JPH0781334B2 - A structure for housing radio wave equipment - Google Patents
A structure for housing radio wave equipmentInfo
- Publication number
- JPH0781334B2 JPH0781334B2 JP62005229A JP522987A JPH0781334B2 JP H0781334 B2 JPH0781334 B2 JP H0781334B2 JP 62005229 A JP62005229 A JP 62005229A JP 522987 A JP522987 A JP 522987A JP H0781334 B2 JPH0781334 B2 JP H0781334B2
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- outside
- building
- band
- radio wave
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
Landscapes
- Building Environments (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Description
【発明の詳細な説明】 この発明は工場、オフイス、体育館、催し物会場などの
如きいわゆる大部屋の構造をしている建物に関する改良
であり、特にその内部での相互の無線通信ないしテレメ
トリー等の電波応用を外部からシールドしつつ行うこと
と、その内部と外界との間の自在な無線通信とを共存さ
せるため工夫に関する。The present invention relates to an improvement of a building having a so-called large room structure such as a factory, office, gymnasium, and venue for entertainment, and in particular, mutual radio communication or radio waves such as telemetry inside the building. The present invention relates to a device for shielding the application from the outside and coexistence of free wireless communication between the inside and the outside.
最近は上記の如き建物内部同志の至近距離の通信であつ
てもケーブルを介した有線通信にかわつて拘束物を持た
ない無線通信を通話や計測やデータ伝送に利用せんとす
ることが広く行われている。利用し得る信号メデイアと
しては、光、超音波、電波、静電ないし電磁誘導などが
あるが、技術上の完成度、信頼性、設計上の自由度ない
し伝送量の大きいことなどの点で総合評価として電波に
まさるものはない。しかるに、電波の有する一番の問題
点は混信ないし干渉による妨害であり、これは受ける方
と出す方の両方の現象を考えねばならないが、電磁界現
象の可逆性を前提に考えれば両者は本質的に共通のもの
である。すなわち一般に、自由空間においては1つの周
波数を複数の目的に共用することはむずかしい。これは
単に異るシステム同志が同一周波数を用いつつも相互に
干渉をおこさぬよう、もしくは干渉が無害であり得るよ
うに、時間的あるいは空間的に使いわければよいという
ような当座の個々の問題に留まらず、広く一般的な電波
行政上の問題として扱われている。更に、実際には意図
して発した電磁波のみならず、意図せざる発射、すなわ
ち諸電子装置による電磁環境汚染の問題まで関連する。Recently, it has been widely practiced to use wireless communication, which has no restraint, instead of wire communication via cables, for telephone calls, measurements, and data transmission, even in the case of short-distance communication within the building as described above. There is. The signal media that can be used include light, ultrasonic waves, radio waves, electrostatic or electromagnetic induction, but in terms of technical perfection, reliability, freedom of design, and large transmission volume, etc. There is nothing better than radio waves for evaluation. However, the biggest problem with radio waves is interference due to interference or interference, which requires consideration of both the receiving and emitting phenomena, but if we consider the reversibility of the electromagnetic field phenomenon, both are essential. Are common to all. That is, it is generally difficult to share one frequency for multiple purposes in free space. This is because the different systems use the same frequency but do not interfere with each other, or the interference can be harmless, such that they can be used either temporally or spatially. It is not only a problem, but is widely treated as a general radio wave administrative problem. Furthermore, not only the electromagnetic waves actually emitted intentionally, but also unintentional emission, that is, the problem of electromagnetic environmental pollution by various electronic devices is actually involved.
そこで、電波利用機器のある一群のものが、移動するこ
とがあつても必ずある閉空間に留りつつ稼動するような
場合、換言すれば無線的な通信を行うが相手は必ずある
空間内にあるような場合、外界からの妨害と外界への妨
害の両方をともに遮断するために該空間を導体又は電波
吸収体の壁にて意図的に閉じ切つてしまうことが行われ
る。これはたとえばある大きなへやとか、ホールとか、
ある建物のある階とかにおいてテレメトリーシステムや
ページングシステム、コードレステレホン、ワイヤレス
マイク、ないし無線式のLAN(ローカルエリアネツトワ
ーク)等々を他との干渉なく利用したいときにはよく採
用される手法である。Therefore, if a group of radio wave-using devices always operates while staying in a certain closed space even if it moves, in other words, wireless communication is performed, but the other party is always in a certain space. In some cases, the space is intentionally closed by the wall of the conductor or the electromagnetic wave absorber in order to block both the disturbance from the outside world and the disturbance to the outside world. This is, for example, a big room, a hall,
This method is often used when you want to use a telemetry system, a paging system, a cordless telephone, a wireless microphone, or a wireless LAN (local area network) on a floor of a building without interfering with others.
しかるにこのような、“シールドルーム”的手法による
と、当然のことながら該空間から意図的に外部との間の
無線通信を行うこともまた同時に阻害されてしまう。こ
れはある場合非常に不便である。たとえばラジオもテレ
ビも受からなくなるか、感度が悪くて音質や画質が極度
におちる。また前記のLANの利用システムそのものが同
時に外界の無線局ないし通信衛生などとの間にまた別の
無線リンクをもうけたい場合などもあり得る。そのよう
な場合、専用のアンテナや無線送受信機をこの空間の外
部にもうけ、それとのやりとりを専用のケーブルなどで
行わなければならないことになる。However, according to such a "shielded room" method, of course, intentionally performing wireless communication with the outside from the space is also hindered at the same time. This is very inconvenient in some cases. For example, both radio and television may not be available, or the sensitivity may be poor and the sound quality and image quality may be severe. There may be a case where the LAN utilization system itself wants to establish another wireless link with a wireless station or communication hygiene in the outside world at the same time. In such a case, a dedicated antenna or wireless transceiver must be provided outside this space, and communication with it must be performed using a dedicated cable or the like.
本発明はそのような不自由さを解消せんとするものであ
り、特にある目的閉空間を前記の如く意図的に“シール
ド”するに当つて、該シールドの効果に意図的に周波数
選択性をもうけ、そのシールド効果のある周波数帯にお
いて前記テレメトリーシステムないしLANなどを運用
し、シールド効果のない、もしくは実用上十分妨害なく
電磁波のやりとりができる周波数帯において外界との無
線通信を運用する、というような利用方法が可能な電波
利用設備を収容する建造物に関する。The present invention is intended to eliminate such inconvenience, and in particular, in intentionally “shielding” a certain target closed space as described above, the effect of the shield is intentionally frequency-selective. In addition, operate the telemetry system or LAN in the frequency band that has the shield effect, and operate the wireless communication with the outside world in the frequency band that does not have the shield effect or the electromagnetic wave can be exchanged without any practical interference. The present invention relates to a building that accommodates radio wave utilization equipment that can be used in various ways.
前記波長選択性の“シールドルーム”を実現するため
に、本発明においては該シールドルームの地上部の隔壁
の少くとも一部もしくは全部を波長選択性のある材料あ
るいは構造もしくはその双方により構成する。In order to realize the wavelength-selective "shield room", in the present invention, at least a part or all of the partition walls above the ground of the shield room are made of a wavelength-selective material and / or structure.
第1図はかかる方式の実現のための壁材料の一実施例を
示すもので、これにおいて、電磁波的立場からのポイン
トは導体11が無数の小開口12を有する点にあり、かかる
パンチングプレートないし極端な場合は金網状の導体が
切れ目なく目的空間をおおいつくす如くもうけられる。
このようなパンチングプレートないし金網の電磁波透過
性は、最も大雑把に言つてその孔ないし網の目の寸法、
特に長径が半波長以上をとる、もしくはその周長が波長
以上となる如き短い波長にとつては大略透明に見え、そ
れ以下となる如き長波長にとつては大略もしくは十分完
全に反射性は連続導体と等価に見える。このことよりた
とえば孔もしくは網の目の径を10cm程度にしておけば1.
5GHzあたりを境にそれ以上では透過性、それ以下では反
射性のかべで出来た閉空間が実現できる。これにより該
閉空間の内部で800MHz〜1GHz以下の周波数を用いるLAN
やテレメトリーは内外間の干渉なく行い得る一方、2GHz
以上においては壁に妨害されることなく通信衛星との間
に無線リンクをもうけることができる。また外界からの
自然光や遠赤外線等はほぼ自在にこの金網を通過できる
ので、目的空間の採光に支障を来すことはない。その場
合、この金網はガラスないし透光性のプラスチツクの板
や膜と重層して併用される。FIG. 1 shows an embodiment of a wall material for realizing such a system. In this, the point from an electromagnetic wave standpoint is that the conductor 11 has innumerable small openings 12, and such punching plate or In an extreme case, the wire mesh-like conductor is made to cover the target space without interruption.
The electromagnetic wave permeability of such a punching plate or wire mesh is most roughly described as the size of the holes or the mesh.
In particular, it appears to be almost transparent at short wavelengths whose major axis is more than half a wavelength or whose perimeter is more than a wavelength, and it is almost or completely completely continuous at long wavelengths that are less than that wavelength. Looks equivalent to a conductor. Therefore, for example, if the diameter of the holes or mesh is set to about 10 cm, 1.
Around 5 GHz, a closed space made of a translucent wall above that and a reflective wall below that can be realized. As a result, a LAN using a frequency of 800 MHz to 1 GHz or less inside the closed space
And telemetry can be performed without interference between inside and outside, while 2GHz
In the above, it is possible to establish a wireless link with the communication satellite without being obstructed by the wall. Further, natural light and far infrared rays from the outside world can pass through the wire net almost freely, so that it does not hinder the lighting of the target space. In this case, this wire mesh is used in combination with glass or a transparent plastic plate or film.
第2図はまた別な実施例を示すもので、この場合壁は多
層構造を成し、特にそのεないしμもしくはその両者が
互いに有意に異る少くとも2種類の物質が交互に重層さ
れた構造を有する。すなわち第1の物質21と第2の物質
22はその電磁波的な波動インピーダンスが有意に異るた
め、このような厚み方向への周期構造はその反射および
透過性にいちじるしい山谷を生ずる。この原理はいわゆ
るダイクロイツクミラーの原理として公知のものであ
り、バンドパスフイルタないしバンドストツプフイルタ
として光学的には広く利用されているものである。たと
えばある周波数近辺をストツプバンドとしたい場合、各
層のその周波数近傍における電磁波的な厚み(伝搬速度
により決る)が大略1/2波長になるようにする。発泡ポ
リエチレンを第1の物質、密なる(発泡せぬ)ポリエチ
レンを第2の物質とすると、前者はほぼ空気と等価、後
者はそれより有意に大なるεを有する(大略2.3程度)
ので上記手法によるダイクロイツクミラーとして有効に
作用することができる。この場合、第1反射帯を大略8G
Hz前後にせんとすると上記第1の物質の厚さは約1.9c
m、第2の物質の厚さは波長がその中では約2/3に短くな
るので約1.3cm程度とする。これらの物質を数層ないし
十数層重ねると8GHzあたりでは良好な反射性と阻止性を
呈し、逆に各層が1/4波長およびその奇数倍に見える、4
GHz帯や12GHz帯では透過性を呈する。それ故にこのよう
な重層体を壁とする密室の内部においては外界と相互干
渉することなく低電力テレメーターや無線式LANを利用
することができる一方、衛星通信や衛星放送に汎用され
る4GHz帯と12GHz帯ではとどこおりなく該通信や放送の
受信を行なうことができる。尚、この構造は各層が1/4
波長以下に見える4GHzより低域でも十分に透明であり、
UHFやVHFのTV、FM放送ないし中、短波のラジオなどへも
全く実用上妨害とならない。FIG. 2 shows another embodiment, in which the wall has a multi-layer structure, in particular at least two substances whose ε or μ or both are significantly different from each other are alternately layered. Have a structure. That is, the first substance 21 and the second substance
Since the wave impedance of 22 is significantly different from that of electromagnetic waves, such a periodic structure in the thickness direction produces peaks and valleys that are remarkable in its reflection and transmission properties. This principle is known as a so-called dichroic mirror principle, and is optically widely used as a bandpass filter or a bandstop filter. For example, when it is desired to set the stop band near a certain frequency, the electromagnetic thickness (determined by the propagation velocity) of each layer in the vicinity of the frequency is set to about 1/2 wavelength. If foamed polyethylene is the first substance and dense (non-foamed) polyethylene is the second substance, the former is almost equivalent to air, and the latter has a significantly larger ε (approximately 2.3).
Therefore, it can effectively act as a dichroic mirror by the above method. In this case, the first reflection band is approximately 8G
The thickness of the above first substance is about 1.9c when it is measured at around Hz.
m, the thickness of the second material is about 1.3 cm because the wavelength is shortened to about 2/3. When several layers or dozens of layers of these materials are stacked, they show good reflectivity and blocking property around 8GHz, and on the contrary, each layer looks at 1/4 wavelength and its odd multiple, 4
It is transparent in the GHz and 12 GHz bands. Therefore, low power telemeters and wireless LANs can be used without interfering with the outside world inside a closed room with such a multi-layered structure, while the 4GHz band commonly used for satellite communication and satellite broadcasting. And, in the 12 GHz band, the communication and broadcast can be received almost anywhere. Each layer of this structure is 1/4
It is sufficiently transparent even in the low range below 4 GHz, which appears below the wavelength,
Practically no interference with UHF or VHF TV, FM broadcasting or medium or short wave radio.
周波数選択性の反射および透過阻止性はまた壁に無数の
共振器を配列せしめることによつても実現し得る。すな
わち第3図は本発明の第3の実施例を示すもので、これ
において壁30は母体としては発泡ポリエチレンなどの本
質的に電磁波に対して殆んど何も妨害も与えない物質で
出来ているが、その中に無数の共振器31を含んでいる。
この場合共振器31は円環であり、阻止周波数帯はその周
長が1波長、ないし径が半波長のなる程度の周波数領域
に生ずる。円環のかわりに四角その他の一周の閉路を成
すわくでもよいこれらの環ないしわく状の導体が無数に
体積分布的にかべ30の中に分布されている。たとえば8G
Hz帯を阻止反射帯とする場合、厚さ25〜50μm程度、平
均直径1.8cm程度の銅箔で出来たリングを厚さ30cm位に
なる発泡ポリエチレンの壁の中に均等に分布させる。Frequency selective reflection and transmission blocking can also be achieved by arranging a myriad of resonators in the wall. That is, FIG. 3 shows a third embodiment of the present invention, in which the wall 30 is made of a material such as foamed polyethylene that does not substantially interfere with electromagnetic waves. However, it contains innumerable resonators 31 in it.
In this case, the resonator 31 is a ring, and the stop frequency band is generated in the frequency region where the circumference is one wavelength or the diameter is half a wavelength. Instead of a ring, a square or other ring-shaped or ring-shaped conductor which may form a closed loop is innumerably distributed in the wall 30 in volume distribution. 8G for example
When the Hz band is used as the blocking reflection band, a ring made of copper foil having a thickness of about 25 to 50 μm and an average diameter of about 1.8 cm is evenly distributed in the foamed polyethylene wall having a thickness of about 30 cm.
このような銅箔のリングは一例としてプリント基板をエ
ツチングないし打抜加工して容易に得られる。しかし必
ずしも銅である必要はなく、鉄などでもよい。うすい鉄
板に銅メツキしたものを打抜加工して得てもよい。また
銅の上に銀、金などをメツキすればそれ自信の共振器と
してのQや、耐候性などを向上せしめることができる。Such a copper foil ring can be easily obtained, for example, by etching or punching a printed circuit board. However, it does not necessarily have to be copper, and may be iron or the like. It may be obtained by punching a thin iron plate with copper plating. Further, by plating silver or gold on copper, the Q as a resonator of its own and the weather resistance can be improved.
リングの分布密度は、リング同志が接触し合わないとい
う条件でリング間の平均距離がその直径と大略等しいよ
うな状態が好ましい。また分布様式は規則性を有するこ
とが製作上は好都合である。この場合、リングの軸の方
向は大略阻止を目的とする電波の進行方向にそろえる
(平行では効果がない)。しかし将にそのような努力を
せずにランダムな方向に分布せしめても、分布の密度を
約倍にすれば本質的に同じ効果が得られる。この目的に
空間分布する共振器として利用できる単位共振器として
はリングのほかに棒、円板、球、ないしは第4図aに示
すようならせん状導体の断片、ないし同図bに示すよう
に2個一対の導体片をローデイングキヤパシタとしてそ
の間をインダクタで結絡したもの、等が有効に利用でき
る。The distribution density of the rings is preferably such that the average distance between the rings is approximately equal to their diameter, provided that the rings do not contact each other. In addition, it is convenient in manufacturing that the distribution pattern has regularity. In this case, the direction of the ring axis is approximately aligned with the traveling direction of the electric wave, which is aimed at blocking (parallel is ineffective). However, even if they are distributed in random directions without such efforts, essentially the same effect can be obtained by doubling the distribution density. Unit resonators that can be used as spatially distributed resonators for this purpose include, in addition to rings, rods, disks, spheres, or spiral conductor fragments as shown in FIG. 4a, or as shown in FIG. 4b. It is possible to effectively use a pair of two conductor pieces which are used as loading capacitors and which are entwined with an inductor.
本発明の実施のために利用できる波長選択性の反射・透
過特性を有する壁は、また導体の表皮効果を利用するこ
とでも実現できる。すなわち一般に電磁波が良く反射す
るには、導体面の厚さとして、いわゆるスキンデツプス
の値、 f=周波数 μ=導体の誘電率(自由空間と同じと考える) η=導電率(体積抵抗率の逆数) C=光速 なる値より十分厚くなければならず、逆にこれより十分
に薄い導体面においては反射はほとんどおこらず透過性
を呈する。このような性質を利用した本発明の第4の実
施例においては、たとえば第5図に示す如くドーム状の
膜による半球かく状の建造物50は公知の如く与圧装置51
によりその内外にわずかな気圧差を維持することにより
ふくらんで建造物たるにふさわしい形状を維持するわけ
であるが、この膜として公知の如くテフロン(登録商
標)等のフツ素樹脂をガラス繊維の布に焼付けたものを
用いるに当り、追加的に厚さ3μm程度のアルミニウム
の薄層を重層するか、もしくは膜に蒸着、スパツタ、化
学メツキと電気メツキの併用等により被着したものを用
いる。アルミニウムの導電率は約3×10-6Ω・cmである
からこれは上記表皮効果由来のカツトオフ周波数として
大略1GHzを与える。すなわちこのような薄い導電層つき
の膜にようエアドームの中では大略2〜3GHz以上の電磁
波は内外間の干渉を生ずることなく低電力テレメータ、
LAN等に独立して利用できるが、大略300〜500MHz以下の
周波数においては内外間に阻害なく無線通信を行い得
る。この種のエアドームにおいては膜の透光性や通気性
を一つの重要な性質として期待する場合があるが、その
要求に前記導電膜がさからわないようにするためには細
かな格子目状のパターンを成さしめ、孔の部分において
通気性および透光性を確保する。格子目のピツチを大略
数mm以下にすれば数十GHzまでは一様な導体に見えるの
で前記主旨には矛盾しない。この場合、適用すべき導電
率は格子目の平均導電率となることに注意を要する。A wall having wavelength-selective reflection / transmission characteristics that can be used for implementing the present invention can also be realized by utilizing a skin effect of a conductor. That is, in general, in order for electromagnetic waves to be reflected well, the thickness of the conductor surface is the so-called skin depth value, f = frequency μ = permittivity of conductor (assumed to be the same as free space) η = conductivity (reciprocal of volume resistivity) C = thickness of light Must be sufficiently thicker than value, conversely thinner conductor surface than this In the case of, there is almost no reflection and it is transparent. In the fourth embodiment of the present invention which utilizes such a property, a hemispherical structure 50 having a dome-shaped membrane as shown in FIG.
By maintaining a slight pressure difference between the inside and the outside, the shape suitable for building is maintained by maintaining a slight difference in pressure between the inside and outside. In using the baked product, a thin layer of aluminum having a thickness of about 3 μm is additionally laminated, or the film is deposited by vapor deposition, sputtering, combined use of chemical plating and electric plating, or the like. Since the conductivity of aluminum is about 3 × 10 −6 Ω · cm, this gives approximately 1 GHz as the cutoff frequency derived from the skin effect. In other words, in an air dome such as a film with such a thin conductive layer, electromagnetic waves of approximately 2 to 3 GHz or more are low power telemeters without causing interference between the inside and outside,
It can be used independently for LAN, etc., but at frequencies below 300-500MHz, wireless communication can be performed between inside and outside without interruption. In this type of air dome, the transparency and air permeability of the film may be expected as one of important properties, but in order to prevent the conductive film from meeting the requirement, a fine grid pattern is required. To ensure breathability and translucency at the holes. If the pitch of the grid is set to about a few mm or less, it looks like a uniform conductor up to several tens of GHz, so it does not contradict the above point. In this case, it should be noted that the conductivity to be applied is the average conductivity of the lattice.
以上に示した如く本発明によれば目的とする閉空間があ
る周波数帯ではシールドされ、また別な周波数帯ではシ
ールドされないので、前者の周波数帯において外界と相
互干渉することなく低電力テレメトリーや無線式LANな
どの電磁波応用を実行でき、かつ後者の周波数帯では外
界との間に無線伝送をつつがなく行うことができて至便
である。As described above, according to the present invention, the target closed space is shielded in a certain frequency band and is not shielded in another frequency band. Therefore, in the former frequency band, low power telemetry or wireless communication can be performed without mutual interference with the outside world. This is convenient because it can be used for electromagnetic wave applications such as LAN expression, and wireless transmission between the outside frequency and the outside frequency is possible in the latter frequency band.
第1、2、3、5図は各々本発明の各異る実施例を示す
ものであり、第4図はその内第3図により説明する実施
例における要素の一部を示すものである。FIGS. 1, 2, 3, and 5 show different embodiments of the present invention, and FIG. 4 shows some of the elements in the embodiment described with reference to FIG.
Claims (1)
択的な反射および透過特性を有し、その中に収容される
電波利用設備をしてその透過域の周波数帯を用いて建物
内外間の無線通信を、またその阻止域もしくは反射域の
周波数帯を用いて該建物内部での電磁波応用を外部の電
磁界に妨害され、もしくは逆にそれを妨害することな
く、行い得しめる如く構成せられたることを特徴とす
る、閉空間を仕切る建造物。1. The inside and outside partition walls on the ground have frequency-selective reflection and transmission characteristics for radio waves, and the radio wave utilization equipment accommodated therein is used to construct the inside and outside of the building by using the frequency band in the transmission range. Between the wireless communication between them, and also by using the frequency band of the stop band or the reflection band, the electromagnetic wave application inside the building can be performed without being disturbed by the external electromagnetic field, or conversely, without being disturbed. A building that divides an enclosed space, characterized by being pushed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62005229A JPH0781334B2 (en) | 1987-01-13 | 1987-01-13 | A structure for housing radio wave equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62005229A JPH0781334B2 (en) | 1987-01-13 | 1987-01-13 | A structure for housing radio wave equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63197399A JPS63197399A (en) | 1988-08-16 |
| JPH0781334B2 true JPH0781334B2 (en) | 1995-08-30 |
Family
ID=11605356
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62005229A Expired - Fee Related JPH0781334B2 (en) | 1987-01-13 | 1987-01-13 | A structure for housing radio wave equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0781334B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6147302A (en) * | 1997-02-05 | 2000-11-14 | Nippon Paint Co., Ltd. | Frequency selective electromagnetic wave shielding material and a method for using the same |
| DE10033259C2 (en) * | 2000-07-10 | 2003-06-26 | Univ Braunschweig Tech | Optical component |
| JP2007287752A (en) * | 2006-04-12 | 2007-11-01 | Orient Sokki Computer Kk | Electromagnetic wave shielding sheet manufacturing method and electromagnetic wave shielding sheet |
| JP2016171138A (en) * | 2015-03-11 | 2016-09-23 | 株式会社国際電気通信基礎技術研究所 | Shield structure |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS555719A (en) * | 1978-06-28 | 1980-01-16 | Suzuki Yasuo | Centrifuge |
| JPS58188193A (en) * | 1982-04-28 | 1983-11-02 | 住友電気工業株式会社 | radio wave absorber |
| JPS594696U (en) * | 1982-07-02 | 1984-01-12 | 日本電気株式会社 | radio wave absorber |
| JPS59205834A (en) * | 1983-05-09 | 1984-11-21 | Japan Radio Co Ltd | Radio communication system in radio wave shielding building |
| JPS60257198A (en) * | 1984-06-01 | 1985-12-18 | グレ−スジャパン株式会社 | Resonance type radio wave absorber |
-
1987
- 1987-01-13 JP JP62005229A patent/JPH0781334B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63197399A (en) | 1988-08-16 |
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| LAPS | Cancellation because of no payment of annual fees |