Research on MDOE methods based on response surface optimization model with adaptive genetic algorithm
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摘要:
多项式响应面模型(PRSM)具有建模简单、计算量较小的特点,在基于现代试验设计(MDOE)方法的风洞试验中得到广泛应用。然而,多项式响应面模型无法对模型拟合后的残差进行处理,会丢失部分模型矩阵信息而导致参数预测误差增加。因此,通过预测值和实测值的差值,构造模型残差目标函数,并根据轮盘赌计算个体适应度值,对遗传算法(GA)的交叉概率和变异概率进行改进,建立一种基于改进自适应遗传算法(IAGA)优化多项式响应面模型的MDOE方法,并应用于飞行器风洞试验。结果表明:MDOE方法仅需传统单变量(OFAT)方法35%左右的试验点,基于改进自适应遗传算法优化后的MDOE方法较基于传统遗传算法的MDOE方法,响应面模型预测误差降低了1.263%,平均迭代速度提高了3.76倍,有效提升风洞试验效率。
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关键词:
- 现代试验设计(MDOE)方法 /
- 多项式响应面模型(PRSM) /
- 遗传算法(GA) /
- 风洞试验 /
- 气动系数
Abstract:The polynomial response surface model (PRSM) was characterized by its simplicity in modeling and low computational cost, making it widely used in wind tunnel tests based on the modern design of experiments (MDOE) method. However, PRSM cannot process residuals after model fitting, leading to a loss of some model matrix information and increased parameter prediction error. To address this, a residual objective function based on the difference between predicted and measured values was constructed. Then, the crossover and mutation probabilities of the genetic algorithm (GA) were improved by calculating individual fitness values using a roulette wheel selection method. This contributed to the establishment of an MDOE method optimized by an improved adaptive genetic algorithm (IAGA) for PRSM, which was applied to aircraft wind tunnel tests. The results showed that the MDOE method required only about 35% of the experimental points needed by the one factor according to OFAT method. Compared with the traditional GA-based MDOE method, the IAGA-based MDOE method decreased the prediction error of the response surface model by 1.263% and increased the average iteration speed by 3.76 times, which effectively improved the efficiency of wind tunnel tests.
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表 1 待定系数与模型形式关系表
Table 1. Relationships between undetermined coefficients and model forms
多项式响应面模型形式 待定系数个数 一元二次多项式 3 二元三次多项式 10 三元四次多项式 35 四元五次多项式 126 表 2 OFAT方法所取的自变量及试验值
Table 2. Variables and experiment values by OFAT method
自变量 试验值 风速V/(m/s) 5,8,10,12,15,20,25 迎角α/(°) −6,−4,−2,0,2,4,6 表 3 阻力系数响应面模型插值数据对比
Table 3. Comparison of interpolation data for drag coefficient response surface model
序号 迎角/(°) 风速/(m/s) OFAT方法
阻力系数GA-MDOE方法 IAGA-MDOE方法 阻力系数 相对误差/% 阻力系数 相对误差/% 1 −6 5 − 0.09298 − 0.09468 1.828 − 0.09361 0.678 2 −6 25 − 1.35134 − 1.37615 1.836 − 1.36049 0.677 3 −2 5 − 0.08756 − 0.08918 1.850 − 0.08816 0.685 4 2 8 − 0.16701 − 0.17007 1.832 − 0.16814 0.677 5 4 18 − 0.63941 − 0.65111 1.830 − 0.64372 0.674 6 6 12 − 0.27897 − 0.28409 1.835 − 0.28086 0.677 7 6 25 −1.127 − 1.14765 1.836 − 1.13459 0.677 表 4 垂向力系数响应面模型插值数据对比
Table 4. Comparison of interpolation data for vertical force coefficient response surface model
序号 迎角/(°) 风速/(m/s) OFAT方法
垂向力系数GA-MDOE方法 IAGA-MDOE方法 垂向力系数 相对误差/% 垂向力系数 相对误差/% 1 −6 5 0.05699 0.058 1.772 0.0574 0.719 2 −6 25 1.1805 1.20088 1.726 1.18797 0.633 3 −2 5 0.05553 0.0565 1.747 0.05585 0.576 4 2 8 0.25867 0.26311 1.716 0.26031 0.634 5 4 18 1.51499 1.54103 1.719 1.52453 0.630 6 6 12 0.70202 0.71413 1.725 0.70643 0.628 7 6 25 3.23964 3.29514 1.713 3.25988 0.625 表 5 滚转力矩系数响应面模型插值数据对比
Table 5. Comparison of interpolation data for rolling moment coefficient response surface model
序号 迎角/(°) 风速/(m/s) OFAT方法
滚转力矩系数GA-MDOE方法 IAGA-MDOE方法 滚转力矩系数 相对误差/% 滚转力矩系数 相对误差/% 1 −6 5 0.05267 0.05349 1.557 0.05304 0.702 2 −6 25 − 0.0199 − 0.02021 1.558 − 0.02004 0.704 3 −2 5 0.00846 0.0086 1.655 0.00852 0.709 4 2 8 − 0.00635 − 0.00645 1.575 − 0.0064 0.787 5 4 18 − 0.0408 − 0.04144 1.569 − 0.04109 0.711 6 6 12 0.08562 0.08694 1.542 0.08622 0.701 7 6 25 − 0.01384 − 0.01405 1.517 − 0.01394 0.723 表 6 俯仰力矩系数响应面模型插值数据对比
Table 6. Comparison of interpolation data for pitching moment coefficient response surface model
序号 迎角/(°) 风速/(m/s) OFAT方法
俯仰力矩系数GA-MDOE方法 IAGA-MDOE方法 俯仰力矩系数 相对误差/% 俯仰力矩系数 相对误差/% 1 −6 5 0.0066 0.00672 1.818 0.00665 0.758 2 −6 25 − 0.30989 − 0.31538 1.772 − 0.31184 0.629 3 −2 5 0.00836 0.00851 1.794 0.00841 0.598 4 2 8 − 0.00539 − 0.00548 1.670 − 0.00542 0.557 5 4 18 0.05038 − 0.05128 1.786 − 0.0507 0.635 6 6 12 − 0.00396 − 0.00403 1.768 − 0.00398 0.505 7 6 25 − 0.01989 − 0.02025 1.810 − 0.02002 0.654 -
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