CN105067564B - A kind of optical fiber gas concentration detection method with temperature compensation capability - Google Patents
A kind of optical fiber gas concentration detection method with temperature compensation capability Download PDFInfo
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Abstract
The present invention provides a kind of optical fiber gas concentration detection method with temperature compensation capability, and process is:One, laser produces the optical signal that two centre wavelengths are λ 1 and λ 2;Two, optical signal is divided into after two beams after being transmitted through optical fiber by optical splitter, passes through the reference gas chamber and the detection air chamber for the under test gas that is stored with of the reference gas that is stored with respectively;Three, repeatedly measurement is by reference gas chamber and the intensity of spectral line for detecting air chamber emergent light;Step 4, linear fit is carried out to described the intensity of spectral line, obtains the temperature influence fitting coefficient of the monochromatic absorption coefficient of light of two kinds of wavelength;Five, according to fitting coefficient, calculate the gas concentration after temperature-compensating.This method establishes the model of temperature compensation of fiber-optic fiber gas detecting system, realize the fiber-optic fiber gas detecting system for considering temperature change factor, suppressed by way of temperature-compensating variation of ambient temperature to detection band come interference, reduce the accuracy of detection that system is improved due to the measurement error that variation of ambient temperature is introduced.
Description
Technical field
The present invention relates to a kind of gas concentration detection method, and in particular to a kind of gas concentration with temperature compensation capability
Detection method, belongs to technical field of optical fiber detection.
Background technology
Industry spot operation be typically under the environmental condition of high temperature, high-moisture, high dust, severe corrosive and high flow rate,
The detection that reliable, safety development depends particularly on rapidly and accurately progress gas concentration that continues to field operation.
Although traditional non-optical gas detecting instrument can reach relatively low test limit, it is easy to by other gases
The intersection of composition is sensitive, and its response speed is slower, and repeatable utilization rate is low, and service life is shorter, it is difficult to which real-time continuous is examined
Survey.To overcome these defects, Diode Laser Absorption Spectroscopy (TDLAS technologies) employs " single line spectrum " technology of uniqueness
With modulated spectrum technology, it can not be disturbed by background gas cross jamming and dust, form pollution, therefore will can test and analyze
Equipment is directly installed on measure field, realizes that the live on-line continuous gas that other spectral absorption technologies can not or be difficult to realize is surveyed
Amount.
Currently for industry spot fiber-optic fiber gas detection, typically using under test gas fiber transparent window (0.8~
1.7 μm) in absworption peak, measure by gas absorb produce light intensity attenuation, so as to deduce out the concentration of under test gas.Specifically adopt
With the method for harmonic detecting, noise spectra of semiconductor lasers light source carries out sinusoidal signal (or triangular wave) and modulated, and modulated optical signal
Harmonic components are directly proportional after being absorbed through gas to gas concentration, by detecting that these harmonic components just can obtain the dense of under test gas
Spend information.The influence for the absorption coefficient change that the change that above-mentioned detection method have ignored under test gas environment temperature is brought.It is real
On border, in actual measuring environment, the change of under test gas environment temperature produces shadow to processes such as rotation, the vibrations of gas molecule
Ring, so as to cause the change of absorption coefficient, influence the detection of gas concentration.Therefore, needed while gas concentration is detected true
Determine the residing environment temperature of gas, the concentration to correct tested gas.How to determine gaseous absorption line with measuring environment temperature
The characteristic of degree change makes it possible to measure the concentration of gas in the environment of temperature change, fails solution very well always.
The content of the invention
In view of this, the present invention provides a kind of optical fiber gas concentration detection method with temperature compensation capability, using this
Method can be directed to traditional dual-wavelength difference gas detection mode, set up the mathematical modeling of temperature-compensating to remove temperature factor
Influence to absorption coefficient, so as to eliminate the error of the introduced gas concentration detection of temperature change, obtains higher detection essence
Degree.
Realize that technical scheme is as follows
A kind of optical fiber gas concentration detection method with temperature compensation capability, detailed process is:
Step one, laser produces the optical signal that two centre wavelengths are λ 1 and λ 2, the suction of wherein λ 1 correspondence under test gas
Receive peak, the absworption peak of the correspondence reference gases of λ 2;
Step 2, optical signal is divided into after two beams after being transmitted through optical fiber by optical splitter, passes through the reference gas that is stored with respectively
Reference gas chamber and the detection air chamber of under test gas of being stored with;
Step 3, repeat step two, repeatedly measurement is by reference gas chamber and the intensity of spectral line for detecting air chamber emergent light;
Step 4, linear fit is carried out using formula (1) to described the intensity of spectral line, is obtained monochromatic absorb of wavelength X 1 and is
Number temperature influence fitting coefficient a1, b1, c1, obtain the monochromatic absorption coefficient temperature influence fitting coefficient a of wavelength X 22, b2, c2;
S=a+bT-1+cT-2 (1)
Wherein, T is the environment temperature in air chamber;
Step 5, according to fitting coefficient, the gas concentration after temperature-compensating is calculated using formula (2);
Wherein, l represents light path, and n is temperature coefficient, and I (λ 1) is the monochromatic harmonic wave light intensity of wavelength X 1, and I (λ 2) is wavelength X
2 monochromatic harmonic wave light intensity, T0For reference temperature 296k, γ0For temperature T0Half high half-breadth of lower Absorption Line, k is that Boltzmann is normal
Amount, P is the pressure of under test gas.
Beneficial effect
This method establishes the model of temperature compensation of fiber-optic fiber gas detecting system, realizes the light for considering temperature change factor
Fine gas concentration detection system, suppressed by way of temperature-compensating variation of ambient temperature to gas concentration detection band come it is dry
Disturb, reduce the accuracy of detection that system is improved due to the measurement error that variation of ambient temperature is introduced.
The detection method can effectively suppress interference of stray light and signal noise, eliminate the light such as source device output optical power shakiness
The interference of temperature factor is also eliminated while the factor influence of road.
Brief description of the drawings
Fig. 1 is the flow chart of detection method;
Fig. 2 is the schematic diagram of this example detection process;
Fig. 3 is the schematic diagram of this example temperature compensation procedure.
Embodiment
The present invention will now be described in detail with reference to the accompanying drawings and examples.
The present embodiment provides a kind of optical fiber gas concentration detection method with temperature compensation capability, by being absorbed to gas
The intensity of spectral line of line is fitted, on carrying out temperature-compensating, suppression because of the gas concentration detection error influence that temperature change is brought
The interference that variation of ambient temperature processed is come to detection band, so as to accurately obtain the concentration of tested gas.
As shown in figure 1, a kind of optical fiber gas concentration detection method with temperature compensation capability of the present invention, detailed process
For:
Step one, laser produces the optical signal that two centre wavelengths are λ 1 and λ 2, the suction of wherein λ 1 correspondence under test gas
Receive peak, the absworption peak of the correspondence reference gases of λ 2;
Step 2, optical signal is divided into after two beams after being transmitted through optical fiber by optical splitter, passes through the reference gas that is stored with respectively
Reference gas chamber and the detection air chamber of under test gas of being stored with;
Step 3, repeat step two, repeatedly measurement is by reference gas chamber and the intensity of spectral line for detecting air chamber emergent light;
Step 4, linear fit is carried out using formula (1) to described the intensity of spectral line, is obtained monochromatic absorb of wavelength X 1 and is
Number temperature influence fitting coefficient a1, b1, c1, obtain the monochromatic absorption coefficient temperature influence fitting coefficient a of wavelength X 22, b2, c2;
S=a+bT-1+cT-2 (1)
Wherein, T is the environment temperature in air chamber;
Step 5, according to fitting coefficient, the gas concentration after temperature-compensating is calculated using formula (2);
Wherein, l represents light path, and n is temperature coefficient, and I (λ 1) is the monochromatic harmonic wave light intensity of wavelength X 1, and I (λ 2) is wavelength X
2 monochromatic harmonic wave light intensity, T0For reference temperature 296k, γ0For temperature T0Half high half-breadth of lower Absorption Line, k is that Boltzmann is normal
Amount, P is the pressure of under test gas.
Influence of the temperature to absorption coefficient is taken into full account in formula (2) of the present invention, by the mathematics for setting up temperature-compensating
Model is to remove influence of the temperature factor to absorption coefficient, compared to existing detection method, the gas that the inventive method is detected
Concentration has higher accuracy of detection.
The derivation to formula (1) and formula (2) is described in detail below:
Be separated by with two wavelength Xs 1 and λ 2 extremely closely (has very big difference on absorption coefficient:Wherein λ 1 absorbs under test gas
On peak, and under test gas absorbs very weak to λ 2 or not absorbed, while also to avoid the absorption of other non-under test gas molecules etc.)
Monochromatic light is simultaneously or difference very short time is interior by under test gas, and light intensity, which is divided by, to be obtained:
Wherein, l represents light path;
Under wavelength X 1, λ 2, such as the absorption coefficient (λ 1) of gas, α (λ 2) can be obtained by calibrating gas measurement,
Then under the conditions of of the same race, the concentration of under test gas can just be obtained by measuring harmonic wave light intensity I (λ 1) and I (λ 2).
However, according to the broadening principle of spectrum line, absorption coefficient changes as ambient temperature changes.Therefore, merely
By measuring the intensity of second harmonic, if not considering the influence of temperature change, it is impossible to accurately obtain surveyed gas concentration.By
In the method using second-harmonic detection, mainly need to consider the compensation effect of second harmonic when carrying out temperature-compensating, its is right
The dependence of temperature can directly result in the deviation of measurement result, it is thus necessary to determine that dependence of the second harmonic for temperature.
Utilization index Function Fitting absorption coefficient:
Density of gas molecules, the line strength of Absorption Line in absorption coefficient and unit volume at gaseous absorption line centre frequency
It is relevant with half high half-breadth of Absorption Line, it can be expressed as:
In formula, N is the density of gas molecules (mol/cm in unit volume3), S is the intensity of spectral line (cm of Absorption Line-1/
(mol·cm3)), γ is half high half-breadth (cm of Absorption Line-1)。
According to the pressure formula of perfect gas, the analytic density of the under test gas in unit volume is:
In formula, P is the pressure of under test gas, and k is Boltzmann constant, and T is thermodynamic temperature.
Pressure does not change during due to detection, and half high half-breadth of Absorption Line is relevant with temperature, and the half of different temperatures Absorption Line
High half-breadth can be expressed as:
In formula, T0、γ0Temperature value and the high half-breadth of Absorption Line half during respectively reference temperature 296k;N is temperature coefficient.
Have:
Variation with temperature, gas absorption spectrum line strength also changes, and gas absorption spectrum line strength can be expressed as into temperature
The function of degree:
NcFor Loschmidt constants, unit is cm-3;E and meRespectively quantities of charge and quality;C is the light velocity;Q (T) is
Molecular partition function;H is Planck (Planck) constant;K is Boltzmann constant;G, W, f be respectively decay factor, energy and
Oscillation intensity.
The intensity of spectral line in view of Absorption Line reduces with the rise of temperature, is fitted, obtained with second order polynomial:
S=a+bT-1+cT-2 (1)
Wherein, a, b, c are fitting coefficient respectively.It can be marked by repeatedly measuring the intensity of spectral line with the numerical relation of temperature
Surely the coefficient is fitted.
Then absorption coefficient temperature influence model is represented by:
α=∈ (aTn-1+bTn-2+cTn-3)
Wherein,For a constant.
Then, it is considered to which the gas concentration (namely model of temperature compensation) after temperature factor of influence is:
Wherein, a1, b1, c1Fitting coefficient is influenceed for the monochromatic absorption coefficient temperature of wavelength X 1;
a2, b2, c2Fitting coefficient is influenceed for the monochromatic absorption coefficient temperature of wavelength X 2;
Due to a1, a2, b1, b2, c1, c2, it is known that being therefore that can obtain temperature by the above-mentioned formula with temperature-compensating
Gas concentration after compensation.
When under test gas is influenceed by variation of ambient temperature, it is the concentration of accurate measurement under test gas, need to be mended by temperature
Repay and suppress the interference that variation of ambient temperature is come to detection band.System gathers gas indoor environment temperature using temperature sensor, to not
The synthermal lower obtained gas concentration that measures carries out temperature-compensating.
Example:
Based on existing bipolar electrode DFBLD Difference Absorption detecting system, as shown in Fig. 2 signal generator produces sine
Ripple, is modulated by the Injection Current for adjusting laser to its output wavelength.By changing two electrodes of semiconductor laser
The current ratio of input, produces the optical signal that two centre wavelengths are λ 1 and λ 2, and λ 2 is reference light, and the correspondence gas molecules of λ 1
Absworption peak, intensity approximately equal.From the light of DFBLD outgoing through optoisolator to fiber coupler, be coupled to light in optical fiber by
Beam splitter is divided into two beams, and light beam is by reference to air chamber to PIN detector, after PIN output signals are mutually amplified through lock, for feeding back
Control the Injection Current of laser, the output frequency of stable laser;Another light beam is by detecting air chamber, to another photodetection
Device, output signal lock is used for the concentration for obtaining under test gas after mutually amplifying.The output light of detection air chamber and reference gas chamber is through photoelectricity
Detector is converted into electric signal, extracts their second harmonic signal by differential mode with lock-in amplifier, then by two
Second harmonic signal feeding divider carries out ratio output, and output quantity carries the gas concentration information containing temperature factor of influence.
According to the model of temperature compensation for above setting up gas concentration, the interference shadow of temperature fluctuation can be eliminated by the method for temperature-compensating
Ring, while also eliminating due to the measurement error that light source fluctuation and external environment influence are caused.
As shown in figure 3, detailed process is:
1. gather the environment temperature in air chamber with temperature sensor;
2. many measurement the intensity of spectral line;
3. second order polynomial fit is carried out to the intensity of spectral line using formula (1)
4. λ 1 is obtained, the temperature influence fitting coefficient of the wavelength of λ 2;
5. gas concentration C (T) is calculated by model of temperature compensation;
The signal of reacting gas concentration through above-mentioned processing is admitted to signal processing device and postponed, at input computer
Reason, display and printing.
In summary, presently preferred embodiments of the present invention is these are only, is not intended to limit the scope of the present invention.
Within the spirit and principles of the invention, any modification, equivalent substitution and improvements made etc., should be included in the present invention's
Within protection domain.
Claims (1)
1. a kind of optical fiber gas concentration detection method with temperature compensation capability, it is characterised in that detailed process is:
Step one, the optical signal that two centre wavelengths of laser generation are λ 1 and λ 2, the absworption peak of wherein λ 1 correspondence under test gas,
The absworption peak of the correspondence reference gases of λ 2;
Step 2, optical signal is divided into after two beams after being transmitted through optical fiber by optical splitter, passes through the ginseng for the reference gas that is stored with respectively
Examine the detection air chamber of air chamber and the under test gas that is stored with;
Step 3, repeat step two, repeatedly measurement is by reference gas chamber and the intensity of spectral line for detecting air chamber emergent light;
Step 4, linear fit is carried out using formula (1) to described the intensity of spectral line, obtains the temperature of the monochromatic absorption coefficient of light of wavelength X 1
Degree influence fitting coefficient a1, b1, c1, obtain the temperature influence fitting coefficient a of the monochromatic absorption coefficient of light of wavelength X 22, b2, c2;
S=a+bT-1+cT-2 (1)
Wherein, T is the environment temperature in air chamber;
Step 5, according to fitting coefficient, the gas concentration after temperature-compensating is calculated using formula (2);
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Wherein, l represents light path, and n is temperature coefficient, and I (λ 1) is the monochromatic harmonic wave light intensity of wavelength X 1, and I (λ 2) is that wavelength X 2 is single
The harmonic wave light intensity of coloured light, T0For reference temperature 296k, γ0For temperature T0Half high half-breadth of lower Absorption Line, k is Boltzmann constant,
P is the pressure of under test gas.
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2014016313A (en) * | 2012-07-11 | 2014-01-30 | Fuji Electric Co Ltd | Laser type gas analyzer |
CN103592253A (en) * | 2013-11-06 | 2014-02-19 | 安徽皖仪科技股份有限公司 | Laser gas analyzer for precise temperature compensation in concentration of gas to be measured |
CN103592261A (en) * | 2013-11-20 | 2014-02-19 | 天津大学 | All-fiber temperature compensating gas sensor and compensating method thereof |
CN104483380A (en) * | 2014-12-19 | 2015-04-01 | 郑州光力科技股份有限公司 | Temperature-compensation-based ultrasonic wave gas concentration measurement method and temperature-compensation-based ultrasonic wave gas concentration measurement device |
CN104535531A (en) * | 2014-12-15 | 2015-04-22 | 北京航天易联科技发展有限公司 | Handheld laser gas concentration monitor and control method thereof |
-
2015
- 2015-07-14 CN CN201510413838.8A patent/CN105067564B/en not_active Expired - Fee Related
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2014016313A (en) * | 2012-07-11 | 2014-01-30 | Fuji Electric Co Ltd | Laser type gas analyzer |
CN103592253A (en) * | 2013-11-06 | 2014-02-19 | 安徽皖仪科技股份有限公司 | Laser gas analyzer for precise temperature compensation in concentration of gas to be measured |
CN103592261A (en) * | 2013-11-20 | 2014-02-19 | 天津大学 | All-fiber temperature compensating gas sensor and compensating method thereof |
CN104535531A (en) * | 2014-12-15 | 2015-04-22 | 北京航天易联科技发展有限公司 | Handheld laser gas concentration monitor and control method thereof |
CN104483380A (en) * | 2014-12-19 | 2015-04-01 | 郑州光力科技股份有限公司 | Temperature-compensation-based ultrasonic wave gas concentration measurement method and temperature-compensation-based ultrasonic wave gas concentration measurement device |
Non-Patent Citations (2)
Title |
---|
Noise characteristics of MEMS gyro’s null drift and temperature compensation;Shiau Jaw-Kuen, et al;《Journal of Applied Science and Engineering》;20121231;第239-246页 * |
可调谐半导体激光吸收光谱式甲烷传感器温度补偿技术;樊荣 等;《煤炭学报》;20150131;第40卷(第1期);第226-231页 * |
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