Radiation impedance of collapsed capacitive micromachined ultrasonic transducers
buir.contributor.author | Atalar, Abdullah | |
buir.contributor.author | Köymen, Hayrettin | |
buir.contributor.orcid | Atalar, Abdullah|0000-0002-1903-1240 | |
dc.citation.epage | 1308 | en_US |
dc.citation.issueNumber | 6 | en_US |
dc.citation.spage | 1301 | en_US |
dc.citation.volumeNumber | 59 | en_US |
dc.contributor.author | Ozgurluk, A. | en_US |
dc.contributor.author | Atalar, Abdullah | en_US |
dc.contributor.author | Köymen, Hayrettin | en_US |
dc.contributor.author | Olçum, S. | en_US |
dc.date.accessioned | 2016-02-08T09:46:08Z | |
dc.date.available | 2016-02-08T09:46:08Z | |
dc.date.issued | 2012 | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.description.abstract | The radiation impedance of a capacitive micromachined ultrasonic transducer (CMUT) array is a critical parameter to achieve high performance. In this paper, we present a calculation of the radiation impedance of collapsed, clamped, circular CMUTs both analytically and using finite element method (FEM) simulations. First, we model the radiation impedance of a single collapsed CMUT cell analytically by expressing its velocity profile as a linear combination of special functions for which the generated pressures are known. For an array of collapsed CMUT cells, the mutual impedance between the cells is also taken into account. The radiation impedances for arrays of 7, 19, 37, and 61 circular collapsed CMUT cells for different contact radii are calculated both analytically and by FEM simulations. The radiation resistance of an array reaches a plateau and maintains this level for a wide frequency range. The variation of radiation reactance with respect to frequency indicates an inductance-like behavior in the same frequency range. We find that the peak radiation resistance value is reached at higher kd values in the collapsed case as compared with the uncollapsed case, where k is the wavenumber and d is the center-to-center distance between two neighboring CMUT cells. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T09:46:08Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2012 | en |
dc.identifier.doi | 10.1109/TUFFC.2012.2321 | en_US |
dc.identifier.issn | 0885-3010 | |
dc.identifier.uri | http://hdl.handle.net/11693/21426 | |
dc.language.iso | English | en_US |
dc.publisher | Institute of Electrical and Electronics Engineers | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1109/TUFFC.2012.2321 | en_US |
dc.source.title | IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control | en_US |
dc.subject | Capacitive micromachined ultrasonic transducer | en_US |
dc.subject | Contact radius | en_US |
dc.subject | Critical parameter | en_US |
dc.subject | FEM simulations | en_US |
dc.subject | Finite element method simulation | en_US |
dc.subject | Frequency ranges | en_US |
dc.subject | Linear combinations | en_US |
dc.subject | Mutual impedance | en_US |
dc.subject | Radiation impedance | en_US |
dc.subject | Radiation resistance | en_US |
dc.subject | Special functions | en_US |
dc.subject | Velocity profiles | en_US |
dc.subject | Wave numbers | en_US |
dc.subject | Wide frequency range | en_US |
dc.subject | Cells | en_US |
dc.subject | Cytology | en_US |
dc.subject | Finite element method | en_US |
dc.subject | Transducers | en_US |
dc.subject | Ultrasonic transducers | en_US |
dc.subject | Radiation | en_US |
dc.title | Radiation impedance of collapsed capacitive micromachined ultrasonic transducers | en_US |
dc.type | Article | en_US |
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