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JP3994658B2 - How to turn on the metal halide lamp - Google Patents
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JP3994658B2 - How to turn on the metal halide lamp - Google Patents

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Publication number
JP3994658B2
JP3994658B2 JP2000358633A JP2000358633A JP3994658B2 JP 3994658 B2 JP3994658 B2 JP 3994658B2 JP 2000358633 A JP2000358633 A JP 2000358633A JP 2000358633 A JP2000358633 A JP 2000358633A JP 3994658 B2 JP3994658 B2 JP 3994658B2
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Japan
Prior art keywords
power
lighting
lamp
metal halide
halide lamp
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JP2002164192A (en
Inventor
拓磨 橋本
淳典 岡田
真吾 東坂
和彦 酒井
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Panasonic Electric Works Co Ltd
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Matsushita Electric Works Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は、メタルハライドランプを点灯するメタルハライドランプの点灯方法に関するものである。
【0002】
【従来の技術】
メタルハライドランプは高輝度、高効率、高演色性という特長をもつことから幅広い分野で用いられている。一般的なメタルハライドランプには、ランプを始動させるための希ガスと、バッファガスの役割を果たす水銀と、所望の光を発する金属ハロゲン化物が封入されている。例えば、金属ハロゲン化物として、沃化ナトリウム、沃化タリウム、及び沃化インジウムが発光管に封入されたメタルハライドランプや、金属ハロゲン化物として沃化ナトリウム及び沃化スカンジウムが発光管に封入されたメタルハライドランプが広く利用されている。
【0003】
メタルハライドランプにおいては各金属の発光量が金属ハロゲン化物の蒸発量に依存するが、それぞれの蒸発量は発光管の最冷点の温度変化によって大きく影響を受ける。また、封入された水銀や金属ハロゲン化物毎に温度に対する蒸気圧特性が異なる。ゆえに、メタルハライドランプに供給する電力を定格値から変化させた場合、発光管最冷点の温度変化を受けて金属の発光量や色バランスが個々に変動するので、全体としての光色が大幅に変化してしまう。このような理由により、近年までは光色特性をほぼ一定に保ったままメタルハライドランプに供給する電力を変化させることにより光出力を自由に変化させる点灯(いわゆる調光点灯)の実現は困難との見方が有力であった。
【0004】
しかし、近年になって、このような光色の変化を低減させ、調光点灯を可能としたメタルハライドランプが考案されるようになってきた(例えば、特開平6−84496号公報、特開平6−111772号公報、あるいは特開平8−203471号公報参照)。
【0005】
【発明が解決しようとする課題】
しかしながら、従来のメタルハライドランプ点灯装置では、定格電力以下の電力をランプに供給して調光点灯を行うと、ランプ寿命が損なわれるのではないかとの危惧があった。現に米国では、既に調光点灯手段を備えたメタルハライドランプ用安定器が市販されており、ランプ寿命への影響を考慮し、調光点灯時のランプ電力を定格電力の50%以上にする、及び、始動時に最低15分間は定格電力で点灯を行う、との見解もあるが、この見解の根拠は必ずしも明確にはなっておらず、ランプ寿命に係る課題は残されたままとなっていた。
【0006】
本発明は上記事情に鑑みて為されたものであり、その目的とするところは、光束維持率に悪影響を与えずにランプ寿命を増大させることができるメタルハライドランプの点灯方法を提供することにある。
【0007】
【課題を解決するための手段】
請求項1の発明は、上記目的を達成するために、一対の電極が気密封入された透光性の容器内に金属ハロゲン化物、水銀、希ガスを封入してなるメタルハライドランプを点灯するメタルハライドランプの点灯方法において、定格電力と、定格電力以下であって定格電力による点灯時の光束維持率以上を確保する電力を点灯手段からメタルハライドランプに供給するとともに、前記点灯手段の供給する電力を変えてメタルハライドランプを始動した場合に、ランプに供給される電力を、略安定する電極温度の電力に対する変化割合が急変する変曲点の電力以上の電力とすることを特徴とし、調光点灯を行っても光束維持率が低下しないだけでなく、定格電力のみの点灯に比べて光束維持率をさらに高め、ランプ寿命を増大させることができる。
【0008】
また、請求項2の発明のように、記点灯手段より、始動から所定時間内に前記定格電力以下の電力をメタルハライドランプに供給することが望ましい。
【0009】
さらに、請求項の発明のように、前記点灯手段より、始動時から前記定格電力以下の電力をメタルハライドランプに供給することが望ましい。
【0010】
また、請求項の発明のように、前記点灯手段より、点灯中に前記定格電力以下の電力をメタルハライドランプに供給する時間を有することが望ましい。
【0011】
【発明の実施の形態】
以下、本発明を実施形態により詳細に説明する。
【0012】
(実施形態1)
上述したように、メタルハライドランプの調光点灯を行うとランプ寿命が低下するとの危惧があった。その理由は以下に述べる様に電極にあると考えられる。通常、メタルハライドランプの電極温度は、定格電力で点灯している際に、陰極時に熱電子が十分に放出し得る温度範囲になるような設計がなされている。しかしながら、調光点灯によって電極温度が低下しすぎると、以下に示すように陰極からの電子放出が不充分になる。
【0013】
陰極時の熱電子放出電流密度Jと、電極の絶対温度Tとの関係は、外部電界Eが印加された場合のリチャードソン-ダッシュマン式、
J=AT2exp{−φ/kT+(e/2kT)・(eE/πε0)1/2} (1)
を用いて表すことができる。
【0014】
上記式(1)において、Aは電極の材質や表面状態に依存する定数であり、φは電極の仕事関数、kはボルツマン定数、eは電荷素量、ε0は真空の誘電率である。式(1)において、外部電界Eが小さく、式(1)の指数部の第2項が第1項に比べて無視できるとする。この時、必要な電流密度Jを得るためには、電極温度には熱電子が放出し得る閾値T0が存在し、T>T0ではメタルハライドランプの点灯に必要な電流は容易に放出可能であるが、T<T0では実質的に電流密度J=0であることがわかる。従って、メタルハライドランプに供給する電力を低下させ過ぎると、電極温度が適正な温度範囲の下限T0よりも低下し、陰極時の熱電子放出が不充分になる。
【0015】
実際には、電極温度がT0以下に低下した場合であっても、陰極近傍の電界E(陰極降下電圧)が強まり、式(1)の指数部第2項が大きくなる(ショットキー効果の増大)ことにより、すぐに電流密度Jがゼロにはならない。また、電界Eが強まると、熱電子放出機構に加え、電界電子放出機構によって、陰極から電子が供給される可能性も考えられるので、電極温度がT0以下に下がってもある程度までは放電が維持されると考えられる。しかしその一方、陰極降下電圧が大きくなると、イオンの衝撃による電極物質の飛散(スパッタリング)の確率が増大すると考えられる。従って、電極温度がT0より低下した状態でメタルハライドランプを点灯した場合には、発光管の黒化が早期に生じ、定格電力のみの点灯に比べて光束維持率が低下する可能性が危惧される。さらに、発光管の黒化は点灯中の発光管温度の上昇を引き起こす。従って、定格電力のみの点灯に比べてランプ電圧の上昇や、発光管内部の不純物ガス濃度の上昇が早期に起こり、その結果、メタルハライドランプの不点灯が早期に生じることにより、ランプ寿命が低下する可能性が危惧される。
【0016】
米国において、ランプ寿命に悪影響を与えないためには、調光点灯時の電力は定格電力の50%以上にするとの見解がなされているのは、上記理由によると考えられる。しかし、熱電子放出が可能な電極温度範囲が、どのメーカのランプであっても、一律に定格電力の50%以上であるとは考え難く、50%という値の根拠は不明確である。そこで、ランプ毎に異なるであろう、ランプ寿命に悪影響が及ばない電力条件について規定できるようにするために、以下に述べる実験を実施した。
【0017】
熱電子放出が可能な電極温度の下限T0がわかれば、光束維持率に悪影響が及ばない電力条件も得られると考えられるが、上述したことから、T<T0における電流密度Jと電極温度Tの関係は、T>T0における電流密度Jと電極温度Tの関係とは異なったものになると考えられる。そこで、点灯維持が可能な電力範囲に対して、電流密度Jと電極温度Tの関係について調べれば、上記下限T0に関する知見が得られると考えた。しかし、メタルハライドランプの点灯中は安定器インピーダンスによる電流制限の下にあり、電流密度Jを直接計ることは困難である。そこで、電流密度Jの変わりにランプ電流で代用し、ランプ電流と電極温度Tの関係について調べた。その結果、光束維持率に悪影響を与えない電力範囲と電極温度Tとの関係が明らかになった。以下、本実験の過程と得られた結果とについて本発明の実施形態1として説明する。
【0018】
図1は本実施形態1を実現するための点灯装置の概略構成図である。ランプ1には松下電器産業株式会社製の400Wメタルハライドランプ(品番:M400・L/BU-SC-P)を用いた。点灯手段たる安定器2としては、定格電力又は定格電力以下であって定格電力による点灯時の光束維持率以上を確保する電力をランプ1に供給できる様に、種々のインピーダンスの安定器を試作して用いた。但し、本実施形態に用いたランプ1、安定器2の組み合わせは一例に過ぎず、特に本実施形態に限定されるものではない。
【0019】
本実施形態の点灯装置を用いて大きさの異なる種々の電力をランプ1に供給してランプ1を始動点灯させた。そして、ランプ1の点灯状態が安定した後における下側電極先端の、アーク端付近の電極表面温度をサーモグラフィ装置を用いて計測した。この様にして計測されたサーモグラフィ装置による相対的な電極温度を、ランプ電流及び電力に対してプロットし、ランプ電流、電力に対する電極温度の変化傾向を調べた結果を図2に示す。図2から明らかなように、全体的に見れば電力の低下とともに電極温度も低下する傾向を持つ。しかしながら、細かく見ると300W〜250Wにかけて変化の傾きが緩やかな領域がある。そして、この領域より低い電力では、供給電力に対する変化割合が急に大きくなっていることがわかり、約250W付近に変曲点が存在することがわかる。
【0020】
図2に見られるように、300W〜250Wにかけては電極温度があまり変化しなかった。この電力範囲における電極近傍の放電状態を観察したところ、陰極輝点の大きさは、電力の低下と共に小さくなった。このことから、この電力範囲においては、電極は熱電子を充分放出し得る温度にあり、電子放出部分の面積が変化することにより、放電維持に必要な電子が供給されていることがわかった。一方、変曲点(250W)以下の電力における電極近傍の放電状態を観察したところ、陰極輝点が不安定でランプ1にちらつきが生じていた。陰極輝点が安定しないことから、変曲点よりも低電力側では熱電子放出に充分な電極温度が得られていないことがわかった。従って、図2で見出された変曲点よりも低電力側ではランプ寿命に悪影響が及ぶ可能性が危惧される。
【0021】
そこで、上記実験結果から予想されること、すなわちランプ1に供給する電力が変曲点よりも高電力か低電力かということとランプ寿命との相関をみるために、ランプ1に供給する電力を400W(定格電力)、270W、及び210Wとし、同種のランプ1を試料に寿命試験を実施した。本寿命試験では一回の点灯時間を5時間30分とし、30分間消灯の後に再び5時間30分の点灯を行う点灯/消灯サイクルを繰り返し実施した。一定時間毎に試験を中断してランプ特性を計測し、その経時変化を調べた。その結果の一部を図3に示す。
【0022】
図3は各ランプ1の光束維持率を点灯時間に対してプロットしたものだが、270W>210W>400Wの順に光束維持率が高い値を示している。従って、定格電力以下の電力をランプ1に供給することには、ランプ1の光束維持率を損ねるどころか、場合によっては却って光束維持率を高める効果があることが見出された。その一方、270Wよりも210Wで点灯させたランプ1の方が、光束維持率が悪いという結果から、先に予想されたとおり、変曲点(250W)よりも低い電力領域では、光束維持率が低下に転じることが明らかになった。また、上述したように変曲点以下の電力においては、陰極輝点が不安定でランプ1にちらつきが見られ、点灯状態が不安定であった。これらのことから、図2で見出された変曲点以下の電力をランプ1に供給することは、定格電力のみの点灯に比べて光束維持率が改善された場合であっても、許容される点灯条件の中に含めるべきではないことが明らかになった。
【0023】
したがって、定格電力と、定格電力以下であって定格電力による点灯時の光束維持率以上を確保する電力をメタルハライドランプに供給可能な点灯手段たる安定器2を備えた本実施形態において、ランプ1に供給する電力を変えて始動した場合に、略安定した電極温度の、電力に対する変化割合が急変する変曲点の電力以上の電力を、安定器2からランプ1に供給すべき電力と規定することによって、調光点灯を行っても光束維持率が低下しないだけでなく、定格電力のみの点灯に比べて光束維持率をさらに高め、ランプ寿命を増大させることができる。
【0024】
(実施形態2)
ところで、既に説明したように、米国ではランプ寿命への影響を考慮して、始動の際には最低15分間は定格電力で点灯を行うとの見解がなされているが、その根拠として以下の理由が考えられる。すなわち、定格電力以下の電力でランプを始動させると、定格電力で始動した場合に比べて電極温度が安定するまでに時間を要する。そこで、この時間内における電極物質のスパッタリングによる発光管黒化の増長によって、光束維持率が低下するというのがその理由と考えられる。しかし、15分間という時間には然したる根拠が見出せない。また、調光点灯時の電力の如何にかかわらず、常に始動時にはランプに定格電力を供給しなければならいのかといった疑問が残る。そこで、調光点灯時の電力の如何にかかわらず、調光始動は常に避ける必要があるのか、もしも必要がある場合には、定格点灯を行う時間は何分間必要かを調べるために、以下に述べる実験を行った。
【0025】
図4は本実施形態の点灯方法を実現する点灯装置の概略構成図である。交流200Vの商用電源と安定器3とはスイッチ4を介する経路とスイッチ4を介さない経路で接続され、安定器3の出力側にランプ1が接続されている。而して、スイッチ4のオン・オフに応じて安定器3からランプ1に供給される電力が定格電力と、定格電力以下の電力とに切り換えられるようになっている。ここで、安定器3としては松下電工株式会社製400W水銀灯調光用安定器(品番:YZ40121433)を用いた。ランプ1には松下電器産業株式会社製の400Wメタルハライドランプ(品番:M400・L/BU-SC-P)を用いた。但し、本実施形態に用いた安定器3、ランプ1の組み合わせは一例に過ぎず、特に本実施形態に限定されるものではない。
【0026】
本実施形態においては、一回の点灯時間を5時間30分とし、30分間消灯の後に再び5時間30分の点灯を行う点灯/消灯サイクルを繰り返す形式の寿命試験を実施した。 本実施形態においては、一回の点灯時間内に定格電力またはそれ以下の電力を次のような時間条件の下にランプ1に供給した。
(a)定格電力(400W)で始動させ、点灯中も400Wの電力をランプ1に入力した。
(b)定格電力(400W)で始動させ、以後30分間は定格電力で点灯し、その後は270W電力をランプ1に入力した。
(c)定格電力(400W)で始動させ、以後15分間は定格電力で点灯し、その後は270Wの電力をランプ1に入力した。
(d)定格電力(400W)で始動させ、以後4分間は定格電力で点灯し、その後は270Wの電力をランプ1に入力した。
(e)270Wの電力で始動させ、点灯中も270Wの電力をランプ1に入力した。
【0027】
一定時間毎に試験を中断してランプ特性を計測し、その経時変化を調べた結果の一部を図5に示す。図5は、本実施形態に用いたランプ1の光束維持率の変化を示す図である。図5において曲線a〜eは上記条件(a)〜(e)に対応している。図5より、光束維持率はe≒d≒c>b>aの順に良いことがわかる。さらに、全てのランプ1は試験開始から数10時間の間に光量が5%程度低下したが、点灯条件(e)、(d)、(c)の下に点灯させたランプ1では、点灯100時間以後に光量の回復現象が見られたことがわかる。
【0028】
本実施形態においては、ランプ1に供給する定格電力以下の電力として270Wを用いたが、ランプ1に供給する定格電力以下の電力は特に本実施形態に限定されるものではなく、実施形態1で説明した電力範囲内にあれば、程度の差こそあれ、特にどの電力であっても同様の結果が得られることが確認できた。
【0029】
上述のようにランプ1を定格電力で点灯させ、かつ、所定時間内に定格電力以下の電力を供給させる、あるいは定格電力以下の電力でランプ1を始動させることにより、調光点灯を行っても光束維持率が低下しないだけでなく、定格電力のみの点灯に比べて、光束維持率をさらに高め、ランプ寿命を増大させることができる。
【0030】
(実施形態3)
本実施形態の点灯方法を実現する点灯装置の構成は実施形態2と同一であるから図示並びに説明は省略する。
【0031】
本実施形態においては、一回の点灯時間を5時間30分とし、30分間消灯の後に再び5時間30分の点灯を行う点灯/消灯サイクルを繰り返す形式の寿命試験を実施した。また、一回の点灯時間内に定格電力以下の電力で点灯する時間を0または2時間とし、定格電力またはそれ以下の電力を、次のような時間条件の下にランプ1に供給した。
(A)定格電力(400W)で始動させ、点灯中も400Wの電力をランプ1に入力した。
(B)定格電力(400W)で始動・点灯させたが、始動の1時間後から3時間後までの2時間は270Wの電力をランプ1に入力した。
(C)定格電力(400W)で始動・点灯させたが、始動の3時間30分後から点灯終了までの2時間は270Wの電力をランプ1に入力した。
(D)270Wの電力で始動・点灯させたが、始動の2時間後から点灯終了までの3時間30分は定格電力(400W)をランプ1に入力した。
【0032】
一定時間毎に試験を中断してランプ特性を計測し、その経時変化を調べた。その結果の一部を図6に示す。図6は、本実施形態に用いたランプ1の光束維持率の変化を示す図である。図6において曲線A〜Dは上記条件(A)〜(D)に対応している。図6より、上記(B),(C),(D)の光束維持率は同程度であり、共に条件(A)より優れていることがわかる。従って、定格電力のみの点灯を行った条件(A)に比べて、定格電力での点灯の合間に定格以下の電力での点灯を2時間行った条件(B),(C),(D)の方が光束維持率が増大していることがわかる。
【0033】
本実施形態においては、定格以下の電力で点灯する時間を2時間としたが、特に2時間に限定されるものではない。程度の差はあるものの、どのような時間であっても定格電力での点灯の合間に定格以下の電力での点灯を行うことによって、定格電力のみの点灯に比べて光束維持率が増大する効果が確認できた。
【0034】
また、本実施形態ではランプ1に供給する定格電力以下の電力として270Wを用いたが、ランプ1に供給する定格電力以下の電力は特に本実施形態に限定されるものではなく、実施形態1で説明した電力範囲内にあれば、程度の差こそあれ、特にどの電力であっても同様の結果が得られることが確認できた。
【0035】
上述のように点灯中に安定器3から定格電力以下の電力をランプ1に供給して点灯させる時間を設けることにより、調光点灯を行っても光束維持率が低下しないだけでなく、定格電力のみの点灯に比べて、光束維持率をさらに高め、ランプ寿命を増大させることができる。
【0036】
【発明の効果】
本発明は上述のように、一対の電極が気密封入された透光性の容器内に金属ハロゲン化物、水銀、希ガスを封入してなるメタルハライドランプを点灯するメタルハライドランプの点灯方法において、定格電力と、定格電力以下であって定格電力による点灯時の光束維持率以上を確保する電力を点灯手段からメタルハライドランプに供給するとともに、前記点灯手段の供給する電力を変えてメタルハライドランプを始動した場合に、ランプに供給される電力を、略安定する電極温度の電力に対する変化割合が急変する変曲点の電力以上の電力とするので、調光点灯を行っても光束維持率が低下しないだけでなく、定格電力のみの点灯に比べて光束維持率をさらに高め、ランプ寿命を増大させることができるという効果がある。
【図面の簡単な説明】
【図1】 本発明の実施形態1の点灯方法を実現するための点灯装置を示す概略構成図である。
【図2】 同上の説明図である。
【図3】 同上の寿命試験結果を示す図である。
【図4】 本発明の実施形態2の点灯方法を実現するための点灯装置を示す概略構成図である。
【図5】 同上の寿命試験結果を示す図である。
【図6】 本発明の実施形態3の寿命試験結果を示す図である。
【符号の説明】
1 メタルハライドランプ
2 安定器
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a method for lighting a metal halide lamp for lighting a metal halide lamp.
[0002]
[Prior art]
Metal halide lamps are used in a wide range of fields because of their high brightness, high efficiency, and high color rendering. A typical metal halide lamp contains a rare gas for starting the lamp, mercury that serves as a buffer gas, and a metal halide that emits desired light. For example, a metal halide lamp in which sodium iodide, thallium iodide, and indium iodide are enclosed in an arc tube as a metal halide, or a metal halide lamp in which sodium iodide and scandium iodide are enclosed in an arc tube as a metal halide. Is widely used.
[0003]
In the metal halide lamp, the light emission amount of each metal depends on the evaporation amount of the metal halide, but the evaporation amount is greatly influenced by the temperature change at the coldest spot of the arc tube. Moreover, the vapor pressure characteristics with respect to temperature differ for each of the enclosed mercury or metal halide. Therefore, if the power supplied to the metal halide lamp is changed from the rated value, the light emission amount and color balance of the metal will fluctuate individually due to the temperature change at the coldest spot of the arc tube, so the overall light color will be greatly It will change. For these reasons, until recently, it has been difficult to realize lighting (so-called dimming lighting) in which the light output can be freely changed by changing the power supplied to the metal halide lamp while keeping the light color characteristic substantially constant. The way of looking was powerful.
[0004]
However, in recent years, metal halide lamps have been devised in which such light color change is reduced and dimming lighting is possible (for example, Japanese Patent Laid-Open Nos. 6-84496 and 6). No. -111772 or JP-A-8-203471).
[0005]
[Problems to be solved by the invention]
However, in the conventional metal halide lamp lighting device, there is a concern that the lamp life may be impaired if the dimming lighting is performed by supplying power equal to or lower than the rated power to the lamp. In fact, in the United States, ballasts for metal halide lamps already equipped with dimming lighting means are commercially available, and considering the effect on lamp life, the lamp power during dimming lighting is set to 50% or more of the rated power, and Although there is a view that lighting is performed at the rated power for at least 15 minutes at the time of starting, the basis of this view is not necessarily clear, and the problem concerning the lamp life remains.
[0006]
The present invention has been made in view of the above circumstances, and an object thereof is to provide a lighting method of a metal halide lamp that can increase the lamp life without adversely affecting the luminous flux maintenance factor. .
[0007]
[Means for Solving the Problems]
In order to achieve the above object, a metal halide lamp for lighting a metal halide lamp in which a metal halide, mercury, and a rare gas are sealed in a translucent container in which a pair of electrodes are hermetically sealed is provided. In the lighting method, the rated power and the power that is equal to or lower than the rated power and that is equal to or higher than the luminous flux maintenance factor at the time of lighting with the rated power are supplied from the lighting means to the metal halide lamp, and the power supplied by the lighting means is changed. When the metal halide lamp is started, the power supplied to the lamp is set to be more than the power at the inflection point at which the rate of change of the electrode temperature with respect to the stable electric power changes suddenly. Not only does the luminous flux maintenance factor not decrease, but the luminous flux maintenance factor can be further increased and the lamp life can be increased as compared with lighting with only the rated power.
[0008]
Also, as in the invention of claim 2, from pre-Symbol lit means, it is desirable to supply the rated power or less power within a predetermined time after starting the metal halide lamp.
[0009]
Further, as in the invention of claim 3 , it is desirable that the lighting means supplies power equal to or lower than the rated power to the metal halide lamp from the start.
[0010]
According to a fourth aspect of the present invention, it is desirable that the lighting means has a time for supplying power equal to or lower than the rated power to the metal halide lamp during lighting.
[0011]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, embodiments of the present invention will be described in detail.
[0012]
(Embodiment 1)
As described above, there is a concern that the lamp life may be reduced when the dimming lighting of the metal halide lamp is performed. The reason is considered to be the electrode as described below. Usually, the electrode temperature of the metal halide lamp is designed to be within a temperature range in which thermionic electrons can be sufficiently emitted when the cathode is lit at the rated power. However, if the electrode temperature is too low due to dimming lighting, electron emission from the cathode becomes insufficient as described below.
[0013]
The relationship between the thermionic emission current density J at the cathode and the absolute temperature T of the electrode is the Richardson-Dashman equation when an external electric field E is applied,
J = AT 2 exp {−φ / kT + (e / 2kT) · (eE / πε 0 ) 1/2 } (1)
Can be used.
[0014]
In the above formula (1), A is a constant depending on the material and surface state of the electrode, φ is the work function of the electrode, k is the Boltzmann constant, e is the elementary charge, and ε 0 is the dielectric constant of vacuum. In the formula (1), it is assumed that the external electric field E is small and the second term of the exponent part of the formula (1) can be ignored as compared with the first term. At this time, in order to obtain the necessary current density J, the electrode temperature has a threshold T 0 at which thermionic electrons can be emitted, and when T> T 0 , the current necessary for lighting the metal halide lamp can be easily emitted. However, it can be seen that the current density J = 0 substantially at T <T 0 . Therefore, if the power supplied to the metal halide lamp is reduced too much, the electrode temperature falls below the lower limit T 0 of the appropriate temperature range, and thermionic emission at the cathode becomes insufficient.
[0015]
Actually, even when the electrode temperature drops below T 0 , the electric field E (cathode drop voltage) near the cathode is strengthened, and the second term in the exponent part of the equation (1) becomes large (of the Schottky effect). Increase), the current density J does not immediately become zero. Further, when the electric field E is strengthened, there is a possibility that electrons are supplied from the cathode by the field electron emission mechanism in addition to the thermionic emission mechanism. Therefore, even if the electrode temperature falls below T 0 , the discharge is caused to some extent. It is thought that it will be maintained. On the other hand, it is considered that the probability of scattering (sputtering) of the electrode material due to ion impact increases as the cathode fall voltage increases. Therefore, when the metal halide lamp is turned on in a state where the electrode temperature is lower than T 0 , the arc tube is blackened early, and there is a possibility that the luminous flux maintenance factor may be reduced as compared with lighting with only the rated power. . Further, the blackening of the arc tube causes an increase in the arc tube temperature during lighting. Accordingly, the lamp voltage rises and the impurity gas concentration inside the arc tube rises early compared to lighting with only the rated power, and as a result, the metal halide lamp is not turned on early, thereby reducing the lamp life. The possibility is feared.
[0016]
In the United States, in order not to adversely affect the lamp life, it is considered that the electric power at the time of dimming lighting is considered to be 50% or more of the rated power for the above reason. However, it is difficult to assume that the temperature range of electrodes that can emit thermoelectrons is 50% or more of the rated power, regardless of the lamp of any manufacturer, and the basis for the value of 50% is unclear. Therefore, in order to be able to specify the power condition that will not affect the lamp life, which will be different for each lamp, the following experiment was conducted.
[0017]
If the lower limit T 0 of the electrode temperature at which thermionic emission is possible is known, it is considered that power conditions that do not adversely affect the luminous flux maintenance factor can be obtained. From the above, the current density J and the electrode temperature at T <T 0 The relationship of T is considered to be different from the relationship between the current density J and the electrode temperature T when T> T 0 . Therefore, it was considered that if the relationship between the current density J and the electrode temperature T is examined with respect to the power range in which lighting can be maintained, knowledge about the lower limit T 0 can be obtained. However, during the lighting of the metal halide lamp, the current is limited by the ballast impedance, and it is difficult to directly measure the current density J. Therefore, instead of the current density J, the lamp current was substituted, and the relationship between the lamp current and the electrode temperature T was examined. As a result, the relationship between the power range that does not adversely affect the luminous flux maintenance factor and the electrode temperature T has been clarified. Hereinafter, the process of this experiment and the obtained results will be described as Embodiment 1 of the present invention.
[0018]
FIG. 1 is a schematic configuration diagram of a lighting device for realizing the first embodiment. As the lamp 1, a 400W metal halide lamp (part number: M400 · L / BU-SC-P) manufactured by Matsushita Electric Industrial Co., Ltd. was used. As the ballast 2 as the lighting means, various types of ballasts of various impedances are manufactured so that the lamp 1 can be supplied with electric power that is rated power or less than the rated power and ensures the luminous flux maintenance rate at the rated power or more when the lamp is turned on. Used. However, the combination of the lamp 1 and the ballast 2 used in the present embodiment is merely an example, and is not particularly limited to the present embodiment.
[0019]
The lamp 1 was started and lit by supplying various electric powers of different sizes to the lamp 1 using the lighting device of the present embodiment. Then, the electrode surface temperature near the arc end at the tip of the lower electrode after the lighting state of the lamp 1 was stabilized was measured using a thermography device. FIG. 2 shows the results of plotting the relative electrode temperatures measured by the thermography apparatus in this way against the lamp current and power, and examining the change tendency of the electrode temperature with respect to the lamp current and power. As apparent from FIG. 2, the electrode temperature tends to decrease as the power decreases as a whole. However, when viewed in detail, there is a region where the gradient of change is gentle from 300 W to 250 W. It can be seen that at power lower than this region, the rate of change with respect to the supplied power suddenly increases, and an inflection point exists in the vicinity of about 250 W.
[0020]
As seen in FIG. 2, the electrode temperature did not change much from 300 W to 250 W. When the discharge state in the vicinity of the electrode in this power range was observed, the size of the cathode bright spot decreased as the power decreased. From this, it has been found that in this power range, the electrode is at a temperature at which thermionic electrons can be sufficiently emitted, and the electrons necessary for maintaining the discharge are supplied by changing the area of the electron emission portion. On the other hand, when the discharge state in the vicinity of the electrode at the power of the inflection point (250 W) or less was observed, the cathode bright spot was unstable and the lamp 1 flickered. Since the cathode bright spot was not stable, it was found that the electrode temperature sufficient for thermionic emission was not obtained on the lower power side than the inflection point. Therefore, there is a concern that the lamp life may be adversely affected on the lower power side than the inflection point found in FIG.
[0021]
Therefore, in order to see the correlation between what is expected from the above experimental results, that is, whether the power supplied to the lamp 1 is higher or lower than the inflection point and the lamp life, the power supplied to the lamp 1 is 400 W (rated power), 270 W, and 210 W were used, and a life test was performed on the same type of lamp 1 as a sample. In this life test, one lighting time was set to 5 hours and 30 minutes, and a lighting / extinguishing cycle in which lighting was performed again for 5 hours and 30 minutes after turning off for 30 minutes was repeatedly performed. The test was interrupted at regular intervals, the lamp characteristics were measured, and the change with time was examined. A part of the result is shown in FIG.
[0022]
FIG. 3 is a plot of the luminous flux maintenance factor of each lamp 1 with respect to the lighting time, and shows a higher value of the luminous flux maintenance factor in the order of 270 W> 210 W> 400 W. Therefore, it has been found that supplying power less than the rated power to the lamp 1 has the effect of increasing the luminous flux maintenance factor in some cases, rather than impairing the luminous flux maintenance factor of the lamp 1. On the other hand, from the result that the lamp 1 that is lit at 210 W rather than 270 W has a lower luminous flux maintenance factor, as expected, the luminous flux maintenance factor is lower in the power region lower than the inflection point (250 W). It turned out to turn down. Further, as described above, at the power lower than the inflection point, the cathode bright spot was unstable and the lamp 1 flickered, and the lighting state was unstable. For these reasons, it is permissible to supply the lamp 1 with power below the inflection point found in FIG. 2 even when the luminous flux maintenance factor is improved as compared with lighting with only the rated power. It became clear that it should not be included in the lighting conditions.
[0023]
Therefore, in the present embodiment provided with the ballast 2 as the lighting means that can supply the metal halide lamp with the rated power and the power that is equal to or lower than the rated power and secures the luminous flux maintenance factor at the time of lighting with the rated power. When starting with a different power supply, specify the power that should be supplied from the ballast 2 to the lamp 1 to be more than the power at the inflection point at which the rate of change of the electrode temperature with respect to the power changes abruptly. Thus, not only the luminous flux maintenance factor does not decrease even when the dimming lighting is performed, but also the luminous flux maintenance factor can be further increased and the lamp life can be increased as compared with lighting with only the rated power.
[0024]
(Embodiment 2)
By the way, as already explained, in the United States, considering the influence on the lamp life, at the time of start-up, there is an opinion that the lamp will be lit at the rated power for a minimum of 15 minutes. Can be considered. That is, when the lamp is started with power less than or equal to the rated power, it takes time for the electrode temperature to stabilize compared to when the lamp is started with rated power. Therefore, it is thought that the reason is that the luminous flux maintenance factor decreases due to the increase in arc tube blackening due to the sputtering of the electrode material within this time. However, no reason can be found in the 15 minute period. Moreover, the question remains whether the rated power must be supplied to the lamp at the time of starting regardless of the power at the time of dimming lighting. Therefore, regardless of the power at the time of dimming lighting, it is necessary to always avoid the dimming start, and if necessary, in order to investigate how many minutes the rated lighting time is required, The experiment described was conducted.
[0025]
FIG. 4 is a schematic configuration diagram of a lighting device that realizes the lighting method of the present embodiment. The AC 200V commercial power supply and the ballast 3 are connected to each other via a path via the switch 4 and a path not via the switch 4, and the lamp 1 is connected to the output side of the ballast 3. Thus, the power supplied from the ballast 3 to the lamp 1 is switched between the rated power and the power less than or equal to the rated power according to the on / off state of the switch 4. Here, as the ballast 3, a 400W mercury lamp dimming ballast (product number: YZ40121433) manufactured by Matsushita Electric Works, Ltd. was used. As the lamp 1, a 400W metal halide lamp (part number: M400 · L / BU-SC-P) manufactured by Matsushita Electric Industrial Co., Ltd. was used. However, the combination of the ballast 3 and the lamp 1 used in the present embodiment is merely an example, and is not particularly limited to the present embodiment.
[0026]
In the present embodiment, a life test was performed in which a lighting time of one time was 5 hours and 30 minutes, and a lighting / lighting cycle in which lighting was performed again for 5 hours and 30 minutes after lighting for 30 minutes was repeated. In the present embodiment, the rated power or lower power is supplied to the lamp 1 under the following time conditions within one lighting time.
(A) The engine was started at the rated power (400 W), and 400 W of power was input to the lamp 1 even during lighting.
(B) The engine was started at the rated power (400 W), turned on at the rated power for 30 minutes, and then 270 W power was input to the lamp 1.
(C) The engine was started at the rated power (400 W), turned on at the rated power for 15 minutes, and then 270 W of power was input to the lamp 1.
(D) The engine was started at the rated power (400 W), turned on at the rated power for 4 minutes, and then 270 W of power was input to the lamp 1.
(E) Power was started at 270 W, and 270 W power was input to the lamp 1 even during lighting.
[0027]
FIG. 5 shows a part of the result of measuring the lamp characteristics by interrupting the test at regular intervals and measuring the change over time. FIG. 5 is a diagram showing a change in the luminous flux maintenance factor of the lamp 1 used in the present embodiment. In FIG. 5, curves a to e correspond to the above conditions (a) to (e). FIG. 5 shows that the luminous flux maintenance factor is good in the order of e≈d≈c>b> a. Further, although all the lamps 1 decreased by about 5% in the tens of hours from the start of the test, the lamps 1 that are turned on under the lighting conditions (e), (d), and (c) are turned on. It can be seen that a recovery phenomenon of the light intensity was observed after the time.
[0028]
In the present embodiment, 270 W is used as the power less than or equal to the rated power supplied to the lamp 1, but the power less than or equal to the rated power supplied to the lamp 1 is not particularly limited to the present embodiment. It was confirmed that the same results could be obtained with any power, so long as it was within the described power range.
[0029]
Even if dimming lighting is performed by lighting the lamp 1 with the rated power as described above and supplying the power below the rated power within a predetermined time or starting the lamp 1 with the power below the rated power. Not only does the luminous flux maintenance factor not decrease, but the luminous flux maintenance factor can be further increased and the lamp life can be increased compared to lighting with only the rated power.
[0030]
(Embodiment 3)
Since the configuration of the lighting device that realizes the lighting method of the present embodiment is the same as that of the second embodiment, illustration and description thereof are omitted.
[0031]
In the present embodiment, a life test was performed in which a lighting time of one time was 5 hours and 30 minutes, and a lighting / lighting cycle in which lighting was performed again for 5 hours and 30 minutes after lighting for 30 minutes was repeated. In addition, the lighting time at a power lower than the rated power within one lighting time was set to 0 or 2 hours, and the power at the rated power or lower was supplied to the lamp 1 under the following time conditions.
(A) The engine was started at the rated power (400 W), and 400 W was input to the lamp 1 even during lighting.
(B) Although the engine was started and lit at the rated power (400 W), 270 W of power was input to the lamp 1 for 2 hours from 1 hour to 3 hours after the start.
(C) Although the engine was started and lit at the rated power (400 W), 270 W of power was input to the lamp 1 for 2 hours from 3 hours 30 minutes after the start until the end of lighting.
(D) The lamp was started and lit with power of 270 W, but the rated power (400 W) was input to the lamp 1 for 3 hours and 30 minutes from 2 hours after the start until the end of lighting.
[0032]
The test was interrupted at regular intervals, the lamp characteristics were measured, and the change with time was examined. A part of the result is shown in FIG. FIG. 6 is a diagram showing a change in the luminous flux maintenance factor of the lamp 1 used in the present embodiment. In FIG. 6, curves A to D correspond to the above conditions (A) to (D). From FIG. 6, it can be seen that the luminous flux maintenance factors of the above (B), (C), and (D) are comparable, and both are superior to the condition (A). Therefore, conditions (B), (C), and (D) in which lighting with power below the rating is performed for 2 hours between lighting with rated power, compared to conditions (A) with lighting only with rated power. It can be seen that the luminous flux maintenance factor is increased.
[0033]
In the present embodiment, the lighting time with the power below the rating is 2 hours, but is not particularly limited to 2 hours. Although there is a difference in degree, the effect of increasing the luminous flux maintenance factor compared to lighting with only the rated power by lighting at less than the rated power between lighting at the rated power at any time Was confirmed.
[0034]
Further, in this embodiment, 270 W is used as the power less than the rated power supplied to the lamp 1, but the power less than the rated power supplied to the lamp 1 is not particularly limited to this embodiment. It was confirmed that the same results could be obtained with any power, so long as it was within the described power range.
[0035]
As described above, by providing the lamp 1 with a time equal to or lower than the rated power supplied from the ballast 3 during lighting, the luminous flux maintenance factor does not decrease even when the dimming lighting is performed. Compared with only lighting, the luminous flux maintenance factor can be further increased and the lamp life can be increased.
[0036]
【The invention's effect】
As described above, the present invention provides a method for lighting a metal halide lamp in which a metal halide lamp is formed by sealing a metal halide, mercury, or a rare gas in a translucent container in which a pair of electrodes are hermetically sealed. When the power is supplied from the lighting means to the metal halide lamp that is equal to or lower than the rated power and ensures the luminous flux maintenance rate at the rated power or higher, and the metal halide lamp is started by changing the power supplied by the lighting means. Since the power supplied to the lamp is set to be equal to or higher than the power at the inflection point at which the rate of change of the electrode temperature with respect to the stable power changes suddenly, not only the luminous flux maintenance rate does not decrease even if dimming is performed. As compared with lighting only with rated power, there is an effect that the luminous flux maintenance factor can be further increased and the lamp life can be increased.
[Brief description of the drawings]
FIG. 1 is a schematic configuration diagram illustrating a lighting device for realizing a lighting method according to a first embodiment of the present invention.
FIG. 2 is an explanatory diagram of the above.
FIG. 3 is a view showing a life test result as described above.
FIG. 4 is a schematic configuration diagram illustrating a lighting device for realizing a lighting method according to a second embodiment of the present invention.
FIG. 5 is a view showing a life test result as described above.
FIG. 6 is a diagram showing a life test result of Embodiment 3 of the present invention.
[Explanation of symbols]
1 Metal halide lamp 2 Ballast

Claims (4)

一対の電極が気密封入された透光性の容器内に金属ハロゲン化物、水銀、希ガスを封入してなるメタルハライドランプを点灯するメタルハライドランプの点灯方法において、定格電力と、定格電力以下であって定格電力による点灯時の光束維持率以上を確保する電力を点灯手段からメタルハライドランプに供給するとともに、前記点灯手段の供給する電力を変えてメタルハライドランプを始動した場合に、ランプに供給される電力を、略安定する電極温度の電力に対する変化割合が急変する変曲点の電力以上の電力とすることを特徴とするメタルハライドランプの点灯方法。In a lighting method of a metal halide lamp in which a metal halide lamp is formed by sealing a metal halide, mercury, or a rare gas in a light-transmitting container in which a pair of electrodes are hermetically sealed, the rated power is equal to or lower than the rated power. Supplying the power to the metal halide lamp from the lighting means to ensure the luminous flux maintenance rate at the time of lighting with the rated power, and when the metal halide lamp is started by changing the power supplied by the lighting means, the power supplied to the lamp A method for lighting a metal halide lamp, characterized in that the power is higher than the power at the inflection point at which the rate of change of the electrode temperature with respect to the stable electrode temperature changes rapidly . 前記点灯手段より、始動から所定時間内に前記定格電力以下の電力をメタルハライドランプに供給することを特徴とする請求項1記載のメタルハライドランプの点灯方法。2. The method for lighting a metal halide lamp according to claim 1 , wherein the lighting means supplies power equal to or lower than the rated power to the metal halide lamp within a predetermined time from starting . 前記点灯手段より、始動時から前記定格電力以下の電力をメタルハライドランプに供給することを特徴とする請求項記載のメタルハライドランプの点灯方法。Lighting method of claim 1 wherein the metal halide lamp and supplying from said lighting means, the power follows the rated power from the start to a metal halide lamp. 前記点灯手段より、点灯中に前記定格電力以下の電力をメタルハライドランプに供給する時間を有することを特徴とする請求項記載のメタルハライドランプの点灯方法 Lighting method of claim 1 wherein the metal halide lamp which comprises said more lighting means, the time for supplying the rated power or less power to the metal halide lamp during operation.
JP2000358633A 2000-11-27 2000-11-27 How to turn on the metal halide lamp Expired - Fee Related JP3994658B2 (en)

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