JPS6222221B2 - - Google Patents
Info
- Publication number
- JPS6222221B2 JPS6222221B2 JP54090182A JP9018279A JPS6222221B2 JP S6222221 B2 JPS6222221 B2 JP S6222221B2 JP 54090182 A JP54090182 A JP 54090182A JP 9018279 A JP9018279 A JP 9018279A JP S6222221 B2 JPS6222221 B2 JP S6222221B2
- Authority
- JP
- Japan
- Prior art keywords
- arc tube
- tube
- metal
- metal halide
- efficiency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- 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
Landscapes
- Discharge Lamps And Accessories Thereof (AREA)
Description
本発明は、メタルハライドランプに関し、その
効率と光色むらを改良するようにしたものであ
る。
メタルハライドランプの発光管内には、高効率
でかつ白色光が得られるように金属ハロゲン化物
が選択されて封入されている。金属ハロゲン化物
は、ランプ点灯中、飽和蒸気圧になるように蒸発
する量よりも余分に封入されている場合が多く、
未蒸発の金属ハロゲン化物は、液状となつて発光
管の最下部か最低温度部に凝縮している。垂直点
灯する場合、通常の発光管の下側電極後方部に凝
縮する。その結果、金属ハロゲン化物が高温にさ
らされず、十分な蒸気圧が得られないために、効
率が低下するとともに、電極後方部温度のばらつ
きによつてランプ間で蒸気圧の差が生じて光色む
らを発生する。
この不都合をなくすため、従来は、電極周囲の
発光管外壁に金属酸化膜を設けたり、金属キヤツ
プで包囲したりする等の保温手段が採られていた
が、十分ではなかつた。発光管は外管内に収納さ
れ、外管内部には保護ガスが封入されているが、
メタルハライドランプが点灯されると、外管内の
保護ガスは、発光管からの熱伝導によつて温度が
上昇し対流を起こす。すなわち、発光管管壁に触
れた高温の保護ガスは、上側に移動し、外管内壁
に触れて温度が低下して下側に移動し、再び発光
管に触れて高温となるような対流を起こす。しか
るに、対流によつて外管内壁に触れて冷却された
保護ガスが、再び発光管管壁に触れるとき、発光
管の下側電極周囲の外壁付近を冷却する。従来の
上記のような金属酸化膜や、金属キヤツプでは、
この対流による冷却作用の影響を受けやすく保温
手段として十分ではなかつた。
なお、対流による発光管の下側電極周囲の外壁
付近の冷却作用の対策として、本発明者は先に、
点灯時下側となる発光管封止部に透光性熱遮蔽
板、例えばマイカ板を配設することを提案した。
しかしながら、マイカ板の耐熱温度は550〜750℃
であり、それ以上の温度では結晶水の分解が始つ
て、水分を放出して脆くなる。水分の放出によつ
てメタルハライドランプの始動電圧が高くなり、
またマイカ板が脆くなつて封止部に対する固定が
困難となつてくる。このため、100W程度の低ワ
ツトメタルハライドランプでは透光性熱遮蔽板と
してマイカ板を使用することは可能であるが、
400W、1000W以上になると、耐熱性の点で十分
ではなくなり使用が困難である。また、耐熱ガラ
スは封止部への固定保持が困難でかつ機械的強度
も十分でない。
本発明は、上記不都合に鑑みてなされたもので
あり、効率と光色むらを十分に改良し得るメタル
ハライドランプを提供するものである。
以下本発明の一実施例を図面とともに説明す
る。
図において、発光管1の内部にはナトリウム、
タリウム、インジウム等のハロゲン化物が封入さ
れ、その両端部には電極2,3が封止られてい
る。両電極はそれぞれステム線4,5に電気的に
接続されている。発光管1に接近するステム線5
には、よく知られた光電子放出による発光管外へ
のナトリウム消失を防ぐため、碍子管や石英管等
の絶縁性保護管6が被覆されている。下側電極3
の周囲の発光管管壁には保温膜7が塗布され、ま
た発光管1の両端部に形成された封止部のうち点
灯時下側となる封止部、すなわち下側電極が封止
られた封止部8には、発光管軸とほぼ直角方向に
金属熱遮蔽板9たとえばニツケル、ステンレス等
の円板がこれから切起して形成されたタブ10を
介して、絶縁性保護管6に取りつけられた止め金
11に溶接されている。金属熱遮蔽板9は、発光
管1の外径をd(mm)としたとき、その最長部巾
D(mm)が1〜2.5dとなる大きさのものである。
発光管1は窒素、ネオン−窒素等の不活性ガスの
保護ガスを封入した外管(図示しない)内に設け
られる。
かかる構成のメタルハライドランプは、D/d
が上記のような範囲になる金属熱遮蔽板を点灯時
下側となる発光管1の封止部8には発光管の管軸
とほぼ直角方向に配設しているので、発光管1の
光を遮断することなく、外管内の保護ガスの対流
による下側電極3周囲の発光管1管壁の冷却作用
の悪影響を受けず、保温効果を著しく向上して、
効率および光色むらを改良することができる。
また、金属熱遮蔽板9は、電気的遊離状態にあ
るので、光電子または電位差によつて発光管1内
の封入物を電気的に誘引することなく、常に安定
した封入物組成となつてアークが安定する。
そして、実験により上記メタルハライドランプ
の効率および光色むら等の改良は、金属熱遮蔽板
の最長部巾D(mm)と発光管の外径d(mm)との
関係が重要であることがわかつた。
すなわち、発光管外径21.5mm、電極間距離41mm
で、端部外壁にグラフアイトの保温膜を塗布した
発光管内にナトリウム、タリウム、インジウムの
沃化物を封入した図示構造の400Wメタルハライ
ドランプについて、金属熱遮蔽板として円板形状
のニツケル板を用い、このニツケル板の外径を
種々変えて、効率および光色むら等の効果を調べ
たところ、第1表に示すような結果が得られた。
なお、光色むらは色温度のばらつきで評価し、ま
た金属熱遮蔽板による影の有無は、ランプ単体3
mの直下で直径1mの円の照射面の照度を測定
し、金属遮蔽板なしの場合を100としたときの照
度相対値比較で評価したものである。
The present invention relates to a metal halide lamp, and its efficiency and light color unevenness are improved. A metal halide is selected and sealed in the arc tube of a metal halide lamp so as to produce white light with high efficiency. Metal halides are often sealed in excess of the amount that evaporates to reach the saturated vapor pressure during lamp operation.
The unevaporated metal halide becomes a liquid and condenses at the lowest or lowest temperature part of the arc tube. When lighting vertically, it condenses at the rear of the lower electrode of a normal arc tube. As a result, the metal halide is not exposed to high temperatures and sufficient vapor pressure cannot be obtained, resulting in a decrease in efficiency, and differences in vapor pressure between lamps occur due to variations in temperature at the rear of the electrode, resulting in light color. Causes unevenness. In order to eliminate this inconvenience, heat insulating means such as providing a metal oxide film on the outer wall of the arc tube around the electrode or surrounding it with a metal cap have been conventionally used, but these measures have not been sufficient. The arc tube is housed in an outer tube, and a protective gas is sealed inside the outer tube.
When a metal halide lamp is lit, the temperature of the protective gas inside the outer bulb increases due to heat conduction from the arc tube, causing convection. In other words, the high-temperature protective gas that touches the wall of the arc tube moves upward, touches the inner wall of the outer tube, lowers its temperature, moves downward, and then touches the arc tube again, creating a convection current that increases the temperature. wake up However, when the protective gas that has been cooled by contacting the inner wall of the outer tube due to convection comes into contact with the wall of the arc tube again, it cools the vicinity of the outer wall around the lower electrode of the arc tube. With conventional metal oxide films and metal caps as mentioned above,
It is susceptible to the cooling effect of this convection and is not sufficient as a heat retention means. In addition, as a measure against the cooling effect of the outer wall around the lower electrode of the arc tube due to convection, the present inventor previously proposed the following:
We proposed that a translucent heat shielding plate, such as a mica plate, be placed in the sealing part of the arc tube, which is the lower side when the lamp is lit.
However, the heat resistance temperature of mica board is 550 to 750℃.
At higher temperatures, crystallization water begins to decompose, releasing moisture and becoming brittle. Due to the release of moisture, the starting voltage of the metal halide lamp increases,
Furthermore, the mica plate becomes brittle and becomes difficult to fix to the sealing portion. For this reason, it is possible to use mica board as a translucent heat shielding plate in low-wattage metal halide lamps of around 100W, but
When it exceeds 400W or 1000W, it becomes difficult to use because the heat resistance is insufficient. Further, heat-resistant glass is difficult to securely hold in the sealing portion and does not have sufficient mechanical strength. The present invention has been made in view of the above-mentioned disadvantages, and it is an object of the present invention to provide a metal halide lamp that can sufficiently improve efficiency and light color unevenness. An embodiment of the present invention will be described below with reference to the drawings. In the figure, inside the arc tube 1 is sodium,
A halide such as thallium or indium is sealed, and electrodes 2 and 3 are sealed at both ends. Both electrodes are electrically connected to stem wires 4 and 5, respectively. Stem wire 5 approaching arc tube 1
is covered with an insulating protective tube 6 such as an insulator tube or a quartz tube to prevent sodium from disappearing outside the arc tube due to well-known photoelectron emission. Lower electrode 3
A heat insulating film 7 is applied to the wall of the arc tube around the arc tube 1, and of the sealing parts formed at both ends of the arc tube 1, the lower sealing part when lit, that is, the lower electrode is sealed. A metal heat shielding plate 9, for example, a disc made of nickel, stainless steel, etc., is inserted into the insulating protective tube 6 through a tab 10 formed by cutting and cutting a metal heat shielding plate 9 into the sealing portion 8 in a direction substantially perpendicular to the arc tube axis. It is welded to the attached clasp 11. The metal heat shielding plate 9 has a width D (mm) at its longest part of 1 to 2.5 d, where d (mm) is the outer diameter of the arc tube 1 .
The arc tube 1 is provided within an outer tube (not shown) filled with a protective gas such as nitrogen, neon-nitrogen, or other inert gas. A metal halide lamp with such a configuration has a D/d
A metal heat shielding plate whose temperature is within the above range is installed in the sealing part 8 of the arc tube 1, which is on the lower side during lighting, in a direction almost perpendicular to the tube axis of the arc tube. Without blocking the light, without being adversely affected by the cooling effect of the wall of the arc tube 1 around the lower electrode 3 due to the convection of the protective gas inside the outer tube, the heat retention effect is significantly improved.
Efficiency and light color unevenness can be improved. Furthermore, since the metal heat shielding plate 9 is in an electrically free state, the inclusions in the arc tube 1 are not electrically attracted by photoelectrons or potential difference, and the composition of the inclusions is always stable and the arc is generated. Stabilize. Experiments have shown that the relationship between the longest width D (mm) of the metal heat shield plate and the outer diameter d (mm) of the arc tube is important for improving the efficiency and light color unevenness of the metal halide lamp. Ta. In other words, the outer diameter of the arc tube is 21.5 mm, and the distance between electrodes is 41 mm.
For a 400W metal halide lamp with the structure shown in which sodium, thallium, and indium iodides are sealed in an arc tube whose end outer wall is coated with a graphite heat-retaining film, a disk-shaped nickel plate is used as the metal heat shield. When the outer diameter of this nickel plate was varied and the effects on efficiency, light color unevenness, etc. were investigated, the results shown in Table 1 were obtained.
In addition, the unevenness of light color is evaluated by the variation in color temperature, and the presence or absence of shadows due to the metal heat shield plate is evaluated based on the lamp itself.
The illuminance of a circular irradiation surface with a diameter of 1 m was measured directly below the irradiation surface, and the evaluation was made by comparing the relative value of the illuminance when the case without a metal shielding plate was set as 100.
【表】
第1表に示すごとく、試料1は円板なし(試料
6)と効率等の諸特性がほとんど変らず、改良効
果がなかつた。試料2は効率が85lm/Wに上昇
し、また色温度のばらつきも4000〜4600Kと少な
くなり、照度相対値は102となつて影は存在しな
かつた。試料3、4は効率が84.5lm/Wに上昇
し、また色温度のばらつきも4000〜4500Kとさら
に少なくなり、照度相対値はそれぞれ99および98
とわずかに低下したが、影の存在はほとんど目視
できなかつた。試料5は色温度は4000〜4500Kで
改善されたが、効率が79lm/Wに低下し、また
照度相対値も90となつて影がはつきりと目視され
た。また、投光器との組合せでも影は解消できな
かつた。
また、発光管外径18.5mm、電極間距離60mmにつ
いてもD/dを変えて実験したところ、同じよう
な結果が得られた。
また、金属熱遮蔽板は円形以外に6角形、8角
形等の多角形その他でもよい。
なお、反射形水銀ランプにおいて、反射形硝子
管のトツプ部の熱を下げる目的で採用されている
ように、発光管から離れた位置に金属熱遮蔽板を
配設した場合は、効率および光色むら等の改良が
行なえなかつた。
なお、特公昭41−2865号公報に提案されている
メタルハライドランプは、発光管を保温するため
に、発光管を囲繞するガラス筒との組合せで反射
性遮蔽板を設けてなるものであり、本発明のよう
に、対流による発光管の下側端部の冷却作用を阻
止するものとは目的が全く異なる。また、この構
造では、反射性遮蔽板が電気的に遊離されておら
ず、これには常に電位が印加されており、したが
つて光電子および電位差によつて、発光管内の封
入物が誘引されて発光管外に消失されるという不
都合がある。
以上説明したように、本発明は、外管内に封入
する保護ガスの対流による冷却を防止して、発光
管最低温度部の温度を上昇させ、発光管からの光
を遮断することなく、効率および光色むら等を防
止することのできるメタルハライドランプを提供
することができる。[Table] As shown in Table 1, Sample 1 had almost no difference in various properties such as efficiency compared to the sample without the disk (Sample 6), and there was no improvement effect. In sample 2, the efficiency increased to 85 lm/W, the variation in color temperature decreased to 4000 to 4600 K, the relative illuminance value was 102, and there was no shadow. For samples 3 and 4, the efficiency increased to 84.5lm/W, the color temperature variation was further reduced to 4000-4500K, and the relative illuminance values were 99 and 98, respectively.
However, the presence of the shadow was almost invisible. In sample 5, the color temperature was improved from 4000 to 4500K, but the efficiency decreased to 79 lm/W, and the relative illuminance value also became 90, so that shadows were clearly visible. Furthermore, even when used in combination with a floodlight, shadows could not be eliminated. Further, similar results were obtained when an experiment was conducted by changing D/d with an arc tube outer diameter of 18.5 mm and an electrode distance of 60 mm. Furthermore, the metal heat shielding plate may be polygonal, such as hexagonal or octagonal, other than circular. In addition, if a metal heat shield plate is installed at a position away from the arc tube, as in the case of reflective mercury lamps, which is used to reduce the heat at the top of the reflective glass tube, the efficiency and light color will be reduced. It was not possible to improve unevenness, etc. The metal halide lamp proposed in Japanese Patent Publication No. 41-2865 has a reflective shielding plate in combination with a glass tube surrounding the arc tube to keep the arc tube warm. The purpose is completely different from that of the invention, which prevents the cooling effect of the lower end of the arc tube by convection. In addition, in this structure, the reflective shielding plate is not electrically isolated and a potential is always applied to it, so that the inclusions in the arc tube are attracted by photoelectrons and potential difference. There is an inconvenience that the light is lost outside the arc tube. As explained above, the present invention prevents cooling of the protective gas sealed in the outer bulb by convection, increases the temperature of the lowest temperature part of the arc tube, and improves efficiency without blocking light from the arc tube. It is possible to provide a metal halide lamp that can prevent light color unevenness and the like.
図は本発明の一実施例であるメタルハライドラ
ンプの要部正面図である。
1……発光管、2,3……電極、8……封止
部、9……金属熱遮蔽板。
The figure is a front view of essential parts of a metal halide lamp which is an embodiment of the present invention. 1... Arc tube, 2, 3... Electrode, 8... Sealing part, 9... Metal heat shielding plate.
Claims (1)
物が封入された発光管と、前記発光管を内蔵し内
部に保護ガスが封入された外管と、前記発光管の
両端部に形成された封止のうち点灯時下側となる
封止部のみに、この発光管の管軸とほぼ直角方向
に電気的に遊離状態でもつて配設された金属熱遮
蔽板とを具備し、前記金属熱遮蔽板の最長部巾D
(mm)とし、前記発光管の外径をd(mm)とする
とき、Dとdとの比D/dを1〜2.5としたこと
を特徴とするメタルハライドランプ。1. An arc tube equipped with electrodes at both ends and a metal halide sealed inside, an outer tube containing the arc tube and filled with a protective gas, and a seal formed at both ends of the arc tube. Only the sealed portion of the arc tube, which is on the lower side when lit, is provided with a metal heat shield plate that is disposed in an electrically free state in a direction substantially perpendicular to the tube axis of the arc tube, and the metal heat shield Width at the longest part of the board D
(mm) and the outer diameter of the arc tube is d (mm), the ratio D/d of D and d is 1 to 2.5.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9018279A JPS5615551A (en) | 1979-07-16 | 1979-07-16 | Metal halide lamp |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9018279A JPS5615551A (en) | 1979-07-16 | 1979-07-16 | Metal halide lamp |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5615551A JPS5615551A (en) | 1981-02-14 |
| JPS6222221B2 true JPS6222221B2 (en) | 1987-05-16 |
Family
ID=13991338
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9018279A Granted JPS5615551A (en) | 1979-07-16 | 1979-07-16 | Metal halide lamp |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5615551A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| NL8101723A (en) * | 1981-04-08 | 1982-11-01 | Philips Nv | HIGH PRESSURE MERCURY DISCHARGE LAMP. 080481 HIGH PRESSURE DISCHARGE LAMP. |
| JPS5961277A (en) * | 1982-09-29 | 1984-04-07 | Toshiba Corp | Forming device of pattern |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51121276U (en) * | 1975-03-24 | 1976-10-01 |
-
1979
- 1979-07-16 JP JP9018279A patent/JPS5615551A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5615551A (en) | 1981-02-14 |
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