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CN118817256A - A moving target detection performance evaluation method for infrared optoelectronic imaging system based on NVThermIP model - Google Patents

A moving target detection performance evaluation method for infrared optoelectronic imaging system based on NVThermIP model Download PDF

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CN118817256A
CN118817256A CN202411009979.9A CN202411009979A CN118817256A CN 118817256 A CN118817256 A CN 118817256A CN 202411009979 A CN202411009979 A CN 202411009979A CN 118817256 A CN118817256 A CN 118817256A
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temperature
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段文博
王怡恬
郭冰涛
蔡鹏程
陈雷
韩琪
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Xian institute of Applied Optics
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Abstract

本发明提供了一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,该方法综合考虑目标的机动性能、目标及背景的辐射差异、红外系统对比度阈值函数及人眼视觉模型对目标探测性能的影响,将目标对比度超过红外光电系统对比度阈值的空间频率加权积分数值作为红外系统获得的目标信息量,从而获得设定观测距离下的目标等效周期数,结合目标传递概率函数计算探测概率,使得红外动目标探测性能计算结果更符合实际。

The present invention provides a method for evaluating the moving target detection performance of an infrared optoelectronic imaging system based on the NVThermIP model. The method comprehensively considers the maneuverability of the target, the radiation difference between the target and the background, the contrast threshold function of the infrared system and the influence of the human eye vision model on the target detection performance, and takes the spatial frequency weighted integral value of the target contrast exceeding the contrast threshold of the infrared optoelectronic system as the target information amount obtained by the infrared system, thereby obtaining the target equivalent period number under the set observation distance, and calculating the detection probability in combination with the target transfer probability function, so that the calculation result of the infrared moving target detection performance is more in line with reality.

Description

一种基于NVThermIP模型的红外光电成像系统动目标探测性 能评估方法A moving target detection performance evaluation method for infrared optoelectronic imaging system based on NVThermIP model

技术领域Technical Field

本发明属于红外光电成像系统性能评估技术领域,具体涉及一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法。The present invention belongs to the technical field of infrared optoelectronic imaging system performance evaluation, and specifically relates to a method for evaluating the moving target detection performance of an infrared optoelectronic imaging system based on an NVThermIP model.

背景技术Background Art

光电成像系统广泛应用于安防监控、无人驾驶、工业检测等领域,随着红外光电成像系统工艺、结构及设计技术的不断提升,对红外光电成像系统的性能评估方法的优化提升提出了更高的要求,以提高对红外光电成像系统论证、设计及分析的准确性。鉴于实验法和半实物仿真法具有复杂多变环境适应性差、经费需求高、难以实现系统性能预测及参数优化等缺点,基于性能理论模型的光电系统评估方法可打破上述技术难点,实现光电系统性能评估及优化设计,并有助于分析系统性能,对精准评价红外光电成像系统性能预测具有重要指导意义。Optoelectronic imaging systems are widely used in security monitoring, unmanned driving, industrial inspection and other fields. With the continuous improvement of infrared optoelectronic imaging system technology, structure and design technology, higher requirements are put forward for the optimization and improvement of infrared optoelectronic imaging system performance evaluation methods, so as to improve the accuracy of demonstration, design and analysis of infrared optoelectronic imaging systems. In view of the shortcomings of experimental methods and semi-physical simulation methods, such as poor adaptability to complex and changing environments, high funding requirements, and difficulty in achieving system performance prediction and parameter optimization, the optoelectronic system evaluation method based on the performance theoretical model can break through the above technical difficulties, realize the performance evaluation and optimization design of the optoelectronic system, and help analyze the system performance, which has important guiding significance for the accurate evaluation of the performance prediction of infrared optoelectronic imaging systems.

目前针对光电系统性能评价的模型一般有三种。第一种是以约翰逊准则为基础的MRTD模型,该模型忽略了眼睛对比度阈值的限制且带有主观因素,性能评估准确性有待提升;第二种是以约翰逊准则为基础的三角形方位辨别阈值性能模型(TOD),该模型忽略了系统最高空间分辨率以内的传递特性,无法对焦平面红外光电成像系统及数字图像处理系统性能进行准确评估;第三种是以目标任务性能(TTP)准则为理论基础的NVThermIP模型,引入传感器成像特性和人眼视觉机制,在低对比度情况下仍具有较好的预测结果,但是一般都是对光电成像系统的静态性能进行评价,无法实现机动目标探测性能的准确评估。At present, there are generally three models for evaluating the performance of optoelectronic systems. The first is the MRTD model based on the Johnson criterion, which ignores the limitation of the eye contrast threshold and has subjective factors, and the accuracy of performance evaluation needs to be improved; the second is the triangle orientation discrimination threshold performance model (TOD) based on the Johnson criterion, which ignores the transfer characteristics within the highest spatial resolution of the system and cannot accurately evaluate the performance of the focal plane infrared optoelectronic imaging system and the digital image processing system; the third is the NVThermIP model based on the target task performance (TTP) criterion, which introduces the imaging characteristics of the sensor and the visual mechanism of the human eye, and still has good prediction results under low contrast conditions, but generally evaluates the static performance of the optoelectronic imaging system and cannot achieve accurate evaluation of the detection performance of maneuvering targets.

在上述研究基础上,出现了对于运动目标探测距离、探测概率等特性进行评估的方法,例如SVM法、帧差法、深度学习法。但这些方法在评估过程中大多没有考虑人眼视觉对动目标探测的影响,导致评估结果准确性差;同时模型本身是从目标探测的角度出发,对红外光电成像系统性能参数和探测能力的研究不够完善,难以实现对动目标探测能力进行精准评估。Based on the above research, there are methods for evaluating the detection distance and detection probability of moving targets, such as SVM method, frame difference method, and deep learning method. However, most of these methods do not consider the impact of human vision on moving target detection during the evaluation process, resulting in poor accuracy of the evaluation results; at the same time, the model itself is based on the perspective of target detection, and the research on the performance parameters and detection capabilities of infrared optoelectronic imaging systems is not perfect, making it difficult to achieve accurate evaluation of moving target detection capabilities.

发明内容Summary of the invention

本发明的目的在于克服现有光电成像系统探测性能评价方法无法实现机动目标探测性能评估或评估准确性差的不足之处,而提供了一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,该方法综合考虑目标的机动性能、目标及背景的辐射差异、红外系统对比度阈值函数及人眼视觉模型对动目标探测性能的影响,使红外动目标探测性能评估结果更符合实际,实现了对光电成像系统机动目标探测性能的准确预测。The purpose of the present invention is to overcome the shortcomings of the existing optoelectronic imaging system detection performance evaluation method that cannot realize the evaluation of maneuvering target detection performance or has poor evaluation accuracy, and provide an infrared optoelectronic imaging system moving target detection performance evaluation method based on the NVThermIP model. The method comprehensively considers the influence of the maneuverability of the target, the radiation difference between the target and the background, the contrast threshold function of the infrared system and the human eye vision model on the moving target detection performance, so that the infrared moving target detection performance evaluation result is more in line with reality, and the accurate prediction of the maneuvering target detection performance of the optoelectronic imaging system is realized.

为实现上述目的,本发明所提供的技术解决方案是:To achieve the above purpose, the technical solution provided by the present invention is:

一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,其特殊之处在于,包括以下步骤:A moving target detection performance evaluation method for an infrared optoelectronic imaging system based on the NVThermIP model includes the following steps:

步骤1,搭建红外光电成像系统动目标探测性能评估系统,所述评估系统包括红外光电成像系统、标准黑体源、测距机、黑色目标、可移动小车、黑色背景和辐射测量计;Step 1, building an infrared optoelectronic imaging system moving target detection performance evaluation system, the evaluation system comprising an infrared optoelectronic imaging system, a standard black body source, a rangefinder, a black target, a movable vehicle, a black background and a radiation meter;

将标准黑体源安装在可移动小车上,黑色目标安装在标准黑体源窗口处;The standard black body source is installed on a movable trolley, and the black target is installed at the window of the standard black body source;

所述红外光电成像系统和辐射测量计架设在可移动小车外,所述辐射测量计用于采集目标本征温度;The infrared photoelectric imaging system and the radiometer are mounted outside the movable vehicle, and the radiometer is used to collect the intrinsic temperature of the target;

步骤2,启动可移动小车,进行黑色目标移动模拟,连续采集目标成像特征,并获取标准黑体源不同温度下的测量参数,所述测量参数包括目标温度、背景温度和探测距离;Step 2, starting the movable vehicle, performing a black target movement simulation, continuously collecting target imaging features, and obtaining measurement parameters of a standard black body source at different temperatures, wherein the measurement parameters include target temperature, background temperature, and detection distance;

步骤3,计算不同探测距离下目标与红外光电成像系统的大气透过率,得到探测距离与大气透过率的关系曲线τ(R);Step 3, calculating the atmospheric transmittance of the target and the infrared photoelectric imaging system at different detection distances, and obtaining a relationship curve τ(R) between the detection distance and the atmospheric transmittance;

步骤4,构建基于NVThermIP的动目标探测概率计算模型,对所述概率计算模型参数进行初始化;所述参数包括目标温度、背景温度、探测距离和红外光电成像系统参数;Step 4: construct a moving target detection probability calculation model based on NVThermIP and initialize the parameters of the probability calculation model; the parameters include target temperature, background temperature, detection distance and infrared photoelectric imaging system parameters;

步骤5,根据步骤2得到的测量参数计算目标辐射出射度MT和背景辐射出射度MB,并根据目标辐射出射度和背景辐射出射度计算目标背景对比度CtgtStep 5, calculating the target radiation emittance MT and the background radiation emittance MB according to the measurement parameters obtained in step 2, and calculating the target background contrast Ctgt according to the target radiation emittance and the background radiation emittance;

所述目标背景对比度 The target background contrast

式中,MT为目标辐射出射度,MB为背景辐射出射度,ΔT为目标与背景的温差,TB为背景温度;Where, MT is the target radiation emittance, MB is the background radiation emittance, ΔT is the temperature difference between the target and the background, and TB is the background temperature;

步骤6,根据红外光电成像系统的调制传递函数MTF和人眼对比度阈值函数CTFeye(f)计算获取系统对比度阈值函数CTFsysStep 6, calculating and obtaining the system contrast threshold function CTF sys according to the modulation transfer function MTF of the infrared optoelectronic imaging system and the contrast threshold function CTF eye (f) of the human eye;

所述红外光电成像系统的调制传递函数MTF=MTFop·MTFdet·MTFcic·MTFdisThe modulation transfer function MTF of the infrared optoelectronic imaging system is MTF op ·MTF det ·MTF cic ·MTF dis ,

式中,MTFop、MTFdet、MTFcic、MTFdis分别为光学系统调制传递函数、红外光电成像系统调制传递函数、光电转化电路调制传递函数和显示器调制传递函数;Where, MTF op , MTF det , MTF cic and MTF dis are the modulation transfer function of the optical system, the modulation transfer function of the infrared photoelectric imaging system, the modulation transfer function of the photoelectric conversion circuit and the modulation transfer function of the display, respectively;

式中,f为空间频率,σ为显示的均方根噪声,L为显示器亮度,α是关于噪声对亮度的校正因子;Where f is the spatial frequency, σ is the displayed RMS noise, L is the display brightness, and α is the correction factor for noise to brightness;

b=0.3(1+100/L)0.15,b=0.3(1+100/L) 0.15 ,

c=0.06,c=0.06,

式中,θ为表现目标角,Atgt为目标面积,M为系统放大倍数,R为目标与红外光电成像系统之间的距离;Where θ is the target angle, Atgt is the target area, M is the system magnification, and R is the distance between the target and the infrared optoelectronic imaging system;

步骤7,以目标背景对比度Ctgt超过系统对比度阈值函数CTFsys的空间频率进行加权积分取代约翰逊准则中的极限空间频率,计算目标任务性能TTP,获取目标图像信息量;Step 7, replace the limit spatial frequency in the Johnson criterion with the spatial frequency at which the target background contrast C tgt exceeds the system contrast threshold function CTF sys by weighted integration, calculate the target task performance TTP, and obtain the target image information;

式中:ξhigh和ξlow为空间频率的上下限,ξhigh为系统对比度阈值函数CTFsys和目标背景对比度Ctgt的交点对应的空间频率值,ξlow取为0;单位为cyc/mrad。In the formula: ξ high and ξ low are the upper and lower limits of the spatial frequency, ξ high is the spatial frequency value corresponding to the intersection of the system contrast threshold function CTF sys and the target background contrast C tgt , and ξ low is taken as 0; the unit is cyc/mrad.

步骤8,根据目标观测距离和目标的临界特征尺寸,计算目标在对应观测距离下的目标任务等效周期数,Step 8, according to the target observation distance and the critical characteristic size of the target, calculate the target task equivalent cycle number at the corresponding observation distance,

所述目标任务等效周期数为 The equivalent cycle number of the target task is

所述目标的临界特征尺寸通过对目标面积Atgt开方得到;The critical characteristic size of the target is obtained by taking the square root of the target area A tgt ;

步骤9,利用50%的点落在目标任务性能曲线TTP的目标传递概率函数计算得到动目标探测概率P;Step 9, using the target transfer probability function where 50% of the points fall on the target task performance curve TTP, the moving target detection probability P is calculated;

E=1.51+0.24(V/V50),E=1.51+0.24(V/V 50 ),

其中,E为目标探测任务等级;V50是完成任务概率为50%的可分辨周期数,由实验测量得到;V为目标任务等效周期数。Where E is the target detection task level; V50 is the number of resolvable cycles with a task completion probability of 50%, which is obtained by experimental measurement; and V is the number of equivalent cycles of the target task.

进一步地,所述步骤2包括以下步骤:Furthermore, the step 2 comprises the following steps:

步骤2.1,设置标准黑体源的温度,通过辐射测量计采集目标及背景的黑体等效温度;Step 2.1, set the temperature of the standard blackbody source, and collect the blackbody equivalent temperature of the target and background through the radiometer;

步骤2.2,设定可移动小车运动速度、运动轨迹和探测距离,小车运动时连续采集目标的红外成像特征;Step 2.2, setting the moving speed, moving trajectory and detection distance of the movable car, and continuously collecting the infrared imaging characteristics of the target when the car moves;

步骤2.3,调节标准黑体源温度,重复执行步骤2.1和2.2,得到不同黑体温度下的测量参数。Step 2.3, adjust the temperature of the standard blackbody source, repeat steps 2.1 and 2.2, and obtain the measurement parameters at different blackbody temperatures.

进一步地,所述步骤3包括以下步骤:Furthermore, the step 3 comprises the following steps:

步骤3.1,固定红外光电成像系统位置和目标的高度不变,等距离调节辐射测量计到目标的距离,采集不同探测距离下目标本征温度;Step 3.1, fix the position of the infrared photoelectric imaging system and the height of the target, adjust the distance from the radiometer to the target at equal distances, and collect the intrinsic temperature of the target at different detection distances;

步骤3.2,将温度与目标本征温度等效的黑体放置于不同位置,测量黑体在红外光电成像系统的辐射亮度,并通过普朗克公式计算黑体辐射亮度值,以目标本体辐射亮度值与黑体辐射亮度值的比值作为对应探测距离下的大气透过率;Step 3.2, place a black body with a temperature equivalent to the intrinsic temperature of the target at different positions, measure the radiation brightness of the black body in the infrared photoelectric imaging system, and calculate the black body radiation brightness value by Planck's formula, and take the ratio of the target body radiation brightness value to the black body radiation brightness value as the atmospheric transmittance at the corresponding detection distance;

步骤3.3,根据步骤3.2得到的不同探测距离下的大气透过率,得到探测距离与大气透过率的关系曲线τ(R)。Step 3.3, according to the atmospheric transmittance at different detection distances obtained in step 3.2, obtain a relationship curve τ(R) between the detection distance and the atmospheric transmittance.

进一步地,所述步骤3.1中,以1米为间隔距离,等间距调节辐射测量计到目标的距离。Furthermore, in step 3.1, the distance between the radiation meter and the target is adjusted at equal intervals with 1 meter as the interval distance.

进一步地,所述步骤5中,目标辐射出射度MT和背景辐射出射度MB根据以下公式式计算得到:Furthermore, in step 5, the target radiation emittance MT and the background radiation emittance MB are calculated according to the following formula:

所述目标辐射出射度MT计算公式为:The target radiation emittance MT calculation formula is:

所述背景辐射出射度MB计算公式为:The background radiation emittance MB calculation formula is:

式中,C1为第一辐射常数,C1=(3.7415±0.0003)×108(W·μm4·m-2);λ1和λ2为红外光电成像系统光谱范围的上下限,单位为μm;C2为第二辐射常数,C2=(1.43879±0.00019)×104(μm·K);TT为目标温度,TB为背景温度,单位为K;ε(λB)和ε(λT)分别为背景光谱发射率和目标光谱发射率。Wherein, C 1 is the first radiation constant, C 1 =(3.7415±0.0003)×10 8 (W·μm 4 ·m -2 ); λ 1 and λ 2 are the upper and lower limits of the spectral range of the infrared optoelectronic imaging system, in μm; C 2 is the second radiation constant, C 2 =(1.43879±0.00019)×10 4 (μm·K); TT is the target temperature, TB is the background temperature, in K; ε(λB) and ε(λT) are the background spectral emissivity and target spectral emissivity, respectively.

本发明的优点是:The advantages of the present invention are:

本发明方法中首先搭建评估实验系统,通过被测红外光电成像系统连续采集目标的成像特征,基于NVThermIP模型探测概率计算过程中,综合考虑目标的机动性能、目标及背景的辐射差异、红外系统对比度阈值函数及人眼视觉模型对动目标探测性能的影响,将目标对比度超过红外光电系统对比度阈值的空间频率加权积分数值作为红外系统获得的目标信息量,从而获得一定观测距离下的目标等效周期数,结合目标传递概率函数计算获得探测概率。通过与实验结果对比,采用本发明方法评估结果准确性高,使红外动目标探测性能评估结果更符合实际情况。In the method of the present invention, an evaluation experimental system is firstly built, and the imaging features of the target are continuously collected by the infrared photoelectric imaging system under test. In the process of calculating the detection probability based on the NVThermIP model, the maneuverability of the target, the radiation difference between the target and the background, the infrared system contrast threshold function and the human eye vision model are comprehensively considered to affect the detection performance of the moving target. The spatial frequency weighted integral value of the target contrast exceeding the contrast threshold of the infrared photoelectric system is used as the target information obtained by the infrared system, so as to obtain the target equivalent cycle number under a certain observation distance, and the detection probability is obtained by combining the target transfer probability function calculation. By comparing with the experimental results, the evaluation results of the method of the present invention are highly accurate, making the evaluation results of the infrared moving target detection performance more in line with the actual situation.

附图说明BRIEF DESCRIPTION OF THE DRAWINGS

本发明的上述和/或附加的方面和优点从结合下面附图对实施例的描述中将变得明显和容易理解,其中:The above and/or additional aspects and advantages of the present invention will become apparent and easily understood from the description of the embodiments in conjunction with the following drawings, in which:

图1是本发明方法中搭建的评估系统示意图;FIG1 is a schematic diagram of an evaluation system constructed in the method of the present invention;

图2是采用本发明模型方法计算动目标探测性能概率的流程框图;FIG2 is a flowchart of calculating the moving target detection performance probability using the model method of the present invention;

图3是采用人工判别动目标探测性能概率的评估计算流程框图;FIG3 is a flowchart of the evaluation calculation process of the probability of detecting moving targets by manual discrimination;

图4是本发明方法评估结果与理论结果对比图。FIG. 4 is a comparison diagram of the evaluation results of the method of the present invention and the theoretical results.

附图标记说明:1-可移动小车,2-黑体固定支架,3-标准黑体源,4-镂空目标,5-红外光电成像系统,6-辐射测量计。Explanation of the reference numerals: 1- movable trolley, 2- blackbody fixing bracket, 3- standard blackbody source, 4- hollow target, 5- infrared photoelectric imaging system, 6- radiation meter.

具体实施方式DETAILED DESCRIPTION

下面详细描述本发明的实施例,所述实施例是示例性的,旨在用于解释本发明,而不能理解为对本发明的限制。Embodiments of the present invention are described in detail below. The embodiments are exemplary and intended to be used to explain the present invention, but should not be construed as limiting the present invention.

参照图1-图2,一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,具体包括以下步骤:1-2, a method for evaluating the moving target detection performance of an infrared optoelectronic imaging system based on the NVThermIP model specifically includes the following steps:

步骤1,搭建评估实验系统。Step 1: Build an evaluation experimental system.

参照图1,所述评估实验系统包括可移动小车1、黑体固定支架2、标准黑体源3、镂空目标4、红外光电成像系统5、测距机、辐射测量计6和黑色纸板。所述的实验前准备工作体现了对实验设备、环境、标定全面性和移动性的考量,以确保实验能够顺利进行并取得准确可靠的标定结果。另外该实验考虑了目标的机动性能,使红外动目标探测性能评估方法更加全面、准确和实用,提高系统的性能和可靠性。Referring to Figure 1, the evaluation experimental system includes a movable trolley 1, a black body fixing bracket 2, a standard black body source 3, a hollow target 4, an infrared photoelectric imaging system 5, a rangefinder, a radiation meter 6 and a black cardboard. The pre-experimental preparations reflect the consideration of experimental equipment, environment, calibration comprehensiveness and mobility to ensure that the experiment can proceed smoothly and obtain accurate and reliable calibration results. In addition, the experiment takes into account the maneuverability of the target, making the infrared moving target detection performance evaluation method more comprehensive, accurate and practical, and improving the performance and reliability of the system.

为模拟不同型号的目标轮廓特性,将黑色纸板裁剪成不同形状,作为镂空目标,便于进行多次试验,评估红外光电成像系统对动目标的探测性能。In order to simulate the contour characteristics of targets of different types, black cardboard was cut into different shapes as hollow targets to facilitate multiple tests and evaluate the detection performance of the infrared optoelectronic imaging system for moving targets.

首先将一个裁剪的镂空目标粘贴在标准黑体源3的窗口位置处,然后将标准黑体源3通过黑体固定支架2安装在可移动小车1上。将红外光电成像系统5和辐射测量计6可移动小车外,所述红外光电成像系统5用于采集不同温度及形状下的目标成像特征,所述辐射测量计6用于获取目标本征温度。在进行评估时,需要先完成对红外光电成像系统的标定工作。First, a cut hollow target is pasted at the window position of the standard black body source 3, and then the standard black body source 3 is installed on the movable trolley 1 through the black body fixing bracket 2. The infrared photoelectric imaging system 5 and the radiometer 6 are placed outside the movable trolley. The infrared photoelectric imaging system 5 is used to collect the imaging characteristics of the target under different temperatures and shapes, and the radiometer 6 is used to obtain the target intrinsic temperature. When conducting the evaluation, the calibration of the infrared photoelectric imaging system needs to be completed first.

采用黑色纸板作为目标背景,用以模拟均匀背景。Black cardboard was used as the target background to simulate a uniform background.

设定标准黑体源3温度,利用靶标固定装置将标准黑体源固定。The temperature of the standard black body source 3 is set, and the standard black body source is fixed by using a target fixing device.

步骤2,目标辐射数据采集及目标轨迹模拟。Step 2: Target radiation data collection and target trajectory simulation.

设置标准黑体源的温度,以该温度作为目标温度,通过辐射测量计采集目标及背景的黑体等效温度。Set the temperature of the standard blackbody source, use this temperature as the target temperature, and collect the blackbody equivalent temperature of the target and background through the radiometer.

设定可移动小车运动速度、运动轨迹和探测距离,启动可移动小车,保持红外光电成像系统5位置不变,通过红外光电成像系统连续采集可移动小车上镂空目标的成像特征。The moving speed, moving trajectory and detection distance of the movable car are set, the movable car is started, the position of the infrared photoelectric imaging system 5 is kept unchanged, and the imaging features of the hollowed-out target on the movable car are continuously collected by the infrared photoelectric imaging system.

通过调节标准黑体源温度,指定不同的目标运动速度、目标尺寸、成像距离等条件,保持红外光电成像系统位置不变,连续采集目标的成像特征。By adjusting the temperature of the standard blackbody source and specifying different target movement speeds, target sizes, imaging distances and other conditions, the position of the infrared photoelectric imaging system is kept unchanged and the imaging features of the target are continuously collected.

在实验过程中,获取不同面元黑体温度下的测量参数,包括:目标温度、背景温度、探测距离等,这些参数为后续进行模型计算提供数据。During the experiment, the measurement parameters at different panel blackbody temperatures are obtained, including target temperature, background temperature, detection distance, etc. These parameters provide data for subsequent model calculations.

步骤3,获取镂空目标4与红外光电成像系统间的大气透过率。Step 3, obtaining the atmospheric transmittance between the hollow target 4 and the infrared photoelectric imaging system.

首先,固定红外光电成像系统位置和目标的高度不变,通每间隔一米调节辐射测量计6到目标的距离,即探测距离,采集目标本征温度;First, the position of the infrared photoelectric imaging system and the height of the target are fixed, and the distance from the radiometer 6 to the target, i.e., the detection distance, is adjusted every one meter to collect the target intrinsic temperature;

然后,将温度与目标本征温度等效的黑体放置于不同位置,测量黑体在红外光电成像系统的辐射亮度,同时通过普朗克公式计算得到黑体辐射亮度值,以目标本体辐射亮度值与黑体辐射亮度值的比值作为对应探测距离下的大气透过率。Then, a black body with a temperature equivalent to the intrinsic temperature of the target is placed at different positions, and the radiation brightness of the black body in the infrared photoelectric imaging system is measured. At the same time, the black body radiation brightness value is calculated by Planck's formula, and the ratio of the target body radiation brightness value to the black body radiation brightness value is used as the atmospheric transmittance at the corresponding detection distance.

采用上述方法,得到不同探测距离下目标与红外光电成像系统的大气透过率数据,据此得到探测距离与大气透过率的关系曲线τ(R)。By adopting the above method, the atmospheric transmittance data of the target and the infrared photoelectric imaging system at different detection distances are obtained, and the relationship curve τ(R) between the detection distance and the atmospheric transmittance is obtained accordingly.

步骤4,建立基于NVThermIP的动目标探测概率计算模型,并对所述概率计算模型参数进行初始化,所述参数包括目标温度、背景温度、探测距离和红外光电成像系统参数。Step 4: Establish a moving target detection probability calculation model based on NVThermIP and initialize the parameters of the probability calculation model, which include target temperature, background temperature, detection distance and infrared photoelectric imaging system parameters.

考虑目标背景对比度、系统噪声对比度阈值、探测距离、目标传递函数对探测性能影响,所构建的动目标探测概率计算模型包括参数初始化模块、目标背景对比度计算模块、红外光电成像系统MTF计算模块、人眼及显示器噪声退化计算模块、系统对比度阈值计算模块、目标任务性能TTP计算模块以及探测概率计算模块。Considering the influence of target background contrast, system noise contrast threshold, detection distance and target transfer function on detection performance, the constructed moving target detection probability calculation model includes parameter initialization module, target background contrast calculation module, infrared optoelectronic imaging system MTF calculation module, human eye and display noise degradation calculation module, system contrast threshold calculation module, target task performance TTP calculation module and detection probability calculation module.

步骤5,目标背景对比度计算。Step 5: Calculate the target-background contrast.

目标背景对比度是通过设置不同温度差异的目标及背景,结合步骤3获得的距离与大气透过率τ(R)的关系曲线进行计算获得。The target-background contrast ratio is calculated by setting the target and background with different temperature differences and combining the relationship curve between the distance and the atmospheric transmittance τ(R) obtained in step 3.

先根据步骤2得到的镂空目标和背景的温度数据,根据以下公式计算目标辐射出射度MT和背景辐射出射度MBFirst, according to the temperature data of the hollowed-out target and background obtained in step 2, the target radiation emittance MT and the background radiation emittance MB are calculated according to the following formula;

式中,C1为第一辐射常数,C1=(3.7415±0.0003)×108(W·μm4·m-2);λ1和λ2为红外光电成像系统光谱范围的上下限;Wherein, C 1 is the first radiation constant, C 1 =(3.7415±0.0003)×10 8 (W·μm 4 ·m -2 ); λ 1 and λ 2 are the upper and lower limits of the spectral range of the infrared optoelectronic imaging system;

C2为第二辐射常数,C2=(1.43879±0.00019)×104(μm·K);TT为目标温度,TB为背景温度,单位为K;ε(λB)和ε(λT)分别为背景光谱发射率和目标光谱发射率。C 2 is the second radiation constant, C 2 =(1.43879±0.00019)×10 4 (μm·K); TT is the target temperature, TB is the background temperature, the unit is K; ε(λB) and ε(λT) are the background spectral emissivity and the target spectral emissivity, respectively.

然后根据公式计算目标背景对比度Ctgt,所述目标背景对比度计算公式为:Then, the target background contrast C tgt is calculated according to the formula, and the target background contrast calculation formula is:

式中,MT为目标辐射出射度,MB为背景辐射出射度,ΔT为目标与背景的温差,TB为背景温度。Where MT is the target radiation emittance, MB is the background radiation emittance, ΔT is the temperature difference between the target and the background, and TB is the background temperature.

步骤6,计算系统对比度阈值函数CTFsysStep 6: Calculate the system contrast threshold function CTF sys .

系统对比度阈值函数是通过将系统各模块的调制作用相叠加得到红外光电系统成像退化效应,计算过程中,引入人眼对比度阈值函数CTFeye进行计算系统对比度阈值函数CTFsys。人眼及显示器噪声通过假设观测者的CTF退化来建模。所述红外光电成像系统的调制传递函数MTF=MTFop·MTFdet·MTFcic·MTFdisThe system contrast threshold function is obtained by superimposing the modulation effects of each module of the system to obtain the infrared photoelectric system imaging degradation effect. In the calculation process, the human eye contrast threshold function CTF eye is introduced to calculate the system contrast threshold function CTF sys . The human eye and display noise are modeled by assuming the observer's CTF degradation. The modulation transfer function MTF of the infrared photoelectric imaging system is MTF = MTF op ·MTF det ·MTF cic ·MTF dis ,

式中,MTFop、MTFdet、MTFcic、MTFdis分别为光学系统调制传递函数、红外光电成像系统调制传递函数、光电转化电路调制传递函数和显示器调制传递函数。Where MTF op , MTF det , MTF cic and MTF dis are the modulation transfer function of the optical system, the modulation transfer function of the infrared photoelectric imaging system, the modulation transfer function of the photoelectric conversion circuit and the modulation transfer function of the display, respectively.

场景中的信号先后受传感器的光学系统、红外光电成像系统、电子电路、显示器和人眼调制,计算上述引入的图像退化MTF。噪声影响通过人眼对比度阈值函数CTF建模:The signal in the scene is modulated by the optical system of the sensor, the infrared photoelectric imaging system, the electronic circuit, the display and the human eye, and the image degradation MTF introduced above is calculated. The noise effect is modeled by the human eye contrast threshold function CTF:

式中,f为空间频率,σ为显示的均方根噪声,L为显示器亮度,α是关于噪声对亮度的校正因子;Where f is the spatial frequency, σ is the displayed RMS noise, L is the display brightness, and α is the correction factor for noise to brightness;

b=0.3(1+100/L)0.15,b=0.3(1+100/L) 0.15 ,

c=0.06,c=0.06,

式中,θ为表现目标角,Atgt为目标面积,M为系统放大倍数,R为目标与红外光电成像系统之间的距离。Where θ is the target angle, Atgt is the target area, M is the system magnification, and R is the distance between the target and the infrared optoelectronic imaging system.

步骤7,以目标背景对比度Ctgt超过系统对比度阈值函数CTFsys的空间频率进行加权积分取代约翰逊准则中的极限空间频率,计算目标任务性能TTP,获取目标图像信息量。Step 7, the spatial frequency at which the target background contrast C tgt exceeds the system contrast threshold function CTF sys is used for weighted integration to replace the limit spatial frequency in the Johnson criterion, calculate the target task performance TTP, and obtain the target image information amount.

目标信号超过系统的阈值,则认为可以获取目标信息。以目标对比度超过红外光电系统对比度阈值的空间频率加权积分数值作为红外系统获得的目标信息量,来定义TTP函数:When the target signal exceeds the threshold of the system, it is considered that the target information can be obtained. The spatial frequency weighted integral value of the target contrast exceeding the contrast threshold of the infrared optoelectronic system is used as the target information obtained by the infrared system to define the TTP function:

式中ξhigh和ξlow为空间频率上下限,ξhigh为系统对比度阈值函数CTFsys和目标背景对比度Ctgt的交点对应的空间频率值,ξlow为0;单位cyc/mrad。Where ξ high and ξ low are the upper and lower limits of the spatial frequency, ξ high is the spatial frequency value corresponding to the intersection of the system contrast threshold function CTF sys and the target background contrast C tgt , and ξ low is 0; the unit is cyc/mrad.

步骤8,结合目标观测距离和目标的临界特征尺寸,计算该目标在此距离下的目标任务等效周期数V。Step 8, combining the target observation distance and the critical characteristic size of the target, calculate the target task equivalent cycle number V of the target at this distance.

所述目标任务等效周期数为 The equivalent cycle number of the target task is

所述目标的临界特征尺寸通过对目标面积开方得到;The critical characteristic size of the target is obtained by taking the square root of the target area;

步骤9,利用50%的点落在目标识别任务曲线TTP的目标传递概率函数计算目标探测概率P。Step 9, calculate the target detection probability P using the target transfer probability function where 50% of the points fall on the target recognition task curve TTP.

所述目标探测概率计算公式为:The target detection probability calculation formula is:

E=1.51+0.24(V/V50)。E = 1.51 + 0.24 (V/V 50 ).

其中,E为目标探测任务等级;V50是完成任务概率为50%可分辨周期数,由实验测量得到;V为目标任务等效周期数。Where E is the target detection task level; V50 is the number of resolvable cycles with a 50% probability of completing the task, which is obtained by experimental measurement; and V is the number of equivalent cycles of the target task.

最为了验证采用本发明基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,对红外光电成像系统在不同目标形状、成像距离、靶标尺寸、目标运动速度下的动目标的探测性能评估的准确性,在系统参数输入设置一致情况下,将基于人眼视觉的实验测量结果与采用本发明方法的评估结果进行了对比分析。In order to verify the moving target detection performance evaluation method of the infrared optoelectronic imaging system based on the NVThermIP model of the present invention, the accuracy of the detection performance evaluation of the infrared optoelectronic imaging system for moving targets under different target shapes, imaging distances, target sizes, and target movement speeds was evaluated. Under the condition that the system parameter input settings were consistent, the experimental measurement results based on human eye vision were compared with the evaluation results of the method of the present invention.

参照图3,对于目标不同形状及不同目标背景差异下的目标,通过人工判别方式计算目标探测概率。按照与本发明方法相同的设置温度,调节标准黑体源温度T1,T2,...,Tn,采集不同温度下各个目标的成像特征,组织多位人员分别对各目标成像结果进行判读,观测者必须对目标是否探测进行判读,即判断目标可探测或不可探测,通过计算可探测到目标的人数与总观测人数间的比值,获得不同目标尺寸及目标背景温差下的实验目标探测概率。3 , for targets with different shapes and different target background differences, the target detection probability is calculated by manual discrimination. According to the same setting temperature as the method of the present invention, the standard black body source temperature T 1 , T 2 , ..., T n is adjusted, the imaging characteristics of each target at different temperatures are collected, and multiple personnel are organized to interpret the imaging results of each target respectively. The observer must judge whether the target is detectable, that is, whether the target is detectable or not. By calculating the ratio between the number of people who can detect the target and the total number of observers, the experimental target detection probability under different target sizes and target background temperature differences is obtained.

采用本发明方法在评估相同条件下红外成光电成像系统对不同目标的探测概率,然后将本发明评估结果与人工平评估结果(理论结果)进行对比分析,参照图4。结果表明,本发明提出的红外动目标探测性能评估方法能够对运动目标进行探测,并且运动目标速度越大,背景温差越大,其探测概率越高,即本发明方法对运动目标的探测性能优于静目标探测。The method of the present invention is used to evaluate the detection probability of different targets of the infrared optoelectronic imaging system under the same conditions, and then the evaluation results of the present invention are compared and analyzed with the artificial level evaluation results (theoretical results), as shown in Figure 4. The results show that the infrared moving target detection performance evaluation method proposed in the present invention can detect moving targets, and the greater the speed of the moving target and the greater the background temperature difference, the higher the detection probability, that is, the detection performance of the method of the present invention for moving targets is better than that for static targets.

以上所述,仅为本发明的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明公开的技术范围内,可轻易想到各种等效的修改或替换,这些修改或替换都应涵盖在本发明的保护范围之内。The above description is only a specific implementation mode of the present invention, but the protection scope of the present invention is not limited thereto. Any technician familiar with the technical field can easily think of various equivalent modifications or substitutions within the technical scope disclosed in the present invention, and these modifications or substitutions should be included in the protection scope of the present invention.

Claims (5)

1.一种基于NVThermIP模型的红外光电成像系统动目标探测性能评估方法,其特征在于,包括以下步骤:1. A method for evaluating the moving target detection performance of an infrared optoelectronic imaging system based on the NVThermIP model, characterized in that it comprises the following steps: 步骤1,搭建红外光电成像系统动目标探测性能评估系统,所述评估系统包括红外光电成像系统、标准黑体源、测距机、黑色目标、可移动小车、黑色背景和辐射测量计;Step 1, building an infrared optoelectronic imaging system moving target detection performance evaluation system, the evaluation system comprising an infrared optoelectronic imaging system, a standard black body source, a rangefinder, a black target, a movable vehicle, a black background and a radiation meter; 将标准黑体源安装在可移动小车上,黑色目标安装在标准黑体源窗口处;The standard black body source is installed on a movable trolley, and the black target is installed at the window of the standard black body source; 所述红外光电成像系统和辐射测量计架设在可移动小车外,所述辐射测量计用于采集目标本征温度;The infrared photoelectric imaging system and the radiometer are mounted outside the movable vehicle, and the radiometer is used to collect the intrinsic temperature of the target; 步骤2,启动可移动小车,进行黑色目标移动模拟,连续采集目标成像特征,并获取不同标准黑体源温度下的测量参数,所述测量参数包括目标温度、背景温度和探测距离;Step 2, starting the movable vehicle, performing a black target movement simulation, continuously collecting target imaging features, and obtaining measurement parameters at different standard blackbody source temperatures, wherein the measurement parameters include target temperature, background temperature, and detection distance; 步骤3,计算不同探测距离下目标与红外光电成像系统的大气透过率,得到探测距离与大气透过率的关系曲线τ(R);Step 3, calculating the atmospheric transmittance of the target and the infrared photoelectric imaging system at different detection distances, and obtaining a relationship curve τ(R) between the detection distance and the atmospheric transmittance; 步骤4,构建基于NVThermIP的动目标探测概率计算模型,对所述概率计算模型参数进行初始化;所述参数包括目标温度、背景温度、探测距离和红外光电成像系统参数;Step 4: construct a moving target detection probability calculation model based on NVThermIP and initialize the parameters of the probability calculation model; the parameters include target temperature, background temperature, detection distance and infrared photoelectric imaging system parameters; 步骤5,根据步骤2得到的测量参数计算目标辐射出射度MT和背景辐射出射度MB,并根据目标辐射出射度和背景辐射出射度计算目标背景对比度CtgtStep 5, calculating the target radiation emittance MT and the background radiation emittance MB according to the measurement parameters obtained in step 2, and calculating the target background contrast Ctgt according to the target radiation emittance and the background radiation emittance; 所述目标背景对比度 The target background contrast 式中,MT为目标辐射出射度,MB为背景辐射出射度,ΔT为目标与背景的温差,TB为背景温度;Where, MT is the target radiation emittance, MB is the background radiation emittance, ΔT is the temperature difference between the target and the background, and TB is the background temperature; 步骤6,根据红外光电成像系统的调制传递函数MTF和人眼对比度阈值函数CTFeye(f)计算获取系统对比度阈值函数CTFsysStep 6, calculating and obtaining the system contrast threshold function CTF sys according to the modulation transfer function MTF of the infrared optoelectronic imaging system and the contrast threshold function CTF eye (f) of the human eye; 所述红外光电成像系统的调制传递函数MTF=MTFop·MTFdet·MTFcic·MTFdisThe modulation transfer function MTF of the infrared optoelectronic imaging system is MTF op ·MTF det ·MTF cic ·MTF dis , 式中,MTFop、MTFdet、MTFcic、MTFdis分别为光学系统调制传递函数、红外光电成像系统调制传递函数、光电转化电路调制传递函数和显示器调制传递函数;Where, MTF op , MTF det , MTF cic and MTF dis are the modulation transfer function of the optical system, the modulation transfer function of the infrared photoelectric imaging system, the modulation transfer function of the photoelectric conversion circuit and the modulation transfer function of the display, respectively; 式中,f为空间频率,σ为显示的均方根噪声,L为显示器亮度,α是关于噪声对亮度的校正因子;Where f is the spatial frequency, σ is the displayed RMS noise, L is the display brightness, and α is the correction factor for noise to brightness; b=0.3(1+100/L)0.15,b=0.3(1+100/L) 0.15 , c=0.06,c=0.06, 式中,θ为表现目标角,Atgt为目标面积,M为系统放大倍数,R为目标与红外光电成像系统之间的距离;Where θ is the target angle, Atgt is the target area, M is the system magnification, and R is the distance between the target and the infrared optoelectronic imaging system; 步骤7,以目标背景对比度Ctgt超过系统对比度阈值函数CTFsys的空间频率进行加权积分取代约翰逊准则中的极限空间频率,计算目标任务性能TTP,获取目标图像信息量;Step 7, replace the limit spatial frequency in the Johnson criterion with the spatial frequency at which the target background contrast C tgt exceeds the system contrast threshold function CTF sys by weighted integration, calculate the target task performance TTP, and obtain the target image information; 式中:ξhigh和ξlow为空间频率的上下限,ξhigh为系统对比度阈值函数CTFsys和目标背景对比度Ctgt的交点对应的空间频率值,ξlow取为0;单位为cyc/mrad。In the formula: ξ high and ξ low are the upper and lower limits of the spatial frequency, ξ high is the spatial frequency value corresponding to the intersection of the system contrast threshold function CTF sys and the target background contrast C tgt , and ξ low is taken as 0; the unit is cyc/mrad. 步骤8,根据目标观测距离和目标的临界特征尺寸,计算目标在对应观测距离下的目标任务等效周期数,Step 8: Calculate the target mission equivalent cycle number of the target at the corresponding observation distance according to the target observation distance and the critical characteristic size of the target. 所述目标任务等效周期数为 The target task equivalent cycle number is 所述目标的临界特征尺寸通过对目标面积Atgt开方得到;The critical characteristic size of the target is obtained by taking the square root of the target area A tgt ; 步骤9,利用50%的点落在目标任务性能曲线TTP的目标传递概率函数计算得到动目标探测概率P;Step 9, using the target transfer probability function where 50% of the points fall on the target task performance curve TTP, the moving target detection probability P is calculated; E=1.51+0.24(V/V50),E=1.51+0.24(V/V 50 ), 其中,E为目标探测任务等级;V50是完成任务概率为50%的可分辨周期数,由实验测量得到;V为目标任务等效周期数。Where E is the target detection task level; V50 is the number of resolvable cycles with a task completion probability of 50%, which is obtained by experimental measurement; and V is the number of equivalent cycles of the target task. 2.根据权利要求1所述红外光电成像系统动目标探测性能评估方法,其特征在于,所述步骤2包括以下步骤:2. According to the method for evaluating the moving target detection performance of the infrared optoelectronic imaging system of claim 1, it is characterized in that the step 2 comprises the following steps: 步骤2.1,设置标准黑体源的温度,通过辐射测量计采集目标及背景的黑体等效温度;Step 2.1, set the temperature of the standard blackbody source, and collect the blackbody equivalent temperature of the target and background through the radiometer; 步骤2.2,设定可移动小车运动速度、运动轨迹和探测距离,小车运动时连续采集目标的红外成像特征;Step 2.2, setting the moving speed, moving trajectory and detection distance of the movable car, and continuously collecting the infrared imaging characteristics of the target when the car moves; 步骤2.3,调节标准黑体源温度,重复执行步骤2.1-步骤2.2,得到标准黑体源不同温度下的测量参数。Step 2.3, adjust the temperature of the standard blackbody source, repeat steps 2.1-2.2, and obtain the measurement parameters of the standard blackbody source at different temperatures. 3.根据权利要求1所述红外光电成像系统动目标探测性能评估方法,其特征在于,所述步骤3包括以下步骤:3. According to the method for evaluating the moving target detection performance of the infrared optoelectronic imaging system of claim 1, it is characterized in that the step 3 comprises the following steps: 步骤3.1,固定红外光电成像系统位置和目标的高度不变,等距离调节辐射测量计到目标的距离,采集不同探测距离下目标本征温度;Step 3.1, fix the position of the infrared photoelectric imaging system and the height of the target, adjust the distance from the radiometer to the target at equal distances, and collect the intrinsic temperature of the target at different detection distances; 步骤3.2,将温度与目标本征温度等效的黑体放置于不同位置,测量黑体在红外光电成像系统的辐射亮度,并通过普朗克公式计算黑体辐射亮度值,以目标本体辐射亮度值与黑体辐射亮度值的比值作为对应探测距离下的大气透过率;Step 3.2, place a black body with a temperature equivalent to the intrinsic temperature of the target at different positions, measure the radiation brightness of the black body in the infrared photoelectric imaging system, and calculate the black body radiation brightness value by Planck's formula, and take the ratio of the target body radiation brightness value to the black body radiation brightness value as the atmospheric transmittance at the corresponding detection distance; 步骤3.3,根据步骤3.2得到的不同探测距离下的大气透过率,得到探测距离与大气透过率的关系曲线τ(R)。Step 3.3, according to the atmospheric transmittance at different detection distances obtained in step 3.2, obtain a relationship curve τ(R) between the detection distance and the atmospheric transmittance. 4.根据权利要求3所述红外光电成像系统动目标探测性能评估方法,其特征在于,所述步骤3.1中,以1米为间隔距离,等间距调节辐射测量计到目标的距离。4. The method for evaluating the moving target detection performance of an infrared optoelectronic imaging system according to claim 3 is characterized in that in step 3.1, the distance from the radiation meter to the target is adjusted at equal intervals with an interval of 1 meter. 5.根据权利要求1所述红外光电成像系统动目标探测性能评估方法,其特征在于,所述步骤5中,目标辐射出射度MT和背景辐射出射度MB根据以下公式式计算得到:5. The method for evaluating the moving target detection performance of an infrared optoelectronic imaging system according to claim 1, characterized in that in step 5, the target radiation emittance MT and the background radiation emittance MB are calculated according to the following formula: 所述目标辐射出射度MT计算公式为:The target radiation emittance MT calculation formula is: 所述背景辐射出射度MB计算公式为:The background radiation emittance MB calculation formula is: 式中,C1为第一辐射常数,C1=(3.7415±0.0003)×108(W·μm4·m-2);λ1和λ2为红外光电成像系统光谱范围的上下限;Wherein, C 1 is the first radiation constant, C 1 =(3.7415±0.0003)×10 8 (W·μm 4 ·m -2 ); λ 1 and λ 2 are the upper and lower limits of the spectral range of the infrared optoelectronic imaging system; C2为第二辐射常数,C2=(1.43879±0.00019)×104(μm·K);TT为目标温度,TB为背景温度,单位为K;ε(λB)和ε(λT)分别为背景光谱发射率和目标光谱发射率。C 2 is the second radiation constant, C 2 =(1.43879±0.00019)×10 4 (μm·K); TT is the target temperature, TB is the background temperature, the unit is K; ε(λB) and ε(λT) are the background spectral emissivity and the target spectral emissivity, respectively.
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