Title of Invention

AN OPTO-ACOUSTIC MEASURING ARRANGEMENT

Abstract

The measuring arrangement contains a measuring cell and a reference cell (9, 10), respectively, and microphones (11 and 12) assigned to these cells, to which microphones an electronic evaluation circuit (7, 8) is connected and in which a subtraction of the signals of the microphones (11 and 12) takes place, as well as a radiation source (5) for applying a modulated signal to the measuring cell (9). The modulation frequency of the radiation source (5) coincides with the resonant frequency of the measuring cell (9), and the measuring cell and the reference cell (9 and 10) are open at at least one end to the gas and/or aerosol to be detected. The measuring arrangement is used as smoke alarm, gas alarm, fire hazard alarm or as combined smoke and gas alarm, wherein each of the measuring cells (9) is exposed to a radiation of a wavelength at which a relevant substance to be detected is absorbent and an opto-acoustic effect is produced as a result.

Full Text

The present invention concerns an opto-acoustic measuring arrangement for the detection of gases and/or aerosols, having a measuring cell and a reference cell, respectively, and microphones assigned to these cells, to which microphones an electronic evaluation circuit is connected, in which a subtraction of the signals of the microphones takes place, and having a radiation source for applying a modulated signal to the measuring cell, wherein the modulation frequency of the radiation source coincides with the resonant frequency of the measuring cell. With the opto-acoustic or photo-acoustic effect, an acoustic pressure wave, whose magnitude is directly proportional to the concentration of the relevant gas, is produced by the irradiation by modulated light of a gas to be detected. The acoustic pressure wave is produced because the gas absorbs the light radiation and heats up as a result. This results in a thermal expansion and a periodic pressure fluctuation in accordance with the modulation of the light radiation. The two cells are usually termed the measuring cell and the reference cell, and the measuring arrangement is constructed so that the cells are either separated from each other and the radiation passes through both cells (C. F. Dewey, Jr.: Opto-acoustic Spectroscopy and Detection, [Y. H. Pao, ed.], Academic Press, New York, 1977, 47-77) or the cells are interconnected and the radiation passes only through the measuring cell (G. Busse and D. Herboeck: Differential Helmholz resonator as an opto-acoustic detector, Applied Optics, Vol 18, No. 23, 3959). With the detection of aerosols the behaviour is similar, as these also absorb the modulated radiation, whereby modulated heat and from this modulated pressure are produced as a result. Previously described opto-acoustic sensors for the measurement of aerosols are mostly mono-sensors with only one measuring cell. If, for the aerosol measurement, sensors with two cells, so-called dual sensors having one measuring cell and one reference cell are proposed, then these are constructed so that the reference cell is screened against aerosol. The latter is achieved by filtering the air before it reaches the reference cell. Reference is also made to the severe temperature-dependence of the resonant frequency, which requires correction of the signal magnitude. When the dual principle is employed, the detection sensitivity of opto-acoustic sensors for gases or aerosols is in the region of that of optical smoke alarms. Since the opto-acoustic signals are produced by absorption and not by radiation, both large and even the smallest aerosols were able to be detected to below the p range with the opto-acoustic principle, and light and dark types of smoke were able to be measured to a more or less equal degree. Nevertheless, the opto-acoustic principle is not being used up to now for smoke detection, which is chiefly due to the additional outlay necessitated by the air filtering and the correction of the signal magnitude. An opto-acoustic measuring arrangement of the type stated at the outset, whose costs are competitive with those of a scattered-light detector, shall now be specified by the invention. This problem is solved according to the invention in that the measuring cell and the reference cell are open at at least one end to the gas and/or aerosol to be detected. Since in the opto-acoustic measuring arrangement according to the invention both cells are open to the gas and/or aerosol to be detected, filtering of the gas/aerosol to be investigated is not necessary. Normally the sensor signal is zero, and a signal which requires only a relatively simple electronic circuit for its processing is produced in the measuring cell only in the presence of aerosol or a combustible gas which absorbs the radiation emitted by the radiation source. A first preferred embodiment of the measuring arrangement according to the invention is characterised in that the electronic evaluation circuit contains a differential amplifier and a phase-sensitive rectifier. A second preferred embodiment of the measuring arrangement according to the invention is characterised in that the wavelength of the radiation emitted by the radiation source is chosen so that it is absorbed by the gas to be detected. A first photocell for monitoring the intensity of the radiation emitted by the radiation source is preferably disposed within the range of the radiation source. A third preferred embodiment of the measuring arrangement according to the invention is characterised in that in addition to the measuring cell, a second photocell is disposed which, in the presence of an aerosol, is exposed to the scattered radiation of the radiation source caused by this aerosol. A measuring arrangement constructed in this manner can detect both an aerosol, that is to say smoke, and a gas, and is therefore eminently suitable for use as a so-called dual-criteria alarm for smoke and gas. In practice it behaves in such a way that a specific aerosol is absorbed in a specific wavelength range, the type of aerosol depending on the combustible material. However, since the smoke from a fire nearly always contains mixtures of organic substances, such as wood, for example, which are very absorbent in the entire infrared range and still sufficiently absorbent in the visible light range, the choice of wavelength for optimum aerosol detection is not critical. If only smoke is to be detected, the second photocell is not required because in this case a wavelength can be selected, at which no combustible gases are absorbent. In the detection of smoke and gas, the lateral photocell is always required when a gas whose absorption range is that of aerosol, is to be detected. A fourth preferred embodiment of the measuring arrangement according to the invention is characterised in that the measuring cell is radiated by two radiation sources which are operated at different frequencies. This arrangement is suitable for the detection of smoke and two gases. A further preferred embodiment of the measuring arrangement according to the invention is characterised in that two pairs of measuring cells and reference cells, open at both ends, are provided, each of which has a different length and thus different resonant frequencies, that a microphone is assigned to each reference cell pair and to each measuring cell pair, and that each measuring cell is exposed to a radiation source. The measuring arrangement with the two pairs of measuring cells and reference cells is suitable for the detection of smoke and two gases. By adding a further pair with a measuring cell and a reference cell, the detection range of the measuring arrangement can be extended to a third gas. The invention further concerns an application of said measuring arrangement as a smoke alarm. This application is characterised in that the measuring arrangement has a measuring cell which is exposed to a radiation of a wavelength at which the aerosol to be detected is absorbent and an opto-acoustic effect is produced as a result. The invention further concerns an application of said measuring arrangement as a fire hazard alarm. This application is characterised in that the measuring arrangement has a measuring cell which is exposed to a radiation of a wavelength at which a combustible or explosive substance to be detected is absorbent and an opto-acoustic effect is produced as a result. The invention further concerns an application of said measuring arrangement as a combined smoke and gas alarm. This application is characterised in that the measuring arrangement has a measuring cell which is exposed to a radiation of a wavelength at which a combustible or explosive substance to be detected is absorbent and an opto-acoustic effect is produced as a result, and that in addition to the measuring cell, a photocell is disposed so that it is exposed to scattered light of the radiation, caused by an aerosol. The invention further concerns an application of said measuring arrangement as a combined fire alarm and fire hazard alarm. This application is characterised in that the measuring arrangement has two measuring cells, of which one is exposed to radiation of a wavelength at which the aerosol or a combustible gas to be detected is absorbent, and of which the other is exposed to radiation of a wavelength at which a combustible or explosive substance to be detected is absorbent and an opto-acoustic effect is produced as a result. The invention is explained in further detail below with the aid of exemplary embodiments and the drawings, in which: Fig. 1 shows a schematic representation of a resonant, opto-acoustic dual sensor, open at one end for smoke and gas; Fig. 2 shows a schematic representation of a resonant, opto-acoustic dual sensor, open at both ends for smoke and gas; and Fig. 3 shows a development of the dual sensor of Fig. 2. The opto-acoustic measuring arrangement illustrated in Fig. 1 is a resonant, dual sensor, open at one end, with a tubular measuring cell 1 and a tubular reference cell 2 to each of which a microphone 3 and 4, respectively, is assigned. Furthermore, a radiation source 5, for example an LED, is provided, which exposes the inner space of the measuring cell 1 with radiation of a specific wavelength. In addition to the radiation source 5, a first photocell 6 is disposed for monitoring the intensity of the radiation emitted by the radiation source 5. The outputs of the two microphones 3 and 4 are fed to a differential amplifier 7 in which the microphone signals are subtracted from each other. The output signal of the differential amplifier 7 is fed to a phase-sensitive rectifier (lock-in) 8. Tubes open at one end, with a length I have a resonant frequency vk, which is given by With a length I of 2 cm, this gives a resonant frequency v0 = 4.1 kHz; with a tube open at both ends this resonant frequency is doubled. Standing waves therefore occur in the tube, wherein in the case of the tube open at one end, a pressure antinode (= motion node) occurs at the closed end and a pressure node (= motion antinode) occurs at the open end. In the tube open at both ends, the pressure antinode is located at the centre of the tube and a motion antinode at each open end. The radiation source 5 emits modulated radiation into the measuring cell 1, the modulation frequency of the radiation source 5 coinciding with the resonant frequency of the measuring cell. If the measuring cell 1 contains an aerosol, then this absorbs the modulated radiation, thereby producing modulated heat. The modulated heat produces modulated pressure and thus sound at the frequency of the resonant frequency of the measuring cell 1, as a result of which the air column in the measuring cell is excited into oscillation. The same applies in the presence of a gas in the measuring cell 1. The microphone 3, which is located at the position of a pressure antinode of the standing wave, measures the oscillations (= sound) in the tube. As soon as the microphone 3 measures a sound which coincides with the resonant frequency of the measuring cell 1, there is an aerosol and/or a gas in the measuring cell 1. In contrast to a scattered-light smoke alarm, the illustrated measuring arrangement responds equally well to dark and light aerosols: dark aerosols produce a large signal because when the radiation of the radiation source 5 initially strikes a particle much radiation power is absorbed. And light aerosols likewise produce a large signal, since the radiation at the light particles is reflected many times and in total is absorbed to a great extent. Moreover, the opto-acoustic sensor responds both to large aerosols and to very small ones below the (j range, since the opto-acoustic signals are generated by absorption and not by scattering. The microphone 3 measures not only the resonant oscillations in the measuring cell 1, but also all noises in the room, which can lead to interference. This interference is eliminated by the reference cell 2 and the microphone 4. Since the reference ceil 2 is not exposed to the^ radiation of a radiation source, the microphone 4 also cannot measure any oscillations produced by a radiation source, but exclusively measures the noise in the room. The signals of the reference microphone 4 are subtracted in the differential amplifier 8 from the signals of the measuring microphone 3, thus eliminating the room noise. Vibrations, which have an equal effect on both microphones, are likewise eliminated. The two cells, measuring cell and reference cell, can also be open at both ends. Such an arrangement with a measuring cell 9, open at both ends, a reference cell 10, open at both ends, a measuring microphone 11 and a reference microphone 12, is illustrated in Fig. 2. A second photocell 13, which is disposed in the region between the radiation source 5 and the measuring cell 1, is also shown in Fig. 2. The position of the second photocell 13 is chosen so that in the presence of particles in the area between radiation source 5 and measuring cell 1, a portion of the scattered light of the radiation of the radiation source 5 produced by these particles falls on the photocell 13. The second photocell 13 enables a distinction to be made between aerosol and gas. If both the measuring cell 1 and the second photocell 13 deliver a signal, then an aerosol is present. If only the measuring cell 1 delivers a signal, then either a gas or a very small and therefore non-scattering aerosol is present. If the suppression of room noise and vibrations can be dispensed with, in principle a measuring arrangement without reference cell 2 and the microphone 4 assigned to the former could be adequate. If in such an arrangement the wavelength of the radiation source 5 is placed on the C02 line, then the measuring arrangement will measure very sensitively the concentration of the combustion gas C02 on the one hand and the concentration of aerosol on the other. The measuring arrangement illustrated in Figs. 1 and 2 can be designed as a gas alarm, smoke (aerosol) alarm, as a combined gas and smoke alarm and it can be used in these various forms as a fire alarm or as a fire hazard alarm. A fire alarm detects smoke and/or combustion gases, or generally, substances which characterise a fire. A fire hazard alarm detects, on the one hand, an existing fire by detecting an aerosol or substances occurring in a fire. On the other hand it detects toxic substances occurring in a fire and it recognises the danger of a possible fire or a possible explosion by detecting the presence of combustible substance in the air. Substances which characterise a fire are, in particular, the following; C02, CO, NO, N02, S02, NH3, HCI, HF, HCN, amine and amide, compounds containing hydrocarbons, C, 0 and H; aerosols. Combustible substances are generally hydrocarbons, particularly CH4, C2H6, C3H8, C4H10, C2H2, C2H4, as well as general solvents, alcohol, ether, ketone, aldehyde, amine and amide, in particular methanol, ethanol, n-propanol, diethylether, acetone. Other combustible substances which a fire hazard alarm should detect are compounds containing C, O and H, and carboxylic acids. Toxic substance are C02, CO, NO, N02) S02l NH3, HCI, HF, HCN, H2S, nitrites, phosphoric ester, mercaptans, halogenated compounds. Since the velocity of sound in air is temperature-dependent and can vary by up to 30% in the temperature range of a fire alarm from -20oC to +70C, the resonant frequency can also change accordingly. Water vapour also influences the velocity of sound and thus the resonant frequency. In order to eliminate these influences, the rough range of the resonant frequency and the possible additional expansion of the frequency range by varying water vapour content in the air, can be calculated with a temperature measurement and the modulation frequency of the radiation source varied (swept) in this range. A further possible disturbance consists in frequencies in the room, which coincide with the resonant frequency. Such frequencies excite both cells into oscillation, but cannot be completely subtracted to zero by the differential circuit, because, due to the distance from the centre of the measuring cell 1, 9 to the centre of the reference cell 2, 10, they strike the cells with a time shift and excite these cells into oscillation which has a small phase shift. This phase shift can be minimised by a lowest possible resonant frequency, because the interfering audio frequencies then have a large acoustic wavelength and the phase shift becomes small. Or, the signal of the reference cell 2, 10 can be measured separately and when a signal, which in fact can be generated only from outside, impinges upon the reference cell, the alarm threshold of the measuring arrangement can be increased. Further potential disturbance variables are different lengths of the cells. These disturbance variables can be eliminated by measuring the resonant frequency of one of the two cells and mechanically varying the length of the other cell accordingly. The resonant frequency of the reference cell can also be measured and the radiation source 5 positioned so that its position influences the resonant frequency of the measuring cell and brings it into coincidence with the reference cell. As a further check, monitoring of the microphone sensitivity by means of the zero signals produced by the radiation source in the wall of the measuring cell 1, 9, which occur under all environmental conditions, is recommended. The arrangement illustrated in Figs. 1 and 2 for the measurement/detection of smoke and one gas can be expanded by an additional pair of cells for the measurement/detection of a further gas. According to Fig. 3, an additional measuring cell 14, an additional reference cell 15 and an additional radiation source 16 are provided, where the measuring cell 9 measures aerosol and a first gas and the measuring cell 14 measures a second gas, for example. The two measuring cells 9 and 14 and, correspondingly, also the two reference cells 10 and 15 have different lengths and therefore also different resonant frequencies, and the two measuring cells are exposed to radiation from the radiation sources 5 and 16, respectively, at different wavelengths. The two different resonant frequencies can be measured with just one measuring microphone 11. Likewise, only one reference microphone 12 and only one single photocell 6 are required for monitoring the emission of both radiation sources 5 and 16. The measuring cells and reference cells can have the following dimensions, for example: Measuring cell 9, reference cell 10: length each 2 cm, resonant frequency each 8.2 kHz Measuring cell 14, reference cell 15:length each 2.2 cm, resonant frequency each 7.6 kHz Accordingly, the modulation frequency of the radiation source 5 is 8.2 kHz and that of the radiation source 16 is 7.6 kHz. LEDs are used as radiation sources. The additional outlay for the detection of a second gas is thus only the costs of the second cell pair and for the second radiation source. It is quite obvious that an extension for the detection of a third gas requires only a further cell pair and a further radiation source. Instead of two pairs of measuring and reference cells (9, 10; 14, 15), of different length, which are simultaneously irradiated by two radiation sources 5 and 16, in the arrangement of Fig. 2 the measuring cell 9 of one cell pair can be simultaneously irradiated by two radiation sources 5 and 16 and these can be operated at difference frequencies; for example, the radiation source 5 at the fundamental frequency and the radiation source 16 at the first harmonic. Consequently, compared to the arrangement of Fig. 3, only half the number of cells and microphones are needed and corresponding costs are saved. Apart from the resonant opto-acoustic dual sensors, open at one end or both ends, non-resonant, closed dual sensors are also known (see for example EP-A-0 855 592), which cart likewise be constructed so that the detection of aerosols and gases is possible with them. As can be seen in EP-A-0 855 592, these opto-acoustic dual sensors contain a measuring cell and a reference cell, each of which is sealed against the environment by a diaphragm, and a radiation source. Gas can permeate the cell through the diaphragm. A measuring microphone and a reference microphone are provided, the reference microphone being screened against opto-acoustic signals of the gas/aerosol to be detected. So that aerosol particles can permeate the cells, the pore size of the diaphragms is increased accordingly. But as a result, the diaphragms for frequencies below 500 Hz are acoustically soft, pressure build-up in the cell is no longer possible and the sensitivity is seriously reduced. By increasing the modulation frequency to a few kilohertz, the diaphragms again become acoustically hard and the sensitivity no longer decreases. Any jamming of the diaphragms can be monitored by measuring the reference signal separately, which gives a base noise level, and the sensitivity corrected with the aid of this base level. If the wavelength of the radiation sources is positioned on the C02 line, for example, then the measuring arrangement will measure very sensitively the concentration of the C02 combustion gas. On the other hand, however, the concentration of aerosol is very sensitively measured because cellulose and carbonised cellulose particles are strongly absorbent in the entire infrared range. The volume per cell is approximately 2 times 2 times 2 cm3. WE CLAIM: 1. An opto-acoustic measuring arrangement for the detection of gases and/or aerosols, having a measuring cell and a reference cell (1, 9, 14 and 2, 10, 15) respectively, and microphones (3, 11 and 4, 12) assigned to these cells, to which microphones an electronic evaluation circuit (7, 8) is connected, in which a subtraction of the signals of the microphones (3, 11 and 4, 12) takes place, and having a radiation source (5, 16) for applying a modulated signal to the measuring cell (1, 9, 14), wherein the modulation frequency of the radiation source (5, 16) coincides with the resonant frequency of the measuring cell (1, 9, 14), characterized in that the measuring cell and the reference cell (1, 9, 14 and 2, 10 , 15) are open at at least one end to the gas and/or aerosol to be detected. 2. The measuring arrangement as claimed in claim 1, wherein the electronic evaluation circuit comprises a differential amplifier (7) and a phase-sensitive rectifier (8). 3. The measuring arrangement as claimed in claim 1 or 2, wherein a first photocell (6) for monitoring the intensity of the radiation emitted by the radiation source (5, 16) is disposed in the region of the radiation source (5, 16). 4. The measuring arrangement as claimed in claim 1 or 2, wherein in addition to the measuring cell (9, 14) a second photocell (13) is disposed, which, in the presence of an aerosol, is exposed to the scattered radiation of the radiation source (5, 16) caused by this aerosol. 5. The measuring arrangement as claimed in claim 3 or 4, wherein two pair of measuring cells and reference cells (9, 14, 10, 15), open at both ends, are provided, each of which has a different length and thus different resonant frequencies, that a microphone (11 and 12) is assigned to each reference cell and to each measuring cell pair (9, 14 and 10, 15), and that each measuring cell (9, 14) is exposed to a radiation source (5 and 16). 6. The measuring arrangement as claimed in any one of claims 1 to 5, wherein a sensor for measuring the ambient temperature is provided, and that an adjustment of the modulation frequency of the radiation source (5, 16) to a frequency range corresponding to the measured ambient temperature, and a time-shift of the modulation frequency within this frequency range, takes place. 7. A method for the detection of gases and/or aerosols by an opto-acoustic measuring arrangement comprising the steps of: subtracting the signals of the microphones, applying a modulated signal to the measuring cell wherein coinciding the modulation frequency of the measuring cell with the resonant frequency of the measuring cell characterized in that the measuring cell and the reference cell are being opened at at least one end to the gas and/or aerosol to be detected. 8. The method as claimed in claim 7, wherein emitting radiation with a wavelength that is absorbed by a gas that is to be detected. 9. The method as claimed in claim 7 or 8, wherein irradiating the measuring cell by two radiation sources that are operated by two different frequencies. 10. The method as claimed in claim 9, wherein operating one of the radiation source at the fundamental frequency and the other is operated at the first harmonic.

Documents:

in-pct-2002-0871-che complete specification as granted.pdf

IN-PCT-2002-871-CHE CORRESPONDENCE OTHERS 23-02-2011.pdf

in-pct-2002-871-che-abstract.pdf

in-pct-2002-871-che-claims.pdf

in-pct-2002-871-che-correspondance others.pdf

in-pct-2002-871-che-correspondance po.pdf

in-pct-2002-871-che-description complete .pdf

in-pct-2002-871-che-drawings.pdf

in-pct-2002-871-che-form 1.pdf

in-pct-2002-871-che-form 3.pdf

in-pct-2002-871-che-form 5.pdf

in-pct-2002-871-che-other documents.pdf

in-pct-2002-871-che-pct.pdf