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首页> 外文期刊>Journal of Applied Physics >Formulation of the spherical harmonic coefficients of the entire magnetic field components generated by magnetic moment and current for shimming
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Formulation of the spherical harmonic coefficients of the entire magnetic field components generated by magnetic moment and current for shimming

机译:表示由匀场产生的磁矩和电流产生的整个磁场分量的球谐系数

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摘要

For MRI and NMR magnet design, a highly homogeneous and high magnetic field has to be achieved by active and/or passive shimming. The active and passive shimming commonly homogenize the magnetic field around the magnet center by cancellation of the higher terms of a spherical harmonic series than the 0th term. So far, the spherical harmonic expression in the cylindrical coordinate system is well known for a circular coil, a solenoid coil, and magnetization of ferromagnetic material with/without its volume. In a shimming design, only the z-component of an inhomogeneous magnetic field is compensated because it is dominant to the performance of MRI/NMR. However, various kinds of MRI and NMR systems have recently been developed, and these magnets sometimes have an axially asymmetric configuration or generate a tilted magnetic field. Therefore, the entire x-, y-, and z-components have to be homogenized for such magnets. I derive the spherical harmonic expression of the entire components of magnetic field generated by a circular coil, a dipole coil, and a straight line current. In addition, since the entire magnetization components of the ferromagnetic material having the volume contribute the entire components of the magnetic field around the magnet center, I also derive the equations of the spherical harmonic coefficients of the magnetic field generated by ferromagnetic material. Since these equations need a numerical integration, such as the Gauss quadrature integration, the computation accuracy of the spherical harmonic coefficients is investigated against the number of the evaluation points. We can calculate the highly accurate spherical harmonic coefficients with the small number of the evaluation points.
机译:对于MRI和NMR磁体设计,必须通过主动和/或被动匀场实现高度均匀和高磁场。主动和被动匀场通常通过消除球形谐波序列的高项而不是第0项来使磁体中心周围的磁场均匀化。到目前为止,圆柱坐标系中的球谐表达式对于圆形线圈,螺线管线圈和具有/不具有其体积的铁磁材料的磁化是众所周知的。在匀场设计中,由于非均匀磁场的z分量对MRI / NMR的性能起着主导作用,因此只能对其进行补偿。然而,近来已经开发了各种MRI和NMR系统,并且这些磁体有时具有轴向不对称的构造或产生倾斜的磁场。因此,对于此类磁体,必须将整个x,y和z分量均质化。我推导了由圆形线圈,偶极线圈和直线电流产生的磁场的整个分量的球谐函数表达式。另外,由于具有体积的铁磁材料的整个磁化分量贡献了围绕磁体中心的磁场的全部分量,所以我还导出了由铁磁材料产生的磁场的球谐系数的方程。由于这些方程式需要进行数值积分,例如高斯积分,因此需要针对评估点数量来研究球谐系数的计算精度。我们可以用较少的评估点来计算高精度的球谐系数。

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  • 来源
    《Journal of Applied Physics》 |2014年第16期|1-18|共18页
  • 作者

    Noguchi So;

  • 作者单位

    Graduate School of Information Science and Technology, Hokkaido University, Kita 14 Nishi 9, Kita-ku, Sapporo 060-0814, Japan|c|;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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