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机构地区:[1]大连理工大学工程力学系,大连116023 [2]上海交通大学工程力学系,上海200030
出 处:《动力学与控制学报》2005年第2期1-9,共9页Journal of Dynamics and Control
基 金:国家自然科学基金(10372019);教育部博士点基金资助项目(20010141024)~~
摘 要:摄动法近似应当保辛.本文指出,有限元位移法自动保辛,有限元混合能表示也保辛.摄动法的刚度阵Taylor级数展开能证明保辛;混合能的Taylor级数展开摄动也证明了保辛.但传递辛矩阵的Taylor级数展开摄动却不能保辛.辛矩阵只能在乘法群下保辛,故传递辛矩阵的保辛摄动必须采用正则变换的乘法.虽然刚度阵加法摄动、混合能矩阵加法摄动与传递辛矩阵正则变换乘法摄动都保辛,但这3种摄动近似并不相同.最后通过数值例题给出了对比.The perturbation approximation should be symplectic conservative. The FEM displacement method is naturally symplectic conservative, the mixed energy representation is also shown symplectic conservative. The stiffness matrix, as well as the mixed energy matrix, perturbations based on the Taylor series expansion are all proved symplectic conservative. However, the Taylor series expansion perturbation for the symplectic transfer matrix is not able to reach symplectic conservative. The symplectic conservative perturbation for a transfer symplectic matrix should be based on the canonical transformation method. Although, the perturbation methods of the stiffness matrix, of the mixed energy matrix and of the transfer symplectic matrix multiplicative perturbation are all symplectic conservative, however, they are not identical. Therefore, numerical comparison is given for an example.
关 键 词:Taylor级数展开 数值比较 正则变换 辛矩阵 混合能 矩阵加法 摄动法 有限元 刚度阵 位移法 乘法群 传递 近似 证明
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