Track Irregularity Spectrum of High-Temperature Superconducting Maglev Permanent Magnet Considering Structural Periodicity
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摘要:
为给高温超导钉扎磁浮系统提供较为符合实际的几何不平顺轨道谱,开展考虑结构周期性的高温超导磁浮永磁轨道不平顺谱研究. 为实现包含结构周期性的永磁轨道不平顺谱表征和反演,首先建立高温超导磁浮桥梁、永磁轨道有限元模型,对其施加磁浮列车移动荷载获取最不利荷载作用位置并提取该点位移作为动态不平顺;其次,考虑桥梁徐变上拱造成的永磁轨道变形,叠加列车荷载下周期性动态不平顺结果形成轨道周期性不平顺样本;进一步,考虑永磁轨道拼装随机误差,基于白噪声滤波法得到永磁轨道随机几何不平顺样本,与周期性不平顺叠加,形成永磁轨道不平顺谱;采用4阶多项式和洛伦兹函数对永磁轨道不平顺谱进行拟合,并基于逆傅里叶变换反演拟合谱,以检验拟合算法的有效性;最后,分析列车速度变化对永磁轨道不平顺拟合谱的影响. 结果表明:列车荷载速度变化对永磁轨道不平顺谱的影响主要集中在波长3~100 m范围内;当速度接近与桥梁共振的临界速度时,永磁轨道拟合谱反演不平顺幅值变化较为显著. 本文得到的不平顺谱可方便地应用于高温超导磁浮车辆动力学计算中,为不同速度等级高温超导磁浮列车动力学分析与设计优化提供输入.
Abstract:To provide a more realistic geometric irregularity spectrum for high-temperature superconducting (HTS) pinning-type maglev systems, the irregularity spectrum of permanent magnet (PM) tracks considering structural periodicity was investigated. To achieve the characterization and inversion of the PM track irregularity spectrum that incorporates structural periodicity, a finite element model of an HTS maglev bridge and its PM track was first built. Moving loads from a maglev train were then applied to the model to identify the most unfavorable loading position, and the displacement at this point was extracted as the dynamic irregularity. Next, by considering the deformation of the PM track caused by bridge creep camber and superimposing the periodic dynamic irregularity results from train loads, a sample of periodic track irregularity was formed. Furthermore, random assembly errors of the PM track were modeled using a white noise filtering method to obtain a sample of random geometric irregularity. This was then superimposed with the periodic irregularity to form the overall PM track irregularity spectrum. The irregularity spectrum was fitted using a 4th-order polynomial and a Lorentzian function, and the fitted spectrum was inversely transformed via the inverse Fourier transform to verify the effectiveness of the fitting method. Finally, the influence of train speed on the fitted irregularity spectrum was analyzed. The results show that train speed mainly affects the PM track irregularity spectrum in the wavelength range of 3–100 m; when the speed approaches the critical resonance speed of the bridge, the amplitude of the inverse-transformed irregularity becomes significantly larger. The irregularity spectrum obtained in this study can be readily applied in the dynamics calculations of HTS maglev vehicles, serving as input for the dynamic analysis and design optimization of HTS maglev trains operating at various speed levels.
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表 1 模型材料参数取值
Table 1. Model material parameter values
构件名称 物理量 数值 永磁轨道 弹性模量/Pa 2×1011 密度/( kg•m−3) 7850 泊松比 0.3 轨道板 混凝土等级 C60 弹性模量/Pa 3.65×1010 密度/( kg•m−3) 2500 泊松比 0.2 轨道梁 混凝土等级 C40 弹性模量/Pa 3.3×1010 密度/( kg•m−3) 2500 泊松比 0.2 桥墩 混凝土等级 C40 弹性模量/Pa 3.3×1010 密度/( kg•m−3) 2500 泊松比 0.2 支座 刚度/( N·m−1) 4×1010 阻尼/(N·s·m−1) 1.2×105 表 2 4阶多项式拟合参数
Table 2. 4th order polynomial fitting parameters
参数 a0 a1 a2 a3 a4 拟合值 − 0.6289 0.6996 2.5598 1.5480 0.3580 表 3 周期性谱峰拟合参数值
Table 3. Periodic spectral peak fitting parameter values
谱峰 $\varphi $ $\gamma $ 1 300.0 0.00059 2 208.0 0.00058 3 88.0 0.00050 4 30.0 0.00040 表 4 不同速度谱峰拟合参数
Table 4. Fitting parameters of spectral peaks at different velocity
速度/(km•h−1) 谱峰 $ \varphi $ $\gamma $ 100 1 250.0 0.00060 2 80.0 0.00052 3 35.0 0.00051 4 3.5 0.00050 200 1 248.0 0.00060 2 75.0 0.00052 3 38.0 0.00051 4 4.0 0.00048 300 1 252.0 0.00059 2 78.0 0.00050 3 36.0 0.00049 4 3.8 0.00048 400 1 260.0 0.00059 2 80.0 0.00051 3 40.0 0.00050 4 4.2 0.00048 500 1 255.0 0.00060 2 81.0 0.00051 3 38.0 0.00050 4 5.0 0.00050 600 1 258.0 0.00061 2 80.0 0.00050 3 40.0 0.00050 4 4.6 0.00049 表 5 不同速度随机谱拟合参数
Table 5. Fitting parameters of random spectrum at different speed
速度/(km•h−1) a0 a1 a2 a3 a4 100 − 0.6289 0.6996 2.5598 1.5480 0.3580 200 − 0.6287 0.6971 2.5462 1.5477 0.3610 300 − 0.6276 0.7239 2.6614 1.6748 0.3991 400 − 0.6286 0.7127 2.6354 1.6913 0.4134 500 − 0.6302 0.6893 2.5677 1.6524 0.4081 600 − 0.6287 0.7073 2.6156 1.6864 0.4140 -
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