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    • 1. 发明授权
    • Superconducting bearing device
    • 超导轴承装置
    • US5801469A
    • 1998-09-01
    • US117088
    • 1994-02-08
    • Ryoichi TakahataMotoaki ShibayamaHiroshi Takaichi
    • Ryoichi TakahataMotoaki ShibayamaHiroshi Takaichi
    • F16C32/04F16C39/06H02J15/00H02K7/09
    • F16C32/0438F16C2240/40F16C2300/34
    • A superconducting bearing device comprises an annular permanent magnetic portion 2 disposed concentrically with a rotary body 1 in the form of a vertical shaft, and superconductors 8 opposed to the lower end face of the magnet portion 2 and vertically spaced apart therefrom. The permanent magnet portion 2 comprises a disk 4 fixedly mounted on the rotary body 1, and annular permanent magnets 6a, 6b arranged on the disk 4 at a spacing radially of the rotary body 1. Each of the magnets 6a, 6b has upper and lower ends magnetized to polarities opposite to each other, and the adjacent magnets 6a, 6b are magnetized to polarities opposite to each other at the upper ends, as well as at the lower ends. The radial spacing between the magnets 6a, 6b is optimized in accordance with the radial dimension (width) of the magnets 6a, 6b. This improves the device in load capacity and rigidity and prevents the deflection of axis of the rotary body 1, enabling the bearing device to support the rotary body 1 in a noncontact state with good stability.
    • PCT No.PCT / JP92 / 00301 Sec。 371日期1994年2月8日 102(e)日期1994年2月8日PCT提交1992年3月13日PCT公布。 WO92 / 16762 PCT出版物 日期:1992年10月1日超导轴承装置包括与垂直轴形式的旋转体1同心设置的环形永磁部分2和与磁体部分2的下端面相对并且与其垂直间隔开的超导体8 。 永磁体部分2包括固定地安装在旋转体1上的盘4和以旋转体1的径向间隔设置在盘4上的环形永磁体6a,6b。每个磁体6a,6b具有上下 端部被磁化成彼此相反的极性,并且相邻的磁体6a,6b在上端以及在下端被磁化成彼此相反的极性。 磁体6a,6b之间的径向间隔根据磁体6a,6b的径向尺寸(宽度)进行优化。 这提高了装置的负载能力和刚性,并且防止旋转体1的轴线的偏转,使得轴承装置能够以非常接触的状态将旋转体1支撑在良好的稳定性。
    • 2. 发明授权
    • Superconducting bearing device
    • 超导轴承装置
    • US5739606A
    • 1998-04-14
    • US632612
    • 1996-04-15
    • Ryoichi TakahataMotoaki ShibayamaHiroshi Takaichi
    • Ryoichi TakahataMotoaki ShibayamaHiroshi Takaichi
    • F16C39/06H02K7/09
    • F16C32/0438F16C2300/34
    • A superconducting bearing device comprises an annular permanent magnet portion disposed concentrically with a rotary body in the form of a vertical shaft, and superconductors opposed to the lower end face of the magnet portion and vertically spaced apart therefrom. The permanent magnet portion comprises a disk fixedly mounted on the rotary body, and annular permanent magnets embedded in the disk at a spacing radially of the rotary body. Each of the magnets has upper and lower ends magnetized to polarities opposite to each other, and the adjacent magnets are magnetized to polarities opposite to each other at the upper ends, as well as at the lower ends. The radial spacing between the magnets is optimized in accordance with the radial dimension (width) of the magnets. This improves the device in load capacity and rigidity and prevents the deflection of axis of the rotary body, enabling the bearing device to support the rotary body in a noncontact state with good stability.
    • 超导轴承装置包括与垂直轴形式的旋转体同心地设置的环形永磁体部分,以及与磁体部分的下端面相对并且与其垂直间隔开的超导体。 永磁体部分包括固定地安装在旋转体上的盘,以及以旋转体径向间隔嵌入盘中的环形永久磁体。 每个磁体具有被磁化成彼此相反的极性的上端和下端,并且相邻的磁体在上端以及在下端被磁化成彼此相反的极性。 根据磁体的径向尺寸(宽度)来优化磁体之间的径向间隔。 这提高了装置的负载能力和刚性,并且防止旋转体的轴线的偏转,使得轴承装置能够以非常接触的状态将旋转体支撑在良好的稳定性。
    • 4. 发明授权
    • Superconductor and method of producing same
    • 超导体及其制造方法
    • US5525584A
    • 1996-06-11
    • US452138
    • 1995-05-26
    • Masato MurakamiSang-Im YooNaomichi SakaiHiroshi TakaichiTakamitsu HiguchiShoji Tanaka
    • Masato MurakamiSang-Im YooNaomichi SakaiHiroshi TakaichiTakamitsu HiguchiShoji Tanaka
    • H01L39/12H01B12/00
    • H01L39/126Y10S505/742Y10S505/778Y10S505/779Y10S505/785
    • A high critical temperature and high critical current density superconductor is disclosed which contains a metal oxide expressed by the following formula (I):(R.sup.1.sub.1-x,Ba.sub.x)Ba.sub.2 Cu.sub.3 O.sub.d (I)wherein R.sup.1 stands for at least one element selected from the group consisting of La, Nd, Sm, Eu and Gd, x is a number greater than 0 but not greater than 0.5 and d is a number between 6.2 and 7.2. Fine phases of RE211, RE422 and/or a metal oxide expressed by the formula (R.sup.2.sub.1-z, Ba.sub.z) (Ba.sub.1-y, R.sup.2.sub.y).sub.2 Cu.sub.3 O.sub.p (R.sup.2 =La, Nd, Sm, Eu or Gd) may be dispersed in a matrix of the matrix phase of the formula (I). The above superconductor may be obtained by cooling a melt having a temperature of 1,000.degree.-1,300.degree. C. and containing R.sup.1, Ba, Cu and O at a cooling rate of 5.degree. C./hour or less under a partial pressure of oxygen of between 0.00001 and 0.05 atm, followed by annealing at 250.degree.-600.degree. C. in an oxygen atmosphere.
    • 公开了一种高临界温度和高临界电流密度超导体,其包含由下式(I)表示的金属氧化物:(R11-x,Bax)Ba2Cu3Od(I)其中R1代表选自以下的至少一种元素: 的La,Nd,Sm,Eu和Gd,x是大于0但不大于0.5的数,d是6.2和7.2之间的数。 RE211,RE422和/或由式(R21-z,Baz)(Ba1-y,R2y)2Cu3Op(R2 = La,Nd,Sm,Eu或Gd)表示的金属氧化物的细相可以分散在基质 的式(I)的基质相。 上述超导体可以通过在5℃/小时以下的冷却速度下,在温度为1000〜-1300℃的温度下冷却含有R 1,Ba,Cu和O的熔体, 在0.00001和0.05atm之间,然后在氧气氛中在250-600℃退火。
    • 7. 发明授权
    • Superconductor and method of producing same
    • 超导体及其制造方法
    • US5849667A
    • 1998-12-15
    • US683915
    • 1996-07-19
    • Masato MurakamiSang-Im YooNaomichi SakaiHiroshi TakaichiTakamitsu HiguchiShoji Tanaka
    • Masato MurakamiSang-Im YooNaomichi SakaiHiroshi TakaichiTakamitsu HiguchiShoji Tanaka
    • H01L39/12H01B12/00C04B35/50
    • H01L39/126Y10S505/742Y10S505/778Y10S505/779Y10S505/785
    • A high critical temperature and high critical current density superconductor is disclosed which contains a metal oxide expressed by the following formula (I): (R.sup.1.sub.1-x, Ba.sub.x)Ba.sub.2 Cu.sub.3 O.sub.d (I) wherein R.sup.1 stands for at least one element selected from the group consisting of La, Nd, Sm, Eu and Gd, x is a number greater than 0 but not greater than 0.5 and d is a number between 6.2 and 7.2. Fine phases of RE211, RE422 and/or a metal oxide expressed by the formula (R.sup.2.sub.1-z, Ba.sub.z) (Ba.sub.1-y, R.sup.2.sub.y).sub.2 Cu.sub.3 O.sub.p (R.sup.2 =La, Nd, Sm, Eu or Gd) may be dispersed in a matrix of the matrix phase of the formula (I). The above superconductor may be obtained by cooling a melt having a temperature of 1,000.degree.-1,300.degree. C. and containing R.sup.1, Ba, Cu and O at a cooling rate of 5.degree. C./hour or less under a partial pressure of oxygen of between 0.00001 and 0.05 atm, followed by annealing at 250.degree.-600.degree. C. in an oxygen atmosphere.
    • 公开了一种高临界温度和高临界电流密度超导体,其包含由下式(I)表示的金属氧化物:( R11-x,Bax)Ba2Cu3Od(I)其中R1表示选自以下的至少一种元素: 的La,Nd,Sm,Eu和Gd,x是大于0但不大于0.5的数,d是6.2和7.2之间的数。 RE211,RE422和/或由式(R21-z,Baz)(Ba1-y,R2y)2Cu3Op(R2 = La,Nd,Sm,Eu或Gd)表示的金属氧化物的细相可以分散在基质 的式(I)的基质相。 上述超导体可以通过在5℃/小时以下的冷却速度下,在温度为1000〜-1300℃的温度下冷却含有R 1,Ba,Cu和O的熔体, 在0.00001和0.05atm之间,然后在氧气氛中在250-600℃退火。