JP4063080B2 - Noble gas discharge lamp - Google Patents

Noble gas discharge lamp Download PDF

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Publication number
JP4063080B2
JP4063080B2 JP2003002446A JP2003002446A JP4063080B2 JP 4063080 B2 JP4063080 B2 JP 4063080B2 JP 2003002446 A JP2003002446 A JP 2003002446A JP 2003002446 A JP2003002446 A JP 2003002446A JP 4063080 B2 JP4063080 B2 JP 4063080B2
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electrode
insulating member
gas discharge
discharge lamp
lead wire
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JP2004214149A (en
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正樹 井上
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Ushio Denki KK
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Ushio Denki KK
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Description

【0001】
【発明の属する技術分野】
本発明は、ファクシミリ、複写機、イメージリーダ等の情報機器における原稿照明用、あるいは、液晶パネルディスプレイのバックライト等に利用される希ガス放電灯に関し、特にCIS(密着イメージセンサ)方式の読取り用光源として使用される希ガス放電灯に関する。
【0002】
【従来の技術】
近年スキャナーや複写機の読取り方式として、CIS(密着イメージセンサ)方式が開発され、多くのスキャナー、複写機に使用されている。係るCIS方式では、光源からの光をプラテンとガラス板との間に挟まれた原稿に照射し、その反射光を受光してデジタル化処理することにより、その原稿の内容を読取る、というものであり、構造が簡単かつコンパクトである利点がある。この密着イメージセンサにおいては、例えば特開平4−360458号(特許第2953595号)公報に記載のもののように、光源として発光ダイオード(LED)アレイなどと、レンズ及びセンサなどが一体的に構成され、ユニットとされている。
【0003】
一方、スキャナーや複写機では一般に縮小光学系を使用しており、光源としては希ガス放電灯が使用されている。係る希ガス放電灯は、直管状のガラス管内にキセノンなどの希ガスが封入されており、該ガラス管の外表面上に、例えばアルミニウム(Al)よりなる略矩形の一組の金属箔をガラス管の断面方向で対向する箇所に貼着して、一対の電極が具備されたものである。そしてこの一対の電極に高周波電圧を印加して、希ガスの放電により発生した紫外線を、ガラス管内に形成した蛍光物質層に照射して励起し、可視光の発光を得るというものである。
【0004】
最近では、この希ガス放電灯においても、先述の密着イメージセンサの光源としての利用が考えられているが、そのためには、従来の縮小光学系に使用されていた希ガス放電灯に比較して、ガラス管の外径(以下「管径」という。)を極端に細くする必要がある。具体的には、管径がφ8〜12mm程度であったものが、密着イメージセンサ用途ではφ3〜6mm程度に細くする必要がある。
【0005】
ガラス管を細くすると、電極の幅を狭くして絶縁距離を稼ぐ必要がある。実使用範囲でいうと、縮小光学系用の希ガス放電灯では、管径φ8〜12mmであり、電極幅は5〜9mmであるが、密着イメージセンサ用に管径をφ3〜6mmとすると、電極幅は1mm程度にしなければならない。このように電極の幅が狭くなると、給電用の端子部材などを電極に接続することは困難であり、例えば特許2729100号公報記載の技術のように、給電用のリード線を直接電極に半田付けするのが簡便な方法である。
【0006】
【特許文献1】
特許第2729100号公報
【0007】
【発明が解決しようとする課題】
而して、電極の幅が1mm程度になると電極のリード線の接合部近傍において不具合を生じやすくなるという問題がある。
【0008】
即ち、電極を構成する金属箔の幅が狭くなるために、その機械的強度が低下し、希ガス放電灯の製作時或いは最終形態とした後、電極に接続したリード線を取り回ししていると金属箔が変形したり、ガラス管との接着面積が狭くなるため剥がれたりする不具合を生じる。また、リード線と金属箔とを半田により直接接合したときに、溶融した半田金属が冷却、収縮する過程で金属箔が歪曲するといった不具合を生じることがある。
【0009】
上記のように金属箔が剥がれたり変形したりすると、電極とガラス管との間に不可避の間隙が形成されてしまい、希ガス放電灯の点灯時にガラス管への投入電力が局部的に不足して暗部を形成する、といった事態に至る。このような希ガス放電灯では、発光エリアにおいて所望の照度分布が得られないため、原稿読取り用の光源として使用することができなくなる。
【0010】
そこで、本発明の目的は、原稿照明用として好適に使用することができ、幅が狭い金属箔からなる電極であっても、給電用リード線の接合部近傍における機械的強度が高く、量産に適した希ガス放電灯を提供することにある。
【0011】
【課題を解決するための手段】
そこで本願発明に係る希ガス放電灯は、希ガスが封入されたガラス管と、該ガラス管の外表面上に形成されたガラス管の長さ方向に延在する金属部材よりなる一方の電極と、該一方の電極に接合された給電用のリード線と、該一方の電極と少なくとも1つの誘電体を介して配置された他方の電極と、を具備してなり、前記一方の電極は、該電極上において該電極の長さ方向に互いに離間し、熱収縮性を有するチューブよりなる第一の絶縁部材と第二の絶縁部材と、により被覆され、前記第一の絶縁部材と第二の絶縁部材との離間部分において露出した電極にリード線の接合部が形成されていることを特徴とする。
また、第一の絶縁部材と前記第二の絶縁部材とをつなぐための接続用絶縁部材が形成されていることを特徴とする。
また、前記第一の絶縁部材及び第二の絶縁部材は、前記一方の電極をその長さ方向に1mm以上被覆していることを特徴とする。
【0012】
【発明の実施の形態】
以下、本発明の第一の実施形態を、図1〜図3を参照して説明する。図1は本発明の第一の実施形態に係る希ガス放電灯の、一部断面で示す管軸方向の側面図であり、図2はこの希ガス放電灯を図1中の線分A−Aで切断した断面図である。
ガラス管11は、その両端部(11A、11B)が加熱縮径されて密閉されており、その外表面には一方の電極21と他方の電極22とよりなる一対の電極が、ガラス管11の管壁により構成された二枚の誘電体及び放電空間を介して対向配置されている。また、このガラス管11には所定の希ガスが封入されており、その内表面上には蛍光体が塗布されて蛍光体層30が形成されている。なおこの蛍光体層30はその一部がガラス管の管軸方向に除去されており、これにより光取り出し用のアパーチャ40が形成されている。
【0013】
このガラス管11は、例えば、寸法が外径φ4mm、肉厚0.5mmであり、長さ360mmであり、材質は透明なバリュウムガラスである。
【0014】
上記一対の電極21、22は、例えば、金属箔をテープ状にしてガラス管に貼付することにより形成される。
電極21、22の材質としてはアルミニウムが好適であり、例えば厚さ70μm、長さが358mm、幅が1.5mmである略帯状の金属箔を、ガラス管11の外表面上に貼着して構成される。尚、「電極の長さ」とは電極長手方向の全長であり、「電極の幅」とは電極短手方向の全長をいう。
【0015】
図1に示すように、ガラス管11の一端部11A側に第一の絶縁部材61が、他端部11B側に第二の絶縁部材62が、第一の絶縁部材61と第二の絶縁部材62との間に離間部分Sを形成して、電極21、22或いはガラス管11の外表面に密着して設けられている。
同図において、第一の絶縁部材61が電極21、22の一端部21A、22Aから被覆する距離L1は、例えば0.1mm〜6.0mmであり、好ましくは1mm以上である。また、第二の絶縁部材62が、電極21、22を被覆する距離L2は、例えば0.1mm〜354.5mmであり、1mm以上あればよい。なかでも第二の絶縁部材62は電極21、22の他端部21B、22Bを被覆しているのが好ましい。
【0016】
ここで、第一の絶縁部材61と第二の絶縁部材62との離間部分Sにおいては、電極の露出部21S、22Sが形成されており、当該箇所において給電用のリード線50、50が半田51、51で直接接合されて、リード線接合部52、52が形成されている。
第一の絶縁部材61と第二の絶縁部材62との離間部分Sの電極長さ方向の距離は、リード線を接続できる程度に、例えば2mm以上であるのが好ましく、かつリード線接合部52、52近傍に位置される電極が固定されるよう、例えば5mm以下であるのが好ましい。具体的には3.5mm〜4.5mmであり、中でも、3.0mm〜4.0mmであるのが良い。
【0017】
第一、第二の絶縁部材は、例えば熱収縮性を有する光透過性の絶縁チューブによって、以下のような手順で配設することができる。
【0018】
図3(a)、(b)は、希ガス放電灯の要部を拡大して示す、一方の電極が配置された側面の方向からみた斜視図であり、先に図1、図2で説明した構成と同様の構成については同じ符号を付している。
例えば、図3(a)に示すように、電極21が貼着されたガラス管11に、二つの絶縁チューブ61A、62Aを所定距離離間して配置する。係る絶縁チューブ61A、62Aが装着された状態でガラス管11を例えば150〜200℃に加熱すると、当該絶縁チューブ61A、62Aが熱収縮して、第一、第二の絶縁部材61、62が形成される。
電極21は、これら第一、第二の絶縁部材61、62によりガラス管11の中心方向に押圧されて固定されると共に、第一の絶縁部材61、第二の絶縁部材61の間に電極露出部21Sを形成する。
【0019】
また、図3(b)に示すように、開口穴Hを設けた一つの絶縁チューブ63Aをガラス管11に開口穴Hを電極21に対応させて装着し、熱収縮させることによっても良い。
【0020】
一つの絶縁チューブ63Aを用いる場合も、電極21上にはその長さ方向に、一端部21Aから該開口穴Hの縁部に至るまで第一の絶縁部材61が設けられ、開口穴Hを挟んで該開口穴Hの他方の縁部から電極の他端部に至るまで第二の絶縁部材62が、それぞれ設けられる。尚、開口穴Hの周方向においては、第一の絶縁部材61と第二の絶縁部材62とをつなぐための接続用絶縁部材64がガラス管11を被覆するように形成される。
一方、電極21には開口穴Hに対応して電極露出部21Sが形成される。
【0021】
ここで、絶縁チューブ63Aは、電極の一端部21Aを、少なくとも1mm被覆しており、同図に示す電極の被覆距離L1は例えば1.0mm〜6.0mmである。
開口穴Hは、絶縁チューブの所定箇所を打ち抜いて形成され、その形状は、長円形状、矩形状など適宜であり、その大きさは電極長さ方向に3.5mm〜4.5mm、幅方向に1.5mm〜2.0mmとするのが良い。
【0022】
また更に、上記本発明に係る希ガス放電灯においては、リード線接合部上から、熱収縮性を有する絶縁チューブ等によってガラス管を被覆すると、絶縁性が格段に向上し、リード線接合部の近傍におけるリード線と電極との密着性が増してより好ましいものとなる。
【0023】
以上説明した本発明によれば、リード線の接合部において電極が引っ張られたとしても、当該接合部の、電極長さ方向における両方の側部が、第一、第二の絶縁部材により強固に固定されているので、電極が剥がれにくくて電極が変形するような問題も生じにくくなる。よって、リード線接合部近傍の機械的強度が高くて生産性の良好な希ガス放電灯を提供することができる。また更には、電極とガラス管と間に間隙が形成されるのを防止できるので、点灯中に暗部が形成されることがなく所定の照度分布を得ることができる、希ガス放電灯を提供することが可能になる。従って、その結果、製造作業が簡便で、生産性が良好でありながら、所望の配光分布を得ることが可能で、原稿照明用の光源として好適な、希ガス放電灯を提供することができるようになる。
また、更には、本発明によれば、リード線の引っ張り強度を増大することができるので、製作が容易で量産性に富む、コンパクト化を実現できる希ガス放電灯を提供することができる。
【0024】
以上、本発明の実施形態について説明したが、上記内容に限定されることなく、適宜、変更が可能である。例えば、一対の電極は、両電極の間に少なくとも誘電体層と放電空間を有していれば足り、一方の電極をガラス管の外表面上に、他方の電極をガラス管の内表面上に配設することも可能である。
また、本発明は電極の幅が狭いものに限定されるものではなく比較的大きいもので適用できる。係る場合は、リード線と電極との間に端子部材を配置して電気的接続を行っても良い。
【0025】
【実施例】
図1、2に示す本発明の構成に係る希ガス放電灯を、第一の絶縁部材が電極を被覆している距離L1の大きさを種々変化させて下記手順により製作した。なおガラス管は管径がφ4mmとφ5mmのものを用いた。
全長が360mmのガラス管に厚さ0.5mm、長さ358mm、幅1.5mmのアルミニウム製の箔を貼付して電極を構成した。この電極の一端部側に、第一の絶縁部材用の絶縁チューブの長さを変化させて電極を被覆する距離L1が0.1mm〜6mmの範囲になるように装着した。また、第二の絶縁部材用の絶縁チューブを、第一の絶縁部材との離間部分(電極露出部)の長さSを3.5mm(一定)となるようにかつ電極の他端部を覆うようにして、装着した。しかる後、電極及び絶縁チューブが装着したガラス管を150〜200℃に加熱して第一、第二の絶縁部材を配置した。
上記第一と第二の絶縁部材が離間した部分において電極が露出した箇所に、線経が約1mmのリード線をアルミ半田により接合した。
以上の製作工程においては、半田付けする作業も簡便に行うことができ電極が剥離したり変形したりすることなく、作業性が非常に良好であった。
【0026】
【比較例1】
第一の絶縁部材が電極を被覆する部分の長さL1が0mmである(即ち、第一の絶縁部材を配設していない)ことを除いて、上記実施例と同様の手順に従い比較例1に係る希ガス放電灯を製作した。尚、第二の絶縁部材用の絶縁チューブを電極の一端部より他端部側に所要距離離れた箇所から該電極の他端部まで覆うように装着し、これにより、電極一端部を長さ3.5mmだけ露出させて第二の絶縁部材を配設した。
電極一端部において該電極が露出した箇所に、線経約1mmのリード線をアルミ半田により接合した。
以上の製作工程においては、半田付け作業中に電極が剥離するものが多数発生した。又、電極一端部が剥がれ易くて、その後の製造工程においてリード線の取り回し中に電極が剥離して変形してしまった。
【0027】
【比較例2】
従来技術に係る希ガス放電灯の製作要領即ち、先に電極にリード線を接合してから絶縁チューブを被覆する要領で、下記手順に従い管径がφ3〜φ5mmの希ガス放電灯を製作した。
全長が360mmのガラス管に厚さ0.5mm、長さ358mm、幅1.5mmのアルミニウム製の箔を貼付して電極を構成した。
次いで、この電極の一端から3.5mm離間した箇所における電極上にリード線をアルミ半田により接合した。
以上の製作工程においては、半田付け作業中に電極が歪曲して剥離するものが多数発生し、又、リード線接続後の作業中に電極が外れるものがあった。このように、従来の希ガス放電灯はその製造工程中の不良発生率が高くて生産性に問題があった。
【0028】
【実験例】
上記実施例、比較例1及び比較例2に係る希ガス放電灯についてリード線の引っ張り強度を測定した。ここで「リード線の引っ張り強度」とは、リード線を引っ張ったときに、リード線接合部の破損、電極の変形などによって、破断に至った時の最大張力である。本実験例においては、リード線に荷重測定器を取り付けてリード線を管軸と平行な方向に引っ張って測定した。
【0029】
上記実験例の結果を、図4及び後段の表1に示す。
図4は、上記実験例の結果を示す第一の絶縁部材が電極を被覆する距離(図1中のL1(mm))とリード線の引っ張り強度(単位:N)との関係を示す図である。図4においては、実施例と比較例1の放電灯における引っ張り強度(N)の測定値の平均値を付すと共に、その近似曲線を引いた。下記の表1は上記比較例の希ガス放電灯について、リード線の引っ張り強度を測定した平均値である。
【0030】
【表1】

Figure 0004063080
【0031】
表1の結果、リード線が接続された電極が絶縁部材に被覆されていないものでは、リード線の引っ張り強度が管径がφ5mmのもので約2.98N、管径φ4mmのもので1.96、管径φ3mmのものでは1Nに満たない0.98であった。
このように引っ張り強度が小さいと、製作中に不良となる確率が極めて高くて量産することは不可能である。尚、本実験例により、本発明者らは、リード線の引っ張り強度が5N以上、好ましくは8N以上、より好ましくは10N以上であれば、リード線の取り回し中に電極に不具合を生じにくいという検知を得た。
【0032】
図4に示すように、電極の被覆長さが1mmのとき、管径φ5mmの場合はリード線の引っ張り強度が10N以上であり、十分高い機械的強度が得られることが確認できた。また、比較例2に係る電極が一切絶縁部材で被覆されないものに比較して3倍以上の強度が得られるようになると分かった。更に、管径がφ4mmの場合でも、電極の被覆長さが1mmを超えると、リード線引っ張り強度を8N以上に高くすることが可能であると分かった。
【0033】
尚、比較例1に係る電極の被覆長さが0mmであるものは、比較例2に係るものに比較して若干の強度向上が認められるが、リード線の引っ張り強度が5Nに満たないため、実際の作業では不良の発生率が高くて実使用できるものではなかった。
【0034】
以上のように、本発明に係る第一の絶縁部材と第二の絶縁部材の間にリード線の接合部を形成した希ガス放電灯によれば、リード線の引っ張り強度を高くすることができ、リード線の引っ張り強度を増すことができて生産性が良好であることが判明した。
更には、電極被覆長さを1mm以上にすると、8N以上に高い強度を得ることができると分かった。
【0035】
【発明の効果】
以上説明したように、本発明によれば、幅が狭い電極であっても電極とガラス管の密着強度が高く、リード線の取り回しを容易にできて、電極の給電用導出部において不具合を生じにくい、希ガス放電灯を提供することができる。
その結果、希ガス放電灯のコンパクト化を実現しつつ、生産性良好な希ガス放電灯を提供できる。
【図面の簡単な説明】
【図1】 本発明の第一の実施形態に係る希ガス放電灯の管軸方向断面図である。
【図2】 図1中の線分A−Aで切断した希ガス放電灯の断面図である。
【図3】 本発明の実施形態を説明する図である。
【図4】 実験例の結果を示す、距離L1とリード線の引っ張り強度の関係を示す図である。
【符号の説明】
11 ガラス管
11A 一端部
11B 他端部
21 一方の電極
21A 一端部
21B 他端部
22 他方の電極
22A 一端部
22B 他端部
21S、22S 電極露出部
30 蛍光体層
40 アパーチャ
50 リード線
51 半田
52 リード線接合部
61 第一の絶縁部材
62 第二の絶縁部材
61A、62A、63A 絶縁チューブ
64 つなぎ用絶縁部材
S 離間部分
H 開口穴[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a noble gas discharge lamp used for illuminating a document in information equipment such as a facsimile, a copying machine, and an image reader, or a backlight of a liquid crystal panel display, and more particularly to a CIS (contact image sensor) type reading. The present invention relates to a rare gas discharge lamp used as a light source.
[0002]
[Prior art]
In recent years, a CIS (contact image sensor) method has been developed as a reading method for scanners and copying machines, and is used in many scanners and copying machines. In such a CIS system, light from a light source is irradiated onto a document sandwiched between a platen and a glass plate, and the reflected light is received and digitized to read the content of the document. There is an advantage that the structure is simple and compact. In this contact image sensor, for example, a light emitting diode (LED) array as a light source, a lens, a sensor, and the like are integrally configured as described in JP-A-4-360458 (Patent No. 2955595). It is considered as a unit.
[0003]
On the other hand, a reduction optical system is generally used in a scanner or a copying machine, and a rare gas discharge lamp is used as a light source. In such a rare gas discharge lamp, a rare gas such as xenon is sealed in a straight tubular glass tube, and a set of substantially rectangular metal foils made of, for example, aluminum (Al) is formed on the outer surface of the glass tube. A pair of electrodes are provided by being attached to the opposite portions in the cross-sectional direction of the tube. A high-frequency voltage is applied to the pair of electrodes, and ultraviolet rays generated by rare gas discharge are irradiated to the fluorescent material layer formed in the glass tube and excited to obtain visible light emission.
[0004]
Recently, this rare gas discharge lamp is also considered to be used as the light source of the above-mentioned contact image sensor, but for that purpose, compared with the rare gas discharge lamp used in the conventional reduction optical system. It is necessary to extremely reduce the outer diameter of the glass tube (hereinafter referred to as “tube diameter”). Specifically, the tube diameter of about φ8 to 12 mm needs to be reduced to about φ3 to 6 mm for the contact image sensor application.
[0005]
If the glass tube is made thinner, it is necessary to reduce the width of the electrode and increase the insulation distance. In terms of the actual use range, in the rare gas discharge lamp for the reduction optical system, the tube diameter is 8 to 12 mm and the electrode width is 5 to 9 mm. However, if the tube diameter is 3 to 6 mm for the contact image sensor, The electrode width must be about 1 mm. When the width of the electrode is reduced in this way, it is difficult to connect a power supply terminal member or the like to the electrode. For example, as in the technique described in Japanese Patent No. 2729100, the power supply lead wire is directly soldered to the electrode. This is a simple method.
[0006]
[Patent Document 1]
Japanese Patent No. 2729100 [0007]
[Problems to be solved by the invention]
Thus, when the width of the electrode is about 1 mm, there is a problem that a defect is likely to occur near the joint portion of the electrode lead wire.
[0008]
That is, since the width of the metal foil constituting the electrode is narrowed, its mechanical strength is reduced, and the lead wire connected to the electrode is routed when the rare gas discharge lamp is manufactured or after the final form is formed. There arises a problem that the metal foil is deformed or peeled off because the bonding area with the glass tube is narrowed. Further, when the lead wire and the metal foil are directly joined by solder, there may be a problem that the metal foil is distorted in the process in which the molten solder metal is cooled and contracted.
[0009]
If the metal foil is peeled off or deformed as described above, an inevitable gap is formed between the electrode and the glass tube, and the power supplied to the glass tube is locally insufficient when the rare gas discharge lamp is turned on. To form a dark part. In such a rare gas discharge lamp, since a desired illuminance distribution cannot be obtained in the light emitting area, it cannot be used as a light source for reading a document.
[0010]
Therefore, the object of the present invention can be suitably used for illuminating a document, and even in the case of an electrode made of a metal foil having a narrow width, the mechanical strength in the vicinity of the joint portion of the power supply lead wire is high, and it is suitable for mass production. The object is to provide a suitable rare gas discharge lamp.
[0011]
[Means for Solving the Problems]
Therefore, a rare gas discharge lamp according to the present invention includes a glass tube filled with a rare gas, and one electrode made of a metal member extending in the length direction of the glass tube formed on the outer surface of the glass tube. A lead wire for power supply joined to the one electrode, and the other electrode disposed through the one electrode and at least one dielectric, the one electrode being On the electrode, the first insulating member and the second insulating member are covered with a first insulating member and a second insulating member that are spaced apart from each other in the length direction of the electrode and are made of a heat-shrinkable tube. A lead wire bonding portion is formed on the electrode exposed at a distance from the member.
In addition, a connection insulating member for connecting the first insulating member and the second insulating member is formed .
Further, the first insulating member and the second insulating member cover the one electrode in the length direction by 1 mm or more.
[0012]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, a first embodiment of the present invention will be described with reference to FIGS. FIG. 1 is a side view of the rare gas discharge lamp according to the first embodiment of the present invention in the tube axis direction shown in a partial cross section, and FIG. 2 shows this rare gas discharge lamp along line A-- in FIG. It is sectional drawing cut | disconnected by A. FIG.
Both ends (11A, 11B) of the glass tube 11 are hermetically reduced in diameter and hermetically sealed, and a pair of electrodes including one electrode 21 and the other electrode 22 are formed on the outer surface of the glass tube 11. The two dielectrics formed by the tube wall and the discharge space are arranged to face each other. The glass tube 11 is filled with a predetermined rare gas, and a phosphor layer 30 is formed on the inner surface by applying a phosphor. A part of the phosphor layer 30 is removed in the direction of the tube axis of the glass tube, whereby an aperture 40 for extracting light is formed.
[0013]
The glass tube 11 has, for example, dimensions of an outer diameter of 4 mm, a thickness of 0.5 mm, a length of 360 mm, and a transparent barium glass.
[0014]
The pair of electrodes 21 and 22 is formed, for example, by sticking a metal foil in a tape shape to a glass tube.
The material of the electrodes 21 and 22 is preferably aluminum. For example, a substantially strip-shaped metal foil having a thickness of 70 μm, a length of 358 mm, and a width of 1.5 mm is stuck on the outer surface of the glass tube 11. Composed. The “electrode length” is the total length in the electrode longitudinal direction, and the “electrode width” is the total length in the electrode short direction.
[0015]
As shown in FIG. 1, the first insulating member 61 is on the one end 11A side of the glass tube 11, the second insulating member 62 is on the other end 11B side, the first insulating member 61 and the second insulating member. A separation portion S is formed between the electrodes 62 and 62 and the electrodes 21 and 22 or the outer surface of the glass tube 11 are provided in close contact with each other.
In the figure, the distance L1 covered by the first insulating member 61 from the one end portions 21A and 22A of the electrodes 21 and 22 is, for example, 0.1 mm to 6.0 mm, and preferably 1 mm or more. The distance L2 that the second insulating member 62 covers the electrodes 21 and 22 is, for example, 0.1 mm to 354.5 mm, and may be 1 mm or more. In particular, the second insulating member 62 preferably covers the other end portions 21 </ b> B and 22 </ b> B of the electrodes 21 and 22.
[0016]
Here, in the separation portion S between the first insulating member 61 and the second insulating member 62, exposed portions 21S and 22S of the electrodes are formed, and the lead wires 50 and 50 for power feeding are soldered at the portions. The lead wire joint portions 52 and 52 are formed by direct joining at 51 and 51.
The distance in the electrode length direction of the separation portion S between the first insulating member 61 and the second insulating member 62 is preferably, for example, 2 mm or more so that the lead wire can be connected, and the lead wire joint portion 52. , 52 is preferably 5 mm or less, for example, so that the electrode positioned in the vicinity of 52 is fixed. Specifically, it is 3.5 mm to 4.5 mm, and it is good that it is 3.0 mm to 4.0 mm among them.
[0017]
The first and second insulating members can be arranged by the following procedure, for example, by a light-transmitting insulating tube having heat shrinkability.
[0018]
FIGS. 3A and 3B are enlarged perspective views of the main part of the rare gas discharge lamp, as seen from the direction of the side surface on which one electrode is disposed. The same reference numerals are given to the same configurations as those described above.
For example, as shown in FIG. 3A, two insulating tubes 61A and 62A are arranged at a predetermined distance apart from each other on the glass tube 11 to which the electrode 21 is adhered. When the glass tube 11 is heated to, for example, 150 to 200 ° C. with the insulating tubes 61A and 62A attached, the insulating tubes 61A and 62A are thermally contracted to form the first and second insulating members 61 and 62. Is done.
The electrode 21 is pressed and fixed in the center direction of the glass tube 11 by the first and second insulating members 61 and 62, and the electrode is exposed between the first insulating member 61 and the second insulating member 61. Part 21S is formed.
[0019]
Further, as shown in FIG. 3B, one insulating tube 63A provided with an opening hole H may be attached to the glass tube 11 so that the opening hole H corresponds to the electrode 21 and thermally contracted.
[0020]
Even in the case where one insulating tube 63A is used, the first insulating member 61 is provided on the electrode 21 from the one end 21A to the edge of the opening hole H in the length direction thereof. The second insulating members 62 are provided from the other edge of the opening hole H to the other end of the electrode. In the circumferential direction of the opening hole H, a connecting insulating member 64 for connecting the first insulating member 61 and the second insulating member 62 is formed so as to cover the glass tube 11.
On the other hand, an electrode exposed portion 21S is formed in the electrode 21 corresponding to the opening hole H.
[0021]
Here, the insulating tube 63A covers at least 1 mm of the one end 21A of the electrode, and the electrode covering distance L1 shown in the figure is, for example, 1.0 mm to 6.0 mm.
The opening hole H is formed by punching a predetermined portion of the insulating tube. The shape of the opening hole H is appropriate such as an oval shape or a rectangular shape, and the size thereof is 3.5 mm to 4.5 mm in the electrode length direction, and the width direction. It is good to set it as 1.5 mm-2.0 mm.
[0022]
Furthermore, in the rare gas discharge lamp according to the present invention, when the glass tube is covered with a heat-shrinkable insulating tube or the like from the lead wire joint portion, the insulation property is greatly improved, and the lead wire joint portion is improved. The adhesion between the lead wire and the electrode in the vicinity is increased, which is more preferable.
[0023]
According to the present invention described above, even if the electrode is pulled at the joint portion of the lead wire, both side portions of the joint portion in the electrode length direction are more firmly formed by the first and second insulating members. Since it is fixed, it is difficult for the electrode to be peeled off and the electrode to be deformed. Therefore, it is possible to provide a rare gas discharge lamp having high mechanical strength in the vicinity of the lead wire joint and good productivity. Still further, the present invention provides a rare gas discharge lamp that can prevent a gap from being formed between an electrode and a glass tube, and can obtain a predetermined illuminance distribution without forming a dark portion during lighting. It becomes possible. Therefore, as a result, it is possible to provide a rare gas discharge lamp that is easy to manufacture and can obtain a desired light distribution while having good productivity and is suitable as a light source for document illumination. It becomes like this.
Furthermore, according to the present invention, since the tensile strength of the lead wire can be increased, it is possible to provide a rare gas discharge lamp that is easy to manufacture and has high productivity, and can be made compact.
[0024]
Although the embodiments of the present invention have been described above, the present invention is not limited to the above contents and can be changed as appropriate. For example, it is sufficient for a pair of electrodes to have at least a dielectric layer and a discharge space between both electrodes. One electrode is on the outer surface of the glass tube and the other electrode is on the inner surface of the glass tube. It is also possible to arrange.
Further, the present invention is not limited to the electrode having a narrow width but can be applied to a relatively large electrode. In such a case, a terminal member may be disposed between the lead wire and the electrode for electrical connection.
[0025]
【Example】
The rare gas discharge lamp according to the configuration of the present invention shown in FIGS. 1 and 2 was manufactured according to the following procedure with various changes in the distance L1 with which the first insulating member covered the electrode. Glass tubes with tube diameters of 4 mm and 5 mm were used.
An aluminum foil having a thickness of 0.5 mm, a length of 358 mm, and a width of 1.5 mm was attached to a glass tube having a total length of 360 mm to constitute an electrode. The electrode was mounted on one end side so that the distance L1 covering the electrode by changing the length of the insulating tube for the first insulating member was in the range of 0.1 mm to 6 mm. In addition, the insulating tube for the second insulating member is covered with the other end portion of the electrode so that the length S of the separation portion (electrode exposed portion) from the first insulating member is 3.5 mm (constant). It was attached. Thereafter, the glass tube on which the electrode and the insulating tube were mounted was heated to 150 to 200 ° C., and the first and second insulating members were disposed.
A lead wire having a wire length of about 1 mm was joined to the portion where the electrode was exposed at a portion where the first and second insulating members were separated from each other by aluminum solder.
In the above manufacturing process, the soldering operation can be easily performed, and the workability is very good without the electrodes being peeled off or deformed.
[0026]
[Comparative Example 1]
Comparative Example 1 according to the same procedure as in the above example except that the length L1 of the portion where the first insulating member covers the electrode is 0 mm (that is, the first insulating member is not disposed). A noble gas discharge lamp was manufactured. The insulating tube for the second insulating member is mounted so as to cover from the one end of the electrode to the other end side of the electrode from the required distance to the other end of the electrode. A second insulating member was disposed by exposing 3.5 mm.
A lead wire having a wire length of about 1 mm was joined to the portion where the electrode was exposed at one end of the electrode by aluminum solder.
In the manufacturing process described above, many electrodes were peeled off during the soldering operation. Also, one end of the electrode was easily peeled off, and the electrode was peeled and deformed during the handling of the lead wire in the subsequent manufacturing process.
[0027]
[Comparative Example 2]
A rare gas discharge lamp having a tube diameter of φ3 to φ5 mm was manufactured according to the following procedure in the manner of manufacturing a rare gas discharge lamp according to the prior art, that is, the procedure of first joining lead wires to electrodes and then covering the insulating tube.
An electrode was constructed by attaching an aluminum foil having a thickness of 0.5 mm, a length of 358 mm, and a width of 1.5 mm to a glass tube having a total length of 360 mm.
Next, a lead wire was joined with aluminum solder on the electrode at a position 3.5 mm away from one end of the electrode.
In the above manufacturing process, there are many cases where the electrode is distorted and peeled off during the soldering operation, and the electrode comes off during the operation after the lead wire is connected. Thus, the conventional rare gas discharge lamp has a high defect occurrence rate during the manufacturing process and has a problem in productivity.
[0028]
[Experimental example]
With respect to the rare gas discharge lamps according to the above Examples, Comparative Examples 1 and 2, the tensile strength of the lead wires was measured. Here, “the tensile strength of the lead wire” is the maximum tension when the lead wire is broken due to breakage of the lead wire joint portion, deformation of the electrode, or the like. In this experimental example, a load measuring device was attached to the lead wire, and the lead wire was pulled in a direction parallel to the tube axis.
[0029]
The results of the above experimental example are shown in FIG.
FIG. 4 is a diagram showing the relationship between the distance (L1 (mm) in FIG. 1) at which the first insulating member covers the electrode and the tensile strength (unit: N) of the lead wire showing the results of the above experimental example. is there. In FIG. 4, the average value of the measured values of the tensile strength (N) in the discharge lamps of the example and the comparative example 1 is given, and the approximate curve is drawn. Table 1 below shows average values obtained by measuring the tensile strength of lead wires for the rare gas discharge lamp of the comparative example.
[0030]
[Table 1]
Figure 0004063080
[0031]
As a result of Table 1, when the electrode to which the lead wire is connected is not covered with the insulating member, the tensile strength of the lead wire is about 2.98 N when the tube diameter is 5 mm, and 1.96 when the tube diameter is 4 mm. When the tube diameter was 3 mm, it was 0.98 which was less than 1N.
Thus, if the tensile strength is small, there is a very high probability of being defective during manufacture, and mass production is impossible. In addition, according to this experimental example, the present inventors have detected that if the tensile strength of the lead wire is 5N or more, preferably 8N or more, more preferably 10N or more, it is difficult to cause defects in the electrode during the handling of the lead wire. Got.
[0032]
As shown in FIG. 4, when the electrode coating length was 1 mm, the lead wire had a tensile strength of 10 N or more when the tube diameter was 5 mm, and it was confirmed that sufficiently high mechanical strength was obtained. Moreover, it turned out that the intensity | strength 3 times or more comes to be obtained compared with what the electrode which concerns on the comparative example 2 is not coat | covered with an insulating member at all. Furthermore, even when the tube diameter was 4 mm, it was found that the lead wire tensile strength could be increased to 8 N or more when the electrode coating length exceeded 1 mm.
[0033]
In addition, when the coating length of the electrode according to Comparative Example 1 is 0 mm, a slight strength improvement is recognized as compared with that according to Comparative Example 2, but the tensile strength of the lead wire is less than 5N. In actual work, the occurrence rate of defects was high and was not practically usable.
[0034]
As described above, according to the rare gas discharge lamp in which the lead wire joint is formed between the first insulating member and the second insulating member according to the present invention, the tensile strength of the lead wire can be increased. It has been found that the tensile strength of the lead wire can be increased and the productivity is good.
Furthermore, it has been found that when the electrode coating length is 1 mm or more, a strength as high as 8 N or more can be obtained.
[0035]
【The invention's effect】
As described above, according to the present invention, even if the electrode is narrow, the adhesion strength between the electrode and the glass tube is high, the lead wire can be easily routed, and a problem occurs in the lead-out portion for feeding the electrode. It is difficult to provide a rare gas discharge lamp.
As a result, it is possible to provide a rare gas discharge lamp with good productivity while realizing a compact rare gas discharge lamp.
[Brief description of the drawings]
FIG. 1 is a sectional view in the tube axis direction of a rare gas discharge lamp according to a first embodiment of the present invention.
2 is a cross-sectional view of a rare gas discharge lamp cut along a line AA in FIG. 1. FIG.
FIG. 3 is a diagram illustrating an embodiment of the present invention.
FIG. 4 is a diagram showing the relationship between the distance L1 and the tensile strength of a lead wire, showing the results of an experimental example.
[Explanation of symbols]
11 Glass tube 11A One end 11B The other end 21 One electrode 21A One end 21B The other end 22 The other electrode 22A One end 22B The other end 21S, 22S Electrode exposed portion 30 Phosphor layer 40 Aperture 50 Lead wire 51 Solder 52 Lead wire joint portion 61 First insulating member 62 Second insulating members 61A, 62A, 63A Insulating tube 64 Insulating member S for connecting S Separated portion H Opening hole

Claims (3)

希ガスが封入されたガラス管と、該ガラス管の外表面上に形成されたガラス管の長さ方向に延在する金属部材よりなる一方の電極と、該一方の電極に接合された給電用のリード線と、該一方の電極と少なくとも1つの誘電体を介して配置された他方の電極と、を具備してなり、
前記一方の電極は、該電極上において該電極の長さ方向に互いに離間し、熱収縮性を有するチューブよりなる第一の絶縁部材と第二の絶縁部材と、により被覆され、
前記第一の絶縁部材と第二の絶縁部材との離間部分において露出した電極にリード線の接合部が形成されていることを特徴とする希ガス放電灯。
A glass tube filled with a rare gas, one electrode made of a metal member extending in the length direction of the glass tube formed on the outer surface of the glass tube, and a power supply joined to the one electrode A lead wire, and the other electrode disposed through the one electrode and at least one dielectric,
The one electrode is covered with a first insulating member and a second insulating member which are separated from each other in the length direction of the electrode on the electrode and are made of a heat-shrinkable tube .
A rare gas discharge lamp, wherein a lead wire joint is formed on an electrode exposed at a separation portion between the first insulating member and the second insulating member.
前記第一の絶縁部材と前記第二の絶縁部材とをつなぐための接続用絶縁部材が形成されることを特徴とする請求項1記載の希ガス放電灯。Rare gas discharge lamp of claim 1 wherein said first insulating member and the second insulating member and the connecting insulating member for connecting is formed wherein Rukoto. 前記第一の絶縁部材及び第二の絶縁部材は、前記一方の電極をその長さ方向に1mm以上被覆していることを特徴とする請求項1または2に記載の希ガス放電灯。  The rare gas discharge lamp according to claim 1 or 2, wherein the first insulating member and the second insulating member cover the one electrode in the length direction by 1 mm or more.
JP2003002446A 2003-01-08 2003-01-08 Noble gas discharge lamp Expired - Fee Related JP4063080B2 (en)

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