压电有限元分析中特征值问题的算法

Y. Yong, Y. Cho
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引用次数: 17

摘要

介绍了压电有限元分析中特征值问题的两种算法。第一种算法使用Lanczos特征求解器,第二种算法使用瑞利商迭代方案。在这两种解决方法中,都实现了减少存储需求和解决时间的方案。此外,两种解决方法都寻求保持刚度矩阵的稀疏结构,以实现内存的大量节省。在Lanczos求解方法中,利用一致质量矩阵的结构模式来节省内存和求解时间。在Rayleigh商迭代法中,采用了一种生成良好初始特征对的算法,显著提高了算法的整体收敛速度,以及在紧密间隔特征值区域和重复特征值区域的收敛稳定性。初始特征向量由粗网格插值得到。为了使这种迭代方法有效,精细网格中的特征向量必须与粗网格中的特征向量相似。因此,该方法对于寻找低频范围内的特征对集是有效的,而不是在高频范围内,在高频范围内,粗网格的特征向量与细网格的特征向量不太相似。算例结果表明,与使用静态凝聚法去除压电特征值问题的电势自由度的传统算法相比,所提算法在求解时间和存储需求上有所节省。这种传统方案的缺点是静态凝聚破坏了刚度矩阵的稀疏结构,从而导致内存和求解时间的大幅增加
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Algorithms for eigenvalue problems in piezoelectric finite element analyses
Two algorithms for eigenvalue problems in piezoelectric finite element analyses are introduced. The first algorithm involves the use a Lanczos eigensolver, while the second algorithm uses a Rayleigh quotient iteration scheme. In both solution methods, schemes are implemented to reduce storage requirements and solution time. Also, both solution methods seek to preserve the sparsity structure of the stiffness matrix to realize major savings in memory. In the Lanczos solution method, the structural pattern of the consistent mass matrix is exploited to gain savings in both memory and solution time. In the Rayleigh quotient iteration method, an algorithm for generating good initial eigenpairs is employed to improve significantly its overall convergence rate, and convergence stability in the regions of closely spaced eigenvalues and repeated eigenvalues. The initial eigenvectors are obtained by interpolation from a coarse mesh. In order for this iterative method to be effective, an eigenvector of interest in the fine mesh must resemble an eigenvector in the coarse mesh. Hence, the method is effective for finding the set of eigenpairs in the low frequency range, and not in the high frequency range where the eigenvectors of the coarse mesh does not resemble well their counterparts in the fine mesh. Results of example problems are presented to show the savings in solution time and storage requirements of the proposed algorithms when compared with the conventional algorithm which uses static condensation to remove the electric potential degrees of freedom from the piezoelectric eigenvalue problem. The disadvantage of this conventional scheme is that the static condensation destroys the sparsity structure of the stiffness matrix, which leads to major increases in memory and solution time
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