TWI543483B - Ion or ozone wind generating device and method - Google Patents

Ion or ozone wind generating device and method Download PDF

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TWI543483B
TWI543483B TW103142974A TW103142974A TWI543483B TW I543483 B TWI543483 B TW I543483B TW 103142974 A TW103142974 A TW 103142974A TW 103142974 A TW103142974 A TW 103142974A TW I543483 B TWI543483 B TW I543483B
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electrode
discharge
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power receiving
ion
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TW201543777A (en
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片野明夫
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片野工業股份有限公司
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    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61LMETHODS OR APPARATUS FOR STERILISING MATERIALS OR OBJECTS IN GENERAL; DISINFECTION, STERILISATION OR DEODORISATION OF AIR; CHEMICAL ASPECTS OF BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES; MATERIALS FOR BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES
    • A61L9/00Disinfection, sterilisation or deodorisation of air
    • A61L9/16Disinfection, sterilisation or deodorisation of air using physical phenomena
    • A61L9/22Ionisation
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B13/00Oxygen; Ozone; Oxides or hydroxides in general
    • C01B13/10Preparation of ozone
    • C01B13/11Preparation of ozone by electric discharge
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01TSPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
    • H01T19/00Devices providing for corona discharge
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01TSPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
    • H01T19/00Devices providing for corona discharge
    • H01T19/04Devices providing for corona discharge having pointed electrodes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01TSPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
    • H01T23/00Apparatus for generating ions to be introduced into non-enclosed gases, e.g. into the atmosphere
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61LMETHODS OR APPARATUS FOR STERILISING MATERIALS OR OBJECTS IN GENERAL; DISINFECTION, STERILISATION OR DEODORISATION OF AIR; CHEMICAL ASPECTS OF BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES; MATERIALS FOR BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES
    • A61L2209/00Aspects relating to disinfection, sterilisation or deodorisation of air
    • A61L2209/10Apparatus features
    • A61L2209/13Dispensing or storing means for active compounds
    • A61L2209/134Distributing means, e.g. baffles, valves, manifolds, nozzles
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61LMETHODS OR APPARATUS FOR STERILISING MATERIALS OR OBJECTS IN GENERAL; DISINFECTION, STERILISATION OR DEODORISATION OF AIR; CHEMICAL ASPECTS OF BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES; MATERIALS FOR BANDAGES, DRESSINGS, ABSORBENT PADS OR SURGICAL ARTICLES
    • A61L2209/00Aspects relating to disinfection, sterilisation or deodorisation of air
    • A61L2209/20Method-related aspects
    • A61L2209/21Use of chemical compounds for treating air or the like
    • A61L2209/212Use of ozone, e.g. generated by UV radiation or electrical discharge

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  • Health & Medical Sciences (AREA)
  • Organic Chemistry (AREA)
  • Chemical & Material Sciences (AREA)
  • Animal Behavior & Ethology (AREA)
  • General Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Epidemiology (AREA)
  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Disinfection, Sterilisation Or Deodorisation Of Air (AREA)
  • Oxygen, Ozone, And Oxides In General (AREA)

Description

離子、臭氧風產生裝置及方法 Ion, ozone wind generating device and method

本發明係利用電暈放電使離子風產生之裝置,更詳細而言,係使更大的風量之離子風產生之離子風產生裝置。此外,就某觀點而言本發明係有關用以將垃圾等對象物進行殺菌、除臭之裝置及方法,尤其是在配置對象物的空間之另外的空間進行電暈放電,使離子及臭氧產生且將離子、臭氧風供應到配置有對象物的空間,來進行殺菌、除臭之裝置及方法。更具體而言,本發明係有關裝設在氣密性高的箱子,例如,廚餘與尿布等之污物容器,廚餘處理機,用以收納鞋、靴子等之箱子,馬桶及馬桶水槽,氣密性高的附冷凍、冷藏裝置之貨櫃及附冷凍、冷藏裝置之車輛,冷藏庫,室內、車輛內的空調裝置等,而以進行殺菌、除臭為目的之環境裝置。 The present invention relates to a device for generating ion wind by corona discharge, and more particularly to an ion wind generating device for generating a larger air volume of ion wind. Further, the present invention relates to an apparatus and method for sterilizing and deodorizing an object such as garbage, and in particular, corona discharge is performed in another space in a space where an object is placed, and ions and ozone are generated. Further, an apparatus and a method for sterilizing and deodorizing are provided by supplying ions and ozone wind to a space in which an object is disposed. More specifically, the present invention relates to a container that is installed in a high airtightness, for example, a dirt container such as a kitchen waste and a diaper, a kitchen waste processing machine, a case for storing shoes, boots, etc., a toilet and a toilet sink , an airtight container with a refrigerator and a refrigerating device, a vehicle with a refrigerator and a refrigerating device, a refrigerator, an air conditioner in a room, or a vehicle, and an environmental device for sterilization and deodorization.

伴隨著老齡化社會,與需要看護人口呈比例尿布等之污物容器的需求亦變高,惟由於每次開啟時會釋出惡臭,故造成對看護助理及周圍之負擔與不舒服且不衛生。再者,在各家庭與飲食店等亦存在有廚餘之保管箱子,每次開啟時,由於會伴隨著細菌增生而釋出惡臭,故 主婦等、從業人員的負擔大。廚餘處理機雖亦隨著生化技術的成長而增加,惟在運作時會釋出惡臭到處理機周邊而造成嚴重的問題。再者,於海外、國內的冷凍、冷藏、常溫品等之物流方面利用輸送用貨櫃及貨車等進行輸送為主流且附空調裝置之海上貨櫃、陸上貨櫃、貨櫃型貨車等為多數,惟裝載貨物之剩餘的臭味、空調裝置內之霉味成為問題。並且,倉庫、冷藏庫、室內、車輛等之空調裝置亦因保管物質等使用狀況而使臭氣成為問題。 With the aging society, the demand for dirt containers, such as diapers, which are in need of care of the population, is also high. However, since the stench is released every time it is opened, the burden on the care assistant and the surrounding is uncomfortable and unsanitary. . In addition, there are also storage boxes for food waste in various households and restaurants, and each time it is turned on, it will release malodor with bacterial proliferation. Housewives and other employees have a heavy burden. Although the kitchen waste processor has also increased with the growth of biochemical technology, it will release a foul smell to the periphery of the processor during operation, causing serious problems. In addition, in the logistics of overseas and domestic refrigeration, refrigeration, and room temperature products, most of the sea containers, land containers, and container trucks that are transported by the use of transport containers and trucks, etc. The remaining odor and the musty smell in the air conditioner are problematic. In addition, air conditioners such as warehouses, refrigerators, indoors, and vehicles also cause odors due to the use of substances and the like.

在此,作為上述問題之一解決手法而言, 以往提案有一種噴射式等之簡單型的殺菌除臭劑。但是,使用於污物容器與廚餘之保管箱子時,現狀仍是開啟該容器時會釋出惡臭。此外,使用於空調裝置(例如散佈與循環殺菌方式)時,在空調裝置內部無法清洗之部位,或即使清洗亦殘留異臭、霉味時,臭氣會轉移到下次的積載貨物等,而成為問題。並且,以別的解決手法而言,提案有一種方法與高價格的去除惡臭觸媒,其係將從成為殺菌除臭的對象之空間吸引空氣且利用過濾器吸附或去除汚染物質。但是,因長期的使用故過濾器的交換等之維修為不可缺少,而且過濾器的性能不足夠,故大多為無法得到達到滿足的性能之情況或為即使性能佳但大型且高價格的觸媒本身之維持、管理費更為高價格的情況。 Here, as one of the above problems, In the past, there has been proposed a simple type of sterilization deodorant such as a spray type. However, when used in a storage container for a dirt container and a kitchen waste, the current situation is that when the container is opened, malodor is released. In addition, when it is used in an air conditioner (for example, a dispersion and a circulation sterilization method), when a part that cannot be cleaned inside the air conditioner, or an odor or a musty smell remains even after washing, the odor is transferred to the next stowage cargo, etc. problem. Further, in terms of other solutions, there is a proposal for a method and a high-priced deodorant catalyst for sucking air from a space which is a target for sterilization and deodorization, and adsorbing or removing contaminants by a filter. However, repairs such as exchange of filters are indispensable for long-term use, and the performance of the filter is insufficient, so that most of them fail to achieve satisfactory performance or are large-scale and high-priced catalysts even if performance is good. The maintenance of itself and the higher management costs.

但是近幾年,為了室內的空氣清淨與精神 之恢復(refresh),產生負離子與臭氧之空氣清淨機與空調等正普及中。然後,提案有多數技術,係同時使用使具有 除臭效果之負離子與臭氧產生之負離子、臭氧產生裝置而將對象空間予以除臭等之技術。 But in recent years, for the clean air and spirit of the interior The refrigerating, air purifiers and air conditioners that generate negative ions and ozone are becoming widespread. Then, the proposal has a lot of technology, which is used at the same time to have A technique for deodorizing a target space by an anion having a deodorizing effect, an anion generated by ozone, and an ozone generating device.

首先,專利文獻1之負離子、臭氧產生裝置 係設想為安裝在房間的天花板之裝置,且以正電極位於比負電極更下方之方式而配置。據此,即使不使用風扇與馬達亦可使含有負離子與臭氧之朝下的氣流產生。 First, the negative ion and ozone generating device of Patent Document 1 It is assumed to be a device mounted on the ceiling of a room, and is arranged such that the positive electrode is located below the negative electrode. According to this, even if the fan and the motor are not used, the airflow containing the negative ions and the ozone can be generated.

其次,專利文獻2之負離子、臭氧產生裝置 具備前端為針狀之負電極以及與其平行且設置為同心圓狀之圓筒型的接地電極,而藉由將負電極與接地電極設為可相對性地移動,並在負電極施加高電壓,且調整負電極的前端部與接地電極的端面之距離來產生負離子或臭氧。 Next, the negative ion and ozone generating device of Patent Document 2 a cylindrical electrode having a needle-shaped negative electrode at the front end and a cylindrical shape parallel thereto and arranged in a concentric shape, and the negative electrode and the ground electrode are relatively movable, and a high voltage is applied to the negative electrode. And adjusting the distance between the front end portion of the negative electrode and the end surface of the ground electrode to generate negative ions or ozone.

其次,專利文獻3之負離子、臭氧產生裝 置,係在針狀電極與接地電極間施加直流高電壓且在針狀電極前端部使電暈放電產生,來使臭氧及負離子產生之裝置。 Second, the negative ion and ozone generating device of Patent Document 3 A device that applies a direct current high voltage between the needle electrode and the ground electrode and generates a corona discharge at the tip end portion of the needle electrode to generate ozone and negative ions.

其次,專利文獻4所記載之負離子、臭氧產 生裝置具有正電極,其係在1個處所或複數個處所具備有在周圍具有隆起部的孔之金屬板所構成,且負電極的前端位於前述正電極之孔附近。藉由以此方式來構成,而透過放電產生足夠的氣流,故不另外使用風扇、幫浦等之送風裝置亦可產生使所產生之負離子與臭氧擴散到空間內之氣流。 Next, the negative ion and ozone produced in Patent Document 4 The raw device has a positive electrode which is formed of a metal plate having a hole having a raised portion around the one space or a plurality of places, and the front end of the negative electrode is located near the hole of the positive electrode. By configuring in this manner, a sufficient airflow is generated by the discharge, and the airflow that causes the generated negative ions and ozone to diffuse into the space can be generated without using a fan or a pump.

專利文獻1至4之發明記載有使離子及臭氧 產生且適用於對象物,惟上述技術係以例如配置在垃圾箱 的內部等成為殺菌或脫臭的對象之空間內來進行放電作為前提。例如,若是在垃圾箱中,會有釋出惡臭之有機物由微生物所分解而產生甲烷氣等之可燃性氣體之情況,在此種狀況下進行放電時,會因產生火花而有可能引起火災與爆炸之危險性。 The inventions of Patent Documents 1 to 4 describe the use of ions and ozone. Produced and applied to objects, but the above techniques are, for example, configured in a trash can It is premised that the inside is discharged in the space to be sterilized or deodorized. For example, in a garbage can, a odorous organic substance is decomposed by microorganisms to generate a flammable gas such as methane gas. When the discharge is performed under such conditions, a spark may be generated to cause a fire and The danger of explosion.

因此,為了去除此種危險性,檢討一種外接型殺菌、除臭裝置的開發,係在配置對象物的空間外進行放電而產生離子、臭氧,且將上述產生物導入到配置對象物的空間內(專利文獻5)。 Therefore, in order to remove such a risk, an external type of sterilization and deodorizing device has been developed, and discharge is performed outside the space in which the object to be placed, and ions and ozone are generated, and the product is introduced into the space of the object to be placed. (Patent Document 5).

[先前技術文獻] [Previous Technical Literature] [專利文獻] [Patent Literature]

[專利文獻1]日本實用新案登錄第3100754號 [Patent Document 1] Japanese Utility New Case Registration No. 3100754

[專利文獻2]日本特開2003-342005號公報 [Patent Document 2] Japanese Patent Laid-Open Publication No. 2003-342005

[專利文獻3]日本特開2004-18348號公報 [Patent Document 3] Japanese Patent Laid-Open Publication No. 2004-18348

[專利文獻4]日本特開2005-13831號公報 [Patent Document 4] Japanese Patent Laid-Open Publication No. 2005-13831

[專利文獻5]日本實用新案登錄第3155540號 [Patent Document 5] Japanese Utility New Case Registration No. 3155540

但是,在專利文獻1至5之發明中,雖可可使離子及臭氧產生,但無法使該產生之離子及臭氧廣泛地遍佈,而難以構成為能使離子及臭氧遍及整個房間。更具體而言,在上述技術中,含有該產生之離子及臭氧之離子風的風力本身弱且僅可在特定的方向產生,故為使離子及 臭氧遍及整個房間,必須另設置送風機等來推動離子風,結果,雖可推動離子風,但另一方面,有所含之離子及臭氧被稀釋之缺點。 However, in the inventions of Patent Documents 1 to 5, although ions and ozone can be generated, the generated ions and ozone cannot be widely distributed, and it is difficult to configure ions and ozone throughout the entire room. More specifically, in the above technique, the wind of the ion wind containing the generated ions and ozone is weak in itself and can be generated only in a specific direction, so that the ions and Ozone is spread throughout the room, and a blower or the like must be additionally provided to push the ion wind. As a result, although the ion wind can be promoted, on the other hand, the ion and the ozone are diluted.

本發明係由此種觀點而研創者,其目的係 在提供一種離子、臭氧風產生裝置,係加強含有離子及臭氧之離子風的風力本身且用以使離子、臭氧風廣泛地產生。 The present invention is developed by such a viewpoint, and its purpose is An ion and ozone wind generating device is provided to strengthen the wind power itself containing ion and ozone ion winds and to generate ions and ozone winds widely.

本發明(1)係一種離子、臭氧風產生裝置,其係構成為於放電點(例如,第24圖之放電點322、第32圖之放電點322)與受電點(例如,第24圖之受電點332、第32圖之受電點332)之間使電位差產生產生電暈放電,其藉由將放電點連續配置在成為放電基準之基準線上而形成放電線(例如,第24圖之放電部321、第32圖之放電部321),且藉由將受電點連續配置在成為受電基準之基準線上而形成受電線(例如,第24圖之受電部331、第32圖之受電部331),放電線與受電線係隔離配置,且構成為藉由從放電線朝受電線產生電暈放電,而至少朝受電線之不與放電線相對之側的開放部產生離子風。 The present invention (1) is an ion and ozone wind generating device which is configured to be at a discharge point (for example, the discharge point 322 of FIG. 24, the discharge point 322 of FIG. 32) and a power receiving point (for example, FIG. A potential difference is generated between the power receiving point 332 and the power receiving point 332) in FIG. 32, and a discharge line is formed by continuously arranging the discharge point on a reference line serving as a discharge reference (for example, the discharge portion of FIG. 24) 321. The discharge portion 321) of Fig. 32 is formed by continuously arranging the power receiving points on the reference line serving as the power receiving reference (for example, the power receiving unit 331 of Fig. 24 and the power receiving unit 331 of Fig. 32). The discharge wire is disposed to be separated from the power receiving wire, and is configured to generate ion wind at least toward an opening portion of the receiving wire that does not face the discharge wire by generating a corona discharge from the discharge wire toward the power receiving wire.

本發明(2)係本發明(1)之離子、臭氧風產生裝置,其係針對一條放電線(例如,第29圖之放電部321、第34圖之放電部321)具有複數條受電線(例如,第29圖之受電部331a至331c、第34圖之受電部331a至331c),而該複數條受電線係配置在與配置該一條放電線的平面為相同之平面或與該相同平面平行之複數個平面之任一平面上,並 且,該複數條受電線之各者配置在相互不同之平面上。 The invention (2) is the ion and ozone wind generating device of the invention (1), which has a plurality of electric wires (for example, the discharge portion 321 of Fig. 29 and the discharge portion 321 of Fig. 34). For example, the power receiving units 331a to 331c of Fig. 29 and the power receiving units 331a to 331c of Fig. 34, and the plurality of electric wires are arranged in the same plane as the plane in which the one discharge line is disposed or in parallel with the same plane. On any plane of a plurality of planes, and Moreover, the plurality of wires are arranged on mutually different planes by the respective wires.

本發明(3)係本發明(2)之離子、臭氧風產生裝置,其係前述複數條受電線(例如,第29圖之受電部331a至331c)成為主受電線(例如,第29圖之受電部331a)及副受電線(例如,第29圖之受電部331b及331c)之任一者,且從前述一條放電線(例如,第29圖之放電部321)中之某放電點(例如,第29圖之放電點322)到屬於主受電線中之受電點之與該某放電點之距離為最小之受電點(例如,第29圖之受電點332a)之距離,比從該某放電點到副受電線中之受電點中與該某放電點之距離為最小之受電點(例如,第29圖之受電點332b或332c)之距離更短。 According to a third aspect of the present invention, in the ion and ozone wind generating apparatus of the present invention, the plurality of electric wires (for example, the power receiving units 331a to 331c of Fig. 29) are the main receiving wires (for example, Fig. 29). Any one of the power receiving unit 331a) and the sub-receiving line (for example, the power receiving units 331b and 331c of FIG. 29) and a discharge point from the one discharge line (for example, the discharge portion 321 of FIG. 29) (for example) , the discharge point 322 of FIG. 29 is a distance from the power receiving point of the power receiving point in the main receiving line to the receiving point of the certain discharging point (for example, the power receiving point 332a of FIG. 29), and the discharge is from the certain discharge. The distance from the power receiving point in the secondary receiving line to the receiving point which is the smallest distance from the certain discharging point (for example, the power receiving point 332b or 332c in Fig. 29) is shorter.

本發明(4)係本發明(2)之離子、臭氧風產生裝置,其係從前述一條放電線(例如,第4圖之放電部321)中之某放電點(例如,第4圖之放電點322)到屬於某受電線(例如,第4圖之受電部331A)中之受電點之與該某放電點之距離為最小之受電點(例如,第4圖之受電點332A)之距離,與從該某放電點到屬於與該某受電線不同的受電線(例如,第4圖之受電部331D)中之受電點之與該某放電點之距離為最小之受電點(例如,第4圖之受電點332D)之距離,成為大致相同。 The invention (4) is the ion and ozone wind generating device of the invention (2), which is a discharge point from the one discharge line (for example, the discharge portion 321 of Fig. 4) (for example, the discharge of Fig. 4) Point 322) the distance from the power receiving point (for example, the power receiving point 332A of FIG. 4) whose power receiving point in a certain power receiving line (for example, power receiving unit 331A in FIG. 4) is the smallest distance from the certain discharging point, A power receiving point having a minimum distance from the power receiving point of the power receiving line (for example, the power receiving unit 331D of FIG. 4) different from the certain receiving line to the certain discharging point (for example, the fourth point) The distances of the power receiving points 332D) of the figure are substantially the same.

本發明(5)係本發明(1)至(4)任一者之離子、臭氧風產生裝置,其係放電線(例如,第32圖之放電部321)及受電線(例如,第32圖之受電部331)為線段。 The present invention (5) is an ion or ozone wind generating device according to any one of the inventions (1) to (4), which is a discharge line (for example, the discharge portion 321 of Fig. 32) and a receiving wire (for example, Fig. 32) The power receiving unit 331) is a line segment.

本發明(6)係本發明(5)之離子、臭氧風產生裝置,其係 前述線段為曲線,且放電線(例如,第32圖之放電部321)與受電線(例如,第32圖之受電部331)往相同方向彎曲。 The invention (6) is the ion and ozone wind generating device of the invention (5), The line segment is a curved line, and the discharge line (for example, the discharge portion 321 of FIG. 32) is bent in the same direction as the power receiving wire (for example, the power receiving portion 331 of FIG. 32).

本發明(7)係本發明(1)至(4)之任一者的離子、臭氧風產生裝置,其係放電線(例如,第24圖之放電部321)及受電線(例如,第24圖之受電部331)為環狀。 The present invention (7) is the ion or ozone wind generating device according to any one of the inventions (1) to (4), which is a discharge line (for example, the discharge portion 321 of Fig. 24) and a receiving wire (for example, the 24th) The power receiving unit 331) in the figure has a ring shape.

本發明(8)係本發明(7)之離子、臭氧風產生裝置,其係放電線(例如第24圖之放電部321、第29圖之放電部321)與受電線(例如,第24圖之受電部331、第29圖之受電部331)為相似。 The present invention (8) is the ion or ozone wind generating device according to the invention (7), which is a discharge line (for example, the discharge portion 321 of Fig. 24, the discharge portion 321 of Fig. 29) and a receiving wire (for example, Fig. 24) The power receiving unit 331 and the power receiving unit 331 of Fig. 29 are similar.

<附記> <attachment>

此外,就與前述之本發明的事項相關之事項,預先列記如下,而不限定於上述事項而可實施。 In addition, matters relating to the matters of the present invention described above are listed in advance as follows, and are not limited to the above matters and can be implemented.

另外的態樣之發明(1)係一種離子、臭氧風 產生裝置,其係構成為具備複數組具有針狀電極與對向電極之電極對,且使電位差產生在各個電極對之間並利用電暈放電產生離子、臭氧及離子風;而各個電極對之對向電極係形成平面狀且為環狀或渦狀;並構成為,具備屬於一組電極對之主電極對,以及屬於以沿著主電極對之對向電極的外周包圍主電極對之對向電極的方式,以有規則地且相互鄰接或接近之形態定位對向電極之電極對之副電極對,且至少於副電極對中鄰接的對向電極之外周間的最短距離為對向電極之直徑以下且所有的對向電極之平面狀的法線向量成為大致相同方向;而主電極對之對向電極及副電極對的對向電極係由平板狀的導電構件中之貫穿孔所形 成,且於該平板狀的導電構件,係沿著副電極對之對向電極的外周更形成有貫穿孔。 Another aspect of the invention (1) is an ion, ozone wind a generating device comprising: a plurality of electrode pairs having a plurality of arrays of needle electrodes and counter electrodes; wherein a potential difference is generated between the pair of electrodes and generating ions, ozone, and ion wind by corona discharge; and each electrode pair The counter electrode system is formed in a planar shape and has a ring shape or a spiral shape; and is configured to include a pair of main electrodes belonging to one set of electrode pairs and a pair of outer circumferences surrounding the pair of main electrodes along the counter electrode of the pair of main electrodes In the manner of the electrodes, the pair of secondary electrodes of the pair of electrodes facing the counter electrode are positioned regularly and adjacent to each other or in close proximity, and at least the shortest distance between the outer circumferences of the adjacent counter electrodes in the pair of the secondary electrodes is the counter electrode Below the diameter, the planar normal vectors of all the counter electrodes are substantially in the same direction; and the counter electrode of the counter electrode and the counter electrode pair of the main electrode pair is formed by a through hole in the flat conductive member In the flat conductive member, a through hole is formed along the outer circumference of the counter electrode of the pair of counter electrodes.

另外的態樣之發明(2)係前述另外的態樣之發明(1)的離子、臭氧風產生裝置,其具有對向電極為平面狀之主環狀對向電極以及包圍主環狀對向電極之平面狀的副環狀對向電極;某電極對之針狀電極的前端與該某電極對之主環狀對向電極之最長距離,比該某電極對之針狀電極的前端與該某電極對之副環狀對向電極的最短距離更短。 According to another aspect of the invention, there is provided an ion and ozone wind generating device according to the invention of the above aspect (1), which has a main annular counter electrode having a planar counter electrode and a main annular opposite direction a planar sub-annular counter electrode of the electrode; a longest distance between a front end of the needle electrode of the electrode pair and the main annular counter electrode of the pair of electrodes, and a front end of the needle electrode of the pair of electrodes The shortest distance of the secondary annular counter electrode of an electrode pair is shorter.

另外的態樣的發明(3)係前述另外的態樣的發明(1)或(2)之離子、臭氧風產生裝置,其係所有的電極對之對向電極的形狀大致相同。 In another aspect of the invention (3), the ion or ozone wind generating device of the invention of the above aspect (1) or (2) is characterized in that the shape of the counter electrode of all the electrode pairs is substantially the same.

另外的態樣的發明(4)係一種離子、臭氧風產生裝置,其係構成為具備複數組具有針狀電極與對向電極之電極對,且在各個電極對之間使電位差產生並利用電暈放電產生離子、臭氧及離子風;而各個電極對之對向電極形成為平面狀且為環狀或渦狀;並構成為具備屬於一組電極對之主電極對,以及屬於以沿著主電極對之對向電極的外周包圍主電極對之對向電極之方式,以有規則地且相互鄰接或接近之形態定位對向電極之電極對之副電極對,且至少在副電極對中鄰接的對向電極之外周間的最短距離在對向電極之直徑以下且所有的對向電極之平面狀的法線向量成為大致相同方向;而對向電極具有平面狀的主環狀對向電極以及包圍主環狀對向電極之平面狀的副環狀對向電極;且某電極對之針狀電極的前端與該某電極對之主環狀對向電 極的最長距離比該某電極對之針狀電極的前端與該某電極對之副環狀對向電極的最短距離更短。 Further, the invention (4) is an ion and ozone wind generating device which is configured to include an electrode pair having a needle array electrode and a counter electrode in a complex array, and to generate and utilize a potential difference between each electrode pair. The halo discharge generates ions, ozone and ion wind; and the counter electrode of each electrode pair is formed into a planar shape and is annular or spiral; and is configured to have a pair of main electrodes belonging to a pair of electrode pairs, and belongs to The outer circumference of the opposite electrode of the pair of electrodes surrounds the opposite electrode of the pair of main electrodes, and the pair of auxiliary electrodes of the pair of electrodes of the opposite electrode are positioned regularly and adjacent to each other or close to each other, and at least adjacent to the pair of secondary electrodes The shortest distance between the outer circumferences of the counter electrode is below the diameter of the counter electrode and the planar normal vectors of all the counter electrodes are substantially in the same direction; and the counter electrode has a planar main annular counter electrode and a planar sub-annular counter electrode surrounding the main annular counter electrode; and the front end of the needle electrode of the pair of electrodes is opposite to the main ring of the pair of electrodes The longest distance of the pole is shorter than the shortest distance between the front end of the needle electrode of the pair of electrodes and the auxiliary annular counter electrode of the pair of electrodes.

另外的態樣的發明(5)係前述另外的態樣的發明(4)之離子、臭氧風產生裝置,其係主電極對之對向電極及副電極對之對向電極由平板狀的導電構件之貫穿孔所形成,且於該平板狀的導電構件,係沿著副電極對之對向電極的外周更形成有貫穿孔。 According to another aspect of the invention (5), the ion and ozone wind generating device of the invention (4) of the above aspect is characterized in that the counter electrode of the counter electrode and the counter electrode pair of the main electrode pair is plate-shaped conductive The through hole of the member is formed, and the flat conductive member is formed with a through hole along the outer circumference of the counter electrode of the pair of counter electrodes.

另外的態樣的發明(6)係前述另外的態樣的發明(4)或(5)之離子、臭氧風產生裝置,其係所有的電極對之對向電極的形狀大致相同。 In another aspect of the invention (6), the ion or ozone wind generating device of the invention of the above aspect (4) or (5) is characterized in that the shape of the counter electrode of all the electrode pairs is substantially the same.

另外的態樣的發明(7)係一種離子、臭氧風產生裝置(例如,第15圖及第17圖至第20圖所示之形態),其係具備有複數組具有針狀電極與對向電極之電極對,而構成為在各個電極對之間使電位差產生且利用電暈放電產生離子、臭氧及離子風產生;並且各個電極對之對向電極形成平面狀且為環狀或渦狀;並構成為,具備屬於一組電極對之主電極對,以及屬於以沿著主電極對之對向電極的外周包圍主電極對之對向電極之方式,以有規則地且相互鄰接或接近之形態定位對向電極之電極對之副電極對,且至少在副電極對中鄰接的對向電極之外周間的最短距離在對向電極之直徑以下且所有的對向電極之平面狀的法線向量成為大致相同方向。 Another aspect of the invention (7) is an ion and ozone wind generating device (for example, the patterns shown in Fig. 15 and Figs. 17 to 20), which are provided with a complex array having needle electrodes and an opposite direction. The electrode pair of the electrode is configured to generate a potential difference between the pair of electrodes and generate ions, ozone and ion wind by corona discharge; and the opposite electrode of each electrode pair is formed in a planar shape and is annular or spiral; And configured to have a pair of main electrodes belonging to a pair of electrode pairs, and to belong to the opposite electrode of the main electrode pair along the outer circumference of the counter electrode of the main electrode pair, regularly and adjacent to each other or close to each other Forming the pair of secondary electrodes of the electrode pair of the counter electrode, and at least the shortest distance between the outer circumferences of the adjacent electrodes in the pair of the pair of electrodes is below the diameter of the counter electrode and the planar normal of all the counter electrodes The vectors become roughly the same direction.

另外的態樣的發明(8)係另外的態樣的發明(7)之離子、臭氧風產生裝置(例如,第43圖的右圖所示之形態),其係 主電極對之對向電極及副電極對之對向電極由平板狀的導電構件之貫穿孔所形成,且於該平板狀的導電構件,係沿著副電極對之對向電極的外周更形成有貫穿孔。 The invention (8) of another aspect is an ion and ozone wind generating device of the invention (7) of another aspect (for example, a form shown in the right drawing of Fig. 43), The counter electrode of the counter electrode and the counter electrode pair of the main electrode pair is formed by a through hole of a flat conductive member, and the flat conductive member is formed along the outer circumference of the counter electrode of the counter electrode pair. There are through holes.

另外的態樣的發明(9)係另外的態樣的發明(7)或(8)之離子、臭氧風產生裝置(例如,第15圖及第17圖至20,或第15圖所示之形態),其係對向電極具有平面狀的主環狀對向電極以及包圍主環狀對向電極之平面狀的副環狀對向電極,且某電極對之針狀電極的前端以及該某電極對之主環狀對向電極的最長距離,比該某電極對之針狀電極的前端與該某電極對之副環狀對向電極的最短距離更短。 Another aspect of the invention (9) is an ion or ozone wind generating device of another aspect (7) or (8) (for example, Fig. 15 and Figs. 17 to 20, or Fig. 15 a state in which the counter electrode has a planar main annular counter electrode and a planar sub-annular counter electrode surrounding the main annular counter electrode, and the front end of the needle electrode of the pair of electrodes and the certain The longest distance of the main annular counter electrode of the pair of electrodes is shorter than the shortest distance between the front end of the needle electrode of the pair of electrodes and the sub-annular counter electrode of the pair of electrodes.

另外的態樣的發明(10)係另外的態樣的發明(7)至(9)任一者之離子、臭氧風產生裝置(例如,第15圖所示之形態),其係所有的電極對之對向電極的形狀大致相同。 Further, the invention (10) is an ion or ozone wind generating device (for example, the form shown in Fig. 15) of any of the inventions (7) to (9), which is an electrode of all aspects. The shape of the counter electrode is substantially the same.

在此就本說明書中所使用之各用語加以說 明。所謂「殺菌、除臭對象物」係指只要為細菌會繁殖者或釋出惡臭者,即沒特別限定,例如,可舉出生鮮食品等之廚餘、糞尿、尿布等之髒物、儲存的水等之具體例。所謂「配置殺菌、除臭對象物的空間」,係指只要配置有前述殺菌、除臭對象物,即沒特別限定,例如,氣密性高的箱子,更具體而言,可舉出廚餘與尿布等之污物容器,氣密性高的附冷凍、冷藏裝置之貨櫃及附冷凍、冷藏裝置之車輛等。所謂「環狀」,係廣泛指由中心部開口之由直線及/或曲線所構成之閉曲面,尤其最好為三角形以上(最好是6角形以上)的多角形或圓形、或類圓形狀。所謂「渦狀」例 如係指三角形以上(最好是6角形以上)的多角形或圓形或類圓形狀,且朝向中心而捲成旋渦者,於捲成旋渦之態樣(例如,捲繞數與捲繞寬度,或終點之有無)方面沒特別限定。所謂「平面狀」,一般而言係指於可視為平面之程度之在環狀電極中相對於環內的總面積其厚度較小的電極。更具體而言,雖沒特別限定,但最好是[厚度(mm)]/[環內總面積(cm2)]在1.5以下,更佳的是1以下,更理想的是0.8以下。下限值雖沒特別限定,但例如為0.0001。此外,變形(對平面之變形)亦可為厚度程度。更具體而言,主環狀對向電極的總面積為7cm2、厚度7mm以下,於變形上更理想的亦在7mm以下。所謂某平面狀與別的平面狀為「相同平面」,係指某平面狀與別的平面狀之距離為就一般而言可視為相同平面之程度。例如,從側面看某平面狀與別的平面狀時,某平面狀與別的平面狀為平行,並且有厚度重疊之部分存在之情況等。所謂「前述針狀電極的前端與主環狀對向電極之最長距離」係指於針狀電極的前端與主環狀對向電極的環之內端且為厚度方向最近的部分之距離中,其最長的距離的意思。所謂「前述針狀電極的前端與副環狀對向電極之最短距離」,係指於針狀電極的前端與副環狀對向電極的環之內端且為厚度方向最近的部分之距離中,其最短的距離之意思。所謂「主離子風」係指從主環狀對向電極之中心的開口部發出的離子風。所謂「副離子風」係指從副環狀對向電極發出的離子風。所謂「於電極對之間產生電位差」,例如可舉出施加電壓到針狀電極,且將對向電極設 為接地時產生之電位差,此時,有關針狀電極之極性(陽極、陰極)沒特別限定。 The terms used in this specification are described herein. The "sterilization and deodorization target" is not particularly limited as long as it is a bacteria-producing person or a person who releases a bad smell. For example, it is possible to store food such as food waste, excrement, diaper, etc., and store it. Specific examples of water and the like. The space for arranging the sterilizing and deodorizing object is not particularly limited as long as the sterilizing and deodorizing object is disposed, and for example, a box having high airtightness, and more specifically, a kitchen waste A dirt container such as a diaper, a container with a high airtightness, a container with a freezing and refrigerating device, and a vehicle with a freezing and refrigerating device. The term "ring" generally refers to a closed curved surface composed of a straight line and/or a curved line formed by a central portion, and particularly preferably a polygonal shape or a circle or a circle having a triangular shape or more (preferably a hexagonal shape or more). shape. The term "vortex" means, for example, a polygonal shape or a circular or round-like shape of a triangle or more (preferably a hexagonal shape or more), and is rolled into a vortex toward the center, and is wound into a vortex (for example, winding). There is no particular limitation on the number and winding width, or the presence or absence of the end point. The term "planar" generally means an electrode having a small thickness in the annular electrode relative to the total area in the ring, which is considered to be a plane. More specifically, although not particularly limited, it is preferable that [thickness (mm)] / [total area (cm 2 ) in the ring] is 1.5 or less, more preferably 1 or less, and still more preferably 0.8 or less. The lower limit is not particularly limited, but is, for example, 0.0001. In addition, the deformation (deformation to the plane) may also be the degree of thickness. More specifically, the total area of the main annular counter electrode is 7 cm 2 and a thickness of 7 mm or less, and more preferably 7 mm or less in deformation. The fact that a certain planar shape and the other planar shape are "identical planes" means that the distance between a certain planar shape and another planar shape is generally considered to be the same plane. For example, when a certain planar shape and another planar shape are seen from the side, a certain planar shape is parallel to another planar shape, and a portion having a thickness overlap exists. The "longest distance between the tip end of the needle electrode and the main annular counter electrode" means the distance between the tip end of the needle electrode and the inner end of the ring of the main annular counter electrode and the portion closest to the thickness direction. The meaning of its longest distance. The term "the shortest distance between the tip end of the needle electrode and the sub-annular counter electrode" means the distance between the tip end of the needle electrode and the inner end of the ring of the sub-annular counter electrode and the portion closest to the thickness direction. , the meaning of its shortest distance. The "main ion wind" refers to the ion wind emitted from the opening of the center of the main annular counter electrode. The "secondary ion wind" refers to the ion wind emitted from the secondary annular counter electrode. The term "potential difference between electrode pairs" includes, for example, a potential difference generated when a voltage is applied to the needle electrode and the counter electrode is grounded. At this time, the polarity of the needle electrode (anode, cathode) is not Specially limited.

依據本發明(1)之離子、臭氧風產生裝置,其藉由設置連續形成有放電點之放電線以及連續形成有受電點之受電線,且從該放電線朝向該受電線產生電暈放電,而於該受電線之不與該放電線相對向之側,可廣範圍地且以加強含有離子及臭氧之離子風的風力本身之方式使離子、臭氧風產生。 An ion and ozone wind generating device according to the invention (1), wherein a discharge line in which a discharge point is continuously formed and a power receiving line in which a power receiving point is continuously formed are provided, and a corona discharge is generated from the discharge line toward the power receiving line, On the side of the receiving wire that does not face the discharge line, ions and ozone wind can be generated in a wide range of ways to enhance the wind power of the ion wind containing ions and ozone.

依據本發明(2)之離子、臭氧風產生裝置,藉由從複數條放電線產生離子風,而除了前述效果之外,可更廣泛地使離子風遍佈。 According to the ion and ozone wind generating apparatus of the invention (2), by generating ion wind from a plurality of discharge lines, in addition to the aforementioned effects, the ion wind can be more widely distributed.

依據本發明(3)之離子、臭氧風產生裝置,以被從副受電線產生之離子風推動之形態將從主受電線產生之離子風往前面推出,故可達到即縱使將該離子、臭氧風產生裝置之電極對予以小型化,亦盡可能不刪減電暈放電所產生之離子風的風力之功效。 According to the ion and ozone wind generating device of the invention (3), the ion wind generated from the main receiving wire is pushed forward in a form driven by the ion wind generated by the sub-receiving wire, so that the ion and the ozone can be obtained. The electrode pair of the wind generating device is miniaturized, and the effect of the wind of the ion wind generated by the corona discharge is not removed as much as possible.

依據本發明(4)之離子、臭氧風產生裝置,藉由從放電線之某放電點到屬於某受電線之受電點之與該某放電點之距離成為最小之受電點的距離,與從該某放電點到屬於與該某受電線不同之受電線之受電點之與該某放電點之距離成為最小之受電點的距離大致相同,使得從各受電點產生大致相同的風量之離子風,並可產生立體且廣泛遍佈的離子風。 According to the ion and ozone wind generating apparatus of the invention (4), the distance from the discharge point of the discharge line to the power receiving point of the receiving point of a certain receiving line which is the distance from the certain discharging point becomes the minimum receiving point a discharge point is substantially the same as a distance between the power receiving points of the power receiving lines different from the one of the receiving wires and the power receiving point at which the distance from the certain discharging point is the smallest, so that the ion winds of substantially the same air volume are generated from the respective power receiving points, and It can produce a three-dimensional and widely distributed ion wind.

依據本發明(5)之離子、臭氧風產生裝置, 除了前述效果之外,藉由將離子、臭氧風產生裝置之放電部及受電部設為線段,而在將該離子、臭氧風產生裝置設置在房間的之情況等,可設為適當的形狀。 An ion, ozone wind generating device according to the invention (5), In addition to the above-mentioned effects, the ion and the ozone generating device can be placed in a room by using the discharge portion and the power receiving portion of the ion wind generating device as a line segment, and the like.

依據本發明(6)之離子、臭氧風產生裝置, 除了前述效果之外,藉由將離子、臭氧風產生裝置的放電部及受電部設為曲線狀之線段,且使該放電部與該受電部往相同方向彎曲,而在將該離子、臭氧風產生裝置設置在房間的角落時成為適當的形狀,並可使離子、臭氧風廣泛遍佈且均勻地產生。 An ion, ozone wind generating device according to the invention (6), In addition to the above-described effects, the discharge portion and the power receiving portion of the ion and ozone wind generating device are formed into a curved line segment, and the discharge portion and the power receiving portion are bent in the same direction, and the ion and ozone wind are used. When the generating device is installed at a corner of the room, it becomes an appropriate shape, and ions and ozone winds can be widely distributed and uniformly generated.

依據本發明(7)之離子、臭氧風產生裝置, 除了前述效果之外,藉由將離子、臭氧風產生裝置之放電部及受電部設為環狀,可使離子、臭氧風於該受電部之周圍360度產生,且將該離子、臭氧風產生裝置設置房間的天花板中央等時,可使離子、臭氧風遍佈整個房間。 An ion, ozone wind generating device according to the invention (7), In addition to the above-described effects, by making the discharge portion and the power receiving portion of the ion and ozone wind generating device annular, ions and ozone wind can be generated 360 degrees around the power receiving portion, and the ions and ozone wind can be generated. When the device is installed in the center of the ceiling of the room, the ion and ozone winds can be spread throughout the room.

依據本發明(8)之離子、臭氧風產生裝置, 除了前述效果之外,藉由將離子、臭氧風產生裝置的放電部與受電部設為相似,可使該放電部的放電點與該受電部之受電點的距離均等地接近,可使從該受電部產生之離子、臭氧風的風量均等地接近。 An ion, ozone wind generating device according to the invention (8), In addition to the above-described effects, the discharge portion of the ion and ozone wind generating device is similar to the power receiving portion, so that the distance between the discharge point of the discharge portion and the power receiving point of the power receiving portion can be uniformly obtained. The air volume generated by the power receiving unit and the ozone wind are equally close.

100、100-2、100-3‧‧‧離子、臭氧風產生裝置 100, 100-2, 100-3‧‧‧ ion, ozone wind generator

110、210、310‧‧‧電極對 110, 210, 310‧‧‧ electrode pairs

120(120a至120g)、220‧‧‧針狀電極 120 (120a to 120g), 220‧‧‧ needle electrode

320(320a至320c)‧‧‧放電電極 320 (320a to 320c) ‧‧ discharge electrodes

321(321a至321c)‧‧‧放電部 321 (321a to 321c) ‧ ‧ discharge section

322‧‧‧放電點 322‧‧‧Discharge point

130(130a至130g)、230、330(330a至330c)(330A至330D)‧‧‧對向電極 130 (130a to 130g), 230, 330 (330a to 330c) (330A to 330D) ‧‧ ‧ counter electrode

331(331a至331c)(331A至331D)‧‧‧受電部 331 (331a to 331c) (331A to 331D) ‧‧‧Power Management Department

332(332A至332D)‧‧‧受電點 332 (332A to 332D) ‧ ‧ power receiving point

131至133‧‧‧環狀對向電極 131 to 133‧‧‧ annular counter electrode

139‧‧‧橋接器 139‧‧‧ Bridge

140‧‧‧離子風引導構件 140‧‧‧Ion wind guiding member

141、340‧‧‧噴出口 141, 340‧‧‧ spout

150‧‧‧送風路徑 150‧‧‧Air supply path

200‧‧‧離子風產生裝置 200‧‧‧Ion wind generating device

350‧‧‧蓋罩單元 350‧‧‧ Cover unit

360‧‧‧蓋罩構件 360‧‧‧ Cover member

370‧‧‧蓋構件 370‧‧‧covering components

380‧‧‧固定構件 380‧‧‧Fixed components

400‧‧‧天花板 400‧‧‧ ceiling

500‧‧‧牆壁 500‧‧‧ wall

P‧‧‧前端部 P‧‧‧ front end

第1圖係該裝置的電極對之概念正視圖。 Figure 1 is a conceptual front view of an electrode pair of the device.

第2圖係該裝置的電極對之概念正視圖。 Figure 2 is a conceptual front view of the electrode pair of the device.

第3圖係該裝置之電極對的概念剖面圖。 Figure 3 is a conceptual cross-sectional view of an electrode pair of the device.

第4圖係該裝置之電極對的概念剖面圖。 Figure 4 is a conceptual cross-sectional view of an electrode pair of the device.

第5圖(a)係該裝置之對向電極的概念正視圖,第5圖(b)係離子、臭氧風產生裝置100之概念側視圖。 Fig. 5(a) is a conceptual front view of the counter electrode of the device, and Fig. 5(b) is a conceptual side view of the ion and ozone wind generating device 100.

第6圖(a)係使用位於最內部之輪狀電極131的剖面,表示輪狀電極131與針狀電極120之前端部P的位置關係之圖,第6圖(b)係表示輪狀電極132與前端P的位置關係之圖。 Fig. 6(a) is a view showing a positional relationship between the wheel electrode 131 and the front end portion P of the needle electrode 120 using a cross section of the innermost wheel electrode 131, and Fig. 6(b) shows a wheel electrode. A map of the positional relationship between 132 and the front end P.

第7圖(a)係該裝置之對向電極130的概念正視圖,第7圖(b)係離子、臭氧風產生裝置100之概念側視圖。 Fig. 7(a) is a conceptual front view of the counter electrode 130 of the apparatus, and Fig. 7(b) is a conceptual side view of the ion and ozone wind generating apparatus 100.

第8圖(a)係該裝置的對向電極之概念正視圖,第8圖(b)係離子、臭氧風產生裝置100之概念側視圖。 Fig. 8(a) is a conceptual front view of the counter electrode of the device, and Fig. 8(b) is a conceptual side view of the ion and ozone wind generating device 100.

第9圖(a)係該裝置的對向電極之概念正視圖,第9圖(b)係離子、臭氧風產生裝置100的概念側視圖。 Fig. 9(a) is a conceptual front view of the counter electrode of the device, and Fig. 9(b) is a conceptual side view of the ion and ozone wind generating device 100.

第10圖(a)至(d)係作為本實施形態之對向電極而可使用之板狀對向電極的概略圖。 Fig. 10 (a) to (d) are schematic views of a plate-shaped counter electrode which can be used as a counter electrode of the present embodiment.

第11圖係離子、臭氧風產生裝置100之概念平面圖。 Fig. 11 is a conceptual plan view of the ion and ozone wind generating device 100.

第12圖(a)係該裝置的對向電極130之概念正視圖,第12圖(b)係離子、臭氧風產生裝置100之概念側視圖。 Fig. 12(a) is a conceptual front view of the counter electrode 130 of the apparatus, and Fig. 12(b) is a conceptual side view of the ion and ozone wind generating apparatus 100.

第13圖係離子、臭氧風產生裝置100之概念平面圖。 Fig. 13 is a conceptual plan view of the ion and ozone wind generating device 100.

第14圖(a)係離子、臭氧風產生裝置之概念平面圖,第14圖(b)係離子、臭氧風產生裝置之概念側視圖,第14圖(c)係從離子、臭氧風產生裝置的噴出口側所看的概念正視圖。 Fig. 14(a) is a conceptual plan view of an ion and ozone wind generating device, Fig. 14(b) is a conceptual side view of an ion and ozone wind generating device, and Fig. 14(c) is an ion and ozone generating device. A conceptual front view of the outlet side.

第15圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 15 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第16圖係另外的形態之離子、臭氧風產生裝置的概念作用圖。 Fig. 16 is a conceptual diagram of the action of an ion and an ozone wind generating device of another form.

第17圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 17 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第18圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 18 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第19圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 19 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第20圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 20 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第21圖(a)至(c)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 21 (a) to (c) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

第22圖(a)及(b)係另外的形態之對向電極的概念圖。 Fig. 22 (a) and (b) are conceptual diagrams of the counter electrode of another form.

第23圖(a)及(b)係另外的形態之針狀電極的概念圖。 Fig. 23 (a) and (b) are conceptual diagrams of needle electrodes of another form.

第24圖(a)及(b)係第2實施形態之電極對的概念圖。 Fig. 24 (a) and (b) are conceptual diagrams of electrode pairs of the second embodiment.

第25圖(a)及(b)係第2實施形態之離子、臭氧產生裝置100-2的使用例之圖。 Fig. 25 (a) and (b) are diagrams showing an example of use of the ion or ozone generating apparatus 100-2 of the second embodiment.

第26圖(a)及(b)係第2實施形態之電極對的概念圖。 Fig. 26 (a) and (b) are conceptual diagrams of electrode pairs of the second embodiment.

第27圖係第2實施形態之電極對的概念圖。 Fig. 27 is a conceptual diagram of an electrode pair of the second embodiment.

第28圖係第2實施形態之電極對的概念圖。 Fig. 28 is a conceptual diagram of an electrode pair of the second embodiment.

第29圖(a)至(c)係第2實施形態之放電電極及對向電極的概念圖。 Fig. 29 (a) to (c) are conceptual diagrams of the discharge electrode and the counter electrode of the second embodiment.

第30圖係第2實施形態之放電電極及對向電極的概念圖。 Fig. 30 is a conceptual diagram of a discharge electrode and a counter electrode of the second embodiment.

第31圖(a)至(c)係第2實施形態之放電電極及對向電極的概念圖。 Fig. 31 (a) to (c) are conceptual diagrams of the discharge electrode and the counter electrode of the second embodiment.

第32圖(a)及(b)係第3實施形態之電極對的概念圖。 Fig. 32 (a) and (b) are conceptual diagrams of electrode pairs of the third embodiment.

第33圖(a)及(b)係第3實施形態的離子、臭氧產生裝置100-3之使用例的圖。 Fig. 33 (a) and (b) are diagrams showing an example of use of the ion or ozone generating apparatus 100-3 of the third embodiment.

第34圖(a)至(c)係第3實施形態之放電電極及對向電極的概念圖。 Fig. 34 (a) to (c) are conceptual diagrams of the discharge electrode and the counter electrode of the third embodiment.

第35圖係第3實施形態之放電電極及對向電極的概念圖。 Fig. 35 is a conceptual diagram of a discharge electrode and a counter electrode of the third embodiment.

第36圖(a)至(c)係第3實施形態之放電電極及對向電極的概念圖。 Fig. 36 (a) to (c) are conceptual diagrams of the discharge electrode and the counter electrode of the third embodiment.

第37圖係實驗裝置之對向電極的第1構造圖。 Figure 37 is a first structural view of the counter electrode of the experimental apparatus.

第38圖係實驗裝置之對向電極的第2構造圖。 Figure 38 is a second structural view of the counter electrode of the experimental apparatus.

第39圖係實驗裝置之對向電極的第3構造圖。 Figure 39 is a third structural view of the counter electrode of the experimental apparatus.

第40圖係實驗裝置之對向電極的第4構造圖。 Fig. 40 is a fourth structural view of the counter electrode of the experimental apparatus.

第41圖係實驗裝置之對向電極的第5構造圖。 Figure 41 is a fifth structural view of the counter electrode of the experimental apparatus.

第42圖係使用實驗裝置之測量方法的說明圖。 Fig. 42 is an explanatory diagram of a measuring method using an experimental apparatus.

第43圖係對向電極之變形例的概念圖。 Fig. 43 is a conceptual diagram of a modification of the counter electrode.

第44圖(a)至(d)係另外的形態之針狀電極及對向電極的概念圖。 Fig. 44 (a) to (d) are conceptual diagrams of a needle electrode and a counter electrode of another embodiment.

於說明本發明之離子、臭氧風產生裝置的 詳細情況之前,參照第1圖至第4圖,就本發明之離子、臭氧風產生裝置(後述的第2實施形態之離子、臭氧風產生裝置)的概要加以說明。 For explaining the ion and ozone wind generating device of the present invention In the details, the outline of the ion and ozone wind generator (the ion and ozone wind generator of the second embodiment to be described later) of the present invention will be described with reference to Figs. 1 to 4 .

作為本發明之離子、臭氧風產生裝置100-3 具有之電極對310的一例,如第1圖及第2圖所示,可舉出由具有線狀的放電部(放電線)321之放電電極320以及具有線狀的受電部(受電線)331之對向電極330所構成之電極對310(有關電極對、放電電極、放電部、放電線、放電點、對向電極,受電部、受電線、受電點的詳細內容將後述)。 更詳細而言,放電部321及受電部331為環狀,受電部331比放電部321的直徑更大,而以於與配置有放電部321之平面平行的平面配置有受電部331之方式所構成。 As the ion and ozone wind generating device 100-3 of the present invention As an example of the electrode pair 310, as shown in FIG. 1 and FIG. 2, a discharge electrode 320 having a linear discharge portion (discharge line) 321 and a linear power reception unit (receiving wire) 331 are exemplified. The electrode pair 310 (the electrode pair, the discharge electrode, the discharge portion, the discharge line, the discharge point, the counter electrode, the power receiving unit, the power receiving line, and the power receiving point) of the counter electrode 330 will be described later. More specifically, the discharge portion 321 and the power receiving portion 331 are annular, and the power receiving portion 331 has a larger diameter than the discharge portion 321 and is disposed such that the power receiving portion 331 is disposed on a plane parallel to the plane in which the discharge portion 321 is disposed. Composition.

此外,第1圖之電極對310係藉由將放電部 321及受電部331配置為相同圓心狀,而以於該放電部321與受電部331之間大致均等地產生電暈放電之方式所構成。另一方面,第2圖之電極對310係放電部321在圓外周施加突起(棘)之形狀,而以在該突起的前端上集中性地容易產生電暈放電之方式所構成。再者,第1圖之放電電極320(放電部321)與第2圖之放電電極320(放電部321)為相同的形狀,而放電電極320(放電部321)的外周皆呈邊緣狀(朝向受電部331形成銳角之形狀)。 In addition, the electrode pair 310 of FIG. 1 is by the discharge portion The 321 and the power receiving unit 331 are arranged in the same center shape, and are configured such that the discharge portion 321 and the power receiving unit 331 generate a corona discharge substantially uniformly. On the other hand, in the electrode pair 310 of the second figure, the discharge portion 321 is formed in the shape of a projection (thorn) on the outer circumference of the circle, and is configured such that corona discharge is easily generated in a concentrated manner at the tip end of the projection. Further, the discharge electrode 320 (discharge portion 321) of Fig. 1 has the same shape as the discharge electrode 320 (discharge portion 321) of Fig. 2, and the outer circumference of the discharge electrode 320 (discharge portion 321) is edge-shaped (toward The power receiving unit 331 forms an acute angle).

此外,電極對310係於分散在放電部(放電 線)321上之放電點322與分散在受電部(受電線)331上的受電點332之間產生電位差,且以在多點同時使電暈放電之 離子、臭氧、及離子風產生之方式所構成。亦即,如第1圖及第2圖所示之電極對310,在多點同時透過電暈放電使離子、臭氧、及離子風產生時,離子風會廣泛地飛散而遍佈受電部(受電線)331的周圍360度。因此,例如,藉由將電極對310設為可收納在手掌之程度的大小(最大的直徑為10至20cm程度),且將之設置在方形六張榻榻米的房間的天花板中央,則可使離子風飛散於整個房間,且利用含在該飛散之離子風的臭氧之氧化力,可將滯留在房間內之惡臭成分予以去除(脫臭、除菌)。再者,將電極對310之放電部321與受電部331予以相反地配置時(放電部321位於受電部331的外側時),由於會將離子風朝受電部(受電線)331的中心予以聚集,故例如藉由將電極對310設為收納在手掌之程度的大小(最大的直徑為10至20cm程度),且將之設置在垃圾箱的開口部等,即可防止惡臭成分從垃圾箱漏出。 In addition, the electrode pair 310 is dispersed in the discharge portion (discharge A potential difference is generated between the discharge point 322 on the line 321 and the power receiving point 332 dispersed on the power receiving portion (receiving electric wire) 331, and the corona discharge is simultaneously performed at a plurality of points. It consists of ions, ozone, and ion wind generation. In other words, when the electrode pair 310 shown in FIGS. 1 and 2 is simultaneously subjected to corona discharge to generate ions, ozone, and ion wind at a plurality of points, the ion wind is widely scattered and spread over the power receiving unit (receiving the electric wire). ) 331 around 360 degrees. Therefore, for example, by setting the electrode pair 310 to a size that can be accommodated in the palm (the largest diameter is about 10 to 20 cm), and placing it in the center of the ceiling of a room of six square tatami, the ion can be made. The wind flies in the entire room, and the odorous component of the ozone contained in the scattered ion wind can be used to remove the odorous components remaining in the room (deodorization, sterilization). When the discharge portion 321 of the electrode pair 310 and the power receiving portion 331 are arranged oppositely (when the discharge portion 321 is located outside the power receiving portion 331), the ion wind is concentrated toward the center of the power receiving portion (receiving wire) 331. Therefore, for example, by setting the electrode pair 310 to the extent of the palm (the largest diameter is about 10 to 20 cm), and providing it in the opening of the garbage can, etc., it is possible to prevent the malodorous component from leaking out of the garbage can. .

此外,本發明之離子、臭氧風產生裝置就 該基本的概念而言,係具有一電極對,該電極對具有成為放電部(放電線)321之放電電極與成為受電部(受電線)331的對向電極,而隨著放電時產生之離子的流動方向(向量)產生之氣流成為所謂的離子風,惟在本專利申請案之發明中,亦著眼於透過該空氣流產生之負壓以及朝由該負壓所產生的空間之外氣的吸氣流所引起之離子風的增大效果。 亦即,於環狀的對向電極之內周邊緣部與存在於對向電極的內周側之放電電極之間產生電暈放電時,於該內周邊緣 部附近產生之離子風,會被釋出到環狀的對向電極之不與放電電極相對向之側,此時,於對向電極的環狀部外周側(不與放電電極相對向之側)產生負壓。然後,朝著該負壓產生之空間,尤其將圍繞對向電極的外周之外氣予以吸引,而藉由該被吸引之外氣將被推出到環狀的對向電極之不與放電電極相對之側的離子風之風力增大。 In addition, the ion and ozone wind generating device of the present invention is This basic concept has an electrode pair having a discharge electrode serving as a discharge portion (discharge line) 321 and a counter electrode serving as a power receiving portion (receiving wire) 331, and ions generated as the discharge occurs. The flow direction (vector) generated by the flow direction becomes a so-called ion wind, but in the invention of the present patent application, attention is also directed to the negative pressure generated by the air flow and the space outside the space generated by the negative pressure. The effect of increasing the ion wind caused by the suction flow. That is, when a corona discharge is generated between the inner peripheral edge portion of the annular counter electrode and the discharge electrode existing on the inner peripheral side of the counter electrode, the inner peripheral edge The ion wind generated in the vicinity of the portion is released to the side of the annular counter electrode that is not opposed to the discharge electrode, and at this time, on the outer peripheral side of the annular portion of the counter electrode (the side opposite to the discharge electrode) ) produces a negative pressure. Then, toward the space generated by the negative pressure, in particular, the gas surrounding the outer circumference of the counter electrode is attracted, and by the suction, the gas will be pushed out to the annular counter electrode without being opposed to the discharge electrode. The wind of the ion wind on the side increases.

其次,第3圖係表示第1圖之離子、臭氧風 產生裝置100-3或第2圖之離子、臭氧風產生裝置100-3之具體的使用例之概念剖面圖。第3圖之離子、臭氧風產生裝置100-3具有1個第1圖或第2圖之放電電極320、4個對向電極330。此外,第3圖之離子、臭氧風產生裝置100-3係以透過固定構件380被固定在天花板400之同時,從天花板400供應電力之方式所構成。再者,蓋罩單元350係成為誘導從對向電極330產生的離子風的引導構件,並且發揮保護離子、臭氧風產生裝置100-3的功能。此外,該蓋罩單元350在下部的開口部具有吸氣口,且藉由從該吸氣口進行吸氣,可使產生的離子風增大。 Next, Figure 3 shows the ion and ozone wind of Figure 1. A conceptual cross-sectional view of a specific use example of the generating device 100-3 or the ion and ozone wind generating device 100-3 of Fig. 2 . The ion/ozone wind generating device 100-3 of Fig. 3 has one discharge electrode 320 of the first or second drawing and four counter electrodes 330. Further, the ion and ozone wind generating device 100-3 of Fig. 3 is configured such that the transmission fixing member 380 is fixed to the ceiling 400 and the electric power is supplied from the ceiling 400. In addition, the cover unit 350 serves as a guide member that induces the ion wind generated from the counter electrode 330, and functions as a guard ion and an ozone wind generation device 100-3. Further, the cover unit 350 has an intake port at the opening portion of the lower portion, and the generated ion wind can be increased by sucking air from the intake port.

在此,在第3圖之離子、臭氧風產生裝置 100-3中,4個對向電極330A至330D(受電部331A至331D)成為相同的形狀、內徑,並大致平行地被配置在不同的平面上。因此,配置在與1個放電電極320(放電部321)接近的位置之對向電極{對向電極330B(受電部331B)、對向電極330C(受電部331C)}之受電點(受電點332B,332C),比起配置在遠的位置之對向電極{對向電極330A(受電部 331A)、對向電極330D(受電部331D)}之受電點(受電點332A,受電點332D),其在距離1個放電電極320(放電部321)之放電點322的距離變短。因此,在此1個放電電極320(放電部321)與對向電極{對向電極330B(受電部331B)、對向電極330C(受電部331C)}之間的電暈放電之產生比例變得最大,而從對向電極330B及330C產生之離子風的風力變得最大。然後,在此1個放電電極320(放電部321)與其他的對向電極{對向電極330A(受電部331A)、對向電極330D(受電部331D)}之間的電暈放電之產生比例相對變低,而從對向電極330A及對向電極330D產生之離子風的風力相對變弱。藉由以此方式來構成,以藉由透過對向電極330A及對向電極330D所產生的離子風之順風,而將由對向電極330B及對向電極330C產生之離子風以被推動之形態,推出到330B及對向電極330C之與放電電極320不相對向之側。由此來看,即使將第3圖之電極對310予以小型化,亦得到盡可能不將透過電暈放電產生之離子風的風力削減而廣泛地遍佈之效果。再者,在第3圖中,雖不將對向電極330配置在與放電電極320相同平面上,亦可依將對向電極330配置在相同平面上之方式來予以構成。 Here, the ion and ozone wind generating device in FIG. In 100-3, the four counter electrodes 330A to 330D (power receiving portions 331A to 331D) have the same shape and inner diameter, and are arranged substantially in parallel on different planes. Therefore, the power receiving point (power receiving point 332B) of the counter electrode {counter electrode 330B (power receiving unit 331B) and counter electrode 330C (power receiving unit 331C) disposed at a position close to one discharge electrode 320 (discharge portion 321) , 332C), opposite electrode (opposing electrode 330A (power receiving unit) 331A), the power receiving point of the counter electrode 330D (power receiving unit 331D)} (the power receiving point 332A, the power receiving point 332D), the distance from the discharge point 322 of the one discharge electrode 320 (discharge portion 321) becomes short. Therefore, the ratio of the corona discharge between the one discharge electrode 320 (discharge portion 321) and the counter electrode {counter electrode 330B (power receiving portion 331B) and the counter electrode 330C (power receiving portion 331C) becomes The wind force of the ion wind generated from the counter electrodes 330B and 330C becomes maximum. Then, the ratio of the corona discharge between the one discharge electrode 320 (discharge portion 321) and the other counter electrode {counter electrode 330A (power receiving portion 331A) and counter electrode 330D (power receiving portion 331D)} The relative wind is relatively low, and the wind of the ion wind generated from the counter electrode 330A and the counter electrode 330D is relatively weak. With this configuration, the ion wind generated by the counter electrode 330B and the counter electrode 330C is pushed by the downwind of the ion wind generated by the counter electrode 330A and the counter electrode 330D. It is pushed out to the side where 330B and the counter electrode 330C are not opposed to the discharge electrode 320. From this point of view, even if the electrode pair 310 of FIG. 3 is miniaturized, the effect of reducing the wind force of the ion wind generated by the corona discharge as much as possible is widely obtained. Further, in FIG. 3, the counter electrode 330 is not disposed on the same plane as the discharge electrode 320, and may be configured such that the counter electrode 330 is disposed on the same plane.

其次,第4圖係表示成為第1圖之離子、臭 氧風產生裝置100-3或第2圖之離子、臭氧風產生裝置100-3之與第3圖不同的態樣之使用例的概念剖面圖。與第3圖之離子、臭氧風產生裝置100-3之相異點係以4個對向電極330A至330D(受電部331A至331D)的內徑非為均等之 方式構成之點,於第4圖之離子、臭氧風產生裝置100-3的情況時,放電點322與各受電點(332A至332D)之距離,皆成為均等的距離。藉由以此方式來構成,而可從各受電點(332A至332D)產生大致相同風量之離子風,且可產生立體地且廣泛地遍佈之離子風。再者,在第4圖中亦與第3圖相同,亦可以將放電電極320與對向電極330配置在相同平面之方式來予以構成。 Next, Figure 4 shows the ion and smell that became the first figure. A conceptual cross-sectional view of an example of use of the oxygen wind generating device 100-3 or the ion and ozone wind generating device 100-3 of Fig. 2 different from Fig. 3 . The difference from the ion and ozone wind generating device 100-3 of Fig. 3 is that the inner diameters of the four counter electrodes 330A to 330D (the power receiving portions 331A to 331D) are not equal. In the case of the ion and ozone wind generating device 100-3 of Fig. 4, the distance between the discharge point 322 and each of the power receiving points (332A to 332D) is equal. By configuring in this manner, ion winds of substantially the same amount of wind can be generated from the respective power receiving points (332A to 332D), and ion winds which are stereoscopically and widely distributed can be generated. Further, in the fourth drawing, as in the third drawing, the discharge electrode 320 and the counter electrode 330 may be arranged on the same plane.

本發明之離子、臭氧風產生裝置係作為例 子可舉出如前述方式的構成,而至此種構成為止已研創有種種態樣的離子、臭氧風產生裝置。以下,藉由將這些的一個例子作為本實施形態,且就本實施形態之離子、臭氧風產生裝置加以詳述,而首先進行產生離子風之原理性的說明,且就思及本發明為止所研創之離子、臭氧風產生裝置的態樣依序加以說明。並且,關於於根據與本實施形態相同的理論而反覆創意研發後,而達到研創前述電極對310之點,以及成為前述電極對310的周邊技術之其他的構成,係於第2實施形態及第3實施形態依序加以說明。 The ion and ozone wind generating device of the present invention is taken as an example The configuration of the above-described embodiment is exemplified, and various types of ion and ozone wind generating devices have been developed up to such a configuration. Hereinafter, an example of these will be described as an embodiment of the present invention, and the ion and ozone wind generating device of the present embodiment will be described in detail. First, the principle of generating an ion wind will be described first, and the present invention will be considered. The state of the ion and ozone wind generating device of the research and development is described in order. In addition, regarding the development of the electrode pair 310 based on the same theory as that of the present embodiment, and the other configuration of the peripheral technology of the electrode pair 310, the second embodiment and the second embodiment are used. 3 Embodiments will be described in order.

首先,本實施形態之離子、臭氧風產生裝 置具備具有針狀電極與對向電極之電極對,且以使於前述針狀電極與前述對向電極之間產生電位差之方式來進行電暈放電而產生離子、臭氧及離子風。此外,本實施形態之離子、臭氧風產生裝置具有前述對向電極為平面狀的主環狀對向電極與包圍前述主環狀對向電極之平面狀的副環狀對向電極,且前述針狀電極的前端與前述主環狀對向電極 之最長距離比前述針狀電極的前端與前述副環狀對向電極之最短距離更短。 First, the ion and ozone wind generating device of the embodiment An electrode pair having a needle electrode and a counter electrode is provided, and corona discharge is generated to generate a potential difference between the needle electrode and the counter electrode to generate ions, ozone, and ion wind. Further, the ion and ozone wind generating apparatus according to the present embodiment includes a main annular counter electrode in which the counter electrode is planar and a planar sub-annular counter electrode surrounding the main annular counter electrode, and the needle Front end of the electrode and the aforementioned main annular counter electrode The longest distance is shorter than the shortest distance between the front end of the needle electrode and the sub-annular counter electrode.

透過該構成可得到大風量的離子風。在僅 為筒狀或一個平面圓形的對向電極時,放電係沿著在最短距離之反對極的筒狀電極內側或平面圓形電極之內側進行放電成環狀而產生環狀型離子風,故離子風中心的環狀中心部成為無風狀態。因此在有所發出的離子風有使用誘導無風中心部之能源而產生損失之結果,離子風變弱。藉由以本實施形態藉由設置主環狀對向電極與副環狀對向電極之方式來解決該問題。 With this configuration, a large amount of ion wind can be obtained. In only When it is a cylindrical or a flat circular counter electrode, the discharge system is discharged into a ring shape along the inner side of the cylindrical electrode at the shortest distance and the inner side of the circular electrode to generate a ring-shaped ion wind. The annular center portion of the ion wind center is in a windless state. Therefore, as a result of the loss of the ion wind emitted, the energy generated by the wind-free center portion is used, and the ion wind is weak. This problem is solved by providing the main annular counter electrode and the sub-annular counter electrode in this embodiment.

本實施形態之離子、臭氧風產生裝置具備 具有針狀電極與對向電極之電極對,且藉由以在前述針狀電極與前述對向電極之間產生電位差之方式進行電暈放電來產生離子、臭氧、及離子風。此外,離子風一般而言指一種空氣流,其係於電暈放電時藉由從針狀電極釋出之離子朝對向電極游動之間重覆與空氣分子的衝撞,而從針狀電極朝對向電極產生的空氣流。亦即,依照放電時產生之離子的流動方向而產生之氣流。以下,就本實施形態之離子、臭氧風產生裝置之詳細的構造加以說明。 The ion and ozone wind generating device of the embodiment has An electrode pair having a needle electrode and a counter electrode is provided, and ion, ozone, and ion wind are generated by performing corona discharge so as to generate a potential difference between the needle electrode and the counter electrode. In addition, the ion wind generally refers to an air flow which is caused by a collision between the ions released from the needle electrode and the swimming of the opposite electrode during the corona discharge, and the impact from the air molecules. The flow of air generated towards the opposite electrode. That is, the gas flow generated in accordance with the flow direction of the ions generated at the time of discharge. Hereinafter, the detailed structure of the ion and ozone wind generating device of the present embodiment will be described.

將本實施形態之離子、臭氧風產生裝置之 概略構造表示在第5圖。在此,第5圖(a)係該裝置的對向電極之概念正視圖,第5圖(b)係離子、臭氧風產生裝置100之概念側視圖。本形態之離子、臭氧風產生裝置100具備具有針狀電極120與對向電極130之電極對110。在此, 對向電極130具有位於配置在針狀電極120的延長線軸上之最內部的圓形環狀電極131以及與該電極配置在同軸上的半徑之不同的外側圓形環狀電極132。亦即,該等環狀電極係與環狀平面垂直,且以位於通過該環的重心(圓中心)之軸上之方式而配置。在環狀的對向電極中亦如此藉由使用具有圓形形狀的對向電極,而從針狀對向電極的前端,與對向電極之不同部分的距離成為大致相等,故放電不均現象變少。此外,以此方式藉由將針狀電極配置在環的軸上,尤其使得從主環狀對向電極產生之離子風變強。 The ion and ozone wind generating device of the embodiment The schematic structure is shown in Fig. 5. Here, Fig. 5(a) is a conceptual front view of the counter electrode of the device, and Fig. 5(b) is a conceptual side view of the ion and ozone wind generating device 100. The ion and ozone wind generation device 100 of the present embodiment includes an electrode pair 110 having a needle electrode 120 and a counter electrode 130. here, The counter electrode 130 has an outer circular circular electrode 131 disposed on the extension bobbin of the needle electrode 120 and an outer circular annular electrode 132 different in radius from the electrode. That is, the ring-shaped electrodes are perpendicular to the annular plane and are disposed so as to pass through the axis of the center of gravity (center of the circle) of the ring. In the annular counter electrode as well, by using the counter electrode having a circular shape, the distance from the front end of the needle-shaped counter electrode to the different portion of the counter electrode is substantially equal, so the discharge unevenness is caused. Fewer. Further, in this way, by arranging the needle electrodes on the axis of the ring, in particular, the ion wind generated from the main annular counter electrode becomes strong.

上述環狀電極131及132最好利用橋接器 139等之連結構件以可通電之方式予以橋接,藉由以此方式來構成,可將各環狀電極設為等電位,並可容易調整該等電極的位置關係。例如,以波狀構件連結時,在主環狀對向電極與副環狀對向電極之間形成具有大致三角形的形狀的部分,故於電暈放電產生不均而使離子風不會大量被推出到前方。因此,最好以對產生離子風不造成干擾之方式,以將連結構件與副環狀對向電極之連接部以及連結構件與主環狀對向電極之連接部予以連結之概念直線通過前述主環狀對向電極的重心之方式來配置連結構件。藉由以此方式進行連結,便不容易產生起因於放電不均而導致之離子風的產生不均。 The above ring electrodes 131 and 132 preferably utilize a bridge The connecting member such as 139 can be bridged by being energizable, and by this configuration, each of the ring-shaped electrodes can be equipotential, and the positional relationship of the electrodes can be easily adjusted. For example, when the corrugated members are connected, a portion having a substantially triangular shape is formed between the main annular counter electrode and the sub-annular counter electrode, so that the corona discharge is uneven and the ion wind is not largely removed. Launched to the front. Therefore, it is preferable that the concept of connecting the connection portion between the connection member and the sub-annular counter electrode and the connection portion between the connection member and the main annular counter electrode through the main body so as not to cause interference with the generation of the ion wind The connecting member is disposed in such a manner as to have a center of gravity of the annular counter electrode. By connecting in this manner, uneven generation of ion wind due to uneven discharge is less likely to occur.

構成對向電極之主環狀對向電極及副環狀 對向電極最好配置在相同平面內。比起主環狀對向電極而使副環狀對向電極的放電效率逐漸變弱係因為距離之故, 故藉由配置於相同平面而使該距離容易產生變化故為適當。此外,在三維中距離比即使正確,亦在例如圓頂狀等之形狀時離子風所發生之方向相對於主離子風發生的直進風不會發生為平行風,故效率變得不佳。 a main annular counter electrode and a sub-ring forming a counter electrode The counter electrodes are preferably arranged in the same plane. The discharge efficiency of the sub-annular counter electrode is gradually weakened compared to the main annular counter electrode due to the distance, Therefore, it is appropriate to arrange the same plane so that the distance is easily changed. Further, even if the distance ratio in the three-dimensional medium is correct, the direction in which the ion wind occurs in the shape of, for example, a dome shape does not occur as a parallel wind with respect to the main ion wind, so that the efficiency is not good.

再者,針狀電極120與對向電極130各別連 接在電壓施加手段或接地,而在使用時使在該電極間產生電位差來進行放電。在此,針狀電極120的前端部P與最內部的主環狀對向電極131之位置關係最好為最適合發出離子風之位置關係,而藉由配置在此種距離,隨著成為比對向電極之更位於中心之半徑小的環狀對向電極會發出較強的離子風,結果可得到大風量的離子風。在此種位置關係時,環狀對向電極亦可被配置在相同平面上,亦可被配置在別的平面。再者,從圖中的前端部P到環狀對向電極所示之虛線箭頭符號係表示電暈放電所引起之離子的游動方向。 Furthermore, the needle electrode 120 and the counter electrode 130 are connected separately. It is connected to a voltage application means or ground, and when used, a potential difference is generated between the electrodes to discharge. Here, the positional relationship between the tip end portion P of the needle electrode 120 and the innermost main annular counter electrode 131 is preferably the positional relationship most suitable for emitting the ion wind, and by being disposed at such a distance, it becomes a ratio The annular counter electrode having a smaller radius at the center of the counter electrode emits a strong ion wind, and as a result, a high wind volume ion wind can be obtained. In this positional relationship, the annular counter electrode may also be disposed on the same plane or may be disposed on another plane. Further, the dotted arrow symbol shown from the front end portion P in the drawing to the annular counter electrode indicates the swimming direction of ions caused by corona discharge.

有關適合發出離子風之位置關係使用第6 圖之示意圖加以說明。在第6圖(a)中,使用位於最內部之環狀對向電極131的剖面,表示環狀對向電極131與針狀電極120的前端部P之位置關係,而在第6圖(b)中顯示環狀對向電極132與前端部P的位置關係。 Use the sixth position for the positional relationship suitable for emitting ion wind A schematic diagram of the figure is illustrated. In Fig. 6(a), the cross section of the innermost annular counter electrode 131 is used to show the positional relationship between the annular counter electrode 131 and the tip end portion P of the needle electrode 120, and Fig. 6(b) The positional relationship between the annular counter electrode 132 and the tip end portion P is shown.

首先,於前端部P與環狀對向電極131之位 置關係時,離子朝向電極且依照箭頭符號的方向進行游動。亦即離子風於理論上,係從前端部P具有θ1的角度而產生。因此,整體而言,從以前端部P作為頂點之圓錐的 頂點連結底面的端部之母線方向產生離子風。亦即,雖亦朝著環狀對向電極之外方向產生離子風,惟整體而言主要是離子風從環狀對向電極的中心被推出到前面方向。另一方面,在如第6圖(b)所示之環狀對向電極132為具有較大的半徑之輪狀電極時,離子風於理論上,從前端部P持有θ2的角度而產生。亦即,該角度變得更大,故起因於此電極之離子風被發出到環狀對向電極的外側方向之成分變多,而被推出到前面方向之離子風的風量變小。 First, in the positional relationship between the distal end portion P and the annular counter electrode 131, the ions are directed toward the electrode and are moved in the direction of the arrow symbol. That is, the ion wind is theoretically generated from the front end portion P having an angle of θ 1 . Therefore, as a whole, the ion wind is generated from the direction of the bus bar connecting the end portions of the bottom surface with the apex of the taper having the tip end portion P as the apex. That is, although ion wind is generated toward the outside of the annular counter electrode, the ion wind is mainly pushed out from the center of the annular counter electrode to the front direction as a whole. On the other hand, when the annular counter electrode 132 shown in Fig. 6(b) is a wheel electrode having a large radius, the ion wind theoretically holds an angle of θ 2 from the tip end portion P. produce. That is, since the angle becomes larger, the component of the ion wind that is emitted from the electrode to the outer side of the annular counter electrode increases, and the amount of the ion wind that is pushed out to the front direction becomes smaller.

再者,電暈放電對離針狀電極近的位置之 對向電極係容易發生。環狀對向電極隨著愈位於中心,距離針狀電極的前端部P之距離愈近。亦即,電暈放電發生之機率亦為愈位於中心之環狀對向電極變愈高,故產生之離子風之絶對的風壓亦為愈位於中心之環狀對向電極者會較大。 Furthermore, the corona discharge is close to the needle electrode. The counter electrode system is likely to occur. The closer the annular counter electrode is to the center, the closer the distance from the front end portion P of the needle electrode. That is to say, the probability of occurrence of corona discharge is also higher as the annular counter electrode located at the center becomes higher, so that the absolute wind pressure of the generated ion wind is larger for the annular counter electrode which is located at the center.

以上,如說明所示,位於最內部之環狀對 向電極131作為產生離子風之方向亦有利,並且,離子風所產生之絶對的風壓亦大。因此,如第5圖所示之對向電極係屬於以隨著環狀電極之半徑愈變小,從環狀對向電極發出的離子風就愈強之方式而配置之狀態。藉由以此方式配置,透過從外部的電極發出的離子風而不產生滯留現象,且會被從中心發出的離子風牽引而使風量變大,並可得到利用離子風將透過放電產生的離子及臭氧推出到前面之作用,故殺菌、除臭的效果亦變高。此外,位於最內部之環狀對向電極131與前端部P之距離,在電暈放電中更 理想的是保持在最容易適當地放電之距離。但是,僅將對向電極的環狀部之直徑設為大的直徑時雖放電反應大但放電為環狀,故起因於對向電極之環狀中心不具有對向電極部,而導致無風中心部亦變大且發生放電不均之現象並產生環狀離子風,結果由於所產生之離子風外周與中心部成為無風狀態而環狀離子風將無風域進行誘風,故不會發出強風。由於環狀部的直徑為小直徑時雖會發出風壓強的離子風但產生量少,故藉由將屬於二次產生極之副環狀對向電極配置在主環狀對向電極外周,一邊使得中心以小直徑將主流風加強發出風壓,一邊使外周直徑大而發出風壓雖弱但具有風量之副流風。亦即,本實施形態之對向電極將在大直徑時風壓弱但風量多,而在小直徑時風壓強但風量少之現況的問題予以解決,亦即成為將離子風的產生以相同電位來兼顧大風壓與大產生量之形狀。 Above, as shown in the description, the innermost annular pair It is also advantageous to the electrode 131 as the direction in which the ion wind is generated, and the absolute wind pressure generated by the ion wind is also large. Therefore, the counter electrode shown in FIG. 5 is in a state in which the ion wind emitted from the annular counter electrode is increased as the radius of the ring electrode becomes smaller. By disposing in this manner, the ion wind emitted from the external electrode does not cause a retention phenomenon, and is pulled by the ion wind emitted from the center to increase the air volume, and ions generated by the ion wind to transmit the discharge can be obtained. And ozone has been introduced to the front, so the effect of sterilization and deodorization is also high. In addition, the distance between the innermost annular counter electrode 131 and the front end portion P is more in corona discharge. It is desirable to maintain the distance that is most easily discharged properly. However, when the diameter of the annular portion of the counter electrode is set to a large diameter, the discharge reaction is large but the discharge is annular, so that the annular center of the counter electrode does not have the counter electrode portion, resulting in a windless center. The portion is also enlarged and uneven discharge occurs, and a ring-shaped ion wind is generated. As a result, the outer circumference and the central portion of the ion wind generated become a windless state, and the annular ion wind induces windless wind regions, so that no strong wind is emitted. When the diameter of the annular portion is a small diameter, the ion wind having a strong wind pressure is generated, but the amount of generation is small. Therefore, the sub-annular counter electrode belonging to the secondary generating electrode is disposed on the outer circumference of the main annular counter electrode. The center is made to increase the wind pressure by the main wind at a small diameter, and the outer diameter of the outer circumference is large, and the wind pressure is weak but has a wind flow. That is, the counter electrode of the present embodiment solves the problem that the wind pressure is weak at a large diameter but the air volume is large, and the wind pressure is small at a small diameter but the air volume is small, that is, the generation of the ion wind is the same. The potential is a combination of the wind pressure and the large amount of production.

藉由將對向電極設為平面狀,使得從對向 電極產生之離子風,不受到牆面等的障礙物與離子風之反作用的影響而減速,而將從主環狀對向電極產生之主離子風,與從副環狀對向電極產生之副離子風立即予以合成,故在主離子風產生後,便會立即透過周圍的副離子風可快速得到順風之相乘效應,故可得到更大風量的離子風。另一方面,對向電極例如為筒狀等時,由於在對向電極內存在有牆面,故由對向電極產生之離子風會受到牆面與離子風的反作用之影響而減速。如此,與藉由將對向電極設為平面狀,則與設為筒狀等的情況不同,可得到大風量的離 子風。再者,藉由不將對向電極的形狀設為筒狀等而設為平面狀,可將裝置予以小型化,且以此方式使裝置小型化,亦不會像以往使離子風的風量降低。此外,藉由設為平面狀,使得對向電極之清洗成為容易。再者,例如設為如上述專利文獻9之金網狀的對向電極時,各對向電極不為環狀且各對向電極之平面狀的法線向量亦並非大致相同方向,故容易產生各對向電極之放電不均現象且受到從對向電極發出的離子風之風力不均等化等之影響,而導致從對向電極產生之離子風被減速(利用各對向電極產生之離子風沒被適當地合成),故不理想。 By making the counter electrode flat, making it from the opposite direction The ion wind generated by the electrode is not decelerated by the influence of the obstacle such as the wall surface and the ion wind, but the main ion wind generated from the main annular counter electrode and the sub-ring counter electrode are generated. The ion wind is synthesized immediately, so that after the main ion wind is generated, the sub-ion wind can be quickly transmitted through the surrounding sub-ion wind, so that a larger wind volume ion wind can be obtained. On the other hand, when the counter electrode is, for example, a cylindrical shape, since there is a wall surface in the counter electrode, the ion wind generated by the counter electrode is decelerated by the reaction of the wall surface and the ion wind. In this way, unlike the case where the counter electrode is formed in a planar shape, a large amount of wind can be obtained. Zifeng. In addition, by making the shape of the counter electrode into a cylindrical shape or the like, the device can be downsized, and the device can be miniaturized in this manner, and the air volume of the ion wind can be reduced as in the related art. . Further, by setting it in a planar shape, it is easy to clean the counter electrode. Further, for example, when the counter electrode of the gold mesh shape of Patent Document 9 is used, each of the counter electrodes is not annular, and the planar normal vectors of the counter electrodes are not substantially in the same direction, so that each of the opposing electrodes is likely to be generated. The discharge unevenness of the counter electrode is affected by the wind unevenness of the ion wind emitted from the counter electrode, and the ion wind generated from the counter electrode is decelerated (the ion wind generated by each counter electrode is not It is properly synthesized), so it is not ideal.

本實施形態之離子、臭氧風產生裝置係前 述針狀電極的前端與前述主環狀對向電極的最長距離,比前述針狀電極的前端與前述副環狀對向電極之最短距離更短。藉由將針狀電極與對向電極配置在此種距離關係,而從形成在主環狀對向電極的中心之開口部,產生風壓最強的離子風,且從周邊的副環狀對向電極產生風壓較弱之離子風,故可得到大量的離子風。從此種針狀電極與相對環狀電極的位置關係偏離時,由於離子風係主要從主環狀對向電極與副環狀對向電極之間的空間產生離子風,而成為均等風,故空中釋出離子風變弱,並且於設置引導構件時亦產生反作用。 Before the ion and ozone wind generating device of the present embodiment The longest distance between the tip end of the needle electrode and the main annular counter electrode is shorter than the shortest distance between the tip end of the needle electrode and the sub-annular counter electrode. By arranging the needle electrode and the counter electrode in such a distance relationship, the ion wind having the strongest wind pressure is generated from the opening formed at the center of the main annular counter electrode, and the sub-ring is opposed from the periphery. The electrode generates an ion wind with a weak wind pressure, so a large amount of ion wind can be obtained. When the positional relationship between the needle electrode and the ring-shaped electrode is deviated, the ion wind system mainly generates ion wind from the space between the main ring-shaped counter electrode and the sub-annular counter electrode, and becomes equal wind. The release of the ion wind is weak and also counteracts when the guiding member is provided.

構成對向電極130之環狀對向電極係如第5 圖所示不限定為2個,而如第7圖所示,如環狀對向電極131至133,亦可設置多數環狀對向電極。再者,第7圖(a) 係該裝置之對向電極130的概念正視圖,第7圖(b)係離子、臭氧風產生裝置100之概念側視圖。在此,雖就使用3個環狀對向電極的情況作了說明,以此方式構成對向電極之環狀對向電極係只要滿足與針狀電極之距離關則亦可設置任意個。藉由以此方式設置多數個電極,則即便一個電極電極髒污而不再放電亦可利用其他電極來放電,故提高裝置的動作穩定性。 The annular counter electrode constituting the counter electrode 130 is as in the fifth The figure is not limited to two, and as shown in Fig. 7, as the annular counter electrodes 131 to 133, a plurality of annular counter electrodes may be provided. Furthermore, Figure 7 (a) A conceptual front view of the counter electrode 130 of the device, and Fig. 7(b) is a conceptual side view of the ion and ozone wind generating device 100. Here, the case where three annular counter electrodes are used is described. In this way, the annular counter electrode system constituting the counter electrode may be provided in any number as long as it satisfies the distance from the needle electrode. By providing a plurality of electrodes in this manner, even if one electrode electrode is dirty and is not discharged, it can be discharged by other electrodes, thereby improving the operational stability of the device.

如第8圖所示,本實施形態之對向電極亦可 為多角形。此時,亦將各針狀電極與對向電極,配置在前述針狀電極的前端與前述主環狀對向電極的最長距離比前述針狀電極的前端與前述副環狀對向電極的最短距離更短的位置。再者,第8圖(a)係該裝置的對向電極之概念正視圖,第8圖(b)係離子、臭氧風產生裝置100之概念側視圖。 如此即使為三角形的形狀,從主環狀對向電極產生之離子風亦比從副環狀對向電極產生的離子風更小,而可得到大風量的離子風。再者,在此主環狀對向電極雖表示為圓形狀,惟亦可為三角形以上之多角形。此外環狀對向電極為多角形時,由於邊數愈多則與針狀電極的呈現最短距離之點愈多,因此不易產生放電不均現象故較適合。 As shown in Fig. 8, the counter electrode of this embodiment can also be It is polygonal. In this case, the needle electrode and the counter electrode are disposed so that the longest distance between the tip end of the needle electrode and the main annular counter electrode is shorter than the tip end of the needle electrode and the sub-ring counter electrode. Shorter location. Further, Fig. 8(a) is a conceptual front view of the counter electrode of the device, and Fig. 8(b) is a conceptual side view of the ion and ozone wind generating device 100. Thus, even in the shape of a triangle, the ion wind generated from the main annular counter electrode is smaller than the ion wind generated from the sub-annular counter electrode, and a large wind amount of ion wind can be obtained. Further, although the main annular counter electrode is formed in a circular shape, it may be a polygonal shape of a triangle or more. Further, when the annular counter electrode is polygonal, the more the number of sides is, the more the shortest distance from the needle electrode is present, so that it is less likely to cause uneven discharge.

如第9圖所示,如針狀電極121至123,亦 可設置複數個針狀電極。此時,所有的針狀電極與對向電極位於前述針狀電極的前端與前述主環狀對向電極的最長距離比前述針狀電極的前端與前述副環狀對向電極之最短距離更短的位置。再者,第9圖(a)係該裝置之對向電極的 概念正視圖,第9圖(b)係離子、臭氧風產生裝置100之概念側視圖。藉由以此方式設置複數個針狀電極,比起單極的情況,產生多數絕緣破壞而容易產生分子的衝撞進而推出能力提高,故可使大量的臭氧產生。 As shown in Fig. 9, as for the needle electrodes 121 to 123, A plurality of needle electrodes can be provided. In this case, the longest distance between the needle electrode and the counter electrode at the tip end of the needle electrode and the main annular counter electrode is shorter than the shortest distance between the tip end of the needle electrode and the sub ring counter electrode. s position. Furthermore, Figure 9 (a) is the counter electrode of the device. Conceptual front view, Fig. 9(b) is a conceptual side view of the ion and ozone wind generating device 100. By providing a plurality of needle electrodes in this manner, a large number of insulation breaks occur and a collision of molecules is easily generated, and a large amount of ozone can be generated.

第10圖係表示本發明之對向電極的一例之 概略圖。在此,藉由在板設置孔,而形成對向電極。第10圖(c)係具有圓形狀的對向電極之板狀對向電極130c的概念圖。該對向電極具有第一對向電極130c-1與第二對向電極130c-2。第一對向電極130c-1係在中心形成有圓形狀的主環狀對向電極131c-1,且在其周圍,形成有圓形狀的副環狀對向電極132c-1,且於副環狀對向電極132c-1的外周,復形成有副環狀對向電極133c-1、134c-1、135c-1。此外於上述對向電極之間,形成有連結構件139c-1。再者第二對向電極亦相同,在中心形成有圓形狀的主環狀對向電極131c-2,且在其周圍,形成有圓形狀的副環狀對向電極132c-2,且於副環狀對向電極132c-2的外周,復形成有副環狀對向電極133c-2、134c-2。此外於上述對向電極之間,形成有連結構件139c-2。對上述板狀對向電極於適當的位置配置針狀電極來使用。 Fig. 10 is a view showing an example of the counter electrode of the present invention. Schematic diagram. Here, the counter electrode is formed by providing a hole in the plate. Fig. 10(c) is a conceptual diagram of a plate-like counter electrode 130c having a circular counter electrode. The counter electrode has a first counter electrode 130c-1 and a second counter electrode 130c-2. The first counter electrode 130c-1 is formed with a circular main annular counter electrode 131c-1 at the center, and a circular sub-annular counter electrode 132c-1 is formed around the sub-electrode 130c-1. On the outer circumference of the counter electrode 132c-1, sub-annular counter electrodes 133c-1, 134c-1, and 135c-1 are formed. Further, a connecting member 139c-1 is formed between the counter electrodes. Further, the second counter electrode is also the same, and a main annular counter electrode 131c-2 having a circular shape is formed at the center, and a circular sub-annular counter electrode 132c-2 is formed around the circular sub-electrode 132c-2. Sub-annular counter electrodes 133c-2 and 134c-2 are formed on the outer circumference of the annular counter electrode 132c-2. Further, a connecting member 139c-2 is formed between the counter electrodes. The needle-shaped electrode is disposed at an appropriate position on the plate-shaped counter electrode.

第10圖(b)係表示板狀對向電極130b之概 略構成圖。板狀對向電極130b係主環狀對向電極的形狀為圓形狀,而周圍的副環狀對向電極的形狀為六角形。板狀對向電極130b具有第一對向電極130b-1、第二對向電極130b-2。於第一對向電極130b-1的中心部,形成有圓形狀 的主環狀對向電極131b-1,且於其周圍形成有六角形狀的副環狀對向電極132b-1,復於其外周,形成有副環狀對向電極133b-1、134b-1、135b-1。再者上述對向電極之間係透過連結構件139b-1而連結。 Figure 10(b) shows an overview of the plate-like counter electrode 130b. Slightly composed. The shape of the plate-shaped counter electrode 130b is a circular shape of the main annular counter electrode, and the shape of the surrounding sub-annular counter electrode is hexagonal. The plate-shaped counter electrode 130b has a first counter electrode 130b-1 and a second counter electrode 130b-2. a circular shape is formed at a central portion of the first counter electrode 130b-1 The main annular counter electrode 131b-1 is formed with a hexagonal sub-annular counter electrode 132b-1, and a sub-annular counter electrode 133b-1, 134b-1 is formed on the outer periphery thereof. , 135b-1. Further, the opposing electrodes are connected to each other through the connecting member 139b-1.

第二對向電極130b-2亦相同,在中心形成有圓形狀之主環狀對向電極131b-2,且在其周圍,形成有六角形狀之副環狀對向電極132b-2至134b-2,而上述電極係透過連結構件139b-2而連結。 The second counter electrode 130b-2 is also the same, and a circular main-shaped opposite counter electrode 131b-2 is formed at the center, and a hexagonal-shaped sub-annular counter electrode 132b-2 to 134b is formed around it. 2. The electrodes are connected by the connecting member 139b-2.

第10圖(a)係表示板狀對向電極130a的概略 構成圖。在板狀對向電極130a中,形成有圓形狀的主環狀對向電極,且在其周邊形成有環狀的副環狀對向電極。板狀對向電極130a具有第一對向電極130a-1與第二對向電極130a-2。於第一對向電極130a-1的中心部,形成有圓形狀的主環狀對向電極131a-1,且於其周邊形成有複數個副環狀對向電極132a-1。在第10圖(a)中,表示副環狀對向電極132a-1之代表性的一例,而形成在主環狀對向電極131a-1的周邊之132a-1亦相同地為副環狀對向電極。藉由以此方式形成,使得形成在副環狀對向電極之間的構件成為從主環狀對向電極擴散成放射線狀的狀態,故除了從主環狀對向電極產生的離子風之外,隨著從該主環狀對向電極遠離而離子風的風量連續性地變小。第二對向電極132a-2亦與第一對向電極同樣地在中心具有主環狀對向電極131a-2及副環狀對向電極132a-2。 Fig. 10(a) shows the outline of the plate-like counter electrode 130a. Make up the picture. In the plate-shaped counter electrode 130a, a circular main annular counter electrode is formed, and a ring-shaped sub-annular counter electrode is formed in the periphery thereof. The plate-shaped counter electrode 130a has a first counter electrode 130a-1 and a second counter electrode 130a-2. A circular main annular counter electrode 131a-1 is formed at a central portion of the first counter electrode 130a-1, and a plurality of sub-annular counter electrodes 132a-1 are formed around the center. In Fig. 10(a), a representative example of the sub-annular counter electrode 132a-1 is shown, and 132a-1 formed around the main annular counter electrode 131a-1 is also a sub-ring. Counter electrode. By forming in this manner, the member formed between the sub-annular opposing electrodes is diffused into a radial state from the main annular counter electrode, and therefore, in addition to the ion wind generated from the main annular counter electrode. As the distance from the main annular counter electrode is away, the air volume of the ion wind continuously decreases. Similarly to the first counter electrode, the second counter electrode 132a-2 has a main annular counter electrode 131a-2 and a sub-annular counter electrode 132a-2 at the center.

此外,第10圖(d)係上述板狀對向電極130a 至c之共同的側視圖。 Further, Fig. 10(d) is the above-mentioned plate-shaped counter electrode 130a. A common side view to c.

如第11圖所示,具有複數個本形態之電極 對110之離子、臭氧風產生裝置為較佳者。再者,第11圖係離子、臭氧風產生裝置100之概念平面圖。最好以於配置在中心之電極對的左右配置有2個電極對,且配置在前述左右之2個電極對的離子風產生方向會分別對於配置在中心之電極對的離子風產生方向,交叉之方式來配置。 再者更佳的是從各電極對產生之離子風以焦點集中之方式予以配置。藉由使用此種裝置,可使從各電極對發出的離子風合流,而可得到更大風量的離子風。 As shown in Fig. 11, an electrode having a plurality of the forms An ion and ozone wind generating device of 110 is preferred. Further, Fig. 11 is a conceptual plan view of the ion and ozone wind generating device 100. Preferably, two electrode pairs are disposed on the left and right sides of the electrode pair disposed in the center, and the ion wind generation directions of the two pairs of the left and right electrode pairs are respectively intersected with the ion wind generation direction of the electrode pair disposed at the center. The way to configure. Further preferably, the ion wind generated from each electrode pair is disposed in such a manner as to focus. By using such a device, the ion winds emitted from the respective electrode pairs can be combined to obtain a larger air volume of the ion wind.

如第12圖所示,最好設置有截頭圓錐形的 離子風引導構件140。此外,第12圖(a)係該裝置之對向電極130的概念正視圖,第12圖(b)係離子、臭氧風產生裝置100之概念側視圖。藉由將從位於外側之環狀對向電極產生之離子風聚集於(使之合流)從位於對向電極130的最內部之環狀對向電極131產生之離子風,且將之送到離子風噴出口141,使得被推出到前面之離子風的風量變大。 再者,即使以此方式設置引導構件,在外側產生之離子風比在最內部產生之離子風更小,故不滯留而以被引進到中心的離子風之方式被推出到前方。引導構件具有開口剖面積慢慢地變小之形狀。設置有具有此種形狀之引導構件時,以從對向電極產生之離子風為均等風或中心不發出風壓之環狀風而言,係由於相對送風作用而剖面積變小的形狀,故直進之離子風雖與引導構件的內牆壁衝撞而產生亂 氣流並於引導構件內部產生反作用而成為微風,惟在主離子風強且副離子風弱時即便引導構件被縮小為小直徑時,由於副離子風亦弱,故對引導構件內牆之衝撞亦當然變弱且主離子風係牽引副離子風而將離子風予以聚集並噴出。 As shown in Figure 12, it is best to have a frustoconical shape. Ion wind guiding member 140. Further, Fig. 12(a) is a conceptual front view of the counter electrode 130 of the apparatus, and Fig. 12(b) is a conceptual side view of the ion and ozone wind generating apparatus 100. The ion wind generated from the innermost annular counter electrode 131 located at the opposite electrode 130 is collected (converged) from the ion wind generated by the annular counter electrode located outside and sent to the ion The air outlet 141 causes the amount of wind that is pushed out to the front of the ion wind to become large. Further, even if the guiding member is provided in this manner, the ion wind generated on the outside is smaller than the ion wind generated in the innermost portion, so that it is not retained and is pushed forward in the manner of the ion wind introduced into the center. The guiding member has a shape in which the opening sectional area is gradually reduced. When the guide member having such a shape is provided, the annular wind in which the ion wind generated from the counter electrode is equal wind or the wind pressure is not generated at the center is a shape in which the cross-sectional area is reduced due to the air blowing action. The straight-in ion wind collides with the inner wall of the guiding member to create chaos The airflow reacts inside the guiding member to become a breeze. However, when the main ion wind is strong and the auxiliary ion is weak, even if the guiding member is reduced to a small diameter, since the secondary ion wind is weak, the collision with the inner wall of the guiding member is also Of course, the weakened and main ion wind draws the secondary ion wind and collects and ejects the ion wind.

再者,最好於引導構件140之噴出口141, 設置有送風路徑150。在此,送風路徑雖只要可調整被噴出之離子風的風方向即可而沒特別限定,惟最好為具有與噴出口141相同的直徑之管狀構件。在此,送風路徑的材質沒特別限定,可舉出軟管、氯乙烯管等。該送風路徑係如後述於設置複數個電極對時,可依容易聚集從上述電極對產生的離子風之方式來使用。再者,單獨使用該電極對時,可透過該送風路徑,將離子及臭氧送進到殺菌、除臭對象空間等。 Furthermore, it is preferable that the ejection port 141 of the guiding member 140 is A blowing path 150 is provided. Here, the air blowing path is not particularly limited as long as the wind direction of the ion wind to be ejected can be adjusted, but it is preferably a tubular member having the same diameter as the discharge port 141. Here, the material of the air blowing path is not particularly limited, and examples thereof include a hose and a vinyl chloride tube. This air supply path can be used in such a manner that a plurality of electrode pairs are provided as described later, and the ion wind generated from the electrode pair can be easily collected. Further, when the electrode pair is used alone, ions and ozone can be supplied to the sterilization and deodorizing target space through the air blowing path.

如第13圖所示,較佳為設置複數個設置有 上述引導構件140之電極對110。設置3個電極對110時,於配置在中心之電極對的左右配置有2個電極對,且以配置在左右之2個電極對的離子風產生方向分別交叉於配置在中心之電極對的離子風產生方向之方式予以配置。此外,最好以從各電極對產生之離子風集中於一點之方式予以配置。藉由以此方式來構成,且透過使從各電極對產生之離子風合流而可得到大風量的離子風。 As shown in FIG. 13, it is preferable to set a plurality of settings. The electrode pair 110 of the guiding member 140 described above. When three electrode pairs 110 are provided, two electrode pairs are disposed on the right and left sides of the electrode pair disposed at the center, and the ion wind generation directions of the two electrode pairs disposed on the left and right intersect the ions of the electrode pairs disposed at the center The way the wind produces direction is configured. Further, it is preferable to arrange the ion wind generated from each electrode pair to be concentrated at one point. According to this configuration, a large amount of ion wind can be obtained by merging the ion winds generated from the respective electrode pairs.

如第14圖所示,最好設置6個設置有引導 構件140之電極對110(在此為了容易圖示而省略針狀電極)。第14圖(a)係離子、臭氧風產生裝置之概念平面圖, 第14圖(b)係離子、臭氧風產生裝置之概念側視圖,第14圖(c)係從離子、臭氧風產生裝置的噴出口側所看之概念正視圖。此時,將電極對按各3組設為上下之二段構成,且各別就上述上下段依照之前所示之3個電極對之配置法予以配置{第14圖(a)},且以使從該電極對之群產生之離子風合流之方式將上述3個電極對之群予以配置{第14圖(b)}。在此最好以從各電極對產生之離子風集中於一點之方式予以配置。亦即,藉由如將從位於上下段的中心之電極對產生的離子風予以聚集之角度來配置,可使來自各電極對之離子風合流且可得到大風量的離子風。 As shown in Figure 14, it is best to set 6 settings to guide The electrode pair 110 of the member 140 (the needle electrode is omitted here for ease of illustration). Figure 14 (a) is a conceptual plan view of an ion and ozone wind generating device, Fig. 14(b) is a conceptual side view of the ion and ozone wind generating device, and Fig. 14(c) is a conceptual front view seen from the discharge port side of the ion and ozone wind generating device. In this case, the electrode pairs are arranged in two stages of the upper and lower sides, and the upper and lower sections are respectively arranged in accordance with the arrangement method of the three electrode pairs shown in the above (Fig. 14(a)}, and The group of the three electrode pairs is arranged such that the ion winds are generated from the group of the electrode pairs (Fig. 14(b)}. Here, it is preferable to arrange the ion wind generated from each electrode pair to be concentrated at one point. That is, by arranging the ion winds generated from the electrode pairs located at the center of the upper and lower stages, the ion winds from the respective electrode pairs can be merged and an ion wind of a large amount of wind can be obtained.

依據上述離子、臭氧風產生裝置100,雖可 得到足夠的風量之離子風,惟從小型化與攜帶化之方面而言則更有改良的空間。為此,就比起上述離子、臭氧風產生裝置100,即便利用更低的電壓亦可產生離子風(亦即,可更小型化),並可穩定地產生更強的離子風之屬於本實施形態之殺菌、除臭裝置之另外的形態之離子、臭氧風產生裝置100加以詳述。此外,本實施形態為一例,有關所屬技術區域中具有通常知識者可思及之其他的形態或各種變更例,亦屬本實施形態之技術的範圍(有關具體的變更例將後述之)。此外,在本說明書中作為一例所舉出之實施形態與變更例,不應限定性地理解為使用於特定態樣者,亦可為任何組合。例如,針對某實施形態之變更例,應理解為別的實施形態之變更例,此外,即使獨立記載有某變更例與別的變更例,應理解為亦記載有將該某變更例與該別的 變更例予以組合者。並且,在實施形態與變更例中作為所示之具體的一例之數值{例如,放電電極與對向電極之直徑與長度、厚度、放電電極與對向電極之電壓差、放電電極與對向電極之相隔距離等}係僅為一例,只要不大大脫離各實施形態與變更例的宗旨,應理解為亦可作適當變更。 According to the above ion and ozone wind generating device 100, although I get a sufficient amount of air, but there is room for improvement in terms of miniaturization and portability. Therefore, compared with the above-described ion and ozone wind generating device 100, even if a lower voltage is used, ion wind can be generated (that is, it can be further miniaturized), and a stronger ion wind can be stably generated. The ion and ozone wind generating device 100 of another form of the sterilization and deodorizing device of the form will be described in detail. In addition, this embodiment is an example, and other forms or various modifications which can be considered by a person having ordinary knowledge in the technical field are also within the scope of the technology of the present embodiment (a specific modification will be described later). In addition, the embodiment and the modification examples which are exemplified in the present specification are not limited to those used in a specific aspect, and may be any combination. For example, a modified example of a certain embodiment is understood to be a modified example of another embodiment, and even if a certain modified example and another modified example are separately described, it should be understood that the modified example and the other modified example are also described. of The change example is combined. Further, in the embodiment and the modified example, the numerical value is specifically shown as an example {for example, the diameter and length of the discharge electrode and the counter electrode, the thickness, the voltage difference between the discharge electrode and the counter electrode, and the discharge electrode and the counter electrode. The distances and the like are merely examples, and it should be understood that they may be appropriately changed as long as they are not greatly deviated from the gist of the embodiments and the modifications.

將本實施形態之離子、臭氧風產生裝置100 之概略構造表示於第15圖。本實施形態之離子、臭氧風產生裝置100係主要由1個主電極對以及以包圍主電極對之方式而設置之6個副電極對所構成。如前述,所謂電極對係指具有放電電極(在本實施形態中為針狀電極)與對向電極之1組電極,而主電極對係作為該對向電極而言,具有環狀對向電極130a(以下,設為第1對向電極130a。),而6個副電極對係作為該對向電極而言,具有環狀對向電極130b至130g(以下,設為第2對向電極130b至130g等。)。 再者,任一對向電極皆由板狀構件及/或線狀構件所構成。 The ion and ozone wind generating device 100 of the present embodiment The schematic structure is shown in Fig. 15. The ion and ozone wind generation device 100 of the present embodiment is mainly composed of one main electrode pair and six sub-electrode pairs provided to surround the main electrode pair. As described above, the electrode pair refers to a group of electrodes having a discharge electrode (in the present embodiment, a needle electrode) and a counter electrode, and the main electrode pair as the counter electrode has a ring-shaped counter electrode. 130a (hereinafter, the first counter electrode 130a), and the six sub-electrode pairs have the annular counter electrodes 130b to 130g as the counter electrode (hereinafter, the second counter electrode 130b) To 130g, etc.). Furthermore, any of the counter electrodes is composed of a plate member and/or a linear member.

並且,在本實施形態之離子、臭氧風產生裝置100中,將第1對向電極130a及6個第2對向電極130b至130g設為皆相等之形狀(直徑相等的大致環狀)。然後,在本實施形態之離子、臭氧風產生裝置100中,第2對向電極130b至130g係沿著第1對向電極130a的外周且相互鄰接而配置。結果,於上述第2對向電極130b至130g的外側,形成與上述第2對向電極130b至130g內接之虛擬圓S(於第15圖,以虛線所示之處所)。 In the ion and ozone wind generation device 100 of the present embodiment, the first counter electrode 130a and the six second counter electrodes 130b to 130g have the same shape (a substantially annular shape having the same diameter). In the ion and ozone wind generator 100 of the present embodiment, the second counter electrodes 130b to 130g are disposed adjacent to each other along the outer circumference of the first counter electrode 130a. As a result, on the outer side of the second counter electrode 130b to 130g, a virtual circle S inscribed in the second counter electrode 130b to 130g is formed (in the fifteenth figure, as indicated by a broken line).

更具體而言,假設為大致正六角形狀時, 以6個第2對向電極130b至130g的中心形成該大致正六角形狀之各頂點之方式,以各別鄰接之形態來設置第2對向電極130b至130g。換言之,在本實施形態之離子、臭氧風產生裝置100中,第2對向電極130b至130g係以相互鄰接之對向電極的外周彼此靠接之方式而配置。例如,第2對向電極130b的外周係與鄰接於該第2對向電極130b之第2對向電極130c及130g的外周各別靠接。並且,可定義為使第1對向電極130a,復與該第2對向電極130b至130g之各者接觸之方式(亦即,以配置於由第2對向電極130b至130g所假定出之大致正六角形狀的中心之方式)來予以設置。此外,第2對向電極130b至130g雖可不與相鄰的對向電極鄰接(靠接)而亦可為接近之狀態,惟隔離太遠時,從離子、臭氧風產生裝置100產生之風力降低。 因此,各第2對向電極130b至130g最好是鄰接的對向電極之外周間的距離(尤其是成為最短之距離)為第2對向電極130b至130g之直徑以下(或直徑之1/n以下;n為自然數)。再者,第1對向電極130a雖可不與所有的第2對向電極130b至130g接觸而亦可為接近之狀態,惟最好與第2對向電極130b至130g之至少一部分接觸(此時,較佳係成為外周間的最短之距離亦為第1對向電極130a與第2對向電極130b至130g之直徑以下或直徑之1/n以下;n為自然數)。 More specifically, when it is assumed to be a substantially regular hexagonal shape, The second counter electrode 130b to 130g is provided so as to be adjacent to each other so that the vertices of the substantially regular hexagonal shape are formed at the centers of the six second counter electrodes 130b to 130g. In other words, in the ion and ozone wind generator 100 of the present embodiment, the second counter electrodes 130b to 130g are disposed such that the outer circumferences of the opposing electrodes adjacent to each other are in contact with each other. For example, the outer circumference of the second counter electrode 130b and the outer circumference of the second counter electrode 130c and 130g adjacent to the second counter electrode 130b are respectively in contact with each other. Further, it can be defined as a method in which the first counter electrode 130a is brought into contact with each of the second counter electrodes 130b to 130g (that is, arranged in the second counter electrode 130b to 130g). It is set by the way of the center of the hexagonal shape. Further, the second counter electrode 130b to 130g may be in a state of being close to (adjacent to) the adjacent counter electrode, but the wind generated from the ion and ozone wind generating device 100 is lowered when the isolation is too far. . Therefore, it is preferable that each of the second counter electrodes 130b to 130g has a distance (especially the shortest distance) between the outer circumferences of the adjacent counter electrodes, which is equal to or less than the diameter of the second counter electrodes 130b to 130g (or 1/diameter) n is below; n is a natural number). Further, the first counter electrode 130a may be in close proximity to all of the second counter electrodes 130b to 130g, but preferably in contact with at least a part of the second counter electrodes 130b to 130g (at this time). Preferably, the shortest distance between the outer circumferences is equal to or less than the diameter of the first counter electrode 130a and the second counter electrode 130b to 130g or 1/n or less of the diameter; n is a natural number).

此外,於第1對向電極130a及第2對向電 極130b至130g,係藉由設置針狀電極120(尤其是成為各 個對向電極之放電部的針狀電極120a及120b至120g)作為成對之放電側的電極,而形成主電極對及副電極對。再者,本實施形態之各對向電極(第1對向電極130a及第2對向電極130b至130g)係如前述之2重環狀構造,以橋接器以導通狀態固定主環狀電極及包圍主環狀電極之方式而設置之副環狀電極。在此,關於各個電極對之主環狀電極、副環狀電極及橋接器之各別的功能與具有上述功能的2重環狀電極之離子風的產生原理,如前述故省略之。再者,各對向電極(第1對向電極130a及第2對向電極130b至130g)並不限定為2重環狀構造,亦可一部分或全部為1重環狀構造(或,具有3重以上的環之多重環狀構造)與渦狀構造(關於渦狀構造之具體的態樣如後述)。 In addition, the first counter electrode 130a and the second counter electrode The poles 130b to 130g are provided by the needle electrodes 120 (especially The needle electrodes 120a and 120b to 120g) of the discharge portions of the counter electrodes serve as electrodes on the discharge side of the pair, and a pair of the main electrode and the pair of the sub-electrodes are formed. Further, each of the counter electrodes (the first counter electrode 130a and the second counter electrode 130b to 130g) of the present embodiment has the above-described two-folded ring structure, and the main ring-shaped electrode is fixed in a conductive state by a bridge. A sub-annular electrode provided to surround the main annular electrode. Here, the respective functions of the main ring electrode, the sub ring electrode, and the bridge of each electrode pair and the principle of generating the ion wind of the double ring electrode having the above function are omitted as described above. In addition, each of the counter electrodes (the first counter electrode 130a and the second counter electrode 130b to 130g) is not limited to a two-folded ring structure, and some or all of them may have a one-ring ring structure (or have three The multiple annular structure of the ring having a weight more than the vortex structure (the specific aspect of the vortex structure will be described later).

其次,一邊參照第16圖,一邊就本實施形 態之離子、臭氧風產生裝置100的離子風產生之作用及效果加以說明。再者,茲容補充說明者,在第16圖中,雖有為了容易想像其作用及效果,而以各對向電極位於不同的平面上之方式予以圖示之情況,惟即便是各對向電極位於相同的平面狀之情況,亦可造成相同的作用及效果。 Next, while referring to Figure 16, The action and effect of the ion wind generation by the ion and ozone wind generating device 100 will be described. In addition, in the sixteenth figure, in order to make it easy to imagine the action and effect, it is shown in the case where each counter electrode is located on a different plane, even if it is each opposite direction. When the electrodes are in the same planar shape, the same effects and effects can be caused.

依據本實施形態之離子、臭氧風產生裝置 100,藉由將第1對向電極130a設為大致中心(虛擬圓S的中心附近),且以包圍其周圍之方式設置第2對向電極130b至130g之構成,會由於透過在副電極對所產生的離子風之順風,將在主電極對產生之離子風以被推動之形態被推出到前面,故不削減在主電極對產生之離子風的風力,而被 送達到對象物(副電極對之保護效果)。亦即,即使在將各電極對設為更小的形狀之情況下{例如,對向電極的直徑為1cm程度(適當的範圍為5mm至5cm),將針狀電極與對向電極之相隔距離設為1至2cm程度(適當的範圍為1mm至2cm),將針狀電極與對向電極之電位差設為3至100伏特程度},亦可得到足夠的風量之離子風。 Ion and ozone wind generating device according to the embodiment 100, the first counter electrode 130a is substantially centered (near the center of the virtual circle S), and the second counter electrode 130b to 130g is disposed so as to surround the periphery thereof. The downwind of the generated ion wind is pushed out to the front in the form in which the ion wind generated by the main electrode pair is pushed, so that the wind of the ion wind generated in the main electrode pair is not reduced, but The object is delivered to the object (the protective effect of the secondary electrode pair). That is, even in the case where the electrode pairs are set to a smaller shape {for example, the diameter of the counter electrode is about 1 cm (appropriate range is 5 mm to 5 cm), the distance between the needle electrode and the counter electrode is separated. It is set to a degree of 1 to 2 cm (appropriate range is 1 mm to 2 cm), and the potential difference between the needle electrode and the counter electrode is set to 3 to 100 volts}, and an ion wind of a sufficient air volume can be obtained.

此外,在本實施形態之離子、臭氧風產生 裝置100中,設為使第1對向電極130a的周圍,由鄰接之第2對向電極130b至130g包圍之構成(以儘可能將第2對向電極,設為與第1對向電極130a鄰接的方式之構成)。 藉由設為此種構成,各個電極對所產生之離子風與鄰接之電極對所產生之離子風互相接觸的比例,會比與靜止的外氣互相接觸之比例更增大(亦即,產生之離子風變得難與靜止之外氣互相接觸,而使與外氣的摩擦所引起之抵抗變少)。 In addition, the ion and ozone wind generation in the present embodiment In the device 100, the periphery of the first counter electrode 130a is surrounded by the adjacent second counter electrodes 130b to 130g (the second counter electrode is set as the first counter electrode 130a as much as possible). The composition of the adjacent method). With such a configuration, the ratio of the ion wind generated by each electrode pair to the ion wind generated by the adjacent electrode pair is increased more than the ratio of contact with the stationary outside air (that is, the ratio is generated. The ion wind becomes difficult to contact with the gas outside of the rest, and the resistance caused by the friction with the outside air is reduced.

並且,尤其在第1對向電極130a產生之離 子風其周圍全部會被別的離子風包圍,故變得更難與外氣互相接觸,更可提高前述副電極對之保護效果。以此方式,本實施形態之離子、臭氧風產生裝置100以噴出之離子風整體來看時,由於可得到從離子、臭氧風產生裝置100噴出之離子風與靜止之外氣接觸之區域變少而變得不易受到與外氣之摩擦的影響,並且中心的離子風(在主對向電極對產生之離子風)受到周圍的離子風(在副對向電極對產生之離子風)保護之效果,故可將更強的離子風送達到遠的對象 物。再者,以此方式,藉由使各對向電極鄰接,且儘可能減小存在於各對向電極間之間隙,而在在侷限的空間設置更大的對向電極(或增加對向電極的數目),可產生更大的風量之離子風。 Moreover, especially in the first counter electrode 130a The surrounding wind is surrounded by other ion winds, so it becomes more difficult to contact the outside air, and the protection effect of the pair of secondary electrodes can be improved. In this way, when the ion or ozone wind generator 100 of the present embodiment is viewed as a whole of the ion wind that is ejected, the area where the ion wind ejected from the ion or ozone wind generating device 100 is in contact with the stationary air is reduced. It becomes less susceptible to the influence of friction with the outside air, and the center ion wind (the ion wind generated in the main counter electrode pair) is protected by the surrounding ion wind (the ion wind generated by the pair of counter-electrodes) Therefore, a stronger ion wind can be sent to reach a distant object. Things. Furthermore, in this way, by arranging the opposing electrodes and minimizing the gap existing between the opposing electrodes, a larger counter electrode (or an increasing counter electrode) is provided in the confined space. The number of ions that can produce a larger amount of wind.

此外,如本實施形態之離子、臭氧風產生 裝置100,藉由將對向電極(第1對向電極130a及第2對向電極130b至130g)設為皆相等的形狀,使得在主電極對及副電極對之各個電極對產生之離子風,會各自成為某些程度風量大者(不會局部性地產生風量少的處所等)。並且,藉由將上述第2對向電極130b至130g設為相等的形狀,由於使得在副電極對(尤其是各第2對向電極130b至130g)產生之離子風,其與外氣接觸之區域不受副電極對之設置處所影響而幾乎成為相等,故進一步減少離子風整體之局部性的風量的不均。因此,藉由設為此種構成,而以離子、臭氧風產生裝置100整體來看時,可得到更穩定且風量大的離子風。 In addition, ions and ozone wind are generated as in the present embodiment. In the device 100, the counter electrode (the first counter electrode 130a and the second counter electrode 130b and 130g) have the same shape, so that the ion wind generated in each pair of the main electrode pair and the sub-electrode pair They will each become a certain amount of people with a large amount of wind (the place where the air volume is not generated locally). Further, by setting the second counter electrodes 130b to 130g to have the same shape, the ion wind generated in the pair of sub-electrodes (especially the second counter electrodes 130b to 130g) is in contact with the outside air. Since the area is almost equal to the influence of the arrangement of the pair of the pair of electrodes, the unevenness of the air volume of the locality of the entire ion wind is further reduced. Therefore, by adopting such a configuration, it is possible to obtain an ion wind which is more stable and has a large air volume when viewed as a whole by the ion or ozone wind generator 100.

此外,如第15圖,本形態之離子、臭氧風 產生裝置100係使主電極對及副電極對之各對向電極彼此鄰接,且設為使各個電極可導通(各針狀電極120a至120g亦相同地設為使各個電極可導通)。藉由設為此種構成,而可將各對向電極(各針狀電極)設為等電位,且可容易進行殺菌、除臭裝置整體之電壓的控制,並可使離子風的產生穩定{但是,不限定於此,亦可使各對向電極(各針狀電極)設為不能導通}。 In addition, as shown in Figure 15, the ion and ozone wind of this form The generating apparatus 100 is such that each of the counter electrode of the main electrode pair and the sub-electrode pair is adjacent to each other, and each of the electrodes can be electrically connected (the respective needle electrodes 120a to 120g are also made to be electrically connected to each other). With such a configuration, each of the counter electrodes (each of the needle electrodes) can be set to the same potential, and the sterilization and the voltage of the entire deodorizing device can be easily controlled, and the generation of the ion wind can be stabilized. However, the present invention is not limited thereto, and each of the counter electrodes (each of the needle electrodes) may be made non-conductive}.

再者,依據本形態之離子、臭氧風產生裝 置100,針對一個對向電極(2重環狀對向電極)存在一個針狀電極(以一對一對應之方式而存在),且設為在各個電極對可進行電暈放電之(在複數個電極對可產生離子風)構成,故可保持離子、臭氧風產生裝置100整體的動作穩定性,並由於在各個電極對可得到大的風量之離子風,且復將上述電極對之離子風予以加總,故可得到穩定且大風量的離子風。 Furthermore, the ion and ozone wind generating device according to the present embodiment 100, for one counter electrode (two heavy annular counter electrode) there is one needle electrode (present in a one-to-one correspondence), and it is set to corona discharge in each electrode pair (in the plural Since the electrode pairs are configured to generate ion wind, the operation stability of the ions and the ozone wind generating device 100 as a whole can be maintained, and the ion wind of a large air volume can be obtained in each electrode pair, and the ion wind of the electrode pair can be restored. By adding them together, a stable and high-volume ion wind can be obtained.

以上,如上述說明,依據本實施形態之離 子、臭氧風產生裝置100,藉由設想可發出離子風之虛擬圓,且具備屬於在該虛擬圓的圓周上以相互鄰接或接近之形態定位對向電極之電極對之複數組副電極對,且具備屬於在該虛擬圓之圓周內定位對向電極之電極對之主電極對,而可更穩定地產生更強的離子風。在此,在第15圖中,雖為將主電極對之環狀對向電極以及副電極對之環狀對向電極的大小設為皆相等者,且以將副電極對之6個環狀對向電極,外切於主電極對之環狀對向電極之方式予以設置之構成,惟各對向電極對的形狀及位置關係不限定於此,作為可發揮前述效果(例如,副電極對之保護效果)之構成而言,可考量種種構成。 As described above, according to the above description, according to the present embodiment The ozone wind generating device 100 is assumed to have a virtual circle that can emit an ion wind, and has a plurality of pairs of secondary electrode pairs belonging to electrode pairs that are positioned adjacent to each other or close to each other on the circumference of the virtual circle. Further, a main electrode pair belonging to an electrode pair for positioning the counter electrode in the circumference of the virtual circle is provided, and a stronger ion wind can be generated more stably. Here, in Fig. 15, the size of the annular counter electrode of the main electrode pair and the annular counter electrode of the pair of counter electrodes are all equal, and six pairs of the pair of sub-electrodes are ring-shaped. The counter electrode is configured to be circumscribed to the annular counter electrode of the main electrode pair. However, the shape and positional relationship of each counter electrode pair are not limited thereto, and the above effects can be exhibited (for example, the pair of secondary electrodes The composition of the protective effect can be considered in various configurations.

例如,如第17圖所示,亦可依將副電極對 之環狀對向電極設為比主電極對之環狀對向電極更小的直徑(環直徑),並使其外切於主電極對之環狀對向電極之方式,而將副電極對之環狀對向電極(以各環狀對向電極彼此 鄰接之方式)予以配置。 For example, as shown in Figure 17, the secondary electrode pair can also be used. The annular counter electrode has a smaller diameter (ring diameter) than the annular counter electrode of the main electrode pair, and is circumscribed to the annular counter electrode of the main electrode pair, and the sub-electrode pair Annular counter electrode (with each annular counter electrode Adjacent mode) is configured.

另一方面,如第18圖所示,亦可依將副電 極對之環狀對向電極設為比主電極對之環狀對向電極更大的直徑(環直徑),且使其外切到主電極對之環狀對向電極之方式,而將副電極對之環狀對向電極(以各環狀對向電極彼此鄰接之方式)予以配置。 On the other hand, as shown in Figure 18, The pair of annular counter electrodes are set to have a larger diameter (ring diameter) than the annular counter electrode of the main electrode pair, and are circumscribed to the annular counter electrode of the main electrode pair, and the pair is The annular counter electrode of the pair of electrodes (the manner in which the respective annular counter electrodes are adjacent to each other) is disposed.

再者,如第19圖所示,亦可不將複數個副 電極對之環狀對向電極各者設為相同的形狀,而可將一部分的副電極對之環狀對向電極設為大的直徑(環直徑),而將別的副電極對之環狀對向電極設為更小的直徑(環直徑)。 Furthermore, as shown in Figure 19, it is also possible not to have multiple pairs The annular counter electrode of the electrode pair has the same shape, and a part of the pair of counter electrode pairs may have a large diameter (ring diameter) and a pair of other pair of electrodes. The counter electrode is set to a smaller diameter (ring diameter).

此外,如第20圖所示,亦可設為不將主電 極對之環狀對向電極與副電極對之環狀對向電極配置在相同的平面上(包含主電極對之環狀對向電極之類的平面),而配置在不同的平面上之構成{例如,在第20圖中主電極對係以比副電極對更靠前面側(離子風的噴出方向側)之方式而配置}。 In addition, as shown in Figure 20, it can also be set to not main power The annular counter electrode of the pair of opposite poles and the pair of counter electrode pairs are disposed on the same plane (including a plane such as a ring-shaped counter electrode of the main electrode pair), and are disposed on different planes. {For example, in FIG. 20, the main electrode pair is disposed on the front side (the side in which the ion wind is ejected) of the sub-electrode pair}.

並且,如第21圖所示,主電極對不限定於 一個,亦可設為設置複數個主電極對之構成(例如,第20圖中將第1對向電極130a設為3個)。 Further, as shown in Fig. 21, the main electrode pair is not limited to One may be configured to provide a plurality of main electrode pairs (for example, three first counter electrodes 130a are provided in FIG. 20).

在此,如第22圖所示,主電極對及/或副電 極對之對向電極,不限於多角形狀與圓形狀以及大致圓形狀,亦可為設為渦卷狀的態樣(捲繞數與捲繞寬度僅為一例)。在此,第22圖(a)所示之類的渦卷狀與第22圖(b)所 示之類的渦卷狀的相異點,係朝向中心形成渦卷狀時之旋渦之終點的有無。尤其於將各對向電極設為第22圖(b)所示之類的渦卷狀時,有可容易使各對向電極彼此導通之優點。此外,茲容補充說明者,在將對向電極設為此種渦卷狀時,與多重環狀構造的情況比較,雖有在電暈放電上產生不均之虞慮,惟對向電極本身愈小型化(例如,對向電極的直徑為1cm程度),成為該不均的產生要因之渦卷狀的導線各部與針狀電極之距離誤差(從多重環狀構造之剥離)變小,故變得容易得到與多重環狀構造相同的效果。 Here, as shown in Fig. 22, the main electrode pair and/or the sub-electricity The counter electrode is not limited to a polygonal shape, a circular shape, or a substantially circular shape, and may be in a spiral shape (the number of windings and the winding width are only an example). Here, the scroll shape shown in Fig. 22 (a) and the 22 (b) The spiral-shaped difference point shown is the presence or absence of the end point of the vortex when the scroll is formed toward the center. In particular, when each of the counter electrodes is formed into a spiral shape as shown in Fig. 22(b), there is an advantage that the respective counter electrodes can be easily electrically connected to each other. In addition, when the counter electrode is formed in such a spiral shape, compared with the case of the multi-ring structure, there is a concern that unevenness occurs in the corona discharge, but the counter electrode itself The smaller the size (for example, the diameter of the counter electrode is about 1 cm), the smaller the occurrence of the unevenness is because the distance error between the respective portions of the spiral-shaped wire and the needle electrode (peeling from the multiple annular structure) becomes small. It becomes easy to obtain the same effect as the multiple ring structure.

此外,如第23圖所示,亦可將放電側之電 極(例如針狀電極),設為環狀放電電極120{第23圖(b)},或僅設為針狀電極被橋接成環狀之環狀放電電極120{第23圖(a)}。 In addition, as shown in Figure 23, the electricity on the discharge side can also be The pole (for example, a needle electrode) is a ring-shaped discharge electrode 120 {Fig. 23(b)}, or only a ring-shaped discharge electrode 120 in which a needle electrode is bridged into a ring shape (Fig. 23(a)} .

由於負離子、臭氧產生裝置之小型化(攜帶 化)=離子風的小風力化之事態為是不可避免的趨勢,故如盡可能不削減由電暈放電所產生之離子風的風力並將其被送達到對象物之一些精心設計於商品化方面為重要事項。 但是,既然是盡可能以小型化(攜帶化)為目標,則較佳為不設置送風裝置與升壓型轉換器等之附加裝置,而將設計心力集中投注在負離子、臭氧產生裝置的必要構成之電極構成。依據本實施形態,即使將負離子、臭氧產生裝置予以小型化(可攜化),亦可提供用以適當地使離子風產生之手段。 Miniaturization of negative ions and ozone generating devices (carrying The state of the small wind of the ion wind is an inevitable trend, so if the wind of the ion wind generated by the corona discharge is not reduced as much as possible and some of the object is sent to the object, it is carefully designed and commercialized. Aspects are important matters. However, since it is intended to be miniaturized (portable) as much as possible, it is preferable to concentrate the design effort on the negative ion and the ozone generating device without providing an additional device such as a blower and a boost converter. The electrode is composed. According to the present embodiment, even if the negative ion or ozone generating device is miniaturized (portable), means for appropriately generating the ion wind can be provided.

<第2實施形態> <Second embodiment>

依據本實施形態之上述離子、臭氧風產生裝置100,雖可得到足夠的風量之離子風,惟就產生之離子風為大致單向之觀點而言復有改良的空間{具體而言,由於所產生之離子風朝特定的方向,故例如將上述離子、臭氧風產生裝置100設置在被密閉的房間內之任意的場所時,有產生之離子風不會有效地遍佈整個房間(由於所產生之離子風的風力強,故在被密閉之房間內離子、臭氧分子雖會循環,惟該循環效率低)之可能性}。為此,比起上述離子、臭氧風產生裝置100,有關可使離子風產生在更廣泛的範圍之本實施形態的殺菌、除臭裝置之另外的形態之離子、臭氧風產生裝置100,設為第2實施形態加以詳述。此外,在第2實施形態所示之例示僅為一例,有關屬於本實施形態之技術的範圍之具體的變更例在第3實施形態等予以後述。再者,在本說明書中作為一例所舉出之實施形態與變更例,不應限定性地理解為適用於特定者,亦可為任何組合。例如,針對某實施形態之變更例,應理解為別的實施形態之變更例,此外,即便獨立記載有某變更例與別的變更例,亦應理解為亦記載有將該某變更例與該別的變更例予以組合者。並且,作為在實施形態與變更例所示之具體的一例之數值{例如,放電電極與對向電極的直徑與長度、厚度、放電電極與對向電極之電壓差、放電電極與對向電極之相隔距離,等}係僅為一例,只要不大大脫離各實施形態與變更例的宗旨,應理解為可作適當變更。 According to the ion and ozone wind generation device 100 of the present embodiment, an ion wind having a sufficient air volume can be obtained, but the space in which the ion wind generated is substantially unidirectional is improved. Since the generated ion wind is directed in a specific direction, for example, when the ion or ozone wind generating device 100 is installed in any place in a sealed room, the generated ion wind does not effectively spread throughout the room (due to the generation The wind of the ion wind is strong, so the ion and ozone molecules in the sealed room will circulate, but the cycle efficiency is low. For this reason, the ion or ozone wind generation device 100 of another embodiment of the sterilization and deodorization device of the present embodiment which can generate ion wind in a wider range is used as the ion and ozone wind generation device 100. The second embodiment will be described in detail. In addition, the example shown in the second embodiment is only an example, and a specific modification of the scope of the technology of the present embodiment will be described later in the third embodiment and the like. In addition, the embodiment and the modification examples which are exemplified in the present specification are not limited to being applicable to a specific one, and may be any combination. For example, a modified example of a certain embodiment is understood to be a modified example of another embodiment, and even if a certain modified example and another modified example are separately described, it should be understood that the modified example and the modified example are also described. Other variants are combined. Further, it is a numerical value of a specific example shown in the embodiment and the modified example. For example, the diameter and length of the discharge electrode and the counter electrode, the thickness, the voltage difference between the discharge electrode and the counter electrode, and the discharge electrode and the counter electrode. The distance between the distances and the like is merely an example, and it should be understood that the distance can be appropriately changed without departing from the spirit of the embodiments and the modifications.

首先,第2實施形態及後述之第3實施形態 之離子、臭氧風產生裝置雖就作為該基本的概念而具備具有放電電極與對向電極的電極對之觀點來看與本實施形態相同,惟將放電電極設為線狀的放電部(放電線),且亦將對向電極設為線狀的受電部(受電線)。亦即,使於分散在放電部(放電線)上之放電點與分散在受電部(受電線)上的受電點之間產生電位差,且在多個點同時使電暈放電之離子、臭氧、及離子風產生。此外,如前述,離子風一般而言,係藉由於電暈放電時於從放電點釋出之離子朝受電點游動之間重覆與空氣分子之衝撞,而從放電點朝受電點產生的空氣流。亦即,依照放電時產生之離子的流動方向(向量)而產生之氣流雖為離子風,惟在本專利申請案發明中,亦著眼於利用該空氣流產生的負壓及朝產生該負壓的空間之外氣的吸氣流之離子風的增大效果。例如,從在第5圖所示之離子風的產生處所可知,在環狀的對向電極之內周邊緣部產生電暈放電時,離子風從該內周邊緣部附近被釋出到前面方向(與針狀電極不相對向之側的方向),惟於此時,於對向電極之環狀部背側(不與針狀電極相對之側的面)產生負壓。接著,朝產生該負壓的空間,尤其是圍繞對向電極的外周之外氣被吸引,且利用該被吸引之外氣來增大被推出到前面方向之離子風的風力增大。此係在使分散在放電部(放電線)上之放電點與分散在受電部(受電線)上之受電點之間產生電位差且利用電暈放電使離子、臭氧及離子風產生之情況亦相同,而於受電部(受電線)之不與放電部(放電線)相對向之側的開放部,係產生透過此負壓而增 大之離子風。以下,就根據此種基本概念之本實施形態之離子、臭氧風產生裝置的詳細構造加以說明。 First, the second embodiment and the third embodiment to be described later In the same manner as in the present embodiment, the ion and ozone wind generating device are provided with the electrode pair having the discharge electrode and the counter electrode as the basic concept, but the discharge electrode is a linear discharge portion (discharge line). In addition, the counter electrode is also a linear power receiving unit (receiving wire). In other words, a potential difference is generated between a discharge point dispersed on the discharge portion (discharge line) and a power receiving point distributed on the power receiving unit (receiving wire), and ions, ozone, and corona discharge are simultaneously simultaneously formed at a plurality of points. And ion wind generation. In addition, as described above, the ion wind is generally generated by the collision of the ions released from the discharge point toward the power receiving point due to the collision with the air molecules during the corona discharge, and is generated from the discharge point toward the power receiving point. Air flow. That is, the airflow generated according to the flow direction (vector) of the ions generated during the discharge is an ion wind, but in the invention of the present application, attention is also paid to the use of the negative pressure generated by the air flow and the generation of the negative pressure. The increase in the ion wind of the suction flow outside the space. For example, as is apparent from the generation of the ion wind shown in Fig. 5, when corona discharge is generated at the inner peripheral edge portion of the annular counter electrode, the ion wind is released from the vicinity of the inner peripheral edge portion to the front direction. (the direction opposite to the side opposite to the needle electrode), but at this time, a negative pressure is generated on the back side of the annular portion of the counter electrode (the surface on the side opposite to the needle electrode). Then, the gas which is generated in the space where the negative pressure is generated, in particular, the outer circumference of the counter electrode is attracted, and the air outside the suction is used to increase the wind force of the ion wind pushed out to the front direction. This is the case where a potential difference is generated between a discharge point dispersed on a discharge portion (discharge line) and a power receiving point distributed on a power receiving portion (receiving wire), and ion, ozone, and ion wind are generated by corona discharge. In the open portion of the power receiving unit (receiving wire) that is not opposite to the discharge portion (discharge line), the negative pressure is increased by the negative pressure. Big ion wind. Hereinafter, the detailed structure of the ion and ozone wind generating apparatus according to the present embodiment of the basic concept will be described.

首先,將第2實施形態之離子、臭氧風產生 裝置100-2的概略構造表示於第24圖。第24圖(a)係該裝置的電極對310之概念正視圖,而第24圖(b)係電極對310之概念側視圖。第2實施形態之離子、臭氧風產生裝置100-2係由具有放電電極(在本實施形態中為環狀電極)與對向電極(在本實施形態中為環狀電極)之1組電極對所構成。在此,對向電極及放電電極(尤其是放電電極)藉由線狀構件(但是,不僅以將線狀的電極圍成環狀之方式形成,且亦包含以保留圓盤狀的電極之外周之方式進行穿孔而形成者)所構成,藉此由線狀且環狀的放電電極320與線狀且環狀的對向電極330構成電極對310。此外,放電電極320為線狀時,屬於放電電極320之環的外周邊緣(與對向電極330相對向之側的環緣)之放電部321亦成為線狀,以下,有時將放電電極320與放電部321作為相同構件來形容(亦即,作為構件為相同,尤其是將產生放電之部位稱為放電部321)。此外,對向電極330為線狀時亦相同,有時將對向電極330與受電部331作為相同構件來形容(此時,作為構件雖為相同,惟尤其是將產生受電之部位稱為受電部331)。在此,在本例中,電極對310之對向電極330(受電部331)與放電電極320(放電部321)係配置在大致相同的平面上,並構成為在對向電極330(受電部331)與放電電極320(放電部321)中,為放電電極320(放電部321)之周長較 小。再者,在本例中,由於放電電極320(放電部321)與對向電極330(受電部331)相似,且藉由配置成同心圓狀,使得放電電極320(放電部321)之放電點322與到對向電極330(受電部331)之受電點332(從放電點322來看在最短距離之受電點)為止之距離,係在任一處所皆大致相等,故以放電不均現象變少之方式而構成。 First, the ion and ozone wind of the second embodiment are generated. The schematic structure of the device 100-2 is shown in Fig. 24. Fig. 24(a) is a conceptual front view of the electrode pair 310 of the device, and Fig. 24(b) is a conceptual side view of the electrode pair 310. The ion and ozone wind generation device 100-2 of the second embodiment is a pair of electrode pairs having a discharge electrode (in the present embodiment, a ring-shaped electrode) and a counter electrode (in the present embodiment, a ring-shaped electrode). Composition. Here, the counter electrode and the discharge electrode (especially the discharge electrode) are formed by a linear member (however, not only the wire-shaped electrode is formed in a ring shape but also the outer periphery of the electrode which retains the disk shape) The formation is performed by perforation, whereby the linear and annular discharge electrode 320 and the linear and annular counter electrode 330 constitute the electrode pair 310. Further, when the discharge electrode 320 is linear, the discharge portion 321 which is the outer peripheral edge of the ring of the discharge electrode 320 (the rim on the side opposite to the counter electrode 330) also has a linear shape. Hereinafter, the discharge electrode 320 may be used. The discharge portion 321 is described as the same member (that is, the member is the same, and particularly the portion where the discharge is generated is referred to as the discharge portion 321). In the case where the counter electrode 330 is linear, the counter electrode 330 and the power receiving unit 331 may be described as the same member (in this case, although the members are the same, the portion where the power is generated is referred to as power receiving. Part 331). Here, in this example, the counter electrode 330 (power receiving unit 331) of the electrode pair 310 and the discharge electrode 320 (discharge unit 321) are arranged on substantially the same plane, and are configured as the counter electrode 330 (power receiving unit). 331) and the discharge electrode 320 (discharge portion 321) are the circumference of the discharge electrode 320 (discharge portion 321) small. In the present example, the discharge electrode 320 (discharge portion 321) is similar to the counter electrode 330 (power receiving portion 331), and is arranged in a concentric shape so that the discharge point of the discharge electrode 320 (discharge portion 321) is made. The distance from 322 to the power receiving point 332 of the counter electrode 330 (power receiving unit 331) (the power receiving point at the shortest distance from the discharge point 322) is substantially equal in any place, so that the discharge unevenness is reduced. It is constituted by the way.

藉由以此方式來構成,在放電電極320(放 電部321)與對向電極330(受電部331)之間產生電位差時,可於對向電極330(受電部331)的外周{不與放電電極320(放電部321)相對向之側的開放部}之全方向(360度方向)產生離子風(圖中的閃電線是電暈放電的概念圖,係粗箭頭符號線為關於所產生之離子風的一部分之產生方向的概念圖)。此外,本例之放電電極320(放電部321)與對向電極330(受電部331)係在第24圖(b)中,為了說明的方便,以設置有對向電極330(受電部331)存在的平面與放電電極320(放電部321)存在的平面之距離的方式(隔離著)予以圖示,而實際上,對向電極330(受電部331)與放電電極320(放電部321)最好存在相同平面上{亦即,雖然對向電極330(受電部331)與放電電極320(放電部321)只要存在於大致相同平面上,可創出此種作用,惟於將放電效率予以最大化=將從放電電極320(放電部321)之放電點322到對向電極330(受電部331)之受電點332為止之距離予以最小化之觀點來看,係意指對向電極330(受電部331)與放電電極320(放電部321)最好配置在相同平面上之意思}。 By being configured in this way, at the discharge electrode 320 When a potential difference is generated between the electric portion 321) and the counter electrode 330 (power receiving portion 331), the outer circumference of the counter electrode 330 (power receiving portion 331) can be opened to the side opposite to the discharge electrode 320 (discharge portion 321). The ion direction is generated in the omnidirectional direction (360 degree direction) (the lightning line in the figure is a conceptual diagram of corona discharge, and the thick arrow symbol line is a conceptual diagram about the direction in which a part of the generated ion wind is generated). Further, the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) of the present embodiment are shown in Fig. 24(b), and the counter electrode 330 (power receiving portion 331) is provided for convenience of explanation. The manner in which the existing plane is spaced from the plane where the discharge electrode 320 (discharge portion 321) exists is shown (isolated), and actually, the counter electrode 330 (power receiving portion 331) and the discharge electrode 320 (discharge portion 321) are the most It is preferable to exist on the same plane {that is, although the counter electrode 330 (power receiving portion 331) and the discharge electrode 320 (discharge portion 321) exist on substantially the same plane, this effect can be created, but the discharge efficiency is maximized. = from the viewpoint of minimizing the distance from the discharge point 322 of the discharge electrode 320 (discharge portion 321) to the power receiving point 332 of the counter electrode 330 (power receiving portion 331), it means the counter electrode 330 (power receiving unit) 331) is preferably disposed on the same plane as the discharge electrode 320 (discharge portion 321).

再者,在本例中,雖在放電電極320(放電 部321)之環的外側設置有對向電極330(受電部331),而亦可構成為在對向電極330(受電部331)之環的外側設置放電電極320(放電部321)之方式(亦即,亦可使雙方的配置倒置)。以此方式構成時,朝對向電極330(受電部331)之環的內側中心方向產生離子風。亦即,使於對向電極330(受電部331)的外周{不與放電電極320(放電部321)相對向之側的開放部}之全方向(360度方向)產生離子風時,可使離子風聚集到某特定的空間。茲容補充說明者,此係亦同樣可應用於第2實施形態與第3實施形態所例示之所有的構成。 Furthermore, in this example, although at the discharge electrode 320 (discharge The opposite electrode 330 (power receiving portion 331) is provided on the outer side of the ring of the portion 321), and the discharge electrode 320 (discharge portion 321) is provided outside the ring of the counter electrode 330 (power receiving portion 331). That is, the configuration of both parties can also be reversed. In this configuration, the ion wind is generated toward the inner center direction of the ring of the counter electrode 330 (power receiving portion 331). In other words, when ion wind is generated in the entire direction (the 360-degree direction) of the outer circumference of the counter electrode 330 (power receiving unit 331) (the opening portion that does not face the discharge electrode 320 (discharge portion 321)}, the ion wind can be generated. Ion winds gather in a specific space. It is to be noted that the same applies to all the configurations exemplified in the second embodiment and the third embodiment.

其次,第25圖係例示第2實施形態之離子、 臭氧風產生裝置100-2的使用時及清潔時的一例。於第2實施形態之離子、臭氧風產生裝置100-2之使用時,如第25圖(a)所示,將離子、臭氧風產生裝置100-2安裝在天花板400(例如,方形之六張榻榻米房間的天花板中央附近)來使用。再者,該安裝方法沒特別限定,只要將離子、臭氧風產生裝置100-2固定在天花板400就沒問題(例如,可使用利用螺絲進行裝配等之為人所熟知的方法)。在本例中,以由蓋罩單元350覆蓋離子、臭氧風產生裝置100-2的電極對310之形態來予以構成,而蓋罩單元350由蓋罩構件360與蓋構件370所構成,其中蓋罩構件360係於設置在天花板400時被固定在天花板400,而蓋構件370係成為蓋罩構件360的蓋。再者,於蓋罩構件360與蓋構件370之間設置有噴出口340,從電極對310產生之離子風係 從該噴出口340被噴出到離子、臭氧風產生裝置100-2的外部。再者,噴出口340的形狀係只要為所產生之離子風可通過的形狀則沒問題,例如,亦可設為狹縫狀,亦可設為挖空蓋罩單元350而形成孔之形狀。 Next, Fig. 25 illustrates the ions of the second embodiment, An example of the use and cleaning of the ozone wind generating device 100-2. When the ion or ozone wind generator 100-2 of the second embodiment is used, as shown in Fig. 25(a), the ion and ozone wind generator 100-2 is attached to the ceiling 400 (for example, six squares) It is used near the center of the ceiling in the tatami room. In addition, the mounting method is not particularly limited as long as the ion/ozone wind generating device 100-2 is fixed to the ceiling 400 (for example, a well-known method such as assembly using a screw) can be used. In this example, the electrode unit 310 of the ion and ozone wind generating device 100-2 is covered by the cover unit 350, and the cover unit 350 is composed of a cover member 360 and a cover member 370, wherein the cover The cover member 360 is fixed to the ceiling 400 when it is placed on the ceiling 400, and the cover member 370 is a cover of the cover member 360. Furthermore, a discharge port 340 is provided between the cover member 360 and the cover member 370, and the ion wind system is generated from the electrode pair 310. The discharge port 340 is discharged to the outside of the ion or ozone wind generator 100-2. Further, the shape of the discharge port 340 is not limited as long as it is a shape through which the generated ion wind can pass. For example, the shape of the hole may be formed by hollowing out the cover unit 350.

然後,於第2實施形態之離子、臭氧風產生 裝置100-2之清潔時,如第25圖(b)所示,從蓋罩構件360將蓋構件370予以拆卸。再者,如同圖所示,只要為蓋罩構件360與放電電極320(放電部321)被固定,且蓋構件370與對向電極330(受電部331)被固定之方式來予以構成,則可從離子、臭氧風產生裝置100-2,將蓋構件370與對向電極330(受電部331)同時予以拆卸,且可將污物容易附著之對向電極330(受電部331)與天花板400周邊予以簡單地清潔。再者,離子、臭氧風產生裝置100-2之使用方法與設置場所不限定於此,例如,亦可在桌上使用,或在牆壁上使用{此時,視用途亦可適當地變更放電電極320(放電部321)及對向電極330(受電部331)的內徑}。 Then, the ion and ozone wind are generated in the second embodiment. When the apparatus 100-2 is cleaned, the cover member 370 is detached from the cover member 360 as shown in Fig. 25(b). Further, as shown in the figure, as long as the cover member 360 and the discharge electrode 320 (discharge portion 321) are fixed, and the cover member 370 and the counter electrode 330 (power receiving portion 331) are fixed, it is possible to In the ion/ozone wind generating device 100-2, the cover member 370 and the counter electrode 330 (power receiving unit 331) are simultaneously removed, and the counter electrode 330 (power receiving unit 331) which can easily adhere the dirt and the ceiling 400 can be attached. Simply clean it. Further, the method of using the ion and ozone wind generating device 100-2 and the installation place are not limited thereto, and for example, it may be used on a table or on a wall. {At this time, the discharge electrode may be appropriately changed depending on the application. 320 (discharge portion 321) and counter electrode 330 (power receiving portion 331) inner diameter}.

以上雖為第2實施形態之離子、臭氧風產生 裝置100-2的一例,惟放電電極、對向電極的形狀、數目以及位置關係不限定於此,作為可廣泛地產生離子風之構成而言,可考量種種構成。為此,將這些種種構成的一例顯示於以下。 The above is the ion and ozone wind generated in the second embodiment. In an example of the device 100-2, the shape, the number, and the positional relationship of the discharge electrode and the counter electrode are not limited thereto, and various configurations can be considered as a configuration in which ion wind can be widely generated. For this reason, an example of these various configurations is shown below.

首先,第2實施形態之放電電極320及對向 電極330(受電部331)亦可為多角形,例如,如第26圖所示亦可為三角形。再者,第26圖(a)係該裝置之電極對310 的概念正視圖,第26圖(b)係該裝置的電極對310之概念側視圖。如同圖所示,電極對310即使為三角形的形狀,由於在三角形的各邊上,進行幾乎均等的放電,故可遍及全周使離子風產生(圖中的閃電線為電暈放電之概念圖,粗箭頭符號線係有關所產生之離子風的一部分之產生方向之概念圖)。此外,在本例中,雖將放電電極320(放電部321)及對向電極330(受電部331)設為三角形,惟亦可為三角形以上之多角形(此外,即使不為多角形,亦可為具有多數的凹凸的形狀,或亦可為該凹凸成為波狀)。但是,最好以放電電極320(放電部321)若為三角形則對向電極330(受電部331)亦成為三角形之方式,而使放電電極320(放電部321)與對向電極330(受電部331)之頂點的數相同,此外,更佳的是放電電極320(放電部321)與對向電極330(受電部331)為相似關係。再者,放電電極320(放電部321)與對向電極330為相似關係時,最好放電電極320(放電部321)之環的重心位置與對向電極330(受電部331)之環的重心位置幾乎一致。藉由設為此種構成,使得相互的電極之距離(尤其是放電點322與受電點332之距離)可成為接近均等,故不易產生放電不均之現象(可遍佈全周使離子風產生)。此外,於將放電電極320(放電部321)及對向電極330(受電部331)設為多角形時,藉由加多邊數,使相互的距離(尤其是放電點322與受電點332之距離)更接近均等,而更不易產生放電不均之現象(因此,尤其理想的是電極形狀為圓形)。 First, the discharge electrode 320 and the opposite direction of the second embodiment The electrode 330 (power receiving portion 331) may also be polygonal, and may be triangular as shown in Fig. 26, for example. Furthermore, Fig. 26(a) is an electrode pair 310 of the device. Conceptual front view, Figure 26(b) is a conceptual side view of the electrode pair 310 of the device. As shown in the figure, even if the electrode pair 310 has a triangular shape, since almost uniform discharge is performed on each side of the triangle, ion wind can be generated throughout the entire circumference (the lightning line in the figure is a conceptual diagram of corona discharge). The thick arrow symbol line is a conceptual diagram of the direction in which a portion of the generated ion wind is generated. Further, in this example, the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) are triangular, but may be triangular or more polygonal (in addition, even if it is not polygonal) It may have a shape having a large number of irregularities, or may have a wavy shape. However, it is preferable that the discharge electrode 320 (the discharge portion 321) has a triangular shape, and the counter electrode 330 (the power receiving portion 331) also has a triangular shape, and the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion) are preferably used. The number of vertices of 331) is the same, and it is more preferable that the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) have a similar relationship. Further, when the discharge electrode 320 (discharge portion 321) and the counter electrode 330 have a similar relationship, it is preferable that the center of gravity of the ring of the discharge electrode 320 (discharge portion 321) and the center of gravity of the ring of the counter electrode 330 (power receiving portion 331) The location is almost the same. With such a configuration, the distance between the electrodes (especially the distance between the discharge point 322 and the power receiving point 332) can be made nearly equal, so that uneven discharge is less likely to occur (the ion wind can be generated throughout the entire circumference). . Further, when the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) are polygonal, the mutual distance (especially the distance between the discharge point 322 and the power receiving point 332) is increased by adding a polygonal number. ) is closer to equal, and is less prone to discharge unevenness (hence, it is particularly desirable that the electrode shape is circular).

再者,如第27圖所示,第2實施形態之離 子、臭氧風產生裝置100-2的放電部321(放電電極320的外側360度),亦可為於邊緣部分之放電部321設置有細微的凹凸之形狀(例如,如鋸子的刀刃之形狀,具有多數的凹凸之形狀)。以此方式來構成時,亦由於在放電部321的凸部(放電點322)與受電部331(受電點332)之間產生放電,故與放電部321未設置該細微的凹凸之情況相同,可產生均等的離子風(亦即,意味著在可得到大致均等的離子風之範圍內,可視為在放電部321設置細微的凹凸之構成亦與在放電部321不設置細微的凹凸之構成相同)。 Furthermore, as shown in Fig. 27, the second embodiment is separated from The discharge portion 321 of the ozone wind generating device 100-2 (the outer side of the discharge electrode 320 is 360 degrees) may be provided with a fine concavo-convex shape in the discharge portion 321 of the edge portion (for example, the shape of a blade such as a saw blade, Has a large number of concave and convex shapes). In this configuration, since discharge occurs between the convex portion (discharge point 322) of the discharge portion 321 and the power receiving portion 331 (power receiving point 332), the discharge portion 321 is not provided with the fine unevenness. The uniform ion wind can be generated (that is, the configuration in which the fine unevenness is provided in the discharge portion 321 in the range in which the substantially uniform ion wind can be obtained is also the same as the configuration in which the fine portion is not provided in the discharge portion 321 ).

此外,如第28圖所示,第2實施形態之離 子、臭氧風產生裝置100-2的放電電極320及對向電極330之形狀亦可為板狀。藉由以此方式來構成,使得放電電極320及對向電極330的強度提高而不易損壞。另一方面,尤其藉由將放電電極320的形狀,不設為板狀而設為環狀(例如,設為僅由放電部321構成之線狀電極,亦即或以在同圖所示之保留放電電極320的外周之形態進行穿孔),使得環的開口部成為吸氣口,故可產生更強的離子風。再者,就放電電極320及對向電極330的形狀而言不限定於此,亦可將一方設為板狀,而將另一方設為線狀等(亦即,只要有放電部321與受電部331即可)。 Further, as shown in Fig. 28, the second embodiment is separated from The discharge electrode 320 and the counter electrode 330 of the ozone wind generating device 100-2 may have a plate shape. By being configured in this manner, the strength of the discharge electrode 320 and the counter electrode 330 is increased without being easily damaged. On the other hand, in particular, the shape of the discharge electrode 320 is not limited to a plate shape, and is formed into a ring shape (for example, a linear electrode composed only of the discharge portion 321 or the same as shown in the same figure) The outer circumference of the discharge electrode 320 is retained to be perforated so that the opening of the ring becomes an intake port, so that a stronger ion wind can be generated. In addition, the shape of the discharge electrode 320 and the counter electrode 330 is not limited to this, and one of them may be a plate shape, and the other may be a line or the like (that is, as long as the discharge portion 321 and the power receiving portion are present Part 331 can be).

其次,第2實施形態之離子、臭氧風產生裝 置100-2之放電電極320及/或對向電極330亦可設置複數個,例如,如第29圖所示,亦可設置1個放電電極320(放電部321),且設置3個對向電極330(受電部331){對向電 極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}。此外,如第30圖所示,於設置3個對向電極時,如圖示將1個放電電極320(放電部321)與各個對向電極{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}配置為多層且使電位差產生時,從各個對向電極330(對向電極330a、對向電極330b、對向電極330c)同時產生離子風(圖中的閃電線為電暈放電之概念圖,粗箭頭符號線為關於所產生之離子風的一部分之產生方向之概念圖)。亦即,1個放電電極320(放電部321)之放電點322與各個對向電極{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}之受電點亦即在與從放電點322在最短距離之各受電點(受電點332a、受電點332b、受電點332c)之間同時產生電暈放電。 Next, the ion and ozone wind generating device of the second embodiment A plurality of discharge electrodes 320 and/or counter electrodes 330 of 100-2 may be provided. For example, as shown in FIG. 29, one discharge electrode 320 (discharge portion 321) may be provided, and three opposite directions may be provided. Electrode 330 (power receiving unit 331) {opposite power The pole 330a (power receiving unit 331a), the counter electrode 330b (power receiving unit 331b), and the counter electrode 330c (power receiving unit 331c)}. Further, as shown in Fig. 30, when three counter electrodes are provided, one discharge electrode 320 (discharge portion 321) and each counter electrode {opposing electrode 330a (power receiving portion 331a) are opposed to each other as shown in the figure. When the electrode 330b (power receiving unit 331b) and the counter electrode 330c (power receiving unit 331c) are arranged in a plurality of layers and the potential difference is generated, the counter electrode 330 (the counter electrode 330a, the counter electrode 330b, and the counter electrode 330c) are simultaneously provided. Ion wind is generated (the lightning line in the figure is a conceptual diagram of corona discharge, and the thick arrow symbol line is a conceptual diagram about the direction in which a part of the generated ion wind is generated). In other words, the discharge point 322 of one discharge electrode 320 (discharge unit 321) and each counter electrode {opposing electrode 330a (power receiving unit 331a), counter electrode 330b (power receiving unit 331b), and counter electrode 330c (power receiving unit) The power receiving point of 331c)}, that is, the corona discharge is simultaneously generated between the respective power receiving points (power receiving point 332a, power receiving point 332b, and power receiving point 332c) which are at the shortest distance from the discharging point 322.

在此,在本例中,由於3個對向電極330a 至330c(受電部331a至331c)為相同的形狀、內徑,故配置在與1個放電電極320(放電部321)大致相同平面上之對向電極{對向電極330a(受電部331a)}之受電點(受電點332a)比起其他對向電極{對向電極330b(受電部331b)、對向電極330c(受電部331c)}之受電點(受電點332b、受電點332c),距離1個放電電極320(放電部321)之放電點322之距離變得更短。因此,此1個放電電極320(放電部321)與對向電極330a(受電部331a)之間的電暈放電之產生比例變成最大,且從對向電極330a產生之離子風的風力變得最大。然 後,在此1個放電電極320(放電部321)與對向電極330b(受電部331b)及對向電極330c(受電部331c)之間的電暈放電的產生比例相對變低,而從對向電極330b及對向電極330c產生之離子風的風力亦相對變弱。因此,藉由以此方式來構成,透過由對向電極330b及對向電極330c所產生的離子風之順風,由對向電極330a所產生的離子風以被推動之形態被推出到前面(關於該效果,在本實施形態已如前述)。由此來看,即使將本例所示之電極對予以小型化,亦可達到盡可能不削減透過電暈放電產生之離子風的風力而廣泛地遍佈之效果。 Here, in this example, due to the three counter electrodes 330a Since the 330c (power receiving units 331a to 331c) have the same shape and inner diameter, the counter electrode (opposing electrode 330a (power receiving unit 331a)) disposed on substantially the same plane as the one discharge electrode 320 (discharge portion 321) The power receiving point (power receiving point 332a) is compared with the power receiving point (power receiving point 332b, power receiving point 332c) of the other counter electrode {counter electrode 330b (power receiving unit 331b) and counter electrode 330c (power receiving unit 331c), distance 1 The distance between the discharge points 322 of the discharge electrodes 320 (discharge portions 321) becomes shorter. Therefore, the ratio of the generation of the corona discharge between the one discharge electrode 320 (discharge portion 321) and the counter electrode 330a (power receiving portion 331a) becomes maximum, and the wind force of the ion wind generated from the counter electrode 330a becomes maximum. . Of course Then, the ratio of occurrence of corona discharge between the one discharge electrode 320 (discharge portion 321) and the counter electrode 330b (power receiving portion 331b) and the counter electrode 330c (power receiving portion 331c) is relatively low, and the ratio is relatively low. The wind of the ion wind generated to the electrode 330b and the counter electrode 330c is also relatively weak. Therefore, by being configured in this manner, the ion wind generated by the counter electrode 330a is pushed out to the front by the downwind of the ion wind generated by the counter electrode 330b and the counter electrode 330c (about This effect is as described above in the present embodiment. From this point of view, even if the electrode pair shown in this example is miniaturized, it is possible to achieve an effect of widely spreading the wind of the ion wind generated by the corona discharge as much as possible.

再者,對向電極330a至330c之3個對向電 極亦可不為相同的形狀。例如,亦可藉由將對向電極330a(受電部的直徑)設為最大,而將對向電極330b及對向電極330c(受電部的直徑)設為比其更小,而使1個放電電極320之放電部距離各對向電極的受電部之距離設為均等。於設為此種構成時,從各對向電極產生相同的風量之離子風(因此,可產生立體且廣泛地遍佈之離子風)。 Furthermore, the three opposite electrodes of the opposite electrodes 330a to 330c Extremely not the same shape. For example, by setting the counter electrode 330a (diameter of the power receiving unit) to the maximum, the counter electrode 330b and the counter electrode 330c (diameter of the power receiving unit) can be made smaller than this, and one discharge can be made. The distance between the discharge portion of the electrode 320 and the power receiving portion of each of the counter electrodes is set to be equal. In such a configuration, the ion wind of the same air volume is generated from each of the counter electrodes (thereby, it is possible to generate a three-dimensional and widely distributed ion wind).

此外,第2實施形態之離子、臭氧風產生裝 置100-2之放電電極320亦可構成為不是設置1個而是設置複數個,例如,如第31圖所示,亦可將放電電極320(放電部321)設置3個{放電電極320a(放電部321a)、放電電極320b(放電部321b)、放電電極320c(放電部321c)},且將對向電極330(受電部331)設置3個{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電 部331c)},此時,如圖示亦可依放電電極與對向電極相互不同之方式予以配置(在同圖的例示中,可例示在對向電極間的中間層設置1個放電電極之態樣)。藉由如此構成,即便污物附著於某放電電極或對向電極等而未產生電暈放電現象,亦可藉由該某放電電極或對向電極以外之放電電極或對向電極的電暈放電來產生離子風。 Further, the ion and ozone wind generating device of the second embodiment The discharge electrode 320 of 100-2 may be configured not to be provided in plurality, but may be provided in plural. For example, as shown in FIG. 31, the discharge electrode 320 (discharge portion 321) may be provided with three {discharge electrodes 320a ( The discharge portion 321a), the discharge electrode 320b (discharge portion 321b), the discharge electrode 320c (discharge portion 321c), and the counter electrode 330 (power receiving portion 331) are provided with three {counter electrode 330a (power receiving portion 331a), and Electrode 330b (power receiving unit 331b) and counter electrode 330c (power receiving) In this case, the discharge electrode and the counter electrode may be arranged differently from each other as shown in the drawing (in the example of the same figure, one discharge electrode may be provided in the intermediate layer between the counter electrodes). Aspect). According to this configuration, even if the dirt adheres to a certain discharge electrode, the counter electrode, or the like without causing a corona discharge phenomenon, the corona discharge of the discharge electrode or the counter electrode other than the certain discharge electrode or the counter electrode can be used. To generate ion wind.

再者,在以上的說明中,第2實施形態之放電電極320及對向電極330的形狀,不限定於多角形與圓,只要為環狀即可(例如,即使為星型,亦達到相同的效果)。再者,該放電電極320的環狀內雖亦可為平板狀,惟該環狀內具有吸氣口的功能,故最好放電電極320為在平板開有孔的形狀或由線狀構件(例如,金屬線)製作出環狀之類的形狀。此外,從放電不均現象變少之觀點來看最好是環狀的放電電極320之放電部321(放電部的邊緣)的形狀為銳角。 In addition, in the above description, the shape of the discharge electrode 320 and the counter electrode 330 of the second embodiment is not limited to a polygon and a circle, and may be a ring shape (for example, even if it is a star shape, it is the same). Effect). Further, although the annular shape of the discharge electrode 320 may be a flat plate shape, but the annular shape has a function of an air intake port, it is preferable that the discharge electrode 320 has a shape in which a flat plate is opened or a linear member ( For example, a metal wire) is formed into a shape such as a ring. Further, it is preferable that the shape of the discharge portion 321 (the edge of the discharge portion) of the annular discharge electrode 320 is an acute angle from the viewpoint that the discharge unevenness is small.

<第3實施形態> <Third embodiment>

再者,第2實施形態之放電電極320及對向電極330的形狀係以成為環狀之方式予以構成,而不限定於此,例如,亦可設為將第2實施形態之放電電極320及對向電極330的一部分,以通過重心(放電電極320及對向電極330之幾乎一致的重心)之二條射線予以切割之形狀。為此,將此種構成作為本實施形態之殺菌、除臭裝置之另外的形態之離子、臭氧風產生裝置100-3之第3實施形態來予以詳述。再者,在第3實施形態中,該基本的概念係將放電電 極設為線狀的放電部(放電線),且將對向電極亦設為線狀的受電部(受電線),此點與第2實施形態相同。 In addition, the shape of the discharge electrode 320 and the counter electrode 330 of the second embodiment is configured to be annular, and is not limited thereto. For example, the discharge electrode 320 of the second embodiment and the discharge electrode 320 of the second embodiment may be used. A part of the counter electrode 330 is cut in a shape in which two rays passing through the center of gravity (the almost uniform center of gravity of the discharge electrode 320 and the counter electrode 330) are cut. For this reason, the third embodiment of the ion and ozone wind generating device 100-3 of another embodiment of the sterilization and deodorizing device of the present embodiment will be described in detail. Furthermore, in the third embodiment, the basic concept is to discharge electricity. The pole portion is a linear discharge portion (discharge line), and the counter electrode is also a linear power receiving portion (receiving wire), which is the same as in the second embodiment.

首先,如第32圖所示,第3實施形態之放 電電極320(放電部321)及對向電極330(受電部331)係成為以通過重心之二條射線將在第24圖所示之圓的形狀切割成4分之1的形狀{亦即,放電電極320(放電部321)及對向電極330(受電部331)係在第24圖所示之圓的四分之一的圓弧}。此外,第32圖(a)係第3實施形態之離子、臭氧風產生裝置100-3之電極對310的概念正視圖,而第32圖(b)係第3實施形態之離子、臭氧風產生裝置100-3之電極對310的概念側視圖。藉由以此方式來構成,比起第2實施形態之離子、臭氧風產生裝置100-2,產生離子風之範圍雖變窄(在本例中為90度),但可減小形狀並如後述適用於在房間的角落使用等之使用方法或設置方法(與上述第2實施形態之離子、臭氧風產生裝置100-2不同的使用方法或設置方法)。此外,第3實施形態之離子、臭氧風產生裝置100-3的形狀係只要為利用通過重心之二條射線將第2實施形態之離子、臭氧風產生裝置100-2(環狀)予以切割之形狀即可,切割之範圍(大小與角度)要如何處理皆不構成問題(例如,圓的2分之1、8分之1等),只要配合使用方法(設置場所)適當變更即可。 First, as shown in Fig. 32, the third embodiment is placed. The electric electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) are cut into a shape of a quarter of a circle shown in Fig. 24 by two rays passing through the center of gravity (i.e., discharge). The electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) are an arc of a quarter of a circle shown in Fig. 24. Further, Fig. 32(a) is a conceptual front view of the electrode pair 310 of the ion and ozone wind generating device 100-3 of the third embodiment, and Fig. 32(b) shows the ion and ozone wind generation of the third embodiment. Conceptual side view of electrode pair 310 of device 100-3. According to the configuration of the ion and ozone wind generator 100-2 of the second embodiment, the range of the ion wind is narrowed (in this example, 90 degrees), but the shape can be reduced and The method of use or the method of installation (the use method or the installation method different from the ion and ozone wind generator 100-2 of the second embodiment described above) is applied to the use of the corner of the room or the like. In addition, the shape of the ion or ozone wind generating device 100-3 of the third embodiment is a shape in which the ion and ozone wind generating device 100-2 (annular) of the second embodiment are cut by two rays passing through the center of gravity. That is, the processing range (size and angle) of the cutting does not pose a problem (for example, 1/8 of a circle, etc.), and can be appropriately changed in accordance with the method of use (installation place).

其次,第33圖係例示有第3實施形態之離 子、臭氧風產生裝置100-3的使用時之一例。此外,第33圖(a)係第3實施形態之離子、臭氧風產生裝置100-3之頂 視圖。於第3實施形態之離子、臭氧風產生裝置100-3的使用時,如第33圖(a)所示,將離子、臭氧風產生裝置100-3安裝在牆壁500(例如,方形的六張榻榻米的房間之天花板角附近)來使用。如同圖所示,藉由設為利用通過重心之二條射線將電極對310的形狀,從環狀切割成4分之1的形狀,而成為適合設置在房間的四角落之形狀。此外,藉由設置在房間的四角落,即使放電電極320(放電部321)及對向電極330(受電部331)的形狀不為環狀,亦可使強的離子風遍佈整個房間。此外,藉由將放電電極320及對向電極330設為曲線狀,可更廣泛地使均等的離子風產生(圖中的粗箭頭符號線為有關產生之離子風的一部分之產生方向之概念圖)。此外,第33圖(b)係第3實施形態之離子、臭氧風產生裝置100-3的側視圖。第3實施形態之離子、臭氧風產生裝置100-3係與第2實施形態之離子、臭氧風產生裝置100-2相同,設置有噴出口340,而從該噴出口340朝離子、臭氧風產生裝置100-3的外部噴出離子風(圖中的粗箭頭符號線為有關產生之離子風的一部分之產生方向之概念圖)。再者,離子、臭氧風產生裝置100-3的安裝方法沒特別限定,例如,如第33圖(b)所示,亦可固定於天花板400與牆壁500來使用。此外,離子、臭氧風產生裝置100-3係以蓋罩單元350覆蓋電極對310之形態所構成。蓋罩單元350由蓋罩構件360與蓋構件370所構成,其中蓋罩構件360係設置在天花板400及牆壁500時成為固定在天花板400及牆壁500,而蓋構件370係成為蓋罩構件360 的蓋。此外,於蓋罩構件360與蓋構件370之間設置有噴出口340,而從電極對310產生之離子風從該噴出口340被噴出到離子、臭氧風產生裝置100-3的外部。此外,噴出口340的形狀只要為所產生之離子風可通過的形狀則沒問題,例如,亦可設為狹縫狀,或亦可設為將蓋罩單元350挖空而形成孔的形狀。 Next, Fig. 33 illustrates an example of the third embodiment. An example of the use of the ozone wind generating device 100-3. Further, Fig. 33(a) is the top of the ion and ozone wind generating device 100-3 of the third embodiment. view. In the use of the ion or ozone wind generating device 100-3 of the third embodiment, as shown in Fig. 33(a), the ion and ozone wind generating device 100-3 is attached to the wall 500 (for example, six squares) Use it near the ceiling of the tatami room. As shown in the figure, the shape of the electrode pair 310 is cut from the ring shape by one-fourth shape by the two rays passing through the center of gravity, and is formed into a shape suitable for the four corners of the room. Further, by being provided at the four corners of the room, even if the shape of the discharge electrode 320 (discharge portion 321) and the counter electrode 330 (power receiving portion 331) are not annular, a strong ion wind can be spread throughout the room. Further, by forming the discharge electrode 320 and the counter electrode 330 in a curved shape, uniform ion wind can be generated more widely (the thick arrow symbol line in the figure is a conceptual diagram of the direction in which a part of the generated ion wind is generated). ). Further, Fig. 33(b) is a side view of the ion/ozone wind generating device 100-3 of the third embodiment. The ion and ozone wind generator 100-3 of the third embodiment is similar to the ion and ozone wind generator 100-2 of the second embodiment, and is provided with a discharge port 340 for generating ions and ozone wind from the discharge port 340. The ion wind is ejected from the outside of the device 100-3 (the thick arrow symbol line in the figure is a conceptual diagram regarding the direction in which a part of the generated ion wind is generated). Further, the method of attaching the ion and ozone wind generating device 100-3 is not particularly limited. For example, as shown in FIG. 33(b), it may be fixed to the ceiling 400 and the wall 500 for use. Further, the ion and ozone wind generating device 100-3 is configured by covering the electrode pair 310 with the cover unit 350. The cover unit 350 is composed of a cover member 360 and a cover member 370, wherein the cover member 360 is fixed to the ceiling 400 and the wall 500 when the ceiling 400 and the wall 500 are provided, and the cover member 370 is the cover member 360. Cover. Further, a discharge port 340 is provided between the cover member 360 and the cover member 370, and ion wind generated from the electrode pair 310 is discharged from the discharge port 340 to the outside of the ion or ozone wind generator 100-3. Further, the shape of the discharge port 340 is not limited as long as the shape of the generated ion wind can pass, and for example, it may be a slit shape, or may be a shape in which the cover unit 350 is hollowed out to form a hole.

再者,第3實施形態之離子、臭氧風產生裝 置100-3之放電電極320及/或對向電極330亦可設置複數個,例如,如第34圖所示,亦可設置1個放電電極320(放電部321)、3個對向電極330(受電部331){對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}。此外,如第35圖所示,設置3個對向電極時,在1個放電電極320(放電部321)與各個對向電極{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}之間產生電位差時,從各個對向電極330{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}同時產生離子風(圖中的閃電線為電暈放電的概念圖,而粗箭頭符號線為有關產生之離子風的一部分之產生方向的概念圖)。亦即,於1個放電電極320(放電部321)之放電點322與屬於各個對向電極{對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}之受電點之距離放電點322為最短距離之各受電點(受電點332a、受電點332b、受電點332c)之間同時產生電暈放電。 Furthermore, the ion and ozone wind generating device of the third embodiment A plurality of discharge electrodes 320 and/or counter electrodes 330 of 100-3 may be provided. For example, as shown in FIG. 34, one discharge electrode 320 (discharge portion 321) and three counter electrodes 330 may be provided. (power receiving unit 331) {opposing electrode 330a (power receiving unit 331a), counter electrode 330b (power receiving unit 331b), counter electrode 330c (power receiving unit 331c)}. Further, as shown in Fig. 35, when three counter electrodes are provided, one discharge electrode 320 (discharge portion 321) and each counter electrode {opposing electrode 330a (power receiving portion 331a) and counter electrode 330b (power receiving) When a potential difference is generated between the opposing portion 331b) and the counter electrode 330c (power receiving portion 331c), the counter electrode 330a (power receiving portion 331a), the counter electrode 330b (power receiving portion 331b), and the counter electrode are provided from the respective counter electrodes 330. 330c (power receiving unit 331c)} The ion wind is simultaneously generated (the lightning line in the figure is a conceptual diagram of corona discharge, and the thick arrow symbol line is a conceptual diagram regarding the direction in which a part of the generated ion wind is generated). That is, the discharge point 322 of one discharge electrode 320 (discharge portion 321) belongs to each of the counter electrode {counter electrode 330a (power receiving portion 331a), counter electrode 330b (power receiving portion 331b), and counter electrode 330c ( The corona discharge is simultaneously generated between the respective power receiving points (the power receiving point 332a, the power receiving point 332b, and the power receiving point 332c) at which the power receiving point 321c) is the shortest distance from the power receiving point 322.

在此,由於在本例中,3個對向電極330a 至330c(受電部331a至331c)為相同的形狀、內徑,故與第29圖的電極對310相同,於1個放電電極320(放電部321)與對向電極330a(受電部331a)之間的電暈放電之產生比例變為最大,而從對向電極330a(受電部331a)產生的離子風之風力變最大。然後,在此1個放電電極320(放電部321)與對向電極330b(受電部331b)及對向電極330c(受電部331c)之間的電暈放電之產生比例相對變低,且從對向電極330b(受電部331b)及對向電極330c(受電部331c)產生之離子風的風力相對變弱。因此,藉由以此方式來構成,且利用對向電極330b(受電部331b)及對向電極330c(受電部331c)所產生的離子風之順風,由對向電極330a(受電部331a)產生的離子風以被推動之形態被推出到到前面(關於該效果,在本實施形態已如前述)。據此,即使將第2實施形態所示之環狀的電極對予以小型化,亦藉由對設置場所精心設計,而可達到盡可能不削減透過電暈放電產生之離子風的風力而廣泛地遍佈之效果。 Here, since in this example, three counter electrodes 330a Since the 330c (power receiving units 331a to 331c) have the same shape and inner diameter, they are the same as the electrode pair 310 of FIG. 29, and are connected to the one discharge electrode 320 (discharge portion 321) and the counter electrode 330a (power receiving portion 331a). The ratio of generation of the corona discharge becomes maximum, and the wind of the ion wind generated from the counter electrode 330a (power receiving portion 331a) becomes maximum. Then, the ratio of occurrence of corona discharge between the one discharge electrode 320 (discharge portion 321) and the counter electrode 330b (power receiving portion 331b) and the counter electrode 330c (power receiving portion 331c) is relatively low, and the ratio is relatively low. The wind force of the ion wind generated to the electrode 330b (power receiving unit 331b) and the counter electrode 330c (power receiving unit 331c) is relatively weak. Therefore, by this configuration, the downwind of the ion wind generated by the counter electrode 330b (power receiving unit 331b) and the counter electrode 330c (power receiving unit 331c) is generated by the counter electrode 330a (power receiving unit 331a). The ionic wind is pushed to the front in a pushed state (this effect is as described above in this embodiment). According to this, even if the annular electrode pair shown in the second embodiment is miniaturized, it is possible to achieve a wind force that reduces the ion wind generated by the corona discharge as much as possible by designing the installation site. All over the effect.

再者,第3實施形態之離子、臭氧風產生裝 置100-3係與前述之第2實施形態相同,對向電極330a至330c之3個對向電極可不為相同的形狀,亦可得到與第2實施形態之離子、臭氧風產生裝置100-2相同的效果。 Furthermore, the ion and ozone wind generating device of the third embodiment The set 100-3 is the same as the second embodiment described above, and the three counter electrodes of the counter electrodes 330a to 330c may not have the same shape, and the ion and ozone wind generator 100-2 of the second embodiment may be obtained. The same effect.

再者,第3實施形態之離子、臭氧風產生裝 置100-3之放電電極320可不為1個而亦可構成為設置複數個,例如,如第36圖所示,亦可設置3個放電電極320(放 電部321){放電電極320a(放電部321a)、放電電極320b(放電部321b)、放電電極320c(放電部321c)},且設置3個對向電極330(受電部331){對向電極330a(受電部331a)、對向電極330b(受電部331b)、對向電極330c(受電部331c)}。藉由以此方式來構成,使得與第2實施形態之離子、臭氧風產生裝置100-2相同,即使污物附著於某放電電極或對向電極等不發生電暈放電,亦可透過該某放電電極或對向電極以外的放電電極或對向電極的電暈放電而可產生離子風。 Furthermore, the ion and ozone wind generating device of the third embodiment The number of the discharge electrodes 320 of 100-3 may be set to be plural, or a plurality of discharge electrodes 320 may be provided. For example, as shown in FIG. 36, three discharge electrodes 320 may be provided. Electric portion 321) {discharge electrode 320a (discharge portion 321a), discharge electrode 320b (discharge portion 321b), discharge electrode 320c (discharge portion 321c)}, and three counter electrode 330 (power receiving portion 331) are provided {opposing electrode 330a (power receiving unit 331a), counter electrode 330b (power receiving unit 331b), and counter electrode 330c (power receiving unit 331c). According to the configuration of the ion and ozone wind generator 100-2 of the second embodiment, even if the dirt adheres to a certain discharge electrode or the counter electrode, the corona discharge can be transmitted. Ion wind can be generated by corona discharge of a discharge electrode or a counter electrode other than the discharge electrode or the counter electrode.

以此方式,依據第3實施形態之離子、臭氧 風產生裝置100-3,比起第2實施形態之離子、臭氧風產生裝置100-2,即便離子風產生之範圍雖窄,亦適合於配置在特定的處所之情況與僅於特定的範圍(必要的範圍)內使離子風產生之情況。 In this way, the ions and ozone according to the third embodiment The wind generating device 100-3 is suitable for a specific space and a specific range even if the ion wind generation range is narrower than the ion or ozone wind generating device 100-2 of the second embodiment. The necessary range) is the case where the ion wind is generated.

<有關其他變更例與用途> <related other changes and uses>

本實施形態的離子、臭氧風產生裝置之放電電極的形狀亦可為立體狀(例如球形狀)(此時,在對向電極的受電部所存在之平面切斷放電電極時,立體狀的放電電極的剖面之外周的形狀只要與對向電極的受電部大致相似即可)。 The shape of the discharge electrode of the ion or ozone wind generator of the present embodiment may be three-dimensional (for example, a spherical shape) (in this case, when the discharge electrode is cut in the plane where the power receiving portion of the counter electrode is present, the three-dimensional discharge is performed. The shape of the outer circumference of the cross section of the electrode may be substantially similar to the power receiving portion of the counter electrode.

本實施形態之離子、臭氧風產生裝置除了可作為殺菌、除臭裝置來使用之外,亦可作為離子水/殺菌水產生裝置來使用。 The ion and ozone wind generating device of the present embodiment can be used as an ionized water/sterilizing water generating device, in addition to being used as a sterilization and deodorizing device.

本實施形態之裝置係藉由電暈放電而產生離子及/或臭氧,並且產生大風量的離子風,故可利用離子 風將上述離子及臭氧予以搬運,且使之接觸殺菌、除臭對象物而可作為離子、臭氧風產生裝置來使用。此外因產生大風量的離子風,故不使用幫浦而可使離子及臭氧產生且將之送進到配置殺菌、除臭對象物的空間故可作為外接型殺菌、除臭裝置來使用。 The apparatus of the present embodiment generates ions and/or ozone by corona discharge, and generates a large amount of ion wind, so that ions can be utilized. The wind transports the above-mentioned ions and ozone, and contacts the sterilizing and deodorizing objects to be used as an ion or ozone wind generating device. In addition, since the ion wind is generated by a large amount of air, ions and ozone are generated without using a pump, and the space is sent to a space where the sterilization and deodorizing objects are disposed, so that it can be used as an external sterilization and deodorizing device.

本實施形態之離子、臭氧風產生裝置係可 使用為氣泡石、奈米氣泡供氣源之海水及淡水的殺菌、除臭用。亦即,於奈米氣泡產生器,因必須取進空氣,故藉由結合離子風引導構件與供應路徑且作為奈米氣泡的空氣供氣源來使用,而可使離子/臭氧風在水中進行反應而可簡單地製作離子水/殺菌水。如此一來,關於透過臭氧水與奈米氣泡的相乘效應之皮膚的殺菌清洗所進行之毛孔深處的油脂去除、利用屬於臭氧的特性之漂白作用之美白效果等美容方面之利用、水產類飼養水槽內之殺菌、除臭,以及在耕栽培之培養液的殺菌等,而在厨房等亦以水管的吐出壓作為動力源而產生殺菌水,並利用有效的殺菌、除臭與臭氧水而進行之油脂的分解等,可簡單又便宜且安全地進行。 The ion and ozone wind generating device of the embodiment can be It is used for the sterilization and deodorization of seawater and fresh water which are air supply sources for bubble stones and nano bubbles. That is, in the nano bubble generator, since the air must be taken in, the ion/ozone wind can be performed in the water by combining the ion wind guiding member and the supply path and serving as an air supply source for the nanobubbles. Ion water/sterilized water can be easily produced by the reaction. In this way, the use of the beauty of the pores in the deep pores of the sterilizing and cleaning of the skin by the synergistic effect of the ozone water and the nanobubbles, the use of the whitening effect of the bleaching action which is characteristic of ozone, and the use of aquatic products Sterilization, deodorization, and sterilization of the culture solution in the cultivating water, and the use of the discharge pressure of the water pipe as a power source in the kitchen, etc., and the use of effective sterilization, deodorization, and ozone water. The decomposition of the oil and the like performed can be carried out simply, inexpensively and safely.

並且,在以離子、臭氧風產生裝置的小型 化{例如,將離子、臭氧風產生裝置之外形尺寸,設為長度7cm×寬度7cm×高度3cm程度,亦即,小型化至以單手可容易把持之程度}為目的,而將電極構成進行省空間化時{例如,將直徑1cm程度之對向電極(適當的範圍為5mm至5cm),如第15圖所示予以配置,而將針狀電極與對向電極 之相隔距離設為1至2cm程度(適當的範圍為1mm至2cm)時},由於可將離子、臭氧風產生裝置放入衣服的口袋或背包並進行搬運,故使用者可於需要時(例如,去除附著於本身的身體與衣服之臭味源時)或進可能使之接近殺菌、除臭對象物,而成為可容易使用離子、臭氧風產生裝置。此外,於將離子、臭氧風產生裝置予以小型化時,在飲食店與遊樂場或柏青哥等些遊樂設施係於設施設備常備(例如,飲食店之櫃檯、遊樂設施之遊戲機設備間的間隙),而將來自鄰人的臭味源(例如,煙草之副流煙)予以隔開而提供每個顧客之個人的空氣清淨空間等些用法亦變得容易。 Also, in the small size of the ion and ozone wind generating device For example, the size of the ion and ozone wind generating device is set to be 7 cm in length × 7 cm in width × 3 cm in height, that is, miniaturized to a degree that can be easily grasped by one hand, and the electrode composition is performed. When space is saved {for example, a counter electrode having a diameter of about 1 cm (appropriate range of 5 mm to 5 cm) is disposed as shown in Fig. 15, and the needle electrode and the counter electrode are arranged. When the distance is set to about 1 to 2 cm (appropriate range is 1 mm to 2 cm), since the ion and ozone wind generating device can be placed in a pocket or a backpack of a garment, the user can take it when needed (for example, When the odor source attached to the body and clothes of the body is removed, or the sterilizing or deodorizing object is brought close to it, the ion and ozone wind generating device can be easily used. In addition, when the ion and ozone wind generating devices are miniaturized, some amusement facilities such as restaurants, amusement parks, and Pachinko are kept in the facility (for example, between the counters of the restaurant and the game equipment of the amusement facilities). It is also easy to separate the source of the odor from the neighbor (for example, the sidestream of tobacco) to provide the air clean space of each individual customer.

[實施例] [Examples]

其次,利用實施例及比較例更具體地說明本發明,惟本發明不受到上述例任何限定。 Next, the present invention will be specifically described by way of Examples and Comparative Examples, but the present invention is not limited by the above examples.

≪第1實施例≫ ≪First Embodiment≫ (第1實施例之測量方法及測量條件) (Measurement method and measurement condition of the first embodiment)

關於第1實施例,使用具備第24圖所示之形狀的電極對之離子風產生裝置生離子風,且於對向電極330(受電部331)之外周,等間隔地在從A點到H點為止之8處所測量離子風的風速。再者,將產生離子風時的放電電極與對向電極之電位差(施加電壓)設為7000[V](電流:500μA),且作為測量環境而言,將溫度設為攝氏25度,且將濕度設為60%。然後,將放電電極320(放電部321)之內徑設為3cm,且將對向電極330(受電部331)的內徑設為5cm。 In the first embodiment, the ion wind generating device using the electrode pair having the shape shown in Fig. 24 generates the ion wind, and the counter electrode 330 (power receiving unit 331) is equidistantly spaced from the point A to the H. The wind speed of the ion wind measured at 8 points. In addition, the potential difference (applied voltage) between the discharge electrode and the counter electrode when the ion wind is generated is 7000 [V] (current: 500 μA), and as a measurement environment, the temperature is set to 25 degrees Celsius, and The humidity is set to 60%. Then, the inner diameter of the discharge electrode 320 (discharge portion 321) was set to 3 cm, and the inner diameter of the counter electrode 330 (power receiving portion 331) was set to 5 cm.

在所測量之離子風的風速為1.5m/s以上時 將風速判定設為○記號,未達1.5m/s時將風速判定設為×記號,且將測量結果表示於第1表。 When the measured wind speed of the ion wind is 1.5 m/s or more The wind speed determination is set to ○ mark, and when it is less than 1.5 m/s, the wind speed determination is set to × mark, and the measurement result is shown in the first table.

(第1實施例之側量結果) (side amount result of the first embodiment)

如第1表所示,風速在所有的測量場所為1.5m/s以上故風速判定皆為○記號。由此來看,使用具備第24圖所示之形狀的電極對之離子、臭氧風產生裝置時,遍及360度全方向,產生均等且足夠的風量之離子風。 As shown in the first table, the wind speed is 1.5 m/s or more at all measurement points, so the wind speed is judged as ○ mark. From this point of view, when the ion or ozone wind generating device having the electrode pair having the shape shown in Fig. 24 is used, an ion wind having an equal and sufficient air volume is generated in all directions of 360 degrees.

≪第2實施例≫ ≪Second embodiment≫ (第2實施例之測量方法及測量條件) (Measurement method and measurement condition of the second embodiment)

在第2實施例中,使用具備如第32圖所示之形狀的電極對之離子風產生裝置使離子風產生,在從對向電極330(受電部331)之一方的端部到另一方面的端部為止之間,設置成為從I點到K點為止之等間隔的3點,在該3 處所測量離子風的風速。此外,將使離子風產生時之放電電極與對向電極之電位差(外加電壓)設為7000〔V](電流:500μA),而作為測量環境而言,將溫度設為攝氏25度,將濕度設為60%。然後,放電電極320(放電部321)係設為內徑為3cm之圓的四分之一的圓弧,而對向電極330(受電部331)係設為內徑為5cm之圓的四分之一的圓弧。 In the second embodiment, an ion wind generating device is provided using an electrode pair having an electrode pair having the shape shown in Fig. 32, and the end portion from the counter electrode 330 (power receiving portion 331) is on the other side. Between the ends of the ends, three points are formed at equal intervals from point I to point K. The wind speed of the ion wind is measured at the premises. In addition, the potential difference (applied voltage) between the discharge electrode and the counter electrode when the ion wind is generated is set to 7000 [V] (current: 500 μA), and as a measurement environment, the temperature is set to 25 degrees Celsius, and the humidity is set. Set to 60%. Then, the discharge electrode 320 (discharge portion 321) is a quarter arc of a circle having an inner diameter of 3 cm, and the counter electrode 330 (power receiving portion 331) is a quarter of a circle having an inner diameter of 5 cm. One of the arcs.

在所測量之離子風的風速為1.5m/s以上時 設為○記號,在未達1.5m/s時設為×記號,而將測量結果表示於第2表。 When the measured wind speed of the ion wind is 1.5 m/s or more The ○ mark is set, and when it is less than 1.5 m/s, the × mark is set, and the measurement result is shown in the second table.

≪第1比較例≫ ≪The first comparative example≫ (第1比較例之測量方法及測量條件) (Measurement method and measurement condition of the first comparative example)

關於第1比較例,使用具備第5圖所示之形狀的電極對之離子風產生裝置產生離子風,且在對向電極130的周圍360度以每45度從L點到S點為止之8處所來測量離子風的風速。此外,將使離子風產生時之放電電極(針狀電極)與對向電極之電位差(外加電壓)設為7000[V](電流:500μA),而作為測量環境而言,將溫度設為攝氏25度,且將濕 度設為60%。然後,將對向電極130的內徑設為3cm(圓形環狀電極131)、5cm(外側圓形環狀電極132)。 In the first comparative example, the ion wind generation device using the electrode pair having the shape shown in Fig. 5 generates the ion wind, and the angle of 360 degrees from the point L to the point S every 45 degrees around the counter electrode 130 The location measures the wind speed of the ion wind. In addition, the potential difference (applied voltage) between the discharge electrode (needle electrode) and the counter electrode when the ion wind is generated is set to 7000 [V] (current: 500 μA), and as the measurement environment, the temperature is set to Celsius. 25 degrees and will be wet The degree is set to 60%. Then, the inner diameter of the counter electrode 130 was set to 3 cm (circular annular electrode 131) and 5 cm (outer circular annular electrode 132).

在所測量之離子風的風速為1.5m/s以上時 將風速判定設為○記號,在未達1.5m/s時將風速判定設為×記號,而將測量結果顯示於第3表。 When the measured wind speed of the ion wind is 1.5 m/s or more The wind speed determination is set to the ○ mark, and when the speed is less than 1.5 m/s, the wind speed determination is set to the × mark, and the measurement result is displayed on the third table.

(第1比較例之測量結果) (Measurement result of the first comparative example)

如第3表所示,風速在所有的測量場所未達1.5m/s,故風速判定皆成為×記號。據此,使用具備如第5圖所示之形狀的電極對之離子、臭氧風產生裝置時,於電極對的周圍不產生離子風(或,即使產生亦微弱)。 As shown in Table 3, the wind speed is less than 1.5 m/s at all measurement locations, so the wind speed determination is x mark. According to this, when the ion or ozone wind generating device having the electrode pair having the shape shown in Fig. 5 is used, no ion wind is generated around the electrode pair (or even if it is generated).

〔參考實施例及參考比較例〕 [Reference Example and Reference Comparative Example]

以下,使用參考例及參考比較例,就本發明之離子風產生裝置加以說明,惟不限定於此。 Hereinafter, the ion wind generating device of the present invention will be described using a reference example and a reference comparative example, but is not limited thereto.

(參考實施例及參考比較例之測量方法及測量條件) (Measurement method and measurement conditions of the reference embodiment and the reference comparative example)

就參考第1實施例、參考第2實施例、參考第1比較例、參考第2比較例、參考第3比較例,使用具備第37圖至第41圖所示之對向電極的離子風產生裝置產生離子風,且利用第42圖所示之方法來測量離子風的風速。各裝置的電極大小係如下列第4表所示。此外,將使離子風產生時之針狀電極與對向電極之電位差(外加電壓)設為7000[V](電流:500μA),且將載置有風速計之台的高度設為39mm。此外,作為測量環境而言,將溫度設為攝氏25度,且將濕度設為60%。 With reference to the first embodiment, the second embodiment, the first comparative example, the second comparative example, and the third comparative example, the ion wind generation including the counter electrode shown in FIGS. 37 to 41 is used. The device generates an ion wind and measures the wind speed of the ion wind using the method shown in FIG. The electrode size of each device is shown in Table 4 below. Further, the potential difference (applied voltage) between the needle electrode and the counter electrode when the ion wind was generated was 7000 [V] (current: 500 μA), and the height of the stage on which the anemometer was placed was set to 39 mm. Further, as a measurement environment, the temperature was set to 25 degrees Celsius, and the humidity was set to 60%.

(參考第1實施例) (Refer to the first embodiment)

如第37圖所示,參考第1實施例的構造具有主電極對以及以包圍該主電極對之方式定位之複數組的副電極對,且將各個電極對設為平面狀且環狀 As shown in Fig. 37, the configuration of the first embodiment has a pair of main electrodes and a pair of sub-electrodes aligned in a manner of surrounding the pair of main electrodes, and the respective electrode pairs are planar and annular.

(參考第2實施例) (refer to the second embodiment)

如第38圖所示,參考第2實施例的構造係除了設為各對向電極具有主環狀對向電極與副環狀對向電極之外,具有與第1實施例相同的構造。 As shown in Fig. 38, the structure of the second embodiment has the same structure as that of the first embodiment except that each of the counter electrodes has a main annular counter electrode and a sub-annular counter electrode.

(參考第1比較例) (Refer to the first comparative example)

如第39圖所示,參考第1比較例的構造係設置有以包圍一組電極對的方式鄰接之複數組的電極對。此外,對向電極為圓筒狀。 As shown in Fig. 39, the structure of the first comparative example is provided with an electrode pair of a complex array adjacent to each other so as to surround a group of electrode pairs. Further, the counter electrode is cylindrical.

(參考第2比較例) (Refer to the second comparative example)

第40圖所示,參考第2比較例例的構造係設置有串聯地配置之複數組的電極對。再者,對向電極為圓筒狀。 As shown in Fig. 40, the structure of the second comparative example is provided with electrode pairs of a plurality of arrays arranged in series. Further, the counter electrode is cylindrical.

(參考第3比較例) (Refer to the third comparative example)

如第41圖所示,參考第3比較例的構造係設置有串聯地配置之複數組的電極對。再者,各個電極對為平面狀且環狀。 As shown in Fig. 41, the structure of the third comparative example is provided with electrode pairs of a plurality of arrays arranged in series. Furthermore, each electrode pair is planar and annular.

(參考實施例及參考比較例之測量結果) (Measurement results of reference examples and reference comparative examples)

將上述參考實施例及參考比較例的測量結果表示於下列第5表。如第5表所示,可知在參考第1實施例之離子風產生裝置所產生之離子風的風速,比在參考第1比較例至參考第3比較例的離子風產生裝置所產生的離子風之風速更顯著地變大。 The measurement results of the above reference examples and reference comparative examples are shown in the following Table 5. As shown in the fifth table, it is understood that the wind speed of the ion wind generated by referring to the ion wind generating device of the first embodiment is higher than that of the ion wind generating device of the first comparative example to the third comparative example. The wind speed is more pronounced.

此外,雖於以下具體地敘述,惟從本測量 的結果,亦顯示如本專利申請案發明,(A)具有主電極對與以包圍該主電極對之方式定位之複數組的副電極對,並且,(B)藉由將各個電極對設為平面狀且環狀等,才可達成顯著地使風力增大的效果,而若缺少(A)、(B)之任一的構成,則風力的增幅效果亦小。 In addition, although specifically described below, only from this measurement As a result, as also shown in the patent application of the present application, (A) has a pair of main electrodes and a pair of sub-electrodes positioned in a manner surrounding the pair of main electrodes, and (B) by setting each electrode pair In the case of a flat shape, a ring shape, or the like, an effect of significantly increasing the wind force can be achieved, and if the configuration of either (A) or (B) is lacking, the effect of increasing the wind power is small.

具體而言,將參考第1比較例與參考第2 比較例予以比較時,於對向電極為圓筒狀時,即使將複數個電極對之配置從串聯型配置變更為具有以包圍主電極對之方式定位之複數組的副電極對之配置,風速亦僅變大0.1m/s,而可知風力的增幅效果小。另一方面,將參考第1實施例與參考第3比較例予以比較時,將各個電極對設為平面狀且環狀等時,在將複數個電極對之配置從串聯型配置變更為具有以包圍主電極對之方式定位之複數組的副電極對之配置,風速係大幅變大0.3m/s,而可知風力的增幅效果大。 Specifically, reference will be made to the first comparative example and the reference second When the comparative example is compared, when the counter electrode is cylindrical, the arrangement of the plurality of electrode pairs is changed from the tandem arrangement to the arrangement of the sub-electrode pairs having the complex array positioned so as to surround the main electrode pair, and the wind speed is set. It is only increased by 0.1 m/s, and it is known that the effect of increasing the wind power is small. On the other hand, when the first embodiment is compared with the reference third comparative example, when the respective electrode pairs are formed in a planar shape and a ring shape, the arrangement of the plurality of electrode pairs is changed from the tandem type arrangement to the The arrangement of the sub-electrode pairs of the complex array positioned around the main electrode pair greatly increases the wind speed by 0.3 m/s, and it is known that the effect of increasing the wind power is large.

再者,將參考第2比較例與參考第3比較例 予以比較時,複數個電極對的配置為串聯型配置時,即使將對向電極的形狀從圓筒狀變更為平面狀且環狀等,風速亦僅變大0.1m/s,而可知風力的增幅效果小。另一方面,將第1實施例與第1比較例予以比較時,複數個電極對的配置為具有以包圍主電極對之方式定位之複數組副電極對的配置時,將對向電極的形狀從圓筒狀變更為平面狀且環狀等時,風速大幅增大0.3m/s,可知風力的增幅效果大。 Furthermore, reference will be made to the second comparative example and the reference third comparative example. When the arrangement of the plurality of electrode pairs is a tandem type arrangement, even if the shape of the counter electrode is changed from a cylindrical shape to a planar shape and a ring shape, the wind speed is increased by only 0.1 m/s, and the wind power is known. The increase effect is small. On the other hand, when the first embodiment is compared with the first comparative example, the arrangement of the counter electrode is performed when the plurality of electrode pairs are arranged to have a pair of sub-electrode pairs positioned so as to surround the main electrode pair. When the shape is changed from a cylindrical shape to a flat shape and a ring shape, the wind speed is greatly increased by 0.3 m/s, and it is understood that the effect of increasing the wind power is large.

如以上,本專利申請案發明的參考第1實施 例之離子、臭氧風產生裝置,與參考第1比較例至參考第3比較例之裝置的情況比較,可知產生之風力顯著變大。 再者,可知設置以包圍主電極對之方式定位之複數組的副電極對的配置之離子風的增幅效果,係藉由將各個電極對設為平面狀且環狀等成為顯著。 As described above, the reference to the first embodiment of the present patent application As compared with the case of the apparatus of the first comparative example to the third comparative example, the ion and ozone wind generating apparatus of the example showed that the generated wind power was remarkably large. Further, it is understood that the effect of increasing the ion wind of the arrangement of the pair of sub-electrodes in the complex array positioned so as to surround the pair of main electrodes is remarkable by making each electrode pair planar, annular, or the like.

並且,藉由從參考第1實施例與參考第2 實施例的比較,可知藉由各對向電極具有主環狀對向電極與副環狀對向電極,而達到更顯著的風力之增幅效果。 And by referring to the first embodiment and the reference second Comparing the examples, it can be seen that each of the counter electrodes has a main annular counter electrode and a sub-annular counter electrode, and a more remarkable wind power increasing effect is achieved.

(對向電極之替代例) (an alternative to the counter electrode)

此外,在之前的說明中作為概念圖所表示之對向電極(例如第15圖)之概念,係由將第1對向電極130a及第2對向電極130b至130g之各者以成為平面狀且環狀之方式形成為各別的導電構件,且將該各別的導電構件以相互鄰接之方式予以接合(例如,進行焊接)來進行加工(以下,將此加工概念稱為接合加工)。另一方面,在實施例中作為構 造圖所示之對向電極(例如,第24圖至25)之概念,係藉由在一張平板狀的導電構件貫穿環狀的貫穿孔來進行加工(以下,將此加工概念稱為穿孔加工)。以此方式,會由於加工方法的差異,而如在本例所示,對向電極之整個構造可成為不同的構造。但是,使用第5圖且如前述,考慮產生電暈放電之根本的機制時,在針狀電極與對向電極之距離最接近之對向電極的部位(亦即,環狀的對向電極之內周邊緣部)上產生電暈放電之比例變得最高,故不論是以接合加工及穿孔加工的任一者所加工之對向電極中,在環狀的對向電極之內周邊緣部皆會產生良好的電暈放電,以此點而言沒有不同。接著,實際上於製造對向電極時,雖比起接合加工,穿孔加工較容易形成對向電極,惟此係僅是設想平板狀者作為對向電極之情形(假設,設想圓筒狀者作為對向電極時,透過穿孔加工形成對向電極時容易造成對向電極本身成為無謂地大型化,並且,穿孔加工本身亦變得困難)。亦即,可說實際上於製造對向電極時,將對向電極設為平板狀比將對向電極設為圓筒狀更有利。 In addition, in the above description, the concept of the counter electrode (for example, Fig. 15) shown as a conceptual diagram is such that each of the first counter electrode 130a and the second counter electrode 130b to 130g is planar. Each of the conductive members is formed in a ring shape, and the respective conductive members are joined to each other (for example, by welding) (hereinafter, this processing concept is referred to as bonding processing). On the other hand, in the embodiment as a structure The concept of the counter electrode (for example, Figs. 24 to 25) shown in the drawing is processed by penetrating a circular conductive member through a circular through hole (hereinafter, this processing concept is called perforation). machining). In this way, due to the difference in processing methods, as shown in this example, the entire configuration of the counter electrode can be made different. However, using Fig. 5 and as described above, in consideration of the fundamental mechanism for generating corona discharge, the portion of the counter electrode which is closest to the distance between the needle electrode and the counter electrode (i.e., the annular counter electrode) The ratio of the corona discharge generated on the inner peripheral edge portion is the highest. Therefore, in the counter electrode processed by either the joining process and the piercing process, the inner peripheral edge portion of the annular counter electrode is It will produce a good corona discharge, which is no different in this point. Then, in the case of actually manufacturing the counter electrode, it is easier to form the counter electrode than the bonding process, but it is only a case where the flat plate is assumed to be the counter electrode (assuming that the cylinder is assumed as In the case of the counter electrode, when the counter electrode is formed by the punching process, the counter electrode itself is likely to become unnecessarily large, and the punching process itself becomes difficult. In other words, it can be said that when the counter electrode is actually manufactured, it is more advantageous to form the counter electrode in a flat shape than to make the counter electrode have a cylindrical shape.

但是,考慮根據電暈放電之產生離子風的 機制時,係設想會有比起透過接合加工形成對向電極之情況,透過穿孔加工形成對向電極之情況所產生之離子風會降低之事態。在此,作為產生離子風的機制,一般而言,雖設為於電暈放電時,從針狀電極釋出之離子朝對向電極游動之間反覆與空氣分子的衝撞,藉此從針狀電極朝對向電極產生之空氣流,惟在專利申請案發明中,亦著眼於透 過該空氣流產生之負壓及朝該負壓產生的空間之外氣的吸氣流之離子風的增大效果。例如,如從第5圖所示之離子風的產生處所可清楚知道,於環狀的對向電極之內周邊緣部上產生電暈放電時,離子風雖從該內周邊緣部附近被推出到前面方向,惟此時,於對向電極之環狀部背側(不與針狀電極相對向之側的面)產生負壓。然後,朝產生該負壓之空間,尤其是圍繞對向電極的外周之外氣會被吸引,且透過該被吸引之外氣而使被推出到前面方向之離子風的風力增大(從此點而言,亦可說將對向電極設為平板狀比將對向電極設為圓筒狀更有利)。 However, consider the generation of ion wind according to corona discharge In the case of the mechanism, it is assumed that there is a case where the counter electrode is formed by the joining process, and the ion wind generated by the counter electrode forming the counter electrode is lowered. Here, as a mechanism for generating the ion wind, generally, in the case of corona discharge, the ions released from the needle electrode collide with the air molecules in the collision between the counter electrodes, thereby taking the needle from the needle. The air flow generated by the electrode toward the opposite electrode, but in the invention of the patent application, it is also focused on The negative pressure generated by the air flow and the effect of increasing the ion wind of the airflow outside the space generated by the negative pressure. For example, as is apparent from the generation of the ion wind shown in Fig. 5, when a corona discharge is generated on the inner peripheral edge portion of the annular counter electrode, the ion wind is pushed out from the vicinity of the inner peripheral edge portion. In the front direction, at this time, a negative pressure is generated on the back side of the annular portion of the counter electrode (the surface on the side opposite to the needle electrode). Then, the air is generated toward the space where the negative pressure is generated, in particular, the outer circumference of the counter electrode, and the wind of the ion wind pushed out to the front direction is increased by the outside air being sucked (from this point) In other words, it can be said that it is more advantageous to have the counter electrode in a flat shape than to make the counter electrode a cylindrical shape.

根據此種離子風產生之機制的理解,就透 過穿孔加工形成對向電極的情況之較佳態樣加以詳述。首先,第43圖(左)係透過穿孔加工形成在第15圖(b)所示之對向電極的情況之概念圖,而如同圖所示,藉由針對一張平板狀的導電構件130,將相當於第1對向電極130a以及第2對向電極130b至130g之環狀的貫穿孔予以貫穿而形成整個對向電極。在此,在本例中,鑑於在貫穿環狀的貫穿孔時可能會產生之誤差,而將各個第1對向電極130a及第2對向電極130b至130g以至少數mm(1至3mm)程度相隔之方式予以配置。再者,在本例中,藉由將一張平板狀的導電構件130設為幾近方形,而例如,以可在該大致方形的四角落設置用以軸支導電構件130之孔(用以組裝如第24圖、第42圖所示之實驗裝置之孔)之方式予以構成。 According to the understanding of the mechanism of ion wind generation, A preferred aspect of the case where the counter electrode is formed to form the counter electrode is described in detail. First, Fig. 43 (left) is a conceptual diagram of a case where the counter electrode shown in Fig. 15(b) is formed by punching, and as shown in the figure, by a sheet-like conductive member 130, The through-holes corresponding to the annular shape of the first counter electrode 130a and the second counter electrodes 130b to 130g are penetrated to form the entire counter electrode. Here, in this example, each of the first counter electrode 130a and the second counter electrode 130b to 130g is at least several mm (1 to 3 mm) in view of an error that may occur when the through hole is formed through the annular shape. Configure them separately. Furthermore, in this example, by forming a flat conductive member 130 to be nearly square, for example, a hole for supporting the conductive member 130 can be disposed at the substantially square corners (for The holes of the experimental apparatus shown in Figs. 24 and 42 are assembled.

在將與以此方式形成之第1對向電極130a 及第2對向電極130b至130g之各個對向電極相對的屬於放電部之針狀電極予以設置,且在該電極間使電位差產生時,在第1對向電極130a及第2對向電極130b至130g之內周邊緣部主要產生電暈放電(在本例中,雖成為2重環狀構造,惟在內側的環狀構造之內周邊緣部以及外側的環狀構造之內周邊緣部的雙方產生電暈放電)。然後,離子風從該內周邊緣部附近被推出到前面方向時,於對向電極之環狀部背側(不與針狀電極相對向之側的面)產生負壓(在此,與第16圖所示之作用相同)。但是,設想會有朝產生該負壓的空間,即便欲將尤其是屬於圍繞對向電極的周圍S之外氣之存在於對向電極與針狀電極之間的外氣予以吸引,亦會被導電構件130所遮蔽之事態。為此,如第43圖(右)所示,最好以該應被吸引之外氣可通過導電構件130之方式,設置吸引孔130S。此外,吸引孔130S與第2對向電極130b至130g的外周間之距離隔離太遠時,起因於該被吸引之外氣與產生該負壓的空間之距離變大且離子風的產生方向與該應被吸引之外氣的移動方向之偏差變大,而會有可能使得離子風之風力的增大效果降低之虞。因此,吸引孔130S與第2對向電極130b至130g的外周間之距離最好在第2對向電極130b至130g的直徑以下(或直徑之1/n以下;n為自然數)。 In the first counter electrode 130a to be formed in this manner And the needle electrodes belonging to the discharge portion facing the respective counter electrodes of the second counter electrodes 130b to 130g are provided, and when the potential difference is generated between the electrodes, the first counter electrode 130a and the second counter electrode 130b are formed. In the inner peripheral edge portion of 130 g, a corona discharge is mainly generated (in this example, the inner peripheral edge portion of the inner annular structure and the inner peripheral edge portion of the outer annular structure are formed in a double annular structure. Both sides produce corona discharge). Then, when the ion wind is pushed out from the vicinity of the inner peripheral edge portion to the front direction, a negative pressure is generated on the back side of the annular portion of the counter electrode (the surface on the side opposite to the needle electrode) (here, The effect shown in Figure 16 is the same). However, it is envisaged that there will be a space for generating the negative pressure, and even if it is intended to attract the external air existing between the counter electrode and the needle electrode, especially the gas surrounding the surrounding S of the counter electrode, The situation in which the conductive member 130 is shielded. For this reason, as shown in Fig. 43 (right), it is preferable to provide the suction hole 130S in such a manner that the gas to be attracted can pass through the conductive member 130. Further, when the distance between the suction hole 130S and the outer circumference of the second counter electrode 130b to 130g is too far apart, the distance between the gas to be attracted and the space where the negative pressure is generated becomes large and the direction of generation of the ion wind is The deviation of the moving direction of the gas that should be attracted is increased, and there is a possibility that the effect of increasing the wind of the ion wind is lowered. Therefore, the distance between the outer periphery of the suction hole 130S and the second counter electrode 130b to 130g is preferably equal to or smaller than the diameter of the second counter electrode 130b to 130g (or 1/n or less of the diameter; n is a natural number).

由以上來看,透過穿孔加工形成對向電極 時,藉由以包圍第2對向電極130b至130g的外側(在某第2對向電極上不與其他對向電極鄰接之側)之方式,設置吸 引孔130S,可期待根據本專利申請案發明所著眼之離子風產生的機制之圍繞對向電極的外周之外氣的吸引效果、以及透過該吸引效果而使從對向電極被推出到前面方向之離子風的風力之增大效果。此外,不僅離子風的風力之增大效果,由於含有臭氧之離子風被外氣所稀釋,故亦會有對人體造成不良影響之危險性亦降低之優點。亦即,不另設置用以使離子風的風力增大之裝置與用以去除臭氧之裝置,而藉由本變更例可達成提供可適當地使(良好的)離子風產生之對向電極,並且實際上於製造對向電極時亦(尤其是藉由將對向電極設為平板狀)可容易地形成對向電極。 From the above point of view, the counter electrode is formed by perforation processing. When the outer side of the second counter electrode 130b to 130g is surrounded (the side opposite to the other counter electrode on the second counter electrode) is provided, the suction is provided. The pilot hole 130S can be expected to attract the gas outside the outer circumference of the counter electrode according to the mechanism of the ion wind generated by the invention of the present patent application, and to push the counter electrode out to the front direction through the suction effect. The effect of the wind of the ion wind increases. In addition, not only the effect of increasing the wind force of the ion wind, but also the ozone-containing ion wind is diluted by the outside air, so that the risk of adversely affecting the human body is also reduced. That is, a device for increasing the wind force of the ion wind and a device for removing ozone are not provided, and by this modification, it is possible to provide a counter electrode which can appropriately generate (good) ion wind, and In fact, the counter electrode can be easily formed even when the counter electrode is manufactured (especially by setting the counter electrode to a flat shape).

此外,在本例中,雖僅就將吸引孔130S設 為圓周狀的孔之點予以例示,惟並不限定於此。亦即,透過接合加工而形成之對向電極的形狀更佳,故可舉出以接近該形狀作為宗旨之種種形成方法。例如,在第2對向電極130b至130g中,亦可依沿著不與其他對向電極鄰接之側的圓弧而彎曲之形態,設置吸引孔130S。此外,亦可依包圍第2對向電極130b至130g之方式而環繞設置,例如,亦可依設置複數個沿著該圓弧之大致三角形的孔的方式來構成。此外,若無需將導電構件130設為方形,則亦可將導電構件130本身設為圓形(例如,去除比第30圖之吸引孔130S之更外側部分),或亦可採用如從該圓形更去除不需要的部分(在第2對向電極130b至130g中,以沿著不與其他對向電極鄰接之側的圓弧之方式予以去除)之成形方法。但是,在設為如第30圖(右)所示之形狀時,與透 過接合加工所形成之對向電極的形狀比較,在對向電極之環狀部背側(不與針狀電極相對向之側的面)上可使朝向產生負壓之空間的外氣(尤其是屬於圍繞對向電極的周圍S之外氣之存在於對向電極與針狀電極之間的外氣)之吸引道變窄,故亦可期待強化該外氣的吸引力(吸引之外氣的風力增加)之效果。因此,透過穿孔加工形成對向電極時,最好是考量此種效果後,以成為最適當的形狀之方式來進行設計。 In addition, in this example, only the suction hole 130S is provided. The point of the circumferential hole is exemplified, but is not limited thereto. That is, the shape of the counter electrode formed by the joining process is more preferable, and various methods of forming the object close to the shape are exemplified. For example, in the second counter electrode 130b to 130g, the suction hole 130S may be provided in a shape that is curved along an arc that is not adjacent to the other counter electrode. Further, it may be arranged to surround the second counter electrode 130b to 130g. For example, it may be configured to provide a plurality of substantially triangular holes along the arc. In addition, if it is not necessary to form the conductive member 130 as a square, the conductive member 130 itself may be circular (for example, the outer portion of the suction hole 130S is removed), or may be used as the circle The shape is further removed by a method of forming an unnecessary portion (the second counter electrode 130b to 130g is removed along an arc which is not adjacent to the other counter electrode). However, when it is set to the shape shown in Fig. 30 (right), The shape of the counter electrode formed by the over-joining process is compared with the outside of the annular portion of the counter electrode (the surface on the side opposite to the needle-shaped electrode). It is a narrow attraction channel that belongs to the outside air surrounding the surrounding electrode and the gas existing between the counter electrode and the needle electrode. Therefore, it is also expected to enhance the attraction of the outside air (attracting the outside air) The effect of the wind increases). Therefore, when the counter electrode is formed by the punching process, it is preferable to design the method so as to have the most appropriate shape.

再者,如第44圖(a)及(b)所示,從表面上來 看雖可將其視為具有複數組主電極對,且以包圍此主電極對之方式配置有副電極對之構成{可將在同圖(b)以粗線圖示之複數個環狀對向電極,視為主電極對之環狀對向電極(再者,將配置在外周之以細線所示之環狀對向電極設為副電極對之環狀對向電極)而得到之構成},而有時有作為具有一組主電極對,且以包含主電極對之方式配置有副電極對之集合體而予以構成之情形。於此補充說明者,亦即,如同圖下段範圍內之「主電極對之環狀對向電極概念圖」所示,在各別以粗線表示之環狀對向電極內,將位於中央之環狀對向電極視為主電極對之環狀對向電極,且將以該周圍的粗線所表示之環狀對向電極視為副電極對之環狀對向電極,並可將其理解作為其集合體。因此,即便是沿著如第44圖(b)所示之副電極對的外周設置吸引孔130S時,亦屬於具有一組主電極對,且沿著以包圍該主電極對之方式配置有副電極對者之外周設置有吸引孔130S之概念的 範圍內。 Furthermore, as shown in Fig. 44 (a) and (b), from the surface It can be seen that it can be regarded as having a complex array main electrode pair, and a sub-electrode pair is disposed so as to surround the main electrode pair. {A plurality of ring pairs which can be shown by thick lines in the same figure (b) The electrode is regarded as a ring-shaped counter electrode of the main electrode pair (further, the annular counter electrode which is disposed on the outer circumference by the thin line is a ring-shaped counter electrode of the sub-electrode pair). In some cases, there is a case where a set of main electrode pairs is provided and an assembly of sub-electrode pairs is disposed so as to include a main electrode pair. In addition, as shown in the figure below, the concept diagram of the annular counter electrode of the main electrode pair is shown in the middle of the annular counter electrode, which is indicated by a thick line. The annular counter electrode is regarded as a ring-shaped counter electrode of the main electrode pair, and the annular counter electrode represented by the thick line around the ring is regarded as a ring-shaped counter electrode of the sub-electrode pair, and can be understood As its collection. Therefore, even if the suction hole 130S is provided along the outer circumference of the pair of secondary electrodes as shown in Fig. 44(b), it also has a pair of main electrode pairs, and is disposed along the main electrode pair so as to surround the main electrode pair. The periphery of the electrode pair is provided with the concept of the attraction hole 130S Within the scope.

100-2‧‧‧離子、臭氧風產生裝置 100-2‧‧‧Ion, ozone wind generator

310‧‧‧電極對 310‧‧‧electrode pair

320‧‧‧放電電極 320‧‧‧Discharge electrode

321‧‧‧放電部 321‧‧‧Discharge Department

322‧‧‧放電點 322‧‧‧Discharge point

330‧‧‧對向電極 330‧‧‧ opposite electrode

331‧‧‧受電部 331‧‧‧Power Management Department

332‧‧‧受電點 332‧‧‧Power receiving point

Claims (5)

一種離子、臭氧風產生裝置,係構成為於放電點與受電點之間使電位差產生而產生電暈放電,包括:藉由將放電點連續配置在成為放電基準之基準線上而形成之線狀且環狀之放電部,以及藉由將受電點連續配置在成為受電基準之基準線上而形成之線狀且環狀之受電部,放電部與受電部係位於大致相同平面上且放電部配置於受電部的內周側,或是放電部與受電部係位於大致相同平面上且受電部配置於放電部的內周側,前述經配置之放電線與受電線係被隔離,且構成為,藉由從放電部朝受電部產生電暈放電,而至少朝受電部中之不與放電部相對向之側的開放部產生離子風。 An ion and ozone wind generating device configured to generate a corona discharge by causing a potential difference between a discharge point and a power receiving point, and comprising: forming a discharge line continuously on a reference line to be a discharge reference line The annular discharge portion and the linear and annular power receiving portion formed by continuously arranging the power receiving points on the reference line serving as the power receiving reference, the discharge portion and the power receiving portion are disposed on substantially the same plane, and the discharge portion is disposed on the power receiving portion. The inner peripheral side of the portion, or the discharge portion and the power receiving portion are located on substantially the same plane, and the power receiving portion is disposed on the inner peripheral side of the discharge portion, and the arranged discharge line is isolated from the power receiving line, and is configured by The corona discharge is generated from the discharge portion toward the power receiving portion, and ion wind is generated at least toward the open portion of the power receiving portion that is not opposed to the discharge portion. 如申請專利範圍第1項所述之離子、臭氧風產生裝置,其中,針對一條放電部具有複數條受電部,而該複數條受電部係配置在與配置有該一條放電部的平面為相同之平面或與該相同平面分離且平行之複數個平面之任一平面上,並且,該複數條受電部之各者配置在相互不同之平面上。 The ion and ozone wind generating device according to claim 1, wherein the one discharge portion has a plurality of power receiving portions, and the plurality of power receiving portions are disposed in the same plane as the one in which the one discharge portion is disposed. The plane or any of a plurality of planes separated and parallel to the same plane, and each of the plurality of power receiving sections is disposed on a mutually different plane. 如申請專利範圍第2項所述之離子、臭氧風產生裝置,其中, 前述複數條受電部成為主受電部及副受電部之任一者,從前述一條放電部中之某放電點到屬於主受電部中之受電點之與該某放電點之距離為最小之受電點之距離,比從該某放電點到屬於副受電部中之受電點之與該某放電點之距離為最小之受電點之距離更短。 The ion and ozone wind generating device according to claim 2, wherein The plurality of power receiving units are one of the main power receiving unit and the sub power receiving unit, and the power receiving point from the one of the one of the discharge portions to the power receiving point of the main power receiving unit and the distance from the certain discharging point is the smallest. The distance is shorter than the distance from the certain discharge point to the power receiving point of the power receiving point belonging to the sub power receiving unit which is the smallest distance from the certain discharging point. 如申請專利範圍第2項所述之離子、臭氧風產生裝置,其中,從前述一條放電部中之某放電點到屬於某受電部中之受電點之與該某放電點之距離為最小之受電點之距離,與從該某放電點到屬於與該某受電部不同的受電部中之受電點之與該某放電點之距離為最小之受電點之距離係大致相同。 The ion and ozone wind generating device according to the second aspect of the invention, wherein the power from a discharge point in the one of the discharge portions to the power receiving point in the power receiving portion is the smallest distance from the discharge point The distance between the points is substantially the same as the distance from the certain discharge point to the power receiving point of the power receiving portion belonging to the power receiving unit different from the power receiving unit, which is the smallest distance from the certain discharging point. 如申請專利範圍第1至4項中任一項所述之離子、臭氧風產生裝置,其中,前述放電部在以剖面觀看時,係外周朝向受電部形成銳角之形狀。 The ion or ozone wind generating device according to any one of the first to fourth aspect, wherein the discharge portion has a shape in which an outer circumference forms an acute angle toward the power receiving portion when viewed in a cross section.
TW103142974A 2014-05-12 2014-12-10 Ion or ozone wind generating device and method TWI543483B (en)

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