CN206740648U - A kind of NO2The device of concentration distribution detection - Google Patents

A kind of NO2The device of concentration distribution detection Download PDF

Info

Publication number
CN206740648U
CN206740648U CN201720641036.7U CN201720641036U CN206740648U CN 206740648 U CN206740648 U CN 206740648U CN 201720641036 U CN201720641036 U CN 201720641036U CN 206740648 U CN206740648 U CN 206740648U
Authority
CN
China
Prior art keywords
laser
laser beam
wavelength
air
imaging sensor
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.)
Active
Application number
CN201720641036.7U
Other languages
Chinese (zh)
Inventor
梅亮
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.)
Dalian University of Technology
Original Assignee
Dalian University of Technology
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 Dalian University of Technology filed Critical Dalian University of Technology
Application granted granted Critical
Publication of CN206740648U publication Critical patent/CN206740648U/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The utility model belongs to laser spectrum tech application field, and in particular to a kind of NO2The device of concentration distribution detection.By the vertical 90 degree of placements of first laser device and second laser, second laser is rotated by 90 ° the polarization state of the transmitting laser beam of second laser by half-wave plate so that the polarization state of the transmitting laser beam of first laser device and second laser is vertical direction;After this, the laser beam that first laser device and second laser are sent synthesizes light beam via the polarization spectroscope of 45 degree of placements, then is transmitted into after being collimated by laser beam emitting device in air;The backscatter signal for the laser beam being transmitted into air is collected via laser receiver, after bandpass filter filters out the atmospheric background signal, is imaged onto on a tilted-putted imaging sensor.Using apparatus and method of the present utility model, system architecture is greatly simplified, reduces system cost, improves the stability of system.

Description

A kind of NO2The device of concentration distribution detection
Technical field
The utility model belongs to laser spectrum tech application field, and in particular to a kind of NO2The device of concentration distribution detection.
Background technology
Laser radar (Light Detection and Ranging, Lidar) technology is that a kind of active optical remote sensing is visited Survey technology, it has uniqueness in height/spatial resolution, detectivity, antijamming capability and monitoring etc. in real time Advantage.Since laser comes out, American-European countries begins to laser radar technique being applied in atmosphere environment supervision.Difference is inhaled Laser radar (DIAL) technology of receipts is a kind of special shape in laser radar technique.DIAL technologies are directed to the absorption of gas with various Spectral line, from large-scale pulsed laser successively into air launch different wave length laser pulse (a branch of wavelength is located at gas to be measured The big position of body absorption intensity such as absworption peak, is designated as λon;Other a branch of wavelength is located at the small position of under test gas absorption intensity For example paddy is absorbed, it is designated as λoff), and detect, analyze its backscatter signal so as to obtain under test gas concentration in an atmosphere point Cloth.Currently, the DIAL technologies of main flow depend on into air launch nanosecond order light pulse, and passage time differentiate Mode detects the backscatter signal in different distance, so as to finally realize atmospheric gas (such as NO2) concentration detection.DIAL Technology is due to possessing distance resolution and with unique advantage.It is big using the detection of pulsed DIAL technology During gas dusty gas, requirement harshness of the system to light source is, it is necessary to tunable dual wavelength, high pulse energy, narrow linewidth and stability Good nanosecond order (10-100ns) light-pulse generator, this is exactly the main bugbear of field puzzlement international academic community and the current world The focus of research, and limit the main reason of its commercial applications.
First technology [1] (Ryoichi Toriumi, Hideo Tai, Nobuo Takeuchi, " Tunable solid- state blue laser differentialabsorption lidar system for NO2 monitoring,” Opt.Eng.35 (8) 2371-2375,1996) in, by Nd:YAG laser pumping Ti:Sapphire lasers and use and frequency Mode produce near 450nm tunable pulse type laser output.The laser pulse being transmitted into air, looked in the distance by receiving The backscatter signal that mirror is collected and differentiated by photomultiplier detection range.Enter eventually through difference absorption spectrum analytic approach Row data analysis, obtain NO in air2Concentration distribution.In the art, the atmospheric laser radar signal in different distance It is to be parsed by the time of light pulse return laser light reception device or detector.This method light source, photodetection structure are answered It is miscellaneous, stability is poor, with high costs, it is difficult to practical application.
First technology [2] (Shunxing Hu, et.al., " A new differential absorption lidar for NO2measurements uing Raman-shifted technique,”Chinese Optics Letters 1(8) 435-437,2003) in, using Nd:YAG laser difference pumping D2And CH4The mode of gas cell, produce 395.60nm and 396.82nm pulse lasers export, and using similar to signal detection is carried out by the way of first technology [1], finally realize in air NO2The detection of concentration distribution.But still there is light source in this method, photodetection is complicated, stability is poor, with high costs, The problem of being difficult to practical application.
Utility model content
The utility model provides a kind of NO2The apparatus and method of concentration distribution detection, effectively overcome NO in background technology2It is dense Degree distribution detects faced light source, photodetection is complicated, stability is poor, with high costs, it is difficult to the bottleneck such as practical application Problem.
The technical solution of the utility model:
A kind of NO2Concentration distribution detection device, it is characterised in that the device include first laser device, second laser, Half-wave plate, polarization spectroscope, laser beam emitting device, laser receiver, bandpass filter and imaging sensor, first laser device 90 degree of placements vertical with second laser, second laser make the polarization of the transmitting laser beam of second laser by half-wave plate State is rotated by 90 °, and the polarization state of the transmitting laser beam of first laser device and second laser is vertical direction;First laser device Light beam is synthesized via the polarization spectroscope of 45 degree of placements with the laser beam that second laser is sent, then is filled by Laser emission It is transmitted into after putting collimation in air.
The backscatter signal for the laser beam being transmitted into air is collected via laser receiver, by bandpass filter After piece filters out the atmospheric background signal, it is imaged onto on a tilted-putted imaging sensor;Meeting the bar of Sharpe image-forming principle Under part, imaging sensor carries out blur-free imaging to the laser beam being transmitted into air, and different pixels correspond to different distance Upper laser beam imaging, realize the Range resolution detection to the backscatter signal intensity of air.
Described imaging sensor, laser receiver and laser beam emitting device meets following relation:Imaging sensor institute The optical axis position where plane, lens (or parabolic mirror etc.) the place plane of laser receiver and laser beam emitting device Put (namely light path where transmitting light beam) three to intersect, meet Scheimpflug image-forming principles (Sharpe image-forming principle).
Described first laser device and second laser are diode laser, and its operation wavelength passes through temperature and driving electricity Flow control, wavelength is respectively locked at NO2The larger and smaller part of absorption intensity, claims respectively on absorption line (300-600nm) Be λonAnd λoffWavelength;λ is contrasted by analyzingonWavelength and λoffThe intensity P of the atmospheric backscatter optical signal of wavelengthon, Poff, Calculate the NO in air2Concentration distribution.
Described laser beam emitting device is made up of lens or lens group.
The operation wavelength of the transmission peak wavelength of described bandpass filter and first laser device and second laser matches, First laser device and second laser can be allowed to launch laser beam wavelength identical optical signal and pass through.
Described laser receiver is made up of lens or lens group, or is made up of reflective imaging system.
Described image sensor can be array image sensor or linear array image sensor.
The beneficial effects of the utility model:
The utility model NO2The apparatus and method of concentration distribution detection, using imaging sensor as photodetector, and The distance point of the back scattering optical signal of the light beam to being transmitted into air is realized under conditions of Sharpe image-forming principle is met Distinguish detection, it is very big to simplify system architecture, reduce system requirements.The bar of high-power nanosecond order light-pulse generator is not being needed Under part, using continuous optical diode laser as light source, pass through adjustment work temperature so that its wavelength is located at NO respectively2's On absworption peak and absorption paddy, the differential absorbing detection of Range resolution is realized.Using this technical scheme, system is greatly simplified Structure, system cost is reduced, improve the stability of system.
Brief description of the drawings
Fig. 1 is that the geometrical relationship for needing to meet between laser beam emitting device, laser receiver and imaging sensor three is put down Face figure, namely Sharpe image-forming principle schematic diagram.
Fig. 2 (a) is NO2Absorption spectra line chart of the gas in the range of 300-600nm;First laser device and second laser Operation wavelength is located at NO2In the range of absorption spectra at different absorption intensities.
Fig. 2 (b) is NO2Gas absorption spectrum line partial enlarged drawing and λonAnd λoffWavelength relative position schematic diagram.First laser The operation wavelength of device and second laser is located at NO2In the range of absorption spectra at different absorption intensities.
Fig. 3 is NO2The installation drawing of concentration distribution detection.
In figure:1 first laser device;2 second lasers;3 half-wave plates;4 polarization spectroscopes;
5 laser beam emitting devices;6 laser receivers;7 bandpass filters;8 imaging sensors.
Embodiment
Below in conjunction with the accompanying drawings and technical scheme, specific embodiment of the present utility model is further illustrated.
Embodiment
A kind of NO2The method of concentration distribution detection, step are as follows:
A, first laser device and the temperature and driving current of second laser are controlled, wavelength is output it and is locked in respectively NO2Larger (the λ of absorption intensity on gas absorption spectrum lineon) and smaller part (λoff), the wavelength of first laser device and second laser Design standard is:NO2Gas is in λonAnd λoffThere is different absorption intensities on two wavelength.
B, the output beam of first laser device and second laser is coupled into light beam by polarization spectroscope, this Shu Guang Beam is transmitted among air after being collimated via laser beam emitting device.Wherein the polarization state of the output beam of second laser is by half-wave Piece realizes 90 degree of rotations.
C, the driving current of second laser is arranged to 0 or less than operation threshold after, close second laser;Control the One laser drive current launches laser beam to operation threshold is higher than, and the duration of laser beam is designated as T1, is transmitted into big After first laser device laser beam in gas is via the particulate matter back scattering in air, collected by laser receiver, via After bandpass filter filters out the atmospheric background signal, then photodetection realized by imaging sensor, the signal intensity that is recorded (if For array image sensor, it is necessary to which the image pixel intensities that vertical direction is imaged with laser beam are added up) it is λonWavelength it is big Gas backscatter signal intensity P1;
D, first laser device driving current is arranged to 0 or less than operation threshold after, close first laser device;Control second Laser drive current launches laser beam, duration and the first laser in step C of laser beam to operation threshold is higher than The launch time of device is identical (T1), and the second laser laser beam being transmitted into air dissipates backward via the particulate matter in air After penetrating, collected by laser receiver, after filtering out the atmospheric background signal via bandpass filter, then light realized by imaging sensor Electrical resistivity survey is surveyed, and the signal intensity recorded is (if array image sensor, it is necessary to the picture for vertical direction being imaged with laser beam Plain intensity is added up) it is λoffThe atmospheric backscatter signal intensity P2 of wavelength.
E, first laser device driving current is arranged to 0 or less than operation threshold after, close first laser device;Second is swashed Light device driving current be arranged to 0 or less than operation threshold after, close second laser;Laser receiver collects the atmospheric background letter Number, imaging sensor gathers the atmospheric background signal, recorded to carry out photodetection with the identical time (T1) in step C Signal intensity (if array image sensor, it is necessary to the image pixel intensities that vertical direction is imaged with laser beam are added up) For P3;
F, P1-P3, P2-P3 are calculated and respectively obtains first laser device (λonWavelength) and second laser (λoffWavelength) it is big Gas backscatter signal intensity PonAnd Poff
G, repeat step C-F takes n times P to n times (N can be random natural number)onAnd PoffThe average value of signal is designated as respectively Pon-avgAnd Poff-avg
H, system calibration:System known fixed object of adjusting the distance is measured, and noted down by fixed object reflection Laser beam is in the position of image sensor.According to geometry image-forming principle, image sensor pixel and measurement distance can be calculated Between relation.
I, with reference to the relation between the image sensor and measurement distance obtained in step F, according to atmospheric laser radar side Journey (such as formula 1 or its variation), can ask for NO2Gas concentration distribution C (z):
Wherein, σ (λon) it is NO2Gas is in λonAbsorption cross-section or equivalent absorption section at wavelength, σ (λoff) it is NO2Gas In λoffAbsorption cross-section or equivalent absorption section at wavelength, z is distance,It is the differentiating operator adjusted the distance.

Claims (5)

  1. A kind of 1. NO2The device of concentration distribution detection, it is characterised in that the device includes first laser device, second laser, half Wave plate, polarization spectroscope, laser beam emitting device, laser receiver, bandpass filter and imaging sensor, first laser device and The vertical 90 degree of placements of second laser, second laser make the polarization state of the transmitting laser beam of second laser by half-wave plate It is rotated by 90 °, the polarization state of the transmitting laser beam of first laser device and second laser is vertical direction;First laser device and The laser beam that second laser is sent synthesizes light beam via the polarization spectroscope of 45 degree of placements, then by laser beam emitting device It is transmitted into after collimation in air;
    The backscatter signal for the laser beam being transmitted into air is collected via laser receiver, is filtered by bandpass filter After the atmospheric background signal, it is imaged onto on a tilted-putted imaging sensor;Under conditions of Sharpe image-forming principle is met, Imaging sensor carries out blur-free imaging to the laser beam being transmitted into air, and different pixels correspond to laser in different distance Light beam is imaged, and realizes the Range resolution detection to the backscatter signal intensity of air.
  2. 2. device according to claim 1, it is characterised in that described imaging sensor, laser receiver and laser Emitter meets following relation:Plane, the lens place plane of laser receiver and Laser emission where imaging sensor Optical axis position three where device is intersected, and meets Sharpe image-forming principle.
  3. 3. device according to claim 2, it is characterised in that first laser device and second laser are diode laser Device, its operation wavelength are controlled by temperature and driving current, and wavelength is respectively locked at into NO2Absorption intensity is larger on absorption line And smaller part, it is referred to as λonAnd λoffWavelength;λ is contrasted by analyzingonWavelength and λoffThe atmospheric backscatter light letter of wavelength Number intensity Pon, Poff, calculate air NO2Concentration distribution.
  4. 4. device according to claim 3, it is characterised in that described laser beam emitting device is by lens or lens group structure Into;Described laser receiver is made up of lens, lens group or reflective imaging system.
  5. 5. device according to claim 4, it is characterised in that described imaging sensor is array image sensor or line Array image sensor.
CN201720641036.7U 2016-07-29 2017-06-05 A kind of NO2The device of concentration distribution detection Active CN206740648U (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CN201620828740 2016-07-29
CN2016208287409 2016-07-29

Publications (1)

Publication Number Publication Date
CN206740648U true CN206740648U (en) 2017-12-12

Family

ID=60569312

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201720641036.7U Active CN206740648U (en) 2016-07-29 2017-06-05 A kind of NO2The device of concentration distribution detection

Country Status (1)

Country Link
CN (1) CN206740648U (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761486A (en) * 2018-05-16 2018-11-06 大连理工大学 New pattern laser radar system based on Scheimpflug principles
WO2021122885A1 (en) 2019-12-20 2021-06-24 Centre National De La Recherche Scientifique (Cnrs) System and method for detecting and quantifying gaseous constituents in the atmosphere
CN113075684A (en) * 2021-04-06 2021-07-06 浙江师范大学 Novel Sas atmosphere laser radar based on TDLAS technology

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761486A (en) * 2018-05-16 2018-11-06 大连理工大学 New pattern laser radar system based on Scheimpflug principles
CN108761486B (en) * 2018-05-16 2021-02-19 泛测(北京)环境科技有限公司 Laser radar system based on Scheimpflug principle
WO2021122885A1 (en) 2019-12-20 2021-06-24 Centre National De La Recherche Scientifique (Cnrs) System and method for detecting and quantifying gaseous constituents in the atmosphere
CN113075684A (en) * 2021-04-06 2021-07-06 浙江师范大学 Novel Sas atmosphere laser radar based on TDLAS technology
CN113075684B (en) * 2021-04-06 2023-09-19 浙江师范大学 Novel sand's atmosphere laser radar based on TDLAS technology

Similar Documents

Publication Publication Date Title
CN106124453A (en) A kind of NO2the apparatus and method of concentration distribution detection
US7580127B1 (en) Polarization lidar for the remote detection of aerosol particle shape
US6690472B2 (en) Pulsed laser linescanner for a backscatter absorption gas imaging system
CN102175662B (en) Portable Terahertz remote sensing detector and remote detection method
CN101109702B (en) Large-caliber laser isotope scanner and method for measuring structure constant atmosphere index of refraction
CN109991624B (en) Novel laser radar and detection method based on coaxial optics and single photon detection technology
CN102749627B (en) Full-height laser radar for detecting atmosphere wind field, temperature and density
CN206740648U (en) A kind of NO2The device of concentration distribution detection
CN105911562B (en) A kind of three-dimensional scanning type many reference amounts laser radar system for environmental monitoring
CN202522516U (en) Optical transmissivity test device
CN105319191A (en) Spectrograph type laser radar system detecting bioaerosol
CN105928902A (en) High-spectrum-resolution total atmospheric spectral transmittance measuring method
CN206038529U (en) Terahertz is pumping now terahertz detection time domain spectroscopy system
CN106772426B (en) System for realizing remote laser high-sensitivity single photon imaging
CN106226782A (en) A kind of apparatus and method of air wind speed profile detection
CN109211879A (en) A kind of gas remote measurement device and method
CN206671566U (en) A kind of multi-wavelength polarizes Raman laser radar system
CN114660573A (en) Laser radar system for measuring concentration of atmospheric carbon dioxide and methane column
CN211528208U (en) Optical fiber gas concentration remote sensing detection device based on coherent detection method
CN102998261A (en) Terahertz wave pseudo heat light source-based imaging device
Marchant et al. Aglite lidar: a portable elastic lidar system for investigating aerosol and wind motions at or around agricultural production facilities
CN110161433B (en) Intermediate layer magnetic field remote measuring device based on gated photon counting
CN210090678U (en) Novel laser radar based on coaxial optics and single photon detection technology
Cester Atmospheric aerosol monitoring at the Pierre Auger Observatory
RU2544305C1 (en) Laser location system

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant