JPH0194603A - Superconducting coil presser - Google Patents
Superconducting coil presserInfo
- Publication number
- JPH0194603A JPH0194603A JP25064587A JP25064587A JPH0194603A JP H0194603 A JPH0194603 A JP H0194603A JP 25064587 A JP25064587 A JP 25064587A JP 25064587 A JP25064587 A JP 25064587A JP H0194603 A JPH0194603 A JP H0194603A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- comb
- thickness
- superconducting coils
- superconducting coil
- 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.)
- Granted
Links
- 125000006850 spacer group Chemical group 0.000 claims abstract description 17
- 238000010276 construction Methods 0.000 abstract 1
- 230000002093 peripheral effect Effects 0.000 abstract 1
- 238000005452 bending Methods 0.000 description 7
- 244000126211 Hericium coralloides Species 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 238000009434 installation Methods 0.000 description 2
- 238000010008 shearing Methods 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Landscapes
- Superconductive Dynamoelectric Machines (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、超電導コイルを応用した製品のコイル押えの
装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a coil holding device for products to which superconducting coils are applied.
一般に超電導コイルは通電時に強大な電磁力を発生する
ので強力な拘束装置を必要とする。第6図ないし第8図
は従来のくら型の超電導コイルを押え込むための;イル
押えを示すもので、2分割の中空円盤状のコイル押え1
02の一対を結合ピン103で結合し、−株化している
。コイル押え102には内側に一体型スペーサ104が
内方に突設されており、これにより超電導コイル1を押
え込んでいる。また、各コイル押え102は独立してい
るので端部のフランジ106をコイルキー105で継ぐ
ことにより;イル押え102の集合体を一体化させてい
る。Generally, superconducting coils generate a strong electromagnetic force when energized, so they require a strong restraint device. Figures 6 to 8 show conventional hollow-shaped superconducting coil holders for holding down superconducting coils, which are divided into two hollow disc-shaped coil holders 1
A pair of 02 are connected with a connecting pin 103 and made into a stock. An integrated spacer 104 is provided inside the coil presser 102 and projects inwardly, thereby holding the superconducting coil 1 therein. Further, since each coil presser 102 is independent, the assembly of coil pressers 102 is integrated by connecting the flanges 106 at the ends with coil keys 105.
上記従来の超電導コイルの拘束装置には次の問題があっ
た。The conventional superconducting coil restraint device described above has the following problems.
(1)コイル押え102と1体になりた一体型スペーサ
104で超電導コイル1を押え込むと、コイル押え10
2に曲げモーメントが発生し、これに抵抗し得る強度を
得るためコイル押え102の断面寸法が大きくなる。(1) When the superconducting coil 1 is held down by the integrated spacer 104 that is integrated with the coil holder 102, the coil holder 10
A bending moment is generated in the coil holder 102, and the cross-sectional dimension of the coil holder 102 is increased in order to obtain the strength to resist this.
(2)コイル押え102が薄肉の中空円盤の集合体であ
り個々が不連続であるため組立(超電導コイルlを周方
向に逐一圧縮しながら組立てる必要がある)が困難であ
る。(2) Since the coil holder 102 is a collection of thin hollow disks, each of which is discontinuous, assembly is difficult (it is necessary to assemble the superconducting coil 1 while compressing it one by one in the circumferential direction).
(3) コイル押え102が不連続な中空円盤の集合
体であるのでこれらを一体化するためコイルキー105
が必要となるが、コイル通電時に発生する長手方向電磁
力作用に対し、コイルキー105のみで抵抗する事にな
り、コイル押え102の強度が活かされない。(3) Since the coil presser 102 is a collection of discontinuous hollow disks, the coil key 105 is used to integrate them.
However, only the coil key 105 resists the longitudinal electromagnetic force generated when the coil is energized, and the strength of the coil holder 102 is not utilized.
本発明は上記問題点解決の手段として、縦の両端面が櫛
歯状をなすとともに横断面の内周が拘束すべき超電導コ
イルの外周にはソ一致した半円形をなし相互に上記′W
J歯状の端面な係合し合ってはソーつの筒体を形成可能
な一対の補剛円筒シェルと、その外周が上記補剛円筒シ
ェルの内周面に適合可能にかつ内周迄の厚さが上記超電
導コイルの厚さとはy同一に形成された円弧状のスペー
サとを具備してなることを特徴とする超電導コイル押え
装置を提供しようとするものである。As a means for solving the above-mentioned problems, the present invention has provided a superconducting coil whose vertical end surfaces are comb-like, and whose inner periphery in cross section is a semicircle that coincides with the outer periphery of the superconducting coil to be restrained.
A pair of stiffening cylindrical shells that can be engaged with each other with J-toothed end faces to form a saw cylinder; It is an object of the present invention to provide a superconducting coil holding device characterized in that it includes an arc-shaped spacer whose thickness is the same as the thickness of the superconducting coil.
本発明は上記のように構成されるので、従来、コイル押
えの内方に突設されていた一体型スイーサが分離されて
円弧状のスペーサとして独立し、コイル押えに代って内
周が超電導コイルの外周にはソ一致した半円形の補剛円
筒シェルの一対を用いてコイルを拘束するため、補剛円
筒シェルは−様な内圧のみを受けるとと\なりて全(曲
げモーメントを発生せず、7−プテンシ田ンのみで超電
導コイルを拘束できる。従つて安全性が高まると同時に
小型化できる。Since the present invention is configured as described above, the integrated sweeter, which was conventionally provided inwardly protruding from the coil holder, is separated and becomes independent as an arc-shaped spacer, and the inner periphery of the coil holder is superconducting. Since the coil is restrained by using a pair of semicircular stiffening cylindrical shells on the outer circumference of the coil, if the stiffening cylindrical shell receives only an internal pressure of First, the superconducting coil can be restrained with only a 7-tension pin.Therefore, safety can be increased and the size can be reduced at the same time.
また、従来のよ5にコイル押えを多数分離せず、少数分
割シェル構造としたので、長手方向に分割面をずらすこ
とにより、櫛歯のせん断抵抗力により長手方向の力学的
連続性が保たれ、剛度も高くなる。In addition, unlike the conventional method, the coil retainer is not separated into many parts, but instead has a shell structure that is divided into a small number of parts.By shifting the dividing plane in the longitudinal direction, mechanical continuity in the longitudinal direction is maintained by the shearing resistance of the comb teeth. , the stiffness also increases.
本発明の一実施例を第1図ないし第3図により説明する
。An embodiment of the present invention will be described with reference to FIGS. 1 to 3.
これらの図において超電導コイルlの間には超電導コイ
ル1の厚さと略同−のスペーサ4が略対称に一対挿入さ
れており、その外から一対の補剛円筒シェル構造のコイ
ル押え2で超電導コイルlを圧縮しながら押え込み、櫛
歯部5を係合した上で結合ピン3を櫛歯部5に設けられ
たピン穴に通して組立てる。超電導コイル1の初期圧縮
時及びコイル通電時に発生するコイル周方向力に対して
は、スペーサ4及び超電導コイル1の内方で抵抗するの
でコイル押え2は超電導コイル1の半径方向力のみを一
様内圧として負担すれば良い。In these figures, a pair of spacers 4 having approximately the same thickness as the superconducting coil 1 are inserted symmetrically between the superconducting coils l, and a pair of coil holders 2 having a stiffening cylindrical shell structure are used to hold the superconducting coil from the outside. 1 is pressed while being compressed, the comb tooth portion 5 is engaged, and the connecting pin 3 is passed through the pin hole provided in the comb tooth portion 5 to assemble. The spacer 4 and the inside of the superconducting coil 1 resist the coil circumferential force generated during the initial compression of the superconducting coil 1 and when the coil is energized, so the coil holder 2 uniformizes only the radial force of the superconducting coil 1. It is sufficient to bear the burden as internal pressure.
通電時の軸方向力に対しては、櫛歯部5のせん断力で抵
抗する。The axial force during energization is resisted by the shear force of the comb tooth portions 5.
因みに本装置の場合、最も重要な超電導コイル1がコイ
ル押え2に及ぼす内圧の影響について本実施例と従来例
とを第4図及び第5図によって比較すると次の通りであ
る。Incidentally, in the case of this device, the influence of the internal pressure exerted by the superconducting coil 1 on the coil presser 2, which is the most important, is compared between this embodiment and the conventional example using FIGS. 4 and 5 as follows.
先ず、従来例の第5図では超電導コイル1をコイル押え
102によって押え込むと図示しない超電導コイル10
円筒状コアに一体型スペーサ104の内周が当接し、以
後は導線の集合体である超電導コイル1が成る範囲で見
掛上の容積変化及び形状変化を起すので一体型スイーサ
104から対称状に、半円形の範囲迄伸びたコイル押え
102(第7図に示すよ5に結合ピン103で締結する
迄は対称線に対してキャンチレバーとなる)は一体型ス
ペーサ104を固定端、他端を自由端としたキャンチレ
バーが超電導コイルlの内方に向って押し曲げられたと
同等の結果となり、一体型スペーサ104とキャンチレ
バーに相当する細い部分との断面積の急変する近傍に大
きな曲げ応力が発生することになる。具体的にはコイル
押え102の内周側には接線方向にコンブレッジ曹ン、
同じく外周側にはテンシ冒ンが作用し、内周の上記断面
積急変部位には応力集中を伴った大きな圧縮応力が、外
周には引張応力が発生することになる。結合ピン103
で一対のコイル押え102を円筒状に結合後は第5図の
放射状の矢印の向きに超電導フィルlの復元力が働き、
特に通電時は電磁力の加重によってそれが大きな力とな
って作用するがこれによる接線方向のいわゆる7−プテ
ンシ璽ンは一体Wスペーサ104の存在によつてその応
力流れが一様流とならず、やはり断面急変部で応力集中
を生じ局部的に大きな応力を生じる危険を包蔵する。一
般に7−プテンシ冒ンによる引張応力(単純応力)より
もその外殻が法線方向に曲げを受けて生じる外皮引張応
力の方が格段に大きいので、この従来例の場合は先ずコ
イル押え102を取付ける場合の曲げ応力、取付後のフ
ープテンシ嘗ンに対する断面積急変部の集中応力の2つ
の危険機会を構造的に有することになる。First, in FIG. 5 of the conventional example, when the superconducting coil 1 is held down by the coil presser 102, the superconducting coil 10 (not shown)
The inner periphery of the integrated spacer 104 comes into contact with the cylindrical core, and from then on, an apparent change in volume and shape occurs within the range where the superconducting coil 1, which is an assembly of conducting wires, is formed. , the coil retainer 102 (which acts as a cantilever with respect to the line of symmetry until it is fastened with the connecting pin 103 at 5 as shown in FIG. 7) extends to a semicircular area, and the integral spacer 104 is fixed at one end and the other end is free. The result is the same as if the cantilever at the end was pushed and bent inward of the superconducting coil l, and a large bending stress was generated near the sudden change in the cross-sectional area of the integrated spacer 104 and the thin part corresponding to the cantilever. become. Specifically, on the inner circumferential side of the coil presser 102, there is a combination carbon in the tangential direction,
Similarly, tensile strength acts on the outer periphery, and a large compressive stress accompanied by stress concentration is generated on the inner periphery where the cross-sectional area suddenly changes, and a tensile stress is generated on the outer periphery. Connecting pin 103
After joining the pair of coil holders 102 into a cylindrical shape, the restoring force of the superconducting film l acts in the direction of the radial arrow in FIG.
In particular, when electricity is applied, the electromagnetic force acts as a large force due to the addition of electromagnetic force, but due to the presence of the integrated W spacer 104, the stress flow in the tangential direction is not uniform. , there is still a risk of stress concentration occurring at the section where the cross section suddenly changes, resulting in large local stress. In general, the tensile stress of the outer shell caused by bending the outer shell in the normal direction is much larger than the tensile stress (simple stress) caused by bending the coil holder 102 in this conventional example. There are two structural dangers: bending stress during installation and concentrated stress at the part where the cross-sectional area suddenly changes after installation.
これに比し、本実施例の場合は従来例のように一体型ス
ペーサ104がなく、それに相当する部分はスに一部4
と・して独立させたのでコイル押え2は一様断面となり
、超電導コイルlを押え込む際も第4図に示すようにス
ペーサ4の外周とコイル押え2の内周とは自由に滑り合
い、かつ、法線方向の接離は自由なので殆ど曲げ応力を
発生する危険断面が存在しない。又、7−プテンシ冒ン
に対しても断面急変部も断面変化部も共に存在せず一様
断面なので発生応力はこの種閉鎖系応力としては最も安
全な一様単純応力となる。In contrast, in the case of this embodiment, unlike the conventional example, there is no integrated spacer 104, and the corresponding part is partially 4
Since they are made independent, the coil holder 2 has a uniform cross section, and when holding down the superconducting coil 1, the outer periphery of the spacer 4 and the inner periphery of the coil holder 2 freely slide against each other, as shown in FIG. Moreover, since the contact and separation in the normal direction is free, there are almost no dangerous cross sections that generate bending stress. Furthermore, since the cross section is uniform with no abrupt cross-sectional changes and no cross-sectional changes in the case of 7-pressure expansion, the generated stress is uniform simple stress, which is the safest of this type of closed system stress.
以上説明したように本実施例によれば、コイル押えが円
周方向に一様断面となって、従来のように一体型スイー
サを持たないので、強度上、きわめて有利な超電導コイ
ルの拘束装置を得ることができる。又、従来のように中
空円盤状のコイル押えを超電導コイルの円筒軸方向に多
数羅列した構造ではなく、円筒軸方向に充分な長さを有
する補剛円筒シェル構造のコイル押えを連接し、かつ−
対相互の櫛歯部を噛合わせてピン結合するので従来例に
比し、剛度もきわめて高い構造が得られる。As explained above, according to this embodiment, the coil holder has a uniform cross section in the circumferential direction and does not have an integrated sweeter as in the conventional case, so a superconducting coil restraint device which is extremely advantageous in terms of strength can be achieved. Obtainable. In addition, instead of the conventional structure in which a large number of hollow disk-shaped coil holders are arranged in the cylindrical axis direction of the superconducting coil, coil holders with a stiffened cylindrical shell structure having a sufficient length in the cylindrical axial direction are connected, and −
Since the paired comb tooth portions are engaged with each other and connected by pins, a structure with extremely high rigidity can be obtained compared to the conventional example.
なお、上記実施例は第1図に示すようにコイル押え10
2を縦方向に千鳥状に連接した例で説明したが必ずしも
千鳥状に連接する必要はない。In addition, in the above embodiment, the coil presser 10 is used as shown in FIG.
2 are connected in a staggered manner in the vertical direction, but it is not necessarily necessary to connect them in a staggered manner.
本発明は上記のように構成されるので次の効果を有する
。Since the present invention is configured as described above, it has the following effects.
即ち、コイル間にスイーサーを独立配置することにより
、コイル押えへの曲げモーメント作用がなくなり、コイ
ル押えの構造寸法を小さく、軽量化できる。That is, by arranging the sweeter independently between the coils, there is no bending moment acting on the coil holder, and the structural size and weight of the coil holder can be reduced.
コイル押えは分割補則シェル構造化して軽量化するとと
もに分割面は櫛歯構造とし結合ピンへのせん断力を低く
押えることができる。The coil retainer has a split auxiliary shell structure to reduce weight, and the split surface has a comb-teeth structure to suppress shearing force to the coupling pin.
また長手方向への分割面は、上下シェルでずらす事によ
り長手方向荷重作用に対しても櫛歯で抵抗できる。In addition, by shifting the dividing plane in the longitudinal direction between the upper and lower shells, the comb teeth can resist the action of longitudinal loads.
第1図は本発明の一実施例の正面図、第2図はその左側
面図、第3図は本発明の一実施例を一部破断で示した斜
視図、第4図は上記実施例の構成部材に作用する外力の
負荷状況を説明するために実施例の横断面で示した模式
図、第5図は第4図斜視図である。
l・・・超電導コイル、
2・・・コイル押え(補則円筒シェル)、3・・・結合
ピン、 4・・・スペーサ、5・・・櫛歯部
第6図 第7図
第8図Fig. 1 is a front view of an embodiment of the present invention, Fig. 2 is a left side view thereof, Fig. 3 is a partially cutaway perspective view of an embodiment of the invention, and Fig. 4 is the above embodiment. FIG. 5 is a schematic cross-sectional view of the embodiment for explaining the load condition of external force acting on the structural members, and FIG. 5 is a perspective view of FIG. 4. l...Superconducting coil, 2...Coil holder (supplementary cylindrical shell), 3...Coupling pin, 4...Spacer, 5...Comb teeth part Fig. 6 Fig. 7 Fig. 8
Claims (1)
束すべき超電導コイルの外周にほゞ一致した半円形をな
し相互に上記櫛歯状の端面を係合し合ってほゞ一つの筒
体を形成可能な一対の補剛円筒シェルと、その外周が上
記補剛円筒シェルの内周面に適合可能にかつ内周迄の厚
さが上記超電導コイルの厚さとほゞ同一に形成された円
弧状のスペーサとを具備してなることを特徴とする超電
導コイル押え装置。Both vertical end surfaces are comb-shaped, and the inner periphery of the cross section is semicircular approximately coincident with the outer periphery of the superconducting coil to be restrained. a pair of stiffening cylindrical shells capable of forming two cylindrical bodies, the outer periphery of which can be adapted to the inner circumferential surface of the stiffening cylindrical shell, and the thickness up to the inner periphery being approximately the same as the thickness of the superconducting coil; 1. A superconducting coil holding device comprising: a spacer having an arcuate shape.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62250645A JPH0810655B2 (en) | 1987-10-06 | 1987-10-06 | Superconducting coil retainer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62250645A JPH0810655B2 (en) | 1987-10-06 | 1987-10-06 | Superconducting coil retainer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0194603A true JPH0194603A (en) | 1989-04-13 |
| JPH0810655B2 JPH0810655B2 (en) | 1996-01-31 |
Family
ID=17210940
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62250645A Expired - Fee Related JPH0810655B2 (en) | 1987-10-06 | 1987-10-06 | Superconducting coil retainer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0810655B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5126711A (en) * | 1991-03-28 | 1992-06-30 | Ship & Ocean Foundation | Superconductive coil system |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS456109Y1 (en) * | 1967-06-16 | 1970-03-26 | ||
| JPS473646U (en) * | 1971-02-01 | 1972-09-06 | ||
| JPS61139008A (en) * | 1984-12-11 | 1986-06-26 | Hitachi Ltd | Super-conductive field winding |
-
1987
- 1987-10-06 JP JP62250645A patent/JPH0810655B2/en not_active Expired - Fee Related
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS456109Y1 (en) * | 1967-06-16 | 1970-03-26 | ||
| JPS473646U (en) * | 1971-02-01 | 1972-09-06 | ||
| JPS61139008A (en) * | 1984-12-11 | 1986-06-26 | Hitachi Ltd | Super-conductive field winding |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5126711A (en) * | 1991-03-28 | 1992-06-30 | Ship & Ocean Foundation | Superconductive coil system |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0810655B2 (en) | 1996-01-31 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |