CN109115683A - The installation method of convex lens and high reflection mirror in a kind of optical cavity structure - Google Patents

The installation method of convex lens and high reflection mirror in a kind of optical cavity structure Download PDF

Info

Publication number
CN109115683A
CN109115683A CN201811025993.2A CN201811025993A CN109115683A CN 109115683 A CN109115683 A CN 109115683A CN 201811025993 A CN201811025993 A CN 201811025993A CN 109115683 A CN109115683 A CN 109115683A
Authority
CN
China
Prior art keywords
high reflection
reflection mirror
convex lens
optical
motion seat
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201811025993.2A
Other languages
Chinese (zh)
Inventor
欧阳彬
王玉政
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.)
Shenzhen City Capri Environmental Technology Co Ltd
Original Assignee
Shenzhen City Capri Environmental Technology Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shenzhen City Capri Environmental Technology Co Ltd filed Critical Shenzhen City Capri Environmental Technology Co Ltd
Priority to CN201811025993.2A priority Critical patent/CN109115683A/en
Publication of CN109115683A publication Critical patent/CN109115683A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/01Arrangements or apparatus for facilitating the optical investigation
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/3103Atomic absorption analysis

Landscapes

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

Abstract

The installation method of convex lens and high reflection mirror in a kind of optical cavity structure, the left end of the cavity pipe of the optical cavity structure are equipped with the first high reflection mirror, and the right end of cavity pipe is equipped with the second high reflection mirror;The outside of first high reflection mirror is equipped with the first convex lens, and the outside of the second high reflection mirror is equipped with the second convex lens;The first end of first optical fiber is used to connect the emission port of light source, and the second end of the first optical fiber is placed in the outside focus of the first convex lens;For connecting spectrometer, the second end of the second optical fiber is placed in the outside focus of the second convex lens the first end of second optical fiber;This method comprises: the mirror surface of the mirror surface and the second high reflection mirror that adjust the first high reflection mirror realizes collimation;It adjusts the first convex lens and the first high reflection mirror realizes collimation between the two;It adjusts the second convex lens and the second high reflection mirror realizes collimation between the two.Implement the embodiment of the present application, can effectively, easily detect the concentration of atmospheric molecule, and the atmospheric molecule concentration of super low concentration is effectively detected.

Description

The installation method of convex lens and high reflection mirror in a kind of optical cavity structure
Technical field
This application involves the peaces of convex lens and high reflection mirror in environmental monitoring technology field more particularly to a kind of optical cavity structure Dress method.
Background technique
Along with society, economic continuous development, atmosphere pollution is in world's most area, especially in developing country Area increasingly attracts people's attention.In order to detect the severity of atmosphere pollution, it usually needs using detecting instrument to big Gas molecule (such as NO2、HCHO、CHOCHO、N2O5、NO3, HONO etc.) concentration detected.In the prior art, inspection is being utilized It surveys before the concentration of instrument detection atmospheric molecule, it usually needs the spirit of detecting instrument is first demarcated with the calibrating gas of known concentration Quick coefficient (sensitivity coefficient), and the sensitive system of detecting instrument is demarcated with the calibrating gas of known concentration Number can add additional complexity and step to detection;In addition, the purchase of calibrating gas, transport etc. may costly, it is cumbersome, It is even difficult to calibrating gas (such as N obtained sometimes2O5And NO3), to aggravate detection difficulty;In addition, existing detecting instrument pair It is undesirable in the detection effect of the atmospheric molecule of super low concentration.
Summary of the invention
The installation method of convex lens and high reflection mirror, utilizes the installation in a kind of optical cavity structure disclosed in the embodiment of the present application The optical cavity structure of method installation can not only effectively, easily detect atmospheric molecule (such as NO2、HCHO、CHOCHO、N2O5、NO3、 HONO etc.) concentration, and the atmospheric molecule concentration of super low concentration can be effectively detected.
The embodiment of the present application first aspect discloses the installation method of convex lens and high reflection mirror in a kind of optical cavity structure, described The left end of the cavity pipe of optical cavity structure is equipped with the first high reflection mirror, and the right end of the cavity pipe is equipped with the second high reflection mirror;It is described The outside of first high reflection mirror is equipped with the first convex lens, and the outside of second high reflection mirror is equipped with the second convex lens;First light Fine first end is used to connect the emission port of light source, and the second end of first optical fiber is placed on the outer of first convex lens In the focus of side;For the first end of second optical fiber for connecting spectrometer, the second end of second optical fiber is placed on described second In the outside focus of convex lens;The described method includes:
The mirror surface of the mirror surface and second high reflection mirror that adjust first high reflection mirror realizes collimation;
It adjusts first convex lens and first high reflection mirror realizes collimation between the two;
It adjusts the second convex lens and second high reflection mirror realizes collimation between the two.
Based on the embodiment of the present application in a first aspect, in the first embodiment of the embodiment of the present application first aspect, institute State method further include:
The light intensity value for observing the emergent light for the optical cavity structure that the spectrometer is shown, when the light intensity value maximum, Show first high reflection mirror and second high reflection mirror from each other and first convex lens and described second convex Lens reach entirely collimated from each other, and adjusting finishes.
Based on the embodiment of the present application in a first aspect, or the embodiment of the present application first aspect the first embodiment, this In second of embodiment for applying for embodiment first aspect, the method also includes:
First optical motion seat is set, and the left end of the cavity pipe is arranged in the first optical motion seat, and described First high reflection mirror is fixed on the first optical motion seat;
The first optical motion seat is equipped with the adjusting screw for adjusting the tilt angle of first high reflection mirror.
Second of embodiment based on the embodiment of the present application first aspect, in the third of the embodiment of the present application first aspect In kind embodiment, the method also includes:
Second optical motion seat is set, the outside of the first optical motion seat is arranged in the second optical motion seat, And first convex lens is fixed on the second optical motion seat;
The second optical motion seat is equipped with for adjusting first convex lens relative to first high reflection mirror Tilt angle adjusting screw.
The third embodiment based on the embodiment of the present application first aspect, the 4th of the embodiment of the present application first aspect the In kind embodiment, the method also includes:
Third optical motion seat is set, and the right end of the cavity pipe is arranged in the third optical motion seat, and described Second high reflection mirror is fixed on the third optical motion seat;
The third optical motion seat is equipped with the adjusting screw for adjusting the tilt angle of second high reflection mirror.
The 4th kind of embodiment based on the embodiment of the present application first aspect, the 5th of the embodiment of the present application first aspect the In kind embodiment, the method also includes:
4th optical motion seat is set, the outside of the third optical motion seat is arranged in the 4th optical motion seat, And second convex lens is fixed on the 4th optical motion seat;
The 4th optical motion seat is equipped with for adjusting second convex lens relative to second high reflection mirror Tilt angle adjusting screw.
The 5th kind of embodiment based on the embodiment of the present application first aspect, the 6th of the embodiment of the present application first aspect the In kind embodiment, the mirror surface of the mirror surface for adjusting first high reflection mirror and second high reflection mirror realizes collimation, Include:
The adjusting screw on the first optical motion seat is adjusted to adjust the tilt angle of first high reflection mirror, And/or the adjusting screw on the third optical motion seat is adjusted to adjust the tilt angle of second high reflection mirror, so that The mirror surface of the mirror surface of first high reflection mirror and second high reflection mirror realizes collimation.
The 6th kind of embodiment based on the embodiment of the present application first aspect, the 7th of the embodiment of the present application first aspect the In kind embodiment, the adjusting first convex lens and first high reflection mirror realize collimation between the two, comprising:
When the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror realize collimation, described the is adjusted Adjusting screw on two optical motion seats, to adjust inclination angle of first convex lens relative to first high reflection mirror Degree, so that first convex lens and first high reflection mirror realize collimation between the two.
The 7th kind of embodiment based on the embodiment of the present application first aspect, the 8th of the embodiment of the present application first aspect the In kind embodiment, the second convex lens of the adjusting and second high reflection mirror realize collimation between the two, comprising:
When the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror realize collimation, described the is adjusted Adjusting screw on four optical motion seats, to adjust inclination angle of second convex lens relative to second high reflection mirror Degree, so that second convex lens and second high reflection mirror realize collimation between the two.
The 8th kind of embodiment based on the embodiment of the present application first aspect, the 9th of the embodiment of the present application first aspect the In kind embodiment, the method also includes:
The first bellows and the first mirror are set gradually from the first optical motion seat to the left end of the cavity pipe Seat and chamber mount;
Air inlet pipe for being pumped into from gas to the cavity pipe is set on first microscope base and chamber mount;
The second bellows and the second mirror are set gradually from the third optical motion seat to the right end of the cavity pipe Seat and chamber mount;
The escape pipe of the cavity pipe output gas is provided on second microscope base and chamber mount;
Further it is arranged on first microscope base and chamber mount for inputting purge gass to block in the cavity pipe The first purge gass air inlet pipe for directly being contacted with the mirror surface of first high reflection mirror of gas;
Further it is arranged on second microscope base and chamber mount for inputting purge gass to block in the cavity pipe The second purge gass air inlet pipe for directly being contacted with the mirror surface of second high reflection mirror of gas;
Wherein, the purge gass include pure nitrogen gas.
As can be seen from the above technical solutions, the embodiment of the present application has the advantage that
In the embodiment of the present application, in the optical cavity structure using installation method installation convex lens and high reflection mirror, when When being full of the gas of the atmospheric molecule containing concentration undetermined in the cavity pipe, first convex lens can be to first light The cavity pipe is injected after the collimation of light derived from fibre, so that light leaves after roundtrip is multiple between the high reflection mirror of two sides The cavity pipe simultaneously focuses on second optical fiber via second convex lens, then via described in second optical fiber importing Spectrometer carries out optical absorption measurement.The embodiment of the present application can be by directly measuring atmospheric molecule (such as NO2、HCHO、CHOCHO、 N2O5、NO3, HONO etc.) light absorption measure the concentration of atmospheric molecule, so do not need with the calibrating gas of known concentration come Demarcate detecting instrument sensitivity coefficient, so as to effectively, easily detect atmospheric molecule (such as NO2、HCHO、CHOCHO、N2O5、 HONO etc.) concentration and Atmospheric particulates delustring;In addition, light comes between the high reflection mirror of two sides in the embodiment of the present application Reflection is returned, absorption light path can be dramatically increased, increased multiple is 1/ (1-R), and wherein R is the specular reflectivity of high reflection mirror, Vacation lets R be 0.9999, and the distance between two sides high reflection mirror is 1 meter, then 10000 can be realized (in 1 meter of the spacing) The absorption light path of rice (i.e. 10 kilometers), according to Beer-Lambert law of light absorption, the absorption light path of this overlength can be significant Increase the absorption of atmospheric molecule, so as to which the atmospheric molecule concentration of super low concentration is effectively detected.
Detailed description of the invention
It in order to more clearly explain the technical solutions in the embodiments of the present application, below will be to needed in the embodiment Attached drawing is briefly described, it should be apparent that, the drawings in the following description are only some examples of the present application, for ability For the those of ordinary skill of domain, without creative efforts, it can also be obtained according to these attached drawings other attached Figure.
Fig. 1 is a kind of schematic diagram of atmospheric molecule detection system disclosed in the embodiment of the present application;
Fig. 2 is a kind of structural schematic diagram of optical cavity structure disclosed in the embodiment of the present application;
Fig. 3 is a kind of flow diagram of atmospheric molecule detection method disclosed in the embodiment of the present application;
Fig. 4 is the process of the installation method of convex lens and high reflection mirror in a kind of optical cavity structure disclosed in the embodiment of the present application Schematic diagram.
Specific embodiment
Below in conjunction with the attached drawing in the embodiment of the present application, technical solutions in the embodiments of the present application carries out clear, complete Site preparation description, it is clear that the described embodiments are only a part but not all of the embodiments of the present application.Based on this Embodiment in application, every other reality obtained by those of ordinary skill in the art without making creative efforts Example is applied, shall fall in the protection scope of this application.
It should be noted that the term " includes " of the embodiment of the present application and " having " and their any deformation, it is intended that Be to cover it is non-exclusive include, for example, containing the process, method, system, product or equipment of a series of steps or units not Those of be necessarily limited to be clearly listed step or unit, but may include be not clearly listed or for these processes, side The intrinsic other step or units of method, product or equipment.
The installation method of convex lens and high reflection mirror, utilizes the installation in a kind of optical cavity structure disclosed in the embodiment of the present application The optical cavity structure of method installation can not only effectively, easily detect atmospheric molecule (such as NO2、HCHO、CHOCHO、N2O5、NO3、 HONO etc.) concentration, and the atmospheric molecule concentration of super low concentration can be effectively detected.Attached drawing is combined below to carry out in detail Thin description.
For convex lens and high reflection in a kind of better, the clearer optical cavity structure for understanding the embodiment of the present application description The installation method of mirror, below first to the invention relates to atmospheric molecule detection system be described.
Referring to Fig. 1, Fig. 1 is a kind of schematic diagram of atmospheric molecule detection system disclosed in the embodiment of the present application.In Fig. 1 institute In the atmospheric molecule detection system shown, by identical two sides high reflection mirror (i.e. positioned at the high reflection mirror of left end and positioned at right end High reflection mirror) composition optical cavity, the mirror surface of the two sides high reflection mirror, which is realized, to be collimated, i.e., the mirror surface of the described two sides high reflection mirror is mutual Face;The optical cavity is equipped with air inlet (be equipped with air inlet pipe) and gas outlet (i.e. equipped with escape pipe), can be with by air inlet Gas (such as NO full of the atmospheric molecule containing concentration undetermined in the optical cavity2、HCHO、CHOCHO、N2O5、NO3、HONO Deng);One end of the optical cavity is laid with the first convex lens, and the other end of the optical cavity is laid with the second convex lens.Wherein, first The light emitting mouth of one end connection light source of optical fiber, the light source can be strong to incoherence by thermostat (such as thermoelectric (al) cooler) Light source (such as light emitting diode) carries out the constant temperature light source of constant temperature composition, and the other end of first optical fiber is placed on institute in Fig. 1 In the focus of the first convex lens shown;Wherein, one end of the second optical fiber connects spectrometer (such as wide-band spectrum instrument), and described second The other end of optical fiber is placed in the focus of the second convex lens shown in Fig. 1.The spectrometer (such as wide-band spectrum instrument) It can be connect by data line with control computer.
Optionally, in atmospheric molecule detection system shown in Fig. 1, when the light source is by thermostat (such as thermoelectric-cooled Device) to incoherence intense light source (such as light emitting diode) carry out constant temperature composition constant temperature light source when, constitute the constant temperature light source The thermostat (such as thermoelectric (al) cooler) and the incoherence intense light source (such as light emitting diode) can be by light source and thermostats Drive module controls its work, realizes constant temperature effect.Optionally, in atmospheric molecule detection system shown in Fig. 1, Ke Yiyou Power supply is respectively the light source and thermostat drive module, the constant temperature light source, the spectrometer and control by supply lines Computer (such as computer) power supply.Optionally, in atmospheric molecule detection system shown in Fig. 1, can also include air-extractor and Solenoid valve;Correspondingly, power supply can also be respectively the air-extractor and solenoid valve power supply by supply lines.The pumping The function of equipment is atmospheric molecule (such as NO that will contain concentration undetermined according to the flow velocity set2、HCHO、CHOCHO、N2O5、 NO3, HONO etc.) gas be pumped into the optical cavity by the air inlet of the optical cavity, until containing in the optical cavity full of described There is the gas of the atmospheric molecule of concentration undetermined.For example, the air-extractor can be a metering aspiration pump, or use The combination of pump plus mass flowmenter, or be the combination for pumping supernumerary segment flow tube, the embodiment of the present application is not construed as limiting.Wherein, described Solenoid valve can be connect by data line with the control computer;The function of the solenoid valve is, when input matching voltage signal When, switch state can change;For example, after inputting matching voltage signal, which can for normally opened solenoid valve To close;And the solenoid valve for often closing, inputting matched voltage signal can be such that the solenoid valve opens.Shown in Fig. 1 is big Switch of the purpose primarily as control adscititious gases gas circuit of solenoid valve is added in gas molecular detection system, in order to incite somebody to action Different adscititious gases, which are added in gas circuit, to be chemically reacted, with realize be filled in the optical cavity it is different containing undetermined dense The gas of the atmospheric molecule of degree, to realize the Concentration Testing function of the atmospheric molecule of different concentration undetermined.
It is to be appreciated that for ease of description, only illustrating one in atmospheric molecule detection system shown in Fig. 1 The optical cavity, in practical applications, the quantity of the optical cavity can be not construed as limiting for one or more, the embodiment of the present application.
In atmospheric molecule detection system shown in Fig. 1, by thermoelectric (al) cooler to incoherence intense light source (such as light-emitting diodes Pipe) carry out constant temperature constitute constant temperature light source when, can to avoid due to temperature drift cause source emissioning light spectrum change.Due to the perseverance The light that warm light source is launched can be exported via first optical fiber, and the other end of first optical fiber is placed on again In the focus of first convex lens shown in Fig. 1, it can be close in parallel from the light that first convex lens appears in this way Light (light that the i.e. described constant temperature light source is launched is collimated by first convex lens), and from described in the injection of the high reflection mirror in left side Optical cavity, and be successfully entered the light of the optical cavity roundtrip between the high reflection mirror of two sides and repeatedly dramatically increase absorption light path Afterwards, the optical cavity finally is left from the high reflection mirror on right side, and is focused on second optical fiber via second convex lens, It finally imports the spectrometer and carries out light splitting and photon detection, to obtain in the optical cavity of one wavelength range of covering full of institute The light intensity map I (λ) when the gas of the atmospheric molecule containing concentration undetermined is stated, and is supplied to the control computer, by the control Computer processed calculates the concentration c of the atmospheric molecule of the concentration undetermined according to the light intensity map I (λ) and preset formula.
In the embodiment of the present application, light roundtrip between the high reflection mirror of two sides can dramatically increase absorption light path, inhale The receipts increased multiple of light path is 1/ (1-R), and wherein R is the specular reflectivity of high reflection mirror, it is assumed that R is 0.9999 and two sides is high anti- Penetrating the distance between mirror is 1 meter, then the absorption light path of ten thousand metres (i.e. 10 kilometers), root can be realized (in 1 meter of the spacing) According to Beer-Lambert law of light absorption, the absorption light path of this overlength can dramatically increase the absorption of atmospheric molecule, so as to The atmospheric molecule concentration of super low concentration is effectively detected.
In the embodiment of the present application, different atmospheric molecules is also different to the characteristic absorption of ultraviolet-visible light.Such as it is big Gas molecule NO2There is strong characteristic absorption within the scope of 350-600nm, it is therefore, big containing concentration undetermined when being full of in above-mentioned optical cavity Gas molecule NO2Gas when, the luminous intensity in this wavelength band has obvious decaying, and the ratio to decay at different wave length is not Together, occurrence depends on NO2Absorption at these wavelength is strong and weak.Therefore, in the embodiment of the present application, control computer can be right Light intensity map I (λ) carries out spectral data analysis, to analyze the atmospheric molecule NO of concentration undetermined2And its concentration.
In the embodiment of the present application, in atmospheric molecule detection system shown in Fig. 1, the atmospheric molecule containing concentration undetermined Gas can be pumped into the optical cavity by air-extractor (a such as metering aspiration pump).If the atmosphere containing concentration undetermined Ambient particle object in the gas of molecule is dense, and the delustring as caused by ambient particle object is very strong, can be added in air inlet One particulate filter (such as Particulate filter) is filtered ambient particle object.In other words, particulate filter (as Grain object filter membrane) it may be used to the gas of the atmospheric molecule containing concentration undetermined after particulate filter filtering Into in the optical cavity.
In the embodiment of the present application, in atmospheric molecule detection system shown in Fig. 1, the hardware for needing to process has:
(1) optical cavity structure:
Referring to Fig. 2, Fig. 2 is a kind of structural schematic diagram of optical cavity structure disclosed in the embodiment of the present application.As shown in Fig. 2, The optical cavity structure includes:
The left end of cavity pipe 11, the cavity pipe 11 is equipped with the first high reflection mirror 21, and the right end of the cavity pipe 11 is equipped with Second high reflection mirror 22;Wherein, the cavity pipe 11, first high reflection mirror 21 and second high reflection mirror 22 can be with Constitute the optical cavity described above;
Wherein, the mirror surface of the mirror surface of first high reflection mirror 21 and second high reflection mirror 22 realizes collimation;It is described The outside of first high reflection mirror 21 is equipped with the first convex lens 31, and the outside of second high reflection mirror 22 is equipped with the second convex lens 32;
The first end of first optical fiber 41 is used to connect the emission port of light source, and the second end of first optical fiber 41 is (i.e. described The terminal of first optical fiber) it is placed in the outside focus of first convex lens 31;The first end of second optical fiber 42 is for connecting Spectrometer is connect, the second end (terminal of i.e. described second optical fiber) of second optical fiber 42 is placed on second convex lens In the focus of outside;
When being full of the gas of the atmospheric molecule containing concentration undetermined in the cavity pipe 11, first convex lens 31 is right The cavity pipe is injected and (injected from first high reflection mirror 21 of left end) after the collimation of light derived from first optical fiber 41 11, so that light leaves the cavity pipe 11 after roundtrip is multiple between two sides high reflection mirror (i.e. 21 and 22) and via institute It states the second convex lens 32 to focus on second optical fiber 42, then imports the spectrometer via second optical fiber 42.
Wherein, the spectrometer can carry out light splitting and photon detection, to obtain the luminous intensity of one wavelength range of covering Figure I (λ) is simultaneously supplied to control computer, to calculate the concentration c of the atmospheric molecule of the concentration undetermined.
As an alternative embodiment, in the embodiment of the present application, the optical cavity structure can also include:
The left end of the cavity pipe 11, and institute is arranged in first optical motion seat 51, the first optical motion seat 51 The first high reflection mirror 21 is stated to be fixed on the first optical motion seat 51;
The first optical motion seat 51 is equipped with the tilt angle for adjusting first high reflection mirror 21, so that institute The mirror surface of the mirror surface and second high reflection mirror 22 of stating the first high reflection mirror 21 realizes the adjusting screw 61 of collimation.
As an alternative embodiment, in the embodiment of the present application, the optical cavity structure can also include:
The outer of the first optical motion seat 51 is arranged in second optical motion seat 52, the second optical motion seat 52 Side, and first convex lens 31 is fixed on the second optical motion seat 52;
The second optical motion seat 52 is equipped with high anti-relative to described first for adjusting first convex lens 31 The tilt angle of mirror 21 is penetrated, so that first convex lens 31 and first high reflection mirror 21 realize the tune of collimation between the two Save screw 61.
As an alternative embodiment, in the embodiment of the present application:
The second end of first optical fiber 41 is arranged on the second optical motion seat 52, and second optics is transported It is additionally provided on dynamic seat 52 for the distance between the second end of the first optical fiber 41 and first convex lens 31 described in Level tune, So that the second end of first optical fiber 41 is placed on the optical fiber adjusting knob in the outside focus of first convex lens 31 62。
As an alternative embodiment, in the embodiment of the present application, the optical cavity structure can also include:
The right end of the cavity pipe 11, and institute is arranged in third optical motion seat 53, the third optical motion seat 53 The second high reflection mirror 22 is stated to be fixed on the third optical motion seat 53;
The third optical motion seat 53 is equipped with the tilt angle for adjusting second high reflection mirror 22, so that institute The mirror surface of the mirror surface and first high reflection mirror 21 of stating the second high reflection mirror 22 realizes the adjusting screw 61 of collimation.
As an alternative embodiment, in the embodiment of the present application, the optical cavity structure can also include:
The outer of the third optical motion seat 53 is arranged in 4th optical motion seat 54, the 4th optical motion seat 54 Side, and second convex lens 32 is fixed on the 4th optical motion seat 54;
The 4th optical motion seat 54 is equipped with high anti-relative to described second for adjusting second convex lens 32 The tilt angle of mirror 22 is penetrated, so that second convex lens 32 and second high reflection mirror 22 realize the tune of collimation between the two Save screw 61.
As an alternative embodiment, the second end of second optical fiber 42 is arranged in institute in the embodiment of the present application It states on the 4th optical motion seat 54, and is additionally provided on the 4th optical motion seat 54 for the second optical fiber described in Level tune The distance between 42 second end and second convex lens 32 so that the second end of second optical fiber 42 be placed on it is described Optical fiber adjusting knob 62 in the outside focus of second convex lens 32.
As an alternative embodiment, in the embodiment of the present application:
From the first optical motion seat 51 to being disposed with the first bellows 71 left end of the cavity pipe 11 With the first microscope base and chamber mount 81;
81 are equipped with the air inlet pipe 811 for being pumped into gas to the cavity pipe 11 on first microscope base and chamber mount.
As an alternative embodiment, in the embodiment of the present application:
The second bellows 72 is disposed with from the third optical motion seat 53 to the right end of the cavity pipe 11 With the second microscope base and chamber mount 82;
Second microscope base and chamber mount 82 are equipped with for the escape pipe 821 for 11 output gas of cavity pipe.
As an alternative embodiment, in the embodiment of the present application:
It is additionally provided on first microscope base and chamber mount 81 for inputting purge gass to block in the cavity pipe 11 The first purge gass air inlet pipe 812 that gas is directly contacted with the mirror surface of first high reflection mirror 21;
It is additionally provided on second microscope base and chamber mount 82 for inputting purge gass to block in the cavity pipe 11 The second purge gass air inlet pipe 822 that gas is directly contacted with the mirror surface of second high reflection mirror 22;
Wherein, the purge gass include pure nitrogen gas, and flow velocity is by the diameter that adds in cleaning gas circuit between 50-70 microns Miniflow hole (critical orifice) control at 0.05-0.1 liters/min or so.
(2) light source: the light source can be incoherence intense light source, and incoherence intense light source can be using Gao Gong The single chip LED of rate (5-15W);Wherein, the number of the light source can be configured according to actual needs, this Shen Please embodiment be not construed as limiting.
In the embodiment of the present application, one or more incoherence intense light sources (such as LED) are welded in printable circuit board (PCB) On, then the PCB is fixed on thermoelectric (al) cooler (thermoelectric cooler), so as to by incoherence intense light source (such as LED) constant temperature is near such as 15 degrees Celsius, to realize the high stability of source emissioning light spectrum.Wherein, to the constant of temperature It can be realized by one feed circuit of design, feedback signal can be by a PT104 heat being attached on the thermoelectric (al) cooler Silk (thermistor) is hindered to provide.
It, can since the temperature stability of incoherence intense light source (such as LED) requires very high (positive and negative 0.01 degree Celsius) Between between incoherence intense light source (such as LED) and the PCB and the PCB and the thermoelectric (al) cooler (TE cooler) Gap coats high performance hot glue (thermal glue), to guarantee that efficient heat transfer may be implemented between them.Preferably, should The back side of PCB can be covered with wire, to facilitate the PCB quickly towards radiating on the thermoelectric (al) cooler.In short, any can add The method of heat transmitting between strong incoherence intense light source (such as the LED) → PCB → thermoelectric (al) cooler (TE cooler) is all It single can use or combination uses, the embodiment of the present application is not construed as limiting.
(3) gas circuit: in the embodiment of the present application, when the gas for the atmospheric molecule for needing to contain concentration undetermined toward optical cavity filling When body, a metering aspiration pump can use, perhaps add the combination of mass flowmenter using pump or utilize pump supernumerary segment flow tube The gas of atmospheric molecule containing concentration undetermined is pumped into institute by the air inlet of the optical cavity according to the flow velocity set by combination It states in optical cavity, until the gas full of the atmospheric molecule containing concentration undetermined in the optical cavity.When the past optical cavity of needs When filling zero gas, zero gas is usually from pure nitrogen gas or the steel cylinder of clean air, and zero gas after pressure reducing valve depressurizes, still can by air pressure A little higher than atmospheric pressure, therefore or the opposite direction (i.e. from gas outlet) of air inlet gas circuit from the optical cavity inject the optical cavity, and from Air inlet outflow;A triple valve is added in air inlet, gas circuit is switched to the gas circuit of zero gas from the gas circuit of atmospheric sample.
In the embodiment of the present application, atmospheric molecule detection system shown in FIG. 1 can also be there are three additionally may be used in terms of gas circuit Option:
(A) if, gas need to heat, can additionally plus one section of heating tube, the material of heating tube can be quartz glass (it is heated to 400-600 degrees Celsius if necessary, such as to NOyThe Concentration Testing of (i.e. nitrogenous object) needs first to be pyrolyzed for NOx) Or polyfluortetraethylene pipe (is heated to 100 degrees centigrades if necessary, and heats the aerochemistry activity height generated, Yi Biao Face loss, such as to N2O5Concentration Testing, need first to be pyrolyzed for NO3).The Concentration Testing of the latter is also required to guarantee figure 1 above In the temperature of the gassiness optical cavity and microscope base bracket it is also constant near 100 degrees Celsius, usually by optical cavity pipeline Upper winding heating sheet or heater strip paste heating sheet realization on microscope base bracket simultaneously.Similar to the constant temperature to light source, above-mentioned optical cavity Etc. the holdings of temperature be also required to use a temperature feedback loop.
(B) if, gas need chemical conversion appropriate, such as to nitric oxide NO and ozone O3Detection be respectively necessary for adding Add O3And NO, in order to convert the two in the optical cavity NO of significant light absorption2.It can be in the air inlet of the optical cavity Mouthful plus a gas tee tube, the branch of gas tee tube free time connect ambient atmosphere, the gas tee tube free time another Branch connects ozone generator or nitric oxide steel cylinder, big so that both adscititious gases are added to the external world in the optical cavity It is chemically reacted in gas, generates the NO for having significant light absorption2.Another branch generally also adds a solenoid valve, realizes Adscititious gases (such as O3And NO) opening and closing function.That is, different adscititious gases can be added to institute using solenoid valve It states optical cavity to be chemically reacted, to realize the gas full of the atmospheric molecule containing concentration undetermined in the optical cavity.
(3) if aerosol concentration is excessively high, the surface of high reflecting mirror surface may be attached to and then reduce its reflectivity, at this moment The property of can choose adds a cleaning gas circuit, to completely cut off contact of the ambient atmosphere with mirror surface.Wherein, the purge gass one of gas circuit are cleaned As be higher degree nitrogen, miniflow hole (critical of the flow velocity by the diameter that is added in gas circuit between 50-70 microns Orifice) control is at 0.05-0.1 liters/min or so.
(4) spectrometer and control computer: spectrometer is generally shaped commercial product, may be implemented to be divided, records different waves The functions such as the light intensity of long position.Controlling computer can be computer, control program and spectral data analysis program generally by opening Hair quotient oneself writes.
In the embodiment of the present application, the technical principle of atmospheric molecule detection system shown in FIG. 1 are as follows:
Gas full of the atmospheric molecule containing concentration undetermined in the optical cavity being made of two sides high reflection mirror;By light source (such as constant temperature light source of the thermostat and incoherence intense light source composition) light launched through the first optical fiber by exporting to first convex In the focus of lens, so that the first convex lens injects optical cavity after collimating to light, the light meeting two sides for being successfully entered optical cavity is high anti- It penetrates after roundtrip between mirror repeatedly dramatically increases absorption light path and leaves optical cavity, and focus on the second optical fiber via the second convex lens On, then import spectrometer via the second optical fiber and carry out light splitting and photon detection, to obtain the luminous intensity of one wavelength range of covering Scheme I (λ), λ indicates the wavelength of light;Light intensity map I (λ) is transferred to control computer, is controlled computer combination light intensity map I (λ) The concentration c of the atmospheric molecule of concentration undetermined is calculated with preset formula.
In the embodiment of the present application, control computer can be calculated in conjunction with the light intensity map I (λ) and following preset formula The concentration c of the atmospheric molecule of the concentration undetermined, it may be assumed that
Wherein, the λ indicates the wavelength of the light;The c is the concentration of the atmospheric molecule of the concentration undetermined;It is described σ (λ) is the absorption cross-section of the atmospheric molecule of the concentration undetermined, and the σ (λ) is known;The R (λ) is the high reflection mirror To the reflectivity of the light, and the R (λ) is known;The d is in the optical cavity full of the atmosphere for containing concentration undetermined The length of the part volume of the gas of molecule, and known to the d;The I0(λ) is in the optical cavity first full of without described The light intensity map that the spectrometer measures when zero gas of the atmospheric molecule of concentration undetermined.
As an example it is assumed that first full of without atmospheric molecule NO in the optical cavity2Zero gas when, what the spectrometer measured Light intensity map is I0(λ);The atmospheric molecule NO containing concentration undetermined will be full of in the optical cavity again2Gas, the spectrometer surveys The light intensity map obtained is I (λ), then control computer can be calculated according to the light intensity map I (λ) and following preset formula The atmospheric molecule NO of concentration undetermined2ConcentrationThat is:
Wherein, the λ indicates the wavelength of the light;It is describedFor the atmospheric molecule NO of the concentration undetermined2It is dense Degree;It is describedFor the atmospheric molecule NO of the concentration undetermined2Absorption cross-section, and it is describedIt is known;The R (λ) It is the high reflection mirror to the reflectivity of the light, and the R (λ) is known;The d is to contain in the optical cavity full of described The atmospheric molecule NO of concentration undetermined2Gas part volume length, and known to the d;In formula, I (λ),And R (λ) indicates that luminous intensity I, absorption cross-section σ and specular reflectivity R etc. are the function of wavelength X, changes (before i.e. with wavelength difference Described in text, NO2It is different to the absorption intensity of the light of different wave length).
In the embodiment of the present application, atmospheric molecule detection system shown in FIG. 1 is by directly measuring atmospheric molecule (such as NO2、 HCHO、CHOCHO、N2O5、NO3, HONO etc.) light absorption measure the concentration of atmospheric molecule, so not needing to use known concentration Calibrating gas demarcate the sensitivity coefficient of detecting instrument, so as to effectively, easily detect the concentration of atmospheric molecule and big The delustring of aerated particle object;In addition, light is anti-back and forth between the high reflection mirror of two sides in atmospheric molecule detection system shown in FIG. 1 It penetrates, absorption light path can be dramatically increased, it is ultralow so as to be effectively detected so as to dramatically increase the absorption of atmospheric molecule The atmospheric molecule concentration of concentration.
Based on atmospheric molecule detection system shown in FIG. 1, the embodiment of the present application further discloses a kind of atmospheric molecule detection Method.Referring to Fig. 3, Fig. 3 is a kind of flow diagram of atmospheric molecule detection method disclosed in the embodiment of the present application.Such as Fig. 3 Shown, which may comprise steps of:
301, the optical cavity being made of two sides high reflection mirror is provided, and full of big containing concentration undetermined in the optical cavity The gas of gas molecule;One end of the optical cavity is laid with the first convex lens, and the other end of the optical cavity is laid with the second convex lens.
Wherein, the mirror surface of the two sides high reflection mirror is facing each other.
302, by light that light source is launched by exporting through the first optical fiber to the focus of first convex lens, so that institute It states after the first convex lens collimates light and injects the optical cavity;Wherein, the light for being successfully entered the optical cavity is high on the two sides The optical cavity is left after roundtrip is multiple between reflecting mirror, and is focused on the second optical fiber via second convex lens, then Spectrometer is imported via second optical fiber and carries out light splitting and photon detection, to obtain the light intensity map of one wavelength range of covering I(λ);The λ indicates the wavelength of the light.
In the embodiment of the present application, light roundtrip between the high reflection mirror of two sides can dramatically increase absorption light path, inhale The receipts increased multiple of light path is 1/ (1-R), and wherein R is the specular reflectivity of high reflection mirror, it is assumed that R is 0.9999 and two sides is high anti- Penetrating the distance between mirror is 1 meter, then the absorption light path of ten thousand metres (i.e. 10 kilometers), root can be realized (in 1 meter of the spacing) According to Beer-Lambert law of light absorption, the absorption that the absorption light path of this overlength can dramatically increase atmospheric molecule (disappears Light), so as to which the atmospheric molecule concentration of super low concentration is effectively detected.
303, the light intensity map I (λ) is transferred to control computer, so that the control computer is in conjunction with the light intensity map I (λ) and preset formula calculate the concentration c of the atmospheric molecule of the concentration undetermined.
In the embodiment of the present application, control computer calculates described undetermined dense in conjunction with the light intensity map I (λ) and preset formula The concentration c of the atmospheric molecule of degree, comprising:
The control computer calculates the concentration undetermined in conjunction with the light intensity map I (λ) and following preset formula The concentration c of atmospheric molecule, it may be assumed that
Wherein, the λ indicates the wavelength of the light;The c is the concentration of the atmospheric molecule of the concentration undetermined;It is described σ (λ) is the absorption cross-section of the atmospheric molecule of the concentration undetermined, and the σ (λ) is known;The R (λ) is the high reflection mirror To the reflectivity of the light, and the R (λ) is known;The d is in the optical cavity full of the atmosphere for containing concentration undetermined The length of the part volume of the gas of molecule, and known to the d;The I0(λ) is in the optical cavity first full of without described The light intensity map that the spectrometer measures when zero gas of the atmospheric molecule of concentration undetermined.
As an alternative embodiment, the gas full of the atmospheric molecule containing concentration undetermined in the optical cavity Body, comprising:
Using a metering aspiration pump, the gas of the atmospheric molecule containing concentration undetermined is passed through according to the flow velocity set The air inlet of the optical cavity is pumped into the optical cavity, until full of the atmospheric molecule containing concentration undetermined in the optical cavity Gas;
Alternatively, the atmosphere containing concentration undetermined is divided according to the flow velocity set using the combination of pump plus mass flowmenter The gas of son is pumped into the optical cavity by the air inlet of the optical cavity, until containing concentration undetermined full of described in the optical cavity Atmospheric molecule gas;
Alternatively, the atmospheric molecule of concentration undetermined will be contained according to the flow velocity set using the combination of pump supernumerary segment flow tube Gas is pumped into the optical cavity by the air inlet of the optical cavity, until full of described big containing concentration undetermined in the optical cavity The gas of gas molecule.
As an alternative embodiment, in the atmospheric molecule detection method described in Fig. 3, if described containing needing The ambient particle object determined in the gas of the atmospheric molecule of concentration is dense, then adds a particle in the air inlet of the optical cavity Object filter, so that the gas of the atmospheric molecule containing concentration undetermined passes through the particulate matter mistake of air inlet addition Enter in the optical cavity after filter filtering.
As another optional embodiment, described in the light in the atmospheric molecule detection method described in Fig. 3 The intracavitary gas full of the atmospheric molecule containing concentration undetermined, comprising:
Different adscititious gases are added to the optical cavity using solenoid valve to chemically react, to realize in the optical cavity The interior gas full of the atmospheric molecule containing concentration undetermined.
As an alternative embodiment, the light source includes non-in the atmospheric molecule detection method described in Fig. 3 Coherence's intense light source, wherein incoherence intense light source may include light emitting diode (LED), correspondingly, described in Fig. 3 In atmospheric molecule detection method, constant temperature can also be carried out to the light source using thermostat, to realize constant temperature light source;Wherein, institute Stating thermostat includes thermoelectric (al) cooler.
It is described to utilize thermostat to the light in the atmospheric molecule detection method described in Fig. 3 in the embodiment of the present application Source carries out constant temperature, to realize constant temperature light source, comprising:
The incoherence intense light source is welded on printable circuit board (PCB), then the printable circuit board is fixed On the thermoelectric (al) cooler, and in incoherence intense light source and the printable circuit board and the printable circuit board High performance hot glue is coated in gap between the thermoelectric (al) cooler, to take the photograph coherence's intense light source constant temperature specified Near family name's degree, to realize constant temperature light source;The incoherence intense light source includes one or more light emitting diodes.
In the atmospheric molecule detection method described in Fig. 3, by directly measuring atmospheric molecule (such as gas NO2、HCHO、 CHOCHO、N2O5、NO3, HONO etc.) light absorption measure the concentration of atmospheric molecule, so do not need the standard with known concentration Gas demarcates the sensitivity coefficient of detecting instrument, so as to effectively, easily detecting the concentration and atmosphere of above-mentioned atmospheric molecule The delustring of particulate matter;In addition, in the atmospheric molecule detection method described in Fig. 3, light between the high reflection mirror of two sides back and forth Reflection, can dramatically increase absorption light path, super so as to be effectively detected so as to dramatically increase the absorption of atmospheric molecule The atmospheric molecule concentration of low concentration.
Based on optical cavity structure shown in Fig. 2, the embodiment of the present application further discloses in a kind of optical cavity structure convex lens and high The installation method of reflecting mirror.Referring to Fig. 4, Fig. 4 is anti-for convex lens in a kind of optical cavity structure disclosed in the embodiment of the present application and height Penetrate the flow diagram of the installation method of mirror.Wherein, the optical cavity structure installed using installation method described in Fig. 4 can be with As shown in Figure 2.Wherein, which may comprise steps of:
401, the mirror surface of the mirror surface and second high reflection mirror that adjust first high reflection mirror realizes collimation.
In the embodiment of the present application, the adjusting screw on the adjustable first optical motion seat is high to adjust described first The tilt angle of reflecting mirror, and/or the adjusting screw on the third optical motion seat is adjusted to adjust second high reflection The tilt angle of mirror, so that the mirror surface of the mirror surface of first high reflection mirror and second high reflection mirror realizes collimation.
402, it adjusts first convex lens and first high reflection mirror realizes collimation between the two.
In the embodiment of the present application, realized in the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror quasi- When straight, adjusting screw on the adjustable second optical motion seat, to adjust first convex lens relative to described The tilt angle of one high reflection mirror, so that first convex lens and first high reflection mirror realize collimation between the two.
403, it adjusts the second convex lens and second high reflection mirror realizes collimation between the two.
In the embodiment of the present application, realized in the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror quasi- When straight, adjusting screw on the adjustable 4th optical motion seat, to adjust second convex lens relative to described The tilt angle of two high reflection mirrors, so that second convex lens and second high reflection mirror realize collimation between the two.
As an alternative embodiment, the spectrum can be further looked in the installation method described in Fig. 4 The light intensity value of the emergent light for the optical cavity structure that instrument is shown shows first high reflection mirror when the light intensity value maximum From each other and first convex lens and second convex lens reach complete from each other with second high reflection mirror Collimation, adjusting finish.
For example, in the embodiment of the present application, described first, second, third and the 4th optical motion seat may include But it is not limited to the KC1-T optical adjusting frame of Thorlabs company.
The embodiment of the present application may be implemented it is all in 340-900nm wave-length coverage have feature structure absorb The Concentration Testing of the atmospheric molecule of (structured absorption), comprising:
(a) formaldehyde (HCHO), 1/1000000000th to 10,000,000,000 or so, testing result can be used to detect indoor detection limit Concentration of formaldehyde, and due to the reliability and accuracy of its result, it can be used as " goldstandard " of indoor formaldehyde detection, for calibrating, Verify relatively inexpensive, portable formaldehyde sensor and detection device;
(b) glyoxal (CHOCHO), minimum detection limit is generally 1/100000000000th or so.Since glyoxal is atmosphere benzene And substituted benzene (mainly from motor vehicle exhaust emission, industrial discharge and plant discharging) and isoprene are (mainly from plant Object discharge and vehicle exhaust etc.) important intermediate that is generated during atmospheric oxidn, liquid phase reactor, which is recognized as, may be One of source of secondary particulate, so the detection of glyoxal is extremely important to Atmospheric Chemistry research.In addition, formaldehyde and glyoxal Photodissociation can generate HO2Free radical, the free radical and NO's further reacts the generation that will lead to OH free radical, so monitoring simultaneously Formaldehyde and glyoxal help completely to understand the OH free radical source (note: OH of the main photodissociation aldehyde contribution in atmosphere Free radical is most important oxidative free radical in atmosphere);
(c) nitrogen dioxide (NO2)/nitric oxide (NO)/ozone (O3): where NO2It can directly supervised by this technology It surveys, NO and O3O is added respectively3And NO, they are separately converted to NO2It monitors again afterwards.The embodiment of the present application is practical to be provided together When monitor the reference instrument schemes of these three typical atmosphere pollutions;
(d) nitrogen pentoxide (N2O5)/nitrogen peroxide (NO3): both substances are the nitrogen oxides (NO+NO in atmosphere2) Night is by ozone O3The important activity intermediate of oxidation, helps completely to understand above two nitrogen oxides and exists to their monitoring Oxidation mechanism in atmosphere and its atmospheric chemistry process (such as N specifically participated in2O5It is converted into nitric acid, NO3Oxidation volatile has Machine object);
(e) iodine oxide (IO) and iodine steam (I2): both substances are Marine stratocumulus (MBL, Marine Boundary Layer) inner important activity intermediate, it has great significance to the ozone depletion in catalysis MBL;
(f) nitrous acid (HONO): in contaminated shallow-layer atmosphere, such as 100-300 meters of urban ground etc. most important OH Free radical source.In addition to this, the optical cavity for measuring HONO can measure NO simultaneously2, both of which is that the burning of indoor fuel gas stove is released The important indoor polluted gas released.
(g) aerosol extinction (aerosol extinction): if particulate filter is not added in air inlet (aerosol filter), then particulate matter can enter delustring caused by cavity and then directly measure is shut out the light as particulate matter Value.
Wherein, implement the embodiment of the present application, can measure arbitrarily ultraviolet-visible optical band have absorption atmospheric molecule and Aerosol extinction.In general, the sensitivity of system and method disclosed in the embodiment of the present application is mainly by the following factor Influence:
(1) height in the characteristic absorption section of molecule.This value is higher, sensitiveer to the detection of the molecule, detection limit It is lower.
(2) reflectivity of high reflection mirror, transmissivity height.The former determines the optical length that may finally be realized, the latter Light is then determined when by high reflection mirror, in addition to by reflection, (i.e. 1-R) how many ratio is not damaged lost territory in remaining ratio Success penetrates convex lens.Therefore, the height that comprehensively consider the two values when high reflection mirror is selected, is reasonably selected.
(3) energy density of the unit area of light source.This value is higher, can be imported into optical fiber and eventually enter into the light of optical cavity It is strong higher.When final noise is controlled by shot noise (shot noise), light intensity is stronger, and sensitivity is higher.In 330- In the wave-length coverage of 900nm, the unit area luminous energy and efficiency of light emitting diode (LED) are highest, so generally taking LED does light source.If desired shorter ultraviolet wavelength is used, is also required to consider other light sources such as deuterium lamp or mercury lamp sometimes.
(4) thermal stability of light source.Since what is surveyed is being inhaled on higher smooth background signal by atmospheric molecule The variation of the extremely faint signal caused by receiving, the drift of the background signal caused by even very faint light source thermal drift Shifting is also enough to exceed molecule absorption signal to be measured, and then influences minimum detection limit.When doing light source with LED, generally with thermoelectric cold But device will do constant temperature to it and wrap up heat insulation foam, its temperature is stablized within 0.01 degree Celsius.
(5) thermal stability and mechanical stability of optical cavity.It is required that the optical cavity of design in variation of ambient temperature, collimates (alignment) not because expanding with heat and contract with cold for material has significant change.Secondly, it is intracavitary it is outer have pressure difference when (as done aboard When observation), optical cavity will have enough mechanical strengths, it is ensured that the collimation of two-face mirror does not occur obviously to become because of the extruding of pressure Change.For example, can use carbon fiber pipe does cavity (because its thermal expansion coefficient is small) or with four carbon fiber pipe supports (because of its density Small and high mechanical strength) microscope base bracket and optical motion seat shown in upper figure be so that it keeps collimating under pressure difference environment.
The embodiment of the present application further discloses a kind of computer storage medium, and the computer storage medium is based on storing Calculation machine program, wherein the computer program makes computer execute the atmospheric molecule detection disclosed in the embodiment of the present application Method.
The embodiment of the present application further discloses a kind of computer program product including instruction, the computer program product When running on computers, so that the computer executes the atmospheric molecule detection method disclosed in the embodiment of the present application.
Those of ordinary skill in the art will appreciate that all or part of the steps in the various methods of above-described embodiment is can It is completed with instructing relevant hardware by program, which can be stored in a computer readable storage medium, storage Medium include read-only memory (Read-Only Memory, ROM), random access memory (Random Access Memory, RAM), programmable read only memory (Programmable Read-only Memory, PROM), erasable programmable is read-only deposits Reservoir (Erasable Programmable Read Only Memory, EPROM), disposable programmable read-only memory (One- Time Programmable Read-Only Memory, OTPROM), the electronics formula of erasing can make carbon copies read-only memory (Electrically-Erasable Programmable Read-Only Memory, EEPROM), CD-ROM (Compact Disc Read-Only Memory, CD-ROM) or other disc memories, magnetic disk storage, magnetic tape storage or can For carrying or any other computer-readable medium of storing data.
Above to atmospheric molecule detection system, optical cavity structure disclosed in the embodiment of the present application, atmospheric molecule detection system with And the installation method of convex lens and high reflection mirror is described in detail in optical cavity structure, specific case used herein is to this The principle and embodiment of application is expounded, the present processes that the above embodiments are only used to help understand and Its core concept;At the same time, for those skilled in the art in specific embodiment and is answered according to the thought of the application With in range, there will be changes, in conclusion the contents of this specification should not be construed as limiting the present application.

Claims (10)

1. the installation method of convex lens and high reflection mirror in a kind of optical cavity structure, which is characterized in that the cavity of the optical cavity structure The left end of pipe is equipped with the first high reflection mirror, and the right end of the cavity pipe is equipped with the second high reflection mirror;First high reflection mirror Outside is equipped with the first convex lens, and the outside of second high reflection mirror is equipped with the second convex lens;The first end of first optical fiber is used for The emission port of light source is connected, the second end of first optical fiber is placed in the outside focus of first convex lens;Second For the first end of optical fiber for connecting spectrometer, the outside that the second end of second optical fiber is placed on second convex lens is burnt Point on;The described method includes:
The mirror surface of the mirror surface and second high reflection mirror that adjust first high reflection mirror realizes collimation;
It adjusts first convex lens and first high reflection mirror realizes collimation between the two;
It adjusts the second convex lens and second high reflection mirror realizes collimation between the two.
2. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 1, which is characterized in that described Method further include:
The light intensity value for observing the emergent light for the optical cavity structure that the spectrometer is shown shows when the light intensity value maximum First high reflection mirror and second high reflection mirror are from each other and first convex lens and second convex lens Reach entirely collimated from each other, adjusting finishes.
3. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 1 or 2, which is characterized in that The method also includes:
First optical motion seat is set, and the left end of the cavity pipe, and described first is arranged in the first optical motion seat High reflection mirror is fixed on the first optical motion seat;
The first optical motion seat is equipped with the adjusting screw for adjusting the tilt angle of first high reflection mirror.
4. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 3, which is characterized in that described Method further include:
Second optical motion seat is set, the outside of the first optical motion seat is arranged in the second optical motion seat, and First convex lens is fixed on the second optical motion seat;
The second optical motion seat is equipped with for adjusting the first convex lens inclining relative to first high reflection mirror The adjusting screw of rake angle.
5. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 4, which is characterized in that described Method further include:
Third optical motion seat is set, and the right end of the cavity pipe, and described second is arranged in the third optical motion seat High reflection mirror is fixed on the third optical motion seat;
The third optical motion seat is equipped with the adjusting screw for adjusting the tilt angle of second high reflection mirror.
6. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 5, which is characterized in that described Method further include:
4th optical motion seat is set, the outside of the third optical motion seat is arranged in the 4th optical motion seat, and Second convex lens is fixed on the 4th optical motion seat;
The 4th optical motion seat is equipped with for adjusting the second convex lens inclining relative to second high reflection mirror The adjusting screw of rake angle.
7. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 6, which is characterized in that described The mirror surface of the mirror surface and second high reflection mirror that adjust first high reflection mirror realizes collimation, comprising:
The adjusting screw on the first optical motion seat is adjusted to adjust the tilt angle of first high reflection mirror, and/or The adjusting screw on the third optical motion seat is adjusted to adjust the tilt angle of second high reflection mirror, so that described The mirror surface of the mirror surface of one high reflection mirror and second high reflection mirror realizes collimation.
8. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 7, which is characterized in that described It adjusts first convex lens and first high reflection mirror realizes collimation between the two, comprising:
When the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror realize collimation, second light is adjusted The adjusting screw in kinematic nest is learned, to adjust tilt angle of first convex lens relative to first high reflection mirror, with First convex lens and first high reflection mirror is set to realize collimation between the two.
9. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 8, which is characterized in that described It adjusts the second convex lens and second high reflection mirror realizes collimation between the two, comprising:
When the mirror surface of first high reflection mirror and the mirror surface of second high reflection mirror realize collimation, the 4th light is adjusted The adjusting screw in kinematic nest is learned, to adjust tilt angle of second convex lens relative to second high reflection mirror, with Second convex lens and second high reflection mirror is set to realize collimation between the two.
10. the installation method of convex lens and high reflection mirror in optical cavity structure according to claim 9, which is characterized in that institute State method further include:
From the first optical motion seat to set gradually the left end of the cavity pipe the first bellows and the first microscope base and Chamber mount;
Air inlet pipe for being pumped into from gas to the cavity pipe is set on first microscope base and chamber mount;
From the third optical motion seat to set gradually the right end of the cavity pipe the second bellows and the second microscope base and Chamber mount;
The escape pipe of the cavity pipe output gas is provided on second microscope base and chamber mount;
The gas blocked in the cavity pipe for inputting purge gass is further set on first microscope base and chamber mount The first purge gass air inlet pipe that body is directly contacted with the mirror surface of first high reflection mirror;
The gas blocked in the cavity pipe for inputting purge gass is further set on second microscope base and chamber mount The second purge gass air inlet pipe that body is directly contacted with the mirror surface of second high reflection mirror;
Wherein, the purge gass include pure nitrogen gas.
CN201811025993.2A 2018-09-04 2018-09-04 The installation method of convex lens and high reflection mirror in a kind of optical cavity structure Pending CN109115683A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201811025993.2A CN109115683A (en) 2018-09-04 2018-09-04 The installation method of convex lens and high reflection mirror in a kind of optical cavity structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201811025993.2A CN109115683A (en) 2018-09-04 2018-09-04 The installation method of convex lens and high reflection mirror in a kind of optical cavity structure

Publications (1)

Publication Number Publication Date
CN109115683A true CN109115683A (en) 2019-01-01

Family

ID=64860628

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201811025993.2A Pending CN109115683A (en) 2018-09-04 2018-09-04 The installation method of convex lens and high reflection mirror in a kind of optical cavity structure

Country Status (1)

Country Link
CN (1) CN109115683A (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103149156A (en) * 2013-03-19 2013-06-12 中国气象科学研究院 Double-channel light cavity ring-down atmospheric aerosol extinction instrument and extinction factor measuring method
CN104596955A (en) * 2014-12-11 2015-05-06 中国科学院合肥物质科学研究院 Cavity enhanced absorption spectrum device and method for simultaneous measurement of trace gas concentration and aerosol extinction
CN206710299U (en) * 2017-04-22 2017-12-05 杭州春来科技有限公司 A kind of return gas compartment in former road based on ultraviolet difference absorption spectroscopy techniques
CN207232494U (en) * 2017-10-11 2018-04-13 中国工程物理研究院激光聚变研究中心 A kind of adjustable fixed Mirror frame structure

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103149156A (en) * 2013-03-19 2013-06-12 中国气象科学研究院 Double-channel light cavity ring-down atmospheric aerosol extinction instrument and extinction factor measuring method
CN104596955A (en) * 2014-12-11 2015-05-06 中国科学院合肥物质科学研究院 Cavity enhanced absorption spectrum device and method for simultaneous measurement of trace gas concentration and aerosol extinction
CN206710299U (en) * 2017-04-22 2017-12-05 杭州春来科技有限公司 A kind of return gas compartment in former road based on ultraviolet difference absorption spectroscopy techniques
CN207232494U (en) * 2017-10-11 2018-04-13 中国工程物理研究院激光聚变研究中心 A kind of adjustable fixed Mirror frame structure

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
向必纯 等: "《大学物理实验》", 29 February 2008 *
李润求等: "《安全监测监控原理与仪表》", 28 February 2018 *

Similar Documents

Publication Publication Date Title
Pettersson et al. Measurement of aerosol optical extinction at 532nm with pulsed cavity ring down spectroscopy
Baynard et al. Design and application of a pulsed cavity ring-down aerosol extinction spectrometer for field measurements
Lack et al. Aircraft instrument for comprehensive characterization of aerosol optical properties, part 2: Black and brown carbon absorption and absorption enhancement measured with photo acoustic spectroscopy
Ajtai et al. A novel multi− wavelength photoacoustic spectrometer for the measurement of the UV–vis-NIR spectral absorption coefficient of atmospheric aerosols
Stritzke et al. TDLAS-based NH 3 mole fraction measurement for exhaust diagnostics during selective catalytic reduction using a fiber-coupled 2.2-µm DFB diode laser
US20060290944A1 (en) Method and apparatus for photoacoustic measurements
US5281816A (en) Method and apparatus for detecting hydrocarbon vapors in a monitored area
Rooth et al. Photoacoustic measurement of ammonia in the atmosphere: influence of water vapor and carbon dioxide
US8139222B2 (en) Pressure controlled spectroscopic heating value sensor
US20020026822A1 (en) Vehicle gas emission sampling and analysis assembly
CN108956503A (en) A kind of hydrone density calculating method
Nakayama et al. Measurements of aerosol optical properties in central Tokyo during summertime using cavity ring-down spectroscopy: Comparison with conventional techniques
CN109187355A (en) A kind of purging gas path device applied to optical cavity structure
Thompson et al. A fixed frequency aerosol albedometer
KR20010034643A (en) Device and method for directly measuring calorific energy contained in a fuel gas
CN109100316A (en) A kind of high reflection mirror screening technique applied to optical cavity structure
CN108956502A (en) A kind of atmospheric molecule detection system
CN109187344A (en) A kind of gas circuit structure applied to atmospheric molecule detection system
CN109211807A (en) A kind of atmospheric molecule detection system having pre-reformer before gas is examined
CN109115683A (en) The installation method of convex lens and high reflection mirror in a kind of optical cavity structure
CN108956471A (en) The installation method of convex lens and optical fiber in a kind of optical cavity structure
CN108956475A (en) A kind of optical cavity structure
CN109001132A (en) A kind of atmospheric molecule detection method
CN109060691A (en) A kind of calculation method and equipment of atmospheric molecule concentration
CN109187354A (en) A kind of purging gas path device suitable for optical cavity structure

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
RJ01 Rejection of invention patent application after publication

Application publication date: 20190101

RJ01 Rejection of invention patent application after publication