WO2022110283A1 - Infrared temperature measurement method, apparatus, device, and storage medium - Google Patents

Infrared temperature measurement method, apparatus, device, and storage medium Download PDF

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WO2022110283A1
WO2022110283A1 PCT/CN2020/134228 CN2020134228W WO2022110283A1 WO 2022110283 A1 WO2022110283 A1 WO 2022110283A1 CN 2020134228 W CN2020134228 W CN 2020134228W WO 2022110283 A1 WO2022110283 A1 WO 2022110283A1
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infrared
target
temperature
imaging system
function
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PCT/CN2020/134228
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French (fr)
Chinese (zh)
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李东婧
李红领
邱浩楠
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烟台艾睿光电科技有限公司
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/80Calibration

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  • the invention relates to the technical field of infrared temperature measurement, in particular to an infrared temperature measurement method, device, equipment and storage medium.
  • Infrared imaging temperature measurement technology has a wide range of applications in infrared detection, infrared remote sensing, military target measurement, industrial monitoring, forest fire prevention and other fields. Due to the complex principle of infrared temperature measurement, there are a large number of factors that affect the accuracy of temperature measurement (including lens parameters, environmental variables, distance coefficients, target emissivity, output drift of the infrared detector itself, etc.), especially in the field of long-distance temperature measurement. , it has been difficult to have a better temperature measurement application scheme and algorithm.
  • the traditional single-band calibration temperature measurement scheme is generally used, but the temperature measurement performance within 100m can only be guaranteed; and combined with Planck's radiation law, a dual-band temperature measurement method can also be used, but it needs to be equipped with Dual-band lens, and the application field is concentrated in the high-altitude measurement above 10km, the cost is high, and it is rarely used in civilian products.
  • the "calibration coefficient" or single-variable empirical formula is used to correct the long-distance attenuation, which has low applicability for applications under different ambient temperatures and different lenses, and the calibration is complicated. For forest fire prevention, fire warning, etc., wide field/distance There has been no better application solution for distance temperature measurement requirements.
  • the present invention is proposed to provide an infrared temperature measurement method, device, device and storage medium that overcome the above problems or at least partially solve the above problems.
  • An infrared temperature measurement method comprising:
  • the target imaging ratio correction is performed on the first temperature data to obtain second temperature data.
  • the obtained temperature is subjected to atmospheric attenuation correction according to environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature data , including:
  • the following formula is used to correct the obtained atmospheric attenuation coefficient:
  • the following formula is used to obtain the first temperature data:
  • T out1 is the first temperature data
  • e is the target emissivity
  • T m is the acquired temperature
  • T env is the ambient temperature
  • n is determined by Boltzmann's theorem of the response band.
  • the target proportion correction function is obtained, which specifically includes:
  • the established functional relationship is normalized to obtain a target proportion correction function, and the obtained target proportion correction function is pre-stored in the processor of the infrared imaging system.
  • the method before performing the target imaging ratio correction on the first temperature data according to the acquired target ratio function and the target imaging radius, the method further includes: :
  • the radius of the equal-area circle corresponding to the connected domain is obtained, and the radius of the equal-area circle is used as the imaging radius of the target.
  • the following formula is used to obtain the second temperature data:
  • the embodiment of the present invention also provides an infrared temperature measurement device, comprising:
  • the test temperature acquisition module is used to acquire the temperature actually tested by the infrared imaging system on the target;
  • an atmospheric attenuation correction module configured to perform atmospheric attenuation correction on the acquired temperature according to environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data
  • a correction function acquisition module configured to establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and to acquire a target proportion correction function
  • the imaging ratio correction module is configured to perform target imaging ratio correction on the first temperature data according to the acquired target ratio function and the imaging radius of the target to obtain second temperature data.
  • An embodiment of the present invention further provides an infrared temperature measurement device, including a processor and a memory, wherein the processor implements the above infrared temperature measurement method provided by the embodiment of the present invention when the processor executes the computer program stored in the memory.
  • Embodiments of the present invention further provide a computer-readable storage medium for storing a computer program, wherein when the computer program is executed by a processor, the above-mentioned infrared temperature measurement method provided by the embodiments of the present invention is implemented.
  • an infrared temperature measurement method includes: obtaining the temperature actually measured by the infrared imaging system on the target; The obtained temperature is corrected by atmospheric attenuation to obtain the first temperature data; the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target is established, and the target proportion correction function is obtained; according to the obtained target proportion function and the target The imaging radius is determined, and the target imaging ratio is corrected for the first temperature data to obtain the second temperature data.
  • the above-mentioned infrared temperature measurement method provided by the present invention introduces a two-variable (atmospheric attenuation and target size) correction method, and corrects the attenuation with distance in combination with the actual environment.
  • the reliability, accuracy and universality of temperature measurement, and the non-calibration scheme is used to correct the temperature drift problem of the infrared detector.
  • the workload is greatly reduced, and the traditional single-band calibration is solved. Due to the complexity of the temperature measurement scheme, it can also monitor the high temperature target in time, and realize preventive temperature measurement and inspection functions such as forest fire prevention and fire warning.
  • the present invention also provides a corresponding device, device and computer-readable storage medium for the infrared temperature measurement method, which further makes the above method more practical, and the device, device and computer-readable storage medium have corresponding advantages.
  • FIG. 1 shows a flowchart of an infrared temperature measurement method provided by an embodiment of the present invention
  • FIG. 2 shows a schematic diagram of a point spread function provided by an embodiment of the present invention
  • FIG. 3 shows a flowchart of obtaining a target proportion correction function provided by an embodiment of the present invention
  • FIG. 4 shows a flowchart of acquiring the imaging radius of a target provided by an embodiment of the present invention
  • FIG. 5 shows a schematic structural diagram of an infrared temperature measuring device provided by an embodiment of the present invention.
  • the present invention provides an infrared temperature measurement method, as shown in Figure 1, comprising the following steps:
  • the temperature actually measured by the infrared imaging system on the target is realized through the basic temperature measurement algorithm
  • the traditional atmospheric attenuation correction scheme usually only considers the influence of the external environment, while ignoring the influence of the spectral response function of the imaging system on it. Therefore, the present invention refers to the attenuation of long-wave infrared in the low sea level atmospheric window, And import the spectral response function of the optical system to further correct the atmospheric attenuation coefficient to make it closer to practical applications;
  • the optical lens has a point spread function PSF for the point light source radiation, that is, the square distribution of the radiation generated by the point light source after passing through the optical imaging system, its demonstration diagram is shown in Figure 2. Due to the linear nature of the optical imaging system, the image of a certain point can be considered as the sum of the PSFs of each point in the image. For the infrared imaging system, except that the input radiation decays with the increase of the target distance, the output radiation of the imaging system is the result of the convolution of the input radiation and the PSF:
  • Deconvolution operations can be performed to obtain the input radiation or a correction matrix can be constructed for precise correction, etc. Because the acquisition of the point spread function is more complicated, and the convolution kernel required for accurate correction is too large, it is not conducive to engineering applications. Therefore, the present invention adopts the method of correcting the proportion of target imaging to realize the correction of temperature, which is simple and fast;
  • a two-variable (atmospheric attenuation and target size) correction method is introduced, and the attenuation with distance is corrected in combination with the actual environment, which improves the performance of medium and long-distance targets (such as 500m ⁇ 2km+) temperature measurement reliability, accuracy and universality, and the non-calibration scheme is used to correct the temperature drift problem of infrared detectors.
  • medium and long-distance targets such as 500m ⁇ 2km+
  • the non-calibration scheme is used to correct the temperature drift problem of infrared detectors.
  • step S102 performs atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature.
  • a temperature data which may specifically include the following steps:
  • Step 1 Obtain the spectral transmittance and scattering function of different atmospheric components to infrared radiation, and obtain the atmospheric attenuation coefficient of the infrared imaging system;
  • the absorption of CO 2 /H 2 O and the scattering of infrared radiation by aerosol impurities are mainly considered for long-distance long-wave infrared radiation at altitudes near the horizontal plane (less than 1 km).
  • the spectral transmittance and scattering function of different atmospheric components to infrared radiation can be obtained by using the look-up table method, and the approximate atmospheric attenuation coefficient ⁇ (x) of the response band [ ⁇ 1 , ⁇ 2 ] of the imaging system can be obtained.
  • Step 2 correcting the obtained atmospheric attenuation coefficient according to the normalized spectral response function of the infrared imaging system
  • SRF sys is the normalized spectral response function of the infrared imaging system
  • SRF Dete is the normalized spectral response function of the detector, which reflects the response of the infrared detector to different bands, which is determined by the detector design and can be Obtained by spectral test
  • Transmittance Lens is the normalized transmittance function of infrared lens to infrared radiation in different bands, which is determined by lens material and optical design, and can be obtained by testing
  • M b ⁇ is the infrared spectral radiation emittance of an ideal black body
  • the resulting atmospheric attenuation coefficient can then be corrected using the following formula:
  • ⁇ re is the modified atmospheric attenuation coefficient
  • Step 3 Perform atmospheric attenuation correction on the acquired temperature according to the corrected atmospheric attenuation coefficient to obtain first temperature data
  • the infrared radiation received by the infrared imaging system mainly includes three parts: the energy emitted by the target, the energy reflected by the target, and the energy of the atmospheric environment. According to basic infrared physics, the following formula can be used to obtain the first temperature data:
  • T out1 is the first temperature data
  • e is the target emissivity
  • T m is the acquired temperature
  • T env is the ambient temperature
  • n is determined by the Boltzmann theorem of the response band
  • E aim is the energy emitted by the target
  • E ref is the energy reflected by the target
  • E env is the energy of the atmospheric environment.
  • step S103 establishes the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtains the target proportion correction function, which may be specifically Include the following steps:
  • the established functional relationship is normalized to obtain the target proportion correction function, and the obtained target proportion correction function is pre-stored in the processor of the infrared imaging system.
  • E(r) is the black body at The output energy of the center point of the infrared imaging system when the radius of the pixel occupied in the infrared imaging system is r;
  • E(r max ) is the output of the center point when the black body occupies the full screen; a and b are determined by ⁇ , E(r) and E (r max ) decides.
  • step S104 before performing step S104 to perform target imaging ratio correction on the first temperature data according to the obtained target ratio function and the imaging radius of the target, further It can include: first, select any point in the target imaging (such as a forest fire point, a point with a temperature exceeding 350°C can be selected), perform a difference operation along the row and column directions of the point, and obtain the approximate length and width of the connected domain of the point; then, according to The approximate length and width of the obtained connected domain are obtained, the radius of the equal-area circle corresponding to the connected domain is obtained, and the radius of the equal-area circle is taken as the imaging radius of the target.
  • any point in the target imaging such as a forest fire point, a point with a temperature exceeding 350°C can be selected
  • the first step is to perform a differential operation on the row direction of the target point (the matlab code is as follows):
  • Row_dif is row difference data
  • Col_dif is column difference data
  • the second step is to obtain the row/column difference data.
  • the coordinates between the maximum and minimum values are the edges with the largest change in the row and column directions of the target point, and the coordinate difference is the approximate length and width of the connected domain of the target point:
  • height and width are the approximate length and width of the obtained connected domain, respectively.
  • T out2 is the second temperature data.
  • the temperature measurement accuracy of targets with different temperatures and sizes can reach ⁇ 10°C, which is far better than the result without this correction scheme.
  • an embodiment of the present invention also provides an infrared temperature measurement device. Since the principle of solving the problem of the infrared temperature measurement device is similar to that of the aforementioned infrared temperature measurement method, the implementation of the infrared temperature measurement device can refer to the infrared temperature measurement device. The implementation of the temperature measurement method will not be repeated here.
  • the infrared temperature measurement device provided by the embodiment of the present invention, as shown in FIG. 5 , specifically includes:
  • the test temperature acquisition module 11 is used to acquire the temperature actually tested by the infrared imaging system on the target;
  • the atmospheric attenuation correction module 12 is used for performing atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature data;
  • the correction function acquisition module 13 is used to establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtain the target proportion correction function;
  • the imaging ratio correction module 14 is configured to perform target imaging ratio correction on the first temperature data according to the acquired target ratio function and the imaging radius of the target to obtain second temperature data.
  • the interaction of the above-mentioned four modules can solve the complexity of the traditional single-band calibration temperature measurement scheme, and at the same time, the temperature measurement accuracy of medium and long-distance targets can be improved. Realize the timely monitoring of high temperature targets, and realize preventive temperature measurement and inspection functions such as forest fire prevention and fire warning.
  • the embodiment of the present invention also discloses an infrared temperature measurement device, including a processor and a memory; wherein, the processor implements the infrared temperature measurement method disclosed in the foregoing embodiments when the processor executes the computer program stored in the memory.
  • the present invention also discloses a computer-readable storage medium for storing a computer program; when the computer program is executed by a processor, the infrared temperature measurement method disclosed above is implemented.
  • a software module can be placed in random access memory (RAM), internal memory, read only memory (ROM), electrically programmable ROM, electrically erasable programmable ROM, registers, hard disk, removable disk, CD-ROM, or any other in the technical field. in any other known form of storage medium.
  • RAM random access memory
  • ROM read only memory
  • electrically programmable ROM electrically erasable programmable ROM
  • registers hard disk, removable disk, CD-ROM, or any other in the technical field. in any other known form of storage medium.
  • An infrared temperature measurement method includes: acquiring a temperature actually measured by an infrared imaging system on a target; performing atmospheric attenuation correction on the acquired temperature according to environmental variables and a normalized spectral response function of the infrared imaging system , obtain the first temperature data; establish the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtain the target proportion correction function; according to the obtained target proportion function and the imaging radius of the target, the first The temperature data is subjected to target imaging ratio correction to obtain second temperature data.
  • the above infrared temperature measurement method introduces a two-variable (atmospheric attenuation and target size) correction method, and combines the actual environment to correct the attenuation with distance, which improves the reliability of temperature measurement for medium and long-distance targets (such as 500m ⁇ 2km+) in different environments
  • the non-calibration scheme is used to correct the temperature drift problem of infrared detectors. Under the premise of meeting the accuracy requirements, the workload is greatly reduced, and the traditional single-band calibration temperature measurement scheme is solved. At the same time, it can monitor the high temperature target in time, and realize the preventive temperature measurement and inspection functions such as forest fire prevention and fire warning.
  • the present invention also provides a corresponding device, device and computer-readable storage medium for the infrared temperature measurement method, which further makes the above method more practical, and the device, device and computer-readable storage medium have corresponding advantages.

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Abstract

Provided are an infrared temperature measurement method, apparatus, device, and storage medium: acquiring a temperature actually measured by an infrared imaging system in respect of a target; according to environment variables and a normalized spectral response function of the infrared imaging system, performing atmospheric attenuation correction on the acquired temperature to obtain first temperature data; establishing a functional relationship between an output energy at the center of the infrared imaging system and the imaging radius of the target to obtain a target proportion correction function; according to the obtained target proportion function and the imaging radius of the target, performing target imaging proportion correction on the first temperature data to obtain second temperature data. By means of the method, it is possible to resolve the complexity of a conventional single-band calibrated temperature measurement solution, while also improving the accuracy of temperature measurement of medium- and long-range targets, and to achieve timely monitoring of high-temperature targets and perform forest fire prevention, fire warning, and other preventive temperature measurement and testing functions.

Description

一种红外测温方法、装置、设备及存储介质An infrared temperature measurement method, device, equipment and storage medium
本申请要求于2020年11月24日提交中国专利局、申请号为202011328314.6、发明名称为“一种红外测温方法、装置、设备及存储介质”的中国专利申请的优先权,其全部内容通过引用结合在本申请中。This application claims the priority of the Chinese patent application filed on November 24, 2020 with the application number 202011328314.6 and the invention titled "An infrared temperature measurement method, device, equipment and storage medium", the entire contents of which are approved by Reference is incorporated in this application.
技术领域technical field
本发明涉及红外测温技术领域,具体涉及一种红外测温方法、装置、设备及存储介质。The invention relates to the technical field of infrared temperature measurement, in particular to an infrared temperature measurement method, device, equipment and storage medium.
背景技术Background technique
红外成像测温技术在红外检测、红外遥感、军事目标测量、工业监控、森林防火等领域拥有的广泛应用。由于红外测温原理较为复杂,存在大量影响测温准确度的因素(包括镜头参数、环境变量、距离系数、目标发射率、红外探测器自身输出漂动等),导致尤其在远距离测温领域,一直难以有较好的测温应用方案及算法。Infrared imaging temperature measurement technology has a wide range of applications in infrared detection, infrared remote sensing, military target measurement, industrial monitoring, forest fire prevention and other fields. Due to the complex principle of infrared temperature measurement, there are a large number of factors that affect the accuracy of temperature measurement (including lens parameters, environmental variables, distance coefficients, target emissivity, output drift of the infrared detector itself, etc.), especially in the field of long-distance temperature measurement. , it has been difficult to have a better temperature measurement application scheme and algorithm.
目前,对于红外成像系统,一般使用传统的单波段标定测温方案,但只能保证在100m以内的测温性能;而结合普朗克辐射定律,还可以采用双波段测温法,但需要配备双波段镜头,且应用领域集中在10km以上的高空测量,成本较大,在民品中应用较少。另外,使用“标定系数”或单变量经验公式来修正远距离衰减,对于不同环温、不同镜头下的应用适用性较低,且标定复杂,针对森林防火、火灾预警等,广视场/远距离的测温需求,一直没有较好的应用方案。At present, for infrared imaging systems, the traditional single-band calibration temperature measurement scheme is generally used, but the temperature measurement performance within 100m can only be guaranteed; and combined with Planck's radiation law, a dual-band temperature measurement method can also be used, but it needs to be equipped with Dual-band lens, and the application field is concentrated in the high-altitude measurement above 10km, the cost is high, and it is rarely used in civilian products. In addition, the "calibration coefficient" or single-variable empirical formula is used to correct the long-distance attenuation, which has low applicability for applications under different ambient temperatures and different lenses, and the calibration is complicated. For forest fire prevention, fire warning, etc., wide field/distance There has been no better application solution for distance temperature measurement requirements.
因此,如何解决测温方案的复杂性和提高对中远距离的测温准确性的问题,是本领域技术人员亟待解决的技术问题。Therefore, how to solve the problems of the complexity of the temperature measurement solution and the improvement of the accuracy of temperature measurement for medium and long distances is a technical problem to be solved urgently by those skilled in the art.
发明内容SUMMARY OF THE INVENTION
鉴于上述问题,提出了本发明以便提供一种克服上述问题或者至少部分地解决上述问题的一种红外测温方法、装置、设备及存储介质。In view of the above problems, the present invention is proposed to provide an infrared temperature measurement method, device, device and storage medium that overcome the above problems or at least partially solve the above problems.
一种红外测温方法,包括:An infrared temperature measurement method, comprising:
获取红外成像系统对目标实际测试出的温度;Obtain the temperature actually tested by the infrared imaging system on the target;
根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据;Perform atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data;
建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;establishing a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtaining a target proportion correction function;
根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正,得到第二温度数据。According to the acquired target ratio function and the imaging radius of the target, the target imaging ratio correction is performed on the first temperature data to obtain second temperature data.
优选地,在本发明实施例提供的上述红外测温方法中,根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据,具体包括:Preferably, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, the obtained temperature is subjected to atmospheric attenuation correction according to environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature data , including:
获取不同大气成分对红外辐射的光谱透过率和散射函数,得到所述红外成像系统的大气衰减系数;Obtain the spectral transmittance and scattering function of different atmospheric components to infrared radiation, and obtain the atmospheric attenuation coefficient of the infrared imaging system;
根据所述红外成像系统的归一化光谱响应函数,对得到的大气衰减系数进行修正;Correcting the obtained atmospheric attenuation coefficient according to the normalized spectral response function of the infrared imaging system;
根据修正后的大气衰减系数,对获取的所述温度进行大气衰减修正,得到第一温度数据。Perform atmospheric attenuation correction on the acquired temperature according to the corrected atmospheric attenuation coefficient to obtain first temperature data.
优选地,在本发明实施例提供的上述红外测温方法中,采用下述公式对得到的大气衰减系数进行修正:Preferably, in the above-mentioned infrared temperature measurement method provided in the embodiment of the present invention, the following formula is used to correct the obtained atmospheric attenuation coefficient:
Figure PCTCN2020134228-appb-000001
Figure PCTCN2020134228-appb-000001
Figure PCTCN2020134228-appb-000002
Figure PCTCN2020134228-appb-000002
Figure PCTCN2020134228-appb-000003
Figure PCTCN2020134228-appb-000003
C 1=3.7415×10 8W·μm 4/m 2 C 1 =3.7415×10 8 W·μm 4 /m 2
C 2=1.43879×10 4μm·K C 2 =1.43879×10 4 μm·K
其中,τ re为修正后的大气衰减系数;
Figure PCTCN2020134228-appb-000004
为CO 2对不同波段红外辐射的吸收率;
Figure PCTCN2020134228-appb-000005
为H 2O对不同波段红外辐射的吸收率;τ Aero为气溶胶对红外辐射的散射函数;λ为所述红外成像系统的响应波长;[λ 12]为所述红外成 像系统的响应波段;x为外部输入的目标距离、CO 2含量、相对湿度、环境温度、可见度;SRF sys为所述红外成像系统的归一化光谱响应函数;SRF Dete为探测器的归一化光谱响应函数;Transmittance Lens为红外镜头对不同波段红外辐射的归一化透过率函数;M 为理想黑体的红外光谱辐射出射度;T为对辐射度归一化所用的温度值。
where τ re is the modified atmospheric attenuation coefficient;
Figure PCTCN2020134228-appb-000004
is the absorption rate of CO 2 to infrared radiation in different bands;
Figure PCTCN2020134228-appb-000005
is the absorption rate of H 2 O to infrared radiation in different bands; τ Aero is the scattering function of aerosol to infrared radiation; λ is the response wavelength of the infrared imaging system; [λ 12 ] is the infrared imaging system Response band; x is the external input target distance, CO 2 content, relative humidity, ambient temperature, visibility; SRF sys is the normalized spectral response function of the infrared imaging system; SRF Dete is the normalized spectral response of the detector function; Transmittance Lens is the normalized transmittance function of the infrared lens to infrared radiation in different bands; M is the infrared spectral radiation emittance of an ideal black body; T is the temperature value used for normalizing the radiance.
优选地,在本发明实施例提供的上述红外测温方法中,采用下述公式得到第一温度数据:Preferably, in the above-mentioned infrared temperature measurement method provided in the embodiment of the present invention, the following formula is used to obtain the first temperature data:
Figure PCTCN2020134228-appb-000006
Figure PCTCN2020134228-appb-000006
其中,T out1为所述第一温度数据;e为目标发射率;T m为获取的所述温度;T env为环境温度;n由响应波段的玻尔兹曼定理决定。 Wherein, T out1 is the first temperature data; e is the target emissivity; T m is the acquired temperature; T env is the ambient temperature; n is determined by Boltzmann's theorem of the response band.
优选地,在本发明实施例提供的上述红外测温方法中,建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数,具体包括:Preferably, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target is established, and the target proportion correction function is obtained, which specifically includes:
将所述红外成像系统的光轴对准相同温度、不同半径的圆形黑体,使所述黑体成像在画面正中心,获取所述红外成像系统中心点的输出能量;Align the optical axis of the infrared imaging system with a circular black body of the same temperature and different radii, so that the black body is imaged in the center of the screen, and obtain the output energy of the center point of the infrared imaging system;
以所述黑体在所述红外成像系统中所占像素的半径作为自变量,建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系;Using the radius of the pixel occupied by the black body in the infrared imaging system as an independent variable, establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target;
对建立的所述函数关系进行归一化,获取目标占比修正函数,并将获取的所述目标占比修正函数预存在所述红外成像系统的处理器内。The established functional relationship is normalized to obtain a target proportion correction function, and the obtained target proportion correction function is pre-stored in the processor of the infrared imaging system.
优选地,在本发明实施例提供的上述红外测温方法中,在根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正之前,还包括:Preferably, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, before performing the target imaging ratio correction on the first temperature data according to the acquired target ratio function and the target imaging radius, the method further includes: :
选取目标成像中任意点,沿该点行列方向进行差分运算,获取该点连通域的近似长与宽;Select any point in the target image, perform the difference operation along the row and column directions of the point, and obtain the approximate length and width of the connected domain of the point;
根据获取的所述连通域的近似长与宽,得到所述连通域对应的等面积圆的半径,将所述等面积圆的半径作为目标的成像半径。According to the obtained approximate length and width of the connected domain, the radius of the equal-area circle corresponding to the connected domain is obtained, and the radius of the equal-area circle is used as the imaging radius of the target.
优选地,在本发明实施例提供的上述红外测温方法中,采用下述公式得到第二温度数据:Preferably, in the above-mentioned infrared temperature measurement method provided in the embodiment of the present invention, the following formula is used to obtain the second temperature data:
Figure PCTCN2020134228-appb-000007
Figure PCTCN2020134228-appb-000007
θ(r)=E(r)/E(r max)=a*r^b+1 θ(r)=E(r)/E(r max )=a*r^b+1
其中,T out2为所述第二温度数据;height和width分别为获取的所述连通域的近似长与宽;r'为所述等面积圆的半径;θ为所述目标占比修正函数,E(r)为所述黑体在所述红外成像系统中所占像素的半径为r时所述红外成像系统中心点的输出能量;E(r max)为所述黑体占满全屏幕时的中心点输出;a和b由θ、E(r)和E(r max)决定。 Wherein, T out2 is the second temperature data; height and width are the obtained approximate length and width of the connected domain, respectively; r' is the radius of the equal-area circle; θ is the target ratio correction function, E(r) is the output energy of the center point of the infrared imaging system when the radius of the pixel occupied by the black body in the infrared imaging system is r; E(r max ) is the center when the black body occupies the full screen Point output; a and b are determined by θ, E(r) and E(r max ).
本发明实施例还提供了一种红外测温装置,包括:The embodiment of the present invention also provides an infrared temperature measurement device, comprising:
测试温度获取模块,用于获取红外成像系统对目标实际测试出的温度;The test temperature acquisition module is used to acquire the temperature actually tested by the infrared imaging system on the target;
大气衰减修正模块,用于根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据;an atmospheric attenuation correction module, configured to perform atmospheric attenuation correction on the acquired temperature according to environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data;
修正函数获取模块,用于建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;A correction function acquisition module, configured to establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and to acquire a target proportion correction function;
成像占比修正模块,用于根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正,得到第二温度数据。The imaging ratio correction module is configured to perform target imaging ratio correction on the first temperature data according to the acquired target ratio function and the imaging radius of the target to obtain second temperature data.
本发明实施例还提供了一种红外测温设备,包括处理器和存储器,其中,所述处理器执行所述存储器中保存的计算机程序时实现如本发明实施例提供的上述红外测温方法。An embodiment of the present invention further provides an infrared temperature measurement device, including a processor and a memory, wherein the processor implements the above infrared temperature measurement method provided by the embodiment of the present invention when the processor executes the computer program stored in the memory.
本发明实施例还提供了一种计算机可读存储介质,用于存储计算机程序,其中,所述计算机程序被处理器执行时实现如本发明实施例提供的上述红外测温方法。Embodiments of the present invention further provide a computer-readable storage medium for storing a computer program, wherein when the computer program is executed by a processor, the above-mentioned infrared temperature measurement method provided by the embodiments of the present invention is implemented.
从上述技术方案可以看出,本发明所提供的一种红外测温方法,包括:获取红外成像系统对目标实际测试出的温度;根据环境变量和红外成像系统的归一化光谱响应函数,对获取的温度进行大气衰减修正,得到第一温度数据;建立红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;根据获取的目标占比函数和目标的成像半径,对第一温度数据进行目标成像占比修正,得到第二温度数据。It can be seen from the above technical solutions that an infrared temperature measurement method provided by the present invention includes: obtaining the temperature actually measured by the infrared imaging system on the target; The obtained temperature is corrected by atmospheric attenuation to obtain the first temperature data; the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target is established, and the target proportion correction function is obtained; according to the obtained target proportion function and the target The imaging radius is determined, and the target imaging ratio is corrected for the first temperature data to obtain the second temperature data.
本发明提供的上述红外测温方法,引入双变量(大气衰减及目标大小)修正方式,结合实际环境对随距衰减情况进行修正,提高了在不同环境下,中远距离目标(如500m~2km+)的测温可靠性、准确性和普适性,且使用 非标定式方案来校正红外探测器的温漂问题,在满足精度要求的前提下,大幅减小了工作量,解决了传统单波段标定测温方案的复杂性,同时能做到对高温目标的及时监控,实现森林防火、火灾预警等预防性测温检验功能。此外,本发明还针对红外测温方法提供了相应的装置、设备及计算机可读存储介质,进一步使得上述方法更具有实用性,该装置、设备及计算机可读存储介质具有相应的优点。The above-mentioned infrared temperature measurement method provided by the present invention introduces a two-variable (atmospheric attenuation and target size) correction method, and corrects the attenuation with distance in combination with the actual environment. The reliability, accuracy and universality of temperature measurement, and the non-calibration scheme is used to correct the temperature drift problem of the infrared detector. On the premise of meeting the accuracy requirements, the workload is greatly reduced, and the traditional single-band calibration is solved. Due to the complexity of the temperature measurement scheme, it can also monitor the high temperature target in time, and realize preventive temperature measurement and inspection functions such as forest fire prevention and fire warning. In addition, the present invention also provides a corresponding device, device and computer-readable storage medium for the infrared temperature measurement method, which further makes the above method more practical, and the device, device and computer-readable storage medium have corresponding advantages.
上述说明仅是本发明技术方案的概述,为了能够更清楚了解本发明的技术手段,而可依照说明书的内容予以实施,并且为了让本发明的上述和其它目的、特征和优点能够更明显易懂,以下特举本发明的具体实施方式。The above description is only an overview of the technical solutions of the present invention, in order to be able to understand the technical means of the present invention more clearly, it can be implemented according to the content of the description, and in order to make the above and other objects, features and advantages of the present invention more obvious and easy to understand , the following specific embodiments of the present invention are given.
附图说明Description of drawings
通过阅读下文优选实施方式的详细描述,各种其他的优点和益处对于本领域普通技术人员将变得清楚明了。附图仅用于示出优选实施方式的目的,而并不认为是对本发明的限制。而且在整个附图中,用相同的参考符号表示相同的部件。在附图中:Various other advantages and benefits will become apparent to those of ordinary skill in the art upon reading the following detailed description of the preferred embodiments. The drawings are for the purpose of illustrating preferred embodiments only and are not to be considered limiting of the invention. Also, the same components are denoted by the same reference numerals throughout the drawings. In the attached image:
图1示出了本发明实施例提供的红外测温方法的流程图;1 shows a flowchart of an infrared temperature measurement method provided by an embodiment of the present invention;
图2示出了本发明实施例提供的点扩散函数示意图;FIG. 2 shows a schematic diagram of a point spread function provided by an embodiment of the present invention;
图3示出了本发明实施例提供的获取目标占比修正函数的流程图;3 shows a flowchart of obtaining a target proportion correction function provided by an embodiment of the present invention;
图4示出了本发明实施例提供的获取目标的成像半径的流程图;FIG. 4 shows a flowchart of acquiring the imaging radius of a target provided by an embodiment of the present invention;
图5示出了本发明实施例提供的红外测温装置的结构示意图。FIG. 5 shows a schematic structural diagram of an infrared temperature measuring device provided by an embodiment of the present invention.
具体实施方式Detailed ways
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, rather than all the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the protection scope of the present invention.
本发明提供一种红外测温方法,如图1所示,包括以下步骤:The present invention provides an infrared temperature measurement method, as shown in Figure 1, comprising the following steps:
S101、获取红外成像系统对目标实际测试出的温度;S101. Obtain the temperature actually tested by the infrared imaging system on the target;
在实际应用中,红外成像系统对目标实际测试出的温度是通过基本测温算法实现的;In practical applications, the temperature actually measured by the infrared imaging system on the target is realized through the basic temperature measurement algorithm;
S102、根据环境变量和红外成像系统的归一化光谱响应函数,对获取的温度进行大气衰减修正,得到第一温度数据;S102, performing atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data;
需要说明的是,传统大气衰减修正方案应用时通常只考虑外部环境的影响,而忽略了成像系统的光谱响应函数对其的影响,因此本发明参考长波红外在低海平面大气窗口的衰减情况,并导入光学系统的光谱响应函数,进一步修正大气衰减系数,使其更接近实际应用;It should be noted that the traditional atmospheric attenuation correction scheme usually only considers the influence of the external environment, while ignoring the influence of the spectral response function of the imaging system on it. Therefore, the present invention refers to the attenuation of long-wave infrared in the low sea level atmospheric window, And import the spectral response function of the optical system to further correct the atmospheric attenuation coefficient to make it closer to practical applications;
S103、建立红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;S103, establishing a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtaining a target proportion correction function;
可以理解的是,由于光学镜头对于点光源辐射存在点扩散函数PSF,即一点光源产生的辐射经过光学成像系统后输出的广场分布,其演示图如图2所示。由于光学成像系统的线性特性,即某一点的图像可认为是图像内每个点的PSF的总和。对于红外成像系统而言,除了输入辐射随目标距离增加而衰减外,成像系统的输出辐射是输入辐射与PSF的卷积结果:It can be understood that since the optical lens has a point spread function PSF for the point light source radiation, that is, the square distribution of the radiation generated by the point light source after passing through the optical imaging system, its demonstration diagram is shown in Figure 2. Due to the linear nature of the optical imaging system, the image of a certain point can be considered as the sum of the PSFs of each point in the image. For the infrared imaging system, except that the input radiation decays with the increase of the target distance, the output radiation of the imaging system is the result of the convolution of the input radiation and the PSF:
Figure PCTCN2020134228-appb-000008
Figure PCTCN2020134228-appb-000008
获取输入辐射可以进行反卷积运算或构建校正矩阵进行精确修正等。由于点扩散函数获取较为复杂,且若想精确修正所需要的卷积核过大,不利于工程应用。因此,本发明采用目标成像占比修正的方式实现对温度的修正,简单快捷;Deconvolution operations can be performed to obtain the input radiation or a correction matrix can be constructed for precise correction, etc. Because the acquisition of the point spread function is more complicated, and the convolution kernel required for accurate correction is too large, it is not conducive to engineering applications. Therefore, the present invention adopts the method of correcting the proportion of target imaging to realize the correction of temperature, which is simple and fast;
S104、根据获取的目标占比函数和目标的成像半径,对第一温度数据进行目标成像占比修正,得到第二温度数据。S104. According to the obtained target ratio function and the imaging radius of the target, perform target imaging ratio correction on the first temperature data to obtain second temperature data.
在本发明实施例提供的上述红外测温方法中,引入双变量(大气衰减及目标大小)修正方式,结合实际环境对随距衰减情况进行修正,提高了在不同环境下,中远距离目标(如500m~2km+)的测温可靠性、准确性和普适性,且使用非标定式方案来校正红外探测器的温漂问题,在满足精度要求的前提下,大幅减小了工作量,解决了传统单波段标定测温方案的复杂性,同时能做到对高温目标的及时监控,实现森林防火、火灾预警等预 防性测温检验功能。In the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, a two-variable (atmospheric attenuation and target size) correction method is introduced, and the attenuation with distance is corrected in combination with the actual environment, which improves the performance of medium and long-distance targets (such as 500m~2km+) temperature measurement reliability, accuracy and universality, and the non-calibration scheme is used to correct the temperature drift problem of infrared detectors. On the premise of meeting the accuracy requirements, the workload is greatly reduced, and the The complexity of the traditional single-band calibration temperature measurement scheme, at the same time, it can monitor the high temperature target in time, and realize the preventive temperature measurement and inspection functions such as forest fire prevention and fire warning.
进一步地,在具体实施时,在本发明实施例提供的上述红外测温方法中,步骤S102根据环境变量和红外成像系统的归一化光谱响应函数,对获取的温度进行大气衰减修正,得到第一温度数据,具体可以包括以下步骤:Further, in the specific implementation, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, step S102 performs atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature. A temperature data, which may specifically include the following steps:
步骤一、获取不同大气成分对红外辐射的光谱透过率和散射函数,得到红外成像系统的大气衰减系数;Step 1: Obtain the spectral transmittance and scattering function of different atmospheric components to infrared radiation, and obtain the atmospheric attenuation coefficient of the infrared imaging system;
在实际应用中,对于海拔高度在水平面附近(小于1km)的远距离长波红外辐射主要考虑CO 2/H 2O对辐射的吸收,以及气溶胶杂质对红外辐射的散射。在实施例中,可以使用查表法获得不同大气成分对红外辐射的光谱透过率以及散射函数,得出成像系统的响应波段[λ 12]的大气衰减系数τ(x)的拟合公式: In practical applications, the absorption of CO 2 /H 2 O and the scattering of infrared radiation by aerosol impurities are mainly considered for long-distance long-wave infrared radiation at altitudes near the horizontal plane (less than 1 km). In the embodiment, the spectral transmittance and scattering function of different atmospheric components to infrared radiation can be obtained by using the look-up table method, and the approximate atmospheric attenuation coefficient τ(x) of the response band [λ 1 , λ 2 ] of the imaging system can be obtained. Combined formula:
Figure PCTCN2020134228-appb-000009
Figure PCTCN2020134228-appb-000009
其中,
Figure PCTCN2020134228-appb-000010
为CO 2对不同波段红外辐射的吸收率,可以通过查表获得,可使用400ppm数据;
Figure PCTCN2020134228-appb-000011
为H 2O对不同波段红外辐射的吸收率,可以通过查表获得;τ Aero为气溶胶对红外辐射的散射函数;λ为红外成像系统的响应波长;[λ 12]为红外成像系统的响应波段,由红外成像系统设计决定,可通过光谱响应测试系统测试得到;x为外部输入的目标距离、CO 2含量、相对湿度、环境温度、可见度;
in,
Figure PCTCN2020134228-appb-000010
is the absorption rate of CO 2 to infrared radiation in different bands, which can be obtained by looking up the table, and 400ppm data can be used;
Figure PCTCN2020134228-appb-000011
is the absorption rate of H 2 O to infrared radiation in different bands, which can be obtained by looking up the table; τ Aero is the scattering function of aerosol to infrared radiation; λ is the response wavelength of the infrared imaging system; [λ 12 ] is the infrared imaging The response band of the system is determined by the design of the infrared imaging system and can be obtained by testing the spectral response test system; x is the external input target distance, CO 2 content, relative humidity, ambient temperature, and visibility;
步骤二、根据红外成像系统的归一化光谱响应函数,对得到的大气衰减系数进行修正;Step 2, correcting the obtained atmospheric attenuation coefficient according to the normalized spectral response function of the infrared imaging system;
需要说明的是,可以首先通过下述公式确认红外成像系统的响应波段[λ 12]对应的归一化光谱响应函数: It should be noted that the normalized spectral response function corresponding to the response band [λ 12 ] of the infrared imaging system can be confirmed by the following formula:
Figure PCTCN2020134228-appb-000012
Figure PCTCN2020134228-appb-000012
Figure PCTCN2020134228-appb-000013
Figure PCTCN2020134228-appb-000013
C 1=3.7415×10 8W·μm 4/m 2 C 1 =3.7415×10 8 W·μm 4 /m 2
C 2=1.43879×10 4μm·K C 2 =1.43879×10 4 μm·K
其中,SRF sys为红外成像系统的归一化光谱响应函数;SRF Dete为探测器的归一化光谱响应函数,该函数反映了红外探测器对不同波段的响应情况,由探测器设计决定,可以通过光谱测试得到;Transmittance Lens为红外镜头对不同波段红外辐射的归一化透过率函数,由镜头材料及光学设计决定,可以通过测试得到;M 为理想黑体的红外光谱辐射出射度;T为对辐射度归一化所用的温度值,使用成像系统测试范围的中值来近似代表测温范围,如目标测温范围在0~150℃,T=75℃; Among them, SRF sys is the normalized spectral response function of the infrared imaging system; SRF Dete is the normalized spectral response function of the detector, which reflects the response of the infrared detector to different bands, which is determined by the detector design and can be Obtained by spectral test; Transmittance Lens is the normalized transmittance function of infrared lens to infrared radiation in different bands, which is determined by lens material and optical design, and can be obtained by testing; M is the infrared spectral radiation emittance of an ideal black body; T For the temperature value used to normalize the radiance, the median value of the imaging system test range is used to approximate the temperature measurement range, for example, the target temperature measurement range is 0-150°C, T=75°C;
然后可以采用下述公式对得到的大气衰减系数进行修正:The resulting atmospheric attenuation coefficient can then be corrected using the following formula:
Figure PCTCN2020134228-appb-000014
Figure PCTCN2020134228-appb-000014
其中,τ re为修正后的大气衰减系数; where τ re is the modified atmospheric attenuation coefficient;
步骤三、根据修正后的大气衰减系数,对获取的温度进行大气衰减修正,得到第一温度数据;Step 3: Perform atmospheric attenuation correction on the acquired temperature according to the corrected atmospheric attenuation coefficient to obtain first temperature data;
具体地,红外成像系统接受的红外辐射主要包括三部分:目标发射的能量、目标反射的能量、大气环境的能量,根据基础红外物理可以采用下述公式得到第一温度数据:Specifically, the infrared radiation received by the infrared imaging system mainly includes three parts: the energy emitted by the target, the energy reflected by the target, and the energy of the atmospheric environment. According to basic infrared physics, the following formula can be used to obtain the first temperature data:
Figure PCTCN2020134228-appb-000015
Figure PCTCN2020134228-appb-000015
其中,T out1为第一温度数据;e为目标发射率;T m为获取的温度;T env为环境温度;n由响应波段的玻尔兹曼定理决定;E aim为目标发射的能量;E ref为目标反射的能量;E env为大气环境的能量。 Among them, T out1 is the first temperature data; e is the target emissivity; T m is the acquired temperature; T env is the ambient temperature; n is determined by the Boltzmann theorem of the response band; E aim is the energy emitted by the target; E ref is the energy reflected by the target; E env is the energy of the atmospheric environment.
在具体实施时,在本发明实施例提供的上述红外测温方法中,步骤S103建立红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数,具体可以包括以下步骤:During specific implementation, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, step S103 establishes the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtains the target proportion correction function, which may be specifically Include the following steps:
首先,将红外成像系统的光轴对准相同温度、不同半径的圆形黑体,使黑体成像在画面正中心,获取红外成像系统中心点的输出能量E;在实际应用中,红外成像系统与黑体需要间隔一定距离l,该距离l为该红外成像系统的最小成像距离,即使黑体边缘清晰的最短距离;First, align the optical axis of the infrared imaging system with a circular black body with the same temperature and different radii, so that the black body is imaged in the center of the screen, and obtain the output energy E of the center point of the infrared imaging system; in practical applications, the infrared imaging system and the black body It needs to be separated by a certain distance l, and this distance l is the minimum imaging distance of the infrared imaging system, even if the black body edge is clear and the shortest distance;
然后,以黑体在红外成像系统中所占像素的半径作为自变量,建立红外成像系统中心点的输出能量E与目标的成像半径之间的函数关系;具体 地,该函数关系为E=f(r);Then, taking the radius of the pixel occupied by the black body in the infrared imaging system as the independent variable, the functional relationship between the output energy E of the center point of the infrared imaging system and the imaging radius of the target is established; specifically, the functional relationship is E=f( r);
最后,对建立的函数关系进行归一化,获取目标占比修正函数,并将获取的目标占比修正函数预存在红外成像系统的处理器内。具体地,黑体对应的目标占比修正函数为θ(r)=E(r)/E(r max)=a*r^b+1(推荐拟合表达式);E(r)为黑体在红外成像系统中所占像素的半径为r时红外成像系统中心点的输出能量;E(r max)为黑体占满全屏幕时的中心点输出;a和b由θ、E(r)和E(r max)决定。当目标的成像半径为r'时,目标占比修正函数为θ(r')=a*r'^b+1。 Finally, the established functional relationship is normalized to obtain the target proportion correction function, and the obtained target proportion correction function is pre-stored in the processor of the infrared imaging system. Specifically, the target proportion correction function corresponding to the black body is θ(r)=E(r)/E(r max )=a*r^b+1 (recommended fitting expression); E(r) is the black body at The output energy of the center point of the infrared imaging system when the radius of the pixel occupied in the infrared imaging system is r; E(r max ) is the output of the center point when the black body occupies the full screen; a and b are determined by θ, E(r) and E (r max ) decides. When the imaging radius of the target is r', the target proportion correction function is θ(r')=a*r'^b+1.
具体地,如图3所示,根据不同半径黑体的测温结果,以不同半径黑体在成像系统中所占像素的半径作为自变量([r1,r2,r3,r4]),以红外成像系统对不同半径黑体中心点的测温结果,进行归一化作为因变量([t1,t2,t3,t4]/t5);得出目标占比修正函数θ(r)=a*r^b+1,对其进行拟合,最后将目标占比修正函数的拟合公式存储在成像系统处理器中。Specifically, as shown in Figure 3, according to the temperature measurement results of black bodies with different radii, the radii of the pixels occupied by black bodies with different radii in the imaging system are used as independent variables ([r1, r2, r3, r4]), and the infrared imaging system Normalize the temperature measurement results of the black body center points with different radii as the dependent variable ([t1, t2, t3, t4]/t5); obtain the target proportion correction function θ(r)=a*r^b+ 1. Fit it, and finally store the fitting formula of the target ratio correction function in the imaging system processor.
在具体实施时,在本发明实施例提供的上述红外测温方法中,在执行步骤S104根据获取的目标占比函数和目标的成像半径,对第一温度数据进行目标成像占比修正之前,还可以包括:首先,选取目标成像中任意点(如森林火点,可选取温度超过350℃的点),沿该点行列方向进行差分运算,获取该点连通域的近似长与宽;然后,根据获取的连通域的近似长与宽,得到连通域对应的等面积圆的半径,将等面积圆的半径作为目标的成像半径。In specific implementation, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, before performing step S104 to perform target imaging ratio correction on the first temperature data according to the obtained target ratio function and the imaging radius of the target, further It can include: first, select any point in the target imaging (such as a forest fire point, a point with a temperature exceeding 350°C can be selected), perform a difference operation along the row and column directions of the point, and obtain the approximate length and width of the connected domain of the point; then, according to The approximate length and width of the obtained connected domain are obtained, the radius of the equal-area circle corresponding to the connected domain is obtained, and the radius of the equal-area circle is taken as the imaging radius of the target.
具体地,设温度成像矩阵dataT,成像像高为H,像宽为W,如图4所示,选取测温目标中任意点在成像中的坐标[i0,j0];对点[i0,j0]水平与垂直方向(即行列方向)做差分,得到该测温目标的水平与垂直所占像素个数,即得到包含测温目标连通域的近似长与宽:Specifically, set the temperature imaging matrix dataT, the imaging image height is H, and the image width is W, as shown in Figure 4, select the coordinates [i0, j0] of any point in the temperature measurement target in the imaging; for the point [i0, j0 ] The difference between the horizontal and vertical directions (that is, the row and column directions) is obtained to obtain the number of pixels occupied by the temperature measurement target horizontally and vertically, that is, to obtain the approximate length and width of the connected domain containing the temperature measurement target:
第一步、对目标点的行方向进行差分运算(matlab代码如下):The first step is to perform a differential operation on the row direction of the target point (the matlab code is as follows):
Row_dif=diff(dataT(i0,:));Row_dif=diff(dataT(i0,:));
Col_dif=diff(dataT(:,j0));Col_dif=diff(dataT(:,j0));
其中,Row_dif为行差分数据;Col_dif为列差分数据;Among them, Row_dif is row difference data; Col_dif is column difference data;
第二步、获取行/列差分数据中,最大最小值之间的坐标,即为该目标 点的行列方向上变化最大的边缘,其坐标差即为该目标点连通域的近似长与宽:The second step is to obtain the row/column difference data. The coordinates between the maximum and minimum values are the edges with the largest change in the row and column directions of the target point, and the coordinate difference is the approximate length and width of the connected domain of the target point:
[w1,tmp]=max(Row_dif)[w1,tmp]=max(Row_dif)
[w2,tmp]=min(Row_dif)[w2,tmp]=min(Row_dif)
[h1,tmp]=max(Col_dif)[h1,tmp]=max(Col_dif)
[h2,tmp]=min(Col_dif)[h2,tmp]=min(Col_dif)
height=abs(w1-w2)height=abs(w1-w2)
width=abs(h1–h2)width=abs(h1–h2)
其中,height和width分别为获取的连通域的近似长与宽。Among them, height and width are the approximate length and width of the obtained connected domain, respectively.
接下来,根据获取的连通域的height和width,得到连通域对应的等面积圆的半径
Figure PCTCN2020134228-appb-000016
Next, according to the obtained height and width of the connected domain, the radius of the equal-area circle corresponding to the connected domain is obtained
Figure PCTCN2020134228-appb-000016
在具体实施时,在本发明实施例提供的上述红外测温方法中,采用下述公式得到第二温度数据:During specific implementation, in the above-mentioned infrared temperature measurement method provided by the embodiment of the present invention, the following formula is used to obtain the second temperature data:
Figure PCTCN2020134228-appb-000017
Figure PCTCN2020134228-appb-000017
其中,T out2为第二温度数据。 Wherein, T out2 is the second temperature data.
经实际测试,使用本发明,在1公里范围内,对不同温度、不同大小的目标的测温精度可达到±10℃内,远远优于没有此修正方案的结果。After actual testing, using the present invention, within 1 km, the temperature measurement accuracy of targets with different temperatures and sizes can reach ±10°C, which is far better than the result without this correction scheme.
基于同一发明构思,本发明实施例还提供了一种红外测温装置,由于该红外测温装置解决问题的原理与前述一种红外测温方法相似,因此该红外测温装置的实施可以参见红外测温方法的实施,重复之处不再赘述。Based on the same inventive concept, an embodiment of the present invention also provides an infrared temperature measurement device. Since the principle of solving the problem of the infrared temperature measurement device is similar to that of the aforementioned infrared temperature measurement method, the implementation of the infrared temperature measurement device can refer to the infrared temperature measurement device. The implementation of the temperature measurement method will not be repeated here.
在具体实施时,本发明实施例提供的红外测温装置,如图5所示,具体包括:During specific implementation, the infrared temperature measurement device provided by the embodiment of the present invention, as shown in FIG. 5 , specifically includes:
测试温度获取模块11,用于获取红外成像系统对目标实际测试出的温度;The test temperature acquisition module 11 is used to acquire the temperature actually tested by the infrared imaging system on the target;
大气衰减修正模块12,用于根据环境变量和红外成像系统的归一化光谱响应函数,对获取的温度进行大气衰减修正,得到第一温度数据;The atmospheric attenuation correction module 12 is used for performing atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain the first temperature data;
修正函数获取模块13,用于建立红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;The correction function acquisition module 13 is used to establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtain the target proportion correction function;
成像占比修正模块14,用于根据获取的目标占比函数和目标的成像半径,对第一温度数据进行目标成像占比修正,得到第二温度数据。The imaging ratio correction module 14 is configured to perform target imaging ratio correction on the first temperature data according to the acquired target ratio function and the imaging radius of the target to obtain second temperature data.
在本发明实施例提供的上述红外测温装置中,可以通过上述四个模块的相互作用,解决传统单波段标定测温方案的复杂性,同时,提高对中远距离目标的测温准确性,能做到对高温目标的及时监控,实现森林防火、火灾预警等预防性测温检验功能。In the above-mentioned infrared temperature measurement device provided by the embodiment of the present invention, the interaction of the above-mentioned four modules can solve the complexity of the traditional single-band calibration temperature measurement scheme, and at the same time, the temperature measurement accuracy of medium and long-distance targets can be improved. Realize the timely monitoring of high temperature targets, and realize preventive temperature measurement and inspection functions such as forest fire prevention and fire warning.
关于上述各个模块更加具体的工作过程可以参考前述实施例公开的相应内容,在此不再进行赘述。For more specific working processes of the above-mentioned modules, reference may be made to the corresponding contents disclosed in the foregoing embodiments, which will not be repeated here.
相应的,本发明实施例还公开了一种红外测温设备,包括处理器和存储器;其中,处理器执行存储器中保存的计算机程序时实现前述实施例公开的红外测温方法。Correspondingly, the embodiment of the present invention also discloses an infrared temperature measurement device, including a processor and a memory; wherein, the processor implements the infrared temperature measurement method disclosed in the foregoing embodiments when the processor executes the computer program stored in the memory.
关于上述方法更加具体的过程可以参考前述实施例中公开的相应内容,在此不再进行赘述。For a more specific process of the above method, reference may be made to the corresponding content disclosed in the foregoing embodiments, which will not be repeated here.
进一步的,本发明还公开了一种计算机可读存储介质,用于存储计算机程序;计算机程序被处理器执行时实现前述公开的红外测温方法。Further, the present invention also discloses a computer-readable storage medium for storing a computer program; when the computer program is executed by a processor, the infrared temperature measurement method disclosed above is implemented.
关于上述方法更加具体的过程可以参考前述实施例中公开的相应内容,在此不再进行赘述。For a more specific process of the above method, reference may be made to the corresponding content disclosed in the foregoing embodiments, which will not be repeated here.
本说明书中各个实施例采用递进的方式描述,每个实施例重点说明的都是与其它实施例的不同之处,各个实施例之间相同或相似部分互相参见即可。对于实施例公开的装置、设备、存储介质而言,由于其与实施例公开的方法相对应,所以描述的比较简单,相关之处参见方法部分说明即可。The various embodiments in this specification are described in a progressive manner, and each embodiment focuses on the differences from other embodiments, and the same or similar parts between the various embodiments may be referred to each other. For the apparatuses, devices, and storage media disclosed in the embodiments, since they correspond to the methods disclosed in the embodiments, the descriptions are relatively simple, and reference may be made to the descriptions of the methods for related parts.
专业人员还可以进一步意识到,结合本文中所公开的实施例描述的各示例的单元及算法步骤,能够以电子硬件、计算机软件或者二者的结合来实现,为了清楚地说明硬件和软件的可互换性,在上述说明中已经按照功能一般性地描述了各示例的组成及步骤。这些功能究竟以硬件还是软件方式来执行,取决于技术方案的特定应用和设计约束条件。专业技术人员可以对每个特定的应用来使用不同方法来实现所描述的功能,但是这种实现 不应认为超出本申请的范围。Professionals may further realize that the units and algorithm steps of each example described in conjunction with the embodiments disclosed herein can be implemented in electronic hardware, computer software, or a combination of the two, in order to clearly illustrate the possibilities of hardware and software. Interchangeability, the above description has generally described the components and steps of each example in terms of function. Whether these functions are performed in hardware or software depends on the specific application and design constraints of the technical solution. Skilled artisans may implement the described functionality using different methods for each particular application, but such implementations should not be considered beyond the scope of this application.
结合本文中所公开的实施例描述的方法或算法的步骤可以直接用硬件、处理器执行的软件模块,或者二者的结合来实施。软件模块可以置于随机存储器(RAM)、内存、只读存储器(ROM)、电可编程ROM、电可擦除可编程ROM、寄存器、硬盘、可移动磁盘、CD-ROM、或技术领域内所公知的任意其它形式的存储介质中。The steps of a method or algorithm described in conjunction with the embodiments disclosed herein may be directly implemented in hardware, a software module executed by a processor, or a combination of the two. A software module can be placed in random access memory (RAM), internal memory, read only memory (ROM), electrically programmable ROM, electrically erasable programmable ROM, registers, hard disk, removable disk, CD-ROM, or any other in the technical field. in any other known form of storage medium.
本发明实施例提供的一种红外测温方法,包括:获取红外成像系统对目标实际测试出的温度;根据环境变量和红外成像系统的归一化光谱响应函数,对获取的温度进行大气衰减修正,得到第一温度数据;建立红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;根据获取的目标占比函数和目标的成像半径,对第一温度数据进行目标成像占比修正,得到第二温度数据。上述红外测温方法,引入双变量(大气衰减及目标大小)修正方式,结合实际环境对随距衰减情况进行修正,提高了在不同环境下,中远距离目标(如500m~2km+)的测温可靠性、准确性和普适性,且使用非标定式方案来校正红外探测器的温漂问题,在满足精度要求的前提下,大幅减小了工作量,解决了传统单波段标定测温方案的复杂性,同时能做到对高温目标的及时监控,实现森林防火、火灾预警等预防性测温检验功能。此外,本发明还针对红外测温方法提供了相应的装置、设备及计算机可读存储介质,进一步使得上述方法更具有实用性,该装置、设备及计算机可读存储介质具有相应的优点。An infrared temperature measurement method provided by an embodiment of the present invention includes: acquiring a temperature actually measured by an infrared imaging system on a target; performing atmospheric attenuation correction on the acquired temperature according to environmental variables and a normalized spectral response function of the infrared imaging system , obtain the first temperature data; establish the functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtain the target proportion correction function; according to the obtained target proportion function and the imaging radius of the target, the first The temperature data is subjected to target imaging ratio correction to obtain second temperature data. The above infrared temperature measurement method introduces a two-variable (atmospheric attenuation and target size) correction method, and combines the actual environment to correct the attenuation with distance, which improves the reliability of temperature measurement for medium and long-distance targets (such as 500m ~ 2km+) in different environments In addition, the non-calibration scheme is used to correct the temperature drift problem of infrared detectors. Under the premise of meeting the accuracy requirements, the workload is greatly reduced, and the traditional single-band calibration temperature measurement scheme is solved. At the same time, it can monitor the high temperature target in time, and realize the preventive temperature measurement and inspection functions such as forest fire prevention and fire warning. In addition, the present invention also provides a corresponding device, device and computer-readable storage medium for the infrared temperature measurement method, which further makes the above method more practical, and the device, device and computer-readable storage medium have corresponding advantages.
最后,还需要说明的是,在本文中,诸如第一和第二等之类的关系术语仅仅用来将一个实体或者操作与另一个实体或操作区分开来,而不一定要求或者暗示这些实体或操作之间存在任何这种实际的关系或者顺序。而且,术语“包括”、“包含”或者其任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的过程、方法、物品或者设备不仅包括那些要素,而且还包括没有明确列出的其他要素,或者是还包括为这种过程、方法、物品或者设备所固有的要素。在没有更多限制的情况下,由语句“包括一个……”限定的要素,并不排除在包括所述要素的过程、方法、物品或者设备中还存在另外的相同要素。Finally, it should also be noted that in this document, relational terms such as first and second are used only to distinguish one entity or operation from another, and do not necessarily require or imply these entities or that there is any such actual relationship or sequence between operations. Moreover, the terms "comprising", "comprising" or any other variation thereof are intended to encompass a non-exclusive inclusion such that a process, method, article or device comprising a list of elements includes not only those elements, but also includes not explicitly listed or other elements inherent to such a process, method, article or apparatus. Without further limitation, an element qualified by the phrase "comprising a..." does not preclude the presence of additional identical elements in a process, method, article or apparatus that includes the element.
以上对本发明所提供的红外测温方法、装置、设备及存储介质进行了详细介绍,本文中应用了具体个例对本发明的原理及实施方式进行了阐述,以上实施例的说明只是用于帮助理解本发明的方法及其核心思想;同时,对于本领域的一般技术人员,依据本发明的思想,在具体实施方式及应用范围上均会有改变之处,综上所述,本说明书内容不应理解为对本发明的限制。凡在本发明的精神和原理之内所作的任何修改、等同替换、改进等,均应包含在本发明的权利要求范围之内。The infrared temperature measurement method, device, equipment and storage medium provided by the present invention have been introduced in detail above. Specific examples are used in this paper to illustrate the principles and implementations of the present invention. The descriptions of the above examples are only used to help understanding The method of the present invention and its core idea; at the same time, for those skilled in the art, according to the idea of the present invention, there will be changes in the specific implementation and application scope. In summary, the content of this specification should not be It is construed as a limitation of the present invention. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of the present invention shall be included within the scope of the claims of the present invention.

Claims (10)

  1. 一种红外测温方法,其特征在于,包括:An infrared temperature measurement method, comprising:
    获取红外成像系统对目标实际测试出的温度;Obtain the temperature actually tested by the infrared imaging system on the target;
    根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据;Perform atmospheric attenuation correction on the acquired temperature according to the environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data;
    建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;establishing a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and obtaining a target proportion correction function;
    根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正,得到第二温度数据。According to the acquired target ratio function and the imaging radius of the target, the target imaging ratio correction is performed on the first temperature data to obtain second temperature data.
  2. 根据权利要求1所述的红外测温方法,其特征在于,根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据,具体包括:The infrared temperature measurement method according to claim 1, wherein, according to environmental variables and the normalized spectral response function of the infrared imaging system, atmospheric attenuation correction is performed on the acquired temperature to obtain first temperature data, Specifically include:
    获取不同大气成分对红外辐射的光谱透过率和散射函数,得到所述红外成像系统的大气衰减系数;Obtain the spectral transmittance and scattering function of different atmospheric components to infrared radiation, and obtain the atmospheric attenuation coefficient of the infrared imaging system;
    根据所述红外成像系统的归一化光谱响应函数,对得到的大气衰减系数进行修正;Correcting the obtained atmospheric attenuation coefficient according to the normalized spectral response function of the infrared imaging system;
    根据修正后的大气衰减系数,对获取的所述温度进行大气衰减修正,得到第一温度数据。Perform atmospheric attenuation correction on the acquired temperature according to the corrected atmospheric attenuation coefficient to obtain first temperature data.
  3. 根据权利要求2所述的红外测温方法,其特征在于,采用下述公式对得到的大气衰减系数进行修正:Infrared temperature measurement method according to claim 2, is characterized in that, adopts following formula to correct the atmospheric attenuation coefficient obtained:
    Figure PCTCN2020134228-appb-100001
    Figure PCTCN2020134228-appb-100001
    Figure PCTCN2020134228-appb-100002
    Figure PCTCN2020134228-appb-100002
    Figure PCTCN2020134228-appb-100003
    Figure PCTCN2020134228-appb-100003
    C 1=3.7415×10 8W·μm 4/m 2 C 1 =3.7415×10 8 W·μm 4 /m 2
    C 2=1.43879×10 4μm·K C 2 =1.43879×10 4 μm·K
    其中,τ re为修正后的大气衰减系数;
    Figure PCTCN2020134228-appb-100004
    为CO 2对不同波段红外辐射 的吸收率;
    Figure PCTCN2020134228-appb-100005
    为H 2O对不同波段红外辐射的吸收率;τ Aero为气溶胶对红外辐射的散射函数;λ为所述红外成像系统的响应波长;[λ 12]为所述红外成像系统的响应波段;x为外部输入的目标距离、CO 2含量、相对湿度、环境温度、可见度;SRF sys为所述红外成像系统的归一化光谱响应函数;SRF Dete为探测器的归一化光谱响应函数;Transmittance Lens为红外镜头对不同波段红外辐射的归一化透过率函数;M 为理想黑体的红外光谱辐射出射度;T为对辐射度归一化所用的温度值。
    where τ re is the modified atmospheric attenuation coefficient;
    Figure PCTCN2020134228-appb-100004
    is the absorption rate of CO 2 to infrared radiation in different bands;
    Figure PCTCN2020134228-appb-100005
    is the absorption rate of H 2 O to infrared radiation in different bands; τ Aero is the scattering function of aerosol to infrared radiation; λ is the response wavelength of the infrared imaging system; [λ 12 ] is the infrared imaging system Response band; x is the external input target distance, CO 2 content, relative humidity, ambient temperature, visibility; SRF sys is the normalized spectral response function of the infrared imaging system; SRF Dete is the normalized spectral response of the detector function; Transmittance Lens is the normalized transmittance function of the infrared lens to infrared radiation in different bands; M is the infrared spectral radiation emittance of an ideal black body; T is the temperature value used for normalizing the radiance.
  4. 根据权利要求3所述的红外测温方法,其特征在于,采用下述公式得到第一温度数据:Infrared temperature measurement method according to claim 3, is characterized in that, adopts following formula to obtain first temperature data:
    Figure PCTCN2020134228-appb-100006
    Figure PCTCN2020134228-appb-100006
    其中,T out1为所述第一温度数据;e为目标发射率;T m为获取的所述温度;T env为环境温度;n由响应波段的玻尔兹曼定理决定。 Wherein, T out1 is the first temperature data; e is the target emissivity; T m is the acquired temperature; T env is the ambient temperature; n is determined by Boltzmann's theorem of the response band.
  5. 根据权利要求4所述的红外测温方法,其特征在于,建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数,具体包括:The infrared temperature measurement method according to claim 4, wherein a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target is established, and the target proportion correction function is obtained, which specifically includes:
    将所述红外成像系统的光轴对准相同温度、不同半径的圆形黑体,使所述黑体成像在画面正中心,获取所述红外成像系统中心点的输出能量;Align the optical axis of the infrared imaging system with a circular black body of the same temperature and different radii, so that the black body is imaged in the center of the screen, and obtain the output energy of the center point of the infrared imaging system;
    以所述黑体在所述红外成像系统中所占像素的半径作为自变量,建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系;Using the radius of the pixel occupied by the black body in the infrared imaging system as an independent variable, establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target;
    对建立的所述函数关系进行归一化,获取目标占比修正函数,并将获取的所述目标占比修正函数预存在所述红外成像系统的处理器内。The established functional relationship is normalized to obtain a target proportion correction function, and the obtained target proportion correction function is pre-stored in the processor of the infrared imaging system.
  6. 根据权利要求5所述的红外测温方法,其特征在于,在根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正之前,还包括:The infrared temperature measurement method according to claim 5, wherein, before performing target imaging ratio correction on the first temperature data according to the acquired target ratio function and the target imaging radius, the method further comprises:
    选取目标成像中任意点,沿该点行列方向进行差分运算,获取该点连通域的近似长与宽;Select any point in the target image, perform the difference operation along the row and column directions of the point, and obtain the approximate length and width of the connected domain of the point;
    根据获取的所述连通域的近似长与宽,得到所述连通域对应的等面积圆的半径,将所述等面积圆的半径作为目标的成像半径。According to the obtained approximate length and width of the connected domain, the radius of the equal-area circle corresponding to the connected domain is obtained, and the radius of the equal-area circle is used as the imaging radius of the target.
  7. 根据权利要求6所述的红外测温方法,其特征在于,采用下述公式 得到第二温度数据:Infrared temperature measurement method according to claim 6, is characterized in that, adopts following formula to obtain second temperature data:
    Figure PCTCN2020134228-appb-100007
    Figure PCTCN2020134228-appb-100007
    θ(r)=E(r)/E(r max)=a*r^b+1 θ(r)=E(r)/E(r max )=a*r^b+1
    其中,T out2为所述第二温度数据;height和width分别为获取的所述连通域的近似长与宽;r'为所述等面积圆的半径;θ为所述目标占比修正函数,E(r)为所述黑体在所述红外成像系统中所占像素的半径为r时所述红外成像系统中心点的输出能量;E(r max)为所述黑体占满全屏幕时的中心点输出;a和b由θ、E(r)和E(r max)决定。 Wherein, T out2 is the second temperature data; height and width are the obtained approximate length and width of the connected domain, respectively; r' is the radius of the equal-area circle; θ is the target ratio correction function, E(r) is the output energy of the center point of the infrared imaging system when the radius of the pixel occupied by the black body in the infrared imaging system is r; E(r max ) is the center when the black body occupies the full screen Point output; a and b are determined by θ, E(r) and E(r max ).
  8. 一种红外测温装置,其特征在于,包括:An infrared temperature measuring device, comprising:
    测试温度获取模块,用于获取红外成像系统对目标实际测试出的温度;The test temperature acquisition module is used to acquire the temperature actually tested by the infrared imaging system on the target;
    大气衰减修正模块,用于根据环境变量和所述红外成像系统的归一化光谱响应函数,对获取的所述温度进行大气衰减修正,得到第一温度数据;an atmospheric attenuation correction module, configured to perform atmospheric attenuation correction on the acquired temperature according to environmental variables and the normalized spectral response function of the infrared imaging system to obtain first temperature data;
    修正函数获取模块,用于建立所述红外成像系统中心点的输出能量与目标的成像半径之间的函数关系,获取目标占比修正函数;A correction function acquisition module, configured to establish a functional relationship between the output energy of the center point of the infrared imaging system and the imaging radius of the target, and to acquire a target proportion correction function;
    成像占比修正模块,用于根据获取的所述目标占比函数和目标的成像半径,对所述第一温度数据进行目标成像占比修正,得到第二温度数据。The imaging ratio correction module is configured to perform target imaging ratio correction on the first temperature data according to the acquired target ratio function and the imaging radius of the target to obtain second temperature data.
  9. 一种红外测温设备,其特征在于,包括处理器和存储器,其中,所述处理器执行所述存储器中保存的计算机程序时实现如权利要求1至7任一项所述的红外测温方法。An infrared temperature measurement device, characterized in that it comprises a processor and a memory, wherein the processor implements the infrared temperature measurement method according to any one of claims 1 to 7 when the processor executes a computer program stored in the memory .
  10. 一种计算机可读存储介质,其特征在于,用于存储计算机程序,其中,所述计算机程序被处理器执行时实现如权利要求1至7任一项所述的红外测温方法。A computer-readable storage medium, characterized in that it is used for storing a computer program, wherein when the computer program is executed by a processor, the infrared temperature measurement method according to any one of claims 1 to 7 is implemented.
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