Circular high-Q resonating isotropic strain sensors with large shift of resonance frequency under stress
buir.contributor.author | Demir, Hilmi Volkan | |
buir.contributor.orcid | Demir, Hilmi Volkan|0000-0003-1793-112X | |
dc.citation.epage | 9451 | en_US |
dc.citation.issueNumber | 12 | en_US |
dc.citation.spage | 9444 | en_US |
dc.citation.volumeNumber | 9 | en_US |
dc.contributor.author | Melik, R. | en_US |
dc.contributor.author | Unal, E. | en_US |
dc.contributor.author | Perkgoz, N.K. | en_US |
dc.contributor.author | Puttlitz, C. | en_US |
dc.contributor.author | Demir, Hilmi Volkan | en_US |
dc.date.accessioned | 2016-02-08T10:01:39Z | |
dc.date.available | 2016-02-08T10:01:39Z | |
dc.date.issued | 2009 | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Department of Physics | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | We present circular architecture bioimplant strain sensors that facilitate a strong resonance frequency shift with mechanical deformation. The clinical application area of these sensors is for in vivo assessment of bone fractures. Using a rectangular geometry, we obtain a resonance shift of 330 MHz for a single device and 170 MHz for its triplet configuration (with three side-by-side resonators on chip) under an applied load of 3,920 N. Using the same device parameters with a circular isotropic architecture, we achieve a resonance frequency shift of 500 MHz for the single device and 260 MHz for its triplet configuration, demonstrating substantially increased sensitivity. © 2009 by the authors. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T10:01:39Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2009 | en |
dc.identifier.doi | 10.3390/s91209444 | en_US |
dc.identifier.issn | 14248220 | |
dc.identifier.uri | http://hdl.handle.net/11693/22555 | |
dc.language.iso | English | en_US |
dc.relation.isversionof | 10.3390/s91209444 | en_US |
dc.source.title | Sensors | en_US |
dc.subject | Biomems sensors | en_US |
dc.subject | Circular architecture | en_US |
dc.subject | Frequency shift | en_US |
dc.subject | Q-factor | en_US |
dc.subject | Resonators | en_US |
dc.subject | RFIC | en_US |
dc.subject | Sensitivity | en_US |
dc.subject | Bio-mems sensor | en_US |
dc.subject | Frequency shift | en_US |
dc.subject | Q-factors | en_US |
dc.subject | RFIC | en_US |
dc.subject | Sensitivity | en_US |
dc.subject | Frequency shift keying | en_US |
dc.subject | Natural frequencies | en_US |
dc.subject | Resonators | en_US |
dc.subject | Sensors | en_US |
dc.title | Circular high-Q resonating isotropic strain sensors with large shift of resonance frequency under stress | en_US |
dc.type | Article | en_US |
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