Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications
A numerical method is presented to compute electromagnetic fields inside a 2 mm high resolution, anatomically detailed model of a human head for high-frequency magnetic resonance imaging (MRI) applications. The method uses the biconjugate gradient algorithm in combination with the fast Fourier trans...
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Veröffentlicht in: | Physics in medicine & biology 1996-12, Vol.41 (12), p.2719-2738 |
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creator | Jin, J M Chen, J Chew, W C Gan, H Magin, R L Dimbylow, P J |
description | A numerical method is presented to compute electromagnetic fields inside a 2 mm high resolution, anatomically detailed model of a human head for high-frequency magnetic resonance imaging (MRI) applications. The method uses the biconjugate gradient algorithm in combination with the fast Fourier transform to solve a matrix equation resulting from the discretization of an integrodifferential equation representing the original physical problem. Given the current distribution in an MRI coil, the method can compute both the electric field (thus the specific energy absorption rate (SAR)) and the magnetic field, also known as the B1 field. Results for the SAR and B1 field distribution, excited by a linear and a quadrature birdcage coil, are calculated and presented at 64 MHz, 128 MHz and 256 MHz, corresponding to the operating frequencies of the 1.5 T, 3 T and 6 T MRI systems. It is shown that compared with that at 64 MHz, the SAR at 128 MHz is increased by a factor over 5 and the SAR at 256 MHz is increased by a factor over 10, assuming the same current strength in the coil. Furthermore, compared with the linear excitation, the average SAR for the quadrature excitation is reduced by a factor over 2 and the maximum SAR is reduced by a factor over 3. It is also shown that the B1 field at high frequencies exhibits a strong inhomogeneity, which is attributed to dielectric resonance. |
doi_str_mv | 10.1088/0031-9155/41/12/011 |
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The method uses the biconjugate gradient algorithm in combination with the fast Fourier transform to solve a matrix equation resulting from the discretization of an integrodifferential equation representing the original physical problem. Given the current distribution in an MRI coil, the method can compute both the electric field (thus the specific energy absorption rate (SAR)) and the magnetic field, also known as the B1 field. Results for the SAR and B1 field distribution, excited by a linear and a quadrature birdcage coil, are calculated and presented at 64 MHz, 128 MHz and 256 MHz, corresponding to the operating frequencies of the 1.5 T, 3 T and 6 T MRI systems. It is shown that compared with that at 64 MHz, the SAR at 128 MHz is increased by a factor over 5 and the SAR at 256 MHz is increased by a factor over 10, assuming the same current strength in the coil. Furthermore, compared with the linear excitation, the average SAR for the quadrature excitation is reduced by a factor over 2 and the maximum SAR is reduced by a factor over 3. It is also shown that the B1 field at high frequencies exhibits a strong inhomogeneity, which is attributed to dielectric resonance.</description><identifier>ISSN: 0031-9155</identifier><identifier>EISSN: 1361-6560</identifier><identifier>DOI: 10.1088/0031-9155/41/12/011</identifier><identifier>PMID: 8971965</identifier><identifier>CODEN: PHMBA7</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Algorithms ; Biological and medical sciences ; Electromagnetic Fields ; Fourier Analysis ; Head ; Humans ; Investigative techniques, diagnostic techniques (general aspects) ; Magnetic Resonance Imaging ; Medical sciences ; Miscellaneous. Technology ; Models, Theoretical ; Phantoms, Imaging ; Radiodiagnosis. Nmr imagery. Nmr spectrometry</subject><ispartof>Physics in medicine & biology, 1996-12, Vol.41 (12), p.2719-2738</ispartof><rights>1997 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c469t-f52d2ef38de5f620d78e1b8376c632efa6a54ac2c44a7e1e437e352082a5bc633</citedby><cites>FETCH-LOGICAL-c469t-f52d2ef38de5f620d78e1b8376c632efa6a54ac2c44a7e1e437e352082a5bc633</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/0031-9155/41/12/011/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,778,782,27911,27912,53817,53897</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=2496987$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/8971965$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Jin, J M</creatorcontrib><creatorcontrib>Chen, J</creatorcontrib><creatorcontrib>Chew, W C</creatorcontrib><creatorcontrib>Gan, H</creatorcontrib><creatorcontrib>Magin, R L</creatorcontrib><creatorcontrib>Dimbylow, P J</creatorcontrib><title>Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications</title><title>Physics in medicine & biology</title><addtitle>Phys Med Biol</addtitle><description>A numerical method is presented to compute electromagnetic fields inside a 2 mm high resolution, anatomically detailed model of a human head for high-frequency magnetic resonance imaging (MRI) applications. The method uses the biconjugate gradient algorithm in combination with the fast Fourier transform to solve a matrix equation resulting from the discretization of an integrodifferential equation representing the original physical problem. Given the current distribution in an MRI coil, the method can compute both the electric field (thus the specific energy absorption rate (SAR)) and the magnetic field, also known as the B1 field. Results for the SAR and B1 field distribution, excited by a linear and a quadrature birdcage coil, are calculated and presented at 64 MHz, 128 MHz and 256 MHz, corresponding to the operating frequencies of the 1.5 T, 3 T and 6 T MRI systems. It is shown that compared with that at 64 MHz, the SAR at 128 MHz is increased by a factor over 5 and the SAR at 256 MHz is increased by a factor over 10, assuming the same current strength in the coil. Furthermore, compared with the linear excitation, the average SAR for the quadrature excitation is reduced by a factor over 2 and the maximum SAR is reduced by a factor over 3. It is also shown that the B1 field at high frequencies exhibits a strong inhomogeneity, which is attributed to dielectric resonance.</description><subject>Algorithms</subject><subject>Biological and medical sciences</subject><subject>Electromagnetic Fields</subject><subject>Fourier Analysis</subject><subject>Head</subject><subject>Humans</subject><subject>Investigative techniques, diagnostic techniques (general aspects)</subject><subject>Magnetic Resonance Imaging</subject><subject>Medical sciences</subject><subject>Miscellaneous. Technology</subject><subject>Models, Theoretical</subject><subject>Phantoms, Imaging</subject><subject>Radiodiagnosis. Nmr imagery. Nmr spectrometry</subject><issn>0031-9155</issn><issn>1361-6560</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp9kMtKAzEUhoMoWi9PIMIsxIUwNvfJLKV4A8GNrmOaOamR6WRMpou-vakts1FcBfJ_55yfD6Fzgm8IVmqKMSNlTYSYcjIldIoJ2UMTwiQppZB4H01G4ggdp_SJM6EoP0SHqq5ILcUEvc_Csl8NZvChK4IroAU7xLA0iw4GbwvnoW1S4UIsPvzio3QRvlbQ2XUxIhFS6ExnofD5z3eLwvR96-3PznSKDpxpE5zt3hP0dn_3Onssn18enma3z6Xlsh5KJ2hDwTHVgHCS4qZSQOaKVdJKlgMjjeDGUsu5qYAAZxUwQbGiRswzwk7Q1XZvH0NumAa99MlC25oOwirpSknGlaoyyLagjSGlCE73MRePa02w3njVG2t6Y01zognV2VqeutitX82X0IwzO5E5v9zlJlnTupiF-DRilNey_jl-vcV86Mfwj3u6b1yGb37D_5X8Bu7cnEc</recordid><startdate>19961201</startdate><enddate>19961201</enddate><creator>Jin, J M</creator><creator>Chen, J</creator><creator>Chew, W C</creator><creator>Gan, H</creator><creator>Magin, R L</creator><creator>Dimbylow, P J</creator><general>IOP Publishing</general><general>Institute of Physics</general><scope>IQODW</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>19961201</creationdate><title>Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications</title><author>Jin, J M ; Chen, J ; Chew, W C ; Gan, H ; Magin, R L ; Dimbylow, P J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c469t-f52d2ef38de5f620d78e1b8376c632efa6a54ac2c44a7e1e437e352082a5bc633</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><topic>Algorithms</topic><topic>Biological and medical sciences</topic><topic>Electromagnetic Fields</topic><topic>Fourier Analysis</topic><topic>Head</topic><topic>Humans</topic><topic>Investigative techniques, diagnostic techniques (general aspects)</topic><topic>Magnetic Resonance Imaging</topic><topic>Medical sciences</topic><topic>Miscellaneous. Technology</topic><topic>Models, Theoretical</topic><topic>Phantoms, Imaging</topic><topic>Radiodiagnosis. Nmr imagery. Nmr spectrometry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Jin, J M</creatorcontrib><creatorcontrib>Chen, J</creatorcontrib><creatorcontrib>Chew, W C</creatorcontrib><creatorcontrib>Gan, H</creatorcontrib><creatorcontrib>Magin, R L</creatorcontrib><creatorcontrib>Dimbylow, P J</creatorcontrib><collection>Pascal-Francis</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Physics in medicine & biology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jin, J M</au><au>Chen, J</au><au>Chew, W C</au><au>Gan, H</au><au>Magin, R L</au><au>Dimbylow, P J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications</atitle><jtitle>Physics in medicine & biology</jtitle><addtitle>Phys Med Biol</addtitle><date>1996-12-01</date><risdate>1996</risdate><volume>41</volume><issue>12</issue><spage>2719</spage><epage>2738</epage><pages>2719-2738</pages><issn>0031-9155</issn><eissn>1361-6560</eissn><coden>PHMBA7</coden><abstract>A numerical method is presented to compute electromagnetic fields inside a 2 mm high resolution, anatomically detailed model of a human head for high-frequency magnetic resonance imaging (MRI) applications. The method uses the biconjugate gradient algorithm in combination with the fast Fourier transform to solve a matrix equation resulting from the discretization of an integrodifferential equation representing the original physical problem. Given the current distribution in an MRI coil, the method can compute both the electric field (thus the specific energy absorption rate (SAR)) and the magnetic field, also known as the B1 field. Results for the SAR and B1 field distribution, excited by a linear and a quadrature birdcage coil, are calculated and presented at 64 MHz, 128 MHz and 256 MHz, corresponding to the operating frequencies of the 1.5 T, 3 T and 6 T MRI systems. It is shown that compared with that at 64 MHz, the SAR at 128 MHz is increased by a factor over 5 and the SAR at 256 MHz is increased by a factor over 10, assuming the same current strength in the coil. Furthermore, compared with the linear excitation, the average SAR for the quadrature excitation is reduced by a factor over 2 and the maximum SAR is reduced by a factor over 3. It is also shown that the B1 field at high frequencies exhibits a strong inhomogeneity, which is attributed to dielectric resonance.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><pmid>8971965</pmid><doi>10.1088/0031-9155/41/12/011</doi><tpages>20</tpages></addata></record> |
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subjects | Algorithms Biological and medical sciences Electromagnetic Fields Fourier Analysis Head Humans Investigative techniques, diagnostic techniques (general aspects) Magnetic Resonance Imaging Medical sciences Miscellaneous. Technology Models, Theoretical Phantoms, Imaging Radiodiagnosis. Nmr imagery. Nmr spectrometry |
title | Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications |
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