JPH0341404Y2 - - Google Patents

Info

Publication number
JPH0341404Y2
JPH0341404Y2 JP3608586U JP3608586U JPH0341404Y2 JP H0341404 Y2 JPH0341404 Y2 JP H0341404Y2 JP 3608586 U JP3608586 U JP 3608586U JP 3608586 U JP3608586 U JP 3608586U JP H0341404 Y2 JPH0341404 Y2 JP H0341404Y2
Authority
JP
Japan
Prior art keywords
filament
measurement
light
incandescent
power consumption
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
Application number
JP3608586U
Other languages
Japanese (ja)
Other versions
JPS62149162U (en
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP3608586U priority Critical patent/JPH0341404Y2/ja
Publication of JPS62149162U publication Critical patent/JPS62149162U/ja
Application granted granted Critical
Publication of JPH0341404Y2 publication Critical patent/JPH0341404Y2/ja
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】[Detailed explanation of the idea]

〔産業上の利用分野〕 本考案は、光を利用した種々の計測機器、特に
ポータブルタイプの計測機器用光源として最適な
計測用白熱電球に関するものである。 〔考案の背景〕 光、特に赤外域の光は種々の計測機器において
計測用光源として用いられ、例えばガス濃度計測
機器においては、計測に係るガス中に赤外線を投
射し、当該ガスによる固有の赤外線の吸収量を計
測し、ガス濃度が計測される。 このようなガス濃度計測機器の光源としては、
その吸収波長が近赤外域にあるガスの場合は、バ
ルブを石英で構成したキセノン放電灯や白熱電球
等が用いられるが、炭酸ガスのように吸収波長が
遠赤外域にあるものは黒体放射を利用した黒体炉
が用いられる。 〔考案が解決しようとする問題点〕 前記黒体炉は、キセノン放電灯や白熱電球のよ
うに石英バルブを必要とせず、従つて近赤外から
遠赤外に亘つて広い範囲の光を放射するので、計
測用光源としては理想的であるが、一般的に大型
であり、小型の計測機器、特に持ち運び可能なポ
ータブルタイプの計測機器には適用することがで
きなかつた。 〔問題点を解決するための手段〕 本考案は、単結晶アルミナ管よりなる封体と、
この封体内に設けられたフイラメントとを具え、
10〜30Wの消費電力で点灯される白熱電球であつ
て、前記フイラメントは、長さが2mm以内かつ外
径が2mm以内であり、作動時前記フイラメントの
温度が1800〜2800Kであることを特徴とする。 〔作用〕 斯かる構成によれば、封体が単結晶アルミナ管
よりなり、この単結晶アルミナは赤外域の光を相
当幅広い範囲に亘つて透過するので、赤外域にお
いて幅広い分光放射特性を有し、しかもフイラメ
ントサイズは長さが2mm以内かつ外径が2mm以内
であるので、10〜30Wの低消費電力でも作動時の
フイラメント温度が1800〜2800Kとなり、赤外域
の分光放射強度を高くすることができる。 〔実施例〕 以下図面を参照しながら本考案を詳細に説明す
る。 第1図は本考案に係る計測用白熱電球の一実施
例を示す。 1は封体、2はフイラメント、3および4はリ
ードである。 封体1は、例えば筒状でその全体が単結晶アル
ミナ管よりなる透光部分10と、この透光部分1
0の両端をそれぞれ気密に塞ぐ例えば金属製の口
金11および12とよりなる。具体的には、透光
部分10の端部13および14の外壁に金属層を
固着し、そしてこれらの金属層のそれぞれと口金
11および12とを例えばロウ接により気密に接
続して封体1を形成することができる。 フイラメント2は、例えばタングステンよりな
り、その両端はそれぞれリード3および4を介し
て口金11および12に接続されている。このフ
イラメント2は単コイルもしくは二重コイル状で
あり、その軸方向の長さLは2mm以内、その外径
Dは2mm以内である。このフイラメント2を発熱
させるときには、消費電力が10〜30Wとなるよう
に制御された電流および電圧で通電する。すなわ
ち、フイラメント2としてその大きさが既述の範
囲内のものを用いるときには、10〜30Wの消費電
力でフイラメント2をその温度が1800〜2800Kと
なるように適正に発熱させることができる。消費
電力が過大のときにはフイラメント2の過熱によ
り電球の使用寿命が短くなる場合があり、一方消
費電力が過小のときには放射強度が小さくて計測
に十分な強度の光が得られない場合がある。 また10〜30Wの電力の供給は市販のバツテリー
によつて十分容易に達成することができ、ポータ
ブルタイプの計測用光源とては理想的である。さ
らにフイラメント2の大きさが小さいため、集光
効率を高くでき、高エネルギー密度の小径のビー
ム形成が容易である。 第2図において、曲線Iは単結晶アルミナ(厚
さ:2mm)の分光透過率を示し、曲線は比較用
としての石英(厚さ:2mm)の分光透過率を示
す。同図から理解されるように、単結晶アルミナ
は、赤外域の広い範囲に亘り高い透過率を示すも
のであるのに対し、封体用ガラスとして一般に用
られている石英は、遠赤外域の透過率が単結晶ア
ルミナに比して格段に低いものである。 また同図に伴せて示した、フイラメント温度が
それぞれ1800K、2300K、2800Kにおける分光放
射強度(相対値)曲線から理解されるように、フ
イラメント温度が1800〜2800Kの範囲内にあると
きには、分光放射強度が高くて実用上十分な放射
を得ることができる。 次に、具体的に行つた点灯実験について説明す
る。 〈フイラメントの構成〉 〇 フイラメントの長さ:1.7mm 〇 フイラメントの外径:1.2mm 〇 コイルの素線径:0.2mm 〇 コイルの巻数:5.0ターン 〇 コイルのピツチ:140% 上記構成のフイラメントを具えた本考案に係る
計測用白熱電球を多数作製し、各電球のフイラメ
ントへ供給する電圧および電流を種々の値に設定
して連続点灯する実験を行い、フイラメントの温
度と使用寿命(点灯初期の明るさの80%に低下す
るまでの点灯時間)との関係を調べた。結果を下
記第1表に示す。
[Industrial Application Field] The present invention relates to an incandescent light bulb for measurement that is optimal as a light source for various measuring instruments that utilize light, particularly portable measuring instruments. [Background of the invention] Light, especially light in the infrared region, is used as a measurement light source in various measuring instruments. For example, in gas concentration measuring instruments, infrared rays are projected into the gas involved in measurement, and the unique infrared rays of the gas are emitted. The gas concentration is measured by measuring the amount of gas absorbed. The light source for such gas concentration measuring equipment is
For gases whose absorption wavelength is in the near-infrared region, xenon discharge lamps or incandescent lamps with bulbs made of quartz are used, but for gases whose absorption wavelength is in the far-infrared region, such as carbon dioxide, blackbody radiation is used. A blackbody furnace using . [Problems to be solved by the invention] The blackbody furnace does not require a quartz bulb like a xenon discharge lamp or an incandescent lamp, and therefore emits light in a wide range from near infrared to far infrared. Therefore, although it is ideal as a measurement light source, it is generally large and cannot be applied to small measurement equipment, especially portable type measurement equipment. [Means for solving the problem] The present invention includes an enclosure made of a single crystal alumina tube,
a filament provided within the envelope;
An incandescent light bulb that is lit with a power consumption of 10 to 30 W, wherein the filament has a length of 2 mm or less and an outer diameter of 2 mm, and the temperature of the filament during operation is 1800 to 2800 K. do. [Function] According to this configuration, the envelope is made of a single-crystal alumina tube, and since this single-crystal alumina transmits light in the infrared region over a fairly wide range, it has a wide range of spectral radiation characteristics in the infrared region. Moreover, since the filament size is within 2 mm in length and within 2 mm in outer diameter, the filament temperature during operation is 1800 to 2800 K even with low power consumption of 10 to 30 W, making it possible to increase the spectral radiation intensity in the infrared region. can. [Example] The present invention will be described in detail below with reference to the drawings. FIG. 1 shows an embodiment of an incandescent light bulb for measurement according to the present invention. 1 is an envelope, 2 is a filament, and 3 and 4 are leads. The enclosure 1 includes, for example, a cylindrical transparent portion 10 made entirely of a single-crystal alumina tube, and the transparent portion 1.
It consists of caps 11 and 12 made of metal, for example, which hermetically close both ends of the cap. Specifically, a metal layer is fixed to the outer walls of the ends 13 and 14 of the transparent portion 10, and each of these metal layers and the caps 11 and 12 are hermetically connected, for example, by brazing, to form the enclosure 1. can be formed. The filament 2 is made of tungsten, for example, and its both ends are connected to the bases 11 and 12 via leads 3 and 4, respectively. The filament 2 is in the form of a single coil or a double coil, and its axial length L is within 2 mm, and its outer diameter D is within 2 mm. When the filament 2 is made to generate heat, it is energized with a current and voltage controlled so that the power consumption is 10 to 30W. That is, when using a filament 2 whose size is within the above-mentioned range, the filament 2 can be appropriately heated to a temperature of 1800 to 2800K with power consumption of 10 to 30W. When the power consumption is too high, the service life of the light bulb may be shortened due to overheating of the filament 2. On the other hand, when the power consumption is too low, the radiation intensity is so small that light of sufficient intensity for measurement may not be obtained. Furthermore, the supply of power of 10 to 30 W can be easily achieved using a commercially available battery, making it ideal for a portable measurement light source. Furthermore, since the filament 2 is small in size, the light collection efficiency can be increased, and it is easy to form a small diameter beam with high energy density. In FIG. 2, curve I shows the spectral transmittance of single crystal alumina (thickness: 2 mm), and the curve I shows the spectral transmittance of quartz (thickness: 2 mm) for comparison. As can be understood from the figure, single-crystal alumina exhibits high transmittance over a wide range of infrared regions, whereas quartz, which is commonly used as glass for enclosures, has high transmittance in the far-infrared region. Its transmittance is much lower than that of single crystal alumina. In addition, as can be understood from the spectral radiant intensity (relative value) curves at filament temperatures of 1800K, 2300K, and 2800K shown in the same figure, when the filament temperature is within the range of 1800 to 2800K, the spectral radiant It has high intensity and can provide sufficient radiation for practical use. Next, a lighting experiment conducted specifically will be described. <Filament configuration> 〇 Filament length: 1.7mm 〇 Filament outer diameter: 1.2mm 〇 Coil strand diameter: 0.2mm 〇 Number of coil turns: 5.0 turns 〇 Coil pitch: 140% Equipped with a filament with the above configuration We fabricated a large number of measurement incandescent light bulbs according to the present invention, and conducted experiments in which the voltage and current supplied to the filament of each bulb were set to various values and the lights were lit continuously. We investigated the relationship between the lighting time (until the lighting time decreases to 80%). The results are shown in Table 1 below.

〔考案の効果〕[Effect of idea]

本考案の計測用白熱電球によれば、封体を単結
晶アルミナで構成し、フイラメントの長さを2mm
以内かつ外径を2mm以内としたので、10〜30Wの
低消費電力でフイラメント温度を1800〜2800Kに
できる。その結果、小型であるにもかかわらず、
赤外域の光を効率的に放射できる白熱電球である
ため、赤外域の光を利用する種々の計測機器、特
にポータブルタイプの計測用光源として最適に用
いることができる。
According to the incandescent light bulb for measurement of the present invention, the envelope is made of single crystal alumina, and the length of the filament is 2 mm.
Since the outer diameter is within 2 mm, the filament temperature can be increased to 1800 to 2800 K with low power consumption of 10 to 30 W. As a result, despite its small size,
Since it is an incandescent bulb that can efficiently emit light in the infrared region, it can be optimally used as a light source for various measurement devices that utilize light in the infrared region, especially portable types.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本考案の計測用白熱電球の一実施例を
示す説明用断面図、第2図は、単結晶アルミナの
分光透過率および比較用としての石英の分光透過
率ならびにフイラメント温度がそれぞれ1800K,
2300K,2800Kのときの分光放射強度(相対値)
を示す線図、第3図はガスの濃度を計測する場合
の適用例を示す説明図である。 1……封体、2……フイラメント、3,4……
リード、10……透光部分、11,12……口
金、51……計測用白熱電球、52……集光用反
射鏡、53……ビーム形成用レンズ、54……赤
外線透過フイルター、55……赤外線検出器、5
6……容器。
Figure 1 is an explanatory cross-sectional view showing one embodiment of the incandescent light bulb for measurement of the present invention, and Figure 2 shows the spectral transmittance of single crystal alumina, the spectral transmittance of quartz for comparison, and the filament temperature of 1800K. ,
Spectral radiant intensity at 2300K and 2800K (relative value)
FIG. 3 is an explanatory diagram showing an example of application in measuring the concentration of gas. 1... envelope, 2... filament, 3, 4...
Lead, 10...Transparent portion, 11, 12...Base, 51...Incandescent bulb for measurement, 52...Reflector for focusing, 53...Lens for beam formation, 54...Infrared transmission filter, 55... ...Infrared detector, 5
6...Container.

Claims (1)

【実用新案登録請求の範囲】 単結晶アルミナ管よりなる封体と、この封体内
に設けられたフイラメントとを具え、10〜30Wの
消費電力で点灯される白熱電球であつて、 前記フイラメントは、長さが2mm以内かつ外径
が2mm以内であり、作動時前記フイラメントの温
度が1800〜2800Kであることを特徴とする計測用
白熱電球。
[Claims for Utility Model Registration] An incandescent light bulb comprising an envelope made of a single-crystal alumina tube and a filament disposed within the envelope, which is lit with a power consumption of 10 to 30 W, the filament comprising: An incandescent lamp for measurement, characterized in that the length is within 2 mm and the outer diameter is within 2 mm, and the temperature of the filament during operation is 1800 to 2800 K.
JP3608586U 1986-03-14 1986-03-14 Expired JPH0341404Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3608586U JPH0341404Y2 (en) 1986-03-14 1986-03-14

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3608586U JPH0341404Y2 (en) 1986-03-14 1986-03-14

Publications (2)

Publication Number Publication Date
JPS62149162U JPS62149162U (en) 1987-09-21
JPH0341404Y2 true JPH0341404Y2 (en) 1991-08-30

Family

ID=30846167

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3608586U Expired JPH0341404Y2 (en) 1986-03-14 1986-03-14

Country Status (1)

Country Link
JP (1) JPH0341404Y2 (en)

Also Published As

Publication number Publication date
JPS62149162U (en) 1987-09-21

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