JP6049014B2 - Open type magnetic shield structure with door - Google Patents
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Description
本発明は扉付き開放型磁気シールド構造に関し,とくに磁気シールド対象空間を帯状磁性板で囲む開放型磁気シールド構造に関する。 The present invention relates to an open type magnetic shield structure with a door, and more particularly to an open type magnetic shield structure in which a magnetic shield target space is surrounded by a belt-like magnetic plate.
半導体製造施設等で用いる電子顕微鏡,EB露光装置,EBステッパー等の電子ビーム応用装置は,例えば100nT(1mG)程度の微弱な磁気ノイズでも電子ビームの軌道が変化するので,製品の品質を確保するために外乱磁場(環境磁場)の影響を避ける必要がある。また,医療施設等で用いる脳磁計や心磁計等のSQUID(超電導量子干渉素子)応用装置は,微弱な磁気を正確に測定するため外乱磁場の遮断が求められる。このような外乱磁場の影響を嫌う装置(嫌磁気装置)を外乱磁場から保護して正常な動作を保証するため,施設内に磁気シールドルーム(シールド空間)を設けることが求められる。 An electron beam application apparatus such as an electron microscope, an EB exposure apparatus, or an EB stepper used in a semiconductor manufacturing facility or the like ensures the product quality because the trajectory of the electron beam changes even with a weak magnetic noise of about 100 nT (1 mG), for example. Therefore, it is necessary to avoid the influence of disturbance magnetic field (environmental magnetic field). In addition, SQUID (superconducting quantum interference device) application devices such as magnetoencephalographs and magnetocardiographs used in medical facilities are required to block disturbance magnetic fields in order to accurately measure weak magnetism. In order to protect a device that does not like the influence of a disturbance magnetic field (magnetomagnetic device) from the disturbance magnetic field and to ensure normal operation, it is required to provide a magnetic shield room (shield space) in the facility.
従来の磁気シールドルームは,透磁率μの高いPCパーマロイ,電磁鋼板等の磁性体製の板(以下,磁性板という)により床,壁,天井の全体を隙間なく覆う構造(密閉型シールド構造)とすることが多い。これに対し,図13に示すように,帯状磁性板を簾状又はルーバー状に並べた磁気シールド構造(以下,開放型磁気シールド構造又は開放型シールド構造という)5が開発されている(特許文献1〜4参照)。図示例の開放型シールド構造5は,例えば帯幅30〜50mm程度の複数の帯状磁性板2を長さ方向中心軸Cが同一簾面F上に平行に並ぶように所要の板厚方向間隔dで積み重ねて磁気シールド簾体3とし(図13(A)参照),複数のシールド簾体3a,3b,3c,3dを対応する端縁の重ね合わせ(面接触)9により磁気的に接合して環状に閉じた帯状磁性板(以下,環帯状磁性板という)4を形成し,複数の環帯状磁性板4でシールド対象空間1を囲んだものである(図13(B)参照)。 The conventional magnetic shield room has a structure that covers the entire floor, wall, and ceiling without any gaps with a plate made of a magnetic material such as PC permalloy (high magnetic permeability μ) or magnetic steel plate (hereinafter referred to as a magnetic plate) (sealed shield structure). And often. On the other hand, as shown in FIG. 13, a magnetic shield structure (hereinafter referred to as an open magnetic shield structure or an open shield structure) 5 in which strip-like magnetic plates are arranged in a bowl shape or a louver shape has been developed (Patent Document). 1-4). The open type shield structure 5 of the illustrated example has a required plate thickness direction interval d such that a plurality of belt-like magnetic plates 2 having, for example, a band width of about 30 to 50 mm are aligned in parallel with the longitudinal center axis C on the same saddle surface F. To form a magnetic shield housing 3 (see FIG. 13A), and a plurality of shield housings 3a, 3b, 3c, 3d are magnetically joined by overlapping (surface contact) 9 of corresponding edges. A band-shaped magnetic plate (hereinafter referred to as a ring-shaped magnetic plate) 4 that is closed in an annular shape is formed, and the shield target space 1 is surrounded by a plurality of ring-shaped magnetic plates 4 (see FIG. 13B).
図13(B)の開放型シールド構造は,環帯状磁性板4の相互間隔dを,磁性板4中の磁束の通りやすさ(磁性板のパーミアンス)が間隔d中の磁束の通りやすさ(間隔のパーミアンス)より大きくなるように,すなわち間隔dの断面積Saに対する磁性板4の断面積Smと比透磁率μsとの積(Sm・μs)の割合(Sm・μs/Sa)が1より充分大きくなるように設計することができる。適切な間隔dを設計することにより,空間1に開放性(透視性,透光性,放熱性)を与えつつ,同図に矢印で示すように磁気的に閉じた環帯状磁性板4(磁性体回路)に磁束を集中させて間隔dからの外乱磁場Mの侵入を小さく抑え,磁気シールドルームに相応しい磁気環境(磁気シールド性能)を提供できる。図示例は直流磁場Mが印加された場合を示しているが,交流磁場Mが印加された場合も磁束の方向が変化するだけで同様の効果が得られる。 In the open type shield structure of FIG. 13B, the mutual distance d of the ring-shaped magnetic plates 4 is set so that the magnetic flux in the magnetic plate 4 is easy to pass (permeance of the magnetic plate). The ratio (Sm · μs / Sa) of the product (Sm · μs) of the cross-sectional area Sm of the magnetic plate 4 and the relative permeability μs to the cross-sectional area Sa of the interval d is greater than 1. It can be designed to be large enough. By designing an appropriate distance d, the space 1 is given openness (permeability, translucency, heat dissipation), and magnetically closed annulus-shaped magnetic plate 4 (magnetic) as shown by the arrows in FIG. The magnetic field is concentrated on the body circuit), and the magnetic field (magnetic shield performance) suitable for the magnetic shield room can be provided by suppressing the intrusion of the disturbance magnetic field M from the interval d. The illustrated example shows the case where the DC magnetic field M is applied, but when the AC magnetic field M is applied, the same effect can be obtained only by changing the direction of the magnetic flux.
ただし,図13(B)の開放型シールド構造を磁気シールドルームに適用するためには,人や物が出入りするための比較的大きな扉開口を設ける必要がある。例えば,図10(A1)及び(B1)に示すような環帯状磁性板4で囲まれた開放型シールド構造の磁気シールドルーム1において,図10(A2)及び(B2)のような扉開口11を設けると磁気的に閉じた環帯状磁性板(磁性体回路)が切断されるので,扉開口11を開放したままにすると磁気シールド性能が劣化しうる。密閉型シールド構造では,開口11を閉じる扉の表面に磁性板を取り付け,扉枠を介して扉の磁性板を床,壁,天井の磁性板と面的に接触させることにより,比較的容易に扉開口を磁気的に閉鎖することができる。これに対し開放型シールド構造では,扉開口11で切断された環帯状磁性板(C字型磁性板20)を扉面と面的に接触させることができないので,密閉型シールド構造の扉をそのまま用いても扉開口11を磁気的に閉鎖することは難しい。 However, in order to apply the open type shield structure of FIG. 13B to a magnetic shield room, it is necessary to provide a relatively large door opening for people and objects to enter and exit. For example, in a magnetic shield room 1 having an open shield structure surrounded by an annular belt-like magnetic plate 4 as shown in FIGS. 10A1 and 10B1, a door opening 11 as shown in FIGS. 10A2 and 10B2. Since the ring-shaped magnetic plate (magnetic circuit) that is magnetically closed is cut, if the door opening 11 is left open, the magnetic shielding performance can be deteriorated. In the sealed shield structure, a magnetic plate is attached to the surface of the door that closes the opening 11, and the magnetic plate of the door is brought into surface contact with the magnetic plate of the floor, wall, or ceiling via the door frame. The door opening can be magnetically closed. On the other hand, in the open shield structure, the ring-shaped magnetic plate (C-shaped magnetic plate 20) cut at the door opening 11 cannot be brought into surface contact with the door surface. Even if it is used, it is difficult to magnetically close the door opening 11.
開放型シールド構造に設けた扉開口11を磁気的に閉鎖する方法として,図10(A3)及び(B3)に示すように,磁気シールド簾体3(図13(A))によって扉開口11の扉を構成すると共にその長さ方向端縁に磁性板製の拡張板(L字形アングル等)16を取り付け,対向する開口11の周囲壁面(C字型磁性板20)の長さ方向端縁にも磁性拡張板16を取り付け,両者の対向する面積を板厚方向に拡張する方法が提案されている(特許文献3参照)。扉と周囲壁面との間に多少空隙が存在していても,両者の対向する面積を拡張すれば,その間隙を介して両者を磁気的に結合して磁場の侵入を抑えることが期待できる。また,図10(A4)及び(B4)に示すように,扉開口11の内側周囲に磁性板製の開口枠17を設けると共にその開口枠17を開口11の周囲壁面のC字型磁性板20と接続する方法が提案されている(特許文献2参照)。磁性開口枠17を介して磁束を迂回させることにより,切断された環帯状磁性板(C字型磁性板20)からの磁場の侵入を小さく抑えることが期待できる。 As a method of magnetically closing the door opening 11 provided in the open type shield structure, as shown in FIGS. 10 (A3) and (B3), the magnetic shield housing 3 (FIG. 13 (A)) is used to An extension plate (L-shaped angle or the like) 16 made of a magnetic plate is attached to the lengthwise edge of the door, and the door is formed on the edge in the lengthwise direction of the peripheral wall surface of the opening 11 (C-shaped magnetic plate 20). In addition, a method has been proposed in which a magnetic expansion plate 16 is attached and the opposing area is expanded in the thickness direction (see Patent Document 3). Even if there is a slight gap between the door and the surrounding wall surface, if the area where the two faces each other is expanded, it can be expected that the two will be magnetically coupled through the gap to suppress the penetration of the magnetic field. Further, as shown in FIGS. 10A4 and 10B4, an opening frame 17 made of a magnetic plate is provided around the inner side of the door opening 11, and the opening frame 17 is formed into a C-shaped magnetic plate 20 on the peripheral wall surface of the opening 11. Has been proposed (see Patent Document 2). By diverting the magnetic flux through the magnetic opening frame 17, it can be expected that the intrusion of the magnetic field from the cut ring-shaped magnetic plate (C-shaped magnetic plate 20) can be suppressed to a low level.
しかし,上述した図10(A3)及び図10(A4)の方法は,開放型シールド構造の扉開口11から侵入する微弱磁場を必ずしも十分に抑えることができない問題点がある。本発明者は,幅30mm×長さ280mm×板厚0.5mmの4枚の帯状磁性板2(PCパーマロイ製)を井桁状に接合した環帯状磁性板4(図13(B)参照)を作成し,図10(A1)及び(B1)に示すように,その環帯状磁性板4を板厚方向間隔d=60mmで5段重ねた開放型シールド構造5を作成して磁気シールド性能5を確認する実験を行った。実験では,図12(A)に示す環状コイルLの中央部に開放型シールド構造5を設置し,X方向及びY方向の略一様の微弱磁場M(10μT,直流磁場)を順次印加しながら,内側空間1の評価点S1〜S5の磁場強度をそれぞれ磁気センサ8により測定した。また,数値シミュレーション(三次元非線形磁場解析)により同じ開放型シールド構造5の各評価点S1〜S5の磁場強度を解析したところ,実験値と概ね一致する解析値が得られた。そこで,図10(A2),図10(A3),及び図10(A4)のように94mm幅の扉開口11を設けた開放型シールド構造において,X方向及びY方向の微弱磁場Mを印加した時の評価点S1〜S5の磁場強度をそれぞれ数値シミュレーションにより求め,開口11を設ける前の評価点S1〜S5の磁場強度(磁場強度の基準値)と比較する検証実験を行った。 However, the above-described methods shown in FIGS. 10A3 and 10A4 have a problem that the weak magnetic field entering from the door opening 11 of the open shield structure cannot be sufficiently suppressed. The inventor used an annular belt-like magnetic plate 4 (see FIG. 13B) in which four belt-like magnetic plates 2 (made of PC Permalloy) having a width of 30 mm, a length of 280 mm, and a plate thickness of 0.5 mm were joined in a cross-beam shape. As shown in FIGS. 10 (A1) and (B1), an open type shield structure 5 in which the annular belt-like magnetic plate 4 is stacked in five steps at a thickness direction interval d = 60 mm is created to obtain a magnetic shield performance 5. An experiment to confirm was conducted. In the experiment, an open shield structure 5 is installed at the center of the annular coil L shown in FIG. 12A, and a substantially uniform weak magnetic field M (10 μT, DC magnetic field) in the X and Y directions is sequentially applied. The magnetic field strengths at the evaluation points S1 to S5 in the inner space 1 were measured by the magnetic sensor 8, respectively. Further, when the magnetic field strength at each of the evaluation points S1 to S5 of the same open shield structure 5 was analyzed by a numerical simulation (three-dimensional nonlinear magnetic field analysis), an analytical value almost coincident with the experimental value was obtained. Therefore, weak magnetic fields M in the X and Y directions were applied in an open shield structure having a 94 mm wide door opening 11 as shown in FIGS. 10 (A2), 10 (A3), and 10 (A4). A verification experiment was performed in which the magnetic field strengths of the evaluation points S1 to S5 at the time were respectively obtained by numerical simulation and compared with the magnetic field strengths (reference values of the magnetic field strength) of the evaluation points S1 to S5 before the opening 11 was provided.
図11(A2)のグラフは,図10(A2)のように扉開口11が開放されたままの開放型シールド構造の評価点S1〜S5の磁場強度(基準値に対する比率),及び5点の平均磁場強度(基準値の平均に対する比率)を示す。また図11(A3)のグラフは,図10(A3)のように磁性拡張板16付き扉3と開口周囲とを所要空隙(幅5mm)で対向させた開放型シールド構造の評価点S1〜S5の磁場強度(基準値に対する比率),及び5点の平均磁場強度(基準値の平均に対する比率)を示す。両グラフの比較から分かるように,開口11に磁性拡張板16付き扉3を設けることにより,X方向磁場に対して開口近くの評価点S2の磁場を小さくできるが,他の評価点S1,S3〜S5の磁場を十分に小さくすることはできていない。また,Y方向磁場に対して内側空間1の磁場を全体的に小さくできるが,評価点S2の磁場を十分に小さくすることはできていない。この実験結果から,開口11の扉3に磁性拡張板16を取り付けただけでは,微弱磁場Mを対象とした開放型シールド構造の内側空間1の全体において十分な磁気シールド効果を得ることは難しいことが分かる。 The graph of FIG. 11A2 shows the magnetic field strength (ratio to the reference value) of the evaluation points S1 to S5 of the open type shield structure with the door opening 11 opened as shown in FIG. The average magnetic field strength (ratio of the reference value to the average) is shown. Further, the graph of FIG. 11A3 shows the evaluation points S1 to S5 of the open type shield structure in which the door 3 with the magnetic expansion plate 16 and the periphery of the opening face each other with a required gap (width 5 mm) as shown in FIG. 10A3. The magnetic field strength (ratio to the reference value) and the average magnetic field strength at 5 points (ratio to the average of the reference value) are shown. As can be seen from the comparison of both graphs, by providing the door 3 with the magnetic expansion plate 16 in the opening 11, the magnetic field at the evaluation point S2 near the opening can be reduced with respect to the magnetic field in the X direction, but the other evaluation points S1, S3 The magnetic field of .about.S5 cannot be made sufficiently small. Further, although the magnetic field in the inner space 1 can be reduced as a whole with respect to the Y-direction magnetic field, the magnetic field at the evaluation point S2 cannot be sufficiently reduced. From this experimental result, it is difficult to obtain a sufficient magnetic shielding effect in the entire inner space 1 of the open shield structure for the weak magnetic field M only by attaching the magnetic expansion plate 16 to the door 3 of the opening 11. I understand.
また図11(A4)のグラフは,図10(A4)のように所要厚さ(0.5mm)の磁性開口枠17を設けて磁束を迂回させた開放型シールド構造の評価点S1〜S5の磁場強度(基準値に対する比率),及び5点の平均磁場強度(基準値の平均に対する比率)を示す。図11(A4)と図11(A2)との比較から分かるように,開口11に磁性開口枠17を設けることにより,X方向磁場に対して開口から離れた評価点S3の磁場を小さくできるが,他の評価点S1〜S2,S4〜S5の磁場は逆に大きくなっている。また,Y方向磁場に対しては全体的に磁場が大きくなっており,とくに評価点S2の磁場が大きくなっている。この実験結果から,開口11に磁性開口枠17を設けることによっても,微弱磁場Mを対象とした開放型シールド構造の内側空間1の全体において十分な磁気シールド効果を得ることはできないことが分かる。 Further, the graph of FIG. 11A4 shows the evaluation points S1 to S5 of the open type shield structure in which the magnetic opening frame 17 having the required thickness (0.5 mm) is provided to bypass the magnetic flux as shown in FIG. 10A4. The magnetic field strength (ratio to the reference value) and the average magnetic field strength at 5 points (ratio to the average of the reference value) are shown. As can be seen from a comparison between FIG. 11 (A4) and FIG. 11 (A2), by providing the magnetic aperture frame 17 in the opening 11, the magnetic field at the evaluation point S3 away from the opening can be reduced with respect to the X-direction magnetic field. , The magnetic fields of the other evaluation points S1 to S2 and S4 to S5 are larger. Further, the magnetic field is generally increased with respect to the Y-direction magnetic field, and in particular, the magnetic field at the evaluation point S2 is increased. From this experimental result, it can be seen that even if the magnetic aperture frame 17 is provided in the opening 11, a sufficient magnetic shielding effect cannot be obtained in the entire inner space 1 of the open shield structure for the weak magnetic field M.
図11(A4)の実験結果は,磁性開口枠17を設けることにより磁性体の全体的な配置バランスが崩れ,磁性体回路に流れる磁束が非対称となって磁束の流れにくい場所が生じたため,内部空間1の磁場が全体的に増大したことを示唆している。また図11(A3)の実験結果は,磁性拡張板16の面方向が印加する磁場Mの方向と異なる場合に,磁性体回路に磁束が流れにくくなり,内部空間1に磁場の増大する場所が生じることを示唆している。開放型シールド構造を開口11のある磁気シールドルームに適用するためには,磁性体回路に流れる磁束を乱すことなく扉開口11を磁気的に閉鎖することができ,開口11から侵入する微弱磁場を十分に抑えて内側空間1の全体において十分な磁気シールド効果が得られる技術が必要である。 The experimental result of FIG. 11 (A4) shows that the provision of the magnetic aperture frame 17 disrupts the overall arrangement balance of the magnetic material, and the magnetic flux flowing in the magnetic circuit becomes asymmetrical, resulting in a place where the magnetic flux does not flow easily. This suggests that the magnetic field in space 1 has increased overall. 11A3 shows that when the surface direction of the magnetic expansion plate 16 is different from the direction of the magnetic field M to be applied, it is difficult for the magnetic flux to flow in the magnetic circuit, and there is a place where the magnetic field increases in the internal space 1. Suggests that it will occur. In order to apply the open type shield structure to the magnetic shield room having the opening 11, the door opening 11 can be magnetically closed without disturbing the magnetic flux flowing through the magnetic circuit, and the weak magnetic field entering from the opening 11 can be prevented. There is a need for a technique that can be sufficiently suppressed to obtain a sufficient magnetic shielding effect in the entire inner space 1.
そこで本発明の目的は,内側空間の全体において十分な磁気シールド効果を得ることができる扉付き開放型磁気シールド構造を提供することにある。 Accordingly, an object of the present invention is to provide an open type magnetic shield structure with a door which can obtain a sufficient magnetic shield effect in the entire inner space.
図1の実施例を参照するに,本発明による扉付き開放型磁気シールド構造は,扉12の開口11付き磁気シールド対象空間1をその扉12と平行に貫く第1方向軸Azと所定間隔dzで交差する複数の平行な平面Pz1,Pz2,……上にそれぞれ設けられ且つその空間1を囲みつつ扉開口11で切断された帯状の第1C字型磁性板20z1,20z2,……,第1方向軸Azと交差する複数の平面Pz1,Pz2,……と開口11を閉鎖する扉12との交線に沿ってそれぞれ扉12上に第1C字型磁性板の帯幅面と直角に配置され且つ相互に絶縁された複数の帯状の第1I字型磁性板23z(23z1,23z2,……),第1C字型磁性板20z1,20z2,……の各々の切断部分の両端に第1I字型磁性板23zと対向するように取り付けられたL字型アングル形状の繋ぎ磁性体26z(26z1,26z2,……),及び扉開口11の閉鎖時に繋ぎ磁性体26zを介して第1C字型磁性板20z1,20z2,……と第1I字型磁性板23z1,23z2,……とを密着させる押圧機構を備えてなるものである。 Referring to the embodiment of FIG. 1, an open type magnetic shield structure with a door according to the present invention has a first direction axis Az penetrating the magnetic shield target space 1 with an opening 11 of the door 12 in parallel with the door 12 and a predetermined distance dz. in a plurality of parallel planes which intersect Pz1, Pz2, respectively provided on ...... and the 1C-shaped magnetic plate strip cut in the door opening 11 while surrounding the space 1 20z1,20z2, ......, first A plurality of planes Pz1, Pz2,... Intersecting the direction axis Az are arranged on the door 12 along the intersecting line with the door 12 closing the opening 11, respectively, and perpendicular to the band width surface of the first C-shaped magnetic plate; mutually insulated multiple strip of the 1I-shaped magnetic plate 23z (23z1,23z2, ......), the 1C-shaped magnetic plates 20Z1,20z2, the 1I-shaped magnetic across each cutting portion of ...... Take so as to face the plate 23z The L-shaped angle-shaped connecting magnetic body 26z (26z1, 26z2,...) And the first C-shaped magnetic plates 20z1, 20z2,... Via the connecting magnetic body 26z when the door opening 11 is closed. The first I-shaped magnetic plates 23z1, 23z2,.
好ましくは,図2に示すように,磁気シールド対象空間1を扉12と平行に貫く第2方向軸Axと所定間隔dxで交差する複数の平行な平面Px1,Px2,……上にそれぞれ第1C字型磁性板20z1,20z2,……と入れ子状に設けられ且つその空間1を囲みつつ扉開口11で切断された帯状の第2C字型磁性板20x1,20x2,……,第2方向軸Axと交差する複数の平面Px1,Px2,……と扉12との交線に沿ってそれぞれ扉12上に第2C字型磁性板の帯幅面と直角に配置され且つ相互に絶縁されると共に第1C字型磁性板23z(23z1,23z2,……)と絶縁された複数の帯状の第2I字型磁性板23x(23x1,23x2,……),及び第2C字型磁性板20x1,20x2,……の各々の切断部分の両端に第2I字型磁性板23xと対向するように取り付けられたL字型アングル形状の繋ぎ磁性体26xを設け,押圧機構により扉開口11の閉鎖時に繋ぎ磁性体26xを介して第2C字型磁性板20x1,20x2,……と第2I字型磁性板23x1,23x2,……とを密着させる。 Preferably, as shown in FIG. 2, the first C is respectively formed on a plurality of parallel planes Px1, Px2,... Intersecting a second direction axis Ax penetrating the magnetic shield target space 1 in parallel with the door 12 at a predetermined interval dx . shaped magnetic plate 20z1,20z2, ...... and telescopically arranged and cut in the door opening 11 while surrounding the space 1 a strip of the 2C-shaped magnetic plate 20x1,20x2, ......, a second direction axis Ax A plurality of planes Px1, Px2,... Intersecting with the door 12 are respectively arranged on the door 12 at right angles to the band width surface of the second C-shaped magnetic plate and insulated from each other and the first C A plurality of strip-shaped second I-shaped magnetic plates 23x (23x1, 23x2,...) Insulated from the letter-shaped magnetic plates 23z (23z1, 23z2,...), And the second C-shaped magnetic plates 20x1, 20x2,. Both ends of each cutting part The connecting magnetic 26x of the L-shaped angle shape mounted so as to face the first 2I-shaped magnetic plate 23x provided, the 2C-shaped magnetic plate through the magnetic 26x tether during closing of the door opening 11 by the pressing mechanism 20x1, 20x2,... And the second I-shaped magnetic plates 23x1, 23x2,.
更に好ましくは,図3に示すように,磁気シールド対象空間1を扉12と垂直に貫く第3方向軸Ayと所定間隔dyで交差する複数の平行な平面Py1,Py2,……上にそれぞれ空間1を囲む環帯状磁性板20y1,20y2,……を設け,空間1の周囲に第1C字型磁性板20z1,20z2,……と第2C字型磁性板20x1,20x2,……と環帯状磁性板20y1,20y2,……とを入れ子状に配置する。 More preferably, as shown in FIG. 3, each space is placed on a plurality of parallel planes Py1, Py2,... Intersecting a third direction axis Ay passing through the magnetic shield target space 1 perpendicularly to the door 12 at a predetermined interval dy. Are provided around the space 1, and the first C-shaped magnetic plates 20z1, 20z2,... And the second C-shaped magnetic plates 20x1, 20x2,. The plates 20y1, 20y2,... Are arranged in a nested manner.
更に望ましい実施例では,図3のように磁気シールド対象空間1の周囲に第1C字型磁性板20zと第2C字型磁性板20xと環帯状磁性板20yとを入れ子状に配置すると共に,図4に示すように,第1方向軸Azと交差する複数の第1C字型磁性板20zの間隔dzにそれぞれ磁気シールド対象空間1を囲みつつ扉開口11で切断された帯状の第1C字型導体板30zを設け,開口11の内側周囲に導体開口枠32を固定し,各第1C字型導体板30zの切断部分の両端を導体開口枠32に電気的に接合する。 In a more preferred embodiment, the first C-shaped magnetic plate 20z, the second C-shaped magnetic plate 20x, and the ring-shaped magnetic plate 20y are arranged in a nested manner around the magnetic shield target space 1 as shown in FIG. As shown in FIG. 4, a strip-shaped first C-shaped conductor cut by a door opening 11 while surrounding the magnetic shield target space 1 at intervals dz between a plurality of first C-shaped magnetic plates 20z intersecting the first direction axis Az. The plate 30z is provided, the conductor opening frame 32 is fixed around the inside of the opening 11, and both ends of the cut portion of each first C-shaped conductor plate 30z are electrically joined to the conductor opening frame 32.
図5(A)に示すように,第1C字型導体板30zに代えて又は加えて,第2方向軸Axと交差する複数の第2C字型磁性板20xの間隔dxにそれぞれ磁気シールド対象空間1を囲みつつ扉開口11で切断された帯状の第2C字型導体板30xを設け,各第2C字型導体板30xの切断部分の両端を導体開口枠32に電気的に接合してもよい。また,図5(B)に示すように,第1C字型導体板30z及び第2C字型導体板30xに代えて又は加えて,第3方向軸Ayと交差する複数の環帯状磁性板20yの間隔dyにそれぞれ磁気シールド対象空間1を囲む環帯状導体板30yを設けることもできる。 As shown in FIG. 5A, instead of or in addition to the first C-shaped conductor plate 30z, magnetic shield target spaces are respectively provided at intervals dx between the plurality of second C-shaped magnetic plates 20x intersecting the second direction axis Ax. 1, a belt-like second C-shaped conductor plate 30 x that is cut by the door opening 11 may be provided, and both ends of the cut portion of each second C-shaped conductor plate 30 x may be electrically joined to the conductor opening frame 32. . Further, as shown in FIG. 5B, instead of or in addition to the first C-shaped conductor plate 30z and the second C-shaped conductor plate 30x, a plurality of annular belt-shaped magnetic plates 20y intersecting the third direction axis Ay. An annular belt-shaped conductor plate 30y that surrounds the magnetic shield target space 1 can also be provided at intervals dy.
本発明の扉付き開放型磁気シールド構造によれば,磁気シールド対象空間1を扉12と平行に貫く第1方向軸Azと所定間隔dzで交差する複数の平行な平面Pz1,Pz2,……上にそれぞれ空間1を囲みつつ扉開口11で切断されたC字型磁性板20z1,20z2,……を配置し,第1方向軸Azと交差する複数の平面Pz1,Pz2,……と開口11を閉鎖する扉12との交線に沿ってそれぞれ相互に絶縁しつつ扉12上に複数の帯状のI字型磁性板23z1,23z2,……を配置し,C字型磁性板20z1,20z2,……の各々の切断部分の両端にI字型磁性板23z1,23z2,……と対向するように繋ぎ磁性体26zを取り付け,扉12の閉鎖時に繋ぎ磁性体26zを介してC字型磁性板20z1,20z2,……とI字型磁性板23z1,23z2,……とを密着させて磁気的に接合させるので,次の効果が得られる。 According to the open type magnetic shield structure with a door of the present invention, a plurality of parallel planes Pz1, Pz2,... On the first direction axis Az penetrating the magnetic shield target space 1 in parallel with the door 12 at a predetermined interval dz. C-shaped magnetic plates 20z1, 20z2,... Cut by the door opening 11 while surrounding the space 1, respectively, and a plurality of planes Pz1, Pz2,... And the opening 11 intersecting the first direction axis Az. A plurality of strip-shaped I-shaped magnetic plates 23z1, 23z2,... Are arranged on the door 12 while being insulated from each other along the line of intersection with the door 12 to be closed , and the C-shaped magnetic plates 20z1, 20z2,. The connecting magnetic body 26z is attached to both ends of each cut portion so as to face the I-shaped magnetic plates 23z1, 23z2,... When the door 12 is closed, and the C-shaped magnetic plate 20z1 is connected via the connecting magnetic body 26z. , 20z2, ...... and I Type magnetic plate 23Z1,23z2, since the in close contact to magnetically joining ..., the following effects can be obtained.
(イ)C字型磁性板20zに取り付けた繋ぎ磁性体26zを扉磁性板22と対向させ,扉12の閉鎖時にC字型磁性板20zと扉磁性板22とを面接触させることにより,磁性体回路の連続性を確保して扉開口11を磁気的に閉鎖することができる。
(ロ)また,複数の平面Pz1,Pz2,……と扉12との交線に沿ってそれぞれ相互に絶縁しつつ設けた複数のI字型磁性板23z1,23z2,……によって扉磁性板22を構成し,C字型磁性板20zの各々とI字型磁性板23zの各々とを相互に絶縁しつつ磁気的に接合させることにより,磁性体回路の各々に流れる磁束を乱すことなく扉開口11を磁気的に閉鎖することができる。
(ハ)磁性体回路に流れる磁束を乱すことなく扉開口11を磁気的に閉鎖することにより,扉12の閉鎖時に内側空間の全体において十分な磁気シールド効果を得ることができる。
(ニ)また,複数のC字型磁性板20zの間隔dzにそれぞれ空間1を囲みつつ扉開口11で切断されたC字型導体板30zを設け,開口11の内側周囲に導体開口枠32を固定し,C字型導体板30zの切断部分の両端を導体開口枠32に電気的に接合することにより,磁性体回路と導体回路とを組み合わせた開放型シールド構造とすることができる。
(ホ)磁性体回路による開放型シールド構造は高周波数域において磁気シールド性能が低下しうるのに対し,導体回路による開放型シールド構造は高周波数域において磁気シールド性能が向上するので,両者を組み合わせることにより比較的広い周波数範囲において高い磁気シールド性能を発揮する開放型シールド構造とすることができる。
(A) The connecting magnetic body 26z attached to the C-shaped magnetic plate 20z is opposed to the door magnetic plate 22, and the C-shaped magnetic plate 20z and the door magnetic plate 22 are brought into surface contact with each other when the door 12 is closed. The door opening 11 can be magnetically closed while ensuring the continuity of the body circuit.
(B) Further, the door magnetic plate 22 is formed by a plurality of I-shaped magnetic plates 23z1, 23z2,... Provided while being insulated from each other along the intersecting line with the plurality of planes Pz1, Pz2,. And each of the C-shaped magnetic plate 20z and the I-shaped magnetic plate 23z are magnetically joined to each other while being insulated from each other, so that the magnetic flux flowing in each of the magnetic circuits is not disturbed. 11 can be magnetically closed.
(C) By magnetically closing the door opening 11 without disturbing the magnetic flux flowing in the magnetic circuit, a sufficient magnetic shielding effect can be obtained in the entire inner space when the door 12 is closed.
(D) Further, a C-shaped conductor plate 30z that is cut by the door opening 11 while surrounding the space 1 is provided at intervals dz between the plurality of C-shaped magnetic plates 20z, and a conductor opening frame 32 is provided around the inside of the opening 11. By fixing and electrically joining both ends of the cut portion of the C-shaped conductor plate 30z to the conductor opening frame 32, an open shield structure combining a magnetic circuit and a conductor circuit can be obtained.
(E) While the open shield structure with a magnetic circuit can degrade the magnetic shield performance at high frequencies, the open shield structure with a conductor circuit improves the magnetic shield performance at high frequencies. Thus, an open type shield structure that exhibits high magnetic shielding performance in a relatively wide frequency range can be obtained.
以下,添付図面を参照して本発明を実施するための形態及び実施例を説明する。
図1は,扉開口11を有する磁気シールド対象空間(例えば磁気シールドルーム)1に本発明の扉付き開放型シールド構造を適用した実施例を示す。図示例の開放型シールド構造は,図1(A)のように扉12と平行に磁気シールド対象空間1を貫く第1方向軸Azと所定間隔dzで交差する複数の平行な平面Pz1,Pz2,……を想定し,図1(B)に示すように,その平面Pz1,Pz2,……の上にそれぞれ所定帯幅Wcで空間1を囲むように配置した第1C字型磁性板20z1,20z2,……と,扉12上に第1方向軸Azと平行に配置した扉磁性板22と,C字型磁性板20z1,20z2,……の各々に扉磁性板22と対向するように取り付けた繋ぎ磁性体26z,26z,……とにより構成されている。図示例では各平面Pxを第1方向軸Azと直交させているが,交差角度は直交以外とすることも可能である。また,第1方向軸Azを通す対象空間1内の中心点Oは,例えば対象空間1内の嫌磁気装置の設置位置とすることができる。 FIG. 1 shows an embodiment in which an open shield structure with a door of the present invention is applied to a magnetic shield target space 1 (for example, a magnetic shield room) 1 having a door opening 11. As shown in FIG. 1A, the open type shield structure of the illustrated example includes a plurality of parallel planes Pz1, Pz2, and a first direction axis Az that penetrates the magnetic shield target space 1 in parallel with the door 12 and intersects at a predetermined interval dz. .., And as shown in FIG. 1B, the first C-shaped magnetic plates 20z1, 20z2 are arranged on the planes Pz1, Pz2,... So as to surround the space 1 with a predetermined band width Wc. ,... Are attached on the door 12 so as to face the door magnetic plate 22 on the door magnetic plate 22 arranged in parallel with the first direction axis Az and the C-shaped magnetic plates 20z1, 20z2,. The connecting magnetic bodies 26z, 26z,... In the illustrated example, each plane Px is orthogonal to the first direction axis Az, but the crossing angle may be other than orthogonal. Further, the center point O in the target space 1 passing through the first direction axis Az can be set, for example, as the installation position of the anaerobic device in the target space 1.
図示例のC字型磁性板20zは,図1(C)に示すように各平面Pz上において空間1を囲みつつ扉開口11の部分で切断されたものであり,例えば図13(A)と同様に透磁率μの高いPCパーマロイその他の帯状磁性板2を用い,対象空間1の内面と各平面Pzとの交差線に沿って帯状磁性板2を多角形状に配置して接合することにより作成できる。望ましくは,C字型磁性板20を構成する帯状磁性板2を,複数のPCパーマロイ製薄板と絶縁性薄帯材とを交互に重ね合わせて積層した積層磁性板とする。PCパーマロイの磁気特性は薄いほど高いことが知られており,さらに絶縁性薄帯材を介して必要な板厚tに積層することで断面に流れる渦電流(渦電流損)を小さく抑え,高周波数域における磁気シールド性能の低下を抑えることができる。絶縁性薄帯材の一例は,シート状又はフィルム状(厚さ30μm以下)の紙や樹脂である。 The C-shaped magnetic plate 20z in the illustrated example is cut at the portion of the door opening 11 while surrounding the space 1 on each plane Pz as shown in FIG. 1C. For example, as shown in FIG. Similarly, it is made by using a PC permalloy or other strip-shaped magnetic plate 2 having a high magnetic permeability μ and arranging the strip-shaped magnetic plate 2 in a polygonal shape and joining along the intersecting line between the inner surface of the target space 1 and each plane Pz. it can. Desirably, the strip-shaped magnetic plate 2 constituting the C-shaped magnetic plate 20 is a laminated magnetic plate in which a plurality of PC permalloy thin plates and insulating thin strips are alternately stacked. It is known that the magnetic properties of PC permalloy are higher as they are thinner. Furthermore, by laminating them to the required plate thickness t via an insulating ribbon, the eddy current flowing in the cross section (eddy current loss) is suppressed to a low level. A decrease in magnetic shield performance in the frequency range can be suppressed. An example of the insulating ribbon material is paper or resin in the form of a sheet or film (thickness of 30 μm or less).
また扉12上の扉磁性板22は,図1(D)に示すように,第1方向軸Azと交差する各平面Pz1,Pz2,……と扉本体12との交線に沿ってそれぞれ,相互に絶縁しつつ扉本体12上に配置した複数の帯状の第1I字型磁性板23z1,23z2,……とすることができる。例えば扉本体12を非磁性ステンレス(SUS)製とし,その上にC字型磁性板20zと同様の帯状磁性板2を固定してI字型磁性板23zとし,I字型磁性板23zの相互間に電気絶縁性を確保する。好ましくは,I字型磁性板23zを,C字型磁性板20zと同じ帯幅及び板厚のPCパーマロイ製薄板を絶縁性薄帯材と交互に重ね合わせて積層した積層磁性板とする。C字型磁性板20zとI字型磁性板23zとを同じ帯幅及び板厚の帯状磁性板とすることにより,後述するように,両者を磁気的に結合した磁性体回路に流れる磁束の乱れを小さく抑えることができる。ただし,扉磁性板22はI字型磁性板23zに限定されず,例えば図1(F)に示すように,第1方向軸Azと平行な扉12の面上に設けたプレート状磁性板24とすることも可能である。 Further, as shown in FIG. 1D, the door magnetic plate 22 on the door 12 is respectively along the intersection line between the planes Pz1, Pz2,... Intersecting the first direction axis Az and the door body 12. A plurality of strip-shaped first I-shaped magnetic plates 23z1, 23z2,... Arranged on the door body 12 while being insulated from each other. For example, the door body 12 is made of non-magnetic stainless steel (SUS), and a belt-like magnetic plate 2 similar to the C-shaped magnetic plate 20z is fixed thereon to form an I-shaped magnetic plate 23z. Ensure electrical insulation between them. Preferably, the I-shaped magnetic plate 23z is a laminated magnetic plate in which PC permalloy thin plates having the same band width and thickness as the C-shaped magnetic plate 20z are alternately stacked with an insulating thin strip material. By making the C-shaped magnetic plate 20z and the I-shaped magnetic plate 23z into strip-shaped magnetic plates having the same band width and thickness, as will be described later, turbulence of magnetic flux flowing in the magnetic circuit that magnetically couples the two is described later. Can be kept small. However, the door magnetic plate 22 is not limited to the I-shaped magnetic plate 23z. For example, as shown in FIG. 1F, the plate-like magnetic plate 24 provided on the surface of the door 12 parallel to the first direction axis Az. It is also possible.
C字型磁性板20z上に取り付ける繋ぎ磁性体26zは,各C字型磁性板20zの切断部分に臨む両端に取り付けられるものであり,C字型磁性板20zの帯幅面と直角に配置された扉12上の扉磁性板22と対向するように,例えば図1(E)に示すような磁性板製のL字形アングルとすることができる。繋ぎ磁性体26zを介してC字型磁性板20zと扉磁性板22とを対向させて面接触させることにより,扉12の閉鎖時に磁性体回路の連続性を確保して扉開口11を磁気的に閉鎖することができる。 The connecting magnetic body 26z attached on the C-shaped magnetic plate 20z is attached to both ends facing the cut portion of each C-shaped magnetic plate 20z, and is disposed at right angles to the band width surface of the C-shaped magnetic plate 20z. For example, an L-shaped angle made of a magnetic plate as shown in FIG. 1E can be used so as to face the door magnetic plate 22 on the door 12. By making the C-shaped magnetic plate 20z and the door magnetic plate 22 face each other through the connecting magnetic body 26z, the continuity of the magnetic circuit is ensured when the door 12 is closed, and the door opening 11 is made magnetic. Can be closed.
図6(A)は,図1(D)に示す第1I字型磁性板23zを扉磁性板22とした扉付き開放型シールド構造において,X方向及びY方向の磁場Mを印加した時の内側空間1の評価点S1〜S5における磁場強度を上述した数値シミュレーション(三次元非線形磁場解析)により求め,開口11を設ける前の評価点S1〜S5の磁場強度(磁場強度の基準値)と比較した検証実験の結果を示す。図6(A)のグラフと図11(A2)のグラフとの比較から,X方向磁場に対して内側空間1の磁場を全体的に小さくすることができることが分かる。また,Y方向磁場に対しても,開口近くの評価点S2の磁場が若干大きくなるものの,やはり内側空間1の磁場を全体的に小さくすることができる。この実験結果から,複数のI字型磁性板23zの各々を相互に絶縁しつつC字型磁性板20zと1対1で磁気的に接合することにより,各磁性体回路に流れる磁束を乱すことなく扉開口11を磁気的に閉鎖することができ,その結果として内側空間の全体において十分な磁気シールド効果を得られることが分かる。 FIG. 6A shows an inner side when a magnetic field M in the X direction and the Y direction is applied in the open type shield structure with a door in which the first I-shaped magnetic plate 23z shown in FIG. The magnetic field strength at the evaluation points S1 to S5 in the space 1 is obtained by the above-described numerical simulation (three-dimensional nonlinear magnetic field analysis), and compared with the magnetic field strength (reference value of the magnetic field strength) at the evaluation points S1 to S5 before the opening 11 is provided. The result of a verification experiment is shown. From the comparison between the graph of FIG. 6A and the graph of FIG. 11A2, it can be seen that the magnetic field in the inner space 1 can be reduced as a whole with respect to the magnetic field in the X direction. Further, although the magnetic field at the evaluation point S2 near the opening is slightly increased with respect to the Y-direction magnetic field, the magnetic field in the inner space 1 can be reduced as a whole. From this experimental result, the magnetic flux flowing in each magnetic circuit is disturbed by magnetically joining each of the plurality of I-shaped magnetic plates 23z with the C-shaped magnetic plate 20z in a one-to-one manner while being insulated from each other. It can be seen that the door opening 11 can be magnetically closed, and as a result, a sufficient magnetic shielding effect can be obtained in the entire inner space.
また図6(B)は,扉磁性板22として,図1(D)に示す第1I字型磁性板23zに代えて,図1(F)に示すプレート状磁性板24を用いた開放型シールド構造にX方向及びY方向の磁場Mを印加した時の内側空間1の評価点S1〜S5における磁場強度を,数値シミュレーションにより求めた検証実験結果を示す。図6(B)のグラフと図11(A2)のグラフとの比較から,X方向磁場に対して内側空間1の評価点S1〜S5による磁場のバラツキが大きく,中心点である評価点S1及び開口から離れた評価点S3の磁場は非常に小さくなっているが,開口近くの評価点S2の磁場は大きくなることが分かる。また,Y方向磁場に対しても,評価点S1〜S5による磁場のバラツキが大きく,評価点S1及びS3の磁場は小さくなっているが,X方向磁場に対する場合よりも全体的に内側空間1の磁場が大きくなっている。この実験結果から,扉開口11をプレート状磁性板24で塞いた場合は,磁性体配置のバランスが崩れて磁性体回路に流れる磁束に偏りが生じるために,内部空間1の磁場が全体的に増大すると考えられる。ただし,図6(B)は,内側空間1の特定部位(例えば中心点である評価点S1)の磁場を小さく抑える場合には,I字型磁性板23zに代えてプレート状磁性板24を用いることが有効であることを示している。 FIG. 6B shows an open-type shield that uses a plate-like magnetic plate 24 shown in FIG. 1F as the door magnetic plate 22 in place of the first I-shaped magnetic plate 23z shown in FIG. 1D. The verification experiment result which calculated | required the magnetic field intensity in evaluation point S1-S5 of the inner space 1 when the magnetic field M of a X direction and a Y direction was applied to the structure by numerical simulation is shown. From the comparison between the graph of FIG. 6B and the graph of FIG. 11A2, the variation of the magnetic field due to the evaluation points S1 to S5 in the inner space 1 with respect to the magnetic field in the X direction is large, and the evaluation point S1 that is the central point It can be seen that the magnetic field at the evaluation point S3 far from the opening is very small, but the magnetic field at the evaluation point S2 near the opening is large. Also, the magnetic field variation at the evaluation points S1 to S5 is large with respect to the Y-direction magnetic field, and the magnetic fields at the evaluation points S1 and S3 are small. The magnetic field is increasing. From this experimental result, when the door opening 11 is closed by the plate-shaped magnetic plate 24, the balance of the magnetic material arrangement is lost and the magnetic flux flowing in the magnetic material circuit is biased. It is thought to increase. However, FIG. 6B uses a plate-like magnetic plate 24 in place of the I-shaped magnetic plate 23z in order to keep the magnetic field of a specific part (for example, the evaluation point S1 as the central point) of the inner space 1 small. Shows that it is effective.
本発明の扉付き開放型シールド構造は,必要に応じて,C字型磁性板20zと扉磁性板22とを磁気的に接合して一体とするために,繋ぎ磁性体26zを介して両者を対面させると共に,適当な圧力を加えて接触させることができる。例えば,従来の密閉型シールド構造の磁気シールド扉に用いられている押圧機構(例えばローラ絞りハンドル,ロッドを介したサイドローラ絞り等で構成される機構)を転用することにより,扉磁性板22に押圧力を加えてC字型磁性板20zとの密着度を高めることができる。 In the open shield structure with a door of the present invention, if necessary, the C-shaped magnetic plate 20z and the door magnetic plate 22 are magnetically joined and integrated with each other via a connecting magnetic body 26z. They can be brought into contact with each other by applying appropriate pressure. For example, by diverting a pressing mechanism (for example, a mechanism constituted by a roller throttle handle, a side roller throttle via a rod, etc.) used in a conventional magnetic shield door with a hermetic shield structure, the door magnetic plate 22 is used. A pressing force can be applied to increase the degree of adhesion with the C-shaped magnetic plate 20z.
こうして本発明の目的である「内側空間の全体において十分な磁気シールド効果を得ることができる扉付き開放型磁気シールド構造」の提供が達成できる。 Thus, the provision of an “open type magnetic shield structure with a door capable of obtaining a sufficient magnetic shielding effect in the entire inner space”, which is an object of the present invention, can be achieved.
好ましくは,図2(A)に示すように,磁気シールド対象空間1を扉12と平行に貫く第2方向軸Axと所定間隔dxで交差する複数の平行な平面Px1,Px2,……を想定し,その平面Px1,Px2,……上にそれぞれ,所定帯幅Wcで空間1を囲みつつ扉開口11で切断された帯状の第2C字型磁性板20x1,20x2,……を設け,空間1の周囲に図1(B)の第1C字型磁性板20z1,20z2,……と図2(B)の第2C字型磁性板20x1,20x2,……とを入れ子状に配置する。図2において第2方向軸Axは,図1の第1方向軸Azと異なる方向,例えば方向軸Azと垂直な方向に選択する。また,各平面Pxと第2方向軸Axとの交差角度は直交以外とすることも可能である。 Preferably, as shown in FIG. 2A, a plurality of parallel planes Px1, Px2,... Intersecting the second direction axis Ax penetrating the magnetic shield target space 1 in parallel with the door 12 at a predetermined interval dx is assumed. On the planes Px1, Px2,..., Band-shaped second C-shaped magnetic plates 20x1, 20x2,... Cut around the door opening 11 while surrounding the space 1 with a predetermined band width Wc are provided. 1C-shaped magnetic plates 20z1, 20z2,... In FIG. 1B and second C-shaped magnetic plates 20x1, 20x2,. In FIG. 2, the second direction axis Ax is selected in a direction different from the first direction axis Az in FIG. 1, for example, a direction perpendicular to the direction axis Az. Further, the intersection angle between each plane Px and the second direction axis Ax may be other than orthogonal.
図2(B)に示すように,第2C字型磁性板20xの各々の切断部分の両端には,第1C字型磁性板20zと同様に,扉磁性板22と対向するように繋ぎ磁性体26xを取り付ける。そして,繋ぎ磁性体26xを介してC字型磁性板20xと扉磁性板22とを対向させて面接触させることにより,扉12の閉鎖時に磁性体回路の連続性を確保する。扉磁性板22は,図1(F)のようなプレート状磁性板24とすることも可能であるが,図示例のように第2方向軸Axと交差する複数の平面Px1,Px2,……と扉12との交線に沿ってそれぞれ相互に絶縁しつつ設けた複数の帯状の第2I字型磁性板23x(23x1,23x2,……)とすることが望ましい。 As shown in FIG. 2 (B), both ends of each cut portion of the second C-shaped magnetic plate 20x are joined to face the door magnetic plate 22 in the same manner as the first C-shaped magnetic plate 20z. Install 26x. Then, the C-shaped magnetic plate 20x and the door magnetic plate 22 are opposed to each other through the connecting magnetic body 26x and are brought into surface contact with each other, thereby ensuring the continuity of the magnetic circuit when the door 12 is closed. The door magnetic plate 22 may be a plate-like magnetic plate 24 as shown in FIG. 1 (F), but a plurality of planes Px1, Px2,... Intersecting with the second direction axis Ax as shown in the example. And a plurality of strip-shaped second I-shaped magnetic plates 23x (23x1, 23x2,...) Provided while being insulated from each other along the line of intersection with the door 12.
図1(A)の開放型シールド構造ではZ方向(第1方向軸Azの方向)の外乱磁場Mに対して対応できないが,第1C字型磁性板20z及び第2C字型磁性板20xを組み合わせた図2(A)の開放型シールド構造によれば,Z方向の外来磁場Mに対しても高い磁気シールド効果が期待できる。また,相互に絶縁された図1(B)の第1I字型磁性板23zと図2(B)の第2I字型磁性板23xとにより扉磁性板22を構成し,複数のI字型磁性板23z,23xの各々を相互に絶縁しつつC字型磁性板20z,20xと1対1で磁気的に接合することにより,各磁性体回路に流れる磁束を乱すことなく扉開口11を磁気的に閉鎖することができる。 Although the open shield structure of FIG. 1A cannot cope with the disturbance magnetic field M in the Z direction (the direction of the first direction axis Az), the first C-shaped magnetic plate 20z and the second C-shaped magnetic plate 20x are combined. According to the open type shield structure of FIG. 2A, a high magnetic shielding effect can be expected even with respect to the external magnetic field M in the Z direction. Also, the door magnetic plate 22 is constituted by the first I-shaped magnetic plate 23z of FIG. 1B and the second I-shaped magnetic plate 23x of FIG. The plates 23z and 23x are magnetically joined to the C-shaped magnetic plates 20z and 20x on a one-to-one basis while insulating the plates 23z and 23x from each other, thereby magnetically opening the door opening 11 without disturbing the magnetic flux flowing in each magnetic circuit. Can be closed.
更に好ましくは,図3(A)に示すように,磁気シールド対象空間1を扉12と垂直に貫く第3方向軸Ayと所定間隔dyで交差する複数の平行な平面Py1,Py2,……を想定し,その平面Py1,Py2,……上にそれぞれその空間1を囲む環帯状磁性板20y1,20y2,……を設け,空間1の周囲に図1(B)の第1C字型磁性板20z1,20z2,……と図3(B)の環帯状磁性板20y1,20y2,……との2層を入れ子状に配置する。或いは,空間1の周囲に図1(B)の第1C字型磁性板20z1,20z2,……と図2(B)の第2C字型磁性板20x1,20x2,……と図3(B)の環帯状磁性板20y1,20y2,……との3層を入れ子状に配置する。環帯状磁性板20yは扉開口11と交差しないので,切断部分のない環状に閉じた帯状磁性板とすることができる。 More preferably, as shown in FIG. 3A, a plurality of parallel planes Py1, Py2,... Intersecting with the third direction axis Ay penetrating the magnetic shield target space 1 perpendicularly to the door 12 at a predetermined interval dy. Assuming that ring-shaped magnetic plates 20y1, 20y2,... Surrounding the space 1 are provided on the planes Py1, Py2,..., Respectively, and the first C-shaped magnetic plate 20z1 of FIG. , 20z2,... And two layers of the ring-shaped magnetic plates 20y1, 20y2,. Alternatively, the first C-shaped magnetic plates 20z1, 20z2,... Of FIG. 1B and the second C-shaped magnetic plates 20x1, 20x2,... Of FIG. The three layers of the ring-shaped magnetic plates 20y1, 20y2,. Since the ring-shaped magnetic plate 20y does not intersect the door opening 11, it can be a band-shaped magnetic plate closed in an annular shape without a cut portion.
図3において,第3方向軸Ayは,図1の第1方向軸Az及び図2の第2方向軸Axの何れとも異なる方向,例えば方向軸Az,Axの何れとも垂直な方向に選択する。また,各平面Pyと第3方向軸Ayとの交差角度を直交以外とすることも可能である。図2(A)の開放型シールド構造でも方向の決まっていない(全方向から到来しうる)外乱磁場Mを遮蔽できるが,シールド対象空間1を囲む全ての平面(X−Z平面,X−Y平面,Y−Z平面)にそれぞれ2層の磁性体回路が配置されている図3(A)の開放型シールド構造によれば,方向の決まっていない外乱磁場Mに対する高い磁気シールド効果が期待できる。 In FIG. 3, the third direction axis Ay is selected in a direction different from any of the first direction axis Az in FIG. 1 and the second direction axis Ax in FIG. 2, for example, a direction perpendicular to both of the direction axes Az and Ax. In addition, the crossing angle between each plane Py and the third direction axis Ay may be other than orthogonal. The open shield structure of FIG. 2A can shield the disturbance magnetic field M whose direction is not determined (can come from all directions), but all the planes surrounding the shield target space 1 (XZ plane, XY). According to the open type shield structure of FIG. 3A in which two layers of magnetic circuits are arranged on each of the plane and the YZ plane, a high magnetic shielding effect against the disturbance magnetic field M whose direction is not determined can be expected. .
以上,磁性体回路を用いた扉付き開放型磁気シールド構造について説明したが,磁性体回路を用いた開放型磁気シールド構造は,外乱磁場が直流ないし数Hz以下の低周波数の交流であれば略設計どおりの磁気シールド性能を示すものの,10Hz〜商用周波数以上の高周波数域になるとシールド性能が劣化する問題点がある。図12(B)のグラフは,図10(A1)及び(B1)に示す開放型シールド構造を図12(A)の環状コイルLの中央部に設置し,周波数を1Hz,10Hz,60Hz,200Hzに切り替えながら略一様磁場M(10μT)を印加したときの内側中心の磁場強度の測定値を示す。同グラフは,印加磁場Mの周波数が高くなるに従って開放型シールド構造の内側中心の磁場強度が大きくなること,つまり磁気シールド性能が低下することを示している。高周波数域において磁気シールド性能が劣化する原因は,環帯状磁性板4(磁性体回路)に電磁誘導によって渦電流(渦電流損)が生じるからと推測される。 The open type magnetic shield structure with a door using a magnetic circuit has been described above. However, an open type magnetic shield structure using a magnetic circuit is not necessary if the disturbance magnetic field is a direct current or a low frequency alternating current of several Hz or less. Although the magnetic shield performance is as designed, there is a problem that the shield performance deteriorates in the high frequency range from 10 Hz to the commercial frequency or higher. In the graph of FIG. 12B, the open type shield structure shown in FIGS. 10A1 and 10B1 is installed at the center of the annular coil L of FIG. 12A, and the frequencies are 1 Hz, 10 Hz, 60 Hz, and 200 Hz. The measured value of the magnetic field strength at the inner center when a substantially uniform magnetic field M (10 μT) is applied while switching to is shown. The graph shows that as the frequency of the applied magnetic field M increases, the magnetic field strength at the inner center of the open shield structure increases, that is, the magnetic shield performance decreases. The reason why the magnetic shield performance deteriorates in the high frequency range is presumed to be that eddy current (eddy current loss) is generated in the ring-shaped magnetic plate 4 (magnetic circuit) by electromagnetic induction.
他方,電磁誘導によって導体板に流れる渦電流を利用した磁気シールド構造は,周波数が高いほど有効に働くことが知られている(非特許文献1参照)。そこで,図14(A)に示すように,外寸法280mm×280mm,板厚5mmの銅製及びアルミニウム製の導体板を用いて幅30mmの環帯状導体板6を作成し,その環帯状導体板6(導体回路)を板厚方向間隔d=60mmで5段重ねた開放型シールド構造を図12(A)の環状コイルLの中央部に中心軸方向が磁場方向と一致するように設置し,周波数1Hz,10Hz,60Hz,200Hzの略一様磁場M(10μT)を印加したときの内側中心の磁場強度(実験値)を測定する実験を行った。図14(B)の実験結果は,印加磁場Mの周波数が高くなるに従って開放型シールド構造の内側中心の磁場強度が小さくなること,つまり磁気シールド性能が向上することを示している。また,渦電流に基づく数値シミュレーション(三次元非線形磁場解析)により同じ開放型シールド構造の内側中心の磁場強度を解析したところ,図14(B)に示すように実験値と概ね一致する解析値が得られた。なお,同グラフはアルミニウムよりも導電率の大きい銅の磁気シールド性能が高いことを示している。 On the other hand, it is known that a magnetic shield structure using an eddy current flowing in a conductor plate by electromagnetic induction works more effectively as the frequency is higher (see Non-Patent Document 1). Therefore, as shown in FIG. 14A, a ring-shaped conductor plate 6 having a width of 30 mm is prepared using a copper and aluminum conductor plate having an outer dimension of 280 mm × 280 mm and a plate thickness of 5 mm. An open type shield structure in which (conductor circuit) is stacked in five steps at a plate thickness direction interval d = 60 mm is installed at the center of the annular coil L in FIG. 12A so that the central axis direction coincides with the magnetic field direction. An experiment was conducted to measure the magnetic field strength (experimental value) at the inner center when a substantially uniform magnetic field M (10 μT) of 1 Hz, 10 Hz, 60 Hz, and 200 Hz was applied. The experimental results in FIG. 14B show that the magnetic field strength at the inner center of the open shield structure decreases as the frequency of the applied magnetic field M increases, that is, the magnetic shield performance improves. In addition, when the magnetic field strength at the inner center of the same open shield structure was analyzed by numerical simulation based on eddy current (three-dimensional nonlinear magnetic field analysis), an analytical value almost in agreement with the experimental value as shown in FIG. Obtained. This graph shows that the magnetic shielding performance of copper, which has higher conductivity than aluminum, is higher.
環帯状磁性板4(磁性体回路)を用いた図10(A1)及び(B1)の開放型シールド構造の磁気シールド性能は印加磁場Mの周波数が高くなると低下するのに対し(図12(B)参照),環帯状導体板6(導体回路)を用いた図14(A)の開放型シールド構造の磁気シールド性能は印加磁場Mの周波数が高くなると向上することから(図14(B)参照),両者を組み合わせて配置することにより,高周波数域(10Hz〜商用周波数以上)の外乱磁場Mに対してもシールド性能が劣化しない開放型シールド構造とすることができる(本発明者らの先願である特願2012−236166号参照)。 The magnetic shield performance of the open shield structure shown in FIGS. 10A1 and 10B1 using the ring-shaped magnetic plate 4 (magnetic circuit) decreases as the frequency of the applied magnetic field M increases (FIG. 12B 14), the magnetic shield performance of the open shield structure of FIG. 14A using the ring-shaped conductor plate 6 (conductor circuit) is improved as the frequency of the applied magnetic field M is increased (see FIG. 14B). ), And by combining them, it is possible to obtain an open shield structure in which the shield performance is not deteriorated even with respect to a disturbance magnetic field M in a high frequency range (10 Hz to a commercial frequency or higher). (See Japanese Patent Application No. 2012-236166).
図4は,磁性体回路と導体回路とを組み合わせた本発明の扉付き開放型シールド構造の実施例を示す。図示例の開放型シールド構造は,シールド対象空間1の周囲に図1(B)の第1C字型磁性板20z1,20z2,……と図2(B)の第2C字型磁性板20x1,20x2,……と図3(B)の環帯状磁性板20y1,20y2,……とを入れ子状に配置すると共に,そのうち図4(A)に示すように扉12と平行に磁気シールド対象空間1を貫く第1方向軸Azと所定間隔dzで交差する複数の第1C字型磁性板20z1,20z2,……の間隔dzにそれぞれ,図4(B)に示すように空間1を囲みつつ扉開口11で切断された帯状の第1C字型導体板30z1,30z2,……を配置し,扉開口11の内側周囲に導体開口枠32を固定し,各第1C字型導体板30z1,30z2,……の切断部分の両端を導体開口枠32に電気的に接合したものである。 FIG. 4 shows an embodiment of an open type shield structure with a door according to the present invention in which a magnetic circuit and a conductor circuit are combined. The open type shield structure of the illustrated example has a first C-shaped magnetic plate 20z1, 20z2,... In FIG. 1B and a second C-shaped magnetic plate 20x1, 20x2 in FIG. ,... And the annular belt-like magnetic plates 20y1, 20y2,... Of FIG. 3B are arranged in a nested manner, and the magnetic shield target space 1 is parallel to the door 12 as shown in FIG. As shown in FIG. 4B, the door opening 11 surrounds the space 1 at intervals dz of the plurality of first C-shaped magnetic plates 20z1, 20z2,... Intersecting the first direction axis Az that penetrates at a predetermined interval dz. The first C-shaped conductor plates 30z1, 30z2,..., Which are cut in the above, are arranged, the conductor opening frame 32 is fixed around the inside of the door opening 11, and the first C-shaped conductor plates 30z1, 30z2,. Electrically connect both ends of the cut portion to the conductor opening frame 32 One in which engaged.
C字型導体板30zは,例えば図4(C)に示すように,対象空間1の内面と第1方向軸Azと交差する平面Pxと対象空間1の内面との交差線に沿って,帯幅Wmで適当な長さの複数の帯状導体板を接合することにより作成できる。接合部の接触抵抗により磁気シールド効果が大きく異なりうるため,複数の帯状導体板を接合する方法に代えて,1枚の大きな導体板からC字型導体板30zをくり抜いて作成することも可能である。C字型導体板30zの材質は,例えば銅,アルミニウム等の適当な導体板から対象空間1に必要なシールド性能に応じて適宜選択できるが,上述したように導電率が大きいとシールド性能も高いことから,導電率の大きい材質とすることが望ましい。 For example, as shown in FIG. 4C, the C-shaped conductor plate 30z is formed along a cross line between a plane Px intersecting the inner surface of the target space 1 and the first direction axis Az and the inner surface of the target space 1. It can be created by joining a plurality of strip-shaped conductor plates having a width Wm and an appropriate length. Since the magnetic shielding effect can vary greatly depending on the contact resistance of the joint, it is possible to cut out the C-shaped conductor plate 30z from one large conductor plate instead of the method of joining a plurality of strip-like conductor plates. is there. The material of the C-shaped conductor plate 30z can be appropriately selected according to the shielding performance required for the target space 1 from an appropriate conductor plate such as copper or aluminum, but as described above, the shielding performance is high when the conductivity is large. Therefore, it is desirable to use a material with high conductivity.
また,扉開口11に固定する導体開口枠32は,C字型導体板30zと同じ導体板製とすることができる。例えば,図4(D)に示すように,各C字型導体板30zの切断部分に臨む両端にL字形アングル等の繋ぎ導体36z,36z,……を取り付け,その繋ぎ導体36zによって各C字型導体板30zの切断部分の両端を導体開口枠32に電気的に接合することにより,導体回路の連続性を確保して扉開口11を電気的に閉鎖することができる。接合部の接触抵抗により磁気シールド効果が大きく異なりうるため,例えばC字型導体板30zの切断部分の両端と導体開口枠32との接合部分にそれぞれ鏡状仕上げ面を形成し,その鏡面仕上げ面同士を重ね合わせて押圧することにより接合することが望ましい(本発明者らの先願である特願2012−276652号参照)。 Moreover, the conductor opening frame 32 fixed to the door opening 11 can be made of the same conductor plate as the C-shaped conductor plate 30z. For example, as shown in FIG. 4D, connecting conductors 36z, 36z,... Such as L-shaped angles are attached to both ends facing the cut portion of each C-shaped conductor plate 30z, and each C-shape is connected by the connecting conductor 36z. By electrically joining both ends of the cut portion of the mold conductor plate 30z to the conductor opening frame 32, the continuity of the conductor circuit can be secured and the door opening 11 can be electrically closed. Since the magnetic shield effect can vary greatly depending on the contact resistance of the joint portion, for example, a mirror-like finished surface is formed at each joint portion between the both ends of the cut portion of the C-shaped conductor plate 30z and the conductor opening frame 32. It is desirable to join them by overlapping each other and pressing them (see Japanese Patent Application No. 2012-276652 which is the prior application of the present inventors).
図7(S1)〜(S5)のグラフは,外寸法280mm×280mm,板厚5mmの銅製の環帯状導体板6を用いた図14(A)に示す開放型シールド構造(開口なし),94mm幅の扉開口11を設けたままの開放型シールド構造(枠なし),同じく94mm幅の扉開口11の内側周囲に導体開口枠32を設けた図4(B)に示す開放型シールド構造(枠5mm,枠10mmの2モデル)の4つのモデルを用い,それぞれ中心軸方向の磁場Mを印加した時の内側空間1の評価点S1〜S5における磁場強度を,上述した数値シミュレーション(三次元非線形磁場解析)により求めた検証実験の結果を示す。図7のグラフから,扉開口11を開放したまま(枠なし)では渦電流が流れないため,磁気シールド効果が得られないことが分かる。また,開口枠32を設けた場合は,開口近くの評価点S2において磁場が若干大きくなっている点を除き,開口のない場合に近い磁気シールド性能が得られることが分かる。 The graphs of FIGS. 7 (S1) to (S5) show an open type shield structure (no opening) shown in FIG. 14 (A) using a copper ring-shaped conductor plate 6 having an outer dimension of 280 mm × 280 mm and a thickness of 5 mm, 94 mm. An open type shield structure (with no frame) with the width door opening 11 provided, and an open type shield structure (frame with the same structure shown in FIG. 4B) in which a conductor opening frame 32 is provided around the inner side of the door opening 11 with a width of 94 mm. 4 models (2 models of 5 mm and 10 mm of frame) are used, and the magnetic field strength at the evaluation points S1 to S5 in the inner space 1 when the magnetic field M in the central axis direction is applied to each of the numerical simulations (three-dimensional nonlinear magnetic field) The result of the verification experiment obtained by (Analysis) is shown. From the graph of FIG. 7, it can be seen that the magnetic shield effect cannot be obtained because the eddy current does not flow when the door opening 11 is left open (no frame). In addition, when the opening frame 32 is provided, it can be seen that a magnetic shield performance close to that without the opening can be obtained except that the magnetic field is slightly increased at the evaluation point S2 near the opening.
図4(A)の扉付き開放型シールド構造において,第1C字型導体板30z及び導体開口枠32からなる導体回路は,その中心軸方向(第1方向軸Azの方向)の外乱磁場Mに対してシールド性能を発揮する。また,第2C字型磁性板20x及び扉磁性板22からなる磁性体回路,環帯状磁性板20yからなる磁性体回路も,それぞれ第1方向軸Azの外乱磁場Mに対してシールド性能を発揮する。従って,図4(B)のように磁気シールド対象空間1を囲むC字型導体板30zを配置すると共に扉12に導体開口枠32を配置することにより,第1方向軸Azの方向から到来する外乱磁場Mに対する磁性体回路の高周波数域における磁気シールド性能の低下を,導体回路の高周波数域における磁気シールド性能の向上によって補うことができ,第1方向軸Azの方向から到来する高周波数域(10Hz〜商用周波数以上)の外乱磁場Mに対してもシールド性能が劣化しない扉付き開放型シールド構造とすることができる。 In the open shield structure with a door in FIG. 4A, the conductor circuit composed of the first C-shaped conductor plate 30z and the conductor opening frame 32 is subjected to a disturbance magnetic field M in the central axis direction (the direction of the first direction axis Az). Shield performance is demonstrated. Further, the magnetic circuit composed of the second C-shaped magnetic plate 20x and the door magnetic plate 22 and the magnetic circuit composed of the ring-shaped magnetic plate 20y also exhibit shielding performance against the disturbance magnetic field M having the first direction axis Az. . Therefore, as shown in FIG. 4B, the C-shaped conductor plate 30z surrounding the magnetic shield target space 1 is disposed and the conductor opening frame 32 is disposed on the door 12, thereby arriving from the direction of the first direction axis Az. The decrease in magnetic shield performance in the high frequency range of the magnetic circuit against the disturbance magnetic field M can be compensated by improving the magnetic shield performance in the high frequency range of the conductor circuit, and the high frequency range coming from the direction of the first direction axis Az. It can be set as the open type shield structure with a door which shield performance does not deteriorate with respect to the disturbance magnetic field M (10 Hz-commercial frequency or more).
また,図4(A)のように第1C字型磁性板20zと第2C字型磁性板20xと環帯状磁性板20yとを入れ子状に配置したシールド対象空間において,上述した図4(B)の第1C字型導体板30zに代えて又は加えて,図5(A)に示すように扉12と平行に磁気シールド対象空間1を貫く第2方向軸Axと交差する複数の第2C字型磁性板20xの間隔dxにそれぞれ,空間1を囲みつつ扉開口11で切断された帯状の第2C字型導体板30xを配置し,各第2C字型導体板30xの切断部分の両端を導体開口枠32に電気的に接合することも可能である。第2C字型導体板30x及び導体開口枠32からなる導体回路は,その中心軸方向(第2方向軸Axの方向)の外乱磁場Mに対してシールド性能を発揮するので,図5(A)のように空間1を囲むC字型導体板30xを配置すると共に扉12に導体開口枠32を配置することにより,第2方向軸Axの方向から到来する外乱磁場Mに対する磁性体回路の高周波数域における磁気シールド性能の低下を,導体回路の高周波数域における磁気シールド性能の向上によって補うことができる。 Further, in the shield target space in which the first C-shaped magnetic plate 20z, the second C-shaped magnetic plate 20x, and the ring-shaped magnetic plate 20y are arranged in a nested manner as shown in FIG. In place of or in addition to the first C-shaped conductor plate 30z, a plurality of second C-shaped crossings intersecting the second direction axis Ax penetrating the magnetic shield target space 1 in parallel with the door 12 as shown in FIG. A band-shaped second C-shaped conductor plate 30x that is cut at the door opening 11 while surrounding the space 1 is arranged at intervals dx of the magnetic plates 20x, and both ends of the cut portions of the second C-shaped conductor plates 30x are opened to the conductor. It is also possible to electrically join the frame 32. The conductor circuit composed of the second C-shaped conductor plate 30x and the conductor opening frame 32 exhibits shielding performance against the disturbance magnetic field M in the central axis direction (direction of the second direction axis Ax). By arranging the C-shaped conductive plate 30x surrounding the space 1 and arranging the conductor opening frame 32 on the door 12, the high frequency of the magnetic circuit against the disturbance magnetic field M coming from the direction of the second direction axis Ax The decrease in magnetic shield performance in the high frequency range can be compensated by improving the magnetic shield performance in the high frequency range of the conductor circuit.
更に,図4(A)のように第1C字型磁性板20zと第2C字型磁性板20xと環帯状磁性板20yとを入れ子状に配置したシールド対象空間において,上述した図4(B)の第1C字型導体板30z及び図5(A)の第2C字型導体板30xに代えて又は加えて,図5(B)に示すように磁気シールド対象空間1を扉12と垂直に貫く第3方向軸Ayと交差する複数の環帯状磁性板20yの間隔dyにそれぞれ磁気シールド対象空間1を囲む環帯状導体板30yを設けることも可能である。環帯状導体板30yからなる導体回路は,その中心軸方向(第3方向軸Ayの方向)の外乱磁場Mに対してシールド性能を発揮するので,図5(B)のように空間1を囲む環帯状導体板30yを配置することにより,第3方向軸Ayの方向から到来する外乱磁場Mに対する磁性体回路の高周波数域における磁気シールド性能の低下を,導体回路の高周波数域における磁気シールド性能の向上によって補うことができる。 Further, as shown in FIG. 4A, in the shield object space in which the first C-shaped magnetic plate 20z, the second C-shaped magnetic plate 20x, and the ring-shaped magnetic plate 20y are arranged in a nested manner, the above-described FIG. Instead of or in addition to the first C-shaped conductor plate 30z and the second C-shaped conductor plate 30x of FIG. 5A, the magnetic shield target space 1 passes through the door 12 perpendicularly as shown in FIG. 5B. It is also possible to provide ring-shaped conductor plates 30y surrounding the magnetic shield target space 1 at intervals dy between the plurality of ring-shaped magnetic plates 20y intersecting the third direction axis Ay. The conductor circuit composed of the ring-shaped conductor plate 30y exhibits shielding performance against the disturbance magnetic field M in the central axis direction (the direction of the third direction axis Ay), and therefore surrounds the space 1 as shown in FIG. By disposing the annular belt-like conductor plate 30y, the magnetic shield performance in the high frequency region of the conductor circuit is reduced with respect to the disturbance magnetic field M coming from the direction of the third direction axis Ay. It can be compensated for by improvement.
図8(A)は,図1(B)の第1C字型磁性板20z,図2(B)の第2C字型磁性板20x,図3(B)の環帯状磁性板20y,図4(B)の第1C字型導体板30z,図5(A)の第2C字型導体板30x,及び図5(B)の環帯状導体板30yをそれぞれ周囲に配置した本発明の磁気シールドルーム1の実施例を示す。図示例は,磁気シールドルーム1における非磁性ステンレス(SUS)製の扉12の正面図を示しており,周辺壁には磁性体回路として幅50mm,厚さ0.5mmのPCパーマロイ製薄板を8枚積層した積層磁性板製(合計厚さ4mm)の第1C字型磁性板20z(外層)及び第2C字型磁性板20x(内層)が,水平方向及び垂直方向にそれぞれ200mm間隔で配置されている。また,導体回路として幅50mm,厚さ5mmの銅製の第1C字型導体板30z(外層)及び第2C字型導体板30x(内層)が,水平方向及び垂直方向にそれぞれ200mm間隔で配置されている。更に,扉12には,保持,回転,ロック(開閉)が可能な押圧機構として,従来の密閉型シールド構造の磁気シールド扉に用いられている押圧機構(例えばローラ絞りハンドル,ローラ絞りハンドル,リフトヒンジ,ロッド,サイドローラ絞り等)を取付けられている。
8A shows the first C-shaped magnetic plate 20z of FIG. 1B, the second C-shaped magnetic plate 20x of FIG. 2B, the ring-shaped magnetic plate 20y of FIG. 3B, and FIG. The magnetic shield room 1 of the present invention in which the first C-shaped conductor plate 30z of B), the second C-shaped conductor plate 30x of FIG. 5A, and the ring-shaped conductor plate 30y of FIG. Examples of The illustrated example shows a front view of a door 12 made of non-magnetic stainless steel (SUS) in the magnetic shield room 1, and a PC permalloy thin plate having a width of 50 mm and a thickness of 0.5 mm is formed on the peripheral wall as a magnetic circuit. A first C-shaped magnetic plate 20z (outer layer) and a second C-shaped magnetic plate 20x (inner layer) made of laminated magnetic plates (total thickness 4 mm) are arranged at intervals of 200 mm in the horizontal direction and the vertical direction, respectively. Yes. In addition, a copper first C-shaped conductor plate 30z (outer layer) and a second C-shaped conductor plate 30x (inner layer) having a width of 50 mm and a thickness of 5 mm are disposed as conductor circuits at intervals of 200 mm in the horizontal direction and the vertical direction, respectively. Yes. Further, the door 12 has a pressure mechanism (for example, a roller throttle handle, a roller throttle handle, a lift) used as a magnetic shield door having a conventional sealed shield structure as a pressing mechanism that can be held, rotated, and locked (opened / closed). Hinges, rods, side roller throttles, etc.) are attached.
図8(B)に示すように,扉12の外層には,図1(D)を参照して上述したように第1方向軸Azと交差する各平面Pz1,Pz2,……と扉本体12との交線に沿って複数の帯状の第1I字型磁性板23zが相互に絶縁しつつ配置されている。また,図8(C)に示すように,扉12の内層には,図2(B)に示したように第2方向軸Axと交差する各平面Px1,Px2,……と扉本体12との交線に沿って複数の帯状の第2I字型磁性板23xが相互に絶縁しつつ配置されている。I字型磁性板23z,23xは,例えばステンレス製ビス等によりPCパーマロイの磁気特性が応力によって低下しない範囲内で締め付け,扉本体12に固定することができる。更に,図8(E)に示すように,扉12の内層の内側周囲には導体開口枠32を固定され,図8(D)及び(E)に示すように,第1C字型導体板30z(外層)及び第2C字型導体板30x(内層)がそれぞれLアングル形状の繋ぎ導体36z,36xを介して導体開口枠32に電気的に接合されている。 As shown in FIG. 8B, on the outer layer of the door 12, the planes Pz1, Pz2,... Intersecting the first direction axis Az and the door main body 12 as described above with reference to FIG. A plurality of strip-shaped first I-shaped magnetic plates 23z are arranged along the line of intersection with each other while being insulated from each other. 8C, the inner layer of the door 12 includes the planes Px1, Px2,... Intersecting the second direction axis Ax as shown in FIG. A plurality of strip-shaped second I-shaped magnetic plates 23x are arranged along the crossing line while being insulated from each other. The I-shaped magnetic plates 23z and 23x can be fastened and fixed to the door body 12 with a stainless steel screw or the like within a range where the magnetic characteristics of the PC permalloy are not deteriorated by stress. Further, as shown in FIG. 8 (E), a conductor opening frame 32 is fixed around the inner side of the inner layer of the door 12, and as shown in FIGS. 8 (D) and (E), the first C-shaped conductor plate 30z. The (outer layer) and the second C-shaped conductor plate 30x (inner layer) are electrically joined to the conductor opening frame 32 via L-shaped connecting conductors 36z and 36x, respectively.
図9(A)は図8の楕円VIIIの部分拡大正面図を示し,図9(B)及び(C)は,図9(A)の線B−B及び線C−Cにおける断面図を示す。図9(C)に示すように,第1C字型磁性板20z(外層)と第1I字型磁性板23z(外層)とを磁気的に接合する繋ぎ磁性体26zは,C字型磁性板20zの切断部分の両端に取り付けられたL字形アングル部材27zと,そのアングル部材27zから扉開口11内に張り出した張出し部材28zと,扉本体12の周縁に延在する断面コ字状の被覆部材29zとにより構成されている。アングル部材27z及び張出し部材28zは,例えばステンレス製ボルトを用いて相互に面接触させながらC字型磁性板20zに磁気的に連結されている。また被覆部材29zは,例えばステンレス製ビスを用いてI字型磁性板23zに面接触させながら磁気的に連結されており,扉12の閉鎖時に張出し部材28zと面接触することにより,磁性体回路の水平方向の連続性が確保される。 9A is a partially enlarged front view of the ellipse VIII in FIG. 8, and FIGS. 9B and 9C are cross-sectional views taken along lines BB and CC in FIG. 9A. . As shown in FIG. 9C, the connecting magnetic body 26z for magnetically joining the first C-shaped magnetic plate 20z (outer layer) and the first I-shaped magnetic plate 23z (outer layer) is a C-shaped magnetic plate 20z. L-shaped angle members 27z attached to both ends of the cut portion, a projecting member 28z projecting from the angle member 27z into the door opening 11, and a covering member 29z having a U-shaped cross section extending to the periphery of the door body 12. It is comprised by. The angle member 27z and the overhang member 28z are magnetically coupled to the C-shaped magnetic plate 20z while being in surface contact with each other using, for example, a stainless steel bolt. Further, the covering member 29z is magnetically connected to the I-shaped magnetic plate 23z using, for example, a stainless steel screw and brought into surface contact with the protruding member 28z when the door 12 is closed. Horizontal continuity is ensured.
また,図9(B)に示すように,第2C字型磁性板20x(内層)と第2I字型磁性板23x(内層)とを磁気的に接合する繋ぎ磁性体26xも,C字型磁性板20xの切断部分の両端に取り付けられたL字形アングル部材27xと,そのアングル部材27xから扉開口11内に張り出した張出し部材28xと,扉本体12の周縁に延在する断面コ字状の被覆部材29xとにより構成されている。アングル部材27x及び張出し部材28xは相互に面接触しながらC字型磁性板20xに磁気的に連結されており,被覆部材29xはI字型磁性板23xに面接触しながら磁気的に連結されており,扉12の閉鎖時に張出し部材28xと面接触することにより磁性体回路の垂直方向の連続性が確保される。なお,繋ぎ磁性体26z,26xも,PCパーマロイの磁気特性が応力によって低下しない範囲内で締め付けて固定することにより,磁性体回路を磁気的に一体化することができる。 As shown in FIG. 9B, the connecting magnetic body 26x that magnetically bonds the second C-shaped magnetic plate 20x (inner layer) and the second I-shaped magnetic plate 23x (inner layer) is also C-shaped magnetic. An L-shaped angle member 27x attached to both ends of the cut portion of the plate 20x, a projecting member 28x projecting from the angle member 27x into the door opening 11, and a U-shaped covering extending to the periphery of the door body 12 It is comprised by the member 29x. The angle member 27x and the projecting member 28x are magnetically coupled to the C-shaped magnetic plate 20x while being in surface contact with each other, and the covering member 29x is magnetically coupled to the I-shaped magnetic plate 23x while being in surface contact. In addition, the continuity of the magnetic circuit in the vertical direction is ensured by surface contact with the overhanging member 28x when the door 12 is closed. The connecting magnetic bodies 26z and 26x can also be magnetically integrated by tightening and fixing the magnetic properties of the PC permalloy within a range in which the magnetic characteristics of the PC permalloy do not deteriorate due to stress.
1…磁気シールド対象空間(磁気シールドルーム)
2…帯状磁性板(短冊形磁性板) 3…シールド簾体
4…環帯状磁性板 5…開放型磁気シールド構造
6…環状導体板 8…磁気センサ
9…重ね合わせ部
11…扉開口 12…扉(扉本体)
14…扉枠体 16…拡張板
17…開口枠(磁束迂回路)
20,20x,20y…帯状C字型磁性板
22…扉磁性板 23,23x,23y…帯状磁性板
24…プレート状磁性板 26,26x,26y…繋ぎ磁性体
27…アングル部材 28…張出し部材
29…被覆部材
30,30x,30y…帯状C字型導体板
32…導体開口枠 36,36x,36y…繋ぎ導体
37…アングル部材 38…張出し部材
39…被覆部材
Ax,Ay,Az…軸 C…長さ方向中心軸
F…簾面 d…間隔
I…電流 L…コイル
M…外乱磁場 O…中心点
Px,Py,Pz…平面
Wc…環帯状磁性板の帯幅 Wm…環帯状導体板の帯幅
1 ... Magnetic shield target space (magnetic shield room)
DESCRIPTION OF SYMBOLS 2 ... Strip | belt-shaped magnetic plate (strip-shaped magnetic plate) 3 ... Shield housing | casing 4 ... Ring-band-shaped magnetic plate 5 ... Open type magnetic shield structure 6 ... Annular conductor plate 8 ... Magnetic sensor 9 ... Overlapping part 11 ... Door opening 12 ... Door (Door body)
14 ... Door frame 16 ... Expansion plate 17 ... Opening frame (magnetic flux detour)
20, 20x, 20y ... strip-shaped C-shaped magnetic plate 22 ... door magnetic plate 23, 23x, 23y ... strip-shaped magnetic plate 24 ... plate-shaped magnetic plate 26, 26x, 26y ... connecting magnetic body 27 ... angle member 28 ... projecting member 29 ... Covering member 30, 30x, 30y ... Strip C-shaped conductor plate 32 ... Conductor opening frame 36, 36x, 36y ... Connecting conductor 37 ... Angle member 38 ... Overhang member 39 ... Covering member Ax, Ay, Az ... Shaft C ... Long Center axis F ... Saddle surface d ... Spacing I ... Current L ... Coil M ... Disturbing magnetic field O ... Center point Px, Py, Pz ... Plane Wc ... Band width of ring-shaped magnetic plate Wm ... Band width of ring-shaped conductor plate
Claims (7)
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