T. Hamajima, K. Sato, H. Yamada, N. Harada, M. Tsuda, K. Tsutsumi, H. Hayashi, T. Ezaki
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引用次数: 1
摘要
近年来超导磁体技术的发展使我们能够构建中小规模的超导磁体储能系统(SMES, superconducting Magnetic Energy Storage System),该系统具有高收敛效率和同时快速响应实功率和无功功率的特点,将有效地用于电力管理和质量控制。由于此类中小企业应位于变电站或需求站点附近,超导线圈的杂散场限制了其使用。利用一系列勒让德多项式分析了螺线管外的杂散场;因此,结果适用于各种线圈配置。我们从各种SMES配置中导出了作为Rp的函数的杂散场,其中Rp是与线圈的距离。本文分析了单线圈和环形线圈布置的杂散场与超导线圈主要参数储能E和最大磁场Bm的函数关系。单线圈配置的杂散场减小为E/Bm,环面线圈配置的杂散场减小为(E(n+2)/Bm(2n+1))1/3,其中n为线圈数。
Scaling Law of Stray Fields from SMES Coil Configurations as Functions of Stored Energy and Maximum Magnetic Field
The recent developments of superconducting magnet technology allow us to construct a small and medium-scale SMES (Superconducting Magnetic Energy Storage System), which would be effectively used for electric power management and quality control because of its high convergence efficiency and its simultaneously quick response of real and reactive power. Since a SMES of this kind should be situated in a power substation or near a demand site, a stray field from superconducting coils restricts its use. The stray field outside a solenoid is analyzed by a series of Legendre polynomials; therefore the results are applied to various coil configurations. We derived the stray fields from various SMES configurations as a function of Rp, where Rp is distance from the coil. In this paper we analyzed the stray fields from single solenoid coil and toroidal coil arrangements, as functions of stored energy E and maximum magnetic field Bm, which are the main parameters of superconducting coil. The stray field from the single solenoid coil configuration decreases as E/Bm, and that from the toroidal coil configuration decreases as (E(n+2)/Bm(2n+1))1/3, where n is the number of coils.