JPH03250797A - Laminated plate with low radio wave reflection property - Google Patents
Laminated plate with low radio wave reflection propertyInfo
- Publication number
- JPH03250797A JPH03250797A JP2048055A JP4805590A JPH03250797A JP H03250797 A JPH03250797 A JP H03250797A JP 2048055 A JP2048055 A JP 2048055A JP 4805590 A JP4805590 A JP 4805590A JP H03250797 A JPH03250797 A JP H03250797A
- Authority
- JP
- Japan
- Prior art keywords
- plate
- film
- radio wave
- wave
- reflectance
- 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.)
- Pending
Links
- 239000000758 substrate Substances 0.000 claims description 13
- 238000002310 reflectometry Methods 0.000 claims description 4
- 230000007423 decrease Effects 0.000 abstract description 4
- 239000012528 membrane Substances 0.000 description 7
- 239000011521 glass Substances 0.000 description 6
- 238000002834 transmittance Methods 0.000 description 6
- 239000005357 flat glass Substances 0.000 description 5
- 101700004678 SLIT3 Proteins 0.000 description 4
- 102100027339 Slit homolog 3 protein Human genes 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 239000005329 float glass Substances 0.000 description 4
- 235000019646 color tone Nutrition 0.000 description 3
- 238000009413 insulation Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 229910001369 Brass Inorganic materials 0.000 description 2
- 239000010951 brass Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 229910001220 stainless steel Inorganic materials 0.000 description 2
- 239000010935 stainless steel Substances 0.000 description 2
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical group [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 239000006096 absorbing agent Substances 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000004567 concrete Substances 0.000 description 1
- 239000004035 construction material Substances 0.000 description 1
- 229910001882 dioxygen Inorganic materials 0.000 description 1
- 238000001035 drying Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 239000004570 mortar (masonry) Substances 0.000 description 1
- 229920002037 poly(vinyl butyral) polymer Polymers 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 239000011150 reinforced concrete Substances 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- OGIDPMRJRNCKJF-UHFFFAOYSA-N titanium oxide Inorganic materials [Ti]=O OGIDPMRJRNCKJF-UHFFFAOYSA-N 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Landscapes
- Laminated Bodies (AREA)
- Surface Treatment Of Glass (AREA)
- Joining Of Glass To Other Materials (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野1
本発明は建造物などによる電波の障害を防ぎ、電波を効
率よく透過させる積層板に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application 1] The present invention relates to a laminate that prevents interference with radio waves caused by buildings and the like and efficiently transmits radio waves.
[従来の技術]
近年、テレビ電波の受信にあたり、ビルの反射によるゴ
ースト障害が問題になり、ビルのコンクリート壁などに
フェライト電波吸収体を設けることが実用化されつつあ
る。[Prior Art] In recent years, ghost interference caused by reflection from buildings has become a problem when receiving television radio waves, and the provision of ferrite radio wave absorbers on the concrete walls of buildings is being put into practical use.
一方、窓ガラスは次第に厚いものが使用され、しかも、
金属、金属酸化物などの膜をコーティングしたり、この
ような膜を有するフィルムを貼付けた断熱性能などの機
能を付与したものが増加の傾向にある。厚さの影響はさ
ほどではないが、ガラスより電波に対して反射率が高い
膜をコーティングしたり、フィルムを貼付けると反射率
が100%近くなり、電波障害は避けられなかった。On the other hand, window glass is gradually becoming thicker, and
There is an increasing trend in the number of products that are coated with metal, metal oxide, etc. films, or are coated with films containing such films to provide functions such as heat insulation performance. The effect of thickness is not so great, but if you coat or attach a film that has a higher reflectivity for radio waves than glass, the reflectance will approach 100%, making radio interference unavoidable.
したがって、このような場合には電波の到来方向の窓は
何もコーティングしていないガラスを配設せざるをえず
、色調が同一ビルで異なるという不調和が避けられなか
った。Therefore, in such cases, the windows in the direction in which the radio waves arrive had to be made of uncoated glass, which inevitably led to inconsistencies in the color tones of different buildings.
[発明が解決しようとする問題点]
本発明はこのような点に鑑みてなされたものであり、T
V放送波などの電波に対して反射率を低減せしめた板状
体を提供することを目的とする。[Problems to be solved by the invention] The present invention has been made in view of the above points, and is
It is an object of the present invention to provide a plate-shaped body with reduced reflectance for radio waves such as V broadcast waves.
E問題点を解決するための手段]
本発明は、基板に、該基板より電波に対する反射率が高
い膜もしくはフィルムが形成された板状体において、該
膜もしくはフィルムを、一辺の長さが前記電磁波の波長
λの0.4倍以下になるように分割したことを特徴とす
る。Means for Solving Problem E] The present invention provides a plate-like body in which a film or film having a higher reflectivity for radio waves than the substrate is formed on a substrate, and the film or film has a side length of It is characterized by being divided into 0.4 times or less the wavelength λ of the electromagnetic wave.
[作用]
零発者らは、断熱ガラスなどの電波にたいする反射率の
高い板状体が惹起する電波障害を極力低減すべく鋭意研
究した結果、膜もしくはフィルムを分割することに着目
して本発明をなしたものである。[Function] As a result of intensive research to reduce as much as possible radio wave interference caused by plate-like materials with high reflectivity for radio waves, such as insulating glass, the present inventors focused on dividing membranes or films and developed the present invention. This is what was done.
900fl角、】0鶴厚さの板ガラスにAfを2000
人厚さに蒸着したほぼ100%の反射率を有する断熱ガ
ラスを用意してカンタ−等により一辺長さLが次第に小
さくなるように正方形状に切断して、その都度500M
Hzの電波を入射角0度で照射したときの単位面積あた
りの反射量を測定した。Af 2000 on a plate glass of 900fl square, ]0 Tsuru thickness
Prepare insulating glass with a reflectance of almost 100% that has been vapor-deposited to a thickness of about 100 mm, and cut it into square shapes with a canter or the like so that the side length L gradually decreases, each time having a length of 500 m.
The amount of reflection per unit area was measured when Hz radio waves were irradiated at an incident angle of 0 degrees.
この結果に基づいて、一辺長さしの電波の波長λ(50
0MHzにおいては60備)にだいする比L/λと反射
量の関係を求めたところ、第3図に示すような結果が得
られた。Based on this result, the wavelength λ (50
When the relationship between the ratio L/λ and the amount of reflection was determined at 0 MHz, the results shown in FIG. 3 were obtained.
この結果から明らかなように、L/λを0.4以下、好
ましくは0.3以下とすることにより、反射量が格段に
低下することがわかる。As is clear from this result, it can be seen that by setting L/λ to 0.4 or less, preferably 0.3 or less, the amount of reflection is significantly reduced.
なお、周波数が90MIIzのTV放送波VHF帯から
周波数が770M)lzのTV放送波UHF帯全域まで
同様の傾向があることを確認している。It has been confirmed that a similar tendency exists throughout the TV broadcast wave VHF band with a frequency of 90 MIIz to the TV broadcast wave UHF band with a frequency of 770 M)lz.
このような結果は次のような理由に起因するものと思わ
れる。This result is believed to be due to the following reasons.
すなわち、任意の散乱体に平面波が入射すると、散乱体
には導電電流または分掻電流が流れ、これが2次的な放
射源となって電磁波を発生し、電磁波を反射する。実際
には電子が散乱体の端から端まで動くのではなく、入射
電磁波の周波数に同調して、ある点で電子が振動してい
るだけである。That is, when a plane wave is incident on an arbitrary scatterer, a conductive current or a spacing current flows through the scatterer, which becomes a secondary radiation source, generates electromagnetic waves, and reflects the electromagnetic waves. In reality, the electrons do not move from one end of the scatterer to the other, but only oscillate at a certain point in tune with the frequency of the incident electromagnetic wave.
このような電子の振動によって生じた電子濃度の高い部
位が移動する。これが電磁波を反射させる要因になるも
ので、板状体を分割してL/λを小さくすることにより
、電子が自由に移動できる領域が狭くなりこの結果、単
位面積あたりの反射量が低下するものと推定される。A region with high electron concentration generated by such electron vibration moves. This causes electromagnetic waves to be reflected. By dividing the plate-shaped body and reducing L/λ, the area in which electrons can move freely becomes narrower, and as a result, the amount of reflection per unit area decreases. It is estimated to be.
また、板状体の一辺長さしをλ/2 とすると共振現象
が起こり、最も効率よく電磁波を受信する状態になるの
で、L/λが0.5近傍で極大値が存在する。本発明は
0.5よりさらに小さな0.4以下好ましくは0.3以
下とすることにより反射量を極減させる。Furthermore, if the length of one side of the plate-shaped body is λ/2, a resonance phenomenon occurs and the electromagnetic wave is most efficiently received, so that a maximum value exists when L/λ is around 0.5. In the present invention, the amount of reflection is minimized by setting it to 0.4 or less, preferably 0.3 or less, which is even smaller than 0.5.
また、厚さx (m)の導電性の膜あるいはフィルムに
周波数が「の電波を垂直方向に照射すると、電波の透過
度EはE=exp(−αX)となる。Further, when a conductive membrane or film having a thickness x (m) is irradiated with radio waves having a frequency of "2" in the vertical direction, the transmittance E of the radio waves becomes E=exp(-αX).
ここで、αは導電性の膜の減衰定数でα=4.82π・
f+と表わされるので、例えばXを500人、fを10
0Mt+zとすると透過度Eは0.93となりほとんど
吸収されず、かつ分割することによって反射量も低減さ
せているので、電波を効率よく透過することがわかる。Here, α is the attenuation constant of the conductive film, and α=4.82π・
It is expressed as f+, so for example, if X is 500 people and f is 10
When 0Mt+z, the transmittance E is 0.93, which means that almost no absorption occurs, and the amount of reflection is also reduced by dividing, so it can be seen that radio waves are transmitted efficiently.
[実施例] 以下、図面を参照しながら本発明の詳細な説明する。[Example] Hereinafter, the present invention will be described in detail with reference to the drawings.
第1図は本発明の実施例1、実施例2における積層板の
一部を表わす斜視図、第2図は本発明の実施例3におけ
る積層板の一部を表わす斜視図、第3図はL/λと単位
面積あたりの電波反射量の関係を示す特性図である。FIG. 1 is a perspective view showing a part of a laminate in Example 1 and Example 2 of the present invention, FIG. 2 is a perspective view showing a part of a laminate in Example 3 of the invention, and FIG. FIG. 3 is a characteristic diagram showing the relationship between L/λ and the amount of radio wave reflection per unit area.
丈長」1一
基板1として板ガラスを用い、この板ガラスに断熱性能
を有する膜2をコーティングした例について説明する。An example will be described in which a plate glass is used as the substrate 1 and the plate glass is coated with a film 2 having heat insulating performance.
第1図に示すように、基板1として9031角、板厚1
0富1のフロートガラスを用意して、この基板1に膜2
の一辺長さしが150鶴となるように、まずスリット3
が形成される部分に有機染料をスクリーン印刷し、乾燥
した後DCマグネスパッタリング法によりステンレス#
(S[l5316)をターゲットとして、約10′3
Torrに減圧されたアルゴンガス中でステンレス膜を
85人の厚さに成膜し、次いで金属チタンをターゲット
として、約10”Torrに減圧された酸素ガス中で酸
化チタン膜を100人の厚さに成膜した0次に有機染料
を除去した。As shown in FIG.
Prepare a float glass with a concentration of 0 and 1, and apply a film 2 to this substrate 1.
First, cut slit 3 so that the length of one side is 150 cranes.
An organic dye is screen printed on the area where is formed, and after drying, stainless steel #
(S[l5316) as a target, about 10'3
A stainless steel film was formed to a thickness of 85 mm in argon gas at a reduced pressure of about 10 Torr, and then a titanium oxide film was formed to a thickness of 100 mm in an oxygen gas at a reduced pressure of about 10 Torr using titanium as a target. The zero-order organic dye formed into a film was removed.
このようにして得られた積層板は膜2の一辺長さしが1
50鶴、スリット3の幅が1mであり、色調がシルバー
グレー、可視光透過率が31%、可視光反射率が13%
、日射透過率が25%、日射反射率が11%の良好な断
熱性能を示した。In the thus obtained laminate, the length of one side of the membrane 2 is 1
50 cranes, the width of slit 3 is 1m, the color tone is silver gray, the visible light transmittance is 31%, and the visible light reflectance is 13%.
It showed good heat insulation performance with a solar transmittance of 25% and a solar reflectance of 11%.
さらにこの積層板に100Mt+z (L /λ−0,
05)、300MIlz (L /λ−0,15) 、
500M)lz (L/λ−0,25)の電波を照射し
て反射率を測定したところ、それぞれ反射率は0.5%
、4%、11%となった。分割しない場合の反射率が
それぞれ・18%・15%・25%であるので、格段に
低下しており、TV放送波のU HF帯までの電波に対
して、電波障害を軽減していることがわかる。Furthermore, 100Mt+z (L /λ-0,
05), 300MIlz (L/λ-0,15),
When the reflectance was measured by irradiating radio waves of 500M)lz (L/λ-0,25), the reflectance was 0.5% for each.
, 4%, and 11%. The reflectance when not divided is 18%, 15%, and 25%, respectively, which is significantly lower, and reduces radio wave interference for radio waves from the U to HF bands of TV broadcast waves. I understand.
11九影
ガラスを基板として断熱フィルムを貼付けた例について
説明する。An example in which a heat insulating film is attached to a substrate made of No. 11 Nine Shadow Glass will be described.
第1図に示すように、基板lとして905鶴角、板厚1
0鶴のフロートガラスを用意して、シート抵抗が50〜
60Q/口のAgが蒸着された有機フィルム2′をほぼ
全面に貼付け、その後カッター等でスリット3に相当す
る部分を輻1鶴で切り取り、フィルム2°を、一辺長さ
が150 mWの36個の正方形に分割する。As shown in FIG.
Prepare 0 Tsuru float glass and set the sheet resistance to 50~
An organic film 2' on which Ag of 60Q/hole was vapor-deposited was pasted on almost the entire surface, and then the part corresponding to slit 3 was cut out with a sharp edge 1 crane using a cutter, etc., to form 36 pieces of film 2° each with a side length of 150 mW. Divide into squares.
このようにして得られた積層板は、色調がゴールド、可
視光透過率が60%、可視光反射率が21%、日射透過
率が44%、日射反射率が35%の良好な断熱性能を示
すとともに、さらにこの積層板に100M1lz(L/
λ−0,05) 、300Hz (L / λ= 0
.15)、500MIlz (L /λ−0,25)の
電波を照射して反射率を測定したところ、それぞれ反射
率は0.5%、12%、28%となった。分割しない場
合の反射率がそれぞれ、52%、45%、63%である
ので、格段に低下しており、TV放送波のUHF帯まで
の電波に対して、電波障害を軽減していることがわかる
。犬l潰」−
ガラスを基板として、板状体を積層した例について説明
する。The thus obtained laminate has a gold color, a visible light transmittance of 60%, a visible light reflectance of 21%, a solar transmittance of 44%, and a solar reflectance of 35%, and has good thermal insulation performance. In addition, 100M1lz (L/
λ-0,05), 300Hz (L/λ=0
.. 15) and 500 MIlz (L/λ-0,25) and measured the reflectance, and the reflectance was 0.5%, 12%, and 28%, respectively. The reflectance when not divided is 52%, 45%, and 63%, respectively, which is a significant decrease, and it is clear that radio wave interference is reduced for radio waves up to the UHF band of TV broadcast waves. Recognize. An example in which plate-like bodies are laminated using glass as a substrate will be described.
第2図に示すように、基板1として9151角、板厚4
鶴のフロートガラスを用意して、ポリビニールブチラー
ルなどの中間膜4と板状体2° としての150 u角
(L=1501曹)、板厚611のフロートガラス36
枚をスリット3の幅が3Nになるように積層して仮圧着
した後、通常のオートクレーブ処理をして積層板を得る
。As shown in Figure 2, the board 1 is 9151 square and board thickness is 4.
Prepare a crane float glass, and add an interlayer film 4 such as polyvinyl butyral and a float glass 36 with a 150 u angle (L = 1501 mm) and a plate thickness of 611 mm as a plate-shaped body 2°.
After laminating the sheets so that the width of the slit 3 is 3N and temporarily press-bonding them, a normal autoclave treatment is performed to obtain a laminated sheet.
このようにして得られた積層体は周波数が500Mt(
zの電波に対して、反射率が3,7%となり、lO鶴厚
さの単板ガラスの反射率が8.3%であるので、1/2
以下に低減された。The laminate thus obtained has a frequency of 500 Mt (
For the radio wave of
Reduced to below.
以上、好適な実施例により説明したが、本発明はこれら
限定されるものではなく、種々の応用が可能である。Although the present invention has been described above using preferred embodiments, the present invention is not limited to these embodiments, and various applications are possible.
本発明の基板上に積層される膜あるいはフィルムはシー
ト抵抗がIKQ10以下のものであれば効果が期待でき
るので、各種の公知の膜、フィルムを使用することがで
きる。また、基板上に積層さる板状体は板ガラス以外に
も、ブラスチンク、セラミック、鉄筋コンクリートなど
の構築材あるいは反射率が高い金属などであってもよい
。If the membrane or film laminated on the substrate of the present invention has a sheet resistance of IKQ10 or less, the effect can be expected, and therefore various known membranes or films can be used. In addition to plate glass, the plate-shaped body laminated on the substrate may be made of a construction material such as brass tink, ceramic, reinforced concrete, or a metal with high reflectance.
また、これらの一辺長さは、反射率低減の対象となる電
波の周波数に応じて、TV放送波VHF帯(90MHz
〜220Mtlz)までの場合には545fi以下、
好ましくは409fi以下とすればよく、TV放送波U
HF帯(470MHz 〜770MHz)までの場合に
は1561以下、好ましくは117 u以下とすればよ
い基板としては、ガラス以外にも、分割される膜、フィ
ルムあるいは板状体より電波反射率の低いものであれば
よく、ブラスチンク、モルタル器タイルなど各種のもの
を採用することができる。In addition, the length of each side of these varies depending on the frequency of the radio waves targeted for reflectance reduction.
~220Mtlz) up to 545fi,
Preferably it should be 409fi or less, and TV broadcast waves U
In the case of up to the HF band (470 MHz to 770 MHz), the substrate should be 1561 or less, preferably 117 u or less. In addition to glass, substrates that have a lower radio wave reflectance than the membrane, film, or plate-like material to be divided can be used. Various materials such as brass tink and mortar tiles can be used.
[発明の効果]
本発明の積層板は比較的電波反射率の高い部分を分割し
、その一辺長さを電波の波長λの0.4倍以下、好まし
くは0.3以下とすることにより、電波反射率を低減さ
せ、電波障害を極力少なくするものである。[Effects of the Invention] The laminate of the present invention divides a portion with a relatively high radio wave reflectance, and the length of one side thereof is set to 0.4 times or less, preferably 0.3 or less, to the radio wave wavelength λ. This reduces radio wave reflectance and minimizes radio wave interference.
したがって、ビル等の建築物の窓等において、電波到来
方向に本発明の例えば断熱性能を有する積層板を配設し
、その他の部分に分割しない同種の積層板を配設すれば
、建築物全体が断熱効果を奏するとともに、同し色調と
することができるので美観上も好ましい。Therefore, if a laminate of the present invention having heat-insulating performance is placed in the direction of arrival of radio waves in the windows of a building or other building, and a laminate of the same type that is not divided into other parts is placed, the whole building will be covered. In addition to having a heat insulating effect, they are also aesthetically pleasing because they can be made to have the same color tone.
第1図は本発明の実施例1、実施例2における積層板の
一部を表わす斜視図、第2図は本発明の実施例3におけ
る積層板の一部を表わす斜視図、第3図はL/λと単位
面積あたりの電波反射量の関係を示す特性図である。
1・・・・基板
2・・・・膜、
2″・・板状体
3・・・・スリノ
4・・・・中間膜
2′
ト
フィルム
第
図FIG. 1 is a perspective view showing a part of a laminate in Example 1 and Example 2 of the present invention, FIG. 2 is a perspective view showing a part of a laminate in Example 3 of the invention, and FIG. FIG. 3 is a characteristic diagram showing the relationship between L/λ and the amount of radio wave reflection per unit area. 1...Substrate 2...Membrane, 2''...Plate body 3...Surino 4...Intermediate film 2'
Claims (1)
ィルムもしくは板状体が積層された積層板において、膜
、フィルムもしくは板状体を、一辺の長さが前記電波の
波長λの0.4倍以下になるように分割したことを特徴
とする電波に対して低反射特性を有する積層板。In a laminated plate in which a film, film, or plate-like body having a higher reflectivity for radio waves than the substrate is laminated on a substrate, the film, film, or plate-like body is laminated with a side length of 0.4 of the wavelength λ of the radio wave. A laminate having low reflection characteristics against radio waves, characterized in that it is divided into two parts or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2048055A JPH03250797A (en) | 1990-02-28 | 1990-02-28 | Laminated plate with low radio wave reflection property |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2048055A JPH03250797A (en) | 1990-02-28 | 1990-02-28 | Laminated plate with low radio wave reflection property |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03250797A true JPH03250797A (en) | 1991-11-08 |
Family
ID=12792656
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2048055A Pending JPH03250797A (en) | 1990-02-28 | 1990-02-28 | Laminated plate with low radio wave reflection property |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03250797A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6195034B1 (en) | 1997-03-31 | 2001-02-27 | Nippon Sheet Glass Co., Ltd. | Radio wave absorbing panel |
| US6395398B1 (en) | 1999-03-31 | 2002-05-28 | Central Glass Company, Limited | Frequency selective plate and method for producing same |
| DE19508042B4 (en) * | 1994-03-07 | 2008-05-21 | Nippon Sheet Glass Co., Ltd. | For electromagnetic radiation permeable and heat-reflecting coating and associated manufacturing process and use |
| WO2011074609A1 (en) * | 2009-12-15 | 2011-06-23 | 旭化成せんい株式会社 | Noise absorbing fabric |
-
1990
- 1990-02-28 JP JP2048055A patent/JPH03250797A/en active Pending
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE19508042B4 (en) * | 1994-03-07 | 2008-05-21 | Nippon Sheet Glass Co., Ltd. | For electromagnetic radiation permeable and heat-reflecting coating and associated manufacturing process and use |
| US6195034B1 (en) | 1997-03-31 | 2001-02-27 | Nippon Sheet Glass Co., Ltd. | Radio wave absorbing panel |
| US6504501B2 (en) | 1997-03-31 | 2003-01-07 | Nippon Sheet Glass Co., Ltd. | Radio wave absorbing panel |
| US6395398B1 (en) | 1999-03-31 | 2002-05-28 | Central Glass Company, Limited | Frequency selective plate and method for producing same |
| US6689256B2 (en) | 1999-03-31 | 2004-02-10 | Central Glass Company, Limited | Frequency selective plate and method for producing same |
| WO2011074609A1 (en) * | 2009-12-15 | 2011-06-23 | 旭化成せんい株式会社 | Noise absorbing fabric |
| CN102656962A (en) * | 2009-12-15 | 2012-09-05 | 旭化成纤维株式会社 | Noise absorbing fabric |
| TWI586251B (en) * | 2009-12-15 | 2017-06-01 | Asahi Kasei Fibers Corp | Noise absorbing fabric |
| US9972913B2 (en) | 2009-12-15 | 2018-05-15 | Asahi Kasei Fibers Corporation | Noise absorbing fabric |
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