JPS60250187A - Sound blocking dual-layer glass - Google Patents
Sound blocking dual-layer glassInfo
- Publication number
- JPS60250187A JPS60250187A JP59106944A JP10694484A JPS60250187A JP S60250187 A JPS60250187 A JP S60250187A JP 59106944 A JP59106944 A JP 59106944A JP 10694484 A JP10694484 A JP 10694484A JP S60250187 A JPS60250187 A JP S60250187A
- Authority
- JP
- Japan
- Prior art keywords
- sound
- hollow layer
- air
- layer glass
- sound blocking
- 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
Landscapes
- Securing Of Glass Panes Or The Like (AREA)
- Special Wing (AREA)
- Building Environments (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔技術分野〕
本発明は、遮音性に優れた複層ガラス(ペアガラス)に
関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to double glazing with excellent sound insulation properties.
複層カラスの中空層内に空気中よりも音速の大きなフj
スーを封入すると、音波の屈折により、見掛は上中空層
が厚くなり、また音波の全反射現象により遮音性が高く
なることが知られている。即ち、第3図に示すように空
気中(複層ガラス外)での音速をC1、複層ガラス(3
)の中空層(2)内での音速を02とすれば、第3図図
示の入射音の入射角θ1と係があるので、中空層(2)
内での音速が大きければ(CI<C2)、θ1〈θ2と
なり、中空層(2)を横切る行程(パス)が長くなり、
見掛は上中空層(2)が厚くラス(3)に入射した音波
は全反射されて内部に侵入できないのである。しかしな
がら、例えばヘリウム(ヘリウム中での音速970 m
/ 5ec) 、水素などの音速の大きなガスを封入し
、ガスが長時聞漏れないようにするのけ困難で、技術的
にもコスト的にも問題が多かった。Inside the hollow layer of multi-layered glass, there is a bubble with a higher sound speed than in air.
It is known that when Sue is encapsulated, the upper hollow layer becomes thicker due to the refraction of sound waves, and the sound insulation properties are improved due to the phenomenon of total reflection of sound waves. That is, as shown in Figure 3, the sound velocity in the air (outside the double-glazed glass) is C1, and the double-glazed glass (3
) If the sound speed in the hollow layer (2) is 02, it is related to the incident angle θ1 of the incident sound shown in Figure 3, so the hollow layer (2)
If the sound speed inside the hollow layer (2) is large (CI<C2), θ1<θ2, and the path across the hollow layer (2) becomes longer.
The upper hollow layer (2) is apparently thick, and the sound waves incident on the lath (3) are totally reflected and cannot penetrate inside. However, for example, helium (the speed of sound in helium is 970 m
/5ec), it was difficult to seal in a gas with a high sound velocity such as hydrogen and prevent the gas from leaking out for a long time, and there were many problems in terms of technology and cost.
本発明は叙上の従来技術の欠点に鑑みてなされたもので
あり、その目的とするところけ空気よりも音速の速いガ
スを封入したりすることなく、空気そのままで遮音性を
高めることができ、しかも中空層内に空気゛を完全に密
封する必要もなく、遮音性を高めることにある。The present invention was made in view of the drawbacks of the prior art described above, and its purpose is to improve the sound insulation properties of air as it is without enclosing a gas with a faster sound speed than air. Moreover, there is no need to completely seal air inside the hollow layer, and the purpose is to improve sound insulation.
本発明の遮音複Rガラスは、カラス板(1)間に形成さ
れた中空層(2)内に高温の空気を入れたものであり、
これによって上記目的を達成できるに至った。The sound insulating double R glass of the present invention has high temperature air injected into the hollow layer (2) formed between the glass plates (1),
This made it possible to achieve the above objective.
以下、本発明の実施例を添H図によシ詳述する。第1図
に示すものけ、複層ガラス(3)内に設けたし−タ(4
)Kよって中空層(2)内の空気を暖めるようにしだも
のである。中空層(2)は一対のカラス板+1+を対向
させて形成されており、中空層(2)の四周はシール材
(図示せず)によって封じられているが、完全な気密性
まで必らずしも要求されるものではない。中空層(2)
内においてガラス板(1)の内面にはフィルター状のし
−タ(4)が貼シ付けられており、このし−タ(4)K
通電して中空層(2)内の空気を暖められるようにしで
ある。空気の音速は温度に依存し〔音速C=341+Q
、6T(m/5ec)、T:温度(℃)〕、温度が高く
なれば音速も大きくなるので、空気が暖められている中
空層(2)内では外部よりも音速が大きくなっており、
L記の如く音速の大きなガスを封入した場合と同様の遮
音効果を得ることができるのである。Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings. As shown in Figure 1, the shutter (4) installed inside the double-glazed glass (3)
)K so as to warm the air inside the hollow layer (2). The hollow layer (2) is formed by facing a pair of glass plates +1+, and the four circumferences of the hollow layer (2) are sealed with a sealing material (not shown), but it is not necessary to achieve complete airtightness. It's not even required. Hollow layer (2)
Inside, a filter-like screener (4) is pasted on the inner surface of the glass plate (1), and this screener (4) K
This allows electricity to be applied to warm the air within the hollow layer (2). The speed of sound in air depends on the temperature [speed of sound C=341+Q
, 6T (m/5ec), T: temperature (°C)], the higher the temperature, the higher the speed of sound, so the speed of sound is higher inside the hollow layer (2) where the air is warmed than outside.
It is possible to obtain the same sound insulation effect as in the case where a gas with a high sound velocity is sealed as shown in L.
第2図に示すものけ本発明の例であり、温風暖房用の温
風をガラス板(1)の導入孔(5)より中空層(2)内
へ導き、中空層(2)内の空気の温度を上昇させ、その
後排出孔(6)から熱風を室内へ送るようにしたもので
ある。Figure 2 shows an example of the present invention, in which hot air for hot air heating is guided into the hollow layer (2) through the introduction hole (5) of the glass plate (1). The temperature of the air is raised, and then hot air is sent into the room from the exhaust hole (6).
本発明は叙述の如−く構成されている妙・ら、中空層内
における音速を大きくでき、中空層の見掛けの厚さを大
きくできて遮音性能を大きくできるものであり、しかも
空気以外のガスを中空層内に封入する場合のよう忙完全
な気密性を要求されず、技術的にも簡易であり、コスト
も低廉となる利点がある。The present invention is constructed as described above, and is capable of increasing the sound velocity in the hollow layer, increasing the apparent thickness of the hollow layer, and increasing the sound insulation performance, and moreover, it is possible to increase the sound insulation performance by increasing the sound velocity within the hollow layer. It has the advantage that it does not require complete airtightness as is the case when encapsulating it in a hollow layer, is technically simple, and is inexpensive.
第1図は本発明の一実施例を示す断面図、第2図は本発
明の他側を示す斜視図、第3図及び第4図は従来技術の
説明図である。
f+)・・・ガラス板、(2)・・・中空層。
代理人 弁理士 石 1)長 上
第1図
第3図
第2図
す
第4図FIG. 1 is a sectional view showing one embodiment of the present invention, FIG. 2 is a perspective view showing the other side of the invention, and FIGS. 3 and 4 are explanatory views of the prior art. f+)...Glass plate, (2)...Hollow layer. Agent Patent Attorney Ishi 1) Chief Figure 1 Figure 3 Figure 2 Figure 4
Claims (1)
れて成ることを特徴とする遮音複層ガラスSound-insulating double-glazed glass characterized by having high-temperature air introduced into a hollow layer formed between fl glass plates.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59106944A JPS60250187A (en) | 1984-05-25 | 1984-05-25 | Sound blocking dual-layer glass |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59106944A JPS60250187A (en) | 1984-05-25 | 1984-05-25 | Sound blocking dual-layer glass |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60250187A true JPS60250187A (en) | 1985-12-10 |
Family
ID=14446483
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59106944A Pending JPS60250187A (en) | 1984-05-25 | 1984-05-25 | Sound blocking dual-layer glass |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60250187A (en) |
-
1984
- 1984-05-25 JP JP59106944A patent/JPS60250187A/en active Pending
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