Abstract

Although many families of integration methods have been successfully developed with desired numerical properties, such as second order accuracy, unconditional stability and numerical dissipation, they are generally implicit methods. Thus, an iterative procedure is often involved for each time step in conducting time integration. Many computational efforts will be consumed by implicit methods when compared to explicit methods. In general, the structure-dependent integration methods (SDIMs) are very computationally efficient for solving a general structural dynamic problem. A new family of SDIM is proposed. It exhibits the desired numerical properties of second order accuracy, unconditional stability, explicit formulation and no overshoot. The numerical properties are controlled by a single free parameter. The proposed family method generally has no adverse disadvantage of unusual overshoot in high frequency transient responses that have been found in the currently available implicit integration methods, such as the WBZ-α method, HHT-α method and generalized-α method. Although this family method has unconditional stability for the linear elastic and stiffness softening systems, it becomes conditionally stable for stiffness hardening systems. This can be controlled by a stability amplification factor and its unconditional stability is successfully extended to stiffness hardening systems. The computational efficiency of the proposed method proves that engineers can do the accurate nonlinear analysis very quickly.

Highlights

  • A step-by-step integration method is one of the most effective ways to obtain the responses of the system subject to dynamic loads, such as explosions, blasts and wave propagations, especially earthquake loads

  • The numerical examples are conducted and the results show that a stability amplification factor extended the unconditional stability range of the proposed method to the nonlinear stiffness hardening systems

  • A parameter instantaneous degree of step nonintroduced. It is defined as a ratio of the stiffness at the end of the i-th time linearity is introduced. Fact, it isbedefined as aas ratio of the stiffness at the end of the i -th over the initial stiffness, In and it can expressed time step over the initial stiffness, and it can be expressed as k ki δδi i= =i,k, (18)

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Summary

Introduction

A step-by-step integration method is one of the most effective ways to obtain the responses of the system subject to dynamic loads, such as explosions, blasts and wave propagations, especially earthquake loads. The currently available implicit algorithms, such as the generalized-α method, HHT-α method and WBZ-α method, have the disadvantage of unusual overshoot behavior in high frequency transient responses. These properties preclude them from practical applications. Chang proposed different families of explicit, dissipative algorithms, that generally have uncommon high frequency overshoot behavior [22,23]. The proposed explicit SDIM does not have an unusual overshoot property in both high frequency displacement and velocity responses. There is no unusual overshoot behavior in the proposed family method for the high frequency responses in both displacement and velocity. This method, which is computationally efficient for solving a new series of mass spring system, proves that engineers can perform fast computation with maximum accuracy

Chang–Veerarajan Method
Recursive Matrix Form
Convergence
Consistency and LTE
Stability
Primary Analysis for the Nonlinear System
The Stability Amplification Factor
Numerical
Spectral Radius
Relative Period Error
Overshooting
Numerical Example
Forced Vibration Nonlinear SDOF System with Damping
Free Vibration Responses of an Eight-Storey Building
Forced
Seismic Responses of the Eight-Storey Hardening System
Conclusions
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