CN105510260B - Differential absorption lidar CO based on aerosol disturbance correction2Detection method - Google Patents
Differential absorption lidar CO based on aerosol disturbance correction2Detection method Download PDFInfo
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Abstract
The invention discloses a kind of differential absorption lidar CO based on aerosol disturbance correction2Detection method, first, in CO2Aerosol disturbing influence is considered in retrieving concentration model;Secondly, 1064 are carried outnmWith 1572nmIt is observed while the Mie scattering lidar of wavelength, obtains 1064nmWith 1572nmThe linear empirical relationship of the extinction coefficient of aerosol and backscattering coefficient under wavelength;Finally, the differential absorption lidar CO of conventional dual wavelength alternate emission is carried out2During detection, using 1064nmThe Mie scattering lidar continuous probe of wavelength is obtained based on the linear empirical relationship of extinction coefficient and backscattering coefficientonWavelength andoffExtinction coefficient and backscattering coefficient under wavelength, with reference to CO2Retrieving concentration model obtains CO2Retrieving concentration result.Inversion result of the present invention is more accurate, has good application prospect in Differential Absorption Lidar for Detecting Atmospheric trace gas field.
Description
Technical field
The present invention relates to atmospheric laser radar technical field more particularly to a kind of difference suctions based on aerosol disturbance correction
Receive laser radar CO2Detection method.
Background technology
CO2As the main component of greenhouse gases, there is important influence to global climate by being widely believed that.And current CO2's
Concentration is monitored, the result obtained with various pattern invertings has larger difference, this shows that there are some unknown carbon remittance mechanism.Cause
This high-precision acquisition Atmospheric CO2Concentration changes, and then carries out regionality CO2Source, the research converged, it is growing so as to cope with
Carbon emission stress problems, are of great significance.Differential absorption lidar is in atmospheric sounding CO2It is exclusive with its in terms of concentration
Advantage is the desired detection equipment for observing its vertical profile distribution.Ground differential absorption lidar can be more obtained in troposphere
High-precision CO2Concentration distribution situation, and in troposphere it is the main region that mankind's activity and carbon source, carbon remittance occur, detection
As a result application value is had more.
Differential absorption lidar mainly emits the slightly differentiated laser beam of two beam wavelength, and beam of laser is by CO2Molecule
Strong absorption, referred to as on wavelength lasers;Another beam of laser is by CO2Molecule weak absorbing, referred to as off wavelength lasers, by measuring with height
Spend the Atmospheric CO of variation2The variation of absorption carrys out inverting CO2Concentration distribution.
Classical laser radar equation is:
Wherein, P (r, λ) be wavelength be λ laser beam height r echo signal intensity;P0It is transmitting laser intensity; A
It is telescope size;η is laser radar overlap factor;C is the light velocity;β (r, λ) is that aerosol and the backward of atmospheric molecule dissipate
Penetrate coefficient;α (r, λ) is the extinction coefficient of aerosol and atmospheric molecule;Ng(r) it is that detected number of the gas at height r is close
Degree;σ (λ) is detected absorption cross section of the gas at height r, is the sensitivity function of wavelength.
Differential absorption lidar is substantially Mie scattering mechanism, its main feature is that the size and incident laser of scattering particles
Close or than laser wavelength of incidence bigger, the scattering optical wavelength of Mie scattering is identical with incident light, is a kind of elastic scattering.It will
λ in laser radar equation (1) is exchanged with λonAnd λoff, the laser radar equation of on wavelength and off wavelength is obtained, by swashing for the two
Optical radar equation is divided by, and obtains following form:
Wherein, λonAnd λoffOn wavelength and off wavelength are represented respectively;σg(λon) and σg(λoff) correspond to respectively on wavelength and
The absorption cross section of off wavelength, value can be directly acquired from HITRAN databases.
It is generally believed that since on wavelength and off wavelength are very close, then
It is Δ r=r so as to obtain thickness at height r2-r1Atmosphere in differential absorption lidar detect CO2Concentration equation:
In formula (3), Ng(r) CO at height r is represented2Concentration;r1For lower height, r2For high height.By
Formula (3) is as it can be seen that the difference of the ratio between the density of detected component and echo signal intensity of on wavelength and off wavelength and absorption cross section
It is related.
For at present, the acquisition in real time of real-time dual-wavelength lidar can be achieved on, common 532nm and 1064nm
Mie scattering lidar receives backscatter signal by telescope, by that can distinguish after the half-reflecting half mirror light splitting of plated film
Acquisition.But for CO2For differential absorption lidar, since two wavelength are very close, this real-time acquisition generally can not be real
It is existing.CO international at present, studies in China mechanism is general2The operation wavelength of differential absorption lidar is concentrated mainly on 1.572 μm
Near, and the problem of due to detector, 2.0 μm of system lies on the table mostly.By taking common wavelength combination as an example, on wavelength is
1572.018nm, off wavelength are 1572.150nm, there was only the wavelength difference of 0.132nm, can not pass through the half-reflection and half-transmission of plated film
Mirror or optical filter realize that the echo-signal of dual wavelength detaches.
This means that CO under normal conditions2The signal acquisition of differential absorption lidar is that dual wavelength is alternate, it is necessary to logical
Time difference or space parallax are crossed to distinguish echo-signal.Under normal circumstances, the alternating by wavelength and off wavelength in time
Switch to realize differential absorbing detection.Aerosol will necessarily generate variation in wavelength handoff procedure in this way, so as in formula (2)And α (r, λon)-α(r,λoff) ≠ 0, then formula (3) can not set up.
Invention content
The purpose of the present invention is provide a kind of differential absorption lidar CO based on aerosol disturbance correction for the first time2Detection
Method, to correct aerosol disturbance to CO2The influence that retrieving concentration is brought.
The main thought of the present invention is as follows:
Dual wavelength alternate emission in differential absorption lidar considers the influence of aerosol disturbance, by the delustring of aerosol
Coefficient and backscattering coefficient introduce differential absorption lidar CO2Retrieving concentration model;1064nm is calculated to dissipate with 1572nm meters
Penetrate the linear dependence of aerosol inversion result under laser radar;Utilize aerosol detection knot under 1064nm Mie scattering lidars
Fruit is to differential absorption lidar inverting CO2Concentration is corrected.
In order to achieve the above objectives, a kind of differential absorption lidar based on aerosol disturbance correction provided by the invention
CO2Detection method, including:
Step 1, consider aerosol disturbance to differential absorption lidar inverting CO2The influence of concentration proposes molten based on gas
The CO of glue disturbance correction2Retrieving concentration model:
Wherein:
Δ r represents air layer thickness, Δ r=r2-r1, r1For lower height, r2For high height,
For CO2Concentration at height r;
WithCO under on wavelength and off wavelength at respectively height r2The absorption cross-section of gas
Product;
α(r,λon) and α (r, λoff) it is respectively that aerosol when on wavelength and off wavelength laser radars is used to disappear at height r
Backscatter extinction logarithmic ratio;
β(r1,λon) and β (r1,λoff) it is respectively height r1Place is using aerosol when on wavelength and off wavelength laser radars
Backscattering coefficient;
β(r2,λon) and β (r2,λoff) it is respectively height r2Place is using aerosol when on wavelength and off wavelength laser radars
Backscattering coefficient.
CO of the present invention2Retrieving concentration model on the one hand consider by aerosol disturbed belt come aerosol extinction coefficient with
The variation of backscattering coefficient theoretically corrects for aerosol disturbance to CO2The influence of retrieving concentration.On the other hand road is used
Diameter integrated form, it is contemplated that CO2The variation of aerosol absorption cross section in retrieving concentration path.
Step 2, the Mie scattering lidar detection of 1064nm wavelength is carried out, obtains Mie scattering lidar in each height
Echo signal intensity;By CO2Detection differential absorption lidar launch wavelength is fixed as off wavelength and is detected, and obtains
1572nm wavelength Mie scattering lidar is in the echo signal intensity of each height;According to echo signal intensity, Fernald is utilized
The laser radar method of inversion distinguishes the extinction coefficient of inverting aerosol, linear to be fitted to obtain delustring under 1064nm and 1572nm wavelength
The linear empirical relationship of coefficient.
1064nm Mie scattering lidars are more general, common laser radar systems.By CO2Detection Difference Absorption swashs
The launch wavelength of optical radar is fixed as off wavelength, makes Atmospheric CO2Influence to result of detection is minimum.
Step 3, since the relationship of the extinction coefficient of aerosol and backscattering coefficient can be determined by Lidar Ratios, because
This, each height aerosol under 1064nm and 1572nm wavelength can be obtained with reference to Lidar Ratios and the extinction coefficient of step 2 inverting
Backscattering coefficient, it is linear to be fitted to obtain the linear empirical relationship of backscattering coefficient under 1064nm and 1572nm wavelength.
Step 4, the differential absorption lidar CO of routine on and off dual wavelength alternate emissions is carried out2During detection, use
The Mie scattering lidar continuous probe of 1064nm wavelength, using under Fernald laser radar method of inversion inverting 1064nm wavelength
The extinction coefficient of aerosol, and obtain corresponding backscattering coefficient;With reference to extinction coefficient and the linear warp of backscattering coefficient
Customs examination system obtain 1572nm wavelength under aerosol extinction coefficient and backscattering coefficient, and by divide into constantly on wavelength or
The extinction coefficient and backscattering coefficient of aerosol under off wavelength.
On wavelength and off wavelength are using common wavelength combination, and on wavelength is 1572.018nm, and off wavelength is
1572.150nm, wavelength difference is usually in 0.2nm, therefore it is considered herein that sustained height gas under on wavelength and off wavelength
The extinction coefficient and backscattering coefficient of colloidal sol are equal, thus in the present invention on wavelength and the corresponding extinction coefficient of off wavelength and
Backscattering coefficient shares extinction coefficient and backscattering coefficient under 1572nm wavelength.Due to differential absorption lidar CO2
Detection is that alternately switching is realized, therefore can pass through the delustring system under 1572nm wavelength in time by wavelength and off wavelength
Number corresponds to the moment with backscattering coefficient and is distinguished as on wavelength or off wavelength.
Step 5, the extinction coefficient of aerosol and backscattering coefficient band under the on wavelength and off wavelength that step 4 are obtained
Enter CO2Retrieving concentration model can obtain CO2Retrieving concentration result.
The present invention has the advantages that:
(1) in CO2The extinction coefficient for the aerosol that aerosol disturbed belt comes is considered in retrieving concentration model and is dissipated backward
Penetrate the variation of coefficient.
(2) in CO2CO is considered in retrieving concentration model2The variation of aerosol absorption cross section in inverting path.
(3) it is easy to implement using ripe laser radar system.
(4) aerosol properties that 1064nm laser radar of the present invention based on being similarly Mie scattering measures are ginseng
It examines, to CO2Retrieving concentration model carries out aerosol disturbance correction so that CO2Retrieving concentration result is more accurate.
Description of the drawings
Fig. 1 is the idiographic flow schematic diagram of the method for the present invention.
Specific embodiment
With reference to Fig. 1, the specific embodiment of the invention is described in further detail.
The present invention specifies the CO shown in using formula (1) first2Retrieving concentration model corrects CO2Detection Difference Absorption swashs
Optical radar inversion method, to correct aerosol variation to CO2The influence of retrieving concentration.The features of the present invention has:(1) it considers
The variation of aerosol during on wavelength and off wavelength alternate emissions, in CO2In retrieving concentration model, disappearing for aerosol is introduced
Backscatter extinction logarithmic ratio and backscattering coefficient;(2) integration of Aerosol Extinction and absorption cross section in inverting path is considered to imitate
Should, introduce integral equation.
Secondly, it is observed simultaneously, together using the Mie scattering lidar of 1064nm and 1572nm wavelength, it is ensured that dual wavelength
Laser radar covers same panel region, to ensure that the double laser radar signal of observation simultaneously is with uniformity, observation time 5~10
Minute.The launch wavelength of the Mie scattering lidar of 1572nm wavelength is fixed on off wavelength, it is ensured that Atmospheric CO2To swashing
The influence of optical radar signal is minimum, obtains the laser radar signal that can most reflect current atmospheric situation.
Since the laser radar of dual wavelength belongs to two systems, must there are respective emission system, reception system and acquisition
System, echo-signal are different in signal strength, geometric overlap factor (overlap) height of sustained height, it is therefore necessary to
Determine the correlation of dual-wavelength lidar signal, specific method is as follows:
(1) overlap height of the dual-wavelength lidar signal in different height is determined, with the maximum of overlap height
Value, as the starting point for calculating related coefficient, using the height of 3km as the terminal for calculating related coefficient.
(2) the laser radar signal intensity of dual wavelength is normalized.
(2) correlation coefficient r is calculated:
Wherein, P1,iIt is the 1064nm wavelength laser radar signal strengths after normalization,For P1,iMean value;P2,iTo return
1572nm wavelength laser radar signal strengths after one change,For P2,iMean value;N is number of data points.
If r >=0.96, then it is assumed that the two is highly relevant, can be used for carrying out under calculating dual wavelength between Aerosol Extinction
Relationship.Conversely, it is then unsatisfactory for correcting experiment demand under current atmospheric situation.
By taking Wuhan Area as an example, the extinction coefficient of aerosol and the aerosol particle concentration height phase more than its wavelength dimension
It closes, according to the aerosol particle concentration observed result of Wuhan Area, larger fluctuation will not occur in a short time, therefore, reason
By above thinking, in the observation of a laser radar the whole night, 1064nm wavelength and the corresponding extinction coefficient of 1572nm wavelength have height
Spend correlation.
Fernald laser radar methods are by the Fernald inverting Aerosol Extinctions proposed and backscattering coefficient
Algorithm does not need to be accurately obtained laser radar scaling constant.Using the Fernald laser radars method of inversion to 1064nm and
The laser radar distribution of results of 1572nm wavelength carries out inverting, obtains the Aerosol Extinction of corresponding wavelength, and calculate acquisition
The linear empirical relationship of the two.
Since the ratio of extinction coefficient and backscattering coefficient is Lidar Ratios, and in shorter height, it is believed that laser
Radar ratio is definite value, rule of thumb formula, and the Lidar Ratios of Wuhan Area 532nm wavelength are the laser of 50,1572nm wavelength
Radar ratio is 63.
Finally, the differential absorption lidar CO of conventional dual wavelength alternate emission is carried out2During detection, 1064nm wavelength is carried out
Mie scattering lidar continuous probe, utilize the corresponding aerosol of Fernald laser radar method of inversion inverting 1064nm wavelength
Extinction coefficient.According to the echo-signal that Mie theory, Mie scattering lidar receive, reflection is identical with launch wavelength
Or the situation of the atmospheric aerosol more than launch wavelength.There is a situation where larger air changes or air quality variation
Under, according to the delustring system of the corresponding aerosol of the linear empirical relationship of extinction coefficient and backscattering coefficient acquisition 1572nm wavelength
Number and backscattering coefficient.Since the difference of on wavelength and off wavelength is usually less than 0.2nm, on wavelength and off wavelength
Corresponding extinction coefficient and backscattering coefficient share the corresponding extinction coefficient of 1572nm wavelength and backscattering coefficient.1572nm
The corresponding extinction coefficient of wavelength and backscattering coefficient substitute into CO2Retrieving concentration model, you can obtain more accurate difference and inhale
Receive laser radar CO2Retrieving concentration result.
Claims (1)
1. a kind of differential absorption lidar CO based on aerosol disturbance correction2Detection method, it is characterized in that, including:
Step 1, consider the influence of aerosol disturbance, propose the CO based on aerosol disturbance correction2Retrieving concentration model:
,
Wherein,For CO2Concentration at height r;Δ r represents air layer thickness, Δ r=r2-r1, r1For lower height,
r2For high height, WithCO under on wavelength and off wavelength at respectively height r2Gas
The absorption cross section of body;α(r,λon) and α (r, λoff) it is respectively gas when on wavelength and off wavelength laser radars are used at height r
The extinction coefficient of colloidal sol;β(r1,λon) and β (r1,λoff) it is respectively height r1When place is using on wavelength and off wavelength laser radars
The backscattering coefficient of aerosol;β(r2,λon) and β (r2,λoff) it is respectively height r2Place is using on wavelength and off wavelength lasers
The backscattering coefficient of aerosol during radar;P(r1,λon) and P (r1,λoff) represent on wavelength and off wavelength in height r respectively1
Echo signal intensity;P(r2,λoff) and P (r2,λon) represent on wavelength and off wavelength in height r respectively2Echo-signal it is strong
Degree;
Step 2, the Mie scattering lidar detection of 1064nm wavelength is carried out, obtains echo of the Mie scattering lidar in each height
Signal strength;Meanwhile by CO2Detection differential absorption lidar launch wavelength is fixed as off wavelength and is detected, and obtains
1572nm wavelength Mie scattering lidar is in the echo signal intensity of each height;Utilize Fernald laser radar method of inversion invertings
The extinction coefficient of aerosol, it is linear to be fitted to obtain the linear empirical relationship of extinction coefficient under two wavelength;
Step 3, with reference to Lidar Ratios and the extinction coefficient of step 2 inverting, the backscattering coefficient of aerosol is obtained, it is linear
It is fitted to obtain the linear empirical relationship of backscattering coefficient under two wavelength;
Step 4, the differential absorption lidar CO of on and off dual wavelength alternate emissions is carried out2During detection, using 1064nm wavelength
Mie scattering lidar continuous probe, disappeared using aerosol under Fernald laser radar method of inversion inverting 1064nm wavelength
Backscatter extinction logarithmic ratio, while obtain corresponding backscattering coefficient;With reference to the linear empirical relationship of extinction coefficient and backscattering coefficient, obtain
The extinction coefficient and backscattering coefficient of aerosol under 1572nm wavelength, by the moment by the extinction coefficient under 1572nm wavelength and
Backscattering coefficient divides on wavelength or extinction coefficient and backscattering coefficient under off wavelength;
Step 5, the extinction coefficient under on wavelength and off wavelength and backscattering coefficient are brought into CO2Retrieving concentration model obtains
CO2Retrieving concentration result.
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CN108267725B (en) * | 2018-03-20 | 2021-09-14 | 武汉大学 | CO of multi-wavelength laser radar2Concentration hierarchical inversion method and system |
CN108426856B (en) * | 2018-03-26 | 2019-09-10 | 武汉大学 | Assess laser radar Satellite observation Atmospheric CO2The overall analysis system of concentration performance |
CN109655843A (en) * | 2019-01-16 | 2019-04-19 | 武汉大学 | Detect the pulsed infrared Differential Absorption Laser Radar System of gas concentration lwevel profile |
CN110850393B (en) * | 2019-10-31 | 2023-01-31 | 无锡中科光电技术有限公司 | Laser radar data verification method |
CN111665218B (en) * | 2020-05-21 | 2021-07-02 | 武汉大学 | Method for improving inversion accuracy of carbon dioxide differential absorption laser radar |
CN115201074B (en) * | 2022-06-30 | 2023-03-17 | 中国科学院大气物理研究所 | Method, system, device and computer-readable storage medium for remote sensing inversion of aerosol component distribution |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7755041B2 (en) * | 2005-11-15 | 2010-07-13 | University Of South Florida | Optical and laser differential absorption remote detection of TATP peroxide based explosives |
CN103293117A (en) * | 2013-05-03 | 2013-09-11 | 中国科学院合肥物质科学研究院 | Inversion method of micro-pulse differential absorption lidar water vapor spatial and temporal distribution |
CN103868836A (en) * | 2014-04-03 | 2014-06-18 | 中国科学院合肥物质科学研究院 | Method for measuring backscattering coefficient of atmospheric particulates and ozone concentration profile simultaneously |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
SE0502396L (en) * | 2005-10-31 | 2007-04-17 | Totalfoersvarets Forskningsins | Laser source for the infrared wavelength range |
-
2016
- 2016-01-18 CN CN201610031555.1A patent/CN105510260B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7755041B2 (en) * | 2005-11-15 | 2010-07-13 | University Of South Florida | Optical and laser differential absorption remote detection of TATP peroxide based explosives |
CN103293117A (en) * | 2013-05-03 | 2013-09-11 | 中国科学院合肥物质科学研究院 | Inversion method of micro-pulse differential absorption lidar water vapor spatial and temporal distribution |
CN103868836A (en) * | 2014-04-03 | 2014-06-18 | 中国科学院合肥物质科学研究院 | Method for measuring backscattering coefficient of atmospheric particulates and ozone concentration profile simultaneously |
Non-Patent Citations (3)
Title |
---|
二氧化硫-臭氧-气溶胶多波长差分吸收激光雷达同时观测;曹念文 等;《光学技术》;20150731;第41卷(第4期);第289-295页 * |
地基CO2廓线探测差分吸收激光雷达;韩舸 等;《物理学报》;20151231;第64卷(第24期);第244206页 * |
连续波差分吸收激光雷达测量大气CO2;刘豪 等;《物理学报》;20141231;第63卷(第10期);第104214页 * |
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