JPH01207150A - Dust collecting electrode - Google Patents

Dust collecting electrode

Info

Publication number
JPH01207150A
JPH01207150A JP3316288A JP3316288A JPH01207150A JP H01207150 A JPH01207150 A JP H01207150A JP 3316288 A JP3316288 A JP 3316288A JP 3316288 A JP3316288 A JP 3316288A JP H01207150 A JPH01207150 A JP H01207150A
Authority
JP
Japan
Prior art keywords
conductive layer
layer
insulating layer
space
conductive
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
Application number
JP3316288A
Other languages
Japanese (ja)
Inventor
Hitoshi Nagoshi
名越 均
Taizo Kimura
泰三 木村
Kazunari Takashima
高島 一成
Kojiro Matsuo
松尾 光二郎
Harutoki Nakamura
中村 治時
Minoru Yoshinaka
芳中 實
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP3316288A priority Critical patent/JPH01207150A/en
Publication of JPH01207150A publication Critical patent/JPH01207150A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To lower the resistance value of conductive layers to a specific value or below and to enhance reliability in a high-voltage contact part by laminating a 1st insulating layer and a 1st conductive layer as well as the 2nd insulating layer and the 2nd conductive layer successively and forming a large space layer in the space between the conductive layer and the layer facing said conductive layer. CONSTITUTION:At least the 1st insulating layer 3 and the 1st conductive layer 1 as well as the 2nd insulating layer 4 and the 2nd conductive layer 2 are successively laminated and the space layer t3 larger than the space between the other layers is formed in the space between the conductive layer of at least either of the 1st conductive layer 1 and the 2nd conductive layer 2 and the layer facing said conductive layer and the resistance value of the conductive layer is confined to <=10OMEGA/cm<2>. As a result, the decrease of the dust collection rate with elapsed time is minimized and the reliability in the high-pressure contact part is enhanced.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は塵埃を帯電させて集塵する空気清浄機の集塵電
極に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a dust collection electrode for an air cleaner that collects dust by charging it.

従来の技術 第6図に従来の集塵電極の断面図を示す。すなわち、第
1の絶縁層310表面に第1の導電層30が形成された
フィルムと、第2の絶縁層330表面に第2の導電層3
2が形成されたフィルムとを一定の空間層をもうけて順
次積層・した構造となっていた。
BACKGROUND OF THE INVENTION FIG. 6 shows a cross-sectional view of a conventional dust collecting electrode. That is, a film in which the first conductive layer 30 is formed on the surface of the first insulating layer 310 and a film in which the first conductive layer 30 is formed on the surface of the second insulating layer 330 are formed.
It had a structure in which the films on which No. 2 was formed were sequentially laminated with a certain space layer between them.

発明が解決しようとする課題 上記構成における塵埃が集塵される原理について説明す
る。
Problems to be Solved by the Invention The principle of collecting dust in the above configuration will be explained.

矢印は空気の流れる方向を示している。Arrows indicate the direction of air flow.

第1の導電層30.34に正の高電圧を印加し、第2の
導電層32.36をアース電位とすると、集塵負極の前
方から正に帯電した塵埃は、集塵電極を通過するとき、
電界によるクーロン力により、アース電圧側の導電層3
2.36と第2の絶縁層33.37の表面に付着し集塵
される。しかしながら、アース電圧側の導電層32.3
6に付着した正に帯電した塵埃は、電気的に中和するが
、第2の絶縁層33.37の表面に付着した正に帯電し
た塵埃は、電気的に中和できないため、第2の絶縁層3
3.37の表面に正に帯電していくという現象が生じる
。この第2の絶縁層33.37の表面に正に帯電した電
荷は、正の高電圧が印加されている第1の導電層30.
34と、第2の絶縁層33.37との間の空間層の電界
を緩和する方向に作用し、クーロン力が、弱まり、経時
的に集塵率が急激に低下していくという問題があった。
When a positive high voltage is applied to the first conductive layer 30.34 and the second conductive layer 32.36 is set to the ground potential, positively charged dust from the front of the dust collection negative electrode passes through the dust collection electrode. When,
Due to the Coulomb force caused by the electric field, the conductive layer 3 on the ground voltage side
2.36 and the surfaces of the second insulating layer 33.37 and are collected. However, the conductive layer 32.3 on the ground voltage side
The positively charged dust adhering to the second insulating layer 33 and 37 is electrically neutralized, but the positively charged dust adhering to the surface of the second insulating layer 33 and 37 cannot be electrically neutralized. Insulating layer 3
A phenomenon occurs in which the surface of 3.37 becomes positively charged. The positively charged surface of the second insulating layer 33.37 is transferred to the first conductive layer 30.37 to which a high positive voltage is applied.
34 and the second insulating layer 33.37, the Coulomb force weakens, and the dust collection rate rapidly decreases over time. Ta.

集塵電極の前方から正に蓄電した塵埃が通過する場合も
同様の問題が発生する。
A similar problem occurs when dust that has been positively charged passes from in front of the dust collecting electrode.

課題を解決するだめの手段 そして上記問題点を解決するだめの本発明の技術的手段
は、少なくとも第1の絶縁層と第1の導電層と第2の絶
縁層と第2の導電層とを順次積層してなり、前記第1の
導電層と前記第2の導電層のいずれか一方の導電層と同
導電層に対向する層との間に、他の層間より大なる空間
層を形成し、導電層の抵抗値を10Ω贋以下の値とした
ものである。
Means for solving the problems and technical means of the present invention for solving the above problems include at least a first insulating layer, a first conductive layer, a second insulating layer, and a second conductive layer. The conductive layer is laminated in sequence, and a space layer larger than that between the other layers is formed between one of the first conductive layer and the second conductive layer and a layer facing the same conductive layer. , the resistance value of the conductive layer is 10Ω or less.

作用 このような構成によって、帯電した塵埃は、導電層の表
面のみに付着し、絶縁層の表面に付着せず、したがって
導電層と絶縁フィルムとの間の空間層の電界は緩和せず
、経時的に集塵率が急激に低下することがなくなるもの
である。又導電層の抵抗値を規制することで高圧引出し
部よりの接触を確実なものとすることができる。
Effect With such a configuration, the charged dust adheres only to the surface of the conductive layer and does not adhere to the surface of the insulating layer, so the electric field in the space layer between the conductive layer and the insulating film does not relax, and over time. This prevents the dust collection rate from dropping suddenly. Further, by regulating the resistance value of the conductive layer, contact from the high voltage lead-out portion can be ensured.

実施例 第1図は本発明による集塵電極の一実施例の断面図であ
る。1は第1の導電層、2は第2の導電層、3は第1の
絶縁層、4は第2の絶縁層である。
Embodiment FIG. 1 is a sectional view of an embodiment of a dust collection electrode according to the present invention. 1 is a first conductive layer, 2 is a second conductive layer, 3 is a first insulating layer, and 4 is a second insulating layer.

第2の導電層2と第2の絶縁層4との空間tSは、他の
層間11,12 より大なる空間層となっている。
The space tS between the second conductive layer 2 and the second insulating layer 4 is larger than the other interlayers 11 and 12.

又、第2の導電層2の巾は、第1導電層1の巾より広く
なっている。第2図は第1図で示す本発明の集塵電極を
2層重ね合わせた断面図である。
Further, the width of the second conductive layer 2 is wider than the width of the first conductive layer 1. FIG. 2 is a sectional view of two stacked layers of the dust collection electrode of the present invention shown in FIG. 1.

第2図において、矢印は空気の流れる方向を示している
。第1の導電層1と第1の絶縁層3との空間層、第1の
絶縁層3と第2の導電層2との空間層、第2の絶縁層4
と第1の導電層11との空間層、第1の導電層11と第
1の絶縁層13との空間層、第1の絶縁層13と第2の
導電層12との空間層、上記のこれらの空間層は第2の
導電層2と第2の絶縁層4との空間層又は第2の導電層
12と第2の絶縁層14との空間層に比べて極めて小さ
いため、矢印の方向に流れてきた塵埃を含んだ大部分の
空気は、第2の導電層2と第2の絶縁層4との空間層と
、第2の導電層12と第2の絶縁層14との空間層を通
過する。
In FIG. 2, arrows indicate the direction of air flow. A space layer between the first conductive layer 1 and the first insulating layer 3, a space layer between the first insulating layer 3 and the second conductive layer 2, and a second insulating layer 4
and the first conductive layer 11, a spatial layer between the first conductive layer 11 and the first insulating layer 13, a spatial layer between the first insulating layer 13 and the second conductive layer 12, the above-mentioned Since these spatial layers are extremely small compared to the spatial layer between the second conductive layer 2 and the second insulating layer 4 or the spatial layer between the second conductive layer 12 and the second insulating layer 14, the direction of the arrow Most of the dust-containing air that has flowed into the space layer between the second conductive layer 2 and the second insulating layer 4 and the space layer between the second conductive layer 12 and the second insulating layer 14 pass through.

今、集塵電極の第1の導電層1.11に正の高電圧を印
加し、第2の導電層2.12をアース電位とすると、集
塵電極の前方から正に帯電した塵埃は、集塵電極を通過
するとき、電界によるクーロン力により、アース電圧側
の第2の導電層2゜12の表面に付着し集塵される。そ
してアース電圧側の第2の導電層2.12に付着した正
に帯電した塵埃は電気的に中和する。
Now, if a high positive voltage is applied to the first conductive layer 1.11 of the dust collection electrode and the second conductive layer 2.12 is set to ground potential, the positively charged dust from the front of the dust collection electrode will When passing through the dust collecting electrode, the dust is collected by adhering to the surface of the second conductive layer 2° 12 on the ground voltage side due to the Coulomb force caused by the electric field. The positively charged dust adhering to the second conductive layer 2.12 on the ground voltage side is electrically neutralized.

上記は集塵電極の前方から正に帯電した塵埃について述
べたが、集塵電極の前方から負に帯電した塵埃が通過し
た場合、第1の導電層1.11にアース電圧、第2の導
電層2.12に正の高電圧を印加することにより、第2
の導電層2.12の表面に塵埃を集塵することができ、
電気的に中和する。以上のように本実施例によれば、第
1の導電層1.11と第2の導電層2.12のいずれか
一方の導電層と同導電層に対向する絶縁層との間に、他
の層間より大なる空間層を形成することにより、同大な
る空間層に大部分の空気を通過させ、帯電した塵埃を、
導電層の表面のみに付着せしめ、絶縁層の表面には付着
させず、しだがって導電層と絶縁層の間の空間層の電界
は緩和することはなく、集塵率の低下が極めて少ない。
The above description is about positively charged dust from the front of the dust collection electrode, but when negatively charged dust passes from the front of the dust collection electrode, the ground voltage is applied to the first conductive layer 1.11, and the second conductive layer 1. By applying a high positive voltage to layer 2.12, the second
Dust can be collected on the surface of the conductive layer 2.12,
Neutralize electrically. As described above, according to this embodiment, there is another conductive layer between one of the first conductive layer 1.11 and the second conductive layer 2.12 and the insulating layer facing the same conductive layer. By forming a larger space layer between the layers, most of the air passes through the same space layer, and charged dust is removed.
It is attached only to the surface of the conductive layer and not to the surface of the insulating layer, so the electric field in the space between the conductive layer and the insulating layer is not relaxed, and the drop in the dust collection rate is extremely small. .

なお、第3図は第2図に示した集塵電極の他の部分にお
ける断面図であり、大なる空間層を形成するために、第
2の絶縁層4.14に部分的なデインプル状の突起部1
6が形成しである。この突起部16は空気の流れ方向に
沿った樋状であってもよく、要は、大なる空間層を形成
し、かつ空気の流れに対してほとんど障害とならないも
のであれば良い。
Note that FIG. 3 is a cross-sectional view of another part of the dust collection electrode shown in FIG. Projection 1
6 is formed. The protrusion 16 may be in the shape of a gutter along the direction of air flow, as long as it forms a large spatial layer and hardly obstructs the flow of air.

第4図は本発明実施例と従来例について、経過時間に対
する集塵率の変化を示したものである。
FIG. 4 shows the change in dust collection rate with respect to elapsed time for the embodiment of the present invention and the conventional example.

この結果からも本発明は長時間が経過しても集塵効率の
低下がほとんど生じないことが確認できた。
From this result, it was confirmed that in the present invention, there was almost no decrease in dust collection efficiency even after a long period of time had passed.

又、第1の導電層1,11、第2の導電層2゜12を高
電圧、又はアース電圧とするため、外部よシ、リン青銅
板等の導電材料を用いて確実な接続とさせることが必要
であり、導電層の抵抗値を考慮しておかなければならな
い。もし、抵抗値が高過ぎた場合は、リン青銅板等と接
触している部分の導電層が高圧印加時の接触部の放電に
よシ、導通不可能となる場合がある。第6図は、導電層
の抵抗値と高電圧印加可能回数との関係を示したもので
ある。図よりもわかる通り、導電層の抵抗値を10ΩZ
mlより高い抵抗値とした場合、急激に高電圧印加可能
回数が少なくなるため、少なくとも導電層の抵抗値を1
0Q/cI/を以下としておく必要がある。
In addition, in order to set the first conductive layers 1, 11 and the second conductive layer 2゜12 at high voltage or earth voltage, secure connection is made using an external shield or a conductive material such as a phosphor bronze plate. is necessary, and the resistance value of the conductive layer must be taken into consideration. If the resistance value is too high, the portion of the conductive layer in contact with the phosphor bronze plate or the like may become incapable of conducting due to discharge at the contact portion when high voltage is applied. FIG. 6 shows the relationship between the resistance value of the conductive layer and the number of times a high voltage can be applied. As you can see from the figure, the resistance value of the conductive layer is 10ΩZ
If the resistance value is higher than ml, the number of times that high voltage can be applied will decrease rapidly, so the resistance value of the conductive layer should be at least 1
It is necessary to keep 0Q/cI/ as below.

発明の効果 本発明は、第1の絶縁層と第1の導電層と第2の絶縁層
と第2の導電層とを順次積層してなり、前記第1の導電
層と前記第2の導電層のいずれか一方の導電層と同導電
層と対向する絶縁層との間に、他の層間より大なる空間
層を形成した集塵電極であり、経過時間とともに集塵率
の低下が極めて少なく、かつ、導電層の抵抗値を10Ω
zmlとしたことにより高圧接触部での信頼性も高いも
のとなりその工業的価値は大なるものである。
Effects of the Invention The present invention has a structure in which a first insulating layer, a first conductive layer, a second insulating layer, and a second conductive layer are sequentially laminated, and the first conductive layer and the second conductive layer are laminated in sequence. This is a dust collecting electrode that has a larger space between the conductive layer on one side and the insulating layer facing the conductive layer than on other layers, so the dust collection rate does not decrease over time. , and the resistance value of the conductive layer is 10Ω
By using zml, the reliability at the high pressure contact part is also high, and its industrial value is great.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例を示す集塵電極の断面図であ
る。第2図は本発明の他の実施例を示す集塵電極の断面
図、第3図は同集塵電極の他の部分における断面図、第
4図は同集塵電極と従来の集塵電極の経過時間と集塵率
の変化を示す特性図、第6図は導電層の抵抗値と高電圧
印加可能回数の関係を示した特性図、第6図は従来の集
塵電極の断面図である。 1.11・・・・・・第1の導電層、2.12・・・・
・・第2の導電層、3.13・・・・・・第1の絶縁層
、4.14・・・・・第2の絶縁層、16・・・・・・
突起部。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名4−
 第2の絶縁層 第4図 一赳ヰ眸間(H)− 第5図 一高を圧印にイ丸回致□
FIG. 1 is a sectional view of a dust collecting electrode showing one embodiment of the present invention. Fig. 2 is a sectional view of a dust collecting electrode showing another embodiment of the present invention, Fig. 3 is a sectional view of another part of the same dust collecting electrode, and Fig. 4 is a sectional view of the same dust collecting electrode and a conventional dust collecting electrode. Figure 6 is a characteristic diagram showing the relationship between the resistance value of the conductive layer and the number of times high voltage can be applied. Figure 6 is a cross-sectional view of a conventional dust collection electrode. be. 1.11...First conductive layer, 2.12...
...Second conductive layer, 3.13...First insulating layer, 4.14...Second insulating layer, 16...
protrusion. Name of agent: Patent attorney Toshio Nakao and 1 other person 4-
2nd insulating layer Figure 4: 1 height (H) - Figure 5: 1 height with a coining circle □

Claims (1)

【特許請求の範囲】[Claims] 少なくとも第1の絶縁層と第1の導電層と第2の絶縁層
と第2の導電層とを順次積層してなり、前記第1の導電
層と前記第2の導電層のいずれか一方の導電層と同導電
層に対向する層との間に、他の層間より大なる空間層を
形成し、導電層の抵抗値を10Ω/cm^2以下の値と
した集塵電極。
At least a first insulating layer, a first conductive layer, a second insulating layer, and a second conductive layer are sequentially laminated, and one of the first conductive layer and the second conductive layer A dust collecting electrode in which a space layer larger than that between other layers is formed between a conductive layer and a layer facing the conductive layer, and the resistance value of the conductive layer is set to a value of 10Ω/cm^2 or less.
JP3316288A 1988-02-16 1988-02-16 Dust collecting electrode Pending JPH01207150A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3316288A JPH01207150A (en) 1988-02-16 1988-02-16 Dust collecting electrode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3316288A JPH01207150A (en) 1988-02-16 1988-02-16 Dust collecting electrode

Publications (1)

Publication Number Publication Date
JPH01207150A true JPH01207150A (en) 1989-08-21

Family

ID=12378860

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3316288A Pending JPH01207150A (en) 1988-02-16 1988-02-16 Dust collecting electrode

Country Status (1)

Country Link
JP (1) JPH01207150A (en)

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