CN109765185A - A kind of Laser Photoacoustic Spectroscopy detection device using single photoacoustic cell measurement multicomponent gas - Google Patents

A kind of Laser Photoacoustic Spectroscopy detection device using single photoacoustic cell measurement multicomponent gas Download PDF

Info

Publication number
CN109765185A
CN109765185A CN201910060515.3A CN201910060515A CN109765185A CN 109765185 A CN109765185 A CN 109765185A CN 201910060515 A CN201910060515 A CN 201910060515A CN 109765185 A CN109765185 A CN 109765185A
Authority
CN
China
Prior art keywords
gas
photoacoustic cell
wavelength
quantum cascade
laser
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.)
Granted
Application number
CN201910060515.3A
Other languages
Chinese (zh)
Other versions
CN109765185B (en
Inventor
陈伟根
万福
王有元
杨天荷
王品一
杜林�
谭亚雄
李剑
黄正勇
王飞鹏
周湶
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.)
Beijing Baif Maihak Analytical Instrument Co ltd
Chongqing University
Original Assignee
Chongqing University
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 Chongqing University filed Critical Chongqing University
Priority to CN201910060515.3A priority Critical patent/CN109765185B/en
Publication of CN109765185A publication Critical patent/CN109765185A/en
Application granted granted Critical
Publication of CN109765185B publication Critical patent/CN109765185B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

A kind of optoacoustic spectroscopy detection device using single photoacoustic cell measurement multicomponent gas, the device includes shut-off valve (1), particulate matter filter device (2), gas drier (3), electromagnetic switch valve one (4), pressure sensor (5), electromagnetic switch valve two (6), sonic nozzle (7), vacuum pump (8), quantum cascade laser array module (9), spectroscope module (10), reference gas chamber (11) to be measured, difference resonates photoacoustic cell (12), acoustic-electric conversion module (13), insulating box (14), optical power detector (15), delustring pond (16), locking phase amplifying circuit (17) and industrial personal computer (18);Multiple laser is coupled in a branch of optical path by the quantum cascade laser array module (9).The arrangement achieves single photoacoustic cells to measure various faults gas composition simultaneously.With strong antijamming capability, equipment long-time stability are good, and precision is high, later period non-maintaining advantage, it can be achieved that measurement trace gas to 100% concentration gases.

Description

A kind of Laser Photoacoustic Spectroscopy detection device using single photoacoustic cell measurement multicomponent gas
Technical field
The invention belongs to optoacoustic spectroscopy gas detection technology fields, more particularly in a kind of electric power, nuclear energy, petrochemical industry The on-line monitoring or off-line detection device of characteristic gas component.
Background technique
It can be decomposed inside the equipment such as power transformer, GIS in electric power/nuclear energy industry and generate the various nature of trouble and absolutely of capable of reacting The gas of edge ageing properties;Accurate detection failure and aging character gas are to realize that important transformer equipment operating status diagnoses It is crucial;The raw material of the basic chemical industries such as ethyl alcohol material and fine chemical product is mainly natural gas, accurate real-time monitoring raw material and production Gas component and content in the process are the cores for guaranteeing above-mentioned quality of chemical products.Accurate detection CO, CO in real time2、CH4(first Alkane), C2H4(ethylene), C2H6(ethane), C2H2(acetylene), H2、SO2F2(bifluoride sulfonyl), CF4(carbon tetrafluoride), SO2、H2S and The gases such as COS (hydroxyl sulphur) are to ensuring that it is important that the industry devices such as electric power, nuclear energy, petrochemical industry operational safety or product quality have Meaning.Traditional detection method has chromatography, electrochemical sensor method, nano-sensor method, absorption spectrometry etc..Wherein chromatography Method needs timing replacement chromatographic column, increases testing cost and manpower loss, cannot achieve the long-term on-line monitoring of equipment;Electrochemistry The gaseous species of sensor method detection and sensitivity are all limited;Nano-sensor method poor repeatability is never effectively solved Certainly.Spectroscopic methodology detection gas is novel detection method popular in recent years, wherein shadow of the absorption spectrometry vulnerable to light scattering, refraction It rings, needs the absorption cell of long light path, and higher cost;Structure is complicated for FTIR spectrum method, and quantitative analysis accuracy needs It improves;Raman spectroscopy detection sensitivity is lower, can not detect trace gas.Optoacoustic spectroscopy detection is a kind of no background measurement side Method, the not influence of light scattering have wide application market in field of gas detection.Its core component is mainly by light source, light The module compositions such as sound conversion pool, acoustical-electrical transducer, ambient noise deduction.But traditional photocaustic spectroscopy shakes vulnerable to ambient enviroment Dynamic, noise, temperature change interference, and the resonant frequency for the photoacoustic cell that resonates can generate drift because of the variation of photoacoustic cell internal gas component It moves.When long-term measurement, impurity and corrosive gas under test gas can pollute corrosion microphone, influence its acoustic characteristic.
The interference that difference type photoacoustic cell can effectively weaken ambient enviroment vibration, noise, temperature change are brought, and under test gas is not It is contacted with acoustical-electrical transducer, it is possible to prevente effectively from the corrosion to acoustical-electrical transducer.Resonance photoacoustic cell can be formed pair in photoacoustic cell The standing wave of photoacoustic signal amplifies, and further increases the detection sensitivity of system, and cylinder resonance photoacoustic cell presses standing wave distribution mode Difference can be divided into longitudinal, angular, radial three kinds of resonance modes, wherein working in the resonance photoacoustic cell pond of longitudinal resonance mode Constant highest is most obvious to the standing wave enlarge-effect of photoacoustic signal.But traditional difference type photoacoustic cell is mostly using single photoacoustic cell Cooperate the mode of single laser, difference type photoacoustic cell is only filled with a kind of calibrating gas of component to be detected, is only able to satisfy single gas The detection of body, system structure can become extremely complex when detection gas type is more.
Summary of the invention
The technical problem to be solved in the present invention is to provide a kind of on-line monitoring or offline inspection electric power, nuclear energy, petrochemical industries The device of middle characteristic gas component can carry out real-time online prison to electric power, nuclear energy, petrochemical industry characteristic gas component content Survey or offline inspection have while monitoring Multicomponent, do not consume carrier gas, is pollution-free, strong antijamming capability, apparatus simplified, inspection Survey high sensitivity, it is non-maintaining the features such as.The present invention is the mode using quantum cascade laser array, and multiple laser is coupled to In a branch of optical path, and it is real by way of the ratio preliminary filling certain concentration multicomponent gas being absorbed in photoacoustic cell according to gas The function of single difference resonance type photoacoustic cell measurement multicomponent gas is showed.
The technical scheme is that electric power, nuclear energy, petrochemical industry characteristic gas component on-line monitoring or offline inspection system System, it is connected on equipment characteristic gas air hatch to be monitored or extracts the process gas in process of producing product when detection, Particulate matter filter device, gas drier, electromagnetic switch valve one, pressure sensor, reference to be measured are sequentially connected on shut-off valve Gas chamber, electromagnetic switch valve two, sonic nozzle, vacuum pump, characteristic gas to be detected pass sequentially through above-mentioned module and eventually by true Sky pump discharge;Detection device includes quantum cascade laser array module, spectroscope module, reference gas chamber to be measured, difference resonance Photoacoustic cell, acoustic-electric conversion module, insulating box, optical power detector, delustring pond, locking phase amplifying circuit and industrial personal computer.
Above-mentioned quantum cascade laser array module include laser driving and temperature control module, quantum cascade laser array, Light path calibration laser, all-wave length total reflective mirror, specific wavelength total reflective mirror, each quantum cascade laser can be inspired for single Or the super-narrow line width laser of various features gas component absorption peak, and after being focused by condenser lens by specific wavelength total reflective mirror with All-wave length total reflective mirror is injected in spectroscope module after converging to same optical path, the optoacoustic generated by the laser to different wave length Signal carries out the concentration that detection can be finally inversed by each component gas.Light path calibration laser is the laser of naked eyes visible wavelength, same Sample is by injecting spectroscope module after specific wavelength total reflective mirror and the convergence of all-wave length total reflective mirror, for calibrating quantum cascade laser The optical path of array module is not used in excitation under test gas and generates photoacoustic signal, and light path calibration laser is 0.38 μm -0.78 μm of wavelength Visible light.Laser driving and temperature control module can freely adjust the size of electric current, output voltage range according to the actual situation 0-20V exports electric current 0-1A, and current stability is better than 0.1mA, kHz modulation output can be realized as needed, in conjunction with semiconductor system Cooler (TEC) realizes chip temperature control, precisely adjusts chip wavelength.Laser driving and temperature control module in each laser it Between switched over using analog switch mode, to realize different wavelength output.
Above-mentioned quantum cascade laser array can realize that single laser detects the function of more gas compositions, in which:
1) for when detecting electric power, nuclear energy transformer:
The tunable wave length range of the quantum cascade laser one of configuration is 7.10 μm -7.38 μm, and wavelength covers C2H4、CH4、 C2H2The characteristic absorption peak of three kinds of gas, selected C2H4、CH4、C2H2Gas characteristic absorption peak wavelength is located at 7.10 μm, 7.38 μm,7.37μm;
The tunable wave length range of the quantum cascade laser two of configuration is 4.34 μm -4.54 μm, and wavelength covers CO, CO2Two kinds The characteristic absorption peak of gas, selected CO, CO2Gas characteristic absorption peak wavelength is located at 4.54 μm, 4.34 μm;
The wavelength of the quantum cascade laser three of configuration is 3.35 μm, covers C2H6The characteristic absorption peak of gas, selected C2H6Gas Characteristic absorption peak wavelength is located at 3.35 μm.
2) for detecting electric power GIS equipment SF6When decomposing gas:
The wavelength of the quantum cascade laser one of configuration is 7.07 μm, and wavelength covers H2The characteristic absorption peak of S gas, selected H2S Gas characteristic absorption peak wavelength is located at 7.07 μm;
The tunable wave length range of the quantum cascade laser two of configuration is 4.34 μm -4.54 μm, and wavelength covers CO, CO2Two kinds The characteristic absorption peak of gas, selected CO, CO2Gas characteristic absorption peak wavelength is located at 4.54 μm, 4.34 μm;
The tunable wave length range of the quantum cascade laser three of configuration is 7.43 μm -7.87 μm, and wavelength covers SO2、CF4、 SO2F2The characteristic absorption peak of three kinds of gas, selected SO2、CF4、SO2F2Gas characteristic absorption peak wavelength be located at 7.43 μm, 7.79μm、7.87μm。
3) when for detecting gas in the control of petrochemical industry quality of natural gas:
The wavelength of the quantum cascade laser one of configuration is 7.07 μm -7.43 μm, and wavelength covers H2S、SO2The feature of two kinds of gas Absorption peak, selected H2S、SO2Gas characteristic absorption peak wavelength is located at 7.07 μm, 7.43 μm;
The wavelength of the quantum cascade laser two of configuration is 4.34 μm, and wavelength covers CO2The characteristic absorption peak of gas, selected CO2 Gas characteristic absorption peak wavelength is located at 4.34 μm;
The tunable wave length range of the quantum cascade laser three of configuration is 4.83 μm, and wavelength covers the characteristic absorption of COS gas Peak, selected COS gas characteristic absorption peak wavelength are located at 4.83 μm.
4) for detecting petrochemical industry methanol production equipment conversion combined coefficient monitoring gas:
The wavelength of the quantum cascade laser one of configuration is 7.54 μm, and wavelength covers CH4The characteristic absorption peak of gas, selected CH4 Gas characteristic absorption peak wavelength is located at 7.54 μm;
The tunable wave length range of the quantum cascade laser two of configuration is 4.34 μm -4.54 μm, and wavelength covers CO, CO2Two kinds The characteristic absorption peak of gas, selected CO, CO2Gas characteristic absorption peak wavelength is located at 4.54 μm, 4.34 μm;
Quantum cascade laser three can not be configured when detection petrochemical industry methanol production equipment conversion combined coefficient monitoring gas.
The upper spectroscope module includes one piece of semi-transparent semi-reflecting lens and one piece of total reflective mirror, by quantum cascade laser array mould The laser induced breakdown that block is injected is the identical laser of two beam energies.Semi-transparent semi-reflecting lens in spectroscope module are that broadband is semi-transparent semi-reflecting Mirror, or be made of the narrowband semi-transparent semi-reflecting lens turntable that driving motor controls, turntable converts certain wave according to the optical maser wavelength of transmitting The semi-transparent semi-reflecting lens of section.The angle of semi-transparent semi-reflecting lens and total reflective mirror can be manually adjusted by pedestal.
Above-mentioned reference gas chamber to be measured is the chamber of the two identical sizes hollowed out in a square piece, wherein gas chamber to be measured It is the container that under test gas enters detection device.And gas chamber to be measured and reference gas chamber interior walls are coated with gold or nickel, gas chamber to be measured and ginseng It is more identical than air cell size, diameter 5mm-50mm, length 0.1mm-200mm.The reference gas chamber N pure by one preliminary filling of capillary2、 He, Ar or air, in detection SF6It can the pure SF of preliminary filling when decomposing gas and natural gas component6, standard natural gas to be to offset background Interference of the gas absorption spectrum line to gas absorption spectrum line to be measured.
Above-mentioned difference resonance photoacoustic cell is single order longitudinal resonance photoacoustic cell, is the container that photoacoustic signal generates, material is brass Or stainless steel, it is assembled single piece after the chamber for digging out identical size respectively in two square pieces, and two sides The junction of shape part hollows out out the horn-like cavity that can place acoustic-electric conversion module, and the junction diameter of cavity and photoacoustic cell is 1mm-2mm is 10mm-20mm with acoustic-electric conversion module connected component diameter.Its material is brass or stainless steel, and in photoacoustic cell Wall is coated with gold or nickel, and photoacoustic cell diameter is in 5mm-10mm, and for length in 50mm-200mm, draw ratio is greater than or equal to 12:1, and light Sound pond works in first order resonant mode.Difference of the ratio of filled calibrating gas according to absorption peak absorption intensity selected by gas with various It matches, is respectively positioned in the flat response curve of acoustic-electric conversion module, is obtained with the photoacoustce signal intensity for guaranteeing that gas with various generates Obtain wide detection dynamic range.The photoacoustic spectrum signals that system generates may be expressed as:
Wherein S is the photoacoustic spectrum signals intensity generated, and P is excitation light power, and M is the sensitivity of acoustic-electric conversion module, CcellFor photoacoustic cell pond constant, ηiTo absorb the efficiency that luminous energy is converted into thermal energy, αiFor absorbent components rubbing under incentive optical wavelength That absorption coefficient of light, ciFor the concentration for absorbing component, AbFor the generation efficiency of background signal.When modulating frequency is lower than 10kHz, ηiIt can be approximately constant 1.In a determining system: sensitivity M, the photoacoustic cell of excitation light power P, acoustic-electric conversion module Pond constant CcellIt is definite value, therefore is in acoustic-electric conversion module to meet the photoacoustce signal intensity that each gas generates in photoacoustic cell In flat response curve, ciWith αiProduct should be definite value.Difference resonance photoacoustic cell combination above-mentioned theory basis and actual test Afterwards, by two preliminary filling electric power of inflating port, nuclear energy, petrochemical industry individual features gas composition calibrating gas, ratio system Number are as follows:
1) for when detecting electric power, nuclear energy transformer: difference resonance photoacoustic cell passes through two preliminary filling C of inflating port2H4、CH4、C2H2、 CO、CO2、C2H6And N2Seven kinds of gases.Wherein C2H4、CH4、C2H2、CO、CO2、C2H6Ratio it is directly proportional to its absorption coefficient, This six kinds of void fraction proportionality coefficients of preliminary filling are 700:70:50:5:5:1.
2) for detecting electric power GIS equipment SF6When decomposing gas: difference resonance photoacoustic cell passes through two preliminary filling H of inflating port2S、CO、 CO2、SO2、CF4、SO2F2And N2Seven kinds of gases.Wherein H2S、CO、CO2、SO2、CF4、SO2F2Ratio and its absorption coefficient at Direct ratio, this six kinds of void fraction proportionality coefficients of preliminary filling are 60000:80:80:120:1:10.
3) when for detecting gas in the control of petrochemical industry quality of natural gas: difference resonance photoacoustic cell passes through two preliminary filling H of inflating port2S、 SO2、CO2, COS and N2Five kinds of gases.Wherein H2S、SO2、CO2, the ratio of COS it is directly proportional to its absorption coefficient, preliminary filling this Four kinds of void fraction proportionality coefficients are 4000:10:5:1.
4) when for detecting petrochemical industry methanol production equipment conversion combined coefficient monitoring gas: difference resonance photoacoustic cell passes through inflating port Two preliminary filling CH4, CO, CO and N2Four kinds of gases.Wherein CH4、CO、CO2Ratio it is directly proportional to its absorption coefficient, preliminary filling this Three kinds of void fraction proportionality coefficients are 10:1:1.
Above-mentioned acoustic-electric conversion module is the capacitive microphone for detecting difference photoacoustic signal, sensitivity 30mV/Pa.
Above-mentioned insulating box is Resistant heating insulating box, for maintaining temperature in reference gas chamber to be measured and difference resonance photoacoustic cell At 50 DEG C.
Above-mentioned optical power detector is used to detect the power excursion of laser, and laser drift signal Real-time Feedback is driven to laser And temperature control module, by realizing laser driving and the adjustment of temperature control module parameter to quantum cascade laser array output wave Long and energy is modified.
Above-mentioned delustring pond is used to absorb the laser energy for being not used for excitation photoacoustic signal, be full of high concentration in delustring pond with light The congener gas composition in sound pond, and proportionality coefficient is identical with photoacoustic cell.
Above-mentioned locking phase amplifying circuit and industrial personal computer may filter that other than 1kHz-4kHz for extracting specific wavelength frequency signal Noise signal, the noise of conversion to input terminal is 50nV, temperature drift≤10ppm/ DEG C, the amplification factor of amplifier is adjustable model It encloses not less than 104
Detailed description of the invention
Some specific embodiments of the present invention is described in detail by way of example and not limitation below in reference to attached drawing.Attached drawing In identical appended drawing reference denote same or similar part or part.It should be appreciated by those skilled in the art that these attached drawings It is not necessarily drawn to scale.
Fig. 1 is optoacoustic spectroscopy detection device overall structure diagram of the invention.
Fig. 2 is that laser one detects C2H4、CH4、C2H2Wavelength schematic diagram selected by three kinds of gases.
Fig. 3 is that laser two detects CO, CO2Wavelength schematic diagram selected by two kinds of gases.
Fig. 4 is that laser three detects C2H6Wavelength schematic diagram selected by gas.
Appended drawing reference meaning is as follows in figure:
1- shut-off valve, 2- particulate matter filter device, 3- gas drier, 4- electromagnetic switch valve one, 5- pressure sensor, 6- electricity Magnetic switch valve two, 7- sonic nozzle, 8- vacuum pump, 9- quantum cascade laser array module, the driving of 91- laser and temperature control mould Block, 92- quantum cascade laser array, 921- laser one, 922- laser two, 923- laser three, 924- condenser lens One, 925- condenser lens two, 926- condenser lens three, 93- light path calibration laser, 94- all-wave length total reflective mirror, 95- specific wavelength Total reflective mirror one, 96- specific wavelength total reflective mirror two, 97- specific wavelength total reflective mirror three, 98- specific wavelength total reflective mirror four, 10- light splitting Mirror module, 101- semi-transparent semi-reflecting lens, 102- total reflective mirror, 11- reference gas chamber to be measured, 111- air inlet, 112- exhaust outlet, 113- window Mouth piece one, 114- diaphragm two, 115- diaphragm three, 116- diaphragm four, 117- gas chamber to be measured, 118- reference gas chamber, 119- Inflating port one, 12- difference resonance photoacoustic cell, 121- diaphragm five, 122- diaphragm six, 123- diaphragm seven, 124- diaphragm Eight, 125- photoacoustic cell one, 126- photoacoustic cell two, 127- inflating port two, 13- acoustic-electric conversion module, 131- acoustic-electric modulus of conversion block film Piece, 14- insulating box, 15- optical power detector, 16- delustring pond, 17- locking phase amplifying circuit, 18- industrial personal computer.
Specific embodiment
With reference to the accompanying drawings of the specification and specific embodiment, technical solution of the present invention is described in further detail.
Fig. 1 shows one embodiment that the present invention measures the optoacoustic spectroscopy detection device of multicomponent gas using single photoacoustic cell, The embodiment is for detecting Power Transformer Faults characteristic gas component.As shown in Figure 1, the detection device includes shut-off valve 1, Grain object filter device 2, gas drier 3, electromagnetic switch valve 1, pressure sensor 5, electromagnetic switch valve 26, sonic nozzle 7, vacuum pump 8, quantum cascade laser array module 9, spectroscope module 10, reference gas chamber 11 to be measured, difference resonance photoacoustic cell 12, acoustic-electric conversion module 13, insulating box 14, optical power detector 15, delustring pond 16, locking phase amplifying circuit 17, industrial personal computer 18.
In one embodiment, which passes through the one of shut-off valve 1 Side is connected on transformer vacuum degasser, is then turned off on the gas channels of valve 1 and is connected with particulate matter filter device in turn 2, gas drier 3, electromagnetic switch valve 1, pressure sensor 5, reference gas chamber 11 to be measured, electromagnetic switch valve 26, velocity of sound spray Mouth 7, vacuum pump 8, characteristic gas pass sequentially through above-mentioned module and are discharged eventually by vacuum pump 8;Detection device includes quantum stage Join laser array module 9, spectroscope module 10, reference gas chamber 11 to be measured, difference resonance photoacoustic cell 12, acoustic-electric conversion module 13, insulating box 14, optical power detector 15, delustring pond 16, locking phase amplifying circuit 17 and industrial personal computer 18.
The quantum cascade laser array module 9 includes laser driving and temperature control module 91, quantum cascade laser battle array Column 92, light path calibration laser 93, all-wave length total reflective mirror 94, specific wavelength total reflective mirror 95-98.Quantum cascade laser array 92 wraps Include three quantum cascade laser 921-923, each quantum cascade laser 921-923 can inspire for it is single one or more The super-narrow line width laser of transformer decomposed gas component absorption peak, and pass through specific wavelength after being focused by condenser lens 924-926 Total reflective mirror 95-98 and all-wave length total reflective mirror 94 are injected in spectroscope module 10 after converging to same optical path.Quantum cascade laser 921-923 inspires the laser of different wave length, can by the photoacoustic signal that laser of the detection under test gas to different wave length generates To be finally inversed by the concentration of each component under test gas.Light path calibration laser 93 is the laser of naked eyes visible wavelength, is equally passed through Specific wavelength total reflective mirror 95-98 and all-wave length total reflective mirror 94 inject spectroscope module 10 after converging, and swash for calibrating quanta cascade The optical path of light device array module 9 is not used in excitation under test gas and generates photoacoustic signal.In quantum cascade laser array module 9 Laser driving and temperature control module 91 can freely adjust the size of electric current according to the actual situation, output voltage range 0-20V, defeated Electric current 0-1A out, current stability 0.1mA can realize kHz modulation output, in conjunction with semiconductor cooler (TEC) as needed It realizes chip temperature control, precisely adjusts chip wavelength.Laser driving and temperature control mould in quantum cascade laser array module 9 Block 91 switches over each quantum cascade laser 921-923 using analog switch mode, to realize different wavelength output. Specifically, the visible light that the light path calibration laser 93 in quantum cascade laser array module 9 is 0.55 μm of wavelength.All-wave length is complete Anti- mirror 94, specific wavelength total reflective mirror 95-98 angle can be manually adjusted by pedestal.
Quantum cascade laser array 92 in the quantum cascade laser array module 9 can realize that single laser detection is more The function of gas composition, wherein the tunable wave length range of quantum cascade laser 1 is 7.10 μm -7.38 μm, and wavelength is contained Cover C2H4、CH4、C2H2The characteristic absorption peak of three kinds of gas, as shown in Fig. 2, selected C2H4、CH4、C2H2Characteristic absorption peak wavelength point It Wei Yu not be 7.10 μm, 7.38 μm, 7.37 μm;The tunable wave length range of quantum cascade laser 2 922 is 4.34 μm of -4.54 μ M, wavelength cover CO, CO2The characteristic absorption peak of two kinds of gas, as shown in figure 3, selected CO, CO2Characteristic absorption peak wavelength distinguishes position In 4.54 μm, 4.34 μm;The wavelength of quantum cascade laser 3 923 is 3.35 μm, covers C2H6The characteristic absorption peak of gas, such as Shown in Fig. 4, selected C2H6Characteristic absorption peak wavelength is located at 3.35 μm.
The spectroscope module 10 includes one piece of semi-transparent semi-reflecting lens 101 and one piece of total reflective mirror 102, will be by quanta cascade laser The laser induced breakdown that device array module 9 is injected is the identical laser of two beam energies, and the semi-transparent semi-reflecting lens 101 in spectroscope module 10 are Broadband semi-transparent semi-reflecting lens.Semi-transparent semi-reflecting lens 101 and the angle of total reflective mirror 102 can be manually adjusted by pedestal.
The reference gas chamber 11 to be measured is the cylindrical chamber of the two identical sizes hollowed out in a square piece, respectively to Survey gas chamber 117 and reference gas chamber 118.The material of reference gas chamber 11 to be measured is brass, and gas chamber to be measured 117 and reference gas chamber 118 Inner wall is coated with gold, and gas chamber 117 to be measured is identical as 118 size of reference gas chamber, diameter 20mm, length 100mm.Air inlet 111 Positioned at gas chamber to be measured at the 10mm of entering light side, diameter 3mm, long 4mm, gas outlet 112 is located at gas chamber to be measured apart from light emission side At 10mm, diameter 3mm, long 4mm.Diaphragm 1 and diaphragm 2 114 are respectively with corrosion resistant seal glue in gas to be measured The entering light of room 117 and reference gas chamber 118 is surveyed, can be by diaphragm with the laser guaranteed in quantum cascade laser array module 9 Gas chamber 117 to be measured is injected with reference gas chamber 118, diaphragm 3 115 and diaphragm 4 116 use corrosion resistant seal glue respectively In the flash ranging out of gas chamber 117 to be measured and reference gas chamber 118, to guarantee that the laser for passing through gas chamber 117 to be measured and reference gas chamber 118 can To inject in photoacoustic cell 125,126, the material of diaphragm is made of the quartz material of light transmittance >=99%.Reference gas chamber 118 by The pure N of inflating port one 119 preliminary filling2
The difference resonance photoacoustic cell 12 is assembly after the cylindrical chamber for digging out identical size respectively in two square pieces Made of single piece, which forms photoacoustic cell 1, photoacoustic cell 2 126.The junction of two square pieces hollows out The horn-like cavity of acoustic-electric conversion module 13, the company of horn-like cavity and photoacoustic cell 1, photoacoustic cell 2 126 can be placed out Connecing place's diameter is 2mm, is 7mm with 13 connected component diameter of acoustic-electric conversion module.The material of difference resonance photoacoustic cell 12 is brass, And photoacoustic cell 1,2 126 inner wall of photoacoustic cell are coated with gold, photoacoustic cell 1,2 126 diameter of photoacoustic cell are 8mm, and length is 100mm, draw ratio 25:2.Diaphragm 5 121 and diaphragm 6 122 are respectively with corrosion resistant seal glue in photoacoustic cell one 125 survey with the entering light of photoacoustic cell 2 126, with guarantee can be by diaphragm by the laser of gas chamber 117 to be measured and reference gas chamber 118 It injects in photoacoustic cell 1 and photoacoustic cell 2 126, diaphragm 7 123 and diaphragm 8 124 use corrosion resistant seal glue respectively In the flash ranging out of photoacoustic cell 1 and photoacoustic cell 2 126, to guarantee that the laser for passing through photoacoustic cell 1 and photoacoustic cell 2 126 can To inject in optical power detector 15 and delustring pond 16, the material of diaphragm is made of the quartz material of light transmittance >=99%.Difference Resonance photoacoustic cell 12 is divided to pass through 2 127 preliminary filling of inflating port C2H4、CH4、C2H2、CO、CO2、C2H6And N2Seven kinds of gases, and body Product ratio is respectively 7%, 0.7%, 0.5%, 0.05%, 0.05%, 0.01%, 91.69%.
The acoustic-electric conversion module 13 is to be passed using the condenser type of titanium film for detecting difference photoacoustic signal, acoustic-electric conversion module Sensor, the acoustic-electric conversion module 13 are arranged at the central axis of difference resonance photoacoustic cell 12, are connected to photoacoustic cell 1 With the central closing of photoacoustic cell 2 126, junction is bell shape, diameter 7mm at wide opening, diameter 2mm at slot.Acoustic-electric 13 diameter 14mm of conversion module, the use titanium metal material film of acoustic-electric conversion module diaphragm 131, diameter 12mm, 10 μm of thickness.Acoustic-electric Conversion module 13 is dense under test gas to obtain for detecting the difference photoacoustic signal that under test gas generates in two groups of metal tubes The acoustical signal of degree linearly, sensitivity 10mV/Pa-50mV/Pa.
The insulating box 14 is Resistant heating insulating box, and reference gas chamber 11 to be measured places it with difference resonance photoacoustic cell 12 In, to guarantee that reference gas chamber 11 to be measured maintains 50 DEG C with temperature in difference resonance photoacoustic cell 12.
The optical power detector 15 is used to detect the power excursion of laser, and laser drift signal Real-time Feedback is driven to laser Dynamic and temperature control module 91, by realizing laser driving and the adjustment of 91 parameter of temperature control module to quantum cascade laser array 92 output wavelengths and energy are modified.
The delustring pond 16 is used to absorb the laser energy for being not used for excitation photoacoustic signal, is full of high concentration in delustring pond 16 C2H4、CH4、C2H2、CO、CO2、C2H6Six kinds of gases, and volume ratio coefficient is respectively 85%, 7%, 3%, 2%, 2%, 1%.
The locking phase amplifying circuit 17 and industrial personal computer 18 is for extracting specific wavelength frequency signal, locking phase amplifying circuit 17 and work Control machine 18 may filter that the noise signal other than 1kHz-4kHz, and the noise of conversion to input terminal is 50nV, temperature drift≤ 10ppm/ DEG C, the amplification factor adjustable extent of amplifier is not less than 104
Present invention applicant combines Figure of description to be described in detail and describe implementation example of the invention, but ability Field technique personnel it should be understood that more than implement example be only the preferred embodiments of the invention, in detail explanation be intended merely to help Reader is helped to more fully understand spirit of that invention, and it is not intended to limit the protection scope of the present invention, on the contrary, any based on of the invention Any improvement or modification made by spirit should all be fallen within the scope and spirit of the invention.

Claims (28)

1. a kind of optoacoustic spectroscopy detection device using single photoacoustic cell measurement multicomponent gas, which is characterized in that the device includes Shut-off valve (1), particulate matter filter device (2), gas drier (3), electromagnetic switch valve one (4), pressure sensor (5), electricity Magnetic switch valve two (6), sonic nozzle (7), vacuum pump (8), quantum cascade laser array module (9), spectroscope module (10), Reference gas chamber (11) to be measured, difference are resonated photoacoustic cell (12), acoustic-electric conversion module (13), insulating box (14), optical power detector (15), delustring pond (16), locking phase amplifying circuit (17) and industrial personal computer (18);
Wherein, the gas channels that under test gas is passed through are followed successively by shut-off valve (1), particulate matter filter device (2), gas drier (3), electromagnetic switch valve one (4), pressure sensor (5), reference gas chamber to be measured (11), electromagnetic switch valve two (6), sonic nozzle (7) and vacuum pump (8);
Laser is generated by quantum cascade laser array module (9), enters reference gas chamber to be measured by spectroscope module (10) (11), multiple laser is coupled in a branch of optical path by the quantum cascade laser array module (9).
2. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the quantum cascade laser array module (9) includes laser driving and temperature control module (91), quantum cascade laser battle array Arrange (92), light path calibration laser (93), all-wave length total reflective mirror (94) and specific wavelength total reflective mirror (95-98).
3. the optoacoustic spectroscopy detection device as claimed in claim 2 using single photoacoustic cell measurement multicomponent gas, feature exist In the quantum cascade laser array (92) includes multiple quantum cascade laser and multiple condenser lenses.
4. the optoacoustic spectroscopy detection device as claimed in claim 3 using single photoacoustic cell measurement multicomponent gas, feature exist Be disposed as three in, quantum cascade laser and condenser lens, each quantum cascade laser (921-923) excitation for Single or various ingredients absorption peak super-narrow line width laser in gas is surveyed, and passes through institute after being focused by condenser lens (924-926) It states after specific wavelength total reflective mirror (95-98) converges to same optical path with the all-wave length total reflective mirror (94) and injects the spectroscope mould In block (10).
5. the optoacoustic spectroscopy detection device as claimed in claim 4 using single photoacoustic cell measurement multicomponent gas, feature exist In being switched between the quantum cascade laser (921-923) using analog switch mode, realize that different wavelength is defeated Out.
6. the optoacoustic spectroscopy detection device as claimed in claim 2 using single photoacoustic cell measurement multicomponent gas, feature exist In laser driving and temperature control module (91) can according to the actual situation freely in the quantum cascade laser array module (9) It adjusts the size of electric current and realizes kHz modulation output as needed, realize chip temperature control in conjunction with semiconductor cooler, it is quasi- Really adjust chip wavelength.
7. the optoacoustic spectroscopy detection device as claimed in claim 3 using single photoacoustic cell measurement multicomponent gas, feature exist In single laser inspection can be achieved in the quantum cascade laser array (92) in the quantum cascade laser array module (9) The function of more gas compositions is surveyed,
When for detecting transformer: the tunable wave length range of quantum cascade laser one (921) is 7.10 μm -7.38 μm, wave Length covers C2H4、CH4、C2H2The characteristic absorption peak of three kinds of gas, selected C2H4、CH4、C2H2Gas characteristic absorption peak wavelength difference Positioned at 7.10 μm, 7.38 μm, 7.37 μm;The tunable wave length range of quantum cascade laser two (922) is 4.34 μm of -4.54 μ M, wavelength cover CO, CO2The characteristic absorption peak of two kinds of gas, selected CO, CO2Gas characteristic absorption peak wavelength is located at 4.54 μ m,4.34μm;The wavelength of quantum cascade laser three (923) is 3.35 μm, covers C2H6The characteristic absorption peak of gas, selected C2H6 Gas characteristic absorption peak wavelength is located at 3.35 μm.
8. the optoacoustic spectroscopy detection device as claimed in claim 3 using single photoacoustic cell measurement multicomponent gas, feature exist In single laser inspection can be achieved in the quantum cascade laser array (92) in the quantum cascade laser array module (9) The function of more gas compositions is surveyed,
For detecting GIS equipment SF6When decomposing gas: the wavelength of quantum cascade laser one (921) is 7.07 μm, and wavelength is covered H2The characteristic absorption peak of S gas, selected H2S gas characteristic absorption peak wavelength is located at 7.07 μm;Quantum cascade laser two (922) Tunable wave length range be 4.34 μm -4.54 μm, wavelength covers CO, CO2The characteristic absorption peak of two kinds of gas, selected CO, CO2 Gas characteristic absorption peak wavelength is located at 4.54 μm, 4.34 μm;The tunable wave length range of quantum cascade laser three (923) It is 7.43 μm -7.87 μm, wavelength covers SO2、CF4、SO2F2The characteristic absorption peak of three kinds of gas, selected SO2、CF4、SO2F2Gas Characteristic absorption peak wavelength is located at 7.43 μm, 7.79 μm, 7.87 μm.
9. the optoacoustic spectroscopy detection device as claimed in claim 3 using single photoacoustic cell measurement multicomponent gas, feature exist In single laser inspection can be achieved in the quantum cascade laser array (92) in the quantum cascade laser array module (9) The function of more gas compositions is surveyed,
For detect petrochemical industry quality of natural gas control in gas when: the wavelength of quantum cascade laser one (921) be 7.07 μm- 7.43 μm, wavelength covers H2S、SO2The characteristic absorption peak of two kinds of gas, selected H2S、SO2Gas characteristic absorption peak wavelength distinguishes position In 7.07 μm, 7.43 μm;The wavelength of quantum cascade laser two (922) is 4.34 μm, and wavelength covers CO2The characteristic absorption of gas Peak, selected CO2Gas characteristic absorption peak wavelength is located at 4.34 μm;The tunable wave length range of quantum cascade laser three (923) It is 4.83 μm, wavelength covers the characteristic absorption peak of COS gas, and selected COS gas characteristic absorption peak wavelength is located at 4.83 μm.
10. the optoacoustic spectroscopy detection device as claimed in claim 3 using single photoacoustic cell measurement multicomponent gas, feature exist In single laser inspection can be achieved in the quantum cascade laser array (92) in the quantum cascade laser array module (9) The function of more gas compositions is surveyed,
Gas is monitored when for detecting petrochemical industry methanol production equipment conversion combined coefficient: the wave of quantum cascade laser one (921) A length of 7.54 μm, wavelength covers CH4The characteristic absorption peak of gas, selected CH4Gas characteristic absorption peak wavelength is located at 7.54 μm;Amount The tunable wave length range of qc laser two (922) is 4.34 μm -4.54 μm, and wavelength covers CO, CO2The spy of two kinds of gas Levy absorption peak, selected CO, CO2Gas characteristic absorption peak wavelength is located at 4.54 μm, 4.34 μm.
11. the optoacoustic spectroscopy detection device as claimed in claim 2 using single photoacoustic cell measurement multicomponent gas, feature exist In the laser that, the light path calibration laser (93) is naked eyes visible wavelength, by the specific wavelength total reflective mirror (95-98) with The spectroscope module (10) is injected after all-wave length total reflective mirror (94) convergence.
12. the optoacoustic spectroscopy detection device as claimed in claim 11 using single photoacoustic cell measurement multicomponent gas, feature It is, the visible light that the light path calibration laser (93) is 0.38 μm -0.78 μm of wavelength.
13. the optoacoustic spectroscopy detection device as claimed in claim 2 using single photoacoustic cell measurement multicomponent gas, feature exist In the angle of the all-wave length total reflective mirror (94) and the specific wavelength total reflective mirror (95-98) can be carried out manual by pedestal It adjusts.
14. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the spectroscope module (10) includes one piece of semi-transparent semi-reflecting lens (101) and one piece of total reflective mirror (102), will be by quantum stage Joining the laser induced breakdown that laser array module (9) are injected is the identical laser of two beam energies.
15. the optoacoustic spectroscopy detection device as claimed in claim 14 using single photoacoustic cell measurement multicomponent gas, feature It is, the semi-transparent semi-reflecting lens (101) are broadband semi-transparent semi-reflecting lens, or the narrowband semi-transparent semi-reflecting lens turntable controlled by driving motor It constitutes, turntable converts the semi-transparent semi-reflecting lens of specific band according to the optical maser wavelength of transmitting.
16. the optoacoustic spectroscopy detection device as claimed in claim 14 using single photoacoustic cell measurement multicomponent gas, feature It is, the semi-transparent semi-reflecting lens (101) and the angle of the total reflective mirror (102) can be manually adjusted by pedestal.
17. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the reference gas chamber (11) to be measured includes gas chamber to be measured (117) and reference gas chamber (118), and under test gas passes through air inlet (111) enter the gas chamber (117) to be measured, the reference gas chamber (118) is by inflating port one (119) preliminary filling N2, He, Ar or sky Gas.
18. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In difference resonance photoacoustic cell (12) is single order longitudinal resonance photoacoustic cell, for generating photoacoustic signal;The acoustic-electric modulus of conversion Block (13) is for detecting the difference photoacoustic signal.
19. the optoacoustic spectroscopy detection device as claimed in claim 18 using single photoacoustic cell measurement multicomponent gas, feature It is, when for detecting transformer: difference resonance photoacoustic cell (12) passes through inflating port two (127) preliminary filling C2H4、CH4、C2H2、 CO、CO2、C2H6And N2Seven kinds of gases, wherein C2H4、CH4、C2H2、CO、CO2、C2H6Ratio it is directly proportional to its absorption coefficient, This six kinds of void fraction proportionality coefficients of preliminary filling are 700:70:50:5:5:1.
20. the optoacoustic spectroscopy detection device as claimed in claim 18 using single photoacoustic cell measurement multicomponent gas, feature It is, when for detecting transformer: for detecting GIS equipment SF6When decomposing gas: difference resonance photoacoustic cell (12) passes through Inflating port two (127) preliminary filling H2S、CO、CO2、SO2、CF4、SO2F2And N2Seven kinds of gases, wherein C2H4、CH4、C2H2、CO、CO2、 C2H6Ratio it is directly proportional to its absorption coefficient, this six kinds of void fraction proportionality coefficients of preliminary filling are 60000:80:80: 120:1:10。
21. the optoacoustic spectroscopy detection device as claimed in claim 18 using single photoacoustic cell measurement multicomponent gas, feature It is, when for detecting gas in the control of petrochemical industry quality of natural gas: difference resonance photoacoustic cell (12) passes through inflating port two (127) preliminary filling H2S、SO2、CO2, COS and N2Five kinds of gases, wherein H2S、SO2、CO2, COS ratio and its absorption coefficient at Direct ratio, these four void fraction proportionality coefficients of preliminary filling are 4000:10:5:1.
22. the optoacoustic spectroscopy detection device as claimed in claim 18 using single photoacoustic cell measurement multicomponent gas, feature It is, when for detecting petrochemical industry methanol production equipment conversion combined coefficient monitoring gas: difference resonance photoacoustic cell (12) is logical Overcharge port two (127) preliminary filling CH4, CO, CO and N2Four kinds of gases, wherein CH4、CO、CO2Ratio and its absorption coefficient at Direct ratio, these three void fraction proportionality coefficients of preliminary filling are 10:1:1.
23. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the reference gas chamber (11) to be measured and difference resonance photoacoustic cell (12) are placed in the insulating box (14) to maintain a perseverance Determine temperature.
24. the optoacoustic spectroscopy detection device as claimed in claim 2 using single photoacoustic cell measurement multicomponent gas, feature exist In the optical power detector (15) is used to detect the power excursion of laser, and by power excursion signal Real-time Feedback to described Laser driving and temperature control module (91), by realizing laser driving and the adjustment of temperature control module (91) parameter to institute It states quantum cascade laser array (92) output wavelength and energy is modified.
25. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the delustring pond (16) is used to absorb the laser energy for being not used for excitation photoacoustic signal.
26. as the described in any item optoacoustic spectroscopy using single photoacoustic cell measurement multicomponent gas of claim 19-22 detect dress It sets, which is characterized in that resonating photoacoustic cell (12) congener gas with the difference full of high concentration in the delustring pond (16) Body component.
27. the optoacoustic spectroscopy detection device as described in claim 1 using single photoacoustic cell measurement multicomponent gas, feature exist In the locking phase amplifying circuit (17) and the industrial personal computer (18) are for extracting specific wavelength frequency signal, measurement frequency range 1kHz-4kHz。
28. the optoacoustic spectroscopy detection device as claimed in claim 26 using single photoacoustic cell measurement multicomponent gas, feature It is, the locking phase amplifying circuit (17) and the industrial personal computer (18) may filter that the noise signal other than 1kHz-4kHz, conversion Noise to input terminal is 50nV, and the amplification factor adjustable extent of temperature drift≤10ppm/ DEG C, amplifier is not less than 104
CN201910060515.3A 2019-01-22 2019-01-22 Laser photoacoustic spectrum detection device for measuring multi-component gas by adopting single photoacoustic cell Active CN109765185B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910060515.3A CN109765185B (en) 2019-01-22 2019-01-22 Laser photoacoustic spectrum detection device for measuring multi-component gas by adopting single photoacoustic cell

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910060515.3A CN109765185B (en) 2019-01-22 2019-01-22 Laser photoacoustic spectrum detection device for measuring multi-component gas by adopting single photoacoustic cell

Publications (2)

Publication Number Publication Date
CN109765185A true CN109765185A (en) 2019-05-17
CN109765185B CN109765185B (en) 2021-03-16

Family

ID=66454325

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910060515.3A Active CN109765185B (en) 2019-01-22 2019-01-22 Laser photoacoustic spectrum detection device for measuring multi-component gas by adopting single photoacoustic cell

Country Status (1)

Country Link
CN (1) CN109765185B (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110389106A (en) * 2019-07-25 2019-10-29 国网重庆市电力公司电力科学研究院 A kind of infrared photoacoustic spectra quantitative analysis method of SF6 decomposition components
CN110426371A (en) * 2019-09-10 2019-11-08 国网重庆市电力公司电力科学研究院 A kind of system detecting the HF gas in SF6 electrical equipment
CN111380805A (en) * 2020-01-02 2020-07-07 华中科技大学 Photoacoustic cell with adjustable resonant frequency and adjusting method
CN112067556A (en) * 2020-09-29 2020-12-11 湖北鑫英泰系统技术股份有限公司 Oil-gas detection method and device for oil-immersed equipment
CN112504987A (en) * 2021-02-06 2021-03-16 湖北鑫英泰系统技术股份有限公司 Method and system for identifying mixture of gas ethylene and acetylene in transformer oil
CN113447445A (en) * 2021-06-29 2021-09-28 浙大宁波理工学院 Device for simultaneously detecting at least two different halogenated hydrocarbon gases
CN113758876A (en) * 2021-09-29 2021-12-07 中广核研究院有限公司 Gas detection equipment and system in oil
CN117629898A (en) * 2024-01-25 2024-03-01 杭州泽天春来科技股份有限公司 Signal processing method, system and readable medium of photoacoustic spectrometry gas analyzer
WO2024045341A1 (en) * 2022-09-01 2024-03-07 南方电网科学研究院有限责任公司 Photoacoustic spectrometry-based gas testing apparatus

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101887009A (en) * 2010-03-22 2010-11-17 山东省科学院自动化研究所 Intrinsic safety photoacoustic spectrum gas monitoring system based on optical acoustic sensor
CN102713565A (en) * 2009-09-30 2012-10-03 康宁股份有限公司 Gas sensor based on photoacoustic detection
CN102954948A (en) * 2011-08-26 2013-03-06 中国科学院安徽光学精密机械研究所 Gas sensor based on photoacoustic spectrometry
CN104198393A (en) * 2014-04-29 2014-12-10 贵州电力试验研究院 On-line monitoring system and method for SF6 decomposition gas components in electrical equipment
CN104849214A (en) * 2015-04-20 2015-08-19 北京航天控制仪器研究所 Enhanced multi-group photoacoustic spectrum gas sensing device based on quartz tuning fork
CN108535184A (en) * 2018-04-10 2018-09-14 大连理工大学 A kind of optoacoustic spectroscopy multicomponent trace gas detection instrument and method

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102713565A (en) * 2009-09-30 2012-10-03 康宁股份有限公司 Gas sensor based on photoacoustic detection
CN101887009A (en) * 2010-03-22 2010-11-17 山东省科学院自动化研究所 Intrinsic safety photoacoustic spectrum gas monitoring system based on optical acoustic sensor
CN102954948A (en) * 2011-08-26 2013-03-06 中国科学院安徽光学精密机械研究所 Gas sensor based on photoacoustic spectrometry
CN104198393A (en) * 2014-04-29 2014-12-10 贵州电力试验研究院 On-line monitoring system and method for SF6 decomposition gas components in electrical equipment
CN104849214A (en) * 2015-04-20 2015-08-19 北京航天控制仪器研究所 Enhanced multi-group photoacoustic spectrum gas sensing device based on quartz tuning fork
CN108535184A (en) * 2018-04-10 2018-09-14 大连理工大学 A kind of optoacoustic spectroscopy multicomponent trace gas detection instrument and method

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110389106A (en) * 2019-07-25 2019-10-29 国网重庆市电力公司电力科学研究院 A kind of infrared photoacoustic spectra quantitative analysis method of SF6 decomposition components
CN110426371A (en) * 2019-09-10 2019-11-08 国网重庆市电力公司电力科学研究院 A kind of system detecting the HF gas in SF6 electrical equipment
CN111380805A (en) * 2020-01-02 2020-07-07 华中科技大学 Photoacoustic cell with adjustable resonant frequency and adjusting method
CN111380805B (en) * 2020-01-02 2021-04-06 华中科技大学 Photoacoustic cell with adjustable resonant frequency and adjusting method
CN112067556A (en) * 2020-09-29 2020-12-11 湖北鑫英泰系统技术股份有限公司 Oil-gas detection method and device for oil-immersed equipment
CN112067556B (en) * 2020-09-29 2021-08-17 湖北鑫英泰系统技术股份有限公司 Oil-gas detection method and device for oil-immersed equipment
CN112504987B (en) * 2021-02-06 2021-05-04 湖北鑫英泰系统技术股份有限公司 Method and system for identifying mixture of gas ethylene and acetylene in transformer oil
CN112504987A (en) * 2021-02-06 2021-03-16 湖北鑫英泰系统技术股份有限公司 Method and system for identifying mixture of gas ethylene and acetylene in transformer oil
CN113447445A (en) * 2021-06-29 2021-09-28 浙大宁波理工学院 Device for simultaneously detecting at least two different halogenated hydrocarbon gases
CN113758876A (en) * 2021-09-29 2021-12-07 中广核研究院有限公司 Gas detection equipment and system in oil
WO2024045341A1 (en) * 2022-09-01 2024-03-07 南方电网科学研究院有限责任公司 Photoacoustic spectrometry-based gas testing apparatus
CN117629898A (en) * 2024-01-25 2024-03-01 杭州泽天春来科技股份有限公司 Signal processing method, system and readable medium of photoacoustic spectrometry gas analyzer
CN117629898B (en) * 2024-01-25 2024-05-07 杭州泽天春来科技股份有限公司 Signal processing method, system and readable medium of photoacoustic spectrometry gas analyzer

Also Published As

Publication number Publication date
CN109765185B (en) 2021-03-16

Similar Documents

Publication Publication Date Title
CN109765185A (en) A kind of Laser Photoacoustic Spectroscopy detection device using single photoacoustic cell measurement multicomponent gas
CN104237135B (en) CO gas detecting systems and method based on quartz tuning fork strengthened optoacoustic spectroscopy
CN107064012B (en) Quartz enhanced photoacoustic spectroscopy gas-detecting device and method based on beat effect
Zhao et al. Ultra-high sensitive photoacoustic gas detector based on differential multi-pass cell
CN107677610B (en) Cantilever beam and photoacoustic cell dual-resonance enhanced photoacoustic spectrum detection system and method
CN109765181B (en) Differential type resonance photoacoustic cell for improving gas photoacoustic spectrum detection stability
CN109085133B (en) Off-axis integral cavity atmosphere CH based on real-time reflectivity correction4Concentration measuring device and measuring method thereof
CN106872402A (en) Gas-detecting device and method based on super continuous spectrums laser
Zhang et al. Photoacoustic spectroscopy for detection of trace C2H2 using ellipsoidal photoacoustic cell
CN105136675B (en) A kind of toxic and harmful gas concentration on-line testing method
CN114047136B (en) High-sensitivity combined light source type photoacoustic spectrum gas detection system and method
Yun et al. Photoacoustic detection of dissolved gases in transformer oil
WO2021007782A1 (en) Cavity ring-down spectrometer system
WO2022267286A1 (en) Gas measurement apparatus
CN110411960A (en) A kind of cavity ring-down spectroscopy instrument system
CN114018829B (en) Double-optical comb multicomponent gas detection system with tuning fork resonance enhancement
CN102680412A (en) Method for detecting concentration of trace steam by using photoacoustic spectrometry method
WO2022267555A1 (en) Radial cavity quartz-enhanced photoacoustic spectrophone and gas detection device comprising same
CN110057779A (en) Method and apparatus based on temperature self-compensation TDLAS technology measurement gas concentration
Xiong et al. Photoacoustic spectroscopy gas detection technology research progress
Wang et al. A compact photoacoustic detector for trace acetylene based on 3D-printed differential Helmholtz resonators
CN108535191A (en) LR laser raman gas-detecting device based on diamond shape hysteroscope
CN102495017A (en) Detecting instrument of sulfur hexafluoride gas decomposition products
CN114235699B (en) Trace gas concentration's detection device
CN114002184B (en) Multi-resonance enhanced photoacoustic spectrum multi-component gas simultaneous detection device and 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
CB03 Change of inventor or designer information
CB03 Change of inventor or designer information

Inventor after: Chen Weigen

Inventor after: Tan Yaxiong

Inventor after: Li Jian

Inventor after: Huang Zhengyong

Inventor after: Wang Feipeng

Inventor after: Zhou Quan

Inventor after: Wan Fu

Inventor after: Wang Youyuan

Inventor after: Yang Tianhe

Inventor after: Chen Miao

Inventor after: Wang Pinyi

Inventor after: Huang Zhengwei

Inventor after: Du Lin

Inventor after: Jiang Detao

Inventor before: Chen Weigen

Inventor before: Wang Feipeng

Inventor before: Zhou Quan

Inventor before: Wan Fu

Inventor before: Wang Youyuan

Inventor before: Yang Tianhe

Inventor before: Wang Pinyi

Inventor before: Du Lin

Inventor before: Tan Yaxiong

Inventor before: Li Jian

Inventor before: Huang Zhengyong

TA01 Transfer of patent application right
TA01 Transfer of patent application right

Effective date of registration: 20200131

Address after: 400044 Shapingba District Sha Street, No. 174, Chongqing

Applicant after: Chongqing University

Applicant after: BEIJING BEIFEN-RUILI ANALYTICAL INSTRUMENT (Group) Co.,Ltd.

Address before: 400044 Sha Zheng street, Shapingba District, Chongqing City, No. 127

Applicant before: Chongqing University

GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20231220

Address after: 400044 No. 174 Sha Jie street, Shapingba District, Chongqing

Patentee after: Chongqing University

Patentee after: BEIJING BAIF-MAIHAK ANALYTICAL INSTRUMENT Co.,Ltd.

Address before: 400044 No. 174 Sha Jie street, Shapingba District, Chongqing

Patentee before: Chongqing University

Patentee before: BEIJING BEIFEN-RUILI ANALYTICAL INSTRUMENT (Group) Co.,Ltd.