TW202249063A - Discharge lamp and manufacturing method of electrode used in discharge lamp characterized in that a groove along the circumferential direction of the electrode is formed and the emissivity of the coating layer on the groove is greater than that of the groove, thereby, the electrode obtains the desired heat dissipation effect - Google Patents
Discharge lamp and manufacturing method of electrode used in discharge lamp characterized in that a groove along the circumferential direction of the electrode is formed and the emissivity of the coating layer on the groove is greater than that of the groove, thereby, the electrode obtains the desired heat dissipation effect Download PDFInfo
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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
- H01J61/52—Cooling arrangements; Heating arrangements; Means for circulating gas or vapour within the discharge space
- H01J61/523—Heating or cooling particular parts of the lamp
- H01J61/526—Heating or cooling particular parts of the lamp heating or cooling of electrodes
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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
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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
- H01J61/52—Cooling arrangements; Heating arrangements; Means for circulating gas or vapour within the discharge space
- H01J61/523—Heating or cooling particular parts of the lamp
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J9/00—Apparatus or processes specially adapted for the manufacture, installation, removal, maintenance of electric discharge tubes, discharge lamps, or parts thereof; Recovery of material from discharge tubes or lamps
- H01J9/02—Manufacture of electrodes or electrode systems
- H01J9/04—Manufacture of electrodes or electrode systems of thermionic cathodes
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J9/00—Apparatus or processes specially adapted for the manufacture, installation, removal, maintenance of electric discharge tubes, discharge lamps, or parts thereof; Recovery of material from discharge tubes or lamps
- H01J9/02—Manufacture of electrodes or electrode systems
- H01J9/18—Assembling together the component parts of electrode systems
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Abstract
Description
本發明係關於一種短路電弧型放電燈等之放電燈,且特別有關於一種電極之散熱。The present invention relates to a discharge lamp such as a short-circuit arc type discharge lamp, and particularly relates to heat dissipation of an electrode.
放電燈,其於點燈中,電極尖端部係成為高溫,鎢等之電極材料係熔融、蒸發,放電管係黑化,以導致燈照度降低。為了防止包含電極尖端部之電極之過熱,而藉螺絲狀或凹凸狀之凹槽,使電極軀幹部側面之表面積增大,於該凹槽上,燒結鎢等之粉末或金屬氧化物,而形成散熱層(參照專利文獻1)。 [先行技術文獻] [專利文獻] In a discharge lamp, during lighting, the tip of the electrode becomes high temperature, the electrode material such as tungsten is melted and evaporated, and the discharge tube is blackened, resulting in a decrease in the illuminance of the lamp. In order to prevent overheating of the electrode including the tip of the electrode, the surface area of the side surface of the electrode body is increased by screw-shaped or concave-convex grooves, and tungsten powder or metal oxide is sintered on the groove to form Heat dissipation layer (refer to Patent Document 1). [Prior Art Literature] [Patent Document]
[專利文獻1]日本專利特開2000-306546號公報[Patent Document 1] Japanese Patent Laid-Open No. 2000-306546
[發明所欲解決的問題][Problem to be solved by the invention]
針對被形成於電極表面之凹槽,將電極表面積放大作為目的,而決定凹槽形狀(其淺度、節距等),但是,因為凹槽形狀,散熱性能,亦即,發射率也改變。另外,散熱層之發射率,也因為燒結之金屬氧化物等素材而不同,即使不考慮與凹槽之關係性地,於凹槽形成散熱層,也無法更加提高散熱性能,有時也有散熱效果下降之虞。For the grooves formed on the surface of the electrode, the shape of the groove (its shallowness, pitch, etc.) is determined for the purpose of enlarging the surface area of the electrode, but the heat dissipation performance, that is, the emissivity also changes due to the shape of the groove. In addition, the emissivity of the heat dissipation layer is also different due to the sintered metal oxide and other materials. Even if the heat dissipation layer is formed on the groove without considering the relationship with the groove, the heat dissipation performance cannot be further improved, and sometimes it has a heat dissipation effect. risk of decline.
因此,被要求構成可獲得期望之散熱效果之電極。 [用以解決問題的手段] Therefore, it is required to form an electrode that can obtain a desired heat dissipation effect. [means used to solve a problem]
做為本發明一態樣之放電燈,其包括放電管、及在放電管內,相向配置之一對電極,至少一者之電極,其至少於電極軀幹部的側面中,包括發射率大於電極基材表面之散熱構造。而且,於散熱構造上,形成有更加提高設有散熱構造之電極軀幹部側面部分之發射率之塗層。A discharge lamp as an aspect of the present invention includes a discharge tube, and a pair of electrodes disposed opposite to each other in the discharge tube, and at least one of the electrodes, which is at least on the side of the body of the electrode, includes an electrode with an emissivity greater than that of the electrode. The heat dissipation structure of the substrate surface. Furthermore, on the heat dissipation structure, a coating layer is formed to further increase the emissivity of the side portion of the electrode trunk portion provided with the heat dissipation structure.
而且,由散熱構造所致之散熱功能、及塗層所致之散熱功能所致之電極軀幹部側面部分之散熱效果,其依據電極素材、散熱構造之特性、塗層之反射率等,而可以最有效地工作。其關係到使依據兩個散熱功能之電極軀幹部側面部分之發射率為最高。Moreover, the heat dissipation effect caused by the heat dissipation function of the heat dissipation structure and the heat dissipation effect of the side part of the electrode body due to the heat dissipation function of the coating can be determined according to the electrode material, the characteristics of the heat dissipation structure, and the reflectivity of the coating. work most efficiently. It is concerned with maximizing the emissivity of the side parts of the body of the electrode according to the two heat dissipation functions.
在這種使散熱構造與塗層為層狀之電極軀幹部側面部分中,可獲得用於為了單純地為了提高塗層之散熱性能,而放大塗層面積以形成之凹槽所致之散熱效果,所無法獲得之散熱效果。In the side part of the electrode body where the heat dissipation structure and the coating are layered, the heat dissipation effect of the grooves formed by enlarging the coating area for simply improving the heat dissipation performance of the coating can be obtained. , the heat dissipation effect that cannot be obtained.
作為散熱構造,其可適用凹槽或凹凸形狀、塗層等種種之構造,例如以沿著電極軀幹部之圓周方向或電極軸向之凹槽構成,塗層之發射率大於凹槽之發射率。As a heat dissipation structure, it can be applied to various structures such as grooves or concave-convex shapes, coatings, etc. For example, it is composed of grooves along the circumferential direction of the electrode body or the electrode axial direction, and the emissivity of the coating is greater than that of the grooves. .
作為塗層,其可由發射率較高之素材構成,可依據電極素材、使用溫度等以選擇之。塗層,其由至少包含金屬及/或陶瓷之素材所構成。也可以由至少包含與電極素材相同種類之金屬之塗層所組成。如果考慮提高散熱性能時,例如可至少由鋯及/或鉭等所組成,又,也可以包含鎢、鉬等之電極之素材。As a coating, it can be made of materials with high emissivity, which can be selected according to electrode materials, service temperature, etc. Coating, which is composed of materials including at least metal and/or ceramics. It may also consist of a coating containing at least the same type of metal as the electrode material. In consideration of improving heat dissipation performance, for example, it may be composed of at least zirconium and/or tantalum, and may also contain tungsten, molybdenum, etc. as electrode materials.
散熱構造,其當以沿著電極軀幹部之圓周之凹槽所構成時,結合散熱構造與塗層之發射率,其當以以下公式表示時,可成為0.8以上。 ε=1/(l+(L/S)╳(l/εo-1)) 但是,L係表示凹槽之形成領域之軸方向長度,S係表示總剖面長度。εo係表示塗層之發射率。又,L/S係被定為0.9以下。 When the heat dissipation structure is formed with grooves along the circumference of the electrode body, the emissivity of the heat dissipation structure and the coating can be 0.8 or more when expressed by the following formula. ε=1/(l+(L/S)╳(l/εo-1)) However, L represents the length in the axial direction of the region where the grooves are formed, and S represents the total cross-sectional length. εo represents the emissivity of the coating. Also, the L/S system is set to be 0.9 or less.
塗層之厚度、凹槽之形狀等,其可適用種種構造。例如自電極中心軸至塗層的層表面為止之距離,其可以被構成為比自未設有散熱構造之電極軀幹部側面的電極中心軸算起之距離還要短。The thickness of the coating, the shape of the groove, etc., can be applied to various structures. For example, the distance from the center axis of the electrode to the layer surface of the coating may be shorter than the distance from the center axis of the electrode on the side of the body of the electrode not provided with a heat dissipation structure.
於電極的尖端側錐形部的錐形表面,其也可以設置未被塗層所覆蓋之非塗層散熱構造。或者,也可以於電極的軀幹部側面中,在比散熱構造還要靠近電極支撐棒側,設置未被塗層所覆蓋之非塗層散熱構造。非塗層散熱構造,其可適用於遠離散熱構造之處所。On the tapered surface of the tapered portion on the tip side of the electrode, it may also be provided with a non-coated heat dissipation structure that is not covered by the coating. Alternatively, a non-coated heat dissipation structure that is not covered with a coating may be provided on the side of the trunk portion of the electrode on the side closer to the electrode support rod than the heat dissipation structure. Non-coated heat dissipation structure, which can be applied to places far away from heat dissipation structure.
作為本發明其他態樣之放電燈之製造方法,其特徵在於成型具有柱狀軀幹部與尖端側錐形部之電極,對於軀幹部側面,形成沿著電極圓周方向之凹槽,藉塗佈而於凹槽上,形成發射率大於凹槽之發射率之塗層。 [發明功效] As a method of manufacturing a discharge lamp according to another aspect of the present invention, it is characterized in that an electrode having a columnar body and a tapered portion on the tip side is formed, and grooves along the circumferential direction of the electrode are formed on the side of the body, and are formed by coating. On the grooves, a coating having an emissivity greater than that of the grooves is formed. [Efficacy of the invention]
當依據本發明時,可構成可獲得期望之散熱效果之電極。When according to the present invention, it is possible to constitute an electrode that can obtain a desired heat dissipation effect.
[用以實施發明的形態][Mode for Carrying Out the Invention]
短路電弧型放電燈10,其為可輸出高亮度之光之大型放電燈,其包括透明之石英玻璃製之約略球狀放電管(發光管)12,於放電管12內,相向(同軸)配置有鎢製之一對之電極20,30。於放電管12之兩側,石英玻璃製之密封管13A,13B係與放電管12連設,而一體形成。於放電管12內的放電空間DS中,封入有水銀與鹵素或氬氣等之稀有氣體。Short-circuit arc
做為陰極之電極20,其被電極支撐棒17A所支撐。於密封管13A係密封有貫穿有電極支撐棒17A之玻璃管(未圖示)、與外部電源相連接之導電棒15A、及連接電極支撐棒17A與導電棒15A之金屬箔16A等。針對作為陽極之電極30也同樣地,密封有貫穿有電極支撐棒17B之玻璃管(未圖示)、金屬箔16B、導電棒15B等之裝配件。又,於密封管13A,13B的端部,分別安裝有口金19A,19B。The
當電壓施加於一對之電極20,30時,於電極20,30間,產生電弧放電,光往放電管12的外部放射。在此,投入有1kW以上之電力。自放電管12放射之光,其藉反射鏡(未圖示)以被導引往既定方向。When a voltage is applied to the pair of
圖2為電極(陽極)30之示意俯視圖。而且,關於電極(陰極)20,也可以做成同樣之構造。FIG. 2 is a schematic top view of an electrode (anode) 30 . Furthermore, the electrode (cathode) 20 may also have the same structure.
電極30,其具有電極尖端面32T,由連接成為錐狀之部分(以下,稱做尖端側錐形部)32與電極支撐棒17B之柱狀部分(以下,稱做軀幹部)34所構成。在此,電極30係一體性地構成,但是,其也可以藉SPS等之擴散接合,接合尖端側錐形部32與軀幹部34,而構成電極30。又,也可以透過中間構件以接合之。電極30係由例如鎢所組成。The
於軀幹部34的側面34S,設有散熱構造40(參照圖2的斜線部)。散熱構造40,其與軀幹部34的基材表面34T,亦即,不敢採用特別散熱構造之表面相比較下,發射率係較高,具有提高散熱性之功能。如圖2的放大部所示,散熱構造40,在此,其成為使沿著圓周方向(圍繞電極軸)之凹槽42,以既定節距形成之構造。凹槽42,其可藉例如雷射或切削等以形成之。A
而且,對於設有此散熱構造40(凹槽42)之軀幹部34的側面34S,塗層44係被形成於其上。塗層44,在此,其使用發射率大於凹槽42之成分。例如塗層44係由氮化鋯或碳化鋯、鋯化合物所組成。或者,包含氮化鉭等之鉭類素材或氧化鋁等之陶瓷類素材。又,塗層44,其也可以含有與電極30相同之金屬,亦即,鎢、鉬等。此外,可依據使用溫度,選擇鈦等之金屬類或其氧化物、添加有鎳、鉻等之合金類等。Also, for the
包括由凹槽42所構成之散熱構造40、及塗層44之兩個散熱功能之部分(以下,將此側面部分,稱做散熱功能部J),其形成於軀幹部34的側面34S的一部份。其如先前地,為了使散熱之熱量更多,而以增大電極表面面積為目的,而形成凹槽,並非使凹槽設成作為輔助性之散熱構造,而組合由凹槽42所致之散熱功能與由塗層44所致之散熱功能,其藉於該散熱功能部J中,最大限度地提高散熱功能之組合以構成。The
藉此,散熱性(發射率)係最大限度地被提高,而可抑制電極溫度上昇。因為在凹槽42形成塗層44,其與對於電極基材表面34T之塗層相比較下,接觸面積係變大,可提高塗層之緊密接觸性。Thereby, heat dissipation (emissivity) is maximized, and an increase in electrode temperature can be suppressed. Since the
又,對於軀幹部34的側面34S,設有散熱功能部J,所以,可抑制曝露到電弧、火炬等。因此,對於由燈點燈所致之電極30之溫度上昇,可抑制塗層剝落、變薄之情形。又,凹槽42係包括散熱功能,所以,即使塗層剝落、變薄,也可以維持某程度之散熱性。Moreover, since the
尤其,如圖2所示,以塗層44覆蓋之凹槽42的頂部42P之高度,亦即,自電極軸C至頂部42P(層表面)為止之距離,其位於比軀幹部34的側面34S還要靠近電極中心側之位置。凹槽42的頂部42P,其位於自軀幹部34的側面34S回縮後之位置,藉此,可有效地抑制由電弧或火炬所致之塗層之剝落、變薄之情形。In particular, as shown in FIG. 2, the height of the top 42P of the
於本實施形態中,藉適用組合凹槽42與塗層44之發射率之算出公式,以適宜組合凹槽42之形狀及塗層44之散熱性(發射率),可有效地提高軀幹部34之散熱性(發射率)。以下,針對此以詳述之。In this embodiment, by applying the formula for calculating the emissivity of the
圖3為表示凹槽42之形狀與塗層44之發射率之相關關係之圖表。圖4為表示凹槽之形狀之圖。FIG. 3 is a graph showing the correlation between the shape of the
形成有凹槽之表面之發射率ε,其可藉以下之(1)式以近似性地表示。
ε=l/(1+(L/S)╳(l/εo-1)) ... (1)
但是,L為表示凹槽之形成領域之軸方向(沿著側面34S)之長度,S係表示在凹槽剖面圖上之沿著凹槽之全長(總剖面長)(參照圖4)。
The emissivity ε of the surface on which grooves are formed can be approximated by the following formula (1).
ε=l/(1+(L/S)╳(l/εo-1)) ... (1)
However, L represents the length in the axial direction (along the
L/S之值,其關係到凹槽節距與凹槽之數量,亦即,凹槽形成範圍中之凹槽深度(斜面長度)。L/S之值愈小,則凹槽之深度、節距數量愈大,L/S之值愈接近1,則凹槽愈淺,節距數量也愈少。另外,εo係表示材料固有之發射率。The value of L/S is related to the groove pitch and the number of grooves, that is, the groove depth (slope length) in the groove forming range. The smaller the value of L/S, the larger the depth of the groove and the larger the number of pitches. The closer the value of L/S is to 1, the shallower the groove and the smaller the number of pitches. In addition, εo represents the intrinsic emissivity of a material.
置換材料固有之發射率εo為塗層44之發射率(在此,表示為εcoat),藉此,導出散熱功能部J之發射率ε(在此,表示為εgroove+coat)。但是,塗層44係與凹槽42之大小(深度)相比較下,非常薄,所以,可忽視其厚度。The intrinsic emissivity εo of the replacement material is the emissivity ε of the coating 44 (herein, expressed as εcoat), thereby deriving the emissivity ε of the heat dissipation function part J (herein, expressed as εgroove+coat). However, the
圖3為表示自塗層44之發射率εcoat與凹槽42之L/S之組合,所導出之散熱功能部J之發射率εgroove+coat。例如當形成塗層44之發射率εcoat為0.8,L/S值成為0.35之凹槽42時,散熱功能部J之發射率εgroove+coat係成為0.92。又,當形成塗層44之發射率εcoat為0.5,L/S之值成為0.2之凹槽42時,散熱功能部之發射率εgroove+coat係成為0.83。FIG. 3 shows the emissivity εgroove+coat of the heat dissipation function part J derived from the combination of the emissivity εcoat of the
在此,L/S及塗層44之發射率εcoat係被決定,使得散熱功能部J之發射率εgroove+coat成為0.8以上。但是,沿著圓周方向之凹槽42之L/S係被決定為0.9以下,使得凹槽42不成為與粗面同樣之凹凸形狀。0.8係依據成為例如電極素材之鎢之發射率0.4以被決定。Here, L/S and the emissivity εcoat of the
使包括這種凹槽42及塗層44之兩個散熱功能之部分之發射率εgroove+coat,使用上述(1)公式以導出,藉此,可自由選擇塗層44之成分、及凹槽42之形狀,使得成為期望之發射率。例如採用更高散熱性之成分及形狀,可有效地(協同性)地提高軀幹部34之發射率。尤其,使塗層44之發射率決定為大於凹槽42之發射率,藉此,可構成將塗層44之散熱功能作為主要,將凹槽42之散熱功能作為副之散熱功能部J。The emissivity εgroove+coat of the two heat dissipation functions including the
例如當使用發射率較高之塗層44時,滿足0.8以上之L/S之值係幅度較寬,可選擇之凹槽42之形狀係較多。可最適化組合,所以,即使使L/S較大,亦即,即使使凹槽42較淺,也可維持較高之發射率。又,當凹槽42較淺時,可較容易塗佈(附著)塗層44到凹槽42之深處。For example, when the
藉凹槽42之L/S之值,當錯誤選擇塗層44時,只能獲得與該塗層44之發射率沒有太大差異之發射率,而無法獲得充分之散熱效果。但是,藉參照圖3的表,即使對於種種之凹槽形狀(L/S之值),也可維持較高之發射率εgroove+coat。With the value of L/S of the
對於設有這種散熱功能部J之軀幹部34,於尖端側錐形部32的錐形側面(表面)32S,設有僅形成凹槽,於其上未形成有塗層之散熱構造(非塗層散熱構造)50。For the
於燈點燈中,錐形側面32S係曝露在電弧或火炬,所以,當一時設有塗層時,有可能產生塗層之剝落等,但是,因為未設有該種塗層,所以,可抑制放電管12內被塗層之成分所弄髒。又,決定L/S,使得凹槽42之發射率成為較高,藉此,可更加提高電極30全體之散熱性。During lamp lighting, the tapered
另外,於散熱構造40與散熱構造50之間,設有由電極基材面所組成之側面部分33,而不鄰接地彼此遠離。藉設有這種側面部分33,於燈點燈中,可抑制電弧或火炬,移動往具有塗層之散熱功能部。而且,尖端側錐形部32與軀幹部34之邊界部33P係較圓潤,所以,可保護塗層44不受異常放電之產生及異常放電所致之過熱所影響。In addition, between the
這種放電燈的電極30,其可如下地製造。首先,成型具有柱狀軀幹部與尖端側錐形部之電極,對於軀幹部側面,藉雷射或切削等之加工,以形成沿著圓周方向之凹槽。而且,藉塗佈以在凹槽上形成塗層。此時,決定塗層之發射率大於凹槽之發射率,藉此,可構成發射率較高之散熱功能部。而且,塗佈係在噴塗之外,可採用蒸著、濺鍍、CVD等之已知手段,只要可以均質地塗佈即可。塗佈後之塗層,也可以藉爐(加熱裝置)或雷射以燒結之。The
接著,使用圖5,說明第2實施形態之放電燈。在第2實施形態中,於由凹槽所構成之散熱構造上,重疊有塗層之散熱功能部,其被形成於尖端側錐形部與軀幹部,另外,僅形成有凹槽之散熱構造,其被設於電極支撐棒側。Next, a discharge lamp according to a second embodiment will be described using FIG. 5 . In the second embodiment, on the heat dissipation structure composed of grooves, the heat dissipation function part of the coating layer is formed on the tapered part on the tip side and the trunk part, and the heat dissipation structure formed only with grooves , which is set on the side of the electrode support rod.
圖5為第2實施形態之放電燈的電極之示意俯視圖。陽極30'係包括尖端側錐形部32與軀幹部34。由於凹槽所構成之散熱構造40'上,形成有塗層44'之散熱功能部J,其自軀幹部34之中途橫跨到尖端側錐形部32,以連續性地形成。另外,於軀幹部34的側面34S,在比散熱功能部J還要靠近電極支撐棒17B側,設有僅由沿著圓周方向之凹槽所構成之散熱構造50'(非塗層散熱構造)。Fig. 5 is a schematic plan view of electrodes of a discharge lamp according to a second embodiment. The
例如因為燈之低輸出、電極之尺寸較小等之理由,被形成於尖端側錐形部32之塗層44',其有時可抑制因為有電弧或火炬等,而剝落或消失之情形。因此,於軀幹部34之外,尖端側錐形部32也形成有塗層44',藉此,可提高散熱性。而且,與第1實施形態同樣地,於形成有塗層44'之散熱構造40'與散熱構造50'之間,也可以設置電極基材面之領域。For example, the coating 44' formed on the tapered
在第1、第2實施形態中,雖然藉沿著圓周方向之凹槽以構成散熱構造,但是,其也可以藉沿著電極軸向之凹槽以構成之。又,也可以採用凹槽以外之散熱構造。例如也可以以由噴砂等所做之梨皮粗糙面、黑化抑制體等,構成散熱構造。只要如果將黑化抑制作為主要目的時,採用黑化抑制體,如果要求提高散熱性時,構成凹槽即可。如果要求低成本時,可以採用梨皮粗糙面。只要因應電極形狀、電極素材、切削等之加工容易性等,以決定散熱構造即可。In the first and second embodiments, although the heat dissipation structure is formed by grooves along the circumferential direction, it may also be formed by grooves along the axial direction of the electrodes. Also, heat dissipation structures other than grooves may be used. For example, a pear skin rough surface, blackening suppressor, etc. made by sandblasting or the like may be used to form a heat dissipation structure. If blackening suppression is the main purpose, a blackening suppressor may be used, and if improvement in heat dissipation is required, grooves may be formed. If low cost is required, pear skin rough surface can be used. It is only necessary to determine the heat dissipation structure according to the shape of the electrode, the electrode material, and the ease of processing such as cutting.
又,為了防止被形成於散熱構造上之塗層之剝落,也可以將素材不同之塗層,作為散熱構造以構成之。亦即,可在塗層(散熱構造)上,重疊塗層。In addition, in order to prevent peeling of the coating layer formed on the heat dissipation structure, it is also possible to form a coating layer of a different material as the heat dissipation structure. That is, it is possible to overlay the coating on the coating (radiation structure).
10:放電燈 30:電極 40:散熱構造 42:凹槽 44:塗層 50:散熱構造(非塗層散熱構造) 10: discharge lamp 30: electrode 40: Heat dissipation structure 42: Groove 44: coating 50: Heat dissipation structure (non-coated heat dissipation structure)
圖1為第1實施形態之放電燈之俯視圖。 圖2為第1實施形態之電極之示意俯視圖。 圖3為表示凹槽之形狀與塗層之發射率之相關關係之表之圖。 圖4為表示凹槽形狀之圖。 圖5為第2實施形態之放電燈的電極之示意俯視圖。 Fig. 1 is a plan view of a discharge lamp according to a first embodiment. Fig. 2 is a schematic plan view of the electrodes of the first embodiment. Fig. 3 is a diagram showing a table showing the correlation between the shape of the groove and the emissivity of the coating. Fig. 4 is a diagram showing the shape of grooves. Fig. 5 is a schematic plan view of electrodes of a discharge lamp according to a second embodiment.
17B:電極支撐棒 17B: electrode support rod
30:電極 30: electrode
32:尖端側錐形部 32: Tip side taper
32S:錐形側面 32S: tapered sides
32T:電極尖端面 32T: electrode tip face
33:側面部分 33: side part
33P:邊界部 33P: Boundary
34:軀幹部 34: Torso
34S:側面 34S: side
34T:基材表面 34T: substrate surface
40:散熱構造 40: Heat dissipation structure
42:凹槽 42: Groove
42P:頂部 42P: top
44:塗層 44: coating
50:散熱構造(非塗層散熱構造) 50: Heat dissipation structure (non-coated heat dissipation structure)
Claims (11)
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JP2021091627A JP2022184023A (en) | 2021-05-31 | 2021-05-31 | Discharge lamp and method of manufacturing electrode for discharge lamp |
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