CN103076107B - Terahertz pulse measurement-based burning temperature sensing device and method - Google Patents

Terahertz pulse measurement-based burning temperature sensing device and method Download PDF

Info

Publication number
CN103076107B
CN103076107B CN201310019184.1A CN201310019184A CN103076107B CN 103076107 B CN103076107 B CN 103076107B CN 201310019184 A CN201310019184 A CN 201310019184A CN 103076107 B CN103076107 B CN 103076107B
Authority
CN
China
Prior art keywords
temperature
terahertz
pulse
terahertz pulse
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.)
Active
Application number
CN201310019184.1A
Other languages
Chinese (zh)
Other versions
CN103076107A (en
Inventor
刘亦安
王玲
徐英
邹绍芳
吴开华
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.)
Hangzhou Dianzi University
Hangzhou Electronic Science and Technology University
Original Assignee
Hangzhou Electronic Science and Technology 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 Hangzhou Electronic Science and Technology University filed Critical Hangzhou Electronic Science and Technology University
Priority to CN201310019184.1A priority Critical patent/CN103076107B/en
Publication of CN103076107A publication Critical patent/CN103076107A/en
Application granted granted Critical
Publication of CN103076107B publication Critical patent/CN103076107B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The invention discloses a terahertz pulse measurement-based burning temperature sensing device and a terahertz pulse measurement-based burning temperature sensing method. Laser is emitted from a femtosecond laser device, and is divided into reference laser and detection laser through a beam splitter, the detection laser is focused on a photoconduction antenna type terahertz emitter, terahertz pulses emitted by the terahertz emitter are focused on a ZnTe crystal through an off-axis paraboloid lens group; and the reference layer is collimated and is coincident with terahertz waves focused on the ZnTe crystal after passing through a semi-transmission and self-reflection mirror, parallel grating groups and a polarizing film, the terahertz waves are modulated by using Pockels effect of the ZnTe crystal, and image signals corresponding to collected first reference layer carrying terahertz pulse strength information and second reference laser not carrying the terahertz pulse strength information are input into a computer by a CCD (Charge Coupling Device) detector for subsequence processing. According to the invention, the precision and speed of the non-contact combustion measurement method are increased, and the non-contact measurement of combustion object temperature and temperature distribution is realized.

Description

The temperature of combustion sensing device measured based on terahertz pulse and method
Technical field
The invention belongs to combustion supervision technical field, particularly relate to a kind of temperature of combustion sensing device based on terahertz pulse measurement and method.
Background technology
Combustion phenomena is present in numerous industries such as petrochemical complex, space flight, metallurgy and electric power widely.In combustion reaction process, chemical energy is constantly converted to heat energy and electric energy, constantly carries out conducting heat, mass transfer and chemical reaction process simultaneously.The gaseous products such as carbon dioxide, carbon monoxide, oxynitrides, sulphuric dioxide and water vapor releases heat simultaneously can be produced in combustion process.For ensureing the sustainable development of China's economic, China in Recent Years government and scientific and technological circle pay attention to the investigation and application that energy efficiency improves more.But due to combustion process very complicated, therefore need especially to use among novel combustion supervision technology to the analysis of burning and research, thus promote efficiently, the combustion model of environmental protection and the foundation of pollution formation model.In the testing process of burning, temperature is crucial parameter, and the real-time Measurement accuracy of temperature of combustion and Temperature Distribution all has important effect for all many-sides such as safety in production, raising burning efficiency, reduction pollutants.
Temperature of combustion sensing measuring method substantially can be divided into two classes principle: contact measurement method and contactless measurement.Wherein, the cardinal principle of contact type measurement is the change utilizing the heat-sensitive element such as thermopair, thermal resistance that voltage or resistance can occur when temperature variation, thus obtains the value of temperature.The patent No. is the measurement that the thermopair being enclosed with protection tube and Metal Packaging layer is used for temperature by " thermocouple temperature sensor of fast response time " of CN102607731A.The patent No. is that " fibre optic temperature sensor " of CN102483360A carrys out sensing detection temperature by the light quantity accepted after changing the light reflection of the covered light quantity of the light that transmitted by optical fiber or transmission.The feature of contact type measurement be with low cost, measure reliable, be one of measuring method of widespread use the most at present.But the metering system of contact can produce disturbance to measurand, it is measured response and often cannot follow the tracks of fast-changing temperature, and sensitive element is easy to be subject to the pollution of high temperature or corrosive gas medium and reduces reliability.In addition, utilize the contact type measurement of single thermopair or thermal resistance can only measure single-point, the truth of whole burning object inside cannot be understood.Non-contacting measuring method is another important directions of combustion temperature measurement, and contactless measuring technique method includes optical method, the method for a new generation such as acoustic method, and they mainly utilize light wave or acoustic signals to realize measuring to the response of different temperatures.The patent No. is that " measuring boiler combustion radiation energy and temperature field and the method for control combustion and system thereof " of CN1388340A utilizes CCD to gather burning image, is measured the temperature of burning by the mode of image procossing.The patent No. is that " three dimension temperature field realtion monitor in coal burning boiler " of CN1587930A passes through to arrange the method acceptance of multiple camera in burner hearth from the radiation information of all directions in burner hearth, adopts special noniterative algorithm to calculate the distribution of burner hearth combustion temperature.The advantage of contactless measurement is fast response time, and measurement can not produce interference to burning object.Along with science and technology and the progress of yield-power, study the research that quick, highly sensitive temperature of combustion method for sensing can help people to deepen combustion mechanism, people can be helped again to carry out analysis and control to the pollutant produced in combustion process.
Summary of the invention
The object of the invention is for the deficiencies in the prior art, a kind of temperature of combustion sensing device based on terahertz pulse measurement and method are proposed, improve precision and the measuring speed of existing noncontact combustion measurement method, realize the temperature of burning object and the non-cpntact measurement of Temperature Distribution.
The technical solution adopted for the present invention to solve the technical problems is as follows:
The present invention includes femto-second laser, beam splitter, the first plane mirror, the second plane mirror, the 3rd plane mirror, condenser lens, photoconductive antenna type terahertz transmitter, off axis paraboloidal mirror group, the first semi-transparent reflection mirror, the second semi-transparent reflection mirror, parallel grating group, plane mirror, the first polaroid, the second polaroid, ito glass, ZnTe crystal, ccd detector, computing machine, function generator, high frequency power amplifier, one dimensional optical translation stage.
Laser is launched from femto-second laser, after beam splitter light splitting, be divided into reference laser and exploring laser light two-way, wherein exploring laser light is successively by the first plane mirror, second plane mirror, focus in photoconductive antenna type terahertz transmitter by condenser lens after 3rd plane mirror reflection, photoconductive antenna type terahertz transmitter launches terahertz pulse under the voltage drive effect of exploring laser light and high frequency power amplifier, terahertz pulse becomes parallel THz wave after the collimation of the off axis paraboloidal mirror of off axis paraboloidal mirror group side, and through combustion zone, parallel THz wave converges on ZnTe crystal by the off axis paraboloidal mirror of opposite side, the reference laser that beam splitter separates incides in pair of parallel grating group after the first semi-transparent reflection mirror, reference laser through parallel grating group is reflected back parallel grating group by plane mirror, thus achieve frequency chirp and the time explanation of reference laser, reference laser after time explanation is reflected through the first polaroid by the first semi-transparent reflection mirror, reference laser through the first polaroid reflexes on ZnTe crystal by ito glass, overlap with the THz wave collimation converged on ZnTe crystal, Pockels (Pockels) effect of ZnTe crystal is utilized to realize Terahertz wave modulation, after polarization state is passed the second semi-transparent reflection mirror by the first reference laser that THz wave is modulated, again through the second polaroid, the first reference laser carrying terahertz pulse strength information is reflexed to ccd detector detection by the 4th plane mirror and accepts, simultaneously due to the birefringence effect of ZnTe crystal, do not carry the second reference laser of terahertz pulse strength information through the second semi-transparent reflection mirror, 6th plane mirror, also incide ccd detector after 5th plane mirror reflection and be detected reception, ccd detector by the first reference laser carrying terahertz pulse strength information collected and do not carry terahertz pulse strength information the second reference laser corresponding to picture signal input computing machine carry out subsequent treatment.Function generator produces fundamental frequency sine wave signal and is input to high frequency power amplifier, high frequency power amplifier drives the photoconductive antenna type terahertz transmitter cycle to produce terahertz pulse, and function generator produces the twice that the sampling period of the frequency multiplication square-wave signal control ccd detector of frequency multiplication is terahertz pulse transmission frequency simultaneously.
Described parallel grating group is one group of grating of parallel placement, and the reference laser pulse-echo after parallel grating group chirp spread is returned input path by plane mirror.
The reference laser pulse that described ito glass makes to reflex on ZnTe crystal is coaxial with the terahertz pulse concurrent converged on ZnTe crystal.
Described one dimensional optical translation stage placed the first plane mirror, the second plane mirror, by optical delay method, terahertz pulse is positioned in the duration of synchronizing detection pulse, simultaneously by the adjustment of one dimensional optical translation stage, the image space of terahertz pulse is adjusted to the middle section of ccd detector.
Described function generator produces the voltage signal of two kinds of different frequencies, is fundamental frequency sine wave pulse signal and frequency multiplication rectangular wave pulse signal respectively.Fundamental frequency sine wave signal is input to high frequency power amplifier, periodic voltage excitation photoconductive antenna type terahertz transmitter being formed photoconductive antenna is loaded into after amplifying, the photo-generated carrier of moment is produced when exploring laser light incides in photoconductive antenna type terahertz transmitter, photo-generated carrier gives off terahertz pulse under positive half cycle sinusoidal voltage excitation, and non-radiating is gone out terahertz pulse by photo-generated carrier under the excitation of negative half period sinusoidal voltage.Frequency multiplication rectangular wave pulse signal is input to the sampling synchronization signals of ccd detector as ccd detector, because frequency multiplication rectangular wave pulse signal and fundamental frequency sine wave signal frequency differ one times, in two frame ccd images of therefore adjacent collection, a frame is the image that terahertz pulse exists, one frame is the image not having terahertz pulse, achieved the dynamic corrections of measurement by the method for CCD times of frequency sampling, improve the signal to noise ratio (S/N ratio) of systematic survey.
Based on the temperature of combustion method for sensing that terahertz pulse is measured, comprise the steps:
Step (1) .CCD exports the gray level image of ranging pulse f 1( x) and the gray level image of reference pulse f 2( x).
Step (2). by the gray level image of ranging pulse f 1( x) and the gray level image of reference pulse f 2( x) subtract each other and obtain terahertz pulse signal magnitude f( x)= f 1( x)- f 2( x).
Step (3). judge whether burning is uniform temperature distribution,
If 3-1. temperature of combustion is uniformly distributed, use uniform temperature formula model, uniform temperature formula model describes such as formula (1).
(1)
Wherein, , the change size of air refraction, it is the time delay of terahertz pulse.
P-atmospheric pressure;
xthe volumetric molar concentration of-gas molecule;
L-terahertz pulse is by the distance of combustion zone.
Then according to air refraction change calculations temperature of combustion, the relation of temperature variation and variations in refractive index is described by formula (2).
2)
Wherein, βbe the scale-up factor of variations in refractive index and temperature variation, the changing value of temperature can be obtained by the change size of refractive index, thus obtain the temperature of burning.
If 3-2. judges that burning is not uniform temperature distribution, then use Fast Fourier Transform (FFT) (FFT) method that terahertz pulse signal is converted into spectral signal;
Step (4). use Fu Yite (Voigt) linear function to do matching to the frequency spectrum after FFT conversion, the Fu Yite linear function that fitting function adopts is described by formula (3).
(3)
Wherein, , ;
Wherein:
γ d -Gaussian linear function spectral width;
γ c -Lorentz linear function spectral width;
Obtain Fu Yite linear function spectral width simultaneously :
Wherein, it is the collision live width of spectral line;
it is the doppler linewidth of spectral line;
Step (5). use absorption line method of discrimination to determine absorption line suitable in measure spectrum scope, calculate the absorption coefficient of the different absorption line of m bar according to absorption spectrum when having a flame combustion and absorption spectrum when not having flame combustion a 1, a 2, a m , described by formula (4).
(4)
Wherein, p m -absorption line strengths when having a flame combustion;
q m absorption line strengths during-non-flaming combustion;
Step (6). set the Temperature Distribution of burning as T 1, T 2... T n, by the absorption coefficient of spectral line a m substitute into absorption line system of equations Ax=a with the temperature matrices A of line strength, described by formula (5), if the solution of formula (5) exists and uniquely, then can calculate the ratio x of the combustion zone of different temperatures.
(5)
Wherein, obtain by the line parameters searched in international standard spectra database.
If the absorption coefficient composition of vector of the different spectral line of known m bar , and known temperature matrix A, m>n, then can utilize least square method can estimate the distribution of temperature T .
The idiographic flow that the demarcation of the temperature coefficient in described step (3) and the absorption line of step (5) differentiate is as follows:
A () regulates one dimensional optical translation stage to make terahertz pulse be imaged on CCD central area; Regulate the light splitting ratio of beam splitter to make the intensity of the first reference laser in CCD and the second reference laser equal simultaneously, realize the measurement completing terahertz pulse in a CCD sampling process.
B () places long path cell in combustion zone, realize calibration process.When long path cell is heated to temperature T ntime gather time delay of terahertz pulse, after all demarcation temperature all complete, utilize partial least square method matching temperature T nthe temperature coefficient of temperature survey model is obtained with the linear equation of terahertz pulse delay.
In c temperature of combustion method for sensing that () measures based on terahertz pulse, the selection of spectral line comprises the selection of gas molecule, the determination of spectral line spectral range, the calculating of spectral line temperature control, in measuring process, the larger gas molecule of a kind of absorption coefficient is first selected to do temperature survey, then according to the spectral frequency range of the spectral range determination molecular spectrum of terahertz pulse; According to the line parameters in international spectroscopic data library lookup spectral frequency range, in temperature measurement range interval, calculate the temperature control of all spectral lines , select maximum m bar spectral line S 1, S 2... S mas the spectral line that Temperature Distribution calculates.
Beneficial effect of the present invention is as follows:
The first, the temperature of combustion sensing device measured based on terahertz pulse uses parallel grating group to realize frequency chirp and time explanation, thus achieves the wavelength-division electro-optic sampling of terahertz pulse.By changing the sine wave of signal generator and rect.p. wave frequency and phase place, the clock period of the terahertz pulse that photoconductive antenna type terahertz transmitter gives off and CCD sampling is synchronous, thus the sampling process realizing a CCD just can obtain the measurement of a terahertz pulse, realize the effect obtaining burning object tera-hertz spectra fast.Because the frequency of the sampling of CCD can be very fast, therefore the temperature of combustion sensing device measured based on terahertz pulse can carry out data acquisition with higher sampling rate to burning object, is particularly suitable for this kind of dynamic change of the flame combustion real-time measurement of object faster and the needs of analysis.Therefore the temperature of combustion sensing device measured based on terahertz pulse can, in conflagration change procedure, adopt non-contacting mode measurement to obtain the terahertz light modal data of burning object not disturbing combustible substance under the condition distributed.
The second, because terahertz emission is a kind of electromagenetic wave radiation of low temperature, the measurement of a large amount of background infrared radiation noises to terahertz pulse therefore produced in combustion process does not produce interference substantially, and when therefore using terahertz pulse to measure, signal to noise ratio (S/N ratio) is high especially.The temperature of combustion sensing device measured based on terahertz pulse can realize having higher signal to noise ratio (S/N ratio) and precision than tradition based on the thermometry of infrared radiation measurement.
3rd, photoconductive antenna type terahertz transmitter can launch the THz wave of wavelength coverage at 0.1 ~ 7THz, and the frequency spectrum due to the THz wave of launching covers a large amount of combustion product gas, therefore, it is possible to realize completing H in one-shot measurement process 2o, CO, CO 2, NO, NO 2, NH 3and SO 2deng the monitoring of gas.Simultaneously because terahertz emission is high by 10 for the remolding sensitivity traditional infrared radiation of burning gases 3above, the temperature of combustion method for sensing therefore measured based on terahertz pulse has very high sensitivity.
4th, the temperature of combustion sensing device based on terahertz pulse measurement can be arranged on the both sides of combustion zone flexibly according to the actual conditions of burning object.Owing to only needing a photoconductive antenna type terahertz transmitter as spectral radiation source, the temperature of combustion sensing device structure therefore based on terahertz pulse measurement is very simply compact.The terahertz pulse data processing method adopted, can be realized the data processing under complicated burning condition and analysis by uniform temperature distributed model and non-uniform temperature distributed model.
Accompanying drawing explanation
Fig. 1 is structural representation of the present invention;
Fig. 2 is photoconductive antenna type terahertz transmitter and CCD sample circuit sequential chart;
Fig. 3 is temperature of combustion method for sensing process flow diagram;
Fig. 4 is spectral line method of discrimination process flow diagram;
Fig. 5 is that temperature coefficient demarcates process flow diagram;
In figure, femto-second laser 1, beam splitter 2, first plane mirror 3-1, the second plane mirror 3-2, the 3rd plane mirror 3-3, condenser lens 4, photoconductive antenna type terahertz transmitter 5, off axis paraboloidal mirror group 6, first semi-transparent reflection mirror 7-1, the second semi-transparent reflection mirror 7-2, parallel grating group 8, plane mirror 9, first polaroid 10-1, the second polaroid 10-2, ito glass 11, ZnTe crystal 12, ccd detector 13, computing machine 14, function generator 15, high frequency power amplifier 16, one dimensional optical translation stage 17.
Embodiment
Below in conjunction with accompanying drawing, the present invention is described in further detail.
As shown in Figure 1, based on the temperature of combustion sensing device that terahertz pulse is measured, comprise femto-second laser 1, beam splitter 2, first plane mirror 3-1, second plane mirror 3-2, 3rd plane mirror 3-3, condenser lens 4, photoconductive antenna type terahertz transmitter 5, off axis paraboloidal mirror group 6, first semi-transparent reflection mirror 7-1, second semi-transparent reflection mirror 7-2, parallel grating group 8, plane mirror 9, first polaroid 10-1, second polaroid 10-2, ito glass 11, ZnTe crystal 12, ccd detector 13, computing machine 14, function generator 15, high frequency power amplifier 16, one dimensional optical translation stage 17.
Laser is launched from femto-second laser 1, after beam splitter 2 light splitting, be divided into reference laser and exploring laser light two-way, wherein exploring laser light is successively by the first plane mirror 3-1, second plane mirror 3-2, 3rd plane mirror 3-3 focuses in photoconductive antenna type terahertz transmitter 5 by condenser lens 4 after reflecting, photoconductive antenna type terahertz transmitter 5 launches terahertz pulse under the voltage drive effect of exploring laser light and high frequency power amplifier 16, terahertz pulse becomes parallel THz wave after the collimation of the off axis paraboloidal mirror of off axis paraboloidal mirror group 6 side, and through combustion zone, parallel THz wave converges on ZnTe crystal 12 by the off axis paraboloidal mirror of opposite side, the reference laser that beam splitter 2 separates incides in pair of parallel grating group 8 after the first semi-transparent reflection mirror 7-1, reference laser through parallel grating group 8 is reflected back parallel grating group 8 by plane mirror 9, thus achieve frequency chirp and the time explanation of reference laser, reference laser after time explanation is reflected through the first polaroid 10-1 by the first semi-transparent reflection mirror 7-1, reference laser through the first polaroid 10-1 reflexes on ZnTe crystal 12 by ito glass 11, overlap with the THz wave collimation converged on ZnTe crystal 12, Pockels (Pockels) effect of ZnTe crystal 12 is utilized to realize Terahertz wave modulation, after polarization state is passed the second semi-transparent reflection mirror 7-2 by the first reference laser that THz wave is modulated, again through the second polaroid 10-2, the first reference laser carrying terahertz pulse strength information is reflexed to ccd detector 13 by the 4th plane mirror 3-4 and detects acceptance, simultaneously due to the birefringence effect of ZnTe crystal 12, do not carry the second reference laser of terahertz pulse strength information through the second semi-transparent reflection mirror 7-2, 6th plane mirror 3-6, 5th plane mirror 3-5 also incides ccd detector 13 after reflecting and is detected reception, ccd detector 13 by the first reference laser carrying terahertz pulse strength information collected and do not carry terahertz pulse strength information the second reference laser corresponding to picture signal input computing machine 14 carry out subsequent treatment.Function generator 15 produces fundamental frequency sine wave signal and is input to high frequency power amplifier 16, high frequency power amplifier 16 drives photoconductive antenna type terahertz transmitter 5 cycle to produce terahertz pulse, and function generator 15 produces the twice that the sampling period of the frequency multiplication square-wave signal control ccd detector 13 of frequency multiplication is terahertz pulse transmission frequency simultaneously.
Described parallel grating group 8 is one group of grating of parallel placement, and the reference laser pulse-echo after parallel grating group 8 chirp spread is returned input path by plane mirror 9.
The reference laser pulse that described ito glass 11 makes to reflex on ZnTe crystal 12 is coaxial with the terahertz pulse concurrent converged on ZnTe crystal 12.
Described one dimensional optical translation stage 17 placed the first plane mirror 3-1, the second plane mirror 3-2, by optical delay method, terahertz pulse is positioned in the duration of synchronizing detection pulse, simultaneously by the adjustment of one dimensional optical translation stage 17, the image space of terahertz pulse is adjusted to the middle section of ccd detector 13.
As shown in Figure 2, function generator 15 produces the voltage signal of two kinds of different frequencies, is fundamental frequency sine wave pulse signal and frequency multiplication rectangular wave pulse signal respectively.Fundamental frequency sine wave signal is input to high frequency power amplifier 16, periodic voltage excitation photoconductive antenna type terahertz transmitter 5 being formed photoconductive antenna is loaded into after amplifying, the photo-generated carrier of moment is produced when exploring laser light incides in photoconductive antenna type terahertz transmitter 5, photo-generated carrier gives off terahertz pulse under positive half cycle sinusoidal voltage excitation, and non-radiating is gone out terahertz pulse by photo-generated carrier under the excitation of negative half period sinusoidal voltage.Frequency multiplication rectangular wave pulse signal is input to the sampling synchronization signals of ccd detector 13 as ccd detector 13, because frequency multiplication rectangular wave pulse signal and fundamental frequency sine wave signal frequency differ one times, in two frame ccd images of therefore adjacent collection, a frame is the image that terahertz pulse exists, one frame is the image not having terahertz pulse, achieved the dynamic corrections of measurement by the method for CCD times of frequency sampling, improve the signal to noise ratio (S/N ratio) of systematic survey.
As shown in Figure 3, based on the temperature of combustion method for sensing that terahertz pulse is measured, comprise the steps, specifically comprise FFT conversion, spectral line linear fitting, choice of spectrum and spectral line temperature equation solve.Ccd detector 13 exports the gray level image of ranging pulse f 1( x) and the gray level image of reference pulse f 2( x) (step 310), by the gray level image of ranging pulse f 1( x) and the gray level image of reference pulse f 2( x) subtract each other and obtain terahertz pulse signal magnitude f( x)= f 1( x)- f 2( x) (step 320), judge whether burning is uniform temperature distribution (step 330), if temperature of combustion is uniformly distributed, use uniform temperature formula model (step 390), uniform temperature formula model is described by formula (1).
formula (1)
Wherein, , the change size of air refraction, it is the time delay of measuring the terahertz pulse obtained.
P-atmospheric pressure;
xthe volumetric molar concentration of-gas molecule;
L-terahertz pulse is by the distance of combustion zone.
Then according to air refraction change calculations temperature of combustion (step 391), the relation of temperature variation and variations in refractive index is described by formula (2).
formula (2)
Wherein, for the size of temperature variation, βbe the scale-up factor of variations in refractive index and temperature variation, obtained the changing value of temperature by the large I of the change of refractive index, thus obtain the temperature of burning.
If judge that burning is not uniform temperature distribution (step 330), then need to use Fast Fourier Transform (FFT) (FFT) method that terahertz pulse signal is converted into spectrum signal (step 340); Then use Fu Yite (Voigt) linear function to do matching (step 350) to the frequency spectrum after FFT conversion, the Fu Yite linear function that fitting function adopts is described by formula (3).
formula (3)
Wherein, , ;
Wherein:
γ d --Gaussian linear function spectral width;
γ c -Lorentz linear function spectral width;
Fu Yite linear function spectral width can be obtained simultaneously :
Wherein, it is the collision live width of spectral line; it is the doppler linewidth of spectral line;
Use absorption line method of discrimination to determine absorption line (step 360) suitable in measure spectrum scope, calculate the absorption coefficient of the different absorption line of m bar according to absorption spectrum when having a flame combustion and absorption spectrum when not having flame combustion a 1, a 2, a m (step 370), is described by formula (4).
formula (4)
Wherein, p m --there is absorption line strengths during flame combustion
q m absorption line strengths during-non-flaming combustion
If the Temperature Distribution of burning is T 1, T 2... T n, by the absorption coefficient of spectral line a m absorption line system of equations Ax=a(step 380 is substituted into the temperature matrices A of line strength), described by formula (5), if the solution of formula (5) exists and uniquely, then can calculate the ratio x of the combustion zone of different temperatures.
formula (5
Wherein, can be obtained by the line parameters searched in international standard spectra database.
If the absorption coefficient composition of vector of the different spectral line of known m bar , and known temperature matrix A, m>n, utilizes least square method can estimate the distribution of temperature (step 381).
As shown in Figure 4, comprise the steps based on the selection of spectral line in the temperature of combustion method for sensing of terahertz pulse measurement.Specifically comprise the selection of gas molecule, the determination of spectral line spectral range, the calculating of spectral line temperature control.In measuring process, the larger gas molecule of a kind of absorption coefficient first will be selected to do temperature survey (step 410); According to the spectral frequency range (step 420) of the spectral range determination molecular spectrum of terahertz pulse; According to the line parameters (step 430) in international spectroscopic data library lookup spectral frequency range; According to burning object determination combustion temperature measurement scope (step 440); The temperature control of all spectral lines is calculated in temperature measurement range interval (step 450); Select maximum m bar spectral line S 1, S 2... S mas the spectral line (step 460) that Temperature Distribution calculates.
As shown in Figure 5, calibration process based on the temperature of combustion sensing device of terahertz pulse measurement comprises the steps, the measurement in order to terahertz pulse has larger measurement range to be needed to regulate one dimensional optical translation stage to make terahertz pulse be imaged on CCD central area (step 510); In order to complete the measurement of terahertz pulse in ccd detector 13 sampling process, the light splitting ratio of beam splitter is regulated to make the intensity equal (step 520) of the first reference laser in ccd detector 13 and the second reference laser; In calibration process combustion zone place long path cell, simultaneously by external heating arrangement by the gas-heated in long path cell to the temperature (step 530) of specifying; When long path cell is heated to temperature T ntime gather time delay (step 540) of terahertz pulse; If demarcate the maximum heating temperature range that temperature reaches heating arrangement, end temp collection enters data processing, if demarcate the maximum heating temperature that temperature does not reach heating arrangement, improve the heating-up temperature of long path cell, and circulation performs the time delay (step 550) that step 540 gathers terahertz pulse.Partial least square method matching temperature T is utilized after all demarcation temperature all complete nthe temperature coefficient (step 560) of temperature survey model is obtained with the linear equation of terahertz pulse delay.

Claims (2)

1. based on the temperature of combustion sensing device that terahertz pulse is measured, comprise femto-second laser, beam splitter, the first plane mirror, the second plane mirror, the 3rd plane mirror, condenser lens, photoconductive antenna type terahertz transmitter, off axis paraboloidal mirror group, the first semi-transparent reflection mirror, the second semi-transparent reflection mirror, parallel grating group, plane mirror, the first polaroid, the second polaroid, ito glass, ZnTe crystal, ccd detector, computing machine, function generator, high frequency power amplifier, one dimensional optical translation stage, it is characterized in that:
Laser is launched from femto-second laser, after beam splitter light splitting, be divided into reference laser and exploring laser light two-way, wherein exploring laser light is successively by the first plane mirror, second plane mirror, focus in photoconductive antenna type terahertz transmitter by condenser lens after 3rd plane mirror reflection, photoconductive antenna type terahertz transmitter launches terahertz pulse under the voltage drive effect of exploring laser light and high frequency power amplifier, terahertz pulse becomes parallel THz wave after the collimation of the off axis paraboloidal mirror of off axis paraboloidal mirror group side, and through combustion zone, parallel THz wave converges on ZnTe crystal by the off axis paraboloidal mirror of opposite side, the reference laser that beam splitter separates incides in pair of parallel grating group after the first semi-transparent reflection mirror, reference laser through parallel grating group is reflected back parallel grating group by plane mirror, realize frequency chirp and the time explanation of reference laser, reference laser after time explanation is reflected through the first polaroid by the first semi-transparent reflection mirror, reference laser through the first polaroid reflexes on ZnTe crystal by ito glass, overlap with the THz wave collimation converged on ZnTe crystal, the Pockels effect of ZnTe crystal is utilized to realize Terahertz wave modulation, polarization state is divided into two-way by the reference laser that THz wave is modulated after the second semi-transparent reflection mirror, the laser of transmission is after the second polaroid, after the 4th plane mirror reflection, become the first reference laser again to receive to ccd detector detection, through second semi-transparent reflection mirror reflection laser through the 6th plane mirror, become the second reference laser after 5th plane mirror reflection also to incide ccd detector and be detected reception, ccd detector by the first reference laser carrying terahertz pulse strength information collected and do not carry terahertz pulse strength information the second reference laser corresponding to picture signal input computing machine carry out subsequent treatment, function generator produces fundamental frequency sine wave signal and is input to high frequency power amplifier, high frequency power amplifier drives the photoconductive antenna type terahertz transmitter cycle to produce terahertz pulse, and function generator produces the twice that the sample frequency of the rectangular wave pulse signal control ccd detector of frequency multiplication is terahertz pulse transmission frequency simultaneously,
Described parallel grating group is one group of grating of parallel placement, and the reference laser pulse-echo after parallel grating group chirp spread is returned input path by plane mirror;
The reference laser pulse that described ito glass makes to reflex on ZnTe crystal is coaxial with the terahertz pulse concurrent converged on ZnTe crystal;
Described one dimensional optical translation stage placed the first plane mirror, the second plane mirror, by optical delay method, terahertz pulse is positioned in the duration of synchronizing detection pulse, simultaneously by the adjustment of one dimensional optical translation stage, the image space of terahertz pulse is adjusted to the middle section of ccd detector;
Described function generator produces the voltage signal of two kinds of different frequencies, is fundamental frequency sine wave signal and frequency multiplication rectangular wave pulse signal respectively; Fundamental frequency sine wave signal is input to high frequency power amplifier, periodic voltage excitation photoconductive antenna type terahertz transmitter being formed photoconductive antenna is loaded into after amplifying, the photo-generated carrier of moment is produced when exploring laser light incides in photoconductive antenna type terahertz transmitter, photo-generated carrier gives off terahertz pulse under positive half cycle sinusoidal voltage excitation, and non-radiating is gone out terahertz pulse by photo-generated carrier under the excitation of negative half period sinusoidal voltage; Frequency multiplication rectangular wave pulse signal is input to the sampling synchronization signals of ccd detector as ccd detector, because frequency multiplication rectangular wave pulse signal and fundamental frequency sine wave signal frequency differ one times, in two frame ccd images of therefore adjacent collection, a frame is the image that terahertz pulse exists, one frame is the image not having terahertz pulse, is realized the dynamic corrections measured by the method for CCD times of frequency sampling.
2., as claimed in claim 1 based on the method for the temperature of combustion sensing device of terahertz pulse measurement, it is characterized in that comprising the steps:
Step (1) .CCD exports the gray level image f of ranging pulse 1the gray level image f of (x) and reference pulse 2(x);
Step (2). by the gray level image f of ranging pulse 1the gray level image f of (x) and reference pulse 2x () is subtracted each other and is obtained terahertz pulse signal magnitude f (x)=f 1(x)-f 2(x);
Step (3). judge whether burning is uniform temperature distribution;
If 3-1. temperature of combustion is uniformly distributed, use uniform temperature formula model, uniform temperature formula model describes such as formula (1);
ξΔn=Δt (1)
Wherein, Δ n is the change size of air refraction, and C is the light velocity in vacuum, and Δ t is the time delay of terahertz pulse;
P-atmospheric pressure;
The volumetric molar concentration of X-gas molecule;
L-terahertz pulse is by the distance of combustion zone;
Then, according to air refraction change calculations temperature of combustion, the relation of temperature variation and variations in refractive index is described by formula (2);
ΔT=βΔn (2)
Wherein, β is temperature coefficient, and Δ T is temperature gap;
The funtcional relationship that can obtain after publicity (1) is substituted into formula (2) between temperature variation and terahertz pulse delay is the size of temperature variation is postponed just can obtain by measuring terahertz pulse.
Temperature computation terminates.
If 3-2. judges that burning is not uniform temperature distribution, then use Fast Fourier Transform (FFT) method that terahertz pulse signal is converted into spectral signal;
Step (4). use Fu Yite linear function to do matching to the frequency spectrum after FFT conversion, the Fu Yite linear function that fitting function adopts is described by formula (3);
Φ V ( v 0 ) = [ ( β γ ED π ) + ( 1 - β π · γ C ) ] - - - ( 3 )
Wherein, β = γ ED ( γ C + γ ED ) , γ ED = γ D ln 2 ;
Wherein:
γ d-Gaussian linear function spectral width;
γ c-Lorentz linear function spectral width;
Obtain Fu Yite linear function spectral width Δ v simultaneously v:
Δ v V = 0.5346 Δ v C + ( 0.2166 Δ v C 2 + Δ v D 2 )
Wherein, Δ v cit is the collision live width of spectral line;
Δ v dit is the doppler linewidth of spectral line;
Step (5). use absorption line method of discrimination to determine absorption line suitable in measure spectrum scope, calculate the absorption coefficient a of the different absorption line of m bar according to absorption spectrum when having a flame combustion and absorption spectrum when not having flame combustion 1, a 2... a m, described by formula (4);
a m = P m Q m - - - ( 4 )
Wherein, P m-absorption line strengths when having a flame combustion;
Q mabsorption line strengths during-non-flaming combustion;
Step (6). set the Temperature Distribution of burning as T 1, T 2... T n, by the absorption coefficient a of spectral line msubstitute into absorption line system of equations Ax=a with the temperature matrices A of line strength, described by formula (5), if the solution of formula (5) exists and uniquely, then can calculate the ratio x of the combustion zone of different temperatures;
S 1 ( T 1 ) S 1 ( T 2 ) . . . S 1 ( T n ) S 2 ( T 1 ) S 2 ( T 2 ) . . . S 2 ( T n ) · · · · · · S m ( T 1 ) S m ( T 2 ) . . . S m ( T n ) x 1 x 2 · · x n = a 1 a 2 · · a m - - - ( 5 )
Wherein, S m(T n) obtain by the line parameters searched in international standard spectra database;
If the absorption coefficient composition of vector of the different spectral line of known m bar a = a 1 a 2 · · a m , And known temperature matrix A, m>n, then can utilize least square method can estimate the distribution of temperature T x = x 1 x 2 · · x n ;
The idiographic flow that the demarcation of the temperature coefficient in described step (3) and the absorption line of step (5) differentiate is as follows:
A () regulates one dimensional optical translation stage to make terahertz pulse be imaged on CCD central area; Simultaneously when on-load voltage does not launch terahertz pulse to photoconductive antenna type terahertz transmitter, regulate the light splitting ratio of beam splitter to make the intensity of the first reference laser in CCD and the second reference laser equal, complete initial balance adjustment.In actual measurement process, photoconductive antenna type terahertz transmitter on-load voltage launches terahertz pulse, the change size that the intensity measuring relative second reference laser of the first reference laser occurs, realizes the measurement completing terahertz pulse in a CCD sampling process;
B () places long path cell in combustion zone, realize calibration process; When long path cell is heated to temperature T ntime gather time delay of terahertz pulse, after all demarcation temperature all complete, utilize partial least square method matching temperature T nthe temperature coefficient of temperature survey model is obtained with the linear equation of terahertz pulse delay;
In c temperature of combustion method for sensing that () measures based on terahertz pulse, the selection of spectral line comprises the selection of gas molecule, the determination of spectral line spectral range, the calculating of spectral line temperature control, in measuring process, the larger gas molecule of a kind of absorption coefficient is first selected to do temperature survey, then according to the spectral frequency range of the spectral range determination molecular spectrum of terahertz pulse; According to the line parameters in international spectroscopic data library lookup spectral frequency range, in temperature measurement range interval, calculate the temperature control of all spectral lines select maximum m bar spectral line S 1, S 2... S mas the spectral line that Temperature Distribution calculates.
Temperature computation terminates.
CN201310019184.1A 2013-01-17 2013-01-17 Terahertz pulse measurement-based burning temperature sensing device and method Active CN103076107B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310019184.1A CN103076107B (en) 2013-01-17 2013-01-17 Terahertz pulse measurement-based burning temperature sensing device and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310019184.1A CN103076107B (en) 2013-01-17 2013-01-17 Terahertz pulse measurement-based burning temperature sensing device and method

Publications (2)

Publication Number Publication Date
CN103076107A CN103076107A (en) 2013-05-01
CN103076107B true CN103076107B (en) 2014-12-24

Family

ID=48152715

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310019184.1A Active CN103076107B (en) 2013-01-17 2013-01-17 Terahertz pulse measurement-based burning temperature sensing device and method

Country Status (1)

Country Link
CN (1) CN103076107B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2725026C1 (en) * 2020-01-22 2020-06-29 Федеральное государственное унитарное предприятие "Центральный институт авиационного моторостроения имени П.И. Баранова" Device for measuring temperature in gas flow

Families Citing this family (26)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104165707B (en) * 2014-08-20 2016-09-21 国家电网公司 A kind of based on the femtosecond all-fiber Raman power transformer temp measuring method passed as guiding
CN104330189B (en) * 2014-10-23 2017-02-15 中国航天科工集团第三研究院第八三五八研究所 TDLAS gas temperature measurement detection method based on optical light-splitting system
CN104614315B (en) * 2015-01-16 2017-05-17 北京科技大学 Test sample holder, switching type test system and test method for terahertz absorption spectrum
JP6558164B2 (en) * 2015-09-10 2019-08-14 いすゞ自動車株式会社 Three-dimensional device temperature measuring device, combustion engine temperature measuring device, combustion engine and three-dimensional device temperature measuring method
CN105203223A (en) * 2015-09-15 2015-12-30 哈尔滨工业大学 Device for measuring temperature of flame through one-dimensional scanning on basis of CARS
CN105136329B (en) * 2015-09-15 2018-09-07 哈尔滨工业大学 A kind of CARS spectroscopic temperature measurement experimental provisions based on bifocal lens
CN105043559B (en) * 2015-09-15 2018-04-24 哈尔滨工业大学 A kind of CARS spectrum temperature measuring devices based on bifocal lens
CN105203222A (en) * 2015-09-15 2015-12-30 哈尔滨工业大学 Device for measuring temperature of flame through one-dimensional scanning on basis of Fresnel lens and CARS
CN105509925B (en) * 2015-11-30 2018-11-27 广东怡隆光学科技有限公司 A kind of CCD temperature-detecting device
CN105547485B (en) * 2015-12-04 2018-03-16 哈尔滨工业大学 The general yardstick optical field detection method of flame temperature based on microlens array with modulation laser
CN105571741B (en) * 2015-12-04 2018-06-12 哈尔滨工业大学 The general scale optical field detection method of flame temperature based on microlens array and continuous laser
CN105354859B (en) * 2015-12-09 2018-03-27 华中科技大学 A kind of flame visible radiation scaling method
JP6782612B2 (en) * 2016-11-21 2020-11-11 アズビル株式会社 Flame detection system
CN106768464B (en) * 2016-11-23 2019-02-19 中国特种设备检测研究院 A kind of laser-ultrasound detection method and system in uniform material component inside temperature field
CN107505063B (en) * 2017-07-13 2019-07-12 北京航空航天大学 A kind of laser beam deviation means for correcting and method based on high frequency sinusoidal calibration light
CN108732561B (en) * 2018-07-01 2020-03-13 北京工业大学 Air refractive index compensation method of laser tracking measurement system based on dual-wavelength interference
CN110231102B (en) * 2019-06-28 2020-08-07 西安科技大学 Method for testing temperature of loose coal body based on sound wave velocity
CN110376156A (en) * 2019-07-30 2019-10-25 上海理工大学 The THz wave spectra system that asynchronous optical sampling and double light combs integrate
CN111239090A (en) * 2020-02-13 2020-06-05 华东师范大学重庆研究院 Method and system for measuring single-pulse laser-induced transient molecular fluorescence spectrum
CN112207428B (en) * 2020-10-13 2022-04-01 中国科学院上海光学精密机械研究所 Laser focusing regulation system for realizing 360-degree position type interaction with directional beam line
CN112858212B (en) * 2021-01-12 2022-08-16 江西中医药大学 Method for detecting moxa cone mass by combining terahertz wave and combustion temperature
CN113281297B (en) * 2021-04-09 2023-01-17 北京航空航天大学 Terahertz device for monitoring flame heat release rate pulsation in real time and measuring method
CN113280941A (en) * 2021-04-09 2021-08-20 北京航空航天大学 Terahertz device for monitoring flame temperature field pulsation in real time and measuring method
CN113406264B (en) * 2021-08-20 2021-11-16 中国工程物理研究院流体物理研究所 Explosive burning rate non-contact type measurement experiment device and method based on terahertz waves
CN114295582A (en) * 2021-12-29 2022-04-08 福州大学 Polar liquid reflection type experiment system and measurement method thereof
CN114236570B (en) * 2022-02-23 2022-05-24 成都凯天电子股份有限公司 Laser atmospheric data system and calculation method

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003095991A1 (en) * 2002-05-10 2003-11-20 Rensselaer Polytechnic Institute Tera-hertz ray microscope
JP2004198250A (en) * 2002-12-18 2004-07-15 Tochigi Nikon Corp Time-resolved reflection measuring method and terahertz time-resolved reflection measuring apparatus
US20040208223A1 (en) * 2003-04-18 2004-10-21 Shimadzu Corporation Two-color radiation thermometer
EP1767923A2 (en) * 2004-06-30 2007-03-28 Nikon Corporation Microscope observation method, microscope, differentiation interference microscope, phase difference microscope, interference microscope, image processing method, and image processing device
CN101625269A (en) * 2009-07-27 2010-01-13 北京航空航天大学 Method for simultaneously monitoring two-dimensional distribution of combustion flame temperature field and concentration of combustion flame intermediate product
US20100045970A1 (en) * 2008-08-12 2010-02-25 Raschke Markus B Infrared imaging using thermal radiation from a scanning probe tip
CN101701852A (en) * 2009-09-18 2010-05-05 深圳大学 Electro-optic sampling device used for measuring terahertz optical pulse and measuring method thereof
CN102305757A (en) * 2011-05-20 2012-01-04 西安电子科技大学 Device and method for measuring concentration of high-pressure combustion carbon black particles
US8310671B1 (en) * 2010-09-29 2012-11-13 The United States Of America As Represented By The Administrator Of National Aeronautics And Space Administration Interference-free optical detection for Raman spectroscopy
CN203011574U (en) * 2013-01-17 2013-06-19 杭州电子科技大学 A burning temperature sensing device based on terahertz pulse measurement

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003095991A1 (en) * 2002-05-10 2003-11-20 Rensselaer Polytechnic Institute Tera-hertz ray microscope
JP2004198250A (en) * 2002-12-18 2004-07-15 Tochigi Nikon Corp Time-resolved reflection measuring method and terahertz time-resolved reflection measuring apparatus
US20040208223A1 (en) * 2003-04-18 2004-10-21 Shimadzu Corporation Two-color radiation thermometer
EP1767923A2 (en) * 2004-06-30 2007-03-28 Nikon Corporation Microscope observation method, microscope, differentiation interference microscope, phase difference microscope, interference microscope, image processing method, and image processing device
US20100045970A1 (en) * 2008-08-12 2010-02-25 Raschke Markus B Infrared imaging using thermal radiation from a scanning probe tip
CN101625269A (en) * 2009-07-27 2010-01-13 北京航空航天大学 Method for simultaneously monitoring two-dimensional distribution of combustion flame temperature field and concentration of combustion flame intermediate product
CN101701852A (en) * 2009-09-18 2010-05-05 深圳大学 Electro-optic sampling device used for measuring terahertz optical pulse and measuring method thereof
US8310671B1 (en) * 2010-09-29 2012-11-13 The United States Of America As Represented By The Administrator Of National Aeronautics And Space Administration Interference-free optical detection for Raman spectroscopy
CN102305757A (en) * 2011-05-20 2012-01-04 西安电子科技大学 Device and method for measuring concentration of high-pressure combustion carbon black particles
CN203011574U (en) * 2013-01-17 2013-06-19 杭州电子科技大学 A burning temperature sensing device based on terahertz pulse measurement

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
JP特开2004-198250A 2004.07.15 *
Measurement of solid concentration using Terahertz technique;Liu Yi"an,Huang Zhiyao,Ji Haifeng,Wang Baoliang,Li Haiqing;《仪器仪表学报》;20071130;第28卷(第11期);1951-1955 *
Terahertz Technology;Peter H. Siegel;《IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES》;20020331;第50卷(第3期);910-928 *
基于太赫兹技术的多相流检测研究;刘亦安;《中国博士学位论文全文数据库 基础科学辑》;20110815;全文 *
基于太赫兹时域光谱技术的火焰温度场和浓度场重建研究;刘亦安,冀海峰,王保良,黄志尧,李海青;《中国工程热物理学会2010年多相流学术会议》;20111123;全文 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2725026C1 (en) * 2020-01-22 2020-06-29 Федеральное государственное унитарное предприятие "Центральный институт авиационного моторостроения имени П.И. Баранова" Device for measuring temperature in gas flow

Also Published As

Publication number Publication date
CN103076107A (en) 2013-05-01

Similar Documents

Publication Publication Date Title
CN103076107B (en) Terahertz pulse measurement-based burning temperature sensing device and method
CN203011574U (en) A burning temperature sensing device based on terahertz pulse measurement
CN103557886B (en) A kind of method that high-temperature gas two dimension instantaneous temperature field based on ultraphotic spectrum, distribution of concentration are measured simultaneously
CN101371129B (en) Surface plasmon resonance sensors and methods for detecting samples using the same
CN203216634U (en) High temperature measurement and temperature field reconstruction device based on turnable diode laser absorption spectroscopy
CN106969800B (en) A kind of device and method measuring gas temperature and concentration simultaneously using single spectral line
CN104280362A (en) Online high-temperature water vapor laser spectrum detection system
CN103364371B (en) The absorption coefficient of atmospheric aerosol Novel differential measurement method of coaxial-type photothermal interference
CN103048050B (en) Radiation temperature measurement method and instrument for measuring real temperature of target
CN101644673A (en) Infrared cavity ring-down spectroscopy trace gas detection method based on quantum cascade laser
CN103698298A (en) Device for measuring gas concentration based on short cavity enhanced correlation spectroscopy, and method for measuring gas concentration by adopting device
CN102589714A (en) Temperature measuring device based on high-pressure gas Rayleigh-Brillouin scattering spectrum
CN105466491B (en) The imaging type ignition temperature apparatus for measuring concentration to be filtered based on binary channels molecule
CN103557960A (en) Fabry-Perot fiber-optic temperature sensing system and method
CN201561803U (en) Infrared double-wave length non-contact temperature measuring device
Shen et al. Methane near-infrared laser remote detection under non-cooperative target condition based on harmonic waveform recognition
CN104391132A (en) Device and method for measuring engine combustion flow field speed based on molecular absorption spectrum
CN103528991B (en) System and method for measuring organic matter content of soil
Yang et al. Methane concentration measurement method in rain and fog coexisting weather based on TDLAS
CN113959581A (en) High-precision temperature telemetering system and method
CN102889959A (en) Device for measuring gas pressure based on Rayleigh-Brillouin scattering spectral characteristic
Pan et al. Diode laser-based standoff absorption measurement of water film thickness in retro-reflection
Zhou et al. Noise immune absorption profile extraction for the TDLAS thermometry sensor by using an FMCW interferometer
CN107505063B (en) A kind of laser beam deviation means for correcting and method based on high frequency sinusoidal calibration light
CN104458577A (en) Thermal infrared imager based gas remote detecting device

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
EE01 Entry into force of recordation of patent licensing contract

Application publication date: 20130501

Assignee: Hangzhou Yixing new energy automobile service Co., Ltd

Assignor: HANGZHOU DIANZI University

Contract record no.: X2020330000092

Denomination of invention: Combustion temperature sensing device and method based on terahertz pulse measurement

Granted publication date: 20141224

License type: Common License

Record date: 20201106

EE01 Entry into force of recordation of patent licensing contract