CN110987870A - System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology - Google Patents

System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology Download PDF

Info

Publication number
CN110987870A
CN110987870A CN201911326880.0A CN201911326880A CN110987870A CN 110987870 A CN110987870 A CN 110987870A CN 201911326880 A CN201911326880 A CN 201911326880A CN 110987870 A CN110987870 A CN 110987870A
Authority
CN
China
Prior art keywords
signal
module
gas
concentration
value
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201911326880.0A
Other languages
Chinese (zh)
Inventor
李永刚
张涛
李洪刚
魏莹莹
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TIANJIN TONGYANG TECHNOLOGY DEVELOPMENT CO LTD
Original Assignee
TIANJIN TONGYANG TECHNOLOGY DEVELOPMENT CO LTD
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TIANJIN TONGYANG TECHNOLOGY DEVELOPMENT CO LTD filed Critical TIANJIN TONGYANG TECHNOLOGY DEVELOPMENT CO LTD
Priority to CN201911326880.0A priority Critical patent/CN110987870A/en
Publication of CN110987870A publication Critical patent/CN110987870A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/39Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using tunable lasers

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Analytical Chemistry (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Optics & Photonics (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The utility model provides a system for monitoring gas concentration, includes distributed feedback laser, signal generation module, pyramid prism, off-axis parabolic mirror, photoelectric detection module, signal transmission module, lock phase amplification module and signal processing module, wherein: laser output by the distributed feedback laser is collimated, then passes through a central hole in the off-axis parabolic mirror and a region to be detected of target gas, is reflected back to the off-axis parabolic mirror by the pyramid prism, and the returned laser is converged to a photosensitive region of the photoelectric detection module; the signal transmission module transmits the electric signal acquired by the photoelectric detection module to the phase-locked amplification module; the phase-locked amplification module demodulates the electric signal acquired by the photoelectric detection module by using the reference signal provided by the signal generation module; the signal processing module extracts the 2f signal through a filter and utilizes the filter to carry out smooth filtering on the extracted signal, thereby providing the 2f signal and the direct current signal for subsequent algorithm processing.

Description

System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology
Technical Field
The invention relates to the field of exhaust emission, in particular to a system and a method for monitoring gas concentration in real time based on a wavelength modulation spectrum technology.
Background
The tunable laser absorption spectrum technology can realize in-situ on-line measurement of parameters such as component concentration, temperature, pressure, speed and the like by utilizing the laser absorption characteristics of components in the gas to be measured. Compared with other technologies, the laser absorption spectrum technology has the advantages of accurate measurement, high response speed, non-invasive induction and the like, and has wide application prospect in the field of atmospheric environment detection. The tunable laser absorption spectroscopy technology is mainly divided into a direct absorption spectroscopy technology and a wavelength modulation spectroscopy technology.
The working principle of the direct absorption spectrum technology is that a certain scanning current is injected into a laser, the laser wave band emitted by the laser is driven to completely cover the wave band of a gas absorption peak, the laser passes through an absorption path containing gas to be detected and is absorbed by the gas at a specific position, an absorbed optical signal is converted into an electric signal through a photoelectric detector, and the characteristics of the absorption peak are provided by means of baseline fitting and the like. The direct absorption spectrum technology system is simple and easy to realize, but the measuring result is easily influenced by the emergent light intensity of the laser and the like, and the stability of the measuring result is poor. Therefore, the stability and the measurement accuracy of the system are often improved by the wavelength modulation spectrum technology.
The working principle of the wavelength modulation spectrum is that a high-frequency sinusoidal signal with the frequency f is modulated on the scanning current of a laser, laser emitted by the laser is absorbed by gas to be measured and then converted into an electric signal by a photoelectric detector, a phase-locked amplifier carries out phase-sensitive detection processing by utilizing the mutual irrelevance between an input signal and a noise signal, the electric signal is demodulated by a same-frequency (1f) or frequency-doubling (nf) signal and a complete useful signal is extracted from noise, and the concentration of the gas to be measured can be obtained by the relation between the amplitude of a harmonic signal and the concentration of the gas to be measured. The value of the frequency f is dozens of kHz to hundreds of kHz, and the frequency and the amplitude of the high-frequency sinusoidal modulation signal are changed, so that the optical noise in the direct absorption spectrum technology can be effectively reduced. Meanwhile, the wavelength modulation spectrum technology moves the information to be detected to a high-frequency wave band, so that 1/f low-frequency noise in the system is effectively inhibited, and higher detection precision is obtained.
In actual measurement, the intensity of laser is easily influenced by temperature, dust, vibration and the like to cause intensity change, the inversion concentration error is large only according to a 2f signal, a reference light path is generally arranged by adding a reference cell and the like to eliminate the influence of light intensity change on a measurement result, and the system complexity is high.
Disclosure of Invention
In view of the above, the main object of the present invention is to provide a system and a method for monitoring gas concentration, which are intended to at least partially solve at least one of the above technical problems.
In order to achieve the above object, as an aspect of the present invention, a system for monitoring gas concentration is provided, including a distributed feedback laser, a signal generating module, a corner cube prism, an off-axis parabolic mirror, a photodetection module, a signal transmission module, a phase-locked amplification module, and a signal processing module, wherein:
laser output by the distributed feedback laser is collimated, then passes through a central hole in the off-axis parabolic mirror and a region to be detected of target gas, is reflected back to the off-axis parabolic mirror by the pyramid prism, and the returned laser is converged to a photosensitive region of the photoelectric detection module;
the signal transmission module transmits the electric signal acquired by the photoelectric detection module to the phase-locked amplification module;
the phase-locked amplification module demodulates the electric signal acquired by the photoelectric detection module by using the reference signal provided by the signal generation module;
the signal processing module extracts the 2f signal through a filter and utilizes the filter to carry out smooth filtering on the extracted signal, thereby providing the 2f signal and the direct current signal for subsequent algorithm processing.
The signal generation module generates a sawtooth signal and a sine signal, and modulates the sine signal onto the sawtooth signal as a driving signal of the distributed feedback laser;
the photoelectric detection module is used for converting the received optical signal into an electric signal containing gas concentration information to obtain a direct absorption signal.
The system also comprises a temperature control module, wherein the temperature control module is used for controlling the working temperature of the distributed feedback laser, the internal secondary temperature control can accurately control the temperature to be the required temperature, the error is +/-0.001 ℃, and the stability of the output wavelength of the distributed feedback laser is effectively ensured;
the system also comprises a current driving module, wherein the current driving module converts the modulated voltage signal into a current signal and performs current tuning on the distributed feedback laser, so that the wavelength range of laser emitted by the distributed feedback laser is ensured to completely cover the absorption wavelength of the target gas.
The system utilizes the direct current signal to carry out normalization processing on the 2f signal, a reference air chamber and a reference light path do not need to be arranged inside the system, and the complexity of the system is low.
Wherein the signal processing module extracts an absorption line of the gas by using an FIR filter.
The signal processing module is used for carrying out normalization processing on the 2f signal by using the direct current signal, and quickly inverting the concentration by establishing a second-order relation between the peak value and the concentration of the normalized 2f signal.
The inversion method comprises the following specific steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
The signal generation module, the signal transmission module, the phase-locking amplification module and the signal processing module are integrated on the same circuit board.
The temperature control module and the current driving module are integrated on the same circuit board.
As another aspect of the present invention, there is also provided a method of monitoring a gas concentration, comprising the steps of:
the system is electrified and automatically started, the signal generation module generates waveform voltage, and the current driving module converts a voltage signal into current to drive the laser to generate a laser signal;
the laser signal passes through a target area of the gas to be detected through a central hole of the off-axis parabolic mirror, and the pyramid prism reflects the laser signal to the off-axis parabolic mirror;
the off-axis parabolic mirror converges laser on the photoelectric detection module, the photoelectric detection module converts an optical signal into a voltage signal, the signal transmission module collects the voltage signal and transmits the voltage signal to the phase-locked amplification module, and the phase-locked amplification module analyzes a 2f signal;
judging whether the light intensity meets the requirements, if not, alarming and judging whether the light intensity meets the requirements; and if the requirements are met, acquiring a 2f signal, and obtaining the gas concentration by adopting a quick inversion step.
The rapid inversion method comprises the following steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
Based on the technical scheme, compared with the prior art, the system and the method for monitoring the gas concentration have at least one of the following beneficial effects:
1. according to the method, the absorption signal of the environmental gas is collected in real time to serve as a background curve to be deducted, a reference gas chamber is not required to be arranged in the system, and the influence of the airtightness of the gas chamber, the adsorbability of the gas and the like on the measurement result is avoided;
2. the system of the invention utilizes the FIR filter to extract the absorption spectral line of the gas by selecting proper filter coefficients, thereby reducing the noise interference;
3. according to the method, the 2f signal is normalized by using the direct current signal, the influence of laser light intensity jitter, dust and the like on the light intensity is eliminated, and the concentration is quickly inverted by establishing a second-order linear relation between the peak value and the concentration of the normalized 2f signal;
4. in the system, the functions of the signal generation module, the phase-locking amplification module, the signal processing module and the like are integrated on one circuit board, and the functions of the current driving module and the temperature control module of the laser are integrated on one circuit board, so that the modularization and the integration of the system are facilitated.
Drawings
FIG. 1 is a flowchart of the operation of a hardware system according to an embodiment of the present invention;
FIG. 2 is a flow chart of a monitoring method according to an embodiment of the present invention;
FIG. 3 is a spectrum of the absorption peak and concentration of CO in example 1 of the present invention;
FIG. 4 is a second order nonlinear fit of CO concentration to 2fmean in example 1 of the present invention;
FIG. 5 shows CO in example 2 of the present invention2A spectrum of absorption peaks versus concentration;
FIG. 6 shows CO in example 2 of the present invention2Second order nonlinear fit plot of concentration to 2 fmean.
Detailed Description
In order that the objects, technical solutions and advantages of the present invention will become more apparent, the present invention will be further described in detail with reference to the accompanying drawings in conjunction with the following specific embodiments.
The invention discloses a system and a method for monitoring gas concentration in real time based on a wavelength modulation spectrum technology, which centralize the functions of a signal generation module, a phase-locked amplification module, a signal processing module and the like on one circuit board, centralize the functions of a current driving module and a temperature control module of a laser on one circuit board, and are convenient for the modularization and the integration of a system; by collecting the absorption signal of the environmental gas in real time as a background curve to be deducted, a reference gas chamber is not required to be arranged in the system, so that the influence of the airtightness of the gas chamber, the adsorbability of the gas and the like on the measurement result is avoided; the system of the invention utilizes the FIR filter to extract the absorption spectral line of the gas by selecting proper filter coefficients, thereby reducing the noise interference; the 2f signal is normalized by using the direct current signal, the influence of laser light intensity jitter and the like on light intensity is eliminated, and the concentration is quickly inverted by establishing a second-order relational expression of the normalized 2f signal peak value and the concentration.
Specifically, as shown in fig. 1, it is a flowchart of the hardware system according to the embodiment of the present invention. The invention discloses a system for monitoring gas concentration, which comprises a distributed feedback laser, a signal generation module, a pyramid prism, an off-axis parabolic mirror, a photoelectric detection module, a signal transmission module, a phase-locked amplification module and a signal processing module, wherein:
laser output by the distributed feedback laser is collimated, then passes through a central hole in the off-axis parabolic mirror and a region to be detected of target gas, is reflected back to the off-axis parabolic mirror by the pyramid prism, and the returned laser is converged to a photosensitive region of the photoelectric detection module;
the signal transmission module transmits the electric signal acquired by the photoelectric detection module to the phase-locked amplification module;
the phase-locked amplification module demodulates the electric signal acquired by the photoelectric detection module by using the reference signal provided by the signal generation module;
the signal processing module extracts the 2f signal through a filter and utilizes the filter to carry out smooth filtering on the extracted signal, thereby providing the 2f signal and the direct current signal for subsequent algorithm processing.
The signal generation module generates a sawtooth signal and a sine signal, and modulates the sine signal onto the sawtooth signal as a driving signal of the distributed feedback laser;
the photoelectric detection module is used for converting the received optical signal into an electric signal containing gas concentration information to obtain a direct absorption signal.
The system also comprises a temperature control module, wherein the temperature control module is used for controlling the working temperature of the distributed feedback laser, the internal secondary temperature control can accurately control the temperature to be the required temperature, the error is +/-0.001 ℃, and the stability of the output wavelength of the distributed feedback laser is effectively ensured;
the system also comprises a current driving module, wherein the current driving module converts the modulated voltage signal into a current signal and performs current tuning on the distributed feedback laser, so that the wavelength range of laser emitted by the distributed feedback laser is ensured to completely cover the absorption wavelength of the target gas.
The system utilizes the direct current signal to carry out normalization processing on the 2f signal, a reference air chamber and a reference light path do not need to be arranged inside the system, and the complexity of the system is low.
Wherein the signal processing module extracts an absorption line of the gas by using an FIR filter.
The signal processing module is used for carrying out normalization processing on the 2f signal by using the direct current signal, and quickly inverting the concentration by establishing a second-order relation between the peak value and the concentration of the normalized 2f signal.
The inversion method comprises the following specific steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
The signal generation module, the signal transmission module, the phase-locking amplification module and the signal processing module are integrated on the same circuit board.
The temperature control module and the current driving module are integrated on the same circuit board.
Fig. 2 is a flow chart of a monitoring method according to an embodiment of the present invention. The method comprises the following steps:
the system is electrified and automatically started, the signal generation module generates waveform voltage, and the current driving module converts a voltage signal into current to drive the laser to generate a laser signal;
the laser signal passes through a target area of the gas to be detected through a central hole of the off-axis parabolic mirror, and the pyramid prism reflects the laser signal to the off-axis parabolic mirror;
the off-axis parabolic mirror converges laser on the photoelectric detection module, the photoelectric detection module converts an optical signal into a voltage signal, the signal transmission module collects the voltage signal and transmits the voltage signal to the phase-locked amplification module, and the phase-locked amplification module analyzes a 2f signal;
judging whether the light intensity meets the requirements, if not, alarming and judging whether the light intensity meets the requirements; and if the requirements are met, acquiring a 2f signal, and obtaining the gas concentration by adopting a quick inversion step.
The rapid inversion method comprises the following steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
The technical solution of the present invention is further illustrated by the following specific examples in conjunction with the accompanying drawings.
Example 1
Example 1 to monitor the change in the concentration of CO (carbon monoxide) in the air, the following example was analyzed.
Firstly, a DFB laser with the center wavelength of 2326.8nm is selected, the working temperature of the laser is set to be 29 ℃, the output wavelength of the laser is 2326.56 nm-2327.21 nm, and the absorption peak of CO at the position of 2326.823nm is completely covered.
And adjusting the light path to ensure that the voltage range of the absorbed light intensity of the detector is between 2V and 5V so as to ensure the accuracy of the measurement result.
Before measurement, the measurement concentration of CO needs to be subjected to nonlinear calibration, the maximum value of the measurement concentration is set to 1000ppm, 1000ppm is taken as the initial concentration, one point is selected at every 1000ppm, and 9 points are calibrated to obtain the relation between the absorption peak and the concentration, which is shown in figure 3;
establishing a non-linear relationship between concentration and ratio, as shown in fig. 4;
and the CO with the concentration of 2000ppm, 5000ppm and 10000ppm is measured again for verification, the measurement result is shown in the table 1, the maximum error is about 1%, the measurement precision is high, and the measurement requirement is met.
Table 1 measurement error in example 1
Figure BDA0002328607310000081
Example 2
Example 2 to monitor CO in air2The change in the concentration of (carbon dioxide) was analyzed in the following manner.
Selecting a DFB laser with the center wavelength of 2004nm, setting the working temperature of the laser to be 30 ℃, setting the output wavelength of the laser to be 2003.61-2004.41 nm, and completely covering CO2Absorption peak at 2004.019 nm.
And adjusting the light path to ensure that the maximum voltage value range of the absorption light intensity of the detector is between 2V and 5V so as to ensure the accuracy of the measurement result.
Before measurement, CO needs to be measured2The measured concentration is subjected to nonlinear calibration, the maximum value of the measured concentration is set to 50000ppm, 10000ppm is taken as the initial concentration, one point is selected at intervals of 10000ppm, and 5 points are calibrated in total, so that the relation between the absorption peak and the concentration is obtained and is shown in figure 5;
establishing a non-linear relationship between concentration and ratio, as shown in fig. 6;
again select CO concentrations of 10000ppm, 30000ppm and 50000ppm2The verification is carried out, the measurement result is shown in table 2, the error between the two is very small, the maximum error is within 7 percent, and the measurement requirement is met.
Table 2 measurement error in example 2
Figure BDA0002328607310000091
The above-mentioned embodiments are intended to illustrate the objects, technical solutions and advantages of the present invention in further detail, and it should be understood that the above-mentioned embodiments are only exemplary embodiments of the present invention and are not intended to limit the present invention, and any modifications, equivalents, improvements and the like made within the spirit and principle of the present invention should be included in the protection scope of the present invention.

Claims (10)

1. The utility model provides a system for monitoring gas concentration which characterized in that, includes distributed feedback laser, signal generation module, pyramid prism, off-axis parabolic mirror, photoelectric detection module, signal transmission module, lock phase amplification module and signal processing module, wherein:
laser output by the distributed feedback laser is collimated, then passes through a central hole in the off-axis parabolic mirror and a region to be detected of target gas, is reflected back to the off-axis parabolic mirror by the pyramid prism, and the returned laser is converged to a photosensitive region of the photoelectric detection module;
the signal transmission module transmits the electric signal acquired by the photoelectric detection module to the phase-locked amplification module;
the phase-locked amplification module demodulates the electric signal acquired by the photoelectric detection module by using the reference signal provided by the signal generation module;
the signal processing module extracts the 2f signal through a filter and utilizes the filter to carry out smooth filtering on the extracted signal, thereby providing the 2f signal and the direct current signal for subsequent algorithm processing.
2. The system for monitoring gas concentration of claim 1, wherein the signal generation module generates a sawtooth signal and a sinusoidal signal and modulates the sinusoidal signal onto the sawtooth signal as the driving signal for the distributed feedback laser;
the photoelectric detection module is used for converting the received optical signal into an electric signal containing gas concentration information to obtain a direct absorption signal.
3. The system for monitoring the concentration of the gas as claimed in claim 1, wherein the system further comprises a temperature control module, the temperature control module is used for controlling the working temperature of the distributed feedback laser, the internal secondary temperature control can accurately control the temperature to the required temperature, the error is ± 0.001 ℃, and the stability of the output wavelength of the distributed feedback laser is effectively ensured;
the system also comprises a current driving module, wherein the current driving module converts the modulated voltage signal into a current signal and performs current tuning on the distributed feedback laser, so that the wavelength range of laser emitted by the distributed feedback laser is ensured to completely cover the absorption wavelength of the target gas.
4. The system for monitoring the concentration of the gas as claimed in claim 1, wherein the system utilizes the direct current signal to perform normalization processing on the 2f signal, a reference gas chamber and a reference light path are not required to be arranged inside, and the complexity of the system is low.
5. The system for monitoring gas concentration of claim 1, wherein the signal processing module utilizes a FIR filter to extract absorption lines of the gas.
6. The system for monitoring the concentration of a gas according to claim 1, wherein the signal processing module normalizes the 2f signal using the dc signal and rapidly inverts the concentration by establishing a second order relation between the peak value of the normalized 2f signal and the concentration.
7. The system for monitoring the concentration of a gas according to claim 6, wherein the inversion comprises the following specific steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
8. The system for monitoring the concentration of a gas of claim 1, wherein the signal generation module, the signal transmission module, the phase-locked amplification module and the signal processing module are integrated on the same circuit board.
9. The system for monitoring gas concentration of claim 3, wherein the temperature control module and the current drive module are integrated on the same circuit board.
10. A method for monitoring gas concentration using the system for monitoring gas concentration according to any one of claims 1 to 9, comprising the steps of:
the system is electrified and automatically started, the signal generation module generates waveform voltage, and the current driving module converts a voltage signal into current to drive the laser to generate a laser signal;
the laser signal passes through a target area of the gas to be detected through a central hole of the off-axis parabolic mirror, and the pyramid prism reflects the laser signal to the off-axis parabolic mirror;
the off-axis parabolic mirror converges laser on the photoelectric detection module, the photoelectric detection module converts an optical signal into a voltage signal, the signal transmission module collects the voltage signal and transmits the voltage signal to the phase-locked amplification module, and the phase-locked amplification module analyzes a 2f signal;
judging whether the light intensity meets the requirements, if not, alarming and judging whether the light intensity meets the requirements; and if the requirements are met, acquiring a 2f signal, and obtaining the gas concentration by adopting a quick inversion step.
The rapid inversion method comprises the following steps:
pre-collecting 2f signals and direct absorption signals of different concentrations in a gas area to be detected, and carrying out the following processing:
extracting the maximum value of the 2f wave crest at the position known as the absorption peak, extracting the left wing minimum value and the right wing minimum value of the 2f wave trough at the positions of two wings of the absorption peak, subtracting the average value of the left wing minimum value and the right wing minimum value from the maximum value to obtain the peak value of the 2f absorption peak, and marking as 2 fpeak;
because the number of points of the direct absorption signal is known to be equal to that of the 2f signal, selecting a certain section of direct absorption signal at the position without an absorption peak, and averaging the section of direct absorption signal to be marked as dcmean;
normalizing the peak value 2fpeak of the 2f absorption peak by using the mean value dcmean of the direct absorption signal to obtain a normalized 2f value which is marked as 2 fmean;
establishing a nonlinear relation between the concentration and 2 fmean;
and flushing the gas with the concentration to be measured into the region of the gas to be measured, calculating to obtain the normalized 2f value, and substituting the value into the established nonlinear relation to obtain the true value of the concentration of the gas to be measured.
CN201911326880.0A 2019-12-20 2019-12-20 System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology Pending CN110987870A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201911326880.0A CN110987870A (en) 2019-12-20 2019-12-20 System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201911326880.0A CN110987870A (en) 2019-12-20 2019-12-20 System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology

Publications (1)

Publication Number Publication Date
CN110987870A true CN110987870A (en) 2020-04-10

Family

ID=70073543

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201911326880.0A Pending CN110987870A (en) 2019-12-20 2019-12-20 System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology

Country Status (1)

Country Link
CN (1) CN110987870A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112504981A (en) * 2020-11-25 2021-03-16 天津同阳科技发展有限公司 Method for detecting motor vehicle exhaust emission by using wavelength modulation spectrum technology
CN113533249A (en) * 2021-06-09 2021-10-22 山东师范大学 N2O detection system and method based on open optical path and wavelength modulation
CN114047161A (en) * 2021-10-28 2022-02-15 中南大学 Self-diagnosis method for laser emission wavelength
CN114414517A (en) * 2021-12-17 2022-04-29 山东微感光电子有限公司 Low-power intrinsic safety type laser carbon monoxide sensing control method and system
CN114993987A (en) * 2022-05-16 2022-09-02 北京航空航天大学 Temperature and gas concentration measuring method and system based on absorption spectrum amplitude modulation
CN117747008A (en) * 2024-02-07 2024-03-22 山东省科学院激光研究所 Baseline fitting and noise reduction method and system for gas laser absorption spectrum

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112504981A (en) * 2020-11-25 2021-03-16 天津同阳科技发展有限公司 Method for detecting motor vehicle exhaust emission by using wavelength modulation spectrum technology
CN113533249A (en) * 2021-06-09 2021-10-22 山东师范大学 N2O detection system and method based on open optical path and wavelength modulation
CN114047161A (en) * 2021-10-28 2022-02-15 中南大学 Self-diagnosis method for laser emission wavelength
CN114414517A (en) * 2021-12-17 2022-04-29 山东微感光电子有限公司 Low-power intrinsic safety type laser carbon monoxide sensing control method and system
CN114414517B (en) * 2021-12-17 2024-02-20 山东微感光电子有限公司 Low-power-consumption intrinsic safety type laser carbon monoxide sensing control method and system
CN114993987A (en) * 2022-05-16 2022-09-02 北京航空航天大学 Temperature and gas concentration measuring method and system based on absorption spectrum amplitude modulation
CN114993987B (en) * 2022-05-16 2024-04-30 北京航空航天大学 Temperature and gas concentration measuring method and system based on absorption spectrum amplitude modulation
CN117747008A (en) * 2024-02-07 2024-03-22 山东省科学院激光研究所 Baseline fitting and noise reduction method and system for gas laser absorption spectrum
CN117747008B (en) * 2024-02-07 2024-05-03 山东省科学院激光研究所 Baseline fitting and noise reduction method and system for gas laser absorption spectrum

Similar Documents

Publication Publication Date Title
CN110987870A (en) System and method for monitoring gas concentration in real time based on wavelength modulation spectrum technology
JP5907442B2 (en) Laser gas analyzer
CN102768197B (en) Method and apparatus for detecting gas concentration with the pressure dependency for reducing
CN113252204B (en) Laser absorption spectrum temperature measurement method based on amplitude modulation
US20100242572A1 (en) Wavelength modulation spectroscopy for simultaneous measurement of two or more gas ingredients
WO2014106940A1 (en) Gas absorption spectroscopy device and gas absorption spectroscopy method
CN111474138B (en) Gas concentration measuring device and method based on high-frequency reference optical frequency division multiplexing technology
CN111829982A (en) Multi-component gas concentration detection and temperature error correction method
US6552792B1 (en) Wavelength modulated photoacoustic spectrometer
US20050140979A1 (en) Wavelength modulation spectroscopy method
CN109813639B (en) Infrared light modulation technology-based synchronous measurement device and measurement method for concentration of particulate matters and gas
US11162896B2 (en) Method and gas analyzer for measuring the concentration of a gas component in a measurement gas
CN106483094B (en) Infrared light-emitting light path system for eliminating atmospheric absorption interference and experimental method
CN109696415A (en) A kind of gas absorptivity On-line Measuring Method based on Fast Fourier Transform (FFT)
CN108872146B (en) Laser driving device based on TDLAS and laser generating device based on TDLAS
CN112729544B (en) Laser wavelength locking system and method for scanning absorption spectrum
Kasyutich et al. Mid-infrared laser absorption spectrometers based upon all-diode laser difference frequency generation and a room temperature quantum cascade laser for the detection of CO, N 2 O and NO
CN105866068B (en) Method for extracting harmonic signal peak point of laser absorption spectrum based on recursive least square method
JPH06148072A (en) Method and instrument for measuring concentration of gas
CN211505210U (en) System for monitoring gas concentration in real time based on wavelength modulation spectrum technology
CN112858206A (en) Tunable FPI-based intermediate infrared gas measurement method and device
CN110879215A (en) Tunable laser industrial waste gas online monitoring device and method based on reference compensation
CN116519596A (en) Gas concentration detection device
WO1999039188A1 (en) Method of spectrochemical analysis of impurity in gas
JP2017020929A (en) Isotope concentration calculation method

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination