1.5 t头部核磁共振超导磁体的设计、测试和调光

IF 1.8 3区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC
Yunxing Song;Zhiwen Cheng;Xunhuang Jiang;Jianglan Li;Liang Li;Qiuliang Wang
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引用次数: 0

摘要

超导磁体作为磁共振成像(MRI)系统的核心部件,为系统提供了高强度、稳定、均匀的磁场背景。磁场的强度、稳定性和均匀性直接影响MRI成像质量。本文介绍了由武汉国家强磁场中心研制的1.5 t头磁共振超导磁体的设计、测试和摆振。该磁铁由七个初级线圈和两个屏蔽线圈组成,使用浴池冷却,工作电流为510 A。试验表明,磁体在第一次爬坡后直接达到1.5 T的目标场,没有任何淬灭。在1.5 T的磁场下,磁体的磁场衰减率小于0.02 ppm/hr。经过三轮被动调光后,磁铁在直径26厘米的成像球上实现了2.89 ppm的磁场不均匀性。该磁体的研制成功,为全磁头磁共振超导磁体轻量化技术提供了实际的工程验证。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Design, Test, and Shimming of a 1.5-T Head-Only MRI Superconducting Magnet
As the core component of magnetic resonance imaging (MRI) system, superconducting magnet provides a high-intensity, stable, and homogeneous magnetic field background for the system. The strength, stability, and homogeneity of the magnetic field directly affect the imaging quality of MRI. This article presents the design, test, and shimming of a 1.5-T head-only MRI superconducting magnet developed by the Wuhan National High Magnetic Field Center. The magnet consists of seven primary coils and two shielding coils and is operated at an operating current of 510 A using bath cooling. The test has shown that the magnet reached the target field of 1.5 T directly after the first ramp-up without any quench. Under the magnetic field of 1.5 T, the magnetic field decay rate of the magnet is less than 0.02 ppm/hr. After three rounds of passive shimming, the magnet achieves a magnetic field inhomogeneity of 2.89 ppm over an imaging sphere within a diameter of 26 cm. The successful development of this magnet provides practical engineering validation for the lightweight technology of head-only MRI superconducting magnets.
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来源期刊
IEEE Transactions on Applied Superconductivity
IEEE Transactions on Applied Superconductivity 工程技术-工程:电子与电气
CiteScore
3.50
自引率
33.30%
发文量
650
审稿时长
2.3 months
期刊介绍: IEEE Transactions on Applied Superconductivity (TAS) contains articles on the applications of superconductivity and other relevant technology. Electronic applications include analog and digital circuits employing thin films and active devices such as Josephson junctions. Large scale applications include magnets for power applications such as motors and generators, for magnetic resonance, for accelerators, and cable applications such as power transmission.
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