JPS6251665B2 - - Google Patents
Info
- Publication number
- JPS6251665B2 JPS6251665B2 JP9078384A JP9078384A JPS6251665B2 JP S6251665 B2 JPS6251665 B2 JP S6251665B2 JP 9078384 A JP9078384 A JP 9078384A JP 9078384 A JP9078384 A JP 9078384A JP S6251665 B2 JPS6251665 B2 JP S6251665B2
- Authority
- JP
- Japan
- Prior art keywords
- powder
- electrode
- discharge
- ion generator
- coating
- 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
Links
- 239000012212 insulator Substances 0.000 claims description 13
- 239000000843 powder Substances 0.000 description 68
- 150000002500 ions Chemical class 0.000 description 35
- 238000000576 coating method Methods 0.000 description 26
- 239000011248 coating agent Substances 0.000 description 25
- 239000010410 layer Substances 0.000 description 23
- 230000005684 electric field Effects 0.000 description 13
- 239000003973 paint Substances 0.000 description 6
- 239000007789 gas Substances 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 239000011810 insulating material Substances 0.000 description 2
- 239000011247 coating layer Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000004880 explosion Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000011241 protective layer Substances 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B05—SPRAYING OR ATOMISING IN GENERAL; APPLYING FLUENT MATERIALS TO SURFACES, IN GENERAL
- B05B—SPRAYING APPARATUS; ATOMISING APPARATUS; NOZZLES
- B05B5/00—Electrostatic spraying apparatus; Spraying apparatus with means for charging the spray electrically; Apparatus for spraying liquids or other fluent materials by other electric means
- B05B5/16—Arrangements for supplying liquids or other fluent material
- B05B5/1691—Apparatus to be carried on or by a person or with a container fixed to the discharge device
Landscapes
- Application Of Or Painting With Fluid Materials (AREA)
- Electrostatic Spraying Apparatus (AREA)
Description
【発明の詳細な説明】
この発明は被帯電物を帯電させるための単極性
イオン発生装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a unipolar ion generator for charging an object to be charged.
従来のこの種の単極性イオン発生装置例えば静
電粉体塗装装置等に用いられる直流電圧を印加し
た針電極、線電極、刃型電極等の単極性イオン発
生装置においては、空気その他のガスによつて分
散されて塗料噴出口より噴出する粉体を、塗料噴
出口付近に設けた針あるいは刃型電極等に高い電
圧を印加して、これらの電極に発生するコロナ放
電を利用して粉体を帯電させ、且つ、これらの電
極と被塗物との間に存在する高強度電界の作用に
よつて帯電された塗料粉体を被塗物に吸引して、
被塗物面に塗着することを基本原理とするものが
大部分である。しかしながら、上記の従来行われ
ている単極性イオン発生装置は次に述べるような
原理的な大きな欠点を有し、そのために粉体の塗
着の効率が低くおさえられ、且つ、得られる粉体
層の性質が充分良好なものを得ることができない
というのが実状である。 Conventional unipolar ion generators of this type, such as needle electrodes, wire electrodes, and blade-type electrodes to which DC voltage is applied, used in electrostatic powder coating equipment, etc., do not allow air or other gases to be used. The powder thus dispersed and ejected from the paint spout is dispersed by applying a high voltage to needles or blade-shaped electrodes installed near the paint spout, and using the corona discharge generated in these electrodes to disperse the powder. and attracting the charged paint powder to the object to be coated by the action of a high-intensity electric field existing between these electrodes and the object to be coated,
Most of them are based on the basic principle of coating the surface of the object to be coated. However, the conventional unipolar ion generator described above has the following major drawbacks in principle, and as a result, the efficiency of powder application is kept low, and the resulting powder layer is The reality is that it is not possible to obtain a material with sufficiently good properties.
これらの原因は、装置に印加される電圧と、装
置から流れる放電電流との値を独立に制御するこ
とができないということである。すなわち、装置
に印加される電圧がきまれば単極性イオン発生装
置から被塗物へ流れる電流の値は一義的に決まつ
てしまう。しかるに、例えば粉体塗装に使用され
る被帯電物の粉体の電気抵抗値等の性質は、著し
く広い範囲にわたつて変化する。又、特定の塗着
粉体についてもその保存状態、あるいは作業ガス
の成分、あるいは湿度等によつてその電気抵抗の
値は著しく大きな範囲で変化する。一般的に言つ
て、電気抵抗の著しく高い粉体を厚く塗着したい
場合には、なるべく少ない放電電流で、且つ、印
加電圧はなるべく高い電圧を使用することが要求
される。これに対して、電圧抵抗が低い粉体の場
合には、電流は多く流し、且つ、印加する電圧は
比較的低い方が得られる粉体層の性質は、好まし
い緻密なものとなる。しかるに、従来型の静電粉
体塗装装置の単極性イオン発生装置においては、
大きな電流を得ようとすれば必然的に印加する電
圧は高くなり、又、電流を少なくすれば必然的に
印加する電圧は小さくなつてしまつて、著しく電
気抵抗の高い粉体、又は、電気抵抗の比較的低い
粉体の塗着を有効に行うことは実質上極めて困難
であつた。また粉体の電気抵抗が著しく高い場合
には、被塗物に塗着された粉体層における静電粉
体塗装装置の単極性イオン発生装置から飛来する
イオン電流による電圧降下のために、塗着された
粉体層の内部でいわゆる逆電離現象が起きて、こ
のために粉体層が斑点状に剥離したピンホールな
どの原因となる。この現象は塗粉層が厚くなれば
なるほどまた粉体層を流れる電流密度が大きいほ
ど起りやすい。したがつて電気抵抗が著しく大き
い塗着粉体を使用するときは、単極性イオン発生
装置より被塗物へ流す電流の値はなるべく小さく
保つことが要求される。しかるに前述の如く、単
極性イオン発生装置から被塗物へ流れる電流をコ
ロナ放電によつて得ている場合には、コロナ放電
が本来持つている性質として、放電電流が著しく
小さい場合、すなわち、コロナ放電電極が放電開
始電圧に近い場合には、放電が著しく不安定にな
り、このため従来の静電粉体塗装装置の単極性イ
オン発生装置においては、放電を安定に保とうと
すれば電流が大きくなりすぎて粉体層の塗着が悪
くなり、逆に粉体層の性質を良くするために放電
電流を少なくしようとすれば電圧が下つて電界が
弱くなるために粉体の塗着が悪くなつて粉体の層
厚も得られにくくなり、それに加うるに放電電流
が非常に不安定になるために塗装工程の管理が著
しく困難になるという欠点が見られた。 The reason for this is that the values of the voltage applied to the device and the discharge current flowing from the device cannot be independently controlled. That is, if the voltage applied to the device is determined, the value of the current flowing from the unipolar ion generator to the object to be coated is uniquely determined. However, properties such as the electrical resistance value of the powder of the charged object used in powder coating, for example, vary over a significantly wide range. Furthermore, the electrical resistance value of a particular coating powder varies within a significantly large range depending on its storage conditions, the components of the working gas, humidity, and the like. Generally speaking, when it is desired to thickly apply a powder having extremely high electrical resistance, it is required to use as little discharge current as possible and as high an applied voltage as possible. On the other hand, in the case of powder having a low voltage resistance, the properties of the resulting powder layer will be preferable and dense if a large amount of current is passed and the applied voltage is relatively low. However, in the unipolar ion generator of conventional electrostatic powder coating equipment,
If you try to obtain a large current, the applied voltage will inevitably become high, and if you reduce the current, the applied voltage will inevitably become small. It has been practically extremely difficult to effectively apply powder with a relatively low amount of powder. In addition, if the electrical resistance of the powder is extremely high, the voltage drop due to the ion current coming from the unipolar ion generator of the electrostatic powder coating equipment in the powder layer applied to the object to be coated may cause A so-called reverse ionization phenomenon occurs inside the deposited powder layer, which causes pinholes where the powder layer peels off in spots. This phenomenon is more likely to occur as the powder coating layer becomes thicker and as the current density flowing through the powder layer increases. Therefore, when using a coating powder with extremely high electrical resistance, it is necessary to keep the value of the current flowing from the unipolar ion generator to the object to be coated as small as possible. However, as mentioned above, when the current flowing from the unipolar ion generator to the object to be coated is obtained by corona discharge, the inherent property of corona discharge is that if the discharge current is extremely small, that is, corona discharge When the discharge electrode is close to the discharge start voltage, the discharge becomes extremely unstable, and for this reason, in the unipolar ion generator of conventional electrostatic powder coating equipment, if the discharge is to be kept stable, the current will be large. If the discharge current is too high, the powder layer will not adhere well, and conversely, if you try to reduce the discharge current to improve the properties of the powder layer, the voltage will drop and the electric field will become weaker, resulting in poor powder adhesion. As a result, it became difficult to obtain a powder layer thickness, and in addition, the discharge current became extremely unstable, making it extremely difficult to control the coating process.
さらに粉体を有効に荷電するために、針状電
極、線状電極、刃型電極等の非常に鋭利な形状の
放電電極を用いるために、この部分の粉体が付着
すると、その放電特性は著しく変化してしまい、
これを適切な値に常に維持するためには、塗装装
置の単極性イオン発生装置の放電電流を作業の度
に中断して、これを清掃することが要求される。
又、この粉体の放電電極への付着は、放電電極に
おける電界の集中によつて必然的に起るものであ
つて、これを本質的に防止することは原理的に不
可能である。 Furthermore, in order to effectively charge the powder, a discharge electrode with a very sharp shape such as a needle electrode, a linear electrode, or a blade-shaped electrode is used, so if the powder adheres to this part, its discharge characteristics will change. It has changed significantly,
In order to constantly maintain this at an appropriate value, it is required to interrupt the discharge current of the unipolar ion generator of the coating equipment and clean it after every operation.
Further, the adhesion of this powder to the discharge electrode inevitably occurs due to the concentration of the electric field at the discharge electrode, and it is essentially impossible to prevent this in principle.
従つて、従来の単極性イオン発生装置では、そ
の特性の変化のために度々放電電極の清掃、ある
いは、電圧の調整を行うかしなければ常に位定し
た品質の塗粉層を被塗物上に得ることは不可能で
ある。 Therefore, with conventional unipolar ion generators, due to changes in their characteristics, it is necessary to frequently clean the discharge electrode or adjust the voltage to ensure that a coated powder layer of consistent quality is always maintained on the workpiece. It is impossible to get to.
又、従来の単極性イオン発生装置においては、
粉体の荷電が充分でなく、そのために高い塗着効
率を得ることが困難である。これは、粉体の荷電
にコロナ放電を利用するために、粉体の荷電を行
う領域が限定され、この領域においては必然的に
粉体の濃度が濃くなつているので、粉体を充分に
荷電することができないためである。これを粉体
が分散した領域で粉体を荷電しようとすれば、装
置から被塗物へ流れる電流密度が大きくなつて、
これが特に粉体の電気抵抗の高い場合には、大き
な障害となつて被塗物上で粉体の塗着を阻害する
ことが起こり、また粉体の荷電効率が低くなると
いう大きな欠点があることである。なお、また著
しく抵抗の低い粉体を塗着する場合、すなわち、
金属粉を多く含む静電粉体塗料等を塗着する場合
には、単極性イオン発生装置の電極から火花が発
生しやすくなることがある。これは、塗粉爆発等
の大きな事故を招き易く従来の単極性イオン発生
装置の著しく大きい欠点である。 In addition, in the conventional unipolar ion generator,
The powder is not sufficiently charged, which makes it difficult to obtain high coating efficiency. This is because corona discharge is used to charge the powder, so the area where the powder is charged is limited, and the powder is naturally concentrated in this area, so the powder cannot be charged sufficiently. This is because it cannot be charged. If you try to charge the powder in an area where the powder is dispersed, the density of the current flowing from the device to the object will increase,
Especially when the electrical resistance of the powder is high, this can become a major hindrance and inhibit the application of the powder on the object to be coated, and also has the major disadvantage of lowering the charging efficiency of the powder. It is. Furthermore, when applying powder with extremely low resistance, that is,
When applying an electrostatic powder coating containing a large amount of metal powder, sparks may be easily generated from the electrodes of the unipolar ion generator. This is a significant drawback of conventional unipolar ion generators, as it can easily lead to major accidents such as powder explosions.
この発明は、以上に述べた如き従来の静電粉体
塗装装置等に用いられる被帯電物を帯電させるた
めの単極性イオン発生装置における種々の欠点を
悉く解決して良好な粉体層を被塗物上に塗着する
ことができ、且つ、粉体の性質に応じて所望の厚
みの粉体層を被塗物上に形成することも可能で、
得られる粉体層の性質が安定し、更に塗着の効率
が著しく高く、低抵抗粉体を塗着する場合にも火
花放電の危険を発生することが極めて優れた単極
性イオン発生装置を提供するものである。 The present invention solves all the various drawbacks of the unipolar ion generator used in the conventional electrostatic powder coating apparatus and the like for charging objects as described above, and coats a good powder layer. It is possible to apply the powder onto the object to be coated, and it is also possible to form a powder layer with a desired thickness on the object depending on the properties of the powder.
Provides a unipolar ion generator with stable properties of the resulting powder layer, extremely high coating efficiency, and extremely low risk of spark discharge even when coating low-resistance powder. It is something to do.
本発明による被帯電物を帯電させる単極性イオ
ン発生装置は、絶縁物層の表面に細い線状電極を
露出して設け、また上記絶縁物層内には前記線状
電極と対向して面状電極を埋設し、これに交流電
圧を印加するための電源を接続するようになし、
更に、この線状電極と面状電極からなる無声放電
電極対と被塗物との間に電位差を発生させるよう
にするための電源を接続するようになしたことを
特徴とするものである。 In the unipolar ion generator for charging an object according to the present invention, a thin linear electrode is exposed on the surface of an insulating layer, and a planar electrode is provided in the insulating layer opposite to the linear electrode. The electrodes are buried and a power source is connected to them to apply alternating voltage.
Furthermore, the present invention is characterized in that a power source is connected to generate a potential difference between the silent discharge electrode pair consisting of the linear electrode and the planar electrode and the object to be coated.
この発明の単極性イオン発生装置の使用状態の
一例を図面により説明すると、第3図において、
ホツパー20にためられた塗料粉体19は供給装
置15から塗装装置に入り、エジエクター16に
矢印18によつて示される如く供給される空気に
よつて気流に懸濁した状態で筒状の絶縁物3を経
て塗料噴出口0より被塗物8に向つて塗料が噴出
される。この場合塗粉吐出口0の周辺の絶縁物リ
ング2を形成せる絶縁物層の表面付近には第1図
の如く細い線よりなる線状電極1―1を露出して
設け、又その線状電極より深い所、即ち絶縁物層
内には面状電極1―2が埋設されている。この線
状電極1―1、面状電極1―2は電源9より交流
電圧が印加され、その結果、第2図の拡大詳細図
で示した如く線状電極1―1と面状電極1―2と
の間には1―1.2で示されるような交番電気力
線が形成される。この際線状電極1―1の表面を
前記電気力線の形成を妨げない様に保護層を設け
ても差支えない。この交番電気力線の数、すなわ
ち、電界強度が絶縁物リング2の表面に存在する
気体の火花電圧より強くなると、ここに無声放電
が発生し、正負のイオンが存在するようになる。
従つて第3図に於ける10に示した電源によつて
被塗物とこれらの電極との間に例えば直流電界が
形成されると、この絶縁物リングの前面に形成さ
れた交番電気力線からなる無声放電領域1―1.
2から、そこに電源10によつて形成される電界
によつて極性のきまつた単極性のイオンが絶縁物
リング2の前面より被塗物8に向つてイオン電流
として流れる。このイオン電流は、この被塗物8
と絶縁物リング2との間の空間21に浮遊する粉
体に付着して粉体を帯電させ、その結果、帯電さ
れた粉体は絶縁物リング2と被塗物8との間に形
成される電界の作用によつて被塗物8に吸引され
て、この上に塗粉層を形成する。以上に説明した
ような基本的構造を有する単極性イオン発生装置
においては、該装置の先端すなわち絶縁物リング
2より被塗物8に向つて流れるイオン電流は、絶
縁物リング2と被塗物8との間に形成される電界
の強さが一定の場合には、電源9によつて印加さ
れる交流電圧を調整することによつて絶縁物リン
グ2の前面の無声放電領域1―1.2に形成され
る無声放電の強さを強調することができるので、
これによつて絶縁物リング2と被塗物8との間に
形成される電界が一定であつても、広い範囲にわ
たつてイオン電流の強さを調整することが可能と
なる。このような関係は電源10によつて絶縁物
リング2と被塗物8との間に形成される電界の強
度がかなり広い範囲にわたつて変化しても常に成
立するので、本発明による単極性イオン発生装置
においては、塗着空間21に形成される電界強度
とは独立に、塗着空間21を流れる電流の強さを
自由に調整することが可能となる。 An example of the state of use of the unipolar ion generator of the present invention will be explained with reference to the drawings. In Fig. 3,
The paint powder 19 accumulated in the hopper 20 enters the coating device from the supply device 15, and is suspended in the air flow by the air supplied to the ejector 16 as shown by the arrow 18, and is suspended in the cylindrical insulator. 3, the paint is jetted from the paint spout 0 toward the object 8 to be coated. In this case, near the surface of the insulating layer forming the insulating ring 2 around the coating powder discharge port 0, a linear electrode 1-1 consisting of a thin wire is provided exposed as shown in FIG. A planar electrode 1-2 is buried deeper than the electrode, that is, within the insulating layer. AC voltage is applied from the power source 9 to the linear electrode 1-1 and the planar electrode 1-2, and as a result, as shown in the enlarged detailed view of FIG. 2, the linear electrode 1-1 and the planar electrode 1-2 2, alternating electric lines of force as shown by 1-1.2 are formed. At this time, a protective layer may be provided on the surface of the linear electrode 1-1 so as not to prevent the formation of the electric lines of force. When the number of these alternating electric lines of force, that is, the electric field strength, becomes stronger than the spark voltage of the gas existing on the surface of the insulator ring 2, a silent discharge occurs here, and positive and negative ions come to exist.
Therefore, when a DC electric field is formed, for example, between the object to be coated and these electrodes by the power supply shown at 10 in FIG. Silent discharge region 1-1.
2, unipolar ions with different polarities flow from the front surface of the insulator ring 2 toward the object to be coated 8 as an ion current due to the electric field formed there by the power supply 10. This ionic current is
The powder adheres to the powder floating in the space 21 between the insulator ring 2 and the insulator ring 2 and charges the powder, and as a result, the charged powder is formed between the insulator ring 2 and the object to be coated 8. The powder is attracted to the object 8 to be coated by the action of the electric field, and a coating powder layer is formed thereon. In the unipolar ion generating device having the basic structure as explained above, the ion current flowing from the tip of the device, that is, the insulating ring 2 toward the object 8 to be coated, flows between the insulating ring 2 and the object 8. If the strength of the electric field formed between the It is possible to emphasize the strength of the silent discharge formed in
This makes it possible to adjust the strength of the ionic current over a wide range even if the electric field formed between the insulator ring 2 and the object to be coated 8 is constant. Such a relationship always holds even if the strength of the electric field formed between the insulator ring 2 and the object to be coated 8 by the power supply 10 changes over a fairly wide range, so that the unipolar property according to the present invention In the ion generator, the strength of the current flowing through the coating space 21 can be freely adjusted independently of the electric field strength formed in the coating space 21.
従つて本発明による単極性イオン発生装置にお
いては、極めて高抵抗の粉体を塗着する場合に要
求される極めて強い電界強度において低い電流密
度の電流を安定に供給することも可能となり、逆
に弱い電界強度においても電源9から印加される
交流電圧の値を高くとることによつて大電流を流
すことも可能となり、あらゆる種類の静電粉体塗
着に要求される電流、電圧の条件を自由に充たす
ことが可能となる。これが本発明による単極性イ
オン発生装置の第一の特徴である。次に第2図か
ら明らかな如く線状電極と面状電極との間に形成
される電気力線1―1.2は、必ず外側に凸とな
ることは明らかである。しかもこの電気力線は、
その周期毎にその方向を変化させる。従つて、こ
の絶縁物リング2の前面に存在する帯電粉体は、
この電気力線上における交番運動による遠心力に
よつて絶縁物リング2から遠ざかる方向に反発力
を常に受けることになる。従つて絶縁物リング2
の前面においては、粉体が放電電極に付着するこ
とがなく、従つて従来のコロナ放電を利用した単
極性イオン発生装置の電極における如く、粉体の
付着によつて塗着装置の電圧電流特性が変化する
ことは全く無く、常に安定な性能を維持すること
が可能となる。これが本発明の第二番目の大きな
特徴をなすものである。 Therefore, in the unipolar ion generator according to the present invention, it is possible to stably supply a current with a low current density even in the extremely strong electric field strength required when applying powder with extremely high resistance. Even in a weak electric field strength, it is possible to flow a large current by increasing the value of the AC voltage applied from the power supply 9, and it meets the current and voltage conditions required for all types of electrostatic powder coating. It becomes possible to fill it freely. This is the first feature of the unipolar ion generator according to the present invention. Next, as is clear from FIG. 2, it is clear that the lines of electric force 1-1.2 formed between the linear electrode and the planar electrode always convex outward. Moreover, these electric lines of force are
The direction is changed every cycle. Therefore, the charged powder present on the front surface of the insulator ring 2 is
Due to the centrifugal force caused by the alternating motion on the lines of electric force, a repulsive force is always applied in the direction away from the insulator ring 2. Therefore, insulator ring 2
On the front side, powder does not adhere to the discharge electrode, and therefore, unlike the electrodes of conventional unipolar ion generators using corona discharge, the voltage-current characteristics of the coating device are affected by the powder adhesion. does not change at all, making it possible to always maintain stable performance. This is the second major feature of the present invention.
この発明は上述の如く絶縁物層の表面上に細い
線状電極を露出させ、また絶縁物層内に面状電極
を埋設させ、無声放電電極としてイオン電流を発
生させることができるので、電子複写機のドラム
のような被帯電物を帯電させるための単極性イオ
ン発生装置として好適である。 As described above, this invention exposes a thin linear electrode on the surface of an insulating layer, and also buries a planar electrode in the insulating layer to generate an ionic current as a silent discharge electrode. It is suitable as a unipolar ion generator for charging an object to be charged, such as a machine drum.
この発明は、粉体塗着の単極性イオン発生装置
において、絶縁物層の表面付近に線状電極を露出
して設け、該線状電極より深い位置に該線状電極
と対向して面状電極を設けて無声放電を発生させ
ることによつて、被塗物と単極性イオン発生装置
との間に存在する電圧と、単極性イオン発生装置
かに被塗物へ流れる放電電流とをそれぞれ独立に
調整し、且つ、塗着空間におけるイオン電流の流
れるパターンを粉体の性質・塗膜の厚さに合せて
適切に調整すことによつて塗着の効率を著しく高
め、塗膜の性質をも著しく向上させることを可能
とした。 This invention provides a powder-coated unipolar ion generator, in which a linear electrode is exposed near the surface of an insulating layer, and a planar electrode is provided at a deeper position than the linear electrode, facing the linear electrode. By providing electrodes and generating silent discharge, the voltage that exists between the object to be coated and the unipolar ion generator and the discharge current flowing from the unipolar ion generator to the object to be painted can be independently controlled. By adjusting the flow pattern of the ionic current in the coating space according to the properties of the powder and the thickness of the coating film, the efficiency of coating can be significantly increased and the properties of the coating film can be improved. It was also possible to significantly improve the
又、線状電極を絶縁物層の表面に露出して設
け、又面状電極を絶縁物層に対して前記線状電極
より深い位置に該線状電極と対向して設け、これ
らの間に交流高圧電源を設けたから、線状電極の
みを複数本並設したイオン発生装置の場合、線状
電極の間に交流高圧電源を設けるときに線状電極
相互間の距離を正確に等しくする必要があるが、
この発明の単極性イオン発生装置はそのような必
要がないので、その製造が容易である。更に、線
状電極とこれに対向する面状電極との距離を均一
にすることが容易であり、発生するイオン電流が
均一化される。 Further, a linear electrode is provided exposed on the surface of the insulating material layer, and a planar electrode is provided in a position deeper than the linear electrode in the insulating material layer and facing the linear electrode, and between these, Since an AC high-voltage power supply is provided, in the case of an ion generator in which only a plurality of linear electrodes are installed in parallel, it is necessary to precisely equalize the distance between the linear electrodes when installing the AC high-voltage power supply between the linear electrodes. Yes, but
Since the unipolar ion generator of the present invention does not require such a method, it is easy to manufacture. Furthermore, it is easy to make the distance between the linear electrode and the planar electrode facing it uniform, and the generated ionic current is made uniform.
第1図は本発明の単極性イオン発生装置の要部
を示す断面図、第2図は第1図の部分における交
番電力線の形成状態図、第3図は本発明の一使用
状態を示す縦断面図である。
1―1…線状電極、1―2…面状電極、1―
1.2…交番電力線(無声放電領域)、2…絶縁
物リング、8…被塗物、9…電源、10…電源。
FIG. 1 is a cross-sectional view showing the main parts of the unipolar ion generator of the present invention, FIG. 2 is a diagram showing the formation of an alternating power line in the portion shown in FIG. 1, and FIG. 3 is a longitudinal cross-sectional view showing one state of use of the present invention. It is a front view. 1-1... Linear electrode, 1-2... Planar electrode, 1-
1.2... Alternate power line (silent discharge area), 2... Insulator ring, 8... To be coated, 9... Power source, 10... Power source.
Claims (1)
また上記絶縁物層内に該線状電極と対向して面状
電極を埋設し、且つ線状電極と面状電極との間に
交流高圧電源を設けると共に直流高圧電源の一端
を、上記両電極の何れか一方に接続したことを特
徴とする単極性イオン発生装置。1 Providing exposed linear electrodes on the surface of the insulator layer,
Further, a planar electrode is buried in the insulating layer to face the linear electrode, and an AC high voltage power source is provided between the linear electrode and the planar electrode, and one end of the DC high voltage power source is connected to both of the electrodes. A unipolar ion generator characterized by being connected to either one of the above.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9078384A JPS60132666A (en) | 1984-05-07 | 1984-05-07 | Charge apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9078384A JPS60132666A (en) | 1984-05-07 | 1984-05-07 | Charge apparatus |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP49078221A Division JPS5945425B2 (en) | 1974-07-10 | 1974-07-10 | powder coating equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60132666A JPS60132666A (en) | 1985-07-15 |
| JPS6251665B2 true JPS6251665B2 (en) | 1987-10-30 |
Family
ID=14008193
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9078384A Granted JPS60132666A (en) | 1984-05-07 | 1984-05-07 | Charge apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60132666A (en) |
-
1984
- 1984-05-07 JP JP9078384A patent/JPS60132666A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60132666A (en) | 1985-07-15 |
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