INTERNATIONAL DEVELOPMENTS IN FIRE SENSOR TECHNOLOGY

Brian J. Meacham, P.E., M.Sc. FireTech Dorfstrasse 94 CH-8706 Meilen Switzerland

SUMMARY

There have been a number of developments in fire sensor technology over the past ten years. Some, such as incipient smoke detection systems, have become readily available, while others remain in the research, pre-production, or newly released stage. This second group of sensors utilizes technologies ranging from optical fibers and wax, to integrated video and infrared sensors controlled by artificial intelligence algorithms. This paper presents an overview of several less known, yet promising, fire sensor technologies. Although it does not address specific applications, it illustrates the wide range solutions available for addressing a variety of fire detection needs.

HEAT SENSOR DEVELOPMENTS

There have been several developments in The sensor cable itself is composed of heat sensor technology in recent years. three primary components: an optical Two promising approaches are in the use fiber, a wax-filled tube, and a protective of fiber optic cables as line-type heat de- covering material (jacket). The optical fi- tectors, and the detection of thermal fluc- ber is in parallelI with the wax filled tuations instead of temperature increase. tube, connected to it by an aramid thread (Figure 1). Utilizing an optical reflectom- Ericsson, a Swedish company, has devel- etry technique, a short laser pulse is trans- oped a very sensitive line type heat detec- mitted into the optical fiber 40,000 times tion system using laser and optical fiber per second. As the light pulse travels at a technology.l The sensor cable can be up to 2 km long, and when the length of heated Figure 1: Optical Fiber Line Type Heat Detector Assembly’ cable is at least 200 mm, the fire location can be pinpointed with an accuracy of about +/- 1 m. Up to 100 of these fire or overheat locations can be detected with the +/- 1 m accuracy as long as the separation between hot points is at least 3.5 m. The activation temperature (alarm temperature) of the sensor is between 40°C and 90°C with a +/- 1°C resolution. Although a specific ac- tivation temperature within this range can be selected, it is a function of the sensor materials, and is not currently field ad- justable. t This paper is based on a presentation during the 1993 SFPE Engineering Seminar, Issues in Interna- tional Engineering Practice.

89 near constant velocity along the length of Figure 2: Optical Fiber Line Type Heat Detector Operation’ the fiber, small irregularities within the fiber material cause some of the light to be scattered according to Rayleigh scattering theory.

In the quiescent state, the sensing unit detects the loss of signal due to scatter along the fiber. This defines the &dquo;normal&dquo; signal. When part of the cable assembly (200 mm nominal) becomes heated, the wax in the tube begins to melt and expand. As it does so, microbending of the optical fiber occurs causing a change in the amount of reflected light (Figure 2). The sensor detects this change in light signal, and the distance to the heated part is calculated from the relationship d = (v)(t/2), where t is the time difference from when the light beam through microbending of the fiber, pulse is transmitted until the reflected however, the microbending was induced light is received, and v is the velocity of by a bimetallic effect rather than through the light pulse. This signal evaluation method deformation of a wax filled tube. provides the location resolution of about +/- 1 m. Should a break occur in the fiber, Similar to the Ericsson system, this sys- a separate and unique signal will be re- tem utilizes an optical reflectometry tech- ceived and processed as a trouble condition. nique in which a short light pulse is trans- mitted through the fiber, and the scat- Once the fire is extinguished, the wax cools tered light intensity is measured at the and the cable returns to its ambient state. receiver. In this case, instead of utilizing If there is no damage to the optical fiber, a wax-filled tube to cause microbending of the system re-establishes a base reference the optical fiber, the fiber is coated with signal, and the system returns to normal. a periodically interrupted metallic coat- Should the fire damage the fiber, the dam- ing. As the temperature around the cable aged section can simply be removed and a increases, the metallic coating expands new section spliced in. Through the use of and causes the fiber to deform in a specific . an optical fiber and protective jacket, the manner (Figure 3). Because the radiated sensor cable has proven to be extremely power in the fiber is proportional to the resistant to EMI, RFI, corrosive vapors square of the modulation amplitude, the and severe environmental conditions en- resulting amplitude modulation can be countered in several road tunnel tests translated to a temperature. This results performed throughout Europe. The sensor in a system that can identify both fire cable is currently available for operation location and temperature. in ambient temperatures between -20°C and 120°C, with a version capable of oper- Although this approach provides both lo- ating at up to 300°C anticipated. cation and temperature information, there is some question as to the manufacturability The use of optical fibers for heat detection of the cable assembly with the bimetallic was also studied at the Center Suisse d’ coating. In addition, compromises were made Electronique et de Microtechnique S.A. in with respect to location sensitivity and Neuchatel, Switzerland.2 In this work, the signal resolution. As a result, the sensi- researchers also looked into fire detection tivity is somewhat less than the Ericsson based on the optical power loss of the light system, with a spatial resolution of about

90 Figure 3: Metal Cladded Optical Fiber Line Type Heat Detector2 quency has been about 1 Hz. This is due to the thermal mass and associated heat Fiber Optic Heat Detection System, Switzerland transfer parameters of the sensing ele- ments most often used. However, by using a fast responding pyroelectric sensor that can detect the higher frequency fluctua- tions,5 much earlier thermal detection can result (Figure 4). In fact, laboratory tests have shown such a sensor to respond to open flaming fires in the same time frame as ionization type smoke detectors.44 Figure 4: Thermal Fluctuation Sensor Operating Theory

10 m over the length of cable. Should these items be resolved, the ability to detect the location and temperature of an overheat condition over a several kilometer length of cable could find several applications.

A U.S. company took a slightly different approach in the development of their fiber optic-based fire detection system3. This system, as with the previous two, uses a computer-based controller to transmit light signals along the length of the fiber. GAS SENSORS However, instead of using microbending of the fiber to detect the fire location, heat Gas detection devices have been another from the fire melts the cladding around source of sensor development in recent the fiber allowing light to escape. This in yearns. Because gases are produced in all turn causes a decrease in the signal re- stages of combustion, it would seem that ceived at the controller. As this signal a specific gas signature could be used for continues to decrease, the system transi- reliable fire detection. However, many of tions from trouble (35% reduction) to alarm the gases produced during the combustion (50% reduction). A complete and immedi- process also occur naturally, or are gener- ate loss of signal, indicative of a break in ated by non-threatening combustion pro- the fiber, also results in a trouble signal. cesses such as automobile engines. In addition, This concept is very similar to the more the sensor technology utilized often re- traditional, bimetallic line-type heat de- quires a significant power source, thus tector, but offers greater installation flex- restricting its application as a cost effec- ibility due to the non-conductive nature of tive fire sensor. By focusing on these two the optical fiber. concerns, research has produced gas sens- ing technology that will become more widely In other heat sensor research, recent studies applicable in coming years. have shown a temperature fluctuation in the range of 1 to 20 Hz to be present in One promising gas sensing device is the many fire situations.4Up to now, the maxi- HCI detector developed by researchers at mum detectable thermal fluctuation fre- Bell Labs.’ In this case, a sensor was de- 91 veloped specifically to detect HCI given sensor that could be powered by a stan- off by the pyrolysis or combustion of PVC dard fire detection system.9 The CO sensor cable insulation. Such a sensor provides is made of a solid-state macromolecular two basic data points: an early indication membrane, and is fabricated using inte- of HCI production, which can be damaging grated circuit and large scale integrated to electronic components, and a true indi- circuit technology. This results in a low cation of a PVC cable fire. Because it only power consumption requirement, allowing senses HCI, it does not respond to common the CO sensor to be combined with smoke nuisance signals such as cigarette smoke, and heat sensors in a common housing and steam or dust, yet provides very reliable powered from a fire detection system con- detection of HCI-producing fires such as trol panel. Together, the three sensor sig- burning PVC cable insulation. However, nals provide information that is used to this also means that a different type of differentiate between deceptive phenom- fire detection device is required for detec- ena and actual fire conditions. tion of non-HC1-producing fires. Although it may be more costly in the beginning, FIRE SENSOR DEVELOPMENT such a two-fire signature detection system could be more reliable than a single sensor Much of the research in the area of &dquo;fire&dquo; system, thus becoming more cost effective detection has focused on reducing nuisance operationally over time. alarm problems with ultraviolet (UV) and infrared (IR) radiation sensors. These devices, Another major development comes in the which are used to detect electromagnetic area of increasing the widespread applica- radiation produced during the combustion bility of sensors of more common gases process, are primarily used to detect ra- like CO. It has been shown that semicon- diation from flames. However, they can ductor gas sensors can detect CO at con- also detect radiation from overheated materials centrations in air in the range of a few which can result from numerous deceptive parts per million, considerably lower than phenomena, including sunlight, arc weld- concentrations that might be expected in ing sparks, tungsten lamps and other hot a fire of organic material. The problem, bodies. Middletonl° provides a good dis- however, has been that some of these de- cussion on various approaches that have tectors may also respond to other gases, been used to address this problem, includ- and have required a significant power ing detection of the frequency of flame source (operating temperatures of 300°C flicker, single channel detection with nar- or higher) for operation. row band filtering, dual channel IR detec- . tion, and a combination ofUV and IR detection. In research performed at Harwell Labora- tory in the UK, a hybrid CO detector was In a somewhat new approach to minimiz- developed which could operate at room ing nuisance alarms, researchers in Japan temperature from a low power source like have recently combined multi-wavelength a battery.8 The obvious benefit is that a radiation sensing with algorithms that battery operated spot-type CO detector, determine object temperature, flame tem- similar to a battery powered spot type perature, surface area, and presence of a could be feasible. Tests flames The object temperature algorithm were performed using British Standard is derived from Plank’s law, which states test fires, as well as common nuisance that the intensity of radiation emitted in alarm signatures such as high humidity, hemispherical space is proportional to high velocity and toasting (charring) of temperature and wavelength. Given four bread. Results were good in all cases. discreet wavelengths and measured inten- sities, the temperature of the object is Similar research was also performed in determined by the relationship: Japan, where researchers developed a CO

92 tizing the image and storing the frame in memory. In normal mode, a new scene is where 1..1 and X~ are two of the wavelengths, captured every few seconds and the previ- Pi and P2 are the measured intensities at ous reference frame is replaced. When UV wavelengths 1..1 and ~,Z, and C2 = hc/k. Tem- or IR radiation is detected, the frame cap- peratures below 350°C are calculated us- ture rate increases and the system com- ing wavelength bands 3(4.6 to 5.4 microns) putes size, growth rate, stationarity, mean and 4(8.0 to 9.0), and temperatures over spectral content, spatial variation, and 350°C are calculated using bands 1(2.8 to temporal variation for each new frame. 3.2 microns) and 3. The flame temperature The system then decides if the radiation is and combustion surface area are calcu- produced by a fire, and can discontinue lated in similar fashion. A comparison of tracking, issue an alarm or activate sup- the temperature and surface area with pression systems as required. Tested in an the resonance radiation of the C02 band aircraft hangar environment, the system then determines whether the body is in has successfully detected fires in the range flames. The system also determines the of 0.1 to 0.2 m2 at a distance of 30 m within &dquo;degree of danger&dquo; by evaluating the in- about 0.5 seconds after reaching the threshold crease in radiation energy and C02 ratio. size.

Tests were performed using a variety of This is similar to a combination IR sensor fuels, including methanol, heptane, and and video camera system developed in Europe beech wood cribs. The system was able to that can detect a relatively small fire (3 detect a 10 cm square pan of burning methanol m2) from a significant distance away (2 from a height of 10 m, and was able to km.)14 The optical system is based on a continuously detect changes during the passive infrared sensor array with appro- transition from smoldering to flaming of priate filtering and amplification circuits. the beech crib. A video camera is integrated with the sensor array to remotely image, locate and esti- This approach is similar in concept to mate the distance to the event detected by machine vision fire detection, an area that the sensor. Unlike the machine vision system, has recently been studied in some detail,12>13 however, the image is displayed to an operator In short, machine vision technology is a who manually controls the scanning of the combination of video cameras, computers, sensor to gain additional information and and artificial intelligence techniques. make decisions. Although an operator is Cameras are used to image information required, the sensors’ field of vision is a such as brightness, color and shape. Pat- full 360° for a distance spanning 2 km. tern recognition and image processing techniques process the cameras’ input, and At the other end of the spectrum, research specific algorithms or other artificial in- at the Santa Barbara Research Center resulted telligence techniques are used to deter- in the development of an IR sensor using mine certain information required for a optical fibers that allows remote fire sens- specific decision. ing in enclosed or environmentally harsh areas,.15 The system is composed of optical The machine vision system developed by fibers, IR detection devices, and an em- Goedeke et. a1.12 for fire detection uses bedded microcontroller for signal process- radiation sensors (UV and IR) to detect a ing. The optical fibers act as the sensors, fire, a CCD camera for imaging, and arti- allowing them to be located remotely from ficial intelligence techniques to automati- the signal processing equipment. At the cally evaluate the scene, identify bright end of the fiber, a lens is added to increase regions associated with the radiation and the nominal 20° field of view to 60 or 90°. determine if there is a fire. It does this by Radiant energy is viewed at the sensing capturing a scene from the camera, digi- end of the fiber and transmitted to the

93 microcontroller where the signals are am- SMOKE SENSOR DEVELOPMENT plified, digitized and processed. The sig- nals, which include flicker frequency, modu- There has also been considerable research lation randomness and spectral power ra- in the area of smoke sensor technology. tios, are then analyzed to make a fire/no- Although much of the focus has been on fire decision. Originally designed for use incipient smoke detection systems, there in aircraft engine nacelles, tests have also have also been developments in the more shown the sensor to be useful in open area traditional spot-type devices. One such area fire detection applications such as storage of focus has been to investigate the feasi- areas, cargo holds, and aircraft hangars. bility of a smoke detector that operates on the ionization principal without the use of In a completely different and unique area a radioactive source. of fire sensor research, the detection of acoustical emissions (ultrasonic events) An interesting approach to this situation associated with the combustion of build- has been proposed by researchers at the ing materials has recently been studied. ETH Zirich, Switzerland and the Univer- Grosshandler and Jackson 16 discuss a va- sity of Duisburg, Germany that involved riety of ways in which acoustical radiation development of an electrostatic smoke has been used for fire detection, and sug- detector.&dquo; The detector is based on the gest that detection of acoustical emissions principle that some percentage of smoke could prove beneficial in detecting hidden particles formed during combustion carry structural fires. By applying a small flame an electric charge that can be detected. to various structural materials on which The detector consists basically of a sens- piezoelectric transducers had been mounted, ing electrode sandwiched between two parallel they were able to detect distinct differ- reference grids (Figure 5). ences in the number of acoustical signals emitted per unit time for the different Charged particles that enter the space between materials being tested. This would sug- the electrodes are deflected by the electro- gest that such a method could be used to static potential, with some of the particles detect a fire that could not be seen or precipitating on the sensing electrode. A otherwise sensed in a confined space. current is then established which is pro- portional to the amount of precipitated charge per unit time. Tests have shown this detector to be sensitive to open flam- ing fires, but insensitive to smoldering Figure 5: Electrostatic Smoke Detector Block Diagram&dquo; combustion. This is due in large part to the fact that particles of combustion are initially highly charged, yet as the smoke cools, it coagulates and reduces the net charge as particles of opposite charge combine. The researchers indicate a possible appli- cation of such a sensor in specific applica- tions, such as alcohol fire detection, or in combination with a light scattering type smoke detector to provide a wide range of detection capability.

A somewhat different approach to smoke detection using electrostatic charge was taken by French researchers. 18 Instead of using parallel plate electrodes, they used single point type electrodes, one of which

94 carried a 6kV-12kV potential used to ion- sors that operate on this principle require ize the surrounding air, and the other which separate transmitter and receiver units measured the conductivity of gases pass- spaced at least 10 m apart. This new ing through the volume. This arrangement sensor, however, utilizes an integrated optical showed similar response characteristics: wave guide system containing multi-mode good for flaming fires, not good for smol- channel waveguides that allows the air dering combustion. Other potential draw- path to be reduced to millimeters. backs of this technique include high cur- rent requirements to maintain the high Referring to Figure 6, the signals from voltage charge on the source electrode and Source 1 (Sl) and Source 2 (S2) are split sensitivity to leakage currents along the by means of a Y-junction waveguide at critical insulation path. With a trend to given ratios Kl and K2, and are detected reduce the use of radioactive materials, at two receiver locations (R1 and R2). Individual however, continued research in this area signals are identified by driving the sources may prove beneficial. at different modulation frequencies, and the transmission (T) across the air path is In the area of optical type smoke detec- given by: tors, researchers at Cerberus AG in Swit- zerland have developed an optical sensor for measurement of light extinction that requires an optical path length of only 25 mm 19,20 (Figure 6). Smoke detection by the extinction method is based on Bouguer’s where A1(f1)=K1TS1R1, A2(f1)=(1-K1)SlR2, law, which relates the intensity of the A1(f2)=(1-K2)S2R1, and A2(f2)=K2S2R2. The incident monochromatic light (1;..°) of wave- signal through the wave guide and across length X, and the intensity of the light (I~) the air path under normal conditions pro- transmitted through a path length L of vides the reference value. When smoke smoke with an extinction coefficient K 21: particles enter the path, the signal de- creases until an alarm is given when a predetermined threshold is reached. Be- cause light extinction is used in most smoke Currently available light extinction sen- density measuring devices and smoke de- tector test equipment, and considerable data on the extinction characteristics of Figure 6: Optical Bridge Smoke Extinction Sensor Block smoke from various materials is known, Diagram2° further developments in this area may prove to be useful in evaluation of detector re- sponse and perhaps even computer model- ing of detector response.

Additional research in optical smoke sens- ing technology at Cerberus AG includes the use of two light sources of different wavelengths, the use of two detection angles (forward and backward scatter) and the measurement of the polarization of the scattered light22. Whereas the opera- tion of the previously described optical bridge sensor is based on light extinction principles, all three of these parameters relate to the application of light scatter-

95 ing theory. In particular, they relate spe- identify different smoke characteristics of cifically to broadening the size distribu- burning materials.24.25 By using two inci- tion of particles that can be detected. dent light sources that are polarized, even more information concerning the smoke The scattering of incident light by smoke particles can be determined. particles is often described using Mie theory, which states that the amount of incident CONCLUSION light scattered by a particle is dependent on the size, shape and refractive index of World wide research efforts have resulted the particle, wavelength and intensity of in the development of a number of new fire incident light and the angle of scatter.23 It sensor technologies, many of which have has been shown that this relationship can been described here. Although fire sensor be described for a smoke detector in the research continues, it is clear that the following manner:24 means to detect fire at any stage of devel- opment, under most environmental condi- tions, currently exists. As a result, one might expect that future research may where: focus more on the integration of existing 1. = Intensity of scattered light, (W/m2) sensor technology with signal processing techniques intended to verify fire condi- io = Intensity of the incident light, tions and reduce nuisance alarms. In fact, (W/M2) some of the developments described in this paper have done just that. However, be- Â. = Wavelength of the incident light, (m) cause the goal of a fire detection system is to reliably detect fire at that stage neces- No = Particle concentration in the detec- sary to meet specific objectives, tion chamber, (particle/m3) continued advancements in both sensor technology and signal processing techniques V. = Volume of the detection chamber, (m3) are both needed and welcomed.

1 = Distance from the scattering volume to the scattered light receiver (m), and

il+i2 = Mie scattering coefficients (functions of the scatter angle 6, particle diam- eter d, and refractive index, m)

This relationship indicates that for a fixed scatter angle and wavelength of incident light, the intensity of scattered light re- ceived will be maximized for a specific particle size and refractive index. As a result, by increasing either the number of angles at which scattered light is received, or the quantity of incident light wave- lengths transmitted, a broader range of particle sizes at various refractive indices can be detected. It has been suggested that such information could be used not only to detect smoke across broader par- ticle size and color ranges, but also to

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97 20. Ryser, P., Tompkin, C. and Roth, P., "Optical Sensing of Smoke Particles by Light Extinction Measurement Over a Short Distance," presented at Trans- ducer ’93, Tokyo, Japan, 1993.

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2. Grosshandler, W.L., "An Assessment of Technologies for Advanced Fire Detec- tion," Symposium on Heat Transfer in Fire and Combustion, ASME, Winter Annual Meeting, November 1992.

3. Bukowski, R. W. and Jason, N. H., In- ternational Fire Detection Bibliography 1975-1990, NIST Building and Fire Re- search Laboratory, NISTIR 4661, Sep- tember 1991.

98