• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
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    • 专利摘要:
    Method and device (1) for determining the concentration of a predetermined gas in a sample (2) by means of a tuneable diode laser (4) and a light sensor (6), wherein a wavelength of the diode laser (4) in the sample ( 2) radiated substantially monochromatic light by changing a pumping current (I) of a laser diode of the diode laser (4) is varied over time, the intensity of the light emerging from the sample (2) is measured, and the concentration of the gas in the sample (2) is calculated as a function of the time profile of the pumping current (I) and the time course of the measured intensity, the pumping current (I) having a first time interval (9) with a substantially constant and non-zero fundamental current (10). and a second time portion (11) having a starting from the base current (10) continuously increasing current ramp (12).
    公开号:AT519690A1
    申请号:T50138/2017
    申请日:2017-02-21
    公开日:2018-09-15
    发明作者:Eduard Harrauer Ing
    申请人:Acm Gmbh；
    IPC主号:
    专利说明:

    The invention relates to a method for determining the
    Concentration of a predetermined gas in a sample by means of a tuneable diode laser and a light sensor, wherein a wavelength of the substantially monochromatic light emitted by the diode laser in the sample is varied by changing a pumping current of a laser diode of the diode laser, the intensity the light emerging from the sample is measured and the concentration of the
    Gas in the sample as a function of the time course of the pumping current and the time course of the measured
    Intensity is calculated. Moreover, the invention relates to a
    Device for determining the concentration of a predetermined gas in a sample comprising a tunable diode laser with a laser diode for emitting substantially monochromatic light into the sample, a light sensor for
    Measurement of the intensity of the light emerging from the sample, a control unit for controlling the pumping current of the
    Laser diode, and an evaluation unit, wherein the
    Control unit is arranged to vary the pumping current of the laser diode in time and wherein the evaluation unit connected to the light sensor and the control unit and the
    Calculation of the concentration of the gas as a function of the pumping current predetermined by the control unit and of the
    Light sensor measured intensity is set up.
    Such methods and apparatus enable non-destructive determination of the concentration of a predetermined gas in a sample. This property is particularly in the quality inspection of in closed
    Containers of bottled beverages of interest. Depending on which beverage it is, the concentration of a different gas can be determined. The determined concentration allows, for example, conclusions about the shelf life of the drink.
    A comparable method is already known, for example, from WO 2012/001633 A2 and WO 2008/053507 A2. In each case, a method for determining the pressure and the
    Concentration of oxygen in the head area of a closed
    Wine bottle described based on a measured absorption spectrum. The knowledge of the oxygen content in one
    Wine bottle allows to determine the aging of the wine contained. WO 2012/001633 A2 tries the
    Increase the accuracy of the measurement by using two separate absorption spectra. This approach requires a second light source and a second detector, making the device overall much more expensive and expensive. WO 2008/053507 A2 proposes, to improve the accuracy, to compensate for disturbances caused by the sample container (i.e., the wine bottle) by using previously determined reference parameters of the container.
    In WO 2016/051341 A1, a further method of this type is described, which can be used for the study of still drinks with a nitrogen supplement (the existence of nitrogen, however, is referred to as an interfering factor). The method is adapted for the examination of moving bottles and tries to avoid the inaccuracies caused by the movement by selecting suitable time windows for the measurements.
    Finally, US 5,473,161 A shows a corresponding
    Method for determining the CO2 concentration or the CO2 pressure. It deals with the selection of a suitable wavelength for the measurement of CO2.
    The above documents, apart from the principles of the generic measuring method, if anything, only deal with reducing inaccuracies by adjusting the evaluation, e.g. by merging two measurements or a measurement with a reference measurement or by selecting preferred measurements.
    Methods are also already known which are intended to improve the accuracy of the measurement by adapting the measuring method. For example, US Pat. No. 9,310,295 B2 discloses a method in which the time profile of the pumping current with which the laser diode is driven has high-frequency oscillations whose central value increases in sections in the form of a ramp.
    The gas concentration can then be determined from the amplitude of a specific frequency component of the light sensor
    Signals are determined, thereby providing wavelength independent
    Disruptions in the measured total intensity can be hidden and thus the accuracy of the measurement is improved.
    Immediately before the start of the ramp-like course, the pumping current can oscillate about a constant central value (referred to below as "offset" for short). This offset may be selected so that the pump current in the relevant section remains at or above a threshold value of the laser diode.
    Due to the pumping current oscillations, the offset is chosen to be so far below the central value at the beginning of the ramp that the pumping current in that section only reaches this central value at the beginning of the ramp at the moment of maximum (i.e.
    Essentially a vibration amplitude below). That of the
    Pumping current is not constant in the section before the start of the ramp, and practically always below the central one
    Value at the beginning of the ramp. Due to the deliberately introduced variations in the pumping current in this method, the
    Laser diode and inevitably charged with the temperature control of the diode laser, which reduces their life.
    In addition, these fluctuations have a negative effect on the
    Reproducibility of the course in the section of the ramp, because the heat generated by the laser diode due to the jump of the central value between the constant offset and the beginning of the ramp also increases sharply, which depends on different environmental conditions (and optionally depending on the transfer function of a temperature control ) Different on the temperature and thus also the
    Wavelength of the emitted laser light affects. Depending on the duration of the ramp, such effects can affect the whole
    Relate to ramping.
    A pumping current with a ramp without superimposed high-frequency
    Signal components are shown for example in WO 2013/036378 A1. However, in the preceding the ramp
    No pumping current applied to the laser diode, so a
    Jump of the current value is provided, which has the above-mentioned effects on the reproducibility of
    Wavelength of the emitted laser light has.
    Finally, the US 2008/0123713 A1 deals with the
    Control of the diode laser. In this case, an initial section preceding a current ramp is provided, in which a pumping current, not specified, is applied to the laser diode clearly below the threshold current of the laser diode. At the beginning of the ramp, the current is ramped up to or above the threshold current, so that the above-mentioned disadvantages come to bear here as well.
    It is an object of the invention to improve the accuracy with which the concentration of the gas can be determined compared to the known methods.
    The inventive method of the initially mentioned type provides that the pumping current has a first time portion with a substantially constant and non-zero base current and a second time portion with a starting from the base current continuously increasing current ramp.
    The inventive device of the initially mentioned type provides that the control unit is set up to predetermine a substantially constant and nonzero background current as pumping current during a first time interval and to predetermine a current ramp continuously increasing from the base current during a second time interval.
    The determination of the concentration of a predetermined gas in a sample is carried out by calculation based on measurements of physical quantities. Specifically, an electronic signal of the light sensor incident on the laser light transmitted through the sample is processed. This signal represents the intensity of the light striking the light sensor. From the concentration of the gas can be estimated at a known total pressure, the partial pressure of the gas in the sample.
    The predetermined gas may in particular be nitrogen, CO2 or oxygen. The sample is preferably a volume or
    Partial volume in a container containing a gas mixture and liquids in the form of vapor. The determination of the nitrogen concentration is based on the finding that the measurable partial pressure of water vapor in the sample is also proportional to the partial pressure and thus the concentration of nitrogen in the sample. The ratio of partial pressures can be estimated by a weighting factor, which depends on the ratio of molecular weights.
    The relationship between the time course of the pumping current and the time course of the measured intensity used by the present method essentially corresponds to an absorption spectrum of the sample. Methods for determining such absorption spectra are known by the abbreviation TDLAS (tunable diode laser absorption spectroscopy). The absorption spectrum can be determined from the relative intensity transmitted and measured by the sample as a function of the wavelength of the emitted light. The concentration of the particular gas sought can be determined from the absorption spectrum and using the law of Lambert-Beer, i. based on the broadening of an absorption line.
    In particular, a DFB (distributed feedback) diode can be provided as the laser diode. In a tunable diode laser, the wavelength of the emitted light is adjustable, in particular by changing the current and / or the ambient temperature. The ambient temperature may be, for example, a Peltier element thermally connected to the laser diode. The wavelength of the emitted light is characterized in particular by the central wavelength of the spectrum emitted by the laser diode.
    The pumping current is the current through the laser diode. The basic current is referred to in the present method, a current whose amount is greater than zero. Preferably, the base current and the minimum of the amount of pumping current in operation are the same; i.e. the amount of pumping current does not drop below the level during operation
    Basic current. As current ramp or short ramp, a current is referred to, starting from an initial stream continuously and / or monotonically, preferably strictly monotonous, towards a
    Limit current, which is greater than the initial current in amount, is changed over time. Continuous means in this
    Related that the time course no jumps in the
    Compared to the difference between the limiting current and the base current are significant (e.g., greater than 10%). In the present method, the initial current of the ramp is equal to the base current, i. The ramp starts from the basic flow. Preferably, the base flow corresponds to a lower one
    Current limit (i.e., the lowest current in the course of
    Pumping current) and the limiting current is an upper current limit (i.e., the highest current in the course of the pumping current). The limiting current can vary depending on the wavelength range used, the laser diode used and the quality of these
    Laser diode between 70 and 150 mA (milliamperes), preferably between 80 and 110 mA amount.
    The duration of the ramp and thus of the second temporal
    Section can be pre-determined, for example, a
    Value between 1 and 100 ms (milliseconds), preferably between 5 and 50 ms, in particular 15 ms, can be set. The temporal duration of the first temporal segment is preferably longer than the temporal period of the second temporal segment may be predetermined, for example, a value being at least twice as long, in particular at least four times as long, relative to the temporal duration of the second temporal segment Section is. The time duration of the first time segment may be, for example, between 2 and 500 ms, preferably between 25 and 250 ms, in particular between 80 and 90 ms.
    The first and second temporal portions of the pumping current may be periodically repeated such that the pumping current is periodically pulsed. In this case, one period of the pumping current comprises at least a first temporal segment and a second temporal segment immediately following the first temporal segment
    Section. There may be provided a third temporal portion after the second temporal portion, wherein the
    Pumping current decreases in the third temporal section to the base flow. The duration of a period of the pumping current may be, for example, between 3 and 600 ms, preferably between 30 and 300 ms, in particular of 100 ms.
    Because the current ramp of the pumping current of the laser diode in the second temporal portion of the present method starts from the base current, the temperature change of the diode laser at the beginning of the ramp is minimized. As a result, a lower stress in the control of the diode laser, in particular in connection with the temperature control (for example regulation of a Peltier element), can be achieved in comparison with the prior art. The lower stress can improve the longevity of the device. For the temperature control means a relatively small change in temperature of the diode laser at the beginning of the ramp, that the control deviation remains low and thus generally also the control error is reduced. This improves the reproducibility of the temperature of the diodes and consequently of the emitted wavelength, and thus ultimately also the reproducibility of the measurements carried out, in particular under fluctuating ambient temperature.
    In addition, it has been found to be advantageous that the base current is greater than or equal to the laser threshold of the laser diode. Accordingly, the control unit may be configured to specify as the base current a pumping current greater than or equal to the laser threshold value of the laser diode. The base current preferably corresponds essentially to the laser threshold value of the laser diode. In this case, the laser diode already emits laser light in the first temporal segment and is therefore in the same operating mode as during the measurement, i. E. she "lasers". Passing the pumping current through the laser threshold and the resulting change in operating mode of the laser diode (non-lasers / lasers) can cause a sudden change in temperature in the laser. Such a change in temperature just before the emission of photons relevant to the measurement (i.e., at wavelengths relevant to the measurement) in the second section, would be detrimental and can be avoided by the above-mentioned measure.
    According to a preferred embodiment, the base current may be greater than or equal to 1 mA, preferably between 2 and 10 mA, in particular between 3 and 5 mA. Accordingly, the control unit may be configured to specify a base current of a pump current greater than or equal to 1 mA, preferably between 2 and 10 mA, in particular between 3 and 5 mA.
    The pumping current may have a third time segment after the second time interval, with the pumping current decreasing in the third time interval in at least two stages towards the base current. Accordingly, the
    Control unit be set to specify during a third temporal portion after the second temporal portion in at least two stages to the base current decreasing pumping current. As a step in this context, a change in the pumping current is called, which takes place alternately at different speeds. In particular, the pumping current between comparatively steep flanks of the individual stages can be kept substantially constant for at least 5 μs (microseconds), preferably at least 15 ps, in particular at least 30 ps. This stepwise change exposes the laser diode to a lower instantaneous stress than a single jump to the fundamental current. In particular, the average operating temperature of the laser diode can be kept relatively stable by this type of control, whereby the laser intensity is exposed to lower fluctuations than in a single jump or a correspondingly steep flank. Steep flanks always lead to the temperature stress and thus to an increased requirement for a temperature control (for example a Peltier control). Under these circumstances, a fluctuating ambient temperature leads to a deterioration of the
    Measurement results. With the proposed control, the influence of environmental temperature fluctuations can be minimized. Alternatively, the current following the current ramp in the second section can be regulated in one jump to the base current.
    Moreover, it is advantageous if the light emitted by the diode laser is scattered before entering the sample and / or after exiting the sample. Accordingly, the present device may comprise at least one diffusion element which is arranged to scatter the light emitted by the laser diode before entering the sample and / or after exiting the sample. The scattering can in particular be achieved with one or more diffusion elements through which the light is transmitted or reflected. The extent of scattering or the
    Diffusion elements (e.g., their composition or structure) are designed to compensate for local differences in the intensity of the scattered light. It has been found that the light emitted by a laser diode emits light from the
    Solid angle dependent inhomogeneous distribution of intensity has. This distribution changes in addition
    Dependence on the emitted wavelength. Due to the proposed scattering, this distribution can be at least partially mixed and thus approximated to a more uniform distribution, in particular a normal distribution, which is approximately the same for all wavelengths. The diffusion element can bring about a substantially homogeneous diffusion of the transmitted radiation (eg a ground glass or a sandwich paper) and / or have locally different diffusion and absorption properties (for example in the form of a diaphragm which is achieved by local coloring of an otherwise transparent element, eg glass with splashes of color). The extent of scattering can be determined, for example, by choosing a suitable grating, the skilled person weighing the homogeneity against the remaining intensity of the transmitted radiation. Due to the higher homogeneity of the light, the method becomes more robust (ie less sensitive) to interactions of inhomogeneous optical properties of the sample container (which may be caused eg by local variations of the container material or container geometry, in particular the wall thickness) with different intensity distributions of the emitted one depending on the wavelength laser light. An effect of the scattering is that local peaks (maxima) of the intensity of the laser light can be compensated. Without such compensation, such peaks may result in sensitivity of the measurement for local variations in the optical properties of the sample container. Particularly advantageous is the scattering with wavelength dependent inhomogeneity of the light emitted by the laser diode, i. when the peaks of the intensity distribution occur at different wavelengths at different positions or solid angles.
    In this connection, it is favorable if the light emitted by the diode laser is focused before or immediately after it is scattered. Accordingly, the device may comprise at least one converging lens, which is arranged to focus the light emitted by the laser diode before scattering on or in the diffusion element or, in particular, directly thereafter. The converging lens can be provided in particular in addition to the optics of the diode laser, which is usually tuned to a parallel beam path of the emitted light, for refraction of the laser light. The converging lens is preferably arranged upstream of the diffusion element in the beam path, i. arranged between the diffusion element and diode laser. Focusing the light, especially before it strikes the diffusion element, counteracts a loss of intensity caused by the scattering and therefore allows for greater scattering and hence better mixing and homogeneity (i.e., even lower local variations in the intensity distribution). An intensity loss would be disadvantageous because it would reduce the signal of the measurement and thus the signal-to-noise ratio and would increase the inaccuracy of the measurement.
    According to a preferred embodiment, the laser light emitted by the diode laser has a wavelength between 1300 and 2000 nm (nanometers), preferably between 1750 and 1950 nm, in particular between 1810 and 1850 nm. Accordingly, the diode laser for emitting laser light of a wavelength between 1300 and 2000 nm, preferably between 1750 and 1950 nm, in particular between 1810 and 1850 nm, be set up. For the subject method has been found that in the wavelength range given above as preferred, the highest accuracy of the determined concentration can be achieved. Alternatively, laser light of a wavelength between 1350 and 1550 nm or a correspondingly arranged diode laser can be used. The
    Width of the measured wavelength range preferably corresponds at least to the line width of a water vapor line in said wavelength range.
    Furthermore, in addition to the absorption spectrum, the temperature on the outer wall of a sample container can be measured and taken into account in the calculation of the concentration of the gas. Accordingly, the device can be a
    Temperature measuring device, which is adapted to measure the temperature on an outer wall of a sample container. In particular, the temperature measurement may be a pyrometric measurement (e.g., with an infrared temperature gauge). The measured temperature can be used to compensate for deviations of the measured absorption spectrum from a lower
    Standard conditions (STP) measured absorption spectrum. In particular, this temperature can be used directly on the measured material for compensation calculation of the determined internal pressure (for example of nitrogen) to 20 ° C. (P20).
    In a preferred application of the present method, the predetermined gas is nitrogen and the calculation of the nitrogen concentration comprises a calibrated parameter whose value has previously been determined by calibration with at least one sample having a known nitrogen concentration (reference sample). For example, reference samples with a partial pressure of N2 from 0.5 to 1 bar can be used for the calibration. Accordingly, a preferred application of the present device is to determine the concentration of nitrogen in a closed bottle, especially in a PET bottle. In the case of "still" drinks (without CO2), it is customary to fill the bottles with a drop of liquid nitrogen in addition to the drink before closing them. This bacteriologically protects the beverage in the PET bottle for at least six months. In addition, the stack pressure of the filled bottles is increased. The most accurate determination of the nitrogen concentration allows a reliable determination of the durability. The proposed device allows a particularly accurate determination without it would be necessary to open the bottle. This allows the same sample to be used several times over an extended period of time to test for durability and eliminates the need to
    Keep a collection of samples that need to be opened and destroyed at different times to monitor shelf life over a longer period of time.
    According to a particularly preferred embodiment of the invention, in a method for determining the concentration of a
    Gases in a sample by measuring an absorption spectrum of the sample using a tunable diode laser comprising a laser diode and a Peltier element thermally connected to the laser diode, measuring the absorption spectrum comprising at least the following steps:
    Providing a periodically pulsed pumping current through the laser diode for varying the wavelength of the laser light emitted by the laser diode, wherein a period of the pumping current comprises at least a first portion and a second portion immediately following the first portion, the pumping current being constant in the first portion and Basic current corresponds, the pumping current in the second section continuously increasing between a lower
    Current limit and an upper current limit is changed (in particular in the form of a rising ramp),
    Detecting the intensity of the laser light transmitted through the sample and
    Detecting the detected intensity as a function of an instantaneous value of the pumping current, wherein the value (or level) of the basic current corresponds to the lower current limit value.
    The invention will be described below with reference to particularly preferred
    Embodiments, to which, however, it should not be limited, and further explained with reference to the drawings. In detail:
    Fig. 1 shows schematically an apparatus according to the invention for determining the concentration of a predetermined gas in a sample;
    FIG. 2 schematically shows the optical system of the device according to FIG. 1; FIG.
    3a and 3b a simulated geometric
    Intensity distribution across the image plane of one
    Light sensor intercepted light in a device according to FIG. 2 without diffusion elements (FIG. 3a) or with diffusion elements (FIG. 3b);
    4 shows schematically a period of a pumping current of the laser diode of the device according to FIG. 1.
    FIG. 1 shows a device 1 according to the invention for determining the concentration of a predetermined gas in a sample 2. The device 1 comprises a light source 3 with a tunable diode laser 4 (see Fig. 2). The diode laser 4 comprises a DFB (distributed feedback) laser diode (not shown) for radiating substantially monochromatic light into the sample 2. The diode laser 4 is arranged to emit laser light of a wavelength between 1810 and 1850 nm, i. it is tunable between 1810 and 1850 nm.
    The device 1 also comprises a measuring unit 5 with a light sensor 6 for measuring the intensity of the light emerging from the sample 2. Furthermore, the device 1 comprises a control unit 7 for controlling the pumping current of the laser diode of the diode laser 4. Finally, the device also comprises an evaluation unit 8. The control unit 7 is set up to vary the pumping current of the laser diode of the diode laser 4 over time, in particular periodically to modulate. Specifically, it is set up to predetermine a substantially constant and nonzero background current 10 as the pumping current of the laser diode of the diode laser 4 during a first time interval 9 (see FIG. In the present example, this base current 10 corresponds to the laser threshold value of the diode laser 4. The control unit 7 is also set to predetermine a current ramp 12, which rises continuously from the base current 10, as pumping current of the laser diode of the diode laser 4 during a second time interval 11. Furthermore, control unit is set up to predetermine a pumping current I decreasing in three stages relative to the base current 10 during a third time interval 29. The evaluation unit 8 is connected to the light sensor 6 and to the control unit 7. It is also used to calculate the concentration of the gas as a function of the
    Control unit 7 predetermined pumping current and the from
    Light sensor 6 measured intensity of the light transmitted through the sample 2 set.
    The sample 2 in Fig. 1 is a liquid-empty headspace of a
    Sample container 13 in the form of a closed PET bottle containing a beverage 14 (mainly water). The relative humidity in the headspace is essentially 100%, i. there is water vapor here. The sample container 13 is substantially transparent to light in the infrared region. It is accommodated in a substantially U-shaped insertion holder 15 and is supported by the insertion holder 15 on a closure collar 16 of the sample container 13. An upper part 17 of the device 1 is connected to a base 19 by means of two support elements 18 in the form of rods. On one of the support elements 18 is below the upper part 17, a temperature measuring device 20 in the form of an infrared
    Temperature measuring device arranged. The temperature measuring device 20 is for measuring the temperature on an outer wall of the
    Sample container 13 is established. In the operation of the device 1 is in addition to the absorption spectrum with the
    Temperature measuring device 20, the temperature measured on the outer wall of the sample container 13 and taken into account in the calculation of the concentration of the gas. On the base 19, a display 21 for displaying the determined concentration or the determined partial pressure is provided.
    In Fig. 2, the optical system of the device 1, together with a simplified beam path 22 and the only schematically drawn functional units 3, 5, 7, 8 of the device 1 and their interconnections shown. The optical system of the device 1 comprises two diffusion elements 23, 24. The diffusion elements 23, 24 are each arranged to transmit and scatter the light emitted by the laser diode of the diode laser 4 (emitted). A first
    Diffusion element 23 scatters the light before entering the
    Sample 2. A second diffusion element 24 scatters the light after exiting the sample 2.
    In addition, in each case a converging lens 25, 26 is provided in the light source 3 and the measuring unit 5. A first converging lens 25 in the light source 3 is arranged to focus on the light emitted by the laser diode of the diode laser 4 before scattering on the first diffusion element 23. A second converging lens 26 in the measuring unit 5 is arranged to focus the light emerging from the sample 2 before scattering on the second diffusion element 24. Thus, in operation, the light emitted by the diode laser 4 is focused in each case before it is scattered in one of the diffusion elements 23, 24.
    The effect of the optical system of the device will be understood with reference to Figs. 3a and 3b. 3a shows a geometric intensity distribution, measured on an exemplary measurement and test arrangement, of the laser light emitted by the diode laser 4 in an image plane normal to the optical axis 27 for an optical system, which except for the diffusion elements 23, 24 and converging lenses 25, 26 corresponds to the system shown in Fig. 2. FIG. 3b shows, by comparison, a corresponding geometric intensity distribution using the optical system shown in FIG. With diffusion elements 23, 24 and converging lenses 25, 26. It can be clearly seen that in the distribution in FIG. 3b, the intensity peaks (local maxima) of the distribution in FIG. 3a have been eliminated. The intensity distribution corresponds approximately to an even distribution in the image plane. The uniform intensity distribution thus obtained remains substantially the same with changes in the pumping current and is independent of the type and size of the laser. The converging lenses 25, 26 may also be configured to at least partially compensate for refractions on the sample container.
    Using the apparatus of Figures 1 and 2, the concentration of a predetermined gas, e.g. Nitrogen can be determined in the sample 2 according to the present method. The wavelength (actually the central wavelength of the emission spectrum) of the substantially monochromatic light radiated by the diode laser 4 into the sample 2 is varied and modulated in time by changing the pumping current I of the laser diode of the diode laser 4 (see FIG ). Subsequently, the intensity of the emerging from the sample 2 light with the
    Measuring unit 5 is measured and the concentration of the gas in the
    Sample calculated as a function of the time course of the pump current I and the time course of the measured intensity in the evaluation unit 8. In particular, the
    Line broadening in the from the intensity distribution in
    Depending on the pumping current determined absorption spectrum determined and from this line broadening on the
    Partial pressure of water vapor in the sample closed. Of the
    The relationship between this partial pressure and the partial pressure of the gas being sought (for example nitrogen) can be determined in advance by calibration and subsequently used for the measurement.
    The calibration can be carried out, for example, using one or more reference samples with a known nitrogen concentration.
    In Fig. 4, the time course of a period 28 of
    Pumping current I of the laser diode of the diode laser 4 of the device 1 shown in FIG. 1 schematically. The duration of a period 28 in this example is 100 ms. In operation, the
    Period 28 is repeated in a loop, so that a
    Pulse frequency of the pump current corresponding to the inverse
    Period duration, i. For example, a pulse frequency of 10 Hz. To explain the time course of the pump current I, the period 28 is divided into a first temporal section 9, a second temporal section 11 and a third temporal section 29. The duration of the individual time segments is not shown proportionally.
    As can be seen in FIG. 4, the pumping current I in the first time segment 9 corresponds to a substantially constant and non-zero fundamental current 10. The base current 10 corresponds approximately to the laser threshold value of the laser diode of the diode laser 4. Thus, the laser diode is constantly in laser operation controlled and at the same time the lowest possible
    Temperature development achieved in this operating mode. In the present example, the base current is 5 mA. The duration of the first temporal section 9 in this example is about 84.9 ms.
    In the second temporal section 11, which directly adjoins the first temporal section 9, the pumping current I is changed or raised by the control unit 7 in accordance with a current ramp 12 which rises continuously from the basic current 10 up to a limiting current 30. The duration of the second time segment 11 in this example is exactly 15 ms. In the present example, the limit current is about 100 mA.
    After the second temporal section 11, the third temporal section 29 follows immediately, in which the pumping current I is changed or shut down in three stages 31 toward the basic flow 10. The duration of the individual stages is in each case no more than 35 μs (microseconds), so that a total of a duration of the third temporal portion 29 of at most about 100 microseconds (that is about 0.1 ms) results.
    权利要求:
    Claims (18)
    [1]
    claims
    A method for determining the concentration of a predetermined gas in a sample (2) by means of a tunable diode laser (4) and a light sensor (6), wherein a wavelength emitted by the diode laser (4) in the sample (2) substantially monochromatic light is varied by changing a pumping current (I) of a laser diode of the diode laser (4), the intensity of the light emerging from the sample (2) is measured, and the concentration of the gas in the sample (2) is calculated as a function of the time profile of the pumping current (I) and the time course of the measured intensity, characterized in that the pumping current (I) has a first time interval (9) with a substantially constant and non-zero base current (10). and a second time portion (11) having a starting from the base current (10) continuously increasing current ramp (12).
    [2]
    2. The method according to claim 1, characterized in that the base current (10) is greater than or equal to the laser threshold value of the laser diode.
    [3]
    3. The method according to claim 1 or 2, characterized in that the base current (10) is greater than or equal to 1 mA, preferably between 2 and 10 mA, in particular between 3 and 5 mA.
    [4]
    4. The method according to any one of claims 1 to 3, characterized in that the pumping current (I) after the second temporal portion (11) has a third temporal portion (29), wherein the pumping current (I) in the third temporal portion (29) decreases in at least two stages (31) to the base stream (10) out.
    [5]
    5. The method according to any one of claims 1 to 4, characterized in that the light emitted by the diode laser (4) light is scattered before entering the sample (2) and / or after exiting the sample (2).
    [6]
    6. The method according to claim 5, characterized in that the light emitted by the diode laser (4) is focused before or immediately after it is scattered.
    [7]
    7. The method according to any one of claims 1 to 6, characterized in that the diode laser (4) emitted laser light has a wavelength between 1300 and 2000 nm, preferably between 1750 and 1950 nm, in particular between 1810 and 1850 nm.
    [8]
    8. The method according to any one of claims 1 to 7, characterized in that in addition to the absorption spectrum, a temperature on the outer wall of a sample container (13) measured and taken into account in the calculation of the concentration of the gas.
    [9]
    9. The method according to any one of claims 1 to 8, characterized in that the predetermined gas is nitrogen and the calculation of the nitrogen concentration comprises a calibrated parameter whose value was previously determined by calibration with at least one reference sample having a known nitrogen concentration.
    [10]
    10. Device (1) for determining the concentration of a predetermined gas in a sample (2) comprising a diode laser (4) with a laser diode for emitting substantially monochromatic light into the sample (2), a light sensor (6) for measurement the intensity of the light emerging from the sample (2), a control unit (7) for controlling the pumping current (I) of the laser diode, and an evaluation unit (8), wherein the control unit (7) is arranged, the pumping current (I) of the laser diode to vary over time and wherein the evaluation unit (8) connected to the light sensor (6) and the control unit (7) and for calculating the concentration of the gas in dependence on the predetermined by the control unit (7) pumping current (I) and the light sensor (6) measured intensity is set, characterized in that the control unit (7) is arranged as a pumping current (I) during a first temporal portion (9) a substantially specify a constant and non-zero base current (10) and specify during a second time interval (11), starting from the base current (10) continuously increasing current ramp (12).
    [11]
    11. Device (1) according to claim 10, characterized in that the control unit (7) is arranged to specify a basic current (10) pumping current (I) greater than or equal to a laser threshold value of the laser diode.
    [12]
    12. Device (1) according to claim 10 or 11, characterized in that the control unit (7) is arranged as a base current (10) a pumping current (I) greater than or equal to 1 mA, preferably between 2 and 10 mA, in particular between 3 and 5 mA, to specify.
    [13]
    13. Device (1) according to any one of claims 10 to 12, characterized in that the control unit (7) is arranged, during a third temporal portion (29) after the second temporal portion (11) in at least two stages (31). to the basic flow (10) down to decreasing pumping current (I) to specify.
    [14]
    14. Device (1) according to one of claims 10 to 13, characterized in that the device (1) comprises at least one diffusion element (23, 24) which is used to scatter the light emitted by the laser diode before entering the sample (2 ) and / or after the exit from the sample (2) is established.
    [15]
    15. Device (1) according to claim 14, characterized in that the device (1) comprises at least one converging lens (25, 26) which is used to focus the light emitted by the laser diode before scattering on or in the diffusion element (23, 24 ) or is set up afterwards.
    [16]
    16. Device (1) according to one of claims 10 to 15, characterized in that the diode laser (4) for emitting laser light of a wavelength between 1300 and 2000 nm, preferably between 1750 and 1950 nm, in particular between 1810 and 1850 nm , is set up.
    [17]
    17. Device (1) according to any one of claims 10 to 16, characterized in that the device (1) comprises a temperature measuring device (20) which is adapted to measure the temperature on an outer wall of a sample container (13).
    [18]
    18. Application of a device (1) according to any one of claims 10 to 17 for determining the nitrogen concentration in a closed bottle.
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    同族专利:
    公开号 | 公开日
    AT519690B1|2018-12-15|
    EP3364170A1|2018-08-22|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    WO1987007018A1|1986-05-15|1987-11-19|Hibshman Corporation|Oxygen measurement using visible radiation|
    US5331409A|1992-06-12|1994-07-19|George Thurtell|Tunable diode laser gas analyzer|
    DE102011079342B3|2011-07-18|2012-12-06|Siemens Aktiengesellschaft|Method for controlling a laser diode in a spectrometer|
    DE102013213458A1|2013-07-09|2015-01-15|Siemens Aktiengesellschaft|Method for measuring the concentration of a gas component in a sample gas|
    DE19840345B4|1998-09-04|2004-09-30|Dräger Medical AG & Co. KGaA|Method and device for the quantitative detection of a given gas|
    WO2008048994A2|2006-10-18|2008-04-24|Spectrasensors, Inc.|Detection of moisture in refrigerants|
    EP2610608B1|2011-12-27|2016-07-20|HORIBA, Ltd.|Gas measurement apparatus and method for setting the width of wavelength modulation in a gas measurement apparatus|
    DE102013201459B4|2013-01-30|2017-01-05|Siemens Aktiengesellschaft|Method for measuring the concentration of a gas component in a sample gas|AT521681B1|2018-11-09|2020-04-15|Acm Automatisierung Computertechnik Mess Und Regeltechnik Gmbh|Laboratory gas detector|
    AT521839A1|2018-11-09|2020-05-15|Acm Automatisierung Computertechnik Mess Und Regeltechnik Gmbh|Laboratory gas detector|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA50138/2017A|AT519690B1|2017-02-21|2017-02-21|Method and device for determining the concentration of a predetermined gas|ATA50138/2017A| AT519690B1|2017-02-21|2017-02-21|Method and device for determining the concentration of a predetermined gas|
    EP18157812.1A| EP3364170A1|2017-02-21|2018-02-21|Measuring the concentration of gases in a container|
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