JPS59144338A - Winding method of superconductive magnet - Google Patents
Winding method of superconductive magnetInfo
- Publication number
- JPS59144338A JPS59144338A JP58015209A JP1520983A JPS59144338A JP S59144338 A JPS59144338 A JP S59144338A JP 58015209 A JP58015209 A JP 58015209A JP 1520983 A JP1520983 A JP 1520983A JP S59144338 A JPS59144338 A JP S59144338A
- Authority
- JP
- Japan
- Prior art keywords
- winding
- strain
- tension
- final
- cylinder
- 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
- 238000004804 winding Methods 0.000 title claims abstract description 59
- 238000000034 method Methods 0.000 title claims description 8
- 238000004519 manufacturing process Methods 0.000 abstract description 2
- 230000005284 excitation Effects 0.000 description 3
- 238000010791 quenching Methods 0.000 description 3
- 230000000171 quenching effect Effects 0.000 description 2
- 235000002492 Rungia klossii Nutrition 0.000 description 1
- 244000117054 Rungia klossii Species 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 210000003746 feather Anatomy 0.000 description 1
- 238000007373 indentation Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/04—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing coils
- H01F41/06—Coil winding
- H01F41/094—Tensioning or braking devices
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Manufacture Of Motors, Generators (AREA)
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の技術分１寸〕
本発明は、超電導マグネットに１糸９、特に超電導マグ
ネットを構成する巻枠の簡１ｌｌｓの歪ケ測定しながら
筒部に１裸材を巻く、超電導マグネットの巻線方法に関
する。DETAILED DESCRIPTION OF THE INVENTION [Technical portion of the invention] The present invention involves the measurement of a single thread 9 in a superconducting magnet, particularly a simple 1lls strain on the winding frame constituting the superconducting magnet, while a bare material is placed on the cylindrical portion. The present invention relates to a method of winding a superconducting magnet.
超電導マグネットは、これに励磁すると電磁力（ｌこよ
って、第１図に示すように、線材１に（はフープ力２と
圧縮力３が同時に１乍用するものである。When a superconducting magnet is excited, an electromagnetic force (1) is applied to the wire 1 (1) at the same time as a hoop force 2 and a compressive force 3, as shown in FIG.
これらの力２．３は線材１を動かそうとする力となり、
その動きがマグネットのクエンチ（常電導転移伝搬）の
主な原因となる。このため、このような励磁中の線材の
動きを押えるために会場の際？ｆＭｉに適宜張力を、か
けて行なうのか一般的である。These forces 2.3 become forces that try to move the wire 1,
This movement is the main cause of magnet quench (normal conduction transition propagation). For this reason, is it necessary to suppress the movement of the wire during excitation at the venue? It is common practice to apply appropriate tension to fMi.
超電導マクイ・ットの設計においては、これを収納する
クライオスタット（低畠溶器）でその外径が決シ、被試
験体の大きさでその有効ボア径が決り、さらに発生磁鴇
で巻線部体潰が決定さ几る。In the design of the superconducting maqui-t, the outside diameter is determined by the cryostat that houses it, the effective bore diameter is determined by the size of the test object, and the winding is determined by the generated magnetic tow. It was decided that the body would be crushed.
このような種々の条件：・ζより巻枠面部（第１図４９
の厚みをてきるたけ薄くしなければならない場合かめり
、そうすると巻線における前記線材の張力（クエンチ防
止）によって巻枠筒ｆｉｌ（に圧卵力かかかり歪か生じ
ることとなる。したがって、−ｒ＝当りの面部歪量は層
数か増えるに従って減少していくが、巻、國層認か多い
マグネットでは、その積算された全霊は相当大きくなり
、巻枠の塑性変形をもたらす場合もあり、ひいてはクエ
ンチの原因ともなりかねない。故に、このような場合に
、巷枠筒部の厚みに応じた巻線張力の管理が必要とされ
る。Such various conditions: - From ζ to the winding frame surface (Fig. 1 49
If it is necessary to reduce the thickness of the wire as much as possible, the tension of the wire in the winding (to prevent quenching) will apply an indentation force to the winding frame cylinder fil, causing distortion. = The amount of surface strain per hit decreases as the number of layers increases, but in magnets with a large number of windings and layers, the accumulated strain becomes quite large, which may lead to plastic deformation of the winding frame, and even This may cause quenching.Therefore, in such a case, it is necessary to manage the winding tension according to the thickness of the width frame cylinder.
本発明は上記従来に鑑みなされたもので、＃ｉ羽が巻か
れる巻枠筒部の歪を測定しながら＠騰し、巻進むに従っ
て筒部巻上υ最終歪を推定し、その最終歪推定値が所定
目標値になるように段階的に巻線張力を調節することに
より安定した励磁が１１」能な超電導マグネットを製作
することができる超電導マグネットの巻線方法を提供せ
んとするものである。The present invention has been made in view of the above-mentioned conventional art, and it rises while measuring the strain of the winding frame cylinder part on which the #i feather is wound, and estimates the final strain of winding υ of the cylinder part as the winding progresses, and estimates the final strain. It is an object of the present invention to provide a method for winding a superconducting magnet that can manufacture a superconducting magnet capable of stable excitation by adjusting the winding tension in stages so that the tension reaches a predetermined target value. .
本発明は、超電導マグネットを構成する巻枠の筒部に線
材を巻くにβたり、巻枠′筒部の歪τ１ｉｌｉｊｌ ｊ
定し、巻枠筒部の線材の最終巻上りにおける歪が予め設
定された巻枠筒部の全回像源になるように、巻かれる線
材の張力を所定段階ごとに変化させるよう（７した超電
導マグネットの巻線方法である。In the present invention, when a wire is wound around the cylindrical portion of the winding frame constituting a superconducting magnet, the distortion τ1ilijl j of the winding frame cylindrical portion
The tension of the wire to be wound is changed in each predetermined step so that the strain at the final winding of the wire in the winding frame tube becomes a preset image source for all the turns of the winding frame tube. This is a method of winding a superconducting magnet.
以下、本発明の好ましい実施例を図面により説明する。 Preferred embodiments of the present invention will be described below with reference to the drawings.
本発明の超電導マグネットの巻線方法を使用した巻線装
置を第２図に示すＣ第２図において、本装置は巻線装置
巻取軸１ｕに巻枠１１と歪計１２が固定されてお９、巻
枠１１の一部に設けられた孔１３全通して歪ケージ１４
が巻枠１１の筒部１５の内側に固着さルている。セして
、筒部１５に巻かれる：ａ拐１６の張力を歪計１２の値
に応じて開山１する張力Ｈｉ！Ｉ御部１７を１捕えてい
るものである。A winding device using the superconducting magnet winding method of the present invention is shown in FIG. 2. In FIG. 9. A strain cage 14 is inserted through the entire hole 13 provided in a part of the winding frame 11.
is fixed to the inside of the cylindrical portion 15 of the winding frame 11. The tension in the cylindrical part 15 is set and the tension in the cylindrical part 16 is changed to 1 according to the value of the strain meter 12. It captures the I control section 17.
以上のような構成による巻線装置において、巻取軸１０
の（ロ）転数が１１０−２Ｏｒｐ程度で筒部１５に線ノ
：：；Ｍ １ ｂが巻かれる。歪６土１２は＠取軸１υ
と共に回転し、筒部’＋ ５の歪の読み嘔りか一層巻巌
するごとに回転を止めて行なわれる。この歪計１２の値
により張力制御部１７が＠線の張力を所定段階で変化さ
せ、最終歪目標値になるように開側１している。歪は一
１没的に張力と層数の関数、即ち歪二［（張力、層数）
と表４りされることにより、前。In the winding device configured as described above, the winding shaft 10
The wire No.::;M 1 b is wound around the cylindrical portion 15 at a rotation number of about 110-2 Orp. Distortion 6 earth 12 @take axis 1υ
The rotation is stopped each time the distortion of the cylindrical part '+5 is increased or the winding is further increased. Based on the value of the strain gauge 12, the tension control unit 17 changes the tension of the @ line in predetermined steps, and the open side 1 is set so that the final strain target value is reached. The strain is a function of the tension and the number of layers, that is, the strain is [(tension, number of layers)
By being listed as Table 4.
もつ−Ｃ関ｅｉｆの概略の形會試験谷綴で求めておき、
この形から最終巻−ヒ９歪が推定される。このことから
、巻線装置による巻線を、その−例として歪ど張力の関
係で第３図に示す。第３図において、巻初めは概略計算
により張力を設定して３〜５層巻巌する（曲＠’Ａ）ｃ
この段１溜で「関数［により最終巻上９歪全推定し、始
めの張力では全回標血葡越えることが判断されると（曲
！ ” ）第に！＊目より張力を少し小さくシ、さらに
３〜５層巷房して前記推定を繰り返えす（１緋Ｂ）ｃ−
ｅして、最終段階で巻線層数と歪が缶口標値に達しない
場合には補強巻線（例えはＳＵＳ線）で歪ケ目ａ、値Ｉ
Ｃ近づけている（１緋Ｃ）ｃ
このように、超電・斗マクネット巻線内の緋４オに作用
する電磁力は、内側巻線の力が外１４．ｌｆより太きく
、また勝利の臨界電流に対する裕度も円１イ１１巻勝の
方か少ないため、第３図に示すような過程で内側巻線部
（（最大の押力を生じさせることによって臨界電流近傍
まで女足に励磁でさる超電導マクイツトを製作すること
ができる。Find the outline of the Motsu-C EIF in the exam Tani Tsuzuri,
From this shape, the final volume-hi9 distortion can be estimated. From this, the winding by the winding device is shown in FIG. 3 as an example of the relationship between strain and tension. In Figure 3, at the beginning of the roll, set the tension based on rough calculations and wind 3 to 5 layers (song @'A) c
In this step 1, ``The final winding 9 strains are estimated by the function, and it is determined that the initial tension exceeds the total strain (song!''). *Repeat the above estimation by making the tension a little smaller than the original and making 3 to 5 more layers (1 Hi B) c-
If the number of winding layers and strain do not reach the standard values at the final stage, use reinforcing windings (for example, SUS wire) to increase strain level a and value I.
C is approaching (1 Hi C) c In this way, the electromagnetic force acting on Hi 4 O in the Superden/Dou McNet winding is such that the force of the inner winding is equal to the force of the outer 14. It is thicker than lf, and the margin for the critical current of the win is less than that of the 11th winding, so in the process shown in Fig. It is possible to produce a superconducting microphone that excites a woman's legs to near the critical current.
なお、本実施例では単純形のソレノイドマグネットを示
したが、これに１収らす歪変化の予（ｄ１］がより困雌
なレーストラック形寺の異形マグネットの巷総にも適用
できるもので必ゐ。Although a simple solenoid magnet is shown in this example, it can also be applied to a wide range of irregularly shaped magnets such as those used in race track shapes, where the prediction of strain change (d1) is more difficult. Must.
以上、上記実施例からも明ら力）なように本発明によれ
は、勝利が巻かれる巻枠面とｂの歪を測定し、その歪値
により筒部巻上り最終歪を推定３ぜて、最終的に所定の
正目標値になるようｙｃ段賭的に巻臆張力姿調節するこ
とにより、巻枠筒部の厚みに応じた巻線張力を管理する
ことかでき１、より安定した励磁か可能な超電導マダイ
・ット全製作することができる。As is clear from the above embodiments, according to the present invention, the strain of the winding frame surface and b on which the win is wound is measured, and the final strain of the cylinder part is estimated from the strain value. By adjusting the winding tension in a stepwise manner so as to finally reach a predetermined positive target value, the winding tension can be managed according to the thickness of the winding frame tube 1, resulting in more stable excitation. All possible superconducting materials can be manufactured.
第１図は超電導マクイツトを励磁した場合の電磁力を示
した概略断面図、第２図（・ま本発明の超電導マクネッ
トの巻線方法を使用した巻線装置を示した概略断面図、
第３図は第２図における巻線装置による巻、癲張力と巻
線層数との関係°を示したグラフである。
１．１６・・・・・線材
４．１１・・・・・巷枠
１２ ・・・・・・歪計
１４・・・・・・・・歪ゲージ
１７・・・・・・張力制御部
代理人 弁理士 守 谷 −串Fig. 1 is a schematic sectional view showing the electromagnetic force when a superconducting macnet is excited, and Fig. 2 is a schematic sectional view showing a winding device using the superconducting macnet winding method of the present invention.
FIG. 3 is a graph showing the relationship between winding, winding tension, and number of winding layers using the winding device shown in FIG. 1.16...Wire rod 4.11...Span frame 12...Strain gauge 14...Strain gauge 17...Tension control section substitute Person Patent Attorney Moritani - Kushi
Claims (1)
あたシ、前記巻枠の筒部の歪を測定し、。 該筒部の前記線材の最終巻上ジにおける歪が予め設定さ
れた禮筒部の全回標値になるように、該巻かれる線材の
張力を所定段階ごとに変化させるようにしたことを特徴
とする超電導マグネットの巻線方法。[Scope of Claims] Before winding a wire around a cylindrical portion of a winding frame constituting a superconducting magnet, the distortion of the cylindrical portion of the winding frame is measured. The tension of the wire rod to be wound is changed at each predetermined step so that the strain at the final winding stage of the wire rod in the tube portion becomes a preset total rotation target value of the tube portion. A method of winding a superconducting magnet.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58015209A JPS59144338A (en) | 1983-01-31 | 1983-01-31 | Winding method of superconductive magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58015209A JPS59144338A (en) | 1983-01-31 | 1983-01-31 | Winding method of superconductive magnet |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS59144338A true JPS59144338A (en) | 1984-08-18 |
Family
ID=11882474
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58015209A Pending JPS59144338A (en) | 1983-01-31 | 1983-01-31 | Winding method of superconductive magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59144338A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2008022591A (en) * | 2006-07-10 | 2008-01-31 | Jtekt Corp | Electric motor |
| CN107993836A (en) * | 2017-12-28 | 2018-05-04 | 安徽荣达阀门有限公司 | A kind of air pressure type wire-winding tension device |
-
1983
- 1983-01-31 JP JP58015209A patent/JPS59144338A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2008022591A (en) * | 2006-07-10 | 2008-01-31 | Jtekt Corp | Electric motor |
| CN107993836A (en) * | 2017-12-28 | 2018-05-04 | 安徽荣达阀门有限公司 | A kind of air pressure type wire-winding tension device |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2015515143A5 (en) | ||
| US4364013A (en) | Magnetic transducer comprising a strained magnetic wire in a sheath of non-magnetic material | |
| JP2008216244A (en) | Coil and its manufacturing method for force measuring device | |
| US6171408B1 (en) | Process for manufacturing tape wound core strips and inductive component with a tape wound core | |
| EP1898228A2 (en) | Antenna coil for nmr with reduced magnetic susceptibility | |
| JPS59144338A (en) | Winding method of superconductive magnet | |
| WO2014094029A1 (en) | Method and device for determining the magnetic characteristics of a lamination stack | |
| Wake et al. | AC loss in energy doubler magnets | |
| US2462423A (en) | Ferromagnetic variable highfrequency inductor | |
| Easson et al. | Surface structure and ac losses in superconductive niobium | |
| JPH0470792B2 (en) | ||
| US10695970B2 (en) | Manufacturing method and apparatus | |
| JP2007311457A (en) | Structure and method for magnetic shield | |
| JPS5852812A (en) | Manufacture of wound iron core for transformer | |
| Van Bockstal et al. | Coils with fibre composite reinforcement for pulsed magnetic fields in the 50-70 T range | |
| Salach et al. | Methodology of testing the magnetoelastic characteristics of ring-shaped cores under uniform compressive and tensile stresses | |
| JPS6197908A (en) | Coil winding method | |
| JP2004063128A (en) | Compound-based superconductive wire showing strain dependency and superconductive magnet using it | |
| JP5367468B2 (en) | Estimation method of critical current during superconducting coil fabrication | |
| Seeber et al. | Variation of the residual resistivity ratio of the aluminium stabiliser for the Compact Muon Solenoid (CMS) conductor under dynamic stress at 4.2 K | |
| SU1039403A1 (en) | Method of manufacturing superconductive solenoid | |
| RU1781649C (en) | Process of manufacture of closed ferrous sonde-type converters | |
| CN116299092A (en) | Device and method for realizing gradient magnetization field of extremely weak magnetic material | |
| SU714523A1 (en) | Method of manufacturing tape magnetic circuit | |
| Devine et al. | The magnetomechanical effect in electrolytic iron |