JPH11248628A - Light scattering type particle detecting sensor - Google Patents

Light scattering type particle detecting sensor

Info

Publication number
JPH11248628A
JPH11248628A JP4648998A JP4648998A JPH11248628A JP H11248628 A JPH11248628 A JP H11248628A JP 4648998 A JP4648998 A JP 4648998A JP 4648998 A JP4648998 A JP 4648998A JP H11248628 A JPH11248628 A JP H11248628A
Authority
JP
Japan
Prior art keywords
light
trap
optical
type particle
scattering type
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
JP4648998A
Other languages
Japanese (ja)
Inventor
Naoyuki Nishikawa
尚之 西川
Akiko Honda
亜紀子 本田
Shinji Kirihata
慎司 桐畑
Yutaka Abe
豊 阿部
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP4648998A priority Critical patent/JPH11248628A/en
Publication of JPH11248628A publication Critical patent/JPH11248628A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide a light scattering type particle detecting sensor which can be enhanced further in sensitivity. SOLUTION: A light projecting element 4 and a light receiving element 5 are arranged in an optical room 2 in the form of crossing respective light axes so that scattered light from the light projecting element 4 due to particles of smoke and dust in a detection area (a) of overlapping a projection area of the light projecting element 4 with a receiving area of the light receiving element 5 can be received by the light receiving element 5 to detect particles. In this case, a first cylindrical light trap A which has an opening with the diameter gradually narrower from the opening and a second light trap B which is interconnected to the first light trap A so as to guide light having entered into the first light trap A and has an opening with the diameter wider from the connection to the first light trap A are provided in the optical room 2.

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、粉塵や煙草の煙を
検知したり、あるいは光電式煙感知器等において煙粒子
を感知したりするために用いられる光散乱式粒子検知セ
ンサに関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a light scattering type particle detection sensor used for detecting dust or smoke from cigarettes, or for detecting smoke particles in a photoelectric smoke detector or the like. .

【0002】[0002]

【従来の技術】この種の光散乱式粒子検知センサは、そ
れぞれ光軸を交差させる形で光学室内に配置された投光
素子と受光素子とを備え、投光素子の投光領域と受光素
子の受光領域とが重合する領域である検知領域における
煙や粉塵等の粒子による投光素子からの光の散乱光を受
光素子にて受光することにより粒子を検出するものであ
る。光学室を形成するケースは煙や粉塵等の粒子が流入
しやすく外光が入りにくい構造とするため、2重構造と
したり、煙粒子等の流入部をラビリンス構造としたりし
ている。
2. Description of the Related Art A light scattering type particle detection sensor of this type includes a light projecting element and a light receiving element which are arranged in an optical chamber so that their optical axes cross each other. This is to detect particles by receiving light scattered light from the light emitting element due to particles such as smoke and dust in the detection area where the light receiving area overlaps with the light receiving element. The case that forms the optical chamber has a double structure or a labyrinth structure at the inflow portion of smoke particles and the like in order to make the structure such that particles such as smoke and dust easily flow in and external light does not easily enter.

【0003】従来のこの種の光散乱式粒子検知センサ
は、投光素子からの光が光学室の内壁によって反射さ
れ、その光が迷光となって受光素子に達し、光学的なS
/N比が悪化するという問題点を有している。
In this type of conventional light scattering type particle detection sensor, light from a light projecting element is reflected by the inner wall of an optical chamber, and the light reaches a light receiving element as stray light, and the optical S
There is a problem that the / N ratio deteriorates.

【0004】そこで、この点を改善した光散乱式粒子検
知センサとして図8に示すようなものがある。この光散
乱式粒子検知センサでは、光学室2内に遮光壁11を設
け、投光素子4からの光が受光素子5に入るまでに、遮
光壁11や光学室2の内壁等により囲まれた領域にて複
数回反射される構造をもつようにしている。すなわち、
この光散乱式粒子検知センサでは、反射による光の減衰
を利用し、反射回数を増やすことで迷光のパワーを下げ
ようとしているのである。なお、投光素子4と受光素子
5との間には投光素子4からの光の受光素子5への直接
の回り込みを防止する遮光部10が設けられている。
FIG. 8 shows a light scattering type particle detection sensor which improves this point. In this light scattering type particle detection sensor, a light shielding wall 11 is provided in the optical chamber 2, and is surrounded by the light shielding wall 11, the inner wall of the optical chamber 2, and the like before the light from the light projecting element 4 enters the light receiving element 5. It has a structure that is reflected multiple times in the area. That is,
In this light scattering type particle detection sensor, the power of stray light is reduced by increasing the number of times of reflection by utilizing the attenuation of light due to reflection. In addition, between the light projecting element 4 and the light receiving element 5, there is provided a light shielding unit 10 for preventing light from the light projecting element 4 from directly entering the light receiving element 5.

【0005】また、図9に示す光散乱式粒子検知センサ
では、投光素子4の対向面に光学室2の内壁を鋭角とな
すことにより構成した投光側光トラップBと、受光素子
5の対向面に同様の構成を有する受光側光トラップAを
設けている。これにより、投光素子4から射出されて投
光側光トラップBに導かれた光は、内壁に反射しながら
奥へ進むことになるため、迷光のパワーを下げることが
可能になるとともに、一旦導かれた光が投光素子4側へ
戻らないようになっている。同様に、受光側光トラップ
Aにおいても、導かれた迷光が数回内壁に当たって減衰
するとともに、受光素子5側へ戻らないような構造とな
っている。
In the light-scattering type particle detection sensor shown in FIG. 9, the light-emitting side light trap B formed by forming the inner wall of the optical chamber 2 at an acute angle on the surface facing the light-emitting element 4 and the light-receiving element 5 A light receiving side optical trap A having a similar configuration is provided on the facing surface. Accordingly, the light emitted from the light projecting element 4 and guided to the light projecting side light trap B travels to the back while being reflected on the inner wall, so that the power of the stray light can be reduced, and The guided light does not return to the light emitting element 4 side. Similarly, the light trap A on the light-receiving side has such a structure that the guided stray light hits the inner wall several times and is attenuated, and does not return to the light-receiving element 5 side.

【0006】上述したように、図8及び図9で示した光
散乱式粒子検知センサでは、投光素子4から射出された
光が光学室2の内壁等で反射して受光素子5に入射し測
定精度が悪化することを防止するために、迷光の発生を
抑えることで投光パワーに対する迷光比(迷光パワー/
投光パワー)が微弱になるようにし、煙や粉塵等の粒子
濃度を正確に測定しようとするのである。
As described above, in the light scattering type particle detection sensor shown in FIGS. 8 and 9, the light emitted from the light projecting element 4 is reflected on the inner wall of the optical chamber 2 and enters the light receiving element 5. In order to prevent measurement accuracy from deteriorating, stray light generation (stray light power /
The light emission power) is set to be weak, and the concentration of particles such as smoke and dust is to be accurately measured.

【0007】[0007]

【発明が解決しようとする課題】ところが、上述の構成
の光散乱式粒子検知センサでは、光学室2内に埃等が生
じると急激に迷光パワーが増加してしまうという問題点
を有している。例えば、図8に示す光散乱式粒子検知セ
ンサでは、投光素子4から射出される光が一番最初に反
射する内壁と投光軸とのなす角度が略直角であるため、
この位置に埃が付着していた場合に埃による散乱光が発
生する。理想的な粗面物体に反射した場合、散乱光はラ
ンバート分布となり、これは照射点に対してほぼ全方向
に広がるが、散乱光の強度は入射方向に対して正反射方
向の成分が最も大きいものとなる。すなわち、この光散
乱式粒子検知センサでは、埃による散乱光は壁との角度
が直角に近いため、入射方向に散乱する強度が大きくな
り、それが遮光壁11等で囲まれた領域を飛び出し、強
度の大きな迷光になるのである。受光軸についても、光
軸上の光の受光効率が最も高くなるため、光軸上の埃に
よる迷光の影響は問題になる。
However, the light scattering type particle detection sensor having the above-described structure has a problem that when dust or the like is generated in the optical chamber 2, the power of the stray light rapidly increases. . For example, in the light scattering type particle detection sensor shown in FIG. 8, since the angle between the inner wall where light emitted from the light projecting element 4 is reflected first and the light projecting axis is substantially a right angle,
If dust adheres to this position, scattered light due to dust is generated. When reflected on an ideal rough surface object, the scattered light has a Lambertian distribution, which spreads in almost all directions with respect to the irradiation point, but the intensity of the scattered light has the largest component in the regular reflection direction with respect to the incident direction. It will be. That is, in this light-scattering type particle detection sensor, the intensity of the scattered light due to dust is scattered in the incident direction because the angle with respect to the wall is almost perpendicular, and the scattered light jumps out of the area surrounded by the light shielding wall 11 and the like. It becomes stray light with large intensity. Regarding the light receiving axis, the effect of stray light due to dust on the optical axis poses a problem because the light receiving efficiency of light on the optical axis is highest.

【0008】また、この種の光散乱式粒子検知センサで
は、光トラップの奥の先端部の尖った部分に埃が溜まり
やすい。従って、図9に示す光散乱式粒子検知センサで
は、図10に示すように、光トラップの内壁に向かって
入射した光の多くは複数回反射しないと光トラップから
飛び出さないが、光トラップの奥に溜まった埃に光が直
接入射すると、1回の反射のみで光トラップを飛び出す
ことになる。また、埃に反射した光は全方位に反射する
散乱を生じ、やはり強い光が光りトラップを飛び出す原
因となる。すなわち、受光側光トラップAや投光側光ト
ラップBに埃が溜まると埃による散乱のため、埃がない
ときに比べ、はるかに迷光の発生が大きくなる。さら
に、投光領域の光軸に沿って入射する光は一般的に光強
度が強く、光軸上の埃による迷光の影響は特に問題にな
る。同様に受光領域の光軸についても、光軸上の光が最
も受光効率が良いため、光軸上の埃による迷光の影響は
問題になる。また、図9に示す光散乱式粒子検知センサ
では、製作上、受光側光トラップAや投光側光トラップ
Bの奥に存する頂角を完全に尖らせることは困難であ
る。このため、この部分が若干丸みを帯びた形状となる
と、入射した迷光がわずかな回数の反射をしただけで光
トラップA、Bから出てしまうといったことがあり、十
分に迷光パワーを減衰し得ないことがある。
[0008] In this type of light scattering type particle detection sensor, dust tends to accumulate at the sharp point at the end of the back of the optical trap. Therefore, in the light scattering type particle detection sensor shown in FIG. 9, as shown in FIG. 10, most of the light incident on the inner wall of the optical trap does not jump out of the optical trap unless it is reflected a plurality of times. When light is directly incident on the dust accumulated in the back, the light will jump out of the optical trap by only one reflection. In addition, the light reflected on the dust causes scattering which is reflected in all directions, and the strong light also causes the light to jump out of the trap. That is, if dust accumulates in the light receiving side light trap A or the light projecting side light trap B, the dust is scattered, and the generation of stray light is much larger than when there is no dust. Furthermore, light incident along the optical axis of the light projecting region generally has a high light intensity, and the effect of stray light due to dust on the optical axis is particularly problematic. Similarly, with respect to the optical axis of the light receiving region, the effect of stray light due to dust on the optical axis poses a problem because light on the optical axis has the highest light receiving efficiency. Further, in the light scattering type particle detection sensor shown in FIG. 9, it is difficult to completely sharpen the apex existing in the back of the light receiving side light trap A and the light projecting side light trap B due to manufacturing. For this reason, if this portion has a slightly rounded shape, the incident stray light may exit the optical traps A and B with only a small number of reflections, and the stray light power may be sufficiently attenuated. There may not be.

【0009】本発明は、上記の問題点に鑑みて成された
ものであり、その目的とするところは、さらに一層の高
感度化を図ることができる光散乱式粒子検知センサを提
供することにある。
The present invention has been made in view of the above problems, and an object of the present invention is to provide a light-scattering type particle detection sensor capable of further increasing the sensitivity. is there.

【0010】[0010]

【課題を解決するための手段】請求項1記載の発明は、
それぞれ光軸を交差させる形で光学室内に配置された投
光素子と受光素子とを備え、投光素子の投光領域と受光
素子の受光領域とが重合する領域である検知領域におけ
る煙や粉塵等の粒子による投光素子からの散乱光を受光
素子で受光することにより粒子を検出する光散乱式粒子
検知センサにおいて、開口部より徐々に開口径が細くな
る筒状の第1の光トラップと、第1の光トラップに侵入
した光が導かれるように第1の光トラップに連接し、第
1の光トラップとの連接部から開口径が広くなる第2の
光トラップとを光学室内に設けたことを特徴とするもの
である。
According to the first aspect of the present invention,
A light-emitting element and a light-receiving element arranged in an optical chamber so that the optical axes cross each other, and smoke and dust in a detection area where a light-emitting area of the light-emitting element and a light-receiving area of the light-receiving element overlap. In a light scattering type particle detection sensor that detects particles by receiving light scattered from a light emitting element by a light receiving element by particles such as a first light trap having a cylindrical shape in which an opening diameter is gradually narrower than an opening. A second optical trap, which is connected to the first optical trap so that the light that has entered the first optical trap is guided, and has a larger opening diameter from a connection with the first optical trap, is provided in the optical chamber. It is characterized by having.

【0011】請求項2記載の発明は、請求項1記載の光
散乱式粒子検知センサにおいて、投光素子及び受光素子
の光軸から逸れるように第2の光トラップの開口を配置
するようにしたことを特徴とするものである。
According to a second aspect of the present invention, in the light scattering type particle detection sensor according to the first aspect, the opening of the second optical trap is arranged so as to deviate from the optical axes of the light projecting element and the light receiving element. It is characterized by the following.

【0012】請求項3記載の発明は、請求項1又は請求
項2記載の光散乱式粒子検知センサにおいて、第2の光
トラップの内壁に複数の溝を設けたことを特徴とするも
のである。
According to a third aspect of the present invention, in the light scattering type particle detection sensor according to the first or second aspect, a plurality of grooves are provided on an inner wall of the second optical trap. .

【0013】請求項4記載の発明は、請求項1乃至請求
項3記載の光散乱式粒子検知センサにおいて、第1の光
トラップの開口を投光素子及び受光素子と対向する位置
に設けたことを特徴とするものである。
According to a fourth aspect of the present invention, in the light scattering type particle detection sensor according to the first to third aspects, the opening of the first optical trap is provided at a position facing the light emitting element and the light receiving element. It is characterized by the following.

【0014】[0014]

【発明の実施の形態】以下、本発明の第1の実施の形態
について図1乃至図4に基づき、第2の実施の形態につ
いて図5乃至図7に基づき詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, a first embodiment of the present invention will be described in detail with reference to FIGS. 1 to 4, and a second embodiment with reference to FIGS. 5 to 7. FIG.

【0015】[第1の実施の形態]図1は本発明に係る
第1の実施の形態の光散乱式粒子検知センサの縦断面図
である。図2は本発明に係る第1の実施の形態の光散乱
式粒子検知センサの分解斜視図である。図3は光散乱式
粒子検知センサ内を進行する光の様子を示す縦断面図で
ある。図4は入射した光が反射する様子を示す模式図で
ある。
[First Embodiment] FIG. 1 is a longitudinal sectional view of a light scattering type particle detection sensor according to a first embodiment of the present invention. FIG. 2 is an exploded perspective view of the light scattering type particle detection sensor according to the first embodiment of the present invention. FIG. 3 is a longitudinal sectional view showing a state of light traveling in the light scattering type particle detection sensor. FIG. 4 is a schematic diagram showing how incident light is reflected.

【0016】本実施の形態の光散乱式粒子検知センサで
は、中空の直方型のケース1により光学室2を形成して
いる。ケース1には、光の反射率を下げるとともに、成
型性を考慮して黒色のABS樹脂等が用いられる。な
お、アルミ等に黒色アルマイト処理を施したものを用い
ても、反射率を下げることができ、効果的である。
In the light scattering type particle detection sensor according to the present embodiment, the optical chamber 2 is formed by the hollow rectangular case 1. For the case 1, a black ABS resin or the like is used in consideration of moldability while lowering the light reflectance. It is to be noted that, even when aluminum or the like subjected to black alumite treatment is used, the reflectance can be reduced, which is effective.

【0017】ケース1の左上角に投光素子4と投光レン
ズ17を設け、投光素子4からの投光ビームの光軸が対
角位置にある右下角に向けて射出されるように配置す
る。この投光ビームが通過する範囲を投光領域とする。
ここで投光素子4としては、LEDや半導体レーザ、固
体レーザ等が用いられる。なお、投光レンズ17は必ず
しも必要ではないが、本実施の形態の光散乱式粒子検知
センサでは投光素子4から射出される光を集光させ検知
領域イに集中させるために用いている。
A light projecting element 4 and a light projecting lens 17 are provided at the upper left corner of the case 1, and are arranged such that the optical axis of the light beam emitted from the light projecting element 4 is emitted toward the diagonally lower right corner. I do. The range through which the light beam passes is referred to as a light projecting area.
Here, as the light emitting element 4, an LED, a semiconductor laser, a solid-state laser, or the like is used. Although the light projection lens 17 is not always necessary, the light scattering type particle detection sensor according to the present embodiment is used for condensing light emitted from the light projection element 4 and concentrating the light on the detection area A.

【0018】また、受光素子5と受光レンズ7は、ケー
ス1の右上角に設け、受光素子5から受光レンズ7を通
して見える領域(受光領域)の光軸が対角位置にある左
下角に向くように配置する。受光素子5としては、フォ
トダイオードやフォトトランジスタ等が用いられる。な
お、受光レンズ7は必ずしも必要ではないが、本実施の
形態の光散乱式粒子検知センサでは受光効率をあげるた
めに用いている。
The light receiving element 5 and the light receiving lens 7 are provided at the upper right corner of the case 1 so that the optical axis of a region (light receiving area) that can be seen from the light receiving element 5 through the light receiving lens 7 is directed to the lower left corner at the diagonal position. To place. As the light receiving element 5, a photodiode, a phototransistor, or the like is used. Although the light receiving lens 7 is not always necessary, the light scattering type particle detection sensor according to the present embodiment is used to increase the light receiving efficiency.

【0019】投光側のアパーチャ6は投光素子4の投光
領域の大きさを制御しているほか、迷光の原因となる投
光方向に対して広がる光を除去するために用いられてい
る。受光側のアパーチャ9も受光素子5の受光領域の大
きさを制御するほか、受光素子5の収まる筒内部に反射
した迷光を除去するために用いられている。
The aperture 6 on the light projecting side is used to control the size of the light projecting area of the light projecting element 4 and to remove light spreading in the light projecting direction which causes stray light. . The aperture 9 on the light receiving side is also used for controlling the size of the light receiving area of the light receiving element 5 and for removing stray light reflected inside the cylinder in which the light receiving element 5 fits.

【0020】上述したケース1は、一側面が開口された
矩形箱状で光学室2の一側壁となる面の外面に受光素子
5の出力に応じて適宜信号処理を行う処理回路を構成す
るプリント基板20が装着されたベース1aと、このベ
ース1aの開口に被着されるカバー1bとで構成され
る。
The above-described case 1 has a rectangular box shape with one side opened, and a printed circuit constituting a processing circuit for appropriately performing signal processing in accordance with the output of the light receiving element 5 on the outer surface of the optical chamber 2 serving as one side wall. It comprises a base 1a on which the substrate 20 is mounted, and a cover 1b attached to the opening of the base 1a.

【0021】検知領域イは、投光領域と受光領域とが重
なる領域である。煙草の煙や埃等の粒子は、検知領域イ
に合わせて設けられた流入口3から検知領域イへ流入す
る。なお、この流入口3は煙や埃等の粒子を光学室2内
に流入する目的で設けられているので、検知領域イのす
ぐ下にある必要はなく、別の位置に設けるようにしても
よい。
The detection area A is an area where the light emitting area and the light receiving area overlap. Particles such as cigarette smoke and dust flow into the detection area A from the inflow port 3 provided corresponding to the detection area A. Since the inflow port 3 is provided for the purpose of allowing particles such as smoke and dust to flow into the optical chamber 2, it is not necessary that the inflow port 3 is located immediately below the detection area A, but may be provided at another position. Good.

【0022】投光素子4から出た光は投光レンズ17を
通して検知領域イに入り、検知領域イ内に存在する粒子
に当たった光が散乱し、散乱光の一部が受光素子5に入
る。この流入口3から検知領域イに入る粒子の数が多い
ほど散乱光量が増えるため、受光素子5の受光量も増え
ることになる。従って、受光量を計測することにより、
粒子の数(煙濃度)を計測することができるのである。
The light emitted from the light projecting element 4 enters the detection area A through the light projecting lens 17, and the light hitting the particles existing in the detection area A is scattered, and a part of the scattered light enters the light receiving element 5. . As the number of particles entering the detection area A from the inlet 3 increases, the amount of scattered light increases, so that the amount of light received by the light receiving element 5 also increases. Therefore, by measuring the amount of received light,
The number of particles (smoke density) can be measured.

【0023】本実施の形態の光散乱式粒子検知センサに
おいて、投光素子4から射出される投光ビームの光軸上
で、検知領域イからみて投光素子4と反対側に、筒状で
投光ビームを捕捉する開口を有し開口径が徐々に小さく
なる部分(以下、投光側第1の光トラップB1と記載す
る)を設け、その先端に投光側第1の光トラップB1に
連接するとともに連接部(以下、投光側連接部B3と記
載する)から開口径が広がるような空間(以下、投光側
第2の光トラップB2と記載する)を設ける。投光側第
1の光トラップB1の開口の大きさは、投光素子4から
射出した光が全て投光側第1の光トラップB1に入るの
に十分な大きさを開けておく。なお、投光側第1の光ト
ラップB1の開口の形状に特に制限はなく、長方形のほ
か円形等様々な形状であってもよい。また、投光側第2
の光トラップB2の形状も本実施の形態のように縦断面
形状が円形となるものに限られるものではなく、多角形
状等様々な形状であってもよい。
In the light scattering type particle detection sensor according to the present embodiment, a cylindrical shape is provided on the optical axis of the light beam emitted from the light projecting element 4 on the side opposite to the light projecting element 4 as viewed from the detection area A. A portion (hereinafter, referred to as a first light trap B1 on the light projecting side) having an opening for capturing a light projecting beam and having a gradually decreasing opening diameter is provided, and the first light trap B1 on the light projecting side is provided at the tip thereof. A space (hereinafter, referred to as a light projecting side second optical trap B2) is provided so as to be connected and to have a larger opening diameter from a connecting portion (hereinafter, referred to as a light projecting side connecting portion B3). The size of the opening of the first light trap B1 on the light projecting side is large enough to allow all the light emitted from the light projecting element 4 to enter the first light trap B1 on the light projecting side. The shape of the opening of the first light trap B1 on the light emitting side is not particularly limited, and may be various shapes such as a rectangle and a circle. In addition, the light emitting side second
The shape of the optical trap B2 is not limited to a circular vertical cross-sectional shape as in the present embodiment, but may be various shapes such as a polygonal shape.

【0024】この投光側第1の光トラップB1の開口に
投光素子4から射出した光を入射させると、図3に示す
ように、入射した光は投光側第1の光トラップB1の内
壁で反射を繰り返しながら減衰していく。また、投光側
第1の光トラップB1は筒状になっているので入射光の
壁に当たる角度が浅く、反射した光は最初の光の進行方
向に近い方向、つまり投光側第1の光トラップB1の奥
の方へ向かって反射が繰り返されるため、反射回数が増
えても光は第1の光トラップB1から漏れ出さないよう
になっている。そして、光が一旦投光側第2の光トラッ
プB2へ入り込むと、投光側連接部B3が狭くなってい
ることにより、投光側第2の光トラップB2に入射した
光が第2の光トラップの外に出にくくなる。また、投光
側第2の光トラップB2内でさらに反射を繰り返すた
め、たとえ投光側第2の光トラップB2から飛び出すこ
とがあったとしても、その強度は極めて微小なものとな
っている。この投光側連接部B3を小さくすれば、反射
光が投光側第2の光トラップB2からさらに出にくくな
る。なお、投光側連接部B3の開口面積に対して投光側
第2の光トラップB2の内壁の面積が大きくなるように
すれば、相対的に反射光が投光側第2の光トラップB2
から出にくくなる。従って、投光側第2の光トラップB
2の内壁の面積を大きくして迷光を減少するようにして
もよい。
When the light emitted from the light projecting element 4 is made incident on the opening of the first light trap B1 on the light projecting side, as shown in FIG. Attenuates while repeating reflections on the inner wall. In addition, since the first light trap B1 on the light projecting side has a cylindrical shape, the angle of incidence on the wall of the incident light is small, and the reflected light is in a direction close to the traveling direction of the first light, that is, the first light on the light projecting side. Since the reflection is repeated toward the back of the trap B1, light does not leak out of the first optical trap B1 even if the number of reflections increases. Then, once the light enters the light projecting side second optical trap B2, the light incident on the light projecting side second optical trap B2 becomes the second light due to the narrowing of the light projecting side connecting portion B3. It is difficult to get out of the trap. In addition, since the reflection is further repeated in the second light trap B2 on the light projecting side, even if the light may jump out of the second light trap B2 on the light projecting side, the intensity is extremely small. If the light projecting side connecting portion B3 is made smaller, it becomes more difficult for reflected light to exit from the light projecting side second optical trap B2. If the area of the inner wall of the light projecting side second optical trap B2 is made larger than the opening area of the light projecting side connecting part B3, the reflected light is relatively reflected in the light projecting side second optical trap B2.
Hard to get out of Therefore, the light-emitting side second optical trap B
The stray light may be reduced by increasing the area of the inner wall 2.

【0025】また、壁に付着した埃で光が反射すると、
図4に示すように、全方向への散乱が生じる。本実施の
形態では、たとえ投光軸の先端に埃が付着し、光が投光
側第2の光トラップB2内の全方向に散乱したとして
も、投光側連接部B3が狭く、全方向対する投光側連接
部B3の見込み角が小さくなるため、投光側第2の光ト
ラップB2から出る散乱光を十分に弱くすることが可能
になる。なお、第2の光トラップを広くするほど投光側
連接部B3から出る散乱光の見込み角を小さくすること
ができるので、さらに迷光の減少を図ることが可能にな
る。
Also, when light is reflected by dust adhering to the wall,
As shown in FIG. 4, scattering occurs in all directions. In the present embodiment, even if dust adheres to the tip of the light projecting axis and light is scattered in all directions in the light projecting side second optical trap B2, the light projecting side connecting portion B3 is narrow and omnidirectional. Since the prospective angle of the light projecting side connecting portion B3 becomes small, the scattered light emitted from the light projecting side second optical trap B2 can be sufficiently weakened. It should be noted that the wider the second optical trap, the smaller the expected angle of the scattered light emitted from the light projecting side connecting portion B3, so that it is possible to further reduce stray light.

【0026】以上より投光素子4から投光された光が投
光側第1の光トラップB1から投光側第2の光トラップ
B2に反射しながら入り込むことによって、反射光のみ
ならず散乱光による迷光の発生を十分に減少させること
ができる。
As described above, the light projected from the light projecting element 4 enters from the first light trap B1 on the light projecting side to the second light trap B2 on the light projecting side while being reflected. The generation of stray light due to the above can be sufficiently reduced.

【0027】一方、受光側でも受光素子5へ入射する受
光領域の光軸上で、検知領域イからみて受光素子5と反
対側に、受光領域をカバーするだけの開口をもった、投
光素子4の対面に配したものと同様の形状(受光側第1
の光トラップA1及び受光側第2の光トラップA2より
なる形状)の光トラップを設けている。受光素子5と対
面する光トラップに一旦入った光は、投光側と同様に、
反射光及び散乱光ともに減衰され、外に漏れ出す光が十
分微小になる。これにより、受光素子5に入射する迷光
の強度を微弱に抑えることが可能になる。
On the other hand, on the light receiving side, on the optical axis of the light receiving area which enters the light receiving element 5, a light projecting element having an opening for covering the light receiving area is provided on the opposite side to the light receiving element 5 as viewed from the detection area A. 4 (the light-receiving side first)
(A shape composed of the light trap A1 and the second light trap A2 on the light receiving side). The light once entering the light trap facing the light receiving element 5 is, like the light emitting side,
Both the reflected light and the scattered light are attenuated, and the light leaking outside becomes sufficiently small. Thus, the intensity of the stray light incident on the light receiving element 5 can be suppressed to a very small value.

【0028】光散乱式粒子検知センサでは、粒子による
散乱光は入射される投光パワーに比べてきわめて微弱で
ある。そのため、粒子によって散乱を受けなかった光が
受光素子5に入射するのを如何に阻止するかが、光散乱
式粒子検知センサの高感度化を図る上でのポイントにな
る。例えば、本実施の形態の光散乱式粒子検知センサに
おいて、実際に建築物管理基準の浮遊粉塵濃度の規制レ
ベルである0.1mg/m3の濃度の粒子を観測する場合につい
て検討する。本実施の形態における検知領域イは数cm3
程度であるが、検知領域イに投光される投光強度は数mW
オーダーの大きさであるのに対し、検知領域イで検知さ
れる散乱光強度は数pWオーダーであり、実に投光強度に
対し10-9もの微弱な散乱光を計測する必要がある。
In the light scattering type particle detection sensor, the light scattered by the particles is extremely weak as compared with the incident light power. Therefore, how to prevent light that has not been scattered by the particles from entering the light receiving element 5 is a point in increasing the sensitivity of the light scattering type particle detection sensor. For example, consider the case where the light scattering particle detection sensor according to the present embodiment actually observes particles having a concentration of 0.1 mg / m 3 which is the regulation level of the suspended dust concentration in the building management standard. The detection area A in this embodiment is several cm 3
The intensity of light projected on the detection area b is several mW
In contrast to the order of magnitude, the scattered light intensity detected in the detection area A is on the order of several pW, and it is actually necessary to measure scattered light as weak as 10 -9 with respect to the projected light intensity.

【0029】本実施の形態では、まず入射した光は投光
側第1の光トラップB1を何回も反射しながら奥へ進
み、投光側第2の光トラップB2まで入り込んだ光はほ
とんど外に漏れ出ることはない。投光側第1の光トラッ
プB1及び投光側第2の光トラップB2の内壁に黒色の
ABS樹脂等を用いた場合、反射率は10%以下になる
ので、さらに減衰効果が高く、迷光パワーを十分に減衰
することが可能になる。また、従来の光散乱式粒子検知
センサにおいて、受光素子5に入射していた迷光は、投
光側と同様に、受光側第1の光トラップA1及び受光側
第2の光トラップA2よりなる形状にて十分減衰するこ
とが可能になる。
In this embodiment, firstly, the incident light travels deeply while reflecting the first light trap B1 on the light projecting side many times, and the light that has entered the second light trap B2 on the light projecting side is almost outside. Do not leak to When black ABS resin or the like is used for the inner walls of the first light trap B1 on the light emitting side and the second light trap B2 on the light emitting side, the reflectance becomes 10% or less, so that the attenuation effect is higher and the stray light power is increased. Can be sufficiently attenuated. Further, in the conventional light scattering type particle detection sensor, the stray light incident on the light receiving element 5 has a shape composed of the first light trap A1 on the light receiving side and the second light trap A2 on the light receiving side, similarly to the light projecting side. Can be sufficiently attenuated.

【0030】本実施の形態によれば、投光パワーに対す
る迷光比(迷光パワー/投光パワー)を非常に微小にす
ることができ、粒子濃度の高感度測定を行うことが可能
になる。
According to this embodiment, the ratio of stray light to the power of projected light (stray light power / power of projected light) can be made extremely small, and high sensitivity measurement of particle concentration can be performed.

【0031】なお、投光素子4又は受光素子5のどちら
か一方のみに光トラップを設けた場合、両方に光トラッ
プを設けた場合に比べ、迷光の強度は抑えられないが、
従来の光散乱式粒子検知センサと比較するとその効果は
十分大きなものとなる。
When an optical trap is provided in only one of the light projecting element 4 and the light receiving element 5, the intensity of stray light cannot be suppressed as compared with a case in which an optical trap is provided in both of them.
The effect is sufficiently large as compared with the conventional light scattering type particle detection sensor.

【0032】[第2の実施の形態]図5は本発明に係る
第2の実施の形態の光散乱式粒子検知センサの縦断面図
である。図6は本発明に係る第2の実施の形態の光散乱
式粒子検知センサの分解斜視図である。図7は光散乱式
粒子検知センサ内を進行する光の様子を示す縦断面図で
ある。なお、本実施の形態に係る光散乱式粒子検知セン
サにおいて、第1の実施の形態の図1に示したものと同
等の箇所には同じ番号を付し、その詳細な説明は省略す
る。
[Second Embodiment] FIG. 5 is a longitudinal sectional view of a light scattering type particle detection sensor according to a second embodiment of the present invention. FIG. 6 is an exploded perspective view of the light scattering type particle detection sensor according to the second embodiment of the present invention. FIG. 7 is a longitudinal sectional view showing a state of light traveling in the light scattering type particle detection sensor. In the light scattering type particle detection sensor according to the present embodiment, the same parts as those of the first embodiment shown in FIG. 1 are denoted by the same reference numerals, and detailed description thereof will be omitted.

【0033】本実施の形態の光散乱式粒子検知センサで
は、図5に示すように、第2の光トラップA2、B2を
投光側及び受光側の光軸から逸れるように配置し、第1
の光トラップA1、B1に導かれた光が第1の光トラッ
プA1、B1の奥の第2の光トラップA2、B2へ進む
ような角度で第1の光トラップA1、B1の内壁を設け
ている。特に、投光軸に沿って入射する光は、投光側第
1の光トラップB1の壁面に反射して投光側第2の光ト
ラップB2に入射されるようになっている。このため、
最も強い光強度を有する投光素子4からの直接の光を、
図7に示すように、略完全に投光側第2の光トラップA
2に誘導できるため、迷光の強度をさらに微弱に抑える
ことが可能になる。同様に、受光軸に沿って受光素子5
入射する光は、投光側第1の光トラップB1及び投光側
第2の光トラップB2で十分に減衰されているので、迷
光の影響をさらに抑えることが可能になる。
In the light scattering type particle detection sensor according to the present embodiment, as shown in FIG. 5, the second light traps A2 and B2 are arranged so as to be deviated from the optical axes on the light projecting side and the light receiving side.
The inner walls of the first optical traps A1 and B1 are provided at an angle such that the light guided to the first optical traps A1 and B1 travels to the second optical traps A2 and B2 behind the first optical traps A1 and B1. I have. In particular, the light incident along the light projecting axis is reflected on the wall surface of the first light trap B1 on the light projecting side and is incident on the second light trap B2 on the light projecting side. For this reason,
The direct light from the light emitting element 4 having the highest light intensity is
As shown in FIG. 7, the second light trap A on the light emitting side is almost completely
2, the intensity of stray light can be further reduced. Similarly, along the light receiving axis, the light receiving element 5
The incident light is sufficiently attenuated by the first light trap B1 on the light projecting side and the second light trap B2 on the light projecting side, so that the influence of stray light can be further suppressed.

【0034】また、投光軸の近傍を通る光が当たる壁に
埃が付着した場合でも、最も強い光強度を有する散乱光
の正反射成分は、投光側第2の光トラップB2へ反射さ
れるため、埃による影響は小さいものとなる。
Even when dust adheres to the wall where light passing near the light projecting axis hits, the specular reflection component of the scattered light having the highest light intensity is reflected to the light projecting side second light trap B2. Therefore, the influence of dust is small.

【0035】本実施の形態によれば、光軸に沿って入射
する強度の強い光は、第2の光トラップA2、B2に導
き、減衰することが可能になる。これにより、迷光の光
強度を低下させ、粒子濃度の高感度測定を行うことが可
能になる。なお、図5に示す光散乱式粒子検知センサで
は、光軸に沿って入射する光が第1の光トラップA1、
B1当たる壁は曲面になっているが、平面であってもよ
い。また、本実施の形態に示すような投受光素子5の配
置の場合、投光側の光軸と受光素子5との間のデッドス
ペースや受光側の光軸と投光素子4との間のデッドスペ
ースに第2の光トラップA2、B2を設けることができ
るので、ケース1を大きくすることなく、広い第2の光
トラップA2、B2を設けることが可能になる。
According to the present embodiment, light of high intensity incident along the optical axis can be guided to the second optical traps A2 and B2 and attenuated. This makes it possible to reduce the light intensity of the stray light and perform a highly sensitive measurement of the particle concentration. In the light scattering type particle detection sensor shown in FIG. 5, light incident along the optical axis is the first light trap A1,
The wall corresponding to B1 is a curved surface, but may be a flat surface. In the case of the arrangement of the light emitting and receiving elements 5 as shown in this embodiment, a dead space between the light emitting side optical axis and the light receiving element 5 and a dead space between the light receiving side optical axis and the light emitting element 4 Since the second optical traps A2 and B2 can be provided in the dead space, it is possible to provide the wide second optical traps A2 and B2 without increasing the size of the case 1.

【0036】なお、図5に示すように、第2の光トラッ
プA2、B2の内壁に複数の溝25を設けるようにして
もよい。本実施の形態の光散乱式粒子検知センサでは、
この溝25の一例として、第2のトラップA2、B2の
内壁に複数の鋭角の三角状の凹凸を設けている。これに
より、第2の光トラップA2、B2内の壁面の面積を増
加させることが可能になり、導かれた光の反射回数をさ
らに増加させることが可能になる。第2の光トラップに
設ける溝25としては、鋭角の三角状の凹凸に限らず、
針先を並べたような鋭角の先端を有する突状の凹凸であ
ってもよく、反射回数を増加させる形状であればよい。
この凹凸は深く鋭い程、反射回数が増加し、迷光の強度
を減衰する効果がある。溝25は、第2の光トラップ内
どこに設けてもよく、特に光軸上の光が数回の反射後、
垂直に近い角度で当たる壁に設けると、反射回数が極端
に増加するため、迷光の強度を減衰する効果が高い。
As shown in FIG. 5, a plurality of grooves 25 may be provided on the inner walls of the second optical traps A2 and B2. In the light scattering type particle detection sensor of the present embodiment,
As an example of the groove 25, a plurality of acute-angled triangular irregularities are provided on the inner walls of the second traps A2 and B2. Thereby, the area of the wall surface in the second optical traps A2 and B2 can be increased, and the number of times of reflection of the guided light can be further increased. The groove 25 provided in the second optical trap is not limited to the acute triangular unevenness.
It may be a projection-like unevenness having an acute-angled tip, such as a stylus of needles, or any shape that increases the number of reflections.
The deeper and sharper the irregularities, the more the number of reflections increases, and has the effect of attenuating the intensity of stray light. The groove 25 may be provided anywhere in the second optical trap, and particularly after light on the optical axis has been reflected several times.
When provided on a wall that strikes at an angle close to vertical, the number of reflections increases extremely, so that the effect of attenuating the intensity of stray light is high.

【0037】[0037]

【発明の効果】以上のように、請求項1記載の発明にあ
っては、それぞれ光軸を交差させる形で光学室内に配置
された投光素子と受光素子とを備え、投光素子の投光領
域と受光素子の受光領域とが重合する領域である検知領
域における煙や粉塵等の粒子による投光素子からの散乱
光を受光素子で受光することにより粒子を検出する光散
乱式粒子検知センサにおいて、開口部より徐々に開口径
が細くなる筒状の第1の光トラップと、第1の光トラッ
プに侵入した光が導かれるように第1の光トラップに連
接し、第1の光トラップとの連接部から開口径が広くな
る第2の光トラップとを光学室内に設けたので、光トラ
ップに迷光を導き減衰させることでS/N比が向上され
るため、さらに一層の高感度化を図ることができる光散
乱式粒子検知センサを提供することができるという効果
を奏する。
As described above, according to the first aspect of the present invention, there are provided a light projecting element and a light receiving element which are arranged in the optical chamber so that the optical axes cross each other. A light-scattering type particle detection sensor that detects particles by receiving light scattered from the light-emitting element due to particles such as smoke and dust in the detection area where the light area and the light-receiving area of the light-receiving element overlap. , A cylindrical first optical trap whose opening diameter gradually becomes smaller than the opening, and a first optical trap connected to the first optical trap so that light entering the first optical trap is guided. Since the second optical trap whose opening diameter is widened from the connecting portion with the second optical trap is provided in the optical chamber, the S / N ratio is improved by guiding and attenuating the stray light to the optical trap, thereby further improving the sensitivity. Light scattering type particle detection sensor An effect that can be provided.

【0038】請求項2記載の発明にあっては、請求項1
記載の光散乱式粒子検知センサにおいて、投光素子及び
受光素子の光軸から逸れるように第2の光トラップの開
口を配置するようにしたので、光軸に沿って入射する強
度の強い光を第2の光トラップで十分減衰することがで
きるという効果を奏する。
According to the second aspect of the present invention, there is provided the first aspect.
In the light scattering type particle detection sensor described above, since the opening of the second optical trap is arranged so as to be deviated from the optical axes of the light projecting element and the light receiving element, strong light incident along the optical axis is emitted. There is an effect that the light can be sufficiently attenuated by the second optical trap.

【0039】請求項3記載の発明にあっては、請求項1
又は請求項2記載の光散乱式粒子検知センサにおいて、
第2の光トラップの内壁に複数の溝を設けたので、第2
の光トラップ内での反射回数を増加させることが可能と
なり、光トラップから洩れる迷光をさらに減少させるこ
とができるという効果を奏する。
In the invention according to claim 3, claim 1 is
Or in the light scattering type particle detection sensor according to claim 2,
Since a plurality of grooves are provided on the inner wall of the second optical trap,
This makes it possible to increase the number of reflections within the optical trap, and to further reduce stray light leaking from the optical trap.

【0040】請求項4記載の発明にあっては、請求項1
乃至請求項3記載の光散乱式粒子検知センサにおいて、
第1の光トラップの開口を投光素子及び受光素子と対向
する位置に設けたので、投光素子に対向して配した光ト
ラップでは投光素子から出る光を確実に減衰することで
迷光の発生を防止することができるとともに、受光素子
に対向して配した光トラップでは従来迷光として受光素
子に入射していた光を大幅に減少することができるとい
う効果を奏する。
According to the fourth aspect of the present invention, there is provided the first aspect.
4. The light scattering type particle detection sensor according to claim 3,
Since the opening of the first optical trap is provided at a position facing the light projecting element and the light receiving element, the light trap arranged opposite to the light projecting element reliably attenuates the light emitted from the light projecting element, thereby reducing stray light. In addition to preventing the occurrence of light, the optical trap disposed opposite to the light receiving element has the effect of greatly reducing the light that has conventionally entered the light receiving element as stray light.

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

【図1】本発明に係る第1の実施の形態の光散乱式粒子
検知センサの縦断面図である。
FIG. 1 is a longitudinal sectional view of a light scattering type particle detection sensor according to a first embodiment of the present invention.

【図2】本発明に係る第1の実施の形態の光散乱式粒子
検知センサの分解斜視図である。
FIG. 2 is an exploded perspective view of the light scattering type particle detection sensor according to the first embodiment of the present invention.

【図3】光散乱式粒子検知センサ内を進行する光の様子
を示す縦断面図である。
FIG. 3 is a longitudinal sectional view showing a state of light traveling in a light scattering type particle detection sensor.

【図4】入射した光が反射する様子を示す模式図であ
る。
FIG. 4 is a schematic diagram showing how incident light is reflected.

【図5】本発明に係る第2の実施の形態の光散乱式粒子
検知センサの縦断面図である。
FIG. 5 is a longitudinal sectional view of a light scattering type particle detection sensor according to a second embodiment of the present invention.

【図6】本発明に係る第2の実施の形態の光散乱式粒子
検知センサの分解斜視図である。
FIG. 6 is an exploded perspective view of a light scattering type particle detection sensor according to a second embodiment of the present invention.

【図7】光散乱式粒子検知センサ内を進行する光の様子
を示す縦断面図である。
FIG. 7 is a longitudinal sectional view showing a state of light traveling inside the light scattering type particle detection sensor.

【図8】従来の光散乱式粒子検知センサの縦断面図であ
る。
FIG. 8 is a longitudinal sectional view of a conventional light scattering type particle detection sensor.

【図9】従来の他の光散乱式粒子検知センサの縦断面図
である。
FIG. 9 is a longitudinal sectional view of another conventional light scattering type particle detection sensor.

【図10】入射した光が反射する様子を示す模式図であ
る。
FIG. 10 is a schematic diagram showing how incident light is reflected.

【符号の説明】[Explanation of symbols]

1 ケース 2 光学室 4 投光素子 5 受光素子 A1 受光側第1の光トラップ A2 受光側第2の光トラップ B1 投光側第1の光トラップ B2 投光側第2の光トラップ イ 検知領域 DESCRIPTION OF SYMBOLS 1 Case 2 Optical room 4 Light emitting element 5 Light receiving element A1 First light trap on the light receiving side A2 Second light trap on the light receiving side B1 First light trap on the light emitting side B2 Second light trap on the light emitting side i Detection area

───────────────────────────────────────────────────── フロントページの続き (72)発明者 阿部 豊 大阪府門真市大字門真1048番地松下電工株 式会社内 ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Yutaka Abe 1048 Odakadoma, Kadoma City, Osaka Prefecture Matsushita Electric Works, Ltd.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 それぞれ光軸を交差させる形で光学室内
に配置された投光素子と受光素子とを備え、投光素子の
投光領域と受光素子の受光領域とが重合する領域である
検知領域における煙や粉塵等の粒子による投光素子から
の散乱光を受光素子で受光することにより粒子を検出す
る光散乱式粒子検知センサにおいて、開口部より徐々に
開口径が細くなる筒状の第1の光トラップと、第1の光
トラップに侵入した光が導かれるように第1の光トラッ
プに連接し、第1の光トラップとの連接部から開口径が
広くなる第2の光トラップとを光学室内に設けたことを
特徴とする光散乱式粒子検知センサ。
1. A detection device comprising: a light projecting element and a light receiving element arranged in an optical chamber so as to intersect an optical axis, wherein a light projecting area of the light projecting element and a light receiving area of the light receiving element overlap. In a light scattering type particle detection sensor which detects particles by receiving light scattered from a light emitting element due to particles such as smoke and dust in an area by a light receiving element, a cylindrical second shape having an opening diameter gradually narrower than an opening. A first optical trap and a second optical trap that is connected to the first optical trap so that light that has entered the first optical trap is guided, and that has a larger opening diameter from a connection with the first optical trap. Provided in an optical chamber.
【請求項2】 投光素子及び受光素子の光軸から逸れる
ように第2の光トラップの開口を配置するようにしたこ
とを特徴とする請求項1記載の光散乱式粒子検知セン
サ。
2. The light scattering type particle detection sensor according to claim 1, wherein the opening of the second optical trap is arranged so as to be deviated from the optical axes of the light projecting element and the light receiving element.
【請求項3】 第2の光トラップの内壁に複数の溝を設
けたことを特徴とする請求項1又は請求項2記載の光散
乱式粒子検知センサ。
3. The light scattering type particle detection sensor according to claim 1, wherein a plurality of grooves are provided on an inner wall of the second optical trap.
【請求項4】 第1の光トラップの開口を投光素子及び
受光素子と対向する位置に設けたことを特徴とする請求
項1乃至請求項3記載の光散乱式粒子検知センサ。
4. The light scattering type particle detection sensor according to claim 1, wherein an opening of the first optical trap is provided at a position facing the light emitting element and the light receiving element.
JP4648998A 1998-02-27 1998-02-27 Light scattering type particle detecting sensor Pending JPH11248628A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4648998A JPH11248628A (en) 1998-02-27 1998-02-27 Light scattering type particle detecting sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4648998A JPH11248628A (en) 1998-02-27 1998-02-27 Light scattering type particle detecting sensor

Publications (1)

Publication Number Publication Date
JPH11248628A true JPH11248628A (en) 1999-09-17

Family

ID=12748637

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4648998A Pending JPH11248628A (en) 1998-02-27 1998-02-27 Light scattering type particle detecting sensor

Country Status (1)

Country Link
JP (1) JPH11248628A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005309735A (en) * 2004-04-21 2005-11-04 Nittan Co Ltd Smoke detector
JP2007024545A (en) * 2005-07-12 2007-02-01 Denso Corp Optical gas sensor unit
JP2008287382A (en) * 2007-05-16 2008-11-27 Hochiki Corp Fire alarm
JP2009237720A (en) * 2008-03-26 2009-10-15 Nohmi Bosai Ltd Photoelectric smoke sensor
JP2016008933A (en) * 2014-06-26 2016-01-18 パナソニックIpマネジメント株式会社 Fine particle detection device
US10119908B2 (en) 2015-12-21 2018-11-06 Panasonic Intellectual Property Management Co., Ltd. Particle sensor
WO2020249803A1 (en) * 2019-06-12 2020-12-17 Ams Ag Particulate matter sensor

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005309735A (en) * 2004-04-21 2005-11-04 Nittan Co Ltd Smoke detector
US7248173B2 (en) 2004-04-21 2007-07-24 Nittan Company, Limited Smoke detector
JP4652716B2 (en) * 2004-04-21 2011-03-16 ニッタン株式会社 smoke detector
DE102005018559B4 (en) * 2004-04-21 2017-07-27 Nittan Company Ltd. smoke detector
JP2007024545A (en) * 2005-07-12 2007-02-01 Denso Corp Optical gas sensor unit
JP2008287382A (en) * 2007-05-16 2008-11-27 Hochiki Corp Fire alarm
JP2009237720A (en) * 2008-03-26 2009-10-15 Nohmi Bosai Ltd Photoelectric smoke sensor
JP2016008933A (en) * 2014-06-26 2016-01-18 パナソニックIpマネジメント株式会社 Fine particle detection device
US10119908B2 (en) 2015-12-21 2018-11-06 Panasonic Intellectual Property Management Co., Ltd. Particle sensor
WO2020249803A1 (en) * 2019-06-12 2020-12-17 Ams Ag Particulate matter sensor
CN113939726A (en) * 2019-06-12 2022-01-14 ams有限公司 Particulate matter sensor

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