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JPH0216459B2 - - Google Patents
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JPH0216459B2 - - Google Patents

Info

Publication number
JPH0216459B2
JPH0216459B2 JP56048819A JP4881981A JPH0216459B2 JP H0216459 B2 JPH0216459 B2 JP H0216459B2 JP 56048819 A JP56048819 A JP 56048819A JP 4881981 A JP4881981 A JP 4881981A JP H0216459 B2 JPH0216459 B2 JP H0216459B2
Authority
JP
Japan
Prior art keywords
output
infrared
outputs
circuit
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.)
Expired - Lifetime
Application number
JP56048819A
Other languages
Japanese (ja)
Other versions
JPS57161626A (en
Inventor
Shozo Tanaka
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 JP56048819A priority Critical patent/JPS57161626A/en
Publication of JPS57161626A publication Critical patent/JPS57161626A/en
Publication of JPH0216459B2 publication Critical patent/JPH0216459B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G08SIGNALLING
    • G08BSIGNALLING SYSTEMS, e.g. PERSONAL CALLING SYSTEMS; ORDER TELEGRAPHS; ALARM SYSTEMS
    • G08B13/00Burglar, theft or intruder alarms
    • G08B13/18Actuation by interference with heat, light, or radiation of shorter wavelength; Actuation by intruding sources of heat, light, or radiation of shorter wavelength
    • G08B13/189Actuation by interference with heat, light, or radiation of shorter wavelength; Actuation by intruding sources of heat, light, or radiation of shorter wavelength using passive radiation detection systems
    • G08B13/19Actuation by interference with heat, light, or radiation of shorter wavelength; Actuation by intruding sources of heat, light, or radiation of shorter wavelength using passive radiation detection systems using infrared-radiation detection systems

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Radiation Pyrometers (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Burglar Alarm Systems (AREA)

Description

【発明の詳細な説明】 この発明は赤外エネルギーの変化に応動する赤
外線検知素子を用いて、人体から発せられる赤外
線を検知し侵入者を検出しようとするものであ
る。
DETAILED DESCRIPTION OF THE INVENTION This invention attempts to detect an intruder by detecting infrared rays emitted from a human body using an infrared detection element that responds to changes in infrared energy.

赤外線検知素子を用いた侵入検知装置は従来よ
り知られている。第1図イ,ロに示す従来例は、
放物面反射鏡Aの焦点の近くに上下方向に2個の
赤外線検知素子B,Cを位置させ、この赤外線検
知素子B,Cの出力が逆極性となるような接続を
するとともに、その出力を増巾D,D′し、その
出力をレベル検知回路E,E′を介して出力するよ
うにし、両赤外線検知素子B,Cが同時に所定レ
ベル以上の出力を出したときのみ作動するように
した侵入検知器である。
Intrusion detection devices using infrared detection elements have been known for some time. The conventional example shown in Figure 1 A and B is as follows:
Two infrared sensing elements B and C are located vertically near the focal point of the parabolic reflector A, and are connected so that the outputs of these infrared sensing elements B and C have opposite polarities, and their outputs are are amplified in width D and D', and their outputs are outputted through level detection circuits E and E', so that they are activated only when both infrared detection elements B and C simultaneously output an output of a predetermined level or higher. It is an intrusion detector.

この従来例においては、両赤外線検知素子を逆
極性としているために信号処理回路内の成分から
発生する雑音や、電源ノイズによる誤動作は排除
することができるけれども、両赤外線検知素子が
同時に出力したときのみ作動する構成となつてい
るので、例えば検知器の近くで白熱電灯が点灯す
るとか、太陽光が入射するなどして両検知素子に
同時に赤外エネルギーが入射するような場合誤動
作することとなる。
In this conventional example, since both infrared sensing elements have opposite polarities, it is possible to eliminate noise generated from components in the signal processing circuit and malfunctions due to power supply noise, but when both infrared sensing elements output simultaneously, Since the structure is such that infrared energy is incident on both detection elements at the same time, such as when an incandescent light is turned on near the detector or when sunlight enters, it may malfunction. .

この発明は上記する欠点を改善することを目的
としたものである。
This invention aims to improve the above-mentioned drawbacks.

以下にこの発明赤外線検知器の一実施例にもと
づき詳細に説明する。
An embodiment of the infrared detector of the present invention will be described in detail below.

図において、1は光学系を構成する放物面反射
鏡である。この光学系1は放物面反射鏡でなくと
もよく例えば半放物面反射鏡であつてもよい。
2,3は赤外線検知素子、例えば焦電素子であつ
て赤外線が入射すれば電圧を発生する素子であ
る。この焦電素子2,3は人の移動方向Pに対し
て平行となるように配列されている。したがつて
P方向に移動する人体から発せられる赤外線は、
焦電素子3の受熱範囲4を通過するので焦電素子
3から出力がでる。次いで受熱範囲5を通過する
ので焦電素子2から出力がでる。この2個の焦電
素子2,3の出力を信号処理回路13に入力す
る。この信号処理回路13は増巾回路6と波形整
形回路8と積分および合成回路14と出力回路と
から構成される。そこで前記2個の焦電素子2,
3の出力を増巾器6に入力する。このとき焦電素
子2と3の出力が逆極性になるように接続する。
したがつて増巾器6の出力端7には第5図iに示
すごとく波形aで示す出力が出る。この出力を波
形整形回路8例えば第6図に示すごとくウインド
コンパレーターに入力する。入力Vxが所定レベ
ルVaより大のときはコンパレーター9から入力
Vxが所定レベルVbより小のときはコンパレータ
ー10から矩形波が出力される(第5図,左
欄参照)。この各々の出力を積分回路11,1
1′で積分し合成回路12で合成する。例えば第
7図に示すごとく充電用コンデンサーC1,C2
両端電圧VFが合成電圧出力である。このコンデ
ンサーC1,C2の両端を短絡するトランジスター
Tr1,Tr2のベースB1,B2に前記ウインドコンパ
レーターの両出力を反転して入力するように構成
する。このようにすることにより、トランジスタ
ーTr1,Tr2は波形整形回路8の出力があるとき
不導通状態となり、コンデンサーC1又はC2を充
電する。この合成出力が電圧VG以上となると出
力が出る。
In the figure, numeral 1 is a parabolic reflector that constitutes the optical system. This optical system 1 does not need to be a parabolic reflector and may be, for example, a semi-parabolic reflector.
2 and 3 are infrared detection elements, such as pyroelectric elements, which generate voltage when infrared rays are incident thereon. The pyroelectric elements 2 and 3 are arranged parallel to the moving direction P of the person. Therefore, the infrared rays emitted from a human body moving in the P direction are
Since it passes through the heat receiving range 4 of the pyroelectric element 3, an output is output from the pyroelectric element 3. Then, since it passes through the heat receiving range 5, an output is output from the pyroelectric element 2. The outputs of these two pyroelectric elements 2 and 3 are input to the signal processing circuit 13. This signal processing circuit 13 is comprised of an amplification circuit 6, a waveform shaping circuit 8, an integration and synthesis circuit 14, and an output circuit. Therefore, the two pyroelectric elements 2,
3 is input to the amplifier 6. At this time, the pyroelectric elements 2 and 3 are connected so that their outputs have opposite polarities.
Therefore, at the output terminal 7 of the amplifier 6, an output shown by a waveform a is produced as shown in FIG. 5i. This output is input to a waveform shaping circuit 8, for example, a window comparator as shown in FIG. When the input Vx is higher than the predetermined level Va, input from comparator 9.
When Vx is lower than the predetermined level Vb, a rectangular wave is output from the comparator 10 (see the left column of FIG. 5). The outputs of each of these are integrated into integration circuits 11 and 1.
1' and synthesized by a synthesis circuit 12. For example, as shown in FIG. 7, the voltage VF across charging capacitors C 1 and C 2 is a composite voltage output. A transistor that shorts both ends of this capacitor C 1 and C 2
The configuration is such that both outputs of the window comparator are inverted and inputted to the bases B 1 and B 2 of Tr 1 and Tr 2 . By doing so, the transistors Tr 1 and Tr 2 become non-conductive when there is an output from the waveform shaping circuit 8, and charge the capacitor C 1 or C 2 . When this combined output exceeds the voltage VG, an output is generated.

次いで電源ノイズが同極性に時間おくれをもつ
て発生する場合(第5図右欄波形b参照)、マ
イナス側波形が存在しないため、積分合成出力は
レベルVGを越えることがなく出力が出ない。ま
た照明や太陽光の場合、両赤外線検知素子2,3
に同時に赤外エネルギーが供給されるため両素子
の出力はちようどキヤンセルされて出力がないの
と同じこととなり誤動作にはいたらない。
Next, when power supply noise occurs with the same polarity and a time lag (see waveform b in the right column of Figure 5), since there is no negative side waveform, the integrated and synthesized output does not exceed level VG and no output is produced. In addition, in the case of lighting or sunlight, both infrared detection elements 2 and 3
Since infrared energy is supplied to both elements at the same time, the outputs of both elements are cancelled, which is the same as no output, and no malfunction occurs.

なお第8図は、焦電素子2,3の出力をそれぞ
れ別々に増巾回路6′,6″に入力する場合の実施
例を示したものである。なお赤外線検知素子とし
て半導体赤外線センサーを用いた場合は電源電圧
をこの半導体赤外線センサーと抵抗で分圧し、こ
の分圧点の電圧を増巾回路に入力することとな
る。
Note that FIG. 8 shows an embodiment in which the outputs of the pyroelectric elements 2 and 3 are input to the amplification circuits 6' and 6'' separately. Note that a semiconductor infrared sensor is used as the infrared detection element. If so, the power supply voltage will be divided by this semiconductor infrared sensor and the resistor, and the voltage at this voltage division point will be input to the amplification circuit.

上記する如く本願発明によれば人の通過方向に
対してその検知領域が間隔をもつて配列された2
個の赤外線検知素子に時間的に差異をもつて人体
からの赤外線が集められるようにした光学系と、
前記2個の赤外線検知素子の出力を互いに逆極性
となるように接続するとともにこの赤外線検知素
子の出力波形を波形整形した後各々積分回路によ
り積分し、この各々の積分回路の出力を同極とな
るように合成し、この合成回路の出力が所定のレ
ベル以上であれば出力を出すようにした信号処理
回路とよりなる赤外線検知器としたので、侵入者
の検知は確実に行うことができ、電源ノイズなど
の電気的ノイズに対しても誤動作せず、また照明
の点灯や太陽光によつても誤動作しない信頼性の
高い赤外線検知器が得られる。
As described above, according to the present invention, the detection areas are arranged at intervals in the direction of passage of the person.
an optical system that allows infrared rays from the human body to be collected at different infrared detection elements at different times;
The outputs of the two infrared detecting elements are connected so that they have opposite polarities, and the output waveforms of the infrared detecting elements are waveform-shaped and then integrated by respective integrating circuits. The infrared detector is made up of a signal processing circuit that synthesizes signals so that the intruder is detected, and outputs an output if the output of this synthesis circuit exceeds a predetermined level, making it possible to reliably detect intruders. It is possible to obtain a highly reliable infrared detector that does not malfunction due to electrical noise such as power supply noise, and does not malfunction even when exposed to lighting or sunlight.

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

第1図イ,ロは本願発明の従来例を示し、第1
図イは光学系Aで赤外線検知素子B,C上に集熱
する手段の模式図、同図ロはその信号処理回路図
を示す。第2図乃至第8図は本願発明の一実施例
を説明する図面であつて、第2図は光学系の模式
図、第3図はブロツク図、第4図は増巾回路6の
回路図、第5図は第3図における各回路の出力波
形、第6図乃至第8図は電気回路図を示す。
Figures 1A and 1B show conventional examples of the present invention;
Figure A is a schematic diagram of a means for concentrating heat onto infrared detecting elements B and C in optical system A, and Figure B is a signal processing circuit diagram thereof. 2 to 8 are drawings for explaining one embodiment of the present invention, in which FIG. 2 is a schematic diagram of the optical system, FIG. 3 is a block diagram, and FIG. 4 is a circuit diagram of the amplifier circuit 6. , FIG. 5 shows the output waveforms of each circuit in FIG. 3, and FIGS. 6 to 8 show electrical circuit diagrams.

Claims (1)

【特許請求の範囲】[Claims] 1 人の通過方向に対してその検知領域が間隔を
もつて配列された2個の赤外線検知素子に時間的
に差異をもつて人体からの赤外線が集められるよ
うにした光学系と、前記2個の赤外線検知素子の
出力を互いに逆極性となるように接続するととも
にこの赤外線検知素子の出力波形を波形整形した
後各々積分回路により積分し、この各々の積分回
路の出力を同極となるように合成し、この合成回
路の出力が所定のレベル以上であれば出力を出す
ようにした信号処理回路とよりなる赤外線検知
器。
1. An optical system that collects infrared rays from a human body at different times on two infrared detecting elements whose detection areas are arranged at intervals in the direction in which the person passes; The outputs of the infrared sensing elements are connected so that they have opposite polarities, and the output waveforms of these infrared sensing elements are waveform-shaped and then integrated by each integrating circuit, so that the outputs of each integrating circuit have the same polarity. An infrared detector consisting of a signal processing circuit that performs synthesis and outputs an output if the output of the synthesis circuit exceeds a predetermined level.
JP56048819A 1981-03-31 1981-03-31 Infrared detector Granted JPS57161626A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56048819A JPS57161626A (en) 1981-03-31 1981-03-31 Infrared detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56048819A JPS57161626A (en) 1981-03-31 1981-03-31 Infrared detector

Publications (2)

Publication Number Publication Date
JPS57161626A JPS57161626A (en) 1982-10-05
JPH0216459B2 true JPH0216459B2 (en) 1990-04-17

Family

ID=12813824

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56048819A Granted JPS57161626A (en) 1981-03-31 1981-03-31 Infrared detector

Country Status (1)

Country Link
JP (1) JPS57161626A (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59195179A (en) * 1983-04-20 1984-11-06 Uro Denshi Kogyo Kk Alarming device for intruder
JPS6023991A (en) * 1983-05-09 1985-02-06 榎本 正実 Automatic firing and extinguishing lamp illuminator
JPS60140173A (en) * 1983-12-28 1985-07-25 Denki Onkyo Co Ltd Pyroelectric infrared device
JPH0422319Y2 (en) * 1985-12-23 1992-05-21
JPH0641884B2 (en) * 1986-03-07 1994-06-01 松下電器産業株式会社 Radiation detector
JPS62232097A (en) * 1986-04-01 1987-10-12 セントラル警備保障株式会社 Invader detection for alarming/monitoring system
JP2603616B2 (en) * 1986-06-02 1997-04-23 オムロン株式会社 Reflective photoelectric switch

Also Published As

Publication number Publication date
JPS57161626A (en) 1982-10-05

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