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JPS61239605A - Cylindrical magnetic field device for excitation of diametral orientation - Google Patents

Cylindrical magnetic field device for excitation of diametral orientation

Info

Publication number
JPS61239605A
JPS61239605A JP60079278A JP7927885A JPS61239605A JP S61239605 A JPS61239605 A JP S61239605A JP 60079278 A JP60079278 A JP 60079278A JP 7927885 A JP7927885 A JP 7927885A JP S61239605 A JPS61239605 A JP S61239605A
Authority
JP
Japan
Prior art keywords
excitation
yoke
magnetic field
yokes
pair
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
Application number
JP60079278A
Other languages
Japanese (ja)
Other versions
JPH0315809B2 (en
Inventor
Yukio Moriyama
森山 幸男
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)

Abstract

PURPOSE:To prevent the leakage of magnetic field to outside as well as to contrive miniaturization and light weight of a magnetic field device by a method wherein an outer yoke and an excitation coil are built-in in a pair of electromagnet semiconductors, and these electromagnet semiconductors are coupled on the surface of diameter. CONSTITUTION:End part yokes 3 and 4 are adhered to the upper and the lower parts of a pair of hollow semicylindrical outer barrel-shaped yokes 1 and 2, magnetic pole pieces 5 and 6 are incorporated on the inner surface of the yokes 1 and 2. Special shaped excitation coils 7 and 8 are fitted in said incorporated magnetic pole pieces 5 and 6, and they are placed in the inner space of the yokes 1 and 2 respectively. The rectilinear parts 7 and 8 with the length corresponding to the height of the yokes 1 and 2 and the circular parts 72 and 82 with the outer diameter corresponding to the inner diameter of the yokes 1 and 2 are formed. Then, a pair of electromagnetic semiconductors 101 and 102 are constituted, and they are coupled to the diameter surface respectively, thereby enabling to prevent the leakage of magnetic flux to outside and to obtain a small-sized and light-weighted magnetic field device.

Description

【発明の詳細な説明】 LIJ二!1ullγ所一 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] LIJ2! The present invention relates to a magnetic field device for diametrical excitation having a cylindrical form.

従11L遣庸− 従来、例えば、シリコンウェ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ャンバーの外
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肘の励磁コイル31と、その周辺に、それぞ
れ、配Hされた1対の鉄心3Z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によっ
て鉄心32に誘導し、規定された空間Rを磁極片32.
.322によって挾み励磁する対極電磁石装置3oと、
第6図に示すように、ソレノイドコイル40こよってフ
ィル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とによって代表される。
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, an excitation coil 31 at one elbow, a pair of iron cores 3Z disposed around the excitation coil 31, and a yoke 33 interconnecting these iron cores 32. is formed from, which results in
The magnetic flux induced by the excitation coil 31 is guided to the iron core 32 by the yoke 33, and the defined space R is spread between the magnetic pole pieces 32.
.. a counter electrode electromagnet device 3o which is sandwiched and excited by 322;
As shown in FIG. 6, it is typified by a so-called air-core coil type electromagnet device 40 that excites the internal space R of the fill 41 itself using a solenoid coil 40.

免1麩蕃−KV1j上工(珊1墓 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、αがある。すなわちS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が人外くなり、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4o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j       L−も・0t′を設置
L−“も″)1す6と・励磁空間8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)
消費電力が大赴くなるという欠点があった。
However, each of these typical conventional methods or devices for DC excitation of a space has the following deficiencies. Namely, the former S In the counter electrode electromagnet device 30, compared to the excitation space R, the excitation coil 31 and the yoke section 32 arranged around the periphery are bulky, and the installation space area and weight of the device are also large. In the latter air-core coil type electromagnet device 4o, the excitation direction is limited to the winding axis direction of the coil 41, and a yoke for guiding and concentrating magnetic flux cannot be used as the counter electrode surface. The structure seals the excitation space 8 and the 1st 6, which limits its utility value.
The drawback is that it consumes a lot of power.

本発明は、従来の方法ないしは装置における一I−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
び利点を合わせ持っ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
る慨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 which overcomes the disadvantages of the conventional methods and apparatuses, as well as having the features and advantages of the conventional ones, and whose inner diameter is cylindrical. The object is to obtain a magnetic field device capable of exciting a space in the direction of the diameter of a cylinder.

αを 、′するための 本発明による磁場HfM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】、2の内      
1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とから成り立っている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。
In order to achieve this objective, the magnetic field HfM according to the invention for α and Cylindrical outer yoke 1, 2, each outer yoke], 2
A pair of magnetic pole pieces 5, 6 each assembled in one diameter space, and inside the inner diameter space of each outer cylinder yoke 1, 2,
1 each formed to receive therein a magnetic pole piece 5.6 housed therein and assembled on its inner diameter surface.
The present invention is characterized by a magnetic field device for diametrical excitation having a cylindrical shape, in which a pair of electromagnetic halves constituted by a pair of excitation coils 7.8 are joined to each other in their diametrical planes.

作□−」[ 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、ちょうど1個のコイルのように
密着し、従って、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。
Since the device of the present invention has the above-described configuration, the outer cylindrical yokes 1 and 2 of each electromagnet half are diametrically opposed to each other and fixed together. A cylindrical space R extending in the axial direction is formed in the center of these outer cylinder yokes 1 and 2, and the excitation coil 7.8 installed inside this space R is exactly The magnetic pole pieces 5, 6 and the outer cylinder yokes 1, 2 work together to energize the excitation coils 7, 8 as if they were one coil. Magnetic flux is generated in a direction perpendicular to the central axis.

火−」1□七− 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。
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、IN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っ
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さ
れている、4f1i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。
As shown in FIG. 1, the device of the present invention first includes an outer cylindrical yoke 1.2 having a hollow semi-cylindrical shape, and the upper and lower ends of each outer cylindrical yoke 1, 2, respectively. The upper and lower yokes 3゜4 have a semicircular shape and are fixed to the inner surfaces of the outer cylinder yokes 1 and 2, respectively, and the 4f1i cross-sectional shapes are arcuate. , a pair of magnetic pole pieces 5.6 having a certain thickness and a certain height, each housed inside the inner diameter space of the outer yoke 1, 2.
It consists of a pair of excitation coils 7.8 which have a special shape so that they can be bent and fitted into the magnetic pole pieces 5 and 6 assembled on the inner diameter surfaces of these coils.

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っている
、はぼ外筒継鉄1.2の高さに相当する長さを有してい
るINの直線状部7□81と、それらの各端部を、それ
ぞれ接続する、はぼ外筒継鉄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7□I8□とから成り
立っており、これらの直線状部7..8.と、半円環状
部7□、82とによっ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っている。なお
、各励磁コイル7.8は、それに接続された1、−ド#
i9を介して通電されるようになっており、各1−ドM
9は、各外筒継鉄1,2の底部にあけられた開ITII
、、2.から外部へ引外出されるようになっている。
Here, the shape of each excitation coil 7.8 will be explained in more detail as follows. That is, as shown in Figure 1,
Each excitation coil 7.8 is arranged axially at its end in the diametrical plane of each yoke 1,2, at the height of the cylindrical yoke 1.2. The straight part 7□81 of the IN having a corresponding length and the outer cylinder yoke 1, 2 which connects each end thereof, respectively, have an outer diameter corresponding to the inner diameter. It consists of a pair of semicircular annular portions 7□I8□, and these straight portions 7. .. 8. The magnetic pole piece 5 is placed in the space surrounded by the semicircular annular portions 7□ and 82.
.. 6 can be fitted into each. In addition, each excitation coil 7.8 is connected to the
It is designed to be energized via i9, and each 1-dore M
9 is an open IT II drilled at the bottom of each outer cylinder yoke 1 and 2.
,,2. It is designed to be taken outside.

このように、それぞれ、内径面の上に磁極片5.6を組
みイ1けられると共に内径空間内に励磁コイル7゜8を
収容されれている外筒継鉄1.2から成り立っている各
電磁石半体10.,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によって示されている)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 tube yoke 1.2 consists of an outer cylindrical yoke 1.2, in which a magnetic pole piece 5.6 is assembled on the inner diameter surface, and an excitation coil 7.8 is accommodated in the inner diameter space. Electromagnet half body 10. , 102 are joined to each other in the diameter plane of each outer cylinder yoke 1 and 2 as shown in FIG. The excitation coils 7.8 installed inside each of the excitation coils 7.8 are closely attached to each other as if they were one coil, and each excitation coil 7.8 has a cylindrical shape with a columnar space R. When the coil 7.8 is energized (the direction of the current is indicated by the arrow C), the axis of the coil 7.8 generates magnetic flux in a direction that coincides with the diameter direction of the cylindrical excitation space R. become.

:     このような構成を有する本発明装置は、例
えば、シリコンウェ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例
外上げ装置の真空チャンバー(非磁性金属)の外周部か
ら、内部炉心を直流励磁する(NCZ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、従って、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(注二本MaI?neti
c Field Applied Czochrals
ki法)。
The device of the present invention having such a configuration can be used, for example, as a magnetic field device used in the single crystal production process for silicon wafers. From the beginning, we provide a small and lightweight device for DC excitation of the internal core (NCZ method *),
Furthermore, the magnetic flux leaking around the device of the present invention can be suppressed to a minimum, thereby reducing the impact on adjacent equipment (Note 2).
c Field Applied Czochrals
ki method).

また、本発明装置自体は、2個の電磁石半体10.。Furthermore, the device of the present invention itself consists of two electromagnetic halves 10. .

102に分割することができるので、第4図に示すよう
に、単結晶例外上げ装置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
Since it can be divided into 102 parts, as shown in FIG.
The device of the present invention can be installed extremely easily.

発遭11算】一 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トるもので
あることは、明らかなところである。
Since the present invention has the above-described structure and operation, it is clear that the present invention is outstanding because it exhibits 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、ちょうど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bること 2.4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軽
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. 2.4 It has a cylindrical excitation space whose orientation is changed by 90" with respect to the axial direction of the magnetic coil. 3. The shape of the outer cylinder yoke and the excitation coil are arranged without waste in the cylindrical excitation space, The overall size and weight can be reduced. 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. It is lightweight by preventing leakage of magnetic flux to the outside, and 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 drawings]

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、   
 II′!J3[11”$i″1i″y/jK′!ei
t[#1flffl、14図は、第1及び2図に示す本
発明装置を単結晶引き上げ装置に設置した例を示す一部
縦断正面図、第5及び6図は、それぞれ、従来の空間領
域を直流励磁するための電磁石装置の2例を示す縦断面
図である。 1.2・・・外筒継鉄、3.4・・・端部継鉄、5,6
・・・磁極片、7゜8・・・励磁コイル、7+ +8+
・・・直線状部、72,8□・・・円環状部、10・・
・電磁石装置、10..102・・・電磁石半体。 特許出願人 三菱製鋼磁材株式会社 第3図 第4図
FIG. 1 is an exploded perspective view showing one embodiment of the present invention, and FIG. 2 is a perspective view showing the assembled state.
II′! J3[11"$i"1i"y/jK'!ei
t[#1flffl, Figure 14 is a partially longitudinal front view showing an example in which the apparatus of the present invention shown in Figures 1 and 2 is installed in a single crystal pulling apparatus, and Figures 5 and 6 are respectively FIG. 2 is a vertical cross-sectional view showing two examples of electromagnetic devices for direct current excitation. 1.2... Outer cylinder yoke, 3.4... End yoke, 5, 6
...Magnetic pole piece, 7°8...Exciting coil, 7+ +8+
...Straight portion, 72,8□...Circular portion, 10...
・Electromagnetic device, 10. .. 102...half electromagnet. Patent applicant Mitsubishi Steel Magnetic Materials Co., Ltd. Figure 3 Figure 4

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
立っており、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
体となるようになっ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っている
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. A magnetic field device for diametrical excitation having a cylindrical form with two poles facing each other, including a pair of semi-cylindrical outer yoke and an inner diameter surface of each outer yoke. a pair of magnetic pole pieces configured to be assembled into the respective outer cylinder yokes, and a pair of excitation coils respectively housed within 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 to become an integral body. A magnetic field device for diametrical excitation having a cylindrical shape, characterized in that: 2. A magnetic field device for diametrical excitation having a cylindrical form as claimed in claim 1, wherein semicircular yokes are fixed to the upper and lower ends of each outer cylinder yoke. 3. Each excitation coil has a linear portion extending in the axial direction at each end within the diameter plane of the outer tube yoke and having a length approximately corresponding to the height of the outer tube yoke, and this linear portion. and a pair of semicircular annular portions each having an outer diameter approximately corresponding to the inner diameter of the outer cylinder yoke, the ends of which are connected to each other, and the outer cylinder yoke has an outer diameter substantially 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 true JPS61239605A (en) 1986-10-24
JPH0315809B2 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)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0936290A1 (en) * 1998-02-17 1999-08-18 Kabushiki Kaisha Toshiba 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

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0936290A1 (en) * 1998-02-17 1999-08-18 Kabushiki Kaisha Toshiba 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
JPH0315809B2 (en) 1991-03-04

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