SENSOR AND METHOD FOR DETERMINING THE AIR RATIO OF A FUEL GAS/AIR MIXTURE

Abstract

A sensor for determining an air ratio of a fuel gas/air mixture, wherein a housing is formed, which delimitates a measuring space. The housing has on one side a diffusion passage for coupling with a fuel gas/air mixture flow, wherein the diffusion passage is formed by a gas-permeable separating agent. An electrically operated excitation element is arranged for energy supply into the measuring space in order to induce a chemical reaction of a fuel gas/air mixture in the measuring space. At least one optical detection device is directed into the measuring space with its detection area, wherein the at least one optical detection device detects the intensity of radiation from the reaction position in at least a first wavelength range and produces a signal being allocated to the detected intensity, from which the air ratio is inferable.

Claims

1. A sensor for detecting an air ratio of a fuel gas/air mixture, the sensor comprising: a housing that delimitates at least part of a measuring space, and a diffusion passage that fluidly couples the measuring space with a fuel gas/air mixture flow, wherein the diffusion passage includes a gas-permeable separating member; an electrically operated excitation element for supplying energy into the measuring space in order to induce a chemical reaction of a fuel gas/air mixture in the measuring space, wherein the excitation element is configured to supply energy to a reaction position located in the measuring space, wherein the reaction position is spaced from the housing and the gas-permeable separating member; and at least one optical detection device whose detection area is directed into the measuring space, wherein the at least one optical detection device is configured to detect an intensity of radiation from the reaction position in at least a first wavelength range and produces a signal that is indicative of the detected intensity, from which the air ratio is inferable.

2. The sensor according to claim 1, further comprising a measuring device to quantitatively record an energy level supplied to the excitation element.

3. The sensor according to claim 1, wherein the excitation element comprises an electrical heating device with a current-carrying ohmic heating element, wherein the heating element is arranged within the measuring space at the reaction position and wherein the heating element is supplied by a controllable power or voltage source.

4. The sensor according to claim 1, wherein the excitation element is formed with a plurality of constructively and galvanically separated electrodes, which extend at least in part into the measuring space, wherein the excitation element further comprises a power supply coupled with the electrodes, wherein the reaction position is located between the electrodes.

5. The sensor according to claim 1, wherein the excitation element comprises a laser light source, which radiates light into the measuring space at the reaction position.

6. The sensor according to claim 1, wherein the at least one optical detection device comprises an optically sensitive detector.

7. The sensor according to claim 6, wherein the optically sensitive detector comprises an optical filter for selecting the first wavelength range.

8. The sensor according to claim 1, further comprises optical element arranged between the reaction position and the at least one optical detection device.

9. The sensor according to claim 8, wherein the optical element comprises one or more of a shutter, a light conductor, and a lens.

10. The sensor according to claim 1, further comprising a controller operatively coupled to the excitation element in order to regulate the supply energy to the reaction position, wherein the supply energy is regulated based at least in part on the signal of the at least one optical detection device.

11. The sensor according to claim 1, further comprising an evaluation device operatively coupled to at least one of the at least one optical detection device, the evaluation device is configured to optically monitor the energy supplied by the excitation element to the reaction position.

12. A method for determining an air ratio of a fuel gas/air mixture, the method comprising: fluidly coupling via a gas-permeable separating member a measuring space with a gas flow to be monitored, the gas flow having a fuel gas/air mixture; exciting gases located in the measuring space with an electrically operated excitation element in order to induce a chemical reaction of a fuel gas/air mixture in the measuring space; monitoring the measuring space with an optical detection device in a predetermined spectral region, and detecting an intensity of an optical emission from the chemical reaction of the fuel gas/air mixture in the measuring space; and calculating the air ratio of the fuel gas/air mixture based at least in part on the intensity of the optical emission.

13. The method according to claim 12, wherein the exciting step includes applying power to an ohmic heating element that is positioned in the measuring space.

14. The method according to claim 13, wherein the power is applied to the ohmic heating element such that optical emission from the chemical reaction of the fuel gas/air mixture in the measuring space remains substantially at a predetermined value.

15. The method according to one of claim 12, wherein the air ratio is changed and an applied power to the electrically operated excitation element is reduced until the chemical reaction in the measuring space is only just measurable with a single fuel gas/air mixture, in order to adjust an air ratio of the fuel gas/air mixture to a λ=1.0.

16. The method according to claim 12, wherein the predetermined spectral region comprises a wavelength of 1000 nm.

17. The method according to claim 12, wherein the predetermined spectral region comprises a wavelength range from 900 nm to 1100 nm.

18. A sensor for detecting an air ratio of a fuel gas/air mixture, the sensor comprising: a body with a diffusion passage leading to a measuring space, the diffusion passage fluidly couplable to a fuel gas/air mixture flow; an excitation element for supplying energy into the measuring space in order to induce a chemical reaction of a fuel gas/air mixture in the measuring space; and an optical detection device configured to detect an intensity of an optical emission from the chemical reaction of the fuel gas/air mixture in the measuring space.

19. The sensor of claim 18, wherein the air ratio of the fuel gas/air mixture is based at least in part on the optical emission from the chemical reaction of the fuel gas/air mixture in the measuring space.

20. The sensor of claim 18, further comprising controller for controlling a power level delivered to the excitation element, and wherein the air ratio of the fuel gas/air mixture is based at least in part on the power level that is delivered to the excitation element.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0043] FIG. 1 shows the schematic structure of an embodiment of the invention;

[0044] FIG. 2 shows an example of a radiation intensity flow depending on the air ratio.

DESCRIPTION

[0045] In FIG. 1, a supply line 1 for a fuel gas/air mixture is shown. Along this supply line, the fuel gas/air mixture is supplied in the direction of the arrow 2 to a consumer, for example a heating distiller. In an opening of the line 1, a sensor housing 3 is coupled gas-tightly with the line 1. The sensor housing 3 comprises a cavity 4, which is constructively separated from the gas flow 2 by a sintered pane 5. The sintered pane 5 provides as a separating agent for flame protection and suppression of possible turbulence. The sintered pane 5 is permeable for the gas, such that proportions of the fuel gas/air mixture can diffuse into the measuring space 4 according to arrow 6 at any time from the gas flow 2. In the same way, the substances can enter the gas flow 2 from the space 4 along the direction of the arrow 7.

[0046] In the measuring space 4, a heating wire 8 is arranged in the form of a heating coil. The line routings 9a, 9b to the heating wire 8 are gas-tightly fed through the housing 3 and coupled with a controllable voltage source 10. The heating wire 8 is heated subject to the set voltage at the voltage source 10.

[0047] In this embodiment, two photodiodes 11, 13 are arranged outside the measuring space. The measuring space comprises on its side facing the photodiodes 11, 13 a window 16, through which radiation from the measuring space 4 reaches the photodiodes 11, 13. Between the window 16 and the heating wire 8, a shutter 17 is arranged, which restricts the visual range of the photodiodes 11, 13 to a section of the heating wire 17.

[0048] The photodiode 11 is adjusted with its spectral sensitivity to the wavelength range of the visible light. It thereby measures the light emission of the aforementioned spectrum of the heating coil 8. The photodiode 11 is coupled with an evaluation switch 12, which processes the signals of the photodiode. By means of the measurement of the emitted radiation, a measurement for the temperature of the heating coil 8 is determined and the evaluation switch 12 can control the voltage source 10 in order to approximate the measured dimension for the actual temperature, calculated from the signals of the photodiode 11, to the fixed setpoint.

[0049] A further evaluation switch 14 is coupled with the photodiode 13. The photodiode 13 is selected in this embodiment to detect electromagnetic radiation of reaction products in the area of the heating coil 8. In this embodiment, there is a photodiode, whose sensitivity range is particularly pronounced in the wavelength range of 800 nm to 1100 nm.

[0050] The evaluation switch 12 and the evaluation switch 14 are coupled via the connection 18. Data can be exchanged between the evaluation switches via this connection (in practice, the evaluation switches 12 and 14 can also be merged into one switch).

[0051] The signal of this photodiode 13 is converted by the evaluation switch 14 to emit a measuring signal 15. This measuring signal 15 is used in this embodiment to calculate the current air ratio on the basis of the calibration data.

[0052] With the depicted embodiment of the invention, a rapid and reliable determination of the air ratio of the on-flowing fuel gas/air mixture 2 is possible. If a fuel gas/air mixture passes the measuring space 4 along the arrow direction 2, a part of this fuel gas/air mixture diffuses into the measuring space 4 at all times by the diffusion processes. A small proportion of the molecules of the fuel gas/air mixture comes into contact with the heating wire 8 there. A significant aspect of the invention consists of the exothermic chemical reaction of a small proportion of the fuel gas/air mixture taking place in the measuring space 4 under controlled and safe conditions. As the heating wire 8 is located within the quenching distance of the surrounding walls and the sintered pane 5 also forms a flame protection, this controlled exothermic chemical reaction is safe at all times. The exothermic chemical reaction in the direct proximity of the heating wire 8 is only maintained as energy is continually supplied via the voltage source 10. A self-sustaining combustion in the measuring space 4 is not possible due to the arrangement of the heating wire in the quenching distance. That a stimulated exothermic chemical reaction still occurs in direct proximity to the heating wire 8 is due to the continually supplied energy. In this way, the optical measurement of the chemical reaction and specifically the detection of the intensity of the emitted radiation is possible. The optical detection by the photodiode 13 is thereby adapted by an optical filter such to the chemical reaction that the characteristic excitation levels of the reaction products are measured during the chemical reaction processes. In this embodiment, an emission of a vibration-rotation excitation of water is measured in the range of 1000 nm as a characteristic wave length. The spectral sensitivity of the photodiode 13 is selected accordingly.

[0053] The sensor as per the invention and the method as per the invention aim therefore to achieve an exothermic chemical sample reaction of the on-flowing fuel gas/air mixture, wherein this exothermic chemical sample reaction cannot lead to ignition of the fuel gas/air mixture of the supply gas flow 2.

[0054] The observations during measurements with the structure of the stated embodiment show with a fuel gas consisting primarily of methane that heat is initially dissipated through the gas mixture to the walls 3 when starting the device and during an initial heating of the heating coil 8. With an increase of heating temperature of the heating wire 8, monitored by the photodiode 11, exothermic chemical reaction processes occur on the surface of the heating wire 8. This is measured at least by the photodiode 13. A thin reaction layer thereby initially forms over the heating wire 8, whose light intensity further increases in the monitored wavelength range of 1000 nm with temperature increase. The thickness of the reaction layer and the density of the occurring reaction processes in the reaction position around the heating wire 8 increase thereby with a rising temperature.

[0055] If the mass transfer of fuel gas and oxygen molecules via the diffusion passage is lower than the rate of the molecules reacting at the heating wire, a substantial reaction failure and a subsequent upsurge of the radiation intensity (dependent on the air ratio) ultimately occurs with a further increase of the temperature. A type of pulsating of the light intensity therefore occurs. If however sufficient fuel gas and oxygen molecules are supplied via the diffusion passage for the exothermic chemical reaction processes, such quantities of reaction products are released with an increasing temperature that these surround the heating wire and limit the arriving current of fuel gas and oxygen molecules. A saturation of the exothermic chemical reactions occurs. This then leads to the radiation intensity of the chemical reaction being saturated.

[0056] Accordingly, the temperature of the heating wire 8 is selected such that a continual, non-oscillating and non-saturated chemical reaction is observed on the surface of the heating wire 8. An oscillating or saturated operation can thereby initially be initiated, for example, and the temperature can then be reduced. The evaluation of the emission in non-oscillating operation is in this example the preferred variation, however the oscillating operation can also be used for an evaluation.

[0057] In FIG. 2, a measuring procedure of the sensor device as per the invention is shown as per the embodiment. The data is produced from averaged measurement data and extends over a measuring range of the air ratio of λ=0.70 to λ=1.70. The air ratio was thereby calculated in the gas flow by a conventional gas analysis device. The scaling of the intensity axis (Y-axis) has been selected for a qualitative representation of the measurement values.

[0058] The above described curve progression therefore occurs with a virtually linear procedure for thin mixtures and a steep drop to increasingly fatty mixtures.

[0059] The linear increase of the intensity with an air ratio change of 1.70 to 1.10 can be explained thus that there is always less excess air and this is why the temperature of the reaction layer increases around the heating wire. This ensures that more radicals are formed and the reaction layer around the heating wire expands and/or the density of the water-forming, exothermic chemical reaction processes increases, which leads to a higher light emission in the wavelength range around 1000 nm.

[0060] The maximum of the curve is near the stoichiometric mixture when using methane as the fuel gas, but not exactly λ=1, rather about λ=1.07. The curve moves towards the right with a propane-air mixture. The maximum is then at around λ=0.9 (depending on the heating wire temperature).

[0061] To carry out a calibration at λ=1.0, the sensor as per the invention offers a further use.

[0062] With a specific reduction of the temperature of the heating wire, the effective area of the sensor is in fact restricted. Especially in the range of λ<=1, the detectable reaction processes break down. This allows a fuel gas/air mixture to be provided through the interaction with the burner controller and a variation of the fuel gas/air ratios, which just enables reaction processes.

[0063] Thus, both the mixture ratio is repetitively varied and the temperature of the heating wire is repetitively reduced until a point is determined, which still permits a reaction with radiation emission, from which however a collapse of the reaction (disappearance of the radiation) occurs in each of the direction of both a thinner and fatter mixture.

[0064] The thus determined fuel gas/air mixture has an air ratio of about λ=1.0, independent of the type of fuel gas.

[0065] After this point has been determined, the heating wire is increased back to a normal operating temperature while maintaining the thus adjusted fuel gas/air ratio. The size of the signal then corresponds to the value for an air ratio of λ=1.0.

[0066] There are thus two points, which can be determined characteristically for the burner operation on the basis of the measurements. The point of the aforementioned maximum of radiation intensity represents a fixed point depending on the type of gas. In addition, the sensor can be calibrated to the point λ=1.0.

[0067] The method as per the invention and also the sensor as per the invention could be adapted in many ways. For example, the sensor can be constructed in multiple pieces and it is basically also possible to provide a gas discharge on the sensor, instead of conducting the gas into the gas flow. The essential thing is that a part of the gas flow is diverted and that the emitted emission of a controlled exothermic chemical reaction is optically measured in order to determine the air ratio. Thereupon, an optimization of the fuel gas/air mixture can be carried out. An alternative with an optical measurement of a chemical sample reaction is thereby added to the known methods from prior art, during which electrochemical effects are used substantially to determine the air ratio. Thereby the chemical sample reaction takes place at all times in a controlled manner and in such a dimensioned structure that no self-preserving or uncontrolled exothermic chemical reaction of the fuel gas/air mixture is possible in the measuring space.