JPS6182660A - Halogen bulb - Google Patents

Halogen bulb

Info

Publication number
JPS6182660A
JPS6182660A JP59203672A JP20367284A JPS6182660A JP S6182660 A JPS6182660 A JP S6182660A JP 59203672 A JP59203672 A JP 59203672A JP 20367284 A JP20367284 A JP 20367284A JP S6182660 A JPS6182660 A JP S6182660A
Authority
JP
Japan
Prior art keywords
light
film
envelope
halogen
bulb
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.)
Granted
Application number
JP59203672A
Other languages
Japanese (ja)
Other versions
JPH0439184B2 (en
Inventor
晃 川勝
狩野 利夫
弓削 洋二
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 by Toshiba Corp filed Critical Toshiba Corp
Priority to JP59203672A priority Critical patent/JPS6182660A/en
Priority to KR1019850006908A priority patent/KR890004640B1/en
Priority to US06/778,001 priority patent/US4721877A/en
Priority to DE8585306777T priority patent/DE3585008D1/en
Priority to EP85306777A priority patent/EP0176345B1/en
Priority to CA000491784A priority patent/CA1240219A/en
Priority to CN 85107840 priority patent/CN1020024C/en
Publication of JPS6182660A publication Critical patent/JPS6182660A/en
Priority to US07/098,884 priority patent/US4869927A/en
Publication of JPH0439184B2 publication Critical patent/JPH0439184B2/ja
Granted legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は高効率でしかも均一照明が可能なハロゲン電球
に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a halogen light bulb that is highly efficient and capable of providing uniform illumination.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

たとえば複写機用ハロゲン電球は複数のタングステンフ
ィラメントを短絡線を介して直列接宇売し、管形石英外
囲器内に同心的に封装しである。この電球は放射光中に
大暇の赤外線を含有して原稿を焼損するおそれがある。
For example, a halogen light bulb for a copying machine has a plurality of tungsten filaments connected in series through a short-circuit wire and concentrically sealed in a tubular quartz envelope. This light bulb contains a large amount of infrared rays in the emitted light, which may burn out the original.

そこで、外囲器の内外いずれかの面に可視光透過赤外線
反射膜を設けて赤外線放射を阻止するとともに、反射さ
れた赤外線をフィラメントに帰還されてこれを加熱し高
効率を得るようにした電球が開発された。この電球は放
射光中の赤外線が少ないため原稿を焼t1するおそれが
な(、シかも高効率である。また、彼照射面の照度分布
を均一にするため、フィラメント発光部を不連続にして
配置しであるが、これとて不充分であり、」二記高効率
ハロゲン電球の特性が充分に生かされていないっ また、1個の小形フィラメントをT形石英外囲器内に同
心的に封装した小形ハロゲン電球においても外囲器の内
外いずれかの面に同様な可視)℃透過赤外線反射膜を設
けることによって赤外線放射を、威らし、かつ高効率に
する技術が開発された。
Therefore, a visible light transmitting infrared reflecting film is provided on either the outside or the outside of the envelope to block infrared radiation, and the reflected infrared rays are returned to the filament to heat it and achieve high efficiency. was developed. This bulb is highly efficient, as there is little infrared rays in the emitted light, so there is no risk of burning the original.Also, in order to make the illumination distribution uniform on the irradiation surface, the filament light emitting part is discontinuous. However, this arrangement is insufficient and does not take full advantage of the characteristics of the high-efficiency halogen bulb. A technology has been developed to make the infrared radiation less intimidating and more efficient by providing a similar visible ()° C. transmitting infrared reflecting film on either the inside or outside of the envelope of a small sealed halogen light bulb.

このような′1πトドを反射鏡と組合せて用いると披照
射面にフィラメン1−の光学像が現出するため、照度分
布が不均一になる欠点がある。
When such a '1π star is used in combination with a reflecting mirror, an optical image of the filament 1- appears on the ray surface, which has the disadvantage that the illuminance distribution becomes non-uniform.

これに対し1本件出願人は先に透明外囲器の外面に可視
光透過赤外線反射膜を形成し、かつこの赤外線反射膜上
に散光膜を設けて、赤外線反射膜を透過した可視光を散
光膜で拡散して被照射面における照度分布を均一にする
技術を開発し、特願昭58−95001号として提案し
た。しかしながら、この技術をハロゲン電球に適用する
と、この電球の外囲器温度が非常に高いため、散光膜の
種類によっては長期の反覆点滅により、散光膜が剥離す
るおそれがあり、ハロゲン電球に適した散光膜の選定が
必要とされていた。
In contrast, the applicant first formed a visible light transmitting infrared reflective film on the outer surface of the transparent envelope, and provided a light scattering film on the infrared reflective film to diffuse the visible light that passed through the infrared reflective film. A technique was developed to uniformize the illumination distribution on the irradiated surface by diffusing the light through a film and proposed it in Japanese Patent Application No. 1983-95001. However, when this technology is applied to halogen bulbs, the bulb's envelope temperature is extremely high, so depending on the type of diffuser film, there is a risk that the diffuser film may peel off due to repeated flashing over a long period of time. It was necessary to select a light-diffusing film.

〔発明の目的〕[Purpose of the invention]

本発明は特願昭58−95001号提案の散光膜に所要
の限定を加えることにより同提案の効果を害することな
く、長期反復点滅しても散光膜が剥離するおそれのない
ハロゲン電球を提供することを目的とする。
The present invention provides a halogen light bulb in which the diffusion film proposed in Japanese Patent Application No. 58-95001 is free from peeling even after repeated flashing for a long period of time without impairing the effect of the proposal by adding necessary limitations to the diffusion film. The purpose is to

〔発明の概要〕 透明外囲器外面に設けた可視光透過赤外線反射膜上に多
孔質散光膜を形成したことにより、ハロゲン電球外囲器
の高温に起因する外囲器構成物質と散光膜構成物質との
熱膨張差による歪みを多孔質構造によって吸収して剥離
を防止したものである。
[Summary of the Invention] By forming a porous light scattering film on the visible light transmitting infrared reflecting film provided on the outer surface of the transparent envelope, the material constituting the envelope and the structure of the light scattering film caused by the high temperature of the halogen bulb envelope can be prevented. The porous structure absorbs distortion due to the difference in thermal expansion with the material, preventing peeling.

〔発明の実施例〕[Embodiments of the invention]

本発明のiiY′綱を図示の実施例によって説明する。 The iiY' class of the present invention will be explained with reference to the illustrated embodiments.

図は本発明を適用してなる複写機用ハロゲン電球の一例
を示し、図中、(1)は石英ガラスなどの透明耐熱性ガ
ラスからなる直管形外囲器、(2)はこの外囲器(1)
の外面に形成された可視光透過赤外線反射膜、(3)は
この反射@(2)上に形成された多孔質散光膜、(4)
、(4)は外囲器(1)の両端部を圧潰封止してなる封
止部、(5)、(5)はこれら封止部(4)。
The figure shows an example of a halogen light bulb for a copying machine to which the present invention is applied. Vessel (1)
A visible light transmitting infrared reflective film formed on the outer surface of (3) is a porous light diffusing film formed on this reflection @ (2), (4)
, (4) are sealing parts formed by crushing and sealing both ends of the envelope (1), and (5) and (5) are these sealing parts (4).

(4)内に埋設されたモリブデン導入箔、(6)、(6
)はこれら導入箔(5)、(5)に接続して外囲器(1
)内に延在した内導線、(7)、(7)・・・はこれら
内導線(6)、(6)間に短絡線(8)、(8)・・・
を介して直列接続されて外囲器(1)のほぼ中心線に位
置する複数のフィラメント、(9)、(9)・・・は短
絡FA(8)、(8)を支持するアンカ、(10)、(
10)は導入箔(5)、(5)に図示しない外心、線を
介し接続して外囲器(1)の両端面に装着された口金で
ある。そして、外囲器(1)内にはアルゴンなどの不活
性ガスとともに所要のハロゲンを封入しである。
Molybdenum introduced foil embedded in (4), (6), (6
) is connected to these introduction foils (5) and (5) to form an envelope (1).
), the inner conductors (7), (7)... are short-circuit wires (8), (8)... between these inner conductors (6), (6).
A plurality of filaments (9), (9) . 10), (
Reference numeral 10) designates caps that are connected to the introduction foils (5) and (5) via a wire (not shown) at the outer center and attached to both end surfaces of the envelope (1). The envelope (1) is filled with a necessary halogen along with an inert gas such as argon.

上記赤外線反射膜(2)は第2図に模型的に示すように
酸化チタン(Ti02)などからなる高光屈折率ff1
(2a) (左上リハッチング)とシリカ(SiO□)
などからなる低光屈折率層(2b) (右上リハッチン
グ)とを交互重層してなる多重層膜で、光の干渉により
可視光を良く透過し、赤外線を良く反射する性質を有す
る。なお1図では誇張して示したが各層(2a) 、 
(2b)の厚さは0.2〜0.3μが適当である。
The infrared reflecting film (2) is made of titanium oxide (Ti02) or the like and has a high optical refractive index ff1, as schematically shown in FIG.
(2a) (Top left rehatching) and silica (SiO□)
It is a multilayer film formed by alternately layering low light refractive index layers (2b) (rehatching on the upper right), etc., and has the property of transmitting visible light well and reflecting infrared rays well due to light interference. Although shown exaggerated in Figure 1, each layer (2a),
The appropriate thickness of (2b) is 0.2 to 0.3μ.

上記散光膜(3)は種々のものが考えら′れるが。Various types of light-diffusing film (3) can be considered.

その1例を第3図に模型的に示す。すなわち、この膜(
3)は金属酸化物からなる連続膜体(31)に多数の気
泡(32) 、 (32)・・を内蔵し、かつ膜体(3
1)表面にはこの気泡の変形である多数の円形凹孔(3
3)。
One example is schematically shown in FIG. That is, this film (
3) has a continuous film body (31) made of metal oxide with many bubbles (32), (32)...
1) The surface has many circular concave holes (3
3).

(33)・・・が形成されている。そうして、このよう
な気泡(32)や凹孔(33)によって透過光が散乱さ
れる。
(33)... is formed. The transmitted light is then scattered by such bubbles (32) and recesses (33).

そうして、このような金属酸化物の例としては酸化チタ
ン(Fi02) 、シリカ(Si02) 、アルミナ(
AQ20:+)、ジルコニア(ZrO2)、亜鉛華(Z
nO)、酸化タンタル(Ta205)、酸化!(Sn0
2)、酸化インジウム(In20a)などが適当である
Examples of such metal oxides include titanium oxide (Fi02), silica (Si02), and alumina (
AQ20:+), zirconia (ZrO2), zinc white (Z
nO), tantalum oxide (Ta205), oxidation! (Sn0
2), indium oxide (In20a), etc. are suitable.

つぎに、この電球の12造方法を直脱する。まず。Next, we will go straight from the 12 methods of making light bulbs. first.

通常の方法で管形ハロゲン電球を装作する。一方、テ1
−ライソプ口ピルチタネートを主成分とする有機チタン
化合物を酢酸エステルを主成分とする有機溶剤に溶解し
、チタン含有量2〜10重量%。
Install the tubular halogen bulb in the usual way. On the other hand, Te1
- An organic titanium compound whose main component is pyrutitanate is dissolved in an organic solvent whose main component is acetic acid ester, and the titanium content is 2 to 10% by weight.

粘度約1.ocpsに調整したチタン液を用意する。そ
して、このチタン液に上述のハロゲン電球を浸漬とて約
30cm/分の速度で引上げ、乾燥し、焼成して酸化チ
タンからなる高光屈折率層(2a)を形成する。
Viscosity approximately 1. Prepare titanium liquid adjusted to OCPS. Then, the above-mentioned halogen bulb is immersed in this titanium liquid, pulled up at a speed of about 30 cm/min, dried, and fired to form a high optical refractive index layer (2a) made of titanium oxide.

他方、エチルシリケートを主成分とする有機シリコン化
合物を酢酸エステルを主成分とする有機溶剤に溶解し、
シリコン含有量2〜10重量%、粘度約1.0cpsに
調整したシリコン液を用意する。
On the other hand, an organic silicon compound containing ethyl silicate as the main component is dissolved in an organic solvent containing acetate as the main component,
A silicone liquid adjusted to have a silicon content of 2 to 10% by weight and a viscosity of about 1.0 cps is prepared.

そして、上述の高光屈折率層(2a)を形成したハロゲ
ン電球をこのシリコン液に浸漬して約35cm/分の速
度で引上げ、乾燥し、焼成してシリカからなる低光屈折
率層(2b)を形成する。このようにして、高光屈折率
層(2a)と低光屈折率層(2b)とを合計10層程度
交互に形成し、赤外線反射膜(2)を構成する。
Then, the halogen bulb with the above-mentioned high optical refractive index layer (2a) formed thereon is immersed in this silicone liquid, pulled up at a speed of about 35 cm/min, dried, and fired to form the low optical refractive index layer (2b) made of silica. form. In this way, a total of about ten layers of high optical refractive index layers (2a) and low optical refractive index layers (2b) are alternately formed to constitute an infrared reflective film (2).

さらに、上述の例えば有機チタン化合物の低沸点有機溶
剤溶液に高沸点有機溶剤たとえばフタル酸ジー2−エチ
ルヘキシル(フタル酸ジオクチル。
Furthermore, a high boiling point organic solvent such as di-2-ethylhexyl phthalate (dioctyl phthalate) is added to the above-mentioned solution of the organic titanium compound in a low boiling point organic solvent.

略称DoP)を5〜10容量%添加し、これを低沸点有
機溶剤を加えて適宜の濃度に薄める。そうして、この液
に上述の赤外線反射膜(2)を形成したハロゲン電球を
f1清し、30〜50cm/分の速度で引上げ、乾燥し
、空気中で600 ’Cで約5分間焼成して酸化チタン
からなる散光膜(3)に形成する。しかして、上述のD
OPは無色油状の液体で、5wwnHgの圧力で231
℃で沸騰し、各種低沸点有機溶剤と任意割合いで相互溶
解する。したがって、乾燥工程においては、低沸点有機
溶剤が蒸発するだけで、DOPは有機チタン化合物のゲ
ル状塗膜中に微小液滴となって分散する。そうして、焼
成工程に1むいて、微小液滴は蒸発して気泡となり、有
機チタン化合物が酸化物に変成するとともに気泡が生長
する。特に、表面近くの気泡は凹孔となり、この孔内か
らも蒸発するため急速に大径となる。しかして、DOP
の蒸発温度と有機チタン化合物の分M温度とが接近して
いるため、気泡や凹孔が生長していく過程において有機
チタン化合物分解が開始され、これらの気泡や凹孔を含
んだまま酸化物膜体(31)に形成される。しかして、
塗液の粘度調整によって塗膜を厚くすれば気泡(32)
や凹孔(33)が大きく成長するが、その反面、凹孔(
33)は浅くなって光拡jT!性が劣るものとなる。
5 to 10% by volume of DoP (abbreviated as DoP) is added, and this is diluted to an appropriate concentration by adding a low boiling point organic solvent. Then, the halogen bulb with the above-mentioned infrared reflective film (2) formed in this solution was subjected to f1 cleaning, pulled up at a speed of 30 to 50 cm/min, dried, and baked in air at 600'C for about 5 minutes. Then, a light scattering film (3) made of titanium oxide is formed. However, the above D
OP is a colorless oily liquid with a pressure of 231
It boils at ℃ and is mutually soluble with various low-boiling point organic solvents in arbitrary proportions. Therefore, in the drying process, the low boiling point organic solvent is simply evaporated, and DOP is dispersed in the form of minute droplets in the gel-like coating film of the organic titanium compound. Then, during the firing step, the minute droplets evaporate and become bubbles, and the organic titanium compound is transformed into an oxide and the bubbles grow. In particular, bubbles near the surface form concave pores, and evaporate from within these pores, resulting in a rapid increase in diameter. However, D.O.P.
Since the evaporation temperature of the organic titanium compound and the M temperature of the organic titanium compound are close to each other, decomposition of the organic titanium compound starts in the process of the growth of bubbles and pores, and the oxide is formed while containing these bubbles and pores. It is formed on the membrane body (31). However,
If the coating film is made thicker by adjusting the viscosity of the coating liquid, air bubbles (32)
The concave hole (33) grows large, but on the other hand, the concave hole (33) grows large.
33) becomes shallower and the light expands jT! It becomes inferior in quality.

これに反し、塗膜を簿くすれば気泡(32)や凹孔(3
3)は小さいままで残るので、このような薄い散光膜を
数層重ねて形成してもよい。
On the other hand, if the coating film is kept clean, air bubbles (32) and concave holes (3
Since 3) remains small, several layers of such thin light-diffusing films may be stacked.

実験によれば5薄い散光膜体(31)を数層重層して厚
さ約0.5〜1μの散光膜(3)に形成して電子顕微鏡
で測定したところ、1 mm2当り2〜6万個の気泡(
32)や凹孔(33)が認められ、薄いにもかかわらず
、散光性に優れ、しかも赤外線反射膜(2)には拠り4
H的にも光学的にも何んの異状も認められなかった。
According to experiments, several layers of 5 thin light-diffusing films (31) were stacked to form a light-diffusing film (3) with a thickness of about 0.5 to 1μ, and measurements using an electron microscope revealed that the light scattering film (3) was 20,000 to 60,000 per 1 mm2. bubbles (
32) and concave holes (33) are observed, and although it is thin, it has excellent light scattering properties, and the infrared reflective film (2)
No abnormality was observed either in terms of H or optical.

つぎに、二のハロゲン電球の作用を説明する。Next, we will explain the second function of the halogen light bulb.

端子(10) 、 (to)間に通電してフィラメント
(7) 、 (7)・・ヲ発光させる。すると、フィラ
メン1〜(7) 、 (7)・・から放射された光のう
ち、赤外線は赤外線反射膜(2)によって反射され、そ
のかなりの量かフィラメント(7) 、 (7)  に
帰還してこれを加熱し、効パで向上に役立つ。また、赤
外線反射し′!(2)を透過した可視光は肢)1コ股(
3)によって拡散され、故乱光となって放射される。し
たがって、この電球は波照n−を而の照度分布が均一で
あり、また1反射鏡と組合わせて用いてもフィラメント
(7)の光学像が現れることがない。
Electricity is passed between the terminals (10) and (to) to cause the filaments (7) and (7) to emit light. Then, among the light emitted from filaments 1 to (7), (7), the infrared rays are reflected by the infrared reflecting film (2), and a considerable amount of it returns to the filaments (7), (7). This heats it up and helps improve its effectiveness. It also reflects infrared rays! The visible light transmitted through (2) is
3) and is emitted as scattered light. Therefore, this light bulb has a uniform illuminance distribution, and even when used in combination with one reflecting mirror, no optical image of the filament (7) appears.

さらに1本ハロゲン電球においては散光1役(3)に多
数の2泡(32)やその変形である凹孔(33)が存在
するので、ハロゲン電球外囲C(1)が高温に熱せられ
、外囲器(1)素はと散光膜(3)の酸fヒチタンとの
πさ膨張差が大きくなっても、その歪みが気泡(32)
や凹孔(33)によって吸収されるので、長期反r点減
しても散光膜(3)が剥雛することかない、さらに、本
実施例電球においては散)lコ膜(3)の厚さが0.5
〜1μで(→1めて薄いことも歪み緩和に設\″fち、
1りν;1し、ない原因になる。
Furthermore, in a single halogen bulb, there are a large number of 2 bubbles (32) and a concave hole (33) that is a modification of the 2 bubbles (33) in the diffuser 1 role (3), so the halogen bulb outer envelope C (1) is heated to a high temperature. Even if the difference in pi size expansion between the envelope (1) element and the acid f titanium of the light diffusing film (3) becomes large, the distortion will cause bubbles (32)
Since the light is absorbed by the diffuser and the concave hole (33), the diffuser film (3) will not peel off even if the light point is reduced over a long period of time. Saga 0.5
~1μ (→1 Thinness is also designed to alleviate distortion,
1 ri ν; 1 and causes no.

つぎに、」−記実施1り11に屈する定格150V 2
50Wの複写機用ハロゲン電球について散光膜・露(3
)を形成する萌と形成した後とのホ+I+方向の照度分
布を比やコしまた。このj+、7 lT−を第・1図に
示す。図は横軸に電ト1(の中央勺0どしで軸方向の距
*IC’j” R11の単位でとり、縦「1・111に
照度を中す、一部を100とする(・■対質でと一〕た
ちので、+Il+ ’i帛へ(実線で示す7)は散光し
’j(3)を+r6成したもの1曲腺B(破除で示す。
Next, the rated 150V 2
Diffusion film/dew (3) for 50W halogen light bulb for copying machine
) and compare the illuminance distribution in the H+I+ direction between the time of formation and the time after formation. This j+, 7 lT- is shown in Figure 1. In the figure, the horizontal axis is the distance in the axial direction between the center of the electric light 1 (0 and 0 * ■In the opposite substance and one], +Il+ 'i to the sheet (7 shown by the solid line) is diffused, and 'j (3) is +r6, which is 1 curved gland B (shown by the rupture).

)は1及光11;’1(F)を形成する前のそれぞれの
照度分布を示す。
) shows the respective illuminance distributions before forming the 1st beam 11;'1 (F).

この図か17.散光11;’j (3)の形成により照
度分布が均°にlCったことが1111庁j′できろ。
This figure 17. The formation of diffused light 11;'j (3) made the illuminance distribution uniform.

また、敗i’61E:i (:’! )形n(1前後)
電fp(7)明るさく全光重)f!:比較したところ、
1汝光膜(3)形成による九束何、下は2〜3゛3う程
度に過ぎず、ソこ損失の少ないことも木uQ尤+V;t
 (:’、 )の特徴である4な、、1y、 、+、’
a明は「形ガラス外!I’l a7\)G形ガラス外囲
器を用いたハロゲン電球にも適用でき、T形外囲器の弓
合はフィラメントをほぼ同心的に配設すればよく、゛G
形外囲器の場合は球状部の中心近所に配設すればよい。
Also, defeat i'61E:i (:'!) form n (around 1)
Electric fp (7) Brightness and full light weight) f! : When compared,
1) The formation of the light film (3) causes only about 2~3゛3 damage, and the loss is also small.
The characteristics of (:', ) are 4,,1y, ,+,'
A-mei can also be applied to halogen bulbs using a G-shaped glass envelope, and the arc of the T-shaped envelope can be arranged by arranging the filaments almost concentrically. ,゛G
In the case of a shaped envelope, it may be placed near the center of the spherical part.

さらに、本発明は閉塞または非閉塞形の管形透明外囲器
の外面に上述のとおり可視光透過赤外X′i!反’17
11:、Tと多孔質散光膜とを重層して設け、かつ外v
JJ器の中心部に赤外線反射膜も散光膜もない・ご通の
管形ハロゲン電球を設けたものでもよい。
Furthermore, the present invention provides the visible light transmitting infrared X'i! anti'17
11: T and a porous light scattering film are provided in a layered manner, and an outer v
The center of the JJ device may have neither an infrared reflective film nor a diffuser film, and may be equipped with a common tube-shaped halogen light bulb.

〔発明の効果〕〔Effect of the invention〕

本発明のハロゲン電球は透明外囲8:(の外面に可視光
透過赤外線反射膜を設け、かつこの反射膜上に多孔質散
光膜を設けたので、赤外線放射が少なく、高効率で、被
照射面の照度分布が均一で、反射鏡と組合わせて用いて
もフィラメントの光学像を現示するおそれがなく、しか
も、外囲器が高温にタヘせられるにもかかわらず、長期
反覆点滅しても散光膜が利はするおそれがない利点があ
る。
The halogen light bulb of the present invention has a visible light transmitting infrared reflective film on the outer surface of the transparent envelope 8, and a porous diffuser film is provided on the reflective film, so that it emits less infrared rays, has high efficiency, and can be irradiated. The illuminance distribution on the surface is uniform, there is no risk of displaying an optical image of the filament even when used in combination with a reflector, and even when the envelope is exposed to high temperatures, it does not blink repeatedly for a long period of time. There is also an advantage that there is no possibility that the light diffusing film will be used.

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

第1図は本発明のハロゲン電球の一実施例の断第  1 面図、第2図は第1114’i’i線伜1部分の模型的
拡大断面図、第3図は同じく散光膜の模型的拡大断面図
、第4図は本実施例電球の散光膜の効果を示すグラフで
ある。
FIG. 1 is a cross-sectional first view of an embodiment of the halogen light bulb of the present invention, FIG. 2 is a schematic enlarged cross-sectional view of a portion taken along line 1114'i'i, and FIG. 3 is a model of the light-diffusing film. FIG. 4 is a graph showing the effect of the light-diffusing film of the light bulb of this example.

Claims (2)

【特許請求の範囲】[Claims] (1)透明外囲器と、この外囲器の外面に形成された可
視光透過赤外線反射膜と、この赤外線反射膜上に形成さ
れた多孔質散光膜と、上記外囲器の中心部に配設された
フィラメントとを具備したことを特徴とするハロゲン電
球。
(1) A transparent envelope, a visible light-transmitting infrared reflective film formed on the outer surface of the envelope, a porous light-diffusing film formed on the infrared reflective film, and a central part of the envelope. A halogen light bulb characterized by comprising a filament arranged therein.
(2)散光膜は気泡を内蔵して散光性を呈することを特
徴とする特許請求の範囲第1項記載のハロゲン電球。
(2) The halogen light bulb according to claim 1, wherein the light-diffusing film has bubbles incorporated therein to exhibit light-diffusing properties.
JP59203672A 1984-09-28 1984-09-28 Halogen bulb Granted JPS6182660A (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP59203672A JPS6182660A (en) 1984-09-28 1984-09-28 Halogen bulb
KR1019850006908A KR890004640B1 (en) 1984-09-28 1985-09-19 A light diffusive coating a method of forming the coating and a lamp having the coating
US06/778,001 US4721877A (en) 1984-09-28 1985-09-20 Light diffusive coating and a lamp having the coating
DE8585306777T DE3585008D1 (en) 1984-09-28 1985-09-24 A LIGHT-DISPENSING COVER AND ITS PRODUCTION AND LAMP WITH THIS COVER.
EP85306777A EP0176345B1 (en) 1984-09-28 1985-09-24 A light diffusive coating and its formation and a lamp having the coating
CA000491784A CA1240219A (en) 1984-09-28 1985-09-27 Light diffusive coating, a method of forming the coating, and a lamp having the coating
CN 85107840 CN1020024C (en) 1984-09-28 1985-10-25 Light scattering coating, method of forming coating and lamp having coating
US07/098,884 US4869927A (en) 1984-09-28 1987-09-21 Light diffusive coating, a method of forming the coating and a lamp having the coating

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59203672A JPS6182660A (en) 1984-09-28 1984-09-28 Halogen bulb

Publications (2)

Publication Number Publication Date
JPS6182660A true JPS6182660A (en) 1986-04-26
JPH0439184B2 JPH0439184B2 (en) 1992-06-26

Family

ID=16477936

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59203672A Granted JPS6182660A (en) 1984-09-28 1984-09-28 Halogen bulb

Country Status (1)

Country Link
JP (1) JPS6182660A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003070938A (en) * 2001-09-03 2003-03-11 Bridgestone Sports Co Ltd Golf club set
JP2006522445A (en) * 2003-04-07 2006-09-28 コーニンクレッカ フィリップス エレクトロニクス エヌ ヴィ lighting equipment

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS518785A (en) * 1974-07-11 1976-01-23 Fuji Electric Co Ltd HAKUNETSUDENKYUOMOCHIITASHOMEIKIGU
JPS5713099A (en) * 1980-06-23 1982-01-23 Shin Meiwa Ind Co Ltd Housing guiding apparatus for boom of service car

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS518785A (en) * 1974-07-11 1976-01-23 Fuji Electric Co Ltd HAKUNETSUDENKYUOMOCHIITASHOMEIKIGU
JPS5713099A (en) * 1980-06-23 1982-01-23 Shin Meiwa Ind Co Ltd Housing guiding apparatus for boom of service car

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003070938A (en) * 2001-09-03 2003-03-11 Bridgestone Sports Co Ltd Golf club set
JP2006522445A (en) * 2003-04-07 2006-09-28 コーニンクレッカ フィリップス エレクトロニクス エヌ ヴィ lighting equipment

Also Published As

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