JPH03238391A - Human body detector - Google Patents

Human body detector

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Publication number
JPH03238391A
JPH03238391A JP2034207A JP3420790A JPH03238391A JP H03238391 A JPH03238391 A JP H03238391A JP 2034207 A JP2034207 A JP 2034207A JP 3420790 A JP3420790 A JP 3420790A JP H03238391 A JPH03238391 A JP H03238391A
Authority
JP
Japan
Prior art keywords
output
human body
time
infrared detection
detection elements
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
JP2034207A
Other languages
Japanese (ja)
Other versions
JPH07104416B2 (en
Inventor
Hidekazu Himesawa
秀和 姫澤
Takashi Horii
堀井 貴司
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 JP2034207A priority Critical patent/JPH07104416B2/en
Publication of JPH03238391A publication Critical patent/JPH03238391A/en
Publication of JPH07104416B2 publication Critical patent/JPH07104416B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To prevent the erroneous operation due to noise by judging the latest points of time when the increase and decrease directions of the change in respective outputs until the outputs of infrared detection elements exceed a judging value are inverted as output times. CONSTITUTION:When the outputs of infrared detection elements A - D change, a judging part 5 judges the latest points when the increase and decrease directions of the change in respective output until the outputs of the infrared detection elements A - D exceed a judging value Vth judging the generation of the outputs are inverted as output times. Concretely, the inclinations of the output changes of the detection elements A - D are calculated and times when the polarities of the inclinations are inverted are stored. The times stored previously are erased at the inversion time of polarity and new polarity inversion times are stored. At the point of time when the outputs of the detection elements A - D exceed predetermined voltage Vth, the times ts stored at that time are judged to be output times tA - tD. By this method, the judging value Vth judging the generation of the outputs of the detection elements A - D can be made relatively high. That is, since a peak value is low, noise can be removed.

Description

【発明の詳細な説明】 [産業上の利用分野j 本発明は、人体から放射される赤外線により人体を検出
する赤外線受光式の人体検出装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to an infrared receiving type human body detection device that detects a human body using infrared rays emitted from the human body.

[従来の技術1 赤外線受光式の人体検出装置は、焦電素子等の赤外線検
出素子を用いて、人体とw景との赤外線のエネルギ量の
差(つまりは、人体と背景の温度差)を検出して人体を
検出するものであり、近年広く普及しでおり、これに伴
って信頼性の改善が求められてきでいる。この赤外線受
光式の人体検出装置の誤動作要因としては、検知領域内
での背景の温度変化、内部雑音、ヘッドライトや太陽光
等のエネルギの大きな外乱光の影響等が考えられる。そ
こで、これらの誤動作要因を除去するために、従来から
種々の提案がなされている。その1つとして、4個の赤
外線検出素子を用いて2組の差動出力を得て人体を検出
する方法が提案されている(特開昭58−213396
号公報あるいはwWi昭59−94094号公報)。こ
の人体検出装置の検出動作の一例を第3図及び第4図に
基づいて説明する。この人体検出装置では、背景上にお
いて4つの検知領域I〜■を設定すると共に、これら検
知領域I〜■からの赤外線を夫々受光する赤外線検出素
子A ”、 A −、B +、 B−を備え、検知領域
I、IV及び検知領域■、■毎に各々差動出力■a(赤
外線検出素子A”、A−間の出力差)及び\・′b(赤
外線検出素子B”、B−間の出力差)を得る。第3図(
、)に示すように人体Mが検知領域1.IIIから検知
領域It、rVに移動すると、第4図(a)に示す差動
出力V a、 V bが得られ、また第3図(b)に示
すように人体Mが検知領域1.Itから検知領域■、■
に移動すると、第4図(b)に示す差動出力Va、vh
が得られる。
[Prior art 1 An infrared receiving type human body detection device uses an infrared detection element such as a pyroelectric element to detect the difference in the amount of infrared energy between the human body and the scenery (that is, the temperature difference between the human body and the background). It detects the human body and has become widespread in recent years, and as a result, there has been a demand for improved reliability. Possible causes of malfunction of this infrared receiving type human body detection device include background temperature changes within the detection area, internal noise, and the influence of high-energy disturbance light such as headlights and sunlight. Therefore, various proposals have been made to eliminate these causes of malfunction. One such method has been proposed to detect a human body by obtaining two sets of differential outputs using four infrared detection elements (Japanese Patent Application Laid-Open No. 58-213396
(or wWi No. 59-94094). An example of the detection operation of this human body detection device will be explained based on FIGS. 3 and 4. In this human body detection device, four detection areas I to ■ are set on the background, and infrared detection elements A'', A-, B+, and B- are provided to receive infrared rays from these detection areas I to ■, respectively. , differential output ■a (output difference between infrared detecting elements A", A-) and \'b (infrared detecting elements B", B-) Figure 3 (output difference) is obtained.
, ), the human body M is located in the detection area 1. When the human body M moves from the detection area It, rV to the detection area It, rV, the differential outputs Va, Vb shown in FIG. 4(a) are obtained, and as shown in FIG. 3(b), the human body M moves to the detection area 1. Detection area from It■,■
When moving to , the differential outputs Va, vh shown in FIG. 4(b)
is obtained.

ところで、この人体検出装置では例えば第3図(c)に
示すように人体Mが4つの検知領域I〜■を斜めに横切
った場合、第4図(c)のように差動出力Vaは得られ
るが、検知領域■、■では人体Mが同時に横切るために
出力が打ち消され、差動出力vbが生じない。そこで、
このに体検出装置では人体Mの移動を確実に検出するた
めに、差動出力Va、Vbの内のいずれかが出力を生じ
た場合に人体が存在すると判定する必要がある。ところ
が、このようにして人体Mを検知すると、1個の検知領
域内で生じる温度変化や1@の赤外線検出素子に生じる
内部雑音等により、差動出力Va、Vbの一方が出力を
生じ、誤動作の原因になるという問題があった。
By the way, in this human body detection device, when the human body M diagonally crosses the four detection areas I to ■ as shown in FIG. 3(c), the differential output Va is obtained as shown in FIG. 4(c). However, since the human bodies M cross at the same time in the detection areas (2) and (2), the outputs are canceled and no differential output vb is generated. Therefore,
In order to reliably detect the movement of the human body M, the body detection device needs to determine that a human body is present when either of the differential outputs Va and Vb produces an output. However, when detecting the human body M in this way, one of the differential outputs Va and Vb will generate an output due to temperature changes occurring within one detection area or internal noise occurring in the infrared detection element 1@, resulting in malfunction. There was a problem that it could cause

そこで・、上述の問題点を解消するために本発明者等は
複数の赤外線検出素子の出力を夫々比較して人体を検出
する人体検出装置を提案している(特願昭62−242
09 (1号)。第5図にこの人体検出装置の全体構成
を示す。この人体検出装置は、複数の検知領域A°〜D
゛からなり人体Mに比べて十分に小さい領域からの赤外
線を集光用の光学系1を通して各検知領域A゛〜D゛毎
に夫々受光する複数の赤外線検出素子A−Dからなる赤
外線検出fIS2と、夫々の赤外線検出素子A−Dの各
出力を独立に増幅する増幅部3と、増幅出力を人体検出
に適した信号に変換する信号処理部4と、変換信号のピ
ーク値と出力時刻とを検出すると共にこれらを相互に比
較して人体の有無を判定する判定部5と、判定結果を出
力する出力部6とで構rRされている。
Therefore, in order to solve the above-mentioned problems, the present inventors have proposed a human body detection device that detects a human body by comparing the outputs of a plurality of infrared detection elements (Japanese Patent Application No. 62-242
09 (No. 1). FIG. 5 shows the overall configuration of this human body detection device. This human body detection device has multiple detection areas A° to D.
An infrared detection fIS2 consisting of a plurality of infrared detection elements A to D which receive infrared light from an area sufficiently small compared to the human body M through an optical system 1 for condensing the infrared light from a region sufficiently small compared to the human body M. , an amplification section 3 that independently amplifies each output of each infrared detection element A-D, a signal processing section 4 that converts the amplified output into a signal suitable for human body detection, and a peak value and output time of the converted signal. It consists of a determination section 5 that detects and compares these with each other to determine the presence or absence of a human body, and an output section 6 that outputs the determination result.

この人体検出装置の動作を第6図及び第7図に基プいて
説明する。この人体検出装置では、上述のように検知領
域A゛〜D゛からなる領域を人体Mに比べて十分に小さ
い領域に絞ることにより、領域を通過する人体Mは移動
方向にかかわらず検知領域A゛〜D゛の全域を通過する
ようにしてあり、このため人体Mが検知領域A°〜D”
を通過すると、赤外線検出素子A−Dの各出力のピーク
値VA〜VDはほぼ同一の値になる。従って、赤外線検
出素子A−Dの各出力のピーク値vA〜\7.がほは同
一の値を示すことを、人体Mの存在判定の第1の判定条
件とすることができる。但し、実際には人体Mの表面の
温度分布等により赤外線検出素子A〜Dの各出力のピー
ク値にはある程度のばらつきがあり、また各出力のピー
ク値■8〜VDは周囲温度によって影響を受けるので、
この存在判定に関しては各赤外線検出素子A−Dの出力
を相対的に比較して人体Mの存在判定を行っている。今
、赤外線検出素子AT−Dの各出力のピーク値V^〜V
Dの最大値をV wax、最小値をVeinとすると、
Vma×とV winとの比が所定値S(o<S<1)
より大きければ、各ピーク値VA〜■1のばらつきが小
さく、人体Mが存在すると判定する。つまり、この人体
Mの存在判定の第1の判定条件を式で表すと次のように
なる。
The operation of this human body detection device will be explained based on FIGS. 6 and 7. In this human body detection device, by narrowing down the area consisting of detection areas A to D to a sufficiently small area compared to the human body M as described above, the human body M passing through the area can be detected in the detection area A regardless of the direction of movement. The human body M passes through the entire area from ゛ to D゛, so that the human body M passes through the entire detection area from A to D''.
, the peak values VA to VD of the respective outputs of the infrared detection elements A to D become approximately the same value. Therefore, the peak value vA~\7 of each output of the infrared detection elements A-D. The first determination condition for determining the presence of the human body M may be that the values are the same. However, in reality, there is some variation in the peak value of each output of the infrared detection elements A to D due to the temperature distribution on the surface of the human body M, and the peak value of each output ■8 to VD is affected by the ambient temperature. Because I receive it,
Regarding this presence determination, the presence of the human body M is determined by relatively comparing the outputs of the respective infrared detection elements A to D. Now, the peak value V^~V of each output of the infrared detection element AT-D
If the maximum value of D is V wax and the minimum value is Vein,
The ratio of Vmax and Vwin is a predetermined value S (o<S<1)
If it is larger, it is determined that the variation in each peak value VA~1 is small and that the human body M is present. In other words, the first judgment condition for determining the presence of the human body M is expressed as follows.

V sin/ V wax > S    −(1)但
し、0<S<1 また、人体Mが検知領域A゛〜D゛を通過する場合には
、移動方向にかかわらず全ての検知領域A〜D゛に同時
に侵入することは有り得ない。つまりは、各赤外線検出
素子A−Dの出力信号が立ち上がる時刻(以下、この時
刻を出力時刻と呼r)t^〜1(、には時開差が存在す
る。従って、出力時刻t^〜tDに時間差が存在するこ
とを、人体Mの存在判定の@2の判定条件とすることが
できる。なお、上記時開差は検知領域A゛〜D゛の広さ
及び人体Mの移動速度を考慮すれば、ある範囲に限定さ
れる。
V sin/V wax > S - (1) However, 0<S<1 In addition, when the human body M passes through the detection areas A'' to D'', all the detection areas A to D'' regardless of the direction of movement. It is impossible for both to invade at the same time. In other words, there is a time difference between the times at which the output signals of each infrared detection element A to D rise (hereinafter, this time will be referred to as output time) t^~1(,).Therefore, the output time t^~ The presence of a time difference in tD can be used as the criterion @2 for determining the presence of the human body M.The above time difference is based on the width of the detection areas A'' to D'' and the moving speed of the human body M. Considering this, it is limited to a certain range.

従って、出力時刻1.−10の時間差を、6tとすると
、次式で示す人体Mの存在判定の第2の判定条件が得ら
れる。
Therefore, output time 1. If the time difference of -10 is set to 6t, the second determination condition for determining the presence of the human body M is obtained as shown in the following equation.

Twin< 4t< Tmax    =12)但し、
TvintTs+aには夫々時間差の下限値及び上限値
である。例えば、第7図(a)〜(c)に示す赤外線検
出素子A−Dの出力が得られた場合には、いずれの場合
にも時間差1:J t = tL+ −tAとして求ま
る。
Twin < 4t < Tmax = 12) However,
TvintTs+a is the lower limit value and upper limit value of the time difference, respectively. For example, when the outputs of the infrared detection elements A-D shown in FIGS. 7(a) to (c) are obtained, the time difference is determined as 1:J t = tL+ -tA in any case.

即ち、この人体検出i置においては、赤外線検出素子A
−Dの各出力のピーク値\・′6〜Voが略−定であり
、且つ各出力の出力時刻t7〜[,3に所定範囲のばら
つきがある場合にに体Mが存在すると判定するのである
。このようにして人体Mの有無を判定すると、全般的な
温度変化や太陽光等の外乱光、あるいは局所的な温度変
化や内部雑音等の影響による誤動作を防止でき、信頼性
の高い人体検出装置となる。
That is, in this human body detection position i, the infrared detection element A
If the peak value \・'6~Vo of each output of -D is approximately - constant, and there is variation within a predetermined range at the output time t7~[,3 of each output, it is determined that the body M exists. be. Determining the presence or absence of a human body M in this way prevents malfunctions caused by general temperature changes, disturbance light such as sunlight, local temperature changes, internal noise, etc., and makes the human body detection device highly reliable. becomes.

[発明が解決しようとする課題] ところで、この人体検出装置では各赤外線検出素子A−
Dの出力時刻はそれらの出力レベルが所定の判定値を越
えた時点として判定部5が検出していた。ここで、人体
Mが検知領域A゛〜D°を通過する場合に要する時開は
人体Mの移動速度に反比例し、人体Mの存在判定の第2
の判定条件((2)式)の下限値T sinは最高速度
で移動する人体Mにて得られる赤外線検出素子A−Dの
出力時間差をもとにして設定することになる。従って、
このような出力時刻の検出方法では高速で移動するに体
Mを正確に検出するために上記判定値は低く設定する必
要がある。なお、この人体検出装置では例えば時速36
0II+(秒速0.1輪)から時速36i(秒速10カ
)で移動するに体Mを検出するようにしである。
[Problems to be Solved by the Invention] By the way, in this human body detection device, each infrared detection element A-
The determination unit 5 detected the output time of D as the time when their output levels exceeded a predetermined determination value. Here, the time required for the human body M to pass through the detection areas A゛~D° is inversely proportional to the moving speed of the human body M, and the second
The lower limit T sin of the determination condition (Equation (2)) is set based on the output time difference of the infrared detection elements A and D obtained with the human body M moving at the highest speed. Therefore,
In such an output time detection method, the determination value needs to be set low in order to accurately detect the body M moving at high speed. Note that this human body detection device has a speed of 36 mph, for example.
The body M is detected when the vehicle moves from 0II+ (0.1 wheels per second) to 36i (10 kilometers per second).

また、次の理由によっても上記判定値を低く設定する必
要がある。例えば、外乱光等により赤外線が同時に赤外
線検出素子A−Dに入射され、かつ光源が各赤外線検出
素子A−Dの検知領域の中心から大きくずれた位置にあ
り、赤外線入射光量に差がある場合、第8図に示す赤外
線検出素子A〜Dの出力が得られる。ここで、判定値を
vthに設定しであると、出力時刻に時間差が生じ(t
^〜to)、ピーク値VA−VDが第1の判定条件を満
足すると、上述のようにvi2の判定条件も満足し、外
乱光により誤動作する。しかし、判定値を第8図中Vt
h’で示すように低くすると、赤外線検出素子A−[)
の各出力時刻にはtA′〜ttl”で示すように時間差
が無くなり、(2〉式の判定条件を満足しなくなり、こ
のため外乱光による誤動作を防止できる。従って、上述
のような外乱光による誤動作を防止するためにも判定値
は低く設定する必要がある。
Furthermore, it is necessary to set the above-mentioned judgment value low for the following reason as well. For example, when infrared rays are simultaneously incident on infrared detection elements A-D due to disturbance light, etc., and the light source is located far away from the center of the detection area of each infrared detection element A-D, and there is a difference in the amount of infrared incident light. , the outputs of the infrared detection elements A to D shown in FIG. 8 are obtained. Here, if the judgment value is set to vth, a time difference will occur in the output time (t
^~to), when the peak value VA-VD satisfies the first determination condition, the determination condition of vi2 is also satisfied as described above, and a malfunction occurs due to the disturbance light. However, the judgment value is Vt in Figure 8.
When lowered as shown by h', the infrared detection element A-[)
There is no time difference between the output times of tA' to ttl, as shown by tA' to ttl'', and the judgment condition of equation (2) is no longer satisfied, which makes it possible to prevent malfunctions caused by ambient light. The determination value must be set low to prevent malfunctions.

しかしながら、上述のように出力時刻を検出するための
判定値を低く設定すると、例えば第9図に示すような出
力時刻が異なり、且つピーク値が略一定の雑音が判定部
5に入力されると、第1及V第2の判定条件を共に満足
する場合があり、このため雑音により誤動作する可能性
があった。つまりは、判定値を低く設定すると、雑音に
反応してしまうのである。
However, if the judgment value for detecting the output time is set low as described above, for example, if noise with different output times and a substantially constant peak value is input to the judgment unit 5 as shown in FIG. , the first and the second determination conditions may both be satisfied, and therefore there is a possibility of malfunction due to noise. In other words, if the judgment value is set low, it will react to noise.

本発明は上述の点に鑑みて為されたちのであり、その目
的とするところは、雑音による誤動作の可能性が少ない
人体検出装置を提供することにある。
The present invention has been made in view of the above-mentioned points, and its purpose is to provide a human body detection device that is less likely to malfunction due to noise.

[課題を解決するための手段1 上記目的を達成するために、本発明は判定部が赤外線検
出素子の出力が生じたと判定する判定値を越えるまでの
各出力の変化の増減方向が反転した最新の時点を出力時
刻であると判定するようにしである。
[Means for Solving the Problems 1] In order to achieve the above object, the present invention provides a new method in which the direction of increase/decrease in each output is reversed until the determination unit exceeds the determination value for determining that the output of the infrared detection element has occurred. The point in time is determined to be the output time.

なお、判定部が赤外線検出素子の出力が生じたと判定す
る判定値を越えるまでの各出力の変化の増減割合が増大
した最新の時点を出力時刻と樗定するようにしても、上
述の場合と同一の目的を達處することができる。
Note that even if the output time is determined to be the latest point in time at which the increase/decrease rate of change in each output increases until it exceeds the determination value at which the determination unit determines that the output of the infrared detection element has occurred, the above case will not occur. can achieve the same purpose.

[作用1 本発明は、上述のように判定部が赤外線検出素子の出力
が生じたと判定する判定値を越えるまでの各出力の変化
の増減方向が反転した最新の時点を出力時刻であると判
定することにより、赤外線検出素子の出力が生じたこと
の判定を雑音を除去できる比較的に高い判定値で行って
雑音による誤動作を防止できるようにしたものである。
[Operation 1] As described above, the present invention determines that the latest point in time at which the increase/decrease direction of the change in each output is reversed until the determination unit exceeds the determination value for determining that the output of the infrared detection element has occurred is the output time. By doing so, it is possible to determine whether the output of the infrared detection element has occurred using a relatively high determination value that can remove noise, thereby preventing malfunctions due to noise.

また、判定部が赤外線検出素子の出力が生じたと判定す
る判定値を越えるまでの最新の各出力の変化の増減割合
が増大した時点を出力時刻と判定しても、赤外線検出素
子の出力が生じたことの判定を雑音を除去できる比較的
に高い判定値で行って、雑音による誤動作を防止できる
Furthermore, even if the determination unit determines as the output time the point in time when the increase/decrease rate of the latest change in each output increases until it exceeds the determination value for determining that the output of the infrared detection element has occurred, the output of the infrared detection element has not occurred. By using a relatively high judgment value that can remove noise, malfunctions due to noise can be prevented.

[実施例1] 本実施例の人体検出装置は構成的には第5図に示す従来
の人体検出装置と同じで、本実施例の場合には判定部5
による人体Mの存在判定方法に特徴を有するものである
。なお、以下の説明では赤外線検出素子を4個用いた場
合について説明するが、赤外線検出素子の個数が4@以
外の場合であっても本発明を適用できる。
[Example 1] The human body detection device of this example is structurally the same as the conventional human body detection device shown in FIG.
This method is characterized by a method for determining the presence of a human body M according to the present invention. In addition, although the following description explains the case where four infrared detecting elements are used, the present invention can be applied even when the number of infrared detecting elements is other than four.

まず、本実施例の具体的な構成に関して説明を加えてお
く。本実施例では赤外線検出素子としては常温で動作可
能で安価な焦電素子を用いである。
First, a description will be added regarding the specific configuration of this embodiment. In this embodiment, an inexpensive pyroelectric element that can operate at room temperature is used as the infrared detection element.

なお、焦電素子の他にはサーモパイルを用いることもで
きる。光学系1としては、ミラーまたはレンズを用い、
さらに具体的には多分割ミラーや多分割レンズを用いで
ある。赤外線検出素子A−Dは、光学系1の焦点面上に
配置してあり、背景上には光学系1を通して4つの検知
領域A゛〜D゛が赤外#!検出素子A−Dの配置と同じ
配置で形成されることになる。ここで、検知領域A゛〜
D゛をに体Mが通過すると、各赤外線検出素子A−Dか
らは人体Mと背景との温度差の変化に応じた出力が生じ
る。信号処理部4は帯域フィルタ、マルチプレクサ及び
A/D変換器で構成され、帯域フィルタにて赤外線検出
素子A−Dの出力における必要な周波数成分のみを抽出
し、マルチプレクサ及びA/D変換器により帯域フィル
タを通過した各々の赤外線検出素子A−Dの出力を順次
A/D変換する。判定部5では信号処理部4で処理され
た赤外線検出素子A−Dの各出力から出力時刻L^〜1
゜及びピーク値V、〜vDを求め、上述した(1)、(
2)式の判定条件を満足するか否かを判定する。
Note that a thermopile can also be used in addition to the pyroelectric element. As the optical system 1, a mirror or lens is used,
More specifically, a multi-segment mirror or a multi-segment lens is used. The infrared detecting elements A-D are arranged on the focal plane of the optical system 1, and on the background, through the optical system 1, four detection areas A''-D'' are infrared #! It will be formed in the same arrangement as the arrangement of detection elements A to D. Here, the detection area A~
When the body M passes through D, each of the infrared detection elements A to D generates an output corresponding to a change in the temperature difference between the human body M and the background. The signal processing unit 4 is composed of a bandpass filter, a multiplexer, and an A/D converter. The outputs of each of the infrared detection elements A to D that have passed through the filter are sequentially A/D converted. The determination unit 5 determines the output time L^~1 from each output of the infrared detection elements A to D processed by the signal processing unit 4.
° and the peak values V, ~vD were determined, and the above-mentioned (1), (
2) Determine whether the determination condition of the expression is satisfied.

ところで、本実施例の場合には次のようにして赤外線検
出素子A−Dの出力時刻を判定部5が検出する。例えば
、赤外線検出素子A−Dの出力が第1図に示すように変
化したとすると、判定部5では赤外線検出素子A−Dの
出力が生じたと判定する判定値vthを越えるまでの各
出力の変化の増減方向が反転した最新の時点を出力時刻
であると判定する。具体的には、赤外線検出素子A−D
の出力変化の傾きを求め、その傾きの極性が反転した時
刻を記憶していく。なお、極性反転時には前回記憶した
時刻は梢去して、新たな極性反転時刻を記憶していく。
By the way, in the case of this embodiment, the determination unit 5 detects the output times of the infrared detection elements A to D in the following manner. For example, if the outputs of the infrared detecting elements A-D change as shown in FIG. The latest point in time at which the direction of increase/decrease in change is reversed is determined to be the output time. Specifically, infrared detection elements A-D
The slope of the output change is determined, and the time when the polarity of the slope reverses is memorized. In addition, at the time of polarity reversal, the previously stored time is deleted and a new polarity reversal time is stored.

そして、赤外線検出素子A−Dの出力が所定電圧Vth
を越えた時点で、そのときに記憶しである時刻(第1図
の場合にはts)を出力時刻t^〜tOであると判定す
る。このようにすれば、赤外線検出素子A−Dの出力が
生じたことを判定する判定値vthを比較的に高くする
ことができ、このため雑音による誤動作を防止できる。
Then, the output of the infrared detection elements A-D is set to a predetermined voltage Vth.
At the point in time when the time exceeds , the time stored at that time (ts in the case of FIG. 1) is determined to be the output time t^-tO. In this way, the determination value vth for determining whether the output of the infrared detection elements A to D has occurred can be made relatively high, and therefore malfunctions due to noise can be prevented.

つまり、雑音はそのピーク値が低いので、上述のように
して除去できるのである。また、出力時刻は赤外線検出
素子A−Dの出力の変化の増減方向が反転した時点から
検出しているので、赤外線検出素子A〜Dの出力が生じ
たこととを検出する場合と別個に確実に検出できる。な
お、その出力時刻の検出後の人体Mの存在判定は、上述
した第5図従来例と同様にして判定条件を満たすか否か
によって行う。
In other words, since noise has a low peak value, it can be removed as described above. In addition, since the output time is detected from the point in time when the increase/decrease direction of the change in the output of the infrared detection elements A to D is reversed, it can be reliably determined separately from the case where the output of the infrared detection elements A to D is detected. can be detected. The presence of the human body M after the output time is detected is determined based on whether or not the determination conditions are met in the same manner as in the conventional example shown in FIG.

[実施例2] 本実施例は第1の実施例と出力時刻の検出方法が異なる
もので、上述した第1の実施例では判定部が赤外線検出
素子A−Dの出力が生じたと判定する判定値を越えるま
での各出力の変化の増減方向が反転した最新の時点を出
力時刻であると判定するものであったが、本実施例では
それに加えて赤外線検出素子A−Dの出力が生じたと判
定する判定値を越えるまでの最新の各出力の変化の増減
割合が増大した時点も出力時刻と判定するようにしたも
のである。具体的には、本実施例では赤外線検出素子A
−Dの出力が生じるまでは、第1の実施例と同様にして
出力変化の傾きを求め、傾きの極性が反転した時点と傾
きの絶対値が前回値を上回った時点とを更新して記憶し
ていき、赤外線検出素子A−Dの出力が判定値Vthを
越えた時点で記憶している時刻を出力時刻とする。従っ
て、第2図の場合には判定部5は出力の変化の増減割合
が増大した時点t)、を出力時刻と判定する。本実施例
の場合にも第1の実施例と同様の効果が得られる。
[Example 2] This example differs from the first example in the method of detecting the output time. In the first example described above, the determination unit determines that the output of the infrared detection elements A-D has occurred. The latest point in time when the direction of increase/decrease in each output until it exceeds the value is reversed is determined to be the output time, but in this embodiment, in addition to that, the output time of the infrared detection elements A to D is determined to have occurred. The output time is also determined at the time when the increase/decrease rate of the latest change in each output increases until the determination value is exceeded. Specifically, in this example, the infrared detection element A
-D until the output is generated, the slope of the output change is determined in the same manner as in the first embodiment, and the time when the polarity of the slope is reversed and the time when the absolute value of the slope exceeds the previous value are updated and stored. Then, the time stored at the time when the output of the infrared detection elements A to D exceeds the determination value Vth is set as the output time. Therefore, in the case of FIG. 2, the determination unit 5 determines the time point t) at which the rate of increase/decrease in the output change increases as the output time. In the case of this embodiment as well, the same effects as in the first embodiment can be obtained.

(発明の効果1 本発明は上述のように、判定部が赤外線検出素子の出力
が生じたと判定する判定値を越えるまでの各出力の変化
の増減方向が反転した最新の時点を出力時刻であると判
定しているので、赤外線検出素子の出力が生じたことの
判定を雑音を除去て゛きる比較的に高い判定値で行って
雑音による誤動作を防止できる。
(Advantageous Effect 1 of the Invention As described above, in the present invention, the output time is the latest point in time at which the direction of increase/decrease in the change in each output is reversed until the determination unit exceeds the determination value at which it determines that the output of the infrared detection element has occurred. Therefore, it is possible to determine whether the output of the infrared detection element has occurred using a relatively high determination value that can eliminate noise, thereby preventing malfunctions due to noise.

また、判定部が赤外線検出素子の出力が生じたと判定す
る判定値を越えるまでの各出力の変化の増減割合が増大
した最新の時点を出力時刻と判定しても、赤外線検出素
子の出力が生じたことの判定を雑音を除去できる比較的
に高い判定値で行って、雑音による誤動作を防止できる
Furthermore, even if the determination unit determines as the output time the latest point in time at which the increase/decrease rate of change in each output increases until it exceeds the determination value for determining that the output of the infrared detection element has occurred, the output of the infrared detection element has not occurred. By using a relatively high judgment value that can remove noise, malfunctions due to noise can be prevented.

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

第1図は本発明の一実施例の出力時刻の検出方法の説明
図、第2図は他の実施例の出力時刻の検出方法の説明図
、第3図は従来例の人体検出方法の説明図、第4図は同
上の出力波形図、第5図は他の従来例の構成を示すブロ
ック図、第6図は同上の人体検出方法の説明図、第7図
は同上の出力波形図、@8図は出力時刻を検出する方法
の説明図、第9図は同上の問題点の説明図である。 5は判定部、A−Dは赤外線検出素子、vthは判定値
である。 代理k 弁理士 石 1)長 七 弊 1 :〆 (0) 第4I7j (b) (C) qへ5Lべ1 第3図 (0) 第6図 弔7 IK+ (b) (C) 第8図
FIG. 1 is an explanatory diagram of an output time detection method according to one embodiment of the present invention, FIG. 2 is an explanatory diagram of an output time detection method according to another embodiment, and FIG. 3 is an explanatory diagram of a conventional human body detection method. 4 is an output waveform diagram same as above, FIG. 5 is a block diagram showing the configuration of another conventional example, FIG. 6 is an explanatory diagram of the human body detection method same as above, FIG. 7 is an output waveform diagram same as above, @Figure 8 is an explanatory diagram of the method of detecting the output time, and Figure 9 is an explanatory diagram of the same problem. 5 is a determination unit, A-D is an infrared detection element, and vth is a determination value. Deputy k Patent attorney Ishi 1) Chief Shichie 1:〆(0) 4I7j (b) (C) q 5Lbe1 Figure 3 (0) Figure 6 Condolence 7 IK+ (b) (C) Figure 8

Claims (2)

【特許請求の範囲】[Claims] (1)複数の検知領域で構成され人体に比べて十分に小
さい領域からの赤外線を各検知領域毎に夫々受光する複
数の赤外線検出素子と、これら赤外線検出素子の各出力
のピーク値が略一定であり、且つ各出力の出力時刻に所
定範囲のばらつきがある場合に人体が存在すると判定す
る判定部とを備えた人体検出装置において、上記判定部
が赤外線検出素子の出力が生じたと判定する判定値を越
えるまでの各出力の変化の増減方向が反転した最新の時
点を出力時刻であると判定して成る人体検出装置。
(1) Multiple infrared detection elements that are composed of multiple detection areas and receive infrared rays from an area sufficiently small compared to the human body, and the peak value of each output of these infrared detection elements is approximately constant. and a determination unit that determines that a human body is present when the output times of the respective outputs vary within a predetermined range, wherein the determination unit determines that an output of the infrared detection element has occurred. A human body detection device that determines the latest point in time at which the increase/decrease direction of each output change until exceeding the value is reversed to be the output time.
(2)複数の検知領域で構成され人体に比べて十分に小
さい領域からの赤外線を各検知領域毎に夫々受光する複
数の赤外線検出素子と、これら赤外線検出素子の各出力
のピーク値が略一定であり、且つ各出力の出力時刻に所
定範囲のばらつきがある場合に人体が存在すると判定す
る判定部とを備えた人体検出装置において、上記判定部
が赤外線検出素子の出力が生じたと判定する判定値を越
えるまでの各出力の変化の増減割合が増大した最新の時
点を出力時刻と判定して成る人体検出装置。
(2) Multiple infrared detection elements that are composed of multiple detection areas and receive infrared rays from an area sufficiently small compared to the human body, and the peak value of each output of these infrared detection elements is approximately constant. and a determination unit that determines that a human body is present when the output times of the respective outputs vary within a predetermined range, wherein the determination unit determines that an output of the infrared detection element has occurred. A human body detection device that determines the latest point in time at which the rate of change in each output increases until it exceeds the value as the output time.
JP2034207A 1990-02-15 1990-02-15 Human body detection device Expired - Lifetime JPH07104416B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2034207A JPH07104416B2 (en) 1990-02-15 1990-02-15 Human body detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2034207A JPH07104416B2 (en) 1990-02-15 1990-02-15 Human body detection device

Publications (2)

Publication Number Publication Date
JPH03238391A true JPH03238391A (en) 1991-10-24
JPH07104416B2 JPH07104416B2 (en) 1995-11-13

Family

ID=12407714

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2034207A Expired - Lifetime JPH07104416B2 (en) 1990-02-15 1990-02-15 Human body detection device

Country Status (1)

Country Link
JP (1) JPH07104416B2 (en)

Also Published As

Publication number Publication date
JPH07104416B2 (en) 1995-11-13

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