JP2006351598A - Magnetic-shield blind and its linking structure - Google Patents
Magnetic-shield blind and its linking structure Download PDFInfo
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Abstract
Description
本発明は磁気シールド簾体及びその連結構造に関し、とくに空気や光の透過性のある開放型シールド構造に用いる磁気シールド簾体及びその連結方法に関する。 The present invention relates to a magnetic shield housing and a connection structure thereof, and more particularly to a magnetic shield housing used in an open shield structure that is permeable to air and light and a connection method thereof.
最近の半導体関連施設・医療施設等では、EB(Electron Beam、電子ビーム)露光装置、EB描画機、MRI(Magnetic Resonance Imaging、磁気共鳴画像診断)装置、NMR(Nuclear Magnetic Resonance、核磁気共鳴)装置、SQUID(Superconducting Quantum Interference Device、超電導量子干渉素子)利用の生体磁気測定装置等の強磁気利用装置を使用することが増えており、強磁気利用装置を環境磁気ノイズから保護して正常な動作を保証するため及び/又は強磁気利用装置の磁気的影響から周囲の人や機器を保護するため、磁気シールドルームに対する要求が高まっている。従来の磁気シールドルームは、例えば特許文献1が開示するように、透磁率の高い方向性電磁鋼板、無方向性電磁鋼板、パーマロイ、軟磁性鋼板、アモルファス、液体急冷薄帯を結晶化させた微結晶磁性材料等の磁性材料板(以下、磁性板ということがある)によりシールド対象空間の壁面を覆う構造(以下、密閉型シールド構造ということがある)を基本としている。しかし密閉型シールド構造は、磁性板の材料特性から期待されるようなシールド性能がなかなか得られず、しかも空気や光の透過性がないという問題点がある。 In recent semiconductor-related facilities and medical facilities, EB (Electron Beam) exposure equipment, EB lithography, MRI (Magnetic Resonance Imaging) equipment, NMR (Nuclear Magnetic Resonance) equipment The use of strong magnetic devices such as biomagnetic measuring devices using SQUID (Superconducting Quantum Interference Device) has been increasing, and the strong magnetic devices are protected from environmental magnetic noises and operate normally. In order to guarantee and / or protect the surrounding people and equipment from the magnetic effects of strong magnetic devices, there is an increasing demand for magnetic shield rooms. As disclosed in, for example, Patent Document 1, a conventional magnetic shield room is a microscopic material obtained by crystallizing a directional electrical steel sheet, non-oriented electrical steel sheet, permalloy, soft magnetic steel sheet, amorphous, liquid quenching ribbon with high magnetic permeability. The structure is based on a structure (hereinafter also referred to as a hermetically sealed structure) in which a wall surface of a space to be shielded is covered with a magnetic material plate such as a crystalline magnetic material (hereinafter also referred to as a magnetic plate). However, the hermetic shield structure has a problem in that the shielding performance as expected from the material characteristics of the magnetic plate cannot be obtained easily and there is no air or light permeability.
これに対し本発明者等は、簾状に並べた磁性板の群(以下、磁気シールド簾体という)を用いて隙間のある磁気シールド構造(以下、開放型シールド構造ということがある)を開発し、特許文献2及び特許文献3に開示した。特許文献2の開放型シールド構造を、図10を参照して本発明の理解に必要な限度において説明する。図10(A)は、例えば厚さ0.35mm、幅25mm、長さ300mmの8枚の短冊状磁性板5を、その長さ方向中心軸Cが同一簾面F上にほぼ平行に並ぶように板厚方向に間隔d=30mmで重ねて形成した磁気シールド簾体6の一例を示す。例えば、各磁性板5の長さ方向と直角方向における間隔dの断面積Saに対する磁性板5の断面積Smと磁性板5の比透磁率μsとの積(Sm・μs)の割合(Sm・μs/Sa)を、その間隔d中の磁束密度が磁性板5中の磁束密度に比し十分小さくなるように、例えば(Sm・μs)/Sa>1となるように選択する。 On the other hand, the present inventors have developed a magnetic shield structure with a gap (hereinafter sometimes referred to as an open type shield structure) using a group of magnetic plates arranged in a bowl shape (hereinafter referred to as a magnetic shield case). And disclosed in Patent Document 2 and Patent Document 3. The open type shield structure of Patent Document 2 will be described with reference to FIG. 10 to the extent necessary for understanding the present invention. FIG. 10A shows an example of eight strip-shaped magnetic plates 5 having a thickness of 0.35 mm, a width of 25 mm, and a length of 300 mm, for example, such that their longitudinal central axes C are arranged substantially in parallel on the same saddle surface F. An example of the magnetic shield housing 6 formed by being overlapped with a distance d = 30 mm in the thickness direction is shown. For example, the ratio (Sm · μs) of the product (Sm · μs) of the cross sectional area Sm of the magnetic plate 5 and the relative permeability μs of the magnetic plate 5 to the cross sectional area Sa of the interval d in the direction perpendicular to the length direction of each magnetic plate 5 For example, (Sm · μs) / Sa> 1 is selected so that the magnetic flux density in the interval d is sufficiently smaller than the magnetic flux density in the magnetic plate 5.
図10(A)のような板厚方向間隔dを有する複数の磁気シールド簾体6を、各簾体6の磁性板5の端縁を接合することにより、図10(B)のような磁気的に連続した磁気シールド簾体6の列(以下、列状簾体ということがある)8を形成することができる。同図は、4つの簾体6a、6b、6c、6dをそれぞれ対応する磁性板5の端縁の重ね合わせにより縦列状に接合し、更にその一端側における磁性板5の未接合端縁を他端側の対応する磁性板5の未接合端縁と重ね合わせて接合することにより、磁気的に閉じた環状の列状簾体8(内容積280mm×280mm×280mm)を形成した例である。図中の符号9は磁性板5の端縁の重ね合わせ部を示す。 A plurality of magnetic shield housings 6 having a plate thickness direction interval d as shown in FIG. 10A are joined to the edge of the magnetic plate 5 of each housing 6 so that the magnetic properties as shown in FIG. Thus, a continuous row 8 of magnetic shield housings 6 (hereinafter sometimes referred to as a row housing) 8 can be formed. In the figure, four casings 6a, 6b, 6c, and 6d are joined in a column by overlapping the edges of the corresponding magnetic plates 5, and the unjoined edges of the magnetic plate 5 on one end side are also connected. This is an example in which a magnetically closed annular columnar housing 8 (internal volume 280 mm × 280 mm × 280 mm) is formed by overlapping and joining with the unjoined edge of the corresponding magnetic plate 5 on the end side. Reference numeral 9 in the drawing indicates an overlapping portion of the edge of the magnetic plate 5.
図10(B)の列状簾体8を、図12(A)に示す環状コイル(例えばヘルムホルツ・コイル)Lの中央部に設置し、コイルLの中央部に10〜100μTの一方向磁場Mを形成して列状簾体8の内側の磁気センサ34(例えばガウスメータ)で磁束密度Bを測定し、列状簾体8のシールド係数S(=シールドがない場合の磁束密度B0/シールドがある場合の磁束密度B)を算出した。また比較のため、厚さ0.35mmで幅及び長さが280mm×280mmの4枚の方形磁性板32a、32b、32c、32dにより図10(C)のような立方体形の密閉型磁気シールド体31を作製し、同様に環状コイルLの中央部に設置して密閉型シールド体31のシールド係数Sを算出した。同図(C)の密閉型シールド体31に用いた磁性材料の重量は、同図(B)の列状簾体8で用いた磁性材料の重量とほぼ同じである。 10B is installed at the center of the annular coil (for example, Helmholtz coil) L shown in FIG. 12A, and the unidirectional magnetic field M of 10 to 100 μT is provided at the center of the coil L. And the magnetic flux density B is measured by a magnetic sensor 34 (for example, a gauss meter) inside the columnar housing 8, and the shield coefficient S of the columnar housing 8 (= the magnetic flux density B 0 when there is no shield / the shield is The magnetic flux density B) in some cases was calculated. For comparison, a cubic sealed magnetic shield 31 as shown in FIG. 10C is obtained by four rectangular magnetic plates 32a, 32b, 32c and 32d having a thickness of 0.35 mm and a width and length of 280 mm × 280 mm. Was similarly installed in the center of the annular coil L, and the shield coefficient S of the hermetic shield 31 was calculated. The weight of the magnetic material used for the sealed shield body 31 in FIG. 10C is substantially the same as the weight of the magnetic material used in the row housing 8 in FIG.
表1は、10μT、50μT、100μTの一方向磁場Mに対する列状簾体8及び密閉型シールド体31のシールド係数Sを示す。表1は、10〜100μTの一方向磁場Mに対する列状簾体8のシールド係数Sが、密閉型シールド体31に比し2〜3倍程度高いことを示している。すなわち、図10(B)の列状簾体8は磁束漏洩が少なく、密閉型シールド構造より高いシールド性能と通気性・透光性とを同時に備えた開放型シールド構造といえる。また、所要のシールド性能を得るために必要な磁性材料を密閉型シールドに比して節減し、高度な磁気シールド構造を経済的・効率的に構築できる利点もある。 Table 1 shows the shield coefficient S of the columnar housing 8 and the sealed shield body 31 with respect to the unidirectional magnetic field M of 10 μT, 50 μT, and 100 μT. Table 1 shows that the shield coefficient S of the columnar housing 8 with respect to the unidirectional magnetic field M of 10 to 100 μT is about 2 to 3 times higher than that of the sealed shield body 31. That is, it can be said that the row-like housing 8 in FIG. 10B has an open shield structure that has less magnetic flux leakage and has higher shielding performance and air permeability and translucency than the sealed shield structure. In addition, there is an advantage that an advanced magnetic shield structure can be constructed economically and efficiently by reducing the magnetic material necessary for obtaining the required shield performance as compared with the hermetic shield.
図10(B)の列状簾体8を実際の磁気シールドルームに適用する場合は、図11(A)に示すように、例えば厚さ0.35mmの磁性薄板7の複数枚を重畳した磁性板5を用いる。図示例の磁性板5は、磁性薄板7の重畳により断面積Smを拡大すると共に、各磁性薄板7の端縁を不揃いとして長手方向端面に凹凸を形成したものである。高いシールド性能の列状簾体8を形成するためには磁性板5の接合部からの磁束漏洩を小さく抑えることが重要であるが、図11(B)のように磁性板5を凹凸端面の嵌合によって接合することで、磁性板5の接合部からの磁束漏洩を極めて小さく抑えることができる。また凹凸端面付き磁性板5は、図示例のような直角向きだけでなく、シールドルームのシールド対象面の形状に応じて直線状又は任意の角度で接合することができる。 When the row-shaped housing 8 of FIG. 10 (B) is applied to an actual magnetic shield room, as shown in FIG. 11 (A), for example, a magnetic plate in which a plurality of magnetic thin plates 7 having a thickness of 0.35 mm are superimposed. 5 is used. The magnetic plate 5 in the illustrated example has a cross-sectional area Sm enlarged by superimposition of the magnetic thin plates 7 and irregularities are formed on the end surfaces in the longitudinal direction with the edges of the magnetic thin plates 7 being uneven. In order to form the row-shaped housing 8 having high shielding performance, it is important to suppress the leakage of magnetic flux from the joint portion of the magnetic plate 5 to a small level. However, as shown in FIG. By joining by fitting, the magnetic flux leakage from the joining part of the magnetic plate 5 can be suppressed extremely small. Further, the magnetic plate 5 with concave and convex end faces can be joined not only in a right angle direction as shown in the illustrated example but also in a straight line shape or an arbitrary angle according to the shape of the shield target surface of the shield room.
しかし図10(B)の列状簾体8は、シールド対象空間を囲む磁気的に閉じた磁気回路を形成することでシールド性能を高めているが、列状簾体8に開閉部を設けると閉じた磁気回路を形成できない問題点がある。磁気シールドルームにはドアや窓等の開閉部を設けることが多く、開閉部の周囲には開閉のための空隙Wを設ける必要がある。空隙Wによって磁気回路に不連続部が発生すると、その不連続部から磁束が漏洩してシールド性能が低下する。開放型シールド構造を実際の磁気シールドルームに適用するには、開閉部周囲の空隙Wからの磁束漏洩を小さく抑える対策が必要である。 However, the columnar housing 8 in FIG. 10B improves the shielding performance by forming a magnetically closed magnetic circuit surrounding the shield target space. However, if the columnar housing 8 is provided with an opening / closing part. There is a problem that a closed magnetic circuit cannot be formed. The magnetic shield room is often provided with an opening / closing part such as a door or a window, and a gap W for opening / closing needs to be provided around the opening / closing part. When a discontinuous part is generated in the magnetic circuit due to the air gap W, magnetic flux leaks from the discontinuous part and the shielding performance is deteriorated. In order to apply the open type shield structure to an actual magnetic shield room, it is necessary to take measures to reduce the leakage of magnetic flux from the gap W around the opening / closing part.
図13は、列状簾体8を用いて本発明者らが開発した磁気シールドルーム41の一例を示す(特願2004-332380号参照)。図示例の磁気シールドルーム41は、四方の磁気シールド壁42a、42b、42c、42dに磁気シールド簾体6を配置し、各簾体6を四隅の柱材44で接合すると共に、特定のシールド壁42aに開口部を設けている。開口部の周縁に一対の縦枠体45aと横枠体45bとからなる門型枠体45を設け、枠体45の内側に磁気シールドドア43を設置する。磁気シールドドア43は、隣接するシールド壁42aの磁性板5の群に対応する簾状配置の固定シールド板46a及び可動シールド板46bの群と、各可動シールド板46bを移動させる可動機構48とを有する。門型枠体45と磁気シールドドア43との間に開閉のための空隙W1、W2を設け、門型枠体45の縦枠体45aに可動シールド板46bを挿通するための貫通孔(図示せず)を形成する。可動機構48により、ドア閉鎖時に各可動シールド板46bを貫通孔に挿通して隣接するシールド壁42aの各磁性板5と接合させ、ドア開放時に可動シールド板46bを隣接するシールド壁42aの各磁性板5から離す。 FIG. 13 shows an example of a magnetic shield room 41 developed by the present inventors using the row of enclosures 8 (see Japanese Patent Application No. 2004-332380). In the illustrated magnetic shield room 41, magnetic shield housings 6 are arranged on four sides of the magnetic shield walls 42a, 42b, 42c, 42d, and each housing 6 is joined by column members 44 at four corners, and specific shield walls are provided. An opening is provided in 42a. A portal frame 45 comprising a pair of vertical frame 45a and horizontal frame 45b is provided at the periphery of the opening, and the magnetic shield door 43 is installed inside the frame 45. The magnetic shield door 43 includes a group of fixed shield plates 46a and movable shield plates 46b arranged in a bowl shape corresponding to the group of magnetic plates 5 on the adjacent shield wall 42a, and a movable mechanism 48 that moves each movable shield plate 46b. Have. Openings W1 and W2 for opening and closing are provided between the portal frame 45 and the magnetic shield door 43, and through holes (not shown) for inserting the movable shield plate 46b into the vertical frame 45a of the portal frame 45 are shown. Z). When the door is closed, each movable shield plate 46b is inserted into the through hole and joined to each magnetic plate 5 of the adjacent shield wall 42a by the movable mechanism 48, and when the door is opened, the movable shield plate 46b is connected to each magnet of the adjacent shield wall 42a. Separate from plate 5.
図13の磁気シールドドア43は、ドア閉鎖時に可動シールド板46bを隣接する磁気シールド壁42aの磁性板5と接合させ、磁気シールドドア43と磁気シールド壁42a、42b、42c、42dとの間に閉じた磁気回路を形成するので、ドア周囲の空隙W1、W2からの磁束漏洩を小さく抑えることができる。ただし、図示例の磁気シールドドア43は複雑な可動機構48を用いて可動シールド板46bを移動させるため、製造コストが嵩むと共に重量が非常に大きくなり、透光性も低下する問題点がある。透光性の高い磁気シールド構造を経済的に構築できるという開放型シールド構造の利点を生かすため、可動機構を用いずに磁気シールド壁42aと磁気シールドドア43とを磁気的に結合する技術の開発が望まれている。 The magnetic shield door 43 in FIG. 13 joins the movable shield plate 46b to the magnetic plate 5 of the adjacent magnetic shield wall 42a when the door is closed, and between the magnetic shield door 43 and the magnetic shield walls 42a, 42b, 42c, 42d. Since a closed magnetic circuit is formed, magnetic flux leakage from the air gaps W1 and W2 around the door can be suppressed to a small level. However, since the magnetic shield door 43 in the illustrated example moves the movable shield plate 46b by using a complicated movable mechanism 48, there are problems that the manufacturing cost increases, the weight becomes very large, and the translucency decreases. Development of technology to magnetically connect the magnetic shield wall 42a and the magnetic shield door 43 without using a movable mechanism in order to take advantage of the open type shield structure that can economically construct a highly transparent magnetic shield structure Is desired.
そこで本発明の目的は、空隙を介して磁気的に結合可能な磁気シールド簾体及びその連結構造を提供することにある。 SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic shield housing that can be magnetically coupled through a gap and a connection structure thereof.
本発明者は、磁気シールド簾体6の各磁性体5の長さ方向縁端の面積に着目した。上述したように簾体6は磁性板5の板厚に比して板厚方向間隔dが大きいため、図13のように空隙Wを介して複数の簾体6を磁性体5の長さ方向に縦列配置した場合に、対向する各簾体6の端縁における磁性板5の断面積が間隔dの断面積に比して小さくなる。本発明者は、簾体6の端縁における磁性板5の断面積を間隔dの断面積に比して大きくすれば、対向する簾体6の間の空隙Wからの磁束漏洩を小さく抑え、空隙Wを介して簾体6を磁気的に結合できることを実験的に見出した(後述する実験例1を参照)。本発明は、この知見に基づき完成に至ったものである。 The inventor paid attention to the area of the edge in the longitudinal direction of each magnetic body 5 of the magnetic shield housing 6. As described above, since the casing 6 has a larger plate thickness direction interval d than the thickness of the magnetic plate 5, the plurality of casings 6 are arranged in the length direction of the magnetic body 5 through the gaps W as shown in FIG. 13. Are arranged in tandem, the cross-sectional area of the magnetic plate 5 at the edge of each opposing housing 6 is smaller than the cross-sectional area of the interval d. The inventor suppresses magnetic flux leakage from the gap W between the opposing housings 6 by making the cross-sectional area of the magnetic plate 5 at the edge of the housing 6 larger than the cross-sectional area of the interval d, It was experimentally found that the housing 6 can be magnetically coupled through the gap W (see Experimental Example 1 described later). The present invention has been completed based on this finding.
図1の実施例を参照するに、本発明による磁気シールド簾体10は、長さ方向と交差する矩形断面の短辺を板厚とする磁性板5の群を各磁性板5の長さ方向中心軸Cが同一簾面F上に平行に並ぶように所定板厚方向間隔dで簾状に積層し、各磁性板5の長さ方向一端縁又は両端縁にその端縁面12の面積を板厚方向に拡張する磁性拡張板11を取り付けてなるものである。 Referring to the embodiment of FIG. 1, a magnetic shield housing 10 according to the present invention includes a group of magnetic plates 5 having a short side of a rectangular cross section that intersects the length direction as a plate thickness. Stacked in a bowl shape with a predetermined thickness direction interval d so that the central axes C are arranged in parallel on the same bowl surface F, the area of the edge face 12 is set at one edge or both edges in the length direction of each magnetic plate 5. A magnetic expansion plate 11 extending in the thickness direction is attached.
また図1の実施例を参照するに、本発明による磁性シールド簾体の連結構造は、長さ方向と交差する矩形断面の短辺を板厚とする磁性板5の群を各磁性板5の長さ方向中心軸Cが同一簾面F上に平行に並ぶように所定板厚方向間隔dで積層した複数の磁気シールド簾体10a、10b、10cを各簾体10a、10b、10cの磁性板5の長さ方向に所定空隙Wを介して縦列配置し、空隙Wに臨む各簾体10a、10b、10cの磁性板5の長さ方向端縁にその端縁面12の面積を板厚方向に拡張する磁性拡張板11を取り付け、空隙W付き縦列配置の簾体10a、10b、10cを磁性拡張板11の対向により磁気的に結合してなるものである。 Referring to the embodiment of FIG. 1, the connecting structure of magnetic shield housings according to the present invention is a group of magnetic plates 5 each having a short side of a rectangular cross section that intersects the length direction. A plurality of magnetic shield housings 10a, 10b, 10c, which are stacked at a predetermined thickness direction interval d so that the central axis C in the length direction is arranged in parallel on the same housing surface F, are magnetic plates of the housings 10a, 10b, 10c. 5 are arranged in a row in a longitudinal direction through a predetermined gap W, and the area of the edge surface 12 is defined in the thickness direction at the edge in the length direction of the magnetic plate 5 of each of the housings 10a, 10b, 10c facing the gap W. A magnetic expansion plate 11 is attached to the magnetic expansion plate 11, and the casings 10a, 10b, 10c arranged in a column with a gap W are magnetically coupled to each other by facing the magnetic expansion plate 11.
例えば磁性拡張板11を、図2(B)及び(C)に示すように、磁性板5の長さ方向端縁に一片aが面接触し且つ他片bがその端縁から板厚方向に延びる断面L字形の磁性アングル11aとし、又は同図(D)に示すように、磁性板5の長さ方向端縁に中央脚部aが面接触し且つ頂部両端bがその端縁から板厚方向両側に延びる断面T字形の磁性アングル11bとすることができる。 For example, as shown in FIGS. 2 (B) and 2 (C), the magnetic expansion plate 11 has one piece a in surface contact with the longitudinal edge of the magnetic plate 5 and the other piece b extending from the edge in the plate thickness direction. A magnetic angle 11a having an L-shaped cross section extending or as shown in FIG. 4D, the central leg a is in surface contact with the longitudinal edge of the magnetic plate 5, and the top ends b are plate thicknesses from the edge. A magnetic angle 11b having a T-shaped cross section extending on both sides in the direction can be obtained.
好ましくは、図3(A)に示すように、磁性拡張板11を、隣接する磁性板5の長さ方向端縁に両端片aがそれぞれ面接触し且つ中間部bがその長さ方向端縁間に延在する断面コ字形の磁性アングル11cとする。更に好ましくは、図7(A)に示すように、各磁性拡張板11で拡張された端縁面12に面接触して端縁面12を相互に接続する磁性框16又は磁性枠17を設ける。 Preferably, as shown in FIG. 3 (A), the magnetic extension plate 11 has both end pieces a in surface contact with the longitudinal edge of the adjacent magnetic plate 5 and the intermediate part b is the longitudinal edge. A magnetic angle 11c having a U-shaped cross section extending therebetween is used. More preferably, as shown in FIG. 7 (A), a magnetic rod 16 or a magnetic frame 17 is provided which is in surface contact with the end face 12 extended by each magnetic extension plate 11 and connects the end faces 12 to each other. .
本発明の磁気シールド簾体10は、矩形断面の短辺を板厚とする磁性板5の群を板厚方向に所定間隔dで重ねて簾状に積層し、各磁性板5の長さ方向一端縁又は両端縁にその端縁面12の面積を板厚方向に拡張する磁性拡張板11を取り付けるので、次の顕著な効果を奏する。 The magnetic shield housing 10 of the present invention is formed by laminating a group of magnetic plates 5 having a short side of a rectangular cross section with a thickness in the thickness direction at a predetermined interval d, and laminating the magnetic plates 5 in the length direction. Since the magnetic expansion plate 11 that expands the area of the end surface 12 in the thickness direction is attached to one end edge or both end edges, the following remarkable effects can be obtained.
(イ)磁性板5の長さ方向端縁面12の面積を拡張することにより、簾体10の長さ方向端縁における磁性板5の断面積を間隔dの断面積に比して大きくすることができる。
(ロ)簾体10を磁性板5の長さ方向に空隙Wを介して縦列配置したときに、磁性板5の大きな対向面積を確保し、空隙Wからの磁束漏洩を小さく抑えて簾体10を磁気的に結合することができる。
(ハ)簾体10の間の空隙Wが5mm以下であれば、空隙Wからの磁束漏洩を0.5mT以下に抑えることが可能である。
(ニ)磁性体5の端縁面12のみを板厚方向に拡張するので、端縁以外の部分における板厚間隔dにより簾体10の高い透光性を確保できる。
(ホ)空隙Wを介して縦列配置した簾体10を磁気的に結合できるので、ドアや窓等の開閉部を有する開放型シールド構造を構築する際に利用できる。
(A) By expanding the area of the lengthwise edge surface 12 of the magnetic plate 5, the cross-sectional area of the magnetic plate 5 at the lengthwise edge of the housing 10 is made larger than the cross-sectional area of the interval d. be able to.
(B) When the casings 10 are arranged in tandem through the gap W in the length direction of the magnetic plate 5, a large opposing area of the magnetic plate 5 is secured, and magnetic flux leakage from the gap W is suppressed to be small. Can be magnetically coupled.
(C) If the gap W between the casings 10 is 5 mm or less, the magnetic flux leakage from the gap W can be suppressed to 0.5 mT or less.
(D) Since only the edge surface 12 of the magnetic body 5 is expanded in the plate thickness direction, high translucency of the housing 10 can be ensured by the plate thickness interval d in the portion other than the edge.
(E) Since the casings 10 arranged in tandem via the gap W can be magnetically coupled, it can be used when constructing an open type shield structure having an opening / closing part such as a door or a window.
図1は、本発明の磁気シールド簾体10を用いて構築した磁気シールドルーム1の実施例を示す。図示例の磁気シールドルーム1は、一方の壁2aに本発明の磁気シールド簾体10a、10b、10cを相互に空隙W1、W2を介して縦列配置し、他の三方の壁2b、2c、2dに図10の磁気シールド簾体6を相互に列状に接合して配置し、簾体10a及び10cの空隙W1及びW2と対向しない端縁を壁2b、2dの簾体6と列状に接合したものである。以下、図1を参照して本発明を説明するが、本発明の磁気シールド簾体10はシールドルーム1への適用に限定されず、任意のシールド対象面に適用することができる。また、図7(D)に示すように、本発明の磁気シールド簾体10を従来の密閉型磁気シールドの磁性板32と組み合わせてシールドルーム又はシールド面とすることも可能である。 FIG. 1 shows an embodiment of a magnetic shield room 1 constructed using a magnetic shield housing 10 of the present invention. In the illustrated magnetic shield room 1, magnetic shield housings 10a, 10b, and 10c of the present invention are arranged in tandem on one wall 2a via gaps W1 and W2, and the other three walls 2b, 2c, and 2d are arranged. The magnetic shield housings 6 shown in FIG. 10 are joined together in a row, and the edges of the housings 10a and 10c not facing the gaps W1 and W2 are joined in rows with the housings 6 of the walls 2b and 2d. It is a thing. Hereinafter, the present invention will be described with reference to FIG. 1, but the magnetic shield housing 10 of the present invention is not limited to application to the shield room 1, and can be applied to any shield target surface. As shown in FIG. 7D, the magnetic shield housing 10 of the present invention can be combined with a magnetic plate 32 of a conventional sealed magnetic shield to form a shield room or a shield surface.
図示例の磁気シールド簾体10a、10b、10cは、図10の磁気シールド簾体6と同様に、長さ方向と交差する断面が矩形であってその矩形断面の短辺を板厚し長辺を板幅とした複数枚の短冊状磁性板5を各磁性板5の長さ方向中心軸Cが同一簾面F上に平行に並ぶように板厚方向に所要間隔dで重ね、各磁性板5の空隙W1、W2に臨む長さ方向一端縁又は両端縁に磁性拡張板11を取り付けて端縁面12の面積を板厚方向に拡張したものである。簾体10を構成する各磁性板5は、同じ幅及び長さとすることが望ましい。必要に応じて各磁性板5の中心軸Cを曲線とし、簾面Fを曲面としてもよい。また各磁性板5は中心軸Cが同一簾面F上にあれば足り、中心軸Cの回りの角度位置は磁性板5毎に異なっていてもよい。 The magnetic shield housings 10a, 10b, and 10c in the illustrated example have a rectangular cross section that intersects with the length direction, like the magnetic shield housing 6 in FIG. A plurality of strip-shaped magnetic plates 5 each having a plate width are stacked at a required interval d in the plate thickness direction so that the longitudinal center axes C of the magnetic plates 5 are arranged in parallel on the same saddle surface F. 5, the magnetic expansion plate 11 is attached to one end edge or both end edges in the length direction facing the gaps W1 and W2, and the area of the edge surface 12 is expanded in the plate thickness direction. It is desirable that the magnetic plates 5 constituting the casing 10 have the same width and length. If necessary, the central axis C of each magnetic plate 5 may be a curved line, and the flange surface F may be a curved surface. Each magnetic plate 5 only needs to have the central axis C on the same saddle surface F, and the angular position around the central axis C may be different for each magnetic plate 5.
各簾体10a、10b、10cの磁性板5の板厚方向間隔dは、各簾体10に与えるシールド性能に応じて、間隔dの断面積Saに対する磁性板5の断面積Smと磁性板5の比透磁率μsとの積(Sm・μs)の割合(Sm・μs/Sa)が1より大きくなるように選択する。(Sm・μs/Sa)>1とすることにより、磁性板5中の磁束の通りやすさ(磁性板のパーミアンス)を間隔d中の磁束の通りやすさ(間隔のパーミアンス)より大きくし、間隔dにおける磁束密度を低減して簾体10にシールド性能を与えることができる。また、磁性板5の板厚方向間隔dを磁性板5の幅(矩形断面の長辺)より大きくすることにより、密閉型シールド(図10(C)参照)に比して磁性体5を節減すると共に高い透光性が得られる。高いシールド性能と高い透光性とを同時に得るためには(Sm・μs/Sa)と間隔dとを共に十分大きくすることが望ましい。各簾体10aの磁性板5の板厚方向間隔dは全て同じである必要はなく、磁性板5の位置によって間隔dが相違してもよい。 The thickness d interval of the magnetic plates 5 of the respective housings 10a, 10b, 10c is determined by the cross sectional area Sm of the magnetic plate 5 and the magnetic plate 5 with respect to the cross sectional area Sa of the interval d according to the shielding performance given to the respective housings 10. The ratio (Sm · μs / Sa) of the product (Sm · μs) with the relative permeability μs is selected to be greater than 1. By setting (Sm · μs / Sa)> 1, the easiness of magnetic flux in the magnetic plate 5 (permeance of the magnetic plate) is made larger than the easiness of magnetic flux in the interval d (permeance of the interval), and the interval The magnetic flux density at d can be reduced, and the shield performance can be imparted to the housing 10. Further, by increasing the thickness direction interval d of the magnetic plate 5 to be larger than the width of the magnetic plate 5 (long side of the rectangular cross section), the magnetic body 5 can be saved as compared with the hermetic shield (see FIG. 10C). In addition, high translucency can be obtained. In order to obtain high shielding performance and high translucency at the same time, it is desirable that both (Sm · μs / Sa) and the distance d be sufficiently large. The thicknesses d of the magnetic plates 5 of the respective housings 10a need not be the same in the thickness direction, and the intervals d may be different depending on the positions of the magnetic plates 5.
各簾体10a、10b、10cの磁性板5の端縁に取り付ける磁性拡張板11は、例えば図2(B)及び(C)に示すように、断面L字形の磁性アングル11aとすることができる。同図(B)は、L字形磁性アングル11aの一片aを磁性板5の端縁の表面に載置して面接触させ、他片bをその端縁から板厚方向に延ばして磁性板5の端縁面12の面積を拡張したものである。また同図(C)は、複数枚の磁性薄板7を重畳した凹凸端面付き磁性板5(図11参照)を用い、L字形磁性アングル11aの一片aを磁性板5の凹凸端面に嵌合させて磁性板5と面接触させ、他端bをその端縁から板厚方向に延ばしたものである。L字形磁性アングル11aの幅は、磁性板5の幅(矩形断面の長辺)と一致させることが望ましい。 For example, as shown in FIGS. 2B and 2C, the magnetic expansion plate 11 attached to the edge of the magnetic plate 5 of each housing 10a, 10b, 10c can be a magnetic angle 11a having an L-shaped cross section. . In FIG. 5B, one piece a of the L-shaped magnetic angle 11a is placed on the surface of the edge of the magnetic plate 5 and brought into surface contact, and the other piece b is extended from the edge in the thickness direction of the magnetic plate 5. The area of the edge surface 12 is expanded. FIG. 11C shows a magnetic plate 5 with concave and convex end surfaces (see FIG. 11) in which a plurality of magnetic thin plates 7 are superimposed, and a piece a of L-shaped magnetic angle 11a is fitted to the concave and convex end surfaces of the magnetic plate 5. The other end b is extended from the end edge in the plate thickness direction. The width of the L-shaped magnetic angle 11a is preferably matched with the width of the magnetic plate 5 (long side of the rectangular cross section).
磁性アングル11aの一片aを磁性板5の端縁と面接触させることにより、磁性板5と磁性アングル11aとの接合部からの磁束漏洩を小さく抑えることができる。また、磁性アングル11aを磁性板5の凹凸端面と嵌合させることにより、アングル11aと磁性板5とを2面で面接触させ、接合部からの磁束漏洩を更に小さくすることが期待できる。磁性アングル11の他片bの長さは適当に選択できるが、磁性板5の端縁面12の面積をできるだけ大きくするように、例えば間隔dと実質上同じ長さとすることができる。 By bringing the piece a of the magnetic angle 11a into surface contact with the edge of the magnetic plate 5, the leakage of magnetic flux from the joint between the magnetic plate 5 and the magnetic angle 11a can be kept small. Further, by fitting the magnetic angle 11a with the concave and convex end face of the magnetic plate 5, it can be expected that the angle 11a and the magnetic plate 5 are brought into surface contact with each other to further reduce the leakage of magnetic flux from the joint. The length of the other piece b of the magnetic angle 11 can be appropriately selected. However, for example, the length can be substantially the same as the distance d so that the area of the end face 12 of the magnetic plate 5 is as large as possible.
また磁性拡張板11を、図2(D)に示すように断面T字形の磁性アングル11bとし、その中央脚部aを磁性板5の端縁に面接触させ、頂部両端bをその端縁から板厚方向両側に延ばして磁性板5の端縁面12の面積を拡張することもできる。T字形磁性アングル11bの幅は、磁性板5の幅と一致させることが望ましい。図示例は、一対のL字形アングル11aを背中合わせに組み合わせてT字形磁性アングル11bとし、その中央脚部aを磁性板5の凹凸端面に嵌合させて磁性板5と面接触させたものである。例えば頂部両端bの長さが間隔dの1/2程度のT字形磁性アングル11bを用いることにより、磁性板5の端縁面12の面積を最大化できる。 Further, the magnetic expansion plate 11 has a T-shaped magnetic angle 11b as shown in FIG. 2 (D), its central leg a is brought into surface contact with the edge of the magnetic plate 5, and both ends b of the top portion from the edge. The area of the edge surface 12 of the magnetic plate 5 can be expanded by extending both sides in the plate thickness direction. The width of the T-shaped magnetic angle 11b is preferably matched with the width of the magnetic plate 5. In the illustrated example, a pair of L-shaped angles 11a are combined back to back to form a T-shaped magnetic angle 11b, and the center leg a is fitted to the uneven end surface of the magnetic plate 5 and brought into surface contact with the magnetic plate 5. . For example, the area of the edge surface 12 of the magnetic plate 5 can be maximized by using a T-shaped magnetic angle 11b in which the length of the top end b is about ½ of the distance d.
望ましくは、図3(A)に示すように磁性拡張板11を断面コ字形(かすがい形)の磁性アングル11cとし、その両端片aを隣接する磁性板5の長さ方向端縁にそれぞれ面接触させ、中間部dを隣接する磁性板5の端縁間に延在させて磁性板5の端縁面12の面積を拡張する。L字形又はT字形の磁性アングル11a、11bを用いた場合は図1に示すように隣接する磁性板5の端縁面12の間に間隙又は接合部が生じるが、コ字形磁性アングル11cを用いることにより各磁性板5の端縁面12を一体化し、間隙又は接合部のない端縁面12とすることができる。コ字形磁性アングル11cの幅は、磁性板5の幅と一致させることが望ましい。 Desirably, as shown in FIG. 3 (A), the magnetic expansion plate 11 has a U-shaped magnetic cross section (sharp shape) magnetic angle 11c, and both end pieces a face the edge in the longitudinal direction of the adjacent magnetic plate 5, respectively. The intermediate portion d is extended between the edges of the adjacent magnetic plates 5 to expand the area of the edge surface 12 of the magnetic plate 5. When the L-shaped or T-shaped magnetic angles 11a and 11b are used, a gap or a joint is formed between the edge surfaces 12 of the adjacent magnetic plates 5 as shown in FIG. 1, but the U-shaped magnetic angle 11c is used. As a result, the end surface 12 of each magnetic plate 5 can be integrated to form an end surface 12 having no gap or joint. The width of the U-shaped magnetic angle 11c is desirably matched with the width of the magnetic plate 5.
図1のように空隙W1及びW2を介して磁気シールド簾体10a、10b、10cを縦列配置することにより、周囲に空隙W1及びW2が存在する簾体10bを磁気シールドルーム1の開閉部とすることができる。図7(A)は簾体10bを開閉ドアとした実施例を示す。この実施例では、簾体10bの空隙W1、W2と対向する両端縁に各磁性拡張板11による拡張端縁面12と面接触して各端縁面12を相互に接続する磁性框16を設け、簾体10a、10cの空隙W1、W2と対向する端縁に各拡張端縁面12を面接触により相互に接続する磁性枠17を設けている。また、磁性枠17の頂端を簾体10a、10cの上方の磁性梁18と磁気的に接合して磁性門型枠を形成し、門型枠の底端を床19に固定してドアを囲む四方枠を形成している。四方枠と簾体10bとの間に空隙を介在させ、例えばヒンジ24で簾体10bを隣接する磁性枠17と連結することにより簾体10bを開閉可能とする。 As shown in FIG. 1, the magnetic shield housings 10a, 10b, and 10c are arranged in tandem through the air gaps W1 and W2, so that the housing 10b having the air gaps W1 and W2 around them is used as the opening / closing part of the magnetic shield room 1. be able to. FIG. 7A shows an embodiment in which the housing 10b is an opening / closing door. In this embodiment, magnetic flanges 16 are provided on both ends of the casing 10b facing the gaps W1 and W2 so as to make contact with the extended edge surfaces 12 of the magnetic extension plates 11 and connect the edge surfaces 12 to each other. In addition, a magnetic frame 17 is provided on the end edges of the housings 10a and 10c facing the gaps W1 and W2 to connect the extended end face surfaces 12 to each other by surface contact. Further, the top end of the magnetic frame 17 is magnetically joined to the magnetic beam 18 above the housings 10a and 10c to form a magnetic gate frame, and the bottom end of the gate frame is fixed to the floor 19 to surround the door. A four-sided frame is formed. A gap is interposed between the four-sided frame and the casing 10b, and the casing 10b can be opened and closed by connecting the casing 10b to the adjacent magnetic frame 17 with, for example, a hinge 24.
[実験例1]
本発明の磁気シールド簾体10のシールド性能を確認するため、図1の磁気シールドルームを試作して実験を行った。実験では、図11のように厚さ0.35mmの磁性薄板7を18枚重畳した板厚6.3mm、幅50mmの凹凸端面付き磁性板5を接合して適当な長さとし、その磁性板5を板厚方向に間隔d=300mmで重ねて6個の磁気シールド簾体6a、6b、6c、6d、6e、6fを作製し、図12(B)に示すように各簾体6a、6b、6c、6d、6e、6fをシールド対象空間を囲むように各磁性板5の凹凸端縁で接合し又は空隙W1、W2を介して縦列配置することにより、磁気シールドルーム(間口3.6m×奥行2.7m×高さ1.8m)を形成した。
[Experiment 1]
In order to confirm the shielding performance of the magnetic shield housing 10 of the present invention, the magnetic shield room of FIG. In the experiment, as shown in FIG. 11, a magnetic plate 5 with an uneven end face having a thickness of 6.3 mm and a width of 50 mm, in which 18 magnetic thin plates 7 having a thickness of 0.35 mm are overlapped, is joined to obtain an appropriate length. Six magnetic shield housings 6a, 6b, 6c, 6d, 6e, 6f are produced in the thickness direction with an interval d = 300 mm, and each housing 6a, 6b, 6c, as shown in FIG. 6d, 6e, 6f are joined at the uneven edges of each magnetic plate 5 so as to surround the space to be shielded, or arranged in tandem via the gaps W1, W2, so that the magnetic shield room (frontage 3.6m x depth 2.7m x A height of 1.8 m was formed.
図12(B)の簾体6a、6b、6cは、各磁性板5の空隙W1、W2に臨む凹凸端縁にL字形、T次形又はコ字形の磁性アングル11a、11b又は11cを載置又は嵌合させることにより、図1の磁気シールド簾体10a、10b、10cとすることができる。磁性アングル11a、11b又は11cとして、厚さ0.35mm、幅50mm、各片a、b=100mmの磁性薄板製のL字形アングルを3枚重畳したもの、厚さ0.35mm、幅50mm、両端片a=100mm、中間部d=300mmの磁性薄板製のコ字形アングルを3枚重畳したものを用いた。 12B, the L-shaped, T-order or U-shaped magnetic angles 11a, 11b or 11c are placed on the uneven edges facing the gaps W1 and W2 of the magnetic plates 5, respectively. Alternatively, the magnetic shield housings 10a, 10b, and 10c shown in FIG. Magnetic angle 11a, 11b, or 11c, 0.35mm thick, 50mm wide, each piece a, b = 100mm L-shaped angle made of magnetic thin plate overlapped, 0.35mm thick, 50mm wide, both ends a = 3 mm of U-shaped angle made of magnetic thin plate with an intermediate part d = 300 mm was used.
図12(B)に示すように、試作した磁気シールドルームの内側に環状コイルLを設置し、コイルLに矢印I向きにMRI装置と同程度の直流電流を流して直流磁場Mを形成し、シールドルーム1の空隙W1の外側における漏洩磁束密度を磁気センサ34で測定した。列状配置の簾体6a、6b、6cと直角方向に磁気センサ34を移動させながら漏洩磁束密度の測定を繰り返し、空隙W1からの水平距離と漏洩磁束密度との関係からシールド性能を確認した。先ず簾体6a、6b、6cの間の空隙W1、W2の大きさをW1=20mm、W2=5.0mmとした磁気シールドルームのシールド性能を確認し、次いで空隙W2の大きさを5.0mmで維持しつつ空隙W1の大きさを5.0mm、3.0mmとした磁気シールドルームのシールド性能を確認した。 As shown in FIG. 12B, an annular coil L is installed inside the prototype magnetic shield room, and a direct current of the same level as that of the MRI apparatus is passed through the coil L in the direction of arrow I to form a direct current magnetic field M. The leakage magnetic flux density outside the gap W1 in the shield room 1 was measured by the magnetic sensor 34. The measurement of the leakage magnetic flux density was repeated while moving the magnetic sensor 34 in the direction perpendicular to the rows 6a, 6b, 6c of the row arrangement, and the shielding performance was confirmed from the relationship between the horizontal distance from the gap W1 and the leakage magnetic flux density. First, check the shielding performance of the magnetic shield room with the gaps W1 and W2 between the housings 6a, 6b, and 6c set to W1 = 20mm and W2 = 5.0mm, and then maintain the gap W2 at 5.0mm. However, the shielding performance of the magnetic shield room with the gap W1 of 5.0 mm and 3.0 mm was confirmed.
図4は、空隙W1=20mm、W2=5.0mmとした磁気シールドルームのシールド性能を示す。同図のグラフAは簾体6a、6b、6cの磁性板5の端縁に磁性アングル10を取り付けない場合(図2(A)参照)、グラフBはL字形磁性アングル11aを磁性板5の表面に面接触させた場合(同図(B)参照)、グラフCはL字形磁性アングル11aを磁性板5の凹凸端縁に嵌合させた場合(同図(C)参照)、グラフDはT字形磁性アングル11bを磁性板5の凹凸端縁に嵌合させた場合(同図(D)参照)、グラフEはコ字形磁性アングル11cを磁性板5の凹凸端縁に嵌合させた場合(図3(A)参照)のシールド性能をそれぞれ表わす。またグラフGは、比較のため、空隙W1、W2のない図10(B)の列状簾体8により形成したシールドルーム(図3(C)参照)のシールド性能の表したものである。 FIG. 4 shows the shielding performance of the magnetic shield room with the gap W1 = 20 mm and W2 = 5.0 mm. In the graph A in the figure, when the magnetic angle 10 is not attached to the edge of the magnetic plate 5 of the housings 6a, 6b, 6c (see FIG. 2A), the graph B shows the L-shaped magnetic angle 11a of the magnetic plate 5 When the surface is brought into surface contact (see (B) in the same figure), the graph C is obtained when the L-shaped magnetic angle 11a is fitted to the uneven edge of the magnetic plate 5 (see (C) in the same figure), and the graph D is obtained. When the T-shaped magnetic angle 11b is fitted to the uneven edge of the magnetic plate 5 (see FIG. 4D), the graph E shows the case where the U-shaped magnetic angle 11c is fitted to the uneven edge of the magnetic plate 5. Each of the shielding performances (see FIG. 3A) is represented. For comparison, graph G shows the shielding performance of a shield room (see FIG. 3C) formed by the row housing 8 of FIG. 10B without the gaps W1 and W2.
図4のグラフA〜Eの比較から、空隙W1に臨む磁気シールド簾体6a、6bの端縁に磁性アングル11a、11b、11cを取り付けて端縁面12の面積を拡張することにより、空隙W1からの磁束漏洩を小さくできることが分かる。例えば医療機関におけるMRI室では、室外のペースメーカ装着者に悪影響を及ぼさないように、MRI室の外部漏洩磁束を0.5mT以下に抑えることが望まれている(非特許文献1参照)。図4の実験結果は、磁気シールド簾体6で形成したMRI室に20mm程度の空隙W1が存在する場合に、簾体6の各磁性体5の端縁面12を拡張していないときはMRI室からの外部漏洩磁束を0.5mT以下とするために簾体6から175mm程度離れる必要があるが(グラフA参照)、コ字形磁性アングル11cにより端縁面12を拡張したときはその離隔距離を125mm程度まで短くできることを示している(グラフE参照)。ただし、簾体6からの水平離隔距離が100mm以下の範囲では、端縁面12の拡張のみで空隙W1からの漏洩磁束を0.5mT以下に抑えることは難しく、漏洩磁束を更に小さくするためには後述する磁性目張り21、22を空隙W1に設ける必要がある(グラフF参照)。 From the comparison of the graphs A to E in FIG. 4, by attaching the magnetic angles 11a, 11b, 11c to the end edges of the magnetic shield housings 6a, 6b facing the air gap W1 to expand the area of the end face 12, the air gap W1 It can be seen that the magnetic flux leakage from can be reduced. For example, in an MRI room in a medical institution, it is desired that the external leakage magnetic flux in the MRI room be suppressed to 0.5 mT or less so as not to adversely affect an outdoor pacemaker wearer (see Non-Patent Document 1). The experimental results in FIG. 4 show that the MRI chamber formed by the magnetic shield housing 6 has an air gap W1 of about 20 mm and the end surface 12 of each magnetic body 5 of the housing 6 is not expanded. In order to make the external leakage magnetic flux from the chamber 0.5 mT or less, it is necessary to move away from the housing 6 by about 175 mm (see graph A), but when the end face 12 is expanded by the U-shaped magnetic angle 11c, the separation distance is This shows that it can be shortened to about 125 mm (see graph E). However, in the range where the horizontal separation distance from the housing 6 is 100 mm or less, it is difficult to suppress the leakage magnetic flux from the air gap W1 to 0.5 mT or less only by expanding the end face 12. To further reduce the leakage magnetic flux It is necessary to provide magnetic scales 21 and 22 to be described later in the gap W1 (see graph F).
図5は空隙W1=5.0mm、W2=5.0mmとした磁気シールドルームのシールド性能を示し、図6は空隙W1=3.0mm、W2=5.0mmとしたシールド性能を示す。同図のグラフA〜E及びグラフGはそれぞれ、図4のグラフA〜E及びグラフGと端縁面12が同じ状態のシールド性能を表わしている。図5及び図6のグラフから分かるように、空隙W1の大きさが5〜3mm程度であれば、簾体6からの水平離隔距離が100mm以下の範囲においても端縁面12の拡張によって漏洩磁束を0.5mT以下とすることができ、空隙Wからの磁束漏洩を効果的に抑えることが可能である。また、図6のグラフFは後述する磁性目張り21、22を空隙W1に設けた状態のシールド性能を示すが、コ字形磁性アングル11cを取り付けたグラフEとグラフFとがほぼ重なることから、空隙W1の大きさが3mm程度である場合は、空隙W1からの磁束漏洩を端縁面12の拡張によって空隙W1に磁性目張り21、22を設けた場合と同程度まで抑制できることが分かる。 FIG. 5 shows the shielding performance of the magnetic shield room with the gap W1 = 5.0 mm and W2 = 5.0 mm, and FIG. 6 shows the shielding performance with the gap W1 = 3.0 mm and W2 = 5.0 mm. The graphs A to E and the graph G in the same figure show the shielding performance in the state where the end face 12 is the same as the graphs A to E and the graph G in FIG. As can be seen from the graphs of FIGS. 5 and 6, if the size of the air gap W1 is about 5 to 3 mm, the leakage magnetic flux is expanded by the extension of the end face 12 even when the horizontal separation distance from the housing 6 is 100 mm or less. The magnetic flux leakage from the gap W can be effectively suppressed. Graph F in FIG. 6 shows the shielding performance in a state in which magnetic scales 21 and 22 to be described later are provided in the gap W1, but the graph E and the graph F attached with the U-shaped magnetic angle 11c almost overlap with each other. When the size of W1 is about 3 mm, it can be seen that the leakage of magnetic flux from the air gap W1 can be suppressed to the same level as when the magnetic weatherings 21 and 22 are provided in the air gap W1 by expanding the edge surface 12.
すなわち、本発明の磁気シールド簾体10によれば、簾体10の相互間に空隙Wが存在していても、簾体10の各磁性板5の長さ方向端縁面12の実効面積を拡張することにより空隙Wからの磁束漏洩を小さくすることができ、空隙Wの大きさが5〜3mm程度であれば、空隙Wからの磁束漏洩を0.5mT以下に抑えて空隙Wを介して簾体10を磁気的に結合することが可能である。また、磁性体5の端縁面12のみを板厚方向に拡張し、端縁以外の部分の板厚間隔dは十分大きく維持するので、図10の簾体6と同等の高い透光性を確保できる。更に、図13の実施例のように可動機構を用いることなく磁性拡張版11を取り付けるだけで空隙Wからの磁束漏洩を経済的・効率的に抑制できる。従って、ドアや窓等の開閉部のある磁気シールドルームに開放型シールド構造を適用する場合に有効利用が期待できる。 That is, according to the magnetic shield casing 10 of the present invention, even if there is a gap W between the casings 10, the effective area of the lengthwise edge surface 12 of each magnetic plate 5 of the casing 10 is reduced. By expanding, the magnetic flux leakage from the air gap W can be reduced. If the size of the air gap W is about 5 to 3 mm, the magnetic flux leakage from the air gap W is suppressed to 0.5 mT or less and the The body 10 can be magnetically coupled. Further, since only the edge surface 12 of the magnetic body 5 is expanded in the plate thickness direction, and the plate thickness interval d of the portion other than the edge is kept sufficiently large, high translucency equivalent to that of the housing 6 in FIG. It can be secured. Furthermore, magnetic flux leakage from the gap W can be suppressed economically and efficiently simply by attaching the magnetic expansion plate 11 without using a movable mechanism as in the embodiment of FIG. Therefore, effective use can be expected when an open shield structure is applied to a magnetic shield room having an opening / closing part such as a door or a window.
こうして、本発明の目的である「空隙を介して磁気的に結合可能な磁気シールド簾体及びその連結構造」の提供が達成できる。 Thus, it is possible to provide the “magnetic shield housing that can be magnetically coupled through the air gap and its connecting structure”, which is an object of the present invention.
図7(B)及び(C)は、縦列配置した磁気シールド簾体10a、10bの間の空隙W1を縦列方向と直角方向から覆う磁性目張り21又は22を設けた実施例を示す。上述したように本発明は、簾体10の各磁性板5の端縁面12を十分拡張することにより空隙Wからの磁束漏洩を抑えることができるが、空隙Wが比較的大きく端縁面12の拡張のみでは漏洩磁束を十分に小さくできないときは、空隙Wに磁性目張り21、22を設けることが有効である。同図(B)は磁気シールド簾体10の高さ(磁性板5の積層高さ)と同じ高さの帯状磁性目張り21により空隙W1の全域を覆った実施例、同図(C)は磁性拡張板11の拡張端縁面12に対応する大きさのチップ状磁性目張り22により空隙W1の磁性拡張板11が対向する部位を離散的に覆った実施例である。 FIGS. 7B and 7C show an embodiment in which a magnetic cover 21 or 22 is provided to cover the gap W1 between the magnetic shield housings 10a and 10b arranged in a column from the direction perpendicular to the column direction. As described above, the present invention can suppress magnetic flux leakage from the gap W by sufficiently expanding the end face 12 of each magnetic plate 5 of the housing 10, but the gap W is relatively large and the end face 12 When the leakage magnetic flux cannot be made sufficiently small only by the expansion of, it is effective to provide the magnetic struts 21 and 22 in the gap W. FIG. 5B shows an embodiment in which the entire area of the air gap W1 is covered with a belt-shaped magnetic strip 21 having the same height as the height of the magnetic shield housing 10 (stacking height of the magnetic plates 5), and FIG. This is an embodiment in which the portions of the gap W1 facing the magnetic expansion plate 11 are discretely covered with chip-shaped magnetic strips 22 having a size corresponding to the expansion edge surface 12 of the expansion plate 11.
本発明の磁気シールド簾体10は、磁性拡張板11の拡張端縁面12を介して磁気的に結合するので、空隙W1からの磁束漏洩は主に拡張端縁面12から発生すると考えられる。従って、帯状磁性目張り21で空隙Wの全域を覆わなくても、チップ状磁性目張り22により磁束漏洩が大きい部分を重点的に覆うことにより、空隙Wからの磁束漏洩を十分に抑えることが期待できる。チップ状磁性目張り22により空隙Wからの磁束漏洩を十分に抑えることができれば、帯状磁性目張り21を用いる場合に比し磁性材料を節減できる。図7(A)のように簾体10bを開閉ドアとする場合は、磁性目張り21、22をドアの戸先や四方枠に設置することができる。 Since the magnetic shield housing 10 of the present invention is magnetically coupled via the extended edge surface 12 of the magnetic expansion plate 11, it is considered that magnetic flux leakage from the air gap W1 mainly occurs from the extended edge surface 12. Therefore, even if the entire area of the gap W is not covered with the belt-shaped magnetic strips 21, it is expected that the magnetic flux leakage from the gap W can be sufficiently suppressed by preferentially covering the portion where the magnetic flux leakage is large with the chip-shaped magnetic strips 22. . If the magnetic flux leakage from the air gap W can be sufficiently suppressed by the chip-shaped magnetic strips 22, the magnetic material can be saved as compared with the case where the strip-shaped magnetic strips 21 are used. When the casing 10b is used as an open / close door as shown in FIG. 7A, the magnetic weather covers 21 and 22 can be installed on the door tips and the four-sided frame of the door.
[実験例2]
磁性目張り21によるシールド性能を確認するため、図7(B)に示すように、実験例1で用いた磁気シールドルームの空隙W1を帯状磁性目張り21で覆い、実験例1と同様の手法でシールド性能を測定した。磁性目張り21を設けた場合のシールド性能を図4〜6のグラフGに示す(図3(B)参照)。図4及び図5のグラフGから分かるように、磁性目張り21の設置により空隙W1からの磁束漏洩を十分小さくすることができ、漏洩磁束が0.5mT以下となる空隙W1からの水平離隔距離を75mm程度まで短くすることができる。ただし空隙W1の大きさが3mm程度である場合は、図6を参照して上述したように、磁気シールド簾体10の各磁性板5の端縁面12を大きくすることで空隙W1からの磁束漏洩を最小化することができ、磁性目張り21の設置を省略できる。
[Experiment 2]
In order to confirm the shielding performance by the magnetic weathering 21, as shown in FIG. 7 (B), the gap W1 of the magnetic shield room used in the experimental example 1 is covered with the belt-shaped magnetic weathering 21 and shielded by the same method as in the experimental example 1. Performance was measured. The shield performance in the case where the magnetic weathering 21 is provided is shown in a graph G in FIGS. 4 to 6 (see FIG. 3B). As can be seen from the graph G in FIGS. 4 and 5, by installing the magnetic cover 21, the magnetic flux leakage from the air gap W1 can be made sufficiently small, and the horizontal separation distance from the air gap W1 at which the leakage magnetic flux is 0.5 mT or less is 75 mm. Can be as short as However, when the size of the air gap W1 is about 3 mm, the magnetic flux from the air gap W1 is increased by increasing the end surface 12 of each magnetic plate 5 of the magnetic shield housing 10 as described above with reference to FIG. Leakage can be minimized and the installation of the magnetic weathering 21 can be omitted.
[実験例3]
次に、チップ状磁性目張り22によるシールド性能を確認するため、実験例1で用いた空隙W1=20mmの磁気シールドルームの空隙W1を帯状磁性目張り21及びチップ状磁性目張り21で覆い、実験例1と同様の手法でシールド性能を測定して両者のシールド性能を比較した。本実験では、図8(A)に示すように、磁気シールド簾体10のシールド対象磁場の到来側(磁気シールドルームの内側)に間隔Q=5.0mmを介して磁性目張り21、22を設けて空隙W1を覆った。チップ状磁性目張り22のシールド性能を図9のグラフ1に示し、帯状磁性目張り21のシールド性能を同図のグラフ2に示す。グラフ1とグラフ2との比較から、チップ状磁性目張り22により帯状磁性目張り21とほぼ同等のシールド性能を得ることができ、本発明の磁気シールド簾体10ではチップ状磁性目張り22により空隙Wからの磁束漏洩を経済的・効率的に抑制できることが確認できた。
[Experiment 3]
Next, in order to confirm the shielding performance by the chip-shaped magnetic strip 22, the gap W 1 of the magnetic shield room having the gap W 1 = 20 mm used in Experimental Example 1 is covered with the strip-shaped magnetic strip 21 and the chip-shaped magnetic strip 21. The shield performance was measured using the same method as above, and the shield performance was compared. In this experiment, as shown in FIG. 8A, the magnetic shields 21 and 22 are provided on the arrival side of the magnetic field to be shielded (inside the magnetic shield room) of the magnetic shield housing 10 with a gap Q = 5.0 mm. Covered the gap W1. The shield performance of the chip-shaped magnetic strip 22 is shown in graph 1 of FIG. 9, and the shield performance of the strip-shaped magnetic strip 21 is shown in graph 2 of FIG. From comparison between graphs 1 and 2, the chip-shaped magnetic strips 22 can provide almost the same shielding performance as that of the strip-shaped magnetic strips 21. In the magnetic shield housing 10 of the present invention, the chip-shaped magnetic strips 22 can eliminate the gap W. It was confirmed that the leakage of magnetic flux can be controlled economically and efficiently.
[実験例4]
更に、磁性目張り21の設置位置によるシールド性能の変化を確認するため、図8(B)及び(C)に示すように、磁気シールド簾体10のシールド対象磁場の到来側と反対側(磁気シールドルームの外側)に間隔Q=5.0mmを介して配置した帯状磁性目張り21により空隙W1を覆った場合のシールド性能、及び帯状磁性目張り21により空隙W1の両側を覆った場合のシールド性能をそれぞれ測定した。磁気シールドルームの外側から空隙W1を覆ったときのシールド性能を図9のグラフ3に示し、空隙W1の両側を覆ったときのシールド性能を図9のグラフ4に示す。グラフ2に比してグラフ3のシールド性能がかなり優れていることから、空隙Wに帯状磁性目張り21を設置する場合は、磁気シールドルームの外側に設置することが有効あるとの知見が得られた。また、グラフ3とグラフ4がほぼ同等のシールド性能であることから、帯状磁性目張り21は空隙Wの外側に設置すれば十分であることが分かる。
[Experimental Example 4]
Further, in order to confirm the change in the shield performance depending on the installation position of the magnetic weathering 21, as shown in FIGS. 8B and 8C, the side opposite to the arrival side of the magnetic field to be shielded of the magnetic shield housing 10 (magnetic shield) Measure the shielding performance when the gap W1 is covered by the strip-shaped magnetic strips 21 arranged outside the room with a gap Q = 5.0mm, and the shielding performance when the both sides of the gap W1 are covered by the strip-shaped magnetic strips 21. did. The shield performance when covering the gap W1 from the outside of the magnetic shield room is shown in graph 3 of FIG. 9, and the shield performance when covering both sides of the gap W1 is shown in graph 4 of FIG. Since the shielding performance of Graph 3 is considerably superior to that of Graph 2, the knowledge that it is effective to install the strip-shaped magnetic weathering 21 in the gap W outside the magnetic shield room is obtained. It was. Further, since the graph 3 and the graph 4 have substantially the same shielding performance, it can be seen that it is sufficient that the belt-shaped magnetic strip 21 is installed outside the gap W.
本実験において磁性目張り21を磁気シールドルームの外側に設置することが有効ある理由は、磁気シールドルームの中央部に設置したコイルLから発生する磁力線は外側に向かって膨らむ傾向があり、本発明の磁気シールド簾体10からの漏洩磁束も外側に向かって膨らむ傾向があるからと考えられる。図9のシールド性能は帯状磁性目張り21によるものであるが、実験例3の結果から、チップ状磁性目張り21も磁気シールドルームの外側に設置することが有効あると考えられる。すなわち本発明の磁気シールド簾体10では、チップ状磁性目張り22によって磁束漏洩が大きい空隙Wの部分の外側を重点的に覆うことにより、空隙Wからの磁束漏洩を経済的・効率的に抑制することが期待できる。 The reason why it is effective to install the magnetic cover 21 outside the magnetic shield room in this experiment is that the magnetic field lines generated from the coil L installed at the center of the magnetic shield room tend to bulge outward. This is presumably because the leakage magnetic flux from the magnetic shield housing 10 also tends to bulge outward. Although the shielding performance of FIG. 9 is due to the strip-shaped magnetic strips 21, it can be considered from the results of Experimental Example 3 that it is effective to install the chip-shaped magnetic strips 21 outside the magnetic shield room. That is, in the magnetic shield housing 10 of the present invention, the magnetic flux leakage from the air gap W is economically and efficiently suppressed by mainly covering the outside of the air gap W where the magnetic flux leakage is large by the chip-shaped magnetic strips 22. I can expect that.
1…磁気シールドルーム 2…磁気シールド壁
3…磁気シールド開閉部 5…磁性材料板(磁性板)
6…磁気シールド簾体 7…磁性材料薄板(磁性薄板)
8…列状簾体 9…重ね合わせ部分
10、10a、10b…磁気シールド簾体 11…磁性拡張板
11a…断面L字形の磁性アングル 11b…断面T字形の磁性アングル
11c…断面コ字形の磁性アングル(磁性かすがい)
12…端縁面 16…磁性框
17…磁性枠 18…磁性梁
19…床 21…磁性目張り
22…チップ状磁性目張り 24…ヒンジ
31…密閉型磁気シールド体 32…方形磁性板
34…磁気センサ 41…磁気シールドルーム
42…磁気シールド壁 43…磁気シールドドア
44…柱材 45、45a、45b…枠体
46、46a、46b…磁気シールド板 48…可動機構
a、b…アングルの長さ W…空隙
R…材料板の端縁の凹凸の深さ C…材料板の長さ方向中心軸
F…簾面 d…材料板の板厚方向間隔
I…電流 L…電流担体(コイル)
M…磁場 S…シールド係数
H…磁性目張りの位置 P…磁性目張りの幅
Q…縦列配置の磁気シールド簾体と磁性目張りとの間隙
DESCRIPTION OF SYMBOLS 1 ... Magnetic shield room 2 ... Magnetic shield wall 3 ... Magnetic shield opening / closing part 5 ... Magnetic material board (magnetic board)
6 ... Magnetic shield housing 7 ... Magnetic material thin plate (magnetic thin plate)
8 ... Linear housing 9 ... Overlapping part
10, 10a, 10b ... Magnetic shield housing 11 ... Magnetic expansion plate
11a ... Magnetic angle with L-shaped cross section 11b ... Magnetic angle with T-shaped cross section
11c… Magnetic angle with U-shaped cross section
12 ... Edge 16 ... Magnetic cage
17 ... Magnetic frame 18 ... Magnetic beam
19… Floor 21… Magnetic cover
22 ... chip-shaped magnetic cover 24 ... hinge
31 ... Sealed magnetic shield body 32 ... Square magnetic plate
34… Magnetic sensor 41… Magnetic shield room
42… Magnetic shield wall 43… Magnetic shield door
44: Column material 45, 45a, 45b ... Frame
46, 46a, 46b ... Magnetic shield plate 48 ... Movable mechanism a, b ... Length of angle W ... Gap R ... Depth of unevenness on edge of material plate C ... Center axis F in the length direction of material plate ... Rough surface d ... Thickness direction interval of material plate I ... Current L ... Current carrier (coil)
M ... Magnetic field S ... Shielding factor H ... Magnetic weathering position P ... Magnetic weathering width Q ... Gap between magnetic shield housings arranged in tandem and magnetic weathering
Claims (12)
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JP2005172378A JP4605778B2 (en) | 2005-06-13 | 2005-06-13 | Magnetic shield housing and connection structure thereof |
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JP2005172378A JP4605778B2 (en) | 2005-06-13 | 2005-06-13 | Magnetic shield housing and connection structure thereof |
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JP4605778B2 JP4605778B2 (en) | 2011-01-05 |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2014120703A (en) * | 2012-12-19 | 2014-06-30 | Kajima Corp | Conductor circuit for open type magnetic shield |
JP2014135428A (en) * | 2013-01-11 | 2014-07-24 | Kajima Corp | Open type magnetic shield structure with door |
Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0354895A (en) * | 1989-07-24 | 1991-03-08 | Bouon Kogyo Kk | Shield room |
JPH04153431A (en) * | 1990-10-17 | 1992-05-26 | Shimizu Corp | Magnetic shield room |
JPH1030289A (en) * | 1996-07-17 | 1998-02-03 | Shimizu Corp | Magnetic shield unit wall |
JP2000045650A (en) * | 1998-05-26 | 2000-02-15 | Masako Maekawa | Magnetically shielded building with opening |
JP2000077890A (en) * | 1998-08-27 | 2000-03-14 | Hitachi Ltd | Magnetic shielding room |
JP2002164686A (en) * | 2000-11-27 | 2002-06-07 | Kajima Corp | Method and device for reed screen type magnetic shielding |
WO2005026462A1 (en) * | 2003-09-12 | 2005-03-24 | Nippon Steel Corporation | Magnetic shield panel |
-
2005
- 2005-06-13 JP JP2005172378A patent/JP4605778B2/en not_active Expired - Fee Related
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0354895A (en) * | 1989-07-24 | 1991-03-08 | Bouon Kogyo Kk | Shield room |
JPH04153431A (en) * | 1990-10-17 | 1992-05-26 | Shimizu Corp | Magnetic shield room |
JPH1030289A (en) * | 1996-07-17 | 1998-02-03 | Shimizu Corp | Magnetic shield unit wall |
JP2000045650A (en) * | 1998-05-26 | 2000-02-15 | Masako Maekawa | Magnetically shielded building with opening |
JP2000077890A (en) * | 1998-08-27 | 2000-03-14 | Hitachi Ltd | Magnetic shielding room |
JP2002164686A (en) * | 2000-11-27 | 2002-06-07 | Kajima Corp | Method and device for reed screen type magnetic shielding |
WO2005026462A1 (en) * | 2003-09-12 | 2005-03-24 | Nippon Steel Corporation | Magnetic shield panel |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2014120703A (en) * | 2012-12-19 | 2014-06-30 | Kajima Corp | Conductor circuit for open type magnetic shield |
JP2014135428A (en) * | 2013-01-11 | 2014-07-24 | Kajima Corp | Open type magnetic shield structure with door |
Also Published As
Publication number | Publication date |
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JP4605778B2 (en) | 2011-01-05 |
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