A z-gradient array coil with a dedicated active-shielded array coil for MRI

buir.contributor.authorTakrimi, Manouchehr
buir.contributor.authorAtalar, Ergin
buir.contributor.orcidTakrimi, Manouchehr|0000-0001-5515-2472
buir.contributor.orcidAtalar, Ergin|0000-0002-6874-6103
dc.citation.epage2731en_US
dc.citation.issueNumber6en_US
dc.citation.spage2718en_US
dc.citation.volumeNumber88en_US
dc.contributor.authorTakrimi, Manouchehr
dc.contributor.authorAtalar, Ergin
dc.date.accessioned2023-02-28T17:31:59Z
dc.date.available2023-02-28T17:31:59Z
dc.date.issued2022-08-02
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentNational Magnetic Resonance Research Center (UMRAM)en_US
dc.description.abstractPurpose: An array-based z-gradient coil with a set of programmable power amplifiers can outperform a conventional z-gradient coil and make it highly customizable with a broader range of tunable features. Methods: A dynamically adjustable imaging volume can be achieved using a pair of independent arrays and a modified optimization procedure based on analytic equations. Two modes of operation are provided: (a) standard mode that resembles a conventional coil; (b) advanced mode, where all performance parameters can be adjusted employing a controllable feeding mechanism. Commercial software is used to demonstrate the validity and feasibility of the proposed coil. Results: Primary and shield array diameters are 24 and 30 cm, both of which comprise 12 bundles of 10 turns copper wires. Maximum feeding voltage/current is 250 V/100 A for all array elements. Four distinct magnetic profiles are provided: (a) conventional profile with 140 mm diameter spherical region of interest, 120 mT/m gradient, and up to 4500 T/m/s slew rate; (b) profile of 200 mT/m, 70 mm region of interest, and up to 6900 T/m/s slew rate; (c) 60 mm axially shifted 70 mm region of interest with 120 mT/m strength and 3600 T/m/s slew rate; and (d) profile of 370 mT/m, 120 mm region of interest, and 3700 T/m/s slew rate when the active shield is reverse fed. Conclusion: By using an active-shielded gradient array coil, the magnetic field profile of the imaging volume can be adjusted dynamically, and it can provide new features and a wide range of field profiles for diverse applications in MRI.en_US
dc.description.provenanceSubmitted by Ezgi Uğurlu (ezgi.ugurlu@bilkent.edu.tr) on 2023-02-28T17:31:58Z No. of bitstreams: 1 A_z-gradient_array_coil_with_a_dedicated_active-shielded_array_coil_for_MRI.pdf: 4889548 bytes, checksum: 1a67becb81da8d5e0ba63d7478a571fd (MD5)en
dc.description.provenanceMade available in DSpace on 2023-02-28T17:31:59Z (GMT). No. of bitstreams: 1 A_z-gradient_array_coil_with_a_dedicated_active-shielded_array_coil_for_MRI.pdf: 4889548 bytes, checksum: 1a67becb81da8d5e0ba63d7478a571fd (MD5) Previous issue date: 2022-08-02en
dc.identifier.doi10.1002/mrm.29390en_US
dc.identifier.issn0740-3194
dc.identifier.urihttp://hdl.handle.net/11693/111972
dc.language.isoEnglishen_US
dc.publisherJohn Wiley and Sons Inc.en_US
dc.relation.isversionofhttps://dx.doi.org/10.1002/mrm.29390en_US
dc.source.titleMagnetic Resonance in Medicineen_US
dc.subjectActive shielden_US
dc.subjectArray coilen_US
dc.subjectGradient coilen_US
dc.subjectMagnetic profileen_US
dc.subjectTunable imaging volumeen_US
dc.titleA z-gradient array coil with a dedicated active-shielded array coil for MRIen_US
dc.typeArticleen_US

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