4.2.1   动力弹塑性的运动方程
区分 版本 / Revision No. 改善建议者 改善内容 内容列表
产品功能 Ver.112 R3 / No.2009-03
手册内容 Ver.110 R2 / No.2009-02

 
技术原理

包含了非线性构件(分配了铰特性的构件)的运动方程如下:

                                                                                                                         (4.2.1-1)

 式中:

                         M — 质量矩阵;

                          C — 阻尼矩阵;

                    Q(ut) — 弹塑性恢复力;

 — 在时间 时的各节点的加速度、速度、位移;

                          Rt — 节点上的动力荷载。

 

动力弹塑性分析属于非线性分析不能使用振型叠加法,程序提供Newmark-β直接积分方法。根据Newmark-β法的基本假定,使用t时刻的加速度、速度和位移表现t+Δt时刻的速度和加速度如下:

 

                                                                                                                       (4.2.1-2)

 

                                                                                      (4.2.1-3)

 

可重新整理上面公式如下:

 

                                                                                    (4.2.1-4)

 

                                                                                                      (4.2.1-5)

 

位移、速度、加速度增量为:

 

                                                                                                                                                                        (4.2.1-6)

 

                                                                                                              (4.2.1-7)

 

                                                                                                                         (4.2.1-8)

 

使用完全牛顿-拉普森计算的迭代增量为:

 

                                                                                                                                    (4.2.1-9)

 

                                                                                                                                (4.2.1-10)

 

因此在时间t+Δt时的第(i)次迭代计算时的位移、速度、加速度为:

 

                                                                                                                                                         (4.2.1-11)

 

                                                                                                 (4.2.1-12)

 

                                                                                         (4.2.1-13)

 

在时间t+Δt时的第(i)次迭代计算时的非线性运动方程如下:

 

                                                                                                                         (4.2.1-14)

 

将(4.2.1-12)和(4.2.1-13)代入(4.2.1-14)可得对于位移增量δu(i)的平衡方程:

 

                                                                                                                                                                      (4.2.1-15)

 

式中:

                         KEff — 有效刚度矩阵;

                       ΔPEff — 各迭代计算中的有效荷载向量;

                   K(i)t+Δt — 包含非线性单元的切线刚度矩阵;

 

                          δu(i)— 各迭代计算中的位移增量向量;

                               β Newmark法时间积分参数。

 

                                                                                                                         (4.2.1-16)

 

                                                                                       (4.2.1-17)

 

 

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动力弹塑性分析的一键式操作方法