JP2013072835A - Flame sensor and method for determining flame - Google Patents

Flame sensor and method for determining flame Download PDF

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JP2013072835A
JP2013072835A JP2011214082A JP2011214082A JP2013072835A JP 2013072835 A JP2013072835 A JP 2013072835A JP 2011214082 A JP2011214082 A JP 2011214082A JP 2011214082 A JP2011214082 A JP 2011214082A JP 2013072835 A JP2013072835 A JP 2013072835A
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Yoshio Nakamura
嘉夫 中村
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Hochiki Corp
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Abstract

PROBLEM TO BE SOLVED: To provide a flame sensor that reliably discriminates flames and activates a fire alarm without a malfunction due to arc welding light, by enhancing the discriminability between flames and arc welding light.SOLUTION: A first optical filter 14a selectively transmits light that is emitted by COresonance generated in flame combustion and has a narrow band of wavelength with the center wavelength of about 4.5 μm. A first light receiving element 16a converts the light into an electric signal to output a 4.5 μm light reception signal e1. A second optical filter 14b transmits light of a near-infrared wavelength band of 0.7 to 1.0 μm included in arc welding light. A second light receiving element 16b converts the light into an electric signal to output a near-infrared light reception signal e2. A flame determination part 26 discriminates and determines the presence of flames and a radiation source of arc welding light on the basis of the 4.5 μm light reception signal e1 and corrected near-infrared light reception signal e2 that is delayed by a predetermined time Td to correct time deviation, and when determining the presence of flames, operates an alarm circuit 28 to output a fire alarm signal.

Description

本発明は、火災に伴う炎を検知して発報する炎感知器及び炎判定方法に関する。
The present invention relates to a flame detector and a flame determination method for detecting and reporting a flame associated with a fire.

従来、有炎燃焼により発生する赤外線放射を検出して、炎の有無を検出する炎感知器にあっては、炎と炎以外の赤外線放射体との識別を行うため、有炎燃焼時に発生するCO2の共鳴放射による波長帯域を含む複数の波長帯域における放射強度を検出して、それら複数の波長帯域における検出値の相対比により炎の有無を検出する2波長式、3波長式等の炎検出装置や炎検出方法がよく知られている。 Conventionally, in a flame detector that detects the presence or absence of flame by detecting infrared radiation generated by flaming combustion, it is generated at the time of flaming combustion in order to distinguish between flames and infrared radiators other than flame. Two-wavelength, three-wavelength, etc. flames that detect radiation intensities in a plurality of wavelength bands including a wavelength band due to resonance emission of CO 2 and detect the presence or absence of flames by a relative ratio of detection values in the plurality of wavelength bands Detection devices and flame detection methods are well known.

従来技術の2波長式や3波長式の炎感知器の検出原理は次のようになる。燃焼炎においては、CO2の共鳴放射により4.5μm付近の波長帯域に放射強度のピークがあり、また、このピーク波長の近傍に存在する特徴的な波長としては、例えば、短波長側の3.8μm付近や長波長側の5.1μmに、放射強度が低い波長帯域が存在する。 The detection principle of the conventional two-wavelength or three-wavelength flame detector is as follows. In the combustion flame, there is a peak of radiation intensity in the wavelength band near 4.5 μm due to the resonance radiation of CO 2 , and the characteristic wavelength existing in the vicinity of this peak wavelength is, for example, 3 on the short wavelength side. A wavelength band with low radiation intensity exists in the vicinity of .8 μm and 5.1 μm on the long wavelength side.

なお、放射源としての炎はCO2の共鳴放射により、4.3μm帯に赤外線の放射強度のピークがあることが知られている。しかしながら、炎感知器は放射源から離れた位置で炎からの放射エネルギーを検知しており、このため炎感知器の設置場所で実際に測定した場合にあっては、4.5μm付近に放射強度のピークが現れることが経験的に示されている。したがって、以下では、特に断らない限り、CO2共鳴放射帯とは、4.5μm帯を指すものとする。 It is known that a flame as a radiation source has a peak of infrared radiation intensity in the 4.3 μm band due to CO 2 resonance radiation. However, the flame detector detects the radiant energy from the flame at a position away from the radiation source. For this reason, when actually measured at the place where the flame detector is installed, the radiation intensity is around 4.5 μm. It has been empirically shown that the peak appears. Therefore, hereinafter, unless otherwise specified, the CO 2 resonance radiation band refers to the 4.5 μm band.

このため2波長式の炎感知器にあっては、4.5μm付近の波長帯域と、例えば3.8μm付近の波長帯域における各々の放射エネルギーを狭帯域の光学波長バンドパスフィルタにより選択透過(通過)させて、受光素子により該放射エネルギーを検出して対応する電気信号に変換し、それぞれの検出出力の相対比をとり、所定の閾値と比較することにより炎と判定する。これにより、炎以外の赤外線放射体、例えば、太陽光等の高温放射体や、300°C程度の比較的低温の放射体、人体などの低温放射体等との識別が可能となる。   For this reason, in a two-wavelength flame detector, each radiant energy in a wavelength band near 4.5 μm and a wavelength band near 3.8 μm, for example, is selectively transmitted (passed) by a narrow band optical wavelength bandpass filter. And detecting the radiant energy by the light receiving element and converting it into a corresponding electric signal, taking the relative ratio of the respective detection outputs, and comparing with a predetermined threshold value to determine a flame. This makes it possible to distinguish from infrared radiators other than flames, for example, high-temperature radiators such as sunlight, relatively low-temperature radiators of about 300 ° C., low-temperature radiators such as human bodies, and the like.

また3波長式の炎感知器にあっては、上述した2波長に加え、CO2の共鳴放射帯である4.5μm帯の長波長側の、例えば、5.1μm付近の波長帯域における放射エネルギーを、上記2波長式と同様の手法で検出し、これらの3波長帯域における検出出力の相対比によって炎の有無を判定しており、このような炎検出方法により、炎と炎以外の赤外線放射体との識別性能をさらに向上させることができる。
In addition, in the case of a three-wavelength flame detector, in addition to the two wavelengths described above, the radiation energy in the long wavelength side of the 4.5 μm band, which is the resonance radiation band of CO 2 , for example, in the wavelength band near 5.1 μm. Is detected by the same method as the above-mentioned two-wavelength type, and the presence or absence of flame is determined by the relative ratio of the detection outputs in these three wavelength bands. With such a flame detection method, infrared radiation other than flame and flame is emitted. The identification performance with the body can be further improved.

特公昭55−33119号公報Japanese Patent Publication No.55-33119 特公昭59−34252号公報Japanese Patent Publication No.59-34252

しかしながら、このような従来の炎感知器を工場等に設置していた場合に、アーク溶接作業により炎感知器が誤作動してしまう問題がある。   However, when such a conventional flame detector is installed in a factory or the like, there is a problem that the flame detector malfunctions due to arc welding work.

これはアーク溶接の溶接光には、有炎燃焼時に発生するCO2の共鳴放射による4.5μm付近の赤外線が含まれていることによる。例えばアーク溶接に使用する溶接棒の被覆には、でんぷんなどの有機物が成分として含まれており、有機物が燃焼することで4.5μm付近の赤外線が放射CO2の共鳴放射により出ているほか、高温となっている溶接部位から黒体放射によっても出ており、従来の炎感知器では判別が難しく、アーク溶接光により誤作動するという問題がある。 This is because the arc welding light includes infrared rays in the vicinity of 4.5 μm due to resonance emission of CO 2 generated during flammable combustion. For example, the covering of the welding rod used for arc welding contains organic substances such as starch as an ingredient, and in addition to burning the organic substances, infrared rays in the vicinity of 4.5 μm are emitted by resonance radiation of CO 2 , It is also emitted by black body radiation from the welded part that is at a high temperature, and it is difficult to distinguish with conventional flame detectors, and there is a problem that malfunction occurs due to arc welding light.

この問題を解決するため本願出願人にあっては、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光による第1受光信号を検出すると共に、アーク溶接光により放射される、0.7〜1.0μm付近の波長帯域の近赤外線の光による第2受光信号を検出し、第1受光信号と第2受光信号の相対比に基づいて炎とアーク溶接光の放射線源とを識別判定するようにした炎感知器を提案している。 In order to solve this problem, the applicant of the present application detects the first received light signal by light having a narrow band wavelength centered around 4.5 μm, which is radiated by CO 2 resonance generated during flammable combustion. In addition, a second received light signal is detected by near infrared light in the wavelength band near 0.7 to 1.0 μm radiated by arc welding light, and based on the relative ratio of the first received light signal and the second received light signal. A flame detector that distinguishes between a flame and a radiation source of arc welding light is proposed.

しかしながら、このような炎感知器にあっても、タイミングによってはアーク溶接光を火災による炎と誤って認識してしまう可能性があり、その原因の究明による更なる改良を必要としている。   However, even in such a flame detector, there is a possibility that the arc welding light may be mistakenly recognized as a flame due to a fire depending on the timing, and further improvement by investigating the cause is required.

本発明は、炎とアーク溶接光との識別性を高め、アーク溶接光により誤作動することなく確実に炎の存在を判別して火災発報することを可能とする炎感知器及び炎判定方法を提供することを目的とする。
The present invention relates to a flame detector and a flame determination method capable of improving the distinguishability between a flame and arc welding light and reliably determining the presence of a flame without causing malfunction due to the arc welding light and issuing a fire. The purpose is to provide.

(炎感知器)
本発明は、炎感知器に於いて、
有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第1受光信号を出力する第1検知部と、
所定の波長帯域の近赤外線光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第2受光信号を出力する第2検知部と、
第1検知部からの第1受光信号と第2検知部からの第2受光信号との時間的なずれを補正する補正部と、
補正部で時間的なずれが補正された第1受光信号と第2受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定する炎判定部と、
炎判定部で炎の存在を判定した場合に火災信号を出力する発報回路と、
を備えたことを特徴とする。
(Flame detector)
The present invention provides a flame detector,
Narrowband wavelength light centered around 4.5 μm emitted by CO 2 resonance generated during flammable combustion is selectively transmitted and converted into an electrical signal, and a signal component of a predetermined frequency is converted from the electrical signal. A first detector for selectively extracting and outputting a first light receiving signal;
A second detector that selectively transmits near-infrared light in a predetermined wavelength band, converts the light into an electrical signal, selectively extracts a signal component of a predetermined frequency from the electrical signal, and outputs a second received light signal;
A correction unit that corrects a time lag between the first light reception signal from the first detection unit and the second light reception signal from the second detection unit;
A flame determination unit that discriminates the presence of the flame and the radiation source of the arc welding light based on the first light reception signal and the second light reception signal in which the time lag is corrected by the correction unit;
An alarm circuit that outputs a fire signal when the flame determination unit determines the presence of a flame,
It is provided with.

ここで、補正部は、第2検知部からの第2受光信号を所定時間遅延して第1受光信号との時間ずれを抑制する。   Here, the correction unit delays the second light reception signal from the second detection unit by a predetermined time and suppresses a time shift from the first light reception signal.

第1検知部は、
有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過させる第1光学フィルタと、
第1光学フィルタを透過した透過した光を受光し電気信号に変換して出力する第1受光素子と、
第1受光素子の出力から所定の周波数の信号成分を選択抽出して第1受光信号を出力する第1周波数抽出部と、
を備え、
第2検知部は、
所定の波長帯域の近赤外線光を透過させる第2光学フィルタと、
第2光学フィルタを透過した光を受光し電気信号に変換して出力する第2受光素子と、
第2の受光素子の出力から所定の周波数の信号成分を選択抽出して第2受光信号を出力する第2周波数抽出部と、
を備える。
The first detector is
A first optical filter that selectively transmits light having a narrow band wavelength centered around 4.5 μm, which is emitted by CO 2 resonance generated during flammable combustion;
A first light receiving element that receives the transmitted light that has passed through the first optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A first frequency extracting unit that selectively extracts a signal component of a predetermined frequency from the output of the first light receiving element and outputs a first light receiving signal;
With
The second detector
A second optical filter that transmits near-infrared light in a predetermined wavelength band;
A second light receiving element that receives light transmitted through the second optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A second frequency extracting section for selectively extracting a signal component of a predetermined frequency from the output of the second light receiving element and outputting a second light receiving signal;
Is provided.

第2光学フィルタは、0.7μm乃至1.0μm付近(700nm〜1000nm付近)の波長帯域の近赤外線光を透過させる。   The second optical filter transmits near-infrared light having a wavelength band in the vicinity of 0.7 μm to 1.0 μm (near 700 nm to 1000 nm).

第2光学フィルタと第2受光素子は、近赤外帯域の光を透過させる透過窓を備え、近赤外帯域の所定波長にピーク波長を持つフォトトランジスタまたはフォトダイオードである。   The second optical filter and the second light receiving element are a phototransistor or a photodiode that includes a transmission window that transmits light in the near infrared band and has a peak wavelength at a predetermined wavelength in the near infrared band.

炎判定部は、第1受光信号e1と第2受光信号e2との比率K=e1/e2を求め、当該比率が所定の判定閾値Kth以上の場合に炎の存在を判定する。   The flame determination unit obtains a ratio K = e1 / e2 between the first light reception signal e1 and the second light reception signal e2, and determines the presence of flame when the ratio is equal to or greater than a predetermined determination threshold value Kth.

炎判定部は、
第2受光信号e2が所定の受光閾値eth未満の場合は、第1受光信号e1と第2受光信号e2との比率K=e1/e2を求め、
第2受光信号e2が所定の受光閾値eth以上の場合は、第1受光信号e1と、所定の定数cの比率K=e1/cを求め、
比率が所定の判定閾値Kth以上の場合に炎の存在を判定する。
The flame judgment part
When the second light reception signal e2 is less than the predetermined light reception threshold eth, the ratio K = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained.
When the second light reception signal e2 is equal to or greater than a predetermined light reception threshold eth, a ratio K = e1 / c between the first light reception signal e1 and a predetermined constant c is obtained.
The presence of a flame is determined when the ratio is equal to or greater than a predetermined determination threshold value Kth.

本発明の炎感知器は、更に、
有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光のみを選択透過させて電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出する第3検知部と、
を設け、
炎判定部は、第1検知部、第2検知部及び第3検知部からの第1受光信号、第2受光信号及び第3受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定する。
The flame detector of the present invention further includes:
Only light of a narrow band wavelength centered on a predetermined wavelength adjacent to a wavelength band centered on 4.5 μm emitted by CO 2 resonance generated during flammable combustion is selectively transmitted and converted into an electrical signal. A third detector for selectively extracting a signal component of a predetermined frequency from the electrical signal;
Provided,
The flame determination unit determines the presence of the flame and the radiation source of the arc welding light based on the first light reception signal, the second light reception signal, and the third light reception signal from the first detection unit, the second detection unit, and the third detection unit. Identify and judge.

第3検知部は、
4.5μm付近を中心波長とする波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光を選択透過させる第3光学フィルタと、
第3光学フィルタを透過した透過した光を受光し電気信号に変換して出力する第3受光素子と、
第3受光素子の出力から所定の周波数の信号成分を選択抽出して第3受光信号を出力する第3周波数抽出部と、
を備える。
The third detector
A third optical filter that selectively transmits light having a narrowband wavelength centered on a predetermined wavelength adjacent to a wavelength band centered around 4.5 μm;
A third light receiving element that receives the transmitted light that has passed through the third optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A third frequency extracting section for selectively extracting a signal component of a predetermined frequency from the output of the third light receiving element and outputting a third light receiving signal;
Is provided.

第3光学フィルタは、第1光学フィルタの4.5μm付近の透過波長帯域に隣接した3.8μm付近または5.1μm付近を中心波長とする狭帯域波長の光のみを選択透過させる。   The third optical filter selectively transmits only light having a narrow band wavelength centered around 3.8 μm or 5.1 μm adjacent to the transmission wavelength band near 4.5 μm of the first optical filter.

炎判定部は、
第1受光信号e1と第2受光信号e2との第1比率K1=e1/e2を求めると共に第1受光信号e1と第3受光信号e3との第2比率K2=e1/e3を求め、
第1比率K1が所定の第1判定閾値Kth1以上で且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。
The flame judgment part
A first ratio K1 = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained, and a second ratio K2 = e1 / e3 between the first light reception signal e1 and the third light reception signal e3 is obtained,
The presence of flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.

炎判定部は、
第2受光信号e2が所定の受光閾値eth未満の場合は、第1受光信号e1と第2受光信号e2との第1比率K1=e1/e2を求めると共に第1受光信号e1と第3受光信号e3との第2比率K2=e1/e3を求め、
第2受光信号e2が所定の受光閾値eth以上の場合は、第1受光信号e1と所定の定数cとの第1比率K1=e1/cを求めると共に第1受光信号e1と第3受光信号e3との第2比率K2=e1/e3を求め、第1比率K1が所定の第1判定閾値Kth1以上で且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。
The flame judgment part
When the second light reception signal e2 is less than the predetermined light reception threshold eth, a first ratio K1 = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained and the first light reception signal e1 and the third light reception signal are obtained. A second ratio K2 = e1 / e3 with e3 is obtained,
When the second light reception signal e2 is equal to or greater than the predetermined light reception threshold eth, a first ratio K1 = e1 / c between the first light reception signal e1 and the predetermined constant c is obtained and the first light reception signal e1 and the third light reception signal e3. The second ratio K2 = e1 / e3 is determined, and the presence of flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2. .

炎判定部は、第1信号乃至第3受光信号を積分した積分信号に基づいて炎の存在を判定する。   The flame determination unit determines the presence of a flame based on an integrated signal obtained by integrating the first signal to the third light reception signal.

(炎判定方法)
本発明は、炎判定方法に於いて、
第1検知部により、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第1受光信号を出力し、
第2検知部により、所定の波長帯域の近赤外線光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第2受光信号を出力し、
補正部により、第1検知部からの第1受光信号と第2検知部からの第2受光信号との時間的なずれを補正し、
炎判定部により、補正部で時間的なずれが補正された第1受光信号と第2受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することを特徴とする。
(Flame judgment method)
The present invention provides a flame determination method,
The first detector selectively transmits light having a narrow band wavelength centered around 4.5 μm, which is radiated by CO 2 resonance generated during flammable combustion, and converts it into an electrical signal. The first light receiving signal is output by selectively extracting the signal component of the frequency of
The second detector selectively transmits near-infrared light in a predetermined wavelength band and converts it into an electrical signal, selectively extracts a signal component of a predetermined frequency from the electrical signal, and outputs a second received light signal.
The correction unit corrects a time lag between the first light reception signal from the first detection unit and the second light reception signal from the second detection unit,
The flame determination unit discriminates and determines the presence of the flame and the radiation source of the arc welding light based on the first light reception signal and the second light reception signal whose time shift is corrected by the correction unit.

本発明による炎判定方法の他の特徴は、前述した炎感知器の場合と基本的に同じになる。
Other features of the flame determination method according to the present invention are basically the same as those of the flame detector described above.

本発明の炎感知器によれば、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光による第1受光信号(4.5μm受光信号)を検出すると共に、アーク溶接光により放射される、0.7〜1.0μm付近の波長帯域の近赤外線の光による第2受光信号(近赤外受光信号)を検出し(2波長方式)、第1受光信号と第2受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定したため、アーク溶接作業を行う工場等に設置した場合に、アーク溶接光では誤作動せず、また日光、白熱電球、ハロゲンランプ等でも誤作動せず、火災による炎を確実に検知して報知することができる。 According to the flame detector of the present invention, the first light reception signal (4.5 μm light reception signal) is emitted by light having a narrow band wavelength centered around 4.5 μm, which is radiated by CO 2 resonance generated during flammable combustion. And detecting a second light reception signal (near infrared light reception signal) by near infrared light in a wavelength band near 0.7 to 1.0 μm radiated by arc welding light (two-wavelength method), Since the presence of the flame and the radiation source of the arc welding light are identified and determined based on the first light receiving signal and the second light receiving signal, when installed in a factory or the like where arc welding work is performed, the arc welding light does not malfunction. Also, it does not malfunction even with sunlight, incandescent light bulbs, halogen lamps, etc., and it can reliably detect and notify the fire flames.

この場合、タイミングによってはアーク溶接光を火災による炎と誤判定する場合があり、その原因を究明したところ、アーク溶接作業を行った場合に検知される4.5μm付近を中心波長とする狭帯域波長の光による第1受光信号(4.5μm受光信号)と、アーク溶接光により放射される、0.7〜1.0μm付近の波長帯域の近赤外線の光による第2受光信号(近赤外受光信号)との間に時間的なタイミングずれがあり、両者の例えば相対比を求めて炎の存在を判定する場合、両者の時間的なピークタイミングのずれに起因して相対比が大きくなり、炎と誤判定する場合があることが判明した。   In this case, depending on the timing, the arc welding light may be misjudged as a flame due to fire, and when the cause was investigated, a narrow band centered around 4.5 μm detected when arc welding work was performed. A first light reception signal (4.5 μm light reception signal) based on light of a wavelength and a second light reception signal (near infrared light) emitted by arc welding light and near infrared light in a wavelength band near 0.7 to 1.0 μm. When there is a temporal timing difference between the light reception signal) and the presence of the flame by determining the relative ratio between the two, for example, the relative ratio increases due to the temporal peak timing deviation between the two, It turned out that it might be misjudged as a flame.

このような第1受光信号(4.5μm受光信号)と第2受光信号(近赤外受光信号)のピークタイミングの時間ずれは、アーク溶接作業において溶接棒のスパークによる光が最初に発生して近赤外線を含む可視光が放射され、続いて溶接棒の被覆が燃焼してでんぷん等の有機物の燃焼や高温部の黒体放射によるCO2共鳴放射による4.5μm付近にピークをもつ光が放射されることによるものと推定される。 The time difference between the peak timings of the first light receiving signal (4.5 μm light receiving signal) and the second light receiving signal (near infrared light receiving signal) is caused by the first light generated by the spark of the welding rod in the arc welding operation. Visible light including near-infrared radiation is emitted, followed by burning of the coating of the welding rod, and emission of light having a peak in the vicinity of 4.5 μm due to combustion of organic substances such as starch and CO 2 resonance radiation due to high-temperature black body radiation. It is estimated that

そこで本発明にあっては、時間的に早いタイミングで検知される第2受光信号(近赤外受光信号)を所定時間遅延することで、時間的に遅いタイミングで検知される第1受光信号(4.5μm受光信号)との時間的なずれを抑制して両者の相対比を求めることで、アーク溶接光を炎と誤判定してしまうことを確実に防止することができる。   Therefore, in the present invention, the first light receiving signal (detected at a later timing) is delayed by delaying the second light receiving signal (near-infrared received signal) detected at an earlier time in a predetermined time. It is possible to reliably prevent the arc welding light from being erroneously determined as a flame by suppressing the temporal deviation from the 4.5 μm light reception signal) and obtaining the relative ratio between the two.

また、アーク溶接を行う工場等に本発明による炎感知器を設置することで、工場での火災感知を早めることができる。従来、アーク溶接作業を行う工場では、炎感知器が使用できないために、熱感知器を使用している。なお、煙感知器は通常の状態で工場内に煙が発生するので使用できない。工場で熱感知器を使用する場合、熱感知器は高天井に設置されており、火災に伴う熱気流が高天井に届いて熱感知器で火災を検知するまでには時間がかかり、そのあいだに火災が拡大してしまう可能性が高い。しかしながら、アーク溶接光に対し誤作動することのない本発明の炎感知器を使用することで、アーク溶接を行う工場等の高天井に設置していても火災による炎を早期に検知することができ、火災が大きくなってしまう前に火災を報知することができる。   In addition, by installing the flame detector according to the present invention in a factory where arc welding is performed, fire detection in the factory can be accelerated. Conventionally, in a factory where arc welding work is performed, a flame detector cannot be used, so a heat detector is used. The smoke detector cannot be used because smoke is generated in the factory under normal conditions. When using a heat sensor in a factory, the heat sensor is installed on the high ceiling, and it takes time until the thermal airflow accompanying the fire reaches the high ceiling and the fire is detected by the heat sensor. There is a high possibility that the fire will spread. However, by using the flame detector of the present invention that does not malfunction with respect to arc welding light, it is possible to detect fire flames early even if installed on a high ceiling in a factory or the like where arc welding is performed. It is possible to notify the fire before it becomes large.

また、有炎燃焼によるCO2共鳴で放射される、4.5μm付近の光による第1受光信号と、アーク溶接光による、0.7〜1.0μm付近の近赤外線光による第2受光信号をとの比率を求めることで、炎の場合に求めた比率を、アーク溶接光の場合に求めた比率に対し、充分に大きな値とすることができ、両者の差を大きくすることで、炎の存在とアーク溶接光の放射線源とを識別判定をより正確にできる。 In addition, a first light reception signal by light near 4.5 μm radiated by CO 2 resonance due to flammable combustion and a second light reception signal by near infrared light near 0.7 to 1.0 μm by arc welding light. The ratio obtained in the case of flame can be made sufficiently large with respect to the ratio obtained in the case of arc welding light, and by increasing the difference between the two, It is possible to more accurately discriminate the presence and the radiation source of the arc welding light.

また、アーク溶接光(外乱光)や照明、太陽光による、0.7〜1.0μm付近の近赤外線光の第2受光信号が大きくなりすぎると、有炎燃焼によるCO2共鳴で放射される4.5μm付近の光による第1受光信号との比率が低下して感度が極端に低下する。そこで本発明にあっては、第2受光信号が所定レベルを超えた場合、第2受光信号の代りに所定の定数を使用して第1受光信号との比率を求めることで、外乱光となるアーク溶接光による感度低下を抑制することができる。 In addition, if the second received light signal of near infrared light in the vicinity of 0.7 to 1.0 μm due to arc welding light (disturbance light), illumination, or sunlight becomes too large, it is emitted by CO 2 resonance due to flammable combustion. The ratio with the first received light signal due to light in the vicinity of 4.5 μm is lowered, and the sensitivity is extremely lowered. Therefore, in the present invention, when the second light receiving signal exceeds a predetermined level, disturbance light is obtained by obtaining a ratio with the first light receiving signal by using a predetermined constant instead of the second light receiving signal. Sensitivity deterioration due to arc welding light can be suppressed.

また、CO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光による第1受光信号、アーク溶接光に固有な0.7〜1.0μm付近となる近赤外線の光による第2受光信号の検出に加え、CO2共鳴による4.5μm付近に隣接した3.8μm付近または5.1μm付近を中心波長とする狭帯域波長の光による第3受光信号を検出し((3波長方式)、第1受光信号、第2受光信号及び第3受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することで、工場などに炎感知器を設置した場合にアーク溶接作業を行っても誤作動せず、また日光、白熱電球、ハロゲンランプ等でも誤作動せず、火災による炎を更に確実に検知して報知することができる。
Further, the first received light signal by the light having a narrow band wavelength centered around 4.5 μm, which is emitted by CO 2 resonance, and the near infrared light having a wavelength of 0.7 to 1.0 μm inherent to the arc welding light. In addition to the detection of the second received light signal by, the third received light signal is detected by light having a narrow band wavelength centered around 3.8 μm or 5.1 μm adjacent to the vicinity of 4.5 μm due to CO 2 resonance (( When a flame detector is installed in a factory or the like by identifying and determining the presence of a flame and the radiation source of arc welding light based on the three-wavelength method), the first light-receiving signal, the second light-receiving signal, and the third light-receiving signal Even if arc welding work is performed, malfunction does not occur, nor does it malfunction even in sunlight, incandescent light bulbs, halogen lamps, etc., and it is possible to more reliably detect and report a fire flame.

2波長方式となる本発明による炎感知器の実施形態を示したブロック図The block diagram which showed embodiment of the flame detector by this invention used as a 2 wavelength system 図1の炎判定部の機能構成を示したブロック図The block diagram which showed the function structure of the flame determination part of FIG. 時間的なタイミングずれを持つ近赤外受光信号と4.5μm受光信号と両者の相対比の時間変化を示したタイムチャートTime chart showing temporal changes in the relative ratio between near-infrared light reception signal and 4.5 μm light reception signal with temporal timing shift 時間的なタイミングずれ補償した近赤外受光信号と4.5μm受光信号と両者の相対比の時間変化を示したタイムチャートTime chart showing temporal changes in the relative ratio between near-infrared light receiving signal and 4.5 μm light receiving signal compensated for temporal timing deviation 断続的な溶接作業を行った場合の近赤外受光信号と4.5μm受光信号の実測データを示したタイムチャートTime chart showing measured data of near-infrared light reception signal and 4.5μm light reception signal when intermittent welding work is performed 図2の炎判定部における近赤外受光信号と4.5μm受光信号の時間ずれを補正した積分処理を示した説明図Explanatory drawing which showed the integration process which correct | amended the time shift of the near-infrared light reception signal and 4.5 micrometer light reception signal in the flame determination part of FIG. 図2の炎判定部をプロセッサのプログラム制御で実現する場合の炎判定処理を示したフローチャートThe flowchart which showed the flame determination process in the case of implement | achieving the flame determination part of FIG. 2 by the program control of a processor 炎とアーク溶接光の分光特性を示した放射スペクトル特性図Radiation spectrum diagram showing spectral characteristics of flame and arc welding light アーク溶接光に対する4.5μm積分値と近赤外積分値から算出した比率Kの時間変化を示したタイムチャートTime chart showing time change of ratio K calculated from 4.5 μm integral value and near infrared integral value for arc welding light ヘプタン炎に対する4.5μm積分値と近赤外積分値から算出した比率Kの時間変化を示したタイムチャートTime chart showing time change of ratio K calculated from 4.5μm integral value and near infrared integral value for heptane flame 図1の炎判定部の他の実施形態による機能構成を示したブロック図The block diagram which showed the function structure by other embodiment of the flame determination part of FIG. 図11の炎判定部をプロセッサのプログラム制御で実現する場合の炎判定処理を示したフローチャートThe flowchart which showed the flame determination process in the case of implement | achieving the flame determination part of FIG. 11 by the program control of a processor 3波長方式となる本発明による炎感知器の実施形態を示したブロック図The block diagram which showed embodiment of the flame detector by this invention used as a 3 wavelength system 図13の炎判定部の機能構成を示したブロック図The block diagram which showed the function structure of the flame determination part of FIG. 図14の炎判定部をプロセッサのプログラム制御で実現する場合の炎判定処理を示したフローチャートThe flowchart which showed the flame determination process in the case of implement | achieving the flame determination part of FIG. 14 by the program control of a processor 図13の炎判定部の他の実施形態による機能構成を示したブロック図The block diagram which showed the function structure by other embodiment of the flame determination part of FIG. 図16の炎判定部をプロセッサのプログラム制御で実現する場合の炎判定処理を示したフローチャートThe flowchart which showed the flame determination process in the case of implement | achieving the flame determination part of FIG. 16 by the program control of a processor

図1は本発明による炎感知器の実施形態を示したブロック図であり、2波長方式を例にとっている。図1において、炎感知器10は、第1検知部11aにより有炎燃焼時に発生するCO2の共鳴放射(4.5μm付近の波長帯域の赤外線を出す元は、炎とは限らない)による波長帯域を検知し、第2検知部11bによりアーク溶接光による近赤外線の波長帯域における放射線強度を検知し、炎判定部26で第1検知部11aと第2検知部11bで検知した2つの波長帯域における検知値の相対比により炎の存在を判定する2波長式による炎検知を行う。 FIG. 1 is a block diagram showing an embodiment of a flame detector according to the present invention, taking a two-wavelength system as an example. In FIG. 1, the flame detector 10 is a wavelength generated by the resonance radiation of CO 2 generated by the first detection unit 11 a during the flammable combustion (the source that emits infrared light in the wavelength band near 4.5 μm is not necessarily flame). Two wavelength bands detected by the first detection unit 11a and the second detection unit 11b by the flame determination unit 26, detecting the radiation intensity in the near infrared wavelength band by the arc welding light by the second detection unit 11b. Flame detection is performed by a two-wavelength method in which the presence of a flame is determined based on the relative ratio of the detection values at.

第1検知部11aには、CO2の共鳴放射により4.5μm付近の波長帯域を有する赤外線エネルギーを透過して電気信号に変換して出力する第1光学フィルタ14aと焦電型の第1受光素子16aを備えたセンサモジュール12aと、センサモジュール12aから出力される信号から炎のゆらぎ周波数と知られた所定の周波数帯域、例えば2Hzを中心とした周波数帯域の信号成分のみを通過させる前置フィルタを用いた第1周波数抽出部18aと、第1周波数抽出部18aを通過した信号成分を初段増幅するプリアンプ20aと、プリアンプ20aからの出力を、炎判定処理に適した信号レベルに増幅するメインアンプ22aと、メインアンプ22aから出力される増幅出力(アナログ信号)をデジタル信号となる4.5μm受光信号e1に変換するA/D変換器24aとを設けている。ここで、4.5μm受光信号は特許請求範囲の第1受光信号に対応する。 The first detector 11a includes a first optical filter 14a that transmits infrared energy having a wavelength band of about 4.5 μm through resonance radiation of CO 2 and converts the infrared energy into an electrical signal, and outputs the first optical filter 14a. A sensor module 12a having an element 16a, and a prefilter that passes only signal components in a predetermined frequency band known as a flame fluctuation frequency, for example, a frequency band centered on 2 Hz, from a signal output from the sensor module 12a A first frequency extraction unit 18a using a preamplifier, a preamplifier 20a that amplifies the signal component that has passed through the first frequency extraction unit 18a, and a main amplifier that amplifies the output from the preamplifier 20a to a signal level suitable for flame determination processing The 4.5 μm light reception signal e1 that becomes a digital signal from the amplified output (analog signal) output from the main amplifier 22a and 22a. It is provided an A / D converter 24a for converting. Here, the 4.5 μm light reception signal corresponds to the first light reception signal in the claims.

また第2検知部11bには、700〜1000nm付近(0.7〜1.0μm付近)となる近接赤外線の波長帯域を有する近赤外線エネルギーを透過して電気信号に変換して出力する第2光学フィルタ14bとフォトトランジスタまたはフォトダイオードを用いた第2受光素子16bを備えたセンサモジュール12bと、センサモジュール12bから出力される信号から炎のゆらぎ周波数と知られた所定の周波数帯域、例えば2Hzを中心とした周波数帯域の信号成分のみを通過させる前置フィルタを用いた第2周波数抽出部18bと、第2周波数抽出部18bを通過した信号成分を初段増幅するプリアンプ20bと、プリアンプ20bからの出力を、炎判定処理に適した信号レベルに増幅するメインアンプ22bと、メインアンプ22bから出力される増幅出力(アナログ信号)をデジタル信号となる近赤外受光信号e2に変換するA/D変換器24bとを設けている。   In addition, the second optical unit 11b transmits near-infrared energy having a near-infrared wavelength band in the vicinity of 700 to 1000 nm (near 0.7 to 1.0 μm) to be converted into an electrical signal and output to the second detection unit 11b. A sensor module 12b having a filter 14b and a second light receiving element 16b using a phototransistor or a photodiode, and a predetermined frequency band known as a flame fluctuation frequency from the signal output from the sensor module 12b, for example, 2 Hz. The second frequency extraction unit 18b using a pre-filter that passes only the signal component of the frequency band defined as above, the preamplifier 20b that amplifies the signal component that has passed through the second frequency extraction unit 18b, and the output from the preamplifier 20b The main amplifier 22b that amplifies the signal level suitable for the flame determination process and the main amplifier 22b Amplifying output outputted are provided an A / D converter 24b for converting the (analog signal) to the near-infrared light reception signal e2 as a digital signal.

なお、一般に近赤外線の波長は700〜2500nm付近(0.7〜2.5μm付近)であるが、第2受光素子16bとして使用するフォトトランジスタやフォトダイオードのピーク感度波長に基づき本実施形態にあっては、700〜1000nm付近の近赤外線波長帯域の放射強度を検知するようにしている。また、近赤外受光信号は特許請求範囲の第2受光信号に対応する。   In general, the wavelength of near-infrared light is around 700 to 2500 nm (near 0.7 to 2.5 μm), but this embodiment is based on the peak sensitivity wavelength of the phototransistor or photodiode used as the second light receiving element 16b. Thus, the radiation intensity in the near-infrared wavelength band near 700 to 1000 nm is detected. The near-infrared light reception signal corresponds to the second light reception signal in the claims.

第2受光素子16bとしてフォトトランジスタを使用する場合、フォトトランジスタのケースに設けた透過窓が、近接赤外線の700〜1000nm付近(0.7〜1.0μm付近)の波長帯域を有する近赤外線エネルギーを透過して電気信号に変換して出力する光学波長フィルタ14bとしてそのまま機能し、第2受光素子としてのフォトトランジスタは、ピーク感度波長として例えば800〜900nm付近にある市販品をそのまま使用できる。   When a phototransistor is used as the second light receiving element 16b, the transmission window provided in the case of the phototransistor has a near infrared energy having a wavelength band near 700 to 1000 nm (near 0.7 to 1.0 μm) of the near infrared. It functions as it is as an optical wavelength filter 14b that transmits and converts it into an electrical signal and outputs it. As the phototransistor as the second light receiving element, a commercially available product having a peak sensitivity wavelength in the vicinity of, for example, 800 to 900 nm can be used as it is.

また、第2受光素子16bとして使用するフォトトランジスタとしては透過窓にフィルタを設けないものも使用できる。この場合には、透過窓の特性ではなく、半導体素子の分光特性として、700〜1000nm付近に感度を持つものを使用する。   Further, as the phototransistor used as the second light receiving element 16b, a phototransistor without a filter in the transmission window can be used. In this case, not a transmission window characteristic but a spectral characteristic of a semiconductor element having a sensitivity near 700 to 1000 nm is used.

この点は第2受光素子16bとしてフォトダイオードを使用した場合も同様であり、例えばピーク感度波長を1050nm付近にをもつフォトPINダイオードなどが使用できる。   This is the same when a photodiode is used as the second light receiving element 16b. For example, a photo PIN diode having a peak sensitivity wavelength near 1050 nm can be used.

A/D変換器24a,24bからの4.5μm受光信号e1と近赤外受光信号e2は炎判定部26に入力される。炎判定部26は、4.5μm受光信号e1と近赤外受光信号e2に基づいて炎の存在とアーク溶接光の放射線源との識別判定を行う。   The 4.5 μm light reception signal e 1 and the near infrared light reception signal e 2 from the A / D converters 24 a and 24 b are input to the flame determination unit 26. The flame determination unit 26 performs discrimination determination between the presence of the flame and the radiation source of the arc welding light based on the 4.5 μm light reception signal e1 and the near infrared light reception signal e2.

本発明にあっては、炎判定部26内に、第1検知部11aからの4.5μm受光信号e1と第2検知部11bからの近赤外受光信号e2との時間的なずれを補正する補正部としての機能を設けている。この補正部は、第2検知部11bからの近赤外受光信号e2を所定時間Tdだけ遅延して4.5μm受光信号e1との時間ずれを抑制する。   In the present invention, the time discrepancy between the 4.5 μm light reception signal e1 from the first detection unit 11a and the near infrared light reception signal e2 from the second detection unit 11b is corrected in the flame determination unit 26. A function as a correction unit is provided. This correction unit delays the near-infrared light reception signal e2 from the second detection unit 11b by a predetermined time Td and suppresses a time shift from the 4.5 μm light reception signal e1.

このため炎判定部26は、補正部で時間的なずれが補正された4.5μm受光信号e1と近赤外受光信号e2に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することになる。このように時間的に早いタイミングで検知される近赤外受光信号e2を所定時間Tdだけ遅延することで、時間的に遅いタイミングで検知される4.5μm受光信号e1との時間的なずれを低減し、アーク溶接光を炎と誤判定してしまうことを確実に防止する。   For this reason, the flame determination unit 26 discriminates and determines the presence of the flame and the radiation source of the arc welding light based on the 4.5 μm light reception signal e1 and the near-infrared light reception signal e2 whose time shift is corrected by the correction unit. It will be. By delaying the near-infrared light reception signal e2 detected at a timing earlier in this way by a predetermined time Td, a time lag with respect to the 4.5 μm light reception signal e1 detected at a timing later in time is obtained. And reliably prevent the arc welding light from being misjudged as a flame.

炎判定部26で炎の存在が判定された場合、発報回路28に炎判定信号が出力され、スイッチング素子等をオンすることで、感知器端子30a,30bに接続している受信機からの感知器回線L,C間に発報電流を流し、受信機に火災発報信号を送出する。   When the presence of the flame is determined by the flame determination unit 26, a flame determination signal is output to the alarm circuit 28, and the switching elements and the like are turned on, so that the receivers connected to the sensor terminals 30a and 30b An alarm current is passed between the sensor lines L and C, and a fire alarm signal is sent to the receiver.

炎判定部26は4.5μm受光信号e1とTd時間遅延した近赤外受光信号e2の比率Kとして
K=e1/e2
を求め、当該比率Kが所定の閾値Kth以上の場合に炎の存在を判定する。
The flame determination unit 26 sets K = e1 / e2 as a ratio K between the 4.5 μm light reception signal e1 and the near infrared light reception signal e2 delayed by Td time.
And the presence of flame is determined when the ratio K is equal to or greater than a predetermined threshold value Kth.

図2は図1に設けた炎判定部の機能構成の実施形態を示したブロック図である。図2において、炎判定部26には積分器32aが設けられ、図1のA/D変換器24aからの4.5μm受光信号e1を所定時間単位で積分し、4.5μm積分信号E1を出力する。この積分により受光信号のノイズなどによる急激な変動を抑制する。   FIG. 2 is a block diagram showing an embodiment of the functional configuration of the flame determination unit provided in FIG. In FIG. 2, the flame determination unit 26 is provided with an integrator 32a, which integrates the 4.5 μm light reception signal e1 from the A / D converter 24a of FIG. 1 in units of a predetermined time, and outputs a 4.5 μm integration signal E1. To do. This integration suppresses a rapid fluctuation caused by noise of the received light signal.

また炎判定部26には補正部として機能する遅延器31と積分器32bが設けられる。遅延器31は、図1のA/D変換器24bからの近赤外受光信号e2を所定のTd時間遅延して積分器24bに入力し、積分器32aに入力する4.5μm受光信号e1との時間ずれを補正する。遅延器31でTd時間遅延した近赤外受光信号e2は積分器32bに入力され、積分器32aと同様、所定時間単位で積分することにより近赤外積分信号E2を出力し、ノイズなどによる急激な変動を抑制する。   The flame determination unit 26 is provided with a delay unit 31 and an integrator 32b that function as a correction unit. The delay unit 31 delays the near-infrared light reception signal e2 from the A / D converter 24b of FIG. 1 by a predetermined Td time, inputs it to the integrator 24b, and inputs the 4.5 μm light reception signal e1 input to the integrator 32a. Correct the time lag. The near-infrared light reception signal e2 delayed by the time Td by the delay unit 31 is input to the integrator 32b, and similarly to the integrator 32a, the near-infrared integration signal E2 is output by integration in a predetermined time unit, and suddenly due to noise or the like. Suppresses fluctuations.

遅延器31としてはシフトレジスタ等を使用することができ、クロック入力によるシフト動作により近赤外受光信号e2を入力してから出力するまで時間が所定の遅延時間Tdとなるようにシフト段数を設定している。なお、遅延器31によるデジタル的な遅延動作以外に、例えばA/D変換器24bの前段にアナログ遅延器を設けて遅延するようにしても良い。   A shift register or the like can be used as the delay device 31, and the number of shift stages is set so that the time from when the near-infrared light receiving signal e2 is input to when it is output by the shift operation by clock input becomes a predetermined delay time Td. doing. In addition to the digital delay operation by the delay unit 31, for example, an analog delay unit may be provided before the A / D converter 24b to delay the operation.

積分器32a、32bによる積分動作は、A/D変換器24a,24bのサンプリングにより一定の単位時間に得られる受光信号(デジタル信号)の和を求める。またA/D変換器24a,24bのサンプリング毎に、現時点から一定の単位時間前までに得られた受光信号(デジタル信号)の和となる移動加算による和を求めても良い。   In the integrating operation by the integrators 32a and 32b, the sum of received light signals (digital signals) obtained in a fixed unit time by sampling of the A / D converters 24a and 24b is obtained. In addition, for each sampling of the A / D converters 24a and 24b, a sum by moving addition that is a sum of light reception signals (digital signals) obtained from a current time to a certain unit time before may be obtained.

積分器32aからの4.5μm積分信号E1は比率演算器42に与えられ、また積分器32aからの近赤外積分信号E2は切替器40の切替端子aを介して比率演算器42に与えられ、
K=E1/E2
として比率Kを演算する。尚、この比率Kは4.5μm受光信号e1と近赤外受光信号e2に基づく
K=e1/e2
と実質的に同じ値となる。
The 4.5 μm integrated signal E1 from the integrator 32a is supplied to the ratio calculator 42, and the near-infrared integrated signal E2 from the integrator 32a is supplied to the ratio calculator 42 via the switching terminal a of the switch 40. ,
K = E1 / E2
The ratio K is calculated as follows. The ratio K is K = e1 / e2 based on the 4.5 μm light reception signal e1 and the near infrared light reception signal e2.
And substantially the same value.

比率演算器42で算出された比率Kは比較器44に与えられ、基準電圧源45により設定した所定の判定閾値Kthと比較され、比率Kが判定閾値Kth以上の場合、比較器44は炎判定信号としてHレベル出力を生ずる。   The ratio K calculated by the ratio calculator 42 is given to the comparator 44 and compared with a predetermined determination threshold value Kth set by the reference voltage source 45. When the ratio K is equal to or greater than the determination threshold value Kth, the comparator 44 determines the flame. An H level output is generated as a signal.

図3はアーク溶接を断続的に行った場合の4.5μm受光信号と時間的なタイミングずれを持つ近赤外受光信号及び両者の比率の時間変化を示したタイムチャート(グラフ図)である。   FIG. 3 is a time chart (graph) showing the time variation of the 4.5 μm light reception signal, the near-infrared light reception signal having a temporal timing shift, and the ratio of both when the arc welding is intermittently performed.

図3(A)は受光信号のタイムチャートであり、アーク溶接を行うと、最初に近赤外受光信号e2のピークが現れ、所定時間Tdだけ遅れて4.5μm受光信号e1のピークが現れている。   FIG. 3A is a time chart of the light reception signal. When arc welding is performed, the peak of the near infrared light reception signal e2 appears first, and the peak of the 4.5 μm light reception signal e1 appears after a predetermined time Td. Yes.

図3(B)は図3(A)の4.5μm受光信号e1と近赤外受光信号e2から算出した比率K=e1/e2の時間変化であり、アーク溶接光による2つの受光信号の時間ずれに起因して2箇所に比率K=2以上となるピーク部分を生じ、例えば図2で比較器44に対する判定閾値KthとしてKth=2を設定していた場合、アーク溶接光でありながら炎と誤判定されることになる。   FIG. 3B is a time change of the ratio K = e1 / e2 calculated from the 4.5 μm light reception signal e1 and the near infrared light reception signal e2 in FIG. 3A, and the time of two light reception signals by arc welding light. Due to the deviation, a peak portion having a ratio K = 2 or more is generated at two locations. For example, when Kth = 2 is set as the determination threshold value Kth for the comparator 44 in FIG. A misjudgment will be made.

図4はアーク溶接を断続的に行った場合の4.5μm受光信号と時間的なタイミングずれを補正した近赤外受光信号及び両者の比率の時間変化を示したタイムチャート(グラフ図)である。   FIG. 4 is a time chart (graph) showing a time variation of a 4.5 μm light reception signal, a near-infrared light reception signal in which a temporal timing shift is corrected, and a ratio between the two when the arc welding is intermittently performed. .

図4(A)は受光信号のタイムチャートであり、図3(A)に示した近赤外受光信号e2を所定時間Tdだけ遅延することで、破線で示す近赤外受光信号e2となり、4.5μm受光信号e1との時間ずれが低減し、両者のピークが一致するように補正されている。   FIG. 4A is a time chart of the light reception signal. By delaying the near-infrared light reception signal e2 shown in FIG. 3A by a predetermined time Td, a near-infrared light reception signal e2 indicated by a broken line is obtained. Correction is made so that the time lag with respect to the .5 μm light reception signal e1 is reduced and the peaks of both coincide.

図4(B)は図4(A)の4.5μm受光信号e1とTd時間遅延した近赤外受光信号e2から算出した比率Kの時間変化であり、アーク溶接光による2つの受光信号の時間ずれが低減したため、比率Kのピーク値は例えば判定閾値KthとなるKth=2未満に収まり、アーク溶接光を炎と誤判定することを確実に防止できる。   FIG. 4B is a time change of the ratio K calculated from the 4.5 μm light reception signal e1 of FIG. 4A and the near infrared light reception signal e2 delayed by Td time, and the time of two light reception signals by arc welding light. Since the deviation is reduced, the peak value of the ratio K is, for example, less than Kth = 2, which is the determination threshold value Kth, and it is possible to reliably prevent the arc welding light from being erroneously determined as flame.

図5は断続的な溶接作業を行った場合の4.5μm受光信号e1と近赤外受光信号e2の実測データを示したタイムチャート(グラフ図)であり、例えば近赤外受光信号e2のピークP1に対し4.5μm受光信号e1のピークP2の遅れ時間Td1は0.4秒程度であり、また近赤外受光信号e2のピークP3に対し4.5μm受光信号e1のピークP4の遅れ時間Td2は0.3秒程度でとなっており、これに基づき図2の遅延器31の遅延時間としてTd=0.4秒を設定すれば良い。   FIG. 5 is a time chart (graph) showing actual measurement data of the 4.5 μm light reception signal e1 and the near infrared light reception signal e2 when intermittent welding work is performed, for example, the peak of the near infrared light reception signal e2 The delay time Td1 of the peak P2 of the 4.5 μm light reception signal e1 with respect to P1 is about 0.4 seconds, and the delay time Td2 of the peak P4 of the 4.5 μm light reception signal e1 with respect to the peak P3 of the near infrared light reception signal e2 Based on this, Td = 0.4 seconds may be set as the delay time of the delay device 31 of FIG.

図6は、図2の炎判定部26における4.5μm受光信号と近赤外受光信号との時間ずれを補正した積分処理を示した説明図である。   FIG. 6 is an explanatory diagram showing an integration process in which the time difference between the 4.5 μm light reception signal and the near-infrared light reception signal in the flame determination unit 26 of FIG. 2 is corrected.

図6(A)及び図6(C)はA/D変換器24b、24aにより所定ビット数のデジタル信号に変換した離散的な近赤外受光信号e2と4.5μm受光信号e1を時間軸方向に並べて示しており、時刻t1から近赤外受光信号e2が得られているのに対し、4.5μm受光信号e1は時間的に遅れた時刻t2から得られており、Td時間の時間遅れをもっている。   6 (A) and 6 (C) show time directions of discrete near-infrared light reception signal e2 and 4.5 μm light reception signal e1 converted into digital signals having a predetermined number of bits by A / D converters 24b and 24a. The near-infrared light reception signal e2 is obtained from time t1, whereas the 4.5 μm light reception signal e1 is obtained from time t2 delayed in time, with a time delay of Td time. Yes.

図6(A)のA/D変換器24bからの近赤外受光信号e2は遅延器31によりTd時間遅延され、図6(B)に示す遅延近赤外受光信号e2となり、両者の時間ずれが解消される。   The near-infrared light reception signal e2 from the A / D converter 24b in FIG. 6A is delayed by Td time by the delay unit 31 to become a delayed near-infrared light reception signal e2 shown in FIG. Is resolved.

積分器32aは単位時間Tiの間、4.5μm受光信号e1を加算する離散的な積分動作を行い、4.5μm積分信号E1を出力する。積分器32bは同じタイミングで単位時間Tiの間、近赤外受光信号e2を加算する離散的な積分動作を行い、近赤外積分信号E2を出力する。   The integrator 32a performs a discrete integration operation of adding the 4.5 μm light reception signal e1 during the unit time Ti, and outputs a 4.5 μm integration signal E1. The integrator 32b performs a discrete integration operation of adding the near-infrared light reception signal e2 for the unit time Ti at the same timing, and outputs a near-infrared integration signal E2.

なお、積分器31a,32bの積分としては、A/D変換器24a,24bのサンプリング毎に、現時点から一定の単位時間前までに得られた受光信号(デジタル信号)の和となる移動加算による積分値を求めても良い。   The integration of the integrators 31a and 32b is performed by moving addition that is the sum of the received light signals (digital signals) obtained from the present time until a certain unit time before the sampling of the A / D converters 24a and 24b. An integral value may be obtained.

図7は図2の炎判定部の機能をプロセッサによるプログラムの実行により実現する場合の炎判定処理を示したフローチャートである。図7において、炎判定処理は、ステップS1でA/D変換器24aからの4.5μm受光信号e1を積分した4.5μm積分値E1を読込み、続いてステップS2でA/D変換器24bからの近赤外受光信号e2を所定時間Td遅延して積分した近赤外積分値E2を読込む。   FIG. 7 is a flowchart showing a flame determination process when the function of the flame determination unit in FIG. 2 is realized by executing a program by a processor. In FIG. 7, the flame determination process reads a 4.5 μm integrated value E1 obtained by integrating the 4.5 μm light reception signal e1 from the A / D converter 24a in step S1, and then in step S2 from the A / D converter 24b. A near-infrared integrated value E2 obtained by integrating the near-infrared light receiving signal e2 with a predetermined time Td is read.

続いてステップS3に進み、比率Kを
K=E1/E2
として計算する。
In step S3, the ratio K is set to K = E1 / E2.
Calculate as

続いてステップS4で比率Kが所定の判定閾値Kth以上か否か判定し、判定閾値Kth以上であることを判定した場合はステップS5に進み、炎の存在を判定すると共に炎判定信号を発報回路28に出力して動作させることで、火災発報信号を受信機に出力させる。   Subsequently, in step S4, it is determined whether or not the ratio K is equal to or greater than a predetermined determination threshold value Kth. If it is determined that the ratio K is equal to or greater than the determination threshold value Kth, the process proceeds to step S5. By outputting to the circuit 28 and operating it, a fire alarm signal is output to the receiver.

次に本発明における炎とアーク溶接光の識別判定の原理を説明する。図8は炎とアーク溶接光の分光特性を示した放射スペクトル特性図であり、炎スペクトル46とアーク溶接光スペクトル48につき、有炎燃焼時に発生するCO2の共鳴放射共鳴放射による4.5μm付近の放射強度を略同じ状態として測定した結果を示している。 Next, the principle of discrimination determination between the flame and the arc welding light in the present invention will be described. FIG. 8 is a radiation spectrum characteristic diagram showing the spectral characteristics of the flame and arc welding light. The flame spectrum 46 and the arc welding light spectrum 48 are around 4.5 μm due to the resonance radiation resonance emission of CO 2 generated during flame combustion. The result of having measured the radiant intensity of the substantially the same state is shown.

図8において、炎スペクトル46はCO2の共鳴放射により4.5μm付近に大きな放射強度のピーク値をもっている。アーク溶接光スペクトル48は溶接棒の被覆に含まれるでんぷん等の有機物の燃焼により、CO2の共鳴放射による4.5μm付近に放射強度のピーク値をもち、700〜1000nm付近(0.7〜1.0μm付近)の波長帯域となる近赤外線波長帯域およびそれより短波長側の帯域に放射強度が分布している。 In FIG. 8, the flame spectrum 46 has a peak value of a large radiation intensity in the vicinity of 4.5 μm due to the resonance radiation of CO 2 . The arc welding light spectrum 48 has a peak value of radiant intensity around 4.5 μm due to resonance emission of CO 2 due to combustion of organic substances such as starch contained in the coating of the welding rod, and around 700 to 1000 nm (0.7 to 1). The radiation intensity is distributed in the near-infrared wavelength band, which is a wavelength band of around 0.0 μm), and in the shorter wavelength band.

ここで図1の実施形態に設けた第2フォトセンサ12bにあっては、光学波長フィルタ14bとフォトトランジスタまたはフォトダイオードを用いた第2受光素子16bにより、図4における700〜1000nm付近(0.7〜1.0μm付近)となる近赤外線波長帯域50に放射強度をもつ近赤外線エネルギーを検知している。   Here, in the second photosensor 12b provided in the embodiment of FIG. 1, the optical wavelength filter 14b and the second light receiving element 16b using a phototransistor or a photodiode are used in the vicinity of 700 to 1000 nm (0. Near-infrared energy having a radiant intensity in the near-infrared wavelength band 50 of about 7 to 1.0 μm is detected.

アーク溶接光スペクトラム48が近赤外波長帯域50に分布する理由は、アーク溶接に使用する溶接棒の被覆には例えば長石が含まれており、長石に含まれるカリウムが燃焼する場合に、760nm付近にピークをもつ近赤外線光が特徴的に放射されることによると考えられる。またアルゴンガスを保護用ガスとして用いるTIG溶接(タングステン・イナート・ガス溶接の略)にあっては、アーク溶接に伴うアルゴンガスのプラズマから811nm付近の近赤外線が特徴的に放射されることによると考えられる。このようなアーク溶接に使用する溶接棒の被覆成分の燃焼に起因し、アーク溶接光スペクトル48は、CO2の共鳴放射による4.5μm付近の放射強度のピーク値を持つと共に、第2フォトセンサ12bの検知波長帯域となる700〜1000nm付近(0.7〜1.0μm付近)の近赤外線波長帯域50に放射強度が分布している。 The reason why the arc welding light spectrum 48 is distributed in the near-infrared wavelength band 50 is that, for example, feldspar is included in the coating of the welding rod used for arc welding, and the potassium contained in the feldspar burns around 760 nm. This is considered to be due to the characteristic emission of near-infrared light having a peak at. Moreover, in TIG welding (abbreviation of tungsten inert gas welding) using argon gas as a protective gas, according to the characteristic that near infrared rays near 811 nm are radiated from the argon gas plasma accompanying arc welding. Conceivable. Due to the combustion of the covering component of the welding rod used for such arc welding, the arc welding light spectrum 48 has a peak value of the radiation intensity in the vicinity of 4.5 μm due to the resonance emission of CO 2 , and the second photosensor. The radiation intensity is distributed in the near-infrared wavelength band 50 in the vicinity of 700 to 1000 nm (near 0.7 to 1.0 μm), which is the detection wavelength band of 12b.

この炎スペクトル46とアーク溶接光スペクトル48の分光特性から明らかなように、従来の例えば2波長方式において、CO2の共鳴放射帯である4.5μm付近を中心波長とした狭波長帯域と、その長波長側の例えば、5.1μm付近の狭波長帯域における放射エネルギーを検知し、これらの2波長帯域における検知出力の相対比によっては、炎とアーク溶接光を識別判定することはできないことが分かる。 As is apparent from the spectral characteristics of the flame spectrum 46 and the arc welding light spectrum 48, in the conventional two-wavelength method, for example, a narrow wavelength band centered around 4.5 μm, which is the CO 2 resonance radiation band, For example, it is understood that the radiant energy in a narrow wavelength band near 5.1 μm on the long wavelength side is detected, and the flame and the arc welding light cannot be discriminated and determined depending on the relative ratio of the detected output in these two wavelength bands. .

図9は、断続的にアーク溶接を行った場合のアーク溶接光に対する4.5μm積分信号と近赤外積分信号から算出した比率Kの時間変化を示したタイムチャートである。なお、図9はアーク溶接光における近赤外光に対するCO2共鳴放射による4.5μm付近の光のタイミングずれが小さい場合である。 FIG. 9 is a time chart showing the time change of the ratio K calculated from the 4.5 μm integrated signal and the near-infrared integrated signal with respect to the arc welding light when the arc welding is intermittently performed. FIG. 9 shows a case where the timing deviation of light in the vicinity of 4.5 μm due to CO 2 resonance radiation with respect to near infrared light in arc welding light is small.

図9において、CO2の共鳴放射共鳴放射による4.5μm付近の放射強度を検知した4.5μm積分信号は測定特性52に示すように、アーク溶接を断続的に行う毎にピーク値が生じている。 In FIG. 9, the 4.5 μm integrated signal obtained by detecting the radiation intensity in the vicinity of 4.5 μm due to the resonance radiation of CO 2 has a peak value every time the arc welding is intermittently performed as shown in the measurement characteristic 52. Yes.

この測定特性52となる4.5μm積分信号と共に検知している近赤外線波長帯域の放射強度に対応した近赤外積分信号(図示せず)とに基づき計算した比率K=E1/E2は、比率特性54に示すように変化する。即ち、測定特性52において4.5μm積分信号が大きくなると、比率特性54のように比率Kの値が小さくなる関係にあり、この場合、比率Kは概ねK=2以下に収まっている。   The ratio K = E1 / E2 calculated based on the near-infrared integrated signal (not shown) corresponding to the radiation intensity in the near-infrared wavelength band detected together with the 4.5 μm integrated signal that becomes the measurement characteristic 52 is the ratio It changes as shown by the characteristic 54. That is, when the 4.5 μm integrated signal increases in the measurement characteristic 52, the ratio K decreases as in the ratio characteristic 54. In this case, the ratio K is approximately within K = 2.

図10は、ヘプタン炎に対する4.5μm積分信号と、近赤外積分信号から算出した比率Kの時間変化を示したタイムチャートである。   FIG. 10 is a time chart showing the time change of the ratio K calculated from the 4.5 μm integrated signal and the near-infrared integrated signal for the heptane flame.

図10において、CO2の共鳴放射共鳴放射による4.5μm付近の放射強度を検知した4.5μm積分信号は測定特性56に示すように、炎の大きさの変化に対応して変動している。 In FIG. 10, the 4.5 μm integrated signal obtained by detecting the radiation intensity in the vicinity of 4.5 μm due to the resonance radiation of CO 2 fluctuates in accordance with the change in the size of the flame as indicated by the measurement characteristic 56. .

この測定特性56となる4.5μm積分信号と共に検知している近赤外線波長帯域の放射強度に対応した近赤外積分信号(図示せず)とに基づき計算した比率K=E1/E2は、比率特性58に示すように変化する。即ち、測定特性58において、4.5μm積分信号が大きくなると、比率特性54のように比率Kの値も大きくなる関係にあり、この場合、比率Kは概ねK=50〜200といった大きな値を示している。   The ratio K = E1 / E2 calculated based on the near-infrared integrated signal (not shown) corresponding to the radiation intensity in the near-infrared wavelength band detected together with the 4.5 μm integrated signal that becomes the measurement characteristic 56 is the ratio It changes as shown by the characteristic 58. That is, in the measurement characteristic 58, when the 4.5 μm integral signal becomes large, the value of the ratio K also becomes large like the ratio characteristic 54. In this case, the ratio K generally shows a large value such as K = 50 to 200. ing.

この結果、図9に示したアーク溶接の場合の比率Kが概ねK=2以下であったのに対し、図10のヘプタン炎の場合の比率Kは概ねK=50〜200と非常に大きくなり、このように変化する比率Kを比較判定することで炎の存在とアーク溶接光とを確実に識別判定することができる。   As a result, the ratio K in the arc welding shown in FIG. 9 is approximately K = 2 or less, whereas the ratio K in the heptane flame in FIG. 10 is very large, approximately K = 50 to 200. Thus, by comparing and determining the changing ratio K, it is possible to reliably identify and determine the presence of the flame and the arc welding light.

図11は図1に設けた炎判定部の他の実施形態による機能構成を示したブロック図であり、本実施形態の炎判定部26にあっては、近赤外受光信号e2が極端に大きくなった場合の外乱光となるアーク溶接光による感度低下を抑制するため、近赤外受光信号e2が所定レベルを超えた場合、近赤外受光信号e2の代りに所定の定数cを使用して4.5μm受光信号との比率Kを求めることでアーク溶接光による感度低下を抑制するようにしたことを特徴とする。   FIG. 11 is a block diagram illustrating a functional configuration according to another embodiment of the flame determination unit provided in FIG. 1. In the flame determination unit 26 of the present embodiment, the near-infrared light reception signal e2 is extremely large. In order to suppress a decrease in sensitivity due to arc welding light that becomes disturbance light in the case where the near-infrared light reception signal e2 exceeds a predetermined level, a predetermined constant c is used instead of the near-infrared light reception signal e2. It is characterized in that a decrease in sensitivity due to arc welding light is suppressed by obtaining a ratio K to a 4.5 μm light reception signal.

即ち、炎判定部26は、所定時間Td遅延した近赤外受光信号e2が所定の受光閾値eth未満の場合は、4.5μm受光信号e1と近赤外受光信号e2との比率Kとして
K=e1/e2
を求め、一方、所定時間Td遅延した近赤外受光信号e2が所定の受光閾値eth以上の場合は、4.5μm受光信号e1と、所定の定数cの比率Kとして
K=e1/c
を求め、比率が所定の判定閾値Kth以上の場合に炎の存在を判定することを基本とする。
That is, when the near-infrared light reception signal e2 delayed by the predetermined time Td is less than the predetermined light reception threshold eth, the flame determination unit 26 sets K = the ratio K between the 4.5 μm light reception signal e1 and the near-infrared light reception signal e2. e1 / e2
On the other hand, if the near-infrared light reception signal e2 delayed by a predetermined time Td is equal to or greater than a predetermined light reception threshold eth, the ratio K of 4.5 μm light reception signal e1 and a predetermined constant c is K = e1 / c
And determining the presence of flame when the ratio is equal to or greater than a predetermined determination threshold value Kth.

図11の炎判定部26にあっては、新たに定数設定器34、比較器36及び切替器40を設けており、それ以外の構成は図2の実施形態と同じになる。即ち、炎判定部26には積分器32a、32bが設けられ、図1のA/D変換器24a,24bからの4.5μm受光信号e1と遅延器31でTd時間遅延した近赤外受光信号e2を所定時間単位で積分し、4.5μm積分信号E1と近赤外積分信号E2を出力する。   In the flame determination unit 26 of FIG. 11, a constant setter 34, a comparator 36, and a switcher 40 are newly provided, and other configurations are the same as those of the embodiment of FIG. That is, the flame determination unit 26 is provided with integrators 32a and 32b. The 4.5 μm light reception signal e1 from the A / D converters 24a and 24b in FIG. 1 and the near infrared light reception signal delayed by Td by the delay unit 31 are provided. e2 is integrated in a predetermined time unit, and a 4.5 μm integrated signal E1 and a near-infrared integrated signal E2 are output.

積分器32aからの4.5μm積分信号E1は比率演算器42に与えられ、また積分器32aからの近赤外積分信号E2は切替器40の切替端子aを介して比率演算器42に与えられる。切替器40の他方の切替端子bには所定の定数cを出力する定数設定器34を接続している。   The 4.5 μm integrated signal E1 from the integrator 32a is supplied to the ratio calculator 42, and the near-infrared integrated signal E2 from the integrator 32a is supplied to the ratio calculator 42 via the switching terminal a of the switch 40. . A constant setting device 34 that outputs a predetermined constant c is connected to the other switching terminal b of the switching device 40.

切替器40は比較器36により切替制御される。比較器36は積分器32bからの近赤外積分信号e2と基準電圧源38で設定した所定の受光閾値Ethとを比較しており、近赤外積分信号E42が受光閾値Eth未満の場合のLレベル出力で、図示のように、切替器40を切替端子aに切替え、積分器32bからの近赤外積分信号E2を比率演算器42に与え、比率演算器42は
K=E1/E2
として比率Kを演算する。尚、この比率Kは4.5μm受光信号e1と所定時間Td遅延した近赤外受光信号e2に基づく
K=e1/e2
と実質的に同じ値となる。
The switch 40 is controlled to be switched by the comparator 36. The comparator 36 compares the near-infrared integrated signal e2 from the integrator 32b with the predetermined light reception threshold Eth set by the reference voltage source 38, and the L when the near-infrared integrated signal E42 is less than the light reception threshold Eth. At the level output, as shown in the figure, the switch 40 is switched to the switch terminal a, the near-infrared integrated signal E2 from the integrator 32b is given to the ratio calculator 42, and the ratio calculator 42 is K = E1 / E2.
The ratio K is calculated as follows. The ratio K is K = e1 / e2 based on the 4.5 μm light reception signal e1 and the near infrared light reception signal e2 delayed by a predetermined time Td.
And substantially the same value.

一方、比較器36は近赤外積分信号E2が受光閾値Eth以上となった場合にHレベル出力を生じ、切替器40を切替端子b側に切替え、定数設定器34からの定数cを比率演算器42に与え、率演算器42は
K=E1/c
として比率Kを演算する。尚、この比率Kは4.5μm受光信号e1と定数cに基づく
K=e1/c
と実質的に同じ値となる。
On the other hand, the comparator 36 generates an H level output when the near-infrared integrated signal E2 becomes equal to or greater than the light reception threshold Eth, switches the switch 40 to the switch terminal b side, and calculates the ratio c of the constant c from the constant setter 34. The rate calculator 42 is K = E1 / c.
The ratio K is calculated as follows. This ratio K is K = e1 / c based on the 4.5 μm light reception signal e1 and the constant c.
And substantially the same value.

比率演算器42で算出された比率Kは比較器44に与えられ、基準電圧源45により設定した所定の判定閾値Kthと比較され、比率Kが判定閾値Kth以上の場合、比較器44は炎判定信号としてHレベル出力を生ずる。   The ratio K calculated by the ratio calculator 42 is given to the comparator 44 and compared with a predetermined determination threshold value Kth set by the reference voltage source 45. When the ratio K is equal to or greater than the determination threshold value Kth, the comparator 44 determines the flame. An H level output is generated as a signal.

図12は図11の炎判定部の機能をプロセッサによるプログラムの実行により実現する場合の炎判定処理を示したフローチャートである。図12において、炎判定処理は、ステップS11でA/D変換器24aからの4.5μm受光信号e1を積分した4.5μm積分値E1を読込み、続いてステップS12でA/D変換器24bからの近赤外受光信号e2を所定時間Td遅延した積分した近赤外積分値E2を読込む。   FIG. 12 is a flowchart showing a flame determination process when the function of the flame determination unit in FIG. 11 is realized by executing a program by a processor. In FIG. 12, in the flame determination process, the 4.5 μm integrated value E1 obtained by integrating the 4.5 μm light reception signal e1 from the A / D converter 24a is read in step S11, and then in step S12, the A / D converter 24b reads. A near-infrared integrated value E2 obtained by integrating the near-infrared light receiving signal e2 obtained by delaying by a predetermined time Td is read.

続いてステップS13で近赤外積分値E2が所定の受光閾値Eth未満か否か判別し、受光閾値Eth未満を検知した場合はステップS14に進み、比率Kを
K=E1/E2
として計算する。
Subsequently, in step S13, it is determined whether or not the near-infrared integrated value E2 is less than a predetermined light reception threshold Eth, and if it is less than the light reception threshold Eth, the process proceeds to step S14, and the ratio K is set to K = E1 / E2.
Calculate as

一方、ステップS13で近赤外積分値E2が所定の受光閾値Eth以上となることを検知した場合はステップS15に進み、近赤外積分値E2を定数cに変更し、比率Kを
K=E1/c
として計算する。
On the other hand, if it is detected in step S13 that the near-infrared integrated value E2 is equal to or greater than the predetermined light receiving threshold Eth, the process proceeds to step S15, the near-infrared integrated value E2 is changed to a constant c, and the ratio K is set to K = E1. / C
Calculate as

続いてステップS17で比率Kが所定の判定閾値Kth以上か否か判定し、判定閾値Kth以上であることを判定した場合はステップS18に進み、炎の存在を判定すると共に炎判定信号を発報回路28に出力して動作させることで、火災発報信号を受信機に出力させる。   In step S17, it is determined whether or not the ratio K is equal to or greater than a predetermined determination threshold value Kth. If it is determined that the ratio K is equal to or greater than the determination threshold value Kth, the process proceeds to step S18. By outputting to the circuit 28 and operating it, a fire alarm signal is output to the receiver.

図13は本発明による炎感知器の他の実施形態を示したブロック図であり、3波長方式を例にとっている。図13において、炎感知器10は、有炎燃焼時に発生するCO2の共鳴放射による4.5μm付近の波長帯域と、CO2の共鳴放射による4.5μm付近の波長帯域に隣接した5.1μm付近の波長帯域と、アーク溶接光による近赤外線の0.7〜1.0μm付近の波長帯域における放射強度を検知し、3つの波長帯域における検知値の相対比により炎の有無を検知する3波長式による炎判定を行う。 FIG. 13 is a block diagram showing another embodiment of the flame detector according to the present invention, taking a three-wavelength system as an example. In FIG. 13, the flame detector 10 has a wavelength band of about 4.5 μm due to resonance emission of CO 2 generated during flammable combustion and 5.1 μm adjacent to a wavelength band of about 4.5 μm due to resonance emission of CO 2. Three wavelengths that detect the intensity of radiation in the nearby wavelength band and the near-infrared wavelength band of 0.7 to 1.0 μm of arc welding light, and detect the presence or absence of flames by the relative ratio of the detected values in the three wavelength bands The flame is determined by the formula.

炎感知器10は、第1光学フィルタ14aと第1受光素子16aを備えたセンサモジュール12a、第1周波数抽出部18a、プリアンプ20a、メインアンプ22a及びA/D変換器24aを備えた第1検知部11aにより4.5μm受光信号e1を検知し、また、第2光学フィルタ14bと第2受光素子16bを備えたセンサモジュール12b、第2周波数抽出部18b、プリアンプ20b、メインアンプ22b及びA/D変換器24bを備えた第2検知部11bにより近赤外受光信号e2を検知し、この点は図1の実施形態と同じである。   The flame detector 10 includes a sensor module 12a including a first optical filter 14a and a first light receiving element 16a, a first frequency extraction unit 18a, a preamplifier 20a, a main amplifier 22a, and an A / D converter 24a. The unit 11a detects a 4.5 μm light reception signal e1, and also includes a sensor module 12b including a second optical filter 14b and a second light receiving element 16b, a second frequency extraction unit 18b, a preamplifier 20b, a main amplifier 22b, and an A / D. The near-infrared light reception signal e2 is detected by the second detection unit 11b including the converter 24b, and this is the same as the embodiment in FIG.

これに加え本実施形態にあっては、CO2の共鳴放射による4.5μm付近の波長帯域に隣接した5.1μm付近の波長帯域の放射強度を検知する第3検知部11cを設けており、第3検知部11cには、5.1μm付近を中心波長と擦る狭波長帯域を有する赤外線エネルギーを透過して電気信号に変換して出力する第3光学フィルタ14cと焦電型の第3受光素子16cを備えたセンサモジュール12cと、センサモジュール12cから出力される信号から炎のゆらぎ周波数と知られた所定の周波数帯域、例えば2Hzを中心とした周波数帯域の信号成分のみを通過させる前置フィルタを用いた第3周波数抽出部18cと、第3周波数抽出部18cを通過した信号成分を初段増幅するプリアンプ20cと、プリアンプ20cからの出力を、炎判定処理に適した信号レベルに増幅するメインアンプ22cと、メインアンプ22cから出力される増幅出力(アナログ信号)をデジタル信号となる5.1μm受光信号e3に変換するA/D変換器24cとを設けている。なお、5.1μm受光信号は特許請求の範囲の第3受光信号に対応する。 In addition to this, in the present embodiment, the third detector 11c that detects the radiation intensity in the wavelength band near 5.1 μm adjacent to the wavelength band near 4.5 μm due to the resonance radiation of CO 2 is provided. The third detector 11c includes a third optical filter 14c that transmits infrared energy having a narrow wavelength band that rubs around 5.1 μm with the center wavelength, converts the energy into an electrical signal, and outputs the electrical signal, and a pyroelectric third light receiving element. A pre-filter that passes only signal components in a predetermined frequency band known as a flame fluctuation frequency, for example, a frequency band centered on 2 Hz, from the signal output from the sensor module 12c. The third frequency extraction unit 18c used, the preamplifier 20c that amplifies the signal component that has passed through the third frequency extraction unit 18c, and the output from the preamplifier 20c A main amplifier 22c that amplifies the signal level suitable for constant processing, and an A / D converter 24c that converts the amplified output (analog signal) output from the main amplifier 22c into a 5.1 μm light reception signal e3 that is a digital signal. Provided. The 5.1 μm light reception signal corresponds to the third light reception signal in the claims.

炎判定部260は、A/変換器24a,24b,24cからの4.5μm受光信号e1、近赤外受光信号e2及び5.1μm受光信号e3を入力し、近赤外受光信号e2については所定時間Tdの遅延を行い、当該3つの受光信号e1,e2,e3に基づいて炎の存在とアーク溶接光の放射線源との識別判定を行い、炎の存在を判定した場合、発報回路28に炎判定信号を出力し、スイッチング素子等をオンすることで、感知器端子30a,30bに接続している受信機からの感知器回線に発報電流を流し、受信機に火災発報信号を送出する。   The flame determination unit 260 receives the 4.5 μm light reception signal e1, the near infrared light reception signal e2, and the 5.1 μm light reception signal e3 from the A / converters 24a, 24b, and 24c, and the near infrared light reception signal e2 is predetermined. When the time Td is delayed and the presence of the flame is discriminated from the radiation source of the arc welding light based on the three received light signals e1, e2, e3, and the presence of the flame is determined, By outputting a flame judgment signal and turning on the switching element, etc., an alarm current is sent to the sensor line from the receiver connected to the sensor terminals 30a and 30b, and a fire alarm signal is sent to the receiver. To do.

炎判定部260は4.5μm受光信号e1とTd時間遅延した近赤外受光信号e2の第1比率K1として
K1=e1/e2
を求め、また炎判定部26は4.5μm受光信号e1と5.1μm受光信号e3の第2比率Kとして
K2=e1/e3
を求め、第1比率K1が所定の第1判定閾値Kth1以上で、且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。なお、第2比率K2は炎のみに特徴的に大きく出る出力による信号e1と、その他の光源で特徴的な出力による信号e3を比較するものである。
The flame determination unit 260 sets K1 = e1 / e2 as the first ratio K1 between the 4.5 μm light reception signal e1 and the near-infrared light reception signal e2 delayed by Td time.
Further, the flame determination unit 26 sets K2 = e1 / e3 as the second ratio K of the 4.5 μm light reception signal e1 and the 5.1 μm light reception signal e3.
And the presence of flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2. Note that the second ratio K2 is a comparison between the signal e1 due to the output characteristically generated only by the flame and the signal e3 due to the characteristic output from other light sources.

比率演算器420で算出された第1及び第2比率K1,K2は比較判定部440に与えられる。比較判定部440は、第1比率K1が所定の第1判定閾値Kth1以上で、且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。   The first and second ratios K1 and K2 calculated by the ratio calculator 420 are given to the comparison determination unit 440. The comparison determination unit 440 determines the presence of a flame when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.

このように3番目の波長としてCO2の共鳴放射による4.5μm付近の波長帯域に隣接した5.1μm付近の波長帯域の放射強度を検知して炎判定を行うことで、炎以外の赤外線放射体、例えば、太陽光等の高温放射体や、300°C程度の比較的低温の放射体、人体などの低温放射体等との識別判定をより確実に行うことできる。 In this way, by detecting the radiation intensity in the wavelength band near 5.1 μm adjacent to the wavelength band near 4.5 μm due to the resonance radiation of CO 2 as the third wavelength, infrared determination other than flame is performed. It is possible to more reliably discriminate and discriminate from a body, for example, a high-temperature radiator such as sunlight, a relatively low-temperature radiator of about 300 ° C., a low-temperature radiator such as a human body, and the like.

図14は図13に設けた炎判定部の実施形態となる機能構成を示したブロック図である。図14において、炎判定部260に設けた遅延器31及び積分器32a,32bは図2の2波長方式の実施形態と同じである。これに加え本実施形態では、積分器32cが設けられ、A/D変換器24cからの5.1μm受光信号e3を所定時間単位で積分し、5.1μm積分信号E3を出力する。   FIG. 14 is a block diagram showing a functional configuration as an embodiment of the flame determination unit provided in FIG. In FIG. 14, the delay unit 31 and the integrators 32a and 32b provided in the flame determination unit 260 are the same as those in the embodiment of the two-wavelength system in FIG. In addition, in the present embodiment, an integrator 32c is provided, which integrates the 5.1 μm light reception signal e3 from the A / D converter 24c in a predetermined time unit and outputs a 5.1 μm integration signal E3.

比率演算器420は、積分器32aからの4.5μm積分信号E1、積分器32bからの近赤外積分信号E2及び積分器32cからの5.1μm積分信号E3を入力し、第1比率K1及び第2比率K2として
K1=E1/E2
K2=E1/E3
を求める。
The ratio calculator 420 receives the 4.5 μm integrated signal E1 from the integrator 32a, the near-infrared integrated signal E2 from the integrator 32b, and the 5.1 μm integrated signal E3 from the integrator 32c, and receives the first ratio K1 and As the second ratio K2, K1 = E1 / E2
K2 = E1 / E3
Ask for.

比率演算器420で算出された第1及び第2比率K1,K2は比較判定部440に与えられる。比較判定部440は、第1比率K1が所定の第1判定閾値Kth1以上で、且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。   The first and second ratios K1 and K2 calculated by the ratio calculator 420 are given to the comparison determination unit 440. The comparison determination unit 440 determines the presence of a flame when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.

このように3番目の波長としてCO2の共鳴放射による4.5μm波長帯域に隣接した5.1μm波長帯域の放射強度を検知して炎判定を行うことで、炎以外の赤外線放射体、例えば、太陽光等の高温放射体や、300°C程度の比較的低温の放射体、人体などの低温放射体等との識別判定をより確実に行うことできる。 Thus, by detecting the radiation intensity of the 5.1 μm wavelength band adjacent to the 4.5 μm wavelength band due to the resonance radiation of CO 2 as the third wavelength and performing flame determination, an infrared radiator other than the flame, for example, It is possible to more reliably discriminate and discriminate from a high-temperature radiator such as sunlight, a relatively low-temperature radiator of about 300 ° C., a low-temperature radiator such as a human body, and the like.

図15は図14の炎判定部の機能をプロセッサによるプログラムの実行により実現する場合の炎判定処理を示したフローチャートである。図15において、炎判定処理は、ステップS21でA/D変換器24aからの4.5μm受光信号e1を積分した4.5μm積分値E1を読込み、ステップS22でA/D変換器24bからの近赤外受光信号e2を所定時間Tdだけ遅延して積分した近赤外積分値E2を読込み、更にステップS23でA/D変換器24cからの近赤外受光信号e3を積分した近赤外積分値E3を読込む。   FIG. 15 is a flowchart showing a flame determination process when the function of the flame determination unit in FIG. 14 is realized by executing a program by a processor. In FIG. 15, the flame determination process reads the 4.5 μm integrated value E1 obtained by integrating the 4.5 μm light reception signal e1 from the A / D converter 24a in step S21, and in step S22, the near value from the A / D converter 24b. A near-infrared integrated value E2 obtained by integrating the near-infrared light receiving signal e3 from the A / D converter 24c in step S23 is read after the infrared receiving signal e2 is delayed and integrated by a predetermined time Td. Read E3.

続いてステップS24に進み、第1及び第2比率K1,K2を
K1=E1/E2
K2=E1/E3
として計算する。続いてステップS25で第1比率K1が所定の第1判定閾値Kth1以上か否か判定し、第1判定閾値Kth1以上であることを判定した場合はステップS26に進み、第2比率K2が所定の第2判定閾値Kth2以上か否か判定する。ステップS26で第2比率K2が所定の第2判定閾値Kth2以上であることを判定した場合はステップS27に進み、炎の存在を判定したことで発報回路28を動作させ、火災発報信号を受信機に出力させる。
Then, it progresses to step S24, and 1st and 2nd ratio K1, K2 is set to K1 = E1 / E2.
K2 = E1 / E3
Calculate as Subsequently, in step S25, it is determined whether or not the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1, and if it is determined that the first ratio K1 is equal to or greater than the first determination threshold value Kth1, the process proceeds to step S26, It is determined whether or not the second determination threshold value Kth2 or more. If it is determined in step S26 that the second ratio K2 is equal to or greater than the predetermined second determination threshold value Kth2, the process proceeds to step S27, and the alarm circuit 28 is operated by determining the presence of flame, and the fire alarm signal is transmitted. Output to the receiver.

図16は図13に設けた炎判定部の他の実施形態となる機能構成を示したブロック図である。本実施形態の炎判定部26にあっては、近赤外受光信号e2が極端に大きくなった場合の外乱光となるアーク溶接光による感度低下を抑制するため、近赤外受光信号e2が所定レベルを超えた場合、近赤外受光信号e2の代りに所定の定数cを使用して4.5μm受光信号との比率Kを求めることでアーク溶接光による感度低下を抑制するようにしたことを特徴とする。   FIG. 16 is a block diagram showing a functional configuration according to another embodiment of the flame determination unit provided in FIG. In the flame determination unit 26 of the present embodiment, the near-infrared light reception signal e2 is predetermined in order to suppress a decrease in sensitivity due to arc welding light that becomes disturbance light when the near-infrared light reception signal e2 becomes extremely large. When the level is exceeded, a predetermined constant c is used in place of the near-infrared light receiving signal e2, and the ratio K to the 4.5 μm light receiving signal is obtained to suppress the decrease in sensitivity due to arc welding light. Features.

図16の炎判定部260にあっては、新たに定数設定器34、比較器36及び切替器40を設けており、それ以外の構成は図14の実施形態と同じになる。   In the flame determination unit 260 of FIG. 16, a constant setter 34, a comparator 36, and a switcher 40 are newly provided, and other configurations are the same as those of the embodiment of FIG.

比率演算器420は、積分器32bからの近赤外積分信号E2が基準電圧源38で設定した受光閾値Eth未満の場合の比較器36のLレベル出力で、図示のように、切替器40を切替端子aに切替えて積分器32bからの近赤外積分信号E2を入力し、4.5μm積分信号E1、近赤外積分信号E2及び5.1μm積分信号E3から第1比率K1及び第2比率K2として
K1=E1/E2
K2=E1/E3
を求める。
The ratio calculator 420 is an L level output of the comparator 36 when the near-infrared integrated signal E2 from the integrator 32b is less than the light reception threshold Eth set by the reference voltage source 38, and the switch 40 is switched as shown in the figure. Switching to the switching terminal a and inputting the near infrared integration signal E2 from the integrator 32b, the first ratio K1 and the second ratio from the 4.5 μm integration signal E1, the near infrared integration signal E2, and the 5.1 μm integration signal E3. As K2, K1 = E1 / E2
K2 = E1 / E3
Ask for.

また比率演算器420は、積分器32bからの近赤外積分信号E2が基準電圧源38で設定した受光閾値Eth以上の場合の比較器36のHレベル出力で、切替器40を切替端子bに切替えて定数設定器34bからの定数cを入力し、4.5μm積分信号E1、近赤外積分信号E2に代る定数c及び5.1μm積分信号E3から第1比率K1及び第2比率K2として
K1=E1/c
K2=E1/E3
を求める。
The ratio calculator 420 is an H level output of the comparator 36 when the near-infrared integrated signal E2 from the integrator 32b is equal to or higher than the light reception threshold Eth set by the reference voltage source 38, and the switch 40 is switched to the switch terminal b. The constant c from the constant setter 34b is input and the 4.5 μm integration signal E1, the constant c in place of the near infrared integration signal E2, and the 5.1 μm integration signal E3 are used as the first ratio K1 and the second ratio K2. K1 = E1 / c
K2 = E1 / E3
Ask for.

比率演算器420で算出された第1及び第2比率K1,K2は比較判定部440に与えられる。比較判定部440は、第1比率K1が所定の第1判定閾値Kth1以上で、且つ第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定する。   The first and second ratios K1 and K2 calculated by the ratio calculator 420 are given to the comparison determination unit 440. The comparison determination unit 440 determines the presence of a flame when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.

図17は図16の炎判定部の機能をプロセッサによるプログラムの実行により実現する場合の炎判定処理を示したフローチャートである。図17において、炎判定処理は、ステップS31でA/D変換器24aからの4.5μm受光信号e1を積分した4.5μm積分値E1を読込み、ステップS32でA/D変換器24bからの近赤外受光信号e2を所定時間Tdだけ遅延して積分した近赤外積分値E2を読込み、更にステップS13でA/D変換器24cからの近赤外受光信号e3を積分した近赤外積分値E3を読込む。   FIG. 17 is a flowchart showing a flame determination process when the function of the flame determination unit in FIG. 16 is realized by executing a program by a processor. In FIG. 17, the flame determination process reads the 4.5 μm integrated value E1 obtained by integrating the 4.5 μm light reception signal e1 from the A / D converter 24a in step S31, and in step S32, the near-in process from the A / D converter 24b. The near-infrared integrated value E2 obtained by integrating the near-infrared light receiving signal e3 from the A / D converter 24c in step S13 is read after the infrared receiving signal e2 is delayed and integrated by a predetermined time Td. Read E3.

続いてステップS34で近赤外積分値E2が所定の受光閾値Eth未満か否か判別し、受光閾値Eth未満を検知した場合はステップS35に進み、第1及び第比率K1,K2を
K1=E1/E2
K2=E1/E3
として計算する。
Subsequently, in step S34, it is determined whether or not the near-infrared integrated value E2 is less than a predetermined light reception threshold Eth. If the light reception threshold Eth is detected, the process proceeds to step S35, and the first and first ratios K1 and K2 are set to K1 = E1. / E2
K2 = E1 / E3
Calculate as

一方、ステップS34で近赤外積分値E2が所定の受光閾値Eth以上となることを検知した場合はステップS36に進み、近赤外積分値E2を定数cに変更し、第1及び第比率K1,K2を
K1=E1/c
K2=E1/E3
として計算する。
On the other hand, if it is detected in step S34 that the near-infrared integrated value E2 is equal to or greater than the predetermined light receiving threshold Eth, the process proceeds to step S36, where the near-infrared integrated value E2 is changed to a constant c, and the first and first ratios K1. , K2 with K1 = E1 / c
K2 = E1 / E3
Calculate as

続いてステップS38で第1比率K1が所定の第1判定閾値Kth1以上か否か判定し、第1判定閾値Kth1以上であることを判定した場合はステップS39に進み、第2比率K2が所定の第2判定閾値Kth2以上か否か判定する。ステップS39で第2比率K2が所定の第2判定閾値Kth2以上であることを判定した場合はステップS40に進み、炎の存在を判定していることで発報回路28を動作させ、火災発報信号を受信機に出力させる。   Subsequently, in step S38, it is determined whether or not the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1, and when it is determined that the first ratio K1 is equal to or greater than the first determination threshold value Kth1, the process proceeds to step S39, It is determined whether or not the second determination threshold value Kth2 or more. If it is determined in step S39 that the second ratio K2 is equal to or greater than the predetermined second determination threshold value Kth2, the process proceeds to step S40, and the alarm circuit 28 is operated by determining the presence of the flame, and the fire alarm is generated. The signal is output to the receiver.

なお、上記の実施形態にあっては、近赤外受光信号をリアルタイムで所定時間Td遅延して4.5μm受光信号との時間ずれを低減しているが、近赤外受光信号と4.5μm受光信号をメモリに一時的に記憶し、読出し位置を遅延時間に対応したアドレス分シフトして読み出すことで、時間ずれを補正するようしても良い。   In the above embodiment, the near-infrared light reception signal is delayed by a predetermined time Td in real time to reduce the time shift from the 4.5 μm light reception signal. The time shift may be corrected by temporarily storing the received light signal in the memory and shifting the read position by an address corresponding to the delay time.

また、溶接時、特に溶接開始時の遅延時間Tdのばらつきにより、近赤外受光信号e2と4.5μm受光信号e1が立ち上がるタイミングのずれが所定時間Tdより短かった場合には、比率K1が大きくなり、Kth1を超えてしまうことも考えられるが、例えば近赤外受光信号e2の読み出し終了位置を4.5μm受光信号e1の読み出し終了位置と同じ程度まで伸ばすことにより、この問題への対策を行っても良い。   In addition, when the difference in the rise time of the near-infrared light reception signal e2 and the 4.5 μm light reception signal e1 is shorter than the predetermined time Td due to variations in the delay time Td at the start of welding, particularly the welding start time, the ratio K1 is large. However, Kth1 may be exceeded. For example, the read end position of the near-infrared light reception signal e2 is extended to the same extent as the read end position of the 4.5 μm light reception signal e1 to take measures against this problem. May be.

また、上記の実施形態にあっては、炎の存在を判定した場合に発報回路の動作で受信機からの感知回線の発報電流を流して火災発報信号を送出しているが、発報回路に代えて適宜の伝送回路を設け、炎判定に基づき火災信号を受信側に伝送するようにしても良い。   Also, in the above embodiment, when the presence of a flame is determined, a fire alarm signal is sent by causing the alarm current of the sensing line from the receiver to flow by the operation of the alarm circuit. An appropriate transmission circuit may be provided instead of the information circuit, and the fire signal may be transmitted to the receiving side based on the flame determination.

また上記の実施形態の3波長方式にあっては、CO2の共鳴放射による4.5μm付近の波長帯域に隣接した長波長側の5.1μm付近の波長帯域の放射強度を検知しているが、4.5μm付近の波長帯域に隣接した短波長側の3.8μm付近の波長帯域の放射強度を検知するようにしても良い。 In the three-wavelength system of the above embodiment, the radiation intensity in the wavelength band near 5.1 μm on the long wavelength side adjacent to the wavelength band near 4.5 μm due to the resonance radiation of CO 2 is detected. The radiation intensity in the wavelength band near 3.8 μm on the short wavelength side adjacent to the wavelength band near 4.5 μm may be detected.

また本発明は上記の実施形態に限定されず、その目的と利点を損なうことのない適宜の変形を含み、更に上記の実施形態に示した数値による限定は受けない。
The present invention is not limited to the above-described embodiments, includes appropriate modifications that do not impair the objects and advantages thereof, and is not limited by the numerical values shown in the above-described embodiments.

10:炎感知器
11a,11b,11c:第1〜第3検知部
12a,12b,12c:センサモジュール
14a,14b,14c:第1〜第3光学フィルタ
16a,16b,16c:第1〜第3受光素子
18a,18b,18c:第1〜第3周波数抽出部
20a,20b,20c:プリアンプ
22a,22b,22c:メインアンプ
24a,24b,24c:A/D変換器
26,260:炎判定部
28:発報回路
31:遅延器
32a,32b,32c:積分器
34:定水設定器
36,44:比較器
38,45:基準電圧源
40:切替器
42,420:比率演算器
440:比較判定部
10: Flame detectors 11a, 11b, 11c: First to third detectors 12a, 12b, 12c: Sensor modules 14a, 14b, 14c: First to third optical filters 16a, 16b, 16c: First to third Light receiving elements 18a, 18b, 18c: first to third frequency extraction units 20a, 20b, 20c: preamplifiers 22a, 22b, 22c: main amplifiers 24a, 24b, 24c: A / D converters 26, 260: flame determination unit 28 : Alarm circuit 31: delay units 32a, 32b, 32c: integrator 34: constant water setting unit 36, 44: comparator 38, 45: reference voltage source 40: switch 42, 420: ratio calculator 440: comparison judgment Part

Claims (26)

有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第1受光信号を出力する第1検知部と、
所定の波長帯域の近赤外線光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第2受光信号を出力する第2検知部と、
前記第1検知部からの第1受光信号と前記第2検知部からの第2受光信号との時間的なずれを補正する補正部と、
前記補正部で時間的なずれが補正された前記第1受光信号と第2受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定する炎判定部と、
前記炎判定部で炎の存在を判定した場合に火災信号を出力する発報回路と、
を備えたことを特徴とする炎感知器。
Narrowband wavelength light centered around 4.5 μm emitted by CO 2 resonance generated during flammable combustion is selectively transmitted and converted into an electrical signal, and a signal component of a predetermined frequency is converted from the electrical signal. A first detector for selectively extracting and outputting a first light receiving signal;
A second detector that selectively transmits near-infrared light in a predetermined wavelength band, converts the light into an electrical signal, selectively extracts a signal component of a predetermined frequency from the electrical signal, and outputs a second received light signal;
A correction unit that corrects a time lag between the first light reception signal from the first detection unit and the second light reception signal from the second detection unit;
A flame determination unit that discriminates between the presence of a flame and a radiation source of arc welding light based on the first light reception signal and the second light reception signal in which the time shift is corrected by the correction unit;
An alarm circuit that outputs a fire signal when the flame determination unit determines the presence of flame,
A flame detector characterized by comprising:
請求項1記載の炎感知器に於いて、
前記補正部は、前記第2検知部からの第2受光信号を所定時間遅延して前記第1受光信号との時間ずれを抑制することを特徴とする炎感知器。
The flame detector according to claim 1,
The flame detector is characterized in that the correction unit delays the second light reception signal from the second detection unit for a predetermined time and suppresses a time lag from the first light reception signal.
請求項1記載の炎感知器に於いて、
前記第1検知部は、
有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過させる第1光学フィルタと、
前記第1光学フィルタを透過した透過した光を受光し電気信号に変換して出力する第1受光素子と、
前記第1受光素子の出力から所定の周波数の信号成分を選択抽出して第1受光信号を出力する第1周波数抽出部と、
を備え、
前記第2検知部は、
所定の波長帯域の近赤外線光を透過させる第2光学フィルタと、
前記第2光学フィルタを透過した光を受光し電気信号に変換して出力する第2受光素子と、
前記第2の受光素子の出力から所定の周波数の信号成分を選択抽出して第2受光信号を出力する第2周波数抽出部と、
を備えたことを特徴とする炎感知器。
The flame detector according to claim 1,
The first detector is
A first optical filter that selectively transmits light having a narrow band wavelength centered around 4.5 μm, which is emitted by CO 2 resonance generated during flammable combustion;
A first light receiving element that receives the transmitted light that has passed through the first optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A first frequency extraction unit that selectively extracts a signal component of a predetermined frequency from the output of the first light receiving element and outputs a first light receiving signal;
With
The second detector is
A second optical filter that transmits near-infrared light in a predetermined wavelength band;
A second light receiving element that receives light transmitted through the second optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A second frequency extracting section for selectively extracting a signal component of a predetermined frequency from the output of the second light receiving element and outputting a second light receiving signal;
A flame detector characterized by comprising:
請求項3記載の炎感知器に於いて、前記第2光学フィルタは、0.7μm乃至1.0μm付近の波長帯域の近赤外線光を透過させることを特徴とする炎感知器。
4. The flame sensor according to claim 3, wherein the second optical filter transmits near-infrared light having a wavelength band in the vicinity of 0.7 μm to 1.0 μm.
請求項3記載の炎感知器に於いて、前記第2光学フィルタと第2受光素子は、近赤外帯域の光を透過させる透過窓を備え、近赤外帯域の所定波長にピーク波長を持つフォトトランジスタまたはフォトダイオードであることを特徴とする炎感知器。
4. The flame detector according to claim 3, wherein the second optical filter and the second light receiving element include a transmission window that transmits light in the near infrared band, and has a peak wavelength at a predetermined wavelength in the near infrared band. A flame detector, which is a phototransistor or a photodiode.
請求項1記載の炎感知器に於いて、前記判定部は、
前記第1受光信号e1と第2受光信号e2との比率K−e1/e2を求め、当該比率Kが所定の閾値Kth以上の場合に炎の存在を判定することを特徴とする炎感知器。
The flame detector according to claim 1, wherein the determination unit includes:
A flame detector characterized in that a ratio K-e1 / e2 between the first light receiving signal e1 and the second light receiving signal e2 is obtained, and the presence of a flame is determined when the ratio K is equal to or greater than a predetermined threshold value Kth.
請求項1記載の炎感知器に於いて、前記判定部は、
前記第2受光信号e2が所定の受光閾値eth未満の場合は、前記第第1受光信号e1と前記第2受光信号e2との比率K=e1/e2を求め、
前記第2受光信号e2が前記受光閾値eth以上の場合は、前記第1受光信号e1と所定の定数cの比率K=e1/cを求め、
前記比率Kが所定の判定閾値Kth以上の場合に炎の存在を判定することを特徴とする炎感知器。
The flame detector according to claim 1, wherein the determination unit includes:
When the second light reception signal e2 is less than a predetermined light reception threshold eth, a ratio K = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained.
When the second light reception signal e2 is equal to or greater than the light reception threshold eth, a ratio K = e1 / c between the first light reception signal e1 and a predetermined constant c is obtained.
The flame detector, wherein the presence of flame is determined when the ratio K is equal to or greater than a predetermined determination threshold value Kth.
請求項1記載の炎感知器に於いて、更に、
有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光のみを選択透過させて電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出する第3検知部と、
を設け、
前記炎判定部は、前記第1検知部、第2検知部及び第3検知部からの前記第1受光信号、第2受光信号及び第3受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することを特徴とする炎感知器。
The flame detector of claim 1, further comprising:
Only light of a narrow band wavelength centered on a predetermined wavelength adjacent to a wavelength band centered on 4.5 μm emitted by CO 2 resonance generated during flammable combustion is selectively transmitted and converted into an electrical signal. A third detector for selectively extracting a signal component of a predetermined frequency from the electrical signal;
Provided,
The flame determination unit includes the presence of flame and radiation of arc welding light based on the first light reception signal, the second light reception signal, and the third light reception signal from the first detection unit, the second detection unit, and the third detection unit. A flame sensor characterized by distinguishing and determining a source.
請求項8記載の炎感知器に於いて、前記第3検知部は、
4.5μm付近を中心波長とする波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光を選択透過させる第3光学フィルタと、
前記第3光学フィルタを透過した透過した光を受光し電気信号に変換して出力する第3受光素子と、
前記第3受光素子の出力から所定の周波数の信号成分を選択抽出して第3受光信号を出力する第3周波数抽出部と、
を備えることを特徴とする炎感知器。
The flame detector according to claim 8, wherein the third detector is
A third optical filter that selectively transmits light having a narrowband wavelength centered on a predetermined wavelength adjacent to a wavelength band centered around 4.5 μm;
A third light receiving element that receives the transmitted light that has passed through the third optical filter, converts the light into an electrical signal, and outputs the electrical signal;
A third frequency extracting section for selectively extracting a signal component of a predetermined frequency from the output of the third light receiving element and outputting a third light receiving signal;
A flame detector comprising:
請求項9記載の炎感知器に於いて、前記第3光学フィルタは、前記第1光学フィルタの4.5μm付近を中心波長とする透過狭波長帯域に隣接した5.1μm付近または3.8μm付近を中心波長とする狭帯域波長の光のみを選択透過させることを特徴とする炎感知器。
10. The flame sensor according to claim 9, wherein the third optical filter is adjacent to a transmission narrow wavelength band having a central wavelength around 4.5 μm of the first optical filter, near 5.1 μm or near 3.8 μm. A flame detector characterized by selectively transmitting only light having a narrow band wavelength centered at the center wavelength.
請求項8記載の炎感知器に於いて、前記判定部は、
前記第1受光信号e1と前記第2受光信号e2との第1比率K1=e1/e2を求めると共に前記第3受光信号e3と前記第2受光信号e2との第2比率K2=e3/e2を求め、
前記第1比率K1が所定の第1判定閾値Kth1以上で且つ前記第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定することを特徴とする炎感知器。
The flame detector according to claim 8, wherein the determination unit includes:
A first ratio K1 = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained, and a second ratio K2 = e3 / e2 between the third light reception signal e3 and the second light reception signal e2 is obtained. Seeking
The flame detector, wherein the presence of flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.
請求項8記載の炎感知器に於いて、前記判定部は、
前記第2受光信号e2が所定の受光閾値eth以上の場合は、前記第1受光信号e1と前記第2受光信号e2との第1比率K1=e1/e2を求めると共に前記第3受光信号e3と前記第2受光信号e2との第2比率K2=e3/e2を求め、
前記第2受光信号が前記受光閾値eth未満の場合は、前記第1受光信号e1と所定の定数cとの第1比率K1=e1/cを求めると共に前記第3受光信号e3と前記定数cとの第2比率K2=e3/cを求め、前記第1比率K1が所定の第1判定閾値Kth1以上で且つ前記第2比率Kが所定の第2判定閾値Kth2以上の場合に炎の存在を判定することを特徴とする炎感知器。
The flame detector according to claim 8, wherein the determination unit includes:
When the second light receiving signal e2 is equal to or greater than a predetermined light receiving threshold eth, a first ratio K1 = e1 / e2 between the first light receiving signal e1 and the second light receiving signal e2 is obtained and the third light receiving signal e3 is obtained. A second ratio K2 = e3 / e2 with respect to the second received light signal e2 is obtained,
When the second light receiving signal is less than the light receiving threshold eth, a first ratio K1 = e1 / c between the first light receiving signal e1 and a predetermined constant c is obtained and the third light receiving signal e3 and the constant c are obtained. Second ratio K2 = e3 / c is determined, and the presence of flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K is equal to or greater than a predetermined second determination threshold value Kth2. A flame detector characterized by
請求項1又は8記載の炎感知器に於いて、前記判定部は、前記第1信号乃至第3受光信号を積分した積分信号に基づいて炎の存在を判定することを特徴とする炎感知器。
9. The flame detector according to claim 1, wherein the determination unit determines the presence of a flame based on an integrated signal obtained by integrating the first signal to the third light reception signal. .
第1検知部により、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第1受光信号を出力し、
第2検知部により、所定の波長帯域の近赤外線光を選択透過して電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第2受光信号を出力し、
補正部により、前記第1検知部からの第1受光信号と前記第2検知部からの第2受光信号との時間的なずれを補正し、
炎判定部により、前記補正部で時間的なずれが補正された前記第1受光信号と第2受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することを特徴とする炎判定方法。
The first detector selectively transmits light having a narrow band wavelength centered around 4.5 μm, which is radiated by CO 2 resonance generated during flammable combustion, and converts it into an electrical signal. The first light receiving signal is output by selectively extracting the signal component of the frequency of
The second detector selectively transmits near-infrared light in a predetermined wavelength band and converts it into an electrical signal, selectively extracts a signal component of a predetermined frequency from the electrical signal, and outputs a second received light signal.
The correction unit corrects a time lag between the first light reception signal from the first detection unit and the second light reception signal from the second detection unit,
The flame determination unit discriminates and determines the presence of the flame and the radiation source of the arc welding light based on the first light reception signal and the second light reception signal whose time shift is corrected by the correction unit. Flame judgment method.
請求項14記載の炎判定方法に於いて、
前記補正部により、前記第2検知部からの第2受光信号を所定時間遅延して前記第1受光信号との時間ずれを抑制することを特徴とする炎判定方法。
In the flame judgment method according to claim 14,
A flame determination method, wherein the correction unit delays the second light reception signal from the second detection unit for a predetermined time to suppress a time lag with the first light reception signal.
請求項14記載の炎判定方法に於いて、
前記第1検知部は、
第1光学フィルタにより、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする狭帯域波長の光を選択透過し、
第1受光素子により、前記第1光学フィルタを透過した透過した光を受光し電気信号に変換して出力し、
第1周波数抽出部により、前記第1受光素子の出力から所定の周波数の信号成分を選択抽出して第1受光信号を出力し、
前記第2検知部は、
第2光学フィルタにより、所定の波長帯域の近赤外線光を透過し、
第2受光素子により、前記第2光学フィルタを透過した光を受光し電気信号に変換して出力し、
第2周波数抽出部により、前記第2の受光素子の出力から所定の周波数の信号成分を選択抽出して第2受光信号を出力する、
ことを特徴とする炎判定方法。
In the flame judgment method according to claim 14,
The first detector is
The first optical filter selectively transmits light having a narrow band wavelength centered around 4.5 μm, which is emitted by CO 2 resonance generated during flammable combustion,
The first light receiving element receives the transmitted light that has passed through the first optical filter, converts it into an electrical signal, and outputs it.
A first frequency extraction unit selectively extracts a signal component of a predetermined frequency from the output of the first light receiving element and outputs a first light receiving signal;
The second detector is
The second optical filter transmits near infrared light of a predetermined wavelength band,
The second light receiving element receives the light transmitted through the second optical filter, converts it into an electrical signal, and outputs it.
A second frequency extraction unit that selectively extracts a signal component of a predetermined frequency from the output of the second light receiving element and outputs a second light receiving signal;
A flame determination method characterized by the above.
請求項16記載の炎判定方法に於いて、前記第2光学フィルタは、0.7μm乃至1.0μm付近の波長帯域の近赤外線光を透過させることを特徴とする炎判定方法。
17. The flame determination method according to claim 16, wherein the second optical filter transmits near-infrared light in a wavelength band near 0.7 μm to 1.0 μm.
請求項16記載の炎判定方法に於いて、前記第2光学フィルタと第2受光素子は、近赤外帯域の光を透過させる透過窓を備え、近赤外帯域の所定波長にピーク波長を持つフォトトランジスタまたはフォトダイオードであることを特徴とする炎判定方法。
17. The flame determination method according to claim 16, wherein the second optical filter and the second light receiving element include a transmission window that transmits light in a near infrared band, and has a peak wavelength at a predetermined wavelength in the near infrared band. A flame determination method comprising a phototransistor or a photodiode.
請求項16記載の炎判定方法に於いて、前記判定部は、
前記第1受光信号e1と第2受光信号e2との比率を求め、当該比率K=e1/e2が所定の閾値Kth以上の場合に炎の存在を判定することを特徴とする炎判定方法。
The flame determination method according to claim 16, wherein the determination unit includes:
A flame determination method characterized by obtaining a ratio between the first light reception signal e1 and the second light reception signal e2 and determining the presence of a flame when the ratio K = e1 / e2 is equal to or greater than a predetermined threshold value Kth.
請求項16記載の炎判定方法に於いて、前記判定部は、
前記第2受光信号e2が所定の受光閾値eth未満の場合は、前記第第1受光信号e1と前記第2受光信号e2との比率K=e1/e2を求め、
前記第2受光信号e2が所定の受光閾値eth以上の場合は、前記第1受光信号e1と、所定の定数cの比率K=e1/cを求め、
前記比率が所定の判定閾値Kth以上の場合に炎の存在を判定することを特徴とする炎判定方法。
The flame determination method according to claim 16, wherein the determination unit includes:
When the second light reception signal e2 is less than a predetermined light reception threshold eth, a ratio K = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained.
When the second light reception signal e2 is equal to or greater than a predetermined light reception threshold eth, a ratio K = e1 / c between the first light reception signal e1 and a predetermined constant c is obtained.
A flame determination method, wherein the presence of a flame is determined when the ratio is equal to or greater than a predetermined determination threshold value Kth.
請求項16記載の炎判定方法に於いて、更に、
第3検知部により、有炎燃焼時に発生するCO2共鳴により放射される、4.5μm付近を中心波長とする波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光のみを選択透過させて電気信号に変換し、当該電気信号から所定の周波数の信号成分を選択抽出して第3受光信号を出力し、
前記炎判定部は、前記第1検知部、第2検知部及び第3検知部からの前記第1受光信号、第2受光信号及び第3受光信号に基づいて炎の存在とアーク溶接光の放射線源とを識別判定することを特徴とする炎判定方法。
The flame determination method according to claim 16, further comprising:
The third detector selectively transmits only light having a narrow band wavelength centered on a predetermined wavelength adjacent to a wavelength band centered around 4.5 μm and emitted by CO 2 resonance generated during flammable combustion. And converting it into an electrical signal, selectively extracting a signal component of a predetermined frequency from the electrical signal and outputting a third light receiving signal,
The flame determination unit includes the presence of flame and radiation of arc welding light based on the first light reception signal, the second light reception signal, and the third light reception signal from the first detection unit, the second detection unit, and the third detection unit. A flame determination method characterized by discriminating and determining a source.
請求項21記載の炎判定方法に於いて、前記第3検知部は、
第3光学フィルタにより、前記第1光学フィルタの透過波長帯域に隣接した所定波長を中心波長とする狭帯域波長の光のみを選択透過させた光を第3受光素子により受光し電気信号に変換して出力し、
第3周波数抽出部により、前記第3受光素子の出力から所定の周波数の信号成分を選択抽出して第3受光信号を出力する、
ことを特徴とする炎判定方法。
The flame determination method according to claim 21, wherein the third detection unit includes:
With the third optical filter, the third light receiving element receives light that selectively transmits only light having a narrow band wavelength centered on a predetermined wavelength adjacent to the transmission wavelength band of the first optical filter, and converts it into an electrical signal. Output,
A third frequency extraction unit selectively extracts a signal component of a predetermined frequency from the output of the third light receiving element and outputs a third light receiving signal;
A flame determination method characterized by the above.
請求項22記載の炎判定方法に於いて、前記第3光学フィルタは、前記第1光学フィルタの透過波長帯域に隣接した3.8μm付近または5.1μm付近を中心波長とする狭帯域波長の光のみを選択透過させることを特徴とする炎判定方法。
23. The flame determination method according to claim 22, wherein the third optical filter is a light having a narrow band wavelength having a central wavelength near 3.8 μm or 5.1 μm adjacent to the transmission wavelength band of the first optical filter. A flame determination method characterized by selectively allowing only the permeation.
請求項21記載の炎判定方法に於いて、前記判定部は、
前記第1受光信号e1と前記第2受光信号e2との第1比率K1=e1/e2を求めると共に前記第3受光信号e3と前記第2受光信号e2との第2比率K2=e3/e2を求め、
前記第1比率K1が所定の第1判定閾値Kth1以上で且つ前記第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定することを特徴とする炎判定方法。
The flame determination method according to claim 21, wherein the determination unit includes:
A first ratio K1 = e1 / e2 between the first light reception signal e1 and the second light reception signal e2 is obtained, and a second ratio K2 = e3 / e2 between the third light reception signal e3 and the second light reception signal e2 is obtained. Seeking
A flame determination method, wherein the presence of a flame is determined when the first ratio K1 is equal to or greater than a predetermined first determination threshold value Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold value Kth2.
請求項21記載の炎判定方法に於いて、前記判定部は、
前記第2受光信号e2が所定の受光閾値eth以上の場合は、前記第1受光信号e1と前記第2受光信号e2との第1比率K1=e1/e2を求めると共に前記第3受光信号e3と前記第2受光信号e2との第2比率K2=e3/e2を求め、
前記第2受光信号e2が前記受光閾値eth未満の場合は、前記第1受光信号e1と所定の定数cとの第1比率K1=e1/cを求めると共に前記第3受光信号e3と前記定数cとの第2比率K2=e3/cを求め、前記第1比率K1が所定の第1判定閾値Kth1以上で且つ前記第2比率K2が所定の第2判定閾値Kth2以上の場合に炎の存在を判定することを特徴とする炎判定方法。
The flame determination method according to claim 21, wherein the determination unit includes:
When the second light receiving signal e2 is equal to or greater than a predetermined light receiving threshold eth, a first ratio K1 = e1 / e2 between the first light receiving signal e1 and the second light receiving signal e2 is obtained and the third light receiving signal e3 is obtained. A second ratio K2 = e3 / e2 with respect to the second received light signal e2 is obtained,
When the second light reception signal e2 is less than the light reception threshold eth, a first ratio K1 = e1 / c between the first light reception signal e1 and a predetermined constant c is obtained, and the third light reception signal e3 and the constant c are obtained. The second ratio K2 = e3 / c is calculated, and the presence of flame is detected when the first ratio K1 is equal to or greater than a predetermined first determination threshold Kth1 and the second ratio K2 is equal to or greater than a predetermined second determination threshold Kth2. A flame determination method characterized by determining.
請求項16又は21記載の炎判定方法に於いて、前記判定部は、前記第1信号乃至第3受光信号を積分した積分受光信号に基づいて炎の存在を判定することを特徴とする炎判定方法。   The flame determination method according to claim 16 or 21, wherein the determination unit determines the presence of a flame based on an integrated light reception signal obtained by integrating the first signal to the third light reception signal. Method.
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JP2021096095A (en) * 2019-12-16 2021-06-24 富士電機株式会社 Arc beam detector
JP7382816B2 (en) 2019-12-16 2023-11-17 富士電機株式会社 Arc light detection device

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