高超声速巡航导弹蒙皮红外辐射特性

Infrared radiation characteristics of hypersonic cruise missile scarfskin

  • 摘要: 高超声速巡航导弹经气动加热,蒙皮具有较高的温度,可产生强烈的红外辐射。为了对高超声速巡航导弹进行有效探测和预警,研究高超声速巡航导弹红外辐射的空间分布特性具有重要意义。首先,以类X-51A高超声速巡航导弹为研究对象,利用软件SpaceClaim建立高超声速巡航导弹的几何模型。其次,基于流体力学基本守恒定律,利用Fluent软件对高超声速巡航导弹外流场进行数值模拟,获得导弹蒙皮温度和绕流场压强等分布数据。最后,采用蒙特卡罗法对射线的辐射传递过程进行概率模拟计算,得到类X-51A飞行器在典型飞行工况下的中远红外强度空间分布。结果表明:高超声速巡航导弹头部和进气道前段温度较高,当飞行速度分别为5 Ma和6 Ma时,蒙皮最高温度分别可达1 177.304 K和1 654.08 K,且随着飞行速度的增加,蒙皮中红外辐射强度占比越来越大,在α=78.75°方向,蒙皮红外辐射达到最强,对于5 Ma而言,中、远红外辐射强度分别可以达到1.66×104 W/sr和6.0×103 W/sr,而在迎头或者尾向,其红外辐射强度要弱一些。

     

    Abstract: The hypersonic cruise missile undergoes aerodynamic heating, and the scarfskin has a high temperature, generating strong infrared radiation. In order to detect and warn hypersonic cruise missile effectively, it is important to study the spatial distribution characteristics of infrared radiation of hypersonic cruise missile. Firstly, taking X-51A hypersonic cruise missile as the research object, the geometric model of hypersonic cruise missile was established by using software SpaceClaim. Secondly, based on the basic conservation law of hydrodynamics, Fluent software was used to numerically simulate the hypersonic cruise missile's outflow field, and the distribution data such as the missile scarfskin temperature and the pressure around the flow field were obtained. Finally, Monte Carlo method was used to simulate the process of radiation transfer, and the space distribution of middle and far infrared intensity of X-51A aircraft under typical flight conditions was obtained. The results show that the temperature at the head and front section of the inlet of hypersonic cruise missiles is relatively high. At flight speeds of 5 Ma and 6 Ma, the maximum temperature of the skin reaches 1177.304 K and 1654.08 K, respectively. As the flight speed increases, the proportion of infrared radiation intensity in the skin increases. In the direction of α=78.75°, the infrared radiation intensity of the skin reaches its strongest. For 5 Ma, the infrared radiation intensity in the middle and far reaches 1.66×104 W/sr and 6.0×103 W/sr, respectively. However, in the head-on or tail direction, the infrared radiation intensity is weaker.

     

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