METHOD AND APPARATUS FOR SPECTROSCOPIC MEASUREMENT OF THE CONCENTRATION OF A GAZ

Abstract: Method and apparatus for spectroscopic measurement of the concentration of a gas in a sample where you detect the intensity of light from a light source (1) passed through the sample (4) and through a reference cell (5) and generates a signal which represents the concentration of the gas. A laser diode (1) constitutes the light source which is locked to the absorption line of the gas at known concentration and pressure contained in a reference cell (5). The laser light with the properly selected wavelength is distributed via optical fibres (2, 3, 6) and/or glass prisms (19, 20) to the reference cell (5) and the sample (4). Non-gas-related transmission variations in the measurement path or in the optics is automatically compensated for by a special laser modulation which generates a time multiplexed reference. The measurement can be performed in a measurement cell incorporating several reflective mirrors (30) to reflect the laser beam several times inside the measurement cell thereby increasing the effective length of the measurement path. The measurement can also be performed using an optical fiber designed so that the surrounding gas or fluid via the evanescent field affects the laser light so that the concentration of the substance in question in the surrounding fluid or gas can be determined.

Description: METHOD AND APPARATUS FOR SPECTROSCOPIC MEASUREMENT OF THE CONCENTRATION OF A GAS This invention concerns a method and an apparatus to spec- troscopically measure the concentration of a gas in a sample, whereby the intensity of light from a light source is passed through the sample and through a reference cell and is detected, and that a signal is generated which represents the concentration of the gas. The light source consists of a laser diode which is locked onto the absorp¬ tion line of the gas at known pressure and concentration contained in the reference cell. In order to avoid inter¬ ference from the atmosphere the laser light of the selected wavelength is distributed along optical fibers and/ or glass prisms to the reference cell and to the sample. The in¬ vention also comprises an apparatus for spectroscopic measurement of the concentration of a gas, e.g. oxygen in a sample. In the apparatus the modulated intensity of light transmitted through the sample and reference cell is detected and a signal proportional to the ratio of the demodulated intensities is generated which represents the concentration of the gas. Background of the invention Tunable diode lasers have quickly become important for high resolution instruments for analysis of molecule spectra. Most of the applications for diode laser spectroscopy have so far been in basic research. Lead salt diode lasers emitting in the wavelength range of 3-30 urn have been used to study absorption line parameters and for measurement of molecule constants (1,2). The possibility to indirectly determine different parameters such as pressure, tempera¬ ture, or electrical field strength has also been successful- ly demonstrated (3,4). There has been a relatively small interest for the overtone bands around 1 ^ μm since these do not significantly contribute to any new information on the analyzed molecules. The main limitation for practical use of lead salt diode lasers in measurement systems have been the need for cooling of to temperatures below that of liquid nitrogen. AlGaAs and InGaAsP diode lasers emit in the 0.68 - 1.7 urn wavelength range and can operate at temperatures up to 50 degrees centigrade. A characteristic of these lasers compared to lead salt lasers is their high intensity modulation index which requires special signal analysis to obtain optimum sensitivity. A large number of molecules of interest in process control and environmental measurement applications have absorption bands in the 0.7 - 1.7 urn range, although, these are relatively weak overtone bands. The superior performance of AlGaAs and InGaAsP lasers compared with lead salt lasers however, more than outweighs this difference and they have great potential to be used in instrumental applications (5). A very interesting application is for measurement of oxygen concentration, which has many practical applications e.g. in the medical area. Today, oxygen is usually measured using different electrochemical methods. For example semiconductor sensors or the transformation of 0 2 to secondary products for later detection is frequently used. These methods have several limitations. They don't perform real-time measure- ments and are usually not suitable in explosive environments and moreover, they often influence the measurand since a small amount of the measured (oxygen) gas is consumed by the measurement instrument. These measurement instruments are also often sensitive to other types of gases or organic pollutions which results in a considerably limited lifetime. From EP-A1-0015 170 it is known that by using spectrometers with reference and measurements cells and by using optical fibers or glass prism and gas-tight boxes interference with the surrounding environment is avoided. This is true concerning the elimination of unwanted contributions to the measurement result from other paths than the measurement path. However, the problem of eliminating the influence of nongasrelated transmission variations in the measurement path or optical probe is not addressed at all. In DE-A1-3.633.93 the laser is not locked onto the frequency of the absorption line. Instead, the laser current is modulated and the absorption spectrum is studied. The absorption line is then sampled as the current is modulated to determine the gas absorption. Furthermore, the spectrum is sampled on both sides of the line to measure the nongas¬ related attenuation. The signal conditioning is performed directly from the sampled spectrum which results in poor accuracy since the measurement value is the result of the substraction of two, nearly equal, numbers. This method is the most commonly used to avoid measurement errors from attenuation caused by fog, rain etc. Purpose and significant characteristics of the invention The purpose of the present invention is to establish a measurement method which is not influenced by the environ¬ ment outside the measurement volume or cell (the claimed optical probe) or by the environmental properties in the measurement path and in addition has a short response time. This has been obtained by locking a laser diode onto the absorption line of the gas in question in a reference cell containing this gas at known concentration and pressure and thereafter detecting the harmonics at 2f 0 that are generated from the interaction between the absorption line and a triangular modulation current of frequency f 0 superimposed on the laser bias current and furthermore, to avoid interferen¬ ce from the atmosphere optical fibers and/or glass prisms are used for the distribution of the modulated laser light with the selected wavelength to the reference cell and the optical probe or measurement path, and that the signal conditioning compensates for nongasrelated transmission variations in the measurement path or the optical probe by using a time-multiplexed dual-beam technique. The present invention also includes an apparatus for the method descri¬ bed where optical components of with low reflectivity (e.g. AR-coating of optical surfaces) are used to minimize interference problems. Moreover, multiplexing technique can be used to cover several measurement paths with just one laser or to measure several gases with several lasers utilizing the same measurement path and distribution net. Description of the drawings The invention will in the following be described with reference to the enclosed drawings. Fig. 1 shows a schematic of the electrooptical gas sensor according to the invention. Fig. 2 shows the measurement method with the used modulation signals and the corresponding detected waveforms after absorption in the measured gas. Specifically, the intensity modulation of the laser, the frequency modulation of the laser, and the detected intensity variation after passage of the measurement volume are illustrated. Fig. 3a shows computed signals after compensation for the intensity modulation of the laser and the following lock-in detection. Fig. 3b is the same as fig 3a but in this case for an incomplete intensity compensation resulting in a remaining intensity modulation of 1%. Fig. 3c shows the measurement signal as a function of the gas concentration after signal conditioning. Fig.- 3d shows how the output from the laser spectrometer varies with phase error in the lock-in detection. Fig. 3e shows the output signal from the laser diode spectrometer as a function the lasers frequency modulation. Fig. 3f shows the output from the laser spectrometer as a function of the total pressure in the measurement volume. Fig. 4 shows the basic structure of the instrument using optical fibers according to one embodiment of the invention. Fig. 5 shows a laser circuit board for the laser with the reference cell. Fig. 6 shows a system with several laser circuits who's output is multiplexed into one fiber for simultaneous measurement of several gases. Fig. 7 shows a system with one laser circuit which is multiplexed to several fibers for simultaneous measurements of one gas over several different measurement paths. Fig. 8 shows a schematic of the basic apparatus design using glass prisms for light distribution. Fig. 9 shows a schematic of the basic apparatus design using both glass prisms and optical fibers. Fig. 10 shows a block diagram of the measurement system including transmission compensation and lock-in detection. Fig. 11 shows a block diagram of the measurement system using digital modulation and measurement control. Fig. 12 shows, in perspective, an exploded view of the optical measurement probe. Fig. 13a shows a horisontal sectional view through the measurement probe and 13b a vertical sectional view through its lower part. Fig. 14 shows, in perspective, a reference cell. Fig. 15 shows, in a larger scale, a section through the reference cell. Description of the invention The invention concerns a method to analyze gases, e.g. oxygen, using a laser diode spectrometer. A special signal conditioning method for diode laser spectrometers, based on diode lasers with high intensity modulation index, has been developed. Interference from nongasrelated transmission variations such as fog, rain turbulence and varying trans¬ mission through the optics of the apparatus caused by dust particles, condense etc. is taken care of by the intensity modulation compensation in a unique manner. Interference from gases not contained in the measurement volume is eliminated by using glass waveguides in the instrument. The measurements can be performed over an atmospheric path, in an with the instrument integrated measurement volume to which the gas is transferred using e.g. tubes, using the evanescent field of an optical fiber surrounded by a medium containing the gas to be measured, or in a special measure¬ ment cell, a uniquely designed optical probe to which the light is passed in optical fibers. A measurement cell, a self-aligned optical probe that is sufficiently small to be integrated in e.g. the mouth piece of a patient and still gives a measurement path of suffici¬ ent length to perform accurate measurements of oxygen, has been developed specifically to be used with the spectrome- ter. The instrument is designed so that all measurements of different parameters is automatically calibrated if you know the corresponding parameters for the gas in question in a reference cell. This also includes the elimination of influences from fog, rain, dust or condense in the measure- ment volume or in the optics of the instrument itself. This means that you are independent of published numbers on line strength etc. A special compact reference cell that can be included on e.g. a simple standard europe-circuit board has been developed. The measurement results from the measurement volume ( atmospheric path, optical probe or evanescent fiber probe) are compared with the corresponding results from the reference cell. The gas concentration is computed from two lengths (those of the reference cell and the measurement path) and the known concentration in the reference cell. This results in a very simple calibration procedure and high measurement accuracy. Below is a list of a number of application areas for the invented diode laser spectrometer. Medical applications a) Measurement of the oxygen concentration in breathing air. Here a special optical measurement probe has been developed that can be incorporated in e. g. a respirator. The optical probe is connected to the mouth piece at the patient and the light is passed to the probe using optical waveguides (optical fibers). b) Control of anesthetic gases during operation. c) Control of oxygen or humidity in an incubator. d) Studies of metabolism. Here an isotope gas can be used since the high resolution of the instrument is sufficient to discriminate this from the natural abundance of the gas. e) Pharmaceutical production. Inert packaging of medicals. Industrial applications f) Safe measurements of oxygen or other gases in explosive environments such as petrol supplies, oil tankers etc. The light is passed to and from the optical measurement probe using optical waveguides. The probe can also be located in environments with strong electromagnetic interference effects such as in a radar set. g) Measurement of gas concentration in environments with strong radar or radio interference. This means that the laser diode spectrometer can be incorporated in a levelmeter based on microwave technology. h) Control the presence of oxygen in inert environments. i) Control of combustion processes. j ) Automotive industry; analysis of exhaust gases, control of air/fuel mixtures. k) Heating and electricity producing plants; control of combustion, minimization of pollution. 1) Gas production. m) Lamp manufacturing. n) Semiconductor industry; control of gas concentration in different processes, in owns, gloveboxes etc. o) Process control in annealing and oxidation owns. p) Control of fermentation processes. q) Food industry; beer production, packaging. r) Measurement of temperature profiles in oxygen containing atmosphere in process ovens. s) Measurement of pressure in gases t) Measurement of pressure in processes, tanks etc. u) Galvanic insulated measurements of electrical field strength. v) Measurement of gas concentrations in fluids, e.g. gases in a battery or the oxygen contents in a lake or sea using an evanescent fiber probe. x) Measurement of leakage from gas tubes by using an evanescent fiber probe that is deployed in parallel with the gas tube. Diode laser spectroscopy has traditionally been used to analyze the fundamental IR-band at 3 -30 urn. Laser light is selectively absorbed at frequencies v x v 2 v 3 ... which corresponds to fundamental rotational and vibrational transitions. The lasers that have been used in this wave¬ length range are complicated and expensive. A large number of molecules have combination and overtone bands of the 2v x + v _ type in the wavelength range 0.7 - 1.7 μ . These bands usually don't contribute any new information about molecular constants but are well suited for measurements of the concentration of the absorbing gas. This is especially true since in this wavelength range there exists a large number of inexpensive high quality lasers. In the following, measurement of oxygen is used to illustra¬ te the principle of operation of the invention. __ _ _ r~ I -- I-~* iϊ ~ eμs ; CT The oxygen molecule has a number of weak absorption bands generated by magnetic dipole transitions. These bands are located around 630, 690, and 760 nm. The A-band of oxygen covers the wavelength range of 759 - 771 nm and is relative- ly free from interfering molecules why it is suitable for measurement of oxygen using electrooptic techniques. AlGaAs or InGaAsP lasers are suitable light sources for measure¬ ments based on selective absorption of light by discrete molecule lines since they have good spatial and temporal coherence. By using oxygen at known concentration and pressure in a reference cell a normalization signal is obtained and also the laser can be locked to the absorption line of oxygen. This enables very accurate measurements of the oxygen concentration in the measurement volume. AlGaAs, InGaAsP and other semiconductor lasers can easily be frequency modulated by means of the injection current and can therefore be used in differential spectroscopy to obtain a good signal-to-noise ratio. Another characteristic of these lasers, compared with e.g. lead salt lasers, is that apart from the frequency modulation a considerable intensity modulation is obtained at the frequency modulation that is optimum for spectroscopic measurements. The intensity modulation is used to eliminate the influence of nongas- related absorption in the measurement volume or in the instrument itself without having to use the baseline of the absorption spectrum. This provides superior stability and accuracy. When one measure atmospheric gases it is important to eliminate absorption in air paths to ands from the measurement volume. By using glass prisms or optical fibers this unwanted absorption can be avoided. Fig. 1 shows a schematic of the electrooptical gas sensor according to the invention where 1 is a light source, a laser diode , from which the light is distributed in optical waveguides 2 and 3 to a measurement cell 4, which can be an optical probe or an atmospheric path, and to a reference cell 5. The measurement cell 4 and the reference cell 5 is connected with a control unit 8 using optical waveguides 6 or electrical cables 7. The reference cell 5, which contains oxygen at known concentration, pressure, and temperature, provides the parameters necessary to lock the wavelength of the light source to the absorption line, and the parameters necessary to calculate the gas concentration, the temperature, pressure, and electric field strength. This is performed according to the following. A triangular AC-current with frequency f 0 is added to the laser bias current. The bias current is adjusted so that the average wavelength of the laser coincides with that of the absorption line. The light source 1 will, due to the added AC-current, change its wavelength (frequency modulate ) with the frequency f 0 around the averaged value set by the bias current. The light, now frequency modulated around the center of the absorption line of the gas, is passed through the measurement cell (an at- mospheric path, an optical probe, or an evanescent fiber) and is thereafter detected. By feedback of the signal of 3b via an analog regulator to the laser bias current the wavelength of the light source 1 is stabilized to the center of the absorption line. The light from the light source 1 is divided into to branches, one which is passed to the reference cell 5, and one which is passed using optical waveguides 2 to the measurement cell. The measurement signal is then passed back and lock-in detected at frequency 2f 0 . When the light source is modulated with a frequency f 0 and the signal from the detector is demodulated with the frequency 2f 0 , this signal looks according to fig. 3a. The signal 2xf in fig. 3a is proportional to the gas concentra¬ tion. Apart from the variation in absorption caused by variations in the concentration of the measured gas there will be variations in the transmission caused by changes in the transmission of the optics due to rain, dust, or humidity or when the received signal after the measurement path varies due to turbulence, rain, and fog etc. Normally, this is compensated for by measuring the baseline of the absorption spectrum and make a normalization. This baseline value however, is a slowly varying signal with a very low lower frequency limit which imposes drift problems. Furthermore, preamplifiers designed to accommodate these low frequencies have much less sensitivity than AC-coupled amplifiers operating with a small bandwidth. In measurements of gas concentrations it is very important to compensate for absorption that can arise in air paths that exist in the distribution of the light to and from the measurement area. By using glass prisms or optical fibers this unwanted absorption can be eliminated. Furthermore, it is also important to compensate for varying transmission in the instrument itself or in the measurement path that is not related to the measured gas. This can be achieved using a signal conditioning which identifies this component and compensate for it without having to use the baseline of the absorption spectrum. This technique provides superior stability and measurement accuracy. In the system according to the invention a signal pro¬ portional to the atmospheric transmission is generated by sampling at the peak of the received triangularily shaped optical signal. The peak value is compared with the signal from the monitor photodiode. The peaks of the triangular signal is well separated from the absorption peak as illustrated in fig. 2. The relative size of the absorption peak is usually much smaller than what is shown in the figure. This method of measuring both on the peaks of the triangular signal and on the absorption line generates a measurement reference that automatically experiences the same transmission losses as the light absorbed by the absorption line since by definition the beams are coaligned. A "dual-beam spectrometer" has been realized by time- multiplexing of one measurement beam. In ref. 7 the absorp¬ tion is determined from sampling directly in the absorption spectrum around the line. However, no modulation technique is used why the drift problems of this type of instrument is considerably large. In our method it is very easy to calculate the gas concentration using a normalization procedure considering that we know the gas concentration in the reference cell. The concentration is computed from the lengths of the path in the measurement and reference cell and from the measured detector signals from the measurement and reference channels as well as the gas concentration in the reference cell. This method differs considerably from those used in ref. 6, 7, and 8, where the laser light, which is unmodulated, is slowly varied around the absorption line and the resulting spectrum is sampled relative to the baseline. Normally, this is the method used to compensate for nongasrelated transmis- sion variations. The signal conditioning method according to the invention, which has been described here, performs all signal conditioning at high audio frequencies, resulting in superior stability, measurement accuracy and sensitivity. To determine the pressure in the measurement volume we proceed according to the following. Since the width of the absorption line depends on pressure and temperature one parameter has to be isolated if we are going to be able to determine the other. We let the wavelength of the light source sweep over the absorption line. The light is then detected after passage through the gas and the width and the integral of the absorption line is measured simultaneously. The result of the integration gives the integrated line strength which is a parameter whos temperature dependence is known and is available in the literature. Since the pressure and temperature in the reference cell 5 is known, the pressure in the measurement volume can be calculated. The temperature can be measured with high accuracy by using two laser circuits where the lasers are locked to two different rotational transitions in e.g. oxygen. The laser light from the cards are multiplexed together in an optical fiber as shown in fig. 7 and the combined light is passed to the measurement volume. The temperature is then calculated from the difference in absorption in the two wavelengths. This is a new way to apply Mason's method. In this way the temperature can be measured locally and intrinsically safe using the optical probe or alternatively, the average temperature over an atmospheric path can be determined. An electrical field strength is measured in a similar way by sweeping the laser wavelength over the absorption line. In the presence of an electrical field in the gas the absorp¬ tion maximum will be changed or displaced in wavelength. Since we know the position and strength of the absorption line in the reference cell 5, this displacement can be determined which is a measure of the electrical field strength. Strong magnetic fields results in a direct modulation of the gas concentration in a paramagnetic gas as oxygen. The variation in gas concentration gives a direct measure of the magnetic field variations. With the spectrometer configured for a free measurement path field variations between different paths can be analyzed. It is usually advantageous to a large extent use digital electronics to generate the modulation and reference signals in the laser diode spectrometer. For instance it is easier to obtain a high degree of phase stability compared to an analog solution and moreover, it is easier to digitally control the frequency and phase. It is also advantageous to use a (digital) square-wave signal to demodulate the measurement and reference signals in the spectrometer. This avoids a square-wave to sinus-wave transformation which if performed with analog technique can lead to drift in the phase and decreased measurement accuracy . Traditionally, the modulation signal in laser diode spectrometers has been a sine-wave but it would be a clear advantage if a simpler waveform could be used. An ideal alternative would be a triangular wave which is easy to generate from a square-wave with an AC-coupled integra- tor. Figure 2 illustrates the signal conditioning used in the invention. The laser is modulated with the current i(t) = i 0 [ 1 + g(t) ] where g(t) is a triangular wave with the amplitude a 0 The laser will be modulated both in intensity (fig. 2:1), P L P 0 [1 + mg(t)] and in frequency (fig 2:2), v L = v 0 [1 + βg(t)] with the frequency f 0 . Here, m = intensity modulation index of the laser and β is the frequency modulation index. When the optical signal sweeps over the absorption line of the measured gas its frequency modulation will transform into an amplitude modulation according to m (t) -S c m N L /π * /273/T' * v B /[(βg(t)) 2 + Δ v B 2 ] here S, N L and & v B are constants of the molecule line and c m is the gas concentration. A composed signal with the fundamental frequency f 0 is obtained according to fig 2:3 V s (t) = G, P 0 τ mea (i+m g(t)) (1 - α_(t) L mea ) The AC-component of this signal is v s ( t ) = G x P 0 X mea [m g( t ) - ( 1 + m g( t ) ) m ( t ) L mea ] The signal in the measurement channel is now sub- stracted withe monitor signal which after AC-coupling can be expressed as v non (t) = G 2 P 0 m g(t) The detected measurement signal now has the form v t )» G 2 P 0 m g( t ) - G x P 0 r nea [m g( t ) - ( 1 + mg( t ) ) m ( ) L mea ] This signal is sampled at the peaks of the triangular wave and thereafter the analog signal conditioning unit adjusts the gain Gl so that v mea (nT)= G 2 P 0 m gdvTJ-G^ o t_ ea [mg(nT)-(l+mg(t) ) m (nT)L mea ] which results in G 2 m g(nT) G ~ ι. ^ m g(nT) -{ 1 + m g(nT)} α_[nT_L roea ] In all practical applications the residual term due to the extension of the absorption line out to the peak of the triangular wave will be neglectable and the expression for G x becomes Gi = G 2 / mea Consequently, with this method the system will automatically compensate for variations in transmission in the measurement path. The measurement signal after this compensation is v nea - G 2 P 0 ( 1 + m g( t) ) α_[t] L mea The measurement signal is demodulated in two steps according to fig. 10. The first step is the analog signal conditioning unit with the transmission compensation described above. In step two the compensated measurement signal is synchronously demodulated using a square-wave. The compensated measurement signal is divided according to its frequency components 00 v mea (t)=G 2 P 0 L mea {l+m8/τt 2 Σ{[-l] ϋ - 1) 2 }/j 2 cos[j(wt+θ)]} * J-l.3.5 co * Σ H^v). cos [iwt] i=0 By multiplying with a square-wave of frequency 2f 0 and perform a low-pass filtering the final signal is obtained = G 2 P 0 L mea {H 2 (v) m + m8/τt 2 [(H^v)., + H 3 (v) m ) cos[θ]- - H 1 (v) m /18 cos[3θ] + H 3 (v) m /50 cos[5θ]]} The phase θ is adjusted to minimize the interference term. In this case m = 6%. In the vicinity of the line center v = v 0 ~ H 1 (v) m , H 3 (v) πι « 0 and thus the measurement signal after lock-in detection becomes v nea = G 2 P 0 L raea H 2 (v) m In the same manner, the signal from the reference detector finally becomes V ref =G 2 P 0 L ref H 2 (v) r These two signals are sampled, A/D-converted and divided in the computer v mea /v ref = G 2 P 0 L mea H ( v) B / G 2 P 0 L ref H 2 (v) r The signal ^(v),,, is proportional to the gas concentration c i and the laser diode spectrometer calculates the gas con¬ centration in the measurement path as C ne a = C V mea/ V ref ' C L ref C ref/ L mea J The constants L ref and c ref are known while L mea either is measured separately or using the spectrometer. This can be achieved by measuring the phase difference between the reference and measurement signal from which a signal proportional to L mea can be obtained. This means that the instrument after calibration by itself can measure all data necessary to calculate the gas concentration. A computer simulation has been made to verify the function of the laser diode spectrometer. The following parameters have been used. Parameter Modulation frequency, w/2rc Laser modulation IM, m Laser modulation FM, 2β LF Thermal cutoff frequency Absorption at v 0 , a(v 0 )L Pressure broad.coeff. (HWHM),^v B Pressure, p Temperature, T Absorption wavelength Laser center wavelength Phase error, reference signal A triangular wave is generated directly from a digital control unit using an integrating OP-amplifier. The laser bias current is adjusted so that the laser light is absorbed in the gas molecules at the zero crossings of the triangular wave. This triangular wave modulates the laser intensity according around P 0 according to fig. 2, curve 1 and the laser frequency around v 0 according to curve 2 at a frequen- cy f 0 . After passage through the gas volume a measurement signal according to curve 3 in fig. 2 is obtained. The gain G- L is automatically adjusted as previously described and the resulting measurement signal is obtained after substraction of the monitor signal. Lock-in detection at 2f 0 and 3f 0 with digital reference signals provides the final measurement signal and feedback signal. This leads to a straight forward instrumental design and provides higher sensitivity compared with the conventional approach using sine-waves. The detected signals from an absorption line at the different lock-in detection frequencies are shown in fig. 3a. From fig. 3b it is apparent that only 3f 0 is suitable for locking of the laser, since this signal is insensitive to remaining intensity modulation after the first demodulation step. Figure 3c shows that by using this signal conditioning method a linear response for gas concentration measurements is obtained. The measurement itself is performed in a measurement volume that might be an atmospheric path, an evanescent optical fiber, or an optical probe that in a small volume creates a suitable absorption path. The distribution of light both to and from the probe can be performed with optical waveguides. This means that the sensor part of the instrument is entirely optical and is very suitable in potentially explosive or electrically disturbed environments. Moreover, the attenuation in optical fibers is very low why the sensor can be located several kilometers from the control electro- nics. Using optical fibers provides a flexible instrument which may be of modular design according to fig. 4 which shows a measurement cell 4 integrated in the diode laser spec- trometer. Laser light source 1, measurement cell 4, and reference cell 5 can be placed in an instrument box. The different modules can be constructed on standard europe circuit boards in a standard 19" rack. The measurement cell is located inside the instrument and the gas to be analyzed is led to it using flexible hoses 9 and 10. Other parts of the system includes a modulation and control unit 11, a laser and peltier driver 12, an interface 13 and power supply 14. Figure 5 shows an alternative instrumental design where a compact measurement cell 4 is connected to the diode laser spectrometer with optical fibers 2. The measurement cell 4 is designed to be integrated in e.g. a patient mouth piece to measure the oxygen contents. The gas flow through the measurement cell 4 is indicated with arrows. The measurement cell 4 is then connected to the receiver card with optical fibers or electrical wires 6. The instrument is intended to operate completely automatic and therefore the adjustment of laser temperature, bias current, locking to the absorption line, and measurement of the absorption is controlled from a computer, standard PC or equivalent, via an interface 13. On the laser circuit board 16 (fig. 6) those parts are integrated that determines which gas that is to be measured. A molecule is selected by matching a suitable laser 1 and a reference gas contained in the reference cell 5 integrated on the card. A laser module 1 with fiberpigtail, an optical power divider, reference cell, and electronics is mounted on the laser circuit board 16. The reference cell 5 is used to stabilize the laser to the absorption line and to provide normalization values for the calculation of the gas con¬ centration. By locating the laser and the reference cell on the same card splicing of the fiber to the reference cell is avoided which results in a lower instrumental noise. Moreover, a modular design of the instrument is obtained. The collimated light out from the measurement fiber is centered on wavelength of the absorption line of the gas in the reference cell. This means that measurements can be performed in several different measurement situations, e.g. over an atmospheric path, in an evanescent fiber probe, a specially designed optical probe, or in a conventional measurement cell. The modular design of the spectrometer means that several laser circuits can be multiplexed on the same fiber, either with wavelength multiplexing or alternatively with time multiplexing there one laser ciruit at a time is used . In this way it is possible to measure several gases over the same measurement path. You can also choose to multiplex one laser circuit to several measurement fibers and in this way measure one gas on several different measurement paths that can be located kilometers apart. Several components suitable for this multiplexing has been developed in the area of optical fiber communication. Figure 7 shows a device where laser circuits 16a-d, each tuned to an absorption line, are multiplexed into a common measurement fiber 18 by using a fiber multiplexer 17. Another way of avoiding free air paths in the instrument and obtain a compact design is to use glass prisms for light distribution between laser and reference cell and for splitting the light to a measurement and a reference path. Such an arrangement is shown in fig. 8 where the laser light form the laser 1 is distributed to measurement cell 4 and the reference cell 5 by means of beamsplitter 19 and a glass prism 20, and passed on to the detectors of the measurement 4' and reference 5' cells. Other parts of the arrangement are in and outgoing flexible tubes, 9 and 10, to the measurement cell 4 and a peltier cooler 21. Figure 9 show a modified arrangement according to which the instrument can be connected to a compact optical probe of the type sown i fig. 4 using optical fibers 2 and 6. A seal-off valve to the reference cell is marked with 22. A single-mode fiber 2 is connected to the optical probe to maintain good beam quality while a multimode fiber 6 is preferable to pass the light back from the optical probe to collect as much light as possible. Two different methods can be used for the signal conditio¬ ning depending on what degree of instrumental complexity that can be accepted. In the first method, transmission compensation followed by lock-in detection, which is schematically illustrated in fig. 10, the laser is modulated with a triangular wave which is obtained directly from the digital unit and the received signal is demodulated in two steps. Before the phase sensitive lock-in detection an analog signal conditioning is performed 32, where the signal from the monitor photodiode of the laser is used to compensate the measurement signal for unwanted attenuation caused by environmental influences in the measurement path and in the optics of the instrument. The harmonics of the received intensity, which is modulated by the absorption line, is thereafter detected with phase sensitive demodulators (lock-in detection). The intensity variations of the resulting normalized signal will then only by dependent of molecular absorption as described in the invented signal conditioning. The reference signals to the phase sensitive demodulators can be either square-wave or sine-wave, preferably square-w¬ ave. The phase difference between the received modulation signals and the reference signals is optimized automatically by a computer. The phase difference between these signals can also be used to determine the length of the measurement path, a value needed for the gas concentration calculation. The information from the signal on the second harmonic 2f0 is fed to an analog multiplexer and an A/D-converter for calculation of the gas concentration. Information from the third harmonic 3f0 is used to stabilize the laser to the center of the absorption line via a PID-regulator. This signal is also transferred to the computer to verify that the laser operates at the proper wavelength. The second measurement method, schematically shown in fig. 11, uses digital modulation and measurement and is based on that the laser is modulated with a special waveform and that the amplitude of the measurement and reference signals are sampled with an A/D-converter. The gas concentration is then calculated in the computer. Information about the laser wavelength compared to the absorption line is extracted from these sampled values and the laser bias current and tempera¬ ture is adjusted accordingly. The signal analysis is of the same type as that used in ref 8, but with the important difference that we use a preprocessing with analog signal conditioning to compensate for nongasrelated attenuation, which results in higher measurement accuracy. The signal from the measurement cell 4 is fed back to the electronic unit using a multi-mode fiber or alternatively the detector can be located in the measurement cell and the signal led back using ordinary electrical cables. In AlGaAs and InGaAsP lasers a considerable intensity modulation is obtained together with the frequency modulation. In the invention this is used to automatically compensate for nongasrelated variations in the transmission in the measurement path or in the optics of the instrument. Measurement cell In certain measurement applications it is important to have a very compact measurement cell. This can be realized by "folding" the cell a large number of times. Each time this folding occurs means that the beam is reflected against a mirror which adds losses in to the beam path. These losses must be kept low and moreover, the are not allowed to be strongly dependent of the optical wavelength. The minimum cell acceptable cell transmission is set by the signal-to-n¬ oise ratio (SNR) required. One type of mirror that can be used here is dielectric mirrors. They have a limited wavelength range but apart from that they have very good spectral characteristics including low losses. Figure 12 shows in perspective the measurement optical probe and fig. 13 shows a sectional view through it to illustrate the beam path. The measurement optical probe consists of a cylindrical measurement volume, with dimensions e.g. 20x20 mm. The cylinder is divided into 12 segments each of 30 degrees which each contains a dielectric mirror having a reflectance of at least 98%. The beam will be reflected 36 times in the probe which corresponds to a maximum attenuation of 0.9836 = 0.48 (3.2 dB). The probe is fed from a singel-mode fiber (typical 5/125 mm) and a lens which creates a parallel beam with a diameter of approximately 0.8 mm. The effective path length in the probe is approximately 70 cm. The detection of the outcoming beam is either performed directly on a photodiode mounted in the probe or via a fiber with large core diameter in which case the photodiode can be located far away from the measurement volume. A unit 24 for coupling of the light into the optical probe enables the alignment of the beam with a sufficient number of degrees of freedom. The material of the measurement optical probe can be aluminum, stainless steel, or a ceramic. Another type of optical probe is an optical fiber where the evanescent field which propagates outside the core is used. When light propagates in an optical fiber the main part of it is confined to the core but a certain part also pro¬ pagates in the cladding (the evanescent field) . By using a specially designed fiber that only consists of a core and letting this fiber be surrounded by a fluid that constitutes the cladding (or alternatively let a surrounding gas constitute the cladding) the evanescent field and thereby also the total optical field will be influenced in a similar way as when light propagates over an atmospheric path. In this way it is possible to determine the concentration of a specific gas in a surrounding atmosphere or fluid. Further¬ more, OTDR (Optical Time Domain Reflectometr ) can be used to localize point emissions along an evanescent fiber probe. Fiber adapter It must be possible to align the fiber tip so that the light beam after passage through the measurement cell 4 or the reference cell 5 impings upon the photodetector (or out- coupling fiber). This is obtained using a fiber tip equipped with a spherical adapter. This arrangement provides suffici- ent number of degrees of freedom in the alignment. The fiber is aligned once and for all and then locked with a clamping screw. Reference cell Figure 14 shows in perspective the reference cell 5 which consists of a rigid plate 23, an incoupling unit 24 and the measurement volume 25. According to one design it has en effective length of 10 cm and is constructed for 8 passages, i.e. a total measurement path of 80 cm. A seal-off valve 26 and a quartz window 27 between the incoupling unit 24 and the cell is also included in the reference cell. Figure 15 shows in a larger scale a section through the reference cell. Two dielectric mirrors 27 and 28 with high reflectivity (typically better then 0 .98) is mounted at both ends of the cell. In this example the reference beam is reflected 7 times corresponding to a total attenuation of 0.987 = 0.87 (0.6dB). The base plate 23 is designed to fit onto a standard europe circuit board. References 1. R.S. Eng, J.F. Butler, and K.J. Linden, "Tunable diode laserspectroscopy: an invited review, " Optical Engineering, vol. 19, p. 945, 1980. 2. S. Lundqvist, J. Margolis, and J. Reid, "Measurements of pressure broadening coefficients of nitric oxideand oonsing a computerized tunable diode laser spectrometer, " Applied Optics, vol. 21, p. 3109, 1982. 3. H. Ahlberg and S. Lundqvist, "IR-laser spectroscopy for measurement applications in the industrial environment, " 7th International Conference on laser Spectroscopy, SEICOLS 85, Maui, Hawaii, USA, 24-28 juni 1985. In Laser Spectroscopy VII, Springer series in optical sciences; Springer Verlag Berlin, vol. 49, 1985. 4. S. Hjer, H. Ahlberg, and S. Lundqvist, "Measurements of electric fields in gas insulated high voltage components using infrared diode laser spectroscopy, " Applied Optics, vol. 25, p. 2984, 1986. 5. D.T. Cassidy, "Trace gas detection using 1.3 m InGaAsP diode laser transmitter modules," Applied Optics, vol. 27,p. 610, 1986. 6. G. Boisde, G. Chevalier, and J.-J. Perez, Demande de Brevet Europeen 0 015 170 Al, European Patent Office, 18 januari 1980. 7. K. Cerff, H. Giraud, and G. Krieg, Offenlegungsschrift DE 3633931 Al, Deutsches Patentamt, Bundesrepublik Deutsch- land, 4 oktober 1986. 8. G. D. Pitt, D.N. Batchelder, and R.E. Jones, UK Patent Application GB 2 165 640 A, 13 oktober 1984.

Claims: AMENDED CLAIMS [received by the International Bureau on 1 December 1989 (01.12.89); original claims 1-9 amended; other claims unchanged ( 5 pages)] 1. A spectroscopic method to measure the concentration of a gas in a sample in which the intensity of light from a light source ( 1 ) passed through the sample ( 4 ) and through a reference cell ( 5 ) is detected and a signal is generated which represents the concentration of the gas wherein a laser diode ( 1 ) constitutes the light source which is locked to the absorption line of the gas at known pressure and concentration contained in a reference cell (5) , and that to avoid interference from outside the measurement path the laser light is distributed via optical fibers (2,3,6) and/or glass prisms ( 19,20) to the reference cell (5) and the sample (4) c h a r a c t e r i z e d b y , that nongasrelated transmission variations automatically is compensated for by the laser being intensity modulated with a preferably triangular wave audio frequency signal of the period T whereby in a first demodulation step the intensity modulation is used to measure the transmission of the measuring path by forming a first difference signal between a monitoring signal from a monitor diode (31) and a detected measuring signal from a detector (41) and a second differen¬ ce signal between the monitoring signal and a reference signal from a detector (51) whereby the gain level of (Gl ) and (G3) respectively of the recieved signals automatically is adjusted in an analog signal conditioning unit (32) such that first and second difference signals are respectively equal to zero when sampling in a maximum point at the times n * T whereupon in a second demodulation step the harmonics of the intensity which is modulated by the absorption line is detected by phase sensitive demodulators (42, 52, 53). 2 . Method as claimed in 1 , c h a r a c t e r i z e d b y that the laser diode ( 1 ) is current modulated with a signal in the audio frequency range, preferably triangular in shape, obtained from a digital modulation and control unit (11). 3. Method as claimed in 2, c h a r a c t e r i z e d b y , that the detected signals from the sample (4) and reference cell (5) is demodulated in two steps, where the first step (32) uses the intensity modulation of the laser diode and the signal from the monitor photodiode (31) of the laser to automatically compensate for nongasrelated transmission variations in the instrument without having to use the baseline of the spectrum, and thereafter in step two performs lock-in detection with digital reference signals obtained from the modulation and control unit (11 ), whereafter the demodulated signal from the sample (4) is divided with the demodulated signal from the reference cell (5). 4. Method as claimed in any of the preceding claims, c h a r a c t e r i z e d b y , that the phase difference between the signals in the measurement and reference channel is used to determine the length of the measurement path which is necessary for the gas concentration calculation. 5. Method as claimed in any of the preceding claims, c h a r a c t e r i z e d b y , that the laser diode (1) is modulated with the frequency (f), that the measurement signal from the sample (4) is demodulated with the frequency (f ), double or quadruple frequency (2f,4f) and that a signal demodulated with the triple frequency (3f) provides the feedback signal for locking of the laser diode, while the signal at f gives an automatic compensation for nongasrelated transmission variations. 6. Method as claimed in 1 , c h a r a c t e r i z e d b y , that the current modulation of the laser diode (1) is performed using a stepwise modulation whereafter the corresponding points on the absorption spectrum of the gas after compensation for the intensity modulation are measured with an A/D-converter which calculates derivatives and measurement values and also locks the laser diode to the absorption line. 7. Method as claimed in any of the preceding claims, c h a r a c t e r i z e d b y , that the pressure, temperature and/or magnetic and electric field strength is determined by measuring the corresponding relationship of these parameters to the shape, position, and strength of the absorption line. 8. Method as claimed in any of the preceding claims, c h a r a c t e r i z e d b y , that a long effective measurement path is created in a measurement optical probe (4) and/or reference cell (5) by reflecting the light beam several times within the cell. 9. Apparatus for spectroscopic measurement of the concentra¬ tion of a gas in a sample according to the method claimed in 1, incorporating a light source (1) to provide the light beam through the sample (4) and a reference cell (5), and incorporating means for detection of intensity of the light transmitted through the sample and through the reference cell, and also means for generating a signal proportional to the ratio of the demodulated intensities, where the referen¬ ce cell (5) contains the gas to be measured with known concentration and pressure, and the light source (1) is a laser diode locked to the absorption line of the gas in the reference cell (5), and also including means for distribu- tion of the laser light to the reference cell (5) and to the sample (4) consisting of optical fibers (2,3,6) and/or glass prisms to avoid unwanted interference from the atmosphere, c h a r a c t e r i z e d b y , a laser current modulator the intensity of which modulates the laser with a periodic preferably triangular audio frequency signal, an analogue signal conditioning unit (32) which is provided with inputs for a monitoring signal from a monitor diode and for a measuring signal from a detec¬ tor/amplifier (41) and for a reference signal from a detector/amplifier (51) whereby the signal conditioning unit (32) contains controllable amplifiers (Gl) and (G3) the outputs of which are connected to difference amplifiers (Dl) and (D2) respectively, the outputs of said difference amplifiers are connected respectively to sample and hold circuits (SHI) and (SH2) which are triggered from a peak detector (PT) which detects peak values of said monitor signal whereby the signals from respectively sample and hold circuit are filtered in the circuits (PI1) and (PI2) to form a control signal for the settings of the gain of the amplifiers (Gl) and (G3) respectively. 10. Apparatus as claimed in 9 , c h a r a c t e r i z e d b y , that the measurement is performed in a measurement cell (4) to which the laser light is distributed, and that in the measurement cell reflecting means (30) are provided to reflect the laser beam several times thereby increasing the effective length of the measurement path inside the measure¬ ment cell. 11. Apparatus as claimed in 9 or 10, c h a r a c t e r i z e d b y that the measurement is performed in a measurement cell (4) to which the laser light is distributed, and that coupling means (24) are provided at the measurement cell to align the laser beam with a sufficient number of degrees of freedom. 12. Apparatus as claimed in 10 or 11, c h a r a c t e r i z e d b y . that the measurement cell (4) is formed as a tube, prefe¬ rably cylindrical, and is divided in several segments each of which containing reflective elements, e.g. a dielectric mirror arranged to reflect the laser beam in several planes inside 5 the measurement cell in such a way that the beam pattern automatically repeats itself in consecutive planes. 10 13. Apparatus as claimed in 9-12, c h a r a c t e r i z e d b y , that the reference cell (5) incorporates reflective ele¬ ments, e.g. dielectric mirrors (28,29), to reflect the laser beam several times inside the reference cell. 15 14. Apparatus as claimed in 9, c h a r a c t e r i z e d b y , that the measurement is performed in an optical fiber designed so that the surrounding fluid or gas via the 20 evanescent field affects the laser light so that the concentration of the substance in question in the surroun¬ ding fluid or gas can be determined. STATEMENTUNDERARTICLE19 The characterizing portion of the Claim 1 defining the feature of automatic compensation for nongasrelated transmission varia¬ tions by intensity modulation of the laser has been revised in order to give a more distinct definition of the demodulation steps mainly with respect to the formula in the specification page 16, line 14 and the function of the signal conditioning unit (32) shown in detail in figs 10 and 11. The characterizing portion of the Claim 9 has been revised in order to clearly describe the nescessary means contained in the signal conditioning unit (32) to accomplish the method according to Claim 1.

Inventors: AHLBERG HENRIK, ANDERSSON TORBJOERN, LUNDQVIST STEFAN, TELL ROBERT, AHLBERG, HENRIK, ANDERSSON, TORBJOERN, LUNDQVIST, STEFAN, TELL, ROBERT
Applicants: ALTOPTRONIC AB
Application year: 1989
Main classification: G01J3
IPC codes: G01J1, G01J3, G01N21, H01S5