JP2013214647A - Electromagnetic shield door - Google Patents

Electromagnetic shield door Download PDF

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JP2013214647A
JP2013214647A JP2012084761A JP2012084761A JP2013214647A JP 2013214647 A JP2013214647 A JP 2013214647A JP 2012084761 A JP2012084761 A JP 2012084761A JP 2012084761 A JP2012084761 A JP 2012084761A JP 2013214647 A JP2013214647 A JP 2013214647A
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door
door frame
resonator
gap
dielectrics
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JP5875447B2 (en
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Satoshi Yoneda
諭 米田
Kenji Hirose
健二 廣瀬
Yoshihiko Muronaga
良彦 室永
Takashi Kanemoto
貴志 金本
Naoto Oka
尚人 岡
Chiharu Miyazaki
千春 宮崎
Koichiro Misu
幸一郎 三須
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Mitsubishi Electric Corp
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Mitsubishi Electric Corp
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Abstract

PROBLEM TO BE SOLVED: To materialize an electromagnetic shield door requiring no periodical maintenance since electromagnetic shield characteristics are not deteriorated, having electromagnetic shield characteristics mainly in a high frequency band forming a GHz band or a higher one, and also having broad band electromagnetic shield characteristics.SOLUTION: This electromagnetic shield door includes a conductive door frame 2, a conductive door 1 disposed on the door frame 2, and a plurality of dielectrics disposed along the periphery of at least one of the wall surface of the door 1 and the wall surface of the door frame 2 so as not to make contact with the facing surface thereof in a gap between the door frame 2 and the door 1 in the closed state of the door 1. The dielectric includes a conductor pattern electrically connected to the door 1 or the door frame 2 while having a prescribed width on the surface thereof in the circumferential direction of the door 1 and the door 2, the prescribed width of the conductive pattern is set at the 1/4 wavelength of a frequency in a bandwidth in which electromagnetic shield characteristics are required, conductive patterns on respective surfaces of adjacent dielectrics are electrically connected by a conductor.

Description

この発明は、シールドルームの出入り口等において、電磁波の漏洩と浸入を防止するために用いられる電磁シールド扉に関するものである。   The present invention relates to an electromagnetic shield door used for preventing leakage and intrusion of electromagnetic waves at the entrance and exit of a shield room.

従来の電磁シールド扉の構成例を図15,図16に示す。図15は、従来の電磁シールド扉を示す図であり、図16は、図15の破線A−A’を通るXY断面の拡大図である。電磁シールド扉は図15,図16に示すように、扉1、扉枠2、導電性ガスケット6、ヒンジ7、開閉レバー8から構成されている。扉1と扉枠2は導電性で、ヒンジ7を介して接続され、開閉レバー8の操作により開閉可能な構造を有している。導電性ガスケット6は、導電性かつ弾性の特性を有し、扉1と扉枠2との対向面において、扉1壁面に配置されている。   A configuration example of a conventional electromagnetic shield door is shown in FIGS. FIG. 15 is a view showing a conventional electromagnetic shield door, and FIG. 16 is an enlarged view of an XY section passing through a broken line A-A ′ in FIG. 15. As shown in FIGS. 15 and 16, the electromagnetic shield door includes a door 1, a door frame 2, a conductive gasket 6, a hinge 7, and an opening / closing lever 8. The door 1 and the door frame 2 are electrically conductive, are connected via a hinge 7, and have a structure that can be opened and closed by operating an opening / closing lever 8. The conductive gasket 6 has conductive and elastic characteristics, and is arranged on the wall surface of the door 1 on the facing surface of the door 1 and the door frame 2.

次に、従来の電磁シールド扉の動作について説明する。図16に示すように、扉1が閉じた状態において、導電性ガスケット6が扉枠2に接触し、扉1と扉枠2とが電気的に接続される。前記接続により、扉1と扉枠2間の隙間が全て電気的に接続されるので、扉1と扉枠2の隙間における電磁波の漏洩と浸入を防ぎ、電磁シールド特性を得ることができる。特許文献1では、より高性能な電磁シールド特性を実現するための構成として、導電性クッション材を用いた扉と扉枠間の接続構造について示されている。   Next, the operation of the conventional electromagnetic shield door will be described. As shown in FIG. 16, when the door 1 is closed, the conductive gasket 6 contacts the door frame 2, and the door 1 and the door frame 2 are electrically connected. Since all the gaps between the door 1 and the door frame 2 are electrically connected by the connection, leakage and intrusion of electromagnetic waves in the gap between the door 1 and the door frame 2 can be prevented, and electromagnetic shielding characteristics can be obtained. Patent Document 1 discloses a connection structure between a door and a door frame using a conductive cushion material as a configuration for realizing higher performance electromagnetic shielding characteristics.

特開平7−94886号公報Japanese Patent Laid-Open No. 7-94886

上述したように、従来の電磁シールド扉では、導電性の扉1と導電性の扉枠2の少なくともどちらかに導電性ガスケット6を配置することで、扉1を閉めた状態において扉1と扉枠2が電気的に接触し、電磁シールド特性を実現していた。
しかしながら、扉1の開閉回数が多くなると、導電性ガスケット6の摩耗や金属疲労により電磁シールド特性が劣化するため、定期的なメンテナンスが必要となるという課題があった。
また、従来の電磁シールド扉の構造では、GHz帯以上の高周波帯域において十分な電磁シールド特性の実現が困難であった。
さらに、広帯域な電磁シールド特性の実現が困難であった。
As described above, in the conventional electromagnetic shield door, the door 1 and the door 1 are closed when the door 1 is closed by disposing the conductive gasket 6 on at least one of the conductive door 1 and the conductive door frame 2. The frame 2 is in electrical contact and realizes electromagnetic shielding characteristics.
However, when the number of times of opening and closing the door 1 is increased, electromagnetic shielding characteristics are deteriorated due to wear of the conductive gasket 6 and metal fatigue, so that there is a problem that regular maintenance is required.
Also, with the conventional electromagnetic shield door structure, it has been difficult to realize sufficient electromagnetic shield characteristics in a high frequency band of GHz or higher.
Furthermore, it has been difficult to realize a broadband electromagnetic shielding characteristic.

この発明は、上記のような課題を解決するためになされたものであり、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、広帯域な電磁シールド特性を有する電磁シールド扉の実現を目的とする。   The present invention has been made in order to solve the above-described problems, does not deteriorate the electromagnetic shield characteristics, and does not require periodic maintenance, and has the electromagnetic shield characteristics mainly in the high frequency band of the GHz band or higher. Furthermore, it aims at realization of the electromagnetic shielding door which has a broadband electromagnetic shielding characteristic.

上記目的を達成するため、この発明に係る電磁シールド扉は、導電性の扉枠と、前記扉枠に配置された導電性の扉と、前記扉を閉めた状態における前記扉枠と前記扉の間隙において、前記扉の壁面と前記扉枠の壁面の少なくとも一方の周囲に沿って複数の誘電体を対向面と非接触となるように配置し、前記誘電体は表面に所定の幅を有し前記扉または前記扉枠と電気的に接続された導体パターンを前記扉と扉枠の周方向に備え、前記導体パターンの前記所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、隣接する前記誘電体の各表面の導体パターン間を導電体により電気的に接続することを特徴とする。   In order to achieve the above object, an electromagnetic shield door according to the present invention includes a conductive door frame, a conductive door disposed on the door frame, the door frame in a state where the door is closed, and the door. In the gap, a plurality of dielectrics are disposed so as to be in non-contact with the opposing surface along at least one of the wall surface of the door and the wall surface of the door frame, and the dielectric material has a predetermined width on the surface. A conductor pattern electrically connected to the door or the door frame is provided in a circumferential direction of the door and the door frame, and the predetermined width of the conductor pattern is a quarter of a frequency within a band where electromagnetic shielding characteristics are required. The conductive pattern on each surface of the adjacent dielectric is electrically connected by a conductor.

この発明の電磁シールド扉によれば、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、広帯域な電磁シールド特性を得ることができる。   According to the electromagnetic shield door of the present invention, the electromagnetic shield characteristic is not deteriorated and periodic maintenance is unnecessary, and the electromagnetic shield characteristic is mainly provided in the high frequency band of the GHz band or higher, and further, the broadband electromagnetic shield characteristic is provided. Can be obtained.

この発明の実施の形態1に係る電磁シールド扉を示す図である。It is a figure which shows the electromagnetic shielding door which concerns on Embodiment 1 of this invention. 図1のA−A’を通るXY断面を示す拡大図である。It is an enlarged view which shows XY cross section which passes along A-A 'of FIG. 図2における共振器装荷誘電体を扉への貼付面と反対側から見たYZ平面図である。It is the YZ top view which looked at the resonator loading dielectric material in FIG. 2 from the opposite side to the sticking surface to a door. この発明の実施の形態1における隣接する共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the adjacent resonator loading dielectric material in Embodiment 1 of this invention. この発明の実施の形態1における扉と扉枠の隙間をY方向に伝搬する電磁波の透過係数を示す図である。It is a figure which shows the permeation | transmission coefficient of the electromagnetic wave which propagates the clearance gap between the door and door frame in Embodiment 1 of this invention to a Y direction. この発明の実施の形態2における隣接する共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the adjacent resonator loading dielectric material in Embodiment 2 of this invention. この発明の実施の形態2における隣接する共振器装荷誘電体の接合部に誘電体を配置した例を示す図である。It is a figure which shows the example which has arrange | positioned the dielectric material to the junction part of the resonator loading dielectric material which adjoins in Embodiment 2 of this invention. この発明の実施の形態3における隣接する共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the adjacent resonator loading dielectric material in Embodiment 3 of this invention. この発明の実施の形態4における隣接する共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the adjacent resonator loading dielectric material in Embodiment 4 of this invention. この発明の実施の形態5における図1のC部の共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the resonator loading dielectric material of the C section of FIG. 1 in Embodiment 5 of this invention. この発明の実施の形態6における図1のC部の共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the resonator loading dielectric material of the C section of FIG. 1 in Embodiment 6 of this invention. この発明の実施の形態6における図1のC部の共振器装荷誘電体の接合部に誘電体を配置した例を示す図である。It is a figure which shows the example which has arrange | positioned the dielectric material to the junction part of the resonator loading dielectric material of the C section of FIG. 1 in Embodiment 6 of this invention. この発明の実施の形態7における図1のC部の共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the resonator loading dielectric material of the C section of FIG. 1 in Embodiment 7 of this invention. この発明の実施の形態8における図1のC部の共振器装荷誘電体の接合部の拡大図である。It is an enlarged view of the junction part of the resonator loading dielectric material of the C section of FIG. 1 in Embodiment 8 of this invention. 従来の電磁シールド扉を示す図である。It is a figure which shows the conventional electromagnetic shielding door. 図15のA−A’を通るXY断面を示す拡大図である。FIG. 16 is an enlarged view showing an XY cross section passing through A-A ′ of FIG. 15.

以下、この発明をより詳細に説明するために、この発明を実施するための形態について、添付の図面に従って説明する。
実施の形態1.
図1,図2を用いてこの発明の実施の形態1による電磁シールド扉について説明する。図1は、実施の形態1に係る電磁シールド扉を示す図であり、図2は、図1のA−A’を通るXY断面の拡大図である。電磁シールド扉は、図1,図2に示すように、扉1、扉枠2、共振器装荷誘電体3から構成されている。扉1と扉枠2は導電性で、ヒンジ7を介して接続され、開閉レバー8の操作により開閉可能な構造を有している。
Hereinafter, in order to explain the present invention in more detail, modes for carrying out the present invention will be described with reference to the accompanying drawings.
Embodiment 1 FIG.
An electromagnetic shield door according to Embodiment 1 of the present invention will be described with reference to FIGS. 1 is a diagram showing an electromagnetic shield door according to Embodiment 1, and FIG. 2 is an enlarged view of an XY section passing through AA ′ of FIG. 1. As shown in FIGS. 1 and 2, the electromagnetic shield door includes a door 1, a door frame 2, and a resonator loaded dielectric 3. The door 1 and the door frame 2 are electrically conductive, are connected via a hinge 7, and have a structure that can be opened and closed by operating an opening / closing lever 8.

共振器装荷誘電体3は、共振構造を有し、扉1と扉枠2の間隙の扉1の壁面の周囲に沿って扉枠2と非接触になるように複数配置されている。   The resonator-loaded dielectric 3 has a resonance structure, and a plurality of the resonator-loaded dielectrics 3 are arranged so as to be in non-contact with the door frame 2 along the periphery of the wall surface of the door 1 in the gap between the door 1 and the door frame 2.

次に、図3を用いて共振器装荷誘電体3に配置されている共振構造について説明する。図3は、図2における共振器装荷誘電体3を、扉1への貼付面と反対側から見たYZ平面図である。図3には、共振器装荷誘電体3の扉1への貼付面と反対側表面に、扉1の周方向に沿って配置された帯状の金属導体である導体パターン4a,4b,4c,4d,4e,4f,4g,4hと、共振器装荷誘電体3の内部に、扉1の周方向であるZ軸方向に沿ってスルーホールが列状に配置された貫通スルーホール列5a,5b,5c,5dが示されている。   Next, the resonance structure arranged in the resonator loaded dielectric 3 will be described with reference to FIG. FIG. 3 is a YZ plan view of the resonator-loaded dielectric 3 in FIG. 2 as viewed from the side opposite to the surface to be bonded to the door 1. In FIG. 3, conductor patterns 4a, 4b, 4c, and 4d, which are band-like metal conductors arranged along the circumferential direction of the door 1 on the surface opposite to the surface of the resonator-loaded dielectric 3 attached to the door 1, are shown. , 4e, 4f, 4g, 4h, and through-through-hole rows 5a, 5b, in which through-holes are arranged in a row along the Z-axis direction that is the circumferential direction of the door 1, inside the resonator-loaded dielectric 3. 5c and 5d are shown.

導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法は、それぞれLa,Lb,Lc,Ld,Le,Lf,Lg,Lhであり、各導体パターンのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhは、それぞれ周波数fa,fb,fc,fd,fe,ff,fg,fhにおいて、共振器装荷誘電体3上で4分の1波長となっている(fb=1.5fa,fc=2fa,fd=2.5fa,fe=3.5fa,ff=4fa,fg=5fa,fh=6.5fa)。   The Y-direction dimensions of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are La, Lb, Lc, Ld, Le, Lf, Lg, and Lh, and the Y-direction dimension La of each conductor pattern. , Lb, Lc, Ld, Le, Lf, Lg, and Lh are quarter wavelengths on the resonator loaded dielectric 3 at frequencies fa, fb, fc, fd, fe, ff, fg, and fh, respectively. (Fb = 1.5fa, fc = 2fa, fd = 2.5fa, fe = 3.5fa, ff = 4fa, fg = 5fa, fh = 6.5fa).

貫通スルーホール列5aは導体パターン4aと4bを、貫通スルーホール列5bは導体パターン4cと4dを、貫通スルーホール列5cは導体パターン4eと4fを、貫通スルーホール列5dは導体パターン4gと4hを、それぞれ扉1と電気的に接続している。   The through-through hole row 5a has conductive patterns 4a and 4b, the through-through hole row 5b has conductive patterns 4c and 4d, the through-through hole row 5c has conductive patterns 4e and 4f, and the through-through hole row 5d has conductive patterns 4g and 4h. Are electrically connected to the door 1 respectively.

導体パターン4a,4b,4c,4d,4e,4f,4g,4hと貫通スルーホール列5a,5b,5c,5dは、Y軸方向に、導体パターン4a、貫通スルーホール列5a、導体パターン4b、導体パターン4c、貫通スルーホール列5b、導体パターン4d、導体パターン4e、貫通スルーホール列5c、導体パターン4f、導体パターン4g、貫通スルーホール列5d、導体パターン4hの順に配置されており、導体パターン4bと導体パターン4cのY方向間隔はSa、導体パターン4dと導体パターン4eのY方向間隔はSb、導体パターン4fと導体パターン4gのY方向間隔はScとなっている。   Conductive patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, 4h and through-through hole rows 5a, 5b, 5c, 5d are arranged in the Y-axis direction with conductive pattern 4a, through-through hole row 5a, conductive pattern 4b, The conductor pattern 4c, the through-through hole row 5b, the conductor pattern 4d, the conductor pattern 4e, the through-through hole row 5c, the conductor pattern 4f, the conductor pattern 4g, the through-through hole row 5d, and the conductor pattern 4h are arranged in this order. The distance in the Y direction between 4b and the conductor pattern 4c is Sa, the distance in the Y direction between the conductor pattern 4d and the conductor pattern 4e is Sb, and the distance in the Y direction between the conductor pattern 4f and the conductor pattern 4g is Sc.

図4を用いて隣接する共振器装荷誘電体3の接合部について説明する。図4は、この発明の実施の形態1における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、隣接する共振器装荷誘電体3aと3bとの接合部の拡大図である。図4に示すように、隣接する共振器装荷誘電体3a,3bは、それぞれ図3で示した導体パターン4と貫通スルーホール列5による短絡構造を有し、導電体である銅箔テープ9により接続されている。銅箔テープ9は、共振器装荷誘電体3aと3bの各表面に配置された導体パターン4間を電気的に接続している。   The junction part of the adjacent resonator loading dielectric material 3 is demonstrated using FIG. FIG. 4 shows the resonator loaded dielectrics 3a and 3b adjacent to each other among the resonator loaded dielectrics 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 in the first embodiment of the present invention. It is an enlarged view of the junction part. As shown in FIG. 4, adjacent resonator-loaded dielectrics 3a and 3b each have a short-circuit structure with the conductor pattern 4 and the through-through hole array 5 shown in FIG. It is connected. The copper foil tape 9 electrically connects the conductor patterns 4 disposed on the surfaces of the resonator loaded dielectrics 3a and 3b.

次に、実施の形態1による電磁シールド扉の動作について説明する。導体パターン4aのY方向寸法は、周波数faにおいて、共振器装荷誘電体3上で4分の1波長となっており、Y方向の片端は開放端、Y方向のもう片端は貫通スルーホール列5aに接続されているので、導体パターン4aは、周波数faと、その高調波であるfaの奇数倍の周波数(3fa,5fa,・・・,(2n+1)fa(nは自然数))において共振する片端短絡の共振回路として動作する。同様に、導体パターン4b,4c,4d,4e,4f,4g,4hは、それぞれ、周波数fb,fc,fd,fe,ff,fg,fhと各々の奇数倍の周波数において共振する片端短絡の共振回路として動作する。   Next, the operation of the electromagnetic shield door according to Embodiment 1 will be described. The Y direction dimension of the conductor pattern 4a is a quarter wavelength on the resonator loaded dielectric 3 at the frequency fa, one end in the Y direction is an open end, and the other end in the Y direction is a through-through-hole array 5a. Therefore, the conductor pattern 4a has one end that resonates at a frequency fa and an odd multiple of the frequency fa (3fa, 5fa,..., (2n + 1) fa (n is a natural number)). Operates as a short circuit resonance circuit. Similarly, the conductor patterns 4b, 4c, 4d, 4e, 4f, 4g, and 4h are resonances of one-end short-circuit that resonates at frequencies fb, fc, fd, fe, ff, fg, and fh, respectively, at odd multiples. Operates as a circuit.

ここで、周波数faの電磁波が扉1と扉枠2の隙間をY方向に伝搬する場合を考えると、導体パターン4aが共振して電磁波と電磁界結合し、扉1と扉枠2の隙間をY方向に伝搬する周波数faの電磁波は減衰する。同様に、周波数faの奇数倍の周波数、周波数fb,fc,fd,fe,ff,fg,fhおよび各々の奇数倍の周波数の電磁波が扉1と扉枠2の隙間をY方向に伝搬する場合、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのいずれかが共振して電磁波と電磁界結合するので、扉1と扉枠2の隙間をY方向に伝搬するこれらの周波数の電磁波も減衰する。この結果、周波数fa,fb,fc,fd,fe,ff,fg,fhおよび各々の奇数倍の周波数において、扉1と扉枠2の隙間における電磁波の漏洩と浸入を防ぎ、図5に示すように、周波数fa,1.5fa,2fa,2.5fa,3fa,3.5fa,4fa,4.5fa,5fa,5.5fa,6fa,6.5fa,7fa,7.5faに極を有する広帯域な減衰特性となり、その結果、広帯域な電磁シールド特性が得られる。   Here, when the electromagnetic wave having the frequency fa propagates in the Y direction through the gap between the door 1 and the door frame 2, the conductor pattern 4a resonates and electromagnetically couples with the electromagnetic wave, and the gap between the door 1 and the door frame 2 is reduced. The electromagnetic wave having the frequency fa propagating in the Y direction is attenuated. Similarly, when an electromagnetic wave having an odd multiple of the frequency fa, the frequencies fb, fc, fd, fe, ff, fg, fh, and each odd multiple of the frequency propagates through the gap between the door 1 and the door frame 2 in the Y direction. Any of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, 4h resonates and electromagnetically couples with the electromagnetic wave, so that these frequencies propagate through the gap between the door 1 and the door frame 2 in the Y direction. The electromagnetic waves are also attenuated. As a result, at the frequencies fa, fb, fc, fd, fe, ff, fg, fh and odd multiples of each, leakage and penetration of electromagnetic waves in the gap between the door 1 and the door frame 2 are prevented, as shown in FIG. In addition, a wide band having poles at frequencies fa, 1.5fa, 2fa, 2.5fa, 3fa, 3.5fa, 4fa, 4.5fa, 5fa, 5.5fa, 6fa, 6.5fa, 7fa, 7.5fa As a result, a broadband electromagnetic shielding characteristic is obtained.

また、図4に示すように、銅箔テープ9を有することにより、隣接する共振器装荷誘電体3aと3b間に隙間が存在しても、共振器装荷誘電体3aと3bの導体パターン4は電気的に接続されるため、扉1と扉枠2の間隙において隣接する共振器装荷誘電体3aと3b間の接合部を伝搬する電磁波に対しても、共振器装荷誘電体3の接合部以外を伝搬する電磁波と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Further, as shown in FIG. 4, by having the copper foil tape 9, even if there is a gap between the adjacent resonator loaded dielectrics 3a and 3b, the conductor pattern 4 of the resonator loaded dielectrics 3a and 3b is Since it is electrically connected, the electromagnetic wave propagating through the junction between the resonator loaded dielectrics 3a and 3b adjacent to each other in the gap between the door 1 and the door frame 2 is also other than the junction of the resonator loaded dielectric 3 As in the case of the electromagnetic wave propagating through the antenna, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

実施の形態1によれば、扉1と扉枠2とが非接触であるため、扉1の開閉回数が多くなった場合にも電磁シールド特性が劣化せず、定期的なメンテナンスが不要となる。   According to the first embodiment, since the door 1 and the door frame 2 are not in contact with each other, even when the number of times the door 1 is opened and closed increases, the electromagnetic shielding characteristics are not deteriorated, and periodic maintenance is unnecessary. .

また、実施の形態1によれば、電磁シールド特性が得られる周波数帯域は、共振器装荷誘電体3に配置された共振構造を有する導体パターン4が共振する周波数によって決まるため、誘電体基板を用いた共振構造の製作が比較的容易である、GHz帯やミリ波帯等の高周波帯域において、有効な電磁シールド特性を実現できる。   Further, according to the first embodiment, the frequency band in which the electromagnetic shielding characteristic is obtained is determined by the frequency at which the conductor pattern 4 having the resonance structure arranged in the resonator-loaded dielectric 3 resonates. Therefore, it is possible to realize effective electromagnetic shielding characteristics in a high frequency band such as a GHz band or a millimeter wave band, which is relatively easy to manufacture.

また、実施の形態1によれば、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhを、それぞれ周波数fa,1.5fa,2fa,2.5fa,3.5fa,4fa,5fa,6.5faにおいて、共振器装荷誘電体3上で4分の1波長となるように分散化することにより、周波数faから7.5faまでの広帯域な電磁シールド特性を実現できる。   Further, according to the first embodiment, the Y-direction dimensions La, Lb, Lc, Ld, Le, Lf, Lg, and Lh of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are respectively set to frequencies. In fa, 1.5fa, 2fa, 2.5fa, 3.5fa, 4fa, 5fa, and 6.5fa, the frequency fa is obtained by dispersing the frequency to be a quarter wavelength on the resonator-loaded dielectric 3. To 7.5 fa wide electromagnetic shielding characteristics can be realized.

なお、実施の形態1では、共振器装荷誘電体3を扉1と扉枠2の間隙における扉1の壁面に配置しているが、共振器装荷誘電体3は扉1と扉枠2との対向面における扉枠2の壁面または扉1と扉枠2の両壁面に配置しても構わない。共振器装荷誘電体3を扉枠2の壁面に配置する場合、貫通スルーホール列5は導体パターン4と扉枠2を電気的に接続する。また、扉1と扉枠2の両壁面に共振器装荷誘電体3を配置する場合、共振器装荷誘電体3は互いが非接触になるように配置する。   In the first embodiment, the resonator loaded dielectric 3 is disposed on the wall surface of the door 1 in the gap between the door 1 and the door frame 2, but the resonator loaded dielectric 3 is formed between the door 1 and the door frame 2. You may arrange | position to the wall surface of the door frame 2 in the opposing surface, or both wall surfaces of the door 1 and the door frame 2. FIG. When the resonator loaded dielectric 3 is disposed on the wall surface of the door frame 2, the through-through hole row 5 electrically connects the conductor pattern 4 and the door frame 2. Further, when the resonator-loaded dielectric 3 is disposed on both wall surfaces of the door 1 and the door frame 2, the resonator-loaded dielectric 3 is disposed so as not to contact each other.

また、実施の形態1では、共振器装荷誘電体3に配置する共振構造として片端短絡の共振回路を適用しているが、共振器装荷誘電体3に配置する共振構造は、片端短絡の共振回路に限定する必要はなく、例えば、両端開放、両端短絡、リング型等の共振回路を適用してもよい。なお、両端開放の共振回路の場合、開放端間の最短距離が半波長となる周波数をfとすると、周波数f,2f,3f,・・・,n×fで共振し、両端短絡の共振回路の場合、短絡端間の最短距離が半波長となる周波数をfとすると、周波数f,2f,3f,・・・,n×fで共振する。また、リング型の共振回路の場合、リングの周長が1波長となる周波数をfとすると、周波数f,2f,3f,・・・,n×fで共振する。   In the first embodiment, a one-end short-circuited resonance circuit is applied as the resonance structure arranged in the resonator-loaded dielectric 3, but the resonance structure arranged in the resonator-loaded dielectric 3 is a one-end short-circuited resonance circuit. For example, a resonant circuit such as open at both ends, shorted at both ends, or a ring type may be applied. In the case of a resonant circuit with both ends open, if the frequency at which the shortest distance between the open ends is a half wavelength is f, the resonance circuit resonates at frequencies f, 2f, 3f,. In this case, assuming that the frequency at which the shortest distance between the short-circuit ends is a half wavelength is f, resonance occurs at frequencies f, 2f, 3f,. In the case of a ring-type resonance circuit, if the frequency at which the circumference of the ring is one wavelength is f, resonance occurs at frequencies f, 2f, 3f,.

また、実施の形態1では、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhを、それぞれ周波数fa,1.5fa,2fa,2.5fa,3.5fa,4fa,5fa,6.5faにおいて、共振器装荷誘電体3上で4分の1波長となるように分散化しているが、広帯域な電磁シールド特性が得られるのであれば、分散化する周波数を上記の周波数に限定する必要はない。   In the first embodiment, the Y-direction dimensions La, Lb, Lc, Ld, Le, Lf, Lg, and Lh of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are respectively set to frequencies fa, 1.5fa, 2fa, 2.5fa, 3.5fa, 4fa, 5fa, and 6.5fa are dispersed so as to have a quarter wavelength on the resonator-loaded dielectric 3, but a broadband electromagnetic shield If the characteristics can be obtained, it is not necessary to limit the frequency to be dispersed to the above frequency.

また、実施の形態1では、8つの導体パターン4a,4b,4c,4d,4e,4f,4g,4hと4つの貫通スルーホール列5a,5b,5c,5dを適用しているが、導体パターンの数および貫通スルーホール列の数は上記の数に限定する必要はない。
また、実施の形態1では、導体パターン4a,4b,4c,4d,4e,4f,4g,4hの短絡手段として貫通スルーホール列5a,5b,5c,5dを適用しているが、短絡手段を貫通スルーホール列に限定する必要はなく、例えば、導電性ネジや金属板等により短絡するようにしても構わない。
In the first embodiment, the eight conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, 4h and the four through-through hole rows 5a, 5b, 5c, 5d are applied. And the number of through-hole rows need not be limited to the above numbers.
In the first embodiment, the through-through hole rows 5a, 5b, 5c, and 5d are applied as the short-circuiting means for the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h. It is not necessary to limit to the through-through hole row, and for example, a short circuit may be made with a conductive screw or a metal plate.

また、実施の形態1では、隣接する共振器装荷誘電体3aと3bに配置された導体パターン4間の電気的接続に銅箔テープ9を用いているが、導体パターン4間の電気的接続が得られるのであれば、導体パターン4間の電気的接続手段を銅箔テープ9に限定する必要はない。   In the first embodiment, the copper foil tape 9 is used for the electrical connection between the conductor patterns 4 arranged on the adjacent resonator-loaded dielectrics 3a and 3b. If obtained, it is not necessary to limit the electrical connection means between the conductor patterns 4 to the copper foil tape 9.

以上のように、この発明の実施の形態1における電磁シールド扉によれば、導電性の扉枠2と、扉枠2に配置された導電性の扉1と、扉1を閉めた状態における扉枠2と扉1の間隙において、扉1の壁面と扉枠2の壁面の少なくとも一方の周囲に沿って複数の共振器装荷誘電体3を対向面と非接触となるように配置し、共振器装荷誘電体3は表面に所定の幅を有し扉1または扉枠2と電気的に接続された導体パターン4を扉1と扉枠2の周方向に備え、導体パターン4の所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、隣接する共振器装荷誘電体3aと3bの各表面の導体パターン4間を導電体により電気的に接続するように構成したので、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、広帯域な電磁シールド特性を得ることができる。   As mentioned above, according to the electromagnetic shielding door in Embodiment 1 of this invention, the conductive door frame 2, the conductive door 1 arrange | positioned at the door frame 2, and the door in the state which closed the door 1 In the gap between the frame 2 and the door 1, a plurality of resonator-loaded dielectrics 3 are arranged so as to be in non-contact with the facing surface along at least one of the wall surface of the door 1 and the wall surface of the door frame 2. The loading dielectric 3 has a conductor pattern 4 having a predetermined width on the surface and electrically connected to the door 1 or the door frame 2 in the circumferential direction of the door 1 and the door frame 2, and the conductor pattern 4 has a predetermined width. The electromagnetic shielding characteristic is set to a quarter wavelength of the frequency within the required band, and the conductor patterns 4 on the surfaces of the adjacent resonator-loaded dielectrics 3a and 3b are electrically connected by a conductor. Because it is configured, the electromagnetic shielding characteristics do not deteriorate and periodic maintenance is not required. Mainly it has electromagnetic shielding characteristics in a GHz band or a high frequency band, further, it is possible to obtain a wide-band electromagnetic shielding properties.

実施の形態2.
図1から図3と図6を用いてこの発明の実施の形態2による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図6は、この発明の実施の形態2における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、隣接する共振器装荷誘電体3aと3bとの接合部の拡大図である。図6において、隣接する2つの共振器装荷誘電体3aと3bは図3で示した導体パターン4と貫通スルーホール列5による短絡構造を有し、銅箔テープ9および導体ガスケット10を備える。銅箔テープ9は、共振器装荷誘電体3aと3bの各表面に配置された導体パターン4間を電気的に接続しており、導体ガスケット10は、表面が導電性の特性を有し、隣接する共振器装荷誘電体3aと3b間の隙間を埋めるように配置されている。このように、実施の形態2は、扉1と扉枠2の間隙に配置された、隣接する共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じ構造を有している。
Embodiment 2. FIG.
An electromagnetic shield door according to Embodiment 2 of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 6 shows the resonator loaded dielectrics 3a and 3b adjacent to each other among the resonator loaded dielectrics 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 in the second embodiment of the present invention. It is an enlarged view of the junction part. In FIG. 6, two adjacent resonator loaded dielectrics 3 a and 3 b have a short-circuit structure with the conductor pattern 4 and the through-through hole array 5 shown in FIG. 3, and include a copper foil tape 9 and a conductor gasket 10. The copper foil tape 9 is electrically connected between the conductor patterns 4 arranged on the surfaces of the resonator-loaded dielectrics 3a and 3b, and the conductor gasket 10 has a conductive property on the surface and is adjacent The resonator-loaded dielectrics 3a and 3b are arranged so as to fill the gap. As described above, the second embodiment has the same structure as that of the first embodiment except for the joint portion between the adjacent resonator-loaded dielectrics 3a and 3b arranged in the gap between the door 1 and the door frame 2. doing.

図6に示すように、導体ガスケット10は、表面が導電性の特性を有し、隣接する共振器装荷誘電体3aと3b間の隙間を埋めるように配置されている。このように、実施の形態2は、扉1と扉枠2の間隙に配置された、隣接する共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じ構造を有している。   As shown in FIG. 6, the conductive gasket 10 has a conductive property on the surface, and is disposed so as to fill a gap between the adjacent resonator-loaded dielectrics 3a and 3b. As described above, the second embodiment has the same structure as that of the first embodiment except for the joint portion between the adjacent resonator-loaded dielectrics 3a and 3b arranged in the gap between the door 1 and the door frame 2. doing.

次に、実施の形態2による電磁シールド扉の動作について説明する。実施の形態2は、扉1と扉枠2の間隙に隣接して配置された共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じなので、隣接する共振器装荷誘電体3aと3b間の接合部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the second embodiment will be described. Since the structure of the second embodiment is the same as that of the first embodiment except for the joint portion between the resonator loaded dielectrics 3a and 3b arranged adjacent to the gap between the door 1 and the door frame 2, the adjacent resonator loading is performed. As with the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained for electromagnetic waves propagating through locations other than the junction between the dielectrics 3a and 3b.

また、実施の形態2では、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3bにそれぞれ配置された導体パターン4は、実施の形態1と同様に、銅箔テープ9によって電気的に接続されており、また、隣接する共振器装荷誘電体3aと3b間の隙間に導体ガスケット10が配置されているため、隣接する共振器装荷誘電体3aと3b間には電気的な隙間が存在せず、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3b間の接合部を伝搬する電磁波においても、図5に示された広帯域な電磁シールド特性が得られる。   In the second embodiment, the conductor pattern 4 disposed in each of the resonator loaded dielectrics 3a and 3b adjacent to each other in the gap between the door 1 and the door frame 2 is the copper foil tape 9 as in the first embodiment. And the conductive gasket 10 is disposed in the gap between the adjacent resonator-loaded dielectrics 3a and 3b, so that the adjacent resonator-loaded dielectrics 3a and 3b are electrically connected to each other. In the gap between the door 1 and the door frame 2, the electromagnetic wave propagating through the junction between the adjacent resonator-loaded dielectrics 3 a and 3 b also has the broadband electromagnetic shielding characteristics shown in FIG. 5. can get.

また、実施の形態2では、隣接する共振器装荷誘電体3aと3b間の隙間に導体ガスケット10が配置されているので、隣接する共振器装荷誘電体3aと3b間には空間的な隙間が存在せず、扉開閉動作の繰り返しにより発生しやすい共振器装荷誘電体3aと3bの位置ずれを抑えることができる。   In the second embodiment, since the conductor gasket 10 is disposed in the gap between the adjacent resonator-loaded dielectrics 3a and 3b, there is a spatial gap between the adjacent resonator-loaded dielectrics 3a and 3b. Misalignment of the resonator-loaded dielectrics 3a and 3b that does not exist and is likely to occur due to repeated door opening and closing operations can be suppressed.

すなわち、実施の形態2によれば、実施の形態1と同様の広帯域な電磁シールド特性を有し、かつ、共振器装荷誘電体3の位置ずれを抑えることができる電磁シールド扉を実現できる。   That is, according to the second embodiment, it is possible to realize an electromagnetic shield door that has a broadband electromagnetic shielding characteristic similar to that of the first embodiment and can suppress the displacement of the resonator-loaded dielectric 3.

なお、実施の形態2では、隣接する共振器装荷誘電体3aと3b間の隙間に導体ガスケット10が配置されているが、隣接する共振器装荷誘電体3aと3b間の隙間を空間的にも電気的にも埋めるものであれば、隣接する共振器装荷誘電体3aと3b間の隙間に配置する部材は導体ガスケット10に限定する必要はない。例えば、図6における導体ガスケット10の代わりに誘電体11を配置した例を図7に示す。図7は図6に対して導体ガスケット10の代わりに誘電体11を備える点のみで異なり、その他の構成は図6と同じなので説明は省略する。   In the second embodiment, the conductor gasket 10 is disposed in the gap between the adjacent resonator loaded dielectrics 3a and 3b. However, the gap between the adjacent resonator loaded dielectrics 3a and 3b is also spatially reduced. The member disposed in the gap between the adjacent resonator-loaded dielectrics 3a and 3b need not be limited to the conductor gasket 10 as long as it is electrically filled. For example, FIG. 7 shows an example in which the dielectric 11 is arranged instead of the conductor gasket 10 in FIG. FIG. 7 differs from FIG. 6 only in that a dielectric 11 is provided instead of the conductor gasket 10, and the rest of the configuration is the same as FIG.

また、導電性塗料や導体パターンを共振器装荷誘電体3の側面に配置することにより、共振器装荷誘電体3の側面と導体ガスケット10の電気的接続を強化する構成としてもよい。   Further, the electrical connection between the side surface of the resonator-loaded dielectric 3 and the conductor gasket 10 may be strengthened by disposing conductive paint or a conductor pattern on the side surface of the resonator-loaded dielectric 3.

以上のように、この発明の実施の形態2における電磁シールド扉によれば、隣接する共振器装荷誘電体3aと3b間の隙間に導体ガスケット10または誘電体11を配置するように構成したので、実施の形態1における効果に加え、隣接する共振器装荷誘電体3aと3b間には空間的な隙間が存在せず、扉開閉動作の繰り返しにより発生しやすい、共振器装荷誘電体3の位置ずれを抑えることができる。   As described above, according to the electromagnetic shield door according to the second embodiment of the present invention, the conductor gasket 10 or the dielectric 11 is arranged in the gap between the adjacent resonator-loaded dielectrics 3a and 3b. In addition to the effects of the first embodiment, there is no spatial gap between adjacent resonator-loaded dielectrics 3a and 3b, and the displacement of the resonator-loaded dielectric 3 is likely to occur due to repeated door opening and closing operations. Can be suppressed.

実施の形態3.
図1から図2と図8を用いてこの発明の実施の形態3による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図8は、この発明の実施の形態3における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、隣接する共振器装荷誘電体3aと3bとの接合部の拡大図である。図8において、隣接する共振器装荷誘電体3aと3bは図3で示した導体パターン4と貫通スルーホール列5による短絡構造を有し、フレキシブル基板12を備える。
Embodiment 3 FIG.
An electromagnetic shield door according to Embodiment 3 of the present invention will be described with reference to FIGS. 1 to 2 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 8 shows the resonator loaded dielectrics 3a and 3b adjacent to each other among the resonator loaded dielectrics 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 in the third embodiment of the present invention. It is an enlarged view of the junction part. In FIG. 8, adjacent resonator-loaded dielectrics 3 a and 3 b have a short circuit structure with the conductor pattern 4 and the through-through hole array 5 shown in FIG.

フレキシブル基板12は折り曲げ可能な特性を有する誘電体基板であり、フレキシブル基板12の片側表面には、共振器装荷誘電体3aと3bに配置されている導体パターン4とY方向に同寸法の導体パターンが複数配置されており、各導体パターンは、共振器装荷誘電体3aと3bにそれぞれ配置された導体パターン4を電気的に接続している。このように、実施の形態3は、扉1と扉枠2の間隙に配置された、隣接する共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じ構造を有している。   The flexible substrate 12 is a dielectric substrate having a foldable characteristic, and a conductor pattern having the same dimension in the Y direction as the conductor pattern 4 disposed on the resonator-loaded dielectrics 3a and 3b is provided on one surface of the flexible substrate 12. Are arranged, and each conductor pattern electrically connects the conductor patterns 4 respectively arranged on the resonator-loaded dielectrics 3a and 3b. As described above, the third embodiment has the same structure as that of the first embodiment except for the joint portion between the adjacent resonator-loaded dielectrics 3a and 3b disposed in the gap between the door 1 and the door frame 2. doing.

次に、実施の形態3による電磁シールド扉の動作について説明する。実施の形態3は、扉1と扉枠2の間隙に隣接して配置された共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じなので、隣接する共振器装荷誘電体3aと3b間の接合部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to Embodiment 3 will be described. Since the structure of the third embodiment is the same as that of the first embodiment except for the joint portion between the resonator-loaded dielectrics 3a and 3b disposed adjacent to the gap between the door 1 and the door frame 2, the adjacent resonator loading is performed. As with the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained for electromagnetic waves propagating through locations other than the junction between the dielectrics 3a and 3b.

また、実施の形態3では、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3bにそれぞれ配置された導体パターン4は、フレキシブル基板12に配置された導体パターンによって、実施の形態1と同様に電気的に接続されている。したがって、隣接する共振器装荷誘電体3aと3b間には電気的な隙間が存在せず、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3b間の接合部を伝搬する電磁波においても、図5に示された広帯域な電磁シールド特性が得られる。   In the third embodiment, the conductor pattern 4 disposed in each of the resonator loaded dielectrics 3a and 3b adjacent to each other in the gap between the door 1 and the door frame 2 is implemented by the conductor pattern disposed on the flexible substrate 12. In the same manner as in the first embodiment, they are electrically connected. Therefore, there is no electrical gap between the adjacent resonator-loaded dielectrics 3a and 3b, and the gap between the door 1 and the door frame 2 propagates through the junction between the adjacent resonator-loaded dielectrics 3a and 3b. Even in the case of electromagnetic waves, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

また、実施の形態3では、隣接する共振器装荷誘電体3aと3bの接合部1箇所において1つのフレキシブル基板12を用いるので、隣接する共振器装荷誘電体3aと3bにそれぞれ配置された導体パターン4の電気的接続を簡易に行うことができる。すなわち、実施の形態3により、実施の形態1と同様の広帯域な電磁シールド特性を有し、かつ、隣接する共振器装荷誘電体3aと3bの接合部の構造が簡易である電磁シールド扉を実現できる。   Further, in the third embodiment, since one flexible substrate 12 is used at one joint portion between adjacent resonator-loaded dielectrics 3a and 3b, conductor patterns disposed on adjacent resonator-loaded dielectrics 3a and 3b, respectively. 4 can be easily connected. That is, according to the third embodiment, an electromagnetic shield door having the same broadband electromagnetic shielding characteristics as in the first embodiment and having a simple structure of the joint portion between the adjacent resonator-loaded dielectrics 3a and 3b is realized. it can.

以上のように、この発明の実施の形態3における電磁シールド扉によれば、隣接する共振器装荷誘電体3aと3bの各表面の導体パターン4間を電気的に接続する導電体が、フレキシブル基板12上に配置されるように構成したので、実施の形態1における効果に加え、隣接する共振器装荷誘電体3aと3bにそれぞれ配置された導体パターン4の電気的接続を簡易に行うことができる。   As described above, according to the electromagnetic shield door according to the third embodiment of the present invention, the conductor that electrically connects the conductor patterns 4 on the surfaces of the adjacent resonator-loaded dielectrics 3a and 3b is a flexible substrate. In addition to the effects of the first embodiment, the electrical connection of the conductor patterns 4 respectively disposed on the adjacent resonator-loaded dielectrics 3a and 3b can be easily performed. .

実施の形態4.
図1から図3と図9を用いてこの発明の実施の形態4による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図9は、この発明の実施の形態4における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、隣接する共振器装荷誘電体3aと3bとの接合部の拡大図であり、各部位の説明は図4と同じである。図9において、隣接する共振器装荷誘電体3aと3bの隙間の間隔はdであり、dは電磁シールド特性が要求される周波数帯域の上限周波数fmaxの2分の1波長の寸法となっている。このように、実施の形態3は、扉1と扉枠2の間隙に配置された、隣接する共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じ構造を有している。
Embodiment 4 FIG.
An electromagnetic shield door according to Embodiment 4 of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 9 shows adjacent resonator loaded dielectrics 3a and 3b among the resonator loaded dielectrics 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 according to the fourth embodiment of the present invention. FIG. 4 is an enlarged view of the joint part, and the description of each part is the same as FIG. In FIG. 9, the gap between adjacent resonator-loaded dielectrics 3a and 3b is d, and d is a half wavelength dimension of the upper limit frequency f max of the frequency band in which electromagnetic shielding characteristics are required. Yes. As described above, the third embodiment has the same structure as that of the first embodiment except for the joint portion between the adjacent resonator-loaded dielectrics 3a and 3b disposed in the gap between the door 1 and the door frame 2. doing.

次に、実施の形態4による電磁シールド扉の動作について説明する。実施の形態4は、扉1と扉枠2の間隙に隣接して配置された共振器装荷誘電体3aと3b間の接合部以外の構造は実施の形態1と同じなので、隣接する共振器装荷誘電体3aと3b間の接合部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the fourth embodiment will be described. Since the structure of the fourth embodiment is the same as that of the first embodiment except for the joint portion between the resonator-loaded dielectrics 3a and 3b arranged adjacent to the gap between the door 1 and the door frame 2, the adjacent resonator loading is performed. As with the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained for electromagnetic waves propagating through locations other than the junction between the dielectrics 3a and 3b.

また、図9に示すように、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3bの隙間の間隔がdとなっているので、周波数がfmax以下である電磁波は、隣接する共振器装荷誘電体3aと3bの隙間を伝搬する際に指数関数的に減衰する。したがって、扉1と扉枠2の間隙において、隣接する共振器装荷誘電体3aと3b間の隙間を伝搬する電磁波においても、fmax以下の周波数において広帯域な電磁シールド特性が得られる。すなわち、実施の形態4により、fmax以下の周波数において広帯域な電磁シールド特性を有し、かつ、隣接する共振器装荷誘電体の接合部の構造が簡易である電磁シールド扉を実現できる。 Further, as shown in FIG. 9, in the gap between the door 1 and the door frame 2, the gap between the adjacent resonator loaded dielectrics 3a and 3b is d, so that the electromagnetic wave having a frequency of f max or less is , It attenuates exponentially when propagating through the gap between adjacent resonator-loaded dielectrics 3a and 3b. Therefore, even in the electromagnetic wave propagating in the gap between the adjacent resonator loaded dielectrics 3a and 3b in the gap between the door 1 and the door frame 2, a broadband electromagnetic shielding characteristic can be obtained at a frequency of f max or less. That is, according to the fourth embodiment, an electromagnetic shield door having a broadband electromagnetic shield characteristic at a frequency equal to or lower than f max and a simple structure of a joint portion of adjacent resonator-loaded dielectrics can be realized.

実施の形態4によれば、扉1と扉枠2とが非接触であるため、扉1の開閉回数が多くなった場合にも電磁シールド特性が劣化せず、定期的なメンテナンスが不要となる。   According to the fourth embodiment, since the door 1 and the door frame 2 are not in contact with each other, even when the number of times of opening and closing the door 1 is increased, the electromagnetic shielding characteristics are not deteriorated, and periodic maintenance is not required. .

また、実施の形態4によれば、電磁シールド特性が得られる周波数帯域は、共振器装荷誘電体3に配置された共振構造を有する導体パターン4が共振する周波数によって決まるため、誘電体基板を用いた共振構造の製作が比較的容易である、GHz帯やミリ波帯等の高周波帯域において、有効な電磁シールド特性を実現できる。   Further, according to the fourth embodiment, the frequency band in which the electromagnetic shielding characteristics can be obtained is determined by the frequency at which the conductor pattern 4 having the resonance structure arranged in the resonator-loaded dielectric 3 resonates. Therefore, it is possible to realize effective electromagnetic shielding characteristics in a high frequency band such as a GHz band or a millimeter wave band, which is relatively easy to manufacture.

また、実施の形態4によれば、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhを、それぞれ周波数fa,1.5fa,2fa,2.5fa,3.5fa,4fa,5fa,6.5faにおいて、共振器装荷誘電体3上で4分の1波長となるように分散化することにより、周波数faから7.5faまでの広帯域な電磁シールド特性を実現できる。   Further, according to the fourth embodiment, the Y-direction dimensions La, Lb, Lc, Ld, Le, Lf, Lg, and Lh of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are respectively set to frequencies. In fa, 1.5fa, 2fa, 2.5fa, 3.5fa, 4fa, 5fa, and 6.5fa, the frequency fa is obtained by dispersing the frequency to be a quarter wavelength on the resonator-loaded dielectric 3. To 7.5 fa wide electromagnetic shielding characteristics can be realized.

以上のように、この発明の実施の形態4における電磁シールド扉によれば、導電性の扉1と、扉枠2に配置された導電性の扉1と、扉1を閉めた状態における扉枠2と扉1の間隙において、扉1の壁面と扉枠2の壁面の少なくとも一方の周囲に沿って複数の共振器装荷誘電体3を対向面と非接触となるように配置し、共振器装荷誘電体3は表面に所定の幅を有し扉1または扉枠2と電気的に接続された導体パターン4を扉1と扉枠2の周方向に備え、導体パターン4の所定の幅を電磁シールド特性が要求される帯域内の周波数の4の1波長に設定し、隣接する共振器装荷誘電体3aと3b間の隙間寸法が、電磁シールド特性が要求される上限周波数の2分の1波長以下であるように構成したので、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、fmax以下の周波数において広帯域な周波数に特化した電磁シールド特性を得ることができ、かつ、隣接する共振器装荷誘電体3aと3bの接合部の構造が簡易となる。 As mentioned above, according to the electromagnetic shielding door in Embodiment 4 of this invention, the conductive door 1, the conductive door 1 arrange | positioned at the door frame 2, and the door frame in the state which closed the door 1 In the gap between the door 2 and the door 1, a plurality of resonator-loaded dielectrics 3 are arranged so as to be in non-contact with the opposite surface along at least one of the wall surface of the door 1 and the wall surface of the door frame 2. The dielectric 3 has a conductor pattern 4 having a predetermined width on the surface and electrically connected to the door 1 or the door frame 2 in the circumferential direction of the door 1 and the door frame 2. It is set to one wavelength of 4 of the frequency within the band where the shield characteristic is required, and the gap dimension between the adjacent resonator loaded dielectrics 3a and 3b is a half wavelength of the upper limit frequency where the electromagnetic shield characteristic is required. Since it is configured as follows, the electromagnetic shielding characteristics do not deteriorate and regular maintenance is performed. Nsu is unnecessary, mainly includes an electromagnetic shielding properties in a GHz band or a high frequency band, further, it is possible to obtain an electromagnetic shielding characteristics specific to wideband frequency at frequencies below f max, and the adjacent The structure of the junction between the resonator loaded dielectrics 3a and 3b is simplified.

実施の形態5.
図1から図3と図10を用いてこの発明の実施の形態5による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図10は、この発明の実施の形態5における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、図1の破線Cで示す扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部の拡大図であり、各部位の説明は実施の形態1における図4と同じである。
Embodiment 5 FIG.
An electromagnetic shield door according to Embodiment 5 of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 10 shows a resonator loaded dielectric 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 according to Embodiment 5 of the present invention. It is an enlarged view of the junction part of the resonator loading dielectrics 3c and 3d which adjoin in the direction orthogonal to each other in the corner part in the gap | interval of the door frame 2, and description of each part is the same as FIG. 4 in Embodiment 1. FIG. .

次に、実施の形態5による電磁シールド扉の動作について説明する。実施の形態5では、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の接合部以外の構造は実施の形態1と同じなので、隣接する共振器装荷誘電体3aと3b間の接合部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the fifth embodiment will be described. In the fifth embodiment, the structure other than the joint portion between the resonator loaded dielectrics 3c and 3d adjacent in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2 is the same as that of the first embodiment. As with the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained for electromagnetic waves propagating through locations other than the junction between the resonator-loaded dielectrics 3a and 3b.

また、実施の形態5では、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4が銅箔テープ9によって接続されているので、共振器装荷誘電体3cと3d間に電気的な隙間が存在せず、扉1と扉枠2の間隙におけるコーナー部において、互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の接合部を伝搬する電磁波においても、図5に示された広帯域な電磁シールド特性が得られる。   In the fifth embodiment, the conductor patterns 4 arranged on the resonator-loaded dielectrics 3 c and 3 d adjacent to each other in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2 are connected by the copper foil tape 9. Therefore, there is no electrical gap between the resonator-loaded dielectrics 3c and 3d, and the resonator-loaded dielectric 3c adjacent in the direction perpendicular to each other at the corner in the gap between the door 1 and the door frame 2 is provided. 5b, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

実施の形態5によれば、扉1と扉枠2とが非接触であるため、扉1の開閉回数が多くなった場合にも、コーナー部における電磁シールド特性の劣化を抑えることができる。   According to the fifth embodiment, since the door 1 and the door frame 2 are not in contact with each other, even when the number of times of opening and closing the door 1 is increased, it is possible to suppress the deterioration of the electromagnetic shielding characteristics in the corner portion.

また、実施の形態5によれば、電磁シールド特性が得られる周波数帯域は、共振器装荷誘電体3に配置された共振構造を有する導体パターン4が共振する周波数によって決まるため、誘電体基板を用いた共振構造の製作が比較的容易である、GHz帯やミリ波帯等の高周波帯域において、有効な電磁シールド特性を実現できる。   Further, according to the fifth embodiment, the frequency band in which the electromagnetic shielding characteristics can be obtained is determined by the frequency at which the conductor pattern 4 having the resonance structure arranged in the resonator-loaded dielectric 3 resonates. Therefore, it is possible to realize effective electromagnetic shielding characteristics in a high frequency band such as a GHz band or a millimeter wave band, which is relatively easy to manufacture.

また、実施の形態5によれば、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhを、それぞれ周波数fa,1.5fa,2fa,2.5fa,3.5fa,4fa,5fa,6.5faにおいて、共振器装荷誘電体3上で4分の1波長となるように分散化することにより、周波数faから7.5faまでの広帯域な電磁シールド特性を実現できる。   Further, according to the fifth embodiment, the Y-direction dimensions La, Lb, Lc, Ld, Le, Lf, Lg, and Lh of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are respectively set to frequencies. In fa, 1.5fa, 2fa, 2.5fa, 3.5fa, 4fa, 5fa, and 6.5fa, the frequency fa is obtained by dispersing the frequency to be a quarter wavelength on the resonator-loaded dielectric 3. To 7.5 fa wide electromagnetic shielding characteristics can be realized.

以上のように、この発明の実施の形態5における電磁シールド扉によれば、導電性の扉枠2と、扉枠2に配置された導電性の扉1と、扉1を閉めた状態における扉枠2と扉1の間隙において、扉1の壁面と扉枠2の壁面の少なくとも一方の周囲に沿って複数の共振器装荷誘電体3を対向面と非接触となるように配置し、共振器装荷誘電体3は表面に所定の幅を有し扉1または扉枠2と電気的に接続された導体パターン4を扉1と扉枠2の周方向に備え、導体パターン4の所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3dの各表面の導体パターン4間を導電体により電気的に接続するように構成したので、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、広帯域な周波数に特化した電磁シールド特性を得ることができる。   As mentioned above, according to the electromagnetic shielding door in Embodiment 5 of this invention, the conductive door frame 2, the conductive door 1 arrange | positioned at the door frame 2, and the door in the state which closed the door 1 In the gap between the frame 2 and the door 1, a plurality of resonator-loaded dielectrics 3 are arranged so as to be in non-contact with the facing surface along at least one of the wall surface of the door 1 and the wall surface of the door frame 2. The loading dielectric 3 has a conductor pattern 4 having a predetermined width on the surface and electrically connected to the door 1 or the door frame 2 in the circumferential direction of the door 1 and the door frame 2, and the conductor pattern 4 has a predetermined width. Conductor patterns on the surfaces of the resonator-loaded dielectrics 3c and 3d that are set to a quarter wavelength of the frequency within the band where electromagnetic shielding characteristics are required and are adjacent to each other at the corners of the door 1 and the door frame 2 Since it is configured to electrically connect the four with a conductor, electromagnetic seal Regular maintenance properties not deteriorate is unnecessary, mainly includes an electromagnetic shielding properties in a GHz band or a high frequency band, further, it is possible to obtain an electromagnetic shielding characteristics specific to wide frequency.

実施の形態6.
図1から図3と図11を用いてこの発明の実施の形態6による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図11は、この発明の実施の形態6における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、図1の破線Cで示す扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部の拡大図である。図11において、互いに直交する方向で隣接する共振器装荷誘電体3cと3dは図3で示した導体パターン4と貫通スルーホール列5による短絡構造を有し、銅箔テープ9および導体ガスケット10を備える。銅箔テープ9は、共振器装荷誘電体3cと3dの各表面に配置された導体パターン4間を電気的に接続しており、導電ガスケット10は、表面が導電性の特性を有し、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の隙間を埋めるように配置されている。このように、実施の形態6は、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部以外の構造は実施の形態1と同じ構造を有している。
Embodiment 6 FIG.
An electromagnetic shield door according to Embodiment 6 of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 11 shows a resonator loaded dielectric 3 arranged in plural on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 in Embodiment 6 of the present invention. It is an enlarged view of the junction part of the resonator loading dielectrics 3c and 3d which adjoin in the direction orthogonal to each other in the corner part in the gap | interval of the door frame 2. FIG. In FIG. 11, the resonator loaded dielectrics 3c and 3d which are adjacent to each other in a direction orthogonal to each other have a short-circuit structure by the conductor pattern 4 and the through-through hole array 5 shown in FIG. Prepare. The copper foil tape 9 is electrically connected between the conductor patterns 4 disposed on the surfaces of the resonator-loaded dielectrics 3c and 3d, and the conductive gasket 10 has a conductive property on the surface. 1 and the door frame 2 are arranged so as to fill a gap between the resonator loaded dielectrics 3c and 3d adjacent to each other in a direction orthogonal to each other at a corner portion in the gap between the door frame 2 and the door frame 2. As described above, the structure of the sixth embodiment is the same as that of the first embodiment except for the joint portion between the resonator-loaded dielectrics 3c and 3d adjacent to each other in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2. Have the same structure.

次に、実施の形態6による電磁シールド扉の動作について説明する。実施の形態6は、扉1と扉枠2の間隙におけるコーナー部以外の構造は実施の形態1と同じなので、扉1と扉枠2の間隙におけるコーナー部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the sixth embodiment will be described. The sixth embodiment has the same structure as that of the first embodiment except for the corner portion in the gap between the door 1 and the door frame 2, so that the electromagnetic wave propagating through the portion other than the corner portion in the gap between the door 1 and the door frame 2 is prevented. As in the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

また、実施の形態6では、扉1と扉枠2の間隙におけるコーナー部において、互いに直交する方向で隣接する共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4は、実施の形態5と同様に、銅箔テープ9によって電気的に接続されており、また、共振器装荷誘電体3cと3d間の隙間に導体ガスケット10が配置されている。したがって、共振器装荷誘電体3cと3d間には電気的な隙間が存在せず、扉1と扉枠2の間隙におけるコーナー部で、互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の接合部を伝搬する電磁波においても、図5に示された広帯域な電磁シールド特性が得られる。   Further, in the sixth embodiment, the conductor patterns 4 arranged in the resonator loaded dielectrics 3c and 3d adjacent to each other in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2 are the same as those in the fifth embodiment. Similarly, the copper foil tape 9 is electrically connected, and the conductor gasket 10 is disposed in the gap between the resonator loaded dielectrics 3c and 3d. Accordingly, there is no electrical gap between the resonator-loaded dielectrics 3c and 3d, and the resonator-loaded dielectrics 3c and 3d adjacent in the direction perpendicular to each other at the corner portion in the gap between the door 1 and the door frame 2 are provided. Also in the electromagnetic wave propagating through the junction between the two, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

また、実施の形態6では、互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の隙間に導体ガスケット10が配置されているので、共振器装荷誘電体3cと3d間には空間的な隙間が存在せず、したがって、扉開閉動作の繰り返しにより発生しやすい、共振器装荷誘電体3cと3dの位置ずれを抑えることができる。   Further, in the sixth embodiment, since the conductor gasket 10 is disposed in the gap between the resonator-loaded dielectrics 3c and 3d that are adjacent to each other in the direction orthogonal to each other, the space between the resonator-loaded dielectrics 3c and 3d is spatial. Therefore, it is possible to suppress the displacement of the resonator loaded dielectrics 3c and 3d, which is likely to occur due to repeated door opening and closing operations.

すなわち、実施の形態6により、扉1と扉枠2の間隙におけるコーナー部での電磁シールド特性の劣化を抑えることができるので、実施の形態1と同様の広帯域な電磁シールド特性を有し、かつ、扉1と扉枠2の間隙におけるコーナー部に配置された共振器装荷誘電体3の位置ずれを抑えることができる電磁シールド扉を実現できる。   That is, according to the sixth embodiment, it is possible to suppress the deterioration of the electromagnetic shielding characteristics at the corner portion in the gap between the door 1 and the door frame 2, so that the broadband electromagnetic shielding characteristics similar to those of the first embodiment are obtained, and In addition, an electromagnetic shield door that can suppress the displacement of the resonator loaded dielectric 3 disposed at the corner portion in the gap between the door 1 and the door frame 2 can be realized.

なお、実施の形態6では、扉1と扉枠2の間隙におけるコーナー部で互いに直交する方向で隣接する共振器装荷誘電体3cと3d間の隙間に導体ガスケット10が配置されているが、共振器装荷誘電体3cと3d間の隙間を空間的にも電気的にも埋めるのであれば、共振器装荷誘電体3cと3d間の隙間に配置する部材は導体ガスケット10に限定する必要はない。図11における導体ガスケット10の替わりに、誘電体11を配置した例を図12に示す。図12は図11に対して導体ガスケット10の代わりに誘電体11を備える点のみで異なり、その他の構成は図10と同じなので説明は省略する。   In the sixth embodiment, the conductor gasket 10 is disposed in the gap between the resonator loaded dielectrics 3c and 3d adjacent to each other in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2. The member disposed in the gap between the resonator loaded dielectrics 3c and 3d need not be limited to the conductor gasket 10 as long as the gap between the loaded dielectrics 3c and 3d is spatially and electrically filled. FIG. 12 shows an example in which a dielectric 11 is arranged instead of the conductor gasket 10 in FIG. FIG. 12 differs from FIG. 11 only in that a dielectric 11 is provided instead of the conductor gasket 10, and the other configuration is the same as FIG.

また、導電性塗料や導体パターンを共振器装荷誘電体3の側面に配置することで、共振器装荷誘電体3の側面と導電性ガスケット10の電気的接続を強化する構成としてもよい。   Moreover, it is good also as a structure which reinforces the electrical connection of the side surface of the resonator loading dielectric material 3, and the conductive gasket 10 by arrange | positioning a conductive paint and a conductor pattern on the side surface of the resonator loading dielectric material 3. FIG.

以上のように、この発明の実施の形態6における電磁シールド扉によれば、扉枠2と扉1の間隙における扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3c,3d間の隙間に導電性ガスケット10または誘電体11を配置するように構成したので、実施の形態1における効果に加え、扉枠2と扉1の間隙における扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3d間には空間的な隙間が存在せず、扉開閉動作の繰り返しにより発生しやすい、共振器装荷誘電体3の位置ずれを抑えることができる。   As described above, according to the electromagnetically shielded door according to the sixth embodiment of the present invention, the resonator loaded dielectric 3c that is adjacent to each other at the corner portion of the door 1 and the door frame 2 in the gap between the door frame 2 and the door 1 is perpendicular. In addition to the effects of the first embodiment, the corner portions of the door 1 and the door frame 2 in the gap between the door frame 2 and the door 1 are configured. In FIG. 3, there is no spatial gap between the resonator-loaded dielectrics 3c and 3d that are directly adjacent to each other, and the displacement of the resonator-loaded dielectric 3 that is likely to occur due to repeated door opening and closing operations can be suppressed. .

実施の形態7.
図1から図3と図13を用いてこの発明の実施の形態7による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図13は、この発明の実施の形態7における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、図1の破線Cで示す扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部の拡大図である。図13において、互いに直交する方向で隣接する共振器装荷誘電体3cと3dは図3で示した導体パターン4と貫通スルーホール列5による短絡構造を有し、フレキシブル基板12を備える。
Embodiment 7 FIG.
An electromagnetic shield door according to Embodiment 7 of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 13 shows a resonator loaded dielectric 3 arranged on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 according to Embodiment 7 of the present invention. It is an enlarged view of the junction part of the resonator loading dielectrics 3c and 3d which adjoin in the direction orthogonal to each other in the corner part in the gap | interval of the door frame 2. FIG. In FIG. 13, the resonator loaded dielectrics 3 c and 3 d that are adjacent to each other in a direction orthogonal to each other have the short-circuit structure by the conductor pattern 4 and the through-through hole row 5 shown in FIG.

フレキシブル基板12は折り曲げ可能な特性を有する誘電体基板であり、フレキシブル基板12の片側表面には、実施の形態3のフレキシブル基板12と同様に、導体パターンが複数配置されており、各導体パターンは、共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4を電気的に接続している。このように、実施の形態7は、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部以外の構造は実施の形態1と同じ構造を有している。   The flexible substrate 12 is a dielectric substrate having a foldable characteristic, and a plurality of conductor patterns are arranged on one surface of the flexible substrate 12 in the same manner as the flexible substrate 12 of the third embodiment. The conductor patterns 4 respectively disposed on the resonator loaded dielectrics 3c and 3d are electrically connected. As described above, the seventh embodiment has the same structure as that of the first embodiment except for the joint portion between the resonator-loaded dielectrics 3c and 3d adjacent in the direction perpendicular to each other at the corner portion in the gap between the door 1 and the door frame 2. Have the same structure.

次に、実施の形態7による電磁シールド扉の動作について説明する。実施の形態7は、扉1と扉枠2の間隙におけるコーナー部以外の構造は実施の形態1と同じなので、扉1と扉枠2の間隙におけるコーナー部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the seventh embodiment will be described. Since the structure of the seventh embodiment is the same as that of the first embodiment except for the corner portion in the gap between the door 1 and the door frame 2, the electromagnetic wave propagating through the portion other than the corner portion in the gap between the door 1 and the door frame 2 is prevented. As in the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

また、実施の形態7では、扉1と扉枠2の間隙におけるコーナー部において、互いに直交する方向で隣接する共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4は、フレキシブル基板12に配置された導体パターンによって、実施の形態5と同様に電気的に接続されている。したがって、共振器装荷誘電体3cと3d間には電気的な隙間が存在せず、扉1と扉枠2の間隙のコーナー部を伝搬する電磁波においても、図5に示された広帯域な電磁シールド特性が得られる。   Further, in the seventh embodiment, the conductor patterns 4 arranged in the resonator loaded dielectrics 3c and 3d adjacent to each other in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2 are formed on the flexible substrate 12. Similar to the fifth embodiment, they are electrically connected by the arranged conductor pattern. Therefore, there is no electrical gap between the resonator-loaded dielectrics 3c and 3d, and the electromagnetic wave propagating through the corner portion of the gap between the door 1 and the door frame 2 is also a broadband electromagnetic shield shown in FIG. Characteristics are obtained.

また、実施の形態7では、互いに直交する方向で隣接する共振器装荷誘電体3cと3dの接合部1箇所において1つのフレキシブル基板を用いるので、共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4の電気的接続を簡易に行うことができる。すなわち、実施の形態7により、実施の形態1と同様の広帯域な電磁シールド特性を有し、かつ、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dの接合部の構造が簡易である電磁シールド扉を実現できる。   Further, in the seventh embodiment, since one flexible substrate is used at one place where the resonator-loaded dielectrics 3c and 3d are adjacent to each other in a direction orthogonal to each other, they are arranged on the resonator-loaded dielectrics 3c and 3d, respectively. Electrical connection of the conductor pattern 4 can be easily performed. That is, according to the seventh embodiment, the resonator-loaded dielectric having broadband electromagnetic shielding characteristics similar to those of the first embodiment and adjacent in the direction perpendicular to each other at the corner portion in the gap between the door 1 and the door frame 2 An electromagnetic shield door with a simple structure of the joint portion between 3c and 3d can be realized.

以上のように、この発明の実施の形態7における電磁シールド扉によれば、扉枠2と扉1の間隙における扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3dの各表面の導体パターン4間を電気的に接続する導電体が、フレキシブル基板12上に配置されるように構成したので、実施の形態1における効果に加え、扉枠2と扉1の間隙における扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3dにそれぞれ配置された導体パターン4の電気的接続を簡易に行うことができる。   As described above, according to the electromagnetically shielded door according to the seventh embodiment of the present invention, the resonator loaded dielectric 3c that is adjacent to each other at the corner portion of the door 1 and the door frame 2 in the gap between the door frame 2 and the door 1 is perpendicular. In addition to the effects of the first embodiment, the conductors that electrically connect the conductor patterns 4 on the respective surfaces 3d and 3d are arranged on the flexible substrate 12, so that the door frame 2 and the door 1 Electrical connection of the conductor patterns 4 respectively disposed in the resonator loaded dielectrics 3c and 3d that are adjacent to each other at the corners of the door 1 and the door frame 2 in the gap can be easily performed.

実施の形態8.
図1から図3と図14を用いてこの発明の実施の形態8による電磁シールド扉について説明する。図1から図3は、実施の形態1による電磁シールド扉と同じなので説明は省略する。図14は、この発明の実施の形態8における扉1と扉枠2の間隙の扉1の壁面側に複数配置された共振器装荷誘電体3のうち、図1の破線Cで示す扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部の拡大図である。図14において、共振器装荷誘電体3cと3dの隙間の間隔はdで、dは電磁シールド特性が要求される周波数帯域の上限周波数fmaxの2分の1波長の寸法となっている。このように、実施の形態8は、扉1と扉枠2の間隙におけるコーナー部において互いに直交する方向で隣接する共振器装荷誘電体3cと3dとの接合部以外の構造は実施の形態1と同じ構造を有している。
Embodiment 8 FIG.
An electromagnetic shield door according to an eighth embodiment of the present invention will be described with reference to FIGS. 1 to 3 and FIG. Since FIG. 1 to FIG. 3 are the same as the electromagnetic shield door according to the first embodiment, description thereof is omitted. FIG. 14 shows a resonator loaded dielectric 3 arranged in plural on the wall surface side of the door 1 in the gap between the door 1 and the door frame 2 in Embodiment 8 of the present invention. It is an enlarged view of the junction part of the resonator loading dielectrics 3c and 3d which adjoin in the direction orthogonal to each other in the corner part in the gap | interval of the door frame 2. FIG. In FIG. 14, the gap between the resonator-loaded dielectrics 3c and 3d is d, and d is a half wavelength dimension of the upper limit frequency f max of the frequency band in which electromagnetic shielding characteristics are required. Thus, in the eighth embodiment, the structure other than the joint portion between the resonator-loaded dielectrics 3c and 3d adjacent in the direction orthogonal to each other at the corner portion in the gap between the door 1 and the door frame 2 is the same as that of the first embodiment. Have the same structure.

次に、実施の形態8による電磁シールド扉の動作について説明する。実施の形態8は、扉1と扉枠2の間隙におけるコーナー部以外の構造は実施の形態1と同じなので、扉1と扉枠2の間隙におけるコーナー部以外の箇所を伝搬する電磁波に対しては、実施の形態1と同様に、図5に示された広帯域な電磁シールド特性が得られる。   Next, the operation of the electromagnetic shield door according to the eighth embodiment will be described. In the eighth embodiment, since the structure other than the corner portion in the gap between the door 1 and the door frame 2 is the same as that in the first embodiment, the electromagnetic wave propagating through the portion other than the corner portion in the gap between the door 1 and the door frame 2 is prevented. As in the first embodiment, the broadband electromagnetic shielding characteristics shown in FIG. 5 can be obtained.

また、図14に示すように、扉1と扉枠2の間隙におけるコーナー部において、共振器装荷誘電体3cと3dの隙間の間隔がdとなっているので、周波数がfmax以下である電磁波は、共振器装荷誘電体3cと3dの隙間を伝搬する際に指数関数的に減衰する。したがって、扉1と扉枠2の間隙におけるコーナー部において、共振器装荷誘電体3cと3d間の隙間を伝搬する電磁波においても、fmax以下の周波数において広帯域な電磁シールド特性を有し、かつ、隣接する共振器装荷誘電体3c,3dの接合部の構造が簡易である電磁シールド扉を実現できる。 Further, as shown in FIG. 14, in the corner portion in the gap between the door 1 and the door frame 2, the gap between the resonator loaded dielectrics 3c and 3d is d, so that the electromagnetic wave having a frequency of f max or less. Is exponentially attenuated when propagating through the gap between the resonator loaded dielectrics 3c and 3d. Therefore, even in the electromagnetic wave propagating through the gap between the resonator loaded dielectrics 3c and 3d at the corner portion in the gap between the door 1 and the door frame 2, it has a broadband electromagnetic shielding characteristic at a frequency of f max or less, and An electromagnetic shield door having a simple structure of the joint portion between the adjacent resonator-loaded dielectrics 3c and 3d can be realized.

実施の形態8によれば、扉1と扉枠2とが非接触であるため、扉1の開閉回数が多くなった場合にも電磁シールド特性が劣化せず、定期的なメンテナンスが不要となる。   According to the eighth embodiment, since the door 1 and the door frame 2 are not in contact with each other, even when the number of times of opening and closing the door 1 increases, the electromagnetic shielding characteristics do not deteriorate, and periodic maintenance is not necessary. .

また、実施の形態8によれば、電磁シールド特性が得られる周波数帯域は、共振器装荷誘電体3に配置された共振構造を有する導体パターン4が共振する周波数によって決まるため、誘電体基板を用いた共振構造の製作が比較的容易である、GHz帯やミリ波帯等の高周波帯域において、有効な電磁シールド特性を実現できる。   Further, according to the eighth embodiment, the frequency band in which electromagnetic shielding characteristics can be obtained is determined by the frequency at which the conductor pattern 4 having the resonance structure arranged in the resonator-loaded dielectric 3 resonates. Therefore, it is possible to realize effective electromagnetic shielding characteristics in a high frequency band such as a GHz band or a millimeter wave band, which is relatively easy to manufacture.

また、実施の形態8によれば、導体パターン4a,4b,4c,4d,4e,4f,4g,4hのY方向寸法La,Lb,Lc,Ld,Le,Lf,Lg,Lhを、それぞれ周波数fa,1.5fa,2fa,2.5fa,3.5fa,4fa,5fa,6.5faにおいて、共振器装荷誘電体3上で4分の1波長となるように分散化することにより、周波数faから7.5faまでの広帯域な電磁シールド特性を実現できる。   Further, according to the eighth embodiment, the Y-direction dimensions La, Lb, Lc, Ld, Le, Lf, Lg, and Lh of the conductor patterns 4a, 4b, 4c, 4d, 4e, 4f, 4g, and 4h are respectively set to frequencies. In fa, 1.5fa, 2fa, 2.5fa, 3.5fa, 4fa, 5fa, and 6.5fa, the frequency fa is obtained by dispersing the frequency to be a quarter wavelength on the resonator-loaded dielectric 3. To 7.5 fa wide electromagnetic shielding characteristics can be realized.

以上のように、この発明の実施の形態8における電磁シールド扉によれば、導電性の扉1と、扉枠2に配置された導電性の扉1と、扉1を閉めた状態における扉枠2と扉1の間隙において、扉1の壁面と扉枠2の壁面の少なくとも一方の周囲に沿って複数の共振器装荷誘電体3を対向面と非接触となるように配置し、共振器装荷誘電体3は表面に所定の幅を有し扉1または扉枠2と電気的に接続された導体パターン4を扉1と扉枠2の周方向に備え、導体パターン4の所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3d間の隙間寸法が、電磁シールド特性が要求される上限周波数の2分の1波長以下であるように構成したので、電磁シールド特性が劣化せず定期的なメンテナンスが不要であり、主にGHz帯以上の高周波帯において電磁シールド特性を有し、さらに、fmax以下の周波数において広帯域な周波数に特化した電磁シールド特性を得ることができ、かつ、扉1および扉枠2のコーナー部において互いに直行に隣接する共振器装荷誘電体3cと3dの接合部の構造が簡易となる。 As described above, according to the electromagnetically shielded door according to the eighth embodiment of the present invention, the conductive door 1, the conductive door 1 disposed on the door frame 2, and the door frame in a state in which the door 1 is closed. In the gap between the door 2 and the door 1, a plurality of resonator-loaded dielectrics 3 are arranged so as to be in non-contact with the opposite surface along at least one of the wall surface of the door 1 and the wall surface of the door frame 2. The dielectric 3 has a conductor pattern 4 having a predetermined width on the surface and electrically connected to the door 1 or the door frame 2 in the circumferential direction of the door 1 and the door frame 2. The gap dimension between the resonator-loaded dielectrics 3c and 3d, which are set to a quarter wavelength of the frequency within the band where the shield characteristic is required and is adjacent to each other at the corners of the door 1 and the door frame 2, is electromagnetic Configured so that the shield characteristic is less than half the wavelength of the upper limit frequency required Were so, routine maintenance electromagnetic shielding characteristics do not deteriorate is unnecessary, mainly have electromagnetic shielding properties in a GHz band or a high frequency band, further, specializing in wide frequency at frequencies below f max Electromagnetic shielding characteristics can be obtained, and the structure of the joint portion between the resonator-loaded dielectrics 3c and 3d that are adjacent to each other at the corner portions of the door 1 and the door frame 2 is simplified.

なお、本願発明はその発明の範囲内において、各実施の形態の自由な組み合わせ、あるいは各実施の形態の任意の構成要素の変形、もしくは各実施の形態において任意の構成要素の省略が可能である。   In the present invention, within the scope of the invention, any combination of the embodiments, or any modification of any component in each embodiment, or omission of any component in each embodiment is possible. .

1 扉、2 扉枠、3,3a〜3d 共振器装荷誘電体、4,4a〜4h 導体パターン、5,5a〜5d 貫通スルーホール列、6 導電性ガスケット、7 ヒンジ、8 開閉レバー、9 銅箔テープ、10 導体ガスケット、11 誘電体、12 フレキシブル基板。   DESCRIPTION OF SYMBOLS 1 Door, 2 Door frame, 3, 3a-3d Resonator loading dielectric, 4, 4a-4h Conductor pattern, 5, 5a-5d Through-through hole row, 6 Conductive gasket, 7 Hinge, 8 Opening / closing lever, 9 Copper Foil tape, 10 conductor gasket, 11 dielectric, 12 flexible substrate.

Claims (5)

導電性の扉枠と、
前記扉枠に配置された導電性の扉と、
前記扉を閉めた状態における前記扉枠と前記扉の間隙において、前記扉の壁面と前記扉枠の壁面の少なくとも一方の周囲に沿って複数の誘電体を対向面と非接触となるように配置し、
前記誘電体は表面に所定の幅を有し前記扉または前記扉枠と電気的に接続された導体パターンを前記扉と扉枠の周方向に備え、
前記導体パターンの前記所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、
隣接する前記誘電体の各表面の導体パターン間を導電体により電気的に接続する
ことを特徴とする電磁シールド扉。
A conductive door frame;
A conductive door disposed on the door frame;
In the gap between the door frame and the door when the door is closed, a plurality of dielectrics are arranged so as to be in non-contact with the opposing surface along at least one of the wall surface of the door and the wall surface of the door frame. And
The dielectric has a predetermined width on the surface and a conductive pattern electrically connected to the door or the door frame in the circumferential direction of the door and the door frame,
The predetermined width of the conductor pattern is set to a quarter wavelength of a frequency within a band where electromagnetic shielding characteristics are required;
An electromagnetic shield door, wherein conductor patterns on the surfaces of adjacent dielectrics are electrically connected by a conductor.
隣接する前記誘電体間の隙間に導電体または誘電体を配置する
ことを特徴とする請求項1記載の電磁シールド扉。
The electromagnetic shield door according to claim 1, wherein a conductor or a dielectric is disposed in a gap between adjacent dielectrics.
前記誘電体の側面に導電性塗料または導体パターンを配置し、当該誘電体の側面に配置した前記導電性塗料または導体パターンと前記誘電体間の隙間に配置された導電体または誘電体とを電気的に接続する
ことを特徴とする請求項2記載の電磁シールド扉。
Conductive paint or conductor pattern is disposed on the side surface of the dielectric, and the conductive paint or conductor pattern disposed on the side surface of the dielectric and the conductor or dielectric disposed in the gap between the dielectrics are electrically connected. The electromagnetic shielding door according to claim 2, wherein the electromagnetic shielding door is connected.
前記導体パターン間を電気的に接続する導電体が、フレキシブル基板上に配置される
ことを特徴とする請求項1から請求項3のうちのいずれか1項記載の電磁シールド扉。
The electromagnetic shield door according to any one of claims 1 to 3, wherein a conductor that electrically connects the conductor patterns is disposed on a flexible substrate.
導電性の扉枠と、
前記扉枠に配置された導電性の扉と、
前記扉を閉めた状態における前記扉枠と前記扉の間隙において、前記扉の壁面と前記扉枠の壁面の少なくとも一方の周囲に沿って複数の誘電体を対向面と非接触となるように配置し、
前記誘電体は表面に所定の幅を有し前記扉または前記扉枠と電気的に接続された導体パターンを前記扉と扉枠の周方向に備え、
前記導体パターンの前記所定の幅を電磁シールド特性が要求される帯域内の周波数の4分の1波長に設定し、
隣接する前記誘電体間の隙間寸法が、前記電磁シールド特性が要求される上限周波数の2分の1波長以下である
ことを特徴とする電磁シールド扉。
A conductive door frame;
A conductive door disposed on the door frame;
In the gap between the door frame and the door when the door is closed, a plurality of dielectrics are arranged so as to be in non-contact with the opposing surface along at least one of the wall surface of the door and the wall surface of the door frame. And
The dielectric has a predetermined width on the surface and a conductive pattern electrically connected to the door or the door frame in the circumferential direction of the door and the door frame,
The predetermined width of the conductor pattern is set to a quarter wavelength of a frequency within a band where electromagnetic shielding characteristics are required;
The electromagnetic shielding door, wherein a gap between adjacent dielectrics has a half wavelength or less of an upper limit frequency at which the electromagnetic shielding characteristics are required.
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