基于蒙特卡洛法旋翼飞行器红外辐射特性研究

Study on infrared radiation characteristics of rotorcraft based on Monte Carlo method

  • 摘要: 小型旋翼飞行器的广泛使用给高价值目标安全带来了全新挑战。为了有效探测与防御小型旋翼飞行器,研究小型旋翼飞行器红外辐射的空间分布特性具有重要意义。首先,针对某小型旋翼飞行器,建立了飞行器的几何模型,并对模型进行非结构化网格划分,生成面网格,确定每个面网格的面积和方向矢量;其次,分别对静态、空载飞行10 min和挂载100 g载荷飞行10 min三种工况条件下的旋翼飞行器,进行了温度测量和红外辐射图像采集;最后,基于蒙特卡洛法,考虑辐射网格单元对光束的吸收和反射,计算了旋翼飞行器在不同工况条件下不同探测方向的中远红外辐射强度分布及其规律。测试与计算结果表明,旋翼电机和电池是飞行器的主要红外辐射源;旋翼飞行器飞行时间越长,载荷越大,其红外辐射就越强;在天顶角θ为78°、101°和160°左右方向上,旋翼飞行器的辐射强度呈现峰值,而在天顶角θ为0°、90°和180°方向上,辐射强度较小;旋翼飞行器辐射主要集中在长波红外波段。

     

    Abstract:
    Objective  The wide use of small rotorcraft brings new challenges to the safety of high-value targets. At present, there are many researches on the infrared radiation characteristics of fixed-wing aircraft. The optical characteristics of rotorcraft are mainly reflected in infrared/visible light fusion and infrared small target detection, etc. However, there are few theoretical studies on the characteristics of temperature distribution, infrared radiation spectrum and space distribution of rotorcraft. In order to detect and defend small rotorcraft effectively, it is of great significance to study the spatial distribution characteristics of infrared radiation of small rotorcraft.
    Methods  In order to accurately grasp the infrared radiation characteristics of rotorcraft, firstly the geometric model of a small rotorcraft is established (Fig.1), and the model is divided into unstructured grids to generate surface grids (Fig.2), and the area and direction vector of each surface grid are determined. Secondly, temperature measurement and infrared radiation image acquisition are carried out for the rotorcraft at stationary, no-load flight for 10 min and 100 g load flight for 10 min respectively (Fig.3). Finally, based on the Monte Carlo method (Fig.5), and the absorption and reflection of light beams by radiation grid elements are considered, the distribution and law of the middle and far infrared radiation intensity of the rotorcraft under different working conditions and different detection directions are calculated.
    Results and Discussions  According to three different working conditions, the spatial distribution of infrared radiation intensity of the rotorcraft in the band of 3-5 μm and 8-14 μm is calculated (Fig.6). At the zenith angles θ of 78°, 101°, and 160°, the radiation intensity of the rotorcraft presents the peak value. The peak value is the highest at about 78°, and the maximum values are 1.13, 1.28, 1.35 W/sr respectively. When the zenith angle θ is 0°, 90° and 180, the radiation intensity is small. In the horizontal direction, when the circumferential angle φ is about 90° and 270°, the radiation intensity of the rotorcraft is relatively strong. The infrared radiation intensity distribution curve of the rotorcraft at stationary and 100 g load flight for 10 min is compared and analyzed (Fig.7-8). When φ is 90°, the radiation intensity of the band 3-5 μm increased by about 56.1%, and the radiation intensity of the band 8-14 μm increased by about 19.5%. When θ is 78.3°, the radiation intensity of 3-5 μm increases by about 53.7%, and the radiation intensity of 8-14 μm band increases by about 19.5%. It can be seen that a longer flight time and a heavier load will significantly enhance the infrared radiation of the rotorcraft.
    Conclusions  The geometric model of a small rotorcraft is established, and the flight and data collection of the rotorcraft are carried out to obtain the temperature field distribution data of the surface of the rotorcraft. On this basis, Monte Carlo method is used to simulate the radiation transfer process of rays, and the middle and far infrared radiation intensity distribution of the rotorcraft in different detection directions under different working conditions is obtained, and the following conclusions are drawn. The rotor motor and battery is the main infrared radiation source of rotor vehicle; The longer the flight time of the rotorcraft, the larger the load, the larger the output power of the motor and battery, the more waste heat will be released, and the stronger the infrared radiation of the rotorcraft; When the zenith angle θ is 78°, 101° and 160°, the radiation intensity of the rotorcraft shows the peak value, while when the zenith angle θ is 0°, 90° and 180 °, the radiation intensity is small. The radiation intensity of small rotorcraft in 3-5 μm band is about 0.05 W/Sr, and that in 8-14 μm band is about 0.8 W/sr. The radiation intensity of rotorcraft is mainly concentrated in long-wave infrared band.

     

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