrLbff0LXFWNX7fXaik5ZzFC10Z3kPVVCN5leuPz0vitRtCdHf1lR3d2dG-nDV32zU1auuU-0utogZseMMGaImst2DzsOSYVi0XHXey43Dn3Y_NuzSe8Sp5q</recordid><startdate>20020901</startdate><enddate>20020901</enddate><creator>Bloomfield, P.E.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20020901</creationdate><title>Multilayer transducer transfer matrix formalism</title><author>Bloomfield, P.E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c505t-5a5d08e675c8c047b53c008e290c612eb8ed9018a431cabb41fe5b3b724e7f13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2002</creationdate><topic>Acoustics</topic><topic>Biomedical transducers</topic><topic>Cascading</topic><topic>Dielectric losses</topic><topic>Electric potential</topic><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Impedance</topic><topic>Inverse</topic><topic>Mathematical analysis</topic><topic>Mathematics</topic><topic>Matrices</topic><topic>Models, Theoretical</topic><topic>Multilayers</topic><topic>Nonhomogeneous media</topic><topic>Physics</topic><topic>Piezoelectric materials</topic><topic>Piezoelectric transducers</topic><topic>Piezoelectricity</topic><topic>Postal services</topic><topic>Surface treatment</topic><topic>Transducers</topic><topic>Transduction; acoustical devices for the generation and reproduction of sound</topic><topic>Transfer matrices</topic><topic>Ultrasonics</topic><topic>Voltage</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bloomfield, P.E.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>Pascal-Francis</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>IEEE transactions on ultrasonics, ferroelectrics, and frequency control</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Bloomfield, P.E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Multilayer transducer transfer matrix formalism</atitle><jtitle>IEEE transactions on ultrasonics, ferroelectrics, and frequency control</jtitle><stitle>T-UFFC</stitle><addtitle>IEEE Trans Ultrason Ferroelectr Freq Control</addtitle><date>2002-09-01</date><risdate>2002</risdate><volume>49</volume><issue>9</issue><spage>1300</spage><epage>1311</epage><pages>1300-1311</pages><issn>0885-3010</issn><eissn>1525-8955</eissn><coden>ITUCER</coden><abstract>A complete formulation of direct and inverse 4 /spl times/ 4 transfer matrices for parallel and series, electrically connected, mechanically stacked, 1-D thickness mode multilayer piezoelectric transducers is presented. Complex coefficients account for the mechanical, dielectric, and piezoelectric losses. The direct or inverse 4 /spl times/ 4 transfer matrix transfers quantities at the top surface into their values at the bottom surface or vice versa, respectively. The 4 /spl times/ 4 transfer matrices derive from the 3 /spl times/ 3 transfer matrices, which follow from the 3 /spl times/ 3 matrix for the general three-port. For both parallel and series connections, the 3 /spl times/ 3 and 4 /spl times/ 4 direct and inverse transfer matrices are interrelated through transformation symmetries; also, the inverse matrix can be obtained from the direct matrix by changing the sign of both the piezoelectric coefficient and the explicitly occurring complex variable, j. For the electrically parallel connected case, explicit voltage orientation reversals occur at successive piezoelectric layers. Cascading the 4 /spl times/ 4 matrices yields the sum of the currents through the piezoelectric layers for the electrically parallel-connected case and the sum of the voltage differences across the layers for the electrically series-connected case. The resultant matrices are calculated for the cascading of n identical piezoelectric layers connected in parallel and series.</abstract><cop>New York, NY</cop><pub>IEEE</pub><pmid>12243581</pmid><doi>10.1109/TUFFC.2002.1041547</doi><tpages>12</tpages></addata></record> |
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subjects | Acoustics Biomedical transducers Cascading Dielectric losses Electric potential Exact sciences and technology Fundamental areas of phenomenology (including applications) Impedance Inverse Mathematical analysis Mathematics Matrices Models, Theoretical Multilayers Nonhomogeneous media Physics Piezoelectric materials Piezoelectric transducers Piezoelectricity Postal services Surface treatment Transducers Transduction acoustical devices for the generation and reproduction of sound Transfer matrices Ultrasonics Voltage |
title | Multilayer transducer transfer matrix formalism |
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