JPH11191687A - Window structure with electromagnetic shielding property - Google Patents

Window structure with electromagnetic shielding property

Info

Publication number
JPH11191687A
JPH11191687A JP35899697A JP35899697A JPH11191687A JP H11191687 A JPH11191687 A JP H11191687A JP 35899697 A JP35899697 A JP 35899697A JP 35899697 A JP35899697 A JP 35899697A JP H11191687 A JPH11191687 A JP H11191687A
Authority
JP
Japan
Prior art keywords
antenna element
linear antenna
sash frame
radio wave
window glass
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
Application number
JP35899697A
Other languages
Japanese (ja)
Other versions
JP3333729B2 (en
Inventor
Junichi Hirai
淳一 平井
Kimio Kawasaki
公雄 川崎
修一 ▲高▼坂
Shuichi Kosaka
Motoyasu Togashi
元康 冨樫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NIPPON SHEET GLASS KANKYO AMEN
NIPPON SHEET GLASS KANKYO AMENITY KK
Kajima Corp
Original Assignee
NIPPON SHEET GLASS KANKYO AMEN
NIPPON SHEET GLASS KANKYO AMENITY KK
Kajima Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NIPPON SHEET GLASS KANKYO AMEN, NIPPON SHEET GLASS KANKYO AMENITY KK, Kajima Corp filed Critical NIPPON SHEET GLASS KANKYO AMEN
Priority to JP35899697A priority Critical patent/JP3333729B2/en
Publication of JPH11191687A publication Critical patent/JPH11191687A/en
Application granted granted Critical
Publication of JP3333729B2 publication Critical patent/JP3333729B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To obtain a window structure which is capable of ensuring electromagnetic shielding property to a window's peripheral part by a method, wherein a simple structure is additionally provided to eliminate the reflection of electromagnetic waves from metals in the pocket of a metal sash frame and to lessen a resonant coefficient to make a window glass's peripheral edge function as a freely open end, even in a case where the linear antenna element is put in the pocket of the metal sash frame in a tie-in between a window glass, where the linear antenna element is arranged so as to enhance it in electromagnetic shielding property and the metal sash frame, and as a result, the linear antenna element is restrained from deteriorating in shielding property. SOLUTION: A linear antenna element 5 of a prescribed length for resonating with radio waves which is to be blocked is made to serve as an electromagnetic shielding element, a window glass 1 where the elements 5 are arranged regularly, taking their electromagnetic field reflection equivalent area (scattering aperture area) or electromagnetic field reflection equivalent volume (scattering aperture volume) into consideration is fitted in a metal sash frame 2. At this point, a radio wave absorbent 8 is filled between the window glass 1 and the metal sash frame 2.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、建物や自動車や列
車等の乗り物の窓や間仕切りやボックス等の什器の窓
で、電磁シールド性能を持つものに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a window of a vehicle such as a building, a car or a train, and a window of a furniture such as a partition or a box, which has an electromagnetic shielding property.

【0002】[0002]

【従来の技術】採光性・可視性を損なうことなく、しか
も必要な周波数の電波帯のみを選択して電磁シールドが
可能な窓ガラス1として、図12に示すように、遮蔽しよ
うとする電波の周波数(波長)に対応した長さの線状ア
ンテナ素子5を電磁界反射等価面積または体積を考慮し
て窓ガラス1上に規則的に配列させ、この線状アンテナ
素子5で電波を減衰させることとしたものが提案されて
いる。図中2は金属製サッシ枠である。
2. Description of the Related Art As a window glass 1 capable of electromagnetically shielding by selecting only a radio wave band of a required frequency without impairing daylighting and visibility, as shown in FIG. A linear antenna element 5 having a length corresponding to a frequency (wavelength) is regularly arranged on the window glass 1 in consideration of an electromagnetic field reflection equivalent area or volume, and a radio wave is attenuated by the linear antenna element 5. What has been proposed. 2 is a metal sash frame.

【0003】この原理を先に説明すると、導体片が空中
にある場合、図14に示すようにこの面に電波が入射する
と、1部は反射、1部は吸収、残りは透過する。この導
体片による電波の減衰量は導体片の形状や大きさによっ
て異なる。この導体片を端部が開放の線状アンテナ素子
(ダイポール)としたとすれば、電波を反射するととも
に一部は吸収される。
[0003] Explaining this principle first, when a radio wave is incident on this surface as shown in FIG. 14 when a conductor piece is in the air, one part is reflected, one part is absorbed, and the other is transmitted. The amount of attenuation of the radio wave by the conductor piece differs depending on the shape and size of the conductor piece. If this conductor piece is a linear antenna element (dipole) having an open end, the radio wave is reflected and a part is absorbed.

【0004】図15に示すように、平面電磁界に平行に置
かれた半波長(λ/2)の線状アンテナ素子3はアンテ
ナ素子の金属部分の面積のみが電磁波エネルギーを受信
するのではなく、金属面の近傍の電磁界を吸い取ってい
る。その広がりは均一ではないが等価断面積Aeは、下
記式1で計算値が表示される。
As shown in FIG. 15, a linear antenna element 3 having a half wavelength (λ / 2) placed in parallel with a plane electromagnetic field is not limited to the area of the metal part of the antenna element, but receives electromagnetic wave energy. , And absorbs the electromagnetic field near the metal surface. Although the spread is not uniform, the calculated value of the equivalent cross-sectional area Ae is expressed by the following equation 1.

【0005】[0005]

【式1】Ae≒0.13λ2 (λ/2×λ/4の面積)[Formula 1] Ae ≒ 0.13λ 2 (area of λ / 2 × λ / 4)

【0006】この受信された電磁波エネルギーは大部分
が反射され、約1/4が電力として受信される。これが
実効開口である。
[0006] Most of the received electromagnetic wave energy is reflected, and about 1/4 is received as electric power. This is the effective aperture.

【0007】図16に示すように、このような半波長(λ
/2)の線状アンテナの受信入力抵抗を短絡すると、理
想的な損失のないアンテナ素子であれば、空間に電力が
すべて反射(散乱)され、その等価な面積は前記の実効
開口の4倍になり、このような線状アンテナ素子3によ
る素子を前記反射等価面積4×Aeに応じて図17に示す
ように窓ガラス1に配列すれば、あたかも金属膜を貼っ
たのと同様な電波反射効果を示す。アンテナ素子は一般
に周波数依存性をもつが、その特性と受信端抵抗=0が
この線状アンテナ素子3による素子の基本動作であり、
もし線状アンテナに損失があれば、電波の一部は電力と
してアンテナ損失抵抗に吸い取られる。
As shown in FIG. 16, such a half wavelength (λ
/ 2) When the input resistance of the linear antenna is short-circuited, if the antenna element has no ideal loss, all the power is reflected (scattered) in space, and its equivalent area is four times the effective aperture. By arranging the elements of such a linear antenna element 3 on the window glass 1 as shown in FIG. 17 according to the reflection equivalent area 4 × Ae, it is possible to obtain the same radio wave reflection as if a metal film was attached. Show the effect. The antenna element generally has frequency dependency, and its characteristics and the receiving end resistance = 0 are the basic operations of the element by the linear antenna element 3,
If the linear antenna has a loss, a part of the radio wave is absorbed by the antenna loss resistor as power.

【0008】しかも線状アンテナ素子3は散在するもの
なので、窓ガラス1の採光性・可視性を損なうこともな
い。なお、線状アンテナ素子3をなす導線の太さは視界
の妨げにならないように細く、かつ損失の少ないものを
選択する。
In addition, since the linear antenna elements 3 are scattered, the lighting and visibility of the window glass 1 are not impaired. Note that the thickness of the conductive wire forming the linear antenna element 3 is selected to be thin and small in loss so as not to obstruct the view.

【0009】しかし、図17に示すように線状アンテナ素
子3を横一列に配置するのでは、水平偏波のみにしか共
振せず実際の電波の偏波面がこのように横一列でない、
様々な偏波面の電波には対応できない。そこで線状アン
テナ素子3はこれを図12、図13に示すような細い線によ
り、中心5aから均等角で放射状にでる等しい長さ辺5
bを3本設けたY字形の素子である端部開放形状の線状
アンテナ素子5とした。線状アンテナ素子5は遮蔽しよ
うとする電磁波の波長をλ、ガラス面に線状アンテナ素
子を配列した時の等価比誘電率をεq とした場合、一辺
の長さが略λ/(4√εq )の横Y字形素子である。
However, arranging the linear antenna elements 3 in a horizontal line as shown in FIG. 17 resonates only with the horizontal polarization, and the polarization plane of the actual radio wave is not in such a horizontal line.
It cannot handle radio waves with various polarization planes. Therefore, the linear antenna element 3 is formed by a thin line as shown in FIGS.
b was provided as a linear antenna element 5 having an open end, which is a Y-shaped element provided with three pieces. When the wavelength of the electromagnetic wave to be shielded is λ and the equivalent relative permittivity when the linear antenna elements are arranged on the glass surface is εq, the length of one side of the linear antenna element 5 is approximately λ / (4√εq ) Is a horizontal Y-shaped element.

【0010】このように形状をY字形として3方に伸び
るようにすれば、電波の偏波面がどのような傾きを持つ
としてもいずれかの素子と共振するので、問題を解消で
きる。さらにこの線状アンテナ5を配置するのに、各辺
5bの端を隣接する線状アンテナ5の中心5aに近づけ
て配列し、全体を魚鱗状の模様に近くなるようにした。
If the shape is extended in three directions as a Y-shape as described above, the problem can be solved because the radio wave resonates with any element regardless of the inclination of the plane of polarization. Further, when arranging the linear antenna 5, the end of each side 5b is arranged close to the center 5a of the adjacent linear antenna 5, so that the whole is close to a fish scale pattern.

【0011】なお、前記線状アンテナ素子5を設ける窓
ガラス1としては、フロート板ガラスまたは熱線吸収ガ
ラス等がよく、またガラス表面またはガラス板間に線状
アンテナ素子5をこのアンテナ素子が有する電磁界反射
等価面積を考慮して定期的に配列させる方法としては、
銀、銅、金などの金属ペーストシルク印刷や導電性フィ
ルム膜の貼り付けによる方法や金属線による素子を接着
などで設置する方法も考えられる。
As the window glass 1 on which the linear antenna element 5 is provided, a float plate glass or a heat ray absorbing glass is preferable, and the linear antenna element 5 has a linear antenna element 5 on the glass surface or between the glass plates. As a method of regularly arranging in consideration of the reflection equivalent area,
A method of printing a metal paste of silver, copper, gold, or the like on a silk screen or attaching a conductive film film, or a method of mounting an element using a metal wire by bonding or the like can be considered.

【0012】[0012]

【発明が解決しようとする課題】ところで、線状アンテ
ナ素子5を配置して電磁遮蔽を行う窓ガラスの場合は、
この線状アンテナ素子5は電気的な接触がなくても(隙
間があっても)遮蔽できるが、前記金属製サッシ枠2と
の関係では、金属製サッシ枠2(のポケット)内に入り
込む線状アンテナ素子5′には直接電磁波はこないが、
隣接する線状アンテナ素子5にきた電磁波が散乱してこ
の線状アンテナ素子5′に到達し、さらに金属製サッシ
枠2の内壁面等で反射して空洞共振し、反対側に抜けて
しまう。このような無効素子となる線状アンテナ素子
5′が位置を占める窓ガラス1の周囲部分では期待され
る電磁遮蔽効果が得られないものとなる。
By the way, in the case of a window glass in which the linear antenna element 5 is arranged to perform electromagnetic shielding,
This linear antenna element 5 can be shielded without any electrical contact (even if there is a gap), but in relation to the metal sash frame 2, a wire that enters the metal sash frame 2 (pocket). Although the electromagnetic wave does not directly enter the antenna element 5 ',
Electromagnetic waves arriving at the adjacent linear antenna element 5 are scattered and reach the linear antenna element 5 ′, and are further reflected on the inner wall surface of the metal sash frame 2, resonate with the cavity, and escape to the opposite side. The expected electromagnetic shielding effect cannot be obtained in the surrounding area of the window glass 1 where the linear antenna element 5 ′ serving as the ineffective element occupies the position.

【0013】なお、図18に示すように窓ガラス1の周囲
部分で金属製サッシ枠2のポケット内に入る部分には線
状アンテナ素子5を設けないようにすれば、線状アンテ
ナ素子5が金属製サッシ枠2のポケット内に入ることを
防止できるが、これでは線状アンテナ素子5の配置面と
金属製サッシ枠2との間の間隔が広くなり、金属製サッ
シ枠2に接触する導電膜6でこの間隔を埋めなければな
らない。このような導電膜6の配設はエレメントの配置
パターンが難しく極めて面倒である。
As shown in FIG. 18, if the linear antenna element 5 is not provided in the area surrounding the window glass 1 and inside the pocket of the metal sash frame 2, the linear antenna element 5 can be Although it is possible to prevent the metal sash frame 2 from entering the pocket, in this case, the interval between the arrangement surface of the linear antenna element 5 and the metal sash frame 2 is increased, and the conductive sash frame 2 is brought into contact with the metal sash frame 2. This space must be filled with the membrane 6. Such an arrangement of the conductive film 6 makes the arrangement pattern of the elements difficult and extremely troublesome.

【0014】また、特開平3-131094号公報などにも見ら
れるようなシーリング材9を導電性のものとしてこれで
金属製サッシ枠2内をシールすることも検討されるが
(図3参照)、この導電性のシーリング材9は線状アン
テナ素子5′と隣接する線状アンテナ素子5とを短絡す
ることになり、欠損素子を増すだけで電磁遮蔽効果を確
保するのに全く意味をなさない。また、導電性のシーリ
ング材9は高価であり、しかも施工が困難である。図3
中、11はバックアップリングを示す。
It is also considered to make the sealing material 9 conductive as shown in Japanese Patent Application Laid-Open No. 3-31094 or the like to seal the inside of the metal sash frame 2 with this (see FIG. 3). However, this conductive sealing material 9 short-circuits the linear antenna element 5 'and the adjacent linear antenna element 5, and has no meaning in securing the electromagnetic shielding effect only by increasing the number of defective elements. . Further, the conductive sealing material 9 is expensive and difficult to construct. FIG.
Reference numeral 11 denotes a backup ring.

【0015】本発明の目的は前記従来例の不都合を解消
し、線状アンテナ素子を配置して電磁遮蔽を行う窓ガラ
スと金属製サッシ枠との取り合いで、線状アンテナ素子
が金属製サッシ枠のポケット内に入り込みむ場合でも、
簡単な構成を付加することで、これが無効素子とならな
いようにして、窓ガラス周囲の電磁遮蔽性能を確保でき
る電磁シールド性能を有する窓構造を提供することにあ
る。
An object of the present invention is to solve the inconvenience of the prior art, and to connect a linear sash frame to a metal sash frame by disposing a linear sash frame and a metal sash frame. Even if you get into your pocket,
An object of the present invention is to provide a window structure having an electromagnetic shielding performance capable of securing an electromagnetic shielding performance around a window glass by adding a simple configuration to prevent the element from becoming an invalid element.

【0016】[0016]

【課題を解決するための手段】本発明は前記目的を達成
するため、遮蔽しようとする電波に共振させる長さの線
状アンテナ素子を電磁遮蔽素子として、その素子の電磁
界反射等価面積(散乱開口面積)または電磁界反射等価
体積(散乱開口体積)を考慮して規則的に配列させた窓
ガラスを金属製サッシ枠に嵌め込むのに、窓ガラスと金
属製サッシ枠間に電波吸収体を充填することを要旨とす
るものである。
According to the present invention, a linear antenna element having a length resonating with a radio wave to be shielded is used as an electromagnetic shielding element. In order to fit a regularly arranged window glass into a metal sash frame in consideration of the aperture area) or the electromagnetic field reflection equivalent volume (scattering aperture volume), a radio wave absorber is inserted between the window glass and the metal sash frame. It is intended to be filled.

【0017】本発明によれば、窓ガラスと金属製サッシ
枠間に電波吸収体を充填することで、電波吸収体の挿入
・損失については、第1に、挿入損失が大きく、第2
に、共振係数:Q=ωL/R(抵抗分)が低下して共振
がしにくくなり、、ガラス端部の金属性サッシの存在を
無くし、あたかもガラス端部を自由空間並みに電波開放
したとの同じような状態とする。
According to the present invention, by filling the radio wave absorber between the window glass and the metal sash frame, the insertion loss of the radio wave absorber is firstly large, and the insertion loss is large.
In addition, the resonance coefficient: Q = ωL / R (resistance) is reduced, and it becomes difficult to resonate, the metallic sash at the glass end is eliminated, and the radio wave is released as if the glass end were at the same level as free space. And the same state.

【0018】[0018]

【発明の実施の形態】以下、本発明の実施形態を図面に
ついて詳細に説明する。図1は本発明の電磁シールド性
能を有する窓構造の1実施形態を示す要部の縦断側面
図、図2は同上斜視図で、図中1は窓ガラス、2は金属
製サッシ枠を示し、窓ガラス1は遮蔽しようとする電波
の周波数に対応した長さの線状アンテナ素子5を電磁界
反射等価面積または体積を考慮して窓ガラス1上に規則
的に配列させ、この線状アンテナ素子5で電波を減衰さ
せることとしている。
Embodiments of the present invention will be described below in detail with reference to the drawings. FIG. 1 is a longitudinal sectional side view of a main part showing an embodiment of a window structure having electromagnetic shielding performance of the present invention, FIG. 2 is a perspective view of the same, and FIG. 1 shows a window glass, 2 shows a metal sash frame, The windowpane 1 has a linear antenna element 5 having a length corresponding to the frequency of a radio wave to be shielded, which is regularly arranged on the windowpane 1 in consideration of an electromagnetic reflection equivalent area or volume. At 5, the radio wave is attenuated.

【0019】なお、線状アンテナ素子は前記のごとき端
部開放型の素子の他に環状型の素子または端部開放型の
素子と環状型の素子の組合せによるものでもよい。
The linear antenna element may be a ring-shaped element or a combination of an open-ended element and a ring-shaped element in addition to the open-ended element as described above.

【0020】図中7は通常窓ガラス1を金属製サッシ枠
2のポケット内に固定するためのセッティングブロック
で、このセッティングブロック7が金属製サッシ枠2の
ポケットの奥で窓ガラス1の端を押さえているとして、
本実施形態前記ポケット内で窓ガラス1と金属製サッシ
枠2間の隙間のうち両側に電波吸収体8を充填した。図
中10はシーリング材、11はバックアップリングである。
In the drawing, reference numeral 7 denotes a setting block for fixing the window glass 1 in the pocket of the metal sash frame 2. As if holding down,
In the present embodiment, both sides of the gap between the window glass 1 and the metal sash frame 2 in the pocket are filled with the radio wave absorber 8. In the figure, 10 is a sealing material, and 11 is a backup ring.

【0021】このような電波吸収体8は電波吸収特性を
有する誘電性材料であり、カーボンゴム・カーボン含有
発泡ウレタン,カーボン含有発泡ポリスチロール、また
は、耐環境性(耐湿性、耐衝撃性等)に優れたエポキシ
変性ウレタンゴムに損失材料として炭素粒子(カーボン
ブラック)を混入したゴムシートなどが挙げられる。市
販の製品としては「ECCOSORB(エコソープ)」
(E&Cエンジニアリング株式会社の商品名)が好適で
ある。
Such a radio wave absorber 8 is a dielectric material having radio wave absorption properties, such as carbon rubber / carbon-containing urethane foam, carbon-containing foam polystyrene, or environmental resistance (moisture resistance, impact resistance, etc.). And a rubber sheet in which carbon particles (carbon black) are mixed as a loss material into an epoxy-modified urethane rubber having excellent properties. "ECCOSORB" is a commercial product.
(Trade name of E & C Engineering Co., Ltd.) is preferable.

【0022】「ECCOSORB(エコソープ)」のL
Sタイプ・26と称されるものの特性を下記表1に示
す。
L of "ECCOSORB"
The characteristics of what is referred to as the S type 26 are shown in Table 1 below.

【0023】 [0023]

【0024】また、他の実施形態として電波吸収体8は
前記ポケット内で窓ガラス1と金属製サッシ枠2間の隙
間のうち片側のみに充填するようにしてもよい。
In another embodiment, the radio wave absorber 8 may be filled in only one side of the gap between the window glass 1 and the metal sash frame 2 in the pocket.

【0025】本発明の効果を試すため、図3に示すよう
な電波吸収体8の無い場合との比較を図4〜図11に示
す。この実験装置としては縦横560mm 開口の金属製サッ
シ枠に縦横600 mm、厚さ8mmのガラスを嵌め込み、この
ガラスの表面には線状アンテナ素子5が印刷してあり、
また、金属製サッシ枠のポケット幅は30mmとしてこの中
に電波吸収体8をガラスの片側または両側に挿入した。
In order to test the effect of the present invention, FIGS. 4 to 11 show a comparison with the case without the radio wave absorber 8 as shown in FIG. In this experimental device, glass of 600 mm in length and 8 mm in thickness was fitted into a metal sash frame with an opening of 560 mm in length and width, and a linear antenna element 5 was printed on the surface of this glass.
The metal sash frame had a pocket width of 30 mm, and the radio wave absorber 8 was inserted into one or both sides of the glass.

【0026】図4は携帯電話のアンテナを縦にした垂直
偏波で、線状アンテナ素子5はこれを図18に示すように
縦向きにした場合であり、図5は同上横向きにした場
合、図6は携帯電話のアンテナを水平にした水平偏波
で、線状アンテナ素子5が縦向きの場合、図7は同上横
向きにした場合で、これらはいずれも電波吸収体8をガ
ラスの片側のみに挿入した場合である。
FIG. 4 shows vertical polarization of the antenna of the mobile phone in the vertical direction. The linear antenna element 5 is in the case where the antenna is in the vertical direction as shown in FIG. 18, and FIG. FIG. 6 shows a case where the antenna of the mobile phone is horizontal and the antenna is horizontal. FIG. 7 shows a case where the linear antenna element 5 is vertical and FIG. 7 shows a case where the antenna is horizontal. This is the case when inserted in

【0027】図8〜図11は電波吸収体8をガラスの両側
に挿入した場合で、図8は垂直偏波で線状アンテナ素子
5が縦向き、図9は垂直偏波で線状アンテナ素子5が横
向き、図10は水平偏波で線状アンテナ素子5が縦向き、
図11は線状アンテナ素子5が横向きの場合である。
8 to 11 show the case where the radio wave absorber 8 is inserted on both sides of the glass. FIG. 8 shows a vertically polarized linear antenna element 5 and FIG. 9 shows a vertically polarized linear antenna element. 5 is horizontal, FIG. 10 is horizontal polarization, and the linear antenna element 5 is vertical,
FIG. 11 shows a case where the linear antenna element 5 is in the horizontal direction.

【0028】これらの測定結果からも判るように、電波
吸収体8を入れた効果はこれを入れない場合と片側のみ
に入れた場合とを比較して17dB程度遮蔽性能が低下す
ることにより、減衰効果があることが判る。
As can be seen from these measurement results, the effect of the insertion of the radio wave absorber 8 is reduced by about 17 dB as compared with the case where the radio wave absorber 8 is not inserted and the case where the radio wave absorber 8 is inserted only on one side. It turns out that it is effective.

【0029】電波吸収体8を両側にいれた場合は入れな
い場合に比較して30dB程度遮蔽性能が向上することに
より十分な減衰効果があることが判る。
It can be seen that a sufficient attenuation effect is obtained when the shielding performance is improved by about 30 dB when the radio wave absorber 8 is inserted on both sides as compared with the case where it is not inserted.

【0030】なお、この電波吸収体8はバックアップリ
ングやセッティングブロック材等を兼用するものでもよ
い。
The radio wave absorber 8 may also serve as a backup ring, a setting block material, and the like.

【0031】[0031]

【発明の効果】以上述べたように本発明の電磁シールド
性能を有する窓構造は、線状アンテナ素子を配置して電
磁遮蔽を行う窓ガラスと金属製サッシ枠との取り合い
で、線状アンテナ素子が金属製サッシ枠のポケット内に
入り込む場合でも、簡単な構成を付加することで、ポケ
ット内での共振係数を下げて、金属による電磁波の反射
をなくし、窓ガラス周囲端部があたかも自由開放端のよ
うなものとし、その結果、当該線状アンテナ素子が遮蔽
性能を低下させる素子とならないようにして、窓ガラス
周囲の電磁遮蔽性能を確保できるものである。
As described above, the window structure having the electromagnetic shielding performance of the present invention has a linear antenna element in which the linear antenna element is arranged to perform electromagnetic shielding and the metal sash frame is engaged. Even if an object gets into the pocket of a metal sash frame, adding a simple structure lowers the resonance coefficient in the pocket, eliminates the reflection of electromagnetic waves by metal, and makes the edge of the window glass as if it were a free open end. As a result, the electromagnetic shielding performance around the window glass can be ensured by preventing the linear antenna element from becoming an element that reduces the shielding performance.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の電磁シールド性能を有する窓構造の1
実施形態を示す縦断側面図である。
FIG. 1 shows a window structure 1 having electromagnetic shielding performance according to the present invention.
It is a longitudinal side view which shows embodiment.

【図2】本発明の電磁シールド性能を有する窓構造の1
実施形態を示す斜視図である。
FIG. 2 shows a window structure 1 having electromagnetic shielding performance according to the present invention.
It is a perspective view showing an embodiment.

【図3】電波吸収材を配置しない場合の窓構造の縦断側
面図である。
FIG. 3 is a vertical side view of the window structure when no radio wave absorbing material is arranged.

【図4】本発明の効果を試すための実験で、電波吸収体
が片側、垂直偏波、線状アンテナ素子縦向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 4 is a graph showing a comparison between a case where the radio wave absorber is one-sided, a vertically polarized wave, and a vertical direction of a linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図5】本発明の効果を試すための実験で、電波吸収体
が片側、垂直偏波、線状アンテナ素子横向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 5 is a graph showing a comparison between the case where the radio wave absorber is one-sided, the vertically polarized wave, and the horizontal direction of the linear antenna element and the case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図6】本発明の効果を試すための実験で、電波吸収体
が片側、水平偏波、線状アンテナ素子縦向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 6 is a graph showing a comparison between a case where the radio wave absorber is one-sided, a horizontally polarized wave, and a vertical direction of a linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図7】本発明の効果を試すための実験で、電波吸収体
が両側、水平偏波、線状アンテナ素子横向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 7 is a graph showing a comparison between a case where the radio wave absorber is on both sides, a horizontally polarized wave, and a horizontal direction of the linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図8】本発明の効果を試すための実験で、電波吸収体
が両側、垂直偏波、線状アンテナ素子縦向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 8 is a graph showing a comparison between a case where the radio wave absorber is on both sides, a vertically polarized wave, and a vertical direction of the linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図9】本発明の効果を試すための実験で、電波吸収体
が両側、垂直偏波、線状アンテナ素子横向きの場合の電
波吸収体の無い場合との比較を示すグラフである。
FIG. 9 is a graph showing a comparison between a case where the radio wave absorber is on both sides, a vertically polarized wave, and a horizontal direction of the linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図10】本発明の効果を試すための実験で、電波吸収
体が両側、水平偏波、線状アンテナ素子縦向きの場合の
電波吸収体の無い場合との比較を示すグラフである。
FIG. 10 is a graph showing a comparison between a case where the radio wave absorber is on both sides, a horizontally polarized wave, and a vertical direction of the linear antenna element and a case where there is no radio wave absorber in an experiment for testing the effect of the present invention.

【図11】本発明の効果を試すための実験で、電波吸収
体が両側、水平偏波、線状アンテナ素子横向きの場合の
電波吸収体の無い場合との比較を示すグラフである。
FIG. 11 is a graph showing a comparison between a case where the radio wave absorber is on both sides, a horizontally polarized wave, and a sideways linear antenna element and no radio wave absorber in an experiment for testing the effect of the present invention.

【図12】電磁シールド性能を有する窓ガラスの斜視図
である。
FIG. 12 is a perspective view of a window glass having electromagnetic shielding performance.

【図13】電磁シールド性能を有する窓ガラスの要部の
正面図である。
FIG. 13 is a front view of a main part of a window glass having electromagnetic shielding performance.

【図14】導電体を線状アンテナ素子(短絡型ダイポー
ル)とした場合の斜視図である。
FIG. 14 is a perspective view when a conductor is a linear antenna element (short-circuit dipole).

【図15】導電体を線状アンテナ素子(短絡型ダイポー
ル)とした場合のその1の電磁界反射等価面積の説明図
である。
FIG. 15 is an explanatory diagram of one electromagnetic field reflection equivalent area when a conductor is a linear antenna element (short-circuit dipole).

【図16】導電体を線状アンテナ素子(短絡型ダイポー
ル)とした場合のその2の電磁界反射等価面積の説明図
である。
FIG. 16 is an explanatory diagram of an electromagnetic field reflection equivalent area of the second case where a conductor is a linear antenna element (short-circuit dipole).

【図17】線状アンテナ素子を配置した窓ガラスの正面
図である。
FIG. 17 is a front view of a window glass on which linear antenna elements are arranged.

【図18】電磁シールド性能を有する窓ガラスで金属製
サッシ枠と線状アンテナ素子の関係を考慮する従来例を
示す説明図である。
FIG. 18 is an explanatory view showing a conventional example in which the relationship between a metal sash frame and a linear antenna element in a window glass having electromagnetic shielding performance is considered.

【符号の説明】[Explanation of symbols]

1…窓ガラス 2…金属製サッ
シ枠 3…線状アンテナ素子 4…線状アンテ
ナ素子 5,5′…線状アンテナ素子 5a…中心 5b…辺 6…導電膜 7…セッティン
グブロック 8…電波吸収体 9…シーリング
材 10…シーリング材 11…バックアッ
プリング
DESCRIPTION OF SYMBOLS 1 ... Window glass 2 ... Metal sash frame 3 ... Linear antenna element 4 ... Linear antenna element 5, 5 '... Linear antenna element 5a ... Center 5b ... Side 6 ... Conductive film 7 ... Setting block 8 ... Radio wave absorber 9: Sealing material 10: Sealing material 11: Backup ring

フロントページの続き (72)発明者 ▲高▼坂 修一 東京都調布市飛田給二丁目19番1号 鹿島 建設株式会社技術研究所内 (72)発明者 冨樫 元康 神奈川県川崎市麻生区白山3−1−1− 504Continued on the front page (72) Inventor ▲ Taka ▼ Shuichi Sakaichi 2-9-1-1, Tobita-shi, Chofu-shi, Tokyo Kashima Construction Co., Ltd. (72) Inventor Motoyasu Togashi 3-1 Shirayama, Aso-ku, Kawasaki-shi, Kanagawa Prefecture. 1-504

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 遮蔽しようとする電波に共振させる長さ
の線状アンテナ素子を電磁遮蔽素子として、その素子の
電磁界反射等価面積(散乱開口面積)または電磁界反射
等価体積(散乱開口体積)を考慮して規則的に配列させ
た窓ガラスを金属製サッシ枠に嵌め込むのに、窓ガラス
と金属製サッシ枠間に電波吸収体を充填することを特徴
とする電磁シールド性能を有する窓構造。
A linear antenna element having a length resonating with a radio wave to be shielded is used as an electromagnetic shielding element, and an electromagnetic field reflection equivalent area (scattering aperture area) or an electromagnetic field reflection equivalent volume (scattering aperture volume) of the element is used. A window structure with electromagnetic shielding performance characterized by filling a radio wave absorber between the window glass and the metal sash frame to fit the window glass regularly arranged in consideration of .
JP35899697A 1997-12-26 1997-12-26 Window structure with electromagnetic shielding performance Expired - Fee Related JP3333729B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP35899697A JP3333729B2 (en) 1997-12-26 1997-12-26 Window structure with electromagnetic shielding performance

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP35899697A JP3333729B2 (en) 1997-12-26 1997-12-26 Window structure with electromagnetic shielding performance

Publications (2)

Publication Number Publication Date
JPH11191687A true JPH11191687A (en) 1999-07-13
JP3333729B2 JP3333729B2 (en) 2002-10-15

Family

ID=18462206

Family Applications (1)

Application Number Title Priority Date Filing Date
JP35899697A Expired - Fee Related JP3333729B2 (en) 1997-12-26 1997-12-26 Window structure with electromagnetic shielding performance

Country Status (1)

Country Link
JP (1) JP3333729B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6062925A (en) * 1997-07-31 2000-05-16 Kvaerner Masa-Yards Oy Service vessel operating method
JP2008199562A (en) * 2007-02-16 2008-08-28 Softbank Bb Corp Relay amplifying device for mobile communication
CN109588033A (en) * 2019-01-04 2019-04-05 邓冬来 The clutter remove device used suitable for automotive interior

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6062925A (en) * 1997-07-31 2000-05-16 Kvaerner Masa-Yards Oy Service vessel operating method
JP2008199562A (en) * 2007-02-16 2008-08-28 Softbank Bb Corp Relay amplifying device for mobile communication
CN109588033A (en) * 2019-01-04 2019-04-05 邓冬来 The clutter remove device used suitable for automotive interior

Also Published As

Publication number Publication date
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