JPH0315809B2 - - Google Patents

Info

Publication number
JPH0315809B2
JPH0315809B2 JP60079278A JP7927885A JPH0315809B2 JP H0315809 B2 JPH0315809 B2 JP H0315809B2 JP 60079278 A JP60079278 A JP 60079278A JP 7927885 A JP7927885 A JP 7927885A JP H0315809 B2 JPH0315809 B2 JP H0315809B2
Authority
JP
Japan
Prior art keywords
excitation
yoke
pair
outer cylinder
magnetic field
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.)
Expired - Lifetime
Application number
JP60079278A
Other languages
Japanese (ja)
Other versions
JPS61239605A (en
Inventor
Yukio Moryama
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Steel Magnetics KK
Original Assignee
Mitsubishi Steel Magnetics KK
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Steel Magnetics KK filed Critical Mitsubishi Steel Magnetics KK
Priority to JP60079278A priority Critical patent/JPS61239605A/en
Publication of JPS61239605A publication Critical patent/JPS61239605A/en
Publication of JPH0315809B2 publication Critical patent/JPH0315809B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/20Electromagnets; Actuators including electromagnets without armatures

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、円筒状形態を有する直径方位励磁用
磁場装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a magnetic field device for diametrical excitation having a cylindrical form.

従来の技術 従来、例えば、シリコンウエハー用のシリコン
単結晶引き上げ装置の回転円形炉を内蔵する真空
チヤンバーの外周部に設置される磁場装置として
は、その規定された空間領域を直流励磁するため
に、添付図面の第5図に示すように、1対の励磁
コイル31と、その周辺に、それぞれ、配置され
た1対の鉄心32と、これらの鉄心32を相互に
連結する継鉄33とから形成され、これにより、
励磁コイル31が誘起する磁束を、その継鉄33
によつて鉄心32に誘導し、規定された空間Rを
磁極片321,322によつて挟み励磁する対極電
磁石装置30と、第6図に示すように、ソレノイ
ドコイル41によつてコイル41自身の内部空間
Rを励磁する、いわゆる、空心コイル形電磁石装
置40とによつて代表される。
BACKGROUND TECHNOLOGY Conventionally, for example, a magnetic field device installed on the outer periphery of a vacuum chamber containing a rotary circular furnace of a silicon single crystal pulling device for silicon wafers has been used to excite a defined spatial region with direct current. As shown in FIG. 5 of the accompanying drawings, it is formed from a pair of excitation coils 31, a pair of iron cores 32 arranged around the excitation coils, and a yoke 33 that interconnects these iron cores 32. and this results in
The magnetic flux induced by the excitation coil 31 is transferred to its yoke 33.
As shown in FIG . It is typified by a so-called air-core coil type electromagnet device 40 that excites its own internal space R.

発明が解決しようとする問題点 しかしながら、このような従来の代表的な空間
を直流励磁する方法ないしは装置には、それぞ
れ、次に記載するような欠点がある。すなわち、
前者の対極電磁石装置30においては、励磁空間
Rに比べ、周辺に配置される励磁コイル31及び
継鉄部32が大きくなり、装置の設置空間面積及
び装置重量も大きくなるという欠点があり、一
方、後者の空心コイル型電磁石装置40において
は、励磁方位がコイル41の巻き軸方位に限定さ
れと共に磁束を誘導集約する継鉄を対極面に使用
することができないので、(若しも、これを設置
したものとすると、励磁空間Rを密閉する構造と
なり、そのために、その利用価値が限定されると
となる)消費電力が大きくなるという欠点があつ
た。
Problems to be Solved by the Invention However, these typical conventional methods and devices for DC exciting a space each have drawbacks as described below. That is,
The former counter electrode electromagnet device 30 has the disadvantage that the excitation coil 31 and yoke portion 32 arranged around it are larger than the excitation space R, and the installation space area and weight of the device are also large. In the latter air-core coil type electromagnet device 40, the excitation direction is limited to the winding axis direction of the coil 41, and a yoke that induces and concentrates magnetic flux cannot be used on the opposite pole (if this is installed). In this case, the excitation space R would be sealed, which would limit its utility value and increase power consumption.

本発明は、従来の方法ないしは装置における上
記のような欠点を解消すると共に従来のものにお
ける特徴及び利点を合わせ持つている改良された
新規な円筒状形態を有し、その内径円柱状空間を
円柱の直径方位に励磁する機能を有する磁場装置
を得ることを、その目的とするものである。
The present invention has a new and improved cylindrical form that eliminates the above-mentioned drawbacks of the conventional method or apparatus and also has the features and advantages of the conventional method, and the inner diameter of the cylindrical space is made into a cylindrical shape. The object of the present invention is to obtain a magnetic field device having a function of excitation in the diameter direction of .

問題点を解決するための手段 本発明による磁場装置は、この目的を達成する
ために、添付図面の第3図に示すように、対向構
造型式を有する直流励磁式磁場発生装置におい
て、1対の半円筒形の外筒継鉄1,2と、各外筒
継鉄1,2の内径空間内にそれぞれ組み付けられ
るようにされた1対の磁極片5,6と、各外筒継
鉄1,2の内径空間内に、それぞれ、収容される
と共にその内径面上に組み付けられた磁極片5,
6を内部にはめ込むように形成された1対の励磁
コイル7,8とから成り立つている1対の電磁石
半体を、それらの直径面において相互に接合して
成る円筒状形態を有する直径方位励磁用磁場装置
を特徴とするものである。
Means for Solving the Problems In order to achieve this object, the magnetic field device according to the present invention, as shown in FIG. A semi-cylindrical outer yoke 1, 2, a pair of magnetic pole pieces 5, 6 each assembled into the inner diameter space of each outer yoke 1, 2, and each outer yoke 1, Magnetic pole pieces 5, which are housed in the inner diameter spaces of 2 and assembled on the inner diameter surfaces thereof, respectively.
A diametrically azimuthal excitation device having a cylindrical shape formed by joining a pair of electromagnet halves, each consisting of a pair of excitation coils 7 and 8 formed to fit a magnet 6 inside, to each other at their diametrical surfaces. It is characterized by a magnetic field device for use.

作 用 本発明装置は、上記のような構成を有している
ので、各電磁石半体の外筒継鉄1,2は、それら
の直径面において相互に対向されて固着されて一
体となり、これらの外筒継鉄1,2の中心部に
は、軸方向に延びる円柱状の空間部Rが形成さ
れ、この空間部Rの内部に設置されている励磁コ
イル7,8は、ちようど1個のコイルのように密
着し、従つて、これらの励磁コイル7,8に通電
する時は、磁極片5,6及び外筒継鉄1,2が協
同して外筒継鉄1,2の中心軸と直角方向に磁束
を発生するようになる。
Effect Since the device of the present invention has the above-described configuration, the outer cylindrical yokes 1 and 2 of each electromagnet half are fixed to each other with their diametrical surfaces facing each other, and are integrated. A cylindrical space R extending in the axial direction is formed in the center of the outer cylindrical yokes 1 and 2, and the excitation coils 7 and 8 installed inside this space R are Therefore, when the excitation coils 7 and 8 are energized, the magnetic pole pieces 5 and 6 and the outer cylinder yokes 1 and 2 work together to control the outer cylinder yokes 1 and 2. Magnetic flux is generated in a direction perpendicular to the central axis.

実施例 以下、本発明を、その実施例を示す添付図面の
第1及び2図並びにその応用例を示す第4図に基
づいて詳細に説明する。
Embodiments Hereinafter, the present invention will be explained in detail based on FIGS. 1 and 2 of the accompanying drawings showing an embodiment thereof, and FIG. 4 showing an example of its application.

本発明装置は、まず、第1図に示すように、1
対の中空半円筒状の形状を有する外筒継鉄1,2
と、各外筒継鉄1,2の上下端部に、それぞれ、
固着されるようになつている半円環状の形状を有
する上下継鉄3,4と、それぞれ、外筒継鉄1,
2の内面に組み付けられるようになされている、
横断面形状が円弧状で、ある厚さ及びある高さを
有している1対の磁極片5,6と、それぞれ、外
筒継鉄1,2の内径空間の内部に収容されると共
にこれらの内径面の上に組み付けられた磁極片
5,6にはめ込まれるような特殊な形状を有して
いる1対の励磁コイル7,8とから構成されてい
る。
First, as shown in FIG.
A pair of outer cylindrical yokes 1 and 2 having a hollow semi-cylindrical shape
And, on the upper and lower ends of each outer cylinder yoke 1 and 2, respectively,
Upper and lower yokes 3 and 4 having a semicircular shape that are fixed to each other, and outer cylinder yokes 1 and 4, respectively, are fixed to each other.
It is designed to be assembled on the inner surface of 2.
A pair of magnetic pole pieces 5 and 6 each having an arcuate cross-sectional shape, a certain thickness, and a certain height are housed inside the inner diameter spaces of the outer cylinder yokes 1 and 2, respectively. It is composed of a pair of excitation coils 7 and 8 that have a special shape so that they can be fitted into magnetic pole pieces 5 and 6 assembled on the inner diameter surface of the magnet.

ここで、各励磁コイル7,8の形状を更に詳細
に説明すると次のようになる。すなわち、第1図
に示すように、各励磁コイル7,8は、各外筒継
鉄1,2の直径面内にその端部において軸方向に
配置されるようになつている、ほぼ外筒継鉄1,
2の高さに相当する長さを有している1対の直線
状部71,81と、それらの各端部を、それぞれ接
続する、ほぼ外筒継鉄1,2の内径に相当する外
径を有している1対の半円環状部72,82とから
成り立つており、これらの直線状部71,81と、
半円環状部72,82とによつて包囲される空間部
内に磁極片5,6が、それぞれ、はめられるよう
になつている。なお、各励磁コイル7,8は、そ
れに接続されたノード線9を介して通電されるよ
うになつており、各ノード線9は、各外筒継鉄
1,2の底部にあけられた開口11,21から外部
へ引き出されるようになつている。
Here, the shape of each excitation coil 7, 8 will be explained in more detail as follows. That is, as shown in FIG. 1, each excitation coil 7, 8 is a substantially outer cylinder whose end portion is arranged axially within the diametric plane of each outer cylinder yoke 1, 2. Yoke 1,
A pair of linear portions 7 1 and 8 1 having a length corresponding to the height of 2 and each end thereof is connected to each other, and approximately corresponds to the inner diameter of the outer cylinder yokes 1 and 2. It consists of a pair of semicircular annular parts 7 2 and 8 2 having an outer diameter of
The magnetic pole pieces 5 and 6 are fitted into the spaces surrounded by the semicircular annular parts 7 2 and 8 2 , respectively. Each of the excitation coils 7 and 8 is energized via a node wire 9 connected thereto, and each node wire 9 is connected to an opening formed at the bottom of each outer cylinder yoke 1 and 2. 1 1 and 2 1 to the outside.

このように、それぞれ、内径面の上に磁極片
5,6を組み付けられると共に内径空間内に励磁
コイル7,8を収容されている外筒継鉄1,2か
ら成り立つている各電磁石半体101,102は、
第2図に示すように、各外筒継鉄1,2の直径面
において相互に接合され、それらの外部におい
て、適宜な締結具11を介して相互に強固に連結
すると、内部に円柱状の空間部Rを有する円筒形
状を呈するようになり、それぞれの内部に取り付
けられた励磁コイル7,8は、あだかも、1個の
コイルのように密着し、各励磁コイル7,8に通
電(電流の方向が、矢印Cによつて示されてい
る)する時は、そのコイル7,8の軸心は、円筒
状の励磁空間Rの直径方向と一致する方向に磁束
を発生するようになる。
In this way, each electromagnet half body 10 is made up of an outer cylindrical yoke 1, 2, each of which has a magnetic pole piece 5, 6 assembled on its inner diameter surface and an excitation coil 7, 8 accommodated in its inner diameter space. 1,10 2 is
As shown in FIG. 2, when the outer cylinder yokes 1 and 2 are joined to each other in their diametrical planes and are firmly connected to each other via appropriate fasteners 11 on the outside, a cylindrical yoke is formed inside. It now has a cylindrical shape with a space R, and the excitation coils 7 and 8 installed inside each are closely attached as if they were one coil, and each excitation coil 7 and 8 is energized ( When the direction of the current is indicated by arrow C), the axes of the coils 7 and 8 generate magnetic flux in a direction that coincides with the diameter direction of the cylindrical excitation space R. .

このような構成を有する本発明装置は、例え
ば、シリコンウエハー用単結晶製造過程において
使用される磁場装置として、回転円形炉を内蔵す
る単結晶引き上げ装置の真空チヤンバー(非磁性
金属)の外周部から、内部炉心を直流励磁する
(MCZ法*)ための装置として、小形で且つ軽量
のものを提供するものであり、更に、本発明装置
の周辺に漏れる磁束を最小限に押さえることがで
き、従つて、隣接する設備への影響を軽減させる
ことができるものである(注:*Magnetic
Field Applied Czochralski法)。
The device of the present invention having such a configuration is used, for example, as a magnetic field device used in the process of manufacturing single crystals for silicon wafers. The present invention provides a small and lightweight device for direct current excitation of the internal core (MCZ method*).Furthermore, it is possible to minimize the magnetic flux leaking around the device of the present invention, and to It is possible to reduce the impact on adjacent equipment (Note: *Magnetic
Field Applied Czochralski method).

また、本発明装置自体は、2個の電磁石半体1
1,102に分割することができるので、第4図
に示すように、単結晶引き上げ装置20を貫通さ
せる必要無しに、極めて容易に本発明装置を装着
させることが可能となる。
In addition, the device of the present invention itself consists of two electromagnet halves 1
Since it can be divided into 0 1 and 10 2 , as shown in FIG. 4, the device of the present invention can be installed very easily without the need to penetrate the single crystal pulling device 20.

発明の効果 本発明は、上記のような構成及び作用を有して
いるので、次のような優れた効果を発揮すること
のできるものであることは、明らかなところであ
る。
Effects of the Invention Since the present invention has the above-described configuration and operation, it is clear that the present invention can exhibit the following excellent effects.

すなわち 1 本発明装置における励磁コイルは、2個の励
磁コイルを、空心コイル磁場装置と同様に、ち
ようど1個のコイルのように密着させ、励磁空
間を同軸心に配置させることができること 2 励磁コイルの軸方位に対して90°方位を変え
た円柱形状の励磁空間を有すること 3 外筒継鉄及び励磁コイルの形状は、円柱形状
の励磁空間に無駄無く配置され、総体的に小形
且つ軽量化を図ることが可能であること 4 外筒継鉄は、その内面に、それぞれ、内部磁
極片を持ち、励磁コイルの誘起する磁束を有効
に収束することができる共に外部への磁束の漏
れを防止することができること 5 外筒継鉄も励磁コイルも、直径方向に2分さ
れているので、組み立て及び分解が極めて容易
であること などである。
That is, 1. In the excitation coil in the device of the present invention, two excitation coils can be brought into close contact with each other as if they were just one coil, similar to the air-core coil magnetic field device, and the excitation space can be arranged coaxially. It has a cylindrical excitation space whose orientation is changed by 90 degrees with respect to the axial direction of the excitation coil.3 The shape of the outer cylinder yoke and the excitation coil are arranged without waste in the cylindrical excitation space, and are overall small and compact. 4. The outer cylinder yoke has internal magnetic pole pieces on its inner surface, and can effectively converge the magnetic flux induced by the excitation coil, while also preventing leakage of magnetic flux to the outside. 5. Since both the outer cylinder yoke and the excitation coil are divided into two in the diameter direction, assembly and disassembly are extremely easy.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明の1実施例を示す分解斜視
図、第2図は、これを組み立てた状態において示
した斜視図、第3図は、本発明装置の原理を示す
縦断面図、第4図は、第1及び2図に示す本発明
装置を単結晶引き上げ装置に配置した例を示す一
部縦断正面図、第5及び6図は、それぞれ、従来
の空間領域を直流励磁するための電磁石装置の2
例を示す縦断面図である。 1,2……外筒継鉄、3,4……端部継鉄、
5,6……磁極片、7,8……励磁コイル、71
1……直線状部、72,82……円環状部、10
……電磁石装置、101,102……電磁石半体。
FIG. 1 is an exploded perspective view showing one embodiment of the present invention, FIG. 2 is a perspective view showing the assembled state, FIG. 3 is a vertical sectional view showing the principle of the device of the present invention, and FIG. Fig. 4 is a partially longitudinal front view showing an example in which the apparatus of the present invention shown in Figs. 1 and 2 is arranged in a single crystal pulling apparatus, and Figs. Electromagnetic device 2
It is a longitudinal cross-sectional view showing an example. 1, 2... Outer cylinder yoke, 3, 4... End yoke,
5, 6... Magnetic pole piece, 7, 8... Excitation coil, 7 1 ,
8 1 ... linear part, 7 2 , 8 2 ... circular part, 10
...Electromagnet device, 10 1 , 10 2 ...half electromagnet.

Claims (1)

【特許請求の範囲】 1 2極対向構造型式を有する円筒状形態を有す
る直径方位励磁用磁場装置において、1対の半円
筒形の外筒継鉄と、各外筒継鉄の内径面上にそれ
ぞれ組み付けられるようになされた1対の磁極片
と、各外筒継鉄の内径面空間内に、それぞれ、収
容されると共に磁極片をその内部にはめ込むよう
に形成された1対の励磁コイルとから成り立つて
おり、各外筒継鉄がそれらの内部に内蔵されてい
る磁極片及び励磁コイルと共に電磁石半体を形成
し、これらの電磁石半体が相互に直径面において
接合されて一体となるようになつていることを特
徴とする円筒状形態を有する直径方位励磁用磁場
装置。 2 各外筒継鉄の上下端部に、半円環状の継鉄が
固着された特許請求の範囲第1項記載の円筒状形
態を有する直径方位励磁用磁場装置。 3 各励磁コイルが、外筒継鉄の直径面内にその
各端部において軸方向に延びる、外筒継鉄の高さ
にほぼ相当する長さを有する直線状部と、この直
線状部の各端部を相互に連結し且つ外筒継鉄の内
径にほぼ相当する外径を有する半円環状の1対の
半円環状部とから成り立つている特許請求の範囲
第1又は2項記載の円筒状形態を有する直径方位
励磁用磁場装置。
[Scope of Claims] 1. In a magnetic field device for diametrical excitation having a cylindrical form with a two-pole opposing structure, a pair of semi-cylindrical outer yoke and an inner diameter surface of each outer yoke are provided. a pair of magnetic pole pieces that are adapted to be assembled respectively; a pair of excitation coils that are respectively accommodated in the inner diameter surface space of each outer cylinder yoke and formed so as to fit the magnetic pole pieces therein; Each outer cylinder yoke forms an electromagnet half together with the magnetic pole piece and excitation coil built inside them, and these electromagnet halves are joined to each other diametrically so that they become a single body. A magnetic field device for diametrical excitation having a cylindrical shape. 2. A magnetic field device for diametrical excitation having a cylindrical form according to claim 1, wherein semicircular yokes are fixed to the upper and lower ends of each outer cylinder yoke. 3. Each excitation coil has a straight portion extending in the axial direction at each end within the diameter plane of the outer sleeve yoke and having a length approximately corresponding to the height of the outer sleeve yoke, and a straight portion of this straight portion. Claim 1 or 2 comprises a pair of semicircular annular portions having respective ends connected to each other and having an outer diameter approximately corresponding to the inner diameter of the outer cylinder yoke. A magnetic field device for diametrical excitation having a cylindrical form.
JP60079278A 1985-04-16 1985-04-16 Cylindrical magnetic field device for excitation of diametral orientation Granted JPS61239605A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60079278A JPS61239605A (en) 1985-04-16 1985-04-16 Cylindrical magnetic field device for excitation of diametral orientation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60079278A JPS61239605A (en) 1985-04-16 1985-04-16 Cylindrical magnetic field device for excitation of diametral orientation

Publications (2)

Publication Number Publication Date
JPS61239605A JPS61239605A (en) 1986-10-24
JPH0315809B2 true JPH0315809B2 (en) 1991-03-04

Family

ID=13685398

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60079278A Granted JPS61239605A (en) 1985-04-16 1985-04-16 Cylindrical magnetic field device for excitation of diametral orientation

Country Status (1)

Country Link
JP (1) JPS61239605A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3824412B2 (en) * 1998-02-17 2006-09-20 株式会社東芝 Superconducting magnet device for crystal pulling device
CN105696085A (en) * 2014-11-24 2016-06-22 银川隆基硅材料有限公司 Magnetic field device, and monocrystalline growth equipment provided with magnetic field device

Also Published As

Publication number Publication date
JPS61239605A (en) 1986-10-24

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