A z-gradient array coil with a dedicated active-shielded array coil for MRI
buir.contributor.author | Takrimi, Manouchehr | |
buir.contributor.author | Atalar, Ergin | |
buir.contributor.orcid | Takrimi, Manouchehr|0000-0001-5515-2472 | |
buir.contributor.orcid | Atalar, Ergin|0000-0002-6874-6103 | |
dc.citation.epage | 2731 | en_US |
dc.citation.issueNumber | 6 | en_US |
dc.citation.spage | 2718 | en_US |
dc.citation.volumeNumber | 88 | en_US |
dc.contributor.author | Takrimi, Manouchehr | |
dc.contributor.author | Atalar, Ergin | |
dc.date.accessioned | 2023-02-28T17:31:59Z | |
dc.date.available | 2023-02-28T17:31:59Z | |
dc.date.issued | 2022-08-02 | |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | National Magnetic Resonance Research Center (UMRAM) | en_US |
dc.description.abstract | Purpose: 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.provenance | Submitted 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.provenance | Made 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: 2022-08-02 | en |
dc.identifier.doi | 10.1002/mrm.29390 | en_US |
dc.identifier.issn | 0740-3194 | |
dc.identifier.uri | http://hdl.handle.net/11693/111972 | |
dc.language.iso | English | en_US |
dc.publisher | John Wiley and Sons Inc. | en_US |
dc.relation.isversionof | https://dx.doi.org/10.1002/mrm.29390 | en_US |
dc.source.title | Magnetic Resonance in Medicine | en_US |
dc.subject | Active shield | en_US |
dc.subject | Array coil | en_US |
dc.subject | Gradient coil | en_US |
dc.subject | Magnetic profile | en_US |
dc.subject | Tunable imaging volume | en_US |
dc.title | A z-gradient array coil with a dedicated active-shielded array coil for MRI | en_US |
dc.type | Article | en_US |
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