58x
004102
2024-01-05

Main

The Main tab manages the specifications for the method and the time steps.

Time History Analysis Method Type

Two linear time history analysis methods are available for selection in the list in this dialog section (see image Defining Analysis Method and Time Steps):

  • Linear Modal
  • Linear Implicit Newmark

Both analysis methods are geometrically linear, so they are only valid for small deformations. Furthermore, all nonlinear properties of the model are either ignored (for example, the failure of a support is not considered) or replaced (a tension member is represented by a truss).

The linear modal analysis method uses a decoupled system that is based on the model's eigenvalues and mode shapes and is determined in the assigned Modal Analysis Load Case . The multi-degree-of-freedom system ("MDOF") is broken down into many single-degree-of-freedom systems ("SDOF") (diagonalized mass and stiffness matrix). A certain number of eigenvalues is required to ensure accuracy. The solution of the decoupled system is then determined with an implicit (Newmark) solver. The mass matrix settings and stiffness modifications are taken from the assigned modal analysis load case. If the eigenvalues have already been determined, this analysis method is slightly faster than the linear implicit Newmark analysis.

The linear implicit Newmark analysis is a direct time integration method. It requires sufficiently small time steps to achieve precise results. No natural vibration analysis is required for this analysis method. The theoretical background is explained in [1], for example.

Important

If you want to use members of the type Dashpot with defined damping coefficients, select the Linear Implicit Newmark analysis method.

Time Steps

Enter the 'Maximum time' tmax to be analyzed in the calculation. In the 'Saved time step' field, specify the interval Δt in which results are to be saved. Results will only be available for these time steps. The dynamic envelope is also generated from the saved time steps.

Info

Fewer saved time steps reduce the file size and the calculation time. They also have a positive effect on the evaluation of results. Nevertheless, a certain amount of result values is required so that the maximum is not skipped and to generate uniform gradients for the Calculation Diagrams.

In addition to the time steps that are saved, time steps must be defined for the actual calculation. To do this, enter a value in the 'Split saved time steps by' field by which the saved time steps Δt should be divided.

For a successful time history analysis, the time steps should be chosen "appropriately". In the end, the decision is a trade-off between calculation time and accuracy. The following recommendation can be made for the linear time history analysis (see [2]):

  • Taking into account the accelerogram and the transient time diagrams, the shortest length of the discrete excitation should be divided into at least seven time steps.
  • To calculate the time step, the highest frequency f of the model that is relevant for the system response should be used as follows: Δt ≤ 1 / (20f). Similarly, it should be checked whether the highest frequency of the excitation is covered in the condition Δt ≤ 𝜋 / (10ω). If this is not the case, the time step should be corrected.

References
  1. S.C. Chopra. Dynamics of Structures - Theory and Applications to Earthquake Engineering. Prentice Hall.
  2. U. Stelzmann, C. Groth und G. Müller. FEM für Praktiker - Band 2: Strukturdynamik. Expert Verlag, 2008.