共查询到19条相似文献,搜索用时 203 毫秒
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介绍了EBIT(Electron Beam Ion Trap,电子束离子阱)装置零蒸发低温超导磁体系统的研制过程与超导磁体的性能测试结果。该系统中超导磁体由一对上下布置的分离线圈组成,中心最大磁场强度可达4.5T,在中心轴线上±10mm内磁场均匀度优于2×10-4,磁场衰减系数在8h小于1×10-4;同时其低温杜瓦系统采用双冷屏结构,并通过二级G-M制冷机冷却冷屏来降低液氦的蒸发量。超导磁体的性能测试结果表明满足用户基本要求。 相似文献
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提出了一个冷孔直径150 mm、中心磁场为15 T的NbTi/Nb3Sn超导磁体电磁结构.分析了超导磁体各线圈中磁场的分布规律,结合超导材料临界性能,得到了超导磁体的运行电磁裕度.针对线圈结构组份材料的机械性能,采用平均有限元法仿真了超导磁体的应力/应变,最大环向应力和应变分别为112 MPa和0.297%.该结果表明... 相似文献
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超导磁体体积小,能够获得强磁场,磁场稳定度、均匀度很高,因此,在磁学测量设备中应用很广泛.美国Quantum Design公司的高精度磁学测量系统采用的就是超导磁体,最高磁场能够达到7 T.由于超导磁体材料本身缺陷的钉扎作用,在磁体退磁后,磁体内部有剩余磁场,有时能够大于30 Oe.由此产生的磁场误差将导致测试的矫顽力、剩磁等数据不准确,甚至导致反向的磁滞回线.设置的磁场初始值不同,剩余磁场的大小也不同;初始磁场越大,剩余磁场越大.这种剩余磁场效应在软磁材料测试过程中表现得尤为明显,产生的测试误差不可忽略,必须进行磁场误差修正才能得到正确的结果.本文阐明了超导磁体产生剩余磁场的原因、影响因素和规律,详述了测试软磁材料可能遇到的问题,并给出解决方法. 相似文献
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介绍了一套制冷机冷却型小型超导强磁场系统。超导磁体线圈用铌钛超导线绕制,室温孔直径为75mm,磁场中心Φ25mm×250mm区域内最高场强达到3.64T,磁场不均匀性小于3%。在2.62T场强下连续闭环运行了20天,电流衰减率近似为零。采用4K级低温制冷机冷却防辐射冷屏,液氦蒸发率小于0.03升/小时,系统一次可注入液氦50升,补液周期大于60天。 相似文献
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电子真空回旋器件是一种对磁场精度要求较高的微波源装置,一般采用超导磁体提供磁场环境.超导磁体的应用中,磁场分布的实现是超导磁体设计的核心问题.提供回旋器件磁场的高温超导磁体包含较复杂的磁体绕组,为了解决此类设计计算问题,本文提出了一种包含设计区域约束的线性优化方法进行回旋器件高温超导绕组的设计优化,通过分步的约束和线性优化计算,可得到同时满足设计要求和绕组可实现的设计磁场电流分布设计.计算实例的结果给出了一个提供磁场强度1.3 Tesla,长度285 mm的均匀磁场区域,同时满足多位置的磁场要求,设计结果与要求一致度较好,精度满足应用需求.该计算方法是一种可适用于较复杂磁场要求和超导绕组结构的设计优化方法. 相似文献
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O. P. Polyakov P. A. Polyakov 《Bulletin of the Russian Academy of Sciences: Physics》2017,81(8):993-995
Inhomogeneously distributed magnetization that induces a strong magnetic field in a predetermined local area is established in finite permanent magnets. The maximum possible magnetic induction in the vicinity of a magnet’s center is found analytically for a perfect spherical magnet. 相似文献
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设计了一种非浸没式小型化轴向无箔二极管,其阴极发射区位于螺线管中心孔以外,采用螺线管、永磁体和软磁体构成的复合引导磁场系统。采用CST优化设计二极管结构,使其满足800 kV电压下绝缘要求; 优化设计磁场系统结构及物理参数,使其满足引导强流相对论电子束高效率传输的要求。采用粒子模拟(PIC)软件仿真电子束产生及传输过程,验证其高传输效率。设计的阳极筒直径比原结构缩小约40%,在产生同样均匀区轴向磁场强度情况下,引导磁场重量和功耗比原结构降低约40%,仿真结果显示主引导磁场0.85 T下,8 kA电流能够实现100%传输效率。 相似文献
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The desire to do clinical imaging and spectroscopy at magnetic field strengths greater than 2 Tesla (T) necessitates investigation of possible bioeffects at these high fields. A simple T-maze was utilized to evaluate the aversive effects of exposure to three levels of static magnetic field (0, 1.5, and 4 T). The right arm of the maze extended into the center of a 30-cm horizontal bore magnet, while the left arm extended into a mock magnet bore with the same dimensions. The self-shielded design of the magnet reduces the fringe field to zero within 1 m of the bore, placing the start box of the maze outside the 5-G line of the magnet. Each rat performed a total of ten trials at each level of magnetic field strength. A follow-up subset was run at 4 T with the maze reversed. At 0 T, the rats entered the magnet freely. No significant differences from the control were observed at 1.5 T. At 4 T, however, in 97% of the trials the rats would not enter the magnet. In the maze-reversed subset a majority of the rats turned toward the magnet, indicating that they had learned an aversive response from the previous trials at 4 T. However, in only 4 decisions out of 58 did the rats actually enter the magnet. Eighteen decisions to turn around were made at the edge of the magnet in a region of strong field gradients (up to 13 T/m) and a field strength up to 1.75 T.(ABSTRACT TRUNCATED AT 250 WORDS) 相似文献
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介绍了加速器驱动次临界系统(ADS)注入器Ⅱ束流聚焦单元超导螺线管的初步测试。 该测试在高度1 600 mm、 直径510 mm的垂直杜瓦中, 利用型号为cryogenic sms的超导电源对磁体进行了励磁, 并利用霍尔探头测试了其轴向磁场分布情况和漏场情况, 其中心磁场励磁后可达8.20 T, 漏场分布和计算值的相对误差小于10%。 同时, 对励磁过程中骨架的应力应变状态做了测试。 对测试结果的分析表明, 骨架结构设计合理, 应变状态变化平稳, 磁体低温稳定性能良好。The preliminary test of the superconducting solenoid for ADS injectorⅡhas been carried out in order to measure its performances. A vertical dewar with height 1 600 mm and outer diameter 510 mm was employed for this test. The magnet was energized by a cryogenic sms superconducting magnet current source. The axial magnetic distribution and leakage field were also tested through hall probes. The center field can be excited up to 8.20 T and the relative diviation between the measured value and the calculated value of the stray and leakage field is less than 10%. The measurements of the strain and stress status of the magnet skeleton show that the distortion is small and the mechanical performance is robust. 相似文献
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Markiewicz W.D. Read M.E. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1992,20(3):197-204
The design of a 12 T superconducting magnet for a 280 GHz quasi-optical gyrotron is discussed. The gyrotron geometry requires a clear bore perpendicular to the magnetic axis through the center of the magnet, thus forcing the magnet to be formed of two separate sections. This causes the peak field on the windings to be over 14 T, and produces a double-peaked structure in the field. Calculations of mirror and cross bore RF heating and electron beam reflection as a function of the magnet and cross bore dimensions are presented, as are discussions of other tradeoffs in the magnet design. The conclusion of the study is that a suitable magnet is feasible 相似文献