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JPS6146938B2 - - Google Patents
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JPS6146938B2 - - Google Patents

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Publication number
JPS6146938B2
JPS6146938B2 JP5442778A JP5442778A JPS6146938B2 JP S6146938 B2 JPS6146938 B2 JP S6146938B2 JP 5442778 A JP5442778 A JP 5442778A JP 5442778 A JP5442778 A JP 5442778A JP S6146938 B2 JPS6146938 B2 JP S6146938B2
Authority
JP
Japan
Prior art keywords
lens
light bulb
concave
light
lens element
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
JP5442778A
Other languages
Japanese (ja)
Other versions
JPS54146486A (en
Inventor
Nobuyoshi Kuno
Kyokazu Pponda
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
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP5442778A priority Critical patent/JPS54146486A/en
Publication of JPS54146486A publication Critical patent/JPS54146486A/en
Publication of JPS6146938B2 publication Critical patent/JPS6146938B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明はシールドビーム形電球のレンズを改良
したものに関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an improved lens for a sealed beam light bulb.

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

従来、一般に使用されている投光用シールドビ
ーム形電球は、フイラメントからの直射光および
反射鏡からの反射光をレンズによつて拡散して所
定の配光が得られるように構成されているのが普
通である。そして、この種電球は投射光をレンズ
によつて所定の角度に拡散せしめることが特に要
求され、これが従来からの重要な課題であつた。
Hitherto, commonly used sealed beam light bulbs are constructed so that a predetermined light distribution is obtained by diffusing the direct light from the filament and the reflected light from the reflector using a lens. is normal. This type of light bulb is particularly required to diffuse the projected light at a predetermined angle through a lens, and this has been an important problem in the past.

ところが従来のレンズは第1図に示すように、
レンズ1の中心を除く内面に凸状のレンズ素子1
1が多数形成されている。このレンズ素子11は
正面からみるとほぼ円形になつていて、この素子
11に入射する光は均一に放射状に拡散されるの
で反射面に対する位置規制が不用となつて誠に好
ましい。
However, as shown in Figure 1, conventional lenses
Lens element 1 having a convex inner surface except for the center of lens 1
1 is formed in large numbers. This lens element 11 has a substantially circular shape when viewed from the front, and since the light incident on this element 11 is uniformly diffused radially, there is no need to regulate its position with respect to the reflecting surface, which is very preferable.

ところが、レンズ1の肉厚はレンズ中心とその
他の部分では多少異なることから、レンズ製造時
(プレス成形によつて作られる)に若干の歪が発
生している。そして歪は、後処理である程度除去
できるが完全に除去することは困難であるから、
これが反射鏡との封着の際のヒートシヨツク等に
よつてクラツクの原因となり歩留りを低下した
り、電球完成後に破損したりする原因となつてい
る。したがつて、できる限りレンズ1全体の肉厚
は均一であることが望ましいが、レンズ素子1
1,……を設ける必要があるので、どうしても肉
厚差は避けてとおることは出来ない。
However, since the thickness of the lens 1 is slightly different between the center of the lens and other parts, some distortion occurs during lens manufacture (by press molding). Although distortion can be removed to some extent through post-processing, it is difficult to remove it completely.
This causes cracks due to heat shock during sealing with the reflecting mirror, lowering yield, and causing damage to the bulb after it is completed. Therefore, it is desirable that the thickness of the entire lens 1 be as uniform as possible;
Since it is necessary to provide 1,..., the difference in wall thickness cannot be avoided.

一方このレンズ1は先に説明した通り、プレス
成形されるが金型形状が複雑になつたり、出来上
つたレンズ1に不良個所が生ずるなどのことがあ
つた。すなわち、レンズ1に形成されるレンズ素
子11,……が凸状となると、逆にプレス金型の
方には凹部を多数形成しておかなくてはならな
い。しかし、プレス金型に多数の凹部を正確に成
形することが難かしいこと、あるいはレンズ素子
2のみで所定の配光角を得るために素子2の高さ
が高くなるようにしなければならないので金型も
それに応じて成形しなくてはならないからその製
作が難しくなる。また、プレス成形した場合に金
型の個々の凹部内には空気がわずかではあるが残
留する。これが、レンズ1の成形後各レンズ素子
11,……の頂部にしわあるいはあわとして残留
すると、光の透過が悪くこの部分での透過率が低
下してしまい、光束低下を起し易いという欠点が
あつて具合が悪かつた。
On the other hand, as described above, this lens 1 is press-molded, but the shape of the mold becomes complicated, and the finished lens 1 has some defects. That is, if the lens elements 11, . However, it is difficult to accurately form a large number of concave portions in a press mold, or the height of the lens element 2 must be increased in order to obtain a predetermined light distribution angle using only the lens element 2. The mold also has to be molded accordingly, making it difficult to manufacture. Further, when press molding is performed, a small amount of air remains in each concave portion of the mold. If this remains as wrinkles or bubbles on the top of each lens element 11 after the lens 1 is molded, light transmission will be poor and the transmittance in this area will decrease, resulting in a decrease in luminous flux. I felt warm and unwell.

〔発明の目的〕[Purpose of the invention]

本発明はレンズにしわやあわなどの発生がなく
光透過障害の少ない、しかも、レンズにおける肉
厚差を少なくして熱衝撃に強く成形性が向上でき
た拡散性能のよいレンズを有するシールドビーム
形電球を提供することを目的とする。
The present invention is a sealed beam type that has a lens with good diffusion performance that does not cause wrinkles or wrinkles on the lens and has little interference with light transmission, and is also resistant to thermal shock and has improved formability by reducing the difference in wall thickness of the lens. The purpose is to provide light bulbs.

〔発明の概要〕[Summary of the invention]

本発明は反射鏡の開口部にレンズを封着して形
成したパルプ内にフイラメントを封入した電球に
おいて、上記レンズは内面に凹状をなすレンズ素
子が多数個設けられるとともにこの凹状部面に微
細な凹凸状の拡散面を形成していることを特徴と
するシールドビーム形電球を要旨とするものであ
る。
The present invention relates to a light bulb in which a filament is enclosed in a pulp formed by sealing a lens to an opening of a reflecting mirror, in which the lens is provided with a large number of concave lens elements on its inner surface, and a microscopic structure is formed on the surface of the concave portion. The gist of this invention is a sealed beam light bulb that is characterized by forming an uneven diffusing surface.

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

本発明は実施例を図面を参照して説明する。第
2図はシールドビーム形電球で、2はレンズ製反
射鏡、1はこの反射鏡2の前面開口部に封着され
たガラス製レンズで、上記両者を気密封着するこ
とによつてパルプ3が形成されている。なお、パ
ルプ3内にはアルゴンや窒素などの不活性ガスと
ともに発光源であるタングステンフイラメント4
が封入されている。なお、5は反射鏡2端部に取
着された口金である。そして、上記レンズ1は第
3図および第4図に示すような構成となつてい
る。レンズ1の外面は塵埃などの付着が少ない平
滑な湾曲面で、また、内面は外面とほぼ同一曲率
の湾曲面で成形されている。また、レンズ1内面
の中央部12を除く周囲に多数個の凹状部からな
るレンズ素子13,……を形成してある。このレ
ンズ素子13は上面または下面から見て円形に形
成されていて、このレンズ素子13を通過する光
がすべて同じように拡散することができるように
してある。また、このレンズ素子13の凹状部面
には第5図に拡大して示すように多数の微細な粗
面14,……が形成されている。
Embodiments of the present invention will be described with reference to the drawings. Fig. 2 shows a sealed beam type light bulb, in which 2 is a lens reflector, 1 is a glass lens sealed to the front opening of this reflector 2, and by hermetically sealing both, the pulp 3 is formed. In addition, inside the pulp 3, there is a tungsten filament 4, which is a light source, along with an inert gas such as argon or nitrogen.
is included. Note that 5 is a cap attached to the end of the reflecting mirror 2. The lens 1 has a structure as shown in FIGS. 3 and 4. The outer surface of the lens 1 is a smooth curved surface to which little dust adheres, and the inner surface is formed into a curved surface having approximately the same curvature as the outer surface. Further, lens elements 13, . . . consisting of a large number of concave portions are formed around the inner surface of the lens 1, excluding the central portion 12. This lens element 13 is formed in a circular shape when viewed from the top or bottom surface so that all the light passing through this lens element 13 can be equally diffused. Further, a large number of fine rough surfaces 14, . . . are formed on the concave surface of the lens element 13, as shown in an enlarged view in FIG.

上記のような構成とすることにより、同一レン
ズ1において肉厚差が少ないにも拘らず良好な拡
散機能が得られた。
With the above configuration, a good diffusion function was obtained even though the difference in wall thickness was small in the same lens 1.

なお、上記レンズ素子13,……の微細な粗面
14,……の凹凸は1μHmax〜70μHmaxの荒
さ(凹凸面の高さをHmaxの単位で表す。)であ
る。この理由は1μHmax未満の荒さでは表面に
粗面が形成されなくなることから、この粗面によ
る拡散作用がなくなつてしまう。また、逆に荒さ
が70μHmaxを越えると、レンズ素子13の原形
がくずれてしまつてレンズ本来の拡散機能が発揮
できない。本発明者等の実験では、この表面荒さ
は6μHmax〜50μHmaxの範囲で拡散作用がよ
かつたが、1μHmax〜70μHmaxの範囲で実用
化できた。
Incidentally, the unevenness of the finely rough surfaces 14, . . . of the lens elements 13, . The reason for this is that if the roughness is less than 1 μHmax, no rough surface will be formed on the surface, and the diffusion effect due to this rough surface will disappear. On the other hand, if the roughness exceeds 70 μHmax, the original shape of the lens element 13 will be distorted and the original diffusion function of the lens will not be exhibited. In experiments conducted by the present inventors, the diffusion effect was good when the surface roughness was in the range of 6 μHmax to 50 μHmax, but it could be put to practical use in the range of 1 μHmax to 70 μHmax.

なお、レンズ素子13の凹状部を深くして拡散
作用を得ることも考えられるが、そうすると第6
図に示すように原肉厚(b)と凹部の肉厚(a)との差が
大きくなり、レンズ1全体に肉厚の大差が出来て
しまつて熱衝撃に対して弱くなり、この結果レン
ズ1とこれに適合する反射鏡2との封着の際に、
クラツクの発生原因となつて具合が悪い。
Note that it is also possible to obtain a diffusion effect by deepening the concave portion of the lens element 13, but in that case, the sixth
As shown in the figure, the difference between the original wall thickness (b) and the wall thickness of the recess (a) becomes large, creating a large difference in wall thickness throughout the lens 1, which makes the lens vulnerable to thermal shock. When sealing 1 and a matching reflector 2,
It is unwell because it causes cracks.

以上のように本発明においては、レンズ1にお
ける凹状部と凹状部でない部分との肉厚の差を小
さくすることを、レンズ素子12,……の面に更
に微細な粗面を設けることによつて実現すること
が可能となつたものである。
As described above, in the present invention, the difference in wall thickness between the concave portion and the non-concave portion of the lens 1 can be reduced by providing finer rough surfaces on the surfaces of the lens elements 12, . This made it possible to realize this goal.

次に具体的実施例について説明する。湾曲した
肉厚約4mmのレンズ1内面にプレスによつて上面
また下面からみて円形のレンズ素子13,……を
多数個形成した。このレンズ素子13,……の凹
状部の大きさは直径約3.7mm、深さ約0.5mmであ
る。そして、このレンズ素子13,……の凹状部
面に荒さが約6μHmaxの微細な粗面を形成し
た。このようにして形成したレンズ1にフイラメ
ント4を取着した反射鏡2を封着し、第2図示の
ようなシールドビーム形電球に形成した。
Next, specific examples will be described. A large number of lens elements 13, which were circular when viewed from the top or bottom, were formed by pressing on the curved inner surface of the lens 1 having a wall thickness of approximately 4 mm. The size of the concave portion of the lens elements 13, . . . is approximately 3.7 mm in diameter and approximately 0.5 mm in depth. Then, a fine rough surface with a roughness of about 6 μHmax was formed on the concave portion surfaces of the lens elements 13, . A reflecting mirror 2 with a filament 4 attached thereto was sealed to the lens 1 thus formed to form a sealed beam type light bulb as shown in the second figure.

そして、上記レンズ1の拡散作用を確認するた
めに約2mm径の赤色レーザー光をレンズ素子13
の1個に照射し、これの透過拡散光を約50cm離れ
部分にスクリーンを置いて測定した。この測定に
よると放射方向に約0.8〜2.4゜の拡散効果を得る
ことが出来た。これはレンズ素子の凹状部のみに
よる拡散効果と比較すると、レンズ素子の深さを
約0.8mmにしたときに相当し、レンズ素子の深さ
を十分に浅く出来ることが出来た。すなわち、そ
の深さを0.8mmから0.5mmに浅くすることが可能と
なつた。したがつて、それだけ上記レンズの肉厚
の差を小さく出来るので熱衝撃に対して強く出来
る。
Then, in order to confirm the diffusion effect of the lens 1, a red laser beam with a diameter of about 2 mm was applied to the lens element 13.
The transmitted and diffused light was measured by placing a screen approximately 50 cm away. According to this measurement, we were able to obtain a diffusion effect of approximately 0.8 to 2.4 degrees in the radial direction. Compared to the diffusion effect due only to the concave portion of the lens element, this corresponds to when the depth of the lens element is approximately 0.8 mm, and the depth of the lens element can be made sufficiently shallow. In other words, it has become possible to reduce the depth from 0.8 mm to 0.5 mm. Therefore, since the difference in the thickness of the lens can be made smaller, the lens can be made more resistant to thermal shock.

次に他の実施例について説明する。上記実施例
と同様にレンズ素子13,……を円形とし、その
直径を約3.7mm、深さを0.3mmに形成した。そし
て、レンズ素子13,……の凹状部面に荒さが約
60μHmaxの粗面を形成してレンズ1を構成した
ところ、上記実施例とほぼ同様の拡散配光を得る
ことが出来た。この場合、レンズ素子13,……
の原形はほとんどくずすことはない。しかも、レ
ンズ素子13,……の深さを0.3mmまで浅くする
ことが可能となつて好結果を得ることが出来た。
Next, other embodiments will be described. As in the above embodiment, the lens elements 13, . . . were circular, with a diameter of about 3.7 mm and a depth of 0.3 mm. The concave surfaces of the lens elements 13, . . . have roughness of approximately
When the lens 1 was constructed by forming a rough surface of 60 μHmax, it was possible to obtain almost the same diffused light distribution as in the above embodiment. In this case, the lens elements 13,...
The original shape is almost never destroyed. Moreover, it became possible to reduce the depth of the lens elements 13, . . . to 0.3 mm, and good results were obtained.

〔発明の効果〕〔Effect of the invention〕

本発明は以上詳述したように、レンズの内面に
凹状をなすレンズ素子が多数個設けられるととも
にこの凹状部面に微細な凹凸状の拡散面を形成し
ていることを特徴とするシールドビーム形電球で
あつて、レンズの基本となる肉厚より厚くならな
いようレンズ素子を凹状部としてしるため、、レ
ンズのプレス成形時に金型内においてレンズの流
れがよく成形が容易であるばかりかしわやあわの
発生を抑制できる。また、レンズ素子が凹状とい
うことは金型に凸部があることから金型の製作加
工が精度よくかつ容易にできる。また、金型への
粗面の形成も放電加工により容易に行なえる。
As described in detail above, the present invention provides a shielded beam type characterized in that a large number of concave lens elements are provided on the inner surface of the lens, and a finely uneven diffusing surface is formed on the concave surface. Since it is a light bulb, the lens element is made into a concave part so that it does not become thicker than the basic wall thickness of the lens, so that the lens flows easily in the mold during press molding of the lens, and it is easy to mold, and there are no wrinkles or bubbles. can suppress the occurrence of Furthermore, since the lens element is concave, the mold has a convex portion, so the mold can be fabricated with high precision and easily. In addition, a rough surface can be easily formed on the mold by electric discharge machining.

また、本発明はレンズ素子を単に凹状部とした
だけでなく、凹状部面にさらに微細な凹凸状の粗
面を形成し拡散効果をもたらすようにしたので、
レンズ素子凹状部の深さを浅く形成することがで
き、すなわちレンズの肉厚の差が小さくなるので
歪の発生も少なくなり耐熱衝撃強度を向上でき
る。
Furthermore, in the present invention, the lens element is not only made of a concave portion, but also has a rough surface with fine irregularities formed on the surface of the concave portion to bring about a diffusion effect.
Since the depth of the concave portion of the lens element can be made shallow, that is, the difference in lens thickness is reduced, the occurrence of distortion is reduced, and the thermal shock resistance can be improved.

このような本発明の構成とすれば、レンズの光
拡散性能、強度などがすぐれるとともにその製作
が容易で生産性の向上がはかれるなど、種々の利
点を有するシールドビーム形電球を提供できるも
のである。
With this configuration of the present invention, it is possible to provide a sealed beam light bulb that has various advantages, such as excellent light diffusion performance and strength of the lens, and ease of manufacturing and improved productivity. be.

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

第1図は従来の電球に用いたレンズの断面を示
す説明図、第2図ないし第5図は本発明の実施例
を示し、第2図はシールドビーム形電球の一部切
欠断面正面図、第3図はレンズの断面を示す説明
図、第4図はレンズの底面図、第5図はレンズの
要部拡大断面図、第6図はレンズ構成を説明する
ための要部断面図である。 1……レンズ、2……反射鏡、13……レンズ
素子(凹状部)、3……バルブ、14……拡散
面、4……フイラメント。
Fig. 1 is an explanatory diagram showing a cross section of a lens used in a conventional light bulb, Figs. 2 to 5 show embodiments of the present invention, and Fig. 2 is a partially cutaway sectional front view of a sealed beam type light bulb. Fig. 3 is an explanatory diagram showing a cross section of the lens, Fig. 4 is a bottom view of the lens, Fig. 5 is an enlarged sectional view of the main part of the lens, and Fig. 6 is a sectional view of the main part to explain the lens configuration. . 1... Lens, 2... Reflector, 13... Lens element (concave portion), 3... Bulb, 14... Diffusion surface, 4... Filament.

Claims (1)

【特許請求の範囲】 1 反射鏡の開口部にレンズを封着して形成した
パルプ内にフイラメントを封入した電球におい
て、上記レンズは内面に凹状をなすレンズ素子が
多数個設けられるとともにこの凹状部面に微細な
凹凸状の拡散面を形成していることを特徴とする
シールドビーム形電球。 2 レンズ素子の凹状部の微細な拡散面は1μ
Hmax〜70μHmaxの荒さの凹凸をなしているこ
とを特徴とする特許請求の範囲第1項のシールド
ビーム形電球。
[Scope of Claims] 1. A light bulb in which a filament is enclosed in a pulp formed by sealing a lens in an opening of a reflecting mirror, in which the lens is provided with a large number of lens elements each having a concave shape on its inner surface, and the concave portion A sealed beam light bulb that is characterized by a diffuser surface with fine irregularities formed on its surface. 2 The fine diffusion surface of the concave part of the lens element is 1μ
The sealed beam light bulb according to claim 1, characterized in that it has an uneven surface with a roughness of Hmax to 70 μHmax.
JP5442778A 1978-05-10 1978-05-10 Shelded beam bulb Granted JPS54146486A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5442778A JPS54146486A (en) 1978-05-10 1978-05-10 Shelded beam bulb

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5442778A JPS54146486A (en) 1978-05-10 1978-05-10 Shelded beam bulb

Publications (2)

Publication Number Publication Date
JPS54146486A JPS54146486A (en) 1979-11-15
JPS6146938B2 true JPS6146938B2 (en) 1986-10-16

Family

ID=12970412

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5442778A Granted JPS54146486A (en) 1978-05-10 1978-05-10 Shelded beam bulb

Country Status (1)

Country Link
JP (1) JPS54146486A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5884617A (en) * 1981-11-13 1983-05-20 Sumitomo Metal Ind Ltd Method for preventing saw edge for band steel

Also Published As

Publication number Publication date
JPS54146486A (en) 1979-11-15

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