TW484165B - Low-power high-pressure sodium lamp - Google Patents

Low-power high-pressure sodium lamp Download PDF

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Publication number
TW484165B
TW484165B TW086112316A TW86112316A TW484165B TW 484165 B TW484165 B TW 484165B TW 086112316 A TW086112316 A TW 086112316A TW 86112316 A TW86112316 A TW 86112316A TW 484165 B TW484165 B TW 484165B
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Taiwan
Prior art keywords
pressure
lamp
xenon
nano
discharge tube
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TW086112316A
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Chinese (zh)
Inventor
Wolfram Dr Graser
Dieter Dr Schmidt
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Patent Treuhand Ges Fuer Elektrische Gluehlampen Mbh
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Priority claimed from DE19640850A external-priority patent/DE19640850A1/en
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Publication of TW484165B publication Critical patent/TW484165B/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/82Lamps with high-pressure unconstricted discharge having a cold pressure > 400 Torr
    • H01J61/825High-pressure sodium lamps
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/12Selection of substances for gas fillings; Specified operating pressure or temperature
    • H01J61/16Selection of substances for gas fillings; Specified operating pressure or temperature having helium, argon, neon, krypton, or xenon as the principle constituent
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/30Vessels; Containers

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  • Discharge Lamp (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)
  • Vessels And Coating Films For Discharge Lamps (AREA)
  • Secondary Cells (AREA)
  • Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)

Abstract

The low-power high-pressure sodium discharge lamp described here is distinguished by a very high xenon cold filling pressure of at least one bar. The pressure ratio relative to the sodium operating pressure is between 10 and 30. As a result, light efficiencies of approximately 100 lm/W and higher can be achieved for a lamp power of 50 to 100 W.

Description

484165 Α7 Β7 五、發明説明(1 ) 坊術镅城 本發明肇始於一種根據申請專利範圍第1項所載之高 壓鈉放電燈,此處所載的特別是•一種具備有最多100瓦的 功率和很高的氙氣氣壓的的高膣納燈,大致地,這種燈 有一個由氧化鋁做成的圓柱形的放電管,其係容納於一 傾透明的外管內。 g铀坊術 高壓納放電燈設計的基本特徵,早已熟知於一長時間 。同樣地,在這些燈內使用氙氣配合相對地高壓,Μ便 增加照明效率亦已热知於一段時間了,例如,被DEGR00T /VAH VLIET(飛利浦技術圖書館,Deventer, 1986)敘逑 於相關專題論文”高壓納燈”中第299和300頁•提到增加 發光效率10到15X是可能的,只要一在俗稱的超级燈泡 中一使用20到40kPa(200到400nb)的氙冷充壓,取代原 來約30ib的標準充壓即可達到。 經濟部中央標準局員工消費合作社印製 ----------------訂 (請先閱讀背面之注意事項再填寫本頁) 同時,第299頁亦指出在高壓納燈中的照明效率會随 著下降的燈功率而陡然地減低,即使在增氙壓的情況下 ,一個50瓦的燈泡功率其照明效率最多為85流明/瓦(U/ W),而一個約400瓦的燈泡功率,其照明效率約可達到 138U/W。 DE-C 26 00 35 1敘述一個無汞高壓納燈特別適合俗稱 的自穩定操作,它有個PNaB = 4到93nb的納工作壓力,氣 工作壓力PXe(熱)2 sooiBb,且歷力比PNaB / PXe(熱)^ 1/20。考處常用的因素8 (看DE_C 28 14 882,第2行 -3 - _本紙張Λ度適用中國國家標準(CNS ) A4規格(210X297公釐) 484165 A7 B7 五、發明説明(2484165 Α7 Β7 V. Description of the invention (1) Fang Shucheng This invention originated from a high-pressure sodium discharge lamp according to item 1 of the scope of patent application. Especially contained here is a kind of power with a maximum of 100 watts And high xenon pressure high krypton lamps. Generally, this lamp has a cylindrical discharge tube made of alumina, which is housed in a transparent outer tube. The basic characteristics of high-pressure nano-discharge lamp design have been well known for a long time. Similarly, the use of xenon gas in these lamps with relatively high pressure has increased the efficiency of lighting for some time. For example, it was described by DEGR00T / VAH VLIET (Philips Technology Library, Deventer, 1986) on related topics. Papers 299 and 300 in the paper "High-Voltage Sodium Lamps" • It is mentioned that it is possible to increase the luminous efficiency by 10 to 15X, as long as one is in a so-called super-bulb and one uses 20 to 40kPa (200 to 400nb) of xenon cold charge and replaces The original standard pressure of about 30ib can be achieved. Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs ------- Order (Please read the precautions on the back before filling this page) At the same time, page 299 also states that The lighting efficiency in the lamp will decrease sharply with the decrease of the lamp power. Even under the condition of increasing the xenon pressure, the lighting efficiency of a 50-watt bulb power is up to 85 lumens / watt (U / W), while an approx. With a 400-watt bulb power, its lighting efficiency can reach about 138U / W. DE-C 26 00 35 1 describes a mercury-free high-pressure sodium lamp that is particularly suitable for commonly known self-stable operation. It has a PNaB = 4 to 93nb nanometer working pressure, a gas working pressure PXe (heat) 2 sooiBb, and a calendar power ratio PNaB. / PXe (Hot) ^ 1/20. Factors commonly used in examinations 8 (see DE_C 28 14 882, line 2 -3-_ This paper Λ degree applies Chinese National Standard (CNS) A4 specification (210X297 mm) 484165 A7 B7 V. Description of the invention (2

經濟部中央標準局員工消費合作社印製 中間)Μ便於S工作壓力與.®冷充壓PXeK間做轉換_ _ 因而形成一壓力比Pv^/P =2.5,自稱宙協作% Ώ XeE NaB 曰》疋跺作的目 的是去操作一個沒有安定器的高壓納燈。這個操作彳莫@ 需要一個由填充氣體形成的電漿的長衰減時間,&amp; 7達 到此長衰減時間,係使用K 一熟知之方式,即,:$:胃;(:目 當高之氙壓和相當大之放電管内徑(同時參 GROOT/VAN VLIET第126頁和154頁所述的相關專題冑&amp; &gt; 。根據DE GRIOT/VAN VLIET第15 5頁,高壓納燈的自穩 定操作,未發現有任何實際上的應用,主要原因是啟酸j 及系統電壓突然變動的問題。 在DE-C 26 00 35 1舉例描述的高壓纳燈,有400 W高功 率和很大的内徑7.6mm、氣冷充歷是26〇1&amp;1)且壓力比Ργ λβΚ / PNaB約為3.5 。结果,對400W的高功率而言,一個僅 有1101m /tf的發光效率是可達到的。這個參考例子,與 其他的高壓納燈相比,既不針對也未達到特別高的發光 效率。根據 DE GR00T/VAN VLIET .的第 10、18 圖(第 29 9 頁) ,對一個400W的功率而言,發光效率高到138U/W是可 能的。發光效率與燈泡功率有關的這個原理,為了比較 的目的,這裡再一次地Μ第3圖說明。(參閱下文) 一個沒有自穩定功能的無汞高壓納燈描述於DE-B 28 14 882,以此類型而言,氙冷充壓PXeK對納的工作壓力 PNaB的參考值被建議如下式·· ^^〈PxeK /PNaB〈6,PNaB=150至 5 00 毫巴(mb) PXeK / PNaF的壓力比值,依照DE-C 26 00 3 5 1所描述。 一 4一 (請先閲讀背面之注意事項再填i頁) .裝· ’τ -線· 杰纸張尺度適用中國國家標準(CNS ) Μ規格(210X 297公釐) 484165 A7 : μ, ^ ^ΓΆ(^ _______Β7 j彻長-_ 五、發明説明(5 ) 無論如何,DE-B 28 14 88?(第3行,第41f列)中忠告 需遊免增加過多的氙壓而超過這個上限值,因為 述缺點:使起動闲難卻未增加照明效率^ 於一典型實施例中,一個70和100瓦的低功率燈,其Printed in the middle of the Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs) M is convenient for switching between S working pressure and .Cold-charging PXeK _ _ thus forming a pressure ratio Pv ^ / P = 2.5, claiming to be a% of the collaboration of the Ώ XeE NaB said " The purpose of the operation is to operate a high-pressure sodium lamp without a stabilizer. This operation does not require a long decay time of the plasma formed by the filling gas. &Amp; 7 to achieve this long decay time, using a well-known method of K, that is: $: stomach; (: eye when high xenon And the relatively large inner diameter of the discharge tube (see also the related topics described in pages 126 and 154 of GROUP / VAN VLIET 胄 & &gt;. According to DE GRIOT / VAN VLIET page 15 5), the self-stable operation of high-pressure nano-lamps No actual application has been found, the main reason is the problem of the sudden change of the voltage and the system voltage. The high-voltage sodium lamp described in DE-C 26 00 35 1 has 400 W high power and a large inner diameter. 7.6mm, air cooling charge is 2601 &amp; 1) and pressure ratio Pγ λβκ / PNaB is about 3.5. As a result, for high power of 400W, a luminous efficiency of only 1101m / tf can be achieved. This Reference example, compared with other high-voltage nano-lamps, it neither targets nor achieves a particularly high luminous efficiency. According to DE GR00T / VAN VLIET. Figures 10 and 18 (page 29 9), for a 400W power, In other words, it is possible that the luminous efficiency is as high as 138U / W. Luminous efficiency and the function of the lamp The related principle is illustrated again in Figure 3 for comparison purposes. (See below) A mercury-free high-pressure nano-lamp without a self-stabilizing function is described in DE-B 28 14 882. In this type, The reference value of the working pressure PNaB for xenon cold charge PXeK to sodium is suggested as follows: ^^ <PxeK / PNaB <6, PNaB = 150 to 5 00 mbar (mb) PXeK / PNaF pressure ratio, according to DE- As described in C 26 00 3 5 1. One four one (please read the precautions on the back before filling in page i). Installation · 'τ-line · Jie paper size applies Chinese National Standard (CNS) Μ specifications (210X 297 public (Centi) 484165 A7: μ, ^ ^ ΓΆ (^ _______ Β7 j 长长 -_ V. Description of the Invention (5) In any case, the advice in DE-B 28 14 88? (Row 3, column 41f) does not require excessive increase. The xenon pressure exceeds the upper limit because of the disadvantages mentioned below: making starting difficult but not increasing the lighting efficiency ^ In a typical embodiment, a low power lamp of 70 and 100 watts, which

= 230lDb,®冷充壓約500mb。其對應的P / P= 230lDb, ® cold charging pressure is about 500mb. Its corresponding P / P

XeK NaB 壓力比約為2到2· 5。因此,對一個70瓦或100瓦的功率 而言,其發光效率分別可達97或105流明/瓦Πη/ν)。 這些值以打” X ”標於第3圖,Κ便於比較。 發明無;怵 本發明的目的是為了提供一種低功率高壓納燈,如申 請專利範圍第1項之所載,其具有高發光效率。 此目的可藉由申請專利範圍第1項所述的特性來達成 。特別是在依附項之申請專利範圍中發現一些有益的改 善。 低功率高壓納燈,根據本發明其放電管(或稱發光管) 至少含有納及氙。在此狀況下,低功率是可理解的,尤 其是小於或等於1〇〇瓦的燈泡功率。 經濟部中央標準局員工消費合作社印製 在本案例中PKaB是鈉的工作充壓,PXeK是氙的冷充壓 。令人驚訝地,如果Ρ_Β = 20到100毫巴(mb)且PXeK = 1 到5 巴,並且PXeK / PNaB 2 1 〇的條件亦同時被滿足; .則本低功率案例與先前提高的燈泡對照,其發光效率可 增加20¾ ,壓力比PXeK / PNaff介於10到30之間是較有利 的。 可Μ將汞加入燈泡内以增加工作電壓。 -5 - 本紙張尺度適用中國國家標隼(CNS) Α4規格(210Χ 297公釐) 484165 A7 B7 五、發明説明(4 ) 氙壓超過先前已知有著高氙壓的高壓納燈(例如NAV 超级燈,產自OSRAH)其慣用值的3到10的比率。在此 狀況下的结果是發光效率比NAV超級燈增加20J!。 先前已提及Μ增加氙壓來提高高壓納燈的發光效率的 方法(參閲 DE GR00T/VAN VLIET,第 153 頁及第 299-300 頁),在商業上已使用於俗稱的NAV超级(SUPER)燈上 。然而,本發明W增加比NAV-SUPER燈泡還多的氙壓來 達到發光效率提升的目的,其發光效率的增加是意外的 高且到未被知道的程度。因此,例如一涸比俗稱標準燈 泡(有30ab的氛冷充壓)的發光效率高出10到15個百分 比,其相關的氙冷充壓需增加到200到400nb,這敘述於 DE GR00T/VAN VLIET的第300頁。此項更進一步的壓力 增加是被排除的,因為其將使啟動更加困難。 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 本發明的燈泡,令人驚訝的特質是根據已知業務狀態 的特殊用途,除了迄今未被專家納入考慮以外。當然, 它昃已知的一高壓納燈的發光效率明顯地減少對低燈泡 功率而言(DE GR00T/VAH VLIET,第299頁;參閲第3 圖下方)。這項定則是由於低燈泡功率的環境,其輻射 效率更低且電極損失比高燈泡功率高;然而這種解釋是 不正確的。這基本的理由寧可說明放電弧熱損耗的構成 要素有如燈泡功率的一部分,隨著燈泡功率的下降而變 大。而氙在充壓的高壓狀態下可被看成一種媛衝氣體, 使得熱損耗因氙的低熱傳導而降低。這影響作用在發光 效率上更有利於比較小的燈泡功率。在此倩形,氙和鈉 -6 - 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 484165 A7 f 1本撕十月w B7 * 五、發明説明( 經濟部中央標準局員工消費合作社印製 的壓 傳導 對小 顯而 至 外, 1 . bb 延 到 更 2 .高 元 〇 很 更 3, K 產生 對於 的變 前已 ,氙 電壓 點的 力比絕 性。相 功率下 易見的 少1巴 還有更 較少的 長使用 原來存 高的功 氙壓存 件的蒸 這種效 高的氣 加顯而 本發明 相當的 納,在 動或製 知的所 原子對 實際上 溫度所 填加汞 對是重要的,既為相對於氙,納有一高的熱 對於納壓,氙壓愈高,熱損耗的防制愈好。 增加發光效率而言,最後這個方式的效果是 (冷壓)的很高氙氙壓, 多的好處: 熱損耗會使得放電管的 壽命。另外,放電管能 在的壁溫。在這種情形 率密度而增加。 在著擴散性。這將減低 發,導致在電極區間的 應在NAV SUPER燈泡上已 壓情形下,導致使用壽 易見的。 的情形而言,由於它的 貢獻。這個貢獻與放電 室溫時氙是以氣體形式 造誤差,這將有穩定的 有燈泡的情形(例如, 工作電壓的貢獻是不大 僅取決於納原子的數量 影響,及被系統電壓的 的情形,汞添加物亦扮 -7 - 除了可增加發光效率 壁溫相對較低,因而 被降低,使得又再達 ,發光效率亦是隨著 在啟動作業期間電極 放電管壁可減少發黑 經數量化成已知。在 命更加延長的结果是 很高氙壓對工作電壓 管溫度無關,.因為相 存在。對於系统電壓 效應。相對於此,先 根據 DE-B 28 14 8δ2) 的。那些燈泡的工作 ,它是強烈地被最冷 變動或製造誤差所影 演锺定工作電壓的角 I---------批衣------1Τ------手 /、身/ -· (請先閱讀背面之注意事項再填頁) 本紙張尺度適用中國國家標隼(CNS ) Α4規格(210Χ 297公釐)The XeK NaB pressure ratio is approximately 2 to 2.5. Therefore, for a power of 70 watts or 100 watts, the luminous efficiency can reach 97 or 105 lumens / watt (ηη / ν), respectively. These values are marked "X" in Figure 3 for easy comparison. The invention is not; 的 The object of the present invention is to provide a low-power high-voltage sodium lamp, which has high luminous efficiency, as described in item 1 of the patent application scope. This objective can be achieved by the characteristics described in the first patent application. In particular, some beneficial improvements were found in the scope of patent applications under the dependent items. According to the present invention, the discharge tube (or light-emitting tube) of a low-power high-pressure nano-lamp contains at least nano- and xenon. Under this condition, low power is understandable, especially lamp power less than or equal to 100 watts. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs In this case, PKaB is the working pressure of sodium, and PXeK is the cold pressure of xenon. Surprisingly, if P_B = 20 to 100 millibar (mb) and PXeK = 1 to 5 bar, and the conditions of PXeK / PNaB 2 1 〇 are also satisfied at the same time; then this low power case is compared with the previously improved bulb , Its luminous efficiency can be increased by 20¾, the pressure ratio is more favorable between PXeK / PNaff between 10 and 30. Mercury can be added to the bulb to increase the operating voltage. -5-This paper size is applicable to China National Standard (CNS) A4 (210 × 297 mm) 484165 A7 B7 V. Description of the invention (4) The xenon pressure exceeds the previously known high-pressure nanolamps with high xenon pressure (such as NAV Super Lamp, produced by OSRAH) with a ratio of 3 to 10 of its customary value. The result in this situation is a 20J! Increase in luminous efficiency over NAV superlights. The method of increasing the xenon pressure to increase the luminous efficiency of high-pressure nano-lamps has been mentioned previously (see DE GR00T / VAN VLIET, pages 153 and 299-300), and has been commercially used in the commonly known NAV super (SUPER ) On the light. However, the present invention increases the xenon pressure more than the NAV-SUPER bulb to achieve the purpose of improving the luminous efficiency, and the increase of the luminous efficiency is unexpectedly high and to an unknown level. Therefore, for example, the luminous efficiency of a lamp is 10 to 15% higher than that of a commonly known standard bulb (with a 30ab atmosphere cold charge), and the related xenon cold charge pressure needs to be increased to 200 to 400nb, which is described in DE GR00T / VAN VLIET p. 300. This further pressure increase is ruled out as it will make startup more difficult. Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs (please read the notes on the back before filling this page). The surprising characteristic of the light bulb of the present invention is that it is based on a special purpose of a known business state, except that it has not been considered by experts so far other than. Of course, it does not significantly reduce the luminous efficiency of a known high-voltage nanolamp for low lamp power (DE GR00T / VAH VLIET, page 299; see below figure 3). This rule is due to the low lamp power environment, which has lower radiation efficiency and higher electrode losses than high lamp power; however, this interpretation is incorrect. This basic reason would rather explain that the components of arcing heat loss are like a part of the power of the bulb, and become larger as the power of the bulb decreases. Xenon can be regarded as a kind of priming gas under the high pressure state of charge, so that the heat loss is reduced due to the low heat conduction of xenon. This effect is more beneficial to the light efficiency of smaller bulbs. Here, xenon and sodium-6-This paper size is applicable to Chinese National Standard (CNS) A4 (210X297 mm) 484165 A7 f 1 this tear October B7 * V. Description of invention (Employees of Central Bureau of Standards, Ministry of Economic Affairs The piezoconductor printed by the consumer cooperative goes to the small display, 1. bb is extended to 2. high, 〇 is more 3, K produces the right before the change, the force of the xenon voltage point is absolute. Phase power is easier Seeing less than 1 bar and less, using the original high-energy xenon pressure storage steam, this highly efficient gas is obvious, and the present invention is quite acceptable. The addition of mercury to the temperature is important. It means that compared to xenon, there is a high heat to the nanometer. The higher the xenon pressure, the better the prevention of heat loss. In terms of increasing luminous efficiency, the effect of this last method is (Cold pressure) high xenon xenon pressure, many benefits: heat loss will make the life of the discharge tube. In addition, the wall temperature that the discharge tube can be in. In this case the rate density increases. In the diffusion. This will Reduced hair, causing NAV SUPER lights in the electrode section In the case of pressure on the bubble, it is easy to see the use of the case, due to its contribution. This contribution is different from the discharge of xenon in the form of gas at room temperature, which will have a stable situation with a bulb (such as The contribution of the working voltage is not only determined by the number of nanoatoms and the system voltage. Mercury additives also play a role of -7-in addition to increasing the luminous efficiency, the wall temperature is relatively low, so it is lowered. In addition, the luminous efficiency is also known as the amount of blackening of the electrode discharge tube wall can be reduced during the start-up operation. The result of a longer life is that the high xenon pressure has nothing to do with the working voltage tube temperature, because the phase exists. For the effect of system voltage. In contrast, first according to DE-B 28 14 8δ2). For the work of those bulbs, it is strongly influenced by the coldest fluctuation or manufacturing error. ----- Approve clothes ------ 1Τ ------ hand /, body /-· (Please read the precautions on the back before filling in the page) This paper size applies to China National Standard (CNS) Α4 size (210 × 297 mm)

V 484165 A7 B7丨_ 丨修上 經濟部中央標準局員工消費合作社印製 五、發明説明(6 ) 色ο 4,燈泡工作中,很高的氙壓產生特別低的重新啟動峰值 ,這會延長燈泡使用壽命因電極的點火器負載,且提供 更高的安全性Μ防止因系統電壓的突然變動而損壞。 5·在鈉的光譜中,氙會影響納共表線(d線)的光譜輪靡 中的峰值間距變寬,它會受壓力影響而變寬且在它的中 心會自我吸收。這個影響原則上已知(看DE GROOT/VAN VUET,特別是第16a·圖版1C)。结果,納壓能被減低 與相同的色溫度及色顯示相關連。這個效應徹底地作用 在有著至少1巴(冷)的很高氙壓的情形下。在本發明的 倩形中,相對於氙壓,納壓尤其寧可設定低一點,Μ致 於共振線兩翼的峰值間距典型值為lOnm,最多則為12nm 。在這情形的基本先決條件是選擇壓力比PXeK / pNaB ^ 10且P d=20到lOOmb。在這些條件下,最佳發光效率的 產生已經顯現了,相對地,規範於DE-B 28 14 882條件 下的情況,其鈉D線兩翼的峰值間距至少1 5到2 0 n m ,因 為PNaB是相對地高(看上面)。藉由規範於DE GR00T/VAN VLIET, 87頁(3.28)式的幫胯,這可被評估出來。 第3和5項為選擇低工作壓力提供額外的辯解,本發 明典型的納蒸氣壓為20到lOOrab 。在這方面,低納壓有 許多好處: 1.在納蒸氣壓在20到lOOmb的情形下,放電管在最冷點 的溫度僅是840到950k 。最冷點總垦在密閉層附近, 密閉層150k的溫度是比先前已知的燈泡情形更冷(看 一 8- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公釐) I---------^------訂------線 η 1'\ (請先閱讀背面之注意事項再填頁) 484165 A7 __B7 五、發明説明(7 ) DE-B 28 14 882); 2.由納所引起的放電管壁的腐蝕,它寧可發生在管中央 (請先閲讀背面之注意事項再填寫本頁) ,腐蝕會因低納偏壓而減低。结果又是一種使用礴命 的改善。 在DE-B 28 14 882中所提及,對於損害啟動能力的這 項缺點,在低燈泡功率的情況下,藉由改善商業上使用 的燈帽、燈座及啟動裝置,Μ及氙壓不要太高(5barsK 上),則缺點可有效地防止。氙壓限制在3barsM內是較 有利的。這些改善的零件已經使用於商用的金靥鹵化燈 從OSRAH (例如HQI-E 100W/NDL及tfDL),相對地,根據 本發明燈泡的情形,對NAV燈泡而言,使用平常的啟動 裝置要達成啟動是不可能的。 與DE-C 26 00 351相反的,這裡敘述的燈泡既不意圖 亦不適合自穩定操作。在這個倩形,根據本發明之氙的 工作壓力亦是在8到24bars間,比該處所規範的典型值 1.8bars 堪高。 經濟部中央標準局員工消費合作社印製 在DE-C 26 00 351中所提及,放電管的熱在啟動時是 必要的,(另一,一個平常的安定器能被使用),但在 本發明的放電管的情形是不需要的。根據本發明,放電 管寧可有一個附著物(鈮管在頭端打開),藉由已知的 方法,即在高壓填加入氙氣,填加作業完成後再密封起 來,這個方法是可能的。 和納及氙一樣,根據本發明的燈泡,特別能另加汞於 填充物中。發光效率的增加是類似加或不加汞添加物的 一 9 - _本紙逄尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 484165 A7 _____B7__ 五、發明説明.(8 ) 燈泡光度。一個填充汞添加物的典型燈泡使用含納18X 比重的汞合金。 放電管的內徑寧可介於2.5到5hii之間,特別是最多 4mB 。自穩定性是排除於最初被給的這些尺寸大小。利 用比較的方式,規範在DE-C 26 00 351的內徑是比10的 整數次方大。雖然放電管通常是一圓柱體,但也可以有 不同的幾何形狀,例如有一個凸出物在中間。 高壓納燈另外一個好處是有一個電容式啟動輔肋器, 例如沿著放電管的導線。與DE-C 26 00 351對照,根據 本發明的燈泡是不需要預熱的。 這些燈泡通常有附加一個鈮管,有如先前敘述過的, 例如,DE GR00T/VAM VLIET的第 251頁,第8 、 30圖。 如此燈泡能使一個平常的或哼常被用的電子安定器來 操作。 這裡所談的放電管使用圓柱形或橢圓形的外管較好。 圖式簡屋說明_ 本發明藉由下面多個典型實施例來解釋,於圖式中·· 第1圖顯示一高壓納燈; 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 第2圖顯示具有不同氙氣壓(不管是杏含汞)的各高壓 納燈(每個燈有50瓦功率)的發光效率比;以及 第3圖顯示有不同燈泡功率及不同氙壓的各高壓納燈 的發光效率比。 顯示於第1圖的高壓納燈具有50瓦功率,其內有一個 由氧化鋁製成的放電管1 。放電管置於一個由硬質玻璃 本紙張尽度適用中國國家標準(CNS ) A4規格(210X297公釐) 484165 :修正&gt; Α7 ή- 年亡月一日 B7丨補充一 五、發明説明(9 ) 經濟部中央樣準局員工消費合作社印製 做成的圓柱形外管2内,兩.端分別由燈帽3 封於内。外管2是抽成真空。 兩個相距30毫米的電極4 ,分別位於内徑 放電管1的兩端。距離燈帽較遠的第一電極 一個管狀鈮襯套丨5和一附著器6 ,再連接到一引 7連接到一個固體的外部饋電線8 ,此接通 帽3的一個接觸點。 第二個電極4同樣地穿過一個鈪襯套5 ( 器)連接到一個金屬導線15。後者經由一個 到燈帽3的第二個接觸點。 放電管内裝配一個電容式起動輔助裝置, 一個沿著放電管的起動導線17形成。起動導 傳導方式連接到第二電極4 。 例如,一個燈泡經由燈帽内的起動器電路 2 20伏特(V)的交流電壓糸統,則其起動電 (kV) 〇 放電管2内包含一個僅由納及氙氣姐成的 的冷充壓(PXeK )是3巴(bar),而納的工作 是 100 毫巴(mb),结果 PXeK / PNaB = 3 0。 這個燈泡可達到5100流明Um)的光通量及 瓦的發光效率(參閱第2圖,位於3000毫巴 處的實心三角形測量點#1)。與這燈泡相比 瓦燈泡有著300毫巴的氙冷充壓(超级型) 4200流明的光通量及相對應的81流明/瓦的 及頂罩 密 3 . 3毫米的 4 ;是穿過 線7 ,引線 放電管到燈 不需用附著 導體16連接 該裝置是由 線17是K電 連接到一個 壓是4仟伏 充填物。氙 充® ( P船B ) 102流明/ 的氙冷充壓 ,先前的50 ,只能達到 發光效率 (請先閲讀背面之注意事項再填寫本頁) 訂 線 11- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公釐) 484165 A7 __B7_ 五、發明説明(10 ) (參閲第2圖,空心的三角型測量點)。第2圖也標示 出,常見的最多lOOmb低氙壓的更進步的燈泡(標準型) ,其發光效率合計約70流明/瓦在30mb的氙壓下(參閲 第2圖,空心三角形測量點)。 第3圖槪要地說明照DE GROOT/VAN VLIET的方法,發 光效率在燈泡功率上的依存性。由上面範例(1021«/W 對50瓦的燈泡功率而言)是被Κ菱形測量點標示出來。 很清楚地係在習知技術之上方。 在第2典型實施例中,相同設計的燈泡僅工作於一個 巴的氙壓及50毫巴的納壓。其比率是ΡχβΚ/ PFaB =20, 參閲第2圖,在95流明/瓦那實心三角形測量點#2,對 應到的氙冷充壓是1000毫巴,其發光效率實事上仍然比 先前已知的燈泡高。因為比較低的氣壓,使得其比第一 典型實施例更容易啟動。起動電壓是3k V。 這兩個燈泡特別適合具有更強啟動裝置的新裝置。 經濟部中央標準局員工消費合作社印製 (請先閲讀背面之注意事項再填寫本頁) 在第3典型實施例中,相同設計的50瓦燈泡中,另外 加填水銀,其主要目的是為製成汞合金,此汞合金含有 18¾的納,其餘皆為水銀。這燈泡展現了 105流明/瓦 的發光效率(第2園中,實心圓形測量點#3) ·相藺連 的氙冷充壓是2毫巴,納工作壓力為80毫巴,其壓力比 PXeK / PNaB = 2 5 · 0 〇 相當地,第4典型實施例(50瓦),有著1巴的氙冷充 壓及其相關連的同一納/汞(Na/Hg)比,展琨93流明/ 瓦的發光效率(第2圖中,實心圓形測量點林4)。 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 484165 * A7 _ B7 五、發明説明(11 ) 包含汞及有一個較低的氙冷充壓(超鈒型和標準型) 的鈉氣燈,為了比較,它們的發光效率同樣地標示出來 (在第2圖中,空心圓形測量點為了 30毫巴至300毫巴 間)〇 在第5典型實施例中,一個基本上類似的燈泡,其工 作於63瓦的功率。其充填物包含1巴的氙及50奄巴的納 ,但不含水銀。壓力比是Pvy/PiTTi=20,發光效率是V 484165 A7 B7 丨 _ 丨 Reprinted by the Consumers Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs. 5.Invention Note (6) Color ο 4. In the operation of the lamp, the high xenon pressure produces a particularly low restart peak, which will prolong the lamp. The service life is due to the load of the electrode's igniter, and it provides higher safety to prevent damage due to sudden changes in system voltage. 5. In the spectrum of sodium, xenon will affect the broadening of the peak distance in the spectral cycle of the nanocommon line (d line), it will be widened by the pressure and it will absorb itself in its center. This effect is known in principle (see DE GROOT / VAN VUET, especially 16a · Plate 1C). As a result, the nano-pressure can be reduced in association with the same color temperature and color display. This effect works thoroughly at very high xenon pressures of at least 1 bar (cold). In the case of the present invention, the nano-pressure is more preferably set lower than the xenon pressure, and the typical peak distance between the two wings of the resonance line is lOnm, which is at most 12 nm. The basic prerequisites in this case are to select a pressure ratio PXeK / pNaB ^ 10 and Pd = 20 to 100mb. Under these conditions, the production of the optimal luminous efficiency has already appeared. In contrast, under the conditions of DE-B 28 14 882, the peak distance between the two wings of the sodium D line is at least 15 to 20 nm, because PNaB is Relatively high (see above). This can be evaluated with help as specified in DE GR00T / VAN VLIET, page 87 (3.28). Items 3 and 5 provide additional justification for choosing a low working pressure. Typical nano vapor pressures of the present invention are 20 to 100rab. In this regard, the low nano-pressure has many advantages: 1. The temperature of the discharge tube at the coldest point is only 840-950 k at a nano-vapor pressure of 20 to 100 mb. The coldest spot is always near the airtight layer, and the temperature of the airtight layer 150k is colder than the previously known bulb situation (see 8- This paper size applies the Chinese National Standard (CNS) A4 specification (210X 297 mm) I- -------- ^ ------ Order ------ line η 1 '\ (Please read the notes on the back before filling in the page) 484165 A7 __B7 V. Description of the invention (7) DE -B 28 14 882); 2. Corrosion of the wall of the discharge tube caused by the nanometer, it would rather occur in the center of the tube (please read the precautions on the back before filling this page). The corrosion will be reduced due to the low nanometer bias. The result is another improvement in the use of fatality. As mentioned in DE-B 28 14 882, for the disadvantage of impairing the starting ability, in the case of low lamp power, by improving the lamp caps, lamp holders and starting devices used commercially, M and xenon pressure should not be Too high (over 5barsK), the disadvantages can be effectively prevented. It is advantageous to limit the xenon pressure to 3 barsM. These improved parts have been used in commercial gold halide halogen lamps from OSRAH (such as HQI-E 100W / NDL and tfDL). In contrast, according to the situation of the bulb of the present invention, for NAV bulbs, the usual starting device is used to achieve Starting is impossible. In contrast to DE-C 26 00 351, the bulbs described here are neither intended nor suitable for self-stable operation. In this case, the working pressure of xenon according to the present invention is also between 8 and 24 bars, which is higher than the typical value of 1.8 bar in the space. As mentioned in DE-C 26 00 351 printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs, the heat of the discharge tube is necessary at startup (another, a normal stabilizer can be used), but in this The situation with the inventive discharge tube is not necessary. According to the present invention, the discharge tube preferably has an attachment (the niobium tube is opened at the head end). This method is possible by a known method, that is, adding xenon gas under high pressure filling and sealing after the filling operation is completed. As with nano and xenon, the bulb according to the present invention is particularly capable of adding mercury to the filling. The increase in luminous efficiency is similar to that with or without the addition of mercury. 9-_ The paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) 484165 A7 _____B7__ 5. Description of the invention. (8) Light intensity of the bulb. A typical bulb filled with mercury additives uses an amalgam containing 18X specific gravity. The inner diameter of the discharge tube is preferably between 2.5 and 5hii, especially up to 4mB. Self-stability is excluded from these sizes given initially. By means of comparison, the inner diameter of the standard in DE-C 26 00 351 is larger than the integer power of 10. Although the discharge tube is usually a cylinder, it can also have different geometries, such as a protrusion in the middle. Another benefit of high-pressure nano-lamps is the presence of a capacitive starting rib, such as along the wires of a discharge tube. In contrast to DE-C 26 00 351, the lamp according to the invention does not require preheating. These bulbs usually have a niobium tube attached, as described previously, for example, DE GR00T / VAM VLIET, page 251, pages 8 and 30. In this way, the lamp can be operated by an ordinary or humming electronic ballast. The discharge tube discussed here preferably uses a cylindrical or oval outer tube. Brief description of the drawings _ The present invention is explained by the following typical embodiments. In the drawing, the first figure shows a high-voltage sodium lamp; printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the back Note: Please fill in this page again.) Figure 2 shows the luminous efficiency ratio of each high-pressure sodium lamp (each lamp has 50 watts of power) with different xenon gas pressure (regardless of apricot containing mercury); And the luminous efficiency ratio of each high pressure nano lamp with different xenon pressure. The high-voltage nanolamp shown in Fig. 1 has a power of 50 watts and contains a discharge tube 1 made of alumina. The discharge tube is placed on a hard glass paper that applies the Chinese National Standard (CNS) A4 specification (210X297 mm) as much as possible. 484165: Amendment &gt; Α7 ή- The first day of the month B7 丨 Supplement 15, Invention Description (9) Inside the cylindrical outer tube 2 printed by the employee's cooperative of the Central Procurement Bureau of the Ministry of Economic Affairs, the two ends are sealed inside by the lamp cap 3 respectively. The outer tube 2 is evacuated. Two electrodes 4 separated by 30 mm are located at both ends of the inner diameter discharge tube 1 respectively. The first electrode farther from the lamp cap is a tubular niobium bush 5 and an attacher 6, which is then connected to a lead 7 connected to a solid external feeder 8, which connects a contact point of the cap 3. The second electrode 4 is also connected to a metal wire 15 through a cymbal bush 5 (connector). The latter passes a second contact point to the lamp cap 3. The discharge tube is equipped with a capacitive starting aid, and one is formed along the starting wire 17 of the discharge tube. The starter is conductively connected to the second electrode 4. For example, if a light bulb passes an AC voltage system of 20 volts (V) through the starter circuit 2 in the lamp cap, its starting electricity (kV) is contained in the discharge tube 2. The discharge tube 2 contains a cold charge voltage made of only nano and xenon. (PXeK) is 3 bar, and the work of nano is 100 millibar (mb), the result is PXeK / PNaB = 30. This bulb can achieve a luminous flux of 5100 lumens (Um) and a luminous efficiency of watts (see Figure 2, solid triangular measurement point # 1 at 3000 mbar). Compared with this bulb, the watt bulb has a 300 mbar xenon cold charge (super type), a luminous flux of 4200 lumens and a corresponding 81 lumens / watt and a top cover density of 3.3 mm; 4 is through the line 7, The lead discharge tube to the lamp does not need to be connected by an attached conductor 16. The device is electrically connected by wire 17 to K to a 4 volt filling. Xenon Charge® (P Boat B) 102 lumens / xenon cold charge pressure, the previous 50, can only reach the luminous efficiency (please read the precautions on the back before filling this page) Alignment 11- This paper size applies to Chinese national standards (CNS) A4 specification (210X 297 mm) 484165 A7 __B7_ 5. Description of the invention (10) (refer to Figure 2, hollow triangular measuring point). Figure 2 also shows that a more advanced bulb (standard type) with a low xenon pressure of up to 100 mb, which has a total luminous efficiency of about 70 lumens / watt at a xenon pressure of 30 mb (see Figure 2, hollow triangle measurement points) ). Figure 3 illustrates the dependence of the light emission efficiency on the lamp power according to the method of DE GROOT / VAN VLIET. The example above (1021 «/ W for a 50 watt bulb power) is marked by a K diamond measurement point. Clearly tied above the know-how. In the second exemplary embodiment, the bulb of the same design works only with a xenon pressure of one bar and a nanopressure of 50 mbar. Its ratio is PχβΚ / PFaB = 20. Refer to Figure 2. At 95 lumens / Wana solid triangle measurement point # 2, the corresponding xenon cold charge pressure is 1000 mbar, and its luminous efficiency is actually better than previously known. Light bulb is high. The relatively low air pressure makes it easier to start than the first exemplary embodiment. The starting voltage is 3k V. These two bulbs are particularly suitable for new devices with stronger starting devices. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling out this page) In the third exemplary embodiment, the same design of a 50-watt light bulb is additionally filled with mercury. Form amalgam, this amalgam contains 18¾ nanometer, the rest is mercury. This bulb exhibits a luminous efficiency of 105 lumens / watt (in the second circle, a solid circular measurement point # 3) · The connected Xenon cold charge pressure is 2 mbar, the nano working pressure is 80 mbar, and the pressure ratio is PXeK / PNaB = 2 5 · 0 〇 Equivalently, the fourth exemplary embodiment (50 watts) has a cold filling pressure of xenon of 1 bar and its associated same nanometer / mercury (Na / Hg) ratio, showing 93 lumens / Watt luminous efficiency (Figure 2, solid circular measuring point Lin 4). This paper size applies to the Chinese National Standard (CNS) A4 specification (210X297 mm) 484165 * A7 _ B7 V. Description of the invention (11) Contains mercury and has a low xenon cold charge pressure (super krypton type and standard type) Sodium gas lamps, for comparison, their luminous efficiencies are also marked out (in the second figure, the hollow circular measurement point is between 30 mbar and 300 mbar). In the fifth exemplary embodiment, one is basically similar Light bulb, which works at a power of 63 watts. Its filling contains 1 bar of xenon and 50 奄 of sodium, but contains no mercury. The pressure ratio is Pvy / PiTTi = 20, and the luminous efficiency is

XeK NaB 98流明/瓦,這個燈泡可想像成一個具有125瓦功率的 高壓水銀燈的代用品,其有相同的光通量。這燈泡有一 功率降低電路(相位-閫控制,及一啟動電路於燈帽中)。 在一個35瓦燈泡的第6典型實施例中,一個內徑3.3 毫米的放電管,其內電極相距23毫米,且僅充入納及氙 氣。氙冷充壓是PXeK = 2bars,且納工作壓力是PNaB = 90iBb ,因此,壓力比是PXeK/PFaB=22.2。發光效率是98流 明/瓦(參閱第3圖,菱形測量點#6)且實質上比琨有 的同功率燈泡的預期要高。 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 第7典型實施例是一個70瓦的燈泡,其放電管的內徑 為3.3毫米且電極間距為36毫米,放電管內充滿納/汞 汞合金(參閲上述)及氙壓。氙冷充壓是PXeK =2barS, 納工作壓力是PKaB =75«ab。壓力比必然是PXeK / PNaB = 26.7。發光效率是115流明/瓦(參閱第3圖,菱形測 量點#7),此實質上比原先預期在這種功率燈泡下的狀 況要高。 一個70瓦燈泡的第8典型實施例,其放電管的内徑為 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公釐) 484165 修正XeK NaB 98 lumens / watt, this bulb can be imagined as a substitute for a high-pressure mercury lamp with 125 watts of power, which has the same luminous flux. This bulb has a power reduction circuit (phase-chirp control, and a start-up circuit in the lamp cap). In a sixth exemplary embodiment of a 35 watt light bulb, a discharge tube with an inner diameter of 3.3 mm has internal electrodes spaced 23 mm apart and is filled with only nano and xenon. Xenon cold charge pressure is PXeK = 2bars, and the nano-working pressure is PNaB = 90iBb. Therefore, the pressure ratio is PXeK / PFaB = 22.2. The luminous efficiency is 98 lumens / watt (see Figure 3, diamond-shaped measurement point # 6) and is substantially higher than expected for some of the same power bulbs. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling out this page) The 7th exemplary embodiment is a 70-watt light bulb with an inner diameter of the discharge tube of 3.3 mm and an electrode spacing of 36 mm The discharge tube is filled with nano / mercury (see above) and xenon pressure. Xenon cold charge pressure is PXeK = 2barS, and the nano working pressure is PKaB = 75 «ab. The pressure ratio must be PXeK / PNaB = 26.7. The luminous efficiency is 115 lumens / watt (see Figure 3, diamond measurement point # 7), which is substantially higher than originally expected under this type of power bulb. The eighth exemplary embodiment of a 70-watt light bulb, the inner diameter of the discharge tube is the paper size applicable to the Chinese National Standard (CNS) A4 specification (210X 297 mm) 484165 amendment

AVAV

Β7 /ifrXT 五、發明説明(I2 ) 3.7毫米且電極間距為37毫.米,放電管内充滿納/汞及 氙壓。氙冷充壓是PXeK = 1.5bars,鈉工作壓力是 = 85mb,壓力比必然是PXeK/PNaB=17.6,發光效率是 1 0 8流明/瓦。 元件符號對照表:Β7 / ifrXT 5. Description of the invention (I2) 3.7 mm and electrode spacing is 37 mm.m. The discharge tube is filled with nano / mercury and xenon pressure. Xenon cold filling pressure is PXeK = 1.5bars, sodium working pressure is 85mb, the pressure ratio must be PXeK / PNaB = 17.6, and the luminous efficiency is 108 lumens / watt. Component symbol comparison table:

Im, 訂 線 „ ... (請先閱讀背面之注意事項再填象於頁) 經濟部中央標準局員工消費合作社印製 一 14一 1 放電管 2 國柱形外管 3 燈帽 4 電極 5 管狀鈮襯套 6 附著器 7 引線 8 固體外部饋電線 9 頂罩 15 金屬導線 16 導體 17 起動導線 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐)Im, ordering line ... (Please read the precautions on the back before filling in the page) Printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 1-14 1 Discharge tube 2 National cylindrical outer tube 3 Lamp cap 4 Electrode 5 Tubular niobium bushing 6 Attachment 7 Lead 8 Solid external feeder 9 Top cover 15 Metal wire 16 Conductor 17 Starter wire This paper size applies to China National Standard (CNS) A4 (210X297 mm)

Claims (1)

484165 丨修正 六、申請專利範圍 第86 1 123 16號「低功率之高壓鈉燈」專利案(90年11月修正) 六申請專利範圍 1. 一種低功率之高壓納燈,具有一個放電管,其內至少含 有鈉及氙壓,PNaB表示鈉的工作充壓,而PXeK表示氙的冷 充壓,其特徵爲: Ρν“ = 20 到 lOOmb; PxeK:=l到3巴;以及 10‘PXeK/ PNaB‘30 ;且 該燈的功率小於或等於1〇〇瓦(w)。 2·如申請專利範圍第1項之高壓納燈,其中PxeK/pNaBs3〇。 3·如申請專利範圍第1項之高壓納燈,其中pXeK$3巴。 4·如申請專利範圍第1項之高壓納燈,其中該充塡物另含 有录。 5·如申請專利範圍第1項之高壓納燈,其中該放電管係一 圓柱體。 6.如申請專利範圍第5項之高壓納燈,其中該放電管之內 部直徑係於2.5和5毫米之間。 7·如申請專利範圍第6項之高壓納燈,其中該放電管之內 部直徑最大4毫米。 8·如申請專利範圍第1項之高壓納燈,其中該燈另含一電 容式啓動輔助器。 9.如申請專利範圍第1項之高壓納燈,其中在操作期間, 鈉之D-線兩翼的峰値間距最大是I2nm。484165 丨 Amendment VI. Patent Application No. 86 1 123 16 "Low-Power High-Pressure Sodium Lamp" Patent Case (Amended in 1990) 6. Application for Patent Scope 1. A low-power high-pressure sodium lamp with a discharge tube, which Contains at least sodium and xenon pressure, PNaB represents the working charge pressure of sodium, and PXeK represents the cold charge pressure of xenon, which is characterized by: ρν "= 20 to 100mb; PxeK: = 1 to 3 bar; and 10'PXeK / PNaB '30; and the power of the lamp is less than or equal to 100 watts (w). 2. If the high voltage nano lamp of the scope of the patent application, the PxeK / pNaBs 30. 3. The high voltage of the scope of the patent application Nano-lamps, of which pXeK $ 3 bar. 4. If the high-voltage nano-lamps of the first patent application range, the charging material contains additional records. 5. If the high-voltage nano-lamps of the first patent application range, the discharge tube is A cylinder. 6. The high-pressure nano lamp according to item 5 of the patent application, wherein the internal diameter of the discharge tube is between 2.5 and 5 mm. 7. The high-voltage nano lamp according to item 6 of the patent application, where the The maximum internal diameter of the discharge tube is 4mm. High-pressure sodium lamp, in which the lamp also contains a capacitive start-up aid. 9. For example, in the high-voltage sodium lamp in the scope of patent application, the peak-to-ridge distance between the two wings of the sodium D-line is at most I2nm during operation.
TW086112316A 1996-10-02 1997-08-27 Low-power high-pressure sodium lamp TW484165B (en)

Applications Claiming Priority (1)

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DE19640850A DE19640850A1 (en) 1996-10-02 1996-10-02 Low power sodium high pressure lamp

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Publication number Priority date Publication date Assignee Title
DE3842771A1 (en) * 1988-12-19 1990-06-21 Patent Treuhand Ges Fuer Elektrische Gluehlampen Mbh HIGH PRESSURE DISCHARGE LAMP OF SMALL ELECTRICAL POWER AND METHOD FOR OPERATING
US5434472A (en) * 1992-04-15 1995-07-18 United States Philips Corporation High-pressure sodium discharge lamp with getter

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