JPS60140699A - Electric field curtain element - Google Patents
Electric field curtain elementInfo
- Publication number
- JPS60140699A JPS60140699A JP24509883A JP24509883A JPS60140699A JP S60140699 A JPS60140699 A JP S60140699A JP 24509883 A JP24509883 A JP 24509883A JP 24509883 A JP24509883 A JP 24509883A JP S60140699 A JPS60140699 A JP S60140699A
- Authority
- JP
- Japan
- Prior art keywords
- electric field
- solid dielectric
- field curtain
- curtain element
- blade body
- 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
Landscapes
- Mixers With Rotating Receptacles And Mixers With Vibration Mechanisms (AREA)
- Oxygen, Ozone, And Oxides In General (AREA)
- Elimination Of Static Electricity (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
この発明は、電界カーテン理論を応用した静電檄能を有
する電界カーテン素子に関する。詳しくには、電気力学
的、静電的、放電化学的歳能と物理化学的撹4−1ミ混
合機能とを有する電界カーテン素子に関する。
従来、電界カーテン理論に定在波交番不平等電界(単相
型)を応用した電界カーテン素子は、板状の素子でその
表面に線状の接地放電極群か、またその内部iこ板状の
高)主誘導電極か設けられ、高j王誘導電極のターミナ
ルは素子背面に設けられている。両電極の間に単相交;
AL高電圧を印加すると、線状放電極の周囲に定在波の
交番不平等電界が発生し、その作用で帯電物体を反発し
、表面への附着物を払い落す。この場合附着物は素子表
面との接触により、接触帯電し電界の作用をうける。
さらに、電圧を上げると線状放電極から強力な交流沿面
コロナ放電が発生腰豊富な正・負イオンを含むプラズマ
が形成され、すぐれたイオンシ原となる。すなわち、こ
耽に帯電物体が近づくと直ちにその電荷を中和(除電)
し、また外部電界をかけるとこのイオン源から自由に正
又は負のイ′オンを引き出して物体を荷電することかで
bる。また粉体の表面を改質して、その流動性を増し、
溶媒へのぬれを促進する。更に、この放電発生に伴い強
力なオゾンが生ずるので、これをオゾン発生装置として
利用する二とも出来、更には殺菌、脱臭、反応促進、燃
焼促進、脱硫、脱硝にも利用出来る。
胆力、進行波不平管電界(三相型)を応用した電界カー
テン素子は、高純度アルミナよりなる板状の素子で、三
相の線状放電極IjTを有し、素子背面に三相のターミ
ナルか設けられ、三相電極の中の1相を表面に露出させ
たものと、針べての電極を素子の内部に埋設したものと
がある。前者はイオン発生効果に主眼を置き、後者は電
界効果に主Ill!を置いたものである。いま、三相の
交流高電圧を三つのターミナルから三相電極群に印加す
ると、素子の表面に沿って相順方向に移動する進行波不
平等電界が形成さj″Lる。したがって素子」二のダス
ト ′4;の物体1よ、その大部分が先ず電気的反発力
をうけて素子表面から浮」二しその状態で進行波の方向
に電、気的に輸送される。この場合粒子を水平方向の・
みならず垂直方向にも上昇輸送することもでドる。この
進行波不平等電界は相順方向tこ進行する回転進行波電
界(第1モード)、逆方向に進行するやや低い強度の逆
回転進行波電界(第2モード)、正方向に進行する第3
モードの回転進行波電界、・・・と無限個の別々の回転
進行波ミソ^に展開され、それぞれ異なった進行速度と
回転速度を有する。
更に電圧を上げると素子面上に交流コロナ放電か発生し
、正負イオンより成るプラズマが生しる。
電圧を更The present invention relates to an electric field curtain element having electrostatic capability applying electric field curtain theory. Specifically, the present invention relates to an electric field curtain element having electrodynamic, electrostatic, discharge chemical functions, and physicochemical stirring functions. Conventionally, an electric field curtain element that applies a standing wave alternating unequal electric field (single-phase type) to the electric field curtain theory is a plate-shaped element with a group of linear ground discharge electrodes on its surface, or a plate-shaped A high (high) main induction electrode is provided, and a terminal of the high (high) induction electrode is provided on the back side of the element. Single-phase cross between both electrodes;
When an AL high voltage is applied, an alternating unequal electric field of standing waves is generated around the linear discharge electrode, and this action repels the charged object and brushes off the deposits on the surface. In this case, the deposit is contact-electrified by contact with the element surface and is subjected to the action of an electric field. Furthermore, when the voltage is increased, a strong alternating current creeping corona discharge is generated from the linear discharge electrode, forming a plasma containing abundant positive and negative ions, which becomes an excellent source of ions. In other words, when a charged object approaches the device, the charge is immediately neutralized (eliminated).
However, when an external electric field is applied, positive or negative ions are freely extracted from this ion source and the object is charged. We also modify the surface of the powder to increase its fluidity.
Promotes wetting to solvent. Furthermore, since strong ozone is generated as a result of this discharge, it can be used not only as an ozone generator, but also for sterilization, deodorization, reaction promotion, combustion promotion, desulfurization, and denitrification. The electric field curtain element that applies a traveling wave non-tube electric field (three-phase type) is a plate-shaped element made of high-purity alumina, and has a three-phase linear discharge electrode IJT, and a three-phase terminal on the back of the element. There are two types: one in which one phase of the three-phase electrode is exposed on the surface, and the other in which the needle electrode is buried inside the element. The former focuses on the ion generation effect, and the latter focuses on the electric field effect. This is what I put. Now, when a three-phase AC high voltage is applied from the three terminals to the three-phase electrode group, a traveling-wave unequal electric field is formed that moves in the phase forward direction along the surface of the element.Therefore, the element Most of the dust '4; object 1 first floats off the element surface due to electrical repulsion, and in that state is electrically and electrically transported in the direction of the traveling wave. In this case, the particles are
Not only that, but it can also be transported vertically. This traveling-wave unequal electric field consists of a rotating traveling-wave electric field (first mode) that travels in the phase forward direction, a reverse-rotating traveling-wave electric field (second mode) of slightly lower strength that travels in the opposite direction, and a rotating traveling-wave electric field that travels in the forward direction (second mode). 3
The rotating traveling wave electric field of the mode is expanded into an infinite number of separate rotating traveling waves, each with a different traveling speed and rotational speed. When the voltage is further increased, an alternating current corona discharge is generated on the element surface, and a plasma consisting of positive and negative ions is generated. Change the voltage
【こ上げると放電は更に活発となりプラズマの
イオン密度は更に高くなる。これに伴って電気力学的作
用自体も活発となる。この状態では単にダストの輸送の
みでなく、外部直流電界を加えることによりこれを輸送
中に強力に荷電の」二、直;!コミ界の方向にゲストを
駆動させることも出来、また粉体の表面改質も可能とな
る。
この発明は、従来電界カーテン素子か有する電気力学r
メへ静電的、放電化学は能と物理化学的撹拌〈!(1合
(蔑(1ヒを共有する新規な電界カーテシ素子を提供す
ることを「1的とする。
すなわち、この発明による電界カーテン素子は、円筒状
の固体誘電体に放電極を設け、かつ必茨に応じて該放電
極と絶縁して講導電1龜を設け1.該固体誘電体の体内
に長手方向に螺旋状にねしられた複数1161の羽根体
を有し、j青1)合う羽根1本の端縁とおしを交差させ
て配置した、ことを1.5徴とする電界カーテン素子で
ある。
すなわち、固体誘電体の体内に螺り1状にねじられた複
数個の羽根体を配置することによって、1種または2種
以上の流体に撹拌混合作用を発生させることにより、放
電極部での発4ミイオン、プラズマ等とのJな触面禎、
接触反応効率を増大させることか0丁能となる。
この発明に係る電界カーテン素子は、各種産業分野で利
用可1を巳であるが、例えば、粉粒体の1111合除電
、荷電装置、粉粒体輸送装置、オゾン発生装置、脱硝、
脱硫装置、脱史、脱色装置、殺菌装置、反応促進装置、
粉体表面改質装置、静電分級1分別装置、燃焼促進装置
、電気集塵装置、オイル送油管などに利用可能である。
夏、下、添イて1の図面を参照して、この発明の実施例
につき、−1J、体内に説明する。第1図ノ)至第・1
図は、重り^カーテン素子の羽根体を示す。第1図に示
す9()°右回−1を型羽根体]は長手方向に螺旋状1
こねしられている。羽根体〕は固体誘電体5の内側の半
径方向断面を2分割し、固体誘電体5の長手方向tこ1
1.5計方向に90“だけ回転している。第2図には9
0 ’左回転型羽根体2か示されている。
二の羽根体2は、固体誘電体5のその長手方向に反時計
方向にり 0 ’ だけ螺旋状にねしられている。
第3図に示す180°右回転型羽根本3及び第4図に示
118(1’左回転型羽根体4は、固体誘電体5の長手
方向に螺旋状にねじられており、羽根体ニジ及び伺土夫
々時計方向及び反時計方向に回転している。これらの羽
根体1〜・1においては、例えば創出成形法、押出し成
形法又はロストワックスダJ造法等により、容・易に製
造することがで外る。
各羽根体1〜・4は、ステンレス等の金属H料、プラス
チック4・1料又はセラミック4・]料又はそれら4=
A料の複合材料から製造宅れる。固体誘電体5内に配設
される羽根体の連結点においては、羽根体とおしを溶接
又はローイ・IM・により固定してもよいか、羽根体と
固体誘電体の内周面とを4&、 )’f して固定して
もよい。又、羽根体の軸方向端部の中心部に軸方向に凹
溝を形成して隣接する羽根体とを11′>2介して固体
誘電体内に配設してもよい。
次に、このような羽根体と固体誘電体とを組合わせて構
成される電界カーテン素子について説明する。第5図は
、固体誘電体5内に90°右回転型羽根木1と、90′
左回転型羽根体2とを組合わせて配設した電界カーテン
素子6を示す。この電界カーテン素子6は、固体誘電体
5内に羽根体1と羽根体2とを交互に配置し、その羽根
体1及び2の端縁どおしを直交させたちのである。第6
図の電界カーテン素子7は、固体誘電体5内に180゛
回転型の羽根体3及び11の端縁とおしを直交さる
ぜたものである。この外にも、例えは右回Ilv:型羽
根体のみを連結するとか、又は左回転型羽根体のみ杢連
結する等の種々組合わせ態様が考えられる。
次に、固体誘電体に設けられる放電極と必要に応して設
けられる誘導電極の構成について、図面に暴いて述へる
。
第°7図に示した如く、複数個の線状放電極8は固体誘
電体5の内側表面に設けられる。誘導電極″:Jは放電
極2;にλ・]向して放電極8と絶縁した状態で埋設さ
れている。固体誘電体の内側表面に設けられる放電極と
しては、厚膜技術によって0.1〜] 0111111
中、厚さ1〜100μローの線状電極を、間隔1〜10
111111程度で多数並列にlIf、1府するのか有
効である。又、誘導電極は金属蒸着などの技術によって
形成される。
このようにして構成される電界カーテ/素子を、オゾン
発生装置として使用する場合は、乾燥したぢ・で気又は
酸素を固体誘電体内に通流させればよい。
この場合に、各羽根体を触媒作用のある金属4,4 t
;I、セラミック(・(料、プラスチック4・A料など
で形成あるいは触媒なJ旧11することにより1.1υ
一層の反応促進か11能となる。
いま、電2原により4線10、]1を介し′ζ複数個の
放電極(3と誘導・、電1m< !Jの間:こ周期的変
動電圧 −を印ツノ1けると、固体誘電体5内の表面の
放電極)3の間に沿面放電か発生1−る。5−のlLl
+、1−11庵、1カ電休5内に(Jl、給される空気
又は1衰素のl光1本は、各羽根体により仕切られた通
路を+、!旋状に通;Aコし、各羽4艮木の連糸、+1
点において流体は2分、1;すされなが呟固体1、誘電
体中央(・1近の流体は誘電体内ヘーシ\、誘′1L体
内壁イ・j近の流体は誘電体中央へと交互に層がlIl
、L位し−〕つ他方の通路を通流してきたl皮体と混合
される。このJ:うにして、i、f、木は螺旋状の羽根
体により、沿面放電を発生させている放電(4ン面と接
触反応してオゾンがり)率よ(生成される。
また、nij記以外に沿面放電を発生させる方法として
は、相隣る放電極を互に絶縁の」−いくつかに組合けし
、これに多相の周期的変動電圧を印加する方法、複数個
の放電極をすべて共3m導線に並夕IFに接続し、かつ
固体誘電体の背面に放電極に対向して1個又は複数個の
誘導電極を設け、放電園と誘導電極間に単相の周期的変
動電圧を印加する方法等種々ジえられる。そのいずれを
利用してもより)。
又、放電極に印加1べき周期的変動電圧としては、商用
周波数、又はこれより高い周波数の単相又は三相の正弦
波り1本電圧、三角波交流電圧、矩形波交流電圧、くり
返しパルス電圧等を用いることかできる。
更に111f記以外に交番不平で1゛電界を発!1掲ぜ
る方法とし′ζは、第8図に示した如く、第1及び第2
極性の線状電極]5及び1Gは交互に隣り合ってほぼ平
行に絶縁体層13内に配列され、誘電体層】・・1は線
状電極15及び16の上に形成されて、固体誘電体が構
成されている。それ故に、単相または三相の交i!電圧
を電極間に印ツノ1けると、相隣る線状電極15及び1
6間に、第8図に点線で示したような交番不平等電界を
生起でべろ。この場合、微フ111粒子が誘電体ハ41
/目こ接触すると摩擦(f7電、誘導、電荷注入などに
よって荷電粒子となる。
そして、このイ17電粒子は、はぼ電気力線に沿って電
気力学的振動を行なうようになる。また、この現象は、
予め・:1シ電されている粒子が111j記不平等交番
電界に近づいた場合にも、全く同様に発生する。
辿ツバ例えば粉粒体の角°f業分野に利用する場合、電
界カーテン素子6に供給される1種または2独り、」二
のi’i−’電した粉粒体か、放電極8がら沿面放電に
より発生しているイオン源に近つくと直ちにその電荷を
中和(除電)する。この11.5″、羽根体1及び2の
作用により、粉粒体とイオン源との接触が効率よく行な
われる。それとともに、前記同様の山“。
合作用か行なわオ′シる。すなわち、粉ね木を除電しつ
つ2種類以上の粉粒体の混合操作かηJ能となる。
また、1種類の場合は、粉粒体の二次凝集体の生成を防
雨することか可能となる。
なオよ、各羽根体の1fl径及び長さ等の−・j法、及
び捻り角度は任意に設定することができ、利用分野に応
じて適切なものを選択可能である。また、」−記実施例
においては、羽根体は一体歳形としたが、羽根体を半径
方向で分割した分側板状素子を複数枚を積層して形成し
てもよい。更に羽根体は」二記天施例の如く、2分割の
ものに限らす、例えば羽根体か固体誘電本の庫内を3分
割し、長手方向に6i1’(あるいは120°lだけ螺
旋回転する型式のものを使用することも可能で゛ある。
また、固体誘電体の内部又は外側を冷却することによっ
て、イオン発生の電力効率を上げることか11能となる
。[As the temperature rises, the discharge becomes more active and the ion density of the plasma becomes even higher. Along with this, the electrodynamic action itself becomes active. In this state, not only is the dust transported, but by applying an external DC electric field, it becomes strongly charged during transport. It is also possible to drive guests in the direction of the Komi world, and it is also possible to modify the surface of powder. This invention provides an electrodynamic r
Mehe electrostatic, discharge chemistry is the ability and physicochemical stirring <! It is an object of the present invention to provide a novel electric field courtesy element that shares the following characteristics.In other words, the electric field curtain element according to the present invention has a cylindrical solid dielectric body provided with a discharge electrode, and If necessary, a conductor is provided insulated from the discharge electrode. 1. It has a plurality of 1161 blade bodies spirally twisted in the longitudinal direction inside the body of the solid dielectric, This is an electric field curtain element with a 1.5 characteristic in which the edges of one matching blade are arranged so as to intersect with each other.In other words, a plurality of blades are twisted in a spiral shape inside a solid dielectric body. By arranging this, a stirring and mixing effect is generated in one or more types of fluids, thereby creating contact between ions, plasma, etc. generated at the discharge electrode, and
Increasing the catalytic reaction efficiency will result in zero efficiency. The electric field curtain element according to the present invention can be used in various industrial fields, including, for example, 1111 static elimination of powder and granular materials, charging devices, powder and granular transportation devices, ozone generators, denitrification,
Desulfurization equipment, dehistory, decolorization equipment, sterilization equipment, reaction accelerator,
It can be used in powder surface reforming equipment, electrostatic classification 1 classification equipment, combustion promotion equipment, electrostatic precipitators, oil feed pipes, etc. Embodiments of the present invention will be described below with reference to the accompanying drawings. Figure 1) to No. 1
The figure shows the vanes of a weighted curtain element. The 9()° clockwise rotation -1 shown in Figure 1 is a spiral 1 in the longitudinal direction.
Being kneaded. The blade body] divides the inner radial cross section of the solid dielectric 5 into two, and divides the solid dielectric 5 in the longitudinal direction t.
It rotates by 90" in the direction of 1.5 meters. Figure 2 shows 90".
0 'Left-handed rotating type blade body 2 is shown. The second blade 2 is spirally twisted counterclockwise in the longitudinal direction of the solid dielectric 5 by 0'. The 180° clockwise rotation type blade base 3 shown in FIG. 3 and the left rotation type blade body 4 shown in FIG. The blade bodies 1 to 1 are easily manufactured by, for example, a creation molding method, an extrusion molding method, or a lost wax molding method. Each blade body 1 to 4 is made of a metal H material such as stainless steel, a plastic material 4.1 material, or a ceramic material 4.
Manufactured from A-based composite materials. At the connection point of the blade body disposed in the solid dielectric body 5, the blade body and the diaphragm may be fixed by welding or Loi IM, or the blade body and the inner circumferential surface of the solid dielectric body may be fixed by 4&, )'f and fix it. Alternatively, an axial groove may be formed in the center of the axial end of the blade body, and the blade body may be disposed in the solid dielectric body with an interval 11'>2 interposed between the blade body and the adjacent blade body. Next, an electric field curtain element constructed by combining such a blade and a solid dielectric will be described. FIG. 5 shows a 90° clockwise rotation type blade 1 and a 90'
An electric field curtain element 6 arranged in combination with a left-handed rotary blade body 2 is shown. This electric field curtain element 6 has blades 1 and 2 arranged alternately within a solid dielectric 5, with the edges of the blades 1 and 2 perpendicular to each other. 6th
The electric field curtain element 7 shown in the figure has blades 3 and 11 of a 180° rotation type in which the end edges and the bottom are orthogonal to each other in a solid dielectric 5. In addition to this, various combinations can be considered, such as connecting only the right-handed Ilv type blade bodies, or connecting only the left-handed type blade bodies. Next, the configuration of the discharge electrode provided on the solid dielectric and the induction electrode provided as necessary will be explained with reference to the drawings. As shown in FIG. 7, a plurality of linear discharge electrodes 8 are provided on the inner surface of the solid dielectric 5. As shown in FIG. The induction electrode ``J'' is buried in the discharge electrode 2; facing λ· while being insulated from the discharge electrode 8.The discharge electrode provided on the inner surface of the solid dielectric is formed using thick film technology. 1~] 0111111
Linear electrodes with a thickness of 1 to 100μ are placed at intervals of 1 to 10
It is effective to run many IIfs in parallel at about 111111. Further, the induction electrode is formed by a technique such as metal vapor deposition. When the electric field curtain/element constructed in this manner is used as an ozone generator, dry gas or oxygen may be passed through the solid dielectric. In this case, each blade is made of 4,4 t of catalytic metal.
; I, ceramic (・(material, plastic 4, A material, etc.) or catalytic J old 11 1.1υ
This may further promote the reaction. Now, with the electric current 2, the four wires 10,]1 are connected to the multiple discharge electrodes (3 and the induction current, the electric current 1m<! A creeping discharge occurs between the discharge electrodes (3) on the surface of the body (5). 5-lLl
+, 1-11 hermitage, 1 Kadenshu 5 (Jl, supplied air or 1 light of 1 attenuation element passes through the path partitioned by each blade body +, ! spirally; A Koshi, each feather has 4 threads of wood, +1
The fluid at the point is 2 minutes, 1; the fluid near the solid 1, the center of the dielectric (the fluid near 1 is the center of the dielectric, the fluid near the wall I, j of the dielectric is alternately moving to the center of the dielectric) The layer is lIl
, L) and the L skin body flowing through the other passage. This J: In this way, i, f, wood is generated by the spiral blade body, which generates creeping discharge (ozone is generated by contact reaction with the surface). Also, nij In addition to the methods described above, methods for generating creeping discharge include combining adjacent discharge electrodes into several insulated ones and applying a polyphase periodically fluctuating voltage to them; All are connected to a parallel IF with a 3m conductor, and one or more induction electrodes are provided on the back of the solid dielectric opposite the discharge electrode, and a single-phase periodic fluctuation voltage is applied between the discharge field and the induction electrode. There are various methods of applying the . In addition, the periodic varying voltage applied to the discharge electrode may include a single-phase or three-phase sinusoidal voltage at a commercial frequency or a higher frequency, a triangular wave AC voltage, a rectangular wave AC voltage, a repetitive pulse voltage, etc. It is possible to use Furthermore, in addition to 111f, a 1゛ electric field is generated by the alternating box complaint! As shown in Figure 8, 'ζ is the first and second method.
Polar linear electrodes] 5 and 1G are arranged adjacent to each other and substantially parallel in the insulating layer 13, and the dielectric layer]...1 is formed on the linear electrodes 15 and 16 to form a solid dielectric layer. The body is made up of Therefore, single-phase or three-phase alternating i! When a voltage is applied between the electrodes, the adjacent linear electrodes 15 and 1
6, generate an alternating unequal electric field as shown by the dotted lines in Figure 8. In this case, the fine particles 111 are the particles of the dielectric material 41.
When the particles come in contact with each other, they become charged particles due to friction (f7 electricity, induction, charge injection, etc.).Then, these electric particles begin to oscillate electrodynamically along the lines of electric force.Also, This phenomenon is
Exactly the same phenomenon occurs when a particle that has been electrically charged in advance approaches the 111j unequal alternating electric field. For example, when the trailing collar is used in the field of angular powder or granular material, one or two types of powder or granular material supplied to the electric field curtain element 6 may be supplied to the electric field curtain element 6, or from the discharge electrode 8. When approaching an ion source generated by creeping discharge, the charge is immediately neutralized (eliminated). Due to the action of these 11.5" blades 1 and 2, contact between the powder and the ion source is carried out efficiently. At the same time, the same ridge as described above. Let's do some joint work. In other words, it is possible to mix two or more types of granular material while removing static electricity from the powdered wood. Moreover, in the case of one type, it becomes possible to prevent the formation of secondary aggregates of powder and granules. Incidentally, the -j method of the 1 fl diameter and length of each blade body, and the twist angle can be arbitrarily set, and an appropriate one can be selected depending on the field of use. Further, in the embodiment described in ``-'', the blade body is integrally shaped, but it may be formed by laminating a plurality of side plate-like elements obtained by dividing the blade body in the radial direction. Furthermore, the blade body is limited to one that is divided into two parts, as in the Nikiten example.For example, the blade body or the inside of the solid dielectric book cabinet is divided into three parts, and the blade body is spirally rotated by 6i1' (or 120°l) in the longitudinal direction. Alternatively, by cooling the inside or outside of the solid dielectric, it is possible to increase the power efficiency of ion generation.
第1図乃至第・4図は羽根体のコ1(面図、第5図乃至
第6図は電界カーテン素子の(ゲ弐図、第゛7図]5至
第8図は固体誘電体の水平部分断面図を示す。
1.2,3.・1・・羽根体、5・・・固体誘電体、6
.7・・・電界カーテン素子、ト・・放電極、9・・・
誘導電極、 10.11・・・導線、12・・・電源、
13・・・絶縁水層、14・・・誘電体層、15.16
・・線状電極群。
特i’l’lJす傾人小嶋久夫
第1図 第2図
第3図 第4図
第6図
第7図
第8図
3Figures 1 to 4 are side views of the blade body, Figures 5 to 6 are diagrams of the electric field curtain element, Figures 5 to 8 are of the solid dielectric. A horizontal partial cross-sectional view is shown. 1.2, 3. 1... Blade body, 5... Solid dielectric, 6
.. 7... Electric field curtain element, G... Discharge electrode, 9...
Induction electrode, 10.11... Conductor wire, 12... Power supply,
13... Insulating water layer, 14... Dielectric layer, 15.16
... Linear electrode group. Special i'l'lJ's Hisao Kojima Figure 1 Figure 2 Figure 3 Figure 4 Figure 6 Figure 7 Figure 8 Figure 3
Claims (1)
を設けてなる固体誘電体において、該固体誘電体の体内
に長平方向に!!1に状にねじられた複数個の羽根本を
有し、隣り合う羽411本の端縁どおしを交差させて配
置したことを特徴とする電界カーテン素子。 2、前記固体誘電体は円節状をなすことを1、ン徴とす
る′4−’i許請求の範囲第1項に記載の電界カーテン
素子。 3、前記羽根体は長平方向に00°たげねしられ、固体
誘電体の体内を2分割していることを特徴とする1、h
′「請求の範囲12項に記載の電界カーテン素子。 4.1iij記羽根体は長平方向に180’だけねしら
れ、固体誘電体の体内を2分割していることを特徴とす
る特言′1請求の範囲第2項に記載の電界カーテン素子
。 5、前記羽根体は長平方向に6()°だけねしられ、固
体誘電体の体内を3分割していることを特徴とする特許
請求の範囲第2項に記載の電界カーテン素子。[Claims] 1. In a solid dielectric body comprising a discharge electrode and, if necessary, an induction electrode insulated from the discharge electrode, in the longitudinal direction within the body of the solid dielectric body! ! 1. An electric field curtain element having a plurality of blade roots twisted into a single shape, and arranged so that the end edges of 411 adjacent blades intersect with each other. 2. The electric field curtain element according to claim 1, wherein the solid dielectric has a nodal shape. 3. The blade body is bent at 00 degrees in the longitudinal direction and divides the inside of the solid dielectric body into two. 1.h
``The electric field curtain element according to claim 12.Special claim characterized in that the blade body according to 4.1iii is bent by 180' in the longitudinal direction, dividing the inside of the solid dielectric body into two.'' 1. The electric field curtain element according to claim 2. 5. A patent claim characterized in that the blade body is bent by 6 ( ) degrees in the longitudinal direction, dividing the inside of the solid dielectric body into three parts. The electric field curtain element according to the second item in the range.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24509883A JPS60140699A (en) | 1983-12-28 | 1983-12-28 | Electric field curtain element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24509883A JPS60140699A (en) | 1983-12-28 | 1983-12-28 | Electric field curtain element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60140699A true JPS60140699A (en) | 1985-07-25 |
Family
ID=17128575
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24509883A Pending JPS60140699A (en) | 1983-12-28 | 1983-12-28 | Electric field curtain element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60140699A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1991002394A1 (en) * | 1989-08-10 | 1991-02-21 | Commonwealth Scientific And Industrial Research Organisation | Producing electrosuspensions |
CN103619712A (en) * | 2011-05-09 | 2014-03-05 | 奥唑尼卡有限公司 | Disinfection of packaged articles |
-
1983
- 1983-12-28 JP JP24509883A patent/JPS60140699A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1991002394A1 (en) * | 1989-08-10 | 1991-02-21 | Commonwealth Scientific And Industrial Research Organisation | Producing electrosuspensions |
CN103619712A (en) * | 2011-05-09 | 2014-03-05 | 奥唑尼卡有限公司 | Disinfection of packaged articles |
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