Selection field generation using permanent magnets and electromagnets for a magnetic particle imaging scanner

dc.contributor.authorIrfan, Muhammad
dc.contributor.authorMercan Dogan, O.
dc.contributor.authorDoğan, Nurcan
dc.contributor.authorBingolbali, Ayhan
dc.date.accessioned2025-10-29T12:07:51Z
dc.date.issued2022
dc.departmentFakülteler, Mühendislik Fakültesi, Elektronik Mühendisliği Bölümü
dc.departmentFakülteler, Temel Bilimler Fakültesi, Fizik Bölümü
dc.description.abstractThis paper presents a comprehensive study on modeling and implementation of the selection field using NdFeB permanent magnets, electromagnetic coils, and a hybrid system for magnetic particle imaging (MPI). Selection fields were designed for 71 mm internal workspace and their size was based on an 11.25% enhanced ratio of Maxwell configuration. The magnetic particle imaging technique uses a gradient field to define a field of view (FOV) and generate a field-free point (FFP) which is applied to localize superparamagnetic nanoparticles (SPIONs). This study aims to develop a selection field for a new 3D magnetic particle imaging scanner at (?2.15, ?2.15, 4.3) T/m gradient field in (x, y, z) directions, respectively. Three different topologies for gradient fields were numerically modeled in COMSOL and analytically calculated in MATLAB for magnetic flux density (mT) and gradient field strength (T/m). A selection field with NdFeB permanent magnets was practically implemented and its result was compared with the outcomes of a numerical simulation model. Experimental results of permanent magnets selection field topology agreed well with the numerical results from COMSOL. Numerical and analytical results of other selection field topologies were in good agreement. Spatial homogeneity of the selection field topologies was investigated over a range of 40 mm symmetric across the FFP and cost-effective analysis was performed to choose an optimum topology. A hybrid system resulted in better homogeneity over the permanent magnet and electromagnetic topologies with 96.8% spatial homogeneity, and 0.30% relative gradient field strength error. High spatial homogeneity of the gradient field minimizes the image artifacts of the MPI. © 2022 Elsevier B.V., All rights reserved.
dc.identifier.doi10.1016/j.aej.2022.01.028
dc.identifier.endpage7696
dc.identifier.issn1110-0168
dc.identifier.issue10
dc.identifier.scopus2-s2.0-85123712200
dc.identifier.scopusqualityQ1
dc.identifier.startpage7685
dc.identifier.urihttps://doi.org/10.1016/j.aej.2022.01.028
dc.identifier.urihttps://hdl.handle.net/20.500.14854/14176
dc.identifier.volume61
dc.indekslendigikaynakScopus
dc.language.isoen
dc.publisherElsevier B.V.
dc.relation.ispartofAlexandria Engineering Journal
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/openAccess
dc.snmzKA_Scopus_20251020
dc.subjectField free point (FFP)
dc.subjectField of view (FOV)
dc.subjectGradient field
dc.subjectMagnetic particle imaging (MPI)
dc.subjectSuperparamagnetic iron oxide nanoparticles (SPIONs)
dc.titleSelection field generation using permanent magnets and electromagnets for a magnetic particle imaging scanner
dc.typeArticle

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