检索规则说明:AND代表“并且”;OR代表“或者”;NOT代表“不包含”;(注意必须大写,运算符两边需空一格)
检 索 范 例 :范例一: (K=图书馆学 OR K=情报学) AND A=范并思 范例二:J=计算机应用与软件 AND (U=C++ OR U=Basic) NOT M=Visual
作 者:吴腾马 周巧根 樊凯[1,2] 张继东 Wu Tengma;Zhou Qiaogen;Fan Kai;Zhang Jidong(Shanghai Institute of Advanced Research,Chinese Academy of Sciences,Shanghai 201204,China;Shanghai Institute of Applied Physics,Chinese Academy of Sciences,Shanghai 201800,China)
机构地区:[1]中国科学院上海高等研究院,上海201204 [2]中国科学院上海应用物理研究所,上海201800
出 处:《低温与超导》2022年第7期17-20,27,共5页Cryogenics and Superconductivity
基 金:国家自然科学基金(11275254);上海应用物理研究所真空内波荡器项目(1105000503)资助。
摘 要:为消除在线运行时超导波荡器内束流热负荷对超导磁体的影响,并给储存环提供高真空环境,为波荡器安装了一套束流室并对其隔热效果进行研究。通过将波荡器安装至储存环内,实验对比测试了带束流与不带束流时波荡器内束流室与磁体的温度变化情况。结合G-M制冷机的工作特性,利用热平衡法测出了200 mA流强的束流对束流室和磁体产生的热负荷。实验结果显示,通束流后,束流室温度从17.2 K上升至28.3 K,磁体温度从4.3 K上升至4.4 K,束流在束流室上产生的热负荷为17.4 W,在磁体上产生的热负荷为0.2 W。表明束流室可有效屏蔽束流热负荷对磁体的影响,并使磁体工作在4.5 K以下。In order to eliminate the influence of beam heat load to superconducting magnet in superconducting undulator and provide a high vacuum environment to the storage ring during the test for beam,a set of beam chamber was installed and its thermal insulation effect was studied.The temperature variation of the beam chamber and magnet in the undulator was measured and compared while the beam was upload and not,which was stated after the installation of undulator in the storage ring.The thermal load of 200 mA current intensity in beam chamber and magnet was tested while heat balance method was used.The results show that beam chamber temperature increases from 17.2 K to 28.3 K and magnet temperature increases from 4.3 K to 4.4 K separately.The heat load generated by beam current on the beam chamber is 17.4 W.The heat load generated by beam current on the magnet is 0.2 W.It shows that the beam chamber can effectively shield the influence of beam heat load on the magnet and make the magnet work below 4.5 K.
分 类 号:TQ025.2[化学工程] TM265[一般工业技术—材料科学与工程]
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在链接到云南高校图书馆文献保障联盟下载...
云南高校图书馆联盟文献共享服务平台 版权所有©
您的IP:3.138.174.90