Ag/AgCl electrodes in the EEG/fMRI method in 3T MRI scanner
dc.contributor.buuauthor | Akay, Cengiz | |
dc.contributor.buuauthor | Kepçeoğlu, Abdullah | |
dc.contributor.department | Uludağ Üniversitesi/Fen-Edebiyat Fakültesi/Fizik Anabilim Dalı. | tr_TR |
dc.contributor.orcid | 0000-0002-8037-0364 | tr_TR |
dc.contributor.orcid | 0000-0002-4743-5517 | tr_TR |
dc.contributor.researcherid | W-1656-2017 | tr_TR |
dc.contributor.researcherid | R-2290-2019 | tr_TR |
dc.contributor.scopusid | 55884917500 | tr_TR |
dc.contributor.scopusid | 55884290600 | tr_TR |
dc.date.accessioned | 2023-05-08T12:31:41Z | |
dc.date.available | 2023-05-08T12:31:41Z | |
dc.date.issued | 2013-10 | |
dc.description.abstract | This study focuses on the comparison of two different types of EEG electrodes (the first B10-S-150 Ag/AgCl sintered ring electrode with 1, 5 mm touch proof safety socket and 150 cm heavy-duty lead wire and the second, B12-LS-100 Ag/AgCl sintered FE-electrode with 100 cm light-duty lead wire and 1, 5 mm touch proof safety socket with 5 k Omega resistor near sensor) used in the EEG/fMRI method in 3T MRI scanner. We compared these electrodes by their specific absorption rate (SAR) simulation values and the temperature change calculated by PRF method. The experimental setup of the study is described as follows: a phantom is prepared and the electrodes are placed on it. Then, a simulation for SAR values is realized. The temperature change is calculated by MR thermometer. As a result of this study, Ag/AgCl pin electrode is better to be use in EEG/fMRI; because the measured temperature change is expected to be low. | en_US |
dc.identifier.citation | Akay, C. ve Kepçeoğlu, A. (2013). “Ag/AgCl electrodes in the EEG/fMRI method in 3T MRI scanner”. European Physical Journal - Applied Physics, 64(1). | en_US |
dc.identifier.issn | 1286-0042 | |
dc.identifier.issn | 1286-0050 | |
dc.identifier.issue | 1 | tr_TR |
dc.identifier.scopus | 2-s2.0-84885585019 | tr_TR |
dc.identifier.uri | https://doi.org/10.1051/epjap/2013130173 | |
dc.identifier.uri | http://hdl.handle.net/11452/32590 | |
dc.identifier.volume | 64 | tr_TR |
dc.identifier.wos | 000325535600007 | |
dc.indexed.scopus | Scopus | en_US |
dc.indexed.wos | SCIE | en_US |
dc.language.iso | en | en_US |
dc.publisher | Edp Sciences | en_US |
dc.relation.bap | OUAP(F) - 2012/13 | tr_TR |
dc.relation.journal | European Physical Journal-Applied Physics | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi | tr_TR |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Physics | en_US |
dc.subject | EEG | en_US |
dc.subject | Frequency | en_US |
dc.subject | Phantoms | en_US |
dc.subject | Shift | en_US |
dc.subject | Scanning | en_US |
dc.subject | Sintering | en_US |
dc.subject | Wire | en_US |
dc.subject | Ag/AgCl electrodes | en_US |
dc.subject | Lead wire | en_US |
dc.subject | Light-duty | en_US |
dc.subject | Measured temperatures | en_US |
dc.subject | MRI scanners | en_US |
dc.subject | Ring electrodes | en_US |
dc.subject | Specific absorption rate | en_US |
dc.subject | Temperature changes | en_US |
dc.subject | Electrodes | en_US |
dc.subject.scopus | Thin Films; Carbon Films; Fractal Dimensions | en_US |
dc.subject.wos | Physics, applied | en_US |
dc.title | Ag/AgCl electrodes in the EEG/fMRI method in 3T MRI scanner | en_US |
dc.type | Article | |
dc.wos.quartile | Q4 | en_US |
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