JPS58260A - Electric precipitation of dust - Google Patents
Electric precipitation of dustInfo
- Publication number
- JPS58260A JPS58260A JP9775881A JP9775881A JPS58260A JP S58260 A JPS58260 A JP S58260A JP 9775881 A JP9775881 A JP 9775881A JP 9775881 A JP9775881 A JP 9775881A JP S58260 A JPS58260 A JP S58260A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- dust
- thyristor
- charging method
- current
- 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
Links
- 239000000428 dust Substances 0.000 title claims abstract description 40
- 238000001556 precipitation Methods 0.000 title 1
- 239000012717 electrostatic precipitator Substances 0.000 claims description 10
- 238000000034 method Methods 0.000 abstract description 14
- 238000010304 firing Methods 0.000 abstract description 13
- 238000010586 diagram Methods 0.000 description 14
- 230000003247 decreasing effect Effects 0.000 description 2
- 239000012716 precipitator Substances 0.000 description 2
- 230000005611 electricity Effects 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
Landscapes
- Electrostatic Separation (AREA)
Abstract
Description
【発明の詳細な説明】
氷見1iFi電気集塵装置に関する。仁の覆装置として
従来使用されてbるサイリスク制御方式のものは、第1
図回路図に示すよ5に、商用周波数の入力電圧、電流を
サイリスタ8c凰により制御し、高圧トランスMTにて
昇圧したのち、J115!I1gcrにより直流化し、
これを集塵電極EPK印加し、/fルス発生−PIGの
出方にょルサイリスタ8CRを制御するのであるが、従
来〇制御方式で鉱、印加電圧、電流の波形コントロール
φに隈lLがあ)、特に高抵抗ダストの捕集に対して十
分かつ有効な#Ls制御がで禽な込とiう欠点がある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to Himi 1iFi electrostatic precipitator. The type of cyrisk control method conventionally used as a cylindrical overturning device is the first one.
As shown in the circuit diagram in Figure 5, the input voltage and current of the commercial frequency are controlled by the thyristor 8c, and after being boosted by the high voltage transformer MT, J115! Convert to DC using I1gcr,
This is applied to the dust collecting electrode EPK to control the thyristor 8CR according to the output of /f pulse generation-PIG, but in the conventional control method, there is a shadow on the waveform control φ of the applied voltage and current) However, there is a drawback that sufficient and effective #Ls control is not possible, especially for collecting high-resistance dust.
氷見q4紘ζOような事情に鎌みて提案されたもので、
il&抵抗〆ストに対しても集塵効率を改善し、消費電
力を極少くする電気集塵装置を提供することを目的とし
、−次側の商用周波数電源を変圧−、ナイシスタ等電流
制御畳嵩を介して二次側0101高電圧に変換し、これ
を集塵電極に印加し集塵するようにし良電気集塵装置に
おいて、上記−次側に電圧1p1111器又紘可変りア
クタを挿入しこれによって上記二次側出力波形を制御す
ることを41111とする。Himiq4HiroζOIt was proposed in light of the situation,
The purpose is to provide an electrostatic precipitator that improves dust collection efficiency and minimizes power consumption even for IL and resistance strikes. Convert it to a secondary side 0101 high voltage through the secondary side and apply it to the dust collecting electrode to collect dust. It is assumed that 41111 controls the secondary side output waveform by.
氷見−0II施例をINNKついて説明すると、菖2図
紘そO嬉1実總例を示す回路図、第3因囚、OI紘それ
ヤれ菖2図O各部の出力波形図で、同図(2)線電圧調
整−の出力電圧が比較的小さい場合、同mol)a岡出
力電圧が比較的大きい場合をそれぞれ示す、菖4図およ
び第5図はそれぞれjII実施例による集塵効率および
消費電力をそれぞれ示す!1図、516図は本発明の第
211!111例を示すプロ、りgrip、第7!l[
tOgljl!K、第8図囚、(B)はそれぞれ票7図
の一次電圧および電流の波形図で、同図(4)Fi9ア
クタのインダクタンスが比較的大きi場合、同図φ)は
同リアクタのインダクタンスが比較的小さい場合をそれ
ぞれ示す、鎮9図は第715!gの萬圧変圧器の二次電
゛圧、二次電流の関係を示す線図、*1os(4)、俤
)はそれぞれ−次電圧が60Hgの場合の二次電流の波
形図で、同@IcA)はリアクタのインダクタンスが比
較的大きい場合、四図俤)はリアクタのインダクタンス
が比較的小さい場合をそれぞれ示す。To explain the Himi-0II example in terms of INNK, the circuit diagram showing the actual example of Iris 2, the output waveform diagram of each part of the third cause, and the output waveform diagram of each part. (2) When the output voltage of line voltage adjustment is relatively small, the same mol) Figures 4 and 5 show the case where the output voltage of aoka is relatively large, respectively. Indicate the power of each! Figures 1 and 516 show the 211th!111th example of the present invention, the grip, and the 7th! l[
tOgljl! K, Fig. 8, and (B) are the waveform diagrams of the primary voltage and current in Fig. 7, respectively, and (4) in the same figure, when the inductance of the Fi9 actor is relatively large i, the figure φ) is the inductance of the same reactor. Figure 9 shows the cases in which is relatively small. The diagram showing the relationship between the secondary voltage and secondary current of the multi-voltage transformer in g, *1os(4), 俤) is the waveform diagram of the secondary current when the secondary voltage is 60Hg, and the same @IcA) shows the case where the inductance of the reactor is relatively large, and Figure 4) shows the case where the inductance of the reactor is relatively small.
まず、菖2囚の菖l実施例において、1紘hczzov
thco 〜zsovtcllfiするスライダ、り8
D、2はノfルス発生4!ISからの出力信号によシ点
弧角を0〜180@変化するサイリスタ、4はサイリス
タ2で制御された一次電圧50vを二次電圧V、 K昇
圧する高圧トランス、j#i隈流リアすタ、Cは電圧v
2を直流に変換して直流荷電電圧v1.を出力する整流
器、7は集塵電極]cP″eあ為。First, in the example of Iris 2 prisoners, 1 hczzov
thco~zsovtcllfi slider, ri8
D, 2 is Nofrus occurrence 4! Thyristor that changes the firing angle from 0 to 180@ according to the output signal from IS, 4 is a high voltage transformer that boosts the primary voltage 50V controlled by thyristor 2 to secondary voltage V, K, ta, C is the voltage v
2 to DC to obtain a DC charging voltage v1. 7 is a dust collection electrode]cP″eAme.
このような装置において、−次側電圧と、二次側すなわ
ち罵P印加電圧、電流波形の関係を負荷電aX、X一定
O東件のもとに説明する。In such a device, the relationship between the negative side voltage, the secondary side, that is, the applied voltage, and the current waveform will be explained based on the condition that the load voltages aX and X are constant.
まず、中スライダ、りSDを絞り、その出力電圧v1B
を小にすると、jlIa図(4)に示すように、サイリ
スタlIcl0点弧角αが小にな夛、すなわち導通角β
が大になル、IP印加電圧v2.Fi同図(至)破線G
K示すように、滑らかになる。First, reduce the middle slider and SD, and its output voltage v1B
When jlIa is made small, the firing angle α of thyristor lIcl0 becomes small, that is, the conduction angle β
is large, IP applied voltage v2. Fi same figure (to) broken line G
K becomes smooth as shown.
次に、ODスライダ、り8Dの出力電圧v1mを大とす
ると、嶌cmの点弧角αが大となシ、すなわち導通角β
が小となj)1EP印加電圧v2.の8−alIOIi
l!Iで紘一様な電力供給を行ない、1011〜t01
1Ω−5110範囲で紘ダストの逆電離防止のために間
欠的な=ロナ放電つまシ関欠荷電が有効であることが数
多O試験によ〕実証されているので、集塵容易なダスト
に対しては集塵電極EPには上記中に述べた荷電方法を
、逆電離斃生によp集塵困難なダス)K対しては上記(
滲に述べた間欠荷電方法をそれヤれ適用する。Next, if the output voltage v1m of the OD slider 8D is increased, the firing angle α of the cylinder cm becomes large, that is, the conduction angle β
is small j) 1EP applied voltage v2. 8-alIOIi
l! 1011 to t01
It has been proven through numerous O tests that intermittent RONA discharge is effective for preventing reverse ionization of RONA dust in the 1Ω-5110 range, so it is suitable for dust that is easy to collect. For the dust collection electrode EP, the charging method described above is used, and for the dust collecting electrode EP, the charging method described above is used, and for the dust collecting electrode EP, the charging method described above is applied, and for the dust collecting electrode EP,
The intermittent charging method described in detail is then applied.
そうすれば、集塵効率り消費電力を一定とすると、縞4
図に示すように、βd−10〜101sΩ−国のダスト
に対し、従来の一次電圧50v。In this way, assuming that the dust collection efficiency and power consumption are constant, the stripes 4
As shown in the figure, the conventional primary voltage 50v for βd-10~101sΩ-country dust.
801点弧角60°の荷電方式の場合aP点であるが、
本装置で一次電圧80V、8C凰点弧角135@とする
と、火花電圧および電流のピーク値X、。801 In the case of the charging method with a firing angle of 60°, it is the aP point,
In this device, if the primary voltage is 80V and the firing angle is 135@, the peak value of the spark voltage and current is X.
が□大巾に上昇するので、カーブPP′に示すように、
集塵効皐紘10〜2〇−向上し、鵞九消費電力は集塵効
率一定で比較すると、菖5WiAに示すように1従来の
一次電圧65 V 、 8CR点弧角60°の荷電方式
の場合社P点であるが、本装置では一次電圧65 V
、 801点弧角135@とすると、カーブPP’に示
すように、10〜60%低減される。□ rises sharply, so as shown in curve PP',
The dust collection efficiency is improved by 10 to 20 degrees, and the power consumption is compared with the same dust collection efficiency as shown in 5 WiA. In this case, the primary voltage is 65 V.
, 801 and a firing angle of 135@, it is reduced by 10 to 60%, as shown by curve PP'.
ただし、上記実施例において、sDの出力電圧v、1お
よび8CRの点弧角αは集塵電@EP(1各110V/
1%性および集塵電極出口に付設された媒塵モエIO出
力信4#により制御する。However, in the above embodiment, the output voltage v of sD and the firing angle α of 1 and 8CR are
It is controlled by the 1% rate and the dust moe IO output signal 4# attached to the dust collection electrode outlet.
次に、llN611O菖811施例において、21はサ
イリスタ制御−811によ〕制御されるサイリス−11
2紘リアクタ制御回路1aKよ)制、御される可変リア
クタ、JJl’i高圧変圧器、14紘豊流器、2−拡電
気集塵器、2rは媒塵鎖度針、28紘リアクタ制御回路
である。Next, in the llN611O iris 811 embodiment, 21 is the thyristor-11 controlled by the thyristor control-811.
2 Hiro reactor control circuit 1aK) Controlled variable reactor, JJl'i high voltage transformer, 14 Hiro flow generator, 2-expansion electrostatic precipitator, 2r is the medium dust chain gauge, 28 Hiro reactor control circuit It is.
このような装置において、サイリスタ制御回路2Iは、
火花検出器、V/Iと媒塵11f計2rから0フイ一ド
バツク信号により可変リアクタ22の値を自動的に変え
てダス)O性状に応じ九最適技形荷電を行なうφ
すなわち、低抵抗ダストで媒塵濃度が多いとき線、後記
するよ5に、可変リアクタ22を調整してサイリスタの
点弧角αを小にし導通角βを大とし、電me供給時間お
よび量を増加し、電圧の上限り電、夕紘火花検出器によ
って行なう・
オ九JKダストの抵抗値が高く、逆電離が発生すゐと龜
は、これを1x7ivの関係から検出し、集塵器出口に
付設された媒塵a度計21が設魔値より多くなった場合
に#i、、可変リアター11を減少しでサイリスタの点
弧角aを大にし導通角βを小tcL、供給時開の短い魚
唆な/fルス状の電流を供給することKよ)ダストの逆
電離をll脅することなしに十分な電流を供給する仁と
ができる。In such a device, the thyristor control circuit 2I is
The value of the variable reactor 22 is automatically changed by the spark detector, V/I and dust 11f meter 2r, and the value of the variable reactor 22 is automatically changed according to the feedback signal from the dust 11f. When the dust concentration is high, the variable reactor 22 is adjusted to reduce the firing angle α of the thyristor and increase the conduction angle β, increasing the electric current supply time and amount, and increasing the voltage. The resistance of the JK dust is high and reverse ionization occurs, which is detected by the 1x7iv relationship and detected by the medium attached to the precipitator outlet. When the dust a degree meter 21 exceeds the design value #i, the variable reactor 11 is decreased, the firing angle a of the thyristor is increased, the conduction angle β is decreased tcL, and the opening angle during supply is short. It is possible to supply a sufficient current without threatening back ionization of the dust.
薦7頻において、端子A−1閲に商用屑鋏緻電源を印加
すると、サイリスタ制御−mxxからの点弧位相角信号
にょシナイリスタ11が点弧し、−次回路に電fiI、
が流れ、可変リアクー220両端および高圧変圧@22
の一次負にそれすれ
VL−Z c・l。When a commercial power source is applied to the terminal A-1 in the 7th cycle, the ignition phase angle signal from the thyristor control mxx causes the ignition ristor 11 to ignite, and the next circuit receives electricity fiI,
flows, both ends of variable rear cooler 220 and high voltage transformer @22
VL-Z c・l.
VT−Z、・l。VT-Z,・l.
が発生する。occurs.
電流X1紘ナイリスタ210点弧位相角によって制御さ
れ、C−0間の電圧V、は
■、=vL十v?
とな〕、可変97タタ270大小とV、0波形0属係紘
それぞれgssa(A、(至)K示すようKなり、高圧
変圧@18011E@容量を十分に大きくとっテオケば
、1Ii9■に示すよ5に、サイリスタ21位相角位椙
角が小さくなって4、集塵電極2σに#i十分に電圧、
電流を供給することができる。The current X1 is controlled by the firing phase angle of the KONAI RISTOR 210, and the voltage V between C-0 is ■, = vL 10v? ], variable 97 tata 270 magnitude and V, 0 waveform 0 gen hilo respectively gssa (A, (to) K as shown, high voltage transformer @18011E@ capacity is set sufficiently large, as shown in 1Ii9■ 5, the phase angle of the thyristor 21 becomes smaller, and #i is applied to the dust collecting electrode 2σ sufficiently.
Can supply current.
し良がりて^圧変圧器230二次側の電圧電gas紘j
110■に)、(2)に示すよりに、可変リアクタ73
0インダタタンスが小さい場合、電流の時間中O狭い、
かつピーク値の高い、いわゆる急峻な電#l腋廖となる
。I'm glad ^ voltage transformer 230 secondary side voltage gas hiroj
110■), as shown in (2), the variable reactor 73
If the 0 inductance is small, the current is narrow during the time,
Moreover, the peak value is high, resulting in a so-called steep electric curve.
この特性を有用して、可変リアクタ21を調整し、従来
の連続的荷電に代えて間欠的に短時間中0@流を流すこ
とによ)逆電離の発生を抑制し、ma皐10 Ω−tx
s)jJ、上の高抵抗/ストに至るまでのナベでO〆ダ
スト高収皐で捕集することかで龜る。Taking advantage of this characteristic, the occurrence of back ionization can be suppressed by adjusting the variable reactor 21 and passing a 0@ current intermittently for a short time instead of the conventional continuous charging. tx
s) JJ, the high resistance/strike above can be achieved by collecting the dust with a high collection rate.
このよう和して、集塵器の出口に付設した媒應IaR計
O出力114#を荷電制御信号と組合せ、可変リアクタ
ンスのインダクタンスおよびサイリスタ点弧位相角を制
御することKより二次側電圧波形を調整し、少ない消費
電力で所llO集塵効率を得ることができる。In this way, the output 114# of the medium IaR meter attached to the outlet of the precipitator is combined with the charge control signal to control the inductance of the variable reactance and the thyristor firing phase angle. can be adjusted to obtain a desired 110 dust collection efficiency with less power consumption.
以上述べた実施例において、集塵電極に略0.01〜i
sO周期で略0.O1〜1麿のノ臂ルス巾の直流高電圧
を印加し、ダストが逆電層を生起する前に電流を遮断す
ることによシ、高抵抗率のダス)0収應効率をも鳥める
ことかで龜る。In the embodiments described above, approximately 0.01 to i
Approximately 0 in sO period. By applying a DC high voltage with the arm width of O1 to 1 and cutting off the current before the dust generates a reverse electric layer, the dust with high resistivity can be reduced to zero sintering efficiency. It's cloudy because of things.
なお上記実施例において鉱、本発明を間欠荷電方式に適
用した場合について述べたが、本発明0@1実施例の4
のく限定することなく、例えば連続荷電方式に適用して
もよく、さらに連続荷電方式と間欠荷電方式とを適宜切
換えるようKし良電気集塵41にも適用し得ること勿論
である。In the above embodiment, the case where the present invention is applied to an intermittent charging method has been described, but the present invention 0@1 embodiment 4
It goes without saying that the present invention is not limited to the above, and may be applied to, for example, a continuous charging method, and may also be applied to the electrostatic precipitator 41 in which the continuous charging method and the intermittent charging method are appropriately switched.
要するに本発明によれば一次側の商用局a数電源を変圧
器、サイリスタ等電流制御要素を介して二次側の直流高
電圧に変換し、これを集塵電極に印加し集塵するよう処
した電気集塵装置Km−いて、上記−次側に電圧調整器
又は可ffi +77クタを挿入しこれKよりて上記二
次側出力波形を制御することによ)、集塵効率および消
費電力の歇善を8番電気集塵装置を得るから、本 、発
IjI紘麿業上極めて有益なものである。In short, according to the present invention, the primary side commercial station power source is converted to a secondary side DC high voltage through current control elements such as transformers and thyristors, and this is applied to the dust collecting electrode to collect dust. The dust collection efficiency and power consumption can be improved by inserting a voltage regulator or a variable voltage regulator into the downstream side of the electrostatic precipitator K and controlling the output waveform of the secondary side. This book is extremely useful for the IjI Hiromaru business, since it is a good idea to get a No. 8 electrostatic precipitator.
本図面の匍単tag
@1aid公IaO関久荷電方式の電気集塵装置を示す
回路図 am図は本発明0@1実施例を示す回路図、菖
31m囚、俤)絋それぞれ菖2図の各ll5O出力波形
図で、同図(4)は電圧調整器の出力電圧が比較的小i
5−場合、同図俤)は同出力電圧が比軟的大きい場合を
それぞれ示す6314図およびllI45図はそれぞれ
本第1実施例による集塵効率および消費電力をそれぞれ
示す線図、菖SSa氷見@0aI2実施例を示すプロ、
り線図、菖7図唸そOa路図、菖8図(4)、俤)はそ
れぞれ票6図〇−次電圧および電流の波形図で、同図(
2)はりアクIが比軟的大きい場合、同図φ)は同リア
クタが比較的小さい場合を十れぞれ示す。This drawing is a circuit diagram showing an electrostatic precipitator using a charging method. In each ll5O output waveform diagram, (4) shows that the output voltage of the voltage regulator is relatively small i.
Figures 6314 and 1145 are diagrams respectively showing the dust collection efficiency and power consumption according to the first embodiment. Pro showing 0aI2 example,
Figure 6 (4), 迤) are the voltage and current waveform diagrams of Figure 6, respectively.
2) When the beam ac I is relatively large, φ) in the figure shows the case where the reactor is relatively small.
纂9WAa菖1図O^圧変圧器の二次電圧、二次電流の
関係を示す線図、第10図(4)、俤)紘それぞれ一次
電圧が一〇 Hs O場合の二次電流の鉄形図で、同w
A(2)はリアタIが比較的大きい場合、岡11@a9
アタタが比較的小さい場合をそれぞれ示す。Diagram showing the relationship between the secondary voltage and secondary current of an O^ voltage transformer, Fig. 10 (4), 俤)Hiro Each secondary current when the primary voltage is 10 Hs O In the shape diagram, the same w
A(2) is Oka 11@a9 when Reata I is relatively large.
The cases where the atata is relatively small are shown respectively.
1・・・スライダ、り8D% 2・・・サイリスタ、S
・・・/4ルス発生器、4−・・高圧トランスMT1j
・・・@流すアクタ、#−11111% F−・・集應
電極EP。1...Slider, 8D% 2...Thyristor, S
.../4 Lux generator, 4-...High voltage transformer MT1j
...@Flowing Actor, #-11111% F-... Collection electrode EP.
11・・・ずイリスタ、22−・・可変リアクタ\ 2
J・・・蟲圧変圧−114”−!111m、 J J・
・・サイリスク制御■路、1#−電気集塵器、21・・
・媒塵貴度針、Za−・・リアクタ制御回路、α・・・
点弧(位相)角、l−・導通角、#4・・・ダストの電
気抵抗率、L・・・可変リアクタのインダクタンス拳出
願人復代堰人 弁1士 鈴 江 武 薩1113図
(A) (B)
lL、zJL″′″″を
第5図
一5ffl^β」劃11... Zuiristar, 22-... Variable reactor \ 2
J...Mushi pressure transformation-114"-!111m, J J.
・・Sirisk control ■Route, 1#-electrostatic precipitator, 21・・
・Dust purity needle, Za-...Reactor control circuit, α...
Ignition (phase) angle, L-・Conduction angle, #4...Electrical resistivity of dust, L...Inductance of variable reactor Applicant Fukudai Weirjin Ben 1st Master Suzue Takeshi Satsuma 1113 Diagram (A) ) (B) lL, zJL″′″″ in Figure 5-5ffl^β”
Claims (1)
等電流制御要素を介して二次儒omm*電圧に変換し、
これを集塵電極に印加し集塵するよう処し良電気集塵装
置Kj?いて、上記−次側に電圧調叢器又は可変リアク
Iを挿入しこれによって上記二次側出方波形を制御する
ことを4111とする電気集塵装置。- Convert the next commercial frequency power supply to a secondary voltage through a current control element such as a transformer or thyristor,
Apply this to the dust collecting electrode and collect the dust using a good electrostatic precipitator Kj? 4111. An electrostatic precipitator comprising: inserting a voltage regulator or a variable reactor I on the secondary side, and controlling the output waveform on the secondary side thereby.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9775881A JPS58260A (en) | 1981-06-24 | 1981-06-24 | Electric precipitation of dust |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9775881A JPS58260A (en) | 1981-06-24 | 1981-06-24 | Electric precipitation of dust |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58260A true JPS58260A (en) | 1983-01-05 |
Family
ID=14200772
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9775881A Pending JPS58260A (en) | 1981-06-24 | 1981-06-24 | Electric precipitation of dust |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58260A (en) |
-
1981
- 1981-06-24 JP JP9775881A patent/JPS58260A/en active Pending
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