DE202014011447U1 - Optical gas sensor - Google Patents

Abstract

Optical gas sensor (1) for quantitative measurement of a concentration of one or more gases, having a radiation source (2) for emitting light waves (L), a cuvette (3) for receiving a gas to be measured (G) and a detector (4) for Measuring light intensities, characterized in that the radiation source (2) has at least one first emitter (5a) designed as an LED and a second emitter (5b) designed as an LED for emitting light waves (L), the first emitter (5a) being designed is to emit light waves (L) of a first wavelength as a main signal and the second emitter (5b) is designed to emit light waves (L) of a second wavelength different from the first wavelength as a reference signal for checking a measurement result of the main signal, the Light waves (L) of the first and second wavelengths can be emitted separately from one another, the emitters (5a, 5b) each being formed as a spec emit the full width at half maximum of a focal point wavelength, preferably a maximum of 20% of the focal point wavelength, wherein the detector (4) is designed to quantitatively detect an intensity of the emitted light waves (L) of the first wavelength and the second wavelength , and wherein the cuvette (3) has a mirror arrangement with a plane mirror (6) and a concave mirror (7) arranged opposite the plane mirror (6), an optical axis (8) of the concave mirror (7) being arranged perpendicular to the plane mirror (6) and the radiation source (2) and the detector (4) are arranged on the plane mirror (6).

Description

The invention relates to an optical gas sensor for the quantitative measurement of a concentration of one or more gases.

Optical gas sensors enable both a qualitative determination of the presence of one or more gases and a quantitative determination of a concentration of one or more gases. Such gas sensors are e.g. Used in gas detection devices in systems for conveying and processing flammable and / or toxic gases in order to detect gases escaping unintentionally.

STATE OF THE ART

Optical gas sensors are known which have an emitter, a cuvette and a detector. In optical gas sensors, the emitter is a light source, e.g. an incandescent lamp that emits a broad spectrum of light waves, i.e. light waves with a large number of different wavelengths. The cuvette is preferably an essentially closed space in which the gas to be measured is located. The cuvette can have openings to the outside which enable gas exchange between the cuvette and the surroundings of the gas sensor. The detector is a light sensor with which an intensity of light that strikes the detector can preferably be measured. Bandpass filters are connected upstream of the corresponding detectors in order to detect specific wavelengths of light. Such bandpass filters can be designed to pass one or more wavelengths.

During operation, the gas or gas mixture to be measured is introduced into the cuvette. The cuvette can have one or more openings for this purpose. Light waves emitted by the light source are more or less strongly absorbed by the respective gas, depending on the concentration of the constituents of the gas mixture and the absorption wavelengths, and then hit the light sensor, which measures the intensity of these light waves. In this way it can be determined which wavelengths were absorbed by the gas and how much. Because of the known specific absorption properties of different gases, a composition of the gas mixture can be determined from this result.

From the DE 202 02 694 A1 an optical gas sensor with a hollow cylinder-shaped cuvette for receiving the gas to be measured is known. In the longitudinal axial direction of the cuvette, a plane mirror is arranged on one side and a concave mirror on the other side. The concave mirror has several recesses for receiving an incandescent lamp and a light wave detector. Light waves emitted by the incandescent lamp are first reflected several times between the plane mirror and the concave mirror until they hit the light wave detector. This extends an optical path along which these light waves can be absorbed by the gas or gas mixture to be measured. Thus, weakly absorbing gases are easier to measure.

Such a gas sensor has the particular disadvantage that an arrangement of incandescent lamp and light wave detectors on the concave mirror can only be produced with great effort because of the curved surface of the concave mirror.

Furthermore, a large number of the light sources used in optical gas sensors have the disadvantage that they emit a relatively broad spectrum of light waves. This means that not only light waves with wavelengths are emitted that are required for measuring the gas concentration, but also light waves with wavelengths that are not important for measuring the gas concentration and must be filtered out by a bandpass filter to avoid measurement errors. This adversely affects the efficiency of the optical gas sensor.

Incandescent lamps in particular also have the disadvantage that a large proportion of electrical energy is converted into heat, which has to be dissipated as heat loss. This leads to an excessive energy consumption of the gas sensor and is particularly disadvantageous for mobile applications that have an internal power source, e.g. a battery to be powered. The increased power consumption significantly reduces the service life of the battery and thus the service life of the mobile gas sensor.

The publication " Optimizing indium aluminum antimonide LEDs and photodiodes for gas sensing applications, Harvey R. et al., Proceedings of SPIE Vol. 5564, Infrared Detector Materials and Devices, 2004 “Describes possibilities for the design of LEDs and photodiodes for applications in infrared gas measurement technology based on indium aluminum antimony compounds in semiconductor technology. The target gases of such IR LEDs or photodiodes in gas measurement technology are, for example, methane and carbon dioxide.

The W012001633 A2 describes a measuring device with a laser optically metrological detection of a concentration of a gas in a container through a wall of the container. The container is equipped with a partially transparent wall so that the laser beam can penetrate the wall.

The GB2391310 A1 describes an infrared optical measuring device with means for reflection and focusing in order to analyze a gas sample in a gas cell by means of multiple light passes.

The DE1 0047728 B4 shows an infrared optical gas analyzer with a first infrared optical radiation source, with a first multispectral detector, with a second multispectral detector and with a cuvette and a pneumatic diaphragm in the gas duct of the cuvette.

The US799232 A shows a gas detector with a laser arrangement for a metrological detection of concentrations of different gases such as oxygen, carbon monoxide, methane, hydrogen sulfide in a gas sample with the aid of four wavelengths which are provided by the laser arrangement.

The US6791689 BA shows a measuring system for an optical analysis of nitrogen dioxide in a wavelength range of approximately 600 nm.

DISCLOSURE OF THE INVENTION

Proceeding from this prior art, the invention was based on the object of providing an optical gas sensor which at least partially does not have these disadvantages. It is therefore the object of the present invention to provide an optical gas sensor with which in particular concentrations of weakly light wave absorbing gases can be quantitatively measured and which has an improved efficiency.

The above object is achieved by an optical gas sensor for quantitative measurement of a concentration of one or more gases with the features of claim 1.

Further features and details of the invention emerge from the further claims, the description and the drawings.

Accordingly, the object is achieved by an optical gas sensor for quantitative measurement of a concentration of one or more gases, having a radiation source for emitting light waves, a cuvette for receiving a gas to be measured and a detector for measuring light intensities. The radiation source has at least one emitter of light waves, e.g. an LED, and is designed to emit light waves of at least a first wavelength and a second wavelength different from the first wavelength simultaneously and separately from one another. The emitter is designed to emit a spectrum whose full half-width is a maximum of 50% of the focal point wavelength, preferably a discrete spectrum whose full half-width is a maximum of 20% of the focal point wavelength. The detector is designed to quantitatively detect an intensity of the emitted light waves of the first wavelength and the second wavelength. The emitter is preferably designed to convert at least 80% of the electrical energy consumed by the emitter into light waves.

The invention is based on the idea that the use of such an emitter can significantly improve the efficiency of the optical gas sensor. As a result, less heat is produced when generating light waves and thus less electrical energy is used. When an LED converts electrical energy into light waves, less heat is generated than e.g. by an incandescent lamp as used in many conventional gas sensors. The gas sensor therefore has a lower power consumption during operation. This is particularly advantageous for mobile applications, since it enables a charging cycle of a rechargeable battery or a service life of a battery in the mobile application to be significantly extended.

By emitting light waves of different wavelengths separately, e.g. a main signal and a reference signal can be generated, the reference signal being used to check the measurement result of the main signal. The more light waves of different wavelengths that can preferably be generated separately, the more gases can be quantitatively determined with the gas sensor according to the invention. This means that the emitter only emits a relatively narrow-band light spectrum. Because of the absorption properties of gases, the light waves are preferably in the infrared range.

The emitter is designed to emit a spectrum of light waves whose full half-width is a maximum of 50% of a focal point wavelength, preferably a maximum of 20% of the focal point wavelength.

Emitters designed as LEDs have the advantage that they can be used to emit relatively short light pulses without the LEDs afterglowing like an incandescent lamp after the light pulse. The individual LEDs can thus emit light pulses essentially immediately one after the other, so that e.g. The measuring signal and the reference signal extend through a substantially constant gas mixture arranged in the cuvette. This avoids or reduces measurement errors. LEDs also have the advantage that they are suitable for emitting a relatively narrow-band light spectrum and have a particularly good degree of efficiency when converting electrical energy into light waves.

The properties of LEDs, in particular with regard to the narrow band of the emitted spectrum, that is to say half-width and focal point wavelength, are for example in the DE 40 11 462 C2 presented in the technical context.

An example for the quantitative determination of methane is given here. The measurement wavelength is selected to be approx. 3.2 µm, suitable reference wavelengths are 3.1 µm and / or 3.9 µm.

The detector is e.g. a photodiode that generates a current when light waves strike, the current strength of which depends on the intensity of the light waves. Thus, the degree of absorption of the light waves of a certain wavelength by the gas, as well as the type of gas and the composition of the gas mixture can be determined. At least one detector is preferably designed to detect a plurality of different, preferably disjoint wavelength ranges. Thus, with one cuvette and one detector, at least two different gases can be detected in a simple and inexpensive way.

A corresponding bandpass filter can e.g. be arranged in front of the detector to avoid interference. Depending on the design of the gas sensor, the bandpass filter can be designed as a function of the radiation source. In the case of a radiation source with which e.g. Light waves can be emitted in four different wavelengths, accordingly a bandpass filter is preferably arranged in front of the detector, which is permeable to these four wavelengths. Bandpass filters have the further advantage that light waves that are not allowed through by the bandpass filter can be reflected by it. It can thus be advantageous to arrange a bandpass filter on an emitter or radiation source, so that with several radiation sources with bandpass filters arranged in front of them, less reflective surface of a mirror is lost than without a bandpass filter.

The cuvette is preferably designed in such a way that no interfering influences, such as e.g. Light waves from the vicinity of the gas sensor can penetrate the cuvette or strike the detector. This ensures the required accuracy of the measurement results of the gas sensor. Furthermore, the exchange of air between the cuvette and the surroundings of the gas sensor is preferably controllable or relatively small, so that the gas mixture within the cuvette remains essentially constant during a measurement cycle that includes at least one-time emission of a measurement signal and a reference signal. This also avoids or reduces measurement errors.

Furthermore, it can be provided that the radiation source has at least a first emitter and a second emitter, the first emitter being designed to emit light waves of the first wavelength and the second emitter being designed to emit light waves of the second wavelength. The detector and / or at least one emitter have at least one optical filter, e.g. a band pass filter. The emitters are preferably designed as LEDs. Such a radiation source is easy to manufacture and requires a relatively small installation space.

It can particularly preferably be provided that the radiation source is designed to emit a discrete light wave spectrum. The radiation source is thus designed to generate only light waves of a specific wavelength or a relatively narrow wavelength range. It can also be provided that a bandpass filter is arranged in front of the radiation source, which bandpass filter further reduces the wavelength range generated by the radiation source. Particularly preferably, the radiation source can generate a plurality of light waves with wavelengths which are spaced apart from one another within the IR spectrum.

It can preferably be provided that the cuvette has a mirror arrangement with a plane mirror and a concave mirror arranged opposite the plane mirror, an optical axis of the concave mirror being arranged essentially perpendicular to the plane mirror. A distance between the concave mirror and the plane mirror preferably corresponds to an integral fraction of the radius of curvature of the concave mirror. A light beam passes the cuvette between the mirrors several times, e.g. four or six times before it hits the light sensor. This arrangement has the advantage that even weakly absorbing measurement gases can be measured with a relatively compact size of the gas sensor. Preferably, a radius of curvature of the concave mirror can be changed or the concave mirror can be exchanged for concave mirrors with different radii of curvature. This allows the beam path of the light waves within the gas sensor to be designed variably so that the light waves are reflected differently between the concave mirror and the plane mirror, depending on the setting of the radius of curvature of the concave mirror, until they hit the detector. This has the advantage that the gas sensor can be used for measurement gases with weak as well as strong light wave absorption.

Alternatively, the mirror arrangement can have two plane mirrors arranged essentially facing each other, with a corresponding reflection of the light beam, for example, by adjusting the radiation source or at least one mirror is achievable. This variant is particularly simple and can be produced inexpensively.

It is preferred that the angles of incidence to the surface normal of the mirror are as small as possible, i.e. that the light waves hit the mirrors almost perpendicularly. This reduces the influence of disruptive factors such as Reduces moisture on the mirror surfaces, which causes the light waves to be absorbed.

Furthermore, it can preferably be provided that the radiation source and / or the detector are arranged on the plane mirror. Thus, in such an arrangement the radiation source and detector can easily be isolated from the interior of the cuvette, e.g. through a translucent pane or a bandpass filter so that they have no direct contact with the measuring gas. This is particularly advantageous when fluids arranged in the cuvette can potentially damage the radiation source or the detector. Furthermore, an arrangement of radiation source and detector on one level has the advantage that they can be arranged on a common circuit board. Such an arrangement can thus be produced in a particularly simple and inexpensive manner. More preferably, a distance between the radiation source and an intersection of the optical axis with the plane mirror corresponds to a distance between a detector and this intersection. Such a plane mirror is particularly easy to assemble because of its symmetry.

In a particularly preferred embodiment of the gas sensor according to the invention it can be provided that a radiation source and a detector are arranged on the cuvette in such a way that light waves emitted by the radiation source strike the detector directly. In an arrangement that is advantageous for this, the radiation source and detector are not arranged on the same mirror, so that the light waves hit the detector without being reflected. This has the advantage that particularly strongly absorbing gases can be determined. Such a gas sensor preferably has at least two spaced apart radiation sources, at least one radiation source being arranged on the cuvette in such a way that light waves emitted by the radiation source hit the detector only via the mirror arrangement.

The gas sensor is preferably designed such that the radiation source is arranged on the cuvette at a distance from the detector. The emitter is designed to emit light waves with a guided beam path. In the context of the invention, plane mirrors and concave mirrors are regarded as components of the cuvette. Such an arrangement is particularly advantageously suitable for gas sensors which are intended for measuring gases which only weakly absorb light waves. The light waves are emitted as a guided beam path which essentially has no diffuse radiation. This has the advantage that the emitted light is used particularly efficiently for the detection of gases. In addition, this is particularly advantageous for gas sensors which are suitable for the detection of gases which have weak light absorption, since this enables a particularly compact design of the gas sensor.

It is advantageous if exactly one detector is arranged on the cuvette. The detector is designed to detect quantitatively essentially only light waves emitted by the radiation source. For this purpose the detector can e.g. have a corresponding bandpass filter. Such a sensor is particularly suitable for applications that require great precision. Alternatively, the detector can be designed to quantitatively detect a broad spectrum of light waves of different wavelengths, light waves emitted by the radiation source being part of this spectrum. Such a sensor can be manufactured particularly inexpensively. The use of only one detector has the advantage that costs for additional detectors can be saved. Furthermore, with only one detector and the same size, the cuvette has a larger reflecting surface of the mirror, since only one point of a mirror has a detector. In this way, in particular, the accuracy in the measurement of gases which only weakly absorb light waves can be improved.

In a further embodiment of the invention, at least two radiation sources are arranged at a distance from one another on the cuvette. This has e.g. the advantage that the individual radiation sources can have a less complex structure. Furthermore, defective radiation sources can be exchanged separately from one another. This can reduce repair and replacement costs. In a preferred development of the invention, four radiation sources are arranged on the cuvette.

It is particularly preferred that the cuvette has two detectors, the detectors for measuring light intensities from different radiation sources or different emitters, e.g. different LEDs, the two radiation sources are formed. The detectors are preferably arranged in such a way that only light waves from one radiation source can be detected by each detector. Alternatively or additionally, the radiation sources can be switched or modulated differently. This arrangement has the advantage that several measurement gases arranged in the cuvette can be quantitatively determined at the same time.

The gas sensor particularly preferably has at least one double band pass filter, which is preferably arranged on a radiation source. More preferably, the gas sensor has at least one triple band-pass filter, which is preferably arranged on a radiation source. As a result, a spectrum of light waves emitted by the respective radiation source can be divided into wavelengths or wavelength spectra that are clearly separated from one another.

Figure list

• 1 eine Seitenansicht einer ersten Ausführungsform eines erfindungsgemäßen Gassensors;
• 2 eine Draufsicht auf einen Planspiegel des erfindungsgemäßen Gassensors aus 1;
• 3 eine Draufsicht auf einen Planspiegel einer zweiten Ausführungsform eines erfindungsgemäßen Gassensors; und
• 4 eine Draufsicht auf einen Planspiegel einer dritten Ausführungsform eines erfindungsgemäßen Gassensors.

Further measures improving the invention emerge from the following description of some exemplary embodiments of the invention, which are shown in the figures. All of the features and / or advantages arising from the claims, the description or the drawing, including structural details and spatial arrangements, can be essential to the invention both individually and in the various combinations. They each show schematically:

• 1 a side view of a first embodiment of a gas sensor according to the invention;
• 2 a plan view of a plane mirror of the gas sensor according to the invention 1 ;
• 3 a plan view of a plane mirror of a second embodiment of a gas sensor according to the invention; and
• 4th a plan view of a plane mirror of a third embodiment of a gas sensor according to the invention.

In the 1 depicted first embodiment of the optical gas sensor according to the invention 1 has a substantially cylindrical cuvette 3 in which a gas to be measured G or gas mixture is arranged. The cuvette 3 has at least one opening, which cannot be seen in this view, for exchanging the cuvette 3 arranged gas G with gas G from the vicinity of the gas sensor 1 . On one face of the cuvette 3 is a plane mirror 6th and a concave mirror on another face 7th arranged. The plane mirror has a radiation source 2 on leading to the emission of light waves L. two different wavelengths within the IR spectrum and in the direction of the concave mirror 7th is aligned. The radiation source 2 has an emitter designed as an LED 5 on and is designed such that the light waves L. different wavelengths can be emitted separately from one another. Before the emitter 5 an optical filter such as a bandpass filter, double bandpass filter or triple bandpass filter is optionally arranged. From the light source 2 a detector is spaced apart 4th on the plane mirror 6th arranged and in the direction of the concave mirror 7th aligned. The detector 4th is designed to measure the intensity of light waves.

The concave mirror 7th has an optical axis 8th which is essentially perpendicular to the plane mirror 6th is arranged. The distance from the concave mirror 7th to the emitter 5 in this first embodiment is approximately half the radius of curvature of the concave mirror 7th . When using one in front of the emitter 5 arranged optical filter, the distance is slightly greater than half the radius of curvature of the concave mirror 7th . In this illustration there are two different radiation sources 2 emitted light rays L. imaged, with a first beam of light L. by a solid line and a second ray of light L. are indicated schematically by a dashed line. The emitted light rays L. are each from the concave mirror 7th on the plane mirror 6th and back on the concave mirror 7th reflects until it hits the detector 4th to meet. This arrangement is particularly advantageous when the gas to be measured G Light waves L. only weakly absorbed and if the gas sensor 1 must be as compact as possible.

2 shows the plane mirror 6th the first embodiment of the gas sensor 1 in a top view. The plane mirror 6th has a first hole 9 , in which a radiation source 2 with a first emitter 5a and a second emitter 5b is arranged, and a second hole 10 in which the detector 4th is arranged on. This first embodiment of the gas sensor according to the invention 1 is especially used for quantitative measurement of the gas concentration or for the detection of a single gas G suitable. For this are from the first emitter 5a and the second emitter 5b alternating light waves L. emittable with different wavelengths and / or modulated with different frequencies. The detector 4th determines the intensity of these partially absorbed light waves L. . Here are those from the second emitter 5b emitted light waves can be used as a reference signal. The first emitter 5a and the second emitter 5b are designed as LEDs in this embodiment.

In 3 is a plane mirror 6th a second embodiment of the gas sensor according to the invention 1 shown in a top view. The plane mirror 6th has a first hole 9 , in which a radiation source 2 with a first emitter 5a , a second emitter 5b and a third emitter 5c is arranged, and a second hole 10 in which the detector 4th is arranged on. Before the first emitter 5a and / or the second emitter 5b and / or the third emitter 5c an optical filter such as a bandpass filter, double bandpass filter or triple bandpass filter is optionally arranged. The first emitter 5a , the second emitter 5b and the third emitter 5c are in this embodiment designed as an LED. The second embodiment of the gas sensor 1 differs from the first embodiment in that the radiation source 2 additionally a third emitter 5c having. This second embodiment of the gas sensor according to the invention 1 is especially for quantitative measurement or for the detection of two different gases G suitable. For this are from the first emitter 5a , the second emitter 5b and the third emitter 5c Light waves L. emittable at different wavelengths. The detector 4th determines the intensity of these partially absorbed light waves L. . For example, those from the third emitter are used 5c emitted light waves as a reference signal.

In 4th is a plane mirror 6th a third embodiment of the gas sensor according to the invention 1 shown in a top view. The plane mirror 6th has two first holes 9 and two second holes 10 on. In a first hole 9 is a first radiation source 2a with a first emitter 5a and a second emitter 5b arranged. In the other first hole 9 is a second radiation source 2 B with a third emitter 5c and a fourth emitter 5d arranged. In a second hole 10 is a first detector 4a and in the other second hole 10 a second detector 4b arranged. The third embodiment of the gas sensor 1 differs from the first embodiment in that the gas sensor 1 two radiation sources 2 as well as two detectors 4th having. From the first radiation source 2a emitted light waves are preferably exclusively or essentially from the first detector 4a and from the second radiation source 2 B emitted light waves L. exclusively or essentially from the second detector 4b detectable. In operation, the first radiation source 2a and the second radiation source 2 B simultaneous light waves L. emit. The first emitter 5a , the second emitter 5b , the third emitter 5c and the fourth emitter 5d are designed as LEDs in this embodiment. This third embodiment of the gas sensor according to the invention 1 is especially for the simultaneous quantitative measurement or for the detection of two different gases G suitable in a gas mixture. Band pass filters in front of the radiation sources 2 or detectors 4th are arranged, act for light waves of the other radiation sources 2 as a mirror. This increases the efficiency of the gas sensor 1 .

List of reference symbols

1

Gas sensor

2

Radiation source

2a

first radiation source

2 B

second radiation source

3

Cuvette

4th

detector

4a

first detector

4b

second detector

5

Emitter

5a

first emitter

5b

second emitter

5c

third emitter

5d

fourth emitter

6th

Plane mirror

7th

Concave mirror

8th

optical axis

9

first hole

10

second hole

G

gas

L.

Light wave

QUOTES INCLUDED IN THE DESCRIPTION

This list of the documents listed by the applicant was generated automatically and is included solely for the better information of the reader. The list is not part of the German patent or utility model application. The DPMA assumes no liability for any errors or omissions.

Patent literature cited

• DE 20202694 A1 [0005]
• WO 12001633 A2 [0010]
• GB 2391310 A1 [0011]
• DE 10047728 B4 [0012]
• US 799232 A [0013]
• US 6791689 [0014]
• DE 4011462 C2 [0023]

Non-patent literature cited

• Optimizing indium aluminum antimonide LEDs and photodiodes for gas sensing applications, Harvey R. et al., Proceedings of SPIE Vol. 5564, Infrared Detector Materials and Devices, 2004 [0009]

Claims (7)

Optical gas sensor (1) for quantitative measurement of a concentration of one or more gases, having a radiation source (2) for emitting light waves (L), a cuvette (3) for receiving a gas to be measured (G) and a detector (4) for Measuring light intensities, characterized in that the radiation source (2) has at least one first emitter (5a) designed as an LED and a second emitter (5b) designed as an LED for emitting light waves (L), the first emitter (5a) being designed is to emit light waves (L) of a first wavelength as a main signal and the second emitter (5b) is designed to emit light waves (L) of a second wavelength different from the first wavelength as a reference signal for checking a measurement result of the main signal, the Light waves (L) of the first and second wavelengths can be emitted separately from one another, the emitters (5a, 5b) each being formed as a Spe ktrum, the full half-width of which is a maximum of 50% of a focal point wavelength, preferably a maximum of 20% of the focal point wavelength, the detector (4) being designed to quantitatively detect an intensity of the emitted light waves (L) of the first wavelength and the second wavelength , and wherein the cuvette (3) has a mirror arrangement with a plane mirror (6) and a concave mirror (7) arranged opposite the plane mirror (6), an optical axis (8) of the concave mirror (7) being arranged perpendicular to the plane mirror (6) and the radiation source (2) and the detector (4) are arranged on the plane mirror (6). Optical gas sensor (1) according to Claim 1 , characterized in that the detector (4) and / or at least one emitter (5) have at least one optical filter. Optical gas sensor (1) according to one of the preceding claims, characterized in that a radiation source (2) and a detector (4) are arranged on the cuvette (3) in such a way that light waves (L) emitted by the radiation source (2) directly hit the detector. Optical gas sensor (1) according to one of the preceding claims, characterized in that the radiation source (2) is arranged at a distance from the detector (4) on the cuvette (3), the first emitter (5a) and the second emitter (5b) each are designed to emit light waves (L) with a guided beam path. Optical gas sensor (1) according to one of the Claims 1 to 4th , characterized in that exactly one detector (4) is arranged on the cuvette (3). Optical gas sensor (1) according to one of the Claims 1 to 4th , characterized in that at least two radiation sources (2) are arranged at a distance from one another on the cuvette (3). Optical gas sensor (1) according to Claim 6 , characterized in that the cuvette (3) has at least two detectors (4), the detectors (4) being designed to measure light intensities of different radiation sources (2) or different emitters (5) of the two radiation sources (2).

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