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Consideration on Current and Coil Block Placements With Good Homogeneity for MRI Magnets Using Truncated SVD

机译:使用截断SVD的MRI磁体具有均匀性的电流和线圈块放置的考虑

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This paper describes a new method to determine the current and coil block placements with good homogeneity for magnetic resonance imaging (MRI) magnets, and discusses the relationships between the placements and homogeneity, using regularization of the truncated singular value decomposition (SVD). In the first step, the main coil (MC) is modeled as filament loop currents (FLCs) on a solenoid and the shield coil (SC) is modeled by coil blocks. The FLCs are determined so as to get a homogeneous magnetic field using a superposition of eigenmodes obtained by the SVD. In the second step, the FLCs are replaced by MC blocks. The findings are as follows. 1) The obtained FLC distribution in the axial direction has several peaks, which can be suitably replaced by MC blocks and the number of the peaks is equal to the number of MC blocks. 2) There is an optimum length to minimize the absolutely summed current and the 1542-mm length is the optimum for a 525-mm radius with six MC blocks. 3) A one-eigenmode (one MC block) increase or decrease changes the length by $+$87 or $-$105 mm, respectively. 4) Six MC blocks can provide 1-ppm peak-to-peak homogeneity in the 400-mm diameter spherical imaging volume and this is adequate for MRI magnets.
机译:本文介绍了一种确定具有良好同质性的磁共振成像(MRI)磁体的电流和线圈块放置的新方法,并讨论了使用截断奇异值分解(SVD)的正则化来确定这些放置位置和同质性之间的关系。第一步,将主线圈(MC)建模为螺线管上的灯丝回路电流(FLC),并通过线圈模块对屏蔽线圈(SC)建模。使用由SVD获得的本征模的叠加来确定FLC,以便获得均匀的磁场。在第二步中,将FLC替换为MC块。调查结果如下。 1)获得的沿轴向方向的FLC分布具有几个峰,可以适当地用MC块代替,并且峰的数量等于MC块的数量。 2)有一个最佳长度可以最大程度地减少绝对求和的电流,而对于带有六个MC块的525毫米半径,1542毫米长度是最佳的。 3)单本征模式(一个MC块)通过 $ + $ 87或 $-$ 105毫米。 4)六个MC块可在400毫米直径的球形成像体积中提供1-ppm的峰峰均一性,这对于MRI磁体而言已足够。

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