TW202133216A - Barrier discharge lamp, barrier discharge lamp unit and liquid treatment device which has a luminous tube containing silicon dioxide material - Google Patents
Barrier discharge lamp, barrier discharge lamp unit and liquid treatment device which has a luminous tube containing silicon dioxide material Download PDFInfo
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- TW202133216A TW202133216A TW109127595A TW109127595A TW202133216A TW 202133216 A TW202133216 A TW 202133216A TW 109127595 A TW109127595 A TW 109127595A TW 109127595 A TW109127595 A TW 109127595A TW 202133216 A TW202133216 A TW 202133216A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
- H01J65/04—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels
- H01J65/042—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field
- H01J65/046—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field the field being produced by using capacitive means around the vessel
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/04—Electrodes; Screens; Shields
- H01J61/06—Main electrodes
- H01J61/067—Main electrodes for low-pressure discharge lamps
- H01J61/0672—Main electrodes for low-pressure discharge lamps characterised by the construction of the electrode
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/12—Selection of substances for gas fillings; Specified operating pressure or temperature
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/30—Vessels; Containers
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/30—Vessels; Containers
- H01J61/302—Vessels; Containers characterised by the material of the vessel
Abstract
Description
本發明的實施方式是有關於一種阻擋放電燈、阻擋放電燈單元以及液體處理裝置。The embodiment of the present invention relates to a barrier discharge lamp, a barrier discharge lamp unit, and a liquid treatment device.
例如,作為將處於水中的雜質除去的方法,已知有過濾法、活性炭吸附法、離子交換法、蒸餾法、逆滲透膜脫鹽法等。而且近年來,正進行利用紫外線的雜質除去。例如,若對水照射紫外線,則生成氧化力強的羥基自由基。羥基自由基將處於水中的總有機碳(Total Organic Carbon,TOC)經過有機酸而分解為二氧化碳,因而與過濾法等相比,可製造純度更高的純水。作為照射紫外線的光源,可使用低壓水銀燈。For example, as methods for removing impurities in water, filtration methods, activated carbon adsorption methods, ion exchange methods, distillation methods, and reverse osmosis membrane desalination methods are known. In addition, in recent years, impurity removal using ultraviolet rays has been carried out. For example, if water is irradiated with ultraviolet rays, hydroxyl radicals with strong oxidizing power are generated. Hydroxyl radicals decompose Total Organic Carbon (TOC) in water into carbon dioxide through organic acids, so that pure water with higher purity can be produced compared to filtration methods. As a light source for irradiating ultraviolet rays, a low-pressure mercury lamp can be used.
此處,水的吸收係數在500 nm附近達到最小,隨著從500 nm向長波長側或短波長側偏移而增加。低壓水銀燈照射峰值波長為254 nm、185 nm的紫外線,但具有這種波長的紫外線的水的吸收係數小。因此,為了獲得充分純度的純水,需要延長照射時間,或增大施加於低壓水銀燈的電力。但是,若延長照射時間,則生產效率降低。若增大所施加的電力,則低壓水銀燈內的水銀蒸氣壓上升,發光效率降低。Here, the absorption coefficient of water reaches its minimum near 500 nm, and it increases as it shifts from 500 nm to the long-wavelength side or the short-wavelength side. The low-pressure mercury lamp irradiates ultraviolet rays with peak wavelengths of 254 nm and 185 nm, but the absorption coefficient of water with such wavelengths of ultraviolet rays is small. Therefore, in order to obtain pure water of sufficient purity, it is necessary to extend the irradiation time or increase the power applied to the low-pressure mercury lamp. However, if the irradiation time is prolonged, the production efficiency decreases. If the applied power is increased, the mercury vapor pressure in the low-pressure mercury lamp increases, and the luminous efficiency decreases.
因此,提出了採用阻擋放電燈(氙準分子燈),此阻擋放電燈(氙準分子燈)照射具有水的吸收係數更大的172 nm的峰值波長的紫外線。但是,阻擋放電燈的發光效率的溫度依存特性大,因而在將阻擋放電燈用於液體處理的情況下,在提高發光效率的方面有改善的餘地。 [現有技術文獻]Therefore, it has been proposed to use a barrier discharge lamp (xenon excimer lamp), which irradiates ultraviolet rays having a peak wavelength of 172 nm with a greater absorption coefficient of water. However, the luminous efficiency of the barrier discharge lamp has a large temperature-dependent characteristic, so when the barrier discharge lamp is used for liquid treatment, there is room for improvement in improving luminous efficiency. [Prior Art Literature]
[專利文獻] [專利文獻1] 日本專利特開2014-182916號公報[Patent Literature] [Patent Document 1] Japanese Patent Laid-Open No. 2014-182916
[發明所要解決的問題] 本發明所要解決的問題在於提供一種可提高發光效率的阻擋放電燈、阻擋放電燈單元以及液體處理裝置。 [解決問題的技術手段][The problem to be solved by the invention] The problem to be solved by the present invention is to provide a barrier discharge lamp, a barrier discharge lamp unit and a liquid treatment device that can improve the luminous efficiency. [Technical means to solve the problem]
實施方式的阻擋放電燈包括:發光管,呈筒狀,且在內部空間封入有氣體;內部電極,設於所述內部空間;以及外部電極,設於所述發光管的外部。所述發光管的外徑為10 mm以上且25 mm以下。輸入密度為0.3 W/cm以上且1.4 W/cm以下。 [發明的效果]The barrier discharge lamp of the embodiment includes: a luminous tube, which has a cylindrical shape and is filled with gas in an internal space; an internal electrode, which is provided in the internal space; and an external electrode, which is provided outside the luminous tube. The outer diameter of the luminous tube is 10 mm or more and 25 mm or less. The input density is 0.3 W/cm or more and 1.4 W/cm or less. [Effects of the invention]
根據本發明的實施方式,可提供一種可提高發光效率的阻擋放電燈、阻擋放電燈單元以及液體處理裝置。According to the embodiments of the present invention, a barrier discharge lamp, a barrier discharge lamp unit, and a liquid treatment device that can improve luminous efficiency can be provided.
以下,一方面參照圖式一方面對實施方式進行例示。此外,各圖式中,對同樣的結構元件標注相同符號而適當省略詳細說明。Hereinafter, embodiments will be exemplified with reference to the drawings on the one hand. In addition, in each drawing, the same components are denoted by the same reference numerals, and detailed descriptions are appropriately omitted.
(阻擋放電燈1)
圖1的(a)為用於例示本實施方式的阻擋放電燈1的示意圖。
圖1的(b)為圖1的(a)的阻擋放電燈1的A部的示意放大圖。
圖2為圖1的(a)的阻擋放電燈1的B-B線方向的示意截面圖。
如圖1的(a)、圖1的(b)及圖2所示,在阻擋放電燈1,可設置發光管2、導電部3、內部電極4、錨具(anchor)5、支座(holder)6、外部電極7、導線8及導線9。(Barrier discharge lamp 1)
FIG. 1(a) is a schematic diagram for illustrating the
發光管2呈筒狀,具有全長(管軸方向的長度)較管徑更長的形態。發光管2例如可設為圓筒管。發光管2的外徑例如可設為10 mm以上且25 mm以下。The
在發光管2的管軸方向的兩側的端部,分別設有密封部2a。通過設置密封部2a,從而可將發光管2的內部空間氣密地密封。密封部2a例如可使用壓緊密封(pinch seal)法或收縮密封(shrink seal)法而形成。Sealing
在發光管2的外表面,可設置突起部2b。突起部2b可為了在製造阻擋放電燈1時將發光管2的內部空間排氣,或在發光管2的內部空間導入後述的氣體而設置。突起部2b可通過在排氣及氣體的導入後,將由合成石英玻璃所形成的管燒斷而形成。On the outer surface of the
在發光管2的內部空間封入有氣體。阻擋放電燈1中,在內部電極4與外部電極7之間進行介質阻擋放電,對所封入的氣體賦予高的能量電子而生成準分子激發分子。在準分子激發分子還原時,根據氣體的種類而產生具有特定的峰值波長的光。因此,封入至發光管2的內部空間的氣體可根據阻擋放電燈1的用途而適當變更。封入至發光管2的內部空間的氣體例如可設為氪、氙、氬、氖等稀有氣體或使多種稀有氣體混合而成的混合氣體。氣體中,視需要也可還含有鹵素氣體等。A gas is enclosed in the internal space of the
發光管2的內部空間的25℃時的氣體的壓力(封入壓力)例如可設為1.3 kPa~200 kPa左右。發光管2的內部空間的25℃時的氣體的壓力(封入壓力)可通過氣體的標準狀態(標準的環境溫度和壓力(Standard Ambient Temperature and Pressure,SATP):溫度25℃、1 bar)而求出。The gas pressure (sealing pressure) at 25° C. in the internal space of the
例如,在將水等液體所含的雜質分解的情況下,優選將封入的氣體設為氙氣。氙氣的封入壓力例如可設為47 kPa左右。若將封入的氣體設為氙氣,則可產生峰值波長為172 nm的紫外線,因而可有效地進行雜質的分解。For example, when decomposing impurities contained in a liquid such as water, it is preferable that the enclosed gas be xenon. The sealing pressure of xenon gas can be set to about 47 kPa, for example. If the enclosed gas is xenon, ultraviolet rays with a peak wavelength of 172 nm can be generated, so that the decomposition of impurities can be effectively performed.
導電部3設於密封部2a的內部。導電部3可針對一個密封部2a而設置一個。導電部3的平面形狀可設為四邊形。導電部3呈薄膜狀。導電部3例如可由鉬箔所形成。The
內部電極4可具有線圈(coil)4a及線腳(leg)4b。線圈4a及線腳4b可一體地形成。線圈4a及線腳4b可通過對線材進行塑性加工而形成。線材的線徑(直徑)例如可設為0.2 mm~1.0 mm左右。The
線圈4a及線腳4b例如可含有鎢作為主成分。鎢的含量例如可設為50 wt%以上。此時,若使用在鎢中添加有鉀等的摻雜鎢,則可提高線圈4a的尺寸穩定性。The
線圈4a呈螺旋狀,設於發光管2的內部空間。線圈4a在發光管2的內部空間的中央區域,沿著發光管2的管軸而延伸。若將發光管2的管軸方向的鄰接的線材的間隔設為線圈4a的節距尺寸P,則線圈4a的節距尺寸P例如可設為0.5 mm~3.0 mm左右。而且,與發光管2的管軸方向正交的方向的線圈4a的外徑D例如可設為1 mm~5 mm左右。The
線腳4b分別設於線圈4a的兩側的端部。線腳4b呈線狀,從線圈4a的端部沿著發光管2的管軸而延伸。線腳4b的端部在密封部2a的內部與導電部3電性連接。線腳4b的端部的附近可與導電部3進行雷射焊接或電阻焊接。The
如圖2所示,錨具5可設於發光管2的內部空間。錨具5的材料例如可設為與內部電極4的材料相同。錨具5可通過對線材進行塑性加工而形成。例如,錨具5的其中一個端部側可設於線圈4a的外表面。例如,可將錨具5的其中一個端部側捲繞於線圈4a的外表面。例如,錨具5的其中一個端部側可呈螺旋狀。例如,錨具5的另一個端部側可與發光管2的內壁接觸。例如,錨具5的另一個端部側可具有沿著發光管2的內壁彎曲的形狀。此外,例示了將錨具5安裝於線圈4a的情況,但也可增大線圈4a的一部分的直徑而設為錨具5。As shown in FIG. 2, the
通過錨具5的其中一個端部側設於線圈4a的外表面,且錨具5的另一個端部側與發光管2的內壁接觸,從而利用錨具5在發光管2的內部空間支撐線圈4a。而且,通過錨具5電性連接於線圈4a,從而錨具5作為內部電極4發揮功能。即,錨具5作為支撐線圈4a的支撐構件、及內部電極4的一部分發揮功能。One end of the
若錨具5作為內部電極4的一部分發揮功能,則內部電極4(錨具5)與外部電極7之間的距離變小,因而即便啟動電壓低也可啟動。而且,即便維持電壓低也可維持發光。即,可使瞬間點燈性能提高,且點燈狀態也穩定。而且,若內部電極4(錨具5)與外部電極7之間的距離變小,則燈剛啟動後的穩定性也提高。因此,可抑制燈剛啟動後的發光不均,因而可直接利用燈剛啟動後的光。If the
錨具5例如可考慮燈的發光特性或啟動特性、及線圈4a的支撐性能等而設置多個。此時,若將發光管2的管軸方向的鄰接的錨具5的間隔設為錨具5的節距尺寸,則錨具5的節距尺寸例如可設為10 mm~40 mm左右。The
支座6呈筒狀,其中一個端部側設於密封部2a的內部,另一個端部側從密封部2a露出。支座6可針對一個密封部2a而設置一個。支座6例如可由樹脂或陶瓷等無機材料形成。支座6例如可包含塊滑石(steatite)、氧化鋁等。The
外部電極7可設於發光管2的外部。外部電極7例如可使用不鏽鋼、鋁、鎳、銀、金、鉑等金屬而形成。外部電極7在與內部電極4之間產生介質阻擋放電。如上文所述,若產生介質阻擋放電,則在發光管2的內部空間中生成準分子激發分子,在準分子激發分子還原時,根據氣體的種類而產生具有特定的峰值波長的光。例如,在封入有氙氣的情況下,產生峰值波長為172 nm的紫外線。The
在阻擋放電燈1例如用於將水等液體所含的雜質分解的用途的情況下,優選發光管2的內部空間中產生的光照射於發光管2周圍的全方位。因此,外部電極7可使發光管2的內部空間中產生的光透過。例如,對於外部電極7可設有將厚度方向貫穿的孔或狹縫等。此時,外部電極7的遮光率優選設為10%以下。When the
例如,如圖1的(a)所示,外部電極7可設為呈網眼狀。例如,可設為具有平織結構的外部電極7。用於平織結構的線材例如可設為線徑為0.1 mm左右的不鏽鋼線或鋁線等。網眼間隔例如可設為縱2.8 mm左右、橫3 mm左右。For example, as shown in (a) of FIG. 1, the
若設為網眼狀的外部電極7,則容易將遮光率設為10%以下。而且,若設為網眼狀的外部電極7,則可覆蓋發光管2的外表面,因而可增大與內部電極4的相向面積。因此,容易大面積地穩定產生介質阻擋放電。If the
例如,可通過將網眼狀的金屬成形為筒狀,並在筒狀的金屬體的內部插入發光管2,從而設置外部電極7。For example, the
導線8可設於至少一個支座6。導線8的其中一個端部穿過支座6的內部,在密封部2a的內部電性連接於導電部3。導線8的其中一個端部的附近可與導電部3進行雷射焊接或電阻焊接。而且,導線8與支座6之間的間隙由密封材料密封。導線8的另一個端部可從支座6露出。在導線8的另一個端部,可連接壓接端子或連接器等。The
導線9的其中一個端部經由鎳套筒9a而電性連接於外部電極7。在導線9的另一個端部,可連接壓接端子或連接器等。
導線8及導線9例如可電性連接於設於液體處理裝置200的點燈電路201(參照圖7)。One end of the
此處,如上文所述,若將封入至發光管2的內部空間的氣體設為氙氣,則可產生峰值波長為172 nm的紫外線。峰值波長為172 nm的紫外線與從低壓水銀燈照射的峰值波長為254 nm、185 nm的紫外線相比,水的吸收係數更大。因此,若將阻擋放電燈1用於水等液體所含的雜質的分解,則可有效地進行雜質的除去。Here, as described above, if the gas enclosed in the internal space of the
此外,阻擋放電燈1的發光效率的溫度依存特性大,因而若溫度變高,則阻擋放電燈1的發光效率降低。在將阻擋放電燈1用於液體的處理的情況下,無法將阻擋放電燈1直接設於液體中。因此,阻擋放電燈1設於保護管101的內部(參照圖7)。此外,在阻擋放電燈1與保護管101的內壁之間的空間中填充有氣體,因而因阻擋放電燈1的點燈而產生的熱難以散放至液體中。若自阻擋放電燈1的散熱受到抑制,則可能導致阻擋放電燈1的溫度上升,發光效率降低。In addition, since the luminous efficiency of the
圖3為用於例示輸入密度與相對照度(紫外線照度)的關係的曲線圖。
相對照度是使用牛尾(Ushio)電機製造的紫外線照度計UIT-250進行測定。頭部(head)使用VUV-S172,測定距離設為3 mm。
輸入密度為施加電力相對於發光長之比。發光長可設為發光管2的管軸方向的外部電極7的長度。Fig. 3 is a graph illustrating the relationship between input density and relative illuminance (ultraviolet illuminance).
The relative illuminance is measured using an ultraviolet illuminance meter UIT-250 manufactured by Ushio Motor. VUV-S172 is used for the head, and the measuring distance is set to 3 mm.
The input density is the ratio of the applied power to the luminous length. The luminous length can be set to the length of the
如由圖3所得知,若將輸入密度設為0.3 W/cm以上且1.4 W/cm以下,則可使相對照度成為90%以上。這意味著,即便在向周圍的散熱受到抑制那樣的環境下使阻擋放電燈1點燈的情況下,若將輸入密度設為0.3 W/cm以上且1.4 W/cm以下,則也可提高發光效率。As can be seen from Figure 3, if the input density is set to 0.3 W/cm or more and 1.4 W/cm or less, the relative illuminance can be made 90% or more. This means that even when the
而且,如上文所述,在發光管2的內部空間中產生的紫外線經由發光管2而照射至外部。因此,發光管2是由紫外線的透過率高的材料形成。紫外線的透過率高的材料例如可設為合成石英玻璃等含有SiO2
的材料。但是,若峰值波長為172 nm的紫外線入射至含有SiO2
的材料,則有時材料的化學結構經時變化。例如,若紫外線入射至SiO2
,則有時Si與O的鍵被切斷。因此,若使阻擋放電燈1長時間點燈,則發光管2的材料的化學結構產生缺陷,可能導致紫外線的透過率急劇降低,進而照度維持率降低。Furthermore, as described above, the ultraviolet rays generated in the internal space of the
根據本發明人所得的見解,若增多含有SiO2 的材料所含的OH基的量,則即便因紫外線的入射而使得Si與O的鍵被切斷,也可修復化學結構的缺陷。According to the findings obtained by the present inventors, if the amount of OH groups contained in the material containing SiO 2 is increased, even if the bond between Si and O is cut by the incidence of ultraviolet rays, defects in the chemical structure can be repaired.
圖4為用於例示OH基的含量、照度維持率及點燈時間的關係的曲線圖。
如由圖4所得知,若將OH基的含量設為100 ppm以上,則即便為產生峰值波長為172 nm的紫外線的阻擋放電燈1,也可長時間保持高的照度維持率。這意味著,可實現阻擋放電燈1的長壽命化。Fig. 4 is a graph illustrating the relationship between the OH group content, the illuminance maintenance rate, and the lighting time.
As seen from FIG. 4, if the OH group content is 100 ppm or more, even the
但是已判明,若過於增多OH基的含量,則紫外線的透過率降低。 圖5為用於例示OH基的含量與相對紫外線照度的關係的曲線圖。 如由圖5所得知,若OH基的含量超過1500 ppm,則紫外線的透過率降低,因而相對紫外線照度降低。However, it has been found that if the content of OH groups is increased too much, the transmittance of ultraviolet rays decreases. Fig. 5 is a graph illustrating the relationship between the content of OH groups and the relative ultraviolet illuminance. As can be seen from Figure 5, if the content of OH groups exceeds 1500 ppm, the transmittance of ultraviolet rays decreases, and therefore the relative ultraviolet illuminance decreases.
因此,如由圖4及圖5所得知,優選發光管2由合成石英玻璃等含有SiO2
的材料形成,且使OH基的含量成為100 ppm以上且1500 ppm以下。若這樣設定,則即便於發光管2的內部空間中產生峰值波長為172 nm的紫外線,也可長時間保持高的照度維持率。而且,可抑制紫外線的透過率降低。Therefore, as understood from FIGS. 4 and 5, it is preferable that the
圖6的(a)~圖6的(d)為用於例示其他實施方式的阻擋放電燈的示意圖。此外,為了避免變得煩雜,將與上文所述的阻擋放電燈1的結構元件相同的結構元件適當省略。6(a) to 6(d) are schematic diagrams for illustrating barrier discharge lamps of other embodiments. In addition, in order to avoid becoming complicated, the same structural elements as those of the
如圖6的(a)所示,內部電極14可具有線圈14a及線腳4b。線圈14a呈螺旋狀,設於發光管2的內部空間。若將發光管2的管軸方向的鄰接的線材的間隔設為線圈14a的節距尺寸Pa,則線圈14a的節距尺寸Pa例如可設為15 mm~90 mm左右。線圈14a在發光管2的內部空間,沿著發光管2的管軸而延伸。圖1的(a)及圖1的(b)所例示的線圈4a由錨具5支撐,但線圈14a的外側端與發光管2的內壁接觸。此外,也可在線圈14a的外側端與發光管2的內壁之間設置稍許的間隙。此時,也可省略錨具5。As shown in FIG. 6(a), the
若這樣設定,則可減小線圈14a與外部電極7之間的距離,因而即便啟動電壓更低也可啟動。而且,即便維持電壓更低也可維持發光。即,可使瞬間點燈性能進一步提高,且使點燈狀態也更穩定。If it is set in this way, the distance between the
如圖6的(b)所示,外部電極17可呈螺旋狀,且捲繞於發光管2的外表面。
若這樣設定,則可抑制下述情況:在發光管2的內部空間中產生的紫外線向外部照射時,被外部電極17遮擋。As shown in (b) of FIG. 6, the
如圖6的(c)所示,外部電極17可呈螺旋狀,且捲繞於發光管2的外表面。而且,可省略錨具5。
若這樣設定,則可抑制下述情況:在發光管2的內部空間中產生的紫外線向外部照射時,被外部電極17遮擋。而且,可通過省略錨具5而降低製造成本。As shown in (c) of FIG. 6, the
如圖6的(d)所示,外部電極7可設為網眼狀,且內部電極4具有線圈4a及線腳4b。另外,可省略錨具5。
若這樣設定,則可降低製造成本。As shown in (d) of FIG. 6, the
(阻擋放電燈單元100以及液體處理裝置200)
接下來,對阻擋放電燈單元100及液體處理裝置200進行例示。
此外,以下作為一例,對設有圖1的(a)所例示的阻擋放電燈1的情況進行說明,但例如也可設有圖6的(a)~圖6的(d)所例示的阻擋放電燈。(Barrier
圖7為用於例示阻擋放電燈單元100及液體處理裝置200的示意圖。
如圖7所示,在液體處理裝置200,可設置阻擋放電燈單元100、點燈電路201及控制器202。
阻擋放電燈單元100可具有阻擋放電燈1、保護管101、蓋102及密封構件103。FIG. 7 is a schematic diagram for illustrating the barrier
保護管101呈筒狀,具有全長(管軸方向的長度)較管徑更長的形態。保護管101例如可設為圓筒管。保護管101的其中一個端部被堵塞,另一個端部開口。在保護管101的開口側的端部設有凸緣101a。在保護管101的內部空間,可收容阻擋放電燈1。The
如圖7所示,保護管101可設於作為處理對象的液體300(例如水)中。此時,以收容於保護管101的阻擋放電燈1位於液體300的內部的方式設定。蓋102及密封構件103優選以位於液體300的外部的方式設定。保護管101例如可設於在水槽等中不流動的液體300中,也可設於在槽或配管等流路中流動的液體300中。As shown in FIG. 7, the
從阻擋放電燈1照射的紫外線經由保護管101而照射於液體300。因此,保護管101是由紫外線的透過率高的材料形成。保護管101例如由合成石英玻璃等含有SiO2
的材料形成。此時,與上文所述的發光管2的情況同樣地,保護管101優選由合成石英玻璃等含有SiO2
的材料形成,且使OH基的含量成為100 ppm以上且1500 ppm以下。若這樣設定,則即便從阻擋放電燈1照射峰值波長為172 nm的紫外線,也可長時間保持高的照度維持率。這意味著,可實現阻擋放電燈單元100的長壽命化。而且,可抑制紫外線的透過率降低。The ultraviolet rays irradiated from the
蓋102呈板狀,堵塞保護管101的開口。在蓋102設有將厚度方向貫穿的孔。導線8及導線9經由設於蓋102的孔而伸出至外部。導線8與孔的間隙、導線9與孔的間隙由密封材料密封。The
密封構件103設於蓋102與保護管101的凸緣101a之間。密封構件103例如可設為O環等。通過將蓋102及密封構件103安裝於保護管101的凸緣101a,從而以保護管101的內部空間變得氣密的方式密封。The sealing
此處,若在保護管101的內部空間中存在氧,則可能導致從阻擋放電燈1照射的紫外線衰減。因此,優選在保護管101的內部空間中封入氮氣或惰性氣體。此時,若將封入的氣體設為氮氣,則可降低製造成本。Here, if oxygen exists in the internal space of the
點燈電路201例如可具有高頻產生電路。高頻產生電路例如可產生頻率為100 kHz左右且電壓為2 kVp-p的電力。導線8及導線9可電性連接於點燈電路201。而且,點燈電路201具有切換向阻擋放電燈1的電力施加、與電力施加的停止的開關。而且,也可由一個點燈電路201對多個阻擋放電燈1施加電力。The
控制器202可具有中央處理器(Central Processing Unit,CPU)等運算元件、半導體記憶體等記憶元件。控制器202例如可設為電腦。在記憶元件中,可保存控制點燈電路201的控制程序。運算元件可基於保存於記憶元件的控制程序,控制向阻擋放電燈1的電力施加、電力施加的停止等。在控制器202,可設置供操作者輸入資料的輸入部、顯示阻擋放電燈1的運行狀況或異常顯示等的監視器(monitor)、電源開關等。而且,也可由一個控制器202控制多個點燈電路201。The
此處已判明,若過於延長保護管101的內壁、與外部電極7的外側端之間的間隙尺寸S(最短距離),則從保護管101照射的紫外線的相對照度降低。It has been found here that if the gap size S (shortest distance) between the inner wall of the
圖8為用於例示間隙尺寸S與紫外線的相對照度的關係的曲線圖。
圖8的相對照度是輸入密度為1 W/cm的情況下的紫外線的相對照度。而且,將間隙尺寸S為2 mm的情況下的紫外線的相對照度設為100%。
如由圖8所得知,若將間隙尺寸S設為10 mm以下,則可使相對照度成為90%以上。這意味著,可抑制保護管101的內部的紫外線的衰減,可提高紫外線的取出效率。若紫外線的取出效率提高,則可提高液體中的雜質的除去率,或縮短照射時間,或減少施加電力。FIG. 8 is a graph for illustrating the relationship between the gap size S and the relative illuminance of ultraviolet rays.
The relative illuminance in Fig. 8 is the relative illuminance of ultraviolet rays when the input density is 1 W/cm. In addition, the relative illuminance of ultraviolet rays when the gap size S is 2 mm is set to 100%.
As can be seen from FIG. 8, if the gap size S is set to 10 mm or less, the relative illuminance can be made 90% or more. This means that the attenuation of ultraviolet rays inside the
以上,例示了本發明的若干實施方式,但這些實施方式是作為示例而提示,並非意圖限定發明的範圍。這些新穎的實施方式能以其他各種形態實施,能在不偏離發明的主旨的範圍內進行各種省略、替換、變更等。這些實施方式或其變形例包含於發明的範圍或主旨,並且也包含於發明申請專利範圍所記載的發明及其均等範圍。而且,所述各實施方式可相互組合而實施。As mentioned above, although some embodiment of this invention was illustrated, these embodiment is shown as an example and is not intending limiting the range of invention. These novel embodiments can be implemented in various other forms, and various omissions, substitutions, changes, etc. can be made within a range that does not deviate from the gist of the invention. These embodiments or their modifications are included in the scope or spirit of the invention, and are also included in the invention described in the scope of the invention application and its equivalent scope. Furthermore, each of the above-mentioned embodiments can be implemented in combination with each other.
1:阻擋放電燈
2:發光管
2a:密封部
2b:突起部
3:導電部
4:內部電極
4a、14a:線圈
4b:線腳
5:錨具
6:支座
7:外部電極
8、9:導線
9a:鎳套筒
14:內部電極
17:外部電極
100:阻擋放電燈單元
101:保護管
101a:凸緣
102:蓋
103:密封構件
200:液體處理裝置
201:點燈電路
202:控制器
300:液體
D:外徑
P、Pa:節距尺寸
S:間隙尺寸1: Barrier discharge lamp
2:
圖1的(a)為用於例示本實施方式的阻擋放電燈的示意圖。圖1的(b)為圖1的(a)的阻擋放電燈的A部的示意放大圖。 圖2為圖1的(a)的阻擋放電燈的B-B線方向的示意截面圖。 圖3為用於例示輸入密度與相對照度(紫外線照度)的關係的曲線圖。 圖4為用於例示OH基的含量、照度維持率及點燈時間的關係的曲線圖。 圖5為用於例示OH基的含量與相對紫外線照度的關係的曲線圖。 圖6的(a)~圖6的(d)為用於例示其他實施方式的阻擋放電燈的示意圖。 圖7為用於例示阻擋放電燈單元及液體處理裝置的示意圖。 圖8為用於例示間隙尺寸與紫外線的相對照度的關係的曲線圖。FIG. 1(a) is a schematic diagram for illustrating the barrier discharge lamp of this embodiment. Fig. 1(b) is a schematic enlarged view of a part A of the barrier discharge lamp of Fig. 1(a). Fig. 2 is a schematic cross-sectional view in the direction of line B-B of the barrier discharge lamp of Fig. 1(a). Fig. 3 is a graph illustrating the relationship between input density and relative illuminance (ultraviolet illuminance). Fig. 4 is a graph illustrating the relationship between the OH group content, the illuminance maintenance rate, and the lighting time. Fig. 5 is a graph illustrating the relationship between the content of OH groups and the relative ultraviolet illuminance. 6(a) to 6(d) are schematic diagrams for illustrating barrier discharge lamps of other embodiments. Fig. 7 is a schematic diagram for illustrating a barrier discharge lamp unit and a liquid treatment device. FIG. 8 is a graph for illustrating the relationship between the gap size and the relative illuminance of ultraviolet rays.
1:阻擋放電燈1: Barrier discharge lamp
2:發光管2: luminous tube
2a:密封部2a: Sealing part
2b:突起部2b: protrusion
3:導電部3: Conductive part
4:內部電極4: Internal electrode
4a:線圈4a: coil
4b:線腳4b: wire pin
5:錨具5: Anchor
6:支座6: Support
7:外部電極7: External electrode
8、9:導線8, 9: Wire
9a:鎳套筒9a: Nickel sleeve
D:外徑D: Outer diameter
P:節距尺寸P: Pitch size
Claims (6)
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JP2020-032841 | 2020-02-28 | ||
JP2020032841A JP2021136186A (en) | 2020-02-28 | 2020-02-28 | Barrier discharge lamp, barrier discharge lamp unit, and liquid processing device |
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TW202133216A true TW202133216A (en) | 2021-09-01 |
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TW109127595A TW202133216A (en) | 2020-02-28 | 2020-08-13 | Barrier discharge lamp, barrier discharge lamp unit and liquid treatment device which has a luminous tube containing silicon dioxide material |
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JP (1) | JP2021136186A (en) |
CN (1) | CN113327838A (en) |
TW (1) | TW202133216A (en) |
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2020
- 2020-02-28 JP JP2020032841A patent/JP2021136186A/en active Pending
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