JP2000100222A - Lighting system - Google Patents

Lighting system

Info

Publication number
JP2000100222A
JP2000100222A JP10270395A JP27039598A JP2000100222A JP 2000100222 A JP2000100222 A JP 2000100222A JP 10270395 A JP10270395 A JP 10270395A JP 27039598 A JP27039598 A JP 27039598A JP 2000100222 A JP2000100222 A JP 2000100222A
Authority
JP
Japan
Prior art keywords
globe
light source
light
thickness
transmittance
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.)
Pending
Application number
JP10270395A
Other languages
Japanese (ja)
Inventor
Hidetoshi Tsuji
秀敏 辻
Toshihiro Hata
俊博 秦
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.)
Toto Ltd
Original Assignee
Toto 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 Toto Ltd filed Critical Toto Ltd
Priority to JP10270395A priority Critical patent/JP2000100222A/en
Publication of JP2000100222A publication Critical patent/JP2000100222A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To uniform the brightness of a globe surface with a simple method to improve a practical irradiation characteristic and to improve the appearance from the viewpoint of design by relating the light transmittance of a globe that is a non-transparent and light dispersing external member generally proportionally to the distance from a light source so as to set it differently. SOLUTION: Regarding the thickness of a globe, a part 1a nearest to a light source 2 is thickest, a part 1b farther than the part 1a is thinner than the part 1a, and a still farther part 1c is thinner than the part 1b. That is, the thickness of the globe is so set that the globe thickness at the part nearest to the light source 2 is the maximum, and the thickness of its peripheral part is gradually reduced as it parts away from the thickest part. The light emitted from the light source 2 is irradiated through the globe arranged around the light source 2. Thereby, the brightness of the globe surface is uniformed and a uniform luminous intensity distribution can be provided regardless of the distance between the light source 2 and the globe.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は電球等の略点光源を
覆う、完全に透明でない光拡散性の外郭部材であるグロ
ーブを有する照明器具に関するものであり、屋内の天井
面や壁面に取り付けられ照明器具に好適に利用されるも
のである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a luminaire having a globe, which is a light-diffusing outer member that is not completely transparent and covers a substantially point light source such as a light bulb, and is mounted on an indoor ceiling or wall. It is suitably used for lighting equipment.

【0002】[0002]

【従来の技術】従来の照明器具のグローブは、その多く
が内部の点光源等の構成体を外部から遮蔽するためや光
を拡散させて穏やかな光を射出するため等の目的で、そ
のグローブの光射出部を構成する素材を透明でない光拡
散性の乳白色のものにしたり、あるいは、その素材の表
面を乱反射面にしたりしていた。しかしながら、その素
材の色、肉厚及び光の拡散面の性状は一定であり、従っ
て内部の光源から射出される照射光に対する光学的透過
率はグローブ全体に渡って均等であった。
2. Description of the Related Art Many gloves of conventional lighting fixtures are used for shielding internal components such as point light sources from the outside and for diffusing light to emit gentle light. The material forming the light emitting portion is made of a non-transparent, light-diffusing milky white material, or the surface of the material is made a diffuse reflection surface. However, the color, thickness, and properties of the light diffusing surface of the material were constant, and thus, the optical transmittance for irradiation light emitted from an internal light source was uniform throughout the glove.

【0003】[0003]

【発明が解決しようとする課題】前記のような従来の照
明器具のグローブでは光の透過率が均等なため、グロー
ブの略点光源からの距離が異なっている場合、その極端
な例は直方体形状の場合であるが、グローブ中の略点光
源からの距離に反比例してグローブ面の明るさが決まる
性質がある。これは、照度が距離の二乗に逆比例する逆
二乗の法則から言えることであり、以下図面を参照しつ
つ詳細を述べる。
Since the light transmittance of the gloves of the conventional lighting equipment as described above is uniform, if the distance of the gloves from the approximate point light source is different, an extreme example is a rectangular parallelepiped shape. However, the brightness of the globe surface is determined in inverse proportion to the distance from the point light source in the globe. This can be said from the inverse square law in which the illuminance is inversely proportional to the square of the distance, and will be described in detail below with reference to the drawings.

【0004】図3において、光源の光度をI(cd)、
光源から最も近いグローブ7a付近の内面までの距離を
S1(m)、その部分の内面照度をE7a(lx)、グ
ローブ7aより遠いグローブ7c付近の内面までの距離
をS2(m)、その部分の内面照度をE7c(lx)と
する。グローブ内面照度E7a,E7cは、逆二乗の法
則から次の式であらわすことができる。 E7a=I/S12 (lx) E7c=I/S22 (lx) S1<S2であることからE7a>E7cとなり、グロ
ーブ7c付近の内面はグローブ7a付近の内面より暗い
ことになる。
In FIG. 3, the luminous intensity of the light source is I (cd),
The distance from the light source to the inner surface near the globe 7a
S1 (m), the inner surface illuminance of that part is E7a (lx),
Distance to inner surface near globe 7c farther than lobe 7a
Is S2 (m), and the inner surface illuminance of that part is E7c (lx).
I do. Globe inner illuminance E7a, E7c is calculated by the inverse square method.
From the rule, it can be expressed by the following equation. E7a = I / S1Two(Lx) E7c = I / S2Two(Lx)  Since S1 <S2, E7a> E7c, and
The inner surface near the globe 7c is darker than the inner surface near the glove 7a.
Will be.

【0005】次に、グローブ7a付近外面、およびグロ
ーブ7c付近外面の輝度について以下述べる。前記の通
り従来の光拡散性のグローブは、その透過率が均等であ
ることから、微少面は完全拡散面であり、その透過率を
τとすると、グローブ7a付近外面の輝度L7a(cd
/m2)、およびグローブ7c付近の外面輝度L7c
(cd/m2)は次の式であらわすことができる。 L7a=τE7a/π (cd/m2) L7c=τE7c/π (cd/m2) 前記のとおりE7a>E7cであることから、L7a>
L7cとなり、グローブ7c付近の外面はグローブ7a
付近の外面より輝度が低いことになる。即ち、グローブ
7c付近の外面はグローブ7a付近の外面より薄暗く見
える。
Next, the brightness of the outer surface near the globe 7a and the outer surface near the globe 7c will be described below. As described above, the conventional light-diffusing glove has the same transmittance, so that the minute surface is a perfect diffusion surface. If the transmittance is τ, the brightness L7a (cd
/ M 2 ) and the outer surface luminance L7c near the globe 7c
(Cd / m 2 ) can be expressed by the following equation. L7a = τE7a / π (cd / m 2 ) L7c = τE7c / π (cd / m 2 ) Since E7a> E7c as described above, L7a>
L7c, and the outer surface near the glove 7c is the glove 7a.
The brightness will be lower than the nearby outer surface. That is, the outer surface near the globe 7c looks dimer than the outer surface near the globe 7a.

【0006】さらに、輝度は光度の面積密度であること
から、輝度と光度は比例する。したがって、前記L7a
>L7cの関係式からして、グローブ7c付近の光度I
7cはグローブ7a付近の光度I7aより低いことにな
る。即ち、均等な配光が得られなくなる。
Further, since luminance is the area density of luminous intensity, luminance is proportional to luminous intensity. Therefore, the L7a
> L7c, the luminous intensity I near the globe 7c
7c is lower than the luminous intensity I7a near the globe 7a. That is, uniform light distribution cannot be obtained.

【0007】以上から、従来の技術では、グローブ表面
の明るさが均等でないため、照明器具を使用者が眺めた
場合に、グローブ面の明るさが均一ではなく、デザイン
的に見映えが良いとはいえなかった。また被照射物の照
射される照度も場所により大きく異なり、略点光源から
の距離が離れている方向は実使用上必要な明るさを得ら
れなくなるという問題があった。
[0007] From the above, according to the prior art, since the brightness of the glove surface is not uniform, when the user looks at the lighting fixture, the brightness of the glove surface is not uniform and the design is good. I couldn't say. Further, the illuminance of the object to be illuminated also varies greatly depending on the location, and there is a problem that it is not possible to obtain the brightness required for practical use in a direction where the distance from the point light source is far away.

【0008】本発明は、上記課題を解決するためになさ
れたもので、本発明の目的は、簡易な方法で実使用上照
射特性の良い、あるいはデザイン的にも見映えの良い照
明装置を提供することにある。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a lighting device which has a good irradiation characteristic in practical use or a good appearance even in design by a simple method. Is to do.

【0009】[0009]

【課題を解決するための手段および作用・効果】上記目
的を達成するために請求項1は、照明器具を覆う非透明
の光拡散性の外郭部材であるグローブにおいて、その光
透過率を該光源からの距離に略比例に関連付けて異なら
せたので、グローブ表面の明るさが均一で、均等な配光
が得られる。
In order to achieve the above object, a first aspect of the present invention is to provide a glove which is a non-transparent light-diffusing outer member for covering a lighting fixture, wherein the light transmittance of the glove is determined by the light source. The globe surface is made to have a uniform brightness and a uniform light distribution, because the globe surface is made different in relation to the distance from the object.

【0010】上記目的を達成するために請求項2は、透
過率を異ならせる手段が肉厚で、光源から最も近い部分
のグローブ肉厚を最大肉厚とし、その周辺部の肉厚は、
その最大肉厚部から遠ざかるほど徐々に、または段階的
に薄肉厚にしたことである。この手段に対し、肉厚に透
過率は略反比例することから、グローブ表面の明るさが
均一で、均等な配光が得られる。
To achieve the above object, the means for varying the transmittance is thick, the thickness of the globe closest to the light source is the maximum thickness, and the thickness of the peripheral portion is
That is, the thickness is gradually or gradually reduced as the distance from the maximum thickness portion increases. In contrast to this measure, since the transmittance is substantially inversely proportional to the thickness, the brightness of the globe surface is uniform, and a uniform light distribution can be obtained.

【0011】上記目的を達成するために請求項3は、透
過率を異ならせる手段がシボの深さで、光源から最も近
い部分のグローブシボ深さを最大とし、その周辺部のシ
ボ深さは、その最大のシボ深さ部から遠ざかるほど徐々
に、または段階的にシボ深さを浅くしたことである。こ
の手段に対し、シボ深さが深いほど光の乱反射が多くな
り透過率が減少すること、つまりシボ深さに透過率は略
反比例することから、グローブ表面の明るさが均一で、
均等な配光が得られる。
According to a third aspect of the present invention, the means for varying the transmittance is the depth of the grain, the globe grain depth closest to the light source is maximized, and the grain depth of the periphery is: This means that the grain depth is gradually or gradually reduced as the distance from the maximum grain depth increases. In contrast to this measure, the deeper the grain depth is, the more the irregular reflection of light increases and the transmittance decreases.In other words, since the transmittance is approximately inversely proportional to the grain depth, the brightness of the glove surface is uniform,
Even light distribution can be obtained.

【0012】上記目的を達成するために請求項4は、透
過率を異ならせる手段がシボ模様の粗さで、光源から最
も近い部分のグローブシボ模様を最小の粗さとし、その
周辺部のシボ模様は、その最小粗さのシボ模様部から遠
ざかるほど徐々に、または段階的によりシボ粗さの粗い
シボ模様にしたことである。この手段に対し、シボ粗さ
が粗いほど光の乱反射が少なくなり透過率が増加するこ
と、つまりシボ粗さに透過率は略比例することから、グ
ローブ表面の明るさが均一で、均等な配光が得られる。
In order to achieve the above object, it is preferable that the means for making the transmittance different be the roughness of the grain pattern, the globe grain pattern closest to the light source be the minimum roughness, and the grain pattern of the periphery thereof be reduced. That is, as the distance from the grained portion having the minimum roughness is increased, the grained pattern is gradually or gradually made coarser. In contrast to this measure, the rougher the roughness, the less the irregular reflection of light and the higher the transmittance. In other words, since the transmittance is approximately proportional to the roughness, the globe surface has a uniform brightness and uniform distribution. Light is obtained.

【0013】上記目的を達成するために請求項5は、透
過率を異ならせる手段が光拡散性のある乳白色の色の濃
さで、光源から最も近い部分のグローブの光拡散性のあ
る乳白色を最大の濃さとし、その周辺部の乳白色の濃さ
は、その最大部の乳白色の濃さ部から遠ざかるほど徐々
に、または段階的に乳白色の濃さを薄くしたことであ
る。この手段に対し、乳白色の濃さは透過率に略比例す
ることから、グローブ表面の明るさが均一で、均等な配
光が得られる。
In order to achieve the above object, it is preferable that the means for changing the transmittance is a light-diffuse milky white color having a light-diffusive color, and the light-diffuse milky white of the glove closest to the light source. Assuming the maximum density, the milky white density in the periphery thereof means that the milky white density is gradually or stepwise reduced as the distance from the maximum milky white density part increases. In contrast to this measure, since the density of the milky white color is substantially proportional to the transmittance, the brightness of the globe surface is uniform, and a uniform light distribution can be obtained.

【0014】[0014]

【発明の実施の形態】以下、この発明の実施の形態を図
面を参照しつつ説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0015】図1はこの発明の第一および第二の一実施
の形態に係る照明装置の一部を断面した側面図である。
図1において、符号1は非透明で光拡散性の乳白色のグ
ローブで、光源2周りに配置され、取付台5にネジ込み
方式で取付けられ、脱着できる構造であり、グローブ1
と取付台との間には、防水、防湿、防塵のためのOリン
グなどのパッキン4が挟み込まれている。光源2は、ソ
ケット3にねじ込まれており、ソケット3には電気的に
接続された電源線6が設けられている。グローブ1の肉
厚は、光源から最も近い部分の1aが最も厚く、1aよ
り遠い部分の1bは1a部分より薄肉厚で、さらに遠い
1c部分は1b部分より薄肉厚となっている。即ち、グ
ローブ1の肉厚は、光源から最も近い部分のグローブ肉
厚を最大肉厚とし、その周辺部の肉厚は、その最大肉厚
部から遠ざかるほど徐々に薄肉厚になっている。
FIG. 1 is a side sectional view of a part of a lighting device according to the first and second embodiments of the present invention.
In FIG. 1, reference numeral 1 denotes a non-transparent, light-diffusing milky white glove, which is arranged around a light source 2 and is attached to a mounting base 5 by a screw-in system and can be attached and detached.
A packing 4 such as an O-ring for waterproofing, moisture-proofing, and dust-proofing is sandwiched between the and the mounting base. The light source 2 is screwed into a socket 3, and the socket 3 is provided with a power supply line 6 that is electrically connected. Regarding the thickness of the globe 1, the portion 1a closest to the light source is the thickest, the portion 1b farther from the light source 1b is thinner than the portion 1a, and the portion 1c farther from the light source is thinner than the portion 1b. In other words, the thickness of the globe 1 is set such that the thickness of the globe closest to the light source is the maximum thickness, and the thickness of the peripheral portion gradually becomes thinner as the distance from the maximum thickness portion increases.

【0016】つぎに、この照明装置の作用について説明
する。光源2から発せられた光は、この光源2周りに配
置されるグローブ1を通って照射される。光源から最も
近い部分のグローブ1aは、あらかじめ設定された適度
な乳白色の濃さ、肉厚であり、適度な光が照射されてい
る。グローブ1bでは、グローブ1aよりも光源からの
距離が遠いため、同肉厚の場合は薄暗くなりがちだが、
グローブ1aよりも薄肉厚になっていることから、より
透過率が高く、明るさが改善され、グローブ1aと同程
度の明るさとなっている。グローブ1cでは、グローブ
1bよりも光源からの距離が遠いため、同肉厚の場合は
薄暗くなりがちだが、グローブ1bよりも薄肉厚になっ
ていることから、より透過率が高く、明るさが改善さ
れ、グローブ1bと同程度の明るさとなっている。
Next, the operation of the lighting device will be described. Light emitted from the light source 2 is applied through a globe 1 disposed around the light source 2. The portion of the glove 1a closest to the light source has an appropriate milky white density and thickness set in advance, and is irradiated with appropriate light. In the globe 1b, the distance from the light source is longer than that of the globe 1a.
Since it is thinner and thicker than the globe 1a, the transmittance is higher, the brightness is improved, and the brightness is about the same as that of the globe 1a. The globe 1c is farther from the light source than the globe 1b, so it tends to be dim when the thickness is the same, but since the thickness is thinner than the globe 1b, the transmittance is higher and the brightness is improved. And the brightness is about the same as that of the globe 1b.

【0017】以上から、光源から最も近い部分のグロー
ブ肉厚を最大肉厚とし、その周辺部の肉厚は、その最大
肉厚部から遠ざかるほど徐々に薄肉厚になっていること
から、光源とグローブとの距離にかかわらずグローブ表
面の明るさが均一で、均等な配光が得られる。
As described above, the thickness of the globe closest to the light source is the maximum thickness, and the thickness of the peripheral portion is gradually reduced as the distance from the maximum thickness increases. Irrespective of the distance to the globe, the brightness of the globe surface is uniform, and a uniform light distribution can be obtained.

【0018】つぎに、この発明の第三、第四、および第
五の一実施の形態に係る照明装置について説明する。照
明装置の構成は、グローブ1を除いてその他の部分は図
1と同様であることから、グローブ1の詳細について以
下述べる。
Next, a lighting device according to a third, a fourth and a fifth embodiment of the present invention will be described. The structure of the lighting device is the same as that of the other parts except for the globe 1.
The details of the glove 1 will be described below because it is similar to 1.

【0019】前記第二の実施例の場合、透過率を異なら
せる手段はグローブ1の肉厚であったが、第三、第四、
および第五の実施例の場合は同肉厚であり、別の手段で
透過率を異ならせている。
In the case of the second embodiment, the means for making the transmittance different is the thickness of the globe 1, but the third, fourth,
In the case of the fifth embodiment, the thickness is the same, and the transmittance is made different by another means.

【0020】第三の一実施の形態については、透過率を
異ならせる手段がシボの深さで、光源から最も近い部分
のグローブ1のシボ深さが最大で、透過率は最も低く、
その周辺部のシボ深さは、その最大のシボ深さ部から遠
ざかるほど徐々に、または段階的にシボ深さを浅くして
いることから、透過率は徐々に、または段階的高くなっ
ている。
In the third embodiment, the means for making the transmittance different is the grain depth, the grain depth of the globe 1 closest to the light source is the largest, and the transmittance is the lowest.
As the grain depth at the periphery is gradually or gradually reduced as the distance from the maximum grain depth increases, the transmittance is gradually or gradually increased. .

【0021】第四の一実施の形態については、透過率を
異ならせる手段がシボ模様の粗さで、光源から最も近い
部分のグローブ1のシボ模様を最小の粗さとし、その周
辺部のシボ模様は、その最小粗さのシボ模様部から遠ざ
かるほど徐々に、または段階的によりシボ粗さの粗いシ
ボ模様になっていることから、透過率は徐々に、または
段階的高くなっている。シボ模様については、同じ拡大
倍率で比較したときの粗いシボ模様を図2(a)に、そ
れよりも粗くないシボ模様を図2(b)に示す。
In the fourth embodiment, the means for varying the transmittance is the roughness of the grain pattern, the grain pattern of the globe 1 closest to the light source is set to the minimum roughness, and the grain pattern of the peripheral portion is set. The transmittance is gradually or gradually increased as the distance from the grained pattern portion having the minimum roughness gradually increases or gradually increases gradually. Regarding the grain pattern, FIG. 2A shows a rough grain pattern when compared at the same magnification, and FIG. 2B shows a grain pattern that is less coarse than that.

【0022】第五の一実施の形態については、透過率を
異ならせる手段が光拡散性のある乳白色の色の濃さで、
光源から最も近い部分のグローブ1の光拡散性のある乳
白色を最大の濃さで、透過率は最も低く、その周辺部の
乳白色の濃さは、その最大部の乳白色の濃さ部から遠ざ
かるほど徐々に、または段階的に乳白色の濃さを薄くし
ていることから、透過率は徐々に、または段階的高くな
っている。
In the fifth embodiment, the means for making the transmittance different is a light-diffusing milky white color,
The light-diffusing milky white color of the globe 1 closest to the light source is the maximum density, the transmittance is the lowest, and the milky white density in the periphery is the farther from the maximum milky whiteness part. Due to the gradual or stepwise reduction of the milky white density, the transmittance is gradually or stepwise increased.

【0023】これらの照明装置についても、前記第二の
実施例の場合と同じく、光源から遠ざかるほどグローブ
1の透過率が高くなっていることから、同様な作用、す
なわち光源とグローブとの距離にかかわらずグローブ表
面の明るさが均一で、均等な配光が得られる。
As in the case of the above-described second embodiment, the illuminating device is also configured such that the further away from the light source, the more the globe becomes.
Since the transmittance of 1 is high, the same effect is obtained, that is, the brightness of the globe surface is uniform regardless of the distance between the light source and the globe, and a uniform light distribution is obtained.

【0024】以上、発明の実施の形態を独立して述べて
きたが、重複の実施も適用できる。
Although the embodiments of the present invention have been described independently, overlapping implementations are also applicable.

【図面の簡単な説明】[Brief description of the drawings]

【図1】この発明の第一および第二の一実施の形態に係
る照明装置の一部を断面した側面図である。
FIG. 1 is a side sectional view of a part of a lighting device according to first and second embodiments of the present invention.

【図2】この発明の第四の一実施の形態に係る、拡大倍
率を等しくしたときのシボ模様である。
FIG. 2 is a grain pattern when an enlargement magnification is equal according to a fourth embodiment of the present invention.

【図3】従来の照明装置の一部を断面した側面図であ
る。
FIG. 3 is a cross-sectional side view of a part of a conventional lighting device.

【符号の説明】[Explanation of symbols]

1 グローブ 2 光源 3 ソケット 4 パッキン 5 取付台 6 電源線 7 従来の照明装置におけるグローブ I 光度 S 光源からグローブまでの距離 E グローブ内面照度 L 輝度 DESCRIPTION OF SYMBOLS 1 Glove 2 Light source 3 Socket 4 Packing 5 Mounting base 6 Power line 7 Globe in conventional lighting equipment I Luminous intensity S Distance from light source to globe E Luminance inside glove L Luminance

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 照明器具を覆う非透明の光拡散性の外郭
部材であるグローブにおいて、その光透過率を該光源か
らの距離に略比例に関連付けて異ならせた事を特徴とす
る照明装置。
1. A lighting device, wherein a light transmittance of a glove which is a non-transparent light-diffusing outer member for covering a lighting device is made to vary substantially in proportion to a distance from the light source.
【請求項2】 透過率を異ならせる手段が肉厚で、光源
から最も近い部分のグローブ肉厚を最大肉厚とし、その
周辺部の肉厚は、その最大肉厚部から遠ざかるほど徐々
に、または段階的に薄肉厚にしたことを特徴とする請求
項1記載の照明装置。
2. The means for varying the transmittance is thick, the thickness of the globe closest to the light source is the maximum thickness, and the thickness of the periphery is gradually increased as the distance from the maximum thickness increases. 2. The lighting device according to claim 1, wherein the lighting device is formed to have a small thickness in a stepwise manner.
【請求項3】 透過率を異ならせる手段がシボの深さ
で、光源から最も近い部分のグローブシボ深さを最大と
し、その周辺部のシボ深さは、その最大のシボ深さ部か
ら遠ざかるほど徐々に、または段階的にシボ深さを浅く
したことを特徴とする請求項1記載の照明装置。
3. The means for making the transmittance different is the depth of the grain, wherein the depth of the glove grain closest to the light source is maximized, and the depth of the grain in the peripheral portion increases as the distance from the maximum grain depth increases. The lighting device according to claim 1, wherein the embossing depth is gradually or gradually reduced.
【請求項4】 透過率を異ならせる手段がシボ模様の粗
さで、光源から最も近い部分のグローブシボ模様を最小
の粗さとし、その周辺部のシボ模様は、その最小粗さの
シボ模様部から遠ざかるほど徐々に、または段階的によ
りシボ粗さの粗いシボ模様にしたことを特徴とする請求
項1記載の照明装置。
4. The means for making the transmittance different is the roughness of the grain pattern, wherein the glove grain pattern at the portion closest to the light source has the minimum roughness, and the grain pattern at the periphery thereof is from the grain pattern having the minimum roughness. 2. The lighting device according to claim 1, wherein the texture is gradually or gradually increased as the distance increases.
【請求項5】 透過率を異ならせる手段が光拡散性のあ
る乳白色の色の濃さで、光源から最も近い部分のグロー
ブの光拡散性のある乳白色を最大の濃さとし、その周辺
部の乳白色の濃さは、その最大部の乳白色の濃さ部から
遠ざかるほど徐々に、または段階的に乳白色の濃さを薄
くしたことを特徴とする請求項1記載の照明装置。
5. The means for varying the transmittance is a light-diffuse milky white color density, the light-diffusible milky white color of the globe closest to the light source is made the maximum density, and the milky white color at the periphery thereof 2. The lighting device according to claim 1, wherein the density of the milky white is gradually or gradually reduced as the distance from the maximum milky white density part increases.
JP10270395A 1998-09-24 1998-09-24 Lighting system Pending JP2000100222A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10270395A JP2000100222A (en) 1998-09-24 1998-09-24 Lighting system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10270395A JP2000100222A (en) 1998-09-24 1998-09-24 Lighting system

Publications (1)

Publication Number Publication Date
JP2000100222A true JP2000100222A (en) 2000-04-07

Family

ID=17485671

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10270395A Pending JP2000100222A (en) 1998-09-24 1998-09-24 Lighting system

Country Status (1)

Country Link
JP (1) JP2000100222A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010198808A (en) * 2009-02-23 2010-09-09 Sharp Corp Lighting device
EP2769142B1 (en) 2011-10-19 2018-02-21 Philips Lighting Holding B.V. Lighting device with omnidirectional light distribution

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010198808A (en) * 2009-02-23 2010-09-09 Sharp Corp Lighting device
EP2769142B1 (en) 2011-10-19 2018-02-21 Philips Lighting Holding B.V. Lighting device with omnidirectional light distribution
EP2769142B2 (en) 2011-10-19 2020-11-25 Signify Holding B.V. Lighting device with omnidirectional light distribution

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