dc.contributor.author | Kazemivalipour, Ehsan | |
dc.contributor.author | Guerin, Bastien | |
dc.contributor.author | Wald, Lawrence L. | |
dc.date.accessioned | 2025-10-01T16:53:58Z | |
dc.date.available | 2025-10-01T16:53:58Z | |
dc.date.issued | 2025-03-17 | |
dc.identifier.issn | 0740-3194 | |
dc.identifier.issn | 1522-2594 | |
dc.identifier.uri | https://hdl.handle.net/1721.1/162855 | |
dc.description.abstract | Purpose: We characterize electromagnetic (EM) radiation patterns and levelsin conventional MRI systems as a function of field strength and load symmetry,providing a framework for mitigation strategies allowing operation without ashielded room.
Methods: We simulated the far-field radiation pattern and fields at a 10 mradius (|E|10m and |B|10m ) for a solenoidal superconducting MRI with abody birdcage coil operated between 0.25T and 6.5T. Five load configura-tions probed the impact of load-symmetry, ranging from a sphere to a bodyload (least-symmetric). We also assessed simple layered EM absorbers at thebore-ends.
Results: All configurations exceeded regulatory limits for realistic transmit lev-els. At 1.5T, a 300 V rms RF-pulse is 2700-fold the |E|10m limit. Field strengthand load symmetry strongly modulate radiation patterns and levels. The radi-ated power increased by more than four orders of magnitude from 0.25T to6.5T. Spherical load radiation transitioned from a peak gain at the bore-ends(0.25–0.5T) to a donut-shaped pattern, suggesting current loops around the bore(1 T–1.5T), back to bore-axis-directed gain, suggesting propagating waves alongthe bore (2T–6.5T). Transition patterns were seen between these regimes; uni-form radiation at 0.75T and a combined donut/bore-directed pattern at 1.75T.Load asymmetry increased both strength and pattern asymmetry, with the bodyload having the highest and least symmetric radiation with the legs facilitat-ing wave propagation at high-fields. A simple optimized layered absorber atscanner’s service-end reduced 3T peak radiation by 11 dB.
Conclusion: Radiation from unshielded scanners far exceeds regulatory lim-its, particularly at high-field. Mitigation strategies must address load-symmetry,field strength, and wave effects. | en_US |
dc.publisher | Wiley | en_US |
dc.relation.isversionof | https://doi.org/10.1002/mrm.30499 | en_US |
dc.rights | Creative Commons Attribution | en_US |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
dc.source | Wiley | en_US |
dc.title | Simulated radiation levels and patterns of MRI without a Faraday shielded room | en_US |
dc.type | Article | en_US |
dc.identifier.citation | Kazemivalipour E, Guerin B, Wald LL. Simulated radiation levels and patterns of MRI without a Faraday shielded room. Magn Reson Med. 2025; 94: 835-851. | en_US |
dc.contributor.department | Harvard-MIT Program in Health Sciences and Technology | en_US |
dc.relation.journal | Magnetic Resonance in Medicine | en_US |
dc.eprint.version | Final published version | en_US |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
dspace.date.submission | 2025-09-29T14:53:48Z | |
mit.journal.volume | 94 | en_US |
mit.journal.issue | 2 | en_US |
mit.license | PUBLISHER_CC | |