JPH0316902A - Electric power unit for ozone generating tube - Google Patents
Electric power unit for ozone generating tubeInfo
- Publication number
- JPH0316902A JPH0316902A JP22573989A JP22573989A JPH0316902A JP H0316902 A JPH0316902 A JP H0316902A JP 22573989 A JP22573989 A JP 22573989A JP 22573989 A JP22573989 A JP 22573989A JP H0316902 A JPH0316902 A JP H0316902A
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- Japan
- Prior art keywords
- transformer
- ozone
- reactor
- power supply
- voltage
- 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.)
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- Oxygen, Ozone, And Oxides In General (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明はオゾン発生管用電源装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a power supply device for an ozone generating tube.
従来のこの種の電源装置とオゾン発生管との接続は第8
図(イ)の回路図に例示する如く交流電流源出力電圧を
直接オゾン発生管に印加するもの(2)
が知られている。The connection between the conventional power supply device of this type and the ozone generator tube is as follows.
As illustrated in the circuit diagram of Figure (a), a system (2) in which the output voltage of an alternating current source is directly applied to the ozone generator tube is known.
第8図(イ)において、■は交流電流源、38〜3cは
オゾン発生管の構或要素であり3aと3bとは該オゾン
発生管の対向する電極、3cは該両電極間に挿入された
誘電体である。なお前記の電極3a .!:K電体3c
間に示す交互に方向の反転する矢印は前記電源1による
交流電圧V。を前記両電極3aと3b間に印加した場合
に発生する無声放電状態を示し、ioは該無声放電時を
含めた前記オゾン発生管の通電電流を示し、更に前記無
声放電により図示二重矢印の如く酸素02はオゾン03
に変換される。In FIG. 8(a), ■ is an alternating current source, 38 to 3c are structural elements of the ozone generating tube, 3a and 3b are opposing electrodes of the ozone generating tube, and 3c is an electrode inserted between the two electrodes. It is a dielectric material. Note that the electrode 3a. ! :K electric body 3c
The arrows shown in between are the alternating current voltage V from the power source 1. indicates a silent discharge state that occurs when is applied between the electrodes 3a and 3b, io indicates the current flowing through the ozone generating tube including the silent discharge, and furthermore, due to the silent discharge, the state indicated by the double arrow in the figure is Like Oxygen 02 is Ozone 03
is converted to
第8図(口)は前記の各要素38〜3cより或るオゾン
発生管の電気的等価回路図であり、3dは空隙部の等価
容量、3eは誘電体部の等価容量、3fは前記空隙部の
放電維持電圧(Vd)をその正負両方向通電開始電圧と
なす非線形通電素子を示し前記空隙部の等価模擬素子で
ありその電流電圧特性は第10図に示す如くなる。FIG. 8 (opening) is an electrical equivalent circuit diagram of a certain ozone generating tube made of the above-mentioned elements 38 to 3c, where 3d is the equivalent capacity of the air gap, 3e is the equivalent capacity of the dielectric part, and 3f is the air gap. FIG. 10 shows a non-linear energizing element whose discharge sustaining voltage (Vd) of the gap is set as its positive and negative energization starting voltage.
第9図は前記オゾン発生管の充放電状態を示す(3)
等価回路図であり、第8図(ロ)から導かれたものであ
る。前記オゾン発生管の動作状態を模擬する前記非線形
通電素子3fの等価インピーダンスは、前記オゾン発生
管の放電時には小となり放電停止時には極めて大となる
。従って第8図(ロ)に示す如き前記空隙部等価容量3
dと前記通電素子3fとの並列合成インピーダンスは、
前記放電時には前記通電素子3fの値に略等しくなり、
また前記放電停止時には前記等価容量3dの値に略等し
くなり従って該放電停止時は同時に該等価容量3dの充
電時ともなる。従って前記オゾン発生管の等価回路は、
その放電停止状態すなわち前記等価容量3dの充電状態
においては第9図(イ)の充電状態図に示す如く前記両
等価容量3dと30との直列接続となり、またその放電
状態においては第9図(ロ)の放電状態図に示す如く前
記の等価容量3eと通電素子3fとの直列接続となる。FIG. 9 is an equivalent circuit diagram (3) showing the charging/discharging state of the ozone generating tube, which was derived from FIG. 8(b). The equivalent impedance of the nonlinear energizing element 3f, which simulates the operating state of the ozone generating tube, is small when the ozone generating tube is discharging, and becomes extremely large when the discharging is stopped. Therefore, the equivalent capacity 3 of the void portion as shown in FIG. 8(b)
The parallel combined impedance of d and the current-carrying element 3f is:
During the discharge, the value becomes approximately equal to the value of the current-carrying element 3f,
Furthermore, when the discharging is stopped, the value becomes approximately equal to the value of the equivalent capacitance 3d, and therefore, when the discharging is stopped, the equivalent capacitance 3d is also charged at the same time. Therefore, the equivalent circuit of the ozone generator tube is:
In the discharge stopped state, that is, in the charging state of the equivalent capacitance 3d, the two equivalent capacitances 3d and 30 are connected in series as shown in the charging state diagram of FIG. As shown in the discharge state diagram (b), the equivalent capacitance 3e and the current-carrying element 3f are connected in series.
前記オゾン発生管における放電は、その印加交流電圧の
極性に応じ、前記空隙部等価容量3dの(4)
充電が進行しその両端電圧が前記放電維持電圧■4以上
になると共に開始され、該両端電圧が前記印加交流電圧
の極性反転に伴ない前記電圧V,以下に低下すると共に
停止し、同時に前記等価容量3dは前記印加交流電圧の
極性に応じた充電を開始し、以後前記の如き充電と放電
とが繰り返される。The discharge in the ozone generating tube starts as (4) charging of the air gap equivalent capacity 3d progresses and the voltage across it becomes equal to or higher than the discharge sustaining voltage (4), depending on the polarity of the applied AC voltage. The voltage drops below the voltage V due to the polarity reversal of the applied AC voltage and stops, and at the same time, the equivalent capacitance 3d starts charging according to the polarity of the applied AC voltage, and from then on, the charging as described above starts. The discharge is repeated.
第11図は上記動作状態におけるオゾン発生管の電圧・
電流波形図であり、第11図(イ)はその通電電流i。Figure 11 shows the voltage and voltage of the ozone generator tube in the above operating state.
This is a current waveform diagram, and FIG. 11 (a) shows the current i.
を示し、第11図(口)はその印加電圧■。を示す。Figure 11 (opening) shows the applied voltage. shows.
なお前記の如きオゾン発生管によるオゾン生成量は、前
記の如き充放電周期における放電期間が長くなると共に
増加するため、前記オゾン発生管用交流電源としては前
記空隙部等価容量3dの強制充電番;よる充電加速を図
るように第11図(イ)に示す如き矩形波電流を出力す
る交流電流源電源が用いられる。Note that the amount of ozone generated by the ozone generator tube as described above increases as the discharge period in the charge/discharge cycle becomes longer, so as an AC power source for the ozone generator tube, the forced charging number of the gap equivalent capacity 3d is determined. In order to accelerate charging, an alternating current source that outputs a rectangular wave current as shown in FIG. 11(a) is used.
〔発明が解決しようとする課題]
しかしながら、上記の如くオゾン発生管は等価(5)
的に容量性の電気的特性を有するため、前記従来方式の
電源装置においてその電源力率は進相側にて可或り小(
通常0.5〜0.6)となり電源容量の有効利用従って
電源容量の低減を阻害していた。[Problems to be Solved by the Invention] However, as described above, since the ozone generating tube has equivalent (5) capacitive electrical characteristics, the power factor of the power supply in the conventional power supply device is on the leading side. It may be small (
(usually 0.5 to 0.6), which hinders the effective use of the power supply capacity and therefore the reduction of the power supply capacity.
上記に鑑み本発明は前記の如き電源力率の改善と、更に
は前記オゾン発生管の放電期間延長によるオゾン生成量
の増大を可能とするオゾン発生管用電源装置の提供を目
的とするものである。In view of the above, it is an object of the present invention to provide a power supply device for an ozone generating tube, which is capable of improving the power factor of the power source as described above and further increasing the amount of ozone generated by extending the discharge period of the ozone generating tube. .
上記目的を達威するために、本発明のオゾン発生管用電
源装置は、誘電体を介して対向した電極間に無声放電を
発生させてオゾンを生或するオゾン発生管用の電流源特
性を有する交流電源装置において、交流電流源と前記オ
ゾン発生管との間に電圧電流整合用の変圧器を設けると
共に該変圧器の1次側又は2次側の何れか一方或いは両
方において該変圧器に並列にリアクトルを接続設置し、
且つ該リアクトルのインピーダンスを、その等価電気特
性において進相特性を有する前記オゾン発生管に給電す
る前記交流電流源の電源力率補償と(6)
前記リアクトルの蓄積エネルギ放出による前記オゾン発
生管の放電時間の延長とを十分図り得る値となすか、ま
たは前記の電圧電流整合用の変圧器と該変圧器の1次側
又は2次側の何れか一方或いは両方において該変圧器に
並列に設置されたリアクトルとに代えて、該両者の組合
せのなす前記の如き力率補償及び放電時間延長機能と同
様の機能を有する如く組合された3次巻線を有する変圧
器と該変圧器3次巻線に接続されたリアクトルとを設け
るか、或いはまた前記電圧電流整合用の変圧器と該変圧
器の1次側又は2次側の何れか一方或いは両方において
該変圧器に並列に設置されたリアクトルとに代えて、該
両者の組合せのなす等価インピーダンス特性に対しその
励磁インピーダンスを含む総合インピーダンス特性が同
様である変圧器を設けたものである。In order to achieve the above object, the ozone generator tube power supply device of the present invention uses an alternating current source having current source characteristics for an ozone generator tube that generates silent discharge between electrodes facing each other via a dielectric to generate ozone. In the power supply device, a voltage-current matching transformer is provided between the alternating current source and the ozone generating tube, and the transformer is connected in parallel to the transformer on either the primary side or the secondary side, or both. Connect and install the reactor,
and (6) compensating the power factor of the alternating current source that supplies power to the ozone generating tube, which has a phase advancing characteristic in its equivalent electrical characteristics, and (6) discharging the ozone generating tube by releasing the stored energy of the reactor. Either the voltage and current matching transformer is installed in parallel with the transformer on either the primary side or the secondary side of the transformer, or both. In place of the reactor, a transformer having a tertiary winding combined so as to have the same function as the power factor compensation and discharge time extension function described above provided by the combination of the two, and the tertiary winding of the transformer. or a reactor connected to the voltage-current matching transformer and a reactor connected to the transformer on either the primary side or the secondary side of the transformer, or both. Instead, a transformer is provided whose total impedance characteristic including its excitation impedance is the same as the equivalent impedance characteristic formed by the combination of the two.
進相(容量性)特性負荷を有する電源の力率改善は前記
負荷に並列に遅相(誘導性)特性要素であるリアクトル
を接続することにより可能となる。Power factor improvement of a power supply having a phase-leading (capacitive) characteristic load can be achieved by connecting a reactor, which is a phase-lag (inductive) characteristic element, in parallel to the load.
(7)
更にまた前記並列リアクトルの蓄積エネルギの放出電流
は電流源特性を有する交流電源より前記の負荷となるオ
ゾン発生管に対して供給される矩形波交流電流に重畳さ
れることにより、該矩形波電流の正負各半波において前
記オゾン発生管の空隙部等価容量の充電時期に対応する
電流値が増大されることになり、前記空隙部等価容量の
充電従って該空隙部の極間電圧の上昇が加速され、この
結果前記オゾン発生管の放電及び放電停止の繰り返し周
期における放電期間の延長が図られてオゾン生成量の増
大が可能となる。(7) Furthermore, the discharge current of the stored energy of the parallel reactor is superimposed on the rectangular wave alternating current supplied from the alternating current power supply having current source characteristics to the ozone generator tube serving as the load, so that the rectangular In each positive and negative half-wave of the wave current, the current value corresponding to the charging timing of the air gap equivalent capacity of the ozone generating tube is increased, and the air gap equivalent capacity is charged, and therefore the voltage between the electrodes of the air gap increases. is accelerated, and as a result, the discharge period in the repeated cycle of discharge and discharge stop of the ozone generating tube is extended, and the amount of ozone generated can be increased.
本発明は、前記の如く進相負荷となるオゾン発生管と前
記の如き交流電流源との間に電圧電流整合用の変圧器を
設けると共に該変圧器の1次側又は2次側の何れか一方
或いは両方において該変圧器に並列にリアクトルを設置
するか、或いはまた前記変圧器を3次巻線を有するもの
となし該3次巻線に接続されたリアクトルを設置して前
記の如き電源力率の改善とオゾン発生管の放電時間の延
長とを図るものである。The present invention provides a transformer for voltage and current matching between the ozone generator tube serving as a phase-advanced load as described above and the alternating current source as described above, and also provides a transformer for voltage and current matching between the primary side and the secondary side of the transformer. A reactor may be installed in parallel with the transformer in one or both of them, or the transformer may have a tertiary winding, and a reactor connected to the tertiary winding may be installed to provide power supply as described above. This aims to improve the rate and extend the discharge time of the ozone generator tube.
(8)
更に前記の如き整合用変圧器とリアクトルとの組合せを
1台の変圧器にて代行する場合には、前記組合せにおけ
る総合インピニダンスとその励磁インダクタンスL.を
含む前記1台の変圧器の総合インピーダンスとを同様と
なす必要がある。なお前記インダクタンスL.に関し下
記エネルギ式(1)が或立する。(8) Furthermore, when a single transformer is used for the combination of a matching transformer and a reactor as described above, the overall impinidance of the combination and its excitation inductance L. It is necessary to make the total impedance of the one transformer including Note that the inductance L. The following energy equation (1) is established regarding .
1
励磁エネルギ
励磁インダクタンス
励磁電流
鉄心起磁力
鉄心磁束密度
空気透磁率
鉄心体積
(9)
vg :鉄心空隙部体積
上記の式(1)に従い、前記1台の変圧器の総合インピ
ーダンスを略決定する励磁インダクタンスし.を該変圧
器の鉄心体積V1或いは鉄心に設けた空隙部体積V,等
の適当な選定により所要値となすことが可能となる。1 Excitation energy Excitation inductance Excitation current Core magnetomotive force Core magnetic flux density Air permeability Core volume (9) vg: Core void volume Excitation inductance that approximately determines the total impedance of one transformer according to the above equation (1) death. can be set to a required value by appropriately selecting the core volume V1 of the transformer or the void volume V provided in the core.
以下この発明の実施例を図面により説明する。 Embodiments of the present invention will be described below with reference to the drawings.
第1図と第4図と第5図と第6図とはこの発明の実施例
を示す回路図、第2図は第1図における電圧と電流との
基本波ベクトル図、第3図は第l図における電圧と電流
との波形図、第7図は第6図の等価回路図である。1, 4, 5, and 6 are circuit diagrams showing embodiments of the present invention, FIG. 2 is a fundamental wave vector diagram of voltage and current in FIG. 1, and FIG. 3 is a fundamental wave vector diagram of voltage and current in FIG. 1 is a waveform diagram of voltage and current, and FIG. 7 is an equivalent circuit diagram of FIG. 6.
第1図において、1は矩形波交流電流を出力する交流電
流源、2は電圧電流整合用の変圧器、3は前記第8図(
イ〉に示す各構戒要素3a〜3cより或るオゾン発生管
、4は並列リアクトルである。またi6は前記オゾン発
生管3の通電電流、v0は該電流10の通電により生じ
た前記オゾン発生管3の端子電圧、iLは前記リアクト
ル4・の(10)
通電電流、iIは前記両電流i。とjLとの合威電流で
あり前記変圧器2を介して前記電源1より供給される負
荷電流である。In FIG. 1, 1 is an AC current source that outputs a rectangular wave AC current, 2 is a voltage-current matching transformer, and 3 is the above-mentioned FIG.
Among the structural elements 3a to 3c shown in A), one of the ozone generating tubes, 4, is a parallel reactor. Further, i6 is the current flowing through the ozone generating tube 3, v0 is the terminal voltage of the ozone generating tube 3 generated by passing the current 10, iL is the (10) current flowing in the reactor 4, and iI is the current i . and jL, and is the load current supplied from the power supply 1 via the transformer 2.
第2図は前記各電流i。+ il+LLと電圧voと
の基本波におけるベクトル図であり、図示の如く前記リ
アクトル4を用いる場合の力率角θ2は同リアクトルを
用いぬ場合の力率角θ1に比して小となる。なお前記電
源1がらみた力率角は前記変圧器2の励磁電流により前
記角θ2よりも更に小となり、電源力率の改善と無効電
力の低減が図られている。FIG. 2 shows the respective currents i. It is a vector diagram of the fundamental wave of +il+LL and voltage vo, and as shown, the power factor angle θ2 when the reactor 4 is used is smaller than the power factor angle θ1 when the reactor is not used. Note that the power factor angle seen from the power source 1 becomes smaller than the angle θ2 due to the excitation current of the transformer 2, thereby improving the power factor of the power source and reducing reactive power.
更に第3図の(イ)〜(二)各図において、図(二)に
示す電圧V0の波形の充電部に対応する図(ハ)の電流
i。ば図(イ)と図(口)とにそれぞれ示す電流11と
iLとの差として与えられるために前記電流11より大
となり、前記電圧voの波形に関し前記第11図(口)
に示す前記リアクトル4不設置の場合に比し、前記オゾ
ン発生管3の空隙部等価容量3dの充電が加速されるた
めに図示充電期間は短縮されている。一方前記(11)
オゾン発生管3の充放電期間の和は前記交流電流源1の
出力周波数従って前記電流i,の周波数によって規定さ
れ定植となるために、前記の如き充電期間の短縮は放電
期間の延長をもたらすことになり、従って前記オゾン発
生管3におけるオゾン生成量は増加することになる。Furthermore, in each of the diagrams (a) to (ii) of FIG. 3, the current i in diagram (c) corresponds to the charging part of the waveform of voltage V0 shown in diagram (ii). For example, since it is given as the difference between the current 11 and iL shown in FIG.
Compared to the case where the reactor 4 is not installed, the charging period shown in the figure is shortened because the charging of the void equivalent capacity 3d of the ozone generating tube 3 is accelerated. On the other hand, since (11) the sum of the charging and discharging periods of the ozone generating tube 3 is determined by the output frequency of the alternating current source 1 and therefore the frequency of the current i, the shortening of the charging period as described above is due to the discharging period. Therefore, the amount of ozone produced in the ozone generating tube 3 increases.
第4図は、第1図における変圧器2と該変圧器2次側に
おける並列リアクトル4とを変圧器21と該変圧器の1
次側に設けた並列リアクトル41とにより置換したもの
であり、第4図に示す回路全体の動作は前記リアクトル
4lの通電電流を前記変圧器21の1次2次間巻線比に
より該変圧器2次側へ換算した値を用いることにより第
1図に示す回路の場合と同様に扱うことができる。FIG. 4 shows the transformer 2 and the parallel reactor 4 on the secondary side of the transformer in FIG.
The circuit is replaced by a parallel reactor 41 provided on the next side, and the operation of the entire circuit shown in FIG. By using the value converted to the secondary side, it can be handled in the same way as in the case of the circuit shown in FIG.
第5図は、第1図における変圧器2と該変圧器2次側に
おける並列リアクトル4とを3次巻線付の変圧器22と
該変圧器の3次巻線に接続された並列リアクトル42と
により置換したものであり、第5図に示す回路全体の動
作は前記第4図の場合の如く扱うことができる。なお2
2aと22bと(12)
22cとはそれぞれ前記変圧器22の1次巻線と2次巻
線と3次巻線とである。FIG. 5 shows the transformer 2 and the parallel reactor 4 on the secondary side of the transformer in FIG. The operation of the entire circuit shown in FIG. 5 can be handled as in the case of FIG. 4. Note 2
2a, 22b, and (12) 22c are the primary winding, secondary winding, and tertiary winding of the transformer 22, respectively.
第6図は、第1図,第4図或いは第5図において変圧器
と並列リアクトルとの組合せのなす機能を1台の変圧器
23により代行させる場合の回路図であり、第7図はそ
の等価回路図である。FIG. 6 is a circuit diagram when one transformer 23 performs the function of the combination of a transformer and a parallel reactor in FIGS. 1, 4, or 5, and FIG. It is an equivalent circuit diagram.
第7図点線内表示の23は前記変圧器の等価表示であり
、23aと23bと23cとはそれぞれ該変圧器の1次
インピーダンスと2淡インピーダンスと励磁インピーダ
ンスとを示すものである。Reference numeral 23 within the dotted line in FIG. 7 is an equivalent representation of the transformer, and 23a, 23b, and 23c represent the primary impedance, dielectric impedance, and excitation impedance of the transformer, respectively.
なお10は前記オゾン発生管3の通電電流、voは該電
流i。の通電により生じた前記オゾン発生管3の端子電
圧、18は前記変圧器2の励磁電流、i,は前記両電流
10と18との合戒電流であり前記電源1より供給され
る総合負荷電流であり、それぞれのベクトル関係は前記
第2図においてその電流iLを前記電流i。にて置換し
たものと同様となる。なおまた前記励磁インピーダンス
23cに関しては前記エネルギ式(1)が適用される。Note that 10 is the current flowing through the ozone generating tube 3, and vo is the current i. 18 is the excitation current of the transformer 2, i is the combined current of the two currents 10 and 18, and is the total load current supplied from the power source 1. , and the respective vector relationships are such that the current iL is the current i in FIG. It is the same as replacing with . Furthermore, the energy formula (1) is applied to the excitation impedance 23c.
「発明の効果〕
(13)
本発明によれば、オゾン発生管用電源装置において、該
電源装置とその負荷となるオゾン発生管との間に該オゾ
ン発生管の進相特性に応じた適当な励磁インピーダンス
を有する電圧電流整合用変圧器を設けるか、或いは該整
合用変圧器に代えて前記オゾン発生管に並列に適当な値
の遅相特性要素が接続されるように適当な巻数比の変圧
器と該変圧器の1次または2次巻線の何れか一方或いは
両方に並列接続されたリアクトルとの組合せ或いはまた
3次巻線付変圧器と該3次巻線に並列接続されたリアク
トルとの組合せを設けることにより、電源力率の改善に
よる電源所要容量の低減と前記オゾン発生管の放電時間
延長によるオゾン生威量の増大とを図ることが可能とな
る。"Effects of the Invention" (13) According to the present invention, in a power supply device for an ozone generator tube, appropriate excitation is performed between the power supply device and the ozone generator tube serving as a load in accordance with the phase advance characteristic of the ozone generator tube. A voltage-current matching transformer having an impedance is provided, or a transformer with an appropriate turns ratio is provided so that a slow phase characteristic element of an appropriate value is connected in parallel to the ozone generating tube in place of the matching transformer. and a reactor connected in parallel to one or both of the primary or secondary windings of the transformer, or a transformer with a tertiary winding and a reactor connected in parallel to the tertiary winding. By providing a combination, it is possible to reduce the required capacity of the power source by improving the power factor of the power source, and to increase the ozone yield by extending the discharge time of the ozone generating tube.
第1図と第4図と第5図と第6図とはこの発明の実施例
を示す回路図、第2図は第1図における電圧と電流との
基本波ベクトル図、第3図は第1図における電圧と電流
との波形図、第7図は第6図の等価回路図である。
(14)
また第8図(イ)は従来技術の実施例を示す回路図、第
8図(口〉はオゾン発生管の等価回路図、第9図はオゾ
ン発生管の充放電状態の等価回路図、第10図はオゾン
発生管空隙部の電流一電圧特性図、第1l図は第8図く
イ)の状態にあるオゾン発生管の電圧・電流波形図であ
る。
1・・・交流電流源、2,21.23・・・変圧器、2
2・・・(3次巻線付)変圧器、3・・・オゾン発生管
、3a,3b・・・オゾン発生管電極、3c・・・同電
極間誘電体、3d・・・オゾン発生管空隙部等価容量、
3e・・・同誘電体部等価容量、3f・・・同空隙部等
価模擬素子(非線形通電素子)、4,41.’42・・
・並列リアクトル。1, 4, 5, and 6 are circuit diagrams showing embodiments of the present invention, FIG. 2 is a fundamental wave vector diagram of voltage and current in FIG. 1, and FIG. 3 is a fundamental wave vector diagram of voltage and current in FIG. FIG. 1 is a waveform diagram of voltage and current, and FIG. 7 is an equivalent circuit diagram of FIG. 6. (14) Also, Fig. 8 (a) is a circuit diagram showing an example of the conventional technology, Fig. 8 (opening) is an equivalent circuit diagram of an ozone generator tube, and Fig. 9 is an equivalent circuit diagram of the charging and discharging state of the ozone generator tube. 10 is a current-voltage characteristic diagram of the ozone generating tube gap, and FIG. 11 is a voltage/current waveform diagram of the ozone generating tube in the state shown in FIG. 8 (a). 1... AC current source, 2, 21.23... Transformer, 2
2... Transformer (with tertiary winding), 3... Ozone generator tube, 3a, 3b... Ozone generator tube electrode, 3c... Dielectric between the same electrodes, 3d... Ozone generator tube Equivalent volume of void,
3e...Equivalent capacitance of the dielectric part, 3f...Equivalent simulation element (nonlinear current-carrying element) of the gap part, 4, 41. '42...
・Parallel reactor.
Claims (1)
せてオゾンを生成するオゾン発生管用の電流源特性を有
する交流電源装置において、交流電流源と前記オゾン発
生管との間に電圧電流整合用の変圧器を設けると共に該
変圧器の1次側又は2次側の何れか一方或いは両方にお
いて該変圧器に並列にリアクトルを接続設置し、且つ該
リアクトルのインピーダンスを、その等価電気特性にお
いて進相特性を有する前記オゾン発生管に給電する前記
交流電流源の電源力率補償と前記リアクトルの蓄積エネ
ルギ放出による前記オゾン発生管の放電時間の延長とを
十分図り得る値となしたことを特徴とするオゾン発生管
用電源装置。 2)請求項1記載のオゾン発生管用電源装置において、
電圧電流整合用の変圧器と該変圧器の1次側又は2次側
の何れか一方或いは両方において該変圧器に並列に設置
されたリアクトルとに代えて、該両者の組合せのなす前
記の如き力率補償及び放電時間延長機能と同様の機能を
有する如く組合された3次巻線を有する変圧器と該変圧
器3次巻線に接続されたリアクトルとを設けたことを特
徴とするオゾン発生管用電源装置。 3)請求項1記載のオゾン発生管用電源装置において、
電圧電流整合用の変圧器と該変圧器の1次側又は2次側
の何れか一方或いは両方において該変圧器に並列に設置
されたリアクトルとに代えて、該両者の組合せのなす等
価インピーダンス特性に対しその励磁インピーダンスを
含む総合インピーダンス特性が同様である変圧器を設け
たことを特徴とするオゾン発生管用電源装置。[Scope of Claims] 1) An AC power supply device having current source characteristics for an ozone generator tube that generates ozone by generating silent discharge between electrodes facing each other via a dielectric, which comprises: an AC current source and the ozone generator tube; A transformer for voltage and current matching is provided between the transformer and a reactor is connected and installed in parallel to the transformer on either the primary side or the secondary side of the transformer, or both, and the impedance of the reactor is , a value that can sufficiently compensate for the power factor of the alternating current source that supplies power to the ozone generator tube, which has a phase advance characteristic in its equivalent electrical characteristics, and extend the discharge time of the ozone generator tube by releasing the stored energy of the reactor. A power supply device for an ozone generating tube, which is characterized by the following. 2) In the ozone generating tube power supply device according to claim 1,
Instead of a voltage-current matching transformer and a reactor installed in parallel with the transformer on either the primary side or the secondary side of the transformer, or both, a combination of the two as described above can be used. Ozone generation characterized by comprising a transformer having a tertiary winding combined to have functions similar to power factor compensation and discharge time extension functions, and a reactor connected to the tertiary winding of the transformer. Pipe power supply. 3) In the ozone generating tube power supply device according to claim 1,
Instead of a voltage-current matching transformer and a reactor installed in parallel with the transformer on either the primary side or the secondary side of the transformer, or both, equivalent impedance characteristics formed by the combination of the two. 1. A power supply device for an ozone generating tube, characterized in that a transformer having similar overall impedance characteristics including excitation impedance is provided.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1225739A JP2697178B2 (en) | 1989-03-08 | 1989-08-31 | Power supply for ozone generating tube |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5595989 | 1989-03-08 | ||
| JP1-55959 | 1989-03-08 | ||
| JP1225739A JP2697178B2 (en) | 1989-03-08 | 1989-08-31 | Power supply for ozone generating tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0316902A true JPH0316902A (en) | 1991-01-24 |
| JP2697178B2 JP2697178B2 (en) | 1998-01-14 |
Family
ID=26396856
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1225739A Expired - Lifetime JP2697178B2 (en) | 1989-03-08 | 1989-08-31 | Power supply for ozone generating tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2697178B2 (en) |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS50122662U (en) * | 1974-03-23 | 1975-10-07 | ||
| JPS54107895A (en) * | 1978-02-13 | 1979-08-24 | Mitsubishi Electric Corp | Ozonizer |
| JPS54107894A (en) * | 1978-02-13 | 1979-08-24 | Mitsubishi Electric Corp | Ozonizer |
| JPS61295207A (en) * | 1985-06-21 | 1986-12-26 | オツォニア・アクチェンゲゼルシャフト | Ozone generator and its operation method |
-
1989
- 1989-08-31 JP JP1225739A patent/JP2697178B2/en not_active Expired - Lifetime
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS50122662U (en) * | 1974-03-23 | 1975-10-07 | ||
| JPS54107895A (en) * | 1978-02-13 | 1979-08-24 | Mitsubishi Electric Corp | Ozonizer |
| JPS54107894A (en) * | 1978-02-13 | 1979-08-24 | Mitsubishi Electric Corp | Ozonizer |
| JPS61295207A (en) * | 1985-06-21 | 1986-12-26 | オツォニア・アクチェンゲゼルシャフト | Ozone generator and its operation method |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2697178B2 (en) | 1998-01-14 |
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