超级对撞机磁串中的纹波分布

K. Smedley, A. Jayasuriya, C. Christiansen, R. Shafer
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引用次数: 0

摘要

对撞机电源中的电压纹波在磁体线圈中产生纹波电流,进而在偶极子和四极子磁场中产生纹波。由于传输线的影响,磁场中的纹波将是空间和空间的函数。本文的工作对注入模式和对撞机模式的磁串中差模纹波的频谱和空间传播模式进行了深入的分析。子/超谐波。因此,有必要将电源纹波作为频谱分布来考虑。151用实验和解析的方法给出了超导磁体的准确电特性。本文通过分析、数值和实验相结合的研究,对注入模式和对撞机模式下对撞机标准电弧磁线中微分纹波的频率和空间分布进行了全面的研究。该分析方法同样适用于其他磁体串。在第11节中,模拟了各种不平衡情况下的电源电压波形,并利用FFT方法得到了电源电压的频谱。在第111节中,得到了电源电压对驱动点处的串电流和线圈电流的传递函数,第Iv节给出了从驱动点到磁体串两端的电流纹波空间分布。第V节给出了线圈电流到磁体串中任意位置磁场的实验传递函数。一个
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ripple Distribution In Magnet Strings Of Super Collider
The voltage ripple in the power supplies of the Collider generate ripple current in the magnet coil that, in turn, generates ripple in the magnetic field of dipoles and quadrupoles. The ripple in the magnetic field will be a function of the and space due to the transmission line effect. The work reported in this paper gives a thorough analysis the frequency spectrum and the spatial propagation pattern of the differential mode ripple in the magnet strings for the injection mode and the collider mode. sub/super harmonics. Therefore, it is necessary to consider the power supply ripple as a spectrum distribution. 151 presented accurate electric characteristics of the superconducting magnets by eGerimenta1 and analytic method. The work reported in this paper gives an analytical, numerical, and experimental combined study and provides thorough information of the frequency and spatial distributions of the differential ripple in the magnet string of collider standard arc for the injection mode and the collider mode. The analysis method is applicable to other magnet strings as well. In Section 11, the waveforms of the power supply voltage with all possibilities of imbalance were simulated, and the spectrum of the power supply voltage was obtained using FFT method. In Section 111, the transfer functions of power supply voltage to the string current and coil current at the drive point were obtained, Section Iv gives the current ripple spatial distribution from the drive point to both ends of the magnet strings. Section V provides an experimental transfer function from the coil current to the magnetic field at any location in the magnet strings. A
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