留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

C-ADS强流质子直线加速器调谐系统测试分析

张磊 王锋锋 刘鲁北 王若旭 于培炎 高郑 张斌

张磊, 王锋锋, 刘鲁北, 等. C-ADS强流质子直线加速器调谐系统测试分析[J]. 强激光与粒子束, 2018, 30: 125101. doi: 10.11884/HPLPB201830.180155
引用本文: 张磊, 王锋锋, 刘鲁北, 等. C-ADS强流质子直线加速器调谐系统测试分析[J]. 强激光与粒子束, 2018, 30: 125101. doi: 10.11884/HPLPB201830.180155
Zhang Lei, Wang Fengfeng, Liu Lubei, et al. Test and analysis of tuner system for C-ADS high current proton linac[J]. High Power Laser and Particle Beams, 2018, 30: 125101. doi: 10.11884/HPLPB201830.180155
Citation: Zhang Lei, Wang Fengfeng, Liu Lubei, et al. Test and analysis of tuner system for C-ADS high current proton linac[J]. High Power Laser and Particle Beams, 2018, 30: 125101. doi: 10.11884/HPLPB201830.180155

C-ADS强流质子直线加速器调谐系统测试分析

doi: 10.11884/HPLPB201830.180155
基金项目: 

国家自然科学基金项目 91426303

详细信息
    作者简介:

    张磊(1994—), 男, 硕士研究生, 研究方向为精密机械工程, zhanglei@impcas.ac.cn

    通讯作者:

    张斌(1977—), 男, 正高级工程师, 研究方向为精密机械工程, zhangb@impcas.ac.cn

  • 中图分类号: TL5

Test and analysis of tuner system for C-ADS high current proton linac

  • 摘要: 调谐系统是C-ADS超导直线加速器不可或缺的一部分, 在加速器运行过程决定了超导腔的运行频率, 直接影响了粒子加速的效果。为了充分了解调谐系统的工作情况和分析调谐系统出现的问题, 设计了实验对调谐系统进行全方位测试。首先对调谐器的杠杆机构和剪叉机构进行了力学分析, 而后对半波长谐振(HWR) 超导腔在不同状态下进行了电场模拟, 得出设计的调谐力和调谐位移满足HWR腔频率调谐要求。最后通过详细实验, 采用自动、手动等方式测试了恒温器CM1, CM2, CM3中超导腔调谐器工作时的线性度、回程差、直线单元部分的线性度及回程。结果显示: CM1的调谐器基本满足慢调谐需要, CM2存在1200步回程, 主要原因在于直线单元部分; CM3中调谐器的回程差较大, 线性度不高, 需要进一步改进。
  • 图  1  25 MeV ADS加速器直线段

    Figure  1.  Layout of ADS 25 MeV Linac

    图  2  两种不同调谐器结构

    Figure  2.  Two tuners with different structure

    图  3  HWR腔体初始电场分布

    Figure  3.  Original electric field in HWR cavity

    图  4  受力后HWR腔体电场分布

    Figure  4.  Electric field of HWR cavity under force

    图  5  受指定位移后HWR腔体电场分布

    Figure  5.  Electric field of HWR cavity after displacement

    图  6  CM2-3手动测试结果

    Figure  6.  Curves of manual test of tuner in CM2-3

    图  7  CM1-2腔体频率曲线图

    Figure  7.  Curve of CM1-2 cavity frequency

    图  8  CM1-2腔体频率对应电机步进曲线图

    Figure  8.  Curve of tuner test in CM1-2

    图  9  CM2-3腔体频率对应电机步进曲线图

    Figure  9.  Curve of tuner test in CM2-3

    图  10  CM3-1腔体频率对应电机步进曲线图

    Figure  10.  Curve of tuner test in CM3-1

    图  11  直线驱动单元剖面图

    Figure  11.  Crossection of tuner linear driving unit

    图  12  调谐器直线单元测量

    Figure  12.  Test of linear part in tuner

    图  13  CM1-2移动盘位置对应电机步进数关系

    Figure  13.  Curves of the linear part test in CM1-2

    图  14  CM2-3移动盘位置对应电机步进数关系

    Figure  14.  The curve of linear part test in CM1-2

    图  15  CM3-1移动盘位置对应电机步进数关系

    Figure  15.  Curve of linear part test in CM3-1

    表  1  调谐器设计参数

    Table  1.   Parameters of tuner design

    tuner frequency/MHz tuning sensitivity k/(kHz·mm-1) tuning force F/(kN·mm-1) tuning resolution/(step·nm-1) tuning range f1/kHz
    HWR010 162.5 180 2.2 44 180
    HWR015 162.5 110 1.2 64 110
    下载: 导出CSV
  • [1] 方守贤, 王乃彦, 何多慧, 等. 关于加速器驱动次临界系统(ADS)研发促进我国核能可持续发展的建议[J]. 中国科学院院刊, 2009, 24(6): 641-644 https://www.cnki.com.cn/Article/CJFDTOTAL-KYYX200906016.htm

    Fang Shouxian, Wang Naiyan, He Duohui, et al. Suggestions on accelerator driven subcritical system (ADS) research and development to promote sustainable development of nuclear energy in China. High Bulletin of Chinese Academy of Sciences, 2009, 24(6): 641-644 https://www.cnki.com.cn/Article/CJFDTOTAL-KYYX200906016.htm
    [2] Wang Zhijun, He Yuan, Wang Wangsheng. End-to-end simulation of the C-ADS InjectorⅡ with a 3-D field map[J]. Chinese Physics C, 2013, 37: 047003. doi: 10.1088/1674-1137/37/4/047003
    [3] Jia Huan. Design and beam commissioning of beam lines for CADS injector Ⅱ prototype linac. Lanzhou: Institution of Modern Physics, Chinese Academy of Sciences, 2015: 7-11
    [4] He Shoubo. Study of mechanical stability and frequency tuning for low beta superconducting half-wave resonator in high intensity proton linac for China ADS. Lanzhou: Institution of Modern Physics, Chinese Academy of Sciences, 2014: 23-34
    [5] Liu Na. Development of tuner control system of Spoke012 superconducting cavity for C-ADS. Beijing: Institute of High Energy Physics, Chinese Academy of Sciences, 2016: 25-32
    [6] 葛明骐, 赵升初. 700 MHz单Cell超导腔洛伦兹力失谐分析[J]. 高能物理与核物理, 2005, 29(4): 413-417. doi: 10.3321/j.issn:0254-3052.2005.04.016

    Ge Mingqi, Zhao Shengchu. Lorentz force detuning analysis of 700 MHz single-cell superconducting cavity. High Energy Physics and Nuclear Physcis, 2005, 29(4): 413-417 doi: 10.3321/j.issn:0254-3052.2005.04.016
    [7] Mi Zhenghui. Design and research of tuner for superconducting cavity. Beijing: Institute of High Energy Physics, Chinese Academy of Sciences, 2015: 21-25
    [8] Ge M, Furuta F, GruberT, et al. Frequency tuner development at Cornell for the RAON half-wave-resonator[C]//Proceedings of IPAC. 2017: 1134-1137.
    [9] Paparelle R. Overview of recent tuner development on elliptical and low-beta cavities[C]//Proceedings of SRF. 2015.
    [10] He S, He Y, Huang Y, et al. Development of a slow tuner for 162.5 MHz superconducting half-wave resonator in IMP[C]//Proceedings of SRF. 2013: 1115-1117.
  • 加载中
图(15) / 表(1)
计量
  • 文章访问数:  1169
  • HTML全文浏览量:  212
  • PDF下载量:  98
  • 被引次数: 0
出版历程
  • 收稿日期:  2018-06-02
  • 修回日期:  2018-08-29
  • 刊出日期:  2018-12-15

目录

    /

    返回文章
    返回