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JP4765772B2 - Electrostatic atomizer - Google Patents
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JP4765772B2 - Electrostatic atomizer - Google Patents

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JP4765772B2
JP4765772B2 JP2006147380A JP2006147380A JP4765772B2 JP 4765772 B2 JP4765772 B2 JP 4765772B2 JP 2006147380 A JP2006147380 A JP 2006147380A JP 2006147380 A JP2006147380 A JP 2006147380A JP 4765772 B2 JP4765772 B2 JP 4765772B2
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discharge
cooling
value
cooling capacity
discharge current
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JP2007313462A (en
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昭輔 秋定
健二 小幡
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Panasonic Corp
Panasonic Electric Works Co Ltd
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Matsushita Electric Works Ltd
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Description

本発明は静電霧化装置、殊にナノサイズミストを発生させ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, and more particularly to an electrostatic atomizer for generating nano-size mist.

水が供給される放電電極と対向電極との間に高電圧を印加して放電させることで、放電電極が保持している水にレイリー分裂を生じさせて霧化させることでナノメータサイズの帯電微粒子水(ナノサイズミスト)を生成する静電霧化装置がある。   By applying a high voltage between the discharge electrode to which water is supplied and the counter electrode to cause discharge, nanometer-sized charged fine particles are generated by causing Rayleigh splitting in the water held by the discharge electrode and atomization. There are electrostatic atomizers that produce water (nanosize mist).

上記帯電微粒子水は、ラジカルを含んでいるとともに長寿命であって、空間内への拡散を大量に行うことができ、室内の壁面や衣服やカーテンなどに付着した悪臭成分などに効果的に作用し、無臭化することができるといった特徴を有している。   The above charged fine particle water contains radicals and has a long life, can be diffused in a large amount of space, and effectively acts on malodorous substances adhering to indoor walls, clothes, curtains, etc. However, it has a feature that it can be non-brominated.

しかし、水タンクに入れた水を毛細管現象によって放電電極に供給するものでは、水タンクへの水の補給を使用者に強いることになる。この手間を不要とするために空気を冷却することで水を生成する熱交換部を設けて、熱交換部で生成した水(結露水)を放電電極に送ることが考えられるが、この場合、熱交換部で結露水を生成してこの水を放電電極まで送るのに少なくとも数分程度の時間がかかってしまう。   However, in the case of supplying water in the water tank to the discharge electrode by capillary action, the user is forced to replenish the water tank. In order to make this effort unnecessary, it is conceivable to provide a heat exchange part that generates water by cooling the air, and send water (condensation water) generated in the heat exchange part to the discharge electrode. It takes at least several minutes to generate condensed water in the heat exchange section and send this water to the discharge electrode.

放電電極を冷却することで静電霧化させるための水を放電電極上に結露水として生じさせれば、水を放電電極に送らなくてもすむことになるが、この場合、放電電極の冷却について問題が生じる。放電電極を冷やし過ぎれば結露水が放電電極に付き過ぎることになり、放電電極の冷却が不足すれば結露水が放電電極上に生成されずに霧化が生じなくなるからである。   If water for electrostatic atomization is generated on the discharge electrode as condensed water by cooling the discharge electrode, it is not necessary to send water to the discharge electrode. Problems arise. This is because if the discharge electrode is cooled too much, the condensed water will be excessively attached to the discharge electrode, and if the discharge electrode is insufficiently cooled, the condensed water will not be generated on the discharge electrode and atomization will not occur.

このために本発明者らは、放電電圧が一定であるなら、結露水が多いと放電電流が増加し、結露水が少ないと放電電流が減少することに着目し、放電電流を監視して、放電電流値に応じて冷却手段の冷却度合いを調整することを提案した。この場合、放電電極上に常に適切な結露水が確保されることになる。   For this reason, the inventors have observed that if the discharge voltage is constant, the discharge current increases when there is a large amount of condensed water, and the discharge current decreases when the amount of condensed water is small. It was proposed to adjust the cooling degree of the cooling means according to the discharge current value. In this case, appropriate dew condensation water is always ensured on the discharge electrode.

しかし、環境温度や環境湿度によっては、上記制御では結露水が氷結(凍結)してしまう事態を招くことがあり、より適切な制御を行えるものが求められている。
特許第3260150号公報
However, depending on the environmental temperature and the environmental humidity, the above control may cause the condensed water to freeze (freeze), and there is a demand for a more appropriate control.
Japanese Patent No. 3260150

本発明は上記従来の間題点に鑑みて発明したものであって、水の補給の手間が不要である上にナノサイズミストの発生のための安定した放電状態を維持させ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-mentioned conventional problems, and does not require the trouble of replenishing water and is capable of maintaining a stable discharge state for the generation of nano-size mist. An object of the present invention is to provide an atomizing device.

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、放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、
上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、環境温度に応じて設定された範囲内に冷却能力を規制し、該放電電流値から放電電極上の水の凍結が生じたと判定された時に、冷却手段への電圧印加や電極への高圧印加を所定時間停止させ、再開時に冷却手段の冷却能力の上限値を前回値から一定割合下げて冷却能力の規制値を変更することに特徴を有している。環境温度に応じて冷却能力を規制することで氷結を招くことがないようにしているものである。
In order to solve the above-mentioned problems, an electrostatic atomizer according to the present invention generates a discharge electrode , a counter electrode opposite to the discharge electrode, and cools the discharge electrode to generate water on the discharge electrode portion based on moisture in the air. A cooling means for applying a high voltage between the two electrodes to generate a discharge between the two electrodes to atomize the water, and monitoring the discharge current and the cooling means according to the discharge current value. In an electrostatic atomizer provided with a control means for controlling the cooling capacity by
In the cooling capacity control according to the discharge current value, the control means regulates the cooling capacity within a range set according to the environmental temperature, and determines that freezing of water on the discharge electrode has occurred from the discharge current value. When the voltage is applied, the voltage application to the cooling means and the high voltage application to the electrodes are stopped for a predetermined time, and the upper limit value of the cooling capacity of the cooling means is reduced by a certain percentage from the previous value when restarting to change the regulation value of the cooling capacity. It has characteristics. By restricting the cooling capacity according to the environmental temperature, it is intended to prevent freezing.

放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、霧化の安定動作中の冷却度から冷却能力の規制値を算出し、環境温度に応じて設定された範囲内に冷却能力を規制するものであり、各環境温度における冷却手段の冷却能力の上限値を記憶し、該放電電流値から放電電極上の水の凍結が生じたと判定された時に、前記冷却能力の規制値を該上限値に変更するものであってもよい A discharge electrode, a counter electrode opposed to the discharge electrode, a cooling means for cooling the discharge electrode to generate water based on moisture in the air in the discharge electrode portion, and applying a high voltage between the two electrodes In an electrostatic atomizer comprising: a high-voltage power supply for generating a discharge in between to atomize the water; and a control means for monitoring the discharge current and controlling the cooling capacity of the cooling means in accordance with the discharge current value The control means calculates the regulation value of the cooling capacity from the degree of cooling during the stable operation of the atomization and controls the cooling capacity within the range set according to the environmental temperature in controlling the cooling capacity according to the discharge current value. The upper limit value of the cooling capacity of the cooling means at each environmental temperature is stored, and when it is determined from the discharge current value that water on the discharge electrode is frozen, the control value of the cooling capacity is set. You may change to this upper limit .

また、放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、霧化の安定動作中の冷却度から冷却能力の規制値を算出し、環境温度に応じて設定された範囲内に冷却能力を規制するものであり、各環境温度における冷却手段の冷却能力の平均値に所定値を加えた値を、冷却能力の上限値として記憶し、前記冷却能力の規制値を該上限値に変更してもよいFurther , a high voltage is applied between the discharge electrode, a counter electrode opposite to the discharge electrode, a cooling means for cooling the discharge electrode to generate water based on moisture in the air at the discharge electrode portion, and the two electrodes. Electrostatic atomization provided with a high-voltage power supply for generating a discharge between both electrodes to atomize the water, and a control means for monitoring the discharge current and controlling the cooling capacity of the cooling means according to the discharge current value In the apparatus, the control means calculates the regulation value of the cooling capacity from the degree of cooling during the stable operation of the atomization and controls the cooling capacity according to the discharge current value, and falls within a range set according to the environmental temperature. The cooling capacity is regulated, and a value obtained by adding a predetermined value to the average value of the cooling capacity of the cooling means at each environmental temperature is stored as an upper limit value of the cooling capacity, and the regulation value of the cooling capacity is set to the upper limit value. It may be changed .

本発明によれば、環境温度に応じて冷却能力を規制するために氷結を招くことがないものであり、低温環境においても氷結を生じない霧化連続運転が可能となる。   According to the present invention, freezing is not caused in order to regulate the cooling capacity according to the environmental temperature, and an atomization continuous operation that does not cause freezing even in a low temperature environment is possible.

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と、図1に示すように、この静電霧化装置は、放電電極2とこの放電電極2の一端に所要の距離をおいて対向するとともに内周縁が実質的な電極として機能する対向電極3、これら両電極2,3間に放電用の高電圧を印加する高圧電源部4、上記放電電極2の他端が吸熱側に接続されて放電電極2を露点以下の温度に冷却する冷却手段としてのペルチェモジュール5、ペルチェモジュール用の電源部60を内蔵している電源6、そして制御回路Cで構成されたもので、上記対向電極3は接地されており、放電時には放電電極2側に負もしくは正の高電圧(たとえば−4.6kV)が印加される。図中50はペルチェモジュール5の放熱側に配された放熱フィン、8は環境温度センサである。環境湿度も参照する場合は、環境湿度センサも備えたものとする。   Hereinafter, the present invention will be described based on an embodiment shown in the accompanying drawings. As shown in FIG. 1, the electrostatic atomizer is configured to face a discharge electrode 2 and one end of the discharge electrode 2 at a predetermined distance. In addition, the counter electrode 3 whose inner peripheral edge functions as a substantial electrode, the high voltage power source 4 that applies a high voltage for discharge between the electrodes 2 and 3, and the other end of the discharge electrode 2 are connected to the heat absorption side. The counter electrode 3 comprises a Peltier module 5 as a cooling means for cooling the discharge electrode 2 to a temperature below the dew point, a power source 6 incorporating a power source 60 for the Peltier module, and a control circuit C. Is grounded, and a negative or positive high voltage (for example, −4.6 kV) is applied to the discharge electrode 2 side during discharge. In the figure, 50 is a heat radiating fin disposed on the heat radiating side of the Peltier module 5, and 8 is an environmental temperature sensor. When referring to environmental humidity, it is assumed that an environmental humidity sensor is also provided.

上記高圧電源部4は図2にも示すように高圧発生回路40と放電電圧検出回路41と放電電流検出回路42を備えたもので、検出された放電電圧Vv及び放電電流Viは上記制御回路Cに入力され、制御回路Cはこの放電電圧Vv及び放電電流Viを基にペルチェモジュール5の冷却度調整による結露水生成量の調整を行う。   As shown in FIG. 2, the high-voltage power supply unit 4 includes a high-voltage generation circuit 40, a discharge voltage detection circuit 41, and a discharge current detection circuit 42. The detected discharge voltage Vv and discharge current Vi are detected by the control circuit C. The control circuit C adjusts the amount of condensed water generated by adjusting the cooling degree of the Peltier module 5 based on the discharge voltage Vv and the discharge current Vi.

すなわち、放電電極2を冷却することで空気中の水分を放電電極2上に結露させた状態で放電電圧を放電電極2と対向電極3との間に印加する時、放電電極2上の水は図3に示すように対向電極3側に引っ張られてテーラーコーンと称される形状のものとなるとともに、そのテーラーコーンの先端においてレイリー分裂が生じてナノメータサイズの帯電微粒子水が生成されることで霧化がなされる。   That is, when the discharge voltage is applied between the discharge electrode 2 and the counter electrode 3 in a state where moisture in the air is condensed on the discharge electrode 2 by cooling the discharge electrode 2, the water on the discharge electrode 2 is As shown in FIG. 3, it is pulled toward the counter electrode 3 to have a shape called a tailor cone, and at the tip of the tailor cone, Rayleigh splitting occurs and nanometer-sized charged fine particle water is generated. Atomization is done.

この時、放電電極2上の水量が図3(b)に示す状態から少なくなって図3(a)に示すようにテーラーコーンが小さくなれば放電電流も少なくなり、放電電極2上の水量が多くなって図3(c)に示すようにテーラーコーンが大きくなれば放電電流が増大する。ちなみに、−4.4kVの放電電圧の印加時、図3(a)に示す状態では放電電流が3.0μA、図3(b)に示す状態では放電電流が6.0μA、図3(c)に示す状態では放電電流が9.0μAであった。   At this time, if the amount of water on the discharge electrode 2 decreases from the state shown in FIG. 3 (b) and the tailor cone becomes smaller as shown in FIG. 3 (a), the discharge current also decreases, and the amount of water on the discharge electrode 2 decreases. As the number of tailor cones increases as shown in FIG. 3 (c), the discharge current increases. Incidentally, when a discharge voltage of −4.4 kV is applied, the discharge current is 3.0 μA in the state shown in FIG. 3A, the discharge current is 6.0 μA in the state shown in FIG. 3B, and FIG. In the state shown in FIG. 2, the discharge current was 9.0 μA.

つまり、結露水の量にテーラーコーンの形状が関係しているとともにテーラーコーンの高さから放電電流も変化するわけであり、これ故に放電電流を測定することにより、テーラーコーンの高さ(結露水の量)を知ることができる。ここにおいて、放電電極2上の結露水の量が更に少なくなれば、放電電極2上の水と対向電極3間での放電ではなく、放電電極2と対向電極3との間で放電が生じてオゾンの発生などを招くことになる。逆に放電電極2上の水が更に多くなれば、対向電極3と水との距離が短くなりすぎて、大電流が流れることになって狙いの粒子径のミストが得られなくなる。   In other words, the shape of the tailor cone is related to the amount of condensed water, and the discharge current also changes from the height of the tailor cone. Therefore, by measuring the discharge current, the height of the tailor cone (condensed water) The amount). Here, if the amount of condensed water on the discharge electrode 2 is further reduced, a discharge occurs between the discharge electrode 2 and the counter electrode 3 instead of a discharge between the water on the discharge electrode 2 and the counter electrode 3. Ozone will be generated. Conversely, if the amount of water on the discharge electrode 2 further increases, the distance between the counter electrode 3 and the water becomes too short, and a large current flows, so that a mist having a target particle diameter cannot be obtained.

このためにここではある放電電圧の時の放電電流値から放電電極2上の水の量を推定し、この推定に基づき放電電極2を冷却する冷却手段であるペルチェモジュール5の冷却度調整による結露水生成量の調整を行うものであり、放電電流が少ない時はペルチェモジュール5の印加電圧を上昇させて放電電極2をさらに冷却して結露水を増加させ、放電電流が多い時は冷却度合を緩和させて結露水を減少させる方向へフィードバック制御することで、放電電極2上の結露水の量が常にナノサイズミストの発生に適した量となるようにしているものであり、この結果、放電によるナノサイズミストを発生させる静電霧化が途切れたりすることなく連続的になされるものである。   Therefore, here, the amount of water on the discharge electrode 2 is estimated from the discharge current value at a certain discharge voltage, and condensation is achieved by adjusting the cooling degree of the Peltier module 5 which is a cooling means for cooling the discharge electrode 2 based on this estimation. The amount of water generated is adjusted. When the discharge current is small, the applied voltage of the Peltier module 5 is increased to further cool the discharge electrode 2 to increase the amount of condensed water. When the discharge current is large, the degree of cooling is adjusted. The amount of condensed water on the discharge electrode 2 is always suitable for the generation of nano-size mist by performing feedback control in a direction to reduce the amount of condensed water by reducing it. Electrostatic atomization that generates nano-size mist due to is continuously performed without interruption.

ただし、放電電圧が変われば、適切な結露水量を表すことになる放電電流値も変化することから、表1に示すように放電電圧V(n)に応じた最適な放電電流i(n)の範囲を規定し、検出される放電電流i(n)値が上記範囲の中央値i(n)typ付近を維持するようにペルチェモジュール5の印加電圧のデューティ制御を制御回路Cが行うようにしている。   However, if the discharge voltage changes, the discharge current value that represents an appropriate amount of condensed water also changes. Therefore, as shown in Table 1, the optimum discharge current i (n) corresponding to the discharge voltage V (n) The control circuit C controls the duty of the applied voltage of the Peltier module 5 so that the range is defined and the detected discharge current i (n) value is maintained near the median value i (n) typ of the above range. Yes.

放電電流に基づくフィードバック制御の詳細について説明すると、各回路が安定するまでの時間Δtが経過した時点taで制御回路Cは放電電圧検出回路41と放電電流検出回路42から放電電圧値及び放電電流値を取り込み、一定時間毎の平均値を演算して得られた放電電圧値によって上記表1に基づく放電電流制御の放電電流値上限i(n)max、目標値(中央値)i(n)typ、下限i(n)minを取得し、測定された放電電流i(n)値が目標値i(n)typとなるようにペルチェモジュール5に加える印加電圧をデューティ制御でフィードバック制御するものであり、ここではオーバーシュートを避けるために次のように処理している。   The details of the feedback control based on the discharge current will be described. At time ta when the time Δt until each circuit is stabilized has elapsed, the control circuit C receives the discharge voltage value and the discharge current value from the discharge voltage detection circuit 41 and the discharge current detection circuit 42. The discharge current value upper limit i (n) max and target value (median value) i (n) typ of the discharge current control based on the above-mentioned Table 1 is calculated based on the discharge voltage value obtained by calculating the average value at regular intervals. The lower limit i (n) min is obtained, and the applied voltage applied to the Peltier module 5 is feedback-controlled by duty control so that the measured discharge current i (n) value becomes the target value i (n) typ. Here, in order to avoid overshoot, it is processed as follows.

すなわち図4に示すように、時刻taにおいて取り込みを開始した放電電圧値及び放電電流値の平均値v(1),i(1)がΔt時間後の時刻tbにおいて定まり、更に時刻tbにおいて取り込みを開始した放電電圧値及び放電電流値の平均値v(2),i(2)がΔt時間後の時刻tcにおいて定まる時、時刻tb−tc間の上記Δt時間内の放電電流値の差Δi(2)=i(2)−i(1)を求めるとともに、時刻tbでの放電電圧v(1)と前記表1とから求めた時刻tcでの目標放電電流中央値ityp(1)と、時刻tcでの放電電流値i(2)との差Δid(2)とを求め、時刻tb−tc間でのペルチェモジュール5の印加電圧のデューティをD(2)とする時、このデューティD(2)から増分ΔD(2)を
ΔD(2)=a×Δid(2)−b×Δi(2)
(a,bはパラメータ)
で求めて、D(3)=D(2)+ΔD(2)を次の時刻tc−td間でのペルチェモジュール5の印加電圧のデューティとしており、時間Δt毎に以降順次繰り返することで、つまりは
ΔD(n)=a×Δid(n)−b×Δi(n)
をΔt毎に求めて、それまでのデューティD(n-1)に加算して次のデューティD(n)を決定している。放電電流値i(n)と目標放電電流中央値ityp(n)との差分Δid(n)に加えて、放電電流値の差分Δi(n)を考慮することから、前者のみを考慮した場合に生じやすいオーバーシュートを避けることができる。なお、ここで言うデューティ値D(n)及び増分ΔD(n)は、デューティ0〜100%を256分割して割りふったD1〜D256に対応させている。
That is, as shown in FIG. 4, the average values v (1) and i (1) of the discharge voltage value and the discharge current value started to be captured at time ta are determined at time tb after Δt time, and further captured at time tb. When the average value v (2), i (2) of the started discharge voltage value and discharge current value is determined at time tc after Δt time, the difference Δi ( 2) = i (2) −i (1) is calculated, the discharge voltage v (1) at time tb and the target discharge current median value ityp (1) at time tc determined from Table 1 and time The difference Δid (2) from the discharge current value i (2) at tc is obtained, and when the duty of the applied voltage of the Peltier module 5 between time tb-tc is D (2), this duty D (2 ) Increment ΔD (2) from ΔD (2) = a × Δid (2) −b × Δi (2)
(A and b are parameters)
D (3) = D (2) + ΔD (2) is used as the duty of the applied voltage of the Peltier module 5 between the next times tc-td, and is repeated sequentially after each time Δt. ΔD (n) = a × Δid (n) −b × Δi (n)
Is obtained for each Δt and added to the previous duty D (n−1) to determine the next duty D (n). In addition to the difference Δid (n) between the discharge current value i (n) and the target discharge current median value ityp (n), the difference Δi (n) in the discharge current value is taken into account. Overshoot that tends to occur can be avoided. The duty value D (n) and the increment ΔD (n) referred to here correspond to D 1 to D 256 obtained by dividing the duty 0 to 100% by dividing into 256 .

ここにおいて、図5は横軸が環境温度、縦軸が湿度、対応する升目数字は露点−2℃の露点温度を示す。色付けしている範囲は露点が氷点下以下の範囲である。環境温度10℃、環境湿度40%であれば、−5℃まで冷やせばよいことになり、環境温度から計算すると10℃−(−5℃)=15℃冷やすことができれば、結露を生じさせるという点で十分な能力を持つことになる。   Here, in FIG. 5, the horizontal axis represents the environmental temperature, the vertical axis represents the humidity, and the corresponding square number represents the dew point temperature of dew point −2 ° C. The colored area is the dew point below the freezing point. If the environmental temperature is 10 ° C. and the environmental humidity is 40%, it is only necessary to cool to −5 ° C. If calculated from the environmental temperature, it can be condensed by 10 ° C .− (− 5 ° C.) = 15 ° C. You will have enough ability in terms.

そして静電霧化装置では、結露水が氷結しない範囲で制御することが前提となることから、環境温度が下がれば必要ペルチェ冷却能力は低くてよく、その温度に必要な分だけ冷却することができればよい。しかも、全ての環境下で同じ冷却能力をもたせた場合、低温度環境ではその能力範囲内で駆動しても放電電極2の電極温度が氷点下よりもかなり下がることになり、この場合、安定霧化していたものが、外部からの擾乱があった時にこの擾乱に反応して氷結に至る場合も考えられる。   And in the electrostatic atomizer, it is premised that the dew condensation water is controlled in the range where it does not freeze, so if the environmental temperature falls, the necessary Peltier cooling capacity may be low, and it is possible to cool only the amount necessary for that temperature. I can do it. In addition, when the same cooling capacity is provided in all environments, the electrode temperature of the discharge electrode 2 is considerably lower than the freezing point even when driven within the capacity range in a low temperature environment. In some cases, when there was a disturbance from the outside, it would react to this disturbance and lead to freezing.

このためにここではぺルチェ印加電圧の上限値を環境温度(及び環境湿度)に応じて図5に示す必要冷却能力を得られる値に設定することで、つまりは環境に応じた冷却能力を持たせることで、制御中に氷結に至る虞を低減している。各環境温度によるペルチェ印加電圧上限の目安は環境温度+5℃前後が望ましい。環境温度が10℃であれば、電極冷却印加電圧は10+5=15℃冷却できる電圧設定とするのである。 Therefore, here, the upper limit value of the Peltier applied voltage is set to a value that can obtain the required cooling capacity shown in FIG. 5 according to the environmental temperature (and environmental humidity), that is , the cooling capacity according to the environment is provided. This reduces the risk of icing during control. It is desirable that the upper limit of the Peltier applied voltage for each ambient temperature is around + 5 ° C. If the environmental temperature is 10 ° C., the voltage applied to the electrode cooling is set to a voltage that can cool 10 + 5 = 15 ° C.

また、図6はペルチェ印加電圧の変化を示しており、図中V1は環境に応じて設定されるペルチェ印加電圧の上限値である。図に示すように、ペルチェ印加電圧は放電電流値に応じたフィードバック制御によって、電圧値V1を上限とする範囲内で変動するが、その環境下で結露水ができるペルチェ印加電圧が入力され続けているにもかかわらず、放電電流値が0V付近の場合、氷結が生じたと判定することができる。この場合、その環境ではまだ過冷却であることが推定できることから、上記凍結の判定がなされた時点でペルチェモジュール5への電圧印加や電極への高圧印加を所定時間だけ停止させ、その後、これらを再開する時、ぺルチェ印加電圧の上限値を前回値から一定割合下げることが好ましい。この結果、再度の結露水の氷結を防止することができる。制御回路Cにおいて、内部もしくは外部の記憶装置に各環境温度におけるペルチェ印加電圧の上限値を記憶させておくとともに、上記氷結時の上限値変更情報をもとに記憶させている上限値を更新させていけば、常時非氷結の状態での運転が可能となる。 FIG. 6 shows changes in the Peltier applied voltage. In the figure, V1 is the upper limit value of the Peltier applied voltage set according to the environment. As shown, the Peltier applied voltage feedback control in accordance with the discharge current value will vary within the range of the voltage value V1 and upper limit continues to be inputted Peltier applied voltage can condensed water under the circumstances However, when the discharge current value is near 0 V, it can be determined that icing has occurred. In this case, since it can be presumed that the environment is still supercooled in that environment, the voltage application to the Peltier module 5 and the high voltage application to the electrode are stopped for a predetermined time when the determination of freezing is made, and then these are stopped. When restarting, it is preferable to lower the upper limit value of the Peltier applied voltage by a certain percentage from the previous value. As a result, freezing of the condensed water can be prevented again. In the control circuit C, the upper limit value of the Peltier applied voltage at each environmental temperature is stored in an internal or external storage device, and the stored upper limit value is updated based on the upper limit value change information at the time of freezing. By doing so, it is possible to operate in a non-freezing state at all times.

更に図7はペルチェ印加電圧Vと放電電流Iの両者の変化を示しており、放電電流が安定する期間はぺルチェ印加電圧Vもある値で安定する。この安定ペルチェ印加電圧Vは、環境湿度に影響され、環境湿度が高いほど低く、環境湿度が低いほど大きい値をとる。湿度によって結露水のできやすさが変わるからである。   Further, FIG. 7 shows changes in both the Peltier applied voltage V and the discharge current I, and the Peltier applied voltage V is also stabilized at a certain value during the period when the discharge current is stabilized. The stable Peltier applied voltage V is affected by the environmental humidity, and is lower as the environmental humidity is higher and takes a larger value as the environmental humidity is lower. This is because the ease with which condensed water can be produced varies depending on the humidity.

この点に着目し、ここでは制御回路Cにおいて各温度における安定ペルチェ印加電圧の平均値を計算し、この平均値vaに所定値vbを加えた値をペルチェ印加電圧の上限値とするようにしてもよい。この場合も必要以上に結露水を冷却して氷結させてしまうことがなくなる。この場合も上記上限値を内部または外部の記憶装置に記憶させて、次回はこの上限値を採用することで、氷結の虞を更に低減させることができる。 Focusing on this point, here it calculates the average value of the stable Peltier applied voltage definitive in each temperature in the control circuit C, and a value obtained by adding a predetermined value vb on the average value va as the upper limit value of the Peltier applied voltage May be. Also in this case, the condensed water is not cooled more than necessary and freezes. Also in this case, the above upper limit value is stored in an internal or external storage device, and this upper limit value is adopted next time, thereby further reducing the risk of freezing.

同湿度でも温度により氷結割合が変化する上に、低温時のvbの値よりも高温時のvbの値が大きいことが必要となることから、上限値設定のための上記vbの値も各温度毎に設定するとともに各温度時の平均ペルチェ印加電圧を記憶更新させることが、常時非氷結状態での運転に好ましいのはもちろんである。   Even at the same humidity, the icing rate changes depending on the temperature, and it is necessary that the value of vb at the high temperature is larger than the value of vb at the low temperature. Needless to say, it is preferable to always set and change the average Peltier applied voltage at each temperature for operation in a non-icing state.

本発明の実施の形態の一例の回路図である。It is a circuit diagram of an example of an embodiment of the invention. 同上のブロック回路図である。It is a block circuit diagram same as the above. (a)(b)(c)は放電時に放電電極上の結露水で形成されるテーラーコーンの状態を示す説明図である。(a) (b) (c) is explanatory drawing which shows the state of the tailor cone formed with the dew condensation water on a discharge electrode at the time of discharge. 同上の放電電流フィードバックに関する説明図である。It is explanatory drawing regarding a discharge current feedback same as the above. ペルチェ冷却能力についての説明図である。It is explanatory drawing about Peltier cooling capability. ペルチェ印加電圧のタイムチャートである。It is a time chart of a Peltier applied voltage. ペルチェ印加電圧と放電電流のタイムチャートである。It is a time chart of a Peltier applied voltage and discharge current.

符号の説明Explanation of symbols

C 制御回路
2 放電電極
3 対向電極
4 高圧電源部
5 ペルチェモジュール
C Control Circuit 2 Discharge Electrode 3 Counter Electrode 4 High Voltage Power Supply 5 Peltier Module

Claims (3)

放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、
上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、環境温度に応じて設定された範囲内に冷却能力を規制し、該放電電流値から放電電極上の水の凍結が生じたと判定された時に、冷却手段への電圧印加や電極への高圧印加を所定時間停止させ、再開時に冷却手段の冷却能力の上限値を前回値から一定割合下げて冷却能力の規制値を変更することを特徴とする静電霧化装置。
Discharge electrode and a counter electrode opposed thereto, a cooling means for generating a water based on water in the air to the discharge electrode portion to cool the discharge electrode, both electrodes by applying a high voltage between the both electrodes In an electrostatic atomizer comprising: a high-voltage power supply for generating a discharge in between to atomize the water; and a control means for monitoring the discharge current and controlling the cooling capacity of the cooling means in accordance with the discharge current value ,
In the cooling capacity control according to the discharge current value, the control means regulates the cooling capacity within a range set according to the environmental temperature, and determines that freezing of water on the discharge electrode has occurred from the discharge current value. When it is done, the voltage application to the cooling means and the high voltage application to the electrode are stopped for a predetermined time, and the upper limit value of the cooling capacity of the cooling means is reduced by a certain percentage from the previous value when restarting, and the regulation value of the cooling capacity is changed. Electrostatic atomizing device characterized.
放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、
上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、霧化の安定動作中の冷却度から冷却能力の規制値を算出し、環境温度に応じて設定された範囲内に冷却能力を規制するものであり、
各環境温度における冷却手段の冷却能力の上限値を記憶し、該放電電流値から放電電極上の水の凍結が生じたと判定された時に、前記冷却能力の規制値を該上限値に変更することを特徴とする静電霧化装置。
A discharge electrode, a counter electrode opposed to the discharge electrode, a cooling means for cooling the discharge electrode to generate water based on moisture in the air in the discharge electrode portion, and applying a high voltage between the two electrodes In an electrostatic atomizer comprising: a high-voltage power supply for generating a discharge in between to atomize the water; and a control means for monitoring the discharge current and controlling the cooling capacity of the cooling means in accordance with the discharge current value ,
In the cooling capacity control according to the discharge current value, the control means calculates a regulation value of the cooling capacity from the cooling degree during the stable operation of the atomization, and sets the cooling capacity within a range set according to the environmental temperature. To regulate,
The upper limit value of the cooling capacity of the cooling means at each environmental temperature is stored, and when it is determined from the discharge current value that the water on the discharge electrode is frozen, the regulation value of the cooling capacity is changed to the upper limit value. An electrostatic atomizer characterized by .
放電電極とこれに対向する対向電極と、上記放電電極を冷却して放電電極部分に空気中の水分を基に水を生成させる冷却手段と、上記両電極間に高電圧を印加して両電極間に放電を生じさせて上記水を霧化する高圧電源と、放電電流を監視して放電電流値に応じて上記冷却手段による冷却能力を制御する制御手段とを備えた静電霧化装置において、
上記制御手段は、上記放電電流値に応じた冷却能力制御にあたり、霧化の安定動作中の冷却度から冷却能力の規制値を算出し、環境温度に応じて設定された範囲内に冷却能力を規制するものであり、
各環境温度における冷却手段の冷却能力の平均値に所定値を加えた値を、冷却能力の上限値として記憶し、前記冷却能力の規制値を該上限値に変更することを特徴とする静電霧化装置。
A discharge electrode, a counter electrode opposed to the discharge electrode, a cooling means for cooling the discharge electrode to generate water based on moisture in the air in the discharge electrode portion, and applying a high voltage between the two electrodes In an electrostatic atomizer comprising: a high-voltage power supply for generating a discharge in between to atomize the water; and a control means for monitoring the discharge current and controlling the cooling capacity of the cooling means in accordance with the discharge current value ,
In the cooling capacity control according to the discharge current value, the control means calculates a regulation value of the cooling capacity from the cooling degree during the stable operation of the atomization, and sets the cooling capacity within a range set according to the environmental temperature. To regulate,
A value obtained by adding a predetermined value to the average value of the cooling capacity of the cooling means at each environmental temperature is stored as an upper limit value of the cooling capacity, and the regulation value of the cooling capacity is changed to the upper limit value. Atomization device.
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