JPS63134986A - Person number detector - Google Patents

Person number detector

Info

Publication number
JPS63134986A
JPS63134986A JP61281303A JP28130386A JPS63134986A JP S63134986 A JPS63134986 A JP S63134986A JP 61281303 A JP61281303 A JP 61281303A JP 28130386 A JP28130386 A JP 28130386A JP S63134986 A JPS63134986 A JP S63134986A
Authority
JP
Japan
Prior art keywords
mirror
people
visual field
end point
infrared
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP61281303A
Other languages
Japanese (ja)
Other versions
JPH0644045B2 (en
Inventor
Shinji Kirihata
慎司 桐畑
Tsunehiko Araki
恒彦 荒木
Aritaka Yorifuji
依藤 有貴
Takashi Horii
堀井 貴司
Hiroshi Matsuda
啓史 松田
Hidekazu Himezawa
秀和 姫澤
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 JP61281303A priority Critical patent/JPH0644045B2/en
Publication of JPS63134986A publication Critical patent/JPS63134986A/en
Publication of JPH0644045B2 publication Critical patent/JPH0644045B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To obtain a uniform sensitivity distribution over a wide detection area by providing a first mirror for scanning circularly a visual field of an infrared ray detecting element, and a second mirror for reflecting again infrared rays reflected by the first mirror, and making it incident on the infrared ray detecting element. CONSTITUTION:It is supposed that the photodetecting surface S of an infrared ray detecting element is placed in parallel to the floor surface, and the visual field center (c) of the photodetecting surface S is vertical to the horizontal plane. In a radial direction end part of an instantaneous visual field, incident light B1 is made incident on the photodetecting surface S through an end point M3 of a mirror MB, and an end point M1 of a mirror MA, and incident light B2 is made incident on the photodetecting surface S through an end point M4 of the mirror MB, and an end point M2 of the mirror MA. In a directional sensitivity characteristic of the infrared ray detecting element 2, when an angle made by the incident light when the sensitivity becomes zero, and the visual field center (c) of the photodetecting surface is denoted as alphamax, an angle 2theta of the instantaneous visual field in which the photodetecting surface S views an object surface can be taken up to the maximum 2alphamax.

Description

【発明の詳細な説明】 (技術分野) 本発明は、被検知人体から発せられる赤外線を検出して
人数を検出する赤外線受光式の人数検出装置に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to an infrared receiving type people detection device that detects the number of people by detecting infrared rays emitted from a detected human body.

(背景技術) 本発明者らは、簡単且つ安価な構成で広い検知領域を有
する高精度の人数検出装置を既に提案している。第4図
にその構成図を示す。この人数検出装置は、赤外線検出
素子2と、前記赤外線検出素子2の視野を円形走査させ
る円形走査光学系1と、前記赤外線検出素子2の出力信
号を増幅する前置増幅部3と、前記前置増幅部3の出力
信号を人数検出に必要な信号に変換する信号処理部4と
、前記信号処理部4の出力信号に基づいて人数を判定す
る判断部5と、前記判断部5の出力信号から人数情報を
出力する出力部6とから成り、広い検知領域内の人数を
高精度に検出できるようにしたものである。
(Background Art) The present inventors have already proposed a highly accurate number of people detection device that has a simple and inexpensive configuration and a wide detection area. Figure 4 shows its configuration. This number of people detection device includes an infrared detection element 2, a circular scanning optical system 1 that circularly scans the field of view of the infrared detection element 2, a preamplifier 3 that amplifies the output signal of the infrared detection element 2, and a preamplifier 3 that amplifies the output signal of the infrared detection element 2. a signal processing section 4 that converts the output signal of the amplifier section 3 into a signal necessary for detecting the number of people; a determining section 5 that determines the number of people based on the output signal of the signal processing section 4; and an output signal of the determining section 5. and an output section 6 that outputs information on the number of people, and is capable of detecting the number of people within a wide detection area with high precision.

第5図に円形走査光学系の一例を示す、同図(a)に示
すように、赤外線検出素子2の受光面前面より距離Rb
の位置に回転板10を配置し、回転板10中夫の回転軸
11を赤外線検出素子2の受光面の視野中心C上に配置
し、回転板10をモータ等の駆動機構により回転させる
。第5図(b)に示すように、回転板lOに長さLa、
幅Daの長方形状のスリットAを設け、物面Bから輻射
された赤外線のうちスリットAを通過したもののみが、
赤外線検出素子2に入射するように構成する。物面上に
おける瞬時視野は、スリットAの形状と相似であり、回
転板10から物面Bまでの距離をRaとすると、物面上
の瞬時視野長Lv、及び視野幅DVは、次式のようにな
る。
An example of a circular scanning optical system is shown in FIG. 5. As shown in FIG.
The rotary plate 10 is placed at a position, the rotating shaft 11 of the rotary plate 10 is placed on the field of view center C of the light-receiving surface of the infrared detection element 2, and the rotary plate 10 is rotated by a drive mechanism such as a motor. As shown in FIG. 5(b), the rotary plate lO has a length La,
A rectangular slit A with a width Da is provided, and only the infrared rays radiated from the object surface B that pass through the slit A are
The configuration is such that the infrared rays are incident on the infrared detection element 2. The instantaneous visual field on the object plane is similar to the shape of the slit A, and if the distance from the rotary plate 10 to the object plane B is Ra, then the instantaneous visual field length Lv and visual field width DV on the object plane are expressed by the following equation. It becomes like this.

Rb+Ra Lv=□・La      ・・・(1)Rb Rb + Ra Dv=□・Da      ・・・(2)Rb また、円形走査における放射方向において、瞬時視野が
物面Bを見込む視野角をθとすると、θは次式のように
なる。
Rb+Ra Lv=□・La...(1)Rb Rb+Ra Dv=□・Da...(2)Rb Also, in the radial direction in circular scanning, the viewing angle at which the instantaneous visual field looks at the object surface B is θ. Then, θ becomes as shown in the following equation.

Ra θ=jan−’□        ・・・(3)Rb 上記の瞬時視野が赤外線検出素子2の受光面の視野中心
Cを軸として円形走査され、したがって、円形走査方式
による物面Bを見込む全視野角は2θとなる。
Ra θ=jan-'□ ... (3) Rb The above instantaneous field of view is circularly scanned around the field center C of the light-receiving surface of the infrared detection element 2, and therefore the entire field of view looking into the object surface B by the circular scanning method. The angle is 2θ.

人数検出に当たり、物面上の瞬時視野幅Dvが人数分解
能を決定する主要因となり、人数分解能を上げるために
は、瞬時視野幅Dvは小さい方が良い。従って、スリッ
トAの開口幅Daを小さくする必要があるが、赤外線受
光量がこれに比例して小さくなり、充分なS/N比を得
られない場合が生じる。その場合には、スリットAの部
分に凸面シリンドリカルレンズを配置し、走査方向にお
いて集光作用を持たせ、所定の瞬時視野幅Dvを得ると
共に、必要な光学利得を得るようにする。
In detecting the number of people, the instantaneous visual field width Dv on the object plane is the main factor determining the number of people resolution, and in order to increase the number of people resolution, the smaller the instantaneous visual field width Dv is, the better. Therefore, although it is necessary to reduce the opening width Da of the slit A, the amount of infrared light received decreases proportionally, and a sufficient S/N ratio may not be obtained. In that case, a convex cylindrical lens is placed in the slit A to have a condensing effect in the scanning direction to obtain a predetermined instantaneous field of view width Dv and a necessary optical gain.

第5図において、スリットAの部分にシリンドリカルレ
ンズを配した場合、赤外線検出素子2の受光面の直径を
dとすると、物面上の瞬時視野の視野共Lv、視野幅D
vは次式のようになる。
In Fig. 5, when a cylindrical lens is placed in the slit A, and the diameter of the light-receiving surface of the infrared detection element 2 is d, the field of view of the instantaneous field of view on the object surface is Lv, and the field width is D.
v is as shown in the following equation.

Rb + Ra LV=□・La      ・・・(4)h Ra Dv=□・d        ・・・(5)Rb 上式から分かるように、瞬時視野幅Dvは、シリンドリ
カルレンズの開口幅Daによらず、適当なRb、あるい
はdを選択して所定の瞬時視野幅DVを得ることができ
る。また、シリンドリカルレンズの開口幅Daを大きく
することにより光学利得を増大させることができる。
Rb + Ra LV=□・La...(4)h Ra Dv=□・d...(5)Rb As can be seen from the above equation, the instantaneous visual field width Dv is independent of the aperture width Da of the cylindrical lens. , Rb, or d can be selected to obtain a predetermined instantaneous visual field width DV. Furthermore, the optical gain can be increased by increasing the aperture width Da of the cylindrical lens.

また、光学利得を得るための他の手段として、第6図に
示すように、凹面シリンドリカルミラーMを固定した回
転板10を赤外線検出素子2の受光面の視野中心Cを軸
として回転させるように構成しても良い、シリンドリカ
ルミラーMのミラー面から赤外線検出素子2の受光面ま
での距離をRb、シリンドリカルミラーMのミラー面か
ら物面Bまでの距離を−Ra、シリンドリカルミラーM
のミラー長をL+*、ミラー幅をD+s、赤外線検出素
子2の受光面直径をdとすると、物面上の瞬時視野長L
v、及び視野幅Dvは、シリンドリカルレンズを用いた
場合と同様に次式のようになる。
Further, as another means for obtaining optical gain, as shown in FIG. 6, a rotary plate 10 to which a concave cylindrical mirror M is fixed is rotated about the center of field of view C of the light-receiving surface of the infrared detection element 2. The distance from the mirror surface of the cylindrical mirror M to the light receiving surface of the infrared detection element 2 may be Rb, the distance from the mirror surface of the cylindrical mirror M to the object surface B may be -Ra, and the cylindrical mirror M
When the mirror length of is L+*, the mirror width is D+s, and the diameter of the light-receiving surface of the infrared detection element 2 is d, the instantaneous field of view length L on the object surface is
v and the visual field width Dv are expressed by the following equations as in the case of using a cylindrical lens.

Rb + Ra L、v=□・ L−・・・(6) Rb Ra Dv=□・d        ・・・(7)h したがって、適当なRb、あるいはdを選択することに
より、所定の瞬時視野幅Dvを得ることができ、シリン
ドリカルミラーMのミラー幅り一を大きくすることによ
り光学利得を増大させることができる0円形走査におけ
る放射方向において、瞬時視野が物面Bを見込む視野角
θは、実施例1の場合と同様にして次式のようになる。
Rb + Ra L, v=□・L−...(6) Rb Ra Dv=□・d...(7)h Therefore, by selecting an appropriate Rb or d, a predetermined instantaneous visual field width can be obtained. Dv can be obtained and the optical gain can be increased by increasing the mirror width of the cylindrical mirror M. In the radial direction in 0 circular scanning, the viewing angle θ at which the instantaneous field of view looks at the object surface B is determined by Similarly to Example 1, the following equation is obtained.

L− θ==tan−J□・・・(8) Rb また、円形走査方式による物面Bを見込む全視野角は2
θとなる。
L- θ==tan-J
becomes θ.

広い検知領域を得るためには、円形走査方式において、
物面Bを見込む全視野角を大きく取る必要があり、その
ためには、瞬時における受光面が物面Bを見込む角度θ
を大きく取る必要がある。
In order to obtain a wide detection area, in the circular scanning method,
It is necessary to take a large total viewing angle when looking at object surface B, and to do so, the angle θ at which the light-receiving surface looks at object surface B at an instant must be increased.
It is necessary to take a large value.

(3)、(8)式よりθを大きくするためには、スリッ
ト長あるいはシリンドリカルレンズのレンズ長であるL
m、または、シリンドリカルミラーMのミラー長Lmを
大きく取れば良い6しかしながら、赤外線検出素子2の
入射光に対する指向感度特性上、入射光と受光面視野中
心Cのなす角度が大きくなるにつれて、感度は低下し、
ある角度αmax以上では、感度は零となる。赤外線検
出素子2として用いられる焦電素子の指向感度特性の一
例を第7図に示す、この図から明らかなように、円形走
査光学系において、物面上を見込む全視野角は赤外線検
出素子2の指向感度特性により制限を受け、十分広く取
れず、さらには、視野面において、周辺部はど感度が低
下し検知領域内で感度の不均一性を生じるという問題点
があった。
From equations (3) and (8), in order to increase θ, the slit length or the lens length of the cylindrical lens L
m, or the mirror length Lm of the cylindrical mirror M may be increased.6However, due to the directional sensitivity characteristics of the infrared detection element 2 to the incident light, as the angle between the incident light and the center of field of view of the light-receiving surface C increases, the sensitivity decreases. decreases,
Above a certain angle αmax, the sensitivity becomes zero. An example of the directional sensitivity characteristics of the pyroelectric element used as the infrared detecting element 2 is shown in Fig. 7.As is clear from this figure, in the circular scanning optical system, the total viewing angle looking onto the object surface is the same as that of the infrared detecting element 2. It is limited by the directional sensitivity characteristics of the sensor, and cannot be made sufficiently wide.Furthermore, in the field of view, the sensitivity in the peripheral area decreases, resulting in non-uniformity in sensitivity within the detection area.

(発明の目的) 本発明は上述のような点に鑑みてなされたものであり、
その目的とするところは、簡単且つ安価な構成で、広い
検知領域に亘って均一な感度分布を有する人数検出装置
を提供するにある。
(Object of the invention) The present invention has been made in view of the above points, and
The purpose is to provide a number of people detection device that has a simple and inexpensive configuration and has a uniform sensitivity distribution over a wide detection area.

(発明の開示) 第1図は本発明に係る人数検出装置に用いられる2枚の
反射鏡MA+MBを用いた円形走査光学系を側面から見
たときの概略構成図であり、赤外線゛   検出素子2
の受光面Sは、水平面すなわち床面に平行に配置し、受
光面Sの視野中心Cは水平面に垂直であるとする。瞬時
視野の放射方向端部において、入射光B、はミラーM、
の端点M1、ミラーMAの端点M、を介して、受光面S
に入射し、入射光B2はミラーMBの端点M1、ミラー
MAの端点M2を介して受光面Sに入射する。入射光B
、は水平面から垂直にミラーM、に入射するものとする
と、入射光B2が受光面Sの視野中心C1すなわちミラ
ーMA、MBの回転軸となす角が本発明の円形走査光学
系において、受光面Sが物面を見込む瞬時視野角となる
。ミラーMAにより、受光面Sの有効視野角が決定され
、視野中心Cから各々角度θの有効視野角を持つように
受光面Sの下に配置する。
(Disclosure of the Invention) Fig. 1 is a schematic configuration diagram when viewed from the side of a circular scanning optical system using two reflecting mirrors MA+MB used in the number of people detection device according to the present invention.
The light-receiving surface S of is arranged parallel to a horizontal plane, that is, the floor surface, and the field of view center C of the light-receiving surface S is perpendicular to the horizontal surface. At the radial end of the instantaneous field of view, the incident light B is reflected by the mirror M,
through the end point M1 of the mirror MA and the end point M of the mirror MA.
The incident light B2 enters the light receiving surface S via the end point M1 of the mirror MB and the end point M2 of the mirror MA. Incident light B
, is incident on the mirror M perpendicularly from the horizontal plane, then the angle that the incident light B2 makes with the field of view center C1 of the light-receiving surface S, that is, the rotation axis of the mirrors MA and MB, is the angle that the incident light B2 makes with the light-receiving surface in the circular scanning optical system of the present invention. S is the instantaneous viewing angle looking into the object surface. The effective viewing angle of the light-receiving surface S is determined by the mirrors MA, and the mirrors are arranged below the light-receiving surface S so that each mirror has an effective viewing angle of an angle θ from the viewing center C.

このとき入射光B2が受光面Sの視野中心となす角は2
θとなり、受光面Sが物面を見込む瞬時視野角は2θと
なる。入射光B2がミラーMBの端点M4により反射さ
れ、ミラーMAの端点M2に入射する際の光路が水平面
に平行であるとすると、ミラーMA、ミラーMBが水平
面となす角α、βは次式%式% 赤外線検出素子2の指向感度特性において、感度が零と
なる場きの入射光と受光面視野中心Cとのなす角をαw
axとすると、前記光学系により受光面Sが物面を見込
む瞬時視野の角度2θは最大2αwaxまで取ることが
可能である。また、赤外線検出素子2の指向感度特性に
おいて、比較的指向感度特性が均一な範囲を用いること
により、比較的均一な感度分布を有する広い検知領域を
得ることができる。
At this time, the angle that the incident light B2 makes with the visual field center of the light receiving surface S is 2
θ, and the instantaneous viewing angle at which the light-receiving surface S looks at the object surface is 2θ. Assuming that the incident light B2 is reflected by the end point M4 of the mirror MB and the optical path when it enters the end point M2 of the mirror MA is parallel to the horizontal plane, the angles α and β made by the mirror MA and the mirror MB with the horizontal plane are expressed by the following formula % Formula % In the directional sensitivity characteristic of the infrared detection element 2, the angle between the incident light and the center of field of view of the light-receiving surface C when the sensitivity becomes zero is αw
ax, the angle 2θ of the instantaneous field of view at which the light-receiving surface S looks at the object surface by the optical system can be up to 2αwax. Furthermore, by using a range in which the directional sensitivity characteristics of the infrared detection element 2 are relatively uniform, a wide detection area having a relatively uniform sensitivity distribution can be obtained.

円形走査光学系において、人体分解能を向上させるには
、瞬時視野幅を小さくする必要があるが、ミラーMAを
凹面シリンドリカルミラーとすると、焦点距離を大きく
取るためには、円形走査光学系が大きくなってしまうの
で、ミラーMAは平面鏡とし、ミラーM、を凹面シリン
ドリカルミラーとする。凹面シリンドリカルミラーを用
いることにより、走査方向について集光作用を得ること
ができ計 この円形走査光学系は等値的に第2図に示すようになり
、第2図において、等価受光面をS”とし、等価受光面
S′からミラーM日までの距離をRb、ミラーMBから
ピントの合った面までの距離をRa、ミラーMBの焦点
距離をfとすると、の関係があり、ピントの合った面は
、ミラーM日の面と平行となり、水平面とは角度βをな
す。
In a circular scanning optical system, in order to improve human body resolution, it is necessary to reduce the instantaneous field of view width, but if mirror MA is a concave cylindrical mirror, in order to increase the focal length, the circular scanning optical system must become larger. Therefore, mirror MA is a plane mirror, and mirror M is a concave cylindrical mirror. By using a concave cylindrical mirror, a condensing effect can be obtained in the scanning direction. This circular scanning optical system is equivalently shown in Fig. 2, and in Fig. 2, the equivalent light-receiving surface is S'' If the distance from the equivalent light-receiving surface S' to mirror M is Rb, the distance from mirror MB to the in-focus surface is Ra, and the focal length of mirror MB is f, then there is the following relationship. The surface is parallel to the surface of the mirror M and makes an angle β with the horizontal plane.

前記光学系による集光状況は第3図に示すようになる。The light condensing situation by the optical system is shown in FIG.

凹面シリンドリカルミラーMBの幅をLとし、平面ミラ
ーMAにおいて、凹面シリンドリカルミラーMAの端点
M、を介して集光する光線束の平面ミラーMA上での幅
を!3、凹型シリンドリカルミラーM、の端点M、を介
して集光する光線束の平面ミラーMB上での幅12とす
ると、となる0本実施例では、・L<12であり、した
がって一平面ミラーMAは一ルなぐとi、B1.ff言
L長さM、M2であるような長方形であれば良い。
Let the width of the concave cylindrical mirror MB be L, and the width on the plane mirror MA of the beam of light condensed via the end point M of the concave cylindrical mirror MA! 3. If the width of the ray bundle condensed through the end point M of the concave cylindrical mirror M on the plane mirror MB is 12, then 0 In this example, L<12, so it is a single plane mirror. MA is 1 Ru Naguto i, B1. It suffices if it is a rectangle with length M and length M2.

ここで、前記光学系を用いる人数検出装置の回路構成を
第4図に基づいて説明する。赤外線検出素子2の出力は
前置増幅部3で増幅された後、信号処理部4内の帯域フ
ィルターに入力され、不安定な低周波成分と不必要な高
周波成分とをカットし、S/N比を向上させる。帯域フ
ィルターの出力はA/D変換されて5判断部5を構成す
るマイクロコンピュータに出力される。このマイクロコ
ンピュータは円形走査光学系1の回転に同期して1回転
毎にA/D変換された波形を逐次取り込む。
Here, the circuit configuration of the number of people detection device using the optical system will be explained based on FIG. 4. The output of the infrared detection element 2 is amplified by the preamplifier 3 and then input to the bandpass filter in the signal processing unit 4, which cuts unstable low frequency components and unnecessary high frequency components, and improves the S/N. improve the ratio. The output of the bandpass filter is A/D converted and output to the microcomputer forming the judgment section 5. This microcomputer sequentially captures A/D converted waveforms every rotation in synchronization with the rotation of the circular scanning optical system 1.

判断部5においては、予め検知領域内に人体が存在しな
い渇きの出力波形が参照波形データとしてメモリー内に
記憶されており、入力波形は、メモリー内の参照波形と
比較され、人体の有無及び人数が同時に判断される。本
実施例では、入力波形データと参照波形データとで比較
演算3行い、その結果を新たに比較処理波形データとし
、比較処理波形データにおいて、極大値を検出し、極大
値の数を人数としてカウントしている。比較処理波形デ
ータにおいて、検出人数が0の場合には、現在の入力波
形データが雪照波形データとして更新され、メモリー内
に記憶される。このように参照波形データを用いて入力
波形データと比較演算を行うことにより、検知領域内の
環境変化に左右されることなく、高精度な人数検出を行
うことができる。出力部6においては、判断部5から与
えられた人数情報を元に、人数情報を表示するようにな
っている。会議室などでは、室外に人数あるいは混雑度
を表示することにより、室外で他者が室内使用状況を把
握できるようにする。また、個人が使用している部屋に
おいては、人数情報「0人」。
In the judgment unit 5, the output waveform of thirst in which no human body is present in the detection area is stored in memory as reference waveform data, and the input waveform is compared with the reference waveform in the memory to determine the presence or absence of a human body and the number of people. are judged at the same time. In this example, three comparison operations are performed between input waveform data and reference waveform data, the results are used as new comparison processing waveform data, local maximum values are detected in the comparison processing waveform data, and the number of local maximum values is counted as the number of people. are doing. In the comparison processing waveform data, if the detected number of people is 0, the current input waveform data is updated as snowy weather waveform data and stored in the memory. By performing comparison calculations with the input waveform data using the reference waveform data in this way, it is possible to detect the number of people with high precision without being affected by environmental changes within the detection area. The output section 6 displays the number of people information based on the number of people information given from the judgment section 5. In a conference room, etc., the number of people or the degree of congestion is displayed outside the room so that others can grasp the usage status of the room. In addition, in rooms used by individuals, the number of people information is "0 people".

「1人」、「2Å以上」を元に、室内状況を“不在パ、
“在室”、“来客”として室外に表示することにより、
他者が容易かつ端的に室内状況を把握することができる
。さらに、人数情報を元に、空調など各種環境施設を安
定且つ有効に動作させることができる。
Based on “one person” and “more than 2Å”, the indoor situation is determined as “absent person”.
By displaying outside the room as “in room” or “visitor”,
Others can easily and simply understand the indoor situation. Furthermore, various environmental facilities such as air conditioning can be operated stably and effectively based on the information on the number of people.

(発明の効果) 本発明は上述のように、被検知人体から発せられる赤外
線を検出して人数を検出する赤外線受光式の人数検出装
置において、赤外線検出素子の視野を円形走査させる第
1のミラーと、第1のミラーにて反射された赤外線を再
度反射して赤外線検出素子に入射させる第2のミラーと
を設けたから、赤外線検出素子の指向感度特性を有効に
利用することができて、広い検知領域に亘って均一な悠
度分布を得ることができ、しかも簡単且つ安価に構成で
きるという効果がある。
(Effects of the Invention) As described above, the present invention provides an infrared receiving type people detection device that detects the number of people by detecting infrared rays emitted from a human body to be detected. and a second mirror that re-reflects the infrared rays reflected by the first mirror and makes them enter the infrared detecting element, the directional sensitivity characteristics of the infrared detecting element can be effectively used, and a wide range of This has the advantage that a uniform latitude distribution can be obtained over the detection area, and that it can be constructed simply and at low cost.

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

第1図は本発明に係る人数検出装置に用いる光学系の概
略構成図、第2図及び第3図は同上の光学系の動作説明
図、第4図は従来例のブロック図、第5図(a)は従来
例に用いる光学系の概略構成図、同図(b)は同上の要
部底面図、第6図(a)は他の従来例に用いる光学系の
概略構成図、同図(b)は同上の要部底面図、第7図は
同上に用いる赤外線検出素子の指向特性図である。 1は円形走査を学築 2け赤外モ檜出嚢子 3は前置増
幅部、4は信号処理能、5は判断部、6は出力部、MA
、M、はミラーである。
Fig. 1 is a schematic configuration diagram of an optical system used in the people detection device according to the present invention, Figs. 2 and 3 are explanatory diagrams of the operation of the same optical system, Fig. 4 is a block diagram of a conventional example, and Fig. 5 (a) is a schematic configuration diagram of the optical system used in the conventional example, FIG. 6 (b) is a bottom view of the main parts of the same as above, and FIG. (b) is a bottom view of the essential parts of the same as above, and FIG. 7 is a directivity characteristic diagram of the infrared detecting element used in the above. 1 is a circular scanning system, 2 is an infrared camera, 3 is a preamplifier, 4 is a signal processing function, 5 is a judgment unit, 6 is an output unit, MA
,M, is a mirror.

Claims (1)

【特許請求の範囲】[Claims] (1)赤外線検出素子と、前記赤外線検出素子の視野を
走査させる走査光学系と、前記赤外線検出素子の出力信
号を増幅する前置増幅部と、前記前置増幅部の出力信号
を人数検出に必要な信号に変換する信号処理部と、前記
信号処理部の出力信号に基づいて人数を判定する判断部
と、前記判断部の出力信号から人数情報を出力する出力
部とから成る人数検出装置において、前記走査光学系は
前記赤外線検出素子の視野を円形走査させる第1のミラ
ーと、第1のミラーにて反射された赤外線を再度反射し
て赤外線検出素子に入射させる第2のミラーとを備えて
成ることを特徴とする人数検出装置。
(1) An infrared detection element, a scanning optical system that scans the field of view of the infrared detection element, a preamplification section that amplifies the output signal of the infrared detection element, and an output signal of the preamplification section that is used to detect the number of people. A number of people detection device comprising a signal processing section that converts into a necessary signal, a determining section that determines the number of people based on an output signal of the signal processing section, and an output section that outputs number of people information from the output signal of the determining section. , the scanning optical system includes a first mirror that circularly scans the field of view of the infrared detection element, and a second mirror that reflects the infrared rays reflected by the first mirror again and makes them enter the infrared detection element. A number of people detection device characterized by comprising:
JP61281303A 1986-11-26 1986-11-26 People detection device Expired - Fee Related JPH0644045B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61281303A JPH0644045B2 (en) 1986-11-26 1986-11-26 People detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61281303A JPH0644045B2 (en) 1986-11-26 1986-11-26 People detection device

Publications (2)

Publication Number Publication Date
JPS63134986A true JPS63134986A (en) 1988-06-07
JPH0644045B2 JPH0644045B2 (en) 1994-06-08

Family

ID=17637194

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61281303A Expired - Fee Related JPH0644045B2 (en) 1986-11-26 1986-11-26 People detection device

Country Status (1)

Country Link
JP (1) JPH0644045B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60127578U (en) * 1984-02-06 1985-08-27 フジテツク株式会社 Crowd level detection device
JPS61151490A (en) * 1984-12-25 1986-07-10 Agency Of Ind Science & Technol Apparatus for detecting matter

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60127578U (en) * 1984-02-06 1985-08-27 フジテツク株式会社 Crowd level detection device
JPS61151490A (en) * 1984-12-25 1986-07-10 Agency Of Ind Science & Technol Apparatus for detecting matter

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JPH0644045B2 (en) 1994-06-08

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