JPS63305747A - Rotor for superconducting rotary machine - Google Patents
Rotor for superconducting rotary machineInfo
- Publication number
- JPS63305747A JPS63305747A JP14021187A JP14021187A JPS63305747A JP S63305747 A JPS63305747 A JP S63305747A JP 14021187 A JP14021187 A JP 14021187A JP 14021187 A JP14021187 A JP 14021187A JP S63305747 A JPS63305747 A JP S63305747A
- Authority
- JP
- Japan
- Prior art keywords
- field coil
- superconducting
- superconducting field
- liquefied gas
- cooling
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000001816 cooling Methods 0.000 claims abstract description 18
- 238000004891 communication Methods 0.000 claims abstract description 7
- 230000008016 vaporization Effects 0.000 claims abstract description 5
- 238000009834 vaporization Methods 0.000 claims abstract description 5
- 239000007788 liquid Substances 0.000 claims description 23
- 239000012530 fluid Substances 0.000 abstract 3
- 230000002708 enhancing effect Effects 0.000 abstract 1
- 239000003507 refrigerant Substances 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 238000009413 insulation Methods 0.000 description 3
- 229910000831 Steel Inorganic materials 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000007654 immersion Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 239000002887 superconductor Substances 0.000 description 1
- 238000003466 welding Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、超電導発電機などの回転機の回転子(以下
、超電導回転子)に関するもので、特に超電導界磁コイ
ルの冷却方式の改良に関するものである。[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to a rotor for a rotating machine such as a superconducting generator (hereinafter referred to as a superconducting rotor), and particularly relates to an improvement in the cooling method of a superconducting field coil. It is something.
第2図は先行出願の超電導回転子の内部構造を示す断面
図である。図において、(1)は超電導界磁コイル、(
2)はこの超電導界磁コイルを固定するコイル取付軸、
(3)は駆動側の端部軸A、+41は反駆動側の端部軸
B、+61は端部軸A(3)とコイル取付軸の一端を中
継する薄肉円筒で構成したトルクチューブA 、 +6
1は反駆動側に同様に設けたトルクチューブBである。FIG. 2 is a sectional view showing the internal structure of the superconducting rotor of the prior application. In the figure, (1) is a superconducting field coil, (
2) is the coil mounting shaft that fixes this superconducting field coil;
(3) is the end shaft A on the drive side, +41 is the end shaft B on the non-drive side, +61 is the torque tube A composed of a thin cylinder that relays the end shaft A (3) and one end of the coil mounting shaft, +6
1 is a torque tube B similarly provided on the non-drive side.
(7)は上記の超電導界磁コイル(1)とコイル取付軸
(2)およびトルクチューブA(5)およびB(6)の
外周側に設けられこれらを収納する円筒であり、この円
筒の両端部に端部軸A 、 B(31、+4)がそれぞ
れ例えば溶接により一体化接合されて断熱真空部Sを形
成している。(8)は一端がコイル取付軸(2)を介し
て超電導界磁コイル+11に熱的に接触し、他端は真空
部Sから端部軸(4)を貫通して真空部外に突出する伝
熱部材であり、例えば鋼やアルミニウムなどの熱良導性
の複数本の棒状伝熱部材がコイル取付軸(2)の適当箇
所に設けられた孔に挿入されている。(9)ハ伝熱部材
(8)の突出部であり、熱交換能を高めるために放熱フ
ィンが設けられている。(7) is a cylinder provided on the outer circumferential side of the superconducting field coil (1), coil mounting shaft (2), and torque tubes A (5) and B (6) to house them, and both ends of this cylinder are The end shafts A and B (31, +4) are integrally joined to each other by, for example, welding to form a heat insulating vacuum part S. One end of (8) is in thermal contact with the superconducting field coil +11 via the coil mounting shaft (2), and the other end extends from the vacuum section S through the end shaft (4) and projects outside the vacuum section. A plurality of rod-shaped heat transfer members having good thermal conductivity, such as steel or aluminum, are inserted into holes provided at appropriate locations on the coil mounting shaft (2). (9) This is a protruding portion of the heat transfer member (8), and is provided with heat radiation fins to enhance heat exchange performance.
(lαは伝熱部材(8)と端部軸(4)とを熱的に離間
させるように設けた熱絶縁のための真空断熱継手である
。(lα is a vacuum insulation joint for heat insulation provided to thermally separate the heat transfer member (8) and the end shaft (4).
(!l)は超電導界磁コイル+11に通電するための電
流リード、[+21 、α31はそれぞれ端部軸A #
a 131 # +41を支持する軸受A、Bである
。なお、端部軸B(4)端には静止部から回転部の電流
リード(11)に通電するスリップリングを備えるが、
ここでは省略する。また、伝熱部材(8)の突出部(9
)には適当な断熱手段が施されているが、ここでは図示
していない。(!l) is the current lead for energizing the superconducting field coil +11, [+21 and α31 are the end shafts A #
Bearings A and B support a 131 # +41. Note that a slip ring is provided at the end of the end shaft B (4) to conduct electricity from the stationary part to the current lead (11) of the rotating part.
It is omitted here. In addition, the protrusion (9) of the heat transfer member (8)
) is provided with suitable insulation means, but not shown here.
以上のように構成された超電導回転子の冷却はつぎのよ
うにして行なわれる。伝熱部材(8)の突出部(9)を
低温液化ガスなどの冷媒により一定温度に冷却保持する
。このとき、超電導界磁コイルil+の熱(周囲から受
けるもの、及び自己発熱によるもの)は、コイル取付軸
(21から伝熱部材(8)を経て上記冷媒に奪い去られ
る。The superconducting rotor constructed as described above is cooled as follows. The protrusion (9) of the heat transfer member (8) is cooled and maintained at a constant temperature by a refrigerant such as low-temperature liquefied gas. At this time, the heat of the superconducting field coil il+ (those received from the surroundings and those due to self-heating) are taken away by the refrigerant from the coil attachment shaft (21) via the heat transfer member (8).
超電導界磁コイル11)及びコイル取付軸(2)の熱負
荷に対して、十分熱抵抗の小さい伝熱路を構成すること
により、超電導界磁コイル(1)をはソ冷媒温度に冷却
保持する。The superconducting field coil (1) is cooled and maintained at the refrigerant temperature by configuring a heat transfer path with sufficiently low thermal resistance against the heat load of the superconducting field coil 11) and the coil mounting shaft (2). .
従来の超電導回転子は以上のように構成されているので
、突発的に発生する異常な熱負荷があるとき、これを速
やかに除き超電導界磁コイルを所期の温度以下に冷却保
持するために−は伝熱部材の断面積を大きくしなければ
ならず、逆に回転子の寸法に制約があると伝熱部材の断
面積が十分とれず熱負荷変動で温度が上昇するなどの問
題があったO
この発明は上記のような問題点を解消するためになされ
たもので、超電導界磁コイル部に冷媒を用いたヒート・
シンクを設け、一時的な負荷変動に伴う熱を吸収して安
定に冷却できるとともに信頼性の高い超電導回転子を得
ることを目的とする。Conventional superconducting rotors are configured as described above, so when there is an abnormal heat load that suddenly occurs, it is necessary to quickly remove this and keep the superconducting field coil cooled to below the desired temperature. -, the cross-sectional area of the heat transfer member must be increased; conversely, if there are restrictions on the dimensions of the rotor, the cross-sectional area of the heat transfer member may not be sufficient, leading to problems such as temperature rise due to heat load fluctuations. This invention was made to solve the above-mentioned problems, and is a heat exchanger using a refrigerant in the superconducting field coil.
The objective is to provide a highly reliable superconducting rotor that can be stably cooled by providing a sink to absorb heat caused by temporary load fluctuations.
この発明に係る超電導回転機の回転子は、円筒、この円
筒の両端部にそれぞれ設けられ上記円筒内に真空部を形
成する端部軸、この端部軸に断熱的に支持されて上記真
空部に配置される超電導界磁コイル、および一方は上記
超電導界磁コイルに熱的に接触し、他方は上記真空部か
ら上記端部軸を貫通して真空部外に突出する伝熱部材、
上記超電導界磁コイルに熱的に接触して設けられ液化ガ
スを貯蔵する液溜、この液溜と外部とを連通し、液溜の
圧力を一定に保持する連通管を備え、上記伝熱部材の突
出部を冷却することにより上記超電導界磁コイルを冷却
すると共に、上記超電導界磁コイルの熱負荷変動を上記
液化ガスの蒸発潜熱により吸収するようにしたものであ
る。A rotor of a superconducting rotating machine according to the present invention includes a cylinder, an end shaft provided at both ends of the cylinder and forming a vacuum section in the cylinder, and adiabatically supported by the end shaft to form the vacuum section. a heat transfer member, one of which is in thermal contact with the superconducting field coil and the other of which extends from the vacuum section through the end shaft and projects out of the vacuum section;
A liquid reservoir provided in thermal contact with the superconducting field coil to store liquefied gas, a communication pipe communicating the liquid reservoir with the outside and keeping the pressure of the liquid reservoir constant, the heat transfer member The superconducting field coil is cooled by cooling the protrusion of the superconducting field coil, and variations in the thermal load of the superconducting field coil are absorbed by the latent heat of vaporization of the liquefied gas.
この発明における伝熱部材は、超電導界磁コイルを定常
的に冷却し、液溜に貯蔵された液化ガスは超電導界磁コ
イルの突発的な熱負荷変動を吸収するので、冷却安定性
に優れ、信頼性の高い超電導回転機の回転子が得られる
。The heat transfer member according to the present invention constantly cools the superconducting field coil, and the liquefied gas stored in the liquid reservoir absorbs sudden heat load fluctuations of the superconducting field coil, so it has excellent cooling stability. A rotor for a highly reliable superconducting rotating machine can be obtained.
以下、この発明の一実施例を図をもとに説明する。j1
!1図において、α41t;j、超電導界磁コイル+1
1に熱的に接触して設けられだ液溜であり、この例では
コイル取付@(りに一体化させ、伝熱部材(8)の内周
側に環状の空間部を形成するように設けられている。0
υは液溜(14の圧力を一定に保持する連通管であり、
液溜(14)から端部軸B(4)の中心軸部を貫通し、
回転軸シール部(図示せず)を介して一定圧力に制御可
能な例えばバッファタンク(図示せず)に連通している
。6輪は液溜041内に貯蔵される液化ガスである。An embodiment of the present invention will be described below with reference to the drawings. j1
! In Figure 1, α41t;j, superconducting field coil +1
In this example, it is integrated with the coil mounting plate (8) and is provided so as to form an annular space on the inner circumferential side of the heat transfer member (8). 0
υ is a communication pipe that maintains the pressure of the liquid reservoir (14) constant,
The liquid reservoir (14) passes through the center shaft of the end shaft B (4),
It communicates with, for example, a buffer tank (not shown) that can be controlled to a constant pressure via a rotating shaft seal (not shown). Six wheels are liquefied gas stored in the liquid reservoir 041.
上記のように構成された超電導回転子では、超電導界磁
コイルfllはつぎのようにして冷却される。In the superconducting rotor configured as described above, the superconducting field coil fll is cooled as follows.
従来のものと同様に、超電導界磁コイルfi1部の熱は
、伝熱部材(8)を経由して突出部(9)の放熱フィン
から冷媒である低温液化ガスて放出される。ここで、液
溜H内の液化ガスaφとして突出部(9)の冷却温度と
同じか、若しくは僅かに烏い液化点のものを用いるとき
、超電導界磁コイルTl+の熱負荷に較べて冷却能力に
余裕があれば、余剰冷却により液化ガス(16)の気化
していたものは液化され、液溜(14内に一定量が貯え
られる。一方、熱擾乱により一時的に超電導界磁コイル
fl+を含む被冷却部の熱負荷が伝熱部材(8)による
冷却能力を上回るとき、液溜(14)内に貯えた液化ガ
スαeの蒸発潜熱により吸収できる。また、冷媒ガス(
Iφが連通管(161を通して自由に出入りできるよう
にして液溜−内を一定の圧力に保持するとき、超電導界
磁コイル(1)は熱負荷変動があっても常に一定の温度
に冷却保持でき、所期の性能を発揮させることができる
。このよって液溜(+4)内の液化ガス(+61の蒸発
−液化により熱のバッファ機能が得られる。Similar to the conventional one, the heat of the superconducting field coil fi1 is released from the heat dissipation fins of the protrusion (9) via the heat transfer member (8) as a low-temperature liquefied gas that is a refrigerant. Here, when using the liquefied gas aφ in the liquid reservoir H at a liquefaction point that is the same as or slightly below the cooling temperature of the protrusion (9), the cooling capacity is lower than the thermal load of the superconducting field coil Tl+. If there is enough room, the vaporized liquefied gas (16) is liquefied by excess cooling, and a certain amount is stored in the liquid reservoir (14).On the other hand, due to thermal disturbance, the superconducting field coil fl+ is temporarily turned off. When the heat load of the part to be cooled exceeds the cooling capacity of the heat transfer member (8), it can be absorbed by the latent heat of vaporization of the liquefied gas αe stored in the liquid reservoir (14).
When the inside of the liquid reservoir is maintained at a constant pressure by allowing Iφ to freely enter and exit through the communication pipe (161), the superconducting field coil (1) can be cooled and maintained at a constant temperature even when the heat load fluctuates. , it is possible to exhibit the desired performance.Therefore, a heat buffer function is obtained by the evaporation-liquefaction of the liquefied gas (+61) in the liquid reservoir (+4).
なお、上記実施例では液溜Q4)を超電導界磁コイルi
l+を固定するコイル取付軸(2)の内側に設けたが、
超電導界磁コイル11+の外側に設けても同様の効果を
奏する。In the above embodiment, the liquid reservoir Q4) is connected to the superconducting field coil i.
It was installed inside the coil mounting shaft (2) that fixes l+, but
A similar effect can be obtained even if it is provided outside the superconducting field coil 11+.
また、超電導界磁コイルfilを液溜04)内に設置す
る構造としても、もちろん良く、この場合液化ガス(1
61の液浸冷却が行なえ、冷却特性のさらに向上化が図
れる。Of course, a structure in which the superconducting field coil fil is installed in the liquid reservoir 04) may also be used; in this case, the liquefied gas (1
61 liquid immersion cooling can be performed, and the cooling characteristics can be further improved.
以上のようにこの発明によれば、円筒、この円筒の両端
部にそれぞれ設けられ上記円筒内に真空部を形成する端
部軸、この端部軸に断熱的に支持されて上記真空部に配
置される超電導界磁コイル、および一方は上記超電導界
磁コイルに熱的に接触し、他方は上記真空部から上記端
部軸を貫通して真空部外に突出する伝熱部材、上記超電
導界磁コイルに熱的に接触して設けられ液化ガスを貯蔵
する液溜、この液溜と外部とを連通し、液溜の圧力を一
定に保持する連通管を備え、上記伝熱部材の突出部を冷
却することにより、上記超電導界磁コイルを冷却すると
共に、上記超電導界磁コイルの熱負荷変動を上記液化ガ
スの蒸発潜熱により吸収するようにしたので、冷却安定
性に優れ、信頼性の高い超電導回転機の回転子が得られ
る効果がある0As described above, according to the present invention, there is a cylinder, an end shaft provided at each end of the cylinder and forming a vacuum section within the cylinder, and adiabatically supported by the end shaft and disposed in the vacuum section. a superconducting field coil, one of which is in thermal contact with the superconducting field coil, and the other of which is a heat transfer member that extends from the vacuum section through the end shaft and projects out of the vacuum section, and the superconducting field coil. A liquid reservoir provided in thermal contact with the coil to store liquefied gas, a communication pipe communicating this liquid reservoir with the outside and keeping the pressure of the liquid reservoir constant, and a protrusion of the heat transfer member. By cooling, the superconducting field coil is cooled, and fluctuations in the thermal load of the superconducting field coil are absorbed by the latent heat of vaporization of the liquefied gas, resulting in a highly reliable superconductor with excellent cooling stability. 0 which has the effect of obtaining the rotor of a rotating machine
第1図はこの発明の一実施例による超電導回転機の回転
子を示す断面図、第2図は先行の超電導回転機の回転子
を示す断面図である。
図において、(l)は超電導界磁コイル、(2)はコイ
ル取付軸、f3) 、 I+)は端部軸、(7)は円筒
、(8)は伝熱部材、(9)は伝熱部材の突出部、■は
液溜、0ωは連通管、(+6)は液化ガスである。
な3、各図中、同一符号は同一または相当部分を示すも
のとする。FIG. 1 is a sectional view showing a rotor of a superconducting rotating machine according to an embodiment of the present invention, and FIG. 2 is a sectional view showing a rotor of a previous superconducting rotating machine. In the figure, (l) is the superconducting field coil, (2) is the coil mounting shaft, f3), I+) is the end shaft, (7) is the cylinder, (8) is the heat transfer member, and (9) is the heat transfer member. The protruding parts of the members, ■ are the liquid reservoir, 0ω is the communication pipe, and (+6) is the liquefied gas. 3. In each figure, the same reference numerals indicate the same or corresponding parts.
Claims (2)
円筒内に真空部を形成する端部軸、この端部軸に断熱的
に支持されて上記真空部に配置される超電導界磁コイル
、および一方は上記超電導界磁コイルに熱的に接触し、
他方は上記真空部から上記端部軸を貫通して真空部外に
突出する伝熱部材、上記超電導界磁コイルに熱的に接触
して設けられ液化ガスを貯蔵する液溜、この液溜と外部
とを連通し、液溜の圧力を一定に保持する連通管を備え
、上記伝熱部材の突出部を冷却することにより上記超電
導界磁コイルを冷却すると共に、上記超電導界磁コイル
の熱負荷変動を上記液化ガスの蒸発潜熱により吸収する
ようにした超電導回転機の回転子。(1) a cylinder, an end shaft provided at each end of the cylinder to form a vacuum section within the cylinder, a superconducting field coil adiabatically supported by the end shaft and disposed in the vacuum section; and one side is in thermal contact with the superconducting field coil,
The other includes a heat transfer member extending from the vacuum section through the end shaft and protruding out of the vacuum section, a liquid reservoir provided in thermal contact with the superconducting field coil and storing liquefied gas, and the liquid reservoir. It is provided with a communication pipe that communicates with the outside and maintains the pressure of the liquid reservoir constant, and cools the superconducting field coil by cooling the protrusion of the heat transfer member, and also reduces the thermal load of the superconducting field coil. A rotor for a superconducting rotating machine in which fluctuations are absorbed by the latent heat of vaporization of the liquefied gas.
の突出部の冷却温度と同じか、またはわずかに高い特許
請求の範囲第1項記載の超電導回転機の回転子。(2) A rotor for a superconducting rotating machine according to claim 1, wherein the liquefaction point of the liquefied gas stored in the liquid reservoir is the same as or slightly higher than the cooling temperature of the protrusion of the heat transfer member.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14021187A JPS63305747A (en) | 1987-06-04 | 1987-06-04 | Rotor for superconducting rotary machine |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14021187A JPS63305747A (en) | 1987-06-04 | 1987-06-04 | Rotor for superconducting rotary machine |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63305747A true JPS63305747A (en) | 1988-12-13 |
Family
ID=15263503
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14021187A Pending JPS63305747A (en) | 1987-06-04 | 1987-06-04 | Rotor for superconducting rotary machine |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63305747A (en) |
-
1987
- 1987-06-04 JP JP14021187A patent/JPS63305747A/en active Pending
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