COMPACT GAS SENSOR
20220214267 · 2022-07-07
Inventors
Cpc classification
International classification
Abstract
A gas sensor comprises an enclosure configured to receive a gas. The enclosure comprises a sidewall extending, around a transverse axis, between a first wall and a second wall. The sensor also comprises a light source configured to emit a light wave that propagates in the enclosure and forms, from the light source, a first light cone. A measuring photodetector is configured to detect the light wave emitted by the light source and propagated through the enclosure. The first wall and the second wall each comprise at least one reflective surface, forming a portion of an ellipsoid of revolution. Each reflective surface is associated with a rank n, n being an integer greater than or equal to 1.
Claims
1-14. (canceled)
15. A Gas sensor comprising an enclosure configured to receive a gas, the enclosure comprising a sidewall that extends, about a transverse axis, between a first wall and a second wall, the sensor also comprising: a light source configured to emit a light wave that propagates through the enclosure and forms, from the light source, a first light cone; a measuring photodetector configured to detect a light wave emitted by the light source and propagating through the enclosure; the sensor being such that the first wall and the second wall each comprise at least one reflective surface, forming a portion of an ellipsoid of revolution, with each reflective surface being associated with a rank n, n being an integer higher than or equal to 1, such that the sensor comprises: a first reflective surface of rank 1, having a first focal point and a second focal point, the first reflective surface being placed facing the light source, the first reflective surface forming a portion of an ellipsoid of revolution associated with an ellipse the eccentricity of which is lower than or equal to 0.7; at least one reflective surface of rank n strictly higher than 1, each reflective surface of rank n having: a first focal point, coincident with the second focal point of a reflective surface of preceding rank n−1; a second focal point, distinct from the first focal point and coincident with the first focal point of a reflective surface of following rank n+1; a last reflective surface of rank N, comprising a first focal point coincident with the second focal point of a reflective surface of preceding rank, the last reflective surface also comprising a second focal point; such that the light wave emitted by the light source is successively reflected by the N ellipsoidal-of-revolution reflective surfaces, according to their respective rank, before converging towards the second focal point of the last reflective surface in such a way as to form a last light cone, the measuring photodetector being placed so as to lie in the last light cone.
16. The sensor according to claim 15, wherein the light source is placed at the first focal point of the first reflective surface, or at a distance smaller than 1 mm from the latter.
17. The sensor according to claim 15, wherein the measuring photodetector is placed at the second focal point of the last reflective surface, or at a distance smaller than 1 mm from the latter.
18. The sensor according to claim 15, wherein: each reflective surface of rank n is configured to reflect the light wave that it receives in such a way as to form a light cone of rank n+1, the latter extending about a propagation axis of rank n+1; when n<N, the propagation axis of rank n+1 extends from the surface of rank n to the surface of rank n+1 and through the second focal point of the surface of rank n, the latter being coincident with the first focal point of the surface of rank n+1; when n=N, the propagation axis of rank N+1 extends from the surface of rank N to the measuring photodetector; in such a way that the light wave emitted by the light source undergoes a number of reflections corresponding to the number of reflective surfaces before reaching the measuring photodetector.
19. The sensor according to claim 18, wherein, when n<N, each light cone of rank n+1 converges towards the second focal point of the surface of rank n from which it is propagating, then diverges towards the surface of rank n+1 towards which it is propagating.
20. The sensor according to claim 15, wherein the light source and the photodetector are integral with an internal face of the first wall, the internal face being oriented towards the interior of the enclosure.
21. The sensor according to claim 20, wherein: reflective surfaces of even rank are arranged on the internal face of the first wall; reflective surfaces of uneven rank are arranged on an internal face of the second wall.
22. The sensor according to claim 21, wherein the enclosure is formed by assembling the first wall facing the second wall.
23. The sensor according to claim 15, wherein the number of reflective surfaces lying between the light source and the measuring photodetector is uneven.
24. The sensor according to claim 23, wherein the number of reflective surfaces lying between the light source and the measuring photodetector is equal to 5.
25. The sensor according to claim 15, comprising a reference photodetector configured to detect a light wave considered not to be attenuated by the gas.
26. The sensor according to claim 25, comprising a reference reflective surface, forming an ellipsoid of revolution, the reference surface comprising: a first focal point placed at the light source, or at a distance smaller than 1 mm from the latter; a second focal point placed at the measuring photodetector, or at a distance smaller than 1 mm from the latter.
27. A Method for analysing a gas using a sensor according to claim 15, the method comprising the following steps: a) introducing the gas into the enclosure of the sensor; b) illuminating the gas using the light source; c) measuring, with the measuring photodetector, a light intensity of a light wave emitted by the light source and having propagated through the enclosure; d) determining an amount of a gaseous species in the gas, on the basis of the measured light intensity.
28. The method according to claim 27, wherein step d) is implemented by a processing unit on the basis of a signal generated by the measuring photodetector.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0041]
[0042]
[0043]
[0044]
[0045]
DETAILED DESCRIPTION
[0046]
[0047] The first wall 4 comprises an external face 4.sub.e and an internal face 4.sub.i. The second wall 5 comprises an external face 5.sub.e and an internal face 5.sub.i. The respective external faces 4.sub.e, 5.sub.e of the first and second walls 4, 5 are planar and lie parallel to the main XY plane. They are perpendicular to the transverse axis Z about which the annular wall 6 extends. The respective internal faces 4.sub.i, 5.sub.i of the first and second walls 4, 5 are oriented towards the interior of the enclosure 2. The enclosure 2 is connected to connection pins 3, parallel to the transverse axis Z.
[0048] The shape and dimensions of the sensor 1 are in accordance with a format that is conventional in the field of gas detection called the 4R format. The diameter (I) of the enclosure 2 is 20 mm, and its height h is 16.6 mm. On account of the thickness of the sidewall 6, the inside diameter Φ′ of the enclosure 2 is 17 mm. A positive direction of rotation around the transverse axis Z is defined and is considered arbitrarily to be similar to the direction of rotation of the hands of a clock.
[0049] One advantage of the 4R format is this it is widely used in the field of electronics. Thus, a gas sensor 1 that respects this format may easily be connected to existing electronic circuits. Respect of this format facilitates maintenance of measuring systems, by facilitating the replacement of sensors.
[0050] However, one difficulty related to this format is its compactness. The useful volume of the enclosure is small, this requiring the optimization approach described below.
[0051] The enclosure 2 is intended to be occupied by a gas G to be analysed. The gas to be analysed comprises a gaseous species G, a concentration G of which in the gas it is desired to determine. The gaseous species G, absorbs light, and notably infrared light, in an absorption spectral band Δλ.sub.x. The sensor 1 also comprises: [0052] a light source 10 configured to emit a light wave 11 in an emission spectral band Δλ. The emission spectral band may extend between the near ultraviolet and the mid infrared, for example between 200 nm and 20 μm, and most often lies in the infrared, the emission spectral band Δλ being, for example, comprised between 1 μm and 20 μm. [0053] a measuring photodetector 20, configured to detect a light wave 14, called the transmitted light wave, in the absorption spectral band Δλ.sub.x. The transmitted light wave is a light wave emitted by the light source 10, and that is propagated through the enclosure, and that is gradually attenuated as it is propagated through the gas. The measuring photodetector 20 may be associated with a bandpass filter, defining a detection spectral band Δλ.sub.d comprised in the absorption spectral band Δλ.sub.x. [0054] a reference photodetector 20.sub.ref, configured to detect a reference light wave. The reference light wave detected by the reference photodetector 20.sub.ref is considered to be not attenuated by the gas G present in the enclosure. In this example, the reference photodetector 20.sub.ref detects the reference light wave in a reference spectral band Δλ.sub.ref, in which the attenuation of the light wave emitted by the source is considered to be negligible. The reference photodetector may be associated with a reference bandpass filter, defining the reference spectral band Δλ.sub.ref. For example, the reference spectral band Δλ.sub.ref is centered on the wavelength 3.91 μm. Use of a reference photodetector is optional but advantageous. Alternatively, the reference photodetector is not placed in the enclosure 2 containing the gas, in which case the reference spectral band may be similar to the measurement spectral band.
[0055] Preferably, the light source 10, the measuring photodetector 20 and the reference photodetector 20.sub.ref are joined to the same planar holder. It may notably be a question of a circuit board forming the first wall 4 of the enclosure 2. Such an arrangement simplifies the manufacture of the sensor.
[0056] The light source may be pulsed, and emit light pulses the duration of which is generally comprised between 50 ms and 1 s. It may notably be a question of an infrared light source of filament type formed on a suspended membrane, the filament being passed through by an electric current. In this way, the suspended membrane is heated to a temperature comprised between 400° C. and 800° C., so as to emit infrared light.
[0057] The measuring photodetector 20 and the reference photodetector 20.sub.ref may be thermopiles or pyrodetectors or photodiodes. Each photodetector is configured to generate a detection signal, the amplitude A of which corresponds to an intensity I of the detected light wave.
[0058] The intensity I of the light wave detected by the measuring photodetector 20 depends on the concentration C.sub.x of the gaseous species of interest G.sub.x according to the Beer-Lambert relationship:
where: [0059] μ(C.sub.x) is an attenuation coefficient dependent on the sought-after concentration C; [0060] I is the thickness of gas passed through by the light wave in the enclosure; and [0061] I.sub.0 corresponds to the intensity of the wave that is or would be detected by the measuring photodetector 20 in the absence of absorbent gas in the enclosure.
[0062] The comparison between I and I.sub.0, taking the form of a ratio I/I.sub.0, corresponds to an attenuation att caused by the gaseous species G.sub.x in question. During each pulse from the light source 10, it is thus possible to determine μ(C.sub.x), this allowing the quantity C to be estimated given that the relationship between C.sub.x and μ(C.sub.x) is known.
[0063] The intensity I.sub.0 may be determined beforehand, for example, during a calibration, or measured in the absence of gas in the enclosure 2. When the sensor comprises a reference photodetector 20.sub.ref, the intensity I.sub.0 may be estimated from the reference intensity I.sub.ref measured by the reference photodetector. To this end, since the emission spectrum of the light source 10 is known, a function ƒ allowing I.sub.0 to be estimated depending on I.sub.ref according to expression (2) is used:
I.sub.0=ƒ(I.sub.ref) (2)
[0064] The sensor comprises a processing unit 30, which receives the signals measured by the measuring photodetector 20 and the optional reference photodetector 20.sub.ref. The processing unit 30 allows, on the basis of the signals, the computations for estimating the concentration of the sought-after gaseous species to be performed. The processing unit 30, for example, comprises a microprocessor.
[0065] The dimensions of the enclosure 2 in which the gas lies are particularly small. However, it is preferable for the light wave detected by the measuring photodetector 20 to be attenuated enough for the attenuation alt to be more easily quantifiable, given the various noises in the measurement chain. It is therefore preferable for the length I travelled by the rays reaching the measuring photodetector to be large enough. The applicant considers that the attenuation att must be higher than 0.2, and, for example, comprised between 0.2 and 0.3.
[0066] In order to optimize the length l of the paths travelled by the rays reaching the measuring photodetector, an enclosure 2 comprises reflective surfaces of ellipsoidal shape. Thus, the reflective surfaces follow a portion of an ellipsoid of revolution. The reflective surfaces allow the wave emitted by the light source to be reflected multiple times before reaching the measuring photodetector. An increase in the length l travelled, in the enclosure 2, by the rays reaching the measuring photodetector 20 results.
[0067]
[0068] The term ellipsoidal surface S.sub.n designates an ellipsoidal surface of revolution, obtained by rotating in space an ellipse E.sub.n about one of its axes. In the described example, each ellipsoidal surface S.sub.n is associated with one ellipse E.sub.n having a major axis an and a minor axis b.sub.n. By ellipsoidal surface associated with an ellipse, what is meant is an ellipsoidal surface formed by rotating the ellipse about one of its axes. In the example shown, each ellipsoidal surface S.sub.n is obtained by rotating an ellipse E.sub.n with which it is associated about its major axis a.sub.n. Such an ellipsoidal surface is said to be prolate.
[0069] By reflective surface, what is meant is a surface the reflection coefficient of which, in all or some of the emission spectral band Δλ, is higher than 50%, and preferably higher than 80%. In the infrared spectral domain, a reflective wall may be formed using a reflective material such as a metal, gold for example.
[0070] Each ellipsoidal reflective surface S.sub.n has a first focal point P1-n and a second focal point P2-n, the two focal points being distinct from each other. When 1<n<N, the first focal point P1-n is coincident with the second focal point P2-(n−1) of a preceding surface S.sub.n−1. The second focal point P2-n is coincident with the first focal point P1-(n−1) of a following surface S.sub.n+1. When n=1 (first reflective surface S.sub.1), the second focal point P2-1 is coincident with the first focal point P1-2 of the second reflective surface S.sub.2. When n IN′ (last surface) the first focal point P1-N is coincident with the second focal point P2-(N−1) of the proceeding surface S.sub.N−1. The first surface S.sub.1 allows the incident light wave 11 emitted by the light source 10 to be reflected, whereas the last surface S.sub.N allows the light wave having passed through the enclosure 2 to be reflected towards the measuring photodetector 20. In the embodiment shown in
[0071] The light wave 11 emitted by the light source is successively reflected by the various surfaces S.sub.n, according to their respective ranks, considered in increasing order. In other words, the reflective surfaces S.sub.1 . . . S.sub.N lie successively between the light source 10 and the measuring photodetector 20. The term lies successively is to be interpreted with respect to the propagation of light between the light source 10 and the measuring photodetector 20. The path of the light wave, projected onto the first wall 4 or the second wall 5, describes a circular arc.
[0072] Given dimensional constraints relating to the compactness of the sensor, it is preferable for the first ellipse E.sub.1, associated with the first surface S.sub.1, to have an eccentricity lower than 0.8, or even than 0.7 or than 0.5. By eccentricity of an ellipse having a major axis g, and a minor axis p, what is meant is the ratio:
[0073] The eccentricity of an ellipse is strictly comprised between 0 and 1, an eccentricity of zero corresponding to a circle.
[0074] The light source 10 is configured to emit the emission light wave 11 in such a way as to form a cone of light Ω.sub.1, called the first cone, that extends about a first axis Δ.sub.1, towards the first reflective surface S.sub.1. The light source 10 is placed at a vertex of the first cone of light Ω.sub.1. The light source 10 is preferably coincident with the first focal point P1-1 of the first reflective surface S.sub.1.
[0075] The term coincident is to be interpreted with a certain tolerance, and may mean “to be located in the vicinity of,” the vicinity corresponding to a region lying a small distance from a point. By small distance, what is meant is a distance smaller than 1 mm, or even smaller than 0.5 mm.
[0076] The first reflective surface S.sub.1 is configured to reflect the first cone of light Ω.sub.1 to form a second cone of light Ω.sub.2, extending about a second axis Δ.sub.2. The second cone of light converges towards the second focal point P2-1 of the first reflective surface S.sub.1, the latter focal point corresponding to the first focal point P1-2 of the second reflective surface S.sub.2. Downstream of the first focal point P1-2, the second cone of light Ω.sub.2 diverges up to the second reflective surface S.sub.2.
[0077] The second reflective surface S.sub.2 is configured to reflect the second cone of light Ω.sub.2 to form a third cone of light Ω.sub.3, extending about a third axis Δ.sub.3. The third cone of light Ω.sub.3 converges towards the second focal point P2-2 of the second reflective surface S.sub.2, the latter focal point corresponding to the first focal point P1-3 of the third reflective surface S.sub.3. Downstream of the first focal point P1-3, the third cone of light Ω.sub.3 diverges up to the third reflective surface S.sub.3.
[0078] The third reflective surface S.sub.3 is configured to reflect the third cone of light Ω.sub.3 to form a fourth cone of light Ω.sub.4, extending about a fourth axis Δ.sub.4. The fourth cone of light Ω.sub.4 converges towards the second focal point P2-3 of the third reflective surface S.sub.3, the latter focal point corresponding to the first focal point P1-4 of the fourth reflective surface S.sub.4. Downstream of the first focal point P1-4, the fourth cone of light Ω.sub.4 diverges up to the fourth reflective surface S.sub.4.
[0079] The fourth reflective surface S.sub.4 is configured to reflect the fourth cone of light Ω.sub.4 to form a fifth cone of light Ω.sub.5, extending about a fifth axis Δ.sub.5. The fifth cone of light Ω.sub.5 converges towards the second focal point P2-4 of the fourth reflective surface S.sub.4, the latter focal point corresponding to the first focal point P1-5 of the fifth reflective surface S.sub.5. Downstream of the first focal point P1-5, the fifth cone of light 95 diverges up to the fifth reflective surface S.sub.5.
[0080] The fifth reflective surface S.sub.5 is configured to reflect the fifth cone of light Ω.sub.5 to form a sixth cone of light Ω.sub.6, extending about a sixth axis Δ.sub.6. The sixth cone of light Ω.sub.6 converges towards the second focal point P2-5 of the fifth reflective surface S.sub.5. The measuring photodetector 20 is placed in the cone of light Ω.sub.6, upstream or downstream of the second focal point P2-5 or at the second focal point P2-5.
[0081] Thus, the light wave 11 emitted by the light source 10 propagates between the various reflective surfaces S.sub.1 . . . S.sub.N with, in this example, N=5. Between two successive surfaces S.sub.n, S.sub.n+1, the light wave forms a cone Ω.sub.n+1 that converges from the surface S.sub.n towards the second focal point P2-n of the surface S, which forms the apex of the cone Ω+0.1, and which is coincident with the first focal point P1-n+1 of the surface S.sub.n+1. Downstream of the latter focal point, the cone Ω.sub.n+1 diverges up to the surface of rank n+1.
[0082] Thus, the light wave propagates directly from an ellipsoidal reflective surface S of rank n to an ellipsoidal reflective surface S.sub.n+1 of rank n+1. By directly, what is meant is without undergoing a reflection from another surface between the two ellipsoidal reflective surfaces. Thus, between the light source 10 and the measuring photodetector 20, the light wave emitted by the light source undergoes N reflections, i.e., as many reflections as there are ellipsoidal surfaces placed between the light source and the measuring photodetector. This allows losses of signal on each reflection to be minimized.
[0083] Advantageously, as shown in
[0084] When the sensor 1 comprises a reference photodetector 20.sub.ref, the latter may be placed on the same wall as the light source 10. In this case, a reference ellipsoidal reflective surface S.sub.ref is placed on the opposite wall, as shown in
[0085]
[0086] In
[0087] In this embodiment, each reflective surface is arranged on an internal face of a first or second wall: the reflective surfaces of even rank are integrated into the internal face 4 of the first wall 4, whereas the reflective surfaces of uneven rank are integrated into the internal face 5.sub.i of the second wall 5. The integration of the reflective surfaces of ellipsoidal-of-revolution shape into each internal face may be obtained using moulding or machining manufacturing techniques. Moulding is a preferred option, because after the moulds have been formed, it is simple to implement, repetitive and less expensive. According to this embodiment, the enclosure 2 may be formed by simply assembling the first wall 4 against the second wall 5, the sidewall 6 being integrated either into the first wall 4, into the second wall 5, or partially into both walls.
[0088]
[0089] Table 1, below, collates the coordinates of the centres of the light source 10, of the photodetector 20 and of the reference photodetector 20.sub.ref. The centre of the source 10 is considered to be the origin of the coordinate system. The angle of orientation with respect to the axis Z has also been indicated. Table I also presents the main characteristic coordinates of the ellipsoids of revolution forming each reflective surface. For each ellipsoid, the coordinates of the centre, corresponding to the intersection of the major axis a and of the minor axis h of the ellipse associated with each ellipsoidal surface, along the axes X, Y and Z, have been given. The angles of inclination θ.sub.x, θ.sub.y and θ.sub.z of the major axis a with respect to the axes X, Y and Z have also been given. The dimensions of the major axis a and of the minor axis b have also been given. Regarding the angles, the unit is degrees. Regarding the coordinates or dimensions, the unit is millimetres.
TABLE-US-00001 TABLE 1 X Y Z θ.sub.X θ.sub.Y θ.sub.Z a b 10 0.0 0.0 0 0 0 0 20.sub.ref 5.6 4.4 −1.3 0 0 76.4 E.sub.ref 2.8 2.2 −0.3 90 38.2 −7.3 8.1 7.3 20 3.7 10.1 −1.3 0 0 140.3 E.sub.1 −2.8 2.1 0.0 90 −37.5 0 6.7 5.7 E.sub.2 −5.6 5.5 0.5 90 92.5 20 1.8 1.2 E.sub.3 −5.0 8.1 0.9 90 65 0 3.7 3.4 E.sub.4 −2.2 10.4 1.7 90 25 10 3.6 2.6 E.sub.5 1.8 10.8 0.6 90 −19.9 −38.4 5.2 4.5
[0090] The inclination of the respective major axes of each ellipse, from which each ellipsoid is formed, is therefore variable, in particular with respect to the transverse axis Z.
[0091] Simulations have been performed in order to estimate the performance of the configuration described above. The detectable variations in the concentration of a gaseous species as a function of the concentration of said gaseous species in the gas occupying the enclosure 2 have been estimated.
[0092] Embodiments of the disclosure will possibly be applied to gas detection for environmental-monitoring purposes, or used in applications involving the inspection of industrial gases, notably in the food-processing industry, in the petroleum industry, or in the distribution of gas.