JPH10117087A - Structure for reducing reflection interference of building - Google Patents
Structure for reducing reflection interference of buildingInfo
- Publication number
- JPH10117087A JPH10117087A JP28900296A JP28900296A JPH10117087A JP H10117087 A JPH10117087 A JP H10117087A JP 28900296 A JP28900296 A JP 28900296A JP 28900296 A JP28900296 A JP 28900296A JP H10117087 A JPH10117087 A JP H10117087A
- Authority
- JP
- Japan
- Prior art keywords
- radio wave
- wave absorbing
- radio
- building
- wall
- 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.)
- Granted
Links
- 230000005684 electric field Effects 0.000 claims abstract description 16
- 229910000859 α-Fe Inorganic materials 0.000 abstract description 44
- 229910052782 aluminium Inorganic materials 0.000 abstract description 14
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 abstract description 14
- 230000000694 effects Effects 0.000 abstract description 11
- 239000000463 material Substances 0.000 abstract description 5
- 229910052751 metal Inorganic materials 0.000 description 25
- 239000002184 metal Substances 0.000 description 25
- 238000010521 absorption reaction Methods 0.000 description 21
- 239000006096 absorbing agent Substances 0.000 description 12
- 238000013461 design Methods 0.000 description 4
- 230000003014 reinforcing effect Effects 0.000 description 3
- 239000010438 granite Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000012811 non-conductive material Substances 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000006735 deficit Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000002708 enhancing effect Effects 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 239000005357 flat glass Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000003365 glass fiber Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 229910052573 porcelain Inorganic materials 0.000 description 1
- 238000001028 reflection method Methods 0.000 description 1
- 230000011514 reflex Effects 0.000 description 1
- 239000002990 reinforced plastic Substances 0.000 description 1
- 230000002787 reinforcement Effects 0.000 description 1
Landscapes
- Building Environments (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、建造物のテレビゴ
ースト障害等の電波反射障害防止対策のために、フェラ
イトタイル等の磁気的電波吸収部材を有する電波吸収壁
を外壁面に設けた建造物において、前記電波吸収壁では
対応できない外壁面に露出する電波反射構造物の取付構
造を工夫することで電波反射を防止し、電波吸収壁の効
果を一層高めて建造物の電波反射障害問題の解決を図っ
た建造物の反射障害軽減構造に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a building in which a radio wave absorbing wall having a magnetic wave absorbing member such as a ferrite tile is provided on an outer wall surface in order to prevent radio wave reflection obstruction such as television ghost obstruction of the building. In order to solve the problem of radio wave reflection obstruction of a building by preventing the radio wave reflection by devising the mounting structure of the radio wave reflecting structure exposed on the outer wall surface which cannot be handled by the radio wave absorbing wall, further enhancing the effect of the radio wave absorbing wall The present invention relates to a structure for reducing a reflex obstruction of a building which aims at the above.
【0002】[0002]
【従来の技術】従来、建造物の電波反射障害対策として
例えば図7に示すような電波吸収壁が広く用いられてい
る。この図7の電波吸収壁は、磁気的電波吸収部材とし
てのフェライトタイル(フェライト板)1の落下防止を
兼ねた特殊足付き外装タイル(磁器タイル等)3をフェ
ライトタイル1の前面に被せ、フェライトタイル1の背
後に金属製反射メッシュ(電波反射体)をなす鉄筋4を
配置し、フェライトタイル1背面側にコンクリート5を
打設することでプレキャスト・カーテンウォール構造電
波吸収壁を構成したものである。2. Description of the Related Art Conventionally, a radio wave absorbing wall as shown in FIG. The radio wave absorbing wall shown in FIG. 7 is provided with a special legged exterior tile (porcelain tile, etc.) 3 which also serves as a magnetic wave absorbing member to prevent the ferrite tile (ferrite plate) 1 from dropping, and covers the front of the ferrite tile 1. A reinforcing rod 4 forming a metal reflection mesh (radio wave reflector) is arranged behind the tile 1 and concrete 5 is cast on the back side of the ferrite tile 1 to constitute a precast curtain wall structure radio wave absorbing wall. .
【0003】この図7の電波吸収壁は、現在、建造物の
外壁にテレビゴースト対策として広く用いられており、
この電波吸収壁を採用することにより、電波反射障害を
大幅に軽減し得ることが明らかにされている。The radio wave absorbing wall shown in FIG. 7 is currently widely used as a countermeasure for TV ghost on the outer wall of a building.
It has been clarified that the use of this radio wave absorbing wall can significantly reduce radio wave reflection disturbance.
【0004】しかし、実際の建造物は、例えば電波吸収
壁としての動作要件に無関係な窓枠の金属サッシ、ゴン
ドラレール等を有しており、従ってこれらの大きさ、外
壁面全体に占める割合等により電波反射障害防止効果は
大幅に異なる。その理由は、これら窓枠等の建造物外壁
面に露出する電波反射構造物に対し有効な反射防止法が
見あたらないことにある。従って、現状ではいかに優れ
た電波吸収特性の電波吸収壁を用いても、それだけでは
建造物の電波反射を解決することは出来ない。このた
め、電波吸収壁では対応できない建造物の構造に起因す
る電波反射物の反射を是認して、それによる障害は別途
CATV等の建造物側の電波反射障害防止対策以外の方
策がとられている。建造物の窓枠等の電波反射物の構造
によっては電波吸収壁採用の効果が期待できない場合も
生じている。However, an actual building has, for example, a metal sash of a window frame, a gondola rail, and the like irrespective of the operation requirements as a radio wave absorbing wall. The effect of preventing the reflection of radio waves varies greatly depending on the type. The reason is that there is no effective anti-reflection method for radio wave reflecting structures exposed on the outer wall of the building such as window frames. Therefore, at present, even if a radio wave absorption wall having excellent radio wave absorption characteristics is used, the radio wave reflection of a building cannot be solved by itself. For this reason, the reflection of radio wave reflecting objects caused by the structure of the building that cannot be handled by the radio wave absorbing wall is approved, and the obstacles caused by this are taken separately from CATV and other measures other than the measures to prevent radio wave reflection obstacles on the building side. I have. Depending on the structure of a radio wave reflecting object such as a window frame of a building, the effect of adopting a radio wave absorbing wall may not be expected.
【0005】[0005]
【発明が解決しようとする課題】建造物の窓枠等の導電
性構造体は到来電波の電界と平行に配置された場合、一
種のアンテナとして機能し、大きな電波反射体としての
働きをする。図8、及び図8の円P内を拡大して示す図
9及び図10は電波吸収壁としての2体の長方形電波吸
収パネル10A,10B(それぞれ縦4000mm、横3
150mm)を用い、それら2体の電波吸収パネル10
A,10B間に100mmの空隙を設け、この空隙に電波
吸収パネル10A,10Bに対して単独の(独立した)
レール状金属反射物(窓枠の水平部分を模擬したものと
考えることができる)11を到来電波の電界方向に平行
に取り付けた構造を示す。但し、図9及び図10中にお
いて1はフェライトタイル、3はフェライトタイル前面
を覆う外装材としての外装タイル、4は金属製反射メッ
シュ(電波反射体)をなす鉄筋、5はコンクリートであ
る。When a conductive structure such as a window frame of a building is arranged in parallel with an electric field of an incoming radio wave, it functions as a kind of antenna and functions as a large radio wave reflector. 8 and FIG. 9 and FIG. 10 which are enlarged views of the circle P in FIG. 8 show two rectangular radio wave absorbing panels 10A and 10B (4000 mm long and 3 mm wide, respectively) as radio wave absorbing walls.
150 mm) and the two radio wave absorbing panels 10
A gap of 100 mm is provided between A and 10B, and a single (independent) radio wave absorbing panel 10A and 10B is provided in this gap.
This shows a structure in which a rail-shaped metal reflector (which can be considered as simulating a horizontal portion of a window frame) 11 is attached in parallel to the direction of the electric field of an incoming radio wave. However, in FIGS. 9 and 10, 1 is a ferrite tile, 3 is an exterior tile as an exterior material covering the front surface of the ferrite tile, 4 is a reinforcing bar forming a metal reflection mesh (radio wave reflector), and 5 is concrete.
【0006】図11は100mmの空隙を有する前記2体
の電波吸収パネル10A,10B自体の電波吸収特性
(曲線イ)と、図8乃至図10のように前記100mmの
空隙にレール状金属反射物11を配置したときの電波吸
収特性(曲線ロ)を、反射減衰量の周波数特性としてそ
れぞれ示す。100MHzで約20dB程度の優れた電
波吸収特性が確保されている2体の電波吸収パネルに対
し、その接合空隙にレール状金属反射物を装着すること
により、15dB程度に特性劣化し、あたかも電波吸収
パネルそれ自体が15dB程度の特性を持ったものと同
じになる。FIG. 11 shows the radio wave absorption characteristics (curve A) of the two radio wave absorbing panels 10A and 10B themselves having a gap of 100 mm, and a rail-shaped metal reflector in the gap of 100 mm as shown in FIGS. Radio wave absorption characteristics (curve B) when 11 is arranged are shown as frequency characteristics of return loss. By installing a rail-shaped metal reflector in the joint gap of two radio wave absorption panels that have excellent radio wave absorption characteristics of about 20 dB at 100 MHz, the characteristics deteriorate to about 15 dB, as if radio wave absorption The panel itself is the same as a panel having a characteristic of about 15 dB.
【0007】従って、一般の構造物の電波反射対策の場
合、到来電波の電界方向に平行な反射物、例えば金属
棒、金属レール等への対策が最も重要とされており、こ
れらの構造物に対し電波吸収体で覆うとか、金属以外の
例えばガラス繊維入り強化プラスチック等の非導電性材
料で置き換える等の方法が取られる。Therefore, in the case of measures against reflection of radio waves from general structures, measures against reflectors parallel to the direction of the electric field of incoming radio waves, such as metal rods and metal rails, are considered to be the most important. On the other hand, a method of covering with a radio wave absorber or replacing with a non-conductive material other than metal, for example, a reinforced plastic containing glass fiber or the like is used.
【0008】しかし、建造物の窓枠等は、その構造及び
使用目的により、これら構造物の上を電波吸収体で覆う
等の対策はできず、かつ非導電性材料で置き換え可能な
新たな材料も現状では見あたらない。従って、窓枠、そ
の他電波吸収体等で対策を施すことが不可能な建造物外
壁面に存在する電波反射構造物の対策が大きな課題とな
っており、この解決が本発明の主体をなすものである。However, due to the structure and purpose of use of window frames and the like of buildings, it is not possible to take measures such as covering these structures with radio wave absorbers, and new materials that can be replaced with non-conductive materials. Is not found at present. Therefore, countermeasures against radio wave reflecting structures existing on the outer wall of a building where it is impossible to take countermeasures with window frames or other radio wave absorbers have become a major issue, and this solution is the main subject of the present invention. It is.
【0009】本発明は、上記の点に鑑み、電波吸収壁で
は対応できない建造物外壁面に露出する電波反射構造物
の取付構造を工夫して当該電波反射構造物に起因する電
波反射を防止し、電波吸収壁の効果を一層高めて建造物
の電波反射障害問題の解決を図った建造物の反射障害軽
減構造を提供することを目的とする。In view of the above, the present invention devises a mounting structure of a radio wave reflecting structure exposed on the outer wall of a building which cannot be handled by a radio wave absorbing wall, thereby preventing radio wave reflection caused by the radio wave reflecting structure. It is another object of the present invention to provide a structure for reducing a reflection obstruction of a building in which the effect of a radio wave absorbing wall is further enhanced to solve the problem of a radio wave reflection obstruction of the building.
【0010】本発明のその他の目的や新規な特徴は後述
の実施の形態において明らかにする。[0010] Other objects and novel features of the present invention will be clarified in embodiments described later.
【0011】[0011]
【課題を解決するための手段】上記目的を達成するため
に、本発明の建造物の反射障害軽減構造は、磁気的電波
吸収部材を有する電波吸収壁を建造物の電波到来面とな
る外壁面に設け、該外壁面に露出する電波反射構造物を
前記磁気的電波吸収部材の前面よりも電波到来方向から
みて後方位置に配設したことを特徴としている。In order to achieve the above object, a structure for reducing reflection obstruction of a building according to the present invention comprises a radio wave absorbing wall having a magnetic wave absorbing member and an outer wall which serves as a radio wave arrival surface of the building. And a radio wave reflecting structure exposed on the outer wall surface is disposed at a position rearward of the front surface of the magnetic radio wave absorbing member when viewed from a radio wave arrival direction.
【0012】また、本発明の建造物の反射障害軽減構造
において、前記電波反射構造物の到来電波の電界方向に
平行な部分の一方の側に前記電波吸収壁が設けられてお
り、他方の側が電波透過面となっている構成としてもよ
い。In the structure for reducing reflection obstruction of a building according to the present invention, the radio wave absorbing wall is provided on one side of a portion of the radio wave reflecting structure parallel to an electric field direction of an incoming radio wave, and the other side is provided on the other side. It may be configured to be a radio wave transmitting surface.
【0013】磁気的電波吸収部材にフェライトタイルを
用いた磁気的電波吸収体であるフェライト電波吸収体
は、図12及び図13に示す如く、磁気的電波吸収部
材、すなわちフェライトタイル1の背面を電波反射体と
なる金属板2で裏打ちした構造が基本形であり、フェラ
イトタイル1は到来電波の磁界方向に連続に配置する
が、電界方向には空隙を設けても電波吸収特性は十分保
たれることが、理論的にも実験的にも明らかにされてい
る(電子通信学会論文 '79/8 VOL・J61-B No.8、或いは
特公昭55−49798号公報)。この理由は、一般に
波長に比較して十分小さい空隙であれば、その空隙があ
っても電波的に一つの面として捉えることが出来るから
である。As shown in FIG. 12 and FIG. 13, a ferrite electromagnetic wave absorber, which is a magnetic electromagnetic wave absorber using a ferrite tile as a magnetic electromagnetic wave absorbing member, transmits a magnetic wave to the back of the ferrite tile 1. The basic structure is a structure backed by a metal plate 2 serving as a reflector. The ferrite tiles 1 are arranged continuously in the magnetic field direction of the arriving radio wave, but the radio wave absorption characteristics are sufficiently maintained even if a gap is provided in the electric field direction. Has been clarified both theoretically and experimentally (Transactions of the Institute of Electronics and Communication Engineers, '79 / 8 VOL. J61-B No. 8, or JP-B-55-49798). The reason for this is that, generally speaking, if the gap is sufficiently small compared to the wavelength, the gap can be regarded as one surface in terms of radio waves.
【0014】従って、フェライト電波吸収体の設計条件
であるフェライトの背面に同一電位を有する反射体が存
在するならば、フェライト間にある程度空隙を設けても
電波吸収体としての動作が期待できる。特に、フェライ
ト電波吸収体においては磁気的電波吸収部材としてのフ
ェライトに電波集束効果があり、電界方向に比較的大き
な空隙が存在しても電波はフェライト部分に集束して電
波吸収特性を劣化させることはない。他方、磁界方向は
出来るだけ連続化が望まれる。その理由は、磁界方向の
空隙の存在で磁気抵抗が大きくなり、かつ反磁界の発生
により磁気特性が大幅に劣化するためである。この場
合、当然のことであるが、フェライト電波吸収体を構成
するために必要なフェライト背面の反射体は連続化が求
められる。Therefore, if there is a reflector having the same potential on the back surface of the ferrite, which is the design condition of the ferrite radio wave absorber, the operation as the radio wave absorber can be expected even if some gap is provided between the ferrites. In particular, in ferrite radio wave absorbers, ferrite as a magnetic radio wave absorbing member has a radio wave focusing effect, and even if there is a relatively large gap in the direction of the electric field, radio waves are focused on the ferrite part and the radio wave absorption characteristics are degraded. There is no. On the other hand, it is desired that the direction of the magnetic field be as continuous as possible. The reason is that the presence of the air gap in the direction of the magnetic field increases the magnetic resistance, and the generation of the demagnetizing field significantly deteriorates the magnetic characteristics. In this case, as a matter of course, it is required that the reflector on the back side of the ferrite necessary to constitute the ferrite electromagnetic wave absorber be continuous.
【0015】このような磁気的電波吸収部材であるフェ
ライトの特徴に着目し、電波吸収壁を構成するフェライ
ト電波吸収体が十分その特徴を発揮し得るならば、フェ
ライト電波吸収体の基本設計条件として構成された反射
体以外の、電波吸収壁から独立して単独で存在するが電
波吸収壁に比較して十分小さい電波反射構造物であれ
ば、例えば図4の金属製窓枠11のように、電波吸収壁
10の端部等に位置し、片面は電波的に開放部分(電波
透過面であるガラス面12)となる電波反射構造物で
も、電波的に隠すことが可能ではないかとの発想で、そ
の可能性を検討した。Focusing on the characteristics of ferrite which is such a magnetic wave absorbing member, if the ferrite wave absorber constituting the wave absorbing wall can sufficiently exhibit the characteristics, as a basic design condition of the ferrite wave absorber. Other than the configured reflector, a radio wave reflecting structure that exists independently of the radio wave absorbing wall but is sufficiently small as compared with the radio wave absorbing wall, for example, such as the metal window frame 11 in FIG. The idea is that even a radio wave reflecting structure that is located at the end of the radio wave absorption wall 10 and has one side that is open to radio waves (the glass surface 12 that is a radio wave transmitting surface) can be hidden in radio waves. , Examined the possibility.
【0016】図5に示すように、厚さ7.3mmのフェラ
イトタイル21の前面に厚さ14mmの外装タイル(花崗
岩)23を配置し、フェライトタイル21の背後に厚さ
12mmとなるようにコンクリート25を打設し、その背
面に電波反射板(金属板)24を配置してなる幅600
mm、長さ900mmの実用構造の電波吸収パネル20を試
作し、その電波吸収パネル20の中央に到来電波の電界
方向に平行な幅20mmの空隙26を形成し、その空隙部
分にアルミサッシ相当の金属板を、電波吸収パネルの外
装タイル(花崗岩)23前面と同一面上(位置a)、フ
ェライトタイル21の前面と同一面上(位置b)、フェ
ライトタイル21の背面と同一面上(位置c)、最後に
電波反射板24の電波反射面と同一面上(位置d)に、
パネル厚み方向の位置を変えてそれぞれ装着したときの
電波吸収特性を測定した。その測定結果を図6に示す。As shown in FIG. 5, an exterior tile (granite) 23 having a thickness of 14 mm is disposed in front of a ferrite tile 21 having a thickness of 7.3 mm, and a concrete having a thickness of 12 mm is provided behind the ferrite tile 21. 25, and a radio wave reflecting plate (metal plate) 24 is arranged on the back surface thereof.
A prototype of a radio wave absorbing panel 20 having a practical structure of 900 mm in length and 900 mm in length is formed, and a gap 26 having a width of 20 mm is formed in the center of the radio wave absorbing panel 20 in a direction parallel to the electric field direction of the arriving radio wave. The metal plate is placed on the same plane as the front of the exterior tile (granite) 23 of the radio wave absorbing panel (position a), on the same plane as the front of the ferrite tile 21 (position b), and on the same plane as the back of the ferrite tile 21 (position c). ), And finally on the same plane as the radio wave reflecting surface of the radio wave reflecting plate 24 (position d),
The electromagnetic wave absorption characteristics when the panel was mounted at different positions in the thickness direction of the panel were measured. FIG. 6 shows the measurement results.
【0017】図6の反射減衰量の周波数特性において、
位置aの外装タイル23前面と同一面上に金属板が装着
されたときに最も電波吸収特性に影響を及ぼし、金属板
の反射の影響により見掛け上電波吸収パネルの電波吸収
量は最良値に比較して約10dBも劣化する。同様に位
置bの磁気的電波吸収部材であるフェライトタイル21
の前面と同一面上に金属板を装着した場合も位置a程の
特性劣化ではないが、それでも最良値に比較して約5d
B程度は劣化することが確認できた。それに反し、磁気
的電波吸収部材であるフェライトタイル21の背面と同
一面乃至電波反射板24の電波反射面と同一面となる位
置c,dに金属板を装着した場合は、多少中心周波数が
ずれているが電波吸収特性は本来の設計通りの35dB
程度の優れた特性を示すことが確認された。なお、この
程度の中心周波数のずれはフェライト電波吸収体の設計
原理よりフェライトタイルの厚み制御で十分対応できる
範囲である。In the frequency characteristic of the return loss shown in FIG.
When a metal plate is mounted on the same surface as the front surface of the exterior tile 23 at the position a, this has the greatest effect on the radio wave absorption characteristics, and the apparent amount of radio wave absorption of the radio wave absorption panel is compared to the best value due to the influence of the reflection of the metal plate. As a result, the power deteriorates by about 10 dB. Similarly, the ferrite tile 21 which is the magnetic wave absorbing member at the position b
When a metal plate is mounted on the same surface as the front surface, the characteristics are not deteriorated as much as the position a, but it is still about 5 d compared to the best value.
It was confirmed that about B deteriorated. On the other hand, when metal plates are mounted at positions c and d on the same plane as the back surface of the ferrite tile 21 which is a magnetic wave absorbing member or on the same plane as the radio wave reflecting surface of the radio wave reflecting plate 24, the center frequency is slightly shifted. However, the radio wave absorption characteristic is 35dB as originally designed.
It was confirmed that the composition exhibited excellent characteristics. It should be noted that such a shift in the center frequency is within a range that can be sufficiently controlled by controlling the thickness of the ferrite tile according to the design principle of the ferrite electromagnetic wave absorber.
【0018】この結果、磁気的電波吸収部材としてのフ
ェライトの電波集束効果は、電界方向に平行な空隙に電
波反射構造物が存在しても、その位置がフェライトの前
面より後方位置、好ましくはフェライトの背面と同一面
乃至これより後方位置とするならば、十分認められ、こ
の効果を利用することにより、従来建造物の電波反射対
策上大きな障害となっていた、窓枠等のそれ自体電波吸
収体等で処理出来ない構造物を電波的に隠し、この構造
物からの電波反射を抑えることの可能性を明らかにする
ことが出来た。As a result, the radio wave focusing effect of ferrite as a magnetic wave absorbing member is such that even if a radio wave reflecting structure is present in a gap parallel to the direction of the electric field, the position is located behind the front surface of the ferrite, preferably the ferrite. If it is located on the same plane as the back of the building or behind it, it is well recognized. By using this effect, the electromagnetic wave absorption of the window frame etc., which has been a major obstacle to measures against radio wave reflection of buildings in the past. The structure that cannot be processed by the body etc. was concealed by radio waves, and the possibility of suppressing the reflection of radio waves from this structure was clarified.
【0019】[0019]
【発明の実施の形態】以下、本発明に係る建造物の反射
障害軽減構造の実施の形態を図面に従って説明する。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view showing an embodiment of a structure for reducing a reflection obstruction of a building according to the present invention.
【0020】図1は本発明に係る建造物の反射障害軽減
構造の実施の形態であり、図2は本発明を適用する高層
建造物の1例を示す。FIG. 1 shows an embodiment of a structure for reducing a reflection obstruction of a building according to the present invention, and FIG. 2 shows an example of a high-rise building to which the present invention is applied.
【0021】図2に示すような高層建造物30で、窓3
1が到来電波の電界方向に平行に連続的に並び、かつそ
の面積も大きく、従ってその窓枠を構成するアルミサッ
シも電界方向に長く伸び、窓31以外の外壁面に電波吸
収壁40を取り付けても過去の経験によりその効果が余
り期待できない建造物に対し、図1の如き窓枠配置とす
る。すなわち、図1において、電波吸収壁40は磁気的
電波吸収部材としてのフェライトタイル(フェライト
板)41の落下防止を兼ねた外装タイル等の外装材43
をフェライトタイル41の前面に被せ、フェライトタイ
ル41の背後に金属製反射メッシュ(電波反射体)をな
す鉄筋44を配置し、フェライトタイル41背面側にコ
ンクリート45を打設してそれらを一体化してなるプレ
キャスト構造の電波吸収パネルであり、電波透過面とな
る窓ガラス51が取り付けられた窓枠がアルミサッシ5
0で構成されている。そして、アルミサッシ50の到来
電波の電界方向に平行なアルミサッシ水平部50Aは電
波反射体として働くが、少なくともこのアルミサッシ水
平部50Aを電波吸収壁40の磁気的電波吸収部材とし
てのフェライトタイル41背面より多少後方に位置する
ように高層建造物の構造躯体に電波吸収壁40と共に取
り付けている。A high-rise building 30 as shown in FIG.
1 are arranged continuously in parallel with the direction of the electric field of the arriving radio wave and have a large area. Therefore, the aluminum sash constituting the window frame also extends in the direction of the electric field, and the radio wave absorbing wall 40 is attached to the outer wall surface other than the window 31. However, a window frame arrangement as shown in FIG. 1 is used for a building whose effect cannot be expected so much due to past experience. That is, in FIG. 1, the radio wave absorbing wall 40 includes an exterior material 43 such as an exterior tile that also serves to prevent a ferrite tile (ferrite plate) 41 as a magnetic electromagnetic wave absorbing member from falling.
Is placed on the front surface of the ferrite tile 41, a reinforcing bar 44 serving as a metal reflection mesh (radio wave reflector) is arranged behind the ferrite tile 41, and concrete 45 is cast on the back side of the ferrite tile 41 to integrate them. A window frame having a window glass 51 to be a radio wave transmitting surface is an aluminum sash 5
0. The aluminum sash horizontal portion 50A parallel to the electric field direction of the arriving radio wave of the aluminum sash 50 functions as a radio wave reflector, but at least this aluminum sash horizontal portion 50A is used as a ferrite tile 41 as a magnetic radio wave absorbing member of the radio wave absorbing wall 40. The radio wave absorbing wall 40 is attached to the structural body of the high-rise building so as to be located slightly behind the back.
【0022】これにより、窓枠の電波反射問題は解決さ
れ、電波吸収壁本来の特性が発揮され、建造物の反射障
害を解決することができる。As a result, the problem of radio wave reflection of the window frame is solved, the inherent characteristics of the radio wave absorbing wall are exhibited, and the reflection obstacle of the building can be solved.
【0023】なお、この場合の電波吸収壁に窓枠を取り
付けた構造体は、電波吸収壁40の上下両端に窓枠のア
ルミサッシ水平部50Aが取り付けられた状態となり、
電波吸収特性の評価はこのような状態でタイムドメイン
法を用いて行った。その結果をアルミサッシ無しの場合
と比較して図3の反射減衰量の周波数特性のグラフで示
す。図3の曲線ハは本発明の実施の形態に係る窓枠有り
の場合、曲線ニは窓枠無しの場合をそれぞれ示してい
る。但し、電波吸収壁40の縦方向寸法は4000mm、
横方向寸法は3200mm、アルミサッシ水平部50Aの
上下幅は100mmとした。In this case, the structure in which the window frame is mounted on the radio wave absorbing wall is in a state where the aluminum sash horizontal portions 50A of the window frame are mounted on the upper and lower ends of the radio wave absorbing wall 40.
The evaluation of the radio wave absorption characteristics was performed using the time domain method in such a state. The result is compared with the case without the aluminum sash, and is shown in the graph of the frequency characteristic of the return loss in FIG. Curve C in FIG. 3 shows the case with the window frame according to the embodiment of the present invention, and curve D shows the case without the window frame. However, the vertical dimension of the radio wave absorbing wall 40 is 4000 mm,
The horizontal dimension was 3200 mm, and the vertical width of the aluminum sash horizontal portion 50A was 100 mm.
【0024】この図3から、本発明の実施の形態によれ
ば、窓枠無しの場合とほぼ同等の反射減衰量が得られて
いることがわかる。From FIG. 3, it can be seen that according to the embodiment of the present invention, the return loss almost equal to that without the window frame is obtained.
【0025】なお、アルミサッシ50は水平部だけでな
く垂直部も有するが、テレビゴースト障害対策について
言えば、テレビ放送の電波は水平偏波であり、アルミサ
ッシ50の垂直部は電界に対し垂直となるため、電波反
射体としての働きは少なく、とくに配慮は不要である。Although the aluminum sash 50 has not only a horizontal portion but also a vertical portion, the TV broadcast radio wave is a horizontally polarized wave, and the vertical portion of the aluminum sash 50 is perpendicular to the electric field. Therefore, the function as a radio wave reflector is small, and no special consideration is required.
【0026】また、上記実施の形態では、到来電波に対
して電波反射構造物となるアルミサッシ水平部50Aを
電波吸収壁40の磁気的電波吸収部材としてのフェライ
トタイル41の背面よりも多少後方位置としたが、電波
反射構造物が磁気的電波吸収部材の前面よりも電波到来
方向からみて後方位置に配設してあれば電波吸収壁の特
性劣化をある程度防止できることは前述した図5の説明
から明らかである。In the above-described embodiment, the aluminum sash horizontal portion 50A serving as a radio wave reflecting structure for incoming radio waves is positioned slightly behind the back surface of the ferrite tile 41 as the magnetic radio wave absorbing member of the radio wave absorbing wall 40. However, from the description of FIG. 5 described above, it is possible to prevent the deterioration of the characteristics of the radio wave absorbing wall to some extent if the radio wave reflecting structure is disposed at a position behind the front surface of the magnetic radio wave absorbing member when viewed from the radio wave arrival direction. it is obvious.
【0027】以上本発明の実施の形態について説明して
きたが、本発明はこれに限定されることなく請求項の記
載の範囲内において各種の変形、変更が可能なことは当
業者には自明であろう。Although the embodiments of the present invention have been described above, it is obvious to those skilled in the art that the present invention is not limited to the embodiments and various modifications and changes can be made within the scope of the claims. There will be.
【0028】[0028]
【発明の効果】以上説明したように、本発明の建造物の
反射障害軽減構造によれば、窓枠が多いため、或いはゴ
ンドラレール等により、電波吸収壁だけでは十分解決で
きなかった建造物の電波反射障害対策に新しい道を開
き、今後の高層建造物の設計に寄与するところ大きいと
考える。As described above, according to the structure for reducing the reflection obstruction of a building according to the present invention, since there are many window frames or a gondola rail or the like, the structure of the building that could not be sufficiently solved by the radio wave absorbing wall alone is not sufficient. I think that it will be a great way to contribute to the design of high-rise buildings in the future, opening a new way for measures against radio wave reflection.
【図1】本発明に係る建造物の反射障害軽減構造の実施
の形態を示す側断面図である。FIG. 1 is a side sectional view showing an embodiment of a structure for reducing reflection obstruction of a building according to the present invention.
【図2】本発明の実施の形態を適用する高層建造物の1
例を示す正面図である。FIG. 2 shows a high-rise building 1 to which the embodiment of the present invention is applied.
It is a front view showing an example.
【図3】本発明の実施の形態による反射障害軽減効果を
窓枠無しの場合と比較して評価した反射減衰量の周波数
特性を示すグラフである。FIG. 3 is a graph showing a frequency characteristic of a return loss evaluated by comparing the effect of reducing reflection impairment according to the embodiment of the present invention with a case without a window frame.
【図4】電波吸収壁を外壁面に有する建造物における連
窓の窓枠構造の1例を示す正面図である。FIG. 4 is a front view showing an example of a window frame structure of a continuous window in a building having a radio wave absorbing wall on an outer wall surface.
【図5】電波吸収パネルの到来電波の電界方向に平行な
空隙に配置された金属板の配置による反射特性に及ぼす
影響を調べるための構造図である。FIG. 5 is a structural diagram for examining the influence on the reflection characteristics due to the arrangement of a metal plate arranged in a gap parallel to the electric field direction of the arriving radio wave of the radio wave absorption panel.
【図6】図5の電波吸収パネル厚み方向に位置を変えた
金属板配置に対応した反射減衰量の周波数特性をそれぞ
れ示すグラフである。6 is a graph showing frequency characteristics of return loss corresponding to a metal plate arrangement in which the position is changed in the thickness direction of the radio wave absorption panel of FIG. 5;
【図7】特殊足付き外装タイルで固定する構造を持つ電
波吸収壁の従来例を示す斜視図である。FIG. 7 is a perspective view showing a conventional example of a radio wave absorbing wall having a structure to be fixed with an exterior tile with special feet.
【図8】電波吸収パネル間に当該電波吸収パネルから独
立した金属反射物を配置した構造を示す正面図である。FIG. 8 is a front view showing a structure in which a metal reflector independent of the radio wave absorbing panel is arranged between the radio wave absorbing panels.
【図9】図8の円P内を拡大して示す拡大正面図であ
る。9 is an enlarged front view showing a circle P in FIG. 8 in an enlarged manner.
【図10】同じく拡大側断面図である。FIG. 10 is an enlarged side sectional view of the same.
【図11】図8乃至図10の如く電波吸収パネル間に当
該電波吸収パネルから独立した金属反射物を配置した構
造と金属反射物が無い場合を比較した反射減衰量の周波
数特性を示すグラフである。FIG. 11 is a graph showing a frequency characteristic of return loss comparing a structure in which a metal reflector independent of the radio wave absorbing panel is arranged between the radio wave absorbing panels as shown in FIGS. 8 to 10 and a case where there is no metal reflector; is there.
【図12】磁界方向に連続で電界方向に不連続なフェラ
イト配置とした電波吸収壁の基本となる従来例を示す正
面図である。FIG. 12 is a front view showing a conventional example which is a basic example of a radio wave absorbing wall in which ferrites are arranged continuously in a magnetic field direction and discontinuous in an electric field direction.
【図13】同平断面図である。FIG. 13 is a plan sectional view of the same.
1,21,41 フェライトタイル 2 金属板 3,23 外装タイル 4,44 鉄筋 5,25,45 コンクリート 10A,10B,20 電波吸収パネル 11 レール状金属反射物 24 電波反射板 30 高層建造物 31 窓 40 電波吸収壁 43 外装材 50 アルミサッシ 50A アルミサッシ水平部 1,21,41 Ferrite tile 2 Metal plate 3,23 Exterior tile 4,44 Reinforcement 5,25,45 Concrete 10A, 10B, 20 Radio wave absorption panel 11 Rail-shaped metal reflector 24 Radio wave reflector 30 High-rise building 31 Window 40 Electric wave absorption wall 43 Exterior material 50 Aluminum sash 50A Aluminum sash horizontal part
Claims (2)
を建造物の電波到来面となる外壁面に設け、該外壁面に
露出する電波反射構造物を前記磁気的電波吸収部材の前
面よりも電波到来方向からみて後方位置に配設したこと
を特徴とする建造物の反射障害軽減構造。1. A radio wave absorbing wall having a magnetic wave absorbing member is provided on an outer wall surface serving as a radio wave arrival surface of a building, and a radio wave reflecting structure exposed on the outer wall surface is located at a position higher than the front surface of the magnetic wave absorbing member. A structure for reducing reflection obstruction of a building, wherein the structure is disposed at a rear position as viewed from a radio wave arrival direction.
向に平行な部分の一方の側に前記電波吸収壁が設けられ
ており、他方の側が電波透過面となっている請求項1記
載の建造物の反射障害軽減構造。2. The radio wave reflecting structure according to claim 1, wherein the radio wave absorbing wall is provided on one side of a portion of the radio wave reflecting structure parallel to an electric field direction of an incoming radio wave, and the other side is a radio wave transmitting surface. A structure to reduce the reflection obstacles in buildings.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28900296A JP3930928B2 (en) | 1996-10-14 | 1996-10-14 | Structure for reducing reflection reflections in buildings |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28900296A JP3930928B2 (en) | 1996-10-14 | 1996-10-14 | Structure for reducing reflection reflections in buildings |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH10117087A true JPH10117087A (en) | 1998-05-06 |
| JP3930928B2 JP3930928B2 (en) | 2007-06-13 |
Family
ID=17737577
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP28900296A Expired - Fee Related JP3930928B2 (en) | 1996-10-14 | 1996-10-14 | Structure for reducing reflection reflections in buildings |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3930928B2 (en) |
-
1996
- 1996-10-14 JP JP28900296A patent/JP3930928B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JP3930928B2 (en) | 2007-06-13 |
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