JPS585326Y2 - Reflector of square shield beam light bulb - Google Patents

Reflector of square shield beam light bulb

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Publication number
JPS585326Y2
JPS585326Y2 JP1978093663U JP9366378U JPS585326Y2 JP S585326 Y2 JPS585326 Y2 JP S585326Y2 JP 1978093663 U JP1978093663 U JP 1978093663U JP 9366378 U JP9366378 U JP 9366378U JP S585326 Y2 JPS585326 Y2 JP S585326Y2
Authority
JP
Japan
Prior art keywords
flat surface
reflector
paraboloid
revolution
reflecting mirror
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
JP1978093663U
Other languages
Japanese (ja)
Other versions
JPS5510277U (en
Inventor
橋谷田勝利
金松進
Original Assignee
株式会社小糸製作所
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 株式会社小糸製作所 filed Critical 株式会社小糸製作所
Priority to JP1978093663U priority Critical patent/JPS585326Y2/en
Publication of JPS5510277U publication Critical patent/JPS5510277U/ja
Application granted granted Critical
Publication of JPS585326Y2 publication Critical patent/JPS585326Y2/en
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は、新規な角形シールドビーム電球の反射鏡に関
し、特に、強度的に優れると共に省資源化及び軽量化を
図ることができ、更に配光品質上鋭い迷光の発生を皆無
にすることができる角形シールドビーム電球の反射鏡を
提供しようとするものである。
[Detailed description of the invention] The present invention relates to a reflector for a novel rectangular sealed beam light bulb, which has excellent strength, saves resources, and is light in weight, and also has an improved light distribution quality and does not generate sharp stray light. The purpose of this invention is to provide a reflector for a rectangular sealed beam light bulb that can completely eliminate this problem.

各国の自動車産業において、角形シールドビーム電球は
、そのデザイン上の斬新さからその開発に大きく力が入
れられるようになった。
In the automobile industry of various countries, great efforts have been put into the development of rectangular sealed beam light bulbs due to their novel design.

我国においても、当業界において、その開発が推し進め
られている。
In Japan as well, its development is being promoted in this industry.

現在、開発されている角形シールドビーム電球の反射鏡
aは、第1図に斜視図で示したもののように、基本的に
は丸形のシールドビーム電球の反射鏡すをその開口部側
(前方)から見て、横長の長方形を呈するように、上下
及び左右を切除して光軸と略平行を為す部分(平坦面部
)C2c、d、dを付加するという考え方によって形状
が確定されている。
The reflector a of the rectangular sealed beam light bulb currently being developed is basically a round sealed beam light bulb with its opening side (front ) The shape is determined by cutting off the top and bottom, left and right sides, and adding portions (flat surface portions) C2c, d, and d that are approximately parallel to the optical axis so that it has a horizontally long rectangle when viewed from ).

そして、このように形成された角形シールドビーム電球
の反射鏡aはその内面eにアルミ蒸着膜fが付与されて
反射面が形成される。
The reflecting mirror a of the rectangular sealed beam light bulb thus formed has an aluminum vapor deposited film f applied to its inner surface e to form a reflecting surface.

このアルミ蒸着膜fの形成は、例えば以下のようにして
行なわれる。
Formation of this aluminum vapor deposition film f is performed, for example, as follows.

即ち、第3図及び第4図に示されたように、一方が開口
gされた箱体りの内部に蒸発源となるフィラメントコイ
ルiが装置され且つ排気管jが形成されたアルミ蒸着ヘ
ッドにの開口部gにアルミ蒸着膜fを付与すべき反射鏡
aの開口端1を当接すると共に反射鏡すに形成された排
気管mを閉塞具nを用いて閉塞し、これによってアルミ
蒸着ヘッドにと反射鏡aとによって形成された空間0内
を密閉状にし、反射鏡aの内面へのアルミの蒸着を良く
する等のためにアルミ蒸着ヘッドkに形状された排気管
jを通して前記空間0内を高真空にする。
That is, as shown in FIGS. 3 and 4, a filament coil i serving as an evaporation source is installed inside a box body with an opening g on one side, and an aluminum evaporation head is provided with an exhaust pipe j. The opening end 1 of the reflector a to which the aluminum vapor deposition film f is to be applied is brought into contact with the opening g of the reflector, and the exhaust pipe m formed on the reflector is closed using a closing tool n. The inside of the space 0 formed by the reflector a and the reflector a is sealed, and in order to improve the vapor deposition of aluminum onto the inner surface of the reflector a, an exhaust pipe j formed in the aluminum vapor deposition head k is passed through the space 0. to high vacuum.

そして、アルミ蒸着ヘッドにのフィラメントコイルiに
導電し、そのフィラメントコイルi内に装填されている
アルミ箔pを蒸発させ、それを反射鏡aの内面に付着さ
せてアルミ蒸着膜fを形成する。
Electricity is then applied to the filament coil i of the aluminum evaporation head to evaporate the aluminum foil p loaded in the filament coil i and adhere it to the inner surface of the reflecting mirror a to form an aluminum evaporation film f.

反射鏡a内面へのアルミ蒸着膜fの付与は、そのほとん
どが上記のような方法によって行なわれているが、これ
には次のような種々の問題がある。
Most of the methods described above are used to apply the aluminum vapor deposition film f to the inner surface of the reflecting mirror a, but this method has the following various problems.

即ち、反射鏡aの内面eにアルミ蒸着膜fを付与する前
の工程で、アルミ蒸着効率を良くしたり、アルミニュウ
ムと不純ガスとが結合してアルミ蒸着膜fが変色するの
を避けたり、更には不純ガスとフィラメントコイルiと
が結合してタングステン酸化物となりこれによってフィ
ラメントコイルが燃えてしまうことを避けたりするため
に、反射鏡aとアルミ蒸着ヘッドにとによって形成され
る空間0内部を高真空にしているが、空間0内が高真空
化すると、特に左右の平坦面部d、dに比べて面積の大
きい上下の平坦面部c、cや平坦面部Cと回転放物面部
qとの境界部rに引張歪(応力)が集中してそれら平坦
面部C又は境界部rから破壊(爆縮)が生ずることがあ
る( 1000〜2000個に1個位の可成り高い比率
で起っている。
That is, in the step before applying the aluminum evaporation film f to the inner surface e of the reflecting mirror a, it is possible to improve the aluminum evaporation efficiency, to avoid discoloration of the aluminum evaporation film f due to combination of aluminum and impurity gas, Furthermore, in order to prevent the impure gas and the filament coil i from combining to form tungsten oxide and thereby burning the filament coil, the interior of the space 0 formed by the reflector a and the aluminum evaporation head is Although the vacuum is kept high, if the inside of the space 0 becomes high vacuum, the upper and lower flat surfaces c, c, which have a larger area than the left and right flat surfaces d, d, and the boundary between the flat surface C and the paraboloid of revolution q Tensile strain (stress) concentrates on part r, and fracture (implosion) may occur from the flat surface part C or boundary part r (occurs at a fairly high rate of about 1 in 1000 to 2000 pieces). .

)。そして、一旦破壊が生ずると、その破壊力が大きい
ために、反射鏡aの破片が飛散して危険であるばかりで
なく、蒸着装置も損傷を受は易く、しかも一時的にしろ
工程がストップすることになる。
). Once destruction occurs, the destructive force is so great that not only is it dangerous as fragments of the reflector a are scattered, but the vapor deposition equipment is also easily damaged, and the process will stop, even if only temporarily. It turns out.

そこで、従来は、反射鏡aの平坦面部c、dの肉厚を回
転放物面部qのそれと略等しくして平坦面部特に上下の
平坦面部Cを上記引張歪に対して強くすることを考えて
いたが、このようにすると、反射鏡aの質量が多くなっ
てそれだけ材料費が余分にかかると共に重量も多くなっ
て自動車重量の軽量化という自動車メーカーの要望に逆
行することにもなる。
Therefore, in the past, it has been considered to make the wall thicknesses of the flat surface parts c and d of the reflecting mirror a substantially equal to that of the paraboloid of revolution part q to strengthen the flat surface parts, especially the upper and lower flat surface parts C, against the above-mentioned tensile strain. However, if this is done, the mass of the reflector a increases, resulting in additional material costs and weight, which goes against the desire of automobile manufacturers to reduce the weight of automobiles.

又、平坦面部Cの肉厚が均一であると、ガラスを熱加工
した後その部分に残留する応力の大きさはガラスの肉厚
の2乗に比例するので、反射鏡自体の成形の際に平坦面
部Cに応力が残留し易くなり反射鏡aの強度が低下する
という問題がある。
In addition, if the wall thickness of the flat surface portion C is uniform, the magnitude of the stress remaining in that portion after the glass is thermally processed is proportional to the square of the glass wall thickness, so when forming the reflecting mirror itself, There is a problem that stress tends to remain in the flat surface portion C, and the strength of the reflecting mirror a decreases.

又、従来は、これとは別に、反射鏡aの平坦面部Cを反
射鏡aの後方に行くに従って光軸X−Xに近づくような
傾斜をもたせしかもその傾斜角度θを比較的大きくする
ことによって平坦面部Cに加わる引張歪を回転放物面部
qの方へ分散し、これによって上記引張歪に対する強度
を高くすることも考えられたが、反射鏡aの開口部の面
積は決まっているために前記傾斜角度θを大きくすれば
する程有効反射鏡である回転放物面部qの面積が小さく
なる欠点がある。
In addition, in the past, apart from this, the flat surface C of the reflecting mirror a is inclined so that it approaches the optical axis X-X as it goes to the rear of the reflecting mirror a, and the inclination angle θ is made relatively large. It was considered to disperse the tensile strain applied to the flat surface part C toward the paraboloid of revolution part q, thereby increasing the strength against the above tensile strain, but since the area of the opening of the reflecting mirror a is fixed, There is a drawback that the larger the inclination angle θ, the smaller the area of the paraboloid of revolution q, which is an effective reflecting mirror.

又、この種角形前照灯にあっては、他車の運転者や歩行
者に対する眩惑光となるいわゆる有害光線を遮断するた
めに、光源Sの前方の一部分と後方を除いた周囲にシー
ルド板tを設けるようにしているが、平坦面部Cの傾斜
角度θが大きくなればそれだけ平坦面部が光源Sの後方
に回り込んで来ることになるため、その分シールド板t
を光源Sに近づけなければならない。
In addition, in this type of rectangular headlight, a shield plate is installed around the light source S except for the front part and the rear part in order to block so-called harmful rays that dazzle drivers of other vehicles and pedestrians. However, as the inclination angle θ of the flat surface portion C increases, the flat surface portion will come around to the rear of the light source S, so the shield plate t is provided accordingly.
must be brought close to the light source S.

しかし、シールド板tを光源Sに近づけすぎると、シー
ルド板tの温度上昇によってシールド板tから不純ガス
の放出があり、そのガスがタングステンフィラメントコ
イルである光源Sと結合してタングステン酸化物となり
、フィラメントコイルの寿命特性に悪影響を及ぼすとい
う欠点がある。
However, if the shield plate t is brought too close to the light source S, impurity gas will be released from the shield plate t due to the temperature rise of the shield plate t, and this gas will combine with the light source S, which is a tungsten filament coil, and become tungsten oxide. There is a drawback that it has a negative effect on the life characteristics of the filament coil.

更に又、従来の反射鏡aは平坦面部と回転放物面部との
境界部rが角状になるように設計、製作されているため
その部分による反射光は鋭い指向性を持ち、しかもその
方向は製品によってマチマチでありレンズだけでは制御
しきれず、従って、シールド板tにて光源Sからの光源
を遮断し境界部rには光線が照射されないようにしてい
るが、平坦面部Cの傾斜角度θが大きくなればそれだけ
境界部rの位置が後方に移動し且つ光軸X−Xに近づく
ため、シールド板tを光源Sに近づけなければならず、
従って、やはりフィラメントコイルの寿命特性に悪影響
を及ぼすという欠点がある。
Furthermore, since the conventional reflecting mirror a is designed and manufactured so that the boundary part r between the flat surface part and the paraboloid of revolution part is angular, the light reflected by that part has sharp directivity, and moreover, varies depending on the product and cannot be controlled by the lens alone.Therefore, the shield plate t blocks the light source from the light source S to prevent the light beam from being irradiated to the boundary part r, but the inclination angle θ of the flat surface part C As becomes larger, the position of the boundary r moves backward and approaches the optical axis XX, so the shield plate t must be brought closer to the light source S.
Therefore, there is still a drawback that it adversely affects the life characteristics of the filament coil.

そこで本考案は、強度的に優れると共に省資源化及び軽
量化を図ることができ、更に配光品質上鋭い迷光の発生
を皆無にすることができる新規な角形シールドビーム電
球の反射鏡を提供しようとするものであり、回転放物面
をその正面方向から見て略長方形を為すようにその上下
及び左右を適宜に切り取りその各端縁に略光軸方向に沿
って延びる平坦面部を連設した如き形状の硬質ガラス製
の反射鏡において、前記平坦面部の肉厚を反射鏡の開放
端方向に行くに従って徐々に薄くなるように形成し、更
に回転放物面部と平坦面部とをその内側境界部において
凹曲面を以って連続させたことを特徴とし、以下にその
詳細について添付図面に示された具体的な実施例につい
て説明する。
Therefore, the present invention aims to provide a reflector for a new rectangular sealed beam light bulb that is superior in strength, saves resources and is lightweight, and can eliminate the generation of sharp stray light in terms of light distribution quality. The paraboloid of revolution is cut out at the top, bottom, left and right so that it forms a substantially rectangular shape when viewed from the front direction, and a flat surface section extending substantially along the optical axis direction is provided at each edge. In a reflector made of hard glass having such a shape, the thickness of the flat surface portion is formed so as to gradually become thinner toward the open end of the reflector, and the paraboloid of revolution portion and the flat surface portion are further formed at their inner boundary portions. Hereinafter, specific embodiments shown in the accompanying drawings will be described in detail.

第5図は本考案角形シールドビーム電球の反射鏡1を示
し、該反射鏡1は第1図に示されたように、回転放物面
をその開口部方向から見て横長の略長方形を呈するよう
に、上下及び左右を切除して上下及び左右の端縁にそれ
ぞれ平坦面部2,2及び3,3を連設した如き形状に形
成されている。
FIG. 5 shows the reflector 1 of the rectangular sealed beam light bulb of the present invention, and as shown in FIG. 1, the reflector 1 has a horizontally elongated substantially rectangular shape when the paraboloid of revolution is viewed from the direction of its opening. It is formed in such a shape that the top and bottom and left and right sides are cut out and flat surface portions 2, 2 and 3, 3 are connected to the top and bottom and left and right edges, respectively.

そして、前記平坦面部2,2及び3,3は後力即ち回転
放物面部4方向に行くに従って反射鏡1の光軸X/−X
/に近づくように光軸X/−X/に対して角度θ′(こ
の角度θ′は上記した従来の反射鏡aのそれθより小さ
く形成される。
The flat surface portions 2, 2 and 3, 3 move toward the rear force, that is, the optical axis X/-
An angle θ' with respect to the optical axis X/-X/ is formed so as to approach / (this angle θ' is smaller than that of the conventional reflecting mirror a described above).

)をもって傾斜されている。).

又、回転放物面部4の肉厚t1はその全体に亘って略均
−になるように形成されており、各平坦面部2,2及び
3,3の肉厚t2は平坦面部と回転放物面部との境界部
5附近において回転放物面部4の肉厚t1と略等しく開
口端6方向に行くに従って徐々に薄くなるように形成さ
れており、更に前記境界部5の内面は例えば曲率半径3
7IL埒ましくは2.8〜3.5mm位の凹曲面とされ
ている。
Further, the wall thickness t1 of the paraboloid of revolution portion 4 is formed to be approximately uniform over the entire surface, and the wall thickness t2 of each of the flat surface portions 2, 2 and 3, 3 is formed between the flat surface portion and the paraboloid of revolution. It is formed to be approximately equal to the wall thickness t1 of the paraboloid of revolution 4 near the boundary 5 with the surface and gradually become thinner toward the opening end 6, and furthermore, the inner surface of the boundary 5 has a radius of curvature 3, for example.
7IL is preferably a concave curved surface of about 2.8 to 3.5 mm.

即ち、回転放物面部4と平坦面部2,2,3,3とはこ
のような凹曲面5によって連続されている。
That is, the paraboloid of revolution portion 4 and the flat surface portions 2, 2, 3, 3 are continuous by such a concave curved surface 5.

そして、このように形成された反射鏡1は、上記第3図
に示されたアルミ蒸着ヘッドkに装着され、その内面7
にアルミ蒸着膜8が付与される。
The reflecting mirror 1 thus formed is mounted on the aluminum vapor deposition head k shown in FIG.
An aluminum vapor-deposited film 8 is applied to the surface.

尚、9は反射鏡1の略焦点位置に配設された光源、10
は該光源9の前方の一部と後方を除く部分を覆う、即ち
光源9から出射された光線が各平坦面部2,2及び3,
3に照射されないようにするためのシールド板であり、
該シールド板10の前面には光軸X/−X /より下側
に光源9からの直射光を反射鏡1の前方に照射するため
の窓11が形成されている。
In addition, 9 is a light source arranged at approximately the focal point position of the reflecting mirror 1, and 10
covers the part of the light source 9 except for the front part and the rear part, that is, the light beam emitted from the light source 9 covers each flat surface part 2, 2 and 3,
It is a shield plate to prevent irradiation from 3.
A window 11 is formed on the front surface of the shield plate 10 below the optical axis X/-X/ for irradiating direct light from the light source 9 to the front of the reflecting mirror 1.

しかして、光源9から照射された光線の一部はシールド
板10の窓11を通過して反射鏡1の前方に照射され、
他の光線の一部は反射鏡1の有効反射面である回転放物
面部4に向かいここで反射されて反射鏡1の前方に出射
される。
A part of the light beam emitted from the light source 9 passes through the window 11 of the shield plate 10 and is emitted in front of the reflecting mirror 1.
A portion of the other light beams travel toward the paraboloid of revolution portion 4, which is the effective reflecting surface of the reflecting mirror 1, and are reflected there and emitted to the front of the reflecting mirror 1.

そして、更に他の光線の一部は反射鏡1の境界部5に照
射されるが、この境界部5は凹曲面とされているために
方向性、ないしは指向性を持った鋭い反射光とはならず
拡散的に反射される。
Then, some of the other light rays are irradiated onto the boundary part 5 of the reflecting mirror 1, but since this boundary part 5 is a concave curved surface, it is not a sharp reflected light with directionality or directivity. Instead, it is reflected diffusely.

本考案角形シールドビーム電球の反射鏡は、上述したよ
うに、各平坦面部の肉厚を反射鏡の開口端方向に行くに
従って徐々に薄くなるように形成し更に回転放物面部と
平坦面部との境部を凹曲面としたため、該反射鏡の内部
を高真空にしてその内面にアルミ蒸着膜を付与する際に
、各平坦面部に生ずる引張応力は回転放物面部方向へ分
散され、従って、平坦面部又は境界部からの破壊が少な
くなりそれによる危険性を回避し得ると共に装置の損傷
を少なくすることができ、更には工程を一時的にしろス
トップさせる必要がなくなる利点がある。
As mentioned above, the reflector of the rectangular sealed beam light bulb of the present invention is formed so that the wall thickness of each flat surface portion becomes gradually thinner toward the opening end of the reflector, and furthermore, the thickness of each flat surface portion is formed to be gradually thinner as it goes toward the opening end of the reflector, and the thickness of each flat surface portion is formed to be gradually thinner as it goes toward the opening end of the reflector. Since the boundary part is a concave curved surface, when the interior of the reflector is made into a high vacuum and an aluminum vapor deposited film is applied to the inner surface, the tensile stress generated on each flat surface part is dispersed in the direction of the paraboloid of revolution, and therefore the flat surface is There is an advantage that there is less destruction from the surfaces or boundaries, and the danger caused by it can be avoided, damage to the equipment can be reduced, and there is no need to stop the process, even if only temporarily.

又、本考案は、特に平坦面部の肉厚を反射鏡の開口端方
向に行くに従って徐々に薄くなるように形成したため、
その外反射鏡の材料費を削減することができ、しかも自
動車メーカーの要望に沿うように軽量化を図ることがで
きる。
In addition, in the present invention, the thickness of the flat surface portion is made to gradually become thinner toward the opening end of the reflecting mirror.
The material cost of the external reflector can be reduced, and the weight can be reduced to meet the needs of automobile manufacturers.

更に、本考案は平坦面部を上述したように形成したため
、反射鏡自体の成形時に平坦面部に残留する応力が小さ
くなり、平坦面部の強度が低下しない利点もある。
Furthermore, since the flat surface portion of the present invention is formed as described above, stress remaining in the flat surface portion during molding of the reflecting mirror itself is reduced, and there is an advantage that the strength of the flat surface portion does not decrease.

又、本考案は、従来の反射鏡のように、平坦面部の傾斜
角度を大きくしなくとも上記引張歪が一部分に集中する
ことがないようにしたため、有効反射面である回転放物
面部の面積が少なくなることもない。
In addition, unlike conventional reflecting mirrors, the present invention prevents the tensile strain from being concentrated in one part without increasing the inclination angle of the flat surface, so the area of the paraboloid of revolution, which is the effective reflecting surface, is reduced. will not become less.

更に又、本考案は、境界部を凹曲面としたため、その部
分による鋭い迷光の発生がなくなり、シールド板を光源
に近づけて境界部への照射を無理になくす必要がなくな
り、従って光源とシールド板とが近づきすぎて光源、即
ちフィラメントコイルの寿命特性を損なうということも
ない利点がある。
Furthermore, since the boundary part of the present invention is made into a concave curved surface, the generation of sharp stray light due to that part is eliminated, and there is no need to bring the shield plate close to the light source to forcefully eliminate irradiation to the boundary part. There is an advantage that the life characteristics of the light source, that is, the filament coil, will not be impaired due to the fact that they are too close to each other.

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

第1図は角形シールドビーム電球の反射鏡の形成方法を
説明するための斜視図、第2図は従来の角形シールドビ
ーム電球の反射鏡の一例を示す縦断側面図、第3図はア
ルミ蒸着ヘッドの斜視図、第4図はアルミ蒸着ヘッドに
反射鏡を装着した状態を示す斜視図、第5図は本考案角
形シールドビーム電球の反射鏡を示す縦断側面図である
。 符号の説明、1:反射鏡、2,2,3,3・・・平坦面
部、4・・・回転放物面部、5・・・内側境界部、t・
・・肉厚。
Figure 1 is a perspective view for explaining the method of forming the reflector of a square sealed beam light bulb, Figure 2 is a vertical side view showing an example of the reflector of a conventional square sealed beam light bulb, and Figure 3 is an aluminum vapor deposition head. FIG. 4 is a perspective view showing a state in which a reflector is attached to an aluminum vapor deposition head, and FIG. 5 is a vertical sectional side view showing a reflector of the rectangular sealed beam light bulb of the present invention. Explanation of symbols: 1: Reflector, 2, 2, 3, 3...Flat surface part, 4... Paraboloid of rotation part, 5... Inner boundary part, t.
・Thickness.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 回転放物面をその正面方向から見て略長方形を為すよう
にその上下及び左右を適宜に切り取りその各端縁に略光
軸方向に沿って延びる平坦面部を連設した如き形状の硬
質ガラス製の反射鏡において、前記平坦面部の肉厚を反
射鏡の開口端方向に行くに従って徐々に薄くなるように
形成し、更に回転放物面部と平坦面部とをその内側境界
部において凹曲面を以って連続させたことを特徴とする
角形シールドビーム電球の反射鏡。
Made of hard glass with a shape similar to that of a paraboloid of revolution, whose top and bottom, left and right sides are cut out so that it forms a substantially rectangular shape when viewed from the front direction, and a flat surface portion extending approximately along the optical axis direction is provided at each edge of the paraboloid of revolution. In the reflecting mirror, the thickness of the flat surface portion is formed to gradually become thinner toward the opening end of the reflecting mirror, and the paraboloid of revolution portion and the flat surface portion are further formed with a concave curved surface at an inner boundary thereof. A reflector for a rectangular sealed beam light bulb characterized by a series of continuous beams.
JP1978093663U 1978-07-07 1978-07-07 Reflector of square shield beam light bulb Expired JPS585326Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1978093663U JPS585326Y2 (en) 1978-07-07 1978-07-07 Reflector of square shield beam light bulb

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1978093663U JPS585326Y2 (en) 1978-07-07 1978-07-07 Reflector of square shield beam light bulb

Publications (2)

Publication Number Publication Date
JPS5510277U JPS5510277U (en) 1980-01-23
JPS585326Y2 true JPS585326Y2 (en) 1983-01-29

Family

ID=29024991

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1978093663U Expired JPS585326Y2 (en) 1978-07-07 1978-07-07 Reflector of square shield beam light bulb

Country Status (1)

Country Link
JP (1) JPS585326Y2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5470671A (en) * 1977-11-15 1979-06-06 Toshiba Corp Square-shaped sealed beam lamp

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5470671A (en) * 1977-11-15 1979-06-06 Toshiba Corp Square-shaped sealed beam lamp

Also Published As

Publication number Publication date
JPS5510277U (en) 1980-01-23

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