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Generation of long prolate volumes of uniform magnetic field in cylindrical saddle-shaped coils

机译:在圆柱形鞍形线圈中产生长而均匀的均匀磁场

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We investigate the uniformity of the magnetic flux density (referred to as the field uniformity) within a series of coils designed to provide a prolate volume of field uniformity. Computational modelling of two cylindrical coil systems which have a sinusoidal current density distributed on the surface of the cylinder, shows the extent of prolate field uniformity along the cylindrical axis, with height and width of the magnetic volume limited by the radius of the cylinder. The first coil system consists of a cos θ coil--a series of saddle-shaped filament loops spaced uniformly with respect to cos θ on the curved cylindrical surface, where θ is the angle between the radius of the cylinder and the horizontal radial axis (assuming a horizontal cylinder). The second coil system, named the 'ELFcage' coil, consists of saddle-shaped filament loops spaced uniformly with respect to a fixed Δθ, on the cylindrical surface. The volume of field uniformity is also compared with volumes generated by circular Helmholtz and Barker coil designs. For coil diameters of 2 m, the Helmholtz and Barker coils generate a volume of field uniformity within 1% to 3% of the field at the centre that extends ~0.8 m and ~1.4 m respectively along the axis of symmetry. This compares to an extent of 3 m and 6 m for both the cos θ and ELFcage coils wound on a 2 m diameter cylinder (8 m length), for 1% and 3% field uniformity respectively. Importantly, the ELFcage coil shows significantly greater field uniformity along the radial axis compared to the cos θ coil. An array of triaxial magnetometers was used to measure the volume of field uniformity within the cos θ coil system, consisting of two sets of orthogonal cos θ windings to generate radial fields and a solenoid winding to generate an axial field. These measurements confirmed the results obtained from computational modelling. The cos θ coil system is currently in use for calibration of magnetometers and for measuring the magnetic signatures of bulky prolate objects.
机译:我们研究了一系列线圈中的磁通量密度的均匀性(称为场均匀性),这些线圈旨在提供均匀的场均匀性。两个圆柱线圈系统的计算模型具有正弦波电流密度分布在圆柱表面上,显示了沿圆柱轴的扁磁场均匀程度,而磁体积的高度和宽度受圆柱半径限制。第一个线圈系统由一个cosθ线圈组成-一系列鞍形灯丝环,它们相对于曲面圆柱面上的cosθ均匀间隔,其中θ是圆柱体半径与水平径向轴之间的夹角(假设是水平圆柱)。第二个线圈系统,称为“ ELFcage”线圈,由马鞍形灯丝环组成,该灯丝环在圆柱面上相对于固定的Δθ均匀间隔开。场均匀性的体积也与圆形亥姆霍兹和巴克线圈设计产生的体积进行了比较。对于直径为2 m的线圈,亥姆霍兹线圈和Barker线圈在沿对称轴分别向〜0.8 m和〜1.4 m延伸的中心产生1%至3%的场均匀性。相比之下,缠绕在直径为2 m的圆柱体(长度为8 m)上的cosθ和ELFcage线圈的长度分别为3 m和6 m,场均匀性分别为1%和3%。重要的是,与cosθ线圈相比,ELFcage线圈沿径向轴显示出更大的场均匀性。三轴磁力计阵列用于测量cosθ线圈系统内的磁场均匀性,该磁场由两组正交的cosθ绕组(产生径向磁场)和螺线管绕组(产生轴向磁场)组成。这些测量结果证实了从计算模型获得的结果。目前,cosθ线圈系统用于校准磁力计和测量大体积扁长物体的磁信号。

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