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中国物理学会期刊

基于元胞自动机的气动光学光线追迹算法

CSTR: 32037.14.aps.69.20200532

Cellular automata ray tracing in two-dimensional aero-optical flow fields

CSTR: 32037.14.aps.69.20200532
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  • 对于含激波等大密度脉动结构气动光学流场, 沿着直线路径对折射率积分会带来较大的光程误差. 因此, 数值求解光线方程进行光线追迹是必要的. 与数值求解光线方程不同, 元胞自动机(cellular automata, CA)通过给定光线位置和方向变换规则来模拟光线在介质中传输路径. 本文基于已有的实验测量、数值仿真所获得的高超声速流场密度场数据, 分别采用数值求解光线方程法和CA光线追迹算法进行光线追迹, 进而得到光线出射流场后的光程差. 结果表明, CA算法对于二维气动光学流场中光线追迹的适用性, 且较数值求解光线方程方法具有更高的效率.

     

    For the supersonic flow field with large density fluctuation produced by the unsteady flow and turbulent large-scale structures, an effective method to obtain the beam path is to solve the ray equation. Then the optical path difference (OPD), Strehl ratio (SR), optical transmission function (OTF), etc. can be obtained to analyze the optical distortion, and the correction of aero optics effects can be realized to improve the optical system performance. Generally, when the refractive index distribution is arbitrary, the ray equation analytic solution is difficult to obtain.
    Cellular automata (CA) ray tracing algorithm is proposed in this paper for aero-optical calculation in the 2D discrete flow fields. Unlike numerically solving the ray equation (NSRE), the coordinate value and the offset angle are calculated according to the position and direction transformation rules in CA algorithm. The position transformation rule is used to obtain the end point of the beam vector and determine whether the offset angle needs calculating at each iteration, the direction transformation rule is to calculate the offset angles. Then the refractive index field is integrated along the beam path to obtain the optical path length (OPL). The OPD is calculated from OPL. In this paper, aero-optical calculation is based on two types of flow fields. The supersonic shear layer including supersonic mixing layer and boundary layer 2D density distribution is measured by the nano-tracer-based planar laser scattering (NPLS) technique. The supersonic flow field surrounding the optical dome is simulated based on detached-eddy simulation (DES).
    The OPDrms and program running time quantitatively verify the calculation accuracy and high efficiency of CA. The results show that for the 2D supersonic NPLS flow field and the 2D supersonic flow field surrounding the optical dome, the calculation accuracy of CA is approximately equal to NSRE. Moreover, we find that the program running time of NSRE is about four times that of the CA algorithm, so the efficiency of ray tracing is effectively improved. Thus, the CA algorithm provides a new scheme for aero-optical calculation in the 2D supersonic flow field. Meanwhile, it also provides a guideline for the research on the ray tracing in 3D discrete aero-optical flow field.

     

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