Fire sensing system, process for sensing fire and environment monitor

Abstract: The system includes infrared sensors with sensing wavelength bands sensing an infrared radiation from an infrared sources(S). One of the sensing wavelength bands is a CO₂-molecular resonance radiation wavelength band. The system determines whether a disastrous fire occurs or not on the basis of outputs of the sensors and a time change in a ratio of the outputs. The process computes the temperature of the infrared source from a ratio of outputs of infrared sensors (3a, 3b, 3c, 3d) with at least two sensing wavelength bands of an infrared radiation from a monitored area, pro­ duces the intensity of infrared radiation of either of the bands from the computed temperature and computes a heating area from the intensity and the output of a corresponding infrared sensor. The process determines the progress of a fire. The monitor produces a control signal to an air conditioner or room heater-and-cooler from outputs of a sensor and an output of a thermometer.

Description: The present invention relates to fire sensing using an infrared sensing process and more particularly to a fire sensing system separating incident infrared radiation into a plurality of wavelength bands, sensing a change in the absolute value and the ratio of infrared radiation of each separated wavelength band, and determining in response to the sensed change with time whether a disastrous fire has occured or not. The present invention relates to a fire sensing system adapted for use in a fire prevention system used in a residence, a building, a warehouse, etc. requiring reliable and highly-sensitive fire sensing and which is free from false alarms caused by nondisastrous inflaming sources such as an electric heater, a gas heater and a stove. The present invention also relates to technology used with an environment monitor sensing the occurrence of a disastrous indoor fire, and an indoor environment which is unpleasant to a person and producing a signal controlling an alarm or air conditioner. A multitude of prior-art fire sensing methods and systems automatically sensing the occurrence of disastrous fire have been provided. These methods and systems intend to sense the occurrence of a disastrous fire in a predetermined monitored area and must operate so that a malfunction due to a heating source or heater providing a non-disastrous fire, e.g., a stove, rarely occurs and is highly sensitive to the occurrence of a disastrous fire. Prior-art fire sensing systems using, e.g., a phototube, bimetal or a telecamera have been provided. The phototube type fire sensing system malfunctions due to sunshine or light from an electric lamp etc. because the phototube is sensitive to the wavelength of ultraviolet. The bimetal type fire sensing system is insufficiently effective because of low fire-sensitivity of the bimetal. The telecamera type fire sensing system has difficultly in determining a situation of a fire and requires an excessive number of telecameras as well as continuous monitoring by a person, so that a desired performance is difficult to obtain. In such a situation, recently, an infrared radiation sensing process for sensing an infrared radiant from a flame has been appreciated. This infrared radiation sensing process has not only a simple system determining the occurrence of a disastrous fire when it senses infrared radiation of a predetermined level or higher but also a fire sensing system (see Examined Japanese patent application publication No.SHO 56-7196) including a determinant determining whether or not the level of an output signal from an infrared sensor tends to increase over a predetermined period of time. In addition, in order to increase reliability, efforts have been made in developing a technology of separately sensing two or more wavelength bands of an infrared radiation from a flame and of determining whether a disastrous fire occurs or not from the sensed signals. One form of this technology is a system including a sensor for visible or near infrared radiation and a sensor for infrared radiation, the system determining a nondisastrous fire when the intensity of the visible or near infrared radiation is stronger than that of the infrared radiation such as in the case of radiation from an electric lamp etc. Another form of this technology is a system sensing the intrinsic spectral distribution of a flame. The spectral distribution of infrared radiation from an infrared source lacking a flame is generally in agreement with Planck's law of radiation as shown in solid lines A and C of FIG.2 so that the higher the temperature of a heating object, the more the top of the spectral distribution shifts towards a shorter-wavelength band. On the other hand, an infrared radiant object with a flame has a different intrinsic character. That is, it has a spectral distribution with a peak as shown in solid line B of FIG.2. The peak of the spectral distribution of the solid line B is derived from the phenomenon of CO 2 -molecular resonance radiation with about 4.3µm wavelength. Thus, in principle, sensing the peak of about 4.3 µm wavelength caused by CO 2 -molecular resonance radiation senses a flame. Some attempts have been proposed in order to sense the peak of about 4.3 µm wavelength. For example, the art of Unexamined Japanese patent application publication No.SHO 50-2497 senses the amount of radiation at the 4.3 µm wavelength and at two wavelengths before and after the 4.3 µm wavelength and determines the presence of flame when each of the amounts of radiations at the 4.3 µm wavelength and at the two wavelengths before and after the 4.3 µm wavelength equals or exceeds a predetermined value. In addition, the art of Unexamined Japanese patent application publication No.SHO 57-96492 determines whether or not there is a depression between two projections in amount of radiation in order to sense the occurrence of flame. In accordance with a method of determining the occurrence of nondisastrous fire when the radiation intensity of visible or near infrared radiation is greater than the radiation intensity of the other infrared radiation as in light from an electric lamp, the occurrence of a false alarm due to a normal light from the electric lamp is rare. On the other hand, since this method determines as the occurrence of a disastrous fire the presence of a heater such as an electric heater having no or low visible or near infrared radiation, the method produces a false alarm, so that an application of the method is very restricted. In accordance with the method of sensing the amounts of radiation at the 4.3 µm wavelength and two wavelengths before and after the 4.3 µm wavelength and determining the presence of flame when each of the amounts of radiation at the 4.3 µm wavelength and two wavelengths before and after the 4.3 µm wavelength equals or exceeds the predetermined value, this method can sense the presence of flame but not determine whether the flame is derived from a disastrous fire or a normal or inflaming heater. That is, this method entails a drawback in that it can produce a false alarm in response to the occurrence of a flame of a gas range, gas stove or the like. Various prior-art air conditioners sensing indoor conditions by means of a temperature sensor and a humidity sensor in order to control a room cooler and room heater or the air conditioners thereby to produce a comfortable indoor environment have been provided. These prior-art air conditioners control an. indoor temperature in response to a sensing signal from a contact type temperature sensor, e.g., a thermistor, placed in or near the body of the air conditioners. That is, the air conditioners only consider the temperature of air surrounding the temperature sensor as an average indoor temperature to control the room heater and room cooler of the air conditioners. The temperature which a person who is indoors feels is the most important factor for controlling an indoor environment by means of air conditioners or room heaters and room coolers. The temperature of radiation heat which the skin of a human body receives due to infrared radiance from interior surfaces of a room contributes to the temperature which the body of the person feels in addition to the temperature of air in direct contact with the person's skin. For example, heat radiant from a room heater, window arrangement etc. produces a hot feeling on a human body and when a window arrangement and wall of a room absorb heat radiant from human a body this produces the feeling of a bone-reaching chill. Thus, the prior-art method of controlling an environment in response to a single temperature output of the contact type temperature sensor such as the thermistor sensing air in contact with the contact type temperature sensor cannot provide a true comfortable environment for a person. The present invention was made in view of the above-described problems. A primary object of the present invention is to provide a fire sensing system which very rarely produces a false alarm in response to normal conditions of using heaters useful for life environment, e.g., an electric heater, a gas heater and a stove and sensitively sensing the occurrence of disastrous fire. Another object of the present invention is to provide a fire sensing method capable of recognizing the progression of a fire. A further object of the present invention is to provide an environment monitor sensing a change in an indoor environment including the occurrence of a disastrous fire, able to provide an indoor environment comfortable to a person, very rarely producing a false alarm in response to normal use of a heater, and sensitively sensing the occurrence of disastrous fire. DE-A-2819183 and DE-A-3140678 disclose fire sensing systems with three detectors, each detecting a different wavelength band of infrared or near-infrared radiation. JP-A-64/74695 discloses a fire sensing system which comprises at least four band-pass filters separating infrared radiation from a source in a monitored spacing into at least four wavelength bands (λa, λb, λc and λd) ; at least four infrared sensors sensing the separated infrared radiations passing through the band-pass filters respectively; and a signal processor determining whether a disastrous fire occurs or not, and according to a first aspect of the present invention such a fire sensing system is characterised by the pass-band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by the temperature (T) of the infrared source being computed by the signal processor according to the following equation on the basis of the outputs (Va, Vb and Vd) of the infrared sensors other than that of the sensor sensing the CO 2 -molecular resonance radiation band having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi , wherein i is one selected from a, c and d, and j is one selected from a, c and d, and i is not equal to j, thereafter the infrared radiation intensity (P i ) of one of these wavelength bands being computed from the computed temperature (T); and the heating area (S) of the infrared source being computed according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of the wavelength bands, S = 2π Vi Pi' · Ai , and the blackbody radiation intensity of the infrared source of the CO 2 -molecular resonance radiation wavelength band being computed from the computed temperature (T) and the heating area (S); the computed value of the blackbody radiation intensity being compared with the output of the sensor sensing the CO 2 -moBecuoar resonance radiation band, and thereby the signal processor determines that disastrous fire is occurring when the output of the sensor sensing the CO 2 -molecular resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area tends to increase. The fire sensing system of the first aspect of the present invention senses CO 2 -molecular resonance radiation when a useful flaming heater such as a gas heater or a flaming stove provides the infrared source and determines the flaming condition of a flaming heater as a nondisastrous fire since the sensed outputs of the wavelength bands and a ratio of the sensed outputs become constant. Furthermore, this fire sensing system determines the use of a useful inflaming heater such as an electric heater as a non-disastrous fire when the inflaming heater provides the infrared source as the sensed outputs of the wavelength bands and a ratio of the sensed outputs are constant and the fire sensing system does not sense CO 2 -molecular resonance radiation. Thus, this fire sensing system eliminates the occurrence of a malfunction to be incorrectly caused by the normal condition of the useful heater thereby providing accurate fire sensing. According to a second aspect of the present invention a process for sensing a fire comprises separating infrared radiation from a source in a monitored spacing into at least four wavelength bands (λa, λb, λc and λd) through at least four band-pass filters; sensing the separated infrared radiations through at least four infrared sensors individually and determining whether or not a disastrous fire occurs characterised by the pass-band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by computing the temperature (T) of the infrared source according to the following equation on the basis of the outputs (Va, Vc and Vd) of the infrared sensors other than that of the sensor sensing the CO 2 -molecular resonance radiation band having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi , wherein i is one selected from a, c and d, and j is one selected from a, c and d, and i is not equal to j; computing the infrared radiation intensity (P i ) of one of the wavelength bands from the computed temperature (T); computing the heating area (S) of the infrared source according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of these wavelength bands, S = 2π Vi Pi' · Ai , computing the blackbody radiation intensity of the infrared source of the CO 2 -moBecuoar resonance radiation wavelength band from the computed temperature (T) and the heating area (S); and by determining whether a disastrous fire occurs or not by comparing the computed value of the blackbody radiation intensity with the output of the sensor sensing the CO 2 -molecular resonance radiation band, so that it is determined that a disastrous fire is occurring when the output of the sensor sensing the CO 2 -molecular resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area (S) tends to increase. This method may display an increasing heating area on a monitor or the like to provide information about the progression of the disastrous fire. According to a third aspect of the present invention an environmental monitor comprises at least four band-pass filters separating infrared radiation from a monitored spacing into at least four wavelength bands (λa, λb, λc and λd), at least four infrared sensors sensing the separated infrared radiations passing through the band-pass filters respectively; and a signal processor determining whether a disastrous fire occurs or not characteired by the pass band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by the temperature (T) in the monitored spacing being computed by the signal processor according to the following equation on the basis of the outputs (Va, Vc and Vd) of the infrared sensors other than that of the sensor sensing the CO 2 -molecular resonance radiation having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi , wherein i is one selected from a, c, and d, and j is one selected from a, c and d, and i is not equal to j, thereafter the infrared radiation intensity (P i ) of one of these wavelength bands being computed from the computed temperature (T); and the heating area (S) of the monitored spacing being computed according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of the wavelength bands, S = 2π Vi Pi' · Ai , and the blackbody radiation intensity of the infrared source of the CO 2 -molecular resonance radiation wavelength band being computed from the computed temperature (T) and the heating area (S); the computed value of the blackbody radiation intensity being compared with the output of the sensor sensing the CO 2 -molecular resonance radiation band, and thereby the signal processor determining that a diastrous fire is occurring when the output of the sensor sensing the CO 2 -molecular resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area (S) in the monitored spacing tends to increase. The environmental monitor of the third aspect of the present invention measures and continuously monitors the common physical quantity of the radiation temperature in order to control the radiation temperature for environment control and also recognizes an abnormal pattern of the radiation to be the occurrence of a disastrous fire. The environmental monitor senses CO 2 -molecular resonance radiation to accurately determine whether or not an inflaming electric heater, a flaming heater such as a gas heater or a flaming stove, or the occurrence of a disastrous fire causes a change in the temperature of the overall environment. Thus, this environment monitor provides a comfortably controlled environment for a person and fire-sensing free from malfunction. In the accompanying drawings:- FIG.1 is a schematic diagram of the fundamental arrangement of a fire-sensing system of one embodiment of a first aspect of the present invention; FIG.2 is a graph representing a relationship between the wavelength and amount (relative value) of an infrared radiation from an infrared source; FIG.3 is a graph representing a temperature change in the occurrence of disastrous fire; FIG.4 is a graph representing a change in a heating area in the occurrence of disastrous fire; FIG.5 is a circuit blocK diagram of one embodiment of a signal processor; FIG.6 is a graph representing a change in the output of each infrared sensor of the fire-sensing system of FIG.1 in the occurrence of disastrous fire; FIG.7 is a perspective view of one example of a package type infrared sensor; FIG.8 is an illustration of a fire-sensing system with the package type infrared sensor of FIG.7; FIG.9 is an exploded perspective view of the package type infrared sensor of FIG.7, representing the interior thereof; FIG.10 is a circuit diagram of one example of a circuit of the package type infrared sensor of FIG.7; FIG.11 is a circuit block diagram of one embodiment of a signal processor of a fire-sensing system of a second aspect of the present invention; FIG.12 is a graph representing ratios of sensing outputs of infrared sensors of a fire-sensing system of the second aspect of the present invention; FIG.13 is a graph representing ratios of the theoretical values of sensing outputs of the infrared sensors of an experimental system of the second aspect of the present invention; FIG14 is a graph representing ratios of the infrared sensors when the experimental apparatus of the second aspect of the present invention monitors a heating panel; FIG.15(A) is a graph representing a temperature change computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the heating panel; FIG.15(B) is a graph representing a change in heating area computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the heating panel; FIG.15(C) is a graph representing a change in C02-ratio computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the heating panel; FIG.16(A) is a graph representing a temperature change computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors a methanol flame; FIG.16(B) is a graph representing a change in heating area computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the methanol flame; FIG.17(A) is a graph representing a temperature change computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors a setting fire on a news paper; FIG.17(B) is a graph representing a change computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the setting fire on the news paper; FIG.17(C) is a graph representing a change in CO 2 -ratio computed from the sensing output of the infrared sensors when the experimental apparatus of the present invention monitors the setting fire on the news paper; and FIG.18 is a schematic diagram of the fundamental arrangement of one embodiment of an environment monitor of a third aspect of the present invention. The present inventors studied the phenomenal difference between a disastrous fire and nondisastrous fire and concluded as follows: The heating area and the temperature of a heater which is not a disastrous fire are fixed or become constant in a few minutes. For example, the heating area of a room heater is fixed and the temperature of the room heater becomes constant in a few minutes. In addition, the temperatures and heating areas of a match and cigar lighter not only are essentially fixed but also extinguished in a few seconds or minutes. On the other hand, a disastrous fire is characterized in that both the heating area and the temperature of the disastrous fire concurrently increase from the outbreak of the disastrous fire and also tend to increase even a few minutes after the outbreak of the disastrous fire. FIG.3 represents a temperature change during a progression from a smoking condition to a disastrous fire. FIG.4 represents a change in heating area during the progression from the smoking condition to the disastrous fire. In FIGS. 3 and 4 TF represents a flaming point of time. On the other hand, a disastrous fire without a progression from a smoking condition, e.g., an incendiary fire would produce a temperature change from the TF point of time of FIG.3 and a change in heating area from the TF point of time of FIG.4. In a disastrous fire, when infrared radiation from the fire is separated into a plurality of wavelength bands between a short-wavelength band and long-wavelength band, sensing outputs of the wavelength bands increase with time and changes in ratios of the sensing outputs with time have a characteristic behavior. That is, the intensity of each sensing output reflects the area and temperature of a heater and on the other hand, since a ratio of the sensing outputs reflects the temperature of the heater, the sensing outputs of the wavelength bands and the ratio of the sensing outputs tend to concurrently increase in the case of a smoking disastrous fire and then rapidly increase when the smoking fire transfers to a flaming fire. However, the heating area of the heater still increases while an increase in the temperature of the heater tends to stay so that the sensing outputs of the wavelength bands increase and on the other hand, the ratio of the sensing outputs essentially becomes constant. Then, at the point of time when the disastrous fire has transferred to a flaming fire, CO 2 -resonance radiation is significantly increased so that the intensity of the CO 2 -molecular resonance radiation is increased with an increase in a firing area. On the other hand, a flame which has become constant, except that of a disastrous fire, does not produce such a change with time. The inventors also considered the occurrence of a disastrous fire as an environmental change and studied a technology of monitoring the environment of a residential area and fire-sensing technology from the same viewpoint. This study concluded that in order to produce an environment in which a person staying in a room feels most comfortable, the best environment control method monitors not only an air temperature of the interior of the room but also mainly a radiation temperature of the interior of the room. The inventors have conceived that since an infrared sensor can monitor a radiation temperature and since a method of sensing a disastrous fire by means of radiation temperature is also superior, a single infrared sensor can produce an output for controlling an indoor environment by means of an air conditioner or the like and for fire-sensing. Then, the inventors studied in more detail an environment control and fire-sensing performed in response to the radiation temperature. Thus, the inventors discovered that the indoor radiation temperature was computed from ratios of outputs of a plurality of infrared sensors and in addition, from a contact type temperature sensor such as a thermistor to monitor a temperature which a human body staying in a sensed spacing actually felt, in order to control an environment so that the human body felt comfortable. Since the temperature of an indoor environment is usually about 300 K (i.e., 23°C), the top of a radiation wavelength is about 10µm. Thus, the infrared sensor preferably has a band-pass filter with a 10 µm central pass wavelength. On the other hand, when a monitored environment includes an inflaming room heater such as an electric heater, monitoring the environment by means of a single infrared sensor with the 10µm band-pass filter would determine that the temperature of the overall environment had increased even when the electric heater increases the temperature of only a part of the environment. Thus, a monitoring of the environment by means of an infrared sensor with a band-pass filter with approximately a 4 µm central pass wavelength may be preferably added. Since the intensity of 4 µm wavelength infrared radiation from an environment without a room heater is sufficiently lower than that of 10 µm wavelength infrared radiation and since the intensities of 4 µm and 10 µm wavelength infrared radiation from an environment with an inflaming room heater such as an electric heater essentially equal each other, increases in both the intensities of the 4 µm and 10 µm wavelength infrared radiations of the latter case provide a determination that the inflaming room heater heats up and on the other hand, a low intensity of the 4 µm wavelength infrared radiation of the latter case provides a determination that the temperature of the overall environment increases. Thus, the following embodiment of the present invention provides a fire-sensing system producing essentially no false alarm (i.e., very rarely producing a false alarm) in response to a normal operation of a useful heater in a living environment and highly sensitive to a disastrous fire, a fire-sensing method recognizing a progression of a fire in addition to the operations of the above fire-sensing system, and an environment monitor providing an indoor environment comfortable to a person, producing essentially no false alarm (i.e., very rarely producing a false alarm) in response to a normal operation of a useful heater in a living environment. FIG.1 is a schematic diagram of the fundamental arrangement of a fire-sensing system of one embodiment of a first aspect of the present invention; An infrared radiation sensing unit D receives infrared radiation from an infrared source S and separates the infrared radiation into a plurality of wavelength bands to sense the intensity of each of the wavelength bands. The infrared radiation sensing unit D comprises: a rotational chopper 1 periodically chopping the infrared radiation from the infrared source S; four band-pass filters 2a, 2b, 2c and 2d each of which comprises an optical filter with a different pass band, which is not restricted to a particular form; and four infrared sensors 3a, 3b, 3c and 3d each sensing passing infrared radiation through the corresponding one of the band-pass filters 2a to 2d. In accordance with the four-split system of the first embodiment of the present invention, the central wavelengths of the pass bands of the band-pass filters 2a to 2d are suitably selected. One of the band-pass filters 2a to 2d allows the wavelength band (i.e., 4.3 µm) of CO 2 -molecular resonance radiation to pass. As shown, for example, in FIG. 6, the band-pass filter 2c allows CO 2 -molecular resonance radiation to pass. The pass-band central wavelength of 5.5-8 µm should be avoided since steam contained in the air absorbs a large amount of a 5.5-8 µm wavelength infrared radiation. The number of split pass-bands may not be restricted to four but may be two or more e.g. up to at least 5. An optical filter for the band-pass filters 2a to 2d comprises a multilayer film in which, one of ZnSe, ZnS, Ge and other dielectrics are alternatively vacuum deposited one another on a substrate made of Si or the like. The thickness of the multilayer film is determined in accordance with a target pass-band. The infrared sensors 3a to 3d may be semiconductor infrared sensors, thermopiles or pyroelectric infrared sensors. The semiconductor infrared sensor is not preferable since it requires cooling. The thermopile or pyroelectric infrared sensor is preferable. The pyroelectric infrared sensor is most preferable. When each of the infrared sensors 3a to 3d is made with a thermopile, the chopper 1 may be alternatively eliminated. Since the pyroelectric infrared sensor is a differentiation sensor operating in response to only a temperature differential, it is optimum for the inventive system sensing a temperature increase. The pyroelectric infrared sensor has an arrangement in which the top surface and back surface of a thin plate made of a pyroelectric material such as lithium tantalate or Pb x Zr y O 3 have electrodes deposited thereon by vacuum deposition etc. A Si-photodiode may be alternatively used in order to sense a near-infrared band with approximately a 1 µm wavelength. A pulse motor and a direct current motor (i.e., DC motor) suitably rotates the chopper 1. The DC motor requires a rotational speed sensor such as a photointerrupter 4 in order to sense a rotational speed of the chopper 1. The pulse motor requires no interrupter since a driving pulse signal for the pulse motor provides a rotational speed of the pulse motor. A signal processor 10 receives and processes outputs of the infrared sensors 3a to 3d and the rotational speed sensing signal of the chopper 1 from the photointerrupter 4. The signal processor 10 operates on the magnitudes of the outputs of the infrared sensors 3a to 3d, the ratios of the outputs and changes in the magnitudes of the outputs and the ratios of the outputs with time, determines whether the monitored infrared source S is a disastrous fire or not on the basis of the results of the operation, and producing a signal for driving an alarm when monitored infrared source S is determined to be a disastrous fire. FIG.5 represents one example of the signal processor 10. Amplifiers 11a, 11b, 11c and 11d receive outputs of the infrared sensors 3a to 3d and amplify them to desired levels. A phase shifter 12 receives the rotational speed sensing signal from the photointerrupter 4 and produces synchronizing signals SIN and COS 90 degrees phase-shifted from each other. Synchronous detectors 13a 1 , 13b 1 , 13c 1 , and 13d 1 , and 13a 2 , 13b 2 , 13c 2 and 13d 2 receive and detect the outputs of the amplifiers 11a to lid in synchronization with the synchronizing signals SIN and cos. Square multipliers 14a 1 , 14b 1 , 14c 1 , and 14d 1 , and 14a 2 , 14b 2 , 14c 2 and 14d 2 square the detection outputs of the synchronous detectors 13a 1 to 13d 1 and 13a 2 to 13d 2 . Adders 15a, 15b, 15c and 15d add outputs of the square multipliers 14a 1 to 14d 1 and 14a 2 to 14d 2 for each channel. Square root processors 16a, 16b, 16c and 16d square root process outputs of the respective adders 15a to 15d. Thus, an operation of respectively synchronization-sensing 90-degree phase-shifting synchronizing signals of each pair and then producing an average of squared synchronization detecting outputs eliminates a phase deviation caused by a misalignment etc. between chopper 1 and each of the infrared sensors 3a to 3d. A/D converters 17a to 17d A/D convert the outputs of the square root processors 16a to 16d. A microcomputer 18 receives and processes the outputs of the A/D converters 17a to 17d. In the FIG.5 embodiment, analog square multipliers produce mean squares. On the other hand, alternatively, A/D converting synchronization-detected signals and applying them to a microcomputer can provide a mean square of them. Alternatively, A/D converting the outputs of the amplifiers 11a to 11d allows the microcomputer 18 to synchronization detect them. The microcomputer 18 operates on the sensing signals at intervals of a few seconds by timer interruption, stores data of an increase in the temperature of the infrared source and an increase in a heating area and of the presence or absence of CO 2 -molecular resonance radiation, monitors the data to determine whether the temperature and heating area of the infrared source continuously increase or not, determines an occurrence of a disastrous fire when the temperature and heating area of the infrared source are increasing, and operates a driver 19 to turn a relay RLY on thereby to operate an alarm 20. In particular, now the outputs of the infrared sensors 3a to 3d change in the case of a disastrous smoking fire is shown in FIG.6. That is, the outputs a, b, c and d of the infrared sensors 3a to 3d increase with a temperature increase and an increase in a fire-spreading area in the sequence of the outputs d, c, b and a. Since CO 2 -molecular resonance radiation sharply rises at the flaming point of time TF, the output c of the infrared sensor 3c of the outputs of the infrared sensors 3a to 3d sharply rises. Then, since the infrared source flames after the flaming point of time TF, the temperature increase is low and an increase in the amount of infrared radiation caused by an increase in the fire spreading area becomes dominant, so that the outputs a, b, c and d of the infrared sensors 3a to 3d increase but the ratios of the outputs a, b, c and d essentially become constant. Thus, comparing outputs of the infrared sensors 3a to 3d provides the temperature of the infrared source and in particular comparing, e.g., the outputs of the infrared sensors 3a, 3b and 3d of the infrared sensors 3a to 3d at the temperature of the infrared source with predetermined values provides a heating area. In addition, computing from the temperature and heating area of the infrared source produced in the above sequence of operation a blackbody radiation intensity of the infrared source, i.e., an infrared radiation intensity of the CO 2 -molecular resonance radiation wavelength band if the infrared source is a blackbody and comparing the resulting value of the blackbody, radiation intensity with the output of the infrared sensor 3c sensing a CO 2 -molecular resonance radiation band, indicates the presence or absence of CO 2 -molecular resonance radiation. Thus, when the temperature and heating area of the infrared source tend to increase for a fixed period (i.e., a few minutes) but no CO 2 -molecular resonance radiation is recognized, the occurrence of a disastrous smoking fire is determined. When, the temperature and heating area of the infrared source sharply rise at a point of time and CO 2 -molecular resonance radiation is concurrently recognized, the microcomputer 18 determines that the disastrous smoking fire has transferred to a disastrous flaming fire and increases the sound volume of the alarm 20 or changes the intensity of the sound of the alarm so as to alarm the transference. In case in which no infrared radiation is sensed suddenly passes into a case in which CO 2 -molecular resonance radiation is sensed, a heating at a high temperature corresponding to CO 2 -molecular resonance radiation is sensed and the heating area sharply rises, the microcomputer 18 determines the case as an occurrence of incendiary fire. On the other hand, when no increase in a heating area is recognized, the microcomputer 18 determines the case as a presence of a flaming heater, e.g., a flaming stove. Thus, the present invention determines the presence or absence of a disastrous fire on the basis of actual fire phenomenon thereby remarkably reducing the number of occurrences of false alarms, unlike the prior art. FIGS.7-9 illustrate an arrangement and a use of a pyroelectric sensing unit 40 packaging four band-pass filters 42a, 42b, 42c and 42d and four pyroelectric infrared sensors 43a, 43b, 43c and 43d. FIG.10 illustrates a circuit of the pyroelectric sensing unit 40. In the FIGS.7-10 case, the four pyroelectric infrared sensors 43a to 43d together form a single unit unlike the above-described embodiment of the present invention with the four infrared sensors separate from each other. As shown in FIG.9, the infrared sensing unit 40 comprises: four pyroelectric sensors 43a, 43b, 43c and 43d separately mounted within four quadrants of a disc-shaped insulating substrate 41; a window 42 of four-split band-pass filters 42a, 42b, 42c and 42d each provided in front of corresponding one of the respective pyroelectric materials; and a sealing can 46 connecting the insulating substrate 41 to the window 42, the infrared radiation sensing unit 40 providing a packaged sensor sensing the four wavelength bands of infrared radiation. The four-split band-pass filter assembly of the band-pass filters 42a to 42d is made with four dielectric multilayer films each selectively deposited on a single transparent glass substrate or four segment-type band-pass filters attached to a single transparent glass. The pyroelectric infrared sensors 43a to 43d sense the respective wavelength bands of infrared radiation passing through the band-pass filters 42a to 42d. The signal processor 10 processes the resulting sensing outputs of the pyroelectric infrared sensors 43a to 43d as in the above-described embodiment. The sealing can 46 preferably contains partition walls separating the interior spacing of the sealing can 46 into four. As shown in FIG.10, each of the pyroelectric infrared sensors 43a to 43d comprises a pair of pyroelectric elements S 1 and S 2 oppositely polarized and serially connected, one terminal of pyroelectric elements S 1 of the pyroelectric infrared sensors 43a to 43d being connected to a gate terminal of corresponding one of impedance transposition FETs 47a, 47b, 47c and 47d. A drain terminal of each of the impedance transposition FETs 47a to 47d receives the positive voltage V DD of an electric power source. A source terminal of each of the impedance transposition FETs 47a to 47d produce an output signal. A terminal of the other pyroelectric infrared sensing element S2 is connected to ground E. Respective input resistors R 1 , R 2 , R 3 and R 4 are connected between the gate terminals of the impedance transposition FETs 47a to 47d and ground E. The respective impedance transposition FETs 47a to 47d are mounted near the pyroelectric infrared sensors 43a to 43d. The input resistors R 1 to R 4 are mounted on the insulating substrate 41. Each of the impedance transposition FETs 47a to 47d is connected to corresponding one of the infrared sensors 43a to 43d and input resistors R 1 to R 4 by means of a bonding wire or soldering. The connected impedance transposition FETs 47a to 47d, pyroelectric infrared sensors 43a to 43d and input resistors R 1 to R 4 are sealed within the sealing can 46. A fire-sensing system embodying a fire-sensing method of the present invention is essentially the same as the fire-sensing system of FIG.1. FIG.11 represents an example of a signal processor 10. Amplifiers 11a, 11b, 11c and 11d receive outputs of the infrared sensors 3a to 3d and amplify them to desired levels. A/D converters 17a to 17d A/D convert the amplified sensing outputs of the amplifiers 11a to 11d and feed them to the synchronous detector 13. A signal processor 18 comprising a microcomputer or the like receives detection outputs of the synchronous detector 13 and produces a mean square of two detection outputs 90 degree phase-shifted from each other thereby to eliminate a phase shift caused by a spatial displacement between a chopper and infrared sensors, etc. The microcomputer 18 operates on the synchronous detection outputs at intervals of a few seconds by timer interruption, stores data of a temperature increase of the infrared source and an increase in heating area and of the presence or absence of CO 2 -molecular resonance radiation, monitors the data to determine whether the temperature and heating area of the infrared source continuously increases or not, determines the occurrence of a disastrous fire when the temperature and heating area of the infrared source are increasing, operates an alarm 20 and displays an increase in a computed heating area on a monitor 21. The synchronization detector 13 and signal processor 18 are separate. However, a single microcomputer may alternatively replace the synchronous detector 13 and signal processor 18. Computing the temperature and heating area of the infrared source by means of the signal processor 18 will be described hereinafter. Where the intensities per unit area of a surface for receiving infrared radiation falling on the infrared sensors 3a to 3d are Pa, Pb, Pc and Pd and outputs of the synchronous detectors 13a to 13d are Va, Vb, Vc and Vd, the outputs Va to Vd are represented as follows: Va = Pa x Aa, Vb = Pb x Ab, Vc = Pc x Ac, Vd = Pd x Ad , Wherein Aa to Ad are constants determined by the properties of the infrared sensors, band-pass filters and amplifiers. In planck's law of radiation, the blackbody radiation intensity per unit area of an infrared radiation at λ-wavelength from an object at a temperature T is represented by the following equation: P λ, T = C 1 λ5 x 1 exp C 2 λT -1 , wherein C 1 and C 2 are constants determined by the equations C 1 = 2 hc 2 and C 2 = hc/k, h: Planck constant; c: light velocity; k: Boltzmann constant. Substituting λ 1 and λ 2 wavelength bands of two infrared sensors and the infrared intensities P 1 and P 2 of the sensed bands into the equation (1) derives the following approximate equation (2) producing the temperature T: T ≈ C 2 x λ 1 - λ 2 λ 1 λ 2 x 1 ln P 2 P 1 x λ 2 5 λ 1 Substituting the sensing outputs Va and Vd of the infrared sensors 3a and 3d for λa and λd wavelength bands into the infrared intensities P 1 and P 2 of the λ1 and λ2 wavelength bands derives the following equation (3) from the equation (2): T = C' x λa - λd λa λd x 1 ln Vd Va x λd 5 λa , Wherein C' is a constant in which constant C 2 is operated on by constants Aa and Ad of the detection outputs of the wavelength bands. The equation (3) shows that providing two infrared sensors with two different sensing wavelength bands produces the temperature T of a disastrous fire or heater from a ratio of two sensing outputs of the infrared sensors. Thus, the temperature T produced by the equation (3) provides the blackbody radiation intensity Pa' at λa-wavelength per unit area in accordance with Planck's law of radiation, i.e., the equation (1). On the other hand, since the air disperses and absorbs infrared radiation from the heater, the incident intensity of the infrared radiation to the infrared sensor fails to equal the intensity of the infrared radiation from the heater and the incident intensity of the infrared radiation is in inverse proportion to a distance between the infrared sensor and the heater. Since Pa' represents the blackbody radiation intensity per unit area of the heater, the incident intensity of the infrared radiation is considered to be in proportion to the area of the surface of the heater. An experience of the present inventors taught that the sensing output Va' at λa wavelength of a sensing system could be estimated by the following equation (4): Va' = Pa' x S 2πl 2 x Aa , and the computed sensing output Va' well equalled an actual sensing output Va. In the equation (4), S represents the area of the surface of the heater, Aa represents a constant at a λa-wavelength determined by the properties of the infrared sensors, band-pass filters and amplifiers, and 1 represents a distance between the infrared sensor and the heater. Thus, the area S of the surface of the heater is computed by the following equation (5): S = 2π1 2 x Va Pa' x Aa A heating area computed by means of the equation (5) thereby recognizes a progression of a disastrous fire. The above-description with the equations 1-5 have provided a method of obtaining the temperature T and area S of the heater from the sensing outputs of the infrared sensors 3a and 3d. The sensing outputs of the infrared sensors 3a and 3c or the sensing outputs of the infrared sensors 3c and 3d may alternatively provide the temperature T and the area S of the surface of the heater. In addition, an experience of the present inventors taught that changing an infrared sensor used in computation in response to the temperature T of the heater provided a more accurate temperature T and a more accurate area S. FIG.12 represents ratios of sensing outputs of the infrared sensors 3a, 3c, and 3d of the FIG.11 embodiment when the central wavelength λa of the infrared sensor 3a is 3 µm, the central wavelength λc of the infrared sensor 3c is 5 µm, and the central wavelength λd of the infrared sensor 3d is 8.5 µm. FIG.12 shows that the more approximate to each apex each of the central wavelength, the greater the ratios of the sensing outputs of the infrared sensors. As seen in FIG.12, when the temperature of a heater is 300-400°C, the temperature dependency of the ratio of the sensing outputs of the infrared sensors 3c and 3d with the central wavelengths λc and λd is greater and on the other hand, when the temperature of a heater is 400°C or more, the temperature dependency of the ratio, of the sensing outputs of the infrared sensors 3a and 3c with the central wavelengths λa and is c greater. That is, when the heater is at a relatively low temperature such that 300-400 °C is sensed, a combination of the infrared sensors 3c and 3d is good and on the other hand, the heater at a temperature as high as 400°C or more, a combination of the infrared sensors 3a and 3c provides a good measurement accuracy. Thus, providing three temperature-measuring bands provides an accurate temperature and an accurate area of the heater over the range of low temperature to high temperature. In accordance with the above-described computations of the temperature and heating area of the heater performed by the signal processor 18 of the second embodiment, computing the temperature T and heating area S of the heater and substituting the temperature T and the wavelength λco 2 of a CO 2 -molecular resonance radiation band into the equation (1) representing Planck's law of radiation produce the radiation intensity Pco 2 of the CO 2 -molecular resonance radiation band, and substituting the radiation intensity Pco 2 and the heating area S computed by the equation (5) into the equation (4) estimates a sensing output Vb' of an infrared sensor at the CO 2 -molecular radiation band. When the heater is assumed to be a blackbody, the sensing output Vb' has its real value. Thus, when the heater flames, a peak appears at the CO 2 -molecular resonance radiation band as shown in FIG.2. Thus, comparing the estimated sensing output Vb' with an actual sensing output Vb of the infrared sensor 3b determines that the heater flames, when the actual sensing output Vb exceeds the estimated sensing output Vb'. The method of the present invention provides accurate measurements of the temperature and heating area of the heater, provided noise caused when the temperature of the heater is low is accounted for. Thus, this method provides real-time recognition of the progression of the heating area during the spread of a disastrous fire and displays or alarms the situation of an increase in the heating area on a monitor or the like placed in a watchman room. FIG.18 illustrates the fundamental arrangement of one example of an environment control system embodying an environment monitor of the present invention. In this, an upper portion of an inner wall of a room has an air conditioner 51 attached thereto and the inner wall of the room has a temperature sensor 52 such as a thermistor attached thereto under the air conditioner 51. The center of the top inner wall of the monitored room has an infrared radiation sensing unit 53 attached thereto with a pyroelectric infrared sensor facing downwards. The infrared radiation sensing unit 53, air conditioner 51 and temperature sensor 52 are connected through a cable 54 to a signal processor 50, such as a microcomputer, placed in a watchman room or the like. The signal processor 50 computes the radiation temperature in the monitored room from the outputs of infrared radiation sensing unit 53 and transmits the resulting radiation temperature data to the air conditioner 51. The microcomputer of the air conditioner suitably controls the temperature and flow of ventilation in response to the radiation temperature data and sensing signal from the temperature sensor 52 in order to produce a comfortable indoor environment. The signal processor 50 determines the occurrence of a disastrous fire in response to the outputs of the infrared radiation sensing unit 53 thereby to operate an alarm 20 placed in a watchman room, a passageway etc. The signal processor 50 monitoring the overall building may alternatively produce a signal controlling the air conditioner 51 in response to the outputs of the temperature sensor 52 and infrared sensor 53. The air conditioner 51 may include a microcomputer. The infrared radiation sensing system of FIG.1 may provide the infrared radiation sensing unit 53 of the environment control system. That is, the infrared radiation sensing unit 53 comprises a rotational chopper 1 periodically chopping an infrared radiation, infrared filters 2a to 2d and infrared sensors 3a to 3d. The signal processor 50 receiving the sensing outputs of the infrared radiation sensing unit 53 is arranged as shown in FIG.5 or FIG.11. The microcomputer 18 operates on the sensing signals at intervals of a few seconds by timer interruption, stores data of an increase in the temperature of the infrared source and an increase in a heating area and of the presence or absence of CO 2 -molecular resonance radiation in a few minutes monitors on the data whether the temperature and heating area of the infrared source continuously increase or not, determines an occurrence of a disastrous fire when the temperature and heating area of the infrared source are increasing, and operates a driver 19 to turn a relay RLY on thereby to operate an alarm 20. In particular, the outputs of the infrared sensors 3a to 3d change in the case of a disastrous smoking fire as shown in FIG.6. That is, the outputs a, b, c and d of the infrared sensors 3a to 3d increase with a temperature increase and an increase in a fire-spreading area in the sequence of the outputs d, c, b and a. Since CO 2 -molecular resonance radiation sharply rises at the flaming point of time TF, the output of the infrared sensor of the outputs of the infrared sensors 3a to 3d sharply rises. Then, since the infrared source flames after the flaming point of time TF, the temperature increase is low and an increase in the amount of infrared radiation caused by an increase in the fire spreading area becomes main, so that the outputs a, b, c and d of the infrared sensors 3a to 3d increase but the ratios of the outputs a, b, c and d essentially becomes constant. On the other hand, in the case of a nondisastrous fire, the temperature or heating area of the infrared source becomes constant like an extinguished fire after a fixed time. For example, the heating area of a room heater and a cooking heater will not increase and the temperature thereof becomes constant in a fixed time. Thus, comparing the outputs of the infrared sensors 3a to 3d provides a temperature of the infrared source and in particular comparing, e.g., the outputs of the infrared sensors 3a, 3b and 3d of the infrared sensors 3a to 3d at the temperature of the infrared source with predetermined values provides a heating area. In addition, computing, from the temperature and heating area of the infrared source produced in the above sequence of operation, a blackbody radiation intensity of the infrared source, i.e., an infrared radiation intensity of the CO 2 -molecular resonance radiation wavelength band if the infrared source is a blackbody, and comparing the resulting value of the blackbody radiation intensity with the output of the infrared sensor 3c, sensing a CO 2 -molecular resonance radiation band, provide the presence or absence of CO 2 -molecular resonance radiation. Thus, when the temperature and heating area of the infrared source tend to increase for a fixed period (i.e., a few minutes) but no CO 2 -molecular resonance radiation is recognized, the occurrence of a disastrous smoking fire is determined. When, the temperature and heating area of the infrared source sharply rise at a point of time and CO 2 -molecular resonance radiation is concurrently recognized, the microcomputer 18 determines that the disastrous smoking fire has transferred to a disastrous flaming fire and increases the sound volume of the alarm 20 or changes the intensity of a sound of the alarm so as to indicate the change. When a case in which no infrared radiation is sensed suddenly passes into a case in which CO 2 -molecular resonance radiation is sensed, a heating at a high temperature corresponding to CO 2 -molecular resonance radiation is sensed and the heating area sharply rises, the microcomputer 18 determines this as an occurrence of an incendiary fire. On the other hand, when no increase in a heating area is recognized, the microcomputer 18 determines the case as a presence of a flaming heater, e.g., a flaming stove. Thus, the present invention determines the presence or absence of a disastrous fire on the basis of actual fire phenomenon to remarkably reduce the number of occurrences of false alarms, unlike the prior art. During a fire determination routine, a radiation temperature is computed and the resulting temperature data are fed to the air conditioner 51 in order to provide a comfortable indoor environment.

Claims: A fire sensing system comprising at least four band-pass filters (2a,2b,2c,2d;42a,42b,42c,42d) separating infrared radiation from a source in a monitored spacing into at least four wavelength bands (λa, λb, λc and λd) ; at least four infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d) sensing the separated infrared radiations passing through the band-pass filters (2a,2b,2c,2d;42a,42b,42c,42d) respectively; and a signal processor (10,18) determining whether a disastrous fire occurs or not, characterised by the pass-band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by the temperature (T) of the infrared source being computed by the signal processor (10,18) according to the following equation on the basis of the outputs (Va, Vc and Vd) of the infrared sensors (3a,3c,3d) other than that of the sensor (3b) sensing the CO 2 -molecular resonance radiation band having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi , wherein i is one selected from a, c and d, and j is one selected from a, c and d, and i is not equal to j, thereafter the infrared radiation intensity (P i ) of one of these wavelength bands being computed from the computed temperature (T); and the heating areas (S) of the infrared source being computed according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of the wavelength bands, S = 2π Vi Pi'·Ai , and the blackbody radiation intensity of the infrared source of the CO 2 -molecular resonance radiation wavelength band being computed from the computed temperature (T) and the heating area (S); the computed value of the blackbody radiation intensity being compared with the output (Vb) of the sensor (3b) sensing the CO 2 -molecular resonance radiation band, and thereby the signal processor (10) determines that a disastrous fire is occurring when the output (Vb) of the sensor (3b) sensing the CO 2 -molecular resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area (S) tends to increase. A fire sensing system according to claim 1, wherein a chopper (1) periodically chops the infrared radiation from the infrared source in order to provide the infrared radiation to the infrared sensors (3a,3b,3c,3d,43a,43b,43c,43d). A fire sensing system according to claim 2, wherein the signal processor (10,18) detects the outputs of the infrared sensors (3a,3b,3c,3d,43a,43b,43c,43d) synchronous with two periodic signals which are synchronous with the rotation of the chopper (1), the periodic signals having 90-degree different phases and the signal processor (10,18) producing a mean square of the resulting synchronization-detection signals. A process for sensing a fire comprising separating infrared radiation from a source in a monitored spacing into at least four wavelength bands (λa, λb, λc and λd) through at least four band-pass filters (2a,2b,2c,2d;42a,42b,42c,42d); sensing the separated infrared radiations through at least four infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d) individually and determining whether or not a disasterious fire occurs characterised by the pass-band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by computing the temperature (T) of the infrared source according to the following equation on the basis of the outputs (Va, Vc and Vd) of the infrared sensors (3a, 3c, 3d) other than that of the sensor (3b) sensing the CO 2 -molecuoar resonance radiation band having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi wherein i is one selected from a, c and d, and j is one selected from a, c and d, and i is not equal to j; computing the infrared radiation intensity (P i ) of one of the wavelength bands from the computed temperature (T); computing the heating area (S) of the infrared source according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of these wavelength bands, S = 2π Vi Pi'·Ai ; computing the blackbody radiation intensity of the infrared source of the CO 2 -moBecuoar resonance radiation wavelength band from the computed temperature (T) and the heating area (S); and by determining whether a disastrous fire occurs or not by comparing the computed value of the blackbody radiation intensity with the output (Vb) of the sensor (3b) sensing the CO 2 -molecular resonance radiation band, so that it is determined that a disastrous fire is occurring when the output of the sensor (3b) sensing the CO 2 -moBecuoar resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area (S) tends to increase. A process for sensing a fire according to claim 4, wherein the outputs of the infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d) selected for computation depends on a sensed target temperature. A process for sensing a fire according to claim 4 or claim 5, wherein an alarm is driven when a disastrous fire is detected. A process for sensing a fire according to any one of claims 4 to 6, wherein a computed heating area of the infrared source is displayed on a monitor. An environmental monitor comprising at least four band-pass filters (2a,2b,2c,2d;42a,42b,42c,42d) separating infrared radiation from a monitored spacing into at least four wavelength bands (λa, λb, λc and λd), at least four infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d) sensing the separated infrared radiations passing through the band-pass filters (2a,2b,2c,2d;42a,42b,42c,42d) respectively; and a signal processor (10,18) determining whether a disastrous fire occurs or not characterised by the pass band central wavelengths of the at least four wavelength bands (λa,λb,λc and λd) being 3 µm, 4.3 µm, 5 µm, and 8.5 µm, respectively; and by the temperature (T) in the monitored spacing being computed by the signal processor (10,18) according to the following equation on the basis of the outputs (Va, Vc and Vd) of the infrared sensors (3a, 3c, 3d) other than that of the sensor (3b) sensing the CO 2 -molecular resonance radiation having a peak of about 4.3 µm, T = C' λi-λj λi·λj 1 ln Vj Vi · λj λi , wherein i is one selected from a, c, and d, and j is one selected from a, c and d, and i is not equal to j, thereafter the infrared radiation intensity (P i ) of one of these wavelength bands being computed from the computed temperature (T); and the heating area (S) of the monitored spacing being computed according to the following equation on the basis of the computed infrared radiation intensity (P i ), properties of the infrared sensors (A i ) and the output of the infrared sensor (V i ) sensing the one of the wavelength bands, S = 2π Vi Pi'·Ai , and the blackbody radiation intensity of the infrared source of the CO 2 -moBecuoar resonance radiation wavelength band being computed from the computed temperature (T) and the heating area (S); the computed value of the blackbody radiation intensity being compared with the output (Vb) of the sensor (3b) sensing the CO 2 -molecular resonance radiation band, and thereby the signal processor (10,18) determining that a diastrous fire is occurring when the output (Vb) of the sensor (3b) sensing the CO 2 -molecular resonance radiation band is larger than the computed value of the blackbody radiation intensity and the heating area (S) in the monitored spacing tends to increase. An environmental monitor according to claim 8, wherein a contact type temperature sensor (52) measures an indoor air temperature and the signal processor (10,18) produces a signal controlling an air conditioner (51) in response to outputs of the contact type temperature sensor (51) and the infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d). An environmental monitor according to claim 8, wherein a contact type temperature sensor (52) measures an indoor air temperature and wherein the signal processor (10,18) produces a signal controlling a room cooler and a room heater in response to outputs of the temperature sensor ( 5 2 ) a n d the infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d). An environmental monitor according to any one of claims 8 to 10, wherein a chopper (1) periodically chops the infrared radiation from the monitored spacing in order to provide the infrared radiation to the infrared sensors (3a,3b,3c,3d;43a,43b,43c,43d).

Inventors: GOTO HARUHISA, MIYAMOTO KEIICHI, NAYA KAZUNARI, SATO HIROOMI, SEGAWA HIDEO, GOTO, HARUHISA, MIYAMOTO, KEIICHI, NAYA, KAZUNARI, SATO, HIROOMI, SEGAWA, HIDEO, GOTO, HARUHISA, C/O NIPPON MINING CO., LTD., NAYA, KAZUNARI, C/O NIPPON MINING CO., LTD., SEGAWA, HIDEO, C/O NIPPON MINING CO., LTD.
Applicants: JAPAN ENERGY CORP, KAJIMA CORP, JAPAN ENERGY CORPORATION, KAJIMA CORPORATION
Application year: 1990
Main classification: G08B17
IPC codes: G08B17, G01J5, G01N21