JPS63134983A - Person number detector - Google Patents

Person number detector

Info

Publication number
JPS63134983A
JPS63134983A JP61281304A JP28130486A JPS63134983A JP S63134983 A JPS63134983 A JP S63134983A JP 61281304 A JP61281304 A JP 61281304A JP 28130486 A JP28130486 A JP 28130486A JP S63134983 A JPS63134983 A JP S63134983A
Authority
JP
Japan
Prior art keywords
people
slit
distance
detection element
view
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
JP61281304A
Other languages
Japanese (ja)
Inventor
Hiroshi Matsuda
啓史 松田
Tsunehiko Araki
恒彦 荒木
Aritaka Yorifuji
依藤 有貴
Takashi Horii
堀井 貴司
Shinji Kirihata
慎司 桐畑
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 JP61281304A priority Critical patent/JPS63134983A/en
Publication of JPS63134983A publication Critical patent/JPS63134983A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce a photodetecting sensitivity difference in infrared rays due to a distance, and to reduce a level difference in a human body detecting signal due to the distance, by rotating a visual field surface formed by a slit whose opening width is widened as it is placed away from the rotation center. CONSTITUTION:A circular scanning optical system 1 is provided with a slit X whose opening width is widened as it is placed away from the rotation center, and by rotating a visual field surface formed by this slit X, a visual field of an infrared ray detecting element 2 is scanned circularly. When this slit X is placed in front of a cylindrical mirror M, as for a level of a signal obtained by the infrared ray detecting element 2, the level becomes low in the near part, and the level becomes high in the distant part. In such a way, a photodetecting sensitivity difference in infrared rays due to the distance in a detection area can be reduced, and the number of persons can be measured exactly.

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7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の出力信号がら人数情報を
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. FIG. 7 shows its configuration diagram. 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. The output section 6 outputs information on the number of people in a wide range of detection areas, making it possible to detect the number of people within a wide detection area with high precision.

まず、円形走査方式について説明する。検知対象である
人体を上方から見た場合、第9図に示すようになる。こ
れは、第8図(a)に示す高さ170cm、幅50c−
1奥行き20CTIの直方体を直立した人体のモデルと
して、第8図(b)(c)に示すように、1辺が3mの
正方形の頂点に人体モデル’m、i〜TL4を4体配置
し、床面Uから上方3mの点において床面Uに平行な面
に投影した人体モデル机1〜TrL4による2次元像で
ある。図から明らかなように、上方から見た人体像は、
視野中心Cに配置した場合を除いて、人体の側面も見込
むことになり、視野中心Cから放射方向に伸びた像とな
る。
First, the circular scanning method will be explained. When the human body to be detected is viewed from above, it is as shown in FIG. This has a height of 170 cm and a width of 50 cm as shown in Figure 8(a).
Using a rectangular parallelepiped with a depth of 20 CTI as an upright human body model, four human body models 'm, i to TL4 are placed at the vertices of a square with a side of 3 m, as shown in Fig. 8(b) and (c). This is a two-dimensional image projected onto a plane parallel to the floor surface U at a point 3 m above the floor surface U by the human body model desks 1 to TrL4. As is clear from the figure, the human body seen from above is
Except when placed at the center C of the visual field, the side of the human body is also viewed, resulting in an image extending in the radial direction from the center C of the visual field.

また、人体の位置が視野中心Cから離れる程、人体像は
放射方向により伸びた像となる。上記の点を考慮して、
長方形スリット状の視野面を設け、その端点を中心とし
て、視野面を回転させる円形走査方式を用いることによ
り人体を有効且つ効率的に検出、識別すると共に、計数
できることが分かる。
Further, as the position of the human body moves away from the visual field center C, the human body image becomes more elongated in the radial direction. Considering the above points,
It can be seen that human bodies can be effectively and efficiently detected, identified, and counted by providing a rectangular slit-shaped viewing surface and using a circular scanning method in which the viewing surface is rotated around its end point.

第10図に円形走査光学系の一例を示す。同図(、)に
示すように、赤外線検出素子2の受光面前面より距離R
b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10図(b)に示すように、回転板10に長さL
a、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の形状と相以であり
、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。
FIG. 10 shows an example of a circular scanning optical system. As shown in the figure (,), distance R from the front of the light receiving surface of the infrared detection element
The rotary plate 10 is placed at position b, 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. 10(b), the rotating plate 10 has a length L.
A and a rectangular slit A having a width Da are provided so that only the infrared rays radiated from the object surface B that pass through the slit A enter the infrared detecting element 2. The instantaneous field of view on the object plane has the same shape as the slit A, and if the distance from the rotary plate 10 to the object plane B is Ra, then the instantaneous field of view length Lv and the field width Dv on the object plane are calculated by the following formula. become that way.

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。
Further, in the radial direction in circular scanning, if the instantaneous field of view is the viewing angle at which the object surface B is seen, θ is expressed as in the following equation.

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。
The above-mentioned instantaneous field of view is circularly scanned with the field center C of the light-receiving surface of the infrared detection element 2 as an axis, and therefore, the total viewing angle looking into the object surface B by the circular scanning method is 2θ.

第10図において、スリットAの部分に凸面シリンドリ
カルレンズを設けると、所望の光学利得を得ることがで
きる。
In FIG. 10, if a convex cylindrical lens is provided at the slit A, a desired optical gain can be obtained.

また、光学利得を得るための他の手段として、第11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する例もある。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Lm、ミラー幅をDa、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Lv
、及び視野幅Dvは、次式のようになる。
Furthermore, as another means for obtaining optical gain, as shown in FIG. There are also examples of configuration. The distance from the mirror surface of the cylindrical mirror M to the light receiving surface of the infrared detection element 2 is Rb, the distance from the mirror surface of the cylindrical mirror M to the object surface B is Ra, the mirror length of the cylindrical mirror M is Lm, the mirror width is Da, When the diameter of the light-receiving surface of the infrared detection element 2 is d, the instantaneous field of view length Lv on the object surface is
, and the visual field width Dv are expressed by the following equation.

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のミラー幅り曽を−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、次式のようになり、全視野角は2θとなる。
Therefore, by selecting an appropriate Rb or d, a predetermined instantaneous field of view width Dv can be obtained, and the optical gain can be increased by increasing the mirror width R of the cylindrical mirror M. In the radial direction during scanning, the viewing angle θ at which the instantaneous visual field looks at the object surface B is expressed by the following equation, and the total viewing angle is 2θ.

この装置の光学系においては、被検知人体と人体検出装
置との距離が遠くなるほど、赤外線検出感度が落ちるた
めに、近くの人体と遠くの人体とでは得られる信号レベ
ルが大きく変化し、信号処理が複雑化したり、極端な場
合には、小さな信号が検出されない場合があった。
In the optical system of this device, the greater the distance between the detected human body and the human body detection device, the lower the infrared detection sensitivity, so the signal level obtained from a nearby human body and a distant human body changes greatly, and the signal processing In extreme cases, small signals may not be detected.

例えば、第11図に示すように、検出装置の近くに立っ
ている人間Tn、 A 、 a aは、体全体がその視
野の中に入っているのに対し、遠くの位置に立っている
人間TrLcは、体全体の1/2程度、また、さらに遠
くの位置に立っている人間′rrLDは、体全体の11
5程度しか視野内に入らない、このために、遠距離から
の信号レベルは極端に小さくなる。
For example, as shown in FIG. 11, a person Tn, A, aa standing near the detection device has his or her entire body within its field of view, whereas a person standing far away has the entire body within its field of view. TrLc is about 1/2 of the whole body, and a person standing further away, 'rrLD, is about 11% of the whole body.
Only about 500 yen can be seen within the field of view, so the signal level from a long distance becomes extremely low.

また、人間n A、 n eについては、体全体が視野
の内部に入っているが、それでも、近距離の人間冗Aか
ら放射された赤外線の受光レベルに比べると、遠距離の
人間IrrL日から放射された赤外線の受光レベルは小
さくなるという問題があった。
In addition, although the entire body of humans nA and ne is within the field of view, even so, compared to the level of infrared rays emitted from the human A at a close distance, the level of infrared rays received from the human IrrL at a far distance is There has been a problem in that the level of received infrared rays emitted is low.

そこで、検知領域内の人体から得られる出力を出来る限
り均一化することが望まれるが、長方形の開口面によっ
てこれを達成しようとすれば、必要な検知領域よりも赤
外線検出素子2の視野をかなり広くする必要が生じ、こ
のためには、ミラーMの長さを長くしなければならず、
光学系が大きくなってしまうという問題がある。
Therefore, it is desirable to make the output obtained from the human body within the detection area as uniform as possible, but if you try to achieve this with a rectangular aperture, the field of view of the infrared detection element 2 will be considerably larger than the required detection area. It becomes necessary to make the mirror wider, and for this purpose the length of the mirror M must be increased.
There is a problem that the optical system becomes large.

(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、検知領域内の距離による赤外
線の受光感度差を低減し、確実に人数計測を行うことが
できるようにした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 can reduce the difference in infrared reception sensitivity depending on the distance within the detection area and can reliably count the number of people.

(発明の開示) 本発明に係る人数検出装置にあっては、円形走査光学系
1において、第1図に示すように、回転、中心から遠ざ
かるほど開口幅の広くなるスリットXを備えており、こ
のスリットXにて形成される視野面を回転させることに
より、赤外線検出素子2の視野を円形走査させるように
なっている。このスリットXを第11図(b)に示すシ
リンドリカルミラーMの前面に配したときに、赤外線検
出素子2によって得られる信号のレベルは、第2図の破
線に示すようになり、長方形のスリットを用いた同図の
実線の場合に比べると、近くの方はレベルが低下し、遠
くの方はレベルが高くなる。これによって、検知領域内
の距離による赤外線の受光感度差を低減することができ
、人数計測を正確に行うことができるようになる。
(Disclosure of the Invention) In the number of people detection device according to the present invention, as shown in FIG. 1, the circular scanning optical system 1 is provided with a slit X whose aperture width becomes wider as the distance from the rotation center increases. By rotating the field of view formed by this slit X, the field of view of the infrared detection element 2 is made to scan in a circular manner. When this slit Compared to the case of the solid line in the figure used, the level is lower in the vicinity, and the level is higher in the distance. This makes it possible to reduce the difference in infrared light reception sensitivity depending on the distance within the detection area, making it possible to accurately count the number of people.

以下、本発明の原理を従来例と比較しながら説明する。Hereinafter, the principle of the present invention will be explained while comparing it with a conventional example.

まず、ある物体の微小面fldsから放射されるパワー
をPTとし、この面から出るパワーの分布はコサイン則
によるものと考える。@小面WIdSの法線方向と、微
小面積dSがら検出装置を見た方向とのなす角をψとす
る。このとき、赤外線検出素子2の直径をd、シリンド
リカルミラーMのミラー幅をD糟、赤外線検出素子2と
ミラーMとの間の距離をRb、ミラーから微小面積dS
までの距離をRaとすれば、微小面積dSから赤外線検
出素子2が受けるパワーdPは、近似的に次式のように
なる。
First, it is assumed that the power radiated from a microscopic surface flds of a certain object is PT, and the distribution of power emitted from this surface is based on the cosine law. @ Let ψ be the angle between the normal direction of the small surface WIdS and the direction in which the detection device is viewed from the small area dS. At this time, the diameter of the infrared detection element 2 is d, the mirror width of the cylindrical mirror M is D, the distance between the infrared detection element 2 and the mirror M is Rb, and the minute area from the mirror is dS.
If the distance to the infrared detection element 2 is Ra, the power dP received by the infrared detection element 2 from the minute area dS is approximately expressed by the following equation.

赤外線検出素子2の指向特性を考えると、受光面の法線
方向の感度は、はぼコサイン則に従うから、法線方向か
らθ傾いたところからの入射パワーによる素子の出力信
号dS0は、次式のようになる。
Considering the directivity characteristics of the infrared detection element 2, the sensitivity in the normal direction of the light-receiving surface follows the habocosine law, so the output signal dS0 of the element due to the incident power from a point tilted by θ from the normal direction is given by the following formula: become that way.

この式を元に、人体を第8図に示すような直方体と考え
、各距離における素子出力を計算した結果をグラフで表
したものが第6図である。このときのシリンドリカルミ
ラーMの形状は、第11図(b)に示したものをスリッ
ト無しで用いている。
Based on this formula, the human body is considered to be a rectangular parallelepiped as shown in FIG. 8, and the results of calculating the element output at each distance are shown in a graph in FIG. At this time, the shape of the cylindrical mirror M shown in FIG. 11(b) is used without a slit.

赤外線検出素子2として焦電素子を用い、第4、図に示
すように、2人の人間′rrLA、 m sが立った場
合を想定する。第4図において、Qは視野の回転方向、
Foは検出装置の全有効視野を示している。
Fourth, assume that a pyroelectric element is used as the infrared detection element 2, and two people 'rrLA, ms are standing as shown in the figure. In Figure 4, Q is the rotation direction of the field of view,
Fo indicates the entire effective field of view of the detection device.

この場合、1人目の人間′rrL八からの入射パワーは
第5図(a)に示すように大きいが、2人目の人間′a
Bからの入射パワーは第5図(b)に示すように小さい
、したがって、1人目の人間′m、Aによって得られる
信号は第5図(e)に示すように大きくなり、2人目の
人間′aBによって得られる信号は第5図(d)に示す
ように小さくなる。このため、赤外線検出素子2の検出
出力は、第5図(e)に示すようになり、1人目の人間
aAに対応する信号が大き過ぎるために、2人目の人間
’Isに対応する信号が隠れたり、山が小さくなるなど
の問題があり、人数検出のために、山の極大値を求める
ことが不可能であったり、どのレベル以上の極大値を人
体とみなすかなどの問題がある。
In this case, the incident power from the first person 'rrL8 is large as shown in FIG. 5(a), but the incident power from the second person 'a
The incident power from B is small as shown in Fig. 5(b), so the signal obtained by the first person 'm, A is large as shown in Fig. 5(e), and the signal obtained by the second person The signal obtained by 'aB' becomes small as shown in FIG. 5(d). Therefore, the detection output of the infrared detection element 2 becomes as shown in FIG. 5(e), and since the signal corresponding to the first person aA is too large, the signal corresponding to the second person 'Is is There are problems such as the mountain being hidden or the mountain becoming smaller, it is impossible to find the maximum value of the mountain in order to detect the number of people, and there are problems such as which level or higher the maximum value should be regarded as a human body.

そこで、本発明にあっては、第1図に示すようなラッパ
型のスリットXをシリンドリカルミラーMの前面に取り
付けて、ミラーMの開口幅を回転中心から見て外側に行
くほど大きくなるようにしている。第1図において、斜
線を施した部分は遮光部であり、それ以外の部分は透光
部である。このラッパ型のスリットXを付加した場合に
、赤外線検出素子2によって得られる信号は、第2図の
破線に示すようになり、近くの方は信号レベルが低下し
、遠くの方は信号レベルが高くなる。第2図において、
横軸は検出装置からの距離、縦軸は赤外線検出素子2に
より得られる信号のレベルを示しており、実線は比較例
として長方形のスリットを用いたPAキの特性を示して
いる。
Therefore, in the present invention, a trumpet-shaped slit X as shown in FIG. ing. In FIG. 1, the shaded portion is a light-shielding portion, and the other portions are light-transmitting portions. When this trumpet-shaped slit It gets expensive. In Figure 2,
The horizontal axis shows the distance from the detection device, the vertical axis shows the level of the signal obtained by the infrared detection element 2, and the solid line shows the characteristics of a PA using a rectangular slit as a comparative example.

前記ラッパ型のスリットXを付加した場合において、第
4図に示した位置に人体乳A、naが立った場きを想定
する。この場合には、1人目の人間′aAからの入射パ
ワーは第3図(a)の実線に示すように低下し、2人目
の人間′rrL日からの入射パワーは第3[EJ(b)
の実線に示すように高くなる。したがって、1人目の人
間TrLAによって得られる信号は第3図(c)の実線
に示すように小さくなり、2人目の人間’laによって
得られる信号は第3図(d)の実線に示すように大きく
なる。このため、赤外線検出素子2の検出出力は、第3
図(e)の実線に示すようになり、長方形のスリットを
用いた場きには隠れてしまっていた信号が十分に検出で
きるようになる。また、赤外線検出素子2がら見た視野
と検知領域との差がノドさくなるので、検知領域外から
の雑音の影響が少なくなる。なお、第3図(a)〜(e
)において、破線はラッパ型のスリットXと同じ長さの
長方形スリットを用いた場合の特性を比較例として示し
ている。
In the case where the trumpet-shaped slit X is added, it is assumed that human breasts A and na stand at the position shown in FIG. 4. In this case, the incident power from the first person 'aA decreases as shown by the solid line in FIG.
as shown by the solid line. Therefore, the signal obtained by the first person TrLA becomes small as shown by the solid line in FIG. 3(c), and the signal obtained by the second person 'la becomes small as shown by the solid line in FIG. 3(d). growing. Therefore, the detection output of the infrared detection element 2 is
As shown by the solid line in Figure (e), signals that were hidden when a rectangular slit was used can now be fully detected. Furthermore, since the difference between the field of view seen from the infrared detection element 2 and the detection area is narrowed, the influence of noise from outside the detection area is reduced. In addition, Fig. 3 (a) to (e
), the broken line shows the characteristics when a rectangular slit having the same length as the trumpet-shaped slit X is used as a comparative example.

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7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、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 a device for detecting the number of people using the optical system will be explained based on FIG. 7. 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 that constitutes 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
い場キの出力波形が゛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。
In the determination unit 5, the output waveform when a human body is not 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 determined simultaneously.

本実施例では、入力波形データと参照波形データとで比
較演算を行い、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Oの場合には、現在の入力
波形データが参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がら
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 this example, a comparison operation is performed between input waveform data and reference waveform data, the result is 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, when the detected number of people is O, the current input waveform data is updated as reference 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 unit 6 is designed to display the number of people information based on the number of people information given by the determination unit 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、
゛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ftEさせることができる。
Based on “one person” and “more than 2 Å”, the indoor situation is determined as follows:
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、回転中心から遠ざかるほど開口幅の広くな
るスリットにて形成される視野面を回転させることによ
り、赤外線検出素子の視野を円形走査させるようにしな
がら、スリットを介して受光される赤外線の受光量は回
転中心から遠ざかるほど多くなり、これによって距離に
よる赤外線の受光感度差を低減することができ、距離に
よる人体検出信号のレベル差が低減されるので、人数計
測を正確に行うことができるようになるという効果があ
る。
(Effects of the Invention) As described above, the present invention is 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. By rotating the field of view that is formed, the field of view of the infrared detection element is circularly scanned, and the amount of infrared rays received through the slit increases as the distance from the center of rotation increases. Since the difference in light reception sensitivity can be reduced and the difference in the level of the human body detection signal depending on the distance can be reduced, there is an effect that the number of people can be counted accurately.

【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スリットの
正面図、第2図乃至第4図は同上の動作説明図、第5図
及び第6図は従来例の動作説明図、第7図は従来例のブ
ロック図、第8図(a)は同上の動作説明のための人体
モデルを示す斜視図、同図(b)は同上の人体モデルの
配置状況を示す側面図、同図(c)は同上の人体モデル
の配置状況を示す平面図、第9図は同上の人体モデルの
配置状況を上方から見た2次元像を示す平面図、第10
図(a)は従来例に用いる光学系の概略構成図、同図(
1])は同上の要部底面図、第11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
部底面図である。 1は円形走査光学系、2は赤外線検出素子、3は前置増
幅部、4は信号処理部、5は判断部、6は出力部、又は
スリットである。
Fig. 1 is a front view of the slit used in the number of people detection device according to the present invention, Figs. 2 to 4 are explanatory diagrams of the same operation as above, Figs. 5 and 6 are explanatory diagrams of the operation of the conventional example, and Fig. 7 8 is a block diagram of the conventional example, FIG. 8(a) is a perspective view showing a human body model for explaining the operation of the above, FIG. ) is a plan view showing the arrangement of the human body model as above, FIG. 9 is a plan view showing a two-dimensional image of the arrangement of the human body model as seen from above, and
Figure (a) is a schematic diagram of the optical system used in the conventional example;
1]) is a bottom view of the main parts of the same as above, FIG. 11(a) is a schematic configuration diagram of an optical system used in another conventional example, and FIG. 11(b) is a bottom view of the main parts of the same. 1 is a circular scanning optical system, 2 is an infrared detection element, 3 is a preamplification section, 4 is a signal processing section, 5 is a judgment section, and 6 is an output section or slit.

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
円形走査させる円形走査光学系と、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、前記円形
走査光学系は、回転中心から遠ざかるほど開口幅の広く
なるスリットにて形成される視野面を回転させることに
より、赤外線検出素子の視野を円形走査させる光学系で
あることを特徴とする人数検出装置。
(1) An infrared detection element, a circular scanning optical system that circularly 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 A number of people detection unit that includes a signal processing unit that converts into a signal necessary for detection, a determination unit that determines the number of people based on the output signal of the signal processing unit, and an output unit that outputs number of people information from the output signal of the determination unit. In the apparatus, the circular scanning optical system is an optical system that circularly scans the field of view of the infrared detection element by rotating a field of view formed by a slit whose aperture width becomes wider as the distance from the center of rotation increases. A device to detect the number of people.
JP61281304A 1986-11-26 1986-11-26 Person number detector Pending JPS63134983A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61281304A JPS63134983A (en) 1986-11-26 1986-11-26 Person number detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61281304A JPS63134983A (en) 1986-11-26 1986-11-26 Person number detector

Publications (1)

Publication Number Publication Date
JPS63134983A true JPS63134983A (en) 1988-06-07

Family

ID=17637210

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61281304A Pending JPS63134983A (en) 1986-11-26 1986-11-26 Person number detector

Country Status (1)

Country Link
JP (1) JPS63134983A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0249102A (en) * 1988-08-10 1990-02-19 Daikin Ind Ltd Detecting device for human body position
JPH034281U (en) * 1989-05-31 1991-01-17

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0249102A (en) * 1988-08-10 1990-02-19 Daikin Ind Ltd Detecting device for human body position
JPH034281U (en) * 1989-05-31 1991-01-17

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