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    • 6. 发明授权
    • Cryostat with external refrigerator for super-conducting NMR spectrometer
    • 低温恒温器与外部冰箱用于超导NMR分析仪
    • US4291541A
    • 1981-09-29
    • US164451
    • 1980-06-30
    • George D. Kneip, Jr.Marvin H. Anderson
    • George D. Kneip, Jr.Marvin H. Anderson
    • F17C3/08F25D3/10F25D19/00G01R33/3815F17C1/00
    • F25D3/10F17C3/085G01R33/3815F17C2203/016F17C2203/0687F17C2221/014F17C2221/017F17C2270/0509F25D19/006Y10S220/901Y10S505/893
    • An improved cryostat for the superconducting magnet of an NMR spectrometer comprises a nested structure of isothermal shells surrounding a thermally conductive central reservoir of substantially spherical shape containing liquid helium in which the superconducting solenoid remains operational when only partially immersed. A radiation shield surrounding the central reservoir is cooled by the boil-off of escaping helium vapor. The radiation shield is enclosed within a isothermal shell maintained at the temperature of liquid nitrogen by thermal contact with a liquid nitrogen reservoir disposed above the region of the central reservoir and shielded therefrom by a wall of the isothermal shell. An outer radiation shield surrounds the liquid nitrogen reservoir and associated isothermal shell and the outer radiation shield is maintained at a temperatures of the order of 180.degree. K. by an external refrigeration facility. A hermitically sealed containment vessel forms the outer wall of the cryostat and provides a port for evacuating to a very low common pressure all the interior spaces between adjacent nested structures. The spacing between adjacent nested surfaces is maintained by a novel internal mechanical bracing system of low thermal conductivity comprising polyester cords disposed under tension between adjacent shells.
    • 用于NMR光谱仪的超导磁体的改进的低温恒温器包括围绕包含液氦的基本上为球形的导热中心储存器的等温壳体的嵌套结构,其中超导螺线管在仅部分浸入时保持操作。 围绕中央储层的辐射屏蔽体由逸出的氦气蒸气冷却。 通过与设置在中央储存器的区域上方的液氮储存器热接触并保持在液氮温度的等温壳体中,辐射屏蔽被封闭在等温壳体内,并通过等温壳体的壁与其隔开。 外部辐射屏蔽围绕液氮储存器和相关的等温壳,外部辐射屏蔽通过外部制冷设备保持在180°K左右的温度。 密闭的密封容器形成低温恒温器的外壁,并提供用于将相邻嵌套结构之间的所有内部空间抽真空至非常低的共同压力的端口。 相邻嵌套表面之间的间距由新型的低导热性内部机械支撑系统保持,包括在相邻外壳之间张力下布置的聚酯帘线。
    • 8. 发明公开
    • Superconducting lead assembly for a cryocooler-cooled superconducting magnet
    • SupraleitendeZuführungfüreinentieftemperaturgekühltensupraleitenden Magnet。
    • EP0673043A1
    • 1995-09-20
    • EP95301498.2
    • 1995-03-08
    • GENERAL ELECTRIC COMPANY
    • Herd, Kenneth GordonLaskaris, Evangelos TrifonThompson, Paul Shadforth
    • H01F6/06H01F6/02F17C13/00
    • H01F6/065Y10S505/844Y10S505/879Y10S505/893
    • A superconducting magnet lead assembly for a cryocooler-cooled superconducting magnet having a design current of between generally 50 and 250 amperes. A DBCO (Dysprosium Barium Copper Oxide), YBCO (Yttrium Barium Copper Oxide), or BSCCO (Bismuth Strontium Calcium Carbonate) superconducting lead has its ends flexibly, dielectrically, and thermally connected, one end to the generally 30 to 50 Kelvin first stage and the other end to the generally 8 to 30 Kelvin second stage of the cryocooler coldhead. The superconducting lead has a generally constant cross-sectional area along its length. The design current, the lead's length, and the lead's cross-sectional area are chosen such that the design current times the lead's length divided by the lead's cross-sectional area is between generally 720 and 880 amperes per centimeter for a DBCO or YBCO lead and is between generally 180 and 220 amperes per centimeter for a BSCCO lead. The superconducting lead will not itself precipitate a magnet quench (i.e., the superconducting lead does not conduct significant heat between the coldhead stages during the superconductive mode), and the superconducting lead will survive a lead quench from other causes (i.e., the superconducting lead does conduct the resistive heat buildup to the coldhead stages during a lead quench) and thus be acceptable for commercial applications.
    • 一种用于低温冷却超导磁体的超导磁体引线组件,其具有通常为50和250安培之间的设计电流。 DBCO(氧化镝钡氧化物),YBCO(钇钡氧化铜)或BSCCO(铋锶钙氧化铜)超导导线的端部灵活,介电和热连接,一端通常为30至50开尔文第一级 另一端通常是低温冷冻机的8〜30开尔文第二阶段。 超导引线沿其长度具有大致恒定的横截面积。 选择设计电流,引线长度和引线的横截面积,使得引线长度除以引线横截面积的设计电流乘以DBCO或YBCO引线的通常为720至880安培/厘米, 对于BSCCO铅,通常在每厘米180和220安培之间。 超导引线本身不会沉淀出磁体淬火(即,超导引线在超导模式下在冷端级之间不会产生显着的热),并且超导引线将从其他原因引发淬火(即,超导引线 在铅淬火期间对冷头阶段进行电阻积热),因此对于商业应用是可以接受的。