• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    A superconductor has a coolant passage in the internal portion to cool itself by flowing a coolant in the coolant passage. The coolant passage is formed in the stabilizing material portion in such a manner that the inner wall of the coolant passage is wave-shaped, proportion of the cross-sectional area of the coolant passage occupied in the cross-section of the superconductor is 4-22 percent, and a ratio of the circumferential length to the cross-sectional area of the coolant passage is greater 25 (cm-1).
    公开号:SU1199208A3
    申请号:SU803219053
    申请日:1980-11-14
    公开日:1985-12-15
    发明作者:Тада Наофуми；Кимура Хироши；Огата Хизанао
    申请人:Хитачи,Лтд (Фирма)；
    IPC主号:
    专利说明:

    one
    The invention relates to superconductors, more specifically to those with internal-type cooling superconductors, and can be used in large-sized, creating strong magnetic fields of superconducting coils.
    The aim of the invention is to increase the cooling efficiency.
    The stability of a superconductor with an internal type of cooling can be judged by the fact that there is no parameter for stabilization of the expressed by
      uh
    -f 3 A I
    s -
    Pb (VT, l
    less than 0.8
    Here Y is the electrical resistivity (Ohm-cm) of the stabilizing material; J - current conduction (A
    superconductor A is the cross-sectional area (cm of stabilizing material j P is the length of the periphery of the channel (c h is the intensity of heat transfer
    . (W / cm. Hail); T - temperature (deg) of paraconductor j
    Tg - temperature (degrees) of the cooler.
    Suppose now that the heating conditions of the superconductor (the numerator in expression (1), the type of superconductor and the state of the coolant are unchanged, which is why the ratio and the stabilized state can be achieved by increasing P). Regarding the intensity of heat transfer in the case of use as a supercritical gel cooler, it is desirable that the cross-sectional area of the cooler channel is small and the peripheral length is large.
    On the other hand, in the case of an internal cooling type superconductor, when the coolant flow is created by injection, the pressure loss per unit length of the superconductor is expressed as
    .0
    . (2) U Sfr
    where P is the pressure difference; G. - the length of the conductor,
    9208. 2
    Accordingly, when the channel area of the cooler becomes small, the loss of pressure of the cooler becomes large and it is necessary to reduce the length of the channel of the cooler. As a result, the study described leads to the fact that the channel cross-sectional area may be equal to the minimum value of the allowable cooling point of view, and that the peripheral channel length can be increased, with an increase in the cross-section to the greatest extent. In order to increase the peripheral length of the duct, the peripheral length of the cooler duct wall is increased, which is in contact with the cooler.
    When considering a large size, creating strong magnetic fields of a superconducting coil, the conduction current of the superconductor of this coil is equal to several tens of kiloampere, and it turns into a conductor design that includes not only the superconducting superconducting wire capable of conducting such a current, but also stabilizing material, reinforcing element, etc. Accordingly, although the channel cross-sectional area occupied by the full cross section of the superconductor may vary depending on
    5 of these conditions, it is necessary that the ratio of the total circumferential length of the wall of the cooler channel in contact with the cooler to the full area of the channel section of the cooler is more than a certain value (30-40 cm) since, if this ratio is less than this value , stabilization of large size, creating
    5, the strong magnetic fields of the superconducting coil become difficult. The upper limit of the ratio of the total circumferential length of the wall of the cooler channel in contact with the cooler to the total cross-sectional area of the cooler channel is determined by the technology of the conductor and for the coolant channel. The lower limit value of the ratio of the cross-sectional area of the coolant channel to the cross-sectional area of the superconductor from the point of view of the length of the coolant channel
    Sizes that create strong magnet tulle superconducting katusha, is 4%. When this ratio is greater than 22%, the cross section of the conductor must be large, which leads to a decrease in the lot size of the coil current.
    FIG. 1 shows a sectional view of a superconductor with an internal type of cooling according to the invention, a variant of FIG. 2 - the same, the second variant, in FIG. 3 is a plot of the dependencies between the stabilization parameter (about) and the ratios of the peripheral length of the coolant channel to the cross-sectional area of the coolant channel of superconductors with different ratios of the cross-sectional area of the superconductor cross section in FIG. 4 is a graph showing the relationship between the length of the coolant channel and the ratios of the peripheral length of the coolant channel to the coolant channel area of superconductors with different ratios of the coolant channel cross section area to the superconductor cross section.
    FIG. I shows a designed and manufactured superconductor. Its cross-sectional dimensions are equal: width 46 and height 21 mm, critical current of a superconductor 40 kA with magnetic indentation 1 2 T and temperature 5 K K means absolute temperature).
    According to FIG. I superconductor 1 includes a pair of tri-niobium-tin (NbjSn) containing composite superconducting conductors 2 coated with a stabilizing material, such as copper, aluminum, etc., a stabilizer 3, and a pair of reinforcing elements 4. A stabilizer 3 made of copper aluminum or other similar materials, is provided in the central part of the cross section with a channel and a cooler. The cooling channel 4 has a wave-shaped side wall and is provided with a plurality of ribs with a height of 2 mm at an angle of sharpening 30. The reinforcing element 5 is made of stainless steel coated with a heat-conducting material 6, such as copper or other similar material. A pair of reinforcing elements 5 is connected to the stabilizer 3 by soldering silver solder 92084
    or electron-welded welding so that high thermal conductivity can be maintained. The stabilizer and reinforcement assembly is connected to a pair of composite superconducting wires 2 by brazing with silver, electron beam welding, or another similar method, in order to maintain high thermal conductivity. The ratio of the cross-sectional area of the coolant channel to the total cross-sectional area of superconductor 1 is equal to 8.3%, and the ratio of the peripheral length of the wall of the coolant channel 15 that is in contact with the coolant to the cross-sectional area of the coolant channel is then 26.4 cm. In the case when supercritical 20 helium at a temperature of 5 K under a pressure of 8 atm is pumped through the cooler channel of the described superconductor at a flow rate of 5 g / s, and a current passes through the steam-conductor part
    25 coil power of 20 kA. As a result, the described stabilization parameter becomes 0.75, and the superconductor is stabilized. Loss of pressure in the coolant channel
    30 is 2.6 at a channel length of 10 m. The supercritical state is satisfactorily maintained even in the outlet of the channel, and the acceptable value of the channel length is
    is given for a large-sized superconducting coil. In this case, the current density of the entire conductor, including the channel of the cooler, is equal to 41.4 A / mm with magnetic induction
    Q 12 T and may be high for superconductors of this type.
    FIG. 2 shows a superconductor in which the coolant channel is a large
    45 number of components parallel
    channels. The cross-sectional dimensions and parameters of the superconductor I are the same as in the described embodiment and include
    50 how many containing superconducting Nb.Sn superconductors w 1x wires 2, each of which is covered with a stabilizing material, several stabilizers 3, each of which
    55 is equipped with a coolant channel 4, and several reinforcing elements 5, covered with heat-conducting material 6. Stabilizer 4 and a pair of reinforcing-.aix 1lemet1t.p) with heat-conducting mlterlppm 6, located on opposite sides, are connected by soldering silver, 1M solder, electron and - beam welding or another similar method - in order to form node 7, Node 7 is located between a pair of Nb, Sn containing composite superconducting wires 2 and is connected to them in the same manner as indicated. Since the superconductor 1 is divided into several parts (the channel ohm the separator is divided into four elements), the peripheral length of the channel of the cooler 4, which is in contact with the wall 8 of the channel, is larger than the channel section of the cooler 4. The inner surface of the wall of the channel 8 is provided with uneven mi having a radius of 0.5 mm. As a result, the proportion of the cross section of the channel 4 of the cooler 4, which is occupied in the full cross section of the conductor, is 6.2%, and the ratio of the total peripheral length of the wall 8 of the channel of the cooler that is in contact with the cooler to the cross section area of the cooler 4 is 33.5 cm The stability of superconductor 1 under the conditions of the described variant, the stabilization parameter cc is equal to 0.57, while superconductor 1 is more rigid than the described one, and the pressure loss in the channel of cooler 4 is 2.9 at a channel length of 500 m. the critical state is satisfactorily maintained even in the output part of the channel, and an acceptable value for the length of the channel is created for the large-sized superconducting one. When stabilization conditions 086 are similar to the described variant, the current density of the whole CP of the superconductor 1, including the channels of the cooler 4, is 46.6 L / mm with a magnetic induction and 12 T, i.e. more than in superconductor 1. Then, as applied to niobiumol () superconductor. which had the same cross-sectional dimensions as the two options described, examine the cross-sectional area of the coolant channel, its peripheral length in contact with the channel wall, the stability of the superconductor, and the pressure loss in the coolant channel. The cross-sectional areas of the niobium-tin () composite superconducting wires and reinforcing elements are kept constant, and an increase or decrease in the cross-sectional area of the cooler channel is created by increasing or decreasing the cross-sectional area of the stabilizing material. The cross-sectional dimensions of said superconductors, the material of the composite superconducting wire, the cross-sectional area of the reinforcing element, the parameters of the superconductor, the state of the cooler, etc. remain unchanged. However, even when the numerical values and parameters of these superconductors increase, which creates strong magnetic fields, these effects are not significantly reduced. The invention also relates to other superconducting materials, such as vanadium-gallium and niobium titanium.
    权利要求:
    Claims (1)
    [1]
    A SUPERCONDUCTOR COOLED WITH AN INTERNAL TYPE, containing two parallel superconducting wires and a cooling channel extending along the superconducting wires, characterized in that, with a circuit for increasing cooling efficiency, two reinforcing elements are arranged one above the other and between the superconducting wires and a stabilizer, moreover, the stabilizer is located between the reinforcing elements, while the cooling channel passes inside the stabilizer, the inner surface of which is provided with ribs having an acute angle of 30 °, and the ratio of the cross-sectional length of the inner wall of the channel for cooling to the cross-sectional area of this channel is 30-40 cm ', and the cross-sectional area of the cooling channel is 4-22% of the total area of the superconductor.
    SU „„ 1199208
    1 1 99 208
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    同族专利:
    公开号 | 公开日
    JPH0156486B2|1989-11-30|
    DE3042102A1|1981-06-04|
    JPS5671212A|1981-06-13|
    US4334123A|1982-06-08|
    CH654439A5|1986-02-14|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    DE1440838A1|1963-07-27|1969-03-27|Bbc Brown Boveri & Cie|Conductor rail with enlarged surface|
    NL132696C|1966-05-20|
    FR1503956A|1966-10-20|1967-12-01|Comp Generale Electricite|Cryogenic electric cable structure|
    DE2113597B2|1971-03-20|1978-03-09|Kabel- Und Metallwerke Gutehoffnungshuette Ag, 3000 Hannover|High-voltage, superconducting low temp. electric cable - has core of foamed plastic soaked with e.g. liquid helium|
    US4039740A|1974-06-19|1977-08-02|The Furukawa Electric Co., Ltd.|Cryogenic power cable|
    CH597677A5|1975-04-09|1978-04-14|Siemens Ag|
    CH604332A5|1975-12-15|1978-09-15|Bbc Brown Boveri & Cie|
    JPS5457994A|1977-10-18|1979-05-10|Kobe Steel Ltd|Superconductor|JPS56112011A|1980-02-12|1981-09-04|Japan Atomic Energy Res Inst|Composite superconductor|
    JPS6262001B2|1982-07-09|1987-12-24|Hitachi Seisakusho Kk|
    US5248656A|1987-04-06|1993-09-28|Hewlett-Packard Company|Method of making superconductor wires, or capillaries|
    US5132487A|1989-02-20|1992-07-21|Hoersch Robert C|Superconductor transmission line|
    US5620798A|1995-05-17|1997-04-15|The Babcock & Wilcox Company|Aluminum stabilized superconductor supported by aluminum alloy sheath|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    JP54147790A|JPH0156486B2|1979-11-16|1979-11-16|
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