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Modeling a Fluid-Coupled Single Piezoelectric Micromachined Ultrasonic Transducer Using the Finite Difference Method
A complete model was developed to simulate the behavior of a circular clamped axisymmetric fluid-coupled Piezoelectric Micromachined Ultrasonic Transducer (PMUT). Combining Finite Difference and Boundary Element Matrix (FD-BEM), this model is based on the discretization of the partial differential e...
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Published in: | Micromachines (Basel) 2023-11, Vol.14 (11), p.2089 |
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description | A complete model was developed to simulate the behavior of a circular clamped axisymmetric fluid-coupled Piezoelectric Micromachined Ultrasonic Transducer (PMUT). Combining Finite Difference and Boundary Element Matrix (FD-BEM), this model is based on the discretization of the partial differential equation used to translate the mechanical behavior of a PMUT. In the model, both the axial and the transverse displacements are preserved in the equation of motion and used to properly define the neutral line position. To introduce fluid coupling, a Green’s function dedicated to axisymmetric circular radiating sources is employed. The resolution of the behavioral equations is used to establish the equivalent electroacoustic circuit of a PMUT that preserves the average particular velocity, the mechanical power, and the acoustic power. Particular consideration is given to verifying the validity of certain assumptions that are usually made across various steps of previously reported analytical models. In this framework, the advantages of the membrane discretization performed in the FD-BEM model are highlighted through accurate simulations of the first vibration mode and especially the cutoff frequency that many other models do not predict. This high cutoff frequency corresponds to cases where the spatial average velocity of the plate is null and is of great importance for PMUT design because it defines the upper limit above which the device is considered to be mechanically blocked. These modeling results are compared with electrical and dynamic membrane displacement measurements of AlN-based (500 nm thick) PMUTs in air and fluid. The first resonance frequency confrontation showed a maximum relative error of 1.13% between the FD model and Finite Element Method (FEM). Moreover, the model perfectly predicts displacement amplitudes when PMUT vibrates in a fluid, with less than 5% relative error. Displacement amplitudes of 16 nm and 20 nm were measured for PMUT with 340 µm and 275 µm diameters, respectively. This complete PMUT model using the FD-BEM approach is shown to be very efficient in terms of computation time and accuracy. |
doi_str_mv | 10.3390/mi14112089 |
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Combining Finite Difference and Boundary Element Matrix (FD-BEM), this model is based on the discretization of the partial differential equation used to translate the mechanical behavior of a PMUT. In the model, both the axial and the transverse displacements are preserved in the equation of motion and used to properly define the neutral line position. To introduce fluid coupling, a Green’s function dedicated to axisymmetric circular radiating sources is employed. The resolution of the behavioral equations is used to establish the equivalent electroacoustic circuit of a PMUT that preserves the average particular velocity, the mechanical power, and the acoustic power. Particular consideration is given to verifying the validity of certain assumptions that are usually made across various steps of previously reported analytical models. In this framework, the advantages of the membrane discretization performed in the FD-BEM model are highlighted through accurate simulations of the first vibration mode and especially the cutoff frequency that many other models do not predict. This high cutoff frequency corresponds to cases where the spatial average velocity of the plate is null and is of great importance for PMUT design because it defines the upper limit above which the device is considered to be mechanically blocked. These modeling results are compared with electrical and dynamic membrane displacement measurements of AlN-based (500 nm thick) PMUTs in air and fluid. The first resonance frequency confrontation showed a maximum relative error of 1.13% between the FD model and Finite Element Method (FEM). Moreover, the model perfectly predicts displacement amplitudes when PMUT vibrates in a fluid, with less than 5% relative error. Displacement amplitudes of 16 nm and 20 nm were measured for PMUT with 340 µm and 275 µm diameters, respectively. This complete PMUT model using the FD-BEM approach is shown to be very efficient in terms of computation time and accuracy.</description><identifier>ISSN: 2072-666X</identifier><identifier>EISSN: 2072-666X</identifier><identifier>DOI: 10.3390/mi14112089</identifier><language>eng</language><publisher>Basel: MDPI AG</publisher><subject>Acoustics ; Aluminum compounds ; Amplitudes ; characterization ; Circuits ; Deformation ; Diameters ; Differential equations ; Discretization ; Displacement ; Engineering Sciences ; Equations of motion ; Etching ; Finite difference method ; Finite element method ; Green's functions ; Hypotheses ; lumped-element ; Manufacturing ; Mathematical analysis ; Mathematical models ; Mathematical Physics ; Mechanical properties ; Mechanics ; Membranes ; MEMS ; Methods ; Microelectromechanical systems ; Micromachining ; Modelling ; Partial differential equations ; Physics ; Piezoelectricity ; PMUT ; Radiation ; Simulation methods ; Transducers ; Ultrasonic imaging ; Ultrasonic transducers ; ultrasound ; Vibration mode ; Zinc oxides</subject><ispartof>Micromachines (Basel), 2023-11, Vol.14 (11), p.2089</ispartof><rights>COPYRIGHT 2023 MDPI AG</rights><rights>2023 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>Attribution</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c467t-66546e45d089e6136a1da1568592721dc0ccf7a416cba7279c6730dcd94ed143</citedby><cites>FETCH-LOGICAL-c467t-66546e45d089e6136a1da1568592721dc0ccf7a416cba7279c6730dcd94ed143</cites><orcidid>0000-0002-2019-9390 ; 0000-0002-4458-0831 ; 0000-0003-2752-5459 ; 0000-0001-5963-7119</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2893169108/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2893169108?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>230,314,780,784,885,25753,27924,27925,37012,37013,44590,75126</link.rule.ids><backlink>$$Uhttps://hal.science/hal-04612653$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Goepfert, Valentin</creatorcontrib><creatorcontrib>Boulmé, Audren</creatorcontrib><creatorcontrib>Levassort, Franck</creatorcontrib><creatorcontrib>Merrien, Tony</creatorcontrib><creatorcontrib>Rouffaud, Rémi</creatorcontrib><creatorcontrib>Certon, Dominique</creatorcontrib><title>Modeling a Fluid-Coupled Single Piezoelectric Micromachined Ultrasonic Transducer Using the Finite Difference Method</title><title>Micromachines (Basel)</title><description>A complete model was developed to simulate the behavior of a circular clamped axisymmetric fluid-coupled Piezoelectric Micromachined Ultrasonic Transducer (PMUT). Combining Finite Difference and Boundary Element Matrix (FD-BEM), this model is based on the discretization of the partial differential equation used to translate the mechanical behavior of a PMUT. In the model, both the axial and the transverse displacements are preserved in the equation of motion and used to properly define the neutral line position. To introduce fluid coupling, a Green’s function dedicated to axisymmetric circular radiating sources is employed. The resolution of the behavioral equations is used to establish the equivalent electroacoustic circuit of a PMUT that preserves the average particular velocity, the mechanical power, and the acoustic power. Particular consideration is given to verifying the validity of certain assumptions that are usually made across various steps of previously reported analytical models. In this framework, the advantages of the membrane discretization performed in the FD-BEM model are highlighted through accurate simulations of the first vibration mode and especially the cutoff frequency that many other models do not predict. This high cutoff frequency corresponds to cases where the spatial average velocity of the plate is null and is of great importance for PMUT design because it defines the upper limit above which the device is considered to be mechanically blocked. These modeling results are compared with electrical and dynamic membrane displacement measurements of AlN-based (500 nm thick) PMUTs in air and fluid. The first resonance frequency confrontation showed a maximum relative error of 1.13% between the FD model and Finite Element Method (FEM). Moreover, the model perfectly predicts displacement amplitudes when PMUT vibrates in a fluid, with less than 5% relative error. Displacement amplitudes of 16 nm and 20 nm were measured for PMUT with 340 µm and 275 µm diameters, respectively. This complete PMUT model using the FD-BEM approach is shown to be very efficient in terms of computation time and accuracy.</description><subject>Acoustics</subject><subject>Aluminum compounds</subject><subject>Amplitudes</subject><subject>characterization</subject><subject>Circuits</subject><subject>Deformation</subject><subject>Diameters</subject><subject>Differential equations</subject><subject>Discretization</subject><subject>Displacement</subject><subject>Engineering Sciences</subject><subject>Equations of motion</subject><subject>Etching</subject><subject>Finite difference method</subject><subject>Finite element method</subject><subject>Green's functions</subject><subject>Hypotheses</subject><subject>lumped-element</subject><subject>Manufacturing</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Mathematical Physics</subject><subject>Mechanical properties</subject><subject>Mechanics</subject><subject>Membranes</subject><subject>MEMS</subject><subject>Methods</subject><subject>Microelectromechanical systems</subject><subject>Micromachining</subject><subject>Modelling</subject><subject>Partial differential equations</subject><subject>Physics</subject><subject>Piezoelectricity</subject><subject>PMUT</subject><subject>Radiation</subject><subject>Simulation methods</subject><subject>Transducers</subject><subject>Ultrasonic imaging</subject><subject>Ultrasonic transducers</subject><subject>ultrasound</subject><subject>Vibration mode</subject><subject>Zinc oxides</subject><issn>2072-666X</issn><issn>2072-666X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><sourceid>DOA</sourceid><recordid>eNpdkl1rHCEUhofSQEOSm_yCgd60hU39Gp25XLbZJLBLA9lA78TRM7sujm51ptD--jqZ0i8FldfH1-PxFMU1RjeUNuhjbzHDmKC6eVWcEyTIgnP-5fVf6zfFVUpHlJsQTR7Oi2EbDDjr96Uq1260ZrEK48mBKZ-y6KB8tPAjgAM9RKvLrdUx9EofrM_IsxuiSsHnjV1UPplRQyyf02Q3HKBcW28HKD_ZroMIXkO5heEQzGVx1imX4OrXfFHs1re71f1i8_nuYbXcLDTjYsgRV4wDq0x-EXBMucJG4YrXVUMEwUYjrTuhGOa6VYKIRnNBkdGmYWAwoxfFw2xrgjrKU7S9it9lUFa-CCHupYqD1Q5kjQwhtG4xbjFrUdeStuVI0DbfJVQ9eb2fvQ7K_WN1v9zISUOMY8Ir-g1n9t3MnmL4OkIaZG-TBueUhzAmSeqG1owwyjP69j_0GMboc1JeKMwbjOpM3czUXuVYre9CzrvO3UBvdfDQ2awvhWCUUCEm2w_zgfxbKUXofoeMkZxqRf6pFfoT1gSusw</recordid><startdate>20231101</startdate><enddate>20231101</enddate><creator>Goepfert, Valentin</creator><creator>Boulmé, Audren</creator><creator>Levassort, Franck</creator><creator>Merrien, Tony</creator><creator>Rouffaud, Rémi</creator><creator>Certon, Dominique</creator><general>MDPI AG</general><general>MDPI</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7TB</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>FR3</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>L7M</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>7X8</scope><scope>1XC</scope><scope>VOOES</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0002-2019-9390</orcidid><orcidid>https://orcid.org/0000-0002-4458-0831</orcidid><orcidid>https://orcid.org/0000-0003-2752-5459</orcidid><orcidid>https://orcid.org/0000-0001-5963-7119</orcidid></search><sort><creationdate>20231101</creationdate><title>Modeling a Fluid-Coupled Single Piezoelectric Micromachined Ultrasonic Transducer Using the Finite Difference Method</title><author>Goepfert, Valentin ; 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Combining Finite Difference and Boundary Element Matrix (FD-BEM), this model is based on the discretization of the partial differential equation used to translate the mechanical behavior of a PMUT. In the model, both the axial and the transverse displacements are preserved in the equation of motion and used to properly define the neutral line position. To introduce fluid coupling, a Green’s function dedicated to axisymmetric circular radiating sources is employed. The resolution of the behavioral equations is used to establish the equivalent electroacoustic circuit of a PMUT that preserves the average particular velocity, the mechanical power, and the acoustic power. Particular consideration is given to verifying the validity of certain assumptions that are usually made across various steps of previously reported analytical models. In this framework, the advantages of the membrane discretization performed in the FD-BEM model are highlighted through accurate simulations of the first vibration mode and especially the cutoff frequency that many other models do not predict. This high cutoff frequency corresponds to cases where the spatial average velocity of the plate is null and is of great importance for PMUT design because it defines the upper limit above which the device is considered to be mechanically blocked. These modeling results are compared with electrical and dynamic membrane displacement measurements of AlN-based (500 nm thick) PMUTs in air and fluid. The first resonance frequency confrontation showed a maximum relative error of 1.13% between the FD model and Finite Element Method (FEM). Moreover, the model perfectly predicts displacement amplitudes when PMUT vibrates in a fluid, with less than 5% relative error. Displacement amplitudes of 16 nm and 20 nm were measured for PMUT with 340 µm and 275 µm diameters, respectively. This complete PMUT model using the FD-BEM approach is shown to be very efficient in terms of computation time and accuracy.</abstract><cop>Basel</cop><pub>MDPI AG</pub><doi>10.3390/mi14112089</doi><orcidid>https://orcid.org/0000-0002-2019-9390</orcidid><orcidid>https://orcid.org/0000-0002-4458-0831</orcidid><orcidid>https://orcid.org/0000-0003-2752-5459</orcidid><orcidid>https://orcid.org/0000-0001-5963-7119</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Acoustics Aluminum compounds Amplitudes characterization Circuits Deformation Diameters Differential equations Discretization Displacement Engineering Sciences Equations of motion Etching Finite difference method Finite element method Green's functions Hypotheses lumped-element Manufacturing Mathematical analysis Mathematical models Mathematical Physics Mechanical properties Mechanics Membranes MEMS Methods Microelectromechanical systems Micromachining Modelling Partial differential equations Physics Piezoelectricity PMUT Radiation Simulation methods Transducers Ultrasonic imaging Ultrasonic transducers ultrasound Vibration mode Zinc oxides |
title | Modeling a Fluid-Coupled Single Piezoelectric Micromachined Ultrasonic Transducer Using the Finite Difference Method |
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