JPH0368465A - Electric power source for electrostatic precipitator - Google Patents
Electric power source for electrostatic precipitatorInfo
- Publication number
- JPH0368465A JPH0368465A JP20503889A JP20503889A JPH0368465A JP H0368465 A JPH0368465 A JP H0368465A JP 20503889 A JP20503889 A JP 20503889A JP 20503889 A JP20503889 A JP 20503889A JP H0368465 A JPH0368465 A JP H0368465A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- pulse
- power supply
- electrostatic precipitator
- high 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.)
- Granted
Links
- 239000012717 electrostatic precipitator Substances 0.000 title claims description 23
- 239000000428 dust Substances 0.000 claims description 29
- 230000006835 compression Effects 0.000 claims description 13
- 238000007906 compression Methods 0.000 claims description 13
- 239000003990 capacitor Substances 0.000 description 24
- 238000010586 diagram Methods 0.000 description 8
- 238000007600 charging Methods 0.000 description 6
- 238000004804 winding Methods 0.000 description 6
- 150000002500 ions Chemical class 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 229920006395 saturated elastomer Polymers 0.000 description 4
- 239000012716 precipitator Substances 0.000 description 3
- 238000013459 approach Methods 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 2
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000009499 grossing Methods 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 1
- 238000007599 discharging Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000010278 pulse charging Methods 0.000 description 1
- 238000007493 shaping process Methods 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Landscapes
- Electrostatic Separation (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〕
本発明は電気集塵機用高圧電源装置に係り、特に直流高
電圧にコンデンサの充放電によるパルス波形の電圧を重
畳した電圧波形を出力するに好適な電気集塵機用高圧電
源装置に関するものである。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a high voltage power supply device for an electrostatic precipitator, and is particularly suitable for outputting a voltage waveform in which a pulse waveform voltage due to charging and discharging of a capacitor is superimposed on a DC high voltage. This invention relates to a high-voltage power supply device for an electric dust collector.
一般に電気集塵装置においてはダストの電気抵抗が高く
なると逆電離現象と呼ばれる異常放電が発生し集塵性能
を著しく低下させることが知られている。これは集塵室
の集塵電極板上に帯電付着したダストが高抵抗の場合、
ダスト層の電荷放出が悪いためにそのダスト層において
電気的絶縁破壊が生じ、この絶縁破壊によって発生した
イオンが集塵空間の電荷を中和してしまうものである。Generally, in electrostatic precipitators, it is known that when the electrical resistance of dust increases, abnormal discharge called a reverse ionization phenomenon occurs, significantly reducing dust collection performance. This is because if the charged dust attached to the dust collection electrode plate in the dust collection chamber has a high resistance,
Electrical breakdown occurs in the dust layer due to poor charge release in the dust layer, and ions generated by this breakdown neutralize the charge in the dust collection space.
このような逆電離現象の対策として、従来、電気集m機
にはパルス荷電方式と間欠荷電方式とが採用されている
。As a countermeasure against such a reverse ionization phenomenon, a pulse charging method and an intermittent charging method have conventionally been adopted for electric concentrators.
前者の電気集塵機用高圧電源装置は、直流高圧電源装置
と、パルス電源装置との2台の電源装置を用い、直流高
電圧にパルス波形の電圧を重畳する方式がとられている
。即ち、集塵機の放電電極と集塵電極との電極間にコロ
ナ放電開始電圧前後の直流バイアス電圧を印加させた状
態で数パルス7秒以上の高電圧パルスを印加させる荷電
方法が採用されている。第8図にこのような荷電方法が
採用されている従来の電気集塵機の電源装置の全体構成
を示す。The former high-voltage power supply for an electric precipitator uses two power supplies, a DC high-voltage power supply and a pulse power supply, and employs a method in which a pulse waveform voltage is superimposed on the DC high voltage. That is, a charging method is adopted in which a high voltage pulse of several pulses for 7 seconds or more is applied while a DC bias voltage around the corona discharge starting voltage is applied between the discharge electrode and the dust collection electrode of the dust collector. FIG. 8 shows the overall configuration of a conventional electric dust collector power supply device in which such a charging method is adopted.
第8図に於いて、10は集塵機、12は直流高電圧電源
回路、14は高電圧パルス発生電源回路である。集塵機
10は放電電極16と集塵電極18とから構成される。In FIG. 8, 10 is a dust collector, 12 is a DC high voltage power supply circuit, and 14 is a high voltage pulse generation power supply circuit. The dust collector 10 is composed of a discharge electrode 16 and a dust collection electrode 18.
直流高電圧電源回路12は、交流電i1!!20、スイ
ッチングサイリスタ22、昇圧トランス24、整流器2
6からlI威される。The DC high voltage power supply circuit 12 is an AC power i1! ! 20, switching thyristor 22, step-up transformer 24, rectifier 2
I will be threatened from 6.
また、高電圧パルス発生電源回路14は、交流1N28
、サイリスタ30.平滑コンデンサ32、スイッチング
サイリスタ33、ダイオード34、コイル35、昇圧ト
ランス36から構成される。In addition, the high voltage pulse generation power supply circuit 14 has an AC 1N28
, thyristor 30. It is composed of a smoothing capacitor 32, a switching thyristor 33, a diode 34, a coil 35, and a step-up transformer 36.
直流高電圧を源回路12と高電圧パルス発生電源回路1
4とは結合コンデンサ38を介して結合される。DC high voltage source circuit 12 and high voltage pulse generation power source circuit 1
4 through a coupling capacitor 38.
このような構成の電気集塵機では、集塵機10の放電電
極16と集塵電極18との電極間に直流高電圧電源間1
12から出力されるベース電圧が印加され、又、高電圧
パルス発生電源回路14から出力される高電圧パルスが
結合コンデンサ38によってペース電圧に重畳されて印
加されるようになっている。In an electric precipitator having such a configuration, a DC high voltage power source 1 is connected between the discharge electrode 16 and the dust collection electrode 18 of the precipitator 10.
A base voltage outputted from the high voltage pulse generator 12 is applied, and a high voltage pulse outputted from the high voltage pulse generation power supply circuit 14 is superimposed on the pace voltage by a coupling capacitor 38 and applied.
即ち、直流高電圧電源回路12の交流電源20からの電
圧は、昇圧トランス24によって昇圧され、整流器26
により直流に整流され、放電極16と集塵極18との間
にペース電圧として荷電される。一方、パルス発生電源
回路14のサイリスタ30のゲートに電圧が印加されて
導通され、交流電源28からの電圧がコンデンサ32に
充電される。次に、サイリスタ33のゲートに電圧が印
加されて導通されると共にコンデンサ32から放電され
、昇圧トランス36の一次巻1136Aの電圧が昇圧ト
ランス36により、二次巻!36B側で昇圧される。昇
圧トランス36で昇圧された電圧は、コンデンサ38を
介して電気集W1機の放電極の電圧を上昇させる。一方
、パルス発生電源口Vs14のコイル35のインダクタ
ンスLl 、昇圧トランス36のインダクタンスL2
、コンデンサ38の静電容量、及び電気集塵機の放電極
16と集塵極間18の静電容量とで共振回路を構成し、
昇圧した後の次の半サイクル間は、ダイオード34を介
して電流が逆方向に流れて電圧が急激に下がる。このよ
うにしてベース電圧に重畳してパルス波形の電圧(パル
ス電圧)が印加される。That is, the voltage from the AC power supply 20 of the DC high voltage power supply circuit 12 is stepped up by the step-up transformer 24, and then
The current is rectified into direct current and charged as a pace voltage between the discharge electrode 16 and the dust collection electrode 18. On the other hand, a voltage is applied to the gate of the thyristor 30 of the pulse generation power supply circuit 14 to make it conductive, and the capacitor 32 is charged with the voltage from the AC power supply 28 . Next, a voltage is applied to the gate of the thyristor 33 to make it conductive, and at the same time discharge from the capacitor 32, the voltage of the primary winding 1136A of the step-up transformer 36 is changed to the secondary winding by the step-up transformer 36! The voltage is boosted on the 36B side. The voltage boosted by the step-up transformer 36 increases the voltage at the discharge electrode of the electric collector W1 via the capacitor 38. On the other hand, the inductance Ll of the coil 35 of the pulse generation power supply port Vs14 and the inductance L2 of the step-up transformer 36
A resonant circuit is constituted by the capacitance of the capacitor 38 and the capacitance between the discharge electrode 16 and the dust collection electrode 18 of the electrostatic precipitator,
During the next half cycle after boosting the voltage, current flows in the opposite direction through the diode 34 and the voltage drops rapidly. In this way, a pulse waveform voltage (pulse voltage) is applied superimposed on the base voltage.
ところで、従来の電気集塵機用高圧電源装置は、パルス
電圧のパルス幅が長い為、放電極面からイオンの放出が
一様に行われない欠点があった。この為、スパーク電圧
が低く、火花放電が発生し易くなり、集塵能力が低下す
る欠点がある。By the way, conventional high-voltage power supplies for electrostatic precipitators have a drawback that ions are not emitted uniformly from the discharge electrode surface because the pulse width of the pulse voltage is long. For this reason, the spark voltage is low, spark discharge is likely to occur, and the dust collection ability is reduced.
この為、パルス電圧のパルス幅を短くしようとすると、
di/dt が大きくなり、−次側のサイリスタに大き
な負担がかかるようになる。従って、従来、小容量の電
気集塵機ではパルス電圧のパルス幅を短くすることも可
能であったが、大容量の電気集塵機では、サイリスクに
負担がかかり過ぎ、パルス幅を短くすることが出来なか
った。Therefore, if you try to shorten the pulse width of the pulse voltage,
di/dt increases, and a heavy load is placed on the thyristor on the negative side. Therefore, in the past, it was possible to shorten the pulse width of the pulse voltage with small-capacity electrostatic precipitators, but with large-capacity electrostatic precipitators, it was impossible to shorten the pulse width because the burden was too high on the si-risk. .
本発明は、このような事情に鑑みてなされたもので、大
容量の電気集塵機でもパルス幅が短く出来、更に、放電
極からイオンの放出が一様に行われ、スパーク電圧が高
くて集塵能力が低下しない電気業!!装置用電源装置を
提案することを目的とする。The present invention was developed in view of the above circumstances, and it is possible to shorten the pulse width even in a large-capacity electrostatic precipitator, and furthermore, the ions are uniformly released from the discharge electrode, and the spark voltage is high, making it possible to collect dust easily. Electrical industry that does not reduce capacity! ! The purpose is to propose a power supply device for equipment.
本発明は、前記目的を達成する為に、直流高電圧にパル
ス波形の電圧を重畳した電圧を電気集塵機に供給する電
気集塵機用高圧電源装置において、交流電源からの交流
電圧を昇圧、整流し、放電極と集塵極との間に直流高電
圧を印加する直流高電圧発生手段と、交流電源からの交
流電圧をパルス波形の電圧に成形し、これを昇圧する手
段と、昇圧した出力電圧波形を磁気圧縮する磁気パルス
圧縮手段とを備え、この磁気パルス圧縮手段によりパル
ス幅が圧縮されたパルス波形の電圧を前記放電極と集塵
電極との電極間に印加する手段とから成ることを特徴と
している。In order to achieve the above object, the present invention provides a high-voltage power supply device for an electrostatic precipitator that supplies a voltage obtained by superimposing a voltage with a pulse waveform on a high DC voltage to an electrostatic precipitator. A DC high voltage generating means for applying a DC high voltage between a discharge electrode and a dust collection electrode, a means for shaping an AC voltage from an AC power source into a pulse waveform voltage and boosting the voltage, and a boosted output voltage waveform. and a means for applying a voltage having a pulse waveform whose pulse width is compressed by the magnetic pulse compression means between the discharge electrode and the dust collection electrode. It is said that
本発明では、直流高電圧発生手段により集!!機の放電
極と集塵極との間にベース電圧が印加される。一方、磁
気パルス圧縮手段によりパルス電圧が磁気圧縮されてベ
ース電圧に重畳される。これによりパルス幅が短くなり
放電極からのイオン放出が一様になされる。In the present invention, the DC high voltage generation means is used to generate high voltage. ! A base voltage is applied between the discharge electrode and the collection electrode of the machine. On the other hand, the pulse voltage is magnetically compressed by the magnetic pulse compression means and superimposed on the base voltage. This shortens the pulse width and uniformly releases ions from the discharge electrode.
以下添付図面に従って本発明に係る電気集塵機用電源装
置の好ましい実施例を詳説する。Preferred embodiments of a power supply device for an electrostatic precipitator according to the present invention will be described in detail below with reference to the accompanying drawings.
第1図は本発明に係る第1実施例の構造が示され、第8
図に示した従来の電気集塵機用電源装置と同一の部材若
しくは類似の部材には同一の符号を付し、その詳しい説
明は省略する。FIG. 1 shows the structure of the first embodiment according to the present invention, and the structure of the eighth embodiment is shown in FIG.
The same members or similar members as those of the conventional power supply device for an electrostatic precipitator shown in the figure are given the same reference numerals, and detailed explanation thereof will be omitted.
第1図に於いて、10は集塵機、12は直流高電圧電源
回路、14は高電圧パルス発生電源回路である。集ma
12は放電電極16と集塵電極18とから構成される。In FIG. 1, 10 is a dust collector, 12 is a DC high voltage power supply circuit, and 14 is a high voltage pulse generation power supply circuit. collection ma
12 is composed of a discharge electrode 16 and a dust collection electrode 18.
直流高電圧電源回路12は、交流電111!20、スイ
ッチングサイリスタ22、昇圧トランス24、整流器2
6から構成される。The DC high voltage power supply circuit 12 includes an AC power supply 111!20, a switching thyristor 22, a step-up transformer 24, and a rectifier 2.
Consists of 6.
また、高電圧パルス発生電源回路14の一次側には、交
流電源20、ダイオード31、平滑コンデンサ32、ス
イッチングサイリスタ33、ダイオード34、インダク
タ35、昇圧トランス36から構成される。更に、二次
側にはコンデンサ40、過飽和リアクトル42が設多す
られる。過飽和リアクトル42は第2図に示すようにト
ロイダル型磁芯42Aから構成される。トロイダル型磁
芯42Aは、非晶質合金又は合金、若しくはフェライト
等の材料で形成される。Further, the primary side of the high voltage pulse generation power supply circuit 14 includes an AC power supply 20, a diode 31, a smoothing capacitor 32, a switching thyristor 33, a diode 34, an inductor 35, and a step-up transformer 36. Furthermore, a capacitor 40 and a supersaturation reactor 42 are installed on the secondary side. The supersaturation reactor 42 is composed of a toroidal magnetic core 42A as shown in FIG. The toroidal magnetic core 42A is made of a material such as an amorphous alloy or alloy, or ferrite.
第1実施例は、パルス電圧は一定のパルス電圧で運転す
るもので、ダイオード31により交流電R28からの交
流電圧を整流して、コンデンサ32を交流電圧のピーク
値まで充電し、パルス発生回路の直流電源電圧を得てい
る。In the first embodiment, the pulse voltage is operated at a constant pulse voltage, and the diode 31 rectifies the AC voltage from the AC voltage R28 to charge the capacitor 32 to the peak value of the AC voltage, and the DC voltage of the pulse generation circuit is Obtaining power supply voltage.
第1実施例では、電気集塵機10の容量や、パルストラ
ンス36で昇圧後の電圧をもとに、磁気圧縮回路の可飽
和リアクトル42を適当に設計することにより、入力が
あると自動的にパルス圧縮動作を行う。つまりサイリス
タ33をオンさせると、コンデンサ32に蓄えられてい
た電荷は、パルストランスの一次側36Aを通して流れ
、二次側36Bに昇圧されたパルス電圧が現れる(パル
ス幅はりアクドル35.37、パルストランス36の巻
線のインダクタンス及びコンデンサ32.38.40の
容量で決まる〉。この電圧がピークに近くなったとき、
可飽和リアクトル42が飽和し、抵抗は略零に近づく。In the first embodiment, by appropriately designing the saturable reactor 42 of the magnetic compression circuit based on the capacity of the electrostatic precipitator 10 and the voltage boosted by the pulse transformer 36, the saturable reactor 42 of the magnetic compression circuit is automatically pulsed when an input is received. Performs compression operation. In other words, when the thyristor 33 is turned on, the charge stored in the capacitor 32 flows through the primary side 36A of the pulse transformer, and a boosted pulse voltage appears on the secondary side 36B (the pulse width is 35.37 mm, the pulse transformer It is determined by the inductance of the winding 36 and the capacitance of the capacitor 32, 38, and 40. When this voltage is close to its peak,
The saturable reactor 42 becomes saturated and the resistance approaches approximately zero.
直流高電圧電源回路12と高電圧パルス発生電源回路1
4とは総合コンデンサ38を介して結合される。DC high voltage power supply circuit 12 and high voltage pulse generation power supply circuit 1
4 via a general capacitor 38.
前記の如く構成された本発明に係る電気集塵機用電源装
置によれば、直流高電圧電源回路12の交流電源20か
らの電圧は、昇圧トランス24によって昇圧され、整流
器26により直流に整流され、放電極16と集塵極18
との間にベース電圧が印加される。一方、高電圧パルス
発生電源回路14の交流電源28からの交流電圧はダイ
オード31で整流されてコンデンサ32に充電される。According to the power supply device for an electrostatic precipitator according to the present invention configured as described above, the voltage from the AC power supply 20 of the DC high voltage power supply circuit 12 is boosted by the step-up transformer 24, rectified to DC by the rectifier 26, and then discharged. Electrode 16 and dust collection electrode 18
A base voltage is applied between. On the other hand, the AC voltage from the AC power supply 28 of the high voltage pulse generation power supply circuit 14 is rectified by the diode 31 and charged into the capacitor 32.
次に、サイリスタ33のゲートに電圧がE+7加されて
導通されると共にコンデンサ32から放電され、昇圧ト
ランス36の一次巻線36Aの電圧が昇圧トランス36
により、二次巻線36B(IQで昇圧される。昇圧され
た二次側電流はコンデンサ4oを充電する。コンデンサ
40への充電が終了すると徐々に電流が過飽和リアクト
ル42に流れ始め、入力端子がピーク値の時、この時過
飽和リアクトル42は飽和状態になって抵抗値が零に近
づく。Next, voltage E+7 is applied to the gate of the thyristor 33 to make it conductive, and the capacitor 32 is discharged, and the voltage of the primary winding 36A of the step-up transformer 36 is increased to the step-up transformer 36.
As a result, the voltage is boosted by the secondary winding 36B (IQ).The boosted secondary current charges the capacitor 4o.When the charging of the capacitor 40 is finished, the current gradually starts to flow to the supersaturation reactor 42, and the input terminal becomes At the peak value, the supersaturated reactor 42 becomes saturated and the resistance value approaches zero.
これによりコンデンサ4oからの電流が急激に流れ、パ
ルス電圧波形が圧縮される。この時の人力電圧と出力電
圧との波形を示しているのが第3図である。一方、パル
ス発生電源回路14のコイル35.37のインダクタン
スL、 、Lコ、昇圧トランス36のインダクタンスL
’ 、コンデンサ32.38.40の静電容量と電気集
塵機の放電極と集塵極間の静電容量とで共振回路を構成
し、昇圧した後の次の半サイクル間はダイオード34を
介して電流が逆方向に流れて電圧が急激に下がる。As a result, the current from the capacitor 4o rapidly flows, and the pulse voltage waveform is compressed. FIG. 3 shows the waveforms of the human power voltage and the output voltage at this time. On the other hand, the inductances L, , L of the coils 35 and 37 of the pulse generation power supply circuit 14, and the inductance L of the step-up transformer 36
', The capacitance of the capacitors 32, 38, 40 and the capacitance between the discharge electrode and the dust collection electrode of the electrostatic precipitator constitute a resonant circuit, and during the next half cycle after boosting, the voltage is passed through the diode 34. The current flows in the opposite direction and the voltage drops suddenly.
このようにしてベース電圧に重畳してパルス電圧が荷電
される。このように、本発明ではパルス発生電源回路1
4の二次側でパルス幅を圧縮するので、−次側のサイス
フ33に負担をかけない。In this way, the pulse voltage is charged superimposed on the base voltage. In this way, in the present invention, the pulse generation power supply circuit 1
Since the pulse width is compressed on the secondary side of 4, no burden is placed on the secondary side 33.
第4図では本発明に係る第2実施例が示され、コンデン
サ40と過飽和リアクトル42との組合わせは第1実施
例の1段に限らず、複数段、例えば14図に示すように
2&設けてもよい。FIG. 4 shows a second embodiment of the present invention, in which the combination of a capacitor 40 and a supersaturation reactor 42 is not limited to one stage as in the first embodiment, but can be arranged in multiple stages, for example, as shown in FIG. You can.
第5図はパルス電圧が変化し得る場合の他の実施例でコ
ンデンサ32の充電圧をサイリスタ30の位相角制御に
より調節し、パルス電圧の大きさを変えられるようにし
たものである。この場合、パルス発生電源回路14の二
次側コイル36Bに現れる電圧が変化すると、磁気圧縮
回路が飽和するタイミングも変化する。従って、第6図
に示すように直流電圧Vにより、コア42Aのもう一つ
の巻線に電流を流し、コアを偏磁させて、入力電圧が変
化したときでも最適タイミングで磁気圧縮動作が始まる
ようにする。直流電圧Vは、第51!1のサイリスタ3
0の位相角制御と運動して変化するようにし、偏磁の大
きさを調整し、磁気圧縮回路の入力電圧の変化に対応さ
せる。FIG. 5 shows another embodiment in which the pulse voltage can be changed, and the charging voltage of the capacitor 32 is adjusted by controlling the phase angle of the thyristor 30, so that the magnitude of the pulse voltage can be changed. In this case, when the voltage appearing on the secondary coil 36B of the pulse generation power supply circuit 14 changes, the timing at which the magnetic compression circuit is saturated also changes. Therefore, as shown in FIG. 6, a current is applied to the other winding of the core 42A using the DC voltage V to bias the core so that the magnetic compression operation starts at the optimum timing even when the input voltage changes. Make it. The DC voltage V is the 51st!1st thyristor 3
0 phase angle control and the magnitude of the biased magnetism is adjusted to correspond to changes in the input voltage of the magnetic compression circuit.
第7図はパルス電圧を変える場合の他の磁気圧縮回路の
例として示されている。第7図に示すように過飽和リア
クトル42にトリガ回路44を付加し、サイリスタ46
をオンしてトリガのための電流を流して強制的にタイミ
ングをとっている。FIG. 7 shows an example of another magnetic compression circuit in which the pulse voltage is changed. As shown in FIG. 7, a trigger circuit 44 is added to the oversaturation reactor 42, and a thyristor 46
The timing is forcibly determined by turning on the trigger current and forcing the trigger current to flow.
即ち、サイリスタ46にトリガ信号を加えると、コンデ
ンサ47に蓄えられた電荷がサイリスタ46を通してト
リガ用のコイルを流れ、コア42Aは飽和する。That is, when a trigger signal is applied to the thyristor 46, the charge stored in the capacitor 47 flows through the trigger coil through the thyristor 46, and the core 42A becomes saturated.
以上説明したように本発明に係る電気集塵機用電源装置
によれば、磁気パルス圧縮子役を設けてパルス発生手段
からのパルス波形幅を圧縮したので、放電極からのイオ
ンの放出が一様に行われ、集塵能力が低下しない。As explained above, according to the power supply device for an electrostatic precipitator according to the present invention, since the pulse waveform width from the pulse generation means is compressed by providing the magnetic pulse compression child, ions are uniformly emitted from the discharge electrode. Therefore, the dust collection ability will not decrease.
また、パルス電圧波形を磁気圧縮で縮めるので、パルス
電圧は一次側で緩やかに立上げることが出来るので、サ
イリスクに負担をかけるようなことがない。これにより
、従来、小容量の電気集塵機でしかパルス幅を縮めるこ
とは出来なかったが、本発明により大容量の電気集塵機
でも短いパルス幅のパルス電圧を供給できるようになっ
た。Furthermore, since the pulse voltage waveform is compressed by magnetic compression, the pulse voltage can be gradually raised on the primary side, so there is no burden on the silicon risk. As a result, conventionally it was possible to shorten the pulse width only with a small-capacity electrostatic precipitator, but the present invention has made it possible to supply a pulse voltage with a short pulse width even with a large-capacity electrostatic precipitator.
第1図は本発明に係る第1実施例を示すブロック図、第
2図は第1実施例の過飽和リアクトルを示す回路図、第
3図は第1実施例の入出力波形を示す特性図、第4図は
本発明の第2実施例のブロック図、第5図は本発明の第
3実施例を示すブロック図、第6図は第3実施例で用い
られる過飽和リアクトルの回路図、第7図は第3実施例
で用いられる別の過飽和リアクトルの回路図、第8図は
電気集塵機の従来の電源回路図である。
lO・・・電気集塵機、 12・・・直流高電圧電源
回路、 14・・・高電圧パルス発生電源回路、 4
0・・・コンデンサ、 42・・・過飽和リアクトル
。
第 3 図
’A 4 bFIG. 1 is a block diagram showing a first embodiment according to the present invention, FIG. 2 is a circuit diagram showing a supersaturation reactor of the first embodiment, and FIG. 3 is a characteristic diagram showing input and output waveforms of the first embodiment. FIG. 4 is a block diagram of a second embodiment of the present invention, FIG. 5 is a block diagram of a third embodiment of the present invention, FIG. 6 is a circuit diagram of a supersaturation reactor used in the third embodiment, and FIG. The figure is a circuit diagram of another supersaturation reactor used in the third embodiment, and FIG. 8 is a conventional power supply circuit diagram of an electrostatic precipitator. 1O... Electrostatic precipitator, 12... DC high voltage power supply circuit, 14... High voltage pulse generation power supply circuit, 4
0...Capacitor, 42...Supersaturation reactor. Figure 3 'A 4 b
Claims (1)
電気集塵機に供給する電気集塵機用高圧電源装置におい
て、 交流電源からの交流電圧を昇圧、整流し、放電極と集塵
極との間に直流高電圧を印加する直流高電圧発生手段と
、 交流電源からの交流電圧をパルス波形の電圧に成形し、
これを昇圧する手段と、 昇圧した出力電圧波形を磁気圧縮する磁気パルス圧縮手
段とを備え、 この磁気パルス圧縮手段によりパルス幅が圧縮されたパ
ルス波形の電圧を前記放電極と集塵電極との電極間に印
加する手段とから成る電気集塵機用電源装置。(1) In a high-voltage power supply device for an electrostatic precipitator that supplies a voltage obtained by superimposing a pulse waveform voltage on a DC high voltage to an electrostatic precipitator, the AC voltage from the AC power source is boosted and rectified, and the AC voltage is increased between the discharge electrode and the dust collection electrode. a DC high voltage generating means for applying a DC high voltage to the
and magnetic pulse compression means for magnetically compressing the boosted output voltage waveform, and the voltage of the pulse waveform whose pulse width has been compressed by the magnetic pulse compression means is applied to the discharge electrode and the dust collection electrode. A power supply device for an electrostatic precipitator, comprising means for applying voltage between electrodes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20503889A JPH0712449B2 (en) | 1989-08-07 | 1989-08-07 | Power supply for electric dust collector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20503889A JPH0712449B2 (en) | 1989-08-07 | 1989-08-07 | Power supply for electric dust collector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0368465A true JPH0368465A (en) | 1991-03-25 |
| JPH0712449B2 JPH0712449B2 (en) | 1995-02-15 |
Family
ID=16500418
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20503889A Expired - Lifetime JPH0712449B2 (en) | 1989-08-07 | 1989-08-07 | Power supply for electric dust collector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0712449B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04354549A (en) * | 1991-05-30 | 1992-12-08 | Hitachi Plant Eng & Constr Co Ltd | High voltage power supply for electrostatic precipitator |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| SE2051167A1 (en) | 2020-10-02 | 2022-03-22 | Envirotainer Eng Ab | Temperature-controlled transport container and a method for controlling conditions in such container |
-
1989
- 1989-08-07 JP JP20503889A patent/JPH0712449B2/en not_active Expired - Lifetime
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04354549A (en) * | 1991-05-30 | 1992-12-08 | Hitachi Plant Eng & Constr Co Ltd | High voltage power supply for electrostatic precipitator |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0712449B2 (en) | 1995-02-15 |
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