Quasistatic Solutions versus Full-Wave Solutions of Single-Channel Circular RF Receive Coils on Phantoms of Varying Conductivities at 3 Tesla.

IF 0.9 4区 医学 Q4 CHEMISTRY, PHYSICAL
Michael J Beck, Dennis L Parker, J Rock Hadley
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引用次数: 0

Abstract

Purpose: Although full-wave simulations could be used to aid in RF coil design, the algorithms may be too slow for an iterative optimization algorithm. If quasistatic simulations are accurate within the design tolerance, then their use could reduce simulation time by orders of magnitude compared to full-wave simulations. This paper examines the accuracy of quasistatic and full-wave simulations at 3 Tesla.

Methods: Three sets of eight coils ranging from 3-10 cm (24 total) were used to measure SNR on three phantoms with conductivities of 0.3, 0.6, and 0.9 S/m. The phantom conductivities were chosen to represent those typically found in human tissues. The range of coil element sizes represents the sizes of coil elements seen in typical coil designs. SNR was determined using the magnetic and electric fields calculated by quasistatic and full-wave simulations. Each simulated SNR dataset was scaled to minimize the root mean squared error (RMSE) when compared against measured SNR data. In addition, the noise values calculated by each simulation were compared against benchtop measured noise values.

Results: The RMSE was 0.285 and 0.087 for the quasistatic and full-wave simulations, respectively. The maximum and minimum quotient values, when taking the ratio of simulated to measured SNR values, were 1.69 and 0.20 for the quasistatic simulations and 1.29 and 0.75 for the full-wave simulations, respectively. The ratio ranges, for the calculated quasistatic and full-wave total noise values compared to benchtop measured noise values, were 0.83-1.06 and 0.27-3.02, respectively.

Conclusions: Full-wave simulations were on average 3x more accurate than the quasistatic simulations. Full-wave simulations were more accurate in characterizing the wave effects within the sample, though they were not able to fully account for the skin effect when calculating coil noise.

Abstract Image

Abstract Image

Abstract Image

3 特斯拉下不同传导性模型上单通道环形射频接收线圈的准静态解法与全波解法。
目的:虽然全波仿真可用于射频线圈设计,但对于迭代优化算法来说,这种算法可能太慢。如果准静态模拟的精确度在设计容差范围内,那么与全波模拟相比,使用准静态模拟可将模拟时间缩短几个数量级。本文研究了 3 特斯拉条件下准静态模拟和全波模拟的准确性:方法:在三个电导率分别为 0.3、0.6 和 0.9 S/m 的模型上使用三组 8 个线圈(范围在 3-10 厘米之间,共 24 个)测量信噪比。选择的模型电导率代表了人体组织中的典型电导率。线圈元件的尺寸范围代表了典型线圈设计中的线圈元件尺寸。信噪比是通过准静态和全波模拟计算的磁场和电场确定的。每个模拟信噪比数据集都经过缩放,以便在与测量信噪比数据进行比较时将均方根误差(RMSE)降到最低。此外,还将每次模拟计算的噪声值与台式机测量的噪声值进行了比较:准静态模拟和全波模拟的均方根误差分别为 0.285 和 0.087。模拟信噪比值与测量信噪比值之比的最大和最小商值分别为:准静态模拟 1.69 和 0.20,全波模拟 1.29 和 0.75。计算出的准静态和全波总噪声值与台式机测量噪声值的比值范围分别为 0.83-1.06 和 0.27-3.02:全波模拟比准静态模拟平均精确 3 倍。尽管全波模拟在计算线圈噪声时无法完全考虑集肤效应,但在描述样品内部的波效应方面更为准确。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
2.60
自引率
0.00%
发文量
3
审稿时长
>12 weeks
期刊介绍: Concepts in Magnetic Resonance Part B brings together engineers and physicists involved in the design and development of hardware and software employed in magnetic resonance techniques. The journal welcomes contributions predominantly from the fields of magnetic resonance imaging (MRI), nuclear magnetic resonance (NMR), and electron paramagnetic resonance (EPR), but also encourages submissions relating to less common magnetic resonance imaging and analytical methods. Contributors come from both academia and industry, to report the latest advancements in the development of instrumentation and computer programming to underpin medical, non-medical, and analytical magnetic resonance techniques.
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