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JPS5822253B2 - electrostatic filter - Google Patents
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JPS5822253B2 - electrostatic filter - Google Patents

electrostatic filter

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Publication number
JPS5822253B2
JPS5822253B2 JP52118646A JP11864677A JPS5822253B2 JP S5822253 B2 JPS5822253 B2 JP S5822253B2 JP 52118646 A JP52118646 A JP 52118646A JP 11864677 A JP11864677 A JP 11864677A JP S5822253 B2 JPS5822253 B2 JP S5822253B2
Authority
JP
Japan
Prior art keywords
dust
dielectric
discharge
electrode
multipolar
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.)
Expired
Application number
JP52118646A
Other languages
Japanese (ja)
Other versions
JPS5452374A (en
Inventor
神田哲郎
田中昌司
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.)
Chiyoda Corp
Original Assignee
Chiyoda Chemical Engineering and Construction 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 Chiyoda Chemical Engineering and Construction Co Ltd filed Critical Chiyoda Chemical Engineering and Construction Co Ltd
Priority to JP52118646A priority Critical patent/JPS5822253B2/en
Priority to DE19782842718 priority patent/DE2842718A1/en
Publication of JPS5452374A publication Critical patent/JPS5452374A/en
Publication of JPS5822253B2 publication Critical patent/JPS5822253B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は含塵ガスからダストを連続的に除去する静電フ
ィルターに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrostatic filter that continuously removes dust from dust-containing gas.

更に詳しくは、電極間に誘電体を充填し、該電極に電圧
を印加しつつ誘電体の空隙に含塵ガスを流し含塵ガス中
のダストを誘電体に付着させてダストを除去する静電フ
ィルターに関する。
More specifically, it is an electrostatic method in which a dielectric material is filled between electrodes, and while a voltage is applied to the electrodes, a dust-containing gas is flowed into the gap in the dielectric material, causing the dust in the dust-containing gas to adhere to the dielectric material and removing the dust. Regarding filters.

従来から、電圧を印加した誘電体間に含塵ガスを通過さ
せて集塵するいわゆる静電フィルターとして、静電気力
によってダストを誘電体に集める形式のもの、あるいは
含塵ガスを誘電体中を通す前ニ、ダストをコロナ放電に
よって荷電して行う形式のもの等が広く使用されている
Conventionally, so-called electrostatic filters collect dust by passing dust-containing gas between dielectrics to which a voltage is applied, and there are filters that collect dust on the dielectric by electrostatic force, or filters that collect dust by passing dust-containing gas through the dielectric. 2) A method in which dust is charged by corona discharge is widely used.

第1図は従来用いられている方式の1例を示しだもので
あるが、これを従来法の代表例として説明する。
FIG. 1 shows an example of a conventionally used method, and this will be explained as a representative example of the conventional method.

図において含塵ガスは矢印方向に流れ、その間に放電極
4と接地電極5との間に形成されたコロナ放電によって
ダストが荷電された後、高電圧電極1と接地電極2の間
の誘電体3の空隙を通過する間に電界によるクーロン力
によってダストは誘電体3に集められ除塵される。
In the figure, the dust-containing gas flows in the direction of the arrow, and after the dust is charged by the corona discharge formed between the discharge electrode 4 and the ground electrode 5, the dust is charged by the dielectric between the high voltage electrode 1 and the ground electrode 2. While passing through the gap 3, the dust is collected on the dielectric 3 by the Coulomb force caused by the electric field and removed.

この方法に於ては、高電圧電極1に印加する電圧はでき
るだけ高い方が誘電体3の空隙の電界が強くなり、除塵
効率は向上するが、あまり電圧を高くするとスパークと
なり誘電体3を変質まだは燃焼させること、および電流
が安定的に流れず制御が極めてむづかしいという欠点が
ある。
In this method, the higher the voltage applied to the high-voltage electrode 1, the stronger the electric field in the gap in the dielectric 3 and the better the dust removal efficiency, but if the voltage is too high, sparks will occur and the dielectric 3 will be altered. However, it still has disadvantages in that it requires combustion, and that the current does not flow stably and is extremely difficult to control.

また誘電体3に粒状物を用いた場合には、粒状物表面に
集められたダストが、粒状物の移動等によって再び飛散
し、排ガスと共にフィルターの外に排出され、集塵効率
の著しい低下を来ることとなる。
In addition, when particulate matter is used for the dielectric material 3, the dust collected on the surface of the particulate matter will be scattered again due to the movement of the particulate matter, and will be discharged to the outside of the filter together with the exhaust gas, resulting in a significant decrease in dust collection efficiency. It will come.

発明者らは、粒状誘導体を電極間に充填して電極間に高
電圧を印加したところ、誘電体の性質によっては、誘電
体そのものよりも空隙の電界の方が強くなり誘電体を電
極とする多極放電が空隙に発生し、もし空隙にダスト等
が存在すると効率よく荷電される事実を知見し、しかも
このようにして荷電されたダストが粒状誘電体表面に集
積されることから、これを有効に組合せ新規な装置の開
発をみたものである。
The inventors filled the space between electrodes with a granular dielectric and applied a high voltage between the electrodes. Depending on the properties of the dielectric, the electric field in the gap was stronger than that in the dielectric itself, making the dielectric the electrode. We discovered that multipolar discharge occurs in the voids, and that if there is dust, etc. in the voids, the voids are efficiently charged, and that the dust charged in this way is accumulated on the surface of the granular dielectric material. It looks at the development of new devices that can be effectively combined.

この方法の特徴はダストに対する荷電と集塵が同じ場所
で行われることであり、しかも誘電体に粒状のいわゆる
電気絶縁物を用いることにより誘電体が電極となって多
極放電が発生し効率よい荷電が行われることである。
The feature of this method is that dust charging and dust collection are performed at the same place, and by using granular so-called electrical insulators for the dielectric, the dielectric becomes an electrode and multipolar discharge occurs, making it efficient. This means that charging is performed.

更にこの粒状誘電体を移動して循環使用すれば、粒状誘
電体上に集められたダストは大量にならないうちに回収
される。
Furthermore, if this granular dielectric material is moved and used for circulation, the dust collected on the granular dielectric material can be recovered before it becomes a large amount.

その際、誘電体上に集められたダストが何等かの原因で
飛散しても、直ちに多極放電のイオンシャワーによって
荷電せしめられ、再び誘電体上に捕捉されることとなる
At this time, even if the dust collected on the dielectric material is scattered for some reason, it will be immediately charged by the ion shower of the multipolar discharge and will be captured on the dielectric material again.

本発明の装置で最も重要な条件は、粒状誘電体のもつ見
掛けの電気抵抗にある。
The most important condition for the device of the present invention is the apparent electrical resistance of the granular dielectric.

ここで見掛けの電気抵抗とは、一定の容器内に特に加圧
することなく粒子を充填しその両端から一定電流を流し
だときの、充填体としての抵抗を意味する。
The apparent electrical resistance here refers to the resistance of the filled body when particles are filled into a container without any particular pressure applied and a constant current is passed from both ends of the container.

見掛けの抵抗は、充填体のもつ体積固有抵抗のほか充填
された時の見掛けの密度、粒子の相互の接触状態、雰囲
気の状態、例えば温度、湿度、ガスの性状、付着ダスト
の量及び性状等によって変化する。
The apparent resistance is determined by the volume resistivity of the filling body, the apparent density when the body is filled, the state of contact between particles, the state of the atmosphere, such as temperature, humidity, gas properties, amount and properties of attached dust, etc. It changes depending on.

誘電体は常温における体積固有抵抗が101゜Ω−cm
以上の絶縁体、例えば砂利、磁器、ガラス玉、アルミナ
粒等からなる粒子であり、その形状は球9円筒、不定形
等特に制限はない。
The dielectric has a volume resistivity of 101゜Ω-cm at room temperature.
These particles are made of the above-mentioned insulators, such as gravel, porcelain, glass beads, alumina particles, etc., and their shape is not particularly limited, such as spheres, cylinders, irregular shapes, etc.

このような粒状誘電体を充填して見掛けの電気抵抗が5
×108Ω−cmDL上で高電圧を印加すると分極作用
によって粒状誘電体よりも空隙の電界が強くなり、粒状
誘電体を電極とする多極放電が粒状誘電体の空隙に発生
する 粒状誘電体の体積固有抵抗が小さい場合には、電流が粒
状誘電体の内部を流れ、また固有抵抗が大きくとも見掛
けの抵抗が小さい場合には電流が粒子の表面を流れるた
め高電圧を印加することができず、粒状誘電体の空隙の
電界も強くなり得な、いので多極放電を起すことができ
ない。
When filled with such granular dielectric material, the apparent electrical resistance is 5.
×108Ω-cm When a high voltage is applied on the DL, the electric field in the gap becomes stronger than that in the granular dielectric due to the polarization effect, and a multipolar discharge using the granular dielectric as an electrode occurs in the gap in the granular dielectric.The volume of the granular dielectric If the specific resistance is small, current will flow inside the granular dielectric, and even if the specific resistance is large, if the apparent resistance is small, the current will flow on the surface of the particles, so a high voltage cannot be applied. The electric field in the gaps in the granular dielectric cannot become strong, so multipolar discharge cannot occur.

見掛けの電気抵抗が小さい場合でも大電流を流せば多極
放電を形成することができるが、経済的でない。
Even if the apparent electrical resistance is small, it is possible to form a multipolar discharge by flowing a large current, but this is not economical.

このため見掛けの電気抵抗が5×1080−cm以上で
あることが本発明の条件となる。
Therefore, it is a condition of the present invention that the apparent electrical resistance is 5 x 1080-cm or more.

、見掛けの電気抵抗を支配する因子の1つに充填
する誘電体の有する固有の性質に起因するものがある。
One of the factors governing the apparent electrical resistance is due to the inherent properties of the dielectric material.

即ち誘電体の体積固有抵抗ならびに形状がそれである。In other words, it is the volume resistivity and shape of the dielectric.

本発明の目的に使用(〜得る誘電体はその体積間4有抵
抗が1010Ω−m以上の、いわゆる絶縁体でその形状
は直径1〜10mの小粒体が特に望捷しい。
The dielectric material used for the purpose of the present invention is a so-called insulator having a volume resistivity of 1010 Ω-m or more, and is particularly preferably in the form of small particles with a diameter of 1 to 10 m.

絶縁体の体積固有抵抗は常温に於てガラス:〉1013
.硫黄:1016〜1017.長石磁器:1013〜1
014.ステアタイト:10”〜1012酸化チタン:
)io14Ω−cmの夫々の値を示し、それらの値は何
れも温度が上昇するに従って低下オる。
The volume resistivity of the insulator is glass at room temperature: 〉1013
.. Sulfur: 1016-1017. Feldspar porcelain: 1013-1
014. Steatite: 10”~1012 Titanium oxide:
)io14Ω-cm, and all of these values decrease as the temperature increases.

まだ物質固有の電気抵抗には、電流が物質の表面を流れ
るときの表面固有抵抗があるがその値はガス中の水分量
及び付着ダストの電気抵抗によって大きく変化する。
Among the electrical resistances inherent to materials, there is a surface resistivity when a current flows through the surface of the material, but its value varies greatly depending on the amount of water in the gas and the electrical resistance of attached dust.

したがって温度が低く、水分量の多いガスから除塵する
場合は、水分が誘電体表面に付着して電気抵抗を小さく
するのでガスの温度を上げる処置がとられ、カーボン等
の導電性物質の多いダストの場合にはダストが誘電体表
面に付着して電気抵抗を小さくするので付着ダスト除去
Ωため粒状誘電体を循環する速度を速くして電気抵抗を
5X]08Ω−cmJJ、上に保つ処置がとられている
Therefore, when removing dust from a gas with a low temperature and high moisture content, steps are taken to raise the temperature of the gas as the moisture adheres to the dielectric surface and reduces the electrical resistance. In this case, dust adheres to the surface of the dielectric material and reduces the electrical resistance, so in order to remove the adhering dust, the speed of circulation through the granular dielectric material is increased to keep the electrical resistance above 5X]08 Ω-cmJJ. It is being

誘電体の電気抵抗が5×108Ω−cm以上の場合、平
板−平板の電極を使用すると、多極放電が起る電圧を印
加して誘電体の空隙全体に多極放電を発生させると、放
電がスパークとなり安定した放電が得られない。
When the electrical resistance of the dielectric is 5 x 108 Ω-cm or more, if a plate-to-plate electrode is used, a voltage that causes a multipolar discharge is applied to generate a multipolar discharge throughout the gap in the dielectric, and a discharge occurs. sparks and a stable discharge cannot be obtained.

前記の条件下において安定1−だ多極放電を発生させる
だめの1つの方法は無声放電と同じように電極を絶縁体
でさえぎって交流の電圧を印加することである。
One way to generate a stable single-pole multipolar discharge under the above conditions is to block the electrodes with an insulator and apply an alternating current voltage, similar to silent discharge.

電極間が絶縁体でさえぎられているのでスパークが発生
することなく安定である。
Since the space between the electrodes is blocked by an insulator, it is stable without generating sparks.

絶縁体で電極をさえぎる手法は電極を絶縁体で被ふ(し
てもよい。
For the method of blocking the electrode with an insulator, the electrode may be covered with an insulator.

安定した多極放電を得る他の方法は、電極に電界集中部
を設は誘電体及び空隙を流れる電流密度を不均一にする
ことである。
Another method of obtaining a stable multipolar discharge is to provide an electric field concentration area in the electrodes to make the current density flowing through the dielectric and the air gap non-uniform.

すなわち電界集中部の近くの電流密度を大きくして多極
放電を発生させ、電界集中部から遠い所では電流密度を
小さくして、多極放電を発生させず、電流を誘電体内又
は表面を流すことである。
In other words, the current density near the electric field concentration area is increased to generate multipolar discharge, and the current density is decreased in areas far from the electric field concentration area to prevent multipolar discharge from occurring and to allow the current to flow in or on the dielectric surface. That's true.

電流を誘電体内又は表面を流すだめには誘電体の見かげ
電気抵抗が2X1011Ω−cm以下でなげれば十分な
多極放電を発生させることができない。
In order to allow current to flow within or on the dielectric surface, sufficient multipolar discharge cannot be generated unless the apparent electrical resistance of the dielectric is less than 2.times.10.sup.11 .OMEGA.-cm.

ダストは高電気抵抗のものも多く、電気抵抗が時間的に
変動することがあるので、ダストが付着した誘電体の見
掛けの電気抵抗を常に5X108Ω−crn以上でかつ
2X1011Ω−cmJJ、下に保つことは困難である
Dust often has high electrical resistance, and the electrical resistance may fluctuate over time, so the apparent electrical resistance of the dielectric material to which dust is attached must always be kept at 5X108Ω-crn or higher and below 2X1011Ω-cmJJ. It is difficult.

安定な多極放電を得る第3の方法は電極に電界集中部を
設は交流高周波領域を含む電圧を印加することである。
A third method for obtaining stable multipolar discharge is to provide an electric field concentration section in the electrode and apply a voltage including an AC high frequency region.

こうすることにより電界集中部近くの誘電体の空隙で多
極放電が発生し、電界集中部から遠い所では多極放電は
発生しない。
By doing this, multipolar discharge occurs in the dielectric gap near the electric field concentration area, and multipolar discharge does not occur in a place far from the electric field concentration area.

電界集中部から遠い所にある誘電体が無声放電における
絶縁体の働きをして安定な多極放電が得られる。
The dielectric material located far from the electric field concentration area acts as an insulator in silent discharge, resulting in stable multipolar discharge.

いずれの方法においても、電極が電界集中部を有してい
ることが重要であり、電界集中部近くの誘電体の空隙で
は多極放電が発生し、電界集中部から遠い所では多極放
電を発生させないようにすることが放電の安定性条件と
なる。
In either method, it is important that the electrode has an electric field concentration area, and multipolar discharge occurs in the dielectric gap near the electric field concentration area, and multipolar discharge occurs in a place far from the electric field concentration area. Preventing this from occurring is a condition for the stability of discharge.

誘電体を粒状と1−だことにより次の利点が得られる。The following advantages can be obtained by using a granular dielectric material.

すなわち粒状としたことにより空隙率が小さく、低い印
加電圧で放電させるととが可能であること、集塵極とな
る誘電体の粒子の表面積を犬きくできること、まだダス
トが付着1〜だ粒子を移動し、再生することが容易であ
ること等である。
In other words, by forming the particles into particles, the porosity is small and it is possible to discharge with a low applied voltage.The surface area of the dielectric particles that become the dust collecting electrode can be increased to a large extent. It is easy to move and play, etc.

本発明の静電フィルターの他の利点はダストへの荷電と
クーロン力によるダストの誘電体への付着を同一の機構
で行うため従来のように荷電のだめの電極と集塵のだめ
の電極を別々に設置する必要がなく構造が簡単となるこ
とにある。
Another advantage of the electrostatic filter of the present invention is that the charging of dust and the adhesion of dust to a dielectric material by Coulomb force are performed by the same mechanism, so unlike the conventional method, the electrodes for the charging reservoir and the electrode for the dust collecting reservoir are separated. There is no need for installation and the structure is simple.

次に本発明に係わる静電フィルターを図によって説明す
る。
Next, the electrostatic filter according to the present invention will be explained with reference to the drawings.

第2図において高電圧電極9は電界集中部を有する線状
あるいは針状等の電極で構成し、交流高電圧発生器11
に接続する。
In FIG. 2, the high voltage electrode 9 is composed of a linear or needle-shaped electrode having an electric field concentration part, and the AC high voltage generator 11
Connect to.

接地電極8は通気性構造にし、誘電体10を保持する構
造とする。
The ground electrode 8 has a breathable structure and has a structure that holds the dielectric 10.

含塵ガスを矢印の方向に流すと高電圧電極9の近くの誘
電体10からの多極放電によってダストが荷電され、高
電圧電極9から離れたところにある誘電体の表面に集め
られる。
When the dust-containing gas flows in the direction of the arrow, the dust is charged by multipolar discharge from the dielectric 10 near the high voltage electrode 9 and collected on the surface of the dielectric at a distance from the high voltage electrode 9.

実装置として用いる望捷しい態様としては、接地電極8
を両側に設けてその間に誘電体10を充填し、高電圧電
極9を2枚の接地電極8の中央に位置せしめる方法があ
る。
A desirable mode for use as an actual device is that the ground electrode 8
There is a method in which the high-voltage electrode 9 is placed in the center of the two ground electrodes 8 by providing them on both sides and filling the space with a dielectric 10.

このような構成にすると作業者の危険防止上望捷しいば
かりでなく、誘電体10の移動にも極めて便である。
Such a configuration is not only desirable for preventing danger to workers, but also extremely convenient for moving the dielectric 10.

更に本発明の実施の一例を図によって説明する。Furthermore, an example of implementation of the present invention will be explained with reference to the drawings.

第3図において、集塵装置は煙道12の中間に設置され
た、通気性の接地電極8および8′によって保持された
粒状誘電体10ならびに粒状誘電体10内に縦方向に張
った線を碍子13.13’で保持した高電圧電極9から
なる。
In FIG. 3, the precipitator includes a granular dielectric 10 placed in the middle of a flue 12 and supported by permeable ground electrodes 8 and 8' and a line running longitudinally within the granular dielectric 10. It consists of a high voltage electrode 9 held by an insulator 13, 13'.

高電圧電極9は交流高電圧発生器(図示せず)に接続さ
れ、交流し高周波領域を含むの高電圧が印加される。
The high voltage electrode 9 is connected to an AC high voltage generator (not shown), and an AC high voltage including a high frequency range is applied thereto.

接地電極は対向する高電圧電極9の中間にも図中vc8
″として示す様に設置する。
The ground electrode is also connected between the opposing high voltage electrodes 9 at VC8 in the figure.
``Install it as shown.

誘電体粒子は集塵装置内を移動してバルブ19から排出
されるが、その際バルブ19を調節することによりその
装置内の流下速度を変えることができる。
The dielectric particles travel through the precipitator and are discharged through the valve 19, the rate of flow of which can be varied by adjusting the valve 19.

排出された粒子は、振動節20によって粒子に付着した
ダストを除去した後、再びコンベヤー21を経て装置上
部に供給使用される。
The discharged particles are supplied to the upper part of the apparatus via the conveyor 21 again after removing dust attached to the particles by the vibration node 20.

第3図に示す装置において誘電体として4〜6門径で見
掛けの電気抵抗値が5 X 109Ω−crnの砂利を
用い、交流で30〜45KVの電圧を印加したところ接
地電極の面積当り1〜2omAJの電流が流れた。
In the apparatus shown in Fig. 3, gravel with a diameter of 4 to 6 gates and an apparent electrical resistance of 5 x 109 Ω-crn was used as the dielectric material, and when an alternating current voltage of 30 to 45 KV was applied, the difference was 1 to 1 per area of the ground electrode. A current of 2 ohmAJ flowed.

約1.0 ?/Nrn’のダストを含む排ガスを空筒速
度約40 (:rn/secで送り、前記の条件で集塵
し除塵効率99係以上を得た。
Approximately 1.0? Exhaust gas containing dust of /Nrn' was sent at a cylinder speed of about 40 (:rn/sec), and dust was collected under the above conditions to obtain a dust removal efficiency of 99 factors or higher.

この時粒子は装置内線速度50cm/Hrの循環を行っ
た。
At this time, the particles were circulated at a linear velocity of 50 cm/Hr within the apparatus.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来用いられている静電フィルターの機構の説
明図であり、第2図は本発明に係わる静電フィルターの
機構の説明図、第3図は本発明の実施の1例を示す説明
図である。 第2図ならびに第3図において8は接地電極、9は電界
集中部を有する電極ならびに10は移動可能な誘電体を
夫々表わす。
FIG. 1 is an explanatory diagram of a conventional electrostatic filter mechanism, FIG. 2 is an explanatory diagram of an electrostatic filter mechanism according to the present invention, and FIG. 3 is an illustration of an example of the implementation of the present invention. It is an explanatory diagram. In FIGS. 2 and 3, 8 represents a ground electrode, 9 represents an electrode having an electric field concentration portion, and 10 represents a movable dielectric body.

Claims (1)

【特許請求の範囲】 1 電圧を印加した通気性の電極間に充填した誘電体の
空隙に含塵ガスを通過せしめ、含塵ガスからダストを除
去する装置において、誘電体に粒状絶縁物を用い、充填
状態における見掛けの電気抵抗が5×1080−0編上
の条件で、且つ電極の少くとも一方に、電界集中部を有
する電極を用い、電極間に交流電圧を印加することによ
り誘電体の空隙に多極放電を発生させ、荷電と集塵を単
一の区域で行なうことを特徴とする静電フィルター。 2 電極の少くとも一方を絶縁体で被覆する特許請求の
範囲第1項記載の装置。
[Claims] 1. In an apparatus for removing dust from a dust-containing gas by passing a dust-containing gas through a gap in a dielectric filled between breathable electrodes to which a voltage is applied, a granular insulator is used as the dielectric. , the apparent electrical resistance in the filled state is 5 x 1080-0, and at least one electrode has an electric field concentration part, and an alternating current voltage is applied between the electrodes. An electrostatic filter that generates multipolar discharge in the air gap and performs charging and dust collection in a single area. 2. The device according to claim 1, wherein at least one of the electrodes is coated with an insulator.
JP52118646A 1977-10-04 1977-10-04 electrostatic filter Expired JPS5822253B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP52118646A JPS5822253B2 (en) 1977-10-04 1977-10-04 electrostatic filter
DE19782842718 DE2842718A1 (en) 1977-10-04 1978-09-30 Electrostatic precipitator for dust-laden gases - with granular insulating particles circulating between charged electrodes

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52118646A JPS5822253B2 (en) 1977-10-04 1977-10-04 electrostatic filter

Publications (2)

Publication Number Publication Date
JPS5452374A JPS5452374A (en) 1979-04-24
JPS5822253B2 true JPS5822253B2 (en) 1983-05-07

Family

ID=14741700

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52118646A Expired JPS5822253B2 (en) 1977-10-04 1977-10-04 electrostatic filter

Country Status (1)

Country Link
JP (1) JPS5822253B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5535916A (en) * 1978-09-06 1980-03-13 Central Res Inst Of Electric Power Ind Dust collector
JPS583655A (en) * 1981-06-27 1983-01-10 Takuma Sogo Kenkyusho:Kk Electric dust collector equipped with fluidized dust collecting layer

Also Published As

Publication number Publication date
JPS5452374A (en) 1979-04-24

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