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{"title":"Dependence of and field patterns of surface coils on the electrical properties of the sample and the MR operating frequency","authors":"Manushka V. Vaidya, Christopher M. Collins, Daniel K. Sodickson, Ryan Brown, Graham C. Wiggins, Riccardo Lattanzi","doi":"10.1002/cmr.b.21319","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>In high field MRI, the spatial distribution of the radiofrequency magnetic (\n) field is usually affected by the presence of the sample. For hardware design and to aid interpretation of experimental results, it is important both to anticipate and to accurately simulate the behavior of these fields. Fields generated by a radiofrequency surface coil were simulated using dyadic Green's functions, or experimentally measured over a range of frequencies inside an object whose electrical properties were varied to illustrate a variety of transmit (\n) and receive (\n) field patterns. In this work, we examine how changes in polarization of the field and interference of propagating waves in an object can affect the \n spatial distribution. Results are explained conceptually using Maxwell's equations and intuitive illustrations. We demonstrate that the electrical conductivity alters the spatial distribution of distinct polarized components of the field, causing “twisted” transmit and receive field patterns, and asymmetries between \n and \n. Additionally, interference patterns due to wavelength effects are observed at high field in samples with high relative permittivity and near-zero conductivity, but are not present in lossy samples due to the attenuation of propagating EM fields. This work provides a conceptual framework for understanding \n spatial distributions for surface coils and can provide guidance for RF engineers. © 2016 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 46B: 25–40, 2016</p>\n </div>","PeriodicalId":50623,"journal":{"name":"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering","volume":"46 1","pages":"25-40"},"PeriodicalIF":0.9000,"publicationDate":"2016-02-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1002/cmr.b.21319","citationCount":"67","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering","FirstCategoryId":"3","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/cmr.b.21319","RegionNum":4,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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Abstract
In high field MRI, the spatial distribution of the radiofrequency magnetic (
) field is usually affected by the presence of the sample. For hardware design and to aid interpretation of experimental results, it is important both to anticipate and to accurately simulate the behavior of these fields. Fields generated by a radiofrequency surface coil were simulated using dyadic Green's functions, or experimentally measured over a range of frequencies inside an object whose electrical properties were varied to illustrate a variety of transmit (
) and receive (
) field patterns. In this work, we examine how changes in polarization of the field and interference of propagating waves in an object can affect the
spatial distribution. Results are explained conceptually using Maxwell's equations and intuitive illustrations. We demonstrate that the electrical conductivity alters the spatial distribution of distinct polarized components of the field, causing “twisted” transmit and receive field patterns, and asymmetries between
and
. Additionally, interference patterns due to wavelength effects are observed at high field in samples with high relative permittivity and near-zero conductivity, but are not present in lossy samples due to the attenuation of propagating EM fields. This work provides a conceptual framework for understanding
spatial distributions for surface coils and can provide guidance for RF engineers. © 2016 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 46B: 25–40, 2016
表面线圈的磁场模式与样品电学特性和磁流变仪工作频率的关系
在高场MRI中,射频磁场的空间分布通常受到样品存在的影响。对于硬件设计和帮助解释实验结果,预测和准确模拟这些场的行为是很重要的。射频表面线圈产生的场是用二进格林函数模拟的,或者是在一个物体内部的频率范围内进行实验测量,该物体的电学特性是不同的,以说明各种发射()和接收()场模式。在这项工作中,我们研究了场的偏振变化和传播波在物体中的干涉如何影响空间分布。使用麦克斯韦方程组和直观的插图对结果进行了概念性解释。我们证明了电导率改变了场中不同极化分量的空间分布,导致发射和接收场模式“扭曲”,以及和之间的不对称。此外,由于波长效应的干涉模式在高场中观察到具有高相对介电常数和接近零电导率的样品,但由于传播电磁场的衰减而不存在于损耗样品中。这项工作为理解表面线圈的空间分布提供了一个概念框架,并可以为射频工程师提供指导。©2016 Wiley期刊公司机械工程B辑(机械工程),46 (6):25-40,2016
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