JP2007313460A - Electrostatic atomizer - Google Patents

Electrostatic atomizer Download PDF

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JP2007313460A
JP2007313460A JP2006147376A JP2006147376A JP2007313460A JP 2007313460 A JP2007313460 A JP 2007313460A JP 2006147376 A JP2006147376 A JP 2006147376A JP 2006147376 A JP2006147376 A JP 2006147376A JP 2007313460 A JP2007313460 A JP 2007313460A
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discharge electrode
liquid
high voltage
tip angle
electrode
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JP4120685B2 (en
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Tetsuya Maekawa
哲也 前川
Koichi Hirai
康一 平井
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Panasonic Electric Works Co Ltd
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Matsushita Electric Works Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To efficiently and stably form a nanometer sized electrically charged fine particle mist having a radical. <P>SOLUTION: The electrostatic atomizer is provided with a high voltage applying part 1, a discharge electrode 2 to which high voltage generated in the high voltage applying part is applied, a counter electrode 3 opposed to the discharge electrode 2, a liquid supply means 4 for supplying a liquid W to be atomized to the discharge electrode 2 and a detection means 5 for detecting a retained state of the liquid W on the discharge electrode 2. A tailer cone tip angle control means 6 for controlling the tip angle of a tailer cone T of the liquid W which is retained on the discharge electrode 2 to 70-95° based on the information about the retained state of the liquid W on the discharge electrode 2 by the detection means 5 when the high voltage is applied to the discharge electrode 2 is included. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明は、ナノメータサイズの帯電微粒子ミストを発生するための静電霧化装置に関するものである。   The present invention relates to an electrostatic atomizer for generating nanometer-sized charged fine particle mist.

従来から例えば特許文献1により水を静電霧化させてナノメータサイズの帯電微粒子ミストを発生させる静電霧化装置が知られている、この特許文献1に示された放電電極先端に水を供給する手段として放電電極を冷却して表面に水を結露させるようになっている。   Conventionally, for example, Patent Document 1 discloses an electrostatic atomizer that electrostatically atomizes water to generate nanometer-sized charged fine particle mist. Water is supplied to the tip of the discharge electrode shown in Patent Document 1. As a means for this, the discharge electrode is cooled to condense water on the surface.

上記のような従来例において、静電霧化装置によるナノメータサイズの帯電微粒子ミストの発生のメカニズムは、放電電極と対向電極との間にかけられた電圧により放電電極の先端部に供給された水が帯電し、帯電した水にクーロン力が働き、放電電極の先端に供給保持された水の液面が局所的に先端が尖った錐状に盛り上がり(テーラーコーンとなり)、このテーラーコーンの先端部に電荷が集中して高密度化され、高密度された電荷の反発力による液体の分裂・飛散(レイリー分裂)を繰り返して静電霧化を行い、ラジカルを有するナノメータサイズの帯電微粒子ミスト(マイナスイオンミスト)を生成させるようになっている。   In the conventional example as described above, the mechanism of generation of nanometer-sized charged fine particle mist by the electrostatic atomizer is such that the water supplied to the tip of the discharge electrode by the voltage applied between the discharge electrode and the counter electrode is When charged, the Coulomb force acts on the charged water, and the surface of the water supplied and held at the tip of the discharge electrode swells up into a cone with a pointed tip locally (to become a tailor cone). Charges are concentrated and concentrated, and electrostatic atomization is performed by repeatedly dividing and scattering liquids (Rayleigh splitting) due to the repulsive force of the high-density charge, and nanometer-sized charged fine particle mist (radical ions) with radicals. Mist) is generated.

上記ラジカルを有するナノメータサイズの帯電微粒子ミストは脱臭、除菌等の効果を有しているが、この脱臭、除菌等の発現は、ナノメータサイズの帯電微粒子ミスト中に含まれるラジカルが主な効果要因として作用していると考えられる。   The nanometer-sized charged fine particle mist having radicals described above has effects such as deodorization and sterilization. The main effects of this deodorization and sterilization are the radicals contained in the nanometer-size charged fine particle mist. It is thought that it acts as a factor.

ところが、上記従来の静電霧化装置にあっては、放電電極の先端部への水の供給量が一定しない等の理由によりテーラーコーンの先端の角度が安定せず、このため、効率よく且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成し難いという問題があった。
特開2005−296753号公報
However, in the conventional electrostatic atomizer, the angle of the tip of the tailor cone is not stable because the amount of water supplied to the tip of the discharge electrode is not constant. There is a problem that it is difficult to stably generate nanometer-sized charged fine particle mist having radicals.
JP 2005-296653 A

本発明は上記の従来の問題点に鑑みて発明したものであって、効率よく且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができる静電霧化装置を提供することを課題とするものである。   The present invention has been invented in view of the above-described conventional problems, and provides an electrostatic atomizer capable of generating nanometer-sized charged fine particle mist having radicals efficiently and stably. It is to be an issue.

上記課題を解決するために本発明に係る静電霧化装置は、高電圧印加部1と、高電圧印加部1で発生させた高電圧が印加される放電電極2と、放電電極2に対向する対向電極3と、放電電極2に霧化させるべき液体Wを供給する液体供給手段4と、放電電極2に保持される液体Wの保持状態を検知する検知手段5とを備え、上記検知手段5による放電電極2への液体Wの保持状態の情報に基づいて、放電電極2に高電圧を印加させた際に放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御するためのテーラーコーン先端角度制御手段6を設けて成ることを特徴とするものである。   In order to solve the above-mentioned problems, an electrostatic atomizer according to the present invention has a high voltage application unit 1, a discharge electrode 2 to which a high voltage generated by the high voltage application unit 1 is applied, and the discharge electrode 2. The counter electrode 3 to be discharged, the liquid supply means 4 for supplying the liquid W to be atomized to the discharge electrode 2, and the detection means 5 for detecting the holding state of the liquid W held by the discharge electrode 2. 5, the tip angle of the tailor cone T of the liquid W held by the discharge electrode 2 when a high voltage is applied to the discharge electrode 2 based on the information on the holding state of the liquid W to the discharge electrode 2 by 70. Tailor cone tip angle control means 6 for controlling to 95 ° is provided.

このような構成とすることで、放電電極2に保持される液体Wの保持状態を検知手段5により検知し、該検知手段5により検知した液体Wの保持状態の情報に基づいてテーラーコーン先端角度制御手段6により放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御することができ、効率的且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができる。   With such a configuration, the holding state of the liquid W held by the discharge electrode 2 is detected by the detection unit 5, and the tailor cone tip angle is determined based on the information on the holding state of the liquid W detected by the detection unit 5. The tip angle of the tailor cone T of the liquid W held on the discharge electrode 2 can be controlled to 70 ° to 95 ° by the control means 6, and nanometer-sized charged fine particle mist having radicals can be generated efficiently and stably. can do.

また、放電電極2と対向電極3との距離が一定の構造であって、テーラーコーン先端角度制御手段6が、検知手段5により得られた液体Wの保持状態の情報に基づいて、放電電極2に印加する高電圧を制御するものであることが好ましい。   Further, the distance between the discharge electrode 2 and the counter electrode 3 is a constant structure, and the tailor cone tip angle control means 6 is based on the information on the holding state of the liquid W obtained by the detection means 5. It is preferable to control the high voltage applied to.

このように放電電極2に印加する高電圧を制御することで、簡単に放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御して、効率的且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができる。   By controlling the high voltage applied to the discharge electrode 2 in this way, the tip angle of the tailor cone T of the liquid W held on the discharge electrode 2 can be easily controlled to 70 ° to 95 ° for efficient and stable operation. Thus, nanometer-sized charged fine particle mist having radicals can be generated.

また、放電電極2と対向電極3との距離が一定の構造であって、テーラーコーン先端角度制御手段6が、検知手段5により得られた液体Wの保持状態の情報に基づいて、放電電極2に供給する霧化させるべき液体Wの供給量を制御するものであることが好ましい。   Further, the distance between the discharge electrode 2 and the counter electrode 3 is a constant structure, and the tailor cone tip angle control means 6 is based on the information on the holding state of the liquid W obtained by the detection means 5. It is preferable that the supply amount of the liquid W to be atomized to be supplied is controlled.

このように放電電極2に供給する霧化させるべき液体Wの供給量を制御することで、簡単に放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御して、効率的且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができる。   By controlling the supply amount of the liquid W to be atomized supplied to the discharge electrode 2 in this way, the tip angle of the tailor cone T of the liquid W held on the discharge electrode 2 can be easily controlled to 70 ° to 95 °. Thus, nanometer-sized charged fine particle mist having radicals can be generated efficiently and stably.

また、放電電極2と対向電極3との距離が可変の構造で且つ印加する高電圧が一定であり、テーラーコーン先端角度制御手段6が、検知手段5により得られた液体Wの保持情報に基づいて、放電電極2と対向電極3との距離及び放電電極2に供給する霧化させるべき液体Wの供給量を制御するものであることが好ましい。   Further, the distance between the discharge electrode 2 and the counter electrode 3 is variable and the applied high voltage is constant, and the tailor cone tip angle control means 6 is based on the liquid W holding information obtained by the detection means 5. Thus, it is preferable to control the distance between the discharge electrode 2 and the counter electrode 3 and the supply amount of the liquid W to be atomized supplied to the discharge electrode 2.

このような構成とすることで、放電電極2と対向電極3との距離及び放電電極2に供給する霧化させるべき液体Wの供給量を制御することで、簡単に放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御して、効率的且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができる。   With such a configuration, the distance between the discharge electrode 2 and the counter electrode 3 and the supply amount of the liquid W to be atomized supplied to the discharge electrode 2 are controlled, so that the discharge electrode 2 can easily hold the discharge electrode 2. By controlling the tip angle of the tailor cone T of the liquid W to 70 ° to 95 °, nanometer-sized charged fine particle mist having radicals can be generated efficiently and stably.

本発明は、上記のように、放電電極に保持される液体の保持状態を検知する検知手段を備え、検知手段による放電電極への液体の保持状態の情報に基づいて、放電電極に高電圧を印加させた際に放電電極に保持される液体のテーラーコーンの先端角度を70°〜95°に制御するためのテーラーコーン先端角度制御手段を設けてあるので、効率よく且つ安定してラジカルを有するナノメータサイズの帯電微粒子ミストを生成することができ、ナノメータサイズの帯電微粒子ミストに含まれるラジカルにより効率よく且つ安定して脱臭、除菌、アレルゲン不活性化効果、農薬分解効果、有機物分解(汚れ除去)等の効果を発現できる。   As described above, the present invention includes a detecting unit that detects the holding state of the liquid held by the discharge electrode, and applies a high voltage to the discharge electrode based on the information on the holding state of the liquid by the detecting unit. The tailor cone tip angle control means for controlling the tip angle of the tailor cone of the liquid held by the discharge electrode when it is applied to 70 ° to 95 ° is provided, so that it has radicals efficiently and stably. Nanometer-sized charged fine particle mist can be generated, and radicals contained in nanometer-sized charged fine particle mist can efficiently and stably deodorize, sterilize, allergen inactivate effect, agrochemical decomposition effect, organic matter decomposition (soil removal) ) And the like can be exhibited.

以下、本発明を添付図面に示す実施形態に基いて説明する。   Hereinafter, the present invention will be described based on embodiments shown in the accompanying drawings.

図1には本発明の静電霧化装置の概略構成図を示している。本例の静電霧化装置は、高電圧印加部1と、高電圧印加部1で発生させた高電圧が印加される放電電極2と、放電電極2に対向する対向電極3と、放電電極2の先端部に霧化させるべき液体Wを供給する液体供給手段4とを備えて構成してある。   FIG. 1 shows a schematic configuration diagram of the electrostatic atomizer of the present invention. The electrostatic atomizer of this example includes a high voltage application unit 1, a discharge electrode 2 to which a high voltage generated by the high voltage application unit 1 is applied, a counter electrode 3 facing the discharge electrode 2, and a discharge electrode. 2 is provided with a liquid supply means 4 for supplying the liquid W to be atomized to the front end portion.

放電電極2の先端部に霧化させるべき液体Wを供給する液体供給手段4としては、毛細管現象により液溜め部に溜めた液体Wを放電電極2の先端部に供給するようにしたものや、あるいは、空気中の水分を冷却して結露水として生成することで、該結露水を放電電極2の先端部に供給するようにしたもの等が考えらえる。   As the liquid supply means 4 for supplying the liquid W to be atomized to the distal end portion of the discharge electrode 2, the liquid W stored in the liquid reservoir portion by capillary action is supplied to the distal end portion of the discharge electrode 2, Alternatively, it is conceivable that water in the air is cooled and generated as condensed water so that the condensed water is supplied to the tip of the discharge electrode 2.

添付図面に示す実施形態では、冷却手段により放電電極2を冷却して空気中の水分を放電電極2の表面で結露させて結露水を生成する例が示してある。以下の説明において液体Wを水W又は結露水Wとして説明する。   In the embodiment shown in the accompanying drawings, an example is shown in which the discharge electrode 2 is cooled by a cooling means and moisture in the air is condensed on the surface of the discharge electrode 2 to generate condensed water. In the following description, the liquid W is described as water W or condensed water W.

液体供給手段4となる冷却手段は冷却部7と放熱部8とを有するペルチェユニット9により構成してあり、ペルチェユニット9の冷却部7側に放電電極2を接続して放電電極2自体を冷却自在としている。添付図面に示す実施形態では、ペルチェユニット9に連結させてある筐体10の先端に対向電極3を支持させることで、放電電極2と対向電極3とを所定の間隔を隔てて互いに対向する位置に固定してある。   The cooling means to be the liquid supply means 4 is constituted by a Peltier unit 9 having a cooling part 7 and a heat radiating part 8, and the discharge electrode 2 is connected to the cooling part 7 side of the Peltier unit 9 to cool the discharge electrode 2 itself. It is free. In the embodiment shown in the accompanying drawings, the counter electrode 3 is supported at the tip of the casing 10 connected to the Peltier unit 9 so that the discharge electrode 2 and the counter electrode 3 are opposed to each other at a predetermined interval. It is fixed to.

ペルチェユニット9は、一対のペルチェ回路板を互いの回路側が向い合うように対向させ、多数列設してあるBiTe系の熱電素子を両ペルチェ回路板間で挟持するとともに隣接する熱電素子同士を両側の回路で電気的に接続させ、冷却側のペルチェ回路板の絶縁板と冷却用絶縁板とで冷却部7を形成し、放熱側のペルチェ回路板の絶縁板と放熱板又は放熱フィンとで放熱部8を形成したものであり、冷却制御部13によるペルチェ入力リード線11を介して為される熱電素子への通電制御により冷却部7側から放熱部8側に熱が移動するようになっている。   The Peltier unit 9 has a pair of Peltier circuit boards facing each other so that the circuit sides face each other, and sandwiches a number of BiTe-based thermoelectric elements between the two Peltier circuit boards, and adjacent thermoelectric elements are arranged on both sides. The cooling part 7 is formed by the insulating plate of the Peltier circuit board on the cooling side and the insulating board for cooling, and the heat is radiated by the insulating plate of the Peltier circuit board on the heat radiating side and the heat radiating plate or the heat radiating fin. Heat is transferred from the cooling unit 7 side to the heat radiating unit 8 side by energization control to the thermoelectric element performed by the cooling control unit 13 via the Peltier input lead wire 11. Yes.

ペルチェユニット9の冷却部7に接続された放電電極2はアルミニウム、銅、タングステン、チタン、ステンレス等の熱伝導性及び導電性の高い材料を用いて略棒状に形成してあって、ペルチェユニット9により冷されて結露水Wを生成するようになっている。   The discharge electrode 2 connected to the cooling unit 7 of the Peltier unit 9 is formed in a substantially rod shape using a material having high thermal conductivity and conductivity such as aluminum, copper, tungsten, titanium, and stainless steel. The condensed water W is generated by being cooled by the above.

放電電極2の後端部には図1に示すように高電圧印加板12が接続してあり、この高電圧印加板12と対向電極3とは高電圧印加部1にそれぞれ高圧リード線を介して接続してあり、高電圧印加部1から放電電極2と対向電極3との間に高電圧が印加されるようになっている。   A high voltage application plate 12 is connected to the rear end of the discharge electrode 2 as shown in FIG. 1, and the high voltage application plate 12 and the counter electrode 3 are connected to the high voltage application unit 1 via high-voltage leads. The high voltage is applied between the discharge electrode 2 and the counter electrode 3 from the high voltage application unit 1.

上記の構成の静電霧化装置は、熱電素子に対して通電を行うと、各熱電素子内において同一方向への熱の移動が生じ、ペルチェユニット9の冷却部7が冷却される。冷却部7が冷却されることで冷却部7に接続した放電電極2が冷却され、放電電極2の周囲の空気が冷却されることで、空気中の水分が結露等により液化されて放電電極2の先端部に結露水Wが生成される。   In the electrostatic atomizer having the above-described configuration, when the thermoelectric elements are energized, heat is transferred in the same direction in each thermoelectric element, and the cooling unit 7 of the Peltier unit 9 is cooled. When the cooling unit 7 is cooled, the discharge electrode 2 connected to the cooling unit 7 is cooled, and the air around the discharge electrode 2 is cooled, so that moisture in the air is liquefied due to condensation or the like, and the discharge electrode 2 Condensed water W is generated at the tip of the water.

このように、ペルチェユニット9の冷却部7に放電電極2を接続して直接放電電極2を冷却して空気中の水分を結露させることで結露水Wを生成させるので、装置のコンパクト化が図れ、また、従来のように水を補給する手間が必要でなく、更に、空気中の水分を結露させるので水道水のように不純物を含むことがなくて付着物除去の手間が不要となる。   As described above, the discharge electrode 2 is connected to the cooling unit 7 of the Peltier unit 9 to directly cool the discharge electrode 2 to condense moisture in the air, thereby generating condensed water W. Therefore, the apparatus can be made compact. In addition, there is no need to replenish water as in the prior art, and furthermore, since moisture in the air is condensed, impurities such as tap water are not included, and the trouble of removing deposits becomes unnecessary.

上記のようにして放電電極2を冷却して放電電極2の先端部に結露水Wが保持された状態で、高電圧印加部1により放電電極2の先端部側がマイナス電極となって電荷が集中するように該放電電極2と対向電極3との間に5kV程度の高電圧を印加すると、放電電極2の先端部に保持される水Wが帯電し、帯電した水にクーロン力が働き、該水Wの液面が局所的に円錐形状(テイラーコーン)に盛り上がり、円錐形状となった水Wの先端に電荷が集中して電荷の密度が高密度となり、高密度の電荷の反発力ではじけるようにして水が分裂・飛散(レーリー分裂)して静電霧化を行い、ラジカルを有するナノメータサイズの帯電微粒子ミスト(マイナスイオンミスト)を発生させる。   In the state where the discharge electrode 2 is cooled and the condensed water W is held at the tip of the discharge electrode 2 as described above, the tip of the discharge electrode 2 becomes a negative electrode by the high voltage application unit 1 and the charge is concentrated. Thus, when a high voltage of about 5 kV is applied between the discharge electrode 2 and the counter electrode 3, the water W held at the tip of the discharge electrode 2 is charged, and the Coulomb force acts on the charged water, The surface of the water W locally rises to a conical shape (Taylor cone), the charge concentrates on the tip of the conical water W, the charge density becomes high, and the repulsive force of the high-density charge repels. In this way, water splits and scatters (Rayleigh splitting) to perform electrostatic atomization to generate nanometer-sized charged fine particle mist (negative ion mist) having radicals.

ここで、本発明においては、制御部20に放電電極2に保持される液体Wの保持状態を検知する検知手段5及びテーラーコーン先端角度制御手段6を有しており、上記検知手段5によって放電電極2への液体Wの保持状態を検知し、この検知手段5による放電電極2への液体Wの保持状態の検知情報に基づいて、制御部20に設けたテーラーコーン先端角度制御手段6により放電電極2に高電圧を印加させた際に放電電極2に保持される液体WのテーラーコーンTの先端角度を70°〜95°に制御するようになっている。   Here, in the present invention, the control unit 20 has the detection means 5 for detecting the holding state of the liquid W held by the discharge electrode 2 and the tailor cone tip angle control means 6. The holding state of the liquid W in the electrode 2 is detected, and discharge is performed by the tailor cone tip angle control means 6 provided in the control unit 20 based on the detection information of the holding state of the liquid W in the discharge electrode 2 by the detecting means 5. The tip angle of the tailor cone T of the liquid W held by the discharge electrode 2 when a high voltage is applied to the electrode 2 is controlled to 70 ° to 95 °.

放電電極2に保持される液体Wの保持状態を検知する検知手段5としては、放電電極2と対向電極3間に流れる微小な電流を検出する手段(電流計21)や、あるいは放電電極2の先端に対向するように筐体10に設けた開口部23を介してビデオカメラ22を配置して画像により情報を得る手段を挙げることができるが、特に上記例にのみ限定するものではない。また、放電電極2を冷却してその表面に水Wを結露させるような場合には、放電電極2の近傍の空気の温湿度を検知する手段(温度センサ15、湿度センサ16)を付加することが望ましい。   As the detecting means 5 for detecting the holding state of the liquid W held by the discharge electrode 2, a means (ammeter 21) for detecting a minute current flowing between the discharge electrode 2 and the counter electrode 3, or the discharge electrode 2 A means for obtaining information by an image by disposing the video camera 22 through the opening 23 provided in the housing 10 so as to face the front end can be given, but it is not limited to the above example. Further, when the discharge electrode 2 is cooled and water W is condensed on the surface thereof, means for detecting the temperature and humidity of the air in the vicinity of the discharge electrode 2 (temperature sensor 15 and humidity sensor 16) should be added. Is desirable.

下記の表1は先端径の異なる2種類の放電電極2における印加電圧に対するラジカル発生量の変化を示しており、先端径の異なる2種類の電極1、電極2にそれぞれ6μA、9μAの電流を流した時に電圧を変化させた場合におけるテーラーコーンTの先端角度の測定結果を示し、また、図2はこの場合における上記先端径の異なる2種類の放電電極2における印加電圧に対するラジカル発生量の変化を示すグラフである。   Table 1 below shows changes in radical generation amount with respect to applied voltage in two types of discharge electrodes 2 having different tip diameters, and currents of 6 μA and 9 μA were applied to the two types of electrodes 1 and 2 having different tip diameters, respectively. FIG. 2 shows the measurement result of the tip angle of the tailor cone T when the voltage is changed when the voltage is changed, and FIG. 2 shows the change in radical generation amount with respect to the applied voltage in the two types of discharge electrodes 2 having different tip diameters in this case. It is a graph to show.

Figure 2007313460
表1及び図2から明らかなように、ラジカル発生量はテーラーコーンTの先端角度が70°〜95°の間で極大点をとる。先端角度70°より小さい場合には、放電電極2の先端の水Wの量が多い状態となり、エネルギーの伝達効率が悪くなってラジカルを含む帯電微粒子ミストの発生量が減少すると推察される。また、先端角度が95°以上の場合には、先端がボール状となる状態が不定期的に見られ、この状態になると電界の集中が悪くなってラジカルを含む帯電微粒子ミストの発生量が減少すると推察される。よってテーラーコーンTの先端角度を70°〜95°となるように制御することでラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となる。
Figure 2007313460
As is apparent from Table 1 and FIG. 2, the radical generation amount takes a maximum point when the tip angle of the tailor cone T is between 70 ° and 95 °. When the tip angle is smaller than 70 °, it is presumed that the amount of water W at the tip of the discharge electrode 2 is large, the energy transmission efficiency is deteriorated, and the generation amount of charged fine particle mist containing radicals is reduced. In addition, when the tip angle is 95 ° or more, a state in which the tip becomes a ball shape is irregularly observed. In this state, the concentration of the electric field is worsened and the generation amount of charged fine particle mist containing radicals is reduced. I guess that. Therefore, by controlling the tip angle of the tailor cone T to be 70 ° to 95 °, it is possible to efficiently and stably generate charged fine particle mist containing radicals.

上記のようにテーラーコーンTの先端角度を70°〜95°に制御するためのテーラーコーン先端角度制御手段6としては、例えば、検知手段5により検知した液体Wの保持状態に基づいて、高電圧印加部1で印加する電圧を制御する手段、あるいは、検知手段5により検知した液体Wの保持状態に基づいて、放電電極2の先端部への霧化させるべき液体Wの供給量を制御する手段、あるいは、検知手段5により検知した液体Wの保持状態に基づいて、放電電極2と対向電極3との距離の制御及び放電電極2の先端部への霧化させるべき液体Wの供給量を制御する手段等が挙げられる。   The tailor cone tip angle control means 6 for controlling the tip angle of the tailor cone T to 70 ° to 95 ° as described above is based on, for example, a high voltage based on the holding state of the liquid W detected by the detection means 5. Means for controlling the voltage applied by the application unit 1 or means for controlling the supply amount of the liquid W to be atomized to the tip of the discharge electrode 2 based on the holding state of the liquid W detected by the detection unit 5 Alternatively, based on the holding state of the liquid W detected by the detecting means 5, the distance between the discharge electrode 2 and the counter electrode 3 is controlled and the supply amount of the liquid W to be atomized to the tip of the discharge electrode 2 is controlled. The means to do is mentioned.

図1には本発明の一実施形態が示してあり、放電電極2と、放電電極2と対向する対向電極3との距離が一定の場合において、検知手段5(添付図面においてはビデオカメラ22で画像により情報を得ている例が示してある)により検知された放電電極2の先端部における水Wの保持状態の情報に基づいて、高電圧印加部1による放電電極2への印加高電圧を制御するものであり、図1(b)に示すように、検知手段5によりテーラーコーンTの先端角度が70°未満の場合は、テーラーコーン先端角度制御手段6により印加電圧をアップさせることで、テーラーコーンTの先端角度を70°〜95°となるように制御し、また、テーラーコーンTの先端角度が95°を越える場合は、テーラーコーン先端角度制御手段6により印加電圧をダウンさせることで、テーラーコーンTの先端角度を70°〜95°となるように制御する。これにより、印加電圧の制御により簡単にラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となる。   FIG. 1 shows an embodiment of the present invention. When the distance between the discharge electrode 2 and the counter electrode 3 facing the discharge electrode 2 is constant, the detection means 5 (in the attached drawings, the video camera 22 The high voltage applied to the discharge electrode 2 by the high voltage application unit 1 is determined based on the information on the holding state of the water W at the tip of the discharge electrode 2 detected by the image). As shown in FIG. 1 (b), when the tip angle of the tailor cone T is less than 70 ° by the detection means 5, the applied voltage is increased by the tailor cone tip angle control means 6, The tip angle of the tailor cone T is controlled to be 70 ° to 95 °. When the tip angle of the tailor cone T exceeds 95 °, the applied voltage is reduced by the tailor cone tip angle control means 6. Be to, control the tip angle of the Taylor cone T to be a 70 ° to 95 °. This makes it possible to easily and stably generate charged fine particle mist containing radicals by controlling the applied voltage.

次に、図3には本発明の他の実施形態が示してあり、放電電極2と、放電電極2と対向する対向電極3との距離が一定の場合において、検知手段5(添付図面においてはビデオカメラ22で画像により情報を得ている例が示してある)により検知された放電電極2の先端部における水Wの保持状態の情報に基づいて、放電電極2の先端部への水Wの供給量を制御するものであり、図3においては冷却制御部13によるペルチェユニット9の熱電素子への通電量を制御することで、ペルチェユニット9の冷却性能を調整し、これにより放電電極2の表面における結露量、つまり、放電電極2の先端部への水Wの供給量を調整するようになっている。すなわち、本実施形態においては、図3(b)に示すように、検知手段5によりテーラーコーンTの先端角度が70°未満の場合は、テーラーコーン先端角度制御手段6により冷却制御部13によるペルチェユニット9の熱電素子への通電量をダウンさせて冷却性能をダウンさせることでテーラーコーンTの先端角度を70°〜95°となるように制御し、また、テーラーコーンTの先端角度が95°を越える場合は、テーラーコーン先端角度制御手段6により冷却制御部13によるペルチェユニット9の熱電素子への通電量をアップさせて冷却性能を向上させることでテーラーコーンTの先端角度を70°〜95°となるように制御するものである。これにより、放電電極2の先端部への水Wの供給量の調整により簡単にラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となる。   Next, FIG. 3 shows another embodiment of the present invention. When the distance between the discharge electrode 2 and the counter electrode 3 facing the discharge electrode 2 is constant, the detection means 5 (in the attached drawings, Based on the information on the holding state of the water W at the front end of the discharge electrode 2 detected by the video camera 22 using an image), the water W to the front end of the discharge electrode 2 is detected. In FIG. 3, the cooling performance of the Peltier unit 9 is adjusted by controlling the amount of current supplied to the thermoelectric elements of the Peltier unit 9 by the cooling control unit 13 in FIG. The amount of condensation on the surface, that is, the amount of water W supplied to the tip of the discharge electrode 2 is adjusted. That is, in this embodiment, as shown in FIG. 3B, when the tip angle of the tailor cone T is less than 70 ° by the detection means 5, the tail cone cone angle control means 6 causes the Peltier to be controlled by the cooling control unit 13. The tip angle of the tailor cone T is controlled to be 70 ° to 95 ° by lowering the amount of current supplied to the thermoelectric element of the unit 9 to lower the cooling performance, and the tip angle of the tailor cone T is 95 °. Is exceeded, the tail angle of the tailor cone T is increased from 70 ° to 95 by increasing the amount of current supplied to the thermoelectric elements of the Peltier unit 9 by the cooling control unit 13 by the tailor cone tip angle control means 6. It is controlled so that it becomes °. This makes it possible to easily and stably generate charged fine particle mist containing radicals by adjusting the amount of water W supplied to the tip of the discharge electrode 2.

また、上記各実施形態において、オゾン量に制限がある空間で使用する場合、図4のようにオゾン量を検知するオゾン量検知手段14を付加し、印加する高電圧及び水の供給量を制御するようにしてもよく、この場合はオゾン量が制限された範囲の中で、ラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となる。すなわち、図4(b)に示すように、検知手段5によりテーラーコーンTの先端角度が70°未満の場合で且つオゾン量検知手段14で検知したオゾン量が大の場合、冷却性能をダウンさせ、テーラーコーンTの先端角度が70°未満の場合でオゾン量検知手段14で検知したオゾン量が小の場合、印加電圧をアップさせることで、テーラーコーンTの先端角度を70°〜95°となるように制御する。また、テーラーコーンTの先端角度が95°を越える場合で且つオゾン量が大の場合、印加電圧をダウンさせ、テーラーコーンTの先端角度が95°を越える場合でオゾン量が小の場合、冷却性能をアップさせることで、テーラーコーンTの先端角度を70°〜95°となるように制御する。これにより、印加電圧の制御により簡単にラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となり、また、オゾン量も最適化できる。   In each of the above embodiments, when used in a space where the amount of ozone is limited, an ozone amount detecting means 14 for detecting the ozone amount is added as shown in FIG. 4 to control the applied high voltage and water supply amount. In this case, charged fine particle mist containing radicals can be generated efficiently and stably within a range in which the amount of ozone is limited. That is, as shown in FIG. 4B, when the tip angle of the tailor cone T is less than 70 ° by the detecting means 5 and the ozone amount detected by the ozone amount detecting means 14 is large, the cooling performance is lowered. When the tip angle of the tailor cone T is less than 70 ° and the amount of ozone detected by the ozone amount detector 14 is small, the tip angle of the tailor cone T is set to 70 ° to 95 ° by increasing the applied voltage. Control to be. When the tip angle of the tailor cone T exceeds 95 ° and the amount of ozone is large, the applied voltage is reduced, and when the tip angle of the tailor cone T exceeds 95 ° and the amount of ozone is small, cooling is performed. The tip angle of the tailor cone T is controlled to be 70 ° to 95 ° by improving the performance. This makes it possible to easily and stably generate charged fine particle mist containing radicals by controlling the applied voltage, and to optimize the amount of ozone.

また、図5には本発明の更に他の実施形態が示してあり、オゾン量に制限がある空間で使用する場合、図5のようにオゾン量を検知するオゾン量検知手段14を付加し、印加する放電電極2と対向電極3との距離の可変制御及び水の供給量を制御するようになっている。本実施形態においては、放電電極2と対向電極3との距離が可変となった構造となっており、印加する電圧が一定である場合に、検知手段5(添付図面においてはビデオカメラ22で画像により情報を得ている例が示してある)により検知された放電電極2の先端部における水の保持状態の情報に基づいて、放電電極2と対向電極3との距離及び放電電極2の先端部への水Wの供給量を制御するものである。すなわち、本実施形態においては、筐体10の先端部の対向電極3を支持する対向電極支持部10aが筐体10に対して移動自在となっており、対向電極支持部10aは駆動部18の駆動により移動して放電電極2との間の距離を可変するようになっている。本実施形態において、図5(b)に示すように、検知手段5によりテーラーコーンTの先端角度が70°未満の場合で且つオゾン量検知手段14で検知したオゾン量が大の場合、冷却性能をダウンさせ、テーラーコーンTの先端角度が70°未満の場合でオゾン量検知手段14で検知したオゾン量が小の場合、放電電極2と対向電極3との距離が短くなるように制御することで、テーラーコーンTの先端角度を70°〜95°となるように制御する。また、テーラーコーンTの先端角度が95°を越える場合で且つオゾン量が大の場合、放電電極2と対向電極3との距離が長くなるように制御し、テーラーコーンTの先端角度が95°を越える場合でオゾン量が小の場合、冷却能力をアップさせることで、テーラーコーンTの先端角度を70°〜95°となるように制御する。これにより、印加電圧の制御により簡単にラジカルを含む帯電微粒子ミストを効率よく且つ安定して発生させることが可能となり、また、オゾン量も最適化できる。   FIG. 5 shows still another embodiment of the present invention. When used in a space where the ozone amount is limited, an ozone amount detecting means 14 for detecting the ozone amount is added as shown in FIG. Variable control of the distance between the discharge electrode 2 to be applied and the counter electrode 3 and the supply amount of water are controlled. In this embodiment, the distance between the discharge electrode 2 and the counter electrode 3 is variable, and when the applied voltage is constant, the detection means 5 (in the accompanying drawings, the video camera 22 displays an image). The distance between the discharge electrode 2 and the counter electrode 3 and the tip of the discharge electrode 2 are detected based on the information on the water holding state at the tip of the discharge electrode 2 detected by The amount of water W supplied to the water is controlled. That is, in the present embodiment, the counter electrode support portion 10 a that supports the counter electrode 3 at the tip of the housing 10 is movable with respect to the housing 10, and the counter electrode support portion 10 a The distance between the electrode 2 and the discharge electrode 2 is changed by driving. In this embodiment, as shown in FIG. 5B, when the tip angle of the tailor cone T is less than 70 ° by the detection means 5 and the ozone amount detected by the ozone amount detection means 14 is large, the cooling performance When the tip angle of the tailor cone T is less than 70 ° and the ozone amount detected by the ozone amount detecting means 14 is small, the distance between the discharge electrode 2 and the counter electrode 3 is controlled to be short. Thus, the tip angle of the tailor cone T is controlled to be 70 ° to 95 °. When the tip angle of the tailor cone T exceeds 95 ° and the amount of ozone is large, the distance between the discharge electrode 2 and the counter electrode 3 is controlled so that the tip angle of the tailor cone T is 95 °. If the ozone amount is small, the tip angle of the tailor cone T is controlled to be 70 ° to 95 ° by increasing the cooling capacity. This makes it possible to easily and stably generate charged fine particle mist containing radicals by controlling the applied voltage, and to optimize the amount of ozone.

本実施形態においては、高価で回路も含めた設置スペースが必要な高電圧可変装置を使用せずに装置全体を小型化することができ、また放電電極2と対向電極3との間に流れる電流値を一定に保った状態での制御が可能となり、オゾン量に制限のある空間での使用において有効である。   In the present embodiment, the entire device can be reduced in size without using a high voltage variable device that is expensive and requires an installation space including a circuit, and the current flowing between the discharge electrode 2 and the counter electrode 3 can be reduced. Control in a state where the value is kept constant is possible, and it is effective in use in a space where the amount of ozone is limited.

本発明の一実施形態を示し、(a)は概略全体構成図であり、(b)はテーラーコーンの先端角度が70°未満の場合と、95°を越える場合に70°〜95°となるように制御する例を示す概略説明図である。1 shows an embodiment of the present invention, (a) is a schematic overall configuration diagram, (b) is 70 ° to 95 ° when the tip angle of the tailor cone is less than 70 ° and exceeds 95 °. It is a schematic explanatory drawing which shows the example controlled in this way. 先端径の異なる2種類の放電電極における印加電圧に対するラジカル発生量の変化を示すグラフである。It is a graph which shows the change of the radical generation amount with respect to the applied voltage in two types of discharge electrodes from which a tip diameter differs. 本発明の他の実施形態を示し、(a)は概略全体構成図であり、(b)はテーラーコーンの先端角度が70°未満の場合と、95°を越える場合に70°〜95°となるように制御する例を示す概略説明図である。Fig. 4 shows another embodiment of the present invention, in which (a) is a schematic overall configuration diagram, and (b) is 70 ° to 95 ° when the tip angle of the tailor cone is less than 70 ° and more than 95 °. It is a schematic explanatory drawing which shows the example controlled to become. 本発明の更に他の実施形態を示し、(a)は概略全体構成図であり、(b)はテーラーコーンの先端角度が70°未満の場合と、95°を越える場合に70°〜95°となるように制御する例を示す概略説明図である。FIG. 5 shows still another embodiment of the present invention, wherein (a) is a schematic overall configuration diagram, and (b) is 70 ° to 95 ° when the tip angle of the tailor cone is less than 70 ° and more than 95 °. It is a schematic explanatory drawing which shows the example controlled to become. 本発明の更に他の実施形態を示し、(a)は概略全体構成図であり、(b)はテーラーコーンの先端角度が70°未満の場合と、95°を越える場合に70°〜95°となるように制御する例を示す概略説明図である。FIG. 5 shows still another embodiment of the present invention, wherein (a) is a schematic overall configuration diagram, and (b) is 70 ° to 95 ° when the tip angle of the tailor cone is less than 70 ° and more than 95 °. It is a schematic explanatory drawing which shows the example controlled to become.

符号の説明Explanation of symbols

1 高電圧印加部
2 放電電極
3 対向電極
4 液体供給手段
5 検知手段
6 テーラーコーン先端角度制御手段
W 液体
DESCRIPTION OF SYMBOLS 1 High voltage application part 2 Discharge electrode 3 Counter electrode 4 Liquid supply means 5 Detection means 6 Taylor cone tip angle control means W Liquid

Claims (4)

高電圧印加部と、高電圧印加部で発生させた高電圧が印加される放電電極と、放電電極に対向する対向電極と、放電電極に霧化させるべき液体を供給する液体供給手段と、放電電極に保持される液体の保持状態を検知する検知手段とを備え、上記検知手段による放電電極への液体の保持状態の情報に基づいて、放電電極に高電圧を印加させた際に放電電極に保持される液体のテーラーコーンの先端角度を70°〜95°に制御するためのテーラーコーン先端角度制御手段を設けて成ることを特徴とする静電霧化装置。   A high voltage application unit, a discharge electrode to which a high voltage generated by the high voltage application unit is applied, a counter electrode facing the discharge electrode, a liquid supply means for supplying a liquid to be atomized to the discharge electrode, and a discharge Detecting means for detecting the holding state of the liquid held by the electrode, and when the high voltage is applied to the discharge electrode based on the information on the holding state of the liquid to the discharge electrode by the detecting means, An electrostatic atomizer comprising: tailor cone tip angle control means for controlling the tip angle of a held tailor cone of liquid to 70 ° to 95 °. 放電電極と対向電極との距離が一定の構造であって、テーラーコーン先端角度制御手段
が、検知手段により得られた液体の保持状態の情報に基づいて、放電電極に印加する高電圧を制御するものであることを特徴とする請求項1記載の静電霧化装置。
The distance between the discharge electrode and the counter electrode is a constant structure, and the tailor cone tip angle control means controls the high voltage applied to the discharge electrode based on the liquid holding state information obtained by the detection means. The electrostatic atomizer according to claim 1, wherein the apparatus is an electrostatic atomizer.
放電電極と対向電極との距離が一定の構造であって、テーラーコーン先端角度制御手段が、検知手段により得られた液体の保持状態の情報に基づいて、放電電極に供給する霧化させるべき液体の供給量を制御するものであることを特徴とする請求項1記載の静電霧化装置。   The liquid to be atomized supplied to the discharge electrode on the basis of the liquid holding state information obtained by the detection means by the tailor cone tip angle control means with a constant distance between the discharge electrode and the counter electrode The electrostatic atomizer according to claim 1, wherein the supply amount is controlled. 放電電極と対向電極との距離が可変の構造で且つ印加する高電圧が一定であり、テーラーコーン先端角度制御手段が、検知手段により得られた液体の保持情報に基づいて、放電電極と対向電極との距離及び放電電極に供給する霧化させるべき液体の供給量を制御するものであることを特徴とする請求項1記載の静電霧化装置。   The distance between the discharge electrode and the counter electrode is variable, the applied high voltage is constant, and the tailor cone tip angle control means is based on the liquid holding information obtained by the detection means, and the discharge electrode and the counter electrode The electrostatic atomizer according to claim 1, which controls the distance to the discharge electrode and the supply amount of the liquid to be atomized supplied to the discharge electrode.
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JP2009172557A (en) * 2008-01-28 2009-08-06 Panasonic Electric Works Co Ltd Electrostatic atomizer
JP2010230250A (en) * 2009-03-27 2010-10-14 Toshiba Corp Refrigerator
JP2010279861A (en) * 2009-06-02 2010-12-16 Daikin Ind Ltd Electrostatic sprayer
JP2011031184A (en) * 2009-08-03 2011-02-17 Mitsubishi Electric Corp Electrostatic atomizer
JP2012075579A (en) * 2010-09-30 2012-04-19 Sanyo Electric Co Ltd Sterilization device
EP2472545A1 (en) * 2009-08-26 2012-07-04 Panasonic Corporation Discharge device and electrostatic atomization device comprising same
WO2014141604A1 (en) 2013-03-11 2014-09-18 パナソニック株式会社 Active ingredient generating device
JP7301244B1 (en) 2022-06-01 2023-06-30 三菱電機株式会社 Electrostatic mist generator and method for generating electrified mist

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009172557A (en) * 2008-01-28 2009-08-06 Panasonic Electric Works Co Ltd Electrostatic atomizer
JP2010230250A (en) * 2009-03-27 2010-10-14 Toshiba Corp Refrigerator
JP2010279861A (en) * 2009-06-02 2010-12-16 Daikin Ind Ltd Electrostatic sprayer
JP2011031184A (en) * 2009-08-03 2011-02-17 Mitsubishi Electric Corp Electrostatic atomizer
EP2472545A1 (en) * 2009-08-26 2012-07-04 Panasonic Corporation Discharge device and electrostatic atomization device comprising same
EP2472545A4 (en) * 2009-08-26 2013-01-02 Panasonic Corp Discharge device and electrostatic atomization device comprising same
JP2012075579A (en) * 2010-09-30 2012-04-19 Sanyo Electric Co Ltd Sterilization device
WO2014141604A1 (en) 2013-03-11 2014-09-18 パナソニック株式会社 Active ingredient generating device
JP7301244B1 (en) 2022-06-01 2023-06-30 三菱電機株式会社 Electrostatic mist generator and method for generating electrified mist
WO2023233593A1 (en) * 2022-06-01 2023-12-07 三菱電機株式会社 Charged mist generation apparatus and method for generating charged mist

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