JPH0859209A - Electric source for ozonizer - Google Patents

Electric source for ozonizer

Info

Publication number
JPH0859209A
JPH0859209A JP18916794A JP18916794A JPH0859209A JP H0859209 A JPH0859209 A JP H0859209A JP 18916794 A JP18916794 A JP 18916794A JP 18916794 A JP18916794 A JP 18916794A JP H0859209 A JPH0859209 A JP H0859209A
Authority
JP
Japan
Prior art keywords
voltage
current
discharge
pulse
electrode
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
JP18916794A
Other languages
Japanese (ja)
Inventor
Tomofumi Miyashita
朋史 宮下
Hisashi Suwahara
久 諏訪原
Michio Nishino
民智夫 西野
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.)
Meidensha Corp
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Corp
Meidensha Electric Manufacturing 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 Meidensha Corp, Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Corp
Priority to JP18916794A priority Critical patent/JPH0859209A/en
Publication of JPH0859209A publication Critical patent/JPH0859209A/en
Pending legal-status Critical Current

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  • Oxygen, Ozone, And Oxides In General (AREA)

Abstract

PURPOSE: To continuously generate discharge of alternating current without interruption and to increase an amount of ozone generated by superimposing a pulse voltage having fixed electric charge to an AC voltage during inversion of polarity of an AC voltage to be impressed between a high-voltage electrode and an earth electrode and impressing the superimposed voltage. CONSTITUTION: This ozonizer is a silent discharge and impresses an AC voltage or an AC current between a high-voltage electrode and an earth electrode opposingly arranged through a discharging gap and generates ozone in a raw material gas circulated in the discharging gap. The ozonizer is equipped with an electric source for superimposing a pulse voltage or a pulse current having a fixed electric charge on the AC voltage or the AC current and impressing the superimposed voltage during inversion of polarity of the AC voltage or the AC current to be impressed between the high-voltage electrode and the earth electrode of the ozonizer.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、水処理や屎尿処理等に
利用される無声放電式のオゾン発生装置に係り、特に電
極間に印加する電源に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a silent discharge type ozone generator used for water treatment, human waste treatment and the like, and more particularly to a power supply applied between electrodes.

【0002】[0002]

【従来の技術】オゾンは極めて強い酸化力を有し、水の
殺菌、脱臭、脱色等の上下水処理や屎尿処理及び食品関
連における殺菌などの多くの用途に使われている。オゾ
ンの生成法には、紫外線照射法、放射線照射法、プラズ
マ放電法、無声放電法及び水の電気分解法等があるが、
工業的には無声放電法が主体である。
2. Description of the Related Art Ozone has an extremely strong oxidizing power and is used for many purposes such as water and sewage treatment such as water sterilization, deodorization and decolorization, human waste treatment and food related sterilization. The ozone generation method includes an ultraviolet irradiation method, a radiation irradiation method, a plasma discharge method, a silent discharge method, and a water electrolysis method.
The silent discharge method is mainly used industrially.

【0003】図4に無声放電法によるオゾン発生装置の
原理を示す。図4において高電圧電極1と接地電極2
は、両者間に空隙部3が形成されるように誘電体4を介
在させて並設されている。両電極1,2間に例えばAC
電圧を印加して空隙部3で無声放電を発生させ、原料と
なるガス(乾燥空気もしくは酸素)をこの空隙部3に通
すことによりオゾンを発生させている。
FIG. 4 shows the principle of an ozone generator using the silent discharge method. In FIG. 4, the high voltage electrode 1 and the ground electrode 2
Are arranged side by side with a dielectric 4 interposed therebetween so that a void 3 is formed therebetween. AC between both electrodes 1 and 2
A voltage is applied to generate a silent discharge in the void 3, and a raw material gas (dry air or oxygen) is passed through the void 3 to generate ozone.

【0004】オゾンO3の理論収率は、 O2→O+O−118Kcal(吸熱反応) O+O2→O3+25Kcal(発熱反応) より、 3O2→2O3−68Kcal となり、O3を1mol生成するために34Kcal必
要となる。従って理論上の収率は1.2kgO3/KW
hとなる。しかし、消費電力に対するオゾンの生成効率
は理論収率に比べて極めて低く数%に過ぎず、残りの9
0数%の電力は熱となってオゾン生成に寄与していない
というのがオゾン発生装置の現状である。
The theoretical yield of ozone O 3 is O 2 → O + O-118 Kcal (endothermic reaction) O + O 2 → O 3 +25 Kcal (exothermic reaction), resulting in 3O 2 → 2O 3 -68 Kcal, and 1 mol of O 3 is produced. 34 Kcal is required. Therefore, the theoretical yield is 1.2 kgO 3 / KW
h. However, the ozone generation efficiency with respect to the power consumption is extremely low compared to the theoretical yield and is only a few percent, and the remaining 9
The current state of the ozone generator is that 0% or less of electric power does not contribute to ozone generation as heat.

【0005】[0005]

【発明が解決しようとする課題】オゾンの生成量に影響
を及ぼす主な因子としては、電極の形状、電極間ギャッ
プの大きさ、誘電体の形状及び材質、電極の冷却方法、
原料ガスの除湿や冷却方法、印加電圧の波形等が挙げら
れる。
The main factors affecting the amount of ozone produced are the shape of the electrodes, the size of the gap between the electrodes, the shape and material of the dielectric, the cooling method of the electrodes,
Examples of the method include dehumidifying and cooling the source gas, and the waveform of the applied voltage.

【0006】現在のオゾン発生装置は図4で示したよう
に、電極間に空隙が形成されるように誘電体を介在させ
てその空隙部分で放電を起こさせる無声放電を応用する
構造などが主となっている。図4において無声放電が起
こると電極と誘電体間の空隙部3に微小なストリーマ状
放電柱が多数発生し、その放電柱の中を大量の電子が流
れる。その際空隙部分を流れている原料ガス中の酸素分
子O2と電子とが衝突し、衝突電離によって酸素原子O
や励起酸素分子O2*が生成し、酸素分子O2と反応して
オゾンO3が生成される(放電の化学作用)。
As shown in FIG. 4, the current ozone generator mainly has a structure which applies a silent discharge in which a dielectric is interposed so that a gap is formed between electrodes and a discharge is generated in the gap. Has become. In FIG. 4, when silent discharge occurs, a large number of minute streamer-like discharge columns are generated in the void 3 between the electrode and the dielectric, and a large amount of electrons flow in the discharge columns. At that time, oxygen molecules O 2 in the raw material gas flowing in the voids collide with electrons, and due to impact ionization, oxygen atoms O 2 are generated.
And excited oxygen molecules O 2 * are generated and react with the oxygen molecules O 2 to generate ozone O 3 (discharge chemical action).

【0007】ここでオゾン生成の原理を図5とともに詳
細に説明する。図5において、交流電圧を印加して無声
放電を起こさせる場合、誘電体側の電極1が正で接地側
の電極2が負となるAC電圧の正の半波の電圧上昇時
に、発生した微小なストリーマ状放電柱の中を電子が接
地電極2側から高電位となる誘電体4側に移動し、その
電子はある面積で誘電体4の表面に広がって堆積する。
そして次に発生するストリーマ状放電柱はすでに堆積し
ている多数の電子を避けて、まだ電子が堆積していない
誘電体4の表面の別の箇所に到達して同様に多数の電子
を表面に堆積させる。この繰り返しにより電子が堆積す
る箇所が誘電体4の表面に分散して存在するようにな
る。
Here, the principle of ozone generation will be described in detail with reference to FIG. In FIG. 5, when an AC voltage is applied to generate silent discharge, a minute half-wave of an AC voltage in which the dielectric-side electrode 1 is positive and the ground-side electrode 2 is negative is generated, In the streamer-like discharge column, electrons move from the side of the ground electrode 2 to the side of the dielectric 4 having a high potential, and the electrons spread over a surface of the dielectric 4 in a certain area and are deposited.
Then, the streamer-like discharge column generated next avoids a large number of electrons already deposited, reaches another portion of the surface of the dielectric 4 where no electrons are yet deposited, and similarly a large number of electrons are deposited on the surface. Deposit. By repeating this, the places where electrons are deposited are dispersedly present on the surface of the dielectric 4.

【0008】電圧の極性が反転して誘電体4側の電極1
が負で接地側の電極2が正になって無声放電が起こる
と、誘電体表面に堆積していた電子は前記ストリーマ状
放電柱の中を、今度は電位が高くなる接地電極2側へ移
動する。このように電子が電極と誘電体の間を移動する
時に前述のような原料ガス中の酸素分子O2と衝突して
オゾンO3が生成されるわけである。
The polarity of the voltage is reversed and the electrode 1 on the side of the dielectric 4
Is negative and the electrode 2 on the ground side becomes positive and silent discharge occurs, the electrons accumulated on the surface of the dielectric move in the streamer-like discharge column to the side of the ground electrode 2 where the electric potential becomes higher this time. To do. In this way, when the electrons move between the electrode and the dielectric, they collide with oxygen molecules O 2 in the raw material gas as described above to generate ozone O 3 .

【0009】上記のようにオゾン生成は放電電流と深い
関連があるが、オゾン発生装置の電極には、従来例えば
図6に示すような方形波定電流が供給されていた。図6
のように通常の交流を電極に印加すると極性反転時に放
電電流が流れていない時間領域が存在する。放電が連続
している間は、放電空間に紫外光やイオンが存在して一
つの微小放電の後に次の放電が起きやすいが、一旦放電
が停止すると次の放電は連続発生の場合と比較して起き
にくくなる。このように放電が途切れるのはオゾン生成
上好ましくない。
As described above, the ozone generation is closely related to the discharge current. However, the electrodes of the ozone generator have conventionally been supplied with a square wave constant current as shown in FIG. 6, for example. Figure 6
As described above, when a normal alternating current is applied to the electrodes, there is a time region in which no discharge current flows when the polarity is reversed. While the discharge is continuous, ultraviolet light and ions are present in the discharge space, and the next discharge is likely to occur after one minute discharge.However, once the discharge is stopped, the next discharge is compared with the continuous discharge. It becomes difficult to get up. Discontinuing the discharge in this way is not preferable for ozone generation.

【0010】以上のように電極間に単なる交流電流又は
交流電圧を印加してオゾン生成を行う従来の装置は、放
電が途切れてオゾン発生効率が悪いという欠点があっ
た。
As described above, the conventional apparatus for generating ozone by simply applying AC current or AC voltage between the electrodes has a drawback that discharge is interrupted and ozone generation efficiency is poor.

【0011】本発明は上記の点に鑑みてなされたもので
その目的は、交流の放電を途切れることなく連続的に発
生させて投入電力量に対するオゾン発生量を増加させた
オゾン発生装置用電源を提供することにある。
The present invention has been made in view of the above points, and an object thereof is to provide a power supply for an ozone generator in which alternating current discharge is continuously generated without interruption to increase ozone generation amount with respect to input power amount. To provide.

【0012】[0012]

【課題を解決するための手段】本発明は、(1)放電ギ
ャップを介して対向配設された高圧電極および接地電極
間に交流電圧又は交流電流を印加し、前記放電ギャップ
内に流通させた原料ガス中にオゾンを発生させる無声放
電式のオゾン発生装置において、前記高圧電極および接
地電極間に印加する交流電圧又は交流電流の極性反転時
に、所定の電荷量を有したパルス電圧又はパルス電流
を、前記交流電圧又は交流電流に重畳して印加するよう
に構成したことを特徴とし、(2)前記パルス電圧又は
パルス電流は、前記交流電圧又は交流電流に同期してい
ることを特徴とし、(3)前記パルス電圧又はパルス電
流が有している電荷量は、前記放電ギャップの電位差
を、放電開始電圧と放電消滅電圧を加えた分だけ変化さ
せるのに必要な量であることを特徴としている。
According to the present invention, (1) an alternating voltage or an alternating current is applied between a high voltage electrode and a ground electrode, which are arranged to face each other through a discharge gap, and are circulated in the discharge gap. In a silent discharge type ozone generator for generating ozone in a raw material gas, when the polarity of an alternating voltage or an alternating current applied between the high-voltage electrode and the ground electrode is reversed, a pulse voltage or a pulse current having a predetermined charge amount is generated. And (2) the pulse voltage or the pulse current is synchronized with the AC voltage or the AC current, and (2) the pulse voltage or the pulse current is synchronized with the AC voltage or the AC current. 3) The amount of electric charge that the pulse voltage or the pulse current has is an amount required to change the potential difference of the discharge gap by the amount of the discharge start voltage and the discharge extinction voltage. It is characterized in that.

【0013】[0013]

【作用】電極間に供給される電圧又は電流にはパルス電
圧又はパルス電流が重畳されているので、放電ギャップ
間の極性が瞬時に反転し、交流の放電は途切れることな
く連続的に発生する。このため同一電力密度におけるオ
ゾン生成量は従来の装置よりも増加する。
Since the pulse voltage or the pulse current is superimposed on the voltage or current supplied between the electrodes, the polarity between the discharge gaps is instantly reversed, and the AC discharge is continuously generated without interruption. Therefore, the amount of ozone produced at the same power density is higher than that of the conventional device.

【0014】[0014]

【実施例】以下、図面を参照しながら本発明の一実施例
を説明する。本発明では、高圧電極−接地電極間に供給
する電流の極性反転時に同調して、図1に示すように反
転した側の極性に、例えば10μsのパルス電流を重畳
印加するように電源装置を構成した。前記パルス電流の
全電荷量は、放電ギャップ間の電位差を、パルスの印加
前後でちょうどギャップの放電開始電圧と放電消滅電圧
を加えた分だけ変化させるのに必要な量に調整してお
く。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. In the present invention, the power supply device is configured so that, when the polarity of the current supplied between the high voltage electrode and the ground electrode is reversed, a pulse current of, for example, 10 μs is superimposed and applied to the reversed polarity as shown in FIG. did. The total charge amount of the pulse current is adjusted to an amount necessary to change the potential difference between the discharge gaps just before and after applying the pulse by the amount of addition of the discharge start voltage and the discharge extinction voltage of the gap.

【0015】図1の新しい電流波形によりオゾン発生装
置を運転すると、ギャップ間の極性が瞬時に反転し、図
2に示す電流波形のように交流の放電は途切れることな
く連続的に発生する。前記パルスと組み合わせる電源波
形は次の表1のとおりであり、表1の各電源波形を用い
て以下の条件で実験を行った。
When the ozone generator is operated with the new current waveform shown in FIG. 1, the polarity between the gaps is instantly reversed, and the AC discharge is continuously generated without interruption as shown in the current waveform shown in FIG. The power supply waveforms to be combined with the pulse are shown in Table 1 below, and an experiment was carried out under the following conditions using each power supply waveform in Table 1.

【0016】[0016]

【表1】 [Table 1]

【0017】実験条件 ガラス管外形 φ63.4*500(電極部分400) 原料ガス圧力 0.6kgf/cm2G 水温 25℃ 流量 8.5l/min 電源周波数 1KHZ 本発明の表1の実施例の条件下での単位面積当たりの放
電消費電力に対するオゾン発生量の関係を図3に示す。
図3において各実施例番号は表1の実験番号に相当して
おり、図中の従来例番号はパルスと組み合わせない電源
波形を用いて前記条件と同一条件で実験を行った場合の
結果を示している。この図3によれば、従来例に比べて
同一の電力密度でのオゾン生成量が各実施例とも増加し
ているのが判る。尚前記パルス電流はパルス電圧であっ
ても良い。
Experimental conditions Glass tube outer diameter φ63.4 * 500 (electrode portion 400) Raw material gas pressure 0.6 kgf / cm 2 G Water temperature 25 ° C. Flow rate 8.5 l / min Power supply frequency 1 KH Z For the examples of Table 1 of the present invention FIG. 3 shows the relationship between the amount of generated ozone and the discharge power consumption per unit area under the conditions.
In FIG. 3, each example number corresponds to the experiment number in Table 1, and the conventional example number in the figure shows the result when the experiment was performed under the same conditions as above using a power supply waveform not combined with a pulse. ing. According to FIG. 3, it can be seen that the ozone generation amount at the same power density is increased in each of the examples as compared with the conventional example. The pulse current may be a pulse voltage.

【0018】[0018]

【発明の効果】以上のように本発明によれば、無声放電
式のオゾン発生装置において、前記高圧電極および接地
電極間に印加する交流電圧又は交流電流の極性反転時
に、所定の電荷量を有したパルス電圧又はパルス電流
を、前記交流電圧又は交流電流に重畳して印加するよう
に構成したので、交流の放電をとぎらせることなく連続
的に発生させることができ、これによって従来の装置に
比べて同一の放電消費電力でオゾン発生量が増加する。
As described above, according to the present invention, in the silent discharge type ozone generator, a predetermined charge amount is generated when the polarity of the alternating voltage or alternating current applied between the high voltage electrode and the ground electrode is reversed. Since the pulse voltage or pulse current is applied so as to be superimposed on the AC voltage or AC current, the AC discharge can be continuously generated without interruption, and thus the conventional device can be used. In comparison, the amount of ozone generated increases with the same discharge power consumption.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の一実施例による電源の電流波形を示す
波形図。
FIG. 1 is a waveform diagram showing a current waveform of a power supply according to an embodiment of the present invention.

【図2】本発明の電源によってオゾン発生装置を運転し
たときの電流波形を示す波形図。
FIG. 2 is a waveform diagram showing a current waveform when the ozone generator is operated by the power supply of the present invention.

【図3】本発明の各実施例の放電電力に対するオゾン発
生量の関係を表す特性図。
FIG. 3 is a characteristic diagram showing the relationship between the discharge power and the ozone generation amount in each example of the present invention.

【図4】無声放電法によるオゾン発生の概要を表す説明
図。
FIG. 4 is an explanatory diagram showing an outline of ozone generation by a silent discharge method.

【図5】無声放電法によるオゾン生成の原理を示す説明
図。
FIG. 5 is an explanatory diagram showing the principle of ozone generation by the silent discharge method.

【図6】従来のオゾン発生装置用電源により運転したと
きの電流波形を示す波形図。
FIG. 6 is a waveform diagram showing a current waveform when operating with a conventional ozone generator power supply.

【符号の説明】 1…高電圧電極 2…接地電極 3…空隙部 4…誘電体[Explanation of reference numerals] 1 ... High-voltage electrode 2 ... Ground electrode 3 ... Void portion 4 ... Dielectric material

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 放電ギャップを介して対向配設された高
圧電極および接地電極間に交流電圧又は交流電流を印加
し、前記放電ギャップ内に流通させた原料ガス中にオゾ
ンを発生させる無声放電式のオゾン発生装置において、
前記高圧電極および接地電極間に印加する交流電圧又は
交流電流の極性反転時に、所定の電荷量を有したパルス
電圧又はパルス電流を、前記交流電圧又は交流電流に重
畳して印加するように構成したことを特徴とするオゾン
発生装置用電源。
1. A silent discharge type in which an AC voltage or an AC current is applied between a high-voltage electrode and a ground electrode, which are opposed to each other via a discharge gap, to generate ozone in a raw material gas circulated in the discharge gap. In the ozone generator of
When the polarity of the alternating voltage or alternating current applied between the high-voltage electrode and the ground electrode is reversed, a pulse voltage or pulse current having a predetermined charge amount is superimposed and applied to the alternating voltage or alternating current. A power supply for an ozone generator, which is characterized in that
【請求項2】 前記パルス電圧又はパルス電流は、前記
交流電圧又は交流電流に同期していることを特徴とする
請求項1に記載のオゾン発生装置用電源。
2. The power supply for an ozone generator according to claim 1, wherein the pulse voltage or the pulse current is synchronized with the AC voltage or the AC current.
【請求項3】 前記パルス電圧又はパルス電流が有して
いる電荷量は、前記放電ギャップの電位差を、放電開始
電圧と放電消滅電圧を加えた分だけ変化させるのに必要
な量であることを特徴とする請求項1又は2に記載のオ
ゾン発生装置用電源。
3. The amount of electric charge contained in the pulse voltage or the pulse current is an amount necessary to change the potential difference of the discharge gap by an amount corresponding to the addition of the discharge start voltage and the discharge extinction voltage. The ozone generator power source according to claim 1 or 2.
JP18916794A 1994-08-11 1994-08-11 Electric source for ozonizer Pending JPH0859209A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18916794A JPH0859209A (en) 1994-08-11 1994-08-11 Electric source for ozonizer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18916794A JPH0859209A (en) 1994-08-11 1994-08-11 Electric source for ozonizer

Publications (1)

Publication Number Publication Date
JPH0859209A true JPH0859209A (en) 1996-03-05

Family

ID=16236596

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18916794A Pending JPH0859209A (en) 1994-08-11 1994-08-11 Electric source for ozonizer

Country Status (1)

Country Link
JP (1) JPH0859209A (en)

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