JPH0682948B2 - Method for manufacturing plate-like body for magnetic shielding - Google Patents

Method for manufacturing plate-like body for magnetic shielding

Info

Publication number
JPH0682948B2
JPH0682948B2 JP63171915A JP17191588A JPH0682948B2 JP H0682948 B2 JPH0682948 B2 JP H0682948B2 JP 63171915 A JP63171915 A JP 63171915A JP 17191588 A JP17191588 A JP 17191588A JP H0682948 B2 JPH0682948 B2 JP H0682948B2
Authority
JP
Japan
Prior art keywords
superconductor
concrete
magnetic shielding
plate
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
JP63171915A
Other languages
Japanese (ja)
Other versions
JPH0222895A (en
Inventor
寛二 酒井
勝彦 菊田
淳 竹内
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.)
Obayashi Corp
Original Assignee
Obayashi Corp
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 Obayashi Corp filed Critical Obayashi Corp
Priority to JP63171915A priority Critical patent/JPH0682948B2/en
Publication of JPH0222895A publication Critical patent/JPH0222895A/en
Publication of JPH0682948B2 publication Critical patent/JPH0682948B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【発明の詳細な説明】 《産業上の利用分野》 本発明は磁気遮蔽用板状体の製造方法に関するもので、
より具体的にはコンクリートにペロブスカイト結晶構造
をもつ例えばイットリウム・バリウム・銅のセラミック
スの超電導体を混入してなる磁気遮閉用板状体の製造方
法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION << Industrial Application Field >> The present invention relates to a method for manufacturing a magnetic shielding plate,
More specifically, the present invention relates to a method for producing a magnetic shielding plate-like body obtained by mixing concrete with a superconductor made of, for example, yttrium-barium-copper ceramic having a perovskite crystal structure.

《従来の技術》 近年のコンピュータ,ロボット等をはじめとする各種電
子機器の普及にともない、電子機器の外乱要因である磁
気を遮蔽する磁気遮蔽室の要求が高まっている。現状で
は磁気遮閉室は室内側面に鉄等の強磁性体あるいは銅等
の強高導電体より形成したシールド板を取付けて構成し
たものであって、これには性能的に限界があり、また磁
気の侵入を防ぐため隙間をなくさなければならず特殊な
加工が要求され、コスト的にも高価なものとなってい
る。そこで本出願人は先に特願昭62-308700号に係る発
明において、室の周囲を区画するコンクリートに超電導
物質を混入または埋設して、超電導物質の完全反磁性を
利用した磁気遮蔽室の構成を提案している。
<< Prior Art >> With the widespread use of various electronic devices such as computers and robots in recent years, there is an increasing demand for a magnetically shielded room that shields the magnetism that is a disturbance factor of the electronic devices. At present, the magnetically shielded room is constructed by attaching a shield plate made of a ferromagnetic material such as iron or a strong conductive material such as copper on the inner side surface of the room, and this has a limit in performance and the magnetic field. In order to prevent the invasion of the holes, it is necessary to eliminate the gap, special processing is required, and the cost is high. Therefore, in the invention of Japanese Patent Application No. 62-308700, the applicant has previously constructed a magnetically shielded room using the complete diamagnetism of the superconducting substance by mixing or burying the superconducting substance in the concrete that partitions the room. Is proposed.

《発明が解決しようとする課題》 しかし、上記のようなコンクリートにおいては超電導物
質はコンクリート全体に分散した状態となっているた
め、高価な超電導物質を使用する割には磁気遮蔽効果が
低いと言った問題点があった。
<< Problems to be Solved by the Invention >> However, in the concrete as described above, since the superconducting substance is in a state of being dispersed throughout the concrete, it is said that the magnetic shielding effect is low in spite of using an expensive superconducting substance. There was a problem.

本発明は上記の問題点に鑑みてなされ、その目的は磁気
遮蔽効果が極めて優れた板状体を容易に製造することの
できる方法を提供するにある。
The present invention has been made in view of the above problems, and an object thereof is to provide a method capable of easily manufacturing a plate-shaped body having an extremely excellent magnetic shielding effect.

《課題を解決するための手段》 上記目的を達成するため、本発明ではコンクリートに粉
粒体の超電導体を混入し、該コンクリートを板状体の型
枠に流し込むとともに該型枠の片面に磁場を印加して該
超電導体を磁場の印加された側とは反対側に高密度に偏
在させてなるのである。
<< Means for Solving the Problem >> In order to achieve the above object, in the present invention, a superconductor of a powder or granular material is mixed into concrete, and the concrete is poured into a form of a plate-like body and a magnetic field is applied to one side of the form. Is applied to disperse the superconductor at a high density on the side opposite to the side to which the magnetic field is applied.

《実施例》 以下に本発明に係る好適実施例について添附図面を参照
にして説明する。
<< Embodiment >> A preferred embodiment of the present invention will be described below with reference to the accompanying drawings.

図中の符号1は壁材であってコンクリートより成る。こ
の壁材1を流動状としてこれに粉粒状の超電導体2を入
れ、よく混合して分散させ、板状体の型枠3に流し込
む。(第1図) ここで用いられる超電導体2は粒径が0.1〜10mmの粒状
または10〜100μm(ミクロン)の粒状であって、900〜
1000℃の範囲の適温度によって焼結したものである。な
お、超電導体2の混入量と粒径は成形される壁の厚さ、
面積等により適宜加減する。
Reference numeral 1 in the figure is a wall material made of concrete. The wall material 1 is made into a fluid state, and the powdery and granular superconductor 2 is put therein, well mixed and dispersed, and poured into the plate-shaped mold 3. (FIG. 1) The superconductor 2 used here has a particle size of 0.1 to 10 mm or a particle size of 10 to 100 μm (micron),
Sintered at an appropriate temperature in the range of 1000 ° C. The mixing amount and particle size of the superconductor 2 are the thickness of the wall to be molded,
It may be adjusted depending on the area.

またイットリウム系では防水コーティングをしておくこ
とが好ましい。
Further, it is preferable that the yttrium-based material be waterproof coated.

そして、型枠3に超電導体2を混入したコンクリートを
流し込んだ後はコンクリートが流動性を有するうちに磁
石4を型枠3の片面にあてて壁材1に磁場を印加する。
すると第2図に示されるように、超電導体2はその完全
反磁性により磁場の印加された面とは反対側に移動し、
第3図に示されるように壁材1の片側に超電導体2が偏
在するようになり、ここに超電導体2の密集化層が形成
される。後に磁石4を撤去し、壁材1を硬化させてから
型枠3を撤去して成形された板状体によって磁気遮蔽室
等を構成する。
Then, after the concrete containing the superconductor 2 is poured into the mold 3, a magnet 4 is applied to one surface of the mold 3 while the concrete has fluidity, and a magnetic field is applied to the wall material 1.
Then, as shown in FIG. 2, the superconductor 2 moves to the side opposite to the surface to which the magnetic field is applied due to its complete diamagnetism,
As shown in FIG. 3, the superconductor 2 is unevenly distributed on one side of the wall material 1, and the dense layer of the superconductor 2 is formed here. After that, the magnet 4 is removed, the wall material 1 is hardened, and then the mold 3 is removed to form a magnetically shielded room or the like by the molded plate-like body.

《効果》 以上のように本発明によれば、コンクリートに粉粒状の
超電導体を混入し、これを板状体の型枠に流し込むとと
もに型枠の片面に磁場を印加して超電導体を磁場の印加
された側の面とは反対側に高密度に偏在させてなるた
め、この方法で成形された板状体では超電導体の密度の
高い層が形成され、磁気遮蔽効果のむらがなくなり、効
率の良い磁気遮蔽力が得られる。
<< Effects >> As described above, according to the present invention, a powdery and granular superconductor is mixed into concrete, and the superconductor is poured into a mold of a plate-like body and a magnetic field is applied to one surface of the mold to make Since it is unevenly distributed in a high density on the side opposite to the surface on which the voltage is applied, a layer with a high density of superconductors is formed in the plate-shaped body formed by this method, and the unevenness of the magnetic shielding effect is eliminated, and the efficiency is improved. Good magnetic shielding power can be obtained.

【図面の簡単な説明】[Brief description of drawings]

第1図は型枠にコンクリートとこれに混入された超電導
体を流し込んだ状態の部分断面図、第2図は型枠に磁場
を印加した状態の部分断面図、第3図は、第2図の状態
より磁場と型枠を撤去した後の状態の部分断面図であ
る。 1……壁材、2……常温超電導体 3……型枠
FIG. 1 is a partial cross-sectional view of concrete and a superconductor mixed therein in a form, FIG. 2 is a partial cross-sectional view of a form in which a magnetic field is applied, and FIG. 3 is FIG. FIG. 6 is a partial cross-sectional view of a state after removing the magnetic field and the mold from the state of FIG. 1 ... Wall material, 2 ... Room temperature superconductor 3 ... Formwork

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】コンクリートに粉粒状の超電導体を混入
し、該コンクリートを板状体の型枠に流し込むとともに
該型枠片面に磁場を印加して該超電導体を磁場の印可さ
れた側とは反対側に高密度に遍在させてなることを特徴
とする磁気遮蔽用板状体の製造方法。
Claim: What is claimed is: 1. A powdery and granular superconductor is mixed into concrete, the concrete is poured into a plate-shaped mold, and a magnetic field is applied to one surface of the mold to define the side on which the magnetic field is applied. A method of manufacturing a magnetic shielding plate-shaped body, characterized in that it is formed on the opposite side with a high density.
JP63171915A 1988-07-12 1988-07-12 Method for manufacturing plate-like body for magnetic shielding Expired - Lifetime JPH0682948B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63171915A JPH0682948B2 (en) 1988-07-12 1988-07-12 Method for manufacturing plate-like body for magnetic shielding

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63171915A JPH0682948B2 (en) 1988-07-12 1988-07-12 Method for manufacturing plate-like body for magnetic shielding

Publications (2)

Publication Number Publication Date
JPH0222895A JPH0222895A (en) 1990-01-25
JPH0682948B2 true JPH0682948B2 (en) 1994-10-19

Family

ID=15932196

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63171915A Expired - Lifetime JPH0682948B2 (en) 1988-07-12 1988-07-12 Method for manufacturing plate-like body for magnetic shielding

Country Status (1)

Country Link
JP (1) JPH0682948B2 (en)

Also Published As

Publication number Publication date
JPH0222895A (en) 1990-01-25

Similar Documents

Publication Publication Date Title
US4942151A (en) Magnetic preferential orientation of metal oxide superconducting materials
JPS5250598A (en) Rare earth-cobalt magnet
JPH0682948B2 (en) Method for manufacturing plate-like body for magnetic shielding
Hidaka et al. Two-Dimensional Weak Localization in Electron High-Tc Superconductor Nd2− xCexCuOy under High Magnetic Field
EP0310332A2 (en) Preferential orientation of metal oxide superconducting materials
Trzebiatowski et al. MAGNETIC PROPERTIES OF URANIUM-SELENIUM ALLOYS
US5795849A (en) Bulk ceramic superconductor structures
JP2585579B2 (en) Superconductor manufacturing method
JPS6452332A (en) Wire formation for superconductive material
JPS63248183A (en) Electromagnetic-wave sheilding material
JPH0832599B2 (en) Cylindrical structure of oxide superconductor
JPH0410498A (en) Magnetic shield plate
JPS63313897A (en) Magnetic shielding body
MAZDIYASNI et al. High-temperature ceramic superconductors(Quarterly Progress Report No. 1, 24 May- 30 Sep.)(1988)
JPH01138798A (en) Magnetic shielding device utilizing oxide superconductor
JPS63258098A (en) Superconducting electromagnetic shield
JPH01262603A (en) Magnet
SUHL et al. A study of surface properties of superconducting materials for high power microwave applications(Final Technical Report, 1 Aug. 1982- 31 Aug.)(1985)
JPH01260895A (en) Laminated magnetic shielding material
KR19990046592A (en) Structure of focusing plate and bypass route for magnetic shielding
Carlson Bullish on Bearings
JPS63318800A (en) Magnetic field shielding material
JPH0484500A (en) Superconductive magnetic shielding seal material
JPH01260896A (en) Laminated magnetic shielding material
Tokarz et al. Inter-and intragrain magnetization of thallium-based superconductors