JP2007250284A - Plasma electrode - Google Patents

Plasma electrode Download PDF

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JP2007250284A
JP2007250284A JP2006070045A JP2006070045A JP2007250284A JP 2007250284 A JP2007250284 A JP 2007250284A JP 2006070045 A JP2006070045 A JP 2006070045A JP 2006070045 A JP2006070045 A JP 2006070045A JP 2007250284 A JP2007250284 A JP 2007250284A
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plasma electrode
dielectric film
plasma
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metal plate
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Kazuo Shimizu
一男 清水
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Shizuoka University NUC
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Shizuoka University NUC
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a plasma electrode capable of efficiently generating plasma with reduced power consumption, improving a contact circulative property between fluid and the plasma, and facilitating the utilization of plasma for a consumer use or the like. <P>SOLUTION: A dielectric film is formed at least on one surface of the opposing plate faces of metal plates firmly fitted to each other with ruggednesses formed of a height difference within a range of 5 μm or more and 50 μm or less and an arbitrary flat-pattern shape, whereby, microplasma discharge is generated between both the metal plates. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

発明の詳細な説明Detailed Description of the Invention

本発明は、室内空気清浄、オゾン生成、除菌・殺菌、排ガス浄化、水浄化、水中の殺菌のためのプラズマ放電を生起せしめる電極の構成に関する。   The present invention relates to an electrode configuration that causes plasma discharge for indoor air purification, ozone generation, sterilization / sterilization, exhaust gas purification, water purification, and sterilization in water.

技術背景Technical background

産業分野から民生分野まで、さまざま適用分野が期待されるプラズマを生起させるための放電電極は、それぞれの用途に適応したものの研究開発が各方面で進められている。   From the industrial field to the consumer field, research and development of discharge electrodes for generating plasmas that are expected to be applied in various fields are being promoted in various fields.

とりわけ、プラズマにより大気中の酸素からオゾンを生成せしめ、もって空気浄化を図ろうとする利用分野では、民生用需要に適応させるべくさまざまな放電電極が開発されてきている(特許文献1、特許文献2参照)。
特開昭63−190702号公報 特開2005−21319号公報
In particular, in a field of use where ozone is generated from oxygen in the atmosphere by plasma to purify the air, various discharge electrodes have been developed to adapt to consumer demand (Patent Documents 1 and 2). reference).
JP-A-63-190702 JP 2005-21319 A

しかし、従来技術では、空気などの流体をプラズマと接触させ処理するために十分な流通性を確保するがゆえに、放電電極間のギャップが数mm程度となり、そのためにプラズマを生起せしめるための印加電圧を数kV以上とすることが必要となり、消費電力の大きなものとなっている。   However, in the prior art, the flow between the discharge electrodes is about several millimeters because the fluid such as air is in contact with the plasma to ensure sufficient flowability, so that the applied voltage for generating the plasma is therefore Needs to be several kV or more, and power consumption is large.

また電極間のギャップをμmオーダーとし無声放電又は沿面放電を生起せしめ、低電圧で効率的なプラズマ生成を実現する技術(マイクロプラズマ技術)も開発が進められているが、反面そのプラズマ放電範囲が狭小化するために、空気などの流体を流通させるときに非常に大きな圧力差損が生じ、そのための特段の圧入手段等が必要とされている。また、電極がセラミック基材中に埋め込まれている為、長時間運転では熱を持ち、オゾン生成効率が低下する、表面電極に有害ガスなどによる塩基生成により放電持続が出来なくなるなどの問題点があり課題とされてきた。   In addition, a technology (microplasma technology) has been developed to generate a silent discharge or creeping discharge with a gap between the electrodes of the order of μm, thereby realizing efficient plasma generation at a low voltage. In order to reduce the size, a very large pressure differential loss occurs when a fluid such as air is circulated, and a special press-fitting means or the like is required for that purpose. In addition, since the electrode is embedded in the ceramic substrate, there are problems such as heat generated during long-term operation, ozone generation efficiency is reduced, and discharge cannot be sustained due to base generation due to harmful gas on the surface electrode. There has been a problem.

従来技術では、流体とプラズマの接触性とエネルギー消費の低減とを両立させることが困難であり、また、マイクロプラズマ技術ではプラズマ生成の機械的構成も微細部材の複合化が必要となっているため、民生用用途向けなどでのプラズマ応用の大きな制約となっている。   In the conventional technology, it is difficult to achieve both the contact property between the fluid and the plasma and the reduction in energy consumption. In the microplasma technology, the mechanical configuration of plasma generation requires the combination of fine members. This is a major limitation in plasma applications for consumer use.

本願発明者は、前記従来発明の課題に鑑みて、μmオーダーでの電極間のギャップにより消費電力を低減するとともに、流体流通性を向上させることができ、かつ機械的構成も簡使かつ耐久性のあるプラズマ電極を発明するに至った。長時間運転でも影響を及ぼさないような冷却構造を持ち、電極表面が汚染されることによる放電持続低下を抑制したマイクロプラズマ・フィルタによる長時間運転を可能とする室内空気清浄化を提供することを目的とする。
本願請求項1の発明は板面に対して垂直方向に流体を流通させるための1つ以上の流通口が形成された一対の金属板からなるプラズマ電極であって、金属板の対向する板面の少なくとも一方の表面は誘電体膜が形成されて、誘電体膜の表面は、5μm以上50μm以下の範囲の高低差と任意の平面パターン形状とをもった凹凸が形成されて、対向する金属板の板面は、相互に面着固設されて、両金属板間に電圧が印加されてプラズマ放電を生起させることを特徴とするプラズマ電極である。
In view of the problems of the conventional invention, the inventor of the present application can reduce power consumption by a gap between electrodes on the order of μm, improve fluid flowability, and use a mechanical structure with ease and durability. It came to invent the plasma electrode with. Providing indoor air cleaning with a microplasma filter that has a cooling structure that does not affect even long-time operation and suppresses the sustained decrease in discharge due to contamination of the electrode surface. Objective.
The invention of claim 1 of the present application is a plasma electrode composed of a pair of metal plates in which one or more flow ports for allowing fluid to flow in a direction perpendicular to the plate surface are formed, the plate surfaces facing each other. A dielectric film is formed on at least one surface of the metal plate, and the surface of the dielectric film is formed with concavities and convexities having a height difference in the range of 5 μm or more and 50 μm or less and an arbitrary planar pattern shape, and is opposed to a metal plate These plate surfaces are plasma electrodes characterized in that they are surface-attached to each other and a voltage is applied between both metal plates to cause plasma discharge.

本願請求項2の発明は、誘電体膜が形成されたプラズマ電極は、予め金属板表面に形成された誘電体膜の表面に、化学的或いは機械的な除去手段により、5μm以上50μm以下の範囲の高低差と任意の平面パターン形状とをもった凹凸を成形したものであることを特徴とする上記請求項1に記載のプラズマ電極である。   In the invention of claim 2, the plasma electrode on which the dielectric film is formed has a range of 5 μm or more and 50 μm or less on the surface of the dielectric film previously formed on the surface of the metal plate by chemical or mechanical removal means. The plasma electrode according to claim 1, wherein the unevenness having a height difference of 2 and an arbitrary planar pattern shape is formed.

本願請求項3の発明は、誘電体膜が形成されたプラズマ電極は、予め金属板表面に、化学的或いは機械的な除去手段により、55μm以上550μm以下の範囲の高低差と任意の平面パターン形状とをもった凹凸を成形し、そののち金属板表面に誘電体膜を形成したものであることを特徴とする上記請求項1又は請求項2に記載のプラズマ電極である。   According to the invention of claim 3 of the present application, the plasma electrode on which the dielectric film is formed has a height difference in the range of 55 μm or more and 550 μm or less and an arbitrary planar pattern shape on the surface of the metal plate in advance by chemical or mechanical removal means. 3. The plasma electrode according to claim 1 or 2, wherein a concavo-convex shape is formed, and then a dielectric film is formed on the surface of the metal plate.

本願請求項4の発明は、誘電体膜は、チタン酸バリウム及びアルミナを主成分とする材料からなることを特徴とする上記請求項1から3のいずれかに記載のプラズマ電極である。   The invention according to claim 4 is the plasma electrode according to any one of claims 1 to 3, wherein the dielectric film is made of a material mainly composed of barium titanate and alumina.

本願請求項5の発明は、金属板表面に形成される誘電体膜の膜厚は、50μm以上500μm以下であることを特徴とする上記請求項1から4のいずれかに記載のプラズマ電極である。   A fifth aspect of the present invention is the plasma electrode according to any one of the first to fourth aspects, wherein the dielectric film formed on the surface of the metal plate has a thickness of 50 μm or more and 500 μm or less. .

本願請求頂6の発明は、誘電体膜表面には、さらに四フッ化エチレン樹脂又はシリコーン樹脂による樹脂皮膜が形成されていることを特徴とする上記請求項1から5のいずれかに記載のプラズマ電極である。   The invention according to claim 6 of the present application is characterized in that a resin film made of tetrafluoroethylene resin or silicone resin is further formed on the surface of the dielectric film. Electrode.

本願請求項7の発明は、流体を流通させるための流通ロは、誘電体膜が形成されたプラズマ電極表面上での横方向又は縦方向の口径が100μm以上10mm以下、望ましくは200μm以上400μm以下であることを特徴とする上記請求頂1から6のいずれかに記載のプラズマ電極である。   In the invention of claim 7 of the present application, the flow for flowing the fluid is such that the horizontal or vertical diameter on the surface of the plasma electrode on which the dielectric film is formed is 100 μm or more and 10 mm or less, preferably 200 μm or more and 400 μm or less. The plasma electrode according to any one of claims 1 to 6, characterized in that:

本願請求頂8の発明は、誘電体膜が形成されたプラズマ電極面での流通口の開口部面積割合が電極面外周面積の2%以上60%以下、望ましくは20%以上40%以下となるように1つ以上の流通口が形成されていることを特徴とする上記請求項1から7のいずれかに記載のプラズマ電極である。   According to the invention of claim 8 of the present application, the area ratio of the opening of the flow port on the plasma electrode surface on which the dielectric film is formed is 2% to 60%, preferably 20% to 40% of the outer peripheral area of the electrode surface. The plasma electrode according to any one of claims 1 to 7, wherein one or more flow ports are formed as described above.

本願請求項9の発明は、対向する板面の裏面も更に誘電体膜又は樹脂皮膜が形成されていることを特徴とする上記請求項1から8のいずれかに記載のプラズマ電極である。   The invention according to claim 9 is the plasma electrode according to any one of claims 1 to 8, wherein a dielectric film or a resin film is further formed on the back surface of the opposing plate surface.

上述したように、本願発明のプラズマ電極は、消費電力を低減して効率的にプラズマを生起せしめるとともに、流体とプラズマの接触流通性を向上させることができるため、民生用用途などでのプラズマ利用を容易化することができる。また、請求項1から請求項9のプラズマ電極は対を為して配置されるが、複数個のプラズマ電極を流体が流通ロを通過するように配置して全体で一つのプラズマ電極として構成することで、室内空気清浄化の効率向上や、オゾン発生濃度の向上を図ることが出来る。さらにこのような用途では、複数個のプラズマ電極の奇数番目同士と偶数番目同士が各々電気的に接続されて電力が供給される構成により各電極が密接して対向する構成も可能である。   As described above, the plasma electrode of the present invention can generate plasma efficiently by reducing power consumption, and can improve the contact flow between fluid and plasma. Can be facilitated. In addition, the plasma electrodes according to claims 1 to 9 are arranged in pairs, and a plurality of plasma electrodes are arranged so that fluid passes through the flow path to constitute one plasma electrode as a whole. Thus, it is possible to improve the efficiency of cleaning the indoor air and improve the ozone generation concentration. Furthermore, in such an application, it is also possible to adopt a configuration in which the electrodes are closely opposed to each other by a configuration in which odd-numbered and even-numbered plasma electrodes are electrically connected and supplied with power.

以下、本願発明の実施の形態を説明する。
図1は、本願発明のプラズマ電極の断面図及び平面図を模式的に示したものである。開口部の形状は円形、三角形、方形、多角形など任意の形状が可能であり、その他の星型などデザイン性の形状も用いることができる。
Hereinafter, embodiments of the present invention will be described.
FIG. 1 schematically shows a cross-sectional view and a plan view of a plasma electrode of the present invention. The shape of the opening can be any shape such as a circle, a triangle, a rectangle, or a polygon, and other design shapes such as a star shape can also be used.

図1のごとく、一対の金属板の対向してなるプラズマ電極は、少なくとも一方の表面に誘電体膜が形成され、当該誘電体膜の表面には5μm以上50μm以下の高低差と任意の平面パターン形状とをもった凹凸が形成されて、対向する金属板の複面は、相互に面着固設されている。   As shown in FIG. 1, a plasma electrode formed by opposing a pair of metal plates has a dielectric film formed on at least one surface, and the surface of the dielectric film has a height difference of 5 μm or more and 50 μm or less and an arbitrary plane pattern. Concavities and convexities having a shape are formed, and the multiple surfaces of the opposing metal plates are surface-attached to each other.

また、図2のごとく、プラズマ電極には誘電体膜に任意のパターンで凹凸が形成されている。   In addition, as shown in FIG. 2, the plasma electrode has irregularities formed in an arbitrary pattern on the dielectric film.

図3のごとく任意の高低差が低い場合には低電圧でオゾン生成が行われることが認められる。   As shown in FIG. 3, it is recognized that ozone is generated at a low voltage when an arbitrary height difference is low.

図4のごとく誘電体コーティング膜厚は最適値が認められる。本実施例の場合は400μmである。   As shown in FIG. 4, the optimum value of the dielectric coating film thickness is recognized. In the case of this example, it is 400 μm.

図5のごとく沿面放電と比べて、相対湿度が高い場合でも高いオゾン濃度が得られることが認められる。   As shown in FIG. 5, it is recognized that a higher ozone concentration can be obtained even when the relative humidity is higher than the creeping discharge.

図6のごとくホルムアルデヒドを低消費電力で除去することが認められる。
As shown in FIG. 6, it is recognized that formaldehyde is removed with low power consumption.

プラズマ電極を模式的に示した図Diagram showing plasma electrode 誘電体膜により任意の高低差を表面上に作成した写真Photo created on the surface with an arbitrary height difference using a dielectric film 電極間距離を変化させてオゾン生成濃度と放電電圧との関係を示す特性図Characteristic diagram showing the relationship between ozone generation concentration and discharge voltage by changing the distance between electrodes 誘電体膜厚によるオゾン生成濃度と放電電圧との関係を示す図Diagram showing the relationship between ozone generation concentration and discharge voltage depending on dielectric film thickness 相対湿度と生成オゾン濃度との関係を示す図Diagram showing the relationship between relative humidity and generated ozone concentration ホルムアルデヒドの除去特性を示す図Diagram showing the removal characteristics of formaldehyde

Claims (9)

1つ以上の流通口が形成された金属板が相対してして配置されたプラズマ電極であって、金属板の対向する板面の少なくとも一方の表面は誘電体膜が形成され、誘電体膜の表面は5μm以上で50μm以下の高低差と任意の平面パターン形状とをもった凹凸が形成され、対向する金属板の板面は、相互に面着固設されるか、あるいは、5μm以上で100μm以下の間隔を保持すべく固設されて、両金属板間にプラズマ放電を生起させる電力が印加される構造を特徴とするプラズマ電極。 A plasma electrode in which a metal plate having one or more flow ports formed is disposed opposite to each other, and a dielectric film is formed on at least one surface of the opposing plate surfaces of the metal plate. The surface of the metal plate is uneven with an elevation difference of 5 μm or more and 50 μm or less and an arbitrary plane pattern shape, and the plate surfaces of the opposing metal plates are fixed to each other, or are 5 μm or more. A plasma electrode, characterized in that it is fixed to maintain an interval of 100 μm or less, and a power is applied to cause plasma discharge between both metal plates. 誘電体膜が形成されたプラズマ電極は、予め金属板表面に形成された誘電体膜の表面に、化学的或いは機械的な除去手段により、5μm以上50μm以下の範囲の高低差と任意の平面パターン形状とをもった凹凸を成形したものであることを特徴とする上記請求項1に記載のプラズマ電極。   The plasma electrode on which the dielectric film is formed is formed on the surface of the dielectric film previously formed on the surface of the metal plate by a chemical or mechanical removal means, with a height difference in the range of 5 μm to 50 μm and an arbitrary plane pattern. The plasma electrode according to claim 1, wherein the plasma electrode is formed with irregularities having a shape. 誘電体膜が形成されたプラズマ電極は、予め金属板表面に、化学的或いは機械的な除去手段により、55μm以上550μm以下の範囲の高低差と任意の平面パターン形状とをもった凹凸を成形し、該金属板表面に誘電体膜を形成したものであることを特徴とする上記請求項1又は請求項2に記載のプラズマ電極。   The plasma electrode on which the dielectric film is formed is formed in advance on the surface of the metal plate by means of chemical or mechanical removal means, with irregularities having a height difference in the range of 55 μm to 550 μm and an arbitrary plane pattern shape. 3. The plasma electrode according to claim 1, wherein a dielectric film is formed on the surface of the metal plate. 誘電体膜は、チタン酸バリウム及びアルミナを主成分とする材料からなることを特徴とする上記請求項1から3のいずれかに記載のプラズマ電極。   4. The plasma electrode according to claim 1, wherein the dielectric film is made of a material mainly composed of barium titanate and alumina. 金属板表面に形成される誘電体膜の膜厚は、50μm以上500μm以下であることを特徴とする上記請求項1から4のいずれかに記載のプラズマ電極。   5. The plasma electrode according to claim 1, wherein the dielectric film formed on the surface of the metal plate has a thickness of 50 μm or more and 500 μm or less. 誘電体膜表面には、さらに四フッ化エチレン樹脂又はシリコーン樹脂による樹脂皮膜が形成されていることを特徴とする上記請求項1から5のいずれかに記載のプラズマ電極。   6. The plasma electrode according to claim 1, wherein a resin film made of tetrafluoroethylene resin or silicone resin is further formed on the surface of the dielectric film. 流体を流通させるための流通ロは、誘電体膜が形成されたプラズマ電極表面上での横方向又は縦方向の口径が100μm以上10mm以下、望ましくは200μm以上400μm以下であることを特徴とする上記請求頂1から6のいずれかに記載のプラズマ電極。   The flow for flowing the fluid is characterized in that the diameter in the horizontal direction or the vertical direction on the surface of the plasma electrode on which the dielectric film is formed is 100 μm or more and 10 mm or less, preferably 200 μm or more and 400 μm or less. The plasma electrode according to any one of claims 1 to 6. 誘電体膜が形成されたプラズマ電極面での流通口の開口部面積割合が電極面外周面積の2%以上60%以下、望ましくは20%以上40%以下となるように1つ以上の流通口が形成されていることを特徴とする上記請求項1から7のいずれかに記載のプラズマ電極。   One or more flow ports so that the opening area ratio of the flow port on the plasma electrode surface on which the dielectric film is formed is 2% or more and 60% or less, preferably 20% or more and 40% or less of the outer peripheral area of the electrode surface. The plasma electrode according to claim 1, wherein the plasma electrode is formed. 対向する板面の裏面も更に誘電体膜又は樹脂皮膜が形成されていることを特徴とする上記請求項1から8のいずれかに記載のプラズマ電極。   9. The plasma electrode according to claim 1, wherein a dielectric film or a resin film is further formed on the back surface of the opposing plate surface.
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